Changeset 5257
- Timestamp:
- Apr 1, 2022 8:14:22 AM (12 months ago)
- Location:
- trunk
- Files:
-
- 5 edited
Legend:
- Unmodified
- Added
- Removed
-
trunk/GSASIIimgGUI.py
r5175 r5257 205 205 G2frame.ImageZ = GetImageZ(G2frame,data) 206 206 mainSizer = G2frame.dataWindow.GetSizer() 207 mainSizer.Add(wx.StaticText(G2frame.dataWindow, 208 label='Do not change anything here unless you are absolutely sure!'),0) 207 topSizer = wx.BoxSizer(wx.HORIZONTAL) 208 topSizer.Add(wx.StaticText(G2frame.dataWindow,label=' Do not change anything here unless you are absolutely sure!'),0) 209 topSizer.Add((-1,-1),1,wx.EXPAND) 210 topSizer.Add(G2G.HelpButton(G2frame.dataWindow,helpIndex=G2frame.dataWindow.helpKey)) 211 mainSizer.Add(topSizer,0,wx.EXPAND) 209 212 mainSizer.Add(wx.StaticText(G2frame.dataWindow,label=' Image size: %d by %d'%(data['size'][0],data['size'][1])),0) 210 213 pixSize = wx.FlexGridSizer(0,4,5,5) … … 1647 1650 G2frame.Bind(wx.EVT_MENU, OnIntPDFtool, id=G2G.wxID_IMINTEGPDFTOOL) 1648 1651 1649 mainSizer = G2frame.dataWindow.GetSizer() 1652 mainSizer = G2frame.dataWindow.GetSizer() 1653 topSizer = wx.BoxSizer(wx.HORIZONTAL) 1654 topSizer.Add(wx.StaticText(G2frame.dataWindow,label=' Image Controls:')) 1655 topSizer.Add((-1,-1),1,wx.EXPAND) 1656 topSizer.Add(G2G.HelpButton(G2frame.dataWindow,helpIndex=G2frame.dataWindow.helpKey)) 1657 mainSizer.Add(topSizer,0,wx.EXPAND) 1650 1658 mainSizer.Add((5,10),0) 1651 1659 mainSizer.Add(ComboSizer(),0,wx.ALIGN_LEFT) … … 2082 2090 G2frame.GetStatusBar().SetStatusText("To add mask: press a,r,s,x,y,p or f on 2D image for arc/ring/spot/xline/yline/polygon/frame",1) 2083 2091 mainSizer = G2frame.dataWindow.GetSizer() 2092 topSizer = wx.BoxSizer(wx.HORIZONTAL) 2093 topSizer.Add(wx.StaticText(G2frame.dataWindow,label=' Mask Controls:')) 2094 topSizer.Add((-1,-1),1,wx.EXPAND) 2095 topSizer.Add(G2G.HelpButton(G2frame.dataWindow,helpIndex=G2frame.dataWindow.helpKey)) 2096 mainSizer.Add(topSizer,0,wx.EXPAND) 2084 2097 mainSizer.Add((5,10),0) 2085 2098 … … 2671 2684 2672 2685 mainSizer = G2frame.dataWindow.GetSizer() 2686 topSizer = wx.BoxSizer(wx.HORIZONTAL) 2687 topSizer.Add(wx.StaticText(G2frame.dataWindow,label=' Stress/Strain Controls:')) 2688 topSizer.Add((-1,-1),1,wx.EXPAND) 2689 topSizer.Add(G2G.HelpButton(G2frame.dataWindow,helpIndex=G2frame.dataWindow.helpKey)) 2690 mainSizer.Add(topSizer,0,wx.EXPAND) 2673 2691 mainSizer.Add((5,10),0) 2674 2692 mainSizer.Add(SamSizer()) -
trunk/GSASIIphsGUI.py
r5250 r5257 13302 13302 # FillPawleyReflectionsGrid executable starts here 13303 13303 G2frame.GetStatusBar().SetStatusText('To delete a Pawley reflection: select row & press Delete',1) 13304 oldSizer = PawleyRefList.GetSizer()13305 if oldSizer: oldSizer.Clear()13304 # oldSizer = PawleyRefList.GetSizer() 13305 # if oldSizer: oldSizer.Clear(True) 13306 13306 generalData = data['General'] 13307 13307 PawleyPeaks = data['Pawley ref'] 13308 if len(PawleyPeaks) == 0 or not generalData['doPawley']: 13309 msg = ('Pawley refinement not yet set up. Use the "Pawley setup"'+ 13310 ' and "Pawley create" menu commands to change this. '+ 13311 '(Note settings also found on General tab).') 13312 if not generalData['doPawley']: 13313 msg += '\n\nCall Pawley setup?' 13314 else: 13315 msg += '\n\nCall Pawley create?' 13316 dlg = wx.MessageDialog(G2frame,msg,'Pawley not setup', 13317 wx.YES_NO | wx.ICON_QUESTION) 13318 try: 13319 dlg.CenterOnParent() 13320 result = dlg.ShowModal() 13321 if result == wx.ID_YES and not generalData['doPawley']: 13322 wx.CallAfter(OnPawleySet,None) 13323 elif result == wx.ID_YES: 13324 wx.CallAfter(OnPawleyLoad,None) 13325 finally: 13326 dlg.Destroy() 13327 rowLabels = [] 13328 for i in range(len(PawleyPeaks)): rowLabels.append(str(i)) 13329 if generalData['Modulated']: 13330 colLabels = ['h','k','l','m','mul','d','refine','Fsq(hkl)','sig(Fsq)'] 13331 Types = 5*[wg.GRID_VALUE_LONG,]+[wg.GRID_VALUE_FLOAT+':10,4',wg.GRID_VALUE_BOOL,]+ \ 13332 2*[wg.GRID_VALUE_FLOAT+':10,2',] 13333 pos = [6,7] 13334 else: 13335 colLabels = ['h','k','l','mul','d','refine','Fsq(hkl)','sig(Fsq)'] 13336 Types = 4*[wg.GRID_VALUE_LONG,]+[wg.GRID_VALUE_FLOAT+':10,4',wg.GRID_VALUE_BOOL,]+ \ 13337 2*[wg.GRID_VALUE_FLOAT+':10,2',] 13338 pos = [5,6] 13339 PawleyTable = G2G.Table(PawleyPeaks,rowLabels=rowLabels,colLabels=colLabels,types=Types) 13340 G2frame.PawleyRefl.SetTable(PawleyTable, True) 13341 G2frame.PawleyRefl.Bind(wx.EVT_KEY_DOWN, KeyEditPawleyGrid) 13342 G2frame.PawleyRefl.Bind(wg.EVT_GRID_LABEL_LEFT_DCLICK, onRefineDClick) 13343 for r in range(G2frame.PawleyRefl.GetNumberRows()): 13344 for c in range(G2frame.PawleyRefl.GetNumberCols()): 13345 if c in pos: 13346 G2frame.PawleyRefl.SetReadOnly(r,c,isReadOnly=False) 13347 else: 13348 G2frame.PawleyRefl.SetCellStyle(r,c,VERY_LIGHT_GREY,True) 13349 G2frame.PawleyRefl.SetMargins(0,0) 13350 G2frame.PawleyRefl.AutoSizeColumns(False) 13308 # removed because it interfered with normal ops. & crashed GSAS-II 13309 # if len(PawleyPeaks) == 0 or not generalData['doPawley']: 13310 # msg = ('Pawley refinement not yet set up. Use the "Pawley setup"'+ 13311 # ' and "Pawley create" menu commands to change this. '+ 13312 # '(Note settings also found on General tab).') 13313 # if not generalData['doPawley']: 13314 # msg += '\n\nCall Pawley setup?' 13315 # else: 13316 # msg += '\n\nCall Pawley create?' 13317 # dlg = wx.MessageDialog(G2frame,msg,'Pawley not setup', 13318 # wx.YES_NO | wx.ICON_QUESTION) 13319 # try: 13320 # dlg.CenterOnParent() 13321 # result = dlg.ShowModal() 13322 # if result == wx.ID_YES and not generalData['doPawley']: 13323 # wx.CallAfter(OnPawleySet,None) 13324 # elif result == wx.ID_YES: 13325 # wx.CallAfter(OnPawleyLoad,None) 13326 # finally: 13327 # dlg.Destroy() 13351 13328 mainSizer = wx.BoxSizer(wx.VERTICAL) 13352 13329 topSizer = wx.BoxSizer(wx.HORIZONTAL) … … 13355 13332 topSizer.Add(G2G.HelpButton(PawleyRefList,helpIndex=G2frame.dataWindow.helpKey)) 13356 13333 mainSizer.Add(topSizer,0,wx.EXPAND) 13357 mainSizer.Add(G2frame.PawleyRefl) 13334 rowLabels = [] 13335 if len(PawleyPeaks): 13336 for i in range(len(PawleyPeaks)): rowLabels.append(str(i)) 13337 if generalData['Modulated']: 13338 colLabels = ['h','k','l','m','mul','d','refine','Fsq(hkl)','sig(Fsq)'] 13339 Types = 5*[wg.GRID_VALUE_LONG,]+[wg.GRID_VALUE_FLOAT+':10,4',wg.GRID_VALUE_BOOL,]+ \ 13340 2*[wg.GRID_VALUE_FLOAT+':10,2',] 13341 pos = [6,7] 13342 else: 13343 colLabels = ['h','k','l','mul','d','refine','Fsq(hkl)','sig(Fsq)'] 13344 Types = 4*[wg.GRID_VALUE_LONG,]+[wg.GRID_VALUE_FLOAT+':10,4',wg.GRID_VALUE_BOOL,]+ \ 13345 2*[wg.GRID_VALUE_FLOAT+':10,2',] 13346 pos = [5,6] 13347 PawleyTable = G2G.Table(PawleyPeaks,rowLabels=rowLabels,colLabels=colLabels,types=Types) 13348 G2frame.PawleyRefl.SetTable(PawleyTable, True) 13349 G2frame.PawleyRefl.Bind(wx.EVT_KEY_DOWN, KeyEditPawleyGrid) 13350 G2frame.PawleyRefl.Bind(wg.EVT_GRID_LABEL_LEFT_DCLICK, onRefineDClick) 13351 for r in range(G2frame.PawleyRefl.GetNumberRows()): 13352 for c in range(G2frame.PawleyRefl.GetNumberCols()): 13353 if c in pos: 13354 G2frame.PawleyRefl.SetReadOnly(r,c,isReadOnly=False) 13355 else: 13356 G2frame.PawleyRefl.SetCellStyle(r,c,VERY_LIGHT_GREY,True) 13357 G2frame.PawleyRefl.SetMargins(0,0) 13358 G2frame.PawleyRefl.AutoSizeColumns(False) 13359 mainSizer.Add(G2frame.PawleyRefl) 13360 else: 13361 mainSizer.Add(wx.StaticText(PawleyRefList,label=' There are no Pawley reflections')) 13358 13362 SetPhaseWindow(PawleyRefList,mainSizer) 13359 13363 … … 13422 13426 genDlg.Destroy() 13423 13427 13424 if generalData['doPawley'] and res == wx.ID_OK and ( 13425 not startPawley or startDmin != generalData['Pawley dmin']): 13428 if generalData['doPawley'] and res == wx.ID_OK and (not startPawley or startDmin != generalData['Pawley dmin']): 13426 13429 dlg = wx.MessageDialog(G2frame,'Do you want to initialize the Pawley reflections with the settings?','Initialize Pawley?', 13427 13430 wx.YES_NO | wx.ICON_QUESTION) … … 13548 13551 ref[6+im] /= (Sample['Scale'][0] * Vst * Lorenz * pola * ref[3+im]) 13549 13552 else: 13550 ref[6+im] /= ( 0.02*Sample['Scale'][0] * ref[3+im]*cw[indx]) #why 0.02*cw?13553 ref[6+im] /= (Sample['Scale'][0] * ref[3+im]*cw[indx]) 13551 13554 except IndexError: 13552 pass13555 ref[6+im] = 0.0 13553 13556 finally: 13554 13557 wx.EndBusyCursor() … … 13660 13663 oldSizer = MapPeakList.GetSizer() 13661 13664 if oldSizer: oldSizer.Clear() 13665 mainSizer = wx.BoxSizer(wx.VERTICAL) 13666 topSizer = wx.BoxSizer(wx.HORIZONTAL) 13667 topSizer.Add(wx.StaticText(MapPeakList,label='Fourier map peak positions for %s:'%data['General']['Name']),0,WACV) 13668 topSizer.Add((-1,-1),1,wx.EXPAND) 13669 topSizer.Add(G2G.HelpButton(MapPeakList,helpIndex=G2frame.dataWindow.helpKey)) 13670 mainSizer.Add(topSizer,0,wx.EXPAND) 13662 13671 if 'Map Peaks' in data: 13663 mainSizer = wx.BoxSizer(wx.VERTICAL)13664 topSizer = wx.BoxSizer(wx.HORIZONTAL)13665 topSizer.Add(wx.StaticText(MapPeakList,label='Fourier map peak positions for %s:'%data['General']['Name']),0,WACV)13666 topSizer.Add((-1,-1),1,wx.EXPAND)13667 topSizer.Add(G2G.HelpButton(MapPeakList,helpIndex=G2frame.dataWindow.helpKey))13668 mainSizer.Add(topSizer,0,wx.EXPAND)13669 13672 G2frame.GetStatusBar().SetStatusText('Double click any column heading to sort',1) 13670 13673 mapPeaks = data['Map Peaks'] … … 13682 13685 MapPeaks.AutoSizeColumns(False) 13683 13686 mainSizer.Add(MapPeaks) 13684 SetPhaseWindow(MapPeakList,mainSizer) 13687 else: 13688 mainSizer.Add(wx.StaticText(MapPeakList,label=' Map peak list is empty')) 13689 SetPhaseWindow(MapPeakList,mainSizer) 13685 13690 13686 13691 def OnPeaksMove(event): -
trunk/help/gsasII-phase.html
r5250 r5257 25 25 <o:Author>Von Dreele</o:Author> 26 26 <o:LastAuthor>Von Dreele, Robert B.</o:LastAuthor> 27 <o:Revision>4 3</o:Revision>28 <o:TotalTime>72 09</o:TotalTime>27 <o:Revision>48</o:Revision> 28 <o:TotalTime>7295</o:TotalTime> 29 29 <o:Created>2021-06-20T02:30:00Z</o:Created> 30 <o:LastSaved>2022-03- 24T14:35:00Z</o:LastSaved>30 <o:LastSaved>2022-03-31T21:35:00Z</o:LastSaved> 31 31 <o:Pages>1</o:Pages> 32 <o:Words>103 13</o:Words>33 <o:Characters>58 786</o:Characters>32 <o:Words>10342</o:Words> 33 <o:Characters>58951</o:Characters> 34 34 <o:Company>Argonne National Laboratory</o:Company> 35 <o:Lines>4 89</o:Lines>36 <o:Paragraphs>13 7</o:Paragraphs>37 <o:CharactersWithSpaces>6 8962</o:CharactersWithSpaces>35 <o:Lines>491</o:Lines> 36 <o:Paragraphs>138</o:Paragraphs> 37 <o:CharactersWithSpaces>69155</o:CharactersWithSpaces> 38 38 <o:Version>16.00</o:Version> 39 39 </o:DocumentProperties> … … 49 49 <w:WordDocument> 50 50 <w:Zoom>148</w:Zoom> 51 <w:SpellingState>Clean</w:SpellingState>52 <w:GrammarState>Clean</w:GrammarState>53 51 <w:TrackMoves>false</w:TrackMoves> 54 52 <w:TrackFormatting/> … … 953 951 mso-font-kerning:14.0pt;} 954 952 a:link, span.MsoHyperlink 955 {mso-style-priority:99; 953 {mso-style-noshow:yes; 954 mso-style-priority:99; 956 955 color:blue; 957 956 text-decoration:underline; … … 1307 1306 font-family:"Times New Roman",serif; 1308 1307 mso-fareast-font-family:"Times New Roman";} 1309 span.SpellE1310 {mso-style-name:"";1311 mso-spl-e:yes;}1312 span.GramE1313 {mso-style-name:"";1314 mso-gram-e:yes;}1315 1308 .MsoChpDefault 1316 1309 {mso-style-type:export-only; … … 1876 1869 1877 1870 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"'>This 1878 is where to find help on the Phase Tree items in GSAS-II. Note that the window 1879 displayed for this page has multiple tabs. The help information is broken down 1880 by tabsection. <o:p></o:p></span></p>1871 is where to find help on the Phase Tree items in GSAS-II. Note that the window displayed 1872 for this page has multiple tabs. The help information is broken down by tab 1873 section. <o:p></o:p></span></p> 1881 1874 1882 1875 <h2 style='tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><a … … 1902 1895 phase. It also has the controls for Pawley intensity extraction and for 1903 1896 computing Fourier maps for this phase. It can also has the controls for Monte 1904 Carlo/Simulated Annealing for solving structures with flexible rigid molecular <span1905 class=GramE>bodies..</span> <span class=MsoHyperlink><span style='color:windowtext; 1906 text-decoration:none;text-underline:none'><o:p></o:p></span></span></span></p>1897 Carlo/Simulated Annealing for solving structures with flexible rigid molecular 1898 bodies.. <span class=MsoHyperlink><span style='color:windowtext;text-decoration: 1899 none;text-underline:none'><o:p></o:p></span></span></span></p> 1907 1900 1908 1901 <h5 style='margin-left:.5in'>What can I do here?</h5> … … 1943 1936 style='mso-fareast-font-family:"Times New Roman"'>This performs a charge 1944 1937 flipping <i style='mso-bidi-font-style:normal'>ab initio</i> structure solution 1945 using the method of <span class=SpellE>Oszlanyi</span> & <span 1946 class=SpellE>Suto</span> (Acta <span class=SpellE>Cryst</span>. A60, 134-141, 1947 2004). You will need to select a source for the reflection set and perhaps 1948 select an element for normalization by its form factor, a resolution limit 1949 (usually 0.5</span><span style='font-family:"Calibri",sans-serif;mso-fareast-font-family: 1950 "Times New Roman"'>Å</span><span style='mso-fareast-font-family:"Times New Roman"'>) 1951 and a charge flip threshold (usually 0.1); these are found near the bottom of 1952 the <b style='mso-bidi-font-weight:normal'>General</b> window. There are also 1953 Test HKLs to show the progress in phasing with charge flipping cycles. They 1954 show the generally chaotic phase behavior before a solution is found; after 1955 that the phases are essentially fixed. No use is made of this information; it 1956 is just for your edification. A progress bar showing the charge flip residual 1957 is shown while the charge flip is in operation. When the residual is no longer 1958 decreasing (be patient – it doesn’t necessarily fall continuously), press the <b 1959 style='mso-bidi-font-weight:normal'>Cancel</b> button to stop the charge 1960 flipping, otherwise it will stop at 10000 cycles. The resulting map will be 1961 positioned to properly place symmetry operators (NB: depends on the quality of 1962 the resulting phases; the map could be still offset by a few steps), searched 1963 for peaks and the display shifts to <b style='mso-bidi-font-weight:normal'>Map 1964 peaks</b> to show them.<b><o:p></o:p></b></span></p> 1938 using the method of Oszlanyi & Suto (Acta Cryst. A60, 134-141, 2004). You 1939 will need to select a source for the reflection set and perhaps select an 1940 element for normalization by its form factor, a resolution limit (usually 0.5</span><span 1941 style='font-family:"Calibri",sans-serif;mso-fareast-font-family:"Times New Roman"'>Å</span><span 1942 style='mso-fareast-font-family:"Times New Roman"'>) and a charge flip threshold 1943 (usually 0.1); these are found near the bottom of the <b style='mso-bidi-font-weight: 1944 normal'>General</b> window. There are also Test HKLs to show the progress in 1945 phasing with charge flipping cycles. They show the generally chaotic phase 1946 behavior before a solution is found; after that the phases are essentially 1947 fixed. No use is made of this information; it is just for your edification. A 1948 progress bar showing the charge flip residual is shown while the charge flip is 1949 in operation. When the residual is no longer decreasing (be patient – it 1950 doesn’t necessarily fall continuously), press the <b style='mso-bidi-font-weight: 1951 normal'>Cancel</b> button to stop the charge flipping, otherwise it will stop 1952 at 10000 cycles. The resulting map will be positioned to properly place 1953 symmetry operators (NB: depends on the quality of the resulting phases; the map 1954 could be still offset by a few steps), searched for peaks and the display 1955 shifts to <b style='mso-bidi-font-weight:normal'>Map peaks</b> to show them.<b><o:p></o:p></b></span></p> 1965 1956 1966 1957 <p class=MsoListParagraphCxSpMiddle style='margin-left:121.5pt;mso-add-space: … … 2004 1995 style='mso-fareast-font-family:"Times New Roman"'>Transform </span></b><span 2005 1996 style='mso-fareast-font-family:"Times New Roman"'>- This allows for a change in 2006 axes, <span class=GramE>symmetry</span> or unit cell. It is also used to create 2007 a magnetic phase from a chemical (nuclear) phase. One important transformation 2008 that can be done here is for Origin 1 settings to Origin 2 (<a 2009 href="#_Origin_1_->">described below</a>).<b><o:p></o:p></b></span></p> 1997 axes, symmetry or unit cell. It is also used to create a magnetic phase from a 1998 chemical (nuclear) phase. One important transformation that can be done here is 1999 for Origin 1 settings to Origin 2 (<a href="#_Origin_1_->">described below</a>).<b><o:p></o:p></b></span></p> 2010 2000 2011 2001 <p class=MsoListParagraphCxSpMiddle style='margin-left:121.5pt;mso-add-space: … … 2015 2005 </span></span></span><![endif]><b><span style='mso-fareast-font-family:"Times New Roman"'>Compare 2016 2006 – </span></b><span style='mso-fareast-font-family:"Times New Roman"'>Compares 2017 idealized <span class=SpellE>polyhedra</span> (tetrahedron & octahedron) to2018 those obtained from aReverse Monte Carlo run in RMCProfile.<b><o:p></o:p></b></span></p>2007 idealized polyhedra (tetrahedron & octahedron) to those obtained from a 2008 Reverse Monte Carlo run in RMCProfile.<b><o:p></o:p></b></span></p> 2019 2009 2020 2010 <p class=MsoListParagraphCxSpMiddle style='margin-left:121.5pt;mso-add-space: … … 2036 2026 style='mso-fareast-font-family:"Times New Roman"'>Protein quality</span></b><span 2037 2027 style='mso-fareast-font-family:"Times New Roman"'> – evaluate protein quality 2038 by python versions of <span class=SpellE>errat</span> & errat2 codes by <span 2039 class=SpellE>Colovos</span>, C. & <span class=SpellE>Yeates</span>, T.O. Protein 2040 Science 2, 1511-1519 (1991).<b><o:p></o:p></b></span></p> 2028 by python versions of errat & errat2 codes by Colovos, C. & Yeates, 2029 T.O. Protein Science 2, 1511-1519 (1991).<b><o:p></o:p></b></span></p> 2041 2030 2042 2031 <p class=MsoNormal style='tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span … … 2062 2051 </span></span></span></span><![endif]><b style='mso-bidi-font-weight:normal'><span 2063 2052 style='mso-fareast-font-family:"Times New Roman"'>Phase name</span></b><span 2064 style='mso-fareast-font-family:"Times New Roman"'> – this is the name assigned 2065 t o this phase. It can be changed at any time.<span class=MsoHyperlink><span2053 style='mso-fareast-font-family:"Times New Roman"'> – this is the name assigned to 2054 this phase. It can be changed at any time.<span class=MsoHyperlink><span 2066 2055 style='color:windowtext'><o:p></o:p></span></span></span></p> 2067 2056 … … 2087 2076 the phase is initialized; it can be changed later. Be careful about the impact 2088 2077 on Atom site symmetry and multiplicity if you do. GSAS-II will recognize any 2089 legal space group symbol using the short Hermann-<span class=SpellE>Mauguin</span> 2090 forms; put a space between the axial fields (<span class=GramE>e.g.</span> ‘F d 2091 3 m’ not ‘Fd3m’; ‘F d 3 m’ is understood as well as ‘F d -3 m’). For space 2092 groups with a choice of origin (<span class=GramE>e.g.</span> F d 3 m), GSAS-II 2093 always uses the 2<sup>nd</sup> setting where the center of inversion is located 2094 at the origin. The choice of space group will set the available unit cell 2095 parameters.<span class=MsoHyperlink><span style='color:windowtext'><o:p></o:p></span></span></span></p> 2078 legal space group symbol using the short Hermann-Mauguin forms; put a space 2079 between the axial fields (e.g. ‘F d 3 m’ not ‘Fd3m’; ‘F d 3 m’ is understood as 2080 well as ‘F d -3 m’). For space groups with a choice of origin (e.g. F d 3 m), 2081 GSAS-II always uses the 2<sup>nd</sup> setting where the center of inversion is 2082 located at the origin. The choice of space group will set the available unit 2083 cell parameters.<span class=MsoHyperlink><span style='color:windowtext'><o:p></o:p></span></span></span></p> 2096 2084 2097 2085 <p class=MsoListParagraphCxSpMiddle style='margin-left:121.5pt;mso-add-space: … … 2198 2186 <v:imagedata src="gsasII-phase_files/image001.png" o:title="" chromakey="white"/> 2199 2187 </v:shape><![endif]--><![if !vml]><img width=335 height=19 2200 src="gsasII-phase_files/image0 49.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><br>2188 src="gsasII-phase_files/image002.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><br> 2201 2189 <span style='font-family:"Cambria Math",serif;mso-fareast-font-family:"Times New Roman"; 2202 2190 mso-bidi-font-style:italic'>A0-A5 correspond to the reciprocal metric tensor … … 2224 2212 table is shown next on the General page; you may select the isotope (only 2225 2213 relevant for neutron diffraction experiments). The density (just above the 2226 Elements) is computed depending on this choice, the unit cell volume and the 2227 atomfractions/site multiplicities in the entries on the Atoms page.<span2214 Elements) is computed depending on this choice, the unit cell volume and the atom 2215 fractions/site multiplicities in the entries on the Atoms page.<span 2228 2216 class=MsoHyperlink><span style='color:windowtext'><o:p></o:p></span></span></span></p> 2229 2217 … … 2257 2245 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 2258 2246 style='mso-bidi-font-weight:normal'><span style='mso-fareast-font-family:"Times New Roman"'>Pawley 2259 <span class=SpellE>dmin</span></span></b><span style='mso-fareast-font-family: 2260 "Times New Roman"'> – This is the minimum d-spacing to be used in a Pawley 2261 refinement. <b style='mso-bidi-font-weight:normal'>NB:</b> be sure to set this 2262 to match theminimum d-spacing indicated by the powder pattern limits (see <b2247 dmin</span></b><span style='mso-fareast-font-family:"Times New Roman"'> – This 2248 is the minimum d-spacing to be used in a Pawley refinement. <b 2249 style='mso-bidi-font-weight:normal'>NB:</b> be sure to set this to match the 2250 minimum d-spacing indicated by the powder pattern limits (see <b 2263 2251 style='mso-bidi-font-weight:normal'>Limits</b> for the powder data set).</span></p> 2264 2252 … … 2269 2257 style='mso-list:Ignore'>c.<span style='font:7.0pt "Times New Roman"'> 2270 2258 </span></span></span></span><![endif]><b style='mso-bidi-font-weight:normal'><span 2271 style='mso-fareast-font-family:"Times New Roman"'>Pawley <span class=SpellE>dmax</span></span></b><span2259 style='mso-fareast-font-family:"Times New Roman"'>Pawley dmax</span></b><span 2272 2260 style='mso-fareast-font-family:"Times New Roman";mso-bidi-font-weight:bold'> – 2273 2261 This is the maximum d-spacing for reflections in a Pawley refinement. It is … … 2284 2272 style='mso-fareast-font-family:"Times New Roman"'>Pawley neg. wt.</span></b><span 2285 2273 style='mso-fareast-font-family:"Times New Roman"'> – This is the weight for a 2286 penalty function applied during a Pawley refinement on resulting negative intensities.2287 Use with caution; initially try very small values (<span class=GramE>e.g.</span> 2288 .01). Avalue of zero means no penalty is applied.<span class=MsoHyperlink><span2274 penalty function applied during a Pawley refinement on resulting negative 2275 intensities. Use with caution; initially try very small values (e.g. .01). A 2276 value of zero means no penalty is applied.<span class=MsoHyperlink><span 2289 2277 style='color:windowtext;text-decoration:none;text-underline:none'><o:p></o:p></span></span></span></p> 2290 2278 … … 2295 2283 style='mso-list:Ignore'>5.<span style='font:7.0pt "Times New Roman"'> 2296 2284 </span></span></span></span><![endif]><span style='mso-fareast-font-family: 2297 "Times New Roman"'>Fourier map controls are shown next on the General page. 2298 Single crystal data or a completed Rietveld or Pawley refinement is required 2299 before a Fourier map can be computed. Select the desired type of map,the2300 source of the reflection set and the map resolution desired. The peak cutoff is 2301 defined as a percentage of the maximum and defines the lowest level considered 2302 in the peaksearch.<span class=MsoHyperlink><span style='color:windowtext'><o:p></o:p></span></span></span></p>2285 "Times New Roman"'>Fourier map controls are shown next on the General page. Single 2286 crystal data or a completed Rietveld or Pawley refinement is required before a 2287 Fourier map can be computed. Select the desired type of map, the source of the 2288 reflection set and the map resolution desired. The peak cutoff is defined as a 2289 percentage of the maximum and defines the lowest level considered in the peak 2290 search.<span class=MsoHyperlink><span style='color:windowtext'><o:p></o:p></span></span></span></p> 2303 2291 2304 2292 <p class=MsoListParagraphCxSpMiddle style='margin-left:73.2pt;mso-add-space: … … 2319 2307 </span></span></span></span><![endif]><b style='mso-bidi-font-weight:normal'><span 2320 2308 style='mso-fareast-font-family:"Times New Roman"'>Reflection sets </span></b><span 2321 style='mso-fareast-font-family:"Times New Roman"'>– This is the source of structure 2322 factors to be used in a charge flip calculation. These may be either a single 2323 crystal data set, or structure factors extracted from a powder pattern via a 2324 Pawley or LeBail refinement or a Rietveld refinement.<span class=MsoHyperlink><span 2325 style='color:windowtext;text-decoration:none;text-underline:none'><o:p></o:p></span></span></span></p> 2309 style='mso-fareast-font-family:"Times New Roman"'>– This is the source of 2310 structure factors to be used in a charge flip calculation. These may be either 2311 a single crystal data set, or structure factors extracted from a powder pattern 2312 via a Pawley or LeBail refinement or a Rietveld refinement.<span 2313 class=MsoHyperlink><span style='color:windowtext;text-decoration:none; 2314 text-underline:none'><o:p></o:p></span></span></span></p> 2326 2315 2327 2316 <p class=MsoListParagraphCxSpMiddle style='margin-left:121.5pt;mso-add-space: … … 2332 2321 </span></span></span></span><![endif]><b style='mso-bidi-font-weight:normal'><span 2333 2322 style='mso-fareast-font-family:"Times New Roman"'>Normalizing element </span></b><span 2334 style='mso-fareast-font-family:"Times New Roman"'>– This is an element form 2335 factorchosen to normalize the structure factors before charge flipping. <b2323 style='mso-fareast-font-family:"Times New Roman"'>– This is an element form factor 2324 chosen to normalize the structure factors before charge flipping. <b 2336 2325 style='mso-bidi-font-weight:normal'>None</b> (the default) can be selected from 2337 2326 the lower right of the Periodic Table display shown when this is selected.<span … … 2379 2368 style='mso-fareast-font-family:"Times New Roman"'>Test HKLs</span></b><span 2380 2369 style='mso-fareast-font-family:"Times New Roman";mso-bidi-font-weight:bold'> – 2381 plot of phases for selected <span class=SpellE>hkls</span> are shown at end of 2382 charge flipping run. Just for you to look at.</span><span style='mso-fareast-font-family: 2383 "Times New Roman"'><o:p></o:p></span></p> 2370 plot of phases for selected hkls are shown at end of charge flipping run. Just 2371 for you to look at.</span><span style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p> 2384 2372 2385 2373 <p class=MsoListParagraphCxSpMiddle style='margin-left:73.2pt;mso-add-space: … … 2398 2386 This is the source of structure factors to be used in a charge flip 2399 2387 calculation. These may be either a single crystal data set, or structure 2400 factors extracted from a powder pattern via a Pawley or <span class=SpellE>Lebail</span>2401 refinement or aRietveld refinement.<o:p></o:p></span></p>2388 factors extracted from a powder pattern via a Pawley or Lebail refinement or a 2389 Rietveld refinement.<o:p></o:p></span></p> 2402 2390 2403 2391 <p class=MsoListParagraphCxSpMiddle style='margin-left:121.5pt;mso-add-space: … … 2469 2457 point in the structure does not contain a center of symmetry. Origin 1 places 2470 2458 the origin at the highest symmetry setting while Origin 2 places the origin at 2471 a center of symmetry (creating a - <span class=GramE>x,-</span>y,-z symmetry2472 operator, which means that reflection phases can only be 0 or π.) GSAS-II 2473 requires use of the Origin 2 settings because computations are much faster and 2474 simpler without complex structure factors. Alas, the literature contains <span2475 class=GramE>a number of</span> structures reported in Origin 1, where the 2476 origin choice may not be clearly communicated. (The CIF standard does not 2477 require that origin choice be indicated.) When a structure is imported that 2478 uses any of the space groups where an origin choice is possible, a message is 2479 shown in GSAS-II notifying the user that they must confirm that the origin 2480 choice is correct and then provides the opportunity to changeorigins. <o:p></o:p></span></p>2459 a center of symmetry (creating a -x,-y,-z symmetry operator, which means that 2460 reflection phases can only be 0 or π.) GSAS-II requires use of the Origin 2 2461 settings because computations are much faster and simpler without complex structure 2462 factors. Alas, the literature contains a number of structures reported in 2463 Origin 1, where the origin choice may not be clearly communicated. (The CIF 2464 standard does not require that origin choice be indicated.) When a structure is 2465 imported that uses any of the space groups where an origin choice is possible, 2466 a message is shown in GSAS-II notifying the user that they must confirm that 2467 the origin choice is correct and then provides the opportunity to change 2468 origins. <o:p></o:p></span></p> 2481 2469 2482 2470 <p class=MsoNormal style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b><span … … 2506 2494 <tr style='mso-yfti-irow:2'> 2507 2495 <td style='padding:.75pt .75pt .75pt .75pt'> 2508 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 2509 "Times New Roman"'>Ti</span></span><span style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p> 2496 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"'>Ti<o:p></o:p></span></p> 2510 2497 </td> 2511 2498 <td style='padding:.75pt .75pt .75pt .75pt'> … … 2560 2547 <tr style='mso-yfti-irow:2'> 2561 2548 <td style='padding:.75pt .75pt .75pt .75pt'> 2562 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 2563 "Times New Roman"'>Ti</span></span><span style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p> 2549 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"'>Ti<o:p></o:p></span></p> 2564 2550 </td> 2565 2551 <td style='padding:.75pt .75pt .75pt .75pt'> … … 2591 2577 <p class=MsoNormal style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 2592 2578 style='mso-fareast-font-family:"Times New Roman";color:white;mso-color-alt: 2593 windowtext'>where the origin is shifted by (0,1/</span><span class=GramE><span 2594 style='mso-fareast-font-family:"Times New Roman"'>4,-</span></span><span 2595 style='mso-fareast-font-family:"Times New Roman"'>1/8). <o:p></o:p></span></p> 2579 windowtext'>where the origin is shifted by (0,1/4,-1/8). </span><span 2580 style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p> 2596 2581 2597 2582 <p class=MsoNormal style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><!--[if gte vml 1]><v:shape … … 2609 2594 </v:shape><![endif]--><![if !vml]><img width=322 height=190 2610 2595 src="gsasII_files/wrong.png" align=right v:shapes="Picture_x0020_3"><![endif]><span 2611 style='mso-fareast-font-family:"Times New Roman"'>GSAS-II always uses the symmetry 2612 operators for Origin 2; if the structure is input incorrectly with the 2613 coordinates set for Origin 1, there are several <span class=GramE>fairly 2614 obvious</span> signs of problems: (1) the site symmetries and multiplicities 2615 are wrong, often giving an incorrect chemical formula, (2) the interatomic 2616 distances are incorrect, and (3) a plot of the structure is improbable. In this 2617 case incorrect multiplicities gives rise to a density of 7.9 g/cc, double the 2618 correct value. Impossible interatomic distances of 1.88Å for <span 2619 class=SpellE><span class=GramE>Ti-Ti</span></span>, and 1.39Å for <span 2620 class=SpellE>Ti</span>-O are seen. The unit cell contents with the wrong space 2621 group operators <span class=GramE>is</span> shown to the right. <o:p></o:p></span></p> 2596 style='mso-fareast-font-family:"Times New Roman"'>GSAS-II always uses the 2597 symmetry operators for Origin 2; if the structure is input incorrectly with the 2598 coordinates set for Origin 1, there are several fairly obvious signs of 2599 problems: (1) the site symmetries and multiplicities are wrong, often giving an 2600 incorrect chemical formula, (2) the interatomic distances are incorrect, and 2601 (3) a plot of the structure is improbable. In this case incorrect 2602 multiplicities gives rise to a density of 7.9 g/cc, double the correct value. 2603 Impossible interatomic distances of 1.88Å for Ti-Ti, and 1.39Å for Ti-O are 2604 seen. The unit cell contents with the wrong space group operators is shown to 2605 the right. <o:p></o:p></span></p> 2622 2606 2623 2607 <p class=MsoNormal style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 2624 2608 style='mso-fareast-font-family:"Times New Roman"'>With coordinates that match 2625 the space group operations, the correct <span class=SpellE>Ti</span>-O 2626 distances are 1.92Å and 1.97Å and the shortest <span class=SpellE>Ti-Ti</span> 2627 distance is 3.0Å. (Note that interatomic distances can be computed in GSAS-II 2628 using the Phase Atoms tab and the Compute/"Show Distances & 2629 Angles" menu item.) <o:p></o:p></span></p> 2609 the space group operations, the correct Ti-O distances are 1.92Å and 1.97Å and 2610 the shortest Ti-Ti distance is 3.0Å. (Note that interatomic distances can be 2611 computed in GSAS-II using the Phase Atoms tab and the Compute/"Show 2612 Distances & Angles" menu item.) <o:p></o:p></span></p> 2630 2613 2631 2614 <p class=MsoNormal style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><!--[if gte vml 1]><v:shape … … 2672 2655 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>The 2673 2656 HAP parameters include: the phase fraction; the sample contributions to peak 2674 broadening: <span class=SpellE>microstrain</span> and crystallite size; a 2675 LeBail intensity extraction flag; hydrostatic/elastic strain shifts to lattice 2676 parameters; corrections to peak intensities due to experimental effects 2677 (preferred orientation, <span class=GramE>extinction</span> and disordered 2678 solvents).</p> 2657 broadening: microstrain and crystallite size; a LeBail intensity extraction 2658 flag; hydrostatic/elastic strain shifts to lattice parameters; corrections to 2659 peak intensities due to experimental effects (preferred orientation, extinction 2660 and disordered solvents).</p> 2679 2661 2680 2662 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>For 2681 single crystal data, the only parameters are scale, <span class=GramE>extinction</span>2682 and disorderedsolvent. There is no Sample Parameters histogram scale factor.</p>2663 single crystal data, the only parameters are scale, extinction and disordered 2664 solvent. There is no Sample Parameters histogram scale factor.</p> 2683 2665 2684 2666 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b><span … … 2722 2704 2723 2705 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 2724 style='mso-fareast-font-family:"Times New Roman"'>Used for single crystal <span2725 class=GramE>data:</span>relates F<sup>2</sup><sub>obs</sub> to F<sup>2</sup><sub>calc</sub>.<o:p></o:p></span></p>2706 style='mso-fareast-font-family:"Times New Roman"'>Used for single crystal data: 2707 relates F<sup>2</sup><sub>obs</sub> to F<sup>2</sup><sub>calc</sub>.<o:p></o:p></span></p> 2726 2708 2727 2709 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b><span … … 2731 2713 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 2732 2714 style='mso-fareast-font-family:"Times New Roman"'>is computed from size 2733 factor(s) in microns (<span class=SpellE>μm</span> = 10<sup>-6</sup> m), with 2734 the Scherrer constant assumed as unity. Sizes can be computed in three ways: 2735 isotropic, <span class=GramE>uniaxial</span> and ellipsoidal. In isotropic 2736 broadening, crystallites are assumed to average as uniform in all directions 2737 and a single size value is supplied; with uniaxial broadening, a preferred 2738 direction (as a crystallographic axis, such as 0,0,1 is supplied) -- note that 2739 for most crystal systems only one axis makes sense -- and two size parameters 2740 are defined, one for along the axis and one for in the perpendicular plane; 2741 with ellipsoidal, six terms are used to define a broadening tensor that has 2742 arbitrary orientation -- this model may require constraints and is seldom 2743 needed. Note that size broadening is usually Lorentzian, which corresponds to a 2744 <span class=SpellE>LGmix</span> value of 1.0; if this value is between 0. and 2745 1., both Gaussian and Lorentz size broadening is modeled and a value of 0.0 is 2746 pure Gaussian. Values less than 0. or greater than 1. make no physical sense. 2747 Typical sensitivity is to no more than 4 <span class=SpellE>μm</span>; beyond 2748 that the particles are effectively infinite for a diffraction experiment.<o:p></o:p></span></p> 2749 2750 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 2751 class=SpellE><b><span style='mso-fareast-font-family:"Times New Roman"'>Microstrain</span></b></span><b><span 2752 style='mso-fareast-font-family:"Times New Roman"'> peak broadening </span></b><span 2715 factor(s) in microns (μm = 10<sup>-6</sup> m), with the Scherrer constant 2716 assumed as unity. Sizes can be computed in three ways: isotropic, uniaxial and 2717 ellipsoidal. In isotropic broadening, crystallites are assumed to average as 2718 uniform in all directions and a single size value is supplied; with uniaxial 2719 broadening, a preferred direction (as a crystallographic axis, such as 0,0,1 is 2720 supplied) -- note that for most crystal systems only one axis makes sense -- 2721 and two size parameters are defined, one for along the axis and one for in the 2722 perpendicular plane; with ellipsoidal, six terms are used to define a 2723 broadening tensor that has arbitrary orientation -- this model may require 2724 constraints and is seldom needed. Note that size broadening is usually 2725 Lorentzian, which corresponds to a LGmix value of 1.0; if this value is between 2726 0. and 1., both Gaussian and Lorentz size broadening is modeled and a value of 2727 0.0 is pure Gaussian. Values less than 0. or greater than 1. make no physical sense. 2728 Typical sensitivity is to no more than 4 μm; beyond that the particles are 2729 effectively infinite for a diffraction experiment.<o:p></o:p></span></p> 2730 2731 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b><span 2732 style='mso-fareast-font-family:"Times New Roman"'>Microstrain peak broadening </span></b><span 2753 2733 style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p> 2754 2734 2755 2735 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 2756 2736 style='mso-fareast-font-family:"Times New Roman"'>is computed as unitless 2757 fraction of <span class=SpellE>Δd</span>/d (or equivalently ΔQ/Q) times 10<sup>6</sup>. 2758 <span class=SpellE>Microstrain</span> can be represented in three ways: 2759 isotropic, <span class=GramE>uniaxial</span> and generalized. In isotropic 2760 broadening, <span class=SpellE>microstrain</span> broadening assumed to be the 2761 same in all crystallographic directions and a single value is supplied; with 2762 uniaxial broadening, a preferred direction (as a crystallographic axis, such as 2763 0,0,1) is supplied -- note that for most crystal systems only one axis makes 2764 sense -- and two <span class=SpellE>microstrain</span> parameters are defined, 2765 one for along the axis and one for in the perpendicular plane; with 2766 generalized, the Nicole Popa/Peter Stephens second-order expansion model is 2767 used and the number of terms will depend on the crystal system. It is typically 2768 possible to refine all terms when significant anisotropic strain broadening is 2769 present. Note that <span class=SpellE>microstrain</span> broadening is usually 2770 Lorentzian, which corresponds to a <span class=SpellE>LGmix</span> value of 2771 1.0; if this value is between 0. and 1., both Gaussian and Lorentz broadening 2772 is modeled and a value of 0.0 is pure Gaussian. Values less than 0. or greater 2773 than 1. make no physical sense. Typical <span class=SpellE>microstrain</span> 2774 is ~1000.<o:p></o:p></span></p> 2737 fraction of Δd/d (or equivalently ΔQ/Q) times 10<sup>6</sup>. Microstrain can 2738 be represented in three ways: isotropic, uniaxial and generalized. In isotropic 2739 broadening, microstrain broadening assumed to be the same in all 2740 crystallographic directions and a single value is supplied; with uniaxial 2741 broadening, a preferred direction (as a crystallographic axis, such as 0,0,1) 2742 is supplied -- note that for most crystal systems only one axis makes sense -- 2743 and two microstrain parameters are defined, one for along the axis and one for 2744 in the perpendicular plane; with generalized, the Nicole Popa/Peter Stephens 2745 second-order expansion model is used and the number of terms will depend on the 2746 crystal system. It is typically possible to refine all terms when significant 2747 anisotropic strain broadening is present. Note that microstrain broadening is usually 2748 Lorentzian, which corresponds to a LGmix value of 1.0; if this value is between 2749 0. and 1., both Gaussian and Lorentz broadening is modeled and a value of 0.0 2750 is pure Gaussian. Values less than 0. or greater than 1. make no physical 2751 sense. Typical microstrain is ~1000.<o:p></o:p></span></p> 2775 2752 2776 2753 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b><span … … 2798 2775 model is possible with the "<u><span style='color:blue'><a href="#Texture">Texture</a></span></u>" 2799 2776 tab (which usually requires multiple histograms at different sample 2800 orientations or detector settings). The approaches available here are March-<span2801 class=SpellE>Dollase</span>, which requires a definition of a unique axis (in2777 orientations or detector settings). The approaches available here are 2778 March-Dollase, which requires a definition of a unique axis (in 2802 2779 crystallographic coordinates) and the relative amount of excess or depletion of 2803 2780 crystallites in that direction; or Spherical Harmonics, where the selection of … … 2819 2796 2820 2797 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b><span 2821 style='mso-fareast-font-family:"Times New Roman"'>Disordered solvent – <span 2822 class=SpellE>Babinet</span> A & B</span></b><span style='mso-fareast-font-family: 2823 "Times New Roman"'><o:p></o:p></span></p> 2798 style='mso-fareast-font-family:"Times New Roman"'>Disordered solvent – Babinet 2799 A & B</span></b><span style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p> 2824 2800 2825 2801 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 2826 style='mso-fareast-font-family:"Times New Roman"'>This correction, using the <span2827 class=SpellE>Babinet</span> model, is typically used to treat scattering from 2828 solvent that is not well-ordered in protein structures. It probably makes no 2829 sense in most anyother application. <o:p></o:p></span></p>2802 style='mso-fareast-font-family:"Times New Roman"'>This correction, using the 2803 Babinet model, is typically used to treat scattering from solvent that is not 2804 well-ordered in protein structures. It probably makes no sense in most any 2805 other application. <o:p></o:p></span></p> 2830 2806 2831 2807 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b><span … … 2853 2829 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>2.<span 2854 2830 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 2855 style='mso-fareast-font-family:"Times New Roman"'>The plot selection items allow2856 for three dimensional representations of the <span class=SpellE>microstrain</span> 2857 or crystallite size distributions (which are spheres for isotropic treatments); 2858 preferred orientation can be plotted as a Psi scan (a plot of relative2859 crystallite abundance for a particular reflection as a function of azimuthal 2860 angle) or as an inverse pole figure (which shows a stereographic projection of 2861 the probability distribution for different reciprocal lattice directions as 2862 viewed down the sample cylinder axis). For no texture/preferred orientation 2863 this figure wouldbe flat = 1.0.<o:p></o:p></span></p>2831 style='mso-fareast-font-family:"Times New Roman"'>The plot selection items 2832 allow for three dimensional representations of the microstrain or crystallite 2833 size distributions (which are spheres for isotropic treatments); preferred 2834 orientation can be plotted as a Psi scan (a plot of relative crystallite abundance 2835 for a particular reflection as a function of azimuthal angle) or as an inverse 2836 pole figure (which shows a stereographic projection of the probability 2837 distribution for different reciprocal lattice directions as viewed down the 2838 sample cylinder axis). For no texture/preferred orientation this figure would 2839 be flat = 1.0.<o:p></o:p></span></p> 2864 2840 2865 2841 <h4 style='margin-left:.25in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><a … … 2942 2918 style='mso-list:Ignore'>2.<span style='font:7.0pt "Times New Roman"'> 2943 2919 </span></span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Double 2944 left <span class=GramE>click</span> a Type column heading</b>: a dialog box is2945 s hown that allows you to select all atoms with that type.<span2946 class=MsoHyperlink><span style='mso-fareast-font-family:"Times New Roman"; 2947 color:windowtext;text-decoration:none;text-underline:none'><o:p></o:p></span></span></p>2920 left click a Type column heading</b>: a dialog box is shown that allows you to 2921 select all atoms with that type. <span class=MsoHyperlink><span 2922 style='mso-fareast-font-family:"Times New Roman";color:windowtext;text-decoration: 2923 none;text-underline:none'><o:p></o:p></span></span></p> 2948 2924 2949 2925 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: … … 2968 2944 the mouse (<b style='mso-bidi-font-weight:normal'>Alt</b> ignored, <b 2969 2945 style='mso-bidi-font-weight:normal'>Shift</b> & <b style='mso-bidi-font-weight: 2970 normal'>Ctrl</b> allow selection of multiple <span class=GramE>cells</span> but 2971 no use is made of them). An individual data item can be cut/pasted anywhere 2972 including from/to another document. Bad entries are rejected (yellow 2973 background). If any entry is changed, press <b style='mso-bidi-font-weight: 2974 normal'>Enter</b> key or select another atom entry to apply the change.<span 2975 class=MsoHyperlink><span style='color:windowtext;text-decoration:none; 2976 text-underline:none'><o:p></o:p></span></span></span></p> 2946 normal'>Ctrl</b> allow selection of multiple cells but no use is made of them). 2947 An individual data item can be cut/pasted anywhere including from/to another 2948 document. Bad entries are rejected (yellow background). If any entry is 2949 changed, press <b style='mso-bidi-font-weight:normal'>Enter</b> key or select 2950 another atom entry to apply the change.<span class=MsoHyperlink><span 2951 style='color:windowtext;text-decoration:none;text-underline:none'><o:p></o:p></span></span></span></p> 2977 2952 2978 2953 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3016 2991 color:windowtext;text-decoration:none;text-underline:none'><span 3017 2992 style='mso-list:Ignore'>d.<span style='font:7.0pt "Times New Roman"'> 3018 </span></span></span></span><![endif]><span class=SpellE><span class=GramE><b 3019 style='mso-bidi-font-weight:normal'><span style='mso-fareast-font-family:"Times New Roman"'>x,y</span></b></span><b 3020 style='mso-bidi-font-weight:normal'><span style='mso-fareast-font-family:"Times New Roman"'>,z</span></b></span><span 2993 </span></span></span></span><![endif]><b style='mso-bidi-font-weight:normal'><span 2994 style='mso-fareast-font-family:"Times New Roman"'>x,y,z</span></b><span 3021 2995 style='mso-fareast-font-family:"Times New Roman"'> – change atom coordinate. 3022 Fractions (<span class=GramE>e.g.</span> 1/3, 1/4) are allowed.<span 3023 class=MsoHyperlink><span style='color:windowtext;text-decoration:none; 3024 text-underline:none'><o:p></o:p></span></span></span></p> 2996 Fractions (e.g. 1/3, 1/4) are allowed.<span class=MsoHyperlink><span 2997 style='color:windowtext;text-decoration:none;text-underline:none'><o:p></o:p></span></span></span></p> 3025 2998 3026 2999 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3029 3002 color:windowtext;text-decoration:none;text-underline:none'><span 3030 3003 style='mso-list:Ignore'>e.<span style='font:7.0pt "Times New Roman"'> 3031 </span></span></span></span><![endif]><span class=SpellE><span class=GramE><b 3032 style='mso-bidi-font-weight:normal'><span style='mso-fareast-font-family:"Times New Roman"'>frac,Uiso</span></b></span><b 3033 style='mso-bidi-font-weight:normal'><span style='mso-fareast-font-family:"Times New Roman"'>,Uij</span></b></span><span 3034 style='mso-fareast-font-family:"Times New Roman"'> – change these values; 3035 fractions (e.g. 1/3, 1/4) are allowed.<span class=MsoHyperlink><span 3036 style='color:windowtext;text-decoration:none;text-underline:none'><o:p></o:p></span></span></span></p> 3004 </span></span></span></span><![endif]><b style='mso-bidi-font-weight:normal'><span 3005 style='mso-fareast-font-family:"Times New Roman"'>frac,Uiso,Uij</span></b><span 3006 style='mso-fareast-font-family:"Times New Roman"'> – change these values; fractions 3007 (e.g. 1/3, 1/4) are allowed.<span class=MsoHyperlink><span style='color:windowtext; 3008 text-decoration:none;text-underline:none'><o:p></o:p></span></span></span></p> 3037 3009 3038 3010 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3044 3016 style='mso-fareast-font-family:"Times New Roman"'>I/A</span></b><span 3045 3017 style='mso-fareast-font-family:"Times New Roman"'> – select one of <b 3046 style='mso-bidi-font-weight:normal'>I</b>(<span class=SpellE>sotropic</span>) 3047 or <b style='mso-bidi-font-weight:normal'>A</b>(<span class=SpellE>nisotropic</span>); 3048 the <span class=SpellE><b style='mso-bidi-font-weight:normal'>Uiso</b></span><b 3049 style='mso-bidi-font-weight:normal'>/<span class=SpellE>Uij</span></b> entries 3050 will change appropriately. <span class=MsoHyperlink><span style='color:windowtext; 3051 text-decoration:none;text-underline:none'><o:p></o:p></span></span></span></p> 3018 style='mso-bidi-font-weight:normal'>I</b>(sotropic) or <b style='mso-bidi-font-weight: 3019 normal'>A</b>(nisotropic); the <b style='mso-bidi-font-weight:normal'>Uiso/Uij</b> 3020 entries will change appropriately. <span class=MsoHyperlink><span 3021 style='color:windowtext;text-decoration:none;text-underline:none'><o:p></o:p></span></span></span></p> 3052 3022 3053 3023 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: … … 3079 3049 appears with a list of atom parameter names; select one to apply to all 3080 3050 selected atoms. <b style='mso-bidi-font-weight:normal'>Name</b> will rename 3081 selected atoms according to position in table (e.g. <span class=GramE>Na(</span>1) 3082 for Na atom as 1<sup>st</sup> atom in list in row ‘0’). <b style='mso-bidi-font-weight: 3083 normal'>Type</b> will give periodic table popup; selected element valence will 3084 be used for all selected atoms and atoms names will be changed. <b 3085 style='mso-bidi-font-weight:normal'>I/A</b> will give popup with choices to be 3086 used for all selected atoms. <span class=SpellE><span class=GramE><b 3087 style='mso-bidi-font-weight:normal'>x,y</b></span><b style='mso-bidi-font-weight: 3088 normal'>,z</b></span> will give popup for shift to be applied to the parameter 3089 for all selected atoms. <span class=SpellE><b style='mso-bidi-font-weight:normal'>Uiso</b></span> 3090 and <b style='mso-bidi-font-weight:normal'>frac</b> will give popup for new value 3091 to be used for all selected atoms. </p> 3051 selected atoms according to position in table (e.g. Na(1) for Na atom as 1<sup>st</sup> 3052 atom in list in row ‘0’). <b style='mso-bidi-font-weight:normal'>Type</b> will 3053 give periodic table popup; selected element valence will be used for all 3054 selected atoms and atoms names will be changed. <b style='mso-bidi-font-weight: 3055 normal'>I/A</b> will give popup with choices to be used for all selected atoms. 3056 <b style='mso-bidi-font-weight:normal'>x,y,z</b> will give popup for shift to 3057 be applied to the parameter for all selected atoms. <b style='mso-bidi-font-weight: 3058 normal'>Uiso</b> and <b style='mso-bidi-font-weight:normal'>frac</b> will give 3059 popup for new value to be used for all selected atoms. </p> 3092 3060 3093 3061 <p class=MsoListParagraphCxSpMiddle style='margin-left:2.0in;mso-add-space: … … 3108 3076 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>5.<span 3109 3077 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3110 style='mso-bidi-font-weight:normal'>Insert atom</b> – insert an H atom (name= <span3111 class=SpellE>Unk</span>) at 0,0,0 before the selected atom, it is also drawn as 3112 an H atom in thestructure plot (small white ball).</p>3078 style='mso-bidi-font-weight:normal'>Insert atom</b> – insert an H atom (name= 3079 Unk) at 0,0,0 before the selected atom, it is also drawn as an H atom in the 3080 structure plot (small white ball).</p> 3113 3081 3114 3082 <p class=MsoListParagraphCxSpMiddle style='margin-left:2.0in;mso-add-space: … … 3117 3085 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3118 3086 style='mso-bidi-font-weight:normal'>Insert viewpoint</b> – insert an H atom 3119 (name= <span class=SpellE>Unk</span>) before the selected atom with coordinates 3120 matching the location of the viewpoint, it is also drawn as an H atom in the 3121 structure plot.</p> 3087 (name= Unk) before the selected atom with coordinates matching the location of 3088 the viewpoint, it is also drawn as an H atom in the structure plot.</p> 3122 3089 3123 3090 <p class=MsoListParagraphCxSpMiddle style='margin-left:2.0in;mso-add-space: … … 3165 3132 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>b.<span 3166 3133 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3167 style='mso-bidi-font-weight:normal'>Append atom</b> – add an H atom (name= <span3168 class=SpellE>Unk</span>) at 0,0,0 to the end of the atom table, it is also 3169 drawn as an H atom in thestructure plot.</p>3134 style='mso-bidi-font-weight:normal'>Append atom</b> – add an H atom (name= Unk) 3135 at 0,0,0 to the end of the atom table, it is also drawn as an H atom in the 3136 structure plot.</p> 3170 3137 3171 3138 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3174 3141 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3175 3142 style='mso-bidi-font-weight:normal'>Append viewpoint</b> – add an H atom (name= 3176 <span class=SpellE>Unk</span>) to the end of the atom table with coordinates 3177 matching the location of the viewpoint, it is drawn as an H atom in the 3178 structure plot.</p> 3143 Unk) to the end of the atom table with coordinates matching the location of the 3144 viewpoint, it is drawn as an H atom in the structure plot.</p> 3179 3145 3180 3146 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3212 3178 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3213 3179 style='mso-bidi-font-weight:normal'>Reimport atoms </b>– from any importable 3214 phase file (<span class=GramE>e.g.</span> <span class=SpellE>cif</span>, <span 3215 class=SpellE>gpx</span>)</p> 3180 phase file (e.g. cif, gpx)</p> 3216 3181 3217 3182 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: … … 3226 3191 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3227 3192 style='mso-bidi-font-weight:normal'>Show Distances & Angles – </b>compute 3228 distances and angles with <span class=SpellE>esds</span> (if possible) for 3229 selected atoms. A popup dialog box will appear with distance angle controls. 3230 NB: if atoms have been added or their type changed, you may need to do a <b 3231 style='mso-bidi-font-weight:normal'>Reset</b> of this dialog box before 3232 proceeding.</p> 3193 distances and angles with esds (if possible) for selected atoms. A popup dialog 3194 box will appear with distance angle controls. NB: if atoms have been added or 3195 their type changed, you may need to do a <b style='mso-bidi-font-weight:normal'>Reset</b> 3196 of this dialog box before proceeding.</p> 3233 3197 3234 3198 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3236 3200 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>b.<span 3237 3201 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3238 style='mso-bidi-font-weight:normal'>Save Distances & Angles –</b> same as 3239 a. but reports result to a file with extension <span class=GramE>“.<span 3240 class=SpellE>disagl</span></span>”.</p> 3202 style='mso-bidi-font-weight:normal'>Save Distances & Angles –</b> same as a. 3203 but reports result to a file with extension “.disagl”.</p> 3241 3204 3242 3205 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3311 3274 in/out) <o:p></o:p></span></p> 3312 3275 3313 <p class=MsoNormal style='margin-left:1.25in'><span class=SpellE><b><span 3314 style='mso-fareast-font-family:"Times New Roman"'>Shift+Left</span></b></span><b><span 3315 style='mso-fareast-font-family:"Times New Roman"'> Click</span></b><span 3316 style='mso-fareast-font-family:"Times New Roman"'>: <o:p></o:p></span></p> 3276 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: 3277 "Times New Roman"'>Shift+Left Click</span></b><span style='mso-fareast-font-family: 3278 "Times New Roman"'>: <o:p></o:p></span></p> 3317 3279 3318 3280 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: … … 3324 3286 this way. <o:p></o:p></span></p> 3325 3287 3326 <p class=MsoNormal style='margin-left:1.25in'><span class=SpellE><b><span 3327 style='mso-fareast-font-family:"Times New Roman"'>Shift+Right</span></b></span><b><span 3328 style='mso-fareast-font-family:"Times New Roman"'> click</span></b><span 3329 style='mso-fareast-font-family:"Times New Roman"'>: <o:p></o:p></span></p> 3288 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: 3289 "Times New Roman"'>Shift+Right click</span></b><span style='mso-fareast-font-family: 3290 "Times New Roman"'>: <o:p></o:p></span></p> 3330 3291 3331 3292 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 3332 3293 "Times New Roman"'>Holding down the shift key while clicking on an atom with 3333 3294 the right mouse button causes the atom to be selected if previously unselected 3334 and unselected if previously selected. Any previously selected atoms will be <span3335 c lass=GramE>continue</span> to be selected so shift-right click can be used to3336 add atoms to the selection list. If two atoms are overlapped in the current 3337 view, then the top-most atom will usually be selected. Only atoms in the 3338 asymmetric unit can be selected from the plot in this way. (On a Mac, <span3339 class=SpellE>control+mouse</span> click is analternate way to do this.) <o:p></o:p></span></p>3295 and unselected if previously selected. Any previously selected atoms will be 3296 continue to be selected so shift-right click can be used to add atoms to the 3297 selection list. If two atoms are overlapped in the current view, then the 3298 top-most atom will usually be selected. Only atoms in the asymmetric unit can 3299 be selected from the plot in this way. (On a Mac, control+mouse click is an 3300 alternate way to do this.) <o:p></o:p></span></p> 3340 3301 3341 3302 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: … … 3376 3337 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 3377 3338 "Times New Roman"'>Pressing the “k” key cycles through the possible slice 3378 contouring options (none, lines, colors, <span class=SpellE>lines+colors</span>)<o:p></o:p></span></p>3339 contouring options (none, lines, colors, lines+colors)<o:p></o:p></span></p> 3379 3340 3380 3341 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: … … 3391 3352 3392 3353 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 3393 "Times New Roman"'>Pressing the “<span class=GramE>-“ key</span> steps the 3394 viewpoint in negative drawing z-direction (toward from viewer). If structure is 3395 incommensurate, “-” steps the structure and map through the 4<sup>th</sup> 3396 dimension (-tau).<o:p></o:p></span></p> 3354 "Times New Roman"'>Pressing the “-“ key steps the viewpoint in negative drawing 3355 z-direction (toward from viewer). If structure is incommensurate, “-” steps the 3356 structure and map through the 4<sup>th</sup> dimension (-tau).<o:p></o:p></span></p> 3397 3357 3398 3358 <h4 style='margin-left:.25in'><a name="Phase-Draw_Options"><u>Draw Options</u></a></h4> … … 3401 3361 3402 3362 <p class=MsoNormal style='margin-left:.75in'>The Draw Options window provides 3403 access to <span class=GramE>a number of</span> items that control how the 3404 structure is displayed. If a map is available (Fourier of charge flipping), one 3405 can display a 10<span style='font-family:"Calibri",sans-serif'>Å</span>x10<span 3406 style='font-family:"Calibri",sans-serif'>Å</span> contoured slice centered at 3407 the viewpoint. Contouring done as lines, colors or lines & colors combined. 3408 3-D contouring is also available as green (red for negative density) map grid 3409 points. One can also draw individual or stack of <span class=SpellE>hkl</span> 3410 planes across unit cell.</p> 3363 access to a number of items that control how the structure is displayed. If a 3364 map is available (Fourier of charge flipping), one can display a 10<span 3365 style='font-family:"Calibri",sans-serif'>Å</span>x10<span style='font-family: 3366 "Calibri",sans-serif'>Å</span> contoured slice centered at the viewpoint. 3367 Contouring done as lines, colors or lines & colors combined. 3-D contouring 3368 is also available as green (red for negative density) map grid points. One can 3369 also draw individual or stack of hkl planes across unit cell.</p> 3411 3370 3412 3371 <h5 style='margin-left:.5in'>What is drawn here?</h5> … … 3428 3387 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>This 3429 3388 gives a list of the atoms and bonds that are to be rendered as lines, van der 3430 Waals radii balls, sticks, balls & sticks, ellipsoids & sticks or <span3431 class=SpellE>polyhedra</span>. There are four menus for this tab; Edit allows 3432 modification of the list of atoms to be rendered, Compute gives some options 3433 for geometric characterization of selected atoms, Restraints allows definition 3434 of 4 different types of restraints on the structure and Rigid body allows 3435 selection of atoms that forma previously defined rigid body.</p>3389 Waals radii balls, sticks, balls & sticks, ellipsoids & sticks or 3390 polyhedra. There are four menus for this tab; Edit allows modification of the 3391 list of atoms to be rendered, Compute gives some options for geometric characterization 3392 of selected atoms, Restraints allows definition of 4 different types of 3393 restraints on the structure and Rigid body allows selection of atoms that form 3394 a previously defined rigid body.</p> 3436 3395 3437 3396 <h5 style='margin-left:.5in'>What can I do here?</h5> … … 3468 3427 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>3.<span 3469 3428 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3470 style='mso-bidi-font-weight:normal'>Double left <span class=GramE>click</span> 3471 a Name, Type and <span class=SpellE>Sym</span> Op column heading</b>: a dialog 3472 box is shown that allows you to select all atoms with that characteristic. For 3473 example, selecting the Type column will show all the atom types; your choice 3474 will then cause all those atoms to be selected.</p> 3429 style='mso-bidi-font-weight:normal'>Double left click a Name, Type and Sym Op 3430 column heading</b>: a dialog box is shown that allows you to select all atoms 3431 with that characteristic. For example, selecting the Type column will show all 3432 the atom types; your choice will then cause all those atoms to be selected.</p> 3475 3433 3476 3434 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: … … 3478 3436 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>4.<span 3479 3437 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3480 style='mso-bidi-font-weight:normal'>Double left <span class=GramE>click</span> 3481 a Style, Label or Color column</b>: a dialog box is shown that allows you to 3482 select a rendering option for all the atoms. For Color a color choice dialog is 3483 displayed that covers the entire color spectrum. Choose a color by any of the 3484 means available, press the “Add to Custom Colors”, select that color in the 3485 Custom colors display and then press OK. <b style='mso-bidi-font-weight:normal'>NB</b>: 3486 selecting Color will make all atoms have the same color and for Style “blank” 3487 means the atoms aren’t rendered and thus the drawing will not show any atoms or 3488 bonds!</p> 3438 style='mso-bidi-font-weight:normal'>Double left click a Style, Label or Color 3439 column</b>: a dialog box is shown that allows you to select a rendering option 3440 for all the atoms. For Color a color choice dialog is displayed that covers the 3441 entire color spectrum. Choose a color by any of the means available, press the 3442 “Add to Custom Colors”, select that color in the Custom colors display and then 3443 press OK. <b style='mso-bidi-font-weight:normal'>NB</b>: selecting Color will 3444 make all atoms have the same color and for Style “blank” means the atoms aren’t 3445 rendered and thus the drawing will not show any atoms or bonds!</p> 3489 3446 3490 3447 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: … … 3495 3452 operations that can be performed on your selected atoms. You must select one or 3496 3453 more atoms before using any of the menu items. Most of these items can also be 3497 accessed by selecting one or more atoms and <span class=GramE>right-clicking</span> 3498 the mouse.</p> 3454 accessed by selecting one or more atoms and right-clicking the mouse.</p> 3499 3455 3500 3456 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3510 3466 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3511 3467 style='mso-bidi-font-weight:normal'>Atom label</b> – select the item to be 3512 shown as a label for each atom in selection. The choices <span class=GramE>are:</span>3513 none, type, nameor number. (NB: atom labelling slows drawing response time).</p>3468 shown as a label for each atom in selection. The choices are: none, type, name 3469 or number. (NB: atom labelling slows drawing response time).</p> 3514 3470 3515 3471 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3540 3496 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>f.<span 3541 3497 style='font:7.0pt "Times New Roman"'> 3542 </span></span></span><![endif]><span class=GramE><b style='mso-bidi-font-weight: 3543 normal'>View point</b></span> – position the plot view point to the first atom 3544 in the selection.</p> 3498 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>View 3499 point</b> – position the plot view point to the first atom in the selection.</p> 3545 3500 3546 3501 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3559 3514 symmetry operator and unit cell translation selected via a dialog display. 3560 3515 Duplicate atom positions are not retained. Any anisotropic thermal displacement 3561 parameters ( <span class=SpellE>Uij</span>) will be transformed as appropriate.</p>3516 parameters (Uij) will be transformed as appropriate.</p> 3562 3517 3563 3518 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3576 3531 draw atoms</b> – apply a symmetry operator and unit cell translation to the set 3577 3532 of selected atoms; they will be changed in place. Any anisotropic thermal 3578 displacement parameters (<span class=SpellE>Uij</span>) will be transformed as 3579 appropriate.</p> 3533 displacement parameters (Uij) will be transformed as appropriate.</p> 3580 3534 3581 3535 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3612 3566 style='mso-bidi-font-weight:normal'>Create void map </b>– by using a grid of 3613 3567 probe positions, locate points outside of normal contact distances within a 3614 structure. Result is a mesh of small blue points in structural voids ( <span3615 class=GramE>e.g.</span>possible locations of missing water molecules).</p>3568 structure. Result is a mesh of small blue points in structural voids (e.g. 3569 possible locations of missing water molecules).</p> 3616 3570 3617 3571 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3621 3575 style='mso-bidi-font-weight:normal'>Delete atoms</b> – clear the entire draw 3622 3576 atom table; it is then refilled from the Atoms table. You should do this 3623 operation after any changes in the Atoms table, <span class=GramE>e.g.</span> 3624 by a structure refinement.</p> 3577 operation after any changes in the Atoms table, e.g. by a structure refinement.</p> 3625 3578 3626 3579 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3654 3607 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 3655 3608 style='mso-bidi-font-weight:normal'>View pt. dist.</b> - this calculates 3656 distance from <span class=GramE>view-point</span> to all selected draw atoms;3657 result is given on theconsole window.</p>3609 distance from view-point to all selected draw atoms; result is given on the 3610 console window.</p> 3658 3611 3659 3612 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 3668 3621 for the calculated value if a current variance-covariance matrix is available. 3669 3622 The result is shown on the console window; it may be cut & pasted to 3670 another application ( <span class=GramE>e.g.</span>Microsoft Word).</p>3623 another application (e.g. Microsoft Word).</p> 3671 3624 3672 3625 <p class=MsoListParagraphCxSpLast style='margin-left:1.5in;mso-add-space:auto; … … 3676 3629 style='mso-bidi-font-weight:normal'>Best plane</b> – when 4 or more atoms are 3677 3630 selected, a best plane is determined for them. The result is shown on the 3678 console window; it may be cut & pasted to another application (<span 3679 class=GramE>e.g.</span> Microsoft Word). Shown are the atom coordinates 3680 transformed to Cartesian best plane coordinates where the largest range is over 3681 the X-axis and the smallest is over the Z-axis with the origin at the 3682 unweighted center of the selection. Root mean square displacements along each 3683 axis for the best plane are also listed. The Z-axis RMS value indicates the 3684 flatness of the proposed plane. <b style='mso-bidi-font-weight:normal'>NB</b>: 3685 if you select (<span class=GramE>e.g.</span> all) atoms then Best plane will 3686 give Cartesian coordinates for these atoms with respect to a coordinate system 3687 where the X-axis is along the longest axis of the atom grouping and the Z-axis 3688 is along the shortest distance. The origin is at the unweighted center of the 3689 selected atoms.</p> 3631 console window; it may be cut & pasted to another application (e.g. 3632 Microsoft Word). Shown are the atom coordinates transformed to Cartesian best 3633 plane coordinates where the largest range is over the X-axis and the smallest 3634 is over the Z-axis with the origin at the unweighted center of the selection. 3635 Root mean square displacements along each axis for the best plane are also 3636 listed. The Z-axis RMS value indicates the flatness of the proposed plane. <b 3637 style='mso-bidi-font-weight:normal'>NB</b>: if you select (e.g. all) atoms then 3638 Best plane will give Cartesian coordinates for these atoms with respect to a 3639 coordinate system where the X-axis is along the longest axis of the atom grouping 3640 and the Z-axis is along the shortest distance. The origin is at the unweighted 3641 center of the selected atoms.</p> 3690 3642 3691 3643 <p class=MsoNormal style='margin-left:58.5pt'>7. Menu ‘<b>Restraints’</b> – … … 3696 3648 restraint</b> – for selected atom pair (A-B).</p> 3697 3649 3698 <p class=MsoNormal style='margin-left:1.5in;text-indent:-.25in'><span 3699 class=SpellE>b.</span> <b>Add angle restraint</b> – for selected atom triple 3700 (A-B-C)</p> 3650 <p class=MsoNormal style='margin-left:1.5in;text-indent:-.25in'>b. <b>Add angle 3651 restraint</b> – for selected atom triple (A-B-C)</p> 3701 3652 3702 3653 <p class=MsoNormal style='margin-left:1.5in;text-indent:-.25in'>c. <b>Add plane … … 3757 3708 in/out) <o:p></o:p></span></p> 3758 3709 3759 <p class=MsoNormal style='margin-left:1.25in'><span class=SpellE><b><span 3760 style='mso-fareast-font-family:"Times New Roman"'>Shift+Left</span></b></span><b><span 3761 style='mso-fareast-font-family:"Times New Roman"'> Click</span></b><span 3762 style='mso-fareast-font-family:"Times New Roman"'>: <o:p></o:p></span></p> 3710 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: 3711 "Times New Roman"'>Shift+Left Click</span></b><span style='mso-fareast-font-family: 3712 "Times New Roman"'>: <o:p></o:p></span></p> 3763 3713 3764 3714 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: … … 3770 3720 this way. <o:p></o:p></span></p> 3771 3721 3772 <p class=MsoNormal style='margin-left:1.25in'><span class=SpellE><b><span 3773 style='mso-fareast-font-family:"Times New Roman"'>Shift+Right</span></b></span><b><span 3774 style='mso-fareast-font-family:"Times New Roman"'> click</span></b><span 3775 style='mso-fareast-font-family:"Times New Roman"'>: <o:p></o:p></span></p> 3722 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: 3723 "Times New Roman"'>Shift+Right click</span></b><span style='mso-fareast-font-family: 3724 "Times New Roman"'>: <o:p></o:p></span></p> 3776 3725 3777 3726 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 3778 3727 "Times New Roman"'>Holding down the shift key while clicking on an atom with 3779 3728 the right mouse button causes the atom to be selected if previously unselected 3780 and unselected if previously selected. Any previously selected atoms will be <span3781 c lass=GramE>continue</span> to be selected so shift-right click can be used to3782 add atoms to the selection list. If two atoms are overlapped in the current 3783 view, then the top-most atom will usually be selected. Only atoms in the 3784 asymmetric unit can be selected from the plot in this way. (On a Mac, <span3785 class=SpellE>control+mouse</span> click is analternate way to do this.) <o:p></o:p></span></p>3729 and unselected if previously selected. Any previously selected atoms will be 3730 continue to be selected so shift-right click can be used to add atoms to the 3731 selection list. If two atoms are overlapped in the current view, then the 3732 top-most atom will usually be selected. Only atoms in the asymmetric unit can 3733 be selected from the plot in this way. (On a Mac, control+mouse click is an 3734 alternate way to do this.) <o:p></o:p></span></p> 3786 3735 3787 3736 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: … … 3814 3763 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 3815 3764 "Times New Roman"'>Pressing the “s” key brings up a (large) selection of color 3816 schemes for the slice contours. Default – “</span><span class=SpellE>RdYlGn</span><span 3817 style='mso-fareast-font-family:"Times New Roman"'>” (Green – positive, red – 3818 negative & yellow – zero).<o:p></o:p></span></p> 3765 schemes for the slice contours. Default – “</span>RdYlGn<span style='mso-fareast-font-family: 3766 "Times New Roman"'>” (Green – positive, red – negative & yellow – zero).<o:p></o:p></span></p> 3819 3767 3820 3768 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: … … 3823 3771 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 3824 3772 "Times New Roman"'>Pressing the “k” key cycles through the possible slice 3825 contouring options (none, lines, colors, <span class=SpellE>lines+colors</span>)<o:p></o:p></span></p>3773 contouring options (none, lines, colors, lines+colors)<o:p></o:p></span></p> 3826 3774 3827 3775 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: … … 3832 3780 a movie file of the change in the structure along the 4<sup>th</sup> dimension 3833 3781 (tau). Movie controls are found in the GSAS-II <a href="#Preferences">Configuration 3834 Variables</a>. Requires the <span class=SpellE>imageio</span> python package be 3835 available for import – it is not normally available in the GSAS-II version of 3836 python.<o:p></o:p></span></p> 3782 Variables</a>. Requires the imageio python package be available for import – it 3783 is not normally available in the GSAS-II version of python.<o:p></o:p></span></p> 3837 3784 3838 3785 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: … … 3848 3795 3849 3796 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 3850 "Times New Roman"'>Pressing the “<span class=GramE>-“ key</span> steps the 3851 viewpoint in negative drawing z-direction (away from viewer). If structure is 3852 incommensurate, “-” steps the structure and map through the 4<sup>th</sup> 3853 dimension (-tau).<o:p></o:p></span></p> 3797 "Times New Roman"'>Pressing the “-“ key steps the viewpoint in negative drawing 3798 z-direction (away from viewer). If structure is incommensurate, “-” steps the 3799 structure and map through the 4<sup>th</sup> dimension (-tau).<o:p></o:p></span></p> 3854 3800 3855 3801 <h4 style='margin-left:.25in'><a name="Phase-RB_Models">RB Models</a></h4> … … 3900 3846 in/out) <o:p></o:p></span></p> 3901 3847 3902 <p style='margin-left:1.0in'>When a rigid body is being inserted into a structure, 3903 both the rigid body and the crystal structure are displayed. It is useful to 3904 plan for this by preselecting the atoms in the Draw Atoms list and to have 3905 atoms displayed as "Sticks" or "Ball-and-Sticks." The rigid 3906 body will be displayed as "Ball-and-Sticks<span class=GramE>"</span> 3907 but bonds will be in green. Use of the Alt key causes the above mouse movements 3908 to reposition the rigid body rather than change the view of the crystal 3909 structure:</p> 3910 3911 <p class=MsoNormal style='margin-left:1.25in'><span class=SpellE><b><span 3912 style='mso-fareast-font-family:"Times New Roman"'>Alt+Left</span></b></span><b><span 3913 style='mso-fareast-font-family:"Times New Roman"'> drag</span></b><span 3914 style='mso-fareast-font-family:"Times New Roman"'>: <o:p></o:p></span></p> 3848 <p style='margin-left:1.0in'>When a rigid body is being inserted into a 3849 structure, both the rigid body and the crystal structure are displayed. It is 3850 useful to plan for this by preselecting the atoms in the Draw Atoms list and to 3851 have atoms displayed as "Sticks" or "Ball-and-Sticks." The 3852 rigid body will be displayed as "Ball-and-Sticks" but bonds will be 3853 in green. Use of the Alt key causes the above mouse movements to reposition the 3854 rigid body rather than change the view of the crystal structure:</p> 3855 3856 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: 3857 "Times New Roman"'>Alt+Left drag</span></b><span style='mso-fareast-font-family: 3858 "Times New Roman"'>: <o:p></o:p></span></p> 3915 3859 3916 3860 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: … … 3918 3862 down rotates the rigid body around screen x & y axes <o:p></o:p></span></p> 3919 3863 3920 <p class=MsoNormal style='margin-left:1.25in'><span class=SpellE><b><span 3921 style='mso-fareast-font-family:"Times New Roman"'>Alt+Middle</span></b></span><b><span 3922 style='mso-fareast-font-family:"Times New Roman"'> drag</span></b><span 3923 style='mso-fareast-font-family:"Times New Roman"'>: <o:p></o:p></span></p> 3864 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: 3865 "Times New Roman"'>Alt+Middle drag</span></b><span style='mso-fareast-font-family: 3866 "Times New Roman"'>: <o:p></o:p></span></p> 3924 3867 3925 3868 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: … … 3927 3870 down rotates the rigid body around screen z axis (out of screen) <o:p></o:p></span></p> 3928 3871 3929 <p class=MsoNormal style='margin-left:1.25in'><span class=SpellE><b><span 3930 style='mso-fareast-font-family:"Times New Roman"'>Alt+Right</span></b></span><b><span 3931 style='mso-fareast-font-family:"Times New Roman"'> drag</span></b><span 3932 style='mso-fareast-font-family:"Times New Roman"'>: <o:p></o:p></span></p> 3872 <p class=MsoNormal style='margin-left:1.25in'><b><span style='mso-fareast-font-family: 3873 "Times New Roman"'>Alt+Right drag</span></b><span style='mso-fareast-font-family: 3874 "Times New Roman"'>: <o:p></o:p></span></p> 3933 3875 3934 3876 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 3935 "Times New Roman"'>Holding Alt while dragging the mouse with the right button 3936 down translates the rigid body in the screen x & y directions (rotate the 3937 plotto see and move in the rigid body in the third direction.) Pressing the3877 "Times New Roman"'>Holding Alt while dragging the mouse with the right button down 3878 translates the rigid body in the screen x & y directions (rotate the plot 3879 to see and move in the rigid body in the third direction.) Pressing the 3938 3880 "Lock" checkbox next to the origin location prevents the origin from 3939 3881 being changed in this way. <o:p></o:p></span></p> … … 3952 3894 the <a href="#Data">"Data" tab</a>) in a structural study. The sample 3953 3895 orientation relative to the detector axes is specified here and the detector 3954 orientation is specified for each histogram as goniometer omega, chi, <span 3955 class=GramE>phi</span> and azimuth values (details below). These values must be 3956 specified. </p> 3896 orientation is specified for each histogram as goniometer omega, chi, phi and 3897 azimuth values (details below). These values must be specified. </p> 3957 3898 3958 3899 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><o:p> </o:p></p> … … 3960 3901 <p class=MsoNormal style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; 3961 3902 margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>Texture 3962 analysis using GSAS-II employs spherical harmonics modeling, as described by 3963 Bunge, "Texture Analysis in Materials Science" (1982), and 3964 implemented by Von Dreele, J. Appl. <span class=SpellE>Cryst</span>., <b 3965 style='mso-bidi-font-weight:normal'>30</b>, 517-525 (1997) in GSAS. The even 3966 part of the orientation distribution function (ODF) via the general axis 3967 equation</p> 3903 analysis using GSAS-II employs spherical harmonics modeling, as described by Bunge, 3904 "Texture Analysis in Materials Science" (1982), and implemented by 3905 Von Dreele, J. Appl. Cryst., <b style='mso-bidi-font-weight:normal'>30</b>, 3906 517-525 (1997) in GSAS. The even part of the orientation distribution function 3907 (ODF) via the general axis equation</p> 3968 3908 3969 3909 <p class=MsoNormal style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; … … 3998 3938 mso-ascii-font-family:"Cambria Math";mso-hansi-font-family:"Cambria Math"; 3999 3939 font-style:italic;mso-bidi-font-style:normal'><m:ctrlPr></m:ctrlPr></span></m:naryPr><m:sub><i 4000 style='mso-bidi-font-style:normal'><span style='font-family:"Cambria Math",serif'><m:r>n</m:r><m:r>= -</m:r><m:r>L</m:r></span></i></m:sub><m:sup><i3940 style='mso-bidi-font-style:normal'><span style='font-family:"Cambria Math",serif'><m:r>n</m:r><m:r>=</m:r><m:r>-</m:r><m:r>L</m:r></span></i></m:sub><m:sup><i 4001 3941 style='mso-bidi-font-style:normal'><span style='font-family:"Cambria Math",serif'><m:r>L</m:r></span></i></m:sup><m:e><m:sSubSup><m:sSubSupPr><span 4002 3942 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; … … 4026 3966 <v:imagedata src="gsasII-phase_files/image003.png" o:title="" chromakey="white"/> 4027 3967 </v:shape><![endif]--><![if !vml]><img width=357 height=56 4028 src="gsasII-phase_files/image0 50.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p>3968 src="gsasII-phase_files/image004.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p> 4029 3969 4030 3970 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; … … 4048 3988 <v:imagedata src="gsasII-phase_files/image005.png" o:title="" chromakey="white"/> 4049 3989 </v:shape><![endif]--><![if !vml]><img width=44 height=35 4050 src="gsasII-phase_files/image0 51.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span3990 src="gsasII-phase_files/image006.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span 4051 3991 style='mso-spacerun:yes'> </span>and <!--[if gte msEquation 12]><m:oMath><m:sSubSup><m:sSubSupPr><span 4052 3992 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; … … 4064 4004 <v:imagedata src="gsasII-phase_files/image007.png" o:title="" chromakey="white"/> 4065 4005 </v:shape><![endif]--><![if !vml]><img width=40 height=35 4066 src="gsasII-phase_files/image0 52.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>,4006 src="gsasII-phase_files/image008.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>, 4067 4007 take on values according to the sample and crystal symmetries, respectively, 4068 4008 and thus the two inner summations are over only the resulting unique, nonzero … … 4090 4030 <v:imagedata src="gsasII-phase_files/image007.png" o:title="" chromakey="white"/> 4091 4031 </v:shape><![endif]--><![if !vml]><img width=40 height=35 4092 src="gsasII-phase_files/image0 52.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>,4032 src="gsasII-phase_files/image008.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>, 4093 4033 is defined for each reflection, h, <i>via</i> polar and azimuthal coordinates (<span 4094 4034 style='font-family:Symbol'>f</span>, <span style='font-family:Symbol'>b</span>) 4095 4035 of a unit vector coincident with h relative to the reciprocal lattice. For most 4096 4036 crystal symmetries, <span style='font-family:Symbol'>f</span> is the angle 4097 between h and the n- <span class=SpellE>th</span> order major rotation axis of4098 the space group (usually the c-axis) and <span style='font-family:Symbol'>b</span>4099 is the angle between the projections of h and any secondary axis (usuallythe4100 a-axis) onto the normal plane.<span style='mso-spacerun:yes'> </span>In a 4101 s imilar way the sample harmonic factor, <!--[if gte msEquation 12]><m:oMath><m:sSubSup><m:sSubSupPr><span4037 between h and the n-th order major rotation axis of the space group (usually 4038 the c-axis) and <span style='font-family:Symbol'>b</span> is the angle between 4039 the projections of h and any secondary axis (usually the a-axis) onto the 4040 normal plane.<span style='mso-spacerun:yes'> </span>In a similar way the 4041 sample harmonic factor, <!--[if gte msEquation 12]><m:oMath><m:sSubSup><m:sSubSupPr><span 4102 4042 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; 4103 4043 mso-hansi-font-family:"Cambria Math";font-style:italic;mso-bidi-font-style: … … 4114 4054 <v:imagedata src="gsasII-phase_files/image009.png" o:title="" chromakey="white"/> 4115 4055 </v:shape><![endif]--><![if !vml]><img width=44 height=35 4116 src="gsasII-phase_files/image0 53.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>,4056 src="gsasII-phase_files/image010.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>, 4117 4057 is defined according to polar and azimuthal coordinates (<span 4118 4058 style='font-family:Symbol'>y</span>, <span style='font-family:Symbol'>g</span>) … … 4188 4128 <v:imagedata src="gsasII-phase_files/image011.png" o:title="" chromakey="white"/> 4189 4129 </v:shape><![endif]--><![if !vml]><img width=428 height=56 4190 src="gsasII-phase_files/image0 54.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><br>4130 src="gsasII-phase_files/image012.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><br> 4191 4131 Note that this version of the general axis equation differs from that shown in 4192 4132 Von Dreele (1997) in that the assignment of m and n are reversed. </p> … … 4196 4136 a diffraction experiment the crystal reflection coordinates (<span 4197 4137 style='font-family:Symbol'>f</span>, <span style='font-family:Symbol'>b</span>) 4198 are determined by the choice of reflection index ( <span class=SpellE>hkl</span>)4199 while the sample coordinates (<span style='font-family:Symbol'>y</span>, <span 4200 style='font-family:Symbol'>g</span>) are determined by the sample orientation 4201 on the diffractometer. To define the sample coordinates (<span 4202 style='font-family:Symbol'>y</span>, <span style='font-family:Symbol'>g</span>), 4203 we have defined an instrument coordinate system (I, J, K) such that K is normal 4204 to thediffraction plane and J is coincident with the direction of the incident4138 are determined by the choice of reflection index (hkl) while the sample 4139 coordinates (<span style='font-family:Symbol'>y</span>, <span style='font-family: 4140 Symbol'>g</span>) are determined by the sample orientation on the 4141 diffractometer. To define the sample coordinates (<span style='font-family: 4142 Symbol'>y</span>, <span style='font-family:Symbol'>g</span>), we have defined 4143 an instrument coordinate system (I, J, K) such that K is normal to the 4144 diffraction plane and J is coincident with the direction of the incident 4205 4145 radiation beam toward the source. We further define a standard set of 4206 4146 right-handed eulerian goniometer angles (<span style='font-family:Symbol'>W</span>, … … 4236 4176 normal'><span style='font-family:Symbol'>F</span>+</b><b style='mso-bidi-font-weight: 4237 4177 normal'><span style='font-family:Symbol'>F</span><sub>s</sub>)</b><b 4238 style='mso-bidi-font-weight:normal'><span style='font-family:Symbol'>C</span><s pan4239 class=SpellE><sub>s</sub><span style='font-family:Symbol'>W</span><sub>s</sub></span><o:p></o:p></b></p>4178 style='mso-bidi-font-weight:normal'><span style='font-family:Symbol'>C</span><sub>s</sub></b><b 4179 style='mso-bidi-font-weight:normal'><span style='font-family:Symbol'>W</span><sub>s</sub><o:p></o:p></b></p> 4240 4180 4241 4181 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; … … 4246 4186 4247 4187 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; 4248 margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>< span4249 class=GramE><i>cos</i>(</span><spanstyle='font-family:Symbol'>y</span>) = <!--[if gte msEquation 12]><m:oMath><i4188 margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><i>cos</i>(<span 4189 style='font-family:Symbol'>y</span>) = <!--[if gte msEquation 12]><m:oMath><i 4250 4190 style='mso-bidi-font-style:normal'><span style='font-family:"Cambria Math",serif'><m:r>M</m:r></span></i><m:d><m:dPr><span 4251 4191 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; … … 4263 4203 top:15.0pt;mso-text-raise:-15.0pt;mso-ansi-language:EN-US;mso-fareast-language: 4264 4204 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 4265 type="#_x0000_t75" style='width:33. 75pt;height:50.25pt'>4205 type="#_x0000_t75" style='width:33.95pt;height:50.2pt'> 4266 4206 <v:imagedata src="gsasII-phase_files/image013.png" o:title="" chromakey="white"/> 4267 4207 </v:shape><![endif]--><![if !vml]><img width=45 height=67 4268 src="gsasII-phase_files/image0 55.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span4208 src="gsasII-phase_files/image014.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span 4269 4209 style='mso-spacerun:yes'> </span>and<span style='mso-spacerun:yes'> </span><i>tan</i>(<span 4270 4210 style='font-family:Symbol'>g</span>) = <!--[if gte msEquation 12]><m:oMath><m:f><m:fPr><m:type … … 4298 4238 top:15.0pt;mso-text-raise:-15.0pt;mso-ansi-language:EN-US;mso-fareast-language: 4299 4239 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 4300 type="#_x0000_t75" style='width:80. 25pt;height:50.25pt'>4240 type="#_x0000_t75" style='width:80.1pt;height:50.2pt'> 4301 4241 <v:imagedata src="gsasII-phase_files/image015.png" o:title="" chromakey="white"/> 4302 4242 </v:shape><![endif]--><![if !vml]><img width=107 height=67 4303 src="gsasII-phase_files/image0 56.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p>4243 src="gsasII-phase_files/image016.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p> 4304 4244 4305 4245 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; … … 4320 4260 <v:imagedata src="gsasII-phase_files/image017.png" o:title="" chromakey="white"/> 4321 4261 </v:shape><![endif]--><![if !vml]><img width=61 height=35 4322 src="gsasII-phase_files/image0 57.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span4262 src="gsasII-phase_files/image018.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span 4323 4263 style='mso-spacerun:yes'> </span>and <!--[if gte msEquation 12]><m:oMath><m:sSubSup><m:sSubSupPr><span 4324 4264 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; … … 4336 4276 <v:imagedata src="gsasII-phase_files/image019.png" o:title="" chromakey="white"/> 4337 4277 </v:shape><![endif]--><![if !vml]><img width=58 height=35 4338 src="gsasII-phase_files/image0 58.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>,4278 src="gsasII-phase_files/image020.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>, 4339 4279 are developed from (those for <!--[if gte msEquation 12]><m:oMath><m:sSubSup><m:sSubSupPr><span 4340 4280 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; … … 4349 4289 top:3.0pt;mso-text-raise:-3.0pt;mso-ansi-language:EN-US;mso-fareast-language: 4350 4290 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 4351 type="#_x0000_t75" style='width:45. 65pt;height:26.35pt'>4291 type="#_x0000_t75" style='width:45.75pt;height:26.25pt'> 4352 4292 <v:imagedata src="gsasII-phase_files/image017.png" o:title="" chromakey="white"/> 4353 4293 </v:shape><![endif]--><![if !vml]><img width=61 height=35 4354 src="gsasII-phase_files/image0 57.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span4294 src="gsasII-phase_files/image018.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span 4355 4295 style='mso-spacerun:yes'> </span>are similar)</p> 4356 4296 … … 4403 4343 "Times New Roman";mso-fareast-theme-font:minor-fareast;mso-ansi-language:EN-US; 4404 4344 mso-fareast-language:EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape 4405 id="_x0000_i1025" type="#_x0000_t75" style='width:158.2 pt;height:42.1pt'>4345 id="_x0000_i1025" type="#_x0000_t75" style='width:158.25pt;height:42pt'> 4406 4346 <v:imagedata src="gsasII-phase_files/image021.png" o:title="" chromakey="white"/> 4407 4347 </v:shape><![endif]--><![if !vml]><img width=211 height=56 4408 src="gsasII-phase_files/image0 59.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p>4348 src="gsasII-phase_files/image022.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p> 4409 4349 4410 4350 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; … … 4425 4365 top:3.0pt;mso-text-raise:-3.0pt;mso-ansi-language:EN-US;mso-fareast-language: 4426 4366 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 4427 type="#_x0000_t75" style='width:30. 95pt;height:26.35pt'>4367 type="#_x0000_t75" style='width:30.75pt;height:26.25pt'> 4428 4368 <v:imagedata src="gsasII-phase_files/image023.png" o:title="" chromakey="white"/> 4429 4369 </v:shape><![endif]--><![if !vml]><img width=41 height=35 4430 src="gsasII-phase_files/image0 60.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>,4370 src="gsasII-phase_files/image024.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>, 4431 4371 are defined via a Fourier expansion as</p> 4432 4372 … … 4478 4418 <v:imagedata src="gsasII-phase_files/image025.png" o:title="" chromakey="white"/> 4479 4419 </v:shape><![endif]--><![if !vml]><img width=199 height=70 4480 src="gsasII-phase_files/image0 61.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p>4420 src="gsasII-phase_files/image026.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p> 4481 4421 4482 4422 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; … … 4531 4471 <v:imagedata src="gsasII-phase_files/image027.png" o:title="" chromakey="white"/> 4532 4472 </v:shape><![endif]--><![if !vml]><img width=205 height=70 4533 src="gsasII-phase_files/image0 62.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p>4473 src="gsasII-phase_files/image028.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p> 4534 4474 4535 4475 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; 4536 4476 margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>for 4537 <span class=SpellE>n</span> odd.<span style='mso-spacerun:yes'> </span>Each sum 4538 is only over either the even or odd values of s, respectively, because of the 4539 properties of the Fouriercoefficients, <!--[if gte msEquation 12]><m:oMath><m:sSubSup><m:sSubSupPr><span4477 n odd.<span style='mso-spacerun:yes'> </span>Each sum is only over either the 4478 even or odd values of s, respectively, because of the properties of the Fourier 4479 coefficients, <!--[if gte msEquation 12]><m:oMath><m:sSubSup><m:sSubSupPr><span 4540 4480 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; 4541 4481 mso-hansi-font-family:"Cambria Math";font-style:italic;mso-bidi-font-style: … … 4552 4492 <v:imagedata src="gsasII-phase_files/image029.png" o:title="" chromakey="white"/> 4553 4493 </v:shape><![endif]--><![if !vml]><img width=29 height=35 4554 src="gsasII-phase_files/image0 63.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>.<span4494 src="gsasII-phase_files/image030.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>.<span 4555 4495 style='mso-spacerun:yes'> </span>These Fourier coefficients are determined so 4556 4496 that the definition </p> … … 4674 4614 "Times New Roman";mso-fareast-theme-font:minor-fareast;mso-ansi-language:EN-US; 4675 4615 mso-fareast-language:EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape 4676 id="_x0000_i1025" type="#_x0000_t75" style='width:408.7pt;height:55. 25pt'>4616 id="_x0000_i1025" type="#_x0000_t75" style='width:408.7pt;height:55.5pt'> 4677 4617 <v:imagedata src="gsasII-phase_files/image031.png" o:title="" chromakey="white"/> 4678 4618 </v:shape><![endif]--><![if !vml]><img width=545 height=74 4679 src="gsasII-phase_files/image0 64.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p>4619 src="gsasII-phase_files/image032.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p> 4680 4620 4681 4621 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; … … 4710 4650 top:3.0pt;mso-text-raise:-3.0pt;mso-ansi-language:EN-US;mso-fareast-language: 4711 4651 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 4712 type="#_x0000_t75" style='width:10 1.9pt;height:26.35pt'>4652 type="#_x0000_t75" style='width:102pt;height:26.25pt'> 4713 4653 <v:imagedata src="gsasII-phase_files/image033.png" o:title="" chromakey="white"/> 4714 4654 </v:shape><![endif]--><![if !vml]><img width=136 height=35 4715 src="gsasII-phase_files/image0 65.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span4655 src="gsasII-phase_files/image034.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span 4716 4656 style='mso-spacerun:yes'> </span>and <!--[if gte msEquation 12]><m:oMath><m:func><m:funcPr><span 4717 4657 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; … … 4743 4683 top:3.0pt;mso-text-raise:-3.0pt;mso-ansi-language:EN-US;mso-fareast-language: 4744 4684 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 4745 type="#_x0000_t75" style='width:94. 3pt;height:26.35pt'>4685 type="#_x0000_t75" style='width:94.5pt;height:26.25pt'> 4746 4686 <v:imagedata src="gsasII-phase_files/image035.png" o:title="" chromakey="white"/> 4747 4687 </v:shape><![endif]--><![if !vml]><img width=126 height=35 4748 src="gsasII-phase_files/image0 66.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span4688 src="gsasII-phase_files/image036.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span 4749 4689 style='mso-spacerun:yes'> </span>are combined depending on the symmetry and the 4750 4690 value of n (or m) along with appropriate normalization coefficients to give the … … 4762 4702 top:3.0pt;mso-text-raise:-3.0pt;mso-ansi-language:EN-US;mso-fareast-language: 4763 4703 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 4764 type="#_x0000_t75" style='width:45. 65pt;height:26.35pt'>4704 type="#_x0000_t75" style='width:45.75pt;height:26.25pt'> 4765 4705 <v:imagedata src="gsasII-phase_files/image037.png" o:title="" chromakey="white"/> 4766 4706 </v:shape><![endif]--><![if !vml]><img width=61 height=35 4767 src="gsasII-phase_files/image0 67.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span4707 src="gsasII-phase_files/image038.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span 4768 4708 style='mso-spacerun:yes'> </span>and <!--[if gte msEquation 12]><m:oMath><m:sSubSup><m:sSubSupPr><span 4769 4709 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; … … 4782 4722 <v:imagedata src="gsasII-phase_files/image039.png" o:title="" chromakey="white"/> 4783 4723 </v:shape><![endif]--><![if !vml]><img width=63 height=35 4784 src="gsasII-phase_files/image0 68.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>.<span4724 src="gsasII-phase_files/image040.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>.<span 4785 4725 style='mso-spacerun:yes'> </span>For cubic crystal symmetry, the term <!--[if gte msEquation 12]><m:oMath><m:sSubSup><m:sSubSupPr><span 4786 4726 style='font-family:"Cambria Math",serif;mso-ascii-font-family:"Cambria Math"; … … 4799 4739 <v:imagedata src="gsasII-phase_files/image037.png" o:title="" chromakey="white"/> 4800 4740 </v:shape><![endif]--><![if !vml]><img width=61 height=35 4801 src="gsasII-phase_files/image0 67.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span4741 src="gsasII-phase_files/image038.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span 4802 4742 style='mso-spacerun:yes'> </span>is obtained directly from the Fourier 4803 4743 expansion</p> … … 4858 4798 <v:imagedata src="gsasII-phase_files/image041.png" o:title="" chromakey="white"/> 4859 4799 </v:shape><![endif]--><![if !vml]><img width=248 height=72 4860 src="gsasII-phase_files/image0 69.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p>4800 src="gsasII-phase_files/image042.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p> 4861 4801 4862 4802 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; … … 4876 4816 <v:imagedata src="gsasII-phase_files/image043.png" o:title="" chromakey="white"/> 4877 4817 </v:shape><![endif]--><![if !vml]><img width=25 height=39 4878 src="gsasII-phase_files/image0 70.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>,4818 src="gsasII-phase_files/image044.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>, 4879 4819 as tabulated by Bunge (1982). </p> 4880 4820 … … 4896 4836 <v:imagedata src="gsasII-phase_files/image045.png" o:title="" chromakey="white"/> 4897 4837 </v:shape><![endif]--><![if !vml]><img width=29 height=35 4898 src="gsasII-phase_files/image0 71.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>,4838 src="gsasII-phase_files/image046.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]>, 4899 4839 and the three sample orientation angles, <span style='font-family:Symbol'>W</span><sub>s</sub>, 4900 4840 <span style='font-family:Symbol'>C</span><sub>s</sub>, <span style='font-family: … … 4912 4852 top:3.0pt;mso-text-raise:-3.0pt;mso-ansi-language:EN-US;mso-fareast-language: 4913 4853 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 4914 type="#_x0000_t75" style='width:21. 8pt;height:26.35pt'>4854 type="#_x0000_t75" style='width:21.75pt;height:26.25pt'> 4915 4855 <v:imagedata src="gsasII-phase_files/image045.png" o:title="" chromakey="white"/> 4916 4856 </v:shape><![endif]--><![if !vml]><img width=29 height=35 4917 src="gsasII-phase_files/image0 71.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span4857 src="gsasII-phase_files/image046.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]><span 4918 4858 style='mso-spacerun:yes'> </span>and the sample orientation angles <span 4919 4859 style='font-family:Symbol'>W</span><sub>s</sub>, <span style='font-family:Symbol'>C</span><sub>s</sub>, … … 4968 4908 "Times New Roman";mso-fareast-theme-font:minor-fareast;mso-ansi-language:EN-US; 4969 4909 mso-fareast-language:EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape 4970 id="_x0000_i1025" type="#_x0000_t75" style='width:180. 5pt;height:54.25pt'>4910 id="_x0000_i1025" type="#_x0000_t75" style='width:180.75pt;height:54pt'> 4971 4911 <v:imagedata src="gsasII-phase_files/image047.png" o:title="" chromakey="white"/> 4972 4912 </v:shape><![endif]--><![if !vml]><img width=241 height=72 4973 src="gsasII-phase_files/image0 72.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p>4913 src="gsasII-phase_files/image048.png" v:shapes="_x0000_i1025"><![endif]></span><![endif]></p> 4974 4914 4975 4915 <p class=gsastext style='margin-top:0in;margin-right:0in;margin-bottom:12.0pt; … … 5019 4959 5020 4960 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>The 5021 usual arrangement here is to have a capillary sample perpendicular to the diffraction5022 plane. The capillary may be spun about its cylinder axis for powder averaging 5023 a nd to impose cylindrical symmetry on the texture which is perpendicular to the5024 diffraction plane. Thus, <span style='font-family:Symbol'>W</span>, <span 5025 style='font-family:Symbol'>F = 0</span> and <span style='font-family:Symbol'>C 5026 =90.</span></p>4961 usual arrangement here is to have a capillary sample perpendicular to the 4962 diffraction plane. The capillary may be spun about its cylinder axis for powder 4963 averaging and to impose cylindrical symmetry on the texture which is 4964 perpendicular to the diffraction plane. Thus, <span style='font-family:Symbol'>W</span>, 4965 <span style='font-family:Symbol'>F = 0</span> and <span style='font-family: 4966 Symbol'>C =90.</span></p> 5027 4967 5028 4968 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>3) … … 5047 4987 <p class=MsoNormal style='margin-left:.75in'>1. Menu ‘<b>Texture/Refine 5048 4988 texture’ </b>– refines the spherical harmonics texture model using the 5049 predetermined values of <span class=SpellE>Prfo</span> for all histogram5050 reflection sets as demonstratedin <a4989 predetermined values of Prfo for all histogram reflection sets as demonstrated 4990 in <a 5051 4991 href="https://subversion.xray.aps.anl.gov/pyGSAS/Tutorials/2DTexture/Texture%20analysis%20of%202D%20data%20in%20GSAS-II.htm">2DTexture</a> 5052 4992 tutorial.</p> … … 5075 5015 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 5076 5016 </span></span></span><![endif]><span style='mso-fareast-font-family:"Times New Roman"'>as 5077 an "Axial pole distribution" which simulates the intensity of a reflection5078 during a phi scan.<o:p></o:p></span></p>5017 an "Axial pole distribution" which simulates the intensity of a 5018 reflection during a phi scan.<o:p></o:p></span></p> 5079 5019 5080 5020 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5085 5025 </span></span></span><![endif]><span style='mso-fareast-font-family:"Times New Roman"'>as 5086 5026 a "pole figure," where a projection of the probability of finding a 5087 pole (<span class=SpellE>hkl</span>) is plotted as a function of sample 5088 orientation.<o:p></o:p></span></p> 5027 pole (hkl) is plotted as a function of sample orientation.<o:p></o:p></span></p> 5089 5028 5090 5029 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5095 5034 </span></span></span><![endif]><span style='mso-fareast-font-family:"Times New Roman"'>as 5096 5035 an "inverse pole figure," where a projection of the probability of 5097 finding all poles (<span class=SpellE>hkls</span>) is plotted for a selected 5098 sample orientation.<o:p></o:p></span></p> 5036 finding all poles (hkls) is plotted for a selected sample orientation.<o:p></o:p></span></p> 5099 5037 5100 5038 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5105 5043 </span></span></span><![endif]><span style='mso-fareast-font-family:"Times New Roman"'>or 5106 5044 as a "3D pole distribution" that shows the probability of finding a 5107 pole (<span class=SpellE>hkl</span>) is plotted as a function of sample 5108 orientation. <o:p></o:p></span></p> 5045 pole (hkl) is plotted as a function of sample orientation. <o:p></o:p></span></p> 5109 5046 5110 5047 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; 5111 5048 margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5112 5049 style='mso-fareast-font-family:"Times New Roman"'>For Axial distribution, pole 5113 figure and 3D pole distribution one must next select the <span class=SpellE>hkl</span>5114 of the desired pole, for Inverse pole figure one must select a sample direction 5115 (typically 0 01).<o:p></o:p></span></p>5050 figure and 3D pole distribution one must next select the hkl of the desired 5051 pole, for Inverse pole figure one must select a sample direction (typically 0 0 5052 1).<o:p></o:p></span></p> 5116 5053 5117 5054 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5162 5099 5163 5100 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: 5164 auto;text-indent:-.25in;mso-list:l9 level1 lfo14;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>< a5165 name=Phase-Pawley><![if !supportLists]><span style='mso-fareast-font-family: 5166 "Times New Roman"'><span style='mso-list:Ignore'>2.<span style='font:7.0pt "Times New Roman"'> 5167 </span></span></span><![endif]>Select the <b style='mso-bidi-font-weight:normal'>mag</b> 5168 column – the entries will be sorted with the largest at the top.</a></p>5101 auto;text-indent:-.25in;mso-list:l9 level1 lfo14;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5102 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>2.<span 5103 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]>Select 5104 the <b style='mso-bidi-font-weight:normal'>mag</b> column – the entries will be 5105 sorted with the largest at the top.</p> 5169 5106 5170 5107 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: 5171 auto;text-indent:-.25in;mso-list:l9 level1 lfo14;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><a 5172 name="Phase-Pawley_reflections"><![if !supportLists]><span style='mso-fareast-font-family:"Times New Roman"'><span 5173 style='mso-list:Ignore'>3.<span style='font:7.0pt "Times New Roman"'> 5174 </span></span></span><![endif]>Select the </a><span class=SpellE><span 5175 style='mso-bookmark:Pawley'><b style='mso-bidi-font-weight:normal'>dzero</b></span></span><span 5176 style='mso-bookmark:Pawley'> column – the entries will be sorted with the 5177 smallest (distance from origin) at the top.</span></p> 5108 auto;text-indent:-.25in;mso-list:l9 level1 lfo14;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5109 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>3.<span 5110 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]>Select 5111 the <b style='mso-bidi-font-weight:normal'>dzero</b> column – the entries will 5112 be sorted with the smallest (distance from origin) at the top.</p> 5178 5113 5179 5114 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: 5180 auto;text-indent:-.25in;mso-list:l9 level1 lfo14;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5181 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5182 "Times New Roman"'><span style='mso-list:Ignore'>4.<span style='font:7.0pt "Times New Roman"'> 5183 </span></span></span><![endif]>Select the <span class=SpellE><b>dcent</b></span> 5184 column – the entries will be sorted with the smallest distance from the unit 5185 cell center at the top.</span></p> 5115 auto;text-indent:-.25in;mso-list:l9 level1 lfo14;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5116 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>4.<span 5117 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]>Select 5118 the <b>dcent</b> column – the entries will be sorted with the smallest distance 5119 from the unit cell center at the top.</p> 5186 5120 5187 5121 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: 5188 auto;text-indent:-.25in;mso-list:l9 level1 lfo14;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5189 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5190 "Times New Roman"'><span style='mso-list:Ignore'>5.<span style='font:7.0pt "Times New Roman"'> 5191 </span></span></span><![endif]>Menu <b style='mso-bidi-font-weight:normal'>‘Map 5192 peaks<span class=GramE>’ <span style='font-weight:normal'><span 5193 style='mso-spacerun:yes'> </span>–</span></span></b></span></p> 5194 5195 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5196 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><span 5197 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5198 "Times New Roman"'><span style='mso-list:Ignore'>a.<span style='font:7.0pt "Times New Roman"'> 5199 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Move 5200 peaks</b> – this copies selected peaks to the </span><a href="#Phase-Atoms"><span 5201 style='mso-bookmark:Pawley'>Atoms</span><span style='mso-bookmark:Pawley'></span></a><span 5202 style='mso-bookmark:Pawley'> list and the </span><a href="#_Draw_Atoms"><span 5203 style='mso-bookmark:Pawley'>Draw Atoms</span><span style='mso-bookmark:Pawley'></span></a><span 5204 style='mso-bookmark:Pawley'> list. They will be appended to the end of each 5205 list each with the name ‘UNK’ and the atom type as ‘H’. They will also be drawn 5206 as small white spheres at their respective positions in the structure drawing. 5207 You should next go to the </span><a href="#Phase-Atoms"><span style='mso-bookmark: 5208 Pawley'>Atoms</span><span style='mso-bookmark:Pawley'></span></a><span 5209 style='mso-bookmark:Pawley'> page and change the atom type to whatever element 5210 you desire; it will be renamed automatically.</span></p> 5211 5212 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5213 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><span 5214 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5215 "Times New Roman"'><span style='mso-list:Ignore'>b.<span style='font:7.0pt "Times New Roman"'> 5216 </span></span></span><![endif]><span class=GramE><b style='mso-bidi-font-weight: 5217 normal'>View point</b></span><b style='mso-bidi-font-weight:normal'> </b>– this 5218 positions the viewpoint (large 3D RGB cross) at the 1<sup>st</sup> selected 5219 peak.</span></p> 5220 5221 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5222 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><span 5223 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5224 "Times New Roman"'><span style='mso-list:Ignore'>c.<span style='font:7.0pt "Times New Roman"'> 5225 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>View pt</b>. 5226 <b style='mso-bidi-font-weight:normal'>dist</b>. – this calculates distance 5227 from viewpoint to all selected map peaks.</span></p> 5228 5229 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5230 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><span 5231 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5232 "Times New Roman"'><span style='mso-list:Ignore'>d.<span style='font:7.0pt "Times New Roman"'> 5233 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Hide/Show 5234 bonds </b>– toggle display of lines (bonds) between peaks</span></p> 5235 5236 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5237 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><span 5238 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5239 "Times New Roman"'><span style='mso-list:Ignore'>e.<span style='font:7.0pt "Times New Roman"'> 5240 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Calc <span 5241 class=SpellE>dist</span>/ang </b>– if 2 peaks are selected, this calculates the 5242 distance between them. If 3 peaks are selected this calculates the angle 5243 between them; NB: selection order matters. If selection is not 2 or 3 peaks 5244 this is ignored. Output is on the console window.</span></p> 5245 5246 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5247 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><span 5248 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5249 "Times New Roman"'><span style='mso-list:Ignore'>f.<span style='font:7.0pt "Times New Roman"'> 5122 auto;text-indent:-.25in;mso-list:l9 level1 lfo14;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5123 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>5.<span 5124 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]>Menu 5125 <b style='mso-bidi-font-weight:normal'>‘Map peaks’ </b><span 5126 style='mso-spacerun:yes'> </span>–</p> 5127 5128 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5129 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5130 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>a.<span 5131 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5132 style='mso-bidi-font-weight:normal'>Move peaks</b> – this copies selected peaks 5133 to the <a href="#Phase-Atoms">Atoms</a> list and the <a href="#_Draw_Atoms">Draw 5134 Atoms</a> list. They will be appended to the end of each list each with the 5135 name ‘UNK’ and the atom type as ‘H’. They will also be drawn as small white 5136 spheres at their respective positions in the structure drawing. You should next 5137 go to the <a href="#Phase-Atoms">Atoms</a> page and change the atom type to 5138 whatever element you desire; it will be renamed automatically.</p> 5139 5140 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5141 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5142 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>b.<span 5143 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5144 style='mso-bidi-font-weight:normal'>View point </b>– this positions the 5145 viewpoint (large 3D RGB cross) at the 1<sup>st</sup> selected peak.</p> 5146 5147 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5148 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5149 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>c.<span 5150 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5151 style='mso-bidi-font-weight:normal'>View pt</b>. <b style='mso-bidi-font-weight: 5152 normal'>dist</b>. – this calculates distance from viewpoint to all selected map 5153 peaks.</p> 5154 5155 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5156 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5157 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>d.<span 5158 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5159 style='mso-bidi-font-weight:normal'>Hide/Show bonds </b>– toggle display of 5160 lines (bonds) between peaks</p> 5161 5162 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5163 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5164 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>e.<span 5165 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5166 style='mso-bidi-font-weight:normal'>Calc dist/ang </b>– if 2 peaks are 5167 selected, this calculates the distance between them. If 3 peaks are selected 5168 this calculates the angle between them; NB: selection order matters. If 5169 selection is not 2 or 3 peaks this is ignored. Output is on the console window.</p> 5170 5171 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5172 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5173 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>f.<span 5174 style='font:7.0pt "Times New Roman"'> 5250 5175 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Equivalent 5251 5176 peaks </b>– this selects all peaks related to selection by space group 5252 symmetry.</ span></p>5253 5254 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5255 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'>< span5256 style='mso- bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family:5257 "Times New Roman"'><span style='mso-list:Ignore'>g.<span style='font:7.0pt "Times New Roman"'> 5258 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Invert 5259 peak positions </b>– inversion through cell center of map and all positions.</span></p>5260 5261 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5262 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'>< span5263 style='mso- bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family:5264 "Times New Roman"'><span style='mso-list:Ignore'>h.<span style='font:7.0pt "Times New Roman"'> 5265 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Roll 5266 charge flip map </b>– popup allows shifting of the map & all peak positions 5267 by unit cell fractions; can be along combinations of axes.</span></p>5268 5269 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5270 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'>< span5271 style='mso- bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family:5272 "Times New Roman"'><span style='mso-list:Ignore'>i.<spanstyle='font:7.0pt "Times New Roman"'> 5177 symmetry.</p> 5178 5179 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5180 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5181 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>g.<span 5182 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5183 style='mso-bidi-font-weight:normal'>Invert peak positions </b>– inversion 5184 through cell center of map and all positions.</p> 5185 5186 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5187 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5188 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>h.<span 5189 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5190 style='mso-bidi-font-weight:normal'>Roll charge flip map </b>– popup allows 5191 shifting of the map & all peak positions by unit cell fractions; can be 5192 along combinations of axes.</p> 5193 5194 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5195 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5196 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>i.<span 5197 style='font:7.0pt "Times New Roman"'> 5273 5198 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Unique 5274 5199 peaks </b>– this selects only the unique peak positions amongst those selected; 5275 5200 a popup allows selection of atom subset closest to x=0, y=0, z=0 origin or 5276 center.</ span></p>5277 5278 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5279 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'>< span5280 style='mso- bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family:5281 "Times New Roman"'><span style='mso-list:Ignore'>j.<spanstyle='font:7.0pt "Times New Roman"'> 5201 center.</p> 5202 5203 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5204 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5205 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>j.<span 5206 style='font:7.0pt "Times New Roman"'> 5282 5207 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Save 5283 peaks </b>– saves the peak list as a csv file.</ span></p>5284 5285 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5286 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'>< span5287 style='mso- bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family:5288 "Times New Roman"'><span style='mso-list:Ignore'>k.<span style='font:7.0pt "Times New Roman"'> 5289 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Delete 5290 peaks </b>– this deletes selected peaks. The shading on the remaining peaks is5291 changed to reflect any change in the maximum after deletion.</span></p>5208 peaks </b>– saves the peak list as a csv file.</p> 5209 5210 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5211 auto;text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5212 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>k.<span 5213 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5214 style='mso-bidi-font-weight:normal'>Delete peaks </b>– this deletes selected 5215 peaks. The shading on the remaining peaks is changed to reflect any change in 5216 the maximum after deletion.</p> 5292 5217 5293 5218 <p class=MsoListParagraphCxSpLast style='margin-left:1.5in;mso-add-space:auto; 5294 text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'>< span5295 style='mso- bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family:5296 "Times New Roman"'><span style='mso-list:Ignore'>l.<spanstyle='font:7.0pt "Times New Roman"'> 5219 text-indent:-.25in;mso-list:l9 level2 lfo14;tab-stops:list 1.0in'><![if !supportLists]><span 5220 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>l.<span 5221 style='font:7.0pt "Times New Roman"'> 5297 5222 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Clear 5298 5223 peaks </b>– this deletes all the peaks in the map peak list; they are also 5299 removed from the crystal structure drawing plot.</span></p> 5300 5301 <h4 style='margin-left:.25in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5302 style='mso-bookmark:Pawley'>Pawley reflections<span class=MsoHyperlink><span 5303 style='color:#5B9BD5;mso-themecolor:accent1'><o:p></o:p></span></span></span></h4> 5304 5305 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5306 style='mso-bookmark:Pawley'>This gives the list of reflections used in a Pawley 5307 refinement and they can only be seen if the ‘Do Pawley refinement’ flag is set 5308 (see </span><a href="#_General_Phase_Parameters"><span style='mso-bookmark: 5309 Pawley'>General</span><span style='mso-bookmark:Pawley'></span></a><span 5310 style='mso-bookmark:Pawley'>).</span></p> 5311 5312 <h5 style='margin-left:.5in'><span style='mso-bookmark:Pawley'>What can I do 5313 here?</span></h5> 5224 removed from the crystal structure drawing plot.</p> 5225 5226 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><a 5227 name="_Pawley_reflections"></a><o:p> </o:p></p> 5228 5229 <h4>Pawley reflections</h4> 5230 5231 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>This 5232 gives the list of reflections used in a Pawley refinement; for them to be used the 5233 ‘Do Pawley refinement’ flag must be set (see <a 5234 href="#_General_Phase_Parameters">General</a>), otherwise they are ignored.</p> 5235 5236 <h5 style='margin-left:.5in'>What can I do here?</h5> 5314 5237 5315 5238 <p class=MsoListParagraphCxSpFirst style='margin-left:1.0in;mso-add-space:auto; 5316 text-indent:-.25in;mso-list:l3 level1 lfo16;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5317 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5318 "Times New Roman"'><span style='mso-list:Ignore'>1.<span style='font:7.0pt "Times New Roman"'> 5319 </span></span></span><![endif]>Menu <b style='mso-bidi-font-weight:normal'>‘Operations’</b> 5320 –</span></p> 5321 5322 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5323 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5324 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5325 "Times New Roman"'><span style='mso-list:Ignore'>a.<span style='font:7.0pt "Times New Roman"'> 5326 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Pawley settings 5327 </b>– allows setting of Pawley parameters as shown on the </span><a 5328 href="#_General_Phase_Parameters"><span style='mso-bookmark:Pawley'>General</span><span 5329 style='mso-bookmark:Pawley'></span></a><span style='mso-bookmark:Pawley'> tab.</span></p> 5330 5331 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5332 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5333 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5334 "Times New Roman"'><span style='mso-list:Ignore'>b.<span style='font:7.0pt "Times New Roman"'> 5335 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Pawley 5336 create</b> – this creates a new set of Pawley reflections, over writing any 5337 preexisting Pawley set. They are generated with d-spacings larger than the 5338 limit set as ‘Pawley <span class=SpellE>dmin</span>’ in the General tab for 5339 this phase. By <span class=GramE>default</span> the refine flags are not set 5340 and the <span class=SpellE>Fsq</span>(<span class=SpellE>hkl</span>) = 100.0.</span></p> 5341 5342 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5343 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5344 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5345 "Times New Roman"'><span style='mso-list:Ignore'>c.<span style='font:7.0pt "Times New Roman"'> 5346 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Pawley 5347 estimate</b> – this attempts an estimate of <span class=SpellE>Fsq</span>(<span 5348 class=SpellE>hkl</span>) from the peak heights of the reflection as seen in the 5349 1<sup>st</sup> powder pattern of those selected in the </span><a href="#_Data"><span 5350 style='mso-bookmark:Pawley'>Data</span><span style='mso-bookmark:Pawley'></span></a><span 5351 style='mso-bookmark:Pawley'> tab.</span></p> 5352 5353 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5354 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5355 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5356 "Times New Roman"'><span style='mso-list:Ignore'>d.<span style='font:7.0pt "Times New Roman"'> 5357 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Pawley 5358 update </b>– process Pawley reflection set for negative intensities. These are 5359 set to ½ its absolute value for noncentrosymmetric space groups (0.3 5360 otherwise); the refine flag is turned off. One should repeat Pawley refinement 5361 and then do </span><span style='mso-bookmark:Pawley'><b><span style='font-family: 5239 text-indent:-.25in;mso-list:l3 level1 lfo16;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5240 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>1.<span 5241 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]>Menu 5242 <b style='mso-bidi-font-weight:normal'>‘Operations’</b> –</p> 5243 5244 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5245 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5246 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>a.<span 5247 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5248 style='mso-bidi-font-weight:normal'>Pawley settings </b>– allows setting of 5249 Pawley parameters as shown on the <a href="#_General_Phase_Parameters">General</a> 5250 tab.</p> 5251 5252 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5253 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5254 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>b.<span 5255 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5256 style='mso-bidi-font-weight:normal'>Pawley create</b> – this creates a new set 5257 of Pawley reflections, over writing any preexisting Pawley set. They are 5258 generated with d-spacings larger than the limit set as ‘Pawley dmin’ in the 5259 General tab for this phase. By default, the refine flags are not set and the 5260 Fsq(hkl) = 100.0.</p> 5261 5262 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5263 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5264 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>c.<span 5265 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5266 style='mso-bidi-font-weight:normal'>Pawley estimate</b> – this attempts an 5267 estimate of Fsq(hkl) from the peak heights of the reflection as seen in the 1<sup>st</sup> 5268 powder pattern of those shown as ‘<b>Use’</b> in the <a href="#_Data">Data</a> 5269 tab for this phase.</p> 5270 5271 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5272 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5273 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>d.<span 5274 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5275 style='mso-bidi-font-weight:normal'>Pawley update </b>– process Pawley 5276 reflection set for negative intensities. These are set to ½ its absolute value 5277 for noncentrosymmetric space groups (0.3 otherwise); the refine flag is turned 5278 off. One should repeat Pawley refinement and then do <b><span style='font-family: 5362 5279 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-hansi-theme-font: 5363 5280 minor-latin;mso-bidi-theme-font:minor-latin'>Refine all</span></b> and an 5364 additional refinement. Repeat as needed to remove negative intensities. Set </span><span 5365 style='mso-bookmark:Pawley'><b><span style='font-family:"Calibri",sans-serif; 5281 additional refinement. Repeat as needed to remove negative intensities. Set <b><span 5282 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 5283 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Pawley neg. 5284 wt.</span></b> (see <b><span style='font-family:"Calibri",sans-serif; 5366 5285 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 5367 minor-latin'>Pawley neg. wt.</span></b> (see </span><span style='mso-bookmark: 5368 Pawley'><b><span style='font-family:"Calibri",sans-serif;mso-ascii-theme-font: 5369 minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Pawley 5370 settings</span></b>) to further suppress negatives.</span></p> 5371 5372 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5373 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5374 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5375 "Times New Roman"'><span style='mso-list:Ignore'>e.<span style='font:7.0pt "Times New Roman"'> 5286 minor-latin'>Pawley settings</span></b>) to further suppress negatives.</p> 5287 5288 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5289 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5290 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>e.<span 5291 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5292 style='mso-bidi-font-weight:normal'>Refine all </b>– sets all refine flags</p> 5293 5294 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5295 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5296 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>f.<span 5297 style='font:7.0pt "Times New Roman"'> 5376 5298 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Refine 5377 all </b>– sets all refine flags</span></p> 5378 5379 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5380 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5381 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5382 "Times New Roman"'><span style='mso-list:Ignore'>f.<span style='font:7.0pt "Times New Roman"'> 5383 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Refine 5384 none </b>– clears all refine flags</span></p> 5385 5386 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5387 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5388 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5389 "Times New Roman"'><span style='mso-list:Ignore'>g.<span style='font:7.0pt "Times New Roman"'> 5390 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'>Toggle 5391 selection </b>– toggles all refine flags</span></p> 5299 none </b>– clears all refine flags</p> 5300 5301 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: 5302 auto;text-indent:-.25in;mso-list:l7 level2 lfo18;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5303 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>g.<span 5304 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5305 style='mso-bidi-font-weight:normal'>Toggle selection </b>– toggles all refine 5306 flags</p> 5392 5307 5393 5308 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: 5394 auto;text-indent:-.25in;mso-list:l3 level1 lfo16;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5395 style='mso-bookmark:Pawley'><![if !supportLists]><span style='mso-fareast-font-family: 5396 "Times New Roman"'><span style='mso-list:Ignore'>2.<span style='font:7.0pt "Times New Roman"'> 5397 </span></span></span><![endif]>You can change the refine flags either by 5398 clicking on the box or by selecting one and then selecting the column (a single 5399 click on the column heading). Then type ‘y’ to set the refine flags or ‘n’ to 5400 clear the flags. You should not refine those reflections that fall below the 5401 lower limit or above the upper limit of the powder pattern otherwise you may 5402 have a singular matrix error in your Pawley refinement.</span></p> 5309 auto;text-indent:-.25in;mso-list:l3 level1 lfo16;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><![if !supportLists]><span 5310 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>2.<span 5311 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]>You 5312 can change the refine flags either by clicking on the box or by selecting one 5313 and then selecting the column (a single click on the column heading). Then type 5314 ‘y’ to set the refine flags or ‘n’ to clear the flags. You should not refine 5315 those reflections that are below the lower limit or above the upper limit of 5316 the powder pattern otherwise you will have singular matrix errors in your 5317 Pawley refinement (adds to the refinement time as bad parameters are removed). 5318 Reflections that fall inside excluded regions may also result in refinement 5319 singularities.</p> 5403 5320 5404 5321 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: … … 5408 5325 can delete an individual reflection from the Pawley set by selecting its row 5409 5326 (will be highlighted) and then pressing the Delete key (this is not reversable 5410 & only <span class=GramE>deletes</span>the 1<sup>st</sup> one selected).</p>5327 & only deletes the 1<sup>st</sup> one selected).</p> 5411 5328 5412 5329 <p class=MsoListParagraphCxSpLast style='margin-left:1.0in;mso-add-space:auto; … … 5414 5331 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>4.<span 5415 5332 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]>You 5416 can change the individual <span class=SpellE>Fsq</span>(<span class=SpellE>hkl</span>) 5417 values by selecting it, typing in the new <span class=GramE>value</span> and 5418 then pressing enter or selecting somewhere else in the table.</p> 5333 can change the individual Fsq(hkl) values by selecting it, typing in the new 5334 value and then pressing enter or selecting somewhere else in the table.</p> 5419 5335 5420 5336 <h4 style='margin-left:.25in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><a … … 5425 5341 <a 5426 5342 href="https://subversion.xray.aps.anl.gov/pyGSAS/Tutorials/StackingFaults-I/Stacking%20Faults-I.htm">Stacking 5427 Faults-I</a> tutorial. The computations are done by a modified version of <span 5428 class=SpellE>DIFFaX</span>. See M.M.J. Treacy, J.M. Newsam and M.W. Deem, Proc. 5429 Roy. Soc. <span class=SpellE>Lond</span>. 433A, 499-520 (1991) for more 5430 information on <span class=SpellE>DIFFaX</span> and please cite this if you use 5431 this section of GSAS-II.</p> 5343 Faults-I</a> tutorial. The computations are done by a modified version of 5344 DIFFaX. See M.M.J. Treacy, J.M. Newsam and M.W. Deem, Proc. Roy. Soc. Lond. 5345 433A, 499-520 (1991) for more information on DIFFaX and please cite this if you 5346 use this section of GSAS-II.</p> 5432 5347 5433 5348 <h5 style='margin-left:.5in'>What can I do here?</h5> … … 5443 5358 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>a.<span 5444 5359 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5445 style='mso-bidi-font-weight:normal'>Load from <span class=SpellE>DIFFaX</span> file 5446 – </b><span style='mso-bidi-font-weight:bold'>load parameters from a <span 5447 class=SpellE>DIFFaX</span> input file</span></p> 5360 style='mso-bidi-font-weight:normal'>Load from DIFFaX file – </b><span 5361 style='mso-bidi-font-weight:bold'>load parameters from a DIFFaX input file</span></p> 5448 5362 5449 5363 <p class=MsoListParagraphCxSpMiddle style='margin-left:99.8pt;mso-add-space: … … 5460 5374 style='mso-list:Ignore'>c.<span style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><b 5461 5375 style='mso-bidi-font-weight:normal'>Simulate pattern – </b><span 5462 style='mso-bidi-font-weight:bold'>run <span class=SpellE>DIFFaX</span> to 5463 simulate selected pattern<o:p></o:p></span></p> 5376 style='mso-bidi-font-weight:bold'>run DIFFaX to simulate selected pattern<o:p></o:p></span></p> 5464 5377 5465 5378 <p class=MsoListParagraphCxSpMiddle style='margin-left:99.8pt;mso-add-space: … … 5515 5428 </span></span></span><![endif]><span style='mso-bidi-font-weight:bold'>Next are 5516 5429 descriptions of the layers to be used in the calculations. They can be created 5517 atom-by-atom or imported from another GSAS-II <span class=SpellE>gpx</span> 5518 file. If a layer is already present, then the new layer can be the same; give 5519 it a different name.<o:p></o:p></span></p> 5430 atom-by-atom or imported from another GSAS-II gpx file. If a layer is already 5431 present, then the new layer can be the same; give it a different name.<o:p></o:p></span></p> 5520 5432 5521 5433 <p class=MsoListParagraphCxSpMiddle style='margin-left:63.8pt;mso-add-space: … … 5551 5463 <p class=MsoNormal style='margin-left:.5in'>This tab displays the modulation 5552 5464 functions used for incommensurate structures; it will not appear if the 5553 structure is commensurate (<span class=GramE>i.e.</span> 3D). They include 5554 modulations on atom site fractions, <span class=GramE>positions</span> and 5555 thermal motion parameters. If the structure is magnetic, atom moment modulation 5556 parameters are also shown.</p> 5465 structure is commensurate (i.e. 3D). They include modulations on atom site 5466 fractions, positions and thermal motion parameters. If the structure is 5467 magnetic, atom moment modulation parameters are also shown.</p> 5557 5468 5558 5469 <h5 style='margin-left:.5in'>What can I do here?</h5> … … 5580 5491 <p class=MsoNormal style='margin-left:.5in'>This tab displays Monte 5581 5492 Carlo/Simulated Annealing model parameters and results. Each rigid body is 5582 described by a location (fractional <span class=SpellE><span class=GramE>x,y</span>,z</span>) 5583 and a quaternion description for the orientation (rotation angle & 3D 5584 vector) along with possible bond torsion angles on side chains. Each parameter 5585 has a defined range. The MC/SA controls on the General tab further limit the 5586 MC/SA run. Selection of a result shows a drawing of the structure with unit 5587 cell contents for visualization.</p> 5493 described by a location (fractional x,y,z) and a quaternion description for the 5494 orientation (rotation angle & 3D vector) along with possible bond torsion 5495 angles on side chains. Each parameter has a defined range. The MC/SA controls 5496 on the General tab further limit the MC/SA run. Selection of a result shows a 5497 drawing of the structure with unit cell contents for visualization.</p> 5588 5498 5589 5499 <h5 style='margin-left:.5in'>What can I do here?</h5> … … 5600 5510 5601 5511 <p class=MsoNormal style='margin-left:49.5pt;text-indent:-49.5pt'><span 5602 style='mso-tab-count:2'> </span> <span class=SpellE>b.</span>5603 <b>Add rigid body</b> – add a previously defined rigid body, which may have 5604 adjustable internaltorsion angles.</p>5512 style='mso-tab-count:2'> </span>b. <b>Add rigid body</b> 5513 – add a previously defined rigid body, which may have adjustable internal 5514 torsion angles.</p> 5605 5515 5606 5516 <p class=MsoNormal style='margin-left:49.5pt;text-indent:-49.5pt'><span … … 5616 5526 <p class=MsoNormal style='margin-left:.5in'>This displays 3 different setups 5617 5527 each for <a href="https://doi.org/10.1088/0953-8984/19/33/335218">RMCProfile</a>, 5618 <a href="https://doi.org/10.1002/jcc.24304"><span class=SpellE>fullrmc</span></a> 5619 and <a href="https://doi.org/10.1088/0953-8984/19/33/335219"><span 5620 class=SpellE>PDFfit</span></a> as selected by a radio button at the top of the 5621 window. RMCProfile and <span class=SpellE>fullrmc</span> are “big box” 5622 modelling routines and <span class=SpellE>PDFfit</span> is a “small box” 5623 modelling routine; all for fitting structural models to pair distribution 5624 functions (PDF). Tutorials for using RMCProfile and <span class=SpellE>PDFfit</span> 5625 can be found in the GSAS-II Help; <span class=SpellE>fullrmc</span> is 5528 <a href="https://doi.org/10.1002/jcc.24304">fullrmc</a> and <a 5529 href="https://doi.org/10.1088/0953-8984/19/33/335219">PDFfit</a> as selected by 5530 a radio button at the top of the window. RMCProfile and fullrmc are “big box” 5531 modelling routines and PDFfit is a “small box” modelling routine; all for 5532 fitting structural models to pair distribution functions (PDF). Tutorials for 5533 using RMCProfile and PDFfit can be found in the GSAS-II Help; fullrmc is 5626 5534 currently under construction. These routines all run as stand-alone 5627 5535 applications which are initiated by GSAS-II. When finished, GSAS-II processes … … 5629 5537 The two big box routines can have very long running times; they run as separate 5630 5538 console programs. GSAS-II is active while they are running and can 5631 “interrogate” them for intermediate results. <span class=SpellE>PDFfit</span>5632 has a short running time and GSAS-II is “locked out” until it finishes; its 5633 result can be examinedafter.</p>5539 “interrogate” them for intermediate results. PDFfit has a short running time 5540 and GSAS-II is “locked out” until it finishes; its result can be examined 5541 after.</p> 5634 5542 5635 5543 <h5 style='margin-left:.5in'>What can I do here?</h5> … … 5639 5547 5640 5548 <p class=MsoNormal style='margin-left:.75in;tab-stops:.75in'><span 5641 style='mso-tab-count:1'> </span>1. <b>Setup RMC</b> – this builds the input5642 files and python script (if needed) for running the selected RMC program.</p>5549 style='mso-tab-count:1'> </span>1. <b>Setup RMC</b> – this builds the 5550 input files and python script (if needed) for running the selected RMC program.</p> 5643 5551 5644 5552 <p class=MsoNormal style='margin-left:1.0in;tab-stops:1.0in'><span 5645 5553 style='mso-tab-count:1'> </span>2. <b>Execute</b> – this executes 5646 5554 the chosen RMC program in a new console which will vanish when finishes (after 5647 a “press any key” command). When finished, GSAS-II will extract results and 5648 placethem in appropriate places in the project.</p>5555 a “press any key” command). When finished, GSAS-II will extract results and place 5556 them in appropriate places in the project.</p> 5649 5557 5650 5558 <p class=MsoNormal style='margin-left:1.0in;tab-stops:1.0in'>3. <b>Stop run</b> 5651 – only valid for <span class=SpellE>fullrmc</span>; stops the RMC run &5652 saves progress so it can becontinued later.</p>5559 – only valid for fullrmc; stops the RMC run & saves progress so it can be 5560 continued later.</p> 5653 5561 5654 5562 <p class=MsoNormal style='margin-left:1.0in;tab-stops:1.0in'>4. <b>Plot</b> – 5655 5563 this displays the resulting graphical output from the RMC run. For RMCProfile 5656 and <span class=SpellE>fullrmc</span> this can be 5 or more plots, for <span 5657 class=SpellE>PDFfit</span> it is only the observed and calculated G(r) plot 5658 with a difference curve.</p> 5564 and fullrmc this can be 5 or more plots, for PDFfit it is only the observed and 5565 calculated G(r) plot with a difference curve.</p> 5659 5566 5660 5567 <p class=MsoNormal style='margin-left:1.0in;tab-stops:1.0in'><o:p> </o:p></p> … … 5663 5570 similar. There is a block for “metadata” items for your convenience; they have 5664 5571 no impact on the calculations. Next is timing controls for the big box programs 5665 (<span class=SpellE>PDFfit</span> has none). Then is structural information and 5666 finally the data section for the patterns to be fitted. The big box programs 5667 are for only single runs while <span class=SpellE>PDFfit</span> can be used to 5668 process a sequence of G(r) data collected as a function of, e.g., temperature 5669 (giving Sequential PDFfit2 results).</p> 5572 (PDFfit has none). Then is structural information and finally the data section 5573 for the patterns to be fitted. The big box programs are for only single runs 5574 while PDFfit can be used to process a sequence of G(r) data collected as a 5575 function of, e.g., temperature (giving Sequential PDFfit2 results).</p> 5670 5576 5671 5577 <h4 style='margin-left:.25in'><a name=Phase-ISODISTORT>ISODISTORT</a></h4> … … 5673 5579 <p class=MsoNormal style='margin-left:.5in'>This displays the setup for using 5674 5580 the web-based application, <a href="https://iso.byu.edu/iso/isodistort.php">ISODISTORT</a>, 5675 to identify the possible mode distortions of a parent structure. To use it you must5676 be connected to the internet. Two ISODISTORT Methods are supported in GSAS-II: 5677 Method-1 identifies all possible subgroups that result from simple mode5678 distortions that are associated with a single irreducible representation.5581 to identify the possible mode distortions of a parent structure. To use it you 5582 must be connected to the internet. Two ISODISTORT Methods are supported in 5583 GSAS-II: Method-1 identifies all possible subgroups that result from simple 5584 mode distortions that are associated with a single irreducible representation. 5679 5585 Method-4 is more useful in that it finds the mode decomposition of a parent 5680 5586 structure to give a specified distorted structure and is set up to find only 5681 5587 atom displacement modes. See help pages for <a 5682 5588 href="https://iso.byu.edu/iso/isodistort.php">ISODISTORT</a> for more 5683 information. The ultimate product of using ISODISTORT is a special <span5684 class=SpellE>cif</span> file with constraints describing the mode distortions; 5685 t his is imported into GSAS-II to form a new phase with these constraints.</p>5589 information. The ultimate product of using ISODISTORT is a special cif file 5590 with constraints describing the mode distortions; this is imported into GSAS-II 5591 to form a new phase with these constraints.</p> 5686 5592 5687 5593 <h5 style='margin-left:.5in'>What can I do here?</h5> 5688 5594 5689 5595 <p class=MsoNormal style='margin-left:.5in'>If this is a freshly created phase 5690 (not an imported ISODISTORT <span class=SpellE>cif</span>) then you can choose 5691 the Method (4 is default) and select parent structure and distorted child 5692 structure (for Method 4).</p> 5596 (not an imported ISODISTORT cif) then you can choose the Method (4 is default) 5597 and select parent structure and distorted child structure (for Method 4).</p> 5693 5598 5694 5599 <p class=MsoNormal style='margin-left:.5in'><o:p> </o:p></p> 5695 5600 5696 5601 <p class=MsoNormal style='margin-left:.5in'>If you chose Method 1 & run 5697 ISODISTORT, a table of possible substructures is displayed; a <span5698 class=SpellE>cif</span> file with mode distortion constraints can be produced 5699 from your selection. The table canbe filtered by crystal class.</p>5602 ISODISTORT, a table of possible substructures is displayed; a cif file with 5603 mode distortion constraints can be produced from your selection. The table can 5604 be filtered by crystal class.</p> 5700 5605 5701 5606 <p class=MsoNormal style='margin-left:.5in'><o:p> </o:p></p> 5702 5607 5703 5608 <p class=MsoNormal style='margin-left:.5in'>If this is a phase imported from an 5704 ISODISTORT <span class=SpellE>cif</span> file, the mode displacements are shown5705 with sliders to allow visualization of the displacements in a drawing of the5706 crystal structure (prepare this first before trying a slider). A structure 5707 refinement using this phase will employ the mode distortions as constraints on 5708 the atom coordinates; there should be as many as there are free variable5709 coordinates in thestructure. The values (in <span style='font-family:"Calibri",sans-serif'>Å</span>)5609 ISODISTORT cif file, the mode displacements are shown with sliders to allow 5610 visualization of the displacements in a drawing of the crystal structure 5611 (prepare this first before trying a slider). A structure refinement using this 5612 phase will employ the mode distortions as constraints on the atom coordinates; 5613 there should be as many as there are free variable coordinates in the 5614 structure. The values (in <span style='font-family:"Calibri",sans-serif'>Å</span>) 5710 5615 represent the largest atom shift associated with the mode; shown is a list of 5711 5616 atom coordinates affected by each mode.</p> … … 5718 5623 from the web site with the controls as shown.</p> 5719 5624 5720 <p class=MsoNormal style='margin-left:.5in'>2) <b>Make <span class=SpellE>cif</span> 5721 file</b> – active after table from Method 1 is displayed; generate <span 5722 class=SpellE>cif</span> file by ISODISTORT web site with mode distortion 5723 constraints.</p> 5724 5725 <p class=MsoNormal style='margin-left:.5in'>3) <b>Make <span class=SpellE>PDFfit</span> 5726 phase</b> – active when mode distortions are shown. Makes new phase specific 5727 for fitting PDF data via PDFfit2.</p> 5625 <p class=MsoNormal style='margin-left:.5in'>2) <b>Make cif file</b> – active 5626 after table from Method 1 is displayed; generate cif file by ISODISTORT web site 5627 with mode distortion constraints.</p> 5628 5629 <p class=MsoNormal style='margin-left:.5in'>3) <b>Make PDFfit phase</b> – 5630 active when mode distortions are shown. Makes new phase specific for fitting 5631 PDF data via PDFfit2.</p> 5728 5632 5729 5633 <p class=MsoNormal style='margin-left:.5in'>4) <b>Show modes</b> – active when … … 5736 5640 <h4 style='margin-left:.25in'><a name=Phase-Dysnomia>Dysnomia</a></h4> 5737 5641 5738 <p class=MsoNormal style='margin-left:.5in'>This is displayed if the <b>Use <span5739 class=SpellE>Dysnomia</span></b> box in the General tab is checked. <a5740 href="https://doi.org/10.1017/S088571561300002X"> <span class=SpellE>Dysnomia</span></a>5741 is a maximum entropy method for improving Fourier density maps. The <span 5742 c lass=SpellE>Dysnomia</span> tab gives controls for its operation.</p>5642 <p class=MsoNormal style='margin-left:.5in'>This is displayed if the <b>Use 5643 Dysnomia</b> box in the General tab is checked. <a 5644 href="https://doi.org/10.1017/S088571561300002X">Dysnomia</a> is a maximum 5645 entropy method for improving Fourier density maps. The Dysnomia tab gives 5646 controls for its operation.</p> 5743 5647 5744 5648 <h5 style='margin-left:.5in'>What can I do here?</h5> … … 5746 5650 <p class=MsoNormal style='margin-left:.5in'><b>Operations</b> menu – </p> 5747 5651 5748 <p class=MsoNormal style='margin-left:.5in'>1) <b>Load from <span class=SpellE>Dysnomia</span>5749 file</b> –as previously saved set of controls.</p>5750 5751 <p class=MsoNormal style='margin-left:.5in'>2) <b>Save <span class=SpellE>Dysnomia</span>5752 file</b> – saves data needed to run <span class=SpellE>Dysnomia</span></p>5753 5754 <p class=MsoNormal style='margin-left:.5in'>3) <b>Run <span class=SpellE>Dysnomia</span></b>5755 – execute the routine from GSAS-II (not a separate console). Replaces existing 5756 map withone improved by maximum entropy.</p>5652 <p class=MsoNormal style='margin-left:.5in'>1) <b>Load from Dysnomia file</b> – 5653 as previously saved set of controls.</p> 5654 5655 <p class=MsoNormal style='margin-left:.5in'>2) <b>Save Dysnomia file</b> – saves 5656 data needed to run Dysnomia</p> 5657 5658 <p class=MsoNormal style='margin-left:.5in'>3) <b>Run Dysnomia</b> – execute 5659 the routine from GSAS-II (not a separate console). Replaces existing map with 5660 one improved by maximum entropy.</p> 5757 5661 5758 5662 <p class=MsoNormal><o:p> </o:p></p> … … 5765 5669 </span></div> 5766 5670 5767 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"'><!-- hhmts start -->Last modified: Thu Mar 24 16:28:36 CDT 2022 <!-- hhmts end --><o:p></o:p></span></p> 5671 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"'><!-- hhmts start -->Last 5672 modified: Thu Mar 24 16:28:36 CDT 2022 <!-- hhmts end --><o:p></o:p></span></p> 5768 5673 5769 5674 </div> -
trunk/help/gsasII-phase_files/filelist.xml
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trunk/help/gsasII.html
r5256 r5257 25 25 <o:Author>Von Dreele</o:Author> 26 26 <o:LastAuthor>Von Dreele, Robert B.</o:LastAuthor> 27 <o:Revision>1 79</o:Revision>28 <o:TotalTime>5 558</o:TotalTime>27 <o:Revision>181</o:Revision> 28 <o:TotalTime>5681</o:TotalTime> 29 29 <o:Created>2011-11-28T16:49:00Z</o:Created> 30 <o:LastSaved>2022-03-3 0T20:11:00Z</o:LastSaved>30 <o:LastSaved>2022-03-31T15:52:00Z</o:LastSaved> 31 31 <o:Pages>1</o:Pages> 32 <o:Words>14 193</o:Words>33 <o:Characters>8 0904</o:Characters>32 <o:Words>14672</o:Words> 33 <o:Characters>83636</o:Characters> 34 34 <o:Company>Argonne National Laboratory</o:Company> 35 <o:Lines>6 74</o:Lines>36 <o:Paragraphs>1 89</o:Paragraphs>37 <o:CharactersWithSpaces>9 4908</o:CharactersWithSpaces>35 <o:Lines>696</o:Lines> 36 <o:Paragraphs>196</o:Paragraphs> 37 <o:CharactersWithSpaces>98112</o:CharactersWithSpaces> 38 38 <o:Version>16.00</o:Version> 39 39 </o:DocumentProperties> … … 49 49 <w:WordDocument> 50 50 <w:Zoom>148</w:Zoom> 51 <w:SpellingState>Clean</w:SpellingState>52 <w:GrammarState>Clean</w:GrammarState>53 51 <w:TrackMoves>false</w:TrackMoves> 54 52 <w:TrackFormatting/> … … 975 973 mso-bidi-font-family:"Times New Roman";} 976 974 p 977 {mso-style-priority:99; 975 {mso-style-noshow:yes; 976 mso-style-priority:99; 978 977 mso-margin-top-alt:auto; 979 978 margin-right:0in; … … 1306 1305 font-family:"Times New Roman",serif; 1307 1306 mso-fareast-font-family:"Times New Roman";} 1308 span.SpellE1309 {mso-style-name:"";1310 mso-spl-e:yes;}1311 span.GramE1312 {mso-style-name:"";1313 mso-gram-e:yes;}1314 1307 .MsoChpDefault 1315 1308 {mso-style-type:export-only; … … 2516 2509 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 2517 2510 "Times New Roman"'>The data tree shows contents of a GSAS-II project (which can 2518 be read or saved as a .<span class=SpellE>gpx</span> file) in a hierarchical 2519 view. Clicking on any item in the tree opens that information on the right side 2520 of the window in the "Data Editing" section, where information in 2521 that item can be viewed or edited. For example, the <a 2522 href="gsasII-pwdr.html#PWDR_Sample_Parameters">"Sample Parameters"</a> 2523 item under a ‘PWDR’ entry contains information about how data were collected, 2524 such as the sample temperature <a href="gsasII-pwdr.html#PWDR_Sample_Parameters">(see 2525 below)</a>. The arrow keys (up & down) move the selection to successive 2526 entries in the data tree; both the data window and the associated plot (if any) 2527 will change.<o:p></o:p></span></p> 2511 be read or saved as a .gpx file) in a hierarchical view. Clicking on any item 2512 in the tree opens that information on the right side of the window in the 2513 "Data Editing" section, where information in that item can be viewed 2514 or edited. For example, the <a href="gsasII-pwdr.html#PWDR_Sample_Parameters">"Sample 2515 Parameters"</a> item under a ‘PWDR’ entry contains information about how 2516 data were collected, such as the sample temperature <a 2517 href="gsasII-pwdr.html#PWDR_Sample_Parameters">(see below)</a>. The arrow keys 2518 (up & down) move the selection to successive entries in the data tree; both 2519 the data window and the associated plot (if any) will change.<o:p></o:p></span></p> 2528 2520 2529 2521 <h4 style='margin-left:.5in'><span style='mso-fareast-font-family:"Times New Roman"'>What … … 2586 2578 2587 2579 <p class=MsoNormal style='margin-left:.5in'><span style='mso-no-proof:yes'><img 2588 border=0 width=727 height=55 id="_x0000_i11 15" src=graphbar.jpg2580 border=0 width=727 height=55 id="_x0000_i1128" src=graphbar.jpg 2589 2581 alt="toolbar on plots"></span></p> 2590 2582 … … 2682 2674 2683 2675 <p class=MsoNormal style='margin-left:.5in'><b><span style='mso-fareast-font-family: 2684 "Times New Roman"'>{less <span class=GramE>than}+</span>{greater than}</span></b><span2685 style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p>2676 "Times New Roman"'>{less than}+{greater than}</span></b><span style='mso-fareast-font-family: 2677 "Times New Roman"'><o:p></o:p></span></p> 2686 2678 2687 2679 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: … … 2690 2682 2691 2683 <p class=MsoNormal style='margin-left:.5in'><b><span style='mso-fareast-font-family: 2692 "Times New Roman"'>{greater <span class=GramE>than}+</span>{less than}</span></b><span2693 style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p>2684 "Times New Roman"'>{greater than}+{less than}</span></b><span style='mso-fareast-font-family: 2685 "Times New Roman"'><o:p></o:p></span></p> 2694 2686 2695 2687 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: … … 2698 2690 2699 2691 <p class=MsoNormal style='margin-left:.5in'><b><span style='mso-fareast-font-family: 2700 "Times New Roman"'>{up arrow} <span class=GramE>/{</span>down arrow}</span></b><span2701 style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p>2692 "Times New Roman"'>{up arrow}/{down arrow}</span></b><span style='mso-fareast-font-family: 2693 "Times New Roman"'><o:p></o:p></span></p> 2702 2694 2703 2695 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: … … 2706 2698 2707 2699 <p class=MsoNormal style='margin-left:.5in'><b><span style='mso-fareast-font-family: 2708 "Times New Roman"'>{down arrow} <span class=GramE>/{</span>up arrow}</span></b><span2709 style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></p>2700 "Times New Roman"'>{down arrow}/{up arrow}</span></b><span style='mso-fareast-font-family: 2701 "Times New Roman"'><o:p></o:p></span></p> 2710 2702 2711 2703 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: … … 2714 2706 2715 2707 <p class=MsoNormal style='margin-left:.5in'>Below the toolbar may be a status 2716 bar that on the left may show either an instruction for a keyed input or a <span 2717 class=GramE>pull down</span> selection of keyed input; on the right may be 2718 displayed position dependent information that is updated as the mouse is moved 2719 over the plot region.</p> 2708 bar that on the left may show either an instruction for a keyed input or a pull 2709 down selection of keyed input; on the right may be displayed position dependent 2710 information that is updated as the mouse is moved over the plot region.</p> 2720 2711 2721 2712 <div class=MsoNormal align=center style='text-align:center'><span … … 2748 2739 2749 2740 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 2750 "Times New Roman"'>Open a previously saved GSAS-II project file ({project}.<span2751 class=SpellE>gpx</span>). If you currently have a project file open, you are 2752 asked if itis OK to overwrite it; Cancel will cancel the read process. <o:p></o:p></span></p>2741 "Times New Roman"'>Open a previously saved GSAS-II project file 2742 ({project}.gpx). If you currently have a project file open, you are asked if it 2743 is OK to overwrite it; Cancel will cancel the read process. <o:p></o:p></span></p> 2753 2744 2754 2745 <p style='margin-left:.9in'>Note that as files are saved, copies of the 2755 previous version are saved as backup files, named as {project}.<span 2756 class=SpellE>bak</span>{<span class=SpellE><i>i</i></span>}.<span class=SpellE>gpx</span>, 2757 where <span class=SpellE><i>i</i></span> starts as 0 and is increased after 2758 each save operation. NB: you may open a backup .<span class=SpellE>gpx</span> 2759 file (<span class=GramE>e.g.</span> name.bak3.gpx) to return to a previous 2746 previous version are saved as backup files, named as {project}.bak{<i>i</i>}.gpx, 2747 where <i>i</i> starts as 0 and is increased after each save operation. NB: you 2748 may open a backup .gpx file (e.g. name.bak3.gpx) to return to a previous 2760 2749 version of your project, but if you do so, it is best to immediately use the <b'>Save 2761 As... menu command (you may wish to use <span class=SpellE>name.gpx</span> to2762 overwrite the current version or select a new name.) If you forget <span2763 class=GramE>specify</span> a project name, then name.bak3 will be considered2764 the project name and backups will then be namedname.bak3.bak0.gpx, etc.</p>2750 As... menu command (you may wish to use name.gpx to overwrite the current 2751 version or select a new name.) If you forget specify a project name, then 2752 name.bak3 will be considered the project name and backups will then be named 2753 name.bak3.bak0.gpx, etc.</p> 2765 2754 2766 2755 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 2833 2822 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 2834 2823 "Times New Roman"'>Form the sum of previously read powder patterns; each with a 2835 multiplier. Can be used to accumulate data, subtract <span class=GramE>background</span> 2836 or empty container patterns, etc. Patterns used to form the sum must be of 2837 identical range and step size. Result is a new PWDR entry in the GSAS-II data 2838 tree. <o:p></o:p></span></p> 2824 multiplier. Can be used to accumulate data, subtract background or empty 2825 container patterns, etc. Patterns used to form the sum must be of identical 2826 range and step size. Result is a new PWDR entry in the GSAS-II data tree. <o:p></o:p></span></p> 2839 2827 2840 2828 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 2844 2832 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 2845 2833 "Times New Roman"'>Form the sum of previously read 2-D images; each with a 2846 multiplier. Can be used to accumulate data, subtract <span class=GramE>background</span>2847 or empty container patterns, etc. Images used to form the sum must be of 2848 identical size and source. Result is a new IMG entry in the GSAS-II data tree, 2849 and a GSAS-IIimage file is written for future use. <o:p></o:p></span></p>2834 multiplier. Can be used to accumulate data, subtract background or empty 2835 container patterns, etc. Images used to form the sum must be of identical size 2836 and source. Result is a new IMG entry in the GSAS-II data tree, and a GSAS-II 2837 image file is written for future use. <o:p></o:p></span></p> 2850 2838 2851 2839 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 2860 2848 enter the space group symbol and then the lattice parameters. <br> 2861 2849 Note that nonstandard space group symbols are permitted; space group names must 2862 have spaces between the axial fields (<span class=GramE>e.g.</span> use ‘P n a 2863 21’ not ‘Pna21’). <o:p></o:p></span></p> 2850 have spaces between the axial fields (e.g. use ‘P n a 21’ not ‘Pna21’). <o:p></o:p></span></p> 2864 2851 2865 2852 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 2877 2864 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 2878 2865 "Times New Roman"'>Rename a histogram entry. This should only be done before 2879 the histogram is used in any phases: <span class=GramE>e.g.</span> only rename2880 data immediately afterreading. <o:p></o:p></span></p>2866 the histogram is used in any phases: e.g. only rename data immediately after 2867 reading. <o:p></o:p></span></p> 2881 2868 2882 2869 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 2885 2872 2886 2873 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 2887 "Times New Roman"'>This will remove an item from the data tree. A dialog box with 2888 a list of choices for histograms is presented. Be sure to remove a <span 2889 class=GramE>histograms</span> from all phases before deleting it from the tree. 2890 <o:p></o:p></span></p> 2874 "Times New Roman"'>This will remove an item from the data tree. A dialog box 2875 with a list of choices for histograms is presented. Be sure to remove a 2876 histograms from all phases before deleting it from the tree. <o:p></o:p></span></p> 2891 2877 2892 2878 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 2925 2911 2926 2912 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: 2927 "Times New Roman"'>View LS <span class=SpellE>parms</span></span></b><span2928 style='mso-fareast-font-family:"Times New Roman"'> <o:p></o:p></span></p>2913 "Times New Roman"'>View LS parms</span></b><span style='mso-fareast-font-family: 2914 "Times New Roman"'> <o:p></o:p></span></p> 2929 2915 2930 2916 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: … … 2933 2919 indicate parameters that are not refinable. The total number of refined 2934 2920 parameters is also shown at the top of the list. The value of each parameter is 2935 also given. The parameter names are of the form ‘ <span class=SpellE>p:h:name:id</span>’2936 where ‘p’ is the phase index, ‘h’ is the histogram index and ‘id’ is the item 2937 index (if needed).Indexes all begin with ‘0’ (zero). <o:p></o:p></span></p>2921 also given. The parameter names are of the form ‘p:h:name:id’ where ‘p’ is the 2922 phase index, ‘h’ is the histogram index and ‘id’ is the item index (if needed). 2923 Indexes all begin with ‘0’ (zero). <o:p></o:p></span></p> 2938 2924 2939 2925 <p style='margin-left:.9in'>Note that for atom positions, the coordinate values 2940 (named as ‘<span class=GramE>p::</span><span class=SpellE>A<i>w</i>:n</span>’, 2941 where p is the phase number, n is the atom number and <i>w</i> is x, y or z) is 2942 not a refinable parameter, but the shift in the value is. The refined 2943 parameters are ‘<span class=GramE>p::</span><span class=SpellE>A<i>w</i>:n</span>’. 2944 The reason this is done is that by treating an atom position as <span 2945 class=SpellE>x+<span class=GramE>dx,y</span>+dy,z+dz</span> where the “d” values 2946 indicate shifts from the starting position and the shifts are refined rather 2947 than the <span class=SpellE>x,y</span>, or z values is that this simplifies 2948 symmetry constraints. As an example, suppose we have an atom on a symmetry 2949 constrained site, x,1/2-<span class=GramE>x,z.</span> The process needed to define 2950 this constraint, so that if x moves positively y <span class=GramE>has to</span> 2951 move negatively by the same amount would be messy. With refinement of shifts, 2952 all we need to do is constrain <span class=SpellE>dy</span> (‘<span 2953 class=GramE>0::</span><span class=SpellE>dAy:n</span>’) to be equal to -dx 2954 (-1*‘0::<span class=SpellE>dAx:n</span>’). </p> 2926 (named as ‘p::A<i>w</i>:n’, where p is the phase number, n is the atom number 2927 and <i>w</i> is x, y or z) is not a refinable parameter, but the shift in the 2928 value is. The refined parameters are ‘p::A<i>w</i>:n’. The reason this is done 2929 is that by treating an atom position as x+dx,y+dy,z+dz where the “d” values indicate 2930 shifts from the starting position and the shifts are refined rather than the 2931 x,y, or z values is that this simplifies symmetry constraints. As an example, 2932 suppose we have an atom on a symmetry constrained site, x,1/2-x,z. The process 2933 needed to define this constraint, so that if x moves positively y has to move 2934 negatively by the same amount would be messy. With refinement of shifts, all we 2935 need to do is constrain dy (‘0::dAy:n’) to be equal to -dx (-1*‘0::dAx:n’). </p> 2955 2936 2956 2937 <p style='margin-left:.9in'>Press the window exit button to exit this dialog … … 2976 2957 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"'><span 2977 2958 style='mso-tab-count:1'> </span><span style='mso-spacerun:yes'> 2978 </span><b>Run <span class=SpellE>Fprime</span><o:p></o:p></b></span></p>2959 </span><b>Run Fprime<o:p></o:p></b></span></p> 2979 2960 2980 2961 <p class=MsoNormal style='margin-left:67.5pt'><span style='mso-fareast-font-family: 2981 "Times New Roman"'>This run the utility routine <span class=SpellE>Fprime</span>2982 that displays real and imaginary components of the x-ray form factors for user 2983 selected elements as a function of wavelength/energy. Allows an informed choice 2984 of wavelength forresonant x-ray scattering experiments<o:p></o:p></span></p>2962 "Times New Roman"'>This run the utility routine Fprime that displays real and 2963 imaginary components of the x-ray form factors for user selected elements as a 2964 function of wavelength/energy. Allows an informed choice of wavelength for 2965 resonant x-ray scattering experiments<o:p></o:p></span></p> 2985 2966 2986 2967 <p class=MsoNormal style='margin-left:.75in'><b><span style='mso-fareast-font-family: … … 2993 2974 2994 2975 <p class=MsoNormal style='margin-left:.75in'><b><span style='mso-fareast-font-family: 2995 "Times New Roman"'>Run <span class=SpellE>PlotXNFF</span><o:p></o:p></span></b></p>2976 "Times New Roman"'>Run PlotXNFF<o:p></o:p></span></b></p> 2996 2977 2997 2978 <p class=MsoNormal style='margin-left:1.0in'><span style='mso-fareast-font-family: 2998 "Times New Roman"'>This runs the utility routine <span class=SpellE>PlotXNFF</span>2999 which displays resonant (if any) neutron scattering lengths for all isotopes of 3000 a selected element. It also displays the x-ray and magnetic neutron form 3001 factors for allvalences (if any) for this element.<o:p></o:p></span></p>2979 "Times New Roman"'>This runs the utility routine PlotXNFF which displays 2980 resonant (if any) neutron scattering lengths for all isotopes of a selected 2981 element. It also displays the x-ray and magnetic neutron form factors for all 2982 valences (if any) for this element.<o:p></o:p></span></p> 3002 2983 3003 2984 <ol start=4 type=1> … … 3011 2992 information from external files that can be created and customized easily. See 3012 2993 the <a href="https://gsas-ii.readthedocs.io/en/latest/imports.html">GSAS-II 3013 Import Modules section</a> of the <a href="#Programmers"><s pan class=GramE><strong>Programmers</strong></span><strong>2994 Import Modules section</a> of the <a href="#Programmers"><strong>Programmers 3014 2995 documentation</strong></a> for more information on this. Since it is easy to 3015 2996 support new formats, the documentation below may not list all supported … … 3025 3006 when selected with the mouse shows further submenus with specific imports that 3026 3007 are available. Any of these files can be accessed from a zip file. GSAS-II can 3027 read many different <span class=GramE>image</span> file formats including 3028 MAR345 files, Quantum ADSC files, and tiff files from Perkin-Elmer, Pilatus, 3029 and GE. Although many of these formats have data fields that should contain 3030 relevant information for the exposure (<span class=GramE>e.g.</span> 3031 wavelength), these are rarely filled in correctly by the data acquisition 3032 software. Thus, you should have separately noted this information as it will be 3033 needed. NB: gain maps can be imported but they must be 1000*the gain value 3034 (typically ~1) as integers; GSAS-II will rescale the gain map by 1/1000 and 3035 apply it to the image.<o:p></o:p></span></p> 3008 read many different image file formats including MAR345 files, Quantum ADSC 3009 files, and tiff files from Perkin-Elmer, Pilatus, and GE. Although many of 3010 these formats have data fields that should contain relevant information for the 3011 exposure (e.g. wavelength), these are rarely filled in correctly by the data 3012 acquisition software. Thus, you should have separately noted this information 3013 as it will be needed. NB: gain maps can be imported but they must be 1000*the 3014 gain value (typically ~1) as integers; GSAS-II will rescale the gain map by 3015 1/1000 and apply it to the image.<o:p></o:p></span></p> 3036 3016 3037 3017 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 3041 3021 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 3042 3022 "Times New Roman"'>Creates a new phase by reading unit cell/symmetry/atom 3043 coordinate information. GSAS-II can read information from <span class=GramE>a 3044 number of</span> different format files including: <o:p></o:p></span></p> 3045 3046 <p class=MsoNormal style='margin-left:.9in'><span class=GramE><span 3047 style='mso-fareast-font-family:"Times New Roman"'>GSAS .EXP</span></span><span 3048 style='mso-fareast-font-family:"Times New Roman"'> <o:p></o:p></span></p> 3023 coordinate information. GSAS-II can read information from a number of different 3024 format files including: <o:p></o:p></span></p> 3025 3026 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 3027 "Times New Roman"'>GSAS .EXP <o:p></o:p></span></p> 3049 3028 3050 3029 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3051 "Times New Roman"'>This reads one phase from a (old) GSAS experiment file (<span 3052 class=SpellE>name.EXP</span>). The file name is found in a directory dialog; 3053 you can change directories as needed. <span class=GramE>Only .EXP</span> (or 3054 .exp) file names are shown. If the selected file has more than one phase, a 3055 dialog is shown with the <span class=GramE>choices;</span> only one can be 3056 chosen. If you want more than one, redo this command. After selecting a phase, 3057 a dialog box is shown with the proposed phase name. You can change it if 3058 desired. <o:p></o:p></span></p> 3030 "Times New Roman"'>This reads one phase from a (old) GSAS experiment file 3031 (name.EXP). The file name is found in a directory dialog; you can change 3032 directories as needed. Only .EXP (or .exp) file names are shown. If the 3033 selected file has more than one phase, a dialog is shown with the choices; only 3034 one can be chosen. If you want more than one, redo this command. After 3035 selecting a phase, a dialog box is shown with the proposed phase name. You can 3036 change it if desired. <o:p></o:p></span></p> 3059 3037 3060 3038 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: … … 3063 3041 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3064 3042 "Times New Roman"'>This reads the macromolecular phase information from a 3065 Protein Data Base file (name.PDB or <span class=SpellE>name.ENT</span>). The 3066 file name is found in a directory dialog; you can change directories as needed. 3067 Only .PDB (or .<span class=SpellE>pdb</span>) <span class=GramE>or .ENT</span> 3068 (or .<span class=SpellE>ent</span>) file names are shown. Be careful that the 3069 space group symbol on the ‘CRYST1’ record in the PDB file follows the GSAS-II 3070 conventions (<span class=GramE>e.g.</span> with spaces between axial fields). A 3071 dialog box is shown with the proposed phase name. You can change it if desired. 3072 <o:p></o:p></span></p> 3043 Protein Data Base file (name.PDB or name.ENT). The file name is found in a 3044 directory dialog; you can change directories as needed. Only .PDB (or .pdb) or 3045 .ENT (or .ent) file names are shown. Be careful that the space group symbol on 3046 the ‘CRYST1’ record in the PDB file follows the GSAS-II conventions (e.g. with 3047 spaces between axial fields). A dialog box is shown with the proposed phase 3048 name. You can change it if desired. <o:p></o:p></span></p> 3073 3049 3074 3050 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: … … 3077 3053 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3078 3054 "Times New Roman"'>This reads one phase from a Crystallographic Information 3079 File ({name<span class=GramE>}.CIF</span> (or .<span class=SpellE>cif</span>). 3080 The file name is found in a directory dialog; you can change directories as 3081 needed. If the selected file has more than one phase, a dialog is shown with 3082 the <span class=GramE>choices;</span> only one can be chosen. If you want more 3055 File ({name}.CIF (or .cif). The file name is found in a directory dialog; you 3056 can change directories as needed. If the selected file has more than one phase, 3057 a dialog is shown with the choices; only one can be chosen. If you want more 3083 3058 than one, redo this command. After selecting a phase, a dialog box is shown 3084 3059 with the proposed phase name. You can change it if desired. <o:p></o:p></span></p> 3085 3060 3086 3061 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 3087 "Times New Roman"'>GSAS-II . <span class=SpellE>gpx</span>file <o:p></o:p></span></p>3062 "Times New Roman"'>GSAS-II .gpx file <o:p></o:p></span></p> 3088 3063 3089 3064 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3090 "Times New Roman"'>This reads one phase from a GSAS-II project file ({name}.<span3091 class=SpellE>gpx</span>). The file name is found in a directory dialog; you can 3092 change directories as needed. If the selected file has more than one phase, a 3093 dialog is shown with the choices; If you want more than one, redo this command. 3094 After selecting a phase, a dialog box is shown with the proposed phase name. 3095 You canchange it if desired. <o:p></o:p></span></p>3065 "Times New Roman"'>This reads one phase from a GSAS-II project file 3066 ({name}.gpx). The file name is found in a directory dialog; you can change 3067 directories as needed. If the selected file has more than one phase, a dialog 3068 is shown with the choices; If you want more than one, redo this command. After 3069 selecting a phase, a dialog box is shown with the proposed phase name. You can 3070 change it if desired. <o:p></o:p></span></p> 3096 3071 3097 3072 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: … … 3113 3088 needed for processing a powder diffraction data set, such as data type, 3114 3089 calibration constants (such as wavelength) and default profile parameters are 3115 read from a separate file, either a (old) GSAS instrument parameter file (<span 3116 class=GramE>usually .<span class=SpellE>prm</span></span>, .ins or .<span 3117 class=SpellE>inst</span> extension) or a new GSAS-II .<span class=SpellE>instparm</span> 3118 file. <o:p></o:p></span></p> 3090 read from a separate file, either a (old) GSAS instrument parameter file 3091 (usually .prm, .ins or .inst extension) or a new GSAS-II .instparm file. <o:p></o:p></span></p> 3119 3092 3120 3093 <p style='margin-left:.9in'>Note that it is possible to apply corrections to 3121 3094 the 2-theta, intensity or weight values by adding a Python command(s) to the 3122 instrument <span class=GramE>(.<span class=SpellE>instprm</span></span>) 3123 parameter with a variable named <span class=SpellE>CorrectionCode</span>. See 3124 the <span class=SpellE><tt><span style='font-size:10.0pt'>CorrectionCode.instprm.sample</span></tt></span> 3125 file provided in the GSAS-II source directory for an example of how this is 3126 done. </p> 3095 instrument (.instprm) parameter with a variable named CorrectionCode. See the <tt><span 3096 style='font-size:10.0pt'>CorrectionCode.instprm.sample</span></tt> file 3097 provided in the GSAS-II source directory for an example of how this is done. </p> 3127 3098 3128 3099 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: … … 3131 3102 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3132 3103 "Times New Roman"'>This reads one powder pattern (histogram) from a 3133 Crystallographic Information File ({name<span class=GramE>}.CIF</span>). The file 3134 name is found in a directory dialog; you can change directories as needed. Only 3135 <span class=GramE>one .<span class=SpellE>cif</span></span> can be chosen. If 3136 you want more than one, redo this command. <o:p></o:p></span></p> 3104 Crystallographic Information File ({name}.CIF). The file name is found in a 3105 directory dialog; you can change directories as needed. Only one .cif can be 3106 chosen. If you want more than one, redo this command. <o:p></o:p></span></p> 3137 3107 3138 3108 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 3139 "Times New Roman"'>GSAS-II . <span class=SpellE>gpx</span>file <o:p></o:p></span></p>3109 "Times New Roman"'>GSAS-II .gpx file <o:p></o:p></span></p> 3140 3110 3141 3111 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3142 3112 "Times New Roman"'>This reads powder patterns from a previously created GSAS-II 3143 <span class=SpellE>gpx</span> project file. If the selected file has more than 3144 one powder pattern, a dialog is shown with the choices; one or more can be 3145 selected. It will ask for an appropriate instrument parameter file to go with 3146 the selected powder datasets. <o:p></o:p></span></p>3113 gpx project file. If the selected file has more than one powder pattern, a 3114 dialog is shown with the choices; one or more can be selected. It will ask for 3115 an appropriate instrument parameter file to go with the selected powder data 3116 sets. <o:p></o:p></span></p> 3147 3117 3148 3118 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 3149 "Times New Roman"'>GSAS . <span class=SpellE>fxye</span>files <o:p></o:p></span></p>3119 "Times New Roman"'>GSAS .fxye files <o:p></o:p></span></p> 3150 3120 3151 3121 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3152 3122 "Times New Roman"'>This reads powder patterns (histograms) from the defined 3153 GSAS format powder data files. GSAS file <span class=GramE>types</span> STD,3154 ESD, FXY and FXYE are recognized. Neutron TOF data with a ‘TIME-MAP’ are also 3155 recognized. The file names are found in a directory dialog; you can change 3156 directories as needed. If the selected files have more than one powder pattern, 3157 a dialog is shown withthe choice(s). <o:p></o:p></span></p>3123 GSAS format powder data files. GSAS file types STD, ESD, FXY and FXYE are 3124 recognized. Neutron TOF data with a ‘TIME-MAP’ are also recognized. The file 3125 names are found in a directory dialog; you can change directories as needed. If 3126 the selected files have more than one powder pattern, a dialog is shown with 3127 the choice(s). <o:p></o:p></span></p> 3158 3128 3159 3129 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 3160 "Times New Roman"'>TOPAS . <span class=SpellE>xye</span>files. <o:p></o:p></span></p>3130 "Times New Roman"'>TOPAS .xye files. <o:p></o:p></span></p> 3161 3131 3162 3132 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: … … 3171 3141 "Times New Roman"'>This attempts to read one data set from a file trying the 3172 3142 formats as described above. On occasion, this command may not succeed in 3173 correctly determining a file format. If it fails, retry by selecting the correct3174 format from the list. <o:p></o:p></span></p>3143 correctly determining a file format. If it fails, retry by selecting the 3144 correct format from the list. <o:p></o:p></span></p> 3175 3145 3176 3146 <p class=MsoNormal style='margin-left:.9in'><i><span style='mso-fareast-font-family: 3177 3147 "Times New Roman"'>other supported formats</span></i><span style='mso-fareast-font-family: 3178 "Times New Roman"'>: <span class=GramE>Bruker .RAW</span>; <span class=SpellE>FullProf</span> 3179 .<span class=SpellE>dat</span>; <span class=SpellE>Panalytical</span> .<span 3180 class=SpellE>xrdml</span>; Comma-separated .csv; Rigaku .<span class=SpellE>ras</span> 3181 & .txt <o:p></o:p></span></p> 3148 "Times New Roman"'>: Bruker .RAW; FullProf .dat; Panalytical .xrdml; 3149 Comma-separated .csv; Rigaku .ras & .txt <o:p></o:p></span></p> 3182 3150 3183 3151 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: … … 3189 3157 3190 3158 <p class=MsoNormal style='margin-left:.7in'><span style='mso-fareast-font-family: 3191 "Times New Roman"'>Note that there are also three separate "special" import3192 i tems, as documented below: <o:p></o:p></span></p>3159 "Times New Roman"'>Note that there are also three separate "special" 3160 import items, as documented below: <o:p></o:p></span></p> 3193 3161 3194 3162 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: … … 3199 3167 it using a set of instrument parameters that are read in from a file or one of 3200 3168 the default sets provided when Cancel is pressed at the prompt to select a 3201 file. The user <span class=GramE>is able to</span> specify the data range and3202 step size. One or more crystalline phases must also be provided to perform a 3203 crystallographic simulation. When the "Refine" menu command is 3204 in itially used, the intensities are computed from these phases and the3205 "observed" intensity values are set from these computed values, with 3206 superimposed "random" noise added (increase the scale factor to 3207 minimize this, if desired). Further refinements can then be used to fit to 3208 these simulated data. To reset the "observed" intensity values back 3209 t o zero, to recompute them, use the "Edit range" button on the3210 "PWDR" tree itemthat is created by this option. </span></p>3169 file. The user is able to specify the data range and step size. One or more 3170 crystalline phases must also be provided to perform a crystallographic 3171 simulation. When the "Refine" menu command is initially used, the 3172 intensities are computed from these phases and the "observed" 3173 intensity values are set from these computed values, with superimposed 3174 "random" noise added (increase the scale factor to minimize this, if 3175 desired). Further refinements can then be used to fit to these simulated data. 3176 To reset the "observed" intensity values back to zero, to recompute 3177 them, use the "Edit range" button on the "PWDR" tree item 3178 that is created by this option. </span></p> 3211 3179 3212 3180 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: … … 3217 3185 files as they are added to a directory. The file extension must determine the 3218 3186 importer that will be used and a filter pattern is specified to determine which 3219 files will be read (e.g. use "</span><tt><span style='font-size:10.0pt'>*June23<span 3220 class=GramE>*.<span class=SpellE>fxye</span></span></span></tt><span 3187 files will be read (e.g. use "</span><tt><span style='font-size:10.0pt'>*June23*.fxye</span></tt><span 3221 3188 style='mso-fareast-font-family:"Times New Roman"'>" so that only files 3222 3189 that contain the string "June23" will be read. </span></p> 3223 3190 3224 3191 <p class=MsoNormal style='margin-left:.9in'><a name=FPA><span style='mso-fareast-font-family: 3225 "Times New Roman"'>Fit Instr. profile from fundamental </span></a><span 3226 class=SpellE><span style='mso-bookmark:FPA'><span style='mso-fareast-font-family: 3227 "Times New Roman"'>parms</span></span></span><span style='mso-bookmark:FPA'><span 3228 style='mso-fareast-font-family:"Times New Roman"'>... </span></span></p> 3192 "Times New Roman"'>Fit Instr. profile from fundamental parms... </span></a></p> 3229 3193 3230 3194 <span style='mso-bookmark:FPA'></span> … … 3234 3198 set of fundamental parameters that describe a constant wavelength (most likely 3235 3199 Bragg-Brentano) powder diffraction instrument. The user must first specify the 3236 data range to be used and then a set of <span class=GramE>FP</span> 3237 (fundamental parameter) values. The FP values and a source spectrum can be 3238 supplied using a nomenclature <span class=GramE>similar to</span> <span 3239 class=SpellE>Topas</span> (described further below). They will then be 3240 converted to the SI units and parameter names used in the NIST FPA code. 3241 Alternately a file can be supplied with the parameter values used directly in 3242 that program. With this input, a series of peaks are computed across the 3243 specified data range and the <a 3200 data range to be used and then a set of FP (fundamental parameter) values. The 3201 FP values and a source spectrum can be supplied using a nomenclature similar to 3202 Topas (described further below). They will then be converted to the SI units 3203 and parameter names used in the NIST FPA code. Alternately a file can be 3204 supplied with the parameter values used directly in that program. With this 3205 input, a series of peaks are computed across the specified data range and the <a 3244 3206 href="gsasII-pwdr.html#PWDR_Instrument_Parameters">Instrumental Parameters</a> 3245 3207 that determine the instrumental profile (U, V, W, X, Y and SH/L) are determined … … 3248 3210 3249 3211 <p class=MsoNormal align=center style='text-align:center'><a name=FPAinput><b><span 3250 style='mso-fareast-font-family:"Times New Roman"'>Description of the </span></b></a><span 3251 class=SpellE><span style='mso-bookmark:FPAinput'><b><span style='mso-fareast-font-family: 3252 "Times New Roman"'>Topas</span></b></span></span><span style='mso-bookmark: 3253 FPAinput'><b><span style='mso-fareast-font-family:"Times New Roman"'>-style 3254 fundamental parameters used as FPA input for GSAS-II</span></b></span><span 3212 style='mso-fareast-font-family:"Times New Roman"'>Description of the 3213 Topas-style fundamental parameters used as FPA input for GSAS-II</span></b></a><span 3255 3214 style='mso-bookmark:FPAinput'></span><span style='mso-fareast-font-family:"Times New Roman"'> 3256 3215 <o:p></o:p></span></p> … … 3316 3275 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3317 3276 padding:0in 5.4pt 0in 5.4pt'> 3318 <p class=MsoNormal><span class=SpellE><span style='mso-bidi-font-family:Calibri; 3319 mso-bidi-theme-font:minor-latin'>soller_angle</span></span><span 3320 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3277 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3278 minor-latin'>soller_angle<o:p></o:p></span></p> 3321 3279 </td> 3322 3280 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3332 3290 mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'> 3333 3291 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3334 minor-latin'>Angular limit for divergence in equatorial plane as limited by <span3335 class=SpellE>Soller</span>collimator(s)<o:p></o:p></span></p>3292 minor-latin'>Angular limit for divergence in equatorial plane as limited by 3293 Soller collimator(s)<o:p></o:p></span></p> 3336 3294 </td> 3337 3295 </tr> … … 3363 3321 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3364 3322 padding:0in 5.4pt 0in 5.4pt'> 3365 <p class=MsoNormal><span class=SpellE><span style='mso-bidi-font-family:Calibri; 3366 mso-bidi-theme-font:minor-latin'>filament_length</span></span><span 3367 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3323 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3324 minor-latin'>filament_length<o:p></o:p></span></p> 3368 3325 </td> 3369 3326 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3387 3344 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3388 3345 padding:0in 5.4pt 0in 5.4pt'> 3389 <p class=MsoNormal><span class=SpellE><span style='mso-bidi-font-family:Calibri; 3390 mso-bidi-theme-font:minor-latin'>sample_length</span></span><span 3391 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3346 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3347 minor-latin'>sample_length<o:p></o:p></span></p> 3392 3348 </td> 3393 3349 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3403 3359 mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'> 3404 3360 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3405 minor-latin'>Illuminated sample length in axial direction. <span class=GramE>Typically</span>3406 the same as <span class=SpellE>filament_length</span>.<o:p></o:p></span></p>3361 minor-latin'>Illuminated sample length in axial direction. Typically the same 3362 as filament_length.<o:p></o:p></span></p> 3407 3363 </td> 3408 3364 </tr> … … 3411 3367 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3412 3368 padding:0in 5.4pt 0in 5.4pt'> 3413 <p class=MsoNormal><span class=SpellE><span style='mso-bidi-font-family:Calibri; 3414 mso-bidi-theme-font:minor-latin'>receiving_slit_length</span></span><span 3415 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3369 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3370 minor-latin'>receiving_slit_length<o:p></o:p></span></p> 3416 3371 </td> 3417 3372 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3427 3382 mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'> 3428 3383 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3429 minor-latin'>Length of the receiving slit in axial direction. <span3430 class=GramE>Typically</span> the same as <span class=SpellE>filament_length</span>.<o:p></o:p></span></p>3384 minor-latin'>Length of the receiving slit in axial direction. Typically the 3385 same as filament_length.<o:p></o:p></span></p> 3431 3386 </td> 3432 3387 </tr> … … 3435 3390 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3436 3391 padding:0in 5.4pt 0in 5.4pt'> 3437 <p class=MsoNormal><span class=SpellE><span style='mso-bidi-font-family:Calibri; 3438 mso-bidi-theme-font:minor-latin'>LAC_cm</span></span><span style='mso-bidi-font-family: 3439 Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3392 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3393 minor-latin'>LAC_cm<o:p></o:p></span></p> 3440 3394 </td> 3441 3395 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3443 3397 mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid windowtext .5pt; 3444 3398 mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'> 3445 <p class=MsoNormal><span class=GramE><span style='mso-bidi-font-family:Calibri; 3446 mso-bidi-theme-font:minor-latin'>cm<sup>-1</sup></span></span><span 3447 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3399 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3400 minor-latin'>cm<sup>-1</sup><o:p></o:p></span></p> 3448 3401 </td> 3449 3402 <td width=354 valign=top style='width:265.6pt;border-top:none;border-left: … … 3460 3413 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3461 3414 padding:0in 5.4pt 0in 5.4pt'> 3462 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3463 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3464 color:black'>sample_thickness</span></span><span style='mso-bidi-font-family: 3465 Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3415 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3416 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>sample_thickness</span><span 3417 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3466 3418 </td> 3467 3419 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3485 3437 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3486 3438 padding:0in 5.4pt 0in 5.4pt'> 3487 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3488 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3489 color:black'>convolution_steps</span></span><span style='mso-bidi-font-family: 3490 Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3439 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3440 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>convolution_steps</span><span 3441 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3491 3442 </td> 3492 3443 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3511 3462 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3512 3463 padding:0in 5.4pt 0in 5.4pt'> 3513 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3514 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3515 color:black'>source_width</span></span><span style='mso-bidi-font-family: 3516 Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3464 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3465 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>source_width</span><span 3466 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3517 3467 </td> 3518 3468 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3536 3486 padding:0in 5.4pt 0in 5.4pt'> 3537 3487 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3538 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>tube-<span 3539 class=SpellE>tails_L</span>-tail</span><span style='mso-bidi-font-family: 3540 Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3488 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>tube-tails_L-tail</span><span 3489 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3541 3490 </td> 3542 3491 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3552 3501 mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'> 3553 3502 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3554 minor-latin'>Width for x-ray intensity occurring beyond the <span3555 class=SpellE>Wehnelt</span> shadow as a projection in the axial direction and3556 measured in the positive two-thetadirection.<o:p></o:p></span></p>3503 minor-latin'>Width for x-ray intensity occurring beyond the Wehnelt shadow as 3504 a projection in the axial direction and measured in the positive two-theta 3505 direction.<o:p></o:p></span></p> 3557 3506 </td> 3558 3507 </tr> … … 3562 3511 padding:0in 5.4pt 0in 5.4pt'> 3563 3512 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3564 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>tube-<span 3565 class=SpellE>tails_R</span>-tail</span><span style='mso-bidi-font-family: 3566 Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3513 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>tube-tails_R-tail</span><span 3514 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3567 3515 </td> 3568 3516 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3578 3526 mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'> 3579 3527 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3580 minor-latin'>Width for x-ray intensity occurring beyond the <span3581 class=SpellE>Wehnelt</span> shadow as a projection in the axial direction and3582 measured in the negative two-thetadirection. <o:p></o:p></span></p>3528 minor-latin'>Width for x-ray intensity occurring beyond the Wehnelt shadow as 3529 a projection in the axial direction and measured in the negative two-theta 3530 direction. <o:p></o:p></span></p> 3583 3531 </td> 3584 3532 </tr> … … 3588 3536 padding:0in 5.4pt 0in 5.4pt'> 3589 3537 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3590 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>tube-<span 3591 class=SpellE>tails_rel</span>-I</span><span style='mso-bidi-font-family:Calibri; 3592 mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3538 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>tube-tails_rel-I</span><span 3539 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3593 3540 </td> 3594 3541 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3621 3568 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3622 3569 padding:0in 5.4pt 0in 5.4pt'> 3623 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3624 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3625 color:black'>receiving_slit_width</span></span><span style='mso-fareast-font-family: 3626 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3627 color:black'><o:p></o:p></span></p> 3570 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3571 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>receiving_slit_width<o:p></o:p></span></p> 3628 3572 </td> 3629 3573 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3676 3620 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>) 3677 3621 range in equatorial plane that the entire Si PSD subtends (<i>not implemented 3678 in <span class=SpellE>Topas</span></i>)</span><span style='mso-bidi-font-family:3679 Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p>3622 in Topas</i>)</span><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3623 minor-latin'><o:p></o:p></span></p> 3680 3624 </td> 3681 3625 </tr> … … 3693 3637 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3694 3638 padding:0in 5.4pt 0in 5.4pt'> 3695 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3696 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3697 color:black'>src_mono_mm</span></span><span style='mso-fareast-font-family: 3698 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3699 color:black'><o:p></o:p></span></p> 3639 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3640 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>src_mono_mm<o:p></o:p></span></p> 3700 3641 </td> 3701 3642 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3719 3660 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3720 3661 padding:0in 5.4pt 0in 5.4pt'> 3721 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3722 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3723 color:black'>focus_mono_mm</span></span><span style='mso-fareast-font-family: 3724 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3725 color:black'><o:p></o:p></span></p> 3662 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3663 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>focus_mono_mm<o:p></o:p></span></p> 3726 3664 </td> 3727 3665 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3749 3687 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3750 3688 padding:0in 5.4pt 0in 5.4pt'> 3751 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3752 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3753 color:black'>passband_mistune</span></span><span style='mso-fareast-font-family: 3754 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3755 color:black'><o:p></o:p></span></p> 3689 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3690 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>passband_mistune<o:p></o:p></span></p> 3756 3691 </td> 3757 3692 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3777 3712 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3778 3713 padding:0in 5.4pt 0in 5.4pt'> 3779 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3780 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3781 color:black'>mono_src_proj_mn</span></span><span style='mso-fareast-font-family: 3782 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3783 color:black'><o:p></o:p></span></p> 3714 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3715 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>mono_src_proj_mn<o:p></o:p></span></p> 3784 3716 </td> 3785 3717 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3787 3719 mso-border-top-alt:solid windowtext .5pt;mso-border-left-alt:solid windowtext .5pt; 3788 3720 mso-border-alt:solid windowtext .5pt;padding:0in 5.4pt 0in 5.4pt'> 3789 <p class=MsoNormal><span class=SpellE><span style='mso-bidi-font-family:Calibri; 3790 mso-bidi-theme-font:minor-latin'>μm</span></span><span style='mso-bidi-font-family: 3791 Calibri;mso-bidi-theme-font:minor-latin'> (micron)<o:p></o:p></span></p> 3721 <p class=MsoNormal><span style='mso-bidi-font-family:Calibri;mso-bidi-theme-font: 3722 minor-latin'>μm (micron)<o:p></o:p></span></p> 3792 3723 </td> 3793 3724 <td width=354 valign=top style='width:265.6pt;border-top:none;border-left: … … 3797 3728 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3798 3729 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>Bandwidth 3799 setting for the monochromator as set by the projection width of the <span 3800 class=SpellE>xray</span> source on the monochromator along beam direction and 3801 in the equatorial plane</span><span style='mso-bidi-font-family:Calibri; 3802 mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3730 setting for the monochromator as set by the projection width of the xray 3731 source on the monochromator along beam direction and in the equatorial plane</span><span 3732 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3803 3733 </td> 3804 3734 </tr> … … 3807 3737 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3808 3738 padding:0in 5.4pt 0in 5.4pt'> 3809 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3810 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3811 color:black'>passband_shoulder</span></span><span style='mso-bidi-font-family: 3812 Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3739 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3740 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>passband_shoulder</span><span 3741 style='mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin'><o:p></o:p></span></p> 3813 3742 </td> 3814 3743 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3835 3764 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3836 3765 padding:0in 5.4pt 0in 5.4pt'> 3837 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3838 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3839 color:black'>two_theta_mono</span></span><span style='mso-fareast-font-family: 3840 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3841 color:black'><o:p></o:p></span></p> 3766 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3767 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>two_theta_mono<o:p></o:p></span></p> 3842 3768 </td> 3843 3769 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3862 3788 border-top:none;mso-border-top-alt:solid windowtext .5pt;mso-border-alt:solid windowtext .5pt; 3863 3789 padding:0in 5.4pt 0in 5.4pt'> 3864 <p class=MsoNormal><span class=SpellE><span style='mso-fareast-font-family: 3865 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3866 color:black'>mono_slit_attenuation</span></span><span style='mso-fareast-font-family: 3867 "Times New Roman";mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin; 3868 color:black'><o:p></o:p></span></p> 3790 <p class=MsoNormal><span style='mso-fareast-font-family:"Times New Roman"; 3791 mso-bidi-font-family:Calibri;mso-bidi-theme-font:minor-latin;color:black'>mono_slit_attenuation<o:p></o:p></span></p> 3869 3792 </td> 3870 3793 <td width=71 valign=top style='width:53.05pt;border-top:none;border-left: … … 3894 3817 style='mso-fareast-font-family:"Times New Roman"'>J. Res. of NIST</span></i><span 3895 3818 style='mso-fareast-font-family:"Times New Roman"'>, <b>120</b>, p223. DOI: 3896 10.6028/jres.120.014. If the incident beam <span class=SpellE>monochomator</span> 3897 model is used, please also cite: M.H. Mendenhall, D. Black & J.P. Cline 3898 (2019), <i>J. Appl. <span class=SpellE>Cryst</span>.</i>, <b>52</b>, p1087. 3899 DOI: 10.1107/S1600576719010951. </span></p> 3819 10.6028/jres.120.014. If the incident beam monochomator model is used, please 3820 also cite: M.H. Mendenhall, D. Black & J.P. Cline (2019), <i>J. Appl. 3821 Cryst.</i>, <b>52</b>, p1087. DOI: 10.1107/S1600576719010951. </span></p> 3900 3822 3901 3823 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 3912 3834 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3913 3835 "Times New Roman"'>This reads squared structure factors (as F**2) and sig(F**2) 3914 from a SHELX format .<span class=SpellE>hkl</span> file. The file names are 3915 found in a directory dialog; you can change directories as needed. You must 3916 know the file contains structure factors (as F**2) as the file itself has no 3917 internal indication of this. <o:p></o:p></span></p> 3836 from a SHELX format .hkl file. The file names are found in a directory dialog; 3837 you can change directories as needed. You must know the file contains structure 3838 factors (as F**2) as the file itself has no internal indication of this. <o:p></o:p></span></p> 3918 3839 3919 3840 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: … … 3922 3843 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3923 3844 "Times New Roman"'>This reads structure factors (as F) and sig(F) from a SHELX 3924 format .<span class=SpellE>hkl</span> file. The file names are found in a 3925 directory dialog; you can change directories as needed. You must know the file 3926 contains structure factors (as F values) as the file itself has no internal 3927 indication of this. <o:p></o:p></span></p> 3845 format .hkl file. The file names are found in a directory dialog; you can 3846 change directories as needed. You must know the file contains structure factors 3847 (as F values) as the file itself has no internal indication of this. <o:p></o:p></span></p> 3928 3848 3929 3849 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: … … 3931 3851 3932 3852 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3933 "Times New Roman"'>This reads structure factors (as F**2 or F) and <span 3934 class=GramE>sig(</span>F**2 or F) from a .CIF (or .<span class=SpellE>cif</span>) 3935 or .FCF (or .<span class=SpellE>fcf</span>) format file. The file names are 3853 "Times New Roman"'>This reads structure factors (as F**2 or F) and sig(F**2 or 3854 F) from a .CIF (or .cif) or .FCF (or .fcf) format file. The file names are 3936 3855 found in a directory dialog; you can change directories as needed. The internal 3937 3856 structure of this file indicates in which form the structure factors are used. <o:p></o:p></span></p> … … 3942 3861 <p class=MsoNormal style='margin-left:1.2in'><span style='mso-fareast-font-family: 3943 3862 "Times New Roman"'>This attempts to read one data set from a file trying the 3944 formats as described above. However, since it cannot be determined if SHELX <span 3945 class=GramE>format .<span class=SpellE>hkl</span></span> contains F or F**2 3946 values, do not use this command for those files. On occasion, this command may 3947 not succeed in correctly determining a file format. If it fails, retry by 3948 selecting the correct format from the list. <o:p></o:p></span></p> 3863 formats as described above. However, since it cannot be determined if SHELX 3864 format .hkl contains F or F**2 values, do not use this command for those files. 3865 On occasion, this command may not succeed in correctly determining a file 3866 format. If it fails, retry by selecting the correct format from the list. <o:p></o:p></span></p> 3949 3867 3950 3868 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 3989 3907 or d-spacing from .txt files. Results are placed in the GSAS-II data tree as 3990 3908 ‘PKS file name’. The data format consists of optional comments (each line 3991 starts with ‘#’) followed by positions in a single column. If 1<sup>st</sup> position3992 is larger than last, they are interpreted as d-spacings, otherwise as 2</span><span 3993 style='font-family:Symbol;mso-ascii-font-family:"Times New Roman";mso-fareast-font-family: 3994 "Times New Roman";mso-hansi-font-family:"Times New Roman";mso-char-type:symbol;3995 mso- symbol-font-family:Symbol'><span style='mso-char-type:symbol;mso-symbol-font-family:3996 Symbol'>Q</span></span><span style='mso-fareast-font-family:"Times New Roman"'>. 3997 A second column of intensities is optional.<o:p></o:p></span></p>3909 starts with ‘#’) followed by positions in a single column. If 1<sup>st</sup> 3910 position is larger than last, they are interpreted as d-spacings, otherwise as 3911 2</span><span style='font-family:Symbol;mso-ascii-font-family:"Times New Roman"; 3912 mso-fareast-font-family:"Times New Roman";mso-hansi-font-family:"Times New Roman"; 3913 mso-char-type:symbol;mso-symbol-font-family:Symbol'><span style='mso-char-type: 3914 symbol;mso-symbol-font-family:Symbol'>Q</span></span><span style='mso-fareast-font-family: 3915 "Times New Roman"'>. A second column of intensities is optional.<o:p></o:p></span></p> 3998 3916 3999 3917 <ol start=5 type=1> … … 4007 3925 with information inside GSAS-II. These routines can be created and customized 4008 3926 easily. See the <a href="https://gsas-ii.readthedocs.io/en/latest/exports.html">GSAS-II 4009 Export Modules section</a> of the <a href="#Programmers"><s pan class=GramE><strong>Programmers</strong></span><strong>3927 Export Modules section</a> of the <a href="#Programmers"><strong>Programmers 4010 3928 documentation</strong></a> for more information on this. Since it is easy to 4011 3929 support new formats, the documentation below may not list all supported … … 4027 3945 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 4028 3946 "Times New Roman"'>Phases can be exported in a variety of formats including a 4029 simplified CIF file that contains only the unit cell, <span class=GramE>symmetry</span>4030 and coordinates.<o:p></o:p></span></p>3947 simplified CIF file that contains only the unit cell, symmetry and coordinates. 3948 <o:p></o:p></span></p> 4031 3949 4032 3950 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 4044 3962 4045 3963 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 4046 "Times New Roman"'>Single crystal reflection lists can be exported as text 4047 filesor as a simplified CIF file that contains only structure factors. <o:p></o:p></span></p>3964 "Times New Roman"'>Single crystal reflection lists can be exported as text files 3965 or as a simplified CIF file that contains only structure factors. <o:p></o:p></span></p> 4048 3966 4049 3967 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 4051 3969 "Times New Roman"'> <o:p></o:p></span></p> 4052 3970 4053 <p class=MsoNormal style='margin-left:.9in'><span class=GramE><span 4054 style='mso-fareast-font-family:"Times New Roman"'>This exports</span></span><span 4055 style='mso-fareast-font-family:"Times New Roman"'> selected images as a 4056 portable networks graphics format (PNG) file. Alternately, the image controls 4057 and masks can be written for selected images. If strain analysis has been 4058 performed on images, the results can also be exported here as a spreadsheet 4059 (.csv file). <o:p></o:p></span></p> 3971 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 3972 "Times New Roman"'>This exports selected images as a portable networks graphics 3973 format (PNG) file. Alternately, the image controls and masks can be written for 3974 selected images. If strain analysis has been performed on images, the results 3975 can also be exported here as a spreadsheet (.csv file). <o:p></o:p></span></p> 4060 3976 4061 3977 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 4073 3989 "Times New Roman"'>This allows peak lists from selected powder histograms to be 4074 3990 written to a simple text file. There will be a heading for each PWDR GSAS-II 4075 tree item and columns of values for position, intensity, <span class=GramE>sigma</span>4076 and gammafollow. <o:p></o:p></span></p>3991 tree item and columns of values for position, intensity, sigma and gamma 3992 follow. <o:p></o:p></span></p> 4077 3993 4078 3994 <p class=MsoNormal style='margin-left:.7in'><b><span style='mso-fareast-font-family: … … 4090 4006 <p class=MsoNormal style='margin-left:.9in'><span style='mso-fareast-font-family: 4091 4007 "Times New Roman"'>This allows computed PDFs peak lists from selected 4092 histograms to be written as two simple text files, {name}.gr and {name <span4093 c lass=GramE>}.sq</span>, containing g(r) and s(q), respectively as 2 columns of4094 data; a header on each indicated the source file name and the column headings. 4095 The file name comesfrom the PDF entry in the GSAS-II data tree. <o:p></o:p></span></p>4008 histograms to be written as two simple text files, {name}.gr and {name}.sq, 4009 containing g(r) and s(q), respectively as 2 columns of data; a header on each 4010 indicated the source file name and the column headings. The file name comes 4011 from the PDF entry in the GSAS-II data tree. <o:p></o:p></span></p> 4096 4012 4097 4013 <div class=MsoNormal align=center style='text-align:center'><span … … 4117 4033 "Times New Roman"'>This window provides a place for you to enter whatever text 4118 4034 commentary you wish. Each time you enter this window, a date/time entry is 4119 provided for you. A possibly useful technique is to select a portion of the <span 4120 class=SpellE>project.lst</span> file after a refinement completes (it will 4121 contain refinement results with residuals, new values & <span class=SpellE>esds</span>) 4122 and paste it into this Notebook window so it becomes a part of your project 4123 file.</span> </p> 4035 provided for you. A possibly useful technique is to select a portion of the 4036 project.lst file after a refinement completes (it will contain refinement 4037 results with residuals, new values & esds) and paste it into this Notebook 4038 window so it becomes a part of your project file.</span> </p> 4124 4039 4125 4040 <h5 style='margin-left:.5in'><span style='mso-fareast-font-family:"Times New Roman"'>What … … 4160 4075 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4161 4076 </span></span></span><![endif]><u><span style='mso-fareast-font-family:"Times New Roman"'>analytic 4162 Hessian</span></u><span style='mso-fareast-font-family:"Times New Roman"'>: 4163 Thisis the default option and is usually the most useful. It uses a4077 Hessian</span></u><span style='mso-fareast-font-family:"Times New Roman"'>: This 4078 is the default option and is usually the most useful. It uses a 4164 4079 custom-developed least-squares minimizer that uses singular-value decomposition 4165 4080 (SVD) to reduce the errors caused by correlated variables and the … … 4173 4088 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4174 4089 </span></span></span><![endif]><span style='mso-fareast-font-family:"Times New Roman"'>analytic 4175 Jacobian: This uses a <span class=SpellE>numpy</span>-provided <span 4176 class=SpellE><i>leastsq</i></span> minimizer, which not applicable for problem 4177 with <span class=GramE>a large number of</span> histograms as it requires much 4090 Jacobian: This uses a numpy-provided <i>leastsq</i> minimizer, which not 4091 applicable for problem with a large number of histograms as it requires much 4178 4092 more memory than the Hessian routines. This because it creates a Jacobian 4179 4093 matrix that is shaped N x M (N parameters x M observations) while the Hessian … … 4186 4100 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4187 4101 </span></span></span><![endif]><span style='mso-fareast-font-family:"Times New Roman"'>numeric: 4188 This also uses the <span class=SpellE>numpy</span> <span class=SpellE><i>leastsq</i></span> 4189 <span class=GramE>minimizer, and</span> is also not applicable for larger 4190 problems. Unlike, the "analytic Jacobian", numerical derivatives are 4191 computed rather than use the analytical derivatives that are coded directly 4192 into GSAS-II. This will be slower than the analytical derivatives and will is 4193 often less accurate which results in slower convergence. <i>It is typically 4194 used for code development to check the accuracy of the analytical derivative 4195 formulations. </i><o:p></o:p></span></p> 4102 This also uses the numpy <i>leastsq</i> minimizer, and is also not applicable 4103 for larger problems. Unlike, the "analytic Jacobian", numerical 4104 derivatives are computed rather than use the analytical derivatives that are 4105 coded directly into GSAS-II. This will be slower than the analytical 4106 derivatives and will is often less accurate which results in slower 4107 convergence. <i>It is typically used for code development to check the accuracy 4108 of the analytical derivative formulations. </i><o:p></o:p></span></p> 4196 4109 4197 4110 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4208 4121 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 4209 4122 "Times New Roman"'>Note that the Jacobian refinement tools are the Fortran 4210 MINPACK <span class=SpellE><i>lmdif</i></span> and <span class=SpellE><i>lmder</i></span> 4211 algorithms wrapped in python as provided in the <span class=SpellE>Scipy</span> 4212 package. The Hessian routines were developed for GSAS-II based on routines in <span 4213 class=SpellE>numpy</span> and <span class=SpellE>scipy</span> and using the 4214 material in Numerical Recipes (Press, Flannery, <span class=SpellE>Teulosky</span> 4215 & <span class=SpellE>Vetterling</span>) for the Levenberg-Marquardt. The 4216 purpose is to minimize the sum of the squares of M nonlinear functions in N 4217 variables by a modification of the Levenberg-Marquardt algorithm. The <span 4218 class=SpellE>lmdif</span> and <span class=SpellE>lmder</span> routines were 4219 written by Burton S. <span class=SpellE>Garbow</span>, Kenneth E. <span 4220 class=SpellE>Hillstrom</span>, Jorge J. More (Argonne National Laboratory, 4221 1980). <o:p></o:p></span></p> 4123 MINPACK <i>lmdif</i> and <i>lmder</i> algorithms wrapped in python as provided 4124 in the Scipy package. The Hessian routines were developed for GSAS-II based on 4125 routines in numpy and scipy and using the material in Numerical Recipes (Press, 4126 Flannery, Teulosky & Vetterling) for the Levenberg-Marquardt. The purpose 4127 is to minimize the sum of the squares of M nonlinear functions in N variables 4128 by a modification of the Levenberg-Marquardt algorithm. The lmdif and lmder 4129 routines were written by Burton S. Garbow, Kenneth E. Hillstrom, Jorge J. More 4130 (Argonne National Laboratory, 1980). <o:p></o:p></span></p> 4222 4131 4223 4132 <p class=MsoNormal style='margin-left:1.0in'><b><span style='mso-fareast-font-family: 4224 "Times New Roman"'>Min <span class=GramE>delta-M</span>/M</span></b><span4225 style='mso-fareast-font-family:"Times New Roman"'> <o:p></o:p></span></p>4133 "Times New Roman"'>Min delta-M/M</span></b><span style='mso-fareast-font-family: 4134 "Times New Roman"'> <o:p></o:p></span></p> 4226 4135 4227 4136 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 4228 4137 "Times New Roman"'>A refinement will stop when the change in the minimization 4229 function (M=Σ[w(Io-<span class=SpellE>Ic</span>)<sup>2</sup>]) is less than 4230 this value. The allowed range is 10<sup>-9</sup> to 1.0, with a default of 4231 0.001. A value of 1.0 stops the refinement after a single cycle. Values less 4232 than 10<sup>-4</sup> cause refinements to continue even if there is no 4233 meaningful improvement. <o:p></o:p></span></p> 4138 function (M=Σ[w(Io-Ic)<sup>2</sup>]) is less than this value. The allowed range 4139 is 10<sup>-9</sup> to 1.0, with a default of 0.001. A value of 1.0 stops the 4140 refinement after a single cycle. Values less than 10<sup>-4</sup> cause 4141 refinements to continue even if there is no meaningful improvement. <o:p></o:p></span></p> 4234 4142 4235 4143 <p class=MsoNormal style='margin-left:1.0in'><b><span style='mso-fareast-font-family: … … 4250 4158 weight of 1+λ is applied to the diagonal elements of the Hessian. When λ is 4251 4159 large, this down-weights the significance of the off-diagonal terms in the 4252 Hessian. Thus, when λ is large, the refinement is effectively one of <span4253 class=GramE>steepest-descents</span>, where correlation between variables is 4254 ignored. Note that steepest-descents minimization is typically slow and may not 4255 always find the local minimum. This is only used when with the "analytical 4256 Hessian"minimizer is selected. <o:p></o:p></span></p>4160 Hessian. Thus, when λ is large, the refinement is effectively one of 4161 steepest-descents, where correlation between variables is ignored. Note that 4162 steepest-descents minimization is typically slow and may not always find the 4163 local minimum. This is only used when with the "analytical Hessian" 4164 minimizer is selected. <o:p></o:p></span></p> 4257 4165 4258 4166 <p class=MsoNormal style='margin-left:1.0in'><b><span style='mso-fareast-font-family: … … 4280 4188 4281 4189 <p class=MsoNormal style='margin-left:1.0in'><b><span style='mso-fareast-font-family: 4282 "Times New Roman"'>Min <span class=SpellE>obs</span>/sig</span></b><span4283 style='mso-fareast-font-family:"Times New Roman"'> <o:p></o:p></span></p>4190 "Times New Roman"'>Min obs/sig</span></b><span style='mso-fareast-font-family: 4191 "Times New Roman"'> <o:p></o:p></span></p> 4284 4192 4285 4193 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: … … 4301 4209 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 4302 4210 "Times New Roman"'>Removes reflections that are very poorly fit. Should be used 4303 only with extreme care, since <span class=GramE>poorly-fit</span> reflections4304 could be an indicationthat the structure is wrong. <o:p></o:p></span></p>4211 only with extreme care, since poorly-fit reflections could be an indication 4212 that the structure is wrong. <o:p></o:p></span></p> 4305 4213 4306 4214 <p class=MsoNormal style='margin-left:1.0in'><b><span style='mso-fareast-font-family: … … 4347 4255 4348 4256 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 4349 "Times New Roman"'>Normally, in <span class=GramE>a sequential histograms</span>4350 are fit in the order they are in the data tree (which can be reordered by 4351 dragging tree items), but when this option is selected, the sequential fit is 4352 performed with the lasttree entry first. <o:p></o:p></span></p>4257 "Times New Roman"'>Normally, in a sequential histograms are fit in the order 4258 they are in the data tree (which can be reordered by dragging tree items), but 4259 when this option is selected, the sequential fit is performed with the last 4260 tree entry first. <o:p></o:p></span></p> 4353 4261 4354 4262 <p class=MsoNormal style='margin-left:1.0in'><b><span style='mso-fareast-font-family: … … 4409 4317 4410 4318 <p style='margin-left:1.0in'>Move the mouse cursor across the plot. If on a 4411 diagonal cell, the parameter name, value and <span class=SpellE>esd</span> is4412 shown both as a tool tip and in the right-hand portion of the status bar. If 4413 the cursor is off the diagonal, the two parameter names and their covariance 4414 are shown in the tooltip and the status bar. </p>4319 diagonal cell, the parameter name, value and esd is shown both as a tool tip 4320 and in the right-hand portion of the status bar. If the cursor is off the 4321 diagonal, the two parameter names and their covariance are shown in the tool 4322 tip and the status bar. </p> 4415 4323 4416 4324 <p style='margin-left:1.0in'>Use the Zoom and Pan buttons to focus on some … … 4419 4327 <p style='margin-left:1.0in'>Press ‘s’ – A color scheme selection dialog is 4420 4328 shown. Select a color scheme and press OK, the new color scheme will be 4421 plotted. The default is ‘ <span class=SpellE>RdYlGn</span>’. </p>4329 plotted. The default is ‘RdYlGn’. </p> 4422 4330 4423 4331 <p style='margin-left:1.0in'>Press ‘p’ – Saves the covariance values in a text … … 4429 4337 <span style='mso-bookmark:Constraints'></span> 4430 4338 4431 <p class=MsoNormal style='margin-left:.5in'>This window shows the constraints to4432 be used in a refinement. Constraints are divided with a tab for each type:4433 Phase, Histogram/Phase, Histogram, Global and <span class=SpellE>Sym</span>-Generated.4434 Note that the standard parameters in GSAS-II are divided into three classes and 4435 appearrespectively on the Phase, Histogram and Histogram/Phase tabs: </p>4339 <p class=MsoNormal style='margin-left:.5in'>This window shows the constraints 4340 to be used in a refinement. Constraints are divided with a tab for each type: 4341 Phase, Histogram/Phase, Histogram, Global and Sym-Generated. Note that the 4342 standard parameters in GSAS-II are divided into three classes and appear 4343 respectively on the Phase, Histogram and Histogram/Phase tabs: </p> 4436 4344 4437 4345 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4441 4349 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4442 4350 </span></span></span><![endif]><span style='mso-fareast-font-family:"Times New Roman"'>those 4443 pertaining to quantities in each phase (naming pattern "</span><span 4444 class=GramE><tt><i><span style='font-size:10.0pt'>p</span></i></tt><tt><span 4445 style='font-size:10.0pt'>::</span></tt></span><tt><i><span style='font-size: 4446 10.0pt'>name</span></i></tt><span style='mso-fareast-font-family:"Times New Roman"'>"); 4447 examples include atom coordinates, thermal motion and site fraction parameters; 4448 <o:p></o:p></span></p> 4351 pertaining to quantities in each phase (naming pattern "</span><tt><i><span 4352 style='font-size:10.0pt'>p</span></i></tt><tt><span style='font-size:10.0pt'>::<i>name</i></span></tt><span 4353 style='mso-fareast-font-family:"Times New Roman"'>"); examples include 4354 atom coordinates, thermal motion and site fraction parameters; <o:p></o:p></span></p> 4449 4355 4450 4356 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4454 4360 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4455 4361 </span></span></span><![endif]><span style='mso-fareast-font-family:"Times New Roman"'>those 4456 pertaining to quantities in each histogram (naming pattern ":</span><span 4457 class=SpellE><tt><i><span style='font-size:10.0pt'>h</span></i></tt><tt><span 4458 style='font-size:10.0pt'>:<i>name</i></span></tt></span><span style='mso-fareast-font-family: 4459 "Times New Roman"'>"); such parameters are those that depend only on the 4460 data set the scale factor and profile coefficients (<span class=GramE>e.g.</span> 4461 U, V, W, X and Y); <o:p></o:p></span></p> 4362 pertaining to quantities in each histogram (naming pattern ":</span><tt><i><span 4363 style='font-size:10.0pt'>h</span></i></tt><tt><span style='font-size:10.0pt'>:<i>name</i></span></tt><span 4364 style='mso-fareast-font-family:"Times New Roman"'>"); such parameters are 4365 those that depend only on the data set the scale factor and profile 4366 coefficients (e.g. U, V, W, X and Y); <o:p></o:p></span></p> 4462 4367 4463 4368 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4467 4372 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4468 4373 </span></span></span><![endif]><span style='mso-fareast-font-family:"Times New Roman"'>and 4469 those pertaining to <span class=SpellE>quanitities</span> defined for each4470 histogram in each phase (naming pattern "</span><tt><i><span4471 style='font-size:10.0pt'> p</span></i></tt><tt><span style='font-size:10.0pt'>:<i>h</i>:<i>name</i></span></tt><span4374 those pertaining to quanitities defined for each histogram in each phase 4375 (naming pattern "</span><tt><i><span style='font-size:10.0pt'>p</span></i></tt><tt><span 4376 style='font-size:10.0pt'>:<i>h</i>:<i>name</i></span></tt><span 4472 4377 style='mso-fareast-font-family:"Times New Roman"'>"); these parameters are 4473 4378 quantities that can be dependent on both the phase properties and the sample or 4474 4379 dataset used for the measurement. Examples include phase fractions and 4475 sample-broadening coefficients such as <span class=SpellE>microstrain</span> 4476 and crystallite size. <o:p></o:p></span></p> 4380 sample-broadening coefficients such as microstrain and crystallite size. <o:p></o:p></span></p> 4477 4381 4478 4382 <p class=MsoNormal style='margin-left:.5in'>The following types of constraints … … 4486 4390 "Times New Roman"'>Use this to prevent a parameter from being refined. Most 4487 4391 valuable when refinement of a parameter is selected in a group for refinement 4488 (such as x, y & z for an atom or unit cell parameters). For <span4489 class=GramE>example</span> of the use of this, if the space group for a phase 4490 has a polar axis (e.g. the <i>b</i>-axis in P2<sub>1</sub>), then origin with 4491 respect to <i>b</i> is arbitrary and it is not possible to refine the y 4492 coordinates for all atoms. Place a Hold on any one y coordinate to keep the 4493 structure from drifting up or down the y-axis duringrefinement. <o:p></o:p></span></p>4392 (such as x, y & z for an atom or unit cell parameters). For example of the 4393 use of this, if the space group for a phase has a polar axis (e.g. the <i>b</i>-axis 4394 in P2<sub>1</sub>), then origin with respect to <i>b</i> is arbitrary and it is 4395 not possible to refine the y coordinates for all atoms. Place a Hold on any one 4396 y coordinate to keep the structure from drifting up or down the y-axis during 4397 refinement. <o:p></o:p></span></p> 4494 4398 4495 4399 <p class=MsoNormal style='margin-left:.75in'><b><span style='mso-fareast-font-family: … … 4501 4405 a specified ratio (except for atom coordinates, where the ratios are specified 4502 4406 for the applied shifts, not the actual coordinate values) Examples for typical 4503 use are sets of atoms that should be constrained to have the same displacement <span 4504 class=SpellE>paramaters</span> (aka thermal <span class=SpellE><span 4505 class=GramE>motion,Uiso</span></span>, etc.) or sets of profile coefficients 4407 use are sets of atoms that should be constrained to have the same displacement 4408 paramaters (aka thermal motion,Uiso, etc.) or sets of profile coefficients 4506 4409 U,V,W across multiple data sets. Note that the first selected parameter is 4507 treated as <span class=GramE>independent</span> and the remainder are 4508 "slaved" to that parameter as "dependent parameters." All 4509 parameters in an equivalence must be varied. If any parameter is not varied or 4510 is given a "hold," a warning is displayed and none of the parameters 4511 are refined. <o:p></o:p></span></p> 4410 treated as independent and the remainder are "slaved" to that 4411 parameter as "dependent parameters." All parameters in an equivalence 4412 must be varied. If any parameter is not varied or is given a "hold," 4413 a warning is displayed and none of the parameters are refined. <o:p></o:p></span></p> 4512 4414 4513 4415 <p class=MsoNormal style='margin-left:.75in'><b><span style='mso-fareast-font-family: … … 4518 4420 "Times New Roman"'>Defines a set of parameters whose sum (with possible 4519 4421 non-unitary multipliers) will be equal to a constant. For example, a common use 4520 for this is to specify the sum of occupancies for atoms sharing a site have a 4521 sum fixed to unity or so that the sum of occupancies for an atom type that is 4522 occurs on several sites is fixed to match a <span class=SpellE>compsition</span>-determined 4523 value. Note that all parameters in the equation are considered as 4524 "dependent parameters." If a parameter in a constraint equation is 4525 held or is not varied, that parameter is removed from the equation (the sum 4526 value is modified accordingly). If no parameters remain the equation is 4527 ignored. <o:p></o:p></span></p> 4422 for this is to specify the sum of occupancies for atoms sharing a site have a sum 4423 fixed to unity or so that the sum of occupancies for an atom type that is 4424 occurs on several sites is fixed to match a compsition-determined value. Note 4425 that all parameters in the equation are considered as "dependent 4426 parameters." If a parameter in a constraint equation is held or is not 4427 varied, that parameter is removed from the equation (the sum value is modified 4428 accordingly). If no parameters remain the equation is ignored. <o:p></o:p></span></p> 4528 4429 4529 4430 <p class=MsoNormal style='margin-left:.75in'><b><span style='mso-fareast-font-family: … … 4532 4433 4533 4434 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 4534 "Times New Roman"'>appear <span class=GramE>similar to</span> constraint 4535 equations in that they define a set of parameters and multipliers, but rather 4536 than specifying a value for the expression, a new parameter is assigned to that 4537 sum and these constraints have a very different function. This replaces a 4538 degree of freedom from the original variables with a new one that modifies the 4539 parameters where the shift is applied according to the ratio specified in the 4540 expression. This can be used to create new parameters that redefine the 4541 relationships between items such as coordinates or magnetic moments. The new 4542 parameter may optionally be named by the user. The new var expression creates a 4543 new global parameter, where that new parameter is independent, while all the 4544 parameters in the expression are considered as dependent. The settings of the 4545 refine flags for the dependent parameters is not used. Only if the new var 4546 parameter is marked as refine then it will be refined. However, if any 4547 dependent variable is set as "hold," the new var parameter will not 4548 be refined. <o:p></o:p></span></p> 4435 "Times New Roman"'>appear similar to constraint equations in that they define a 4436 set of parameters and multipliers, but rather than specifying a value for the 4437 expression, a new parameter is assigned to that sum and these constraints have 4438 a very different function. This replaces a degree of freedom from the original 4439 variables with a new one that modifies the parameters where the shift is 4440 applied according to the ratio specified in the expression. This can be used to 4441 create new parameters that redefine the relationships between items such as 4442 coordinates or magnetic moments. The new parameter may optionally be named by 4443 the user. The new var expression creates a new global parameter, where that new 4444 parameter is independent, while all the parameters in the expression are 4445 considered as dependent. The settings of the refine flags for the dependent 4446 parameters is not used. Only if the new var parameter is marked as refine then 4447 it will be refined. However, if any dependent variable is set as 4448 "hold," the new var parameter will not be refined. <o:p></o:p></span></p> 4549 4449 4550 4450 <p class=MsoNormal style='margin-left:.5in'>Note that when new var and 4551 4451 constraint equation constraints are defined, they create new global parameters. 4552 Constraints on these will be rare, but can be managed on the <span 4553 class=SpellE>Globals</span> tab. Finally, some constraints are defined 4554 automatically based on restrictions determined by space group symmetry. These 4555 constraints can be seen, but not changed, using the <span class=SpellE>Sym</span>-Generated 4556 tab. Other constraints (holds) will be created when rigid bodies are specified. 4557 </p> 4452 Constraints on these will be rare, but can be managed on the Globals tab. 4453 Finally, some constraints are defined automatically based on restrictions 4454 determined by space group symmetry. These constraints can be seen, but not 4455 changed, using the Sym-Generated tab. Other constraints (holds) will be created 4456 when rigid bodies are specified. </p> 4558 4457 4559 4458 <h5 style='margin-left:.5in'>What can I do here?</h5> … … 4596 4495 OK. Cancel in either dialog will cancel the operation. The equivalenced 4597 4496 parameters will show as an equation of the form M<sub>1</sub>*P<sub>1</sub>+M<sub>2</sub>*P<sub>2</sub>=0; 4598 usually M1=1.0 and M2=- <span class=GramE>1.0, but</span> can be changed via the4599 ‘Edit’ button. The equation(s) are shown in the window tagged by ‘EQUIV’ to 4600 mark it as anequivalence assignment. <o:p></o:p></span></p>4497 usually M1=1.0 and M2=-1.0, but can be changed via the ‘Edit’ button. The 4498 equation(s) are shown in the window tagged by ‘EQUIV’ to mark it as an 4499 equivalence assignment. <o:p></o:p></span></p> 4601 4500 4602 4501 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4608 4507 style='mso-fareast-font-family:"Times New Roman"'>: If selected, a dialog box 4609 4508 will appear with a list of the available parameters. Select one and press OK; a 4610 second dialog box will appear with only those parameters that can be used in a 4611 constraint with the first one. Choose those and press OK. Cancel in either 4612 dialog will cancel the operation. The equivalenced parameters will show as an 4613 equation of the form M<sub>1</sub>*P<sub>1</sub>+M<sub>2</sub>*P<sub>2</sub>+…=C; 4614 the multipliers M1, M2, … and C can be changed via the ‘Edit’ button. The 4615 equation is shown in the window tagged by ‘CONSTR’ to mark it as a constraint 4616 equationassignment. <o:p></o:p></span></p>4509 second dialog box will appear with only those parameters that can be used in a constraint 4510 with the first one. Choose those and press OK. Cancel in either dialog will 4511 cancel the operation. The equivalenced parameters will show as an equation of 4512 the form M<sub>1</sub>*P<sub>1</sub>+M<sub>2</sub>*P<sub>2</sub>+…=C; the 4513 multipliers M1, M2, … and C can be changed via the ‘Edit’ button. The equation 4514 is shown in the window tagged by ‘CONSTR’ to mark it as a constraint equation 4515 assignment. <o:p></o:p></span></p> 4617 4516 4618 4517 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4636 4535 style='mso-fareast-font-family:"Times New Roman"'>Make atoms equivalent</span></b><span 4637 4536 style='mso-fareast-font-family:"Times New Roman"'>: This provides a shortcut 4638 for establishing constraints when two share a single site. Coordinates and <span4639 class=SpellE>Uiso</span> values are constrained to be the same and site 4640 fractions are constrained to addto 1. <o:p></o:p></span></p>4537 for establishing constraints when two share a single site. Coordinates and Uiso 4538 values are constrained to be the same and site fractions are constrained to add 4539 to 1. <o:p></o:p></span></p> 4641 4540 4642 4541 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4659 4558 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4660 4559 </span></span></span><![endif]><b><span style='mso-fareast-font-family:"Times New Roman"'>Show 4661 <span class=GramE>Errors <span style='font-weight:normal'>:</span></span></span></b><span 4662 style='mso-fareast-font-family:"Times New Roman"'> this button will be active 4663 if serious errors -- that would prevent a refinement from being performed -- 4664 are encountered processing the constraints. <o:p></o:p></span></p> 4560 Errors </span></b><span style='mso-fareast-font-family:"Times New Roman"'>: 4561 this button will be active if serious errors -- that would prevent a refinement 4562 from being performed -- are encountered processing the constraints. <o:p></o:p></span></p> 4665 4563 4666 4564 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4670 4568 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4671 4569 </span></span></span><![endif]><b><span style='mso-fareast-font-family:"Times New Roman"'>Show 4672 <span class=GramE>Warnings <span style='font-weight:normal'>:</span></span></span></b><span 4673 style='mso-fareast-font-family:"Times New Roman"'> this button will be active 4674 if correctable problems are encountered in processing the constraints, such as 4675 a constraint being rejected because a parameter is not varied. These warning 4676 may indicate that the choice of which parameters will be refined is not what 4677 was planned. <o:p></o:p></span></p> 4570 Warnings </span></b><span style='mso-fareast-font-family:"Times New Roman"'>: 4571 this button will be active if correctable problems are encountered in 4572 processing the constraints, such as a constraint being rejected because a 4573 parameter is not varied. These warning may indicate that the choice of which 4574 parameters will be refined is not what was planned. <o:p></o:p></span></p> 4678 4575 4679 4576 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4683 4580 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4684 4581 </span></span></span><![endif]><b><span style='mso-fareast-font-family:"Times New Roman"'>Show 4685 Generated <span class=GramE>Constraints <span style='font-weight:normal'>:</span></span></span></b><span4686 style='mso-fareast-font-family:"Times New Roman"'> After constraints have been 4687 processed, a series of relationships are developed to determine new variables 4688 from the current parameters and "inverse" equations that determine 4689 dependent parameters from the new variables and independent parameters. This 4690 shows the resulting relationships, as well as any"Hold" variables. <o:p></o:p></span></p>4582 Generated Constraints </span></b><span style='mso-fareast-font-family:"Times New Roman"'>: 4583 After constraints have been processed, a series of relationships are developed 4584 to determine new variables from the current parameters and "inverse" 4585 equations that determine dependent parameters from the new variables and 4586 independent parameters. This shows the resulting relationships, as well as any 4587 "Hold" variables. <o:p></o:p></span></p> 4691 4588 4692 4589 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 4696 4593 style='mso-list:Ignore'>·<span style='font:7.0pt "Times New Roman"'> 4697 4594 </span></span></span><![endif]><b><span style='mso-fareast-font-family:"Times New Roman"'>Delete 4698 <span class=GramE>Selected <span style='font-weight:normal'>:</span></span></span></b><span 4699 style='mso-fareast-font-family:"Times New Roman"'> This button will cause all 4700 the selected constraints on the current tab to bedeleted. <o:p></o:p></span></p>4595 Selected </span></b><span style='mso-fareast-font-family:"Times New Roman"'>: 4596 This button will cause all the selected constraints on the current tab to be 4597 deleted. <o:p></o:p></span></p> 4701 4598 4702 4599 <h5 style='margin-left:.5in'><a name=Constraints-SeqRef>Sequential Refinement … … 4709 4606 parameters keyed to a particular constraint number. When sequential refinement 4710 4607 is selected (via the <a href="#Controls">Controls tree item</a>), it becomes 4711 possible to define constraints of form "<span class=GramE><tt><i><span 4712 style='font-size:10.0pt'>p</span></i></tt>:*</span>:<tt><i><span 4713 style='font-size:10.0pt'>name</span></i></tt>" and ":*:<tt><i><span 4714 style='font-size:10.0pt'>name</span></i></tt>" (where "<tt><i><span 4715 style='font-size:10.0pt'>p</span></i></tt>" is a phase number and <tt><i><span 4716 style='font-size:10.0pt'>name</span></i></tt> is a parameter name). The 4717 "*" here is called a wildcard <span class=GramE>and in a constraint</span> 4608 possible to define constraints of form "<tt><i><span style='font-size: 4609 10.0pt'>p</span></i></tt>:*:<tt><i><span style='font-size:10.0pt'>name</span></i></tt>" 4610 and ":*:<tt><i><span style='font-size:10.0pt'>name</span></i></tt>" 4611 (where "<tt><i><span style='font-size:10.0pt'>p</span></i></tt>" is a 4612 phase number and <tt><i><span style='font-size:10.0pt'>name</span></i></tt> is 4613 a parameter name). The "*" here is called a wildcard and in a constraint 4718 4614 or equivalence will cause that to be used for every histogram in turn. </p> 4719 4615 … … 4745 4641 histogram number will be ignored and constraints with a "*" where for 4746 4642 a histogram number will be used. Note that constraints on phase parameters (of 4747 form "</span>< span class=GramE><tt><i><span style='font-size:10.0pt'>p</span></i></tt><span4748 style='mso-fareast-font-family:"Times New Roman"'>::</span>< /span><tt><i><span4643 form "</span><tt><i><span style='font-size:10.0pt'>p</span></i></tt><span 4644 style='mso-fareast-font-family:"Times New Roman"'>::</span><tt><i><span 4749 4645 style='font-size:10.0pt'>name</span></i></tt><span style='mso-fareast-font-family: 4750 4646 "Times New Roman"'>" -- without a histogram number specified) will be used … … 4766 4662 unsatisfiable conflict. <o:p></o:p></span></p> 4767 4663 4768 <p class=MsoNormal style='margin-left:.75in'>Also included when a <span4769 class=GramE>sequential refinements</span>is selected is a menu button labeled <b>"Selected4664 <p class=MsoNormal style='margin-left:.75in'>Also included when a sequential 4665 refinements is selected is a menu button labeled <b>"Selected 4770 4666 histogram."</b> With this it is possible to look at constraint problems 4771 4667 when processing a specific histogram. </p> … … 4797 4693 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 4798 4694 style='mso-fareast-font-family:"Times New Roman"'>You can change the <b 4799 style='mso-bidi-font-weight:normal'>Restraint weight factor</b> – this is used 4800 to scale the weights for the entire set of restraints of this type. Default 4801 valuefor the weight factor is 1.0.<o:p></o:p></span></p>4695 style='mso-bidi-font-weight:normal'>Restraint weight factor</b> – this is used to 4696 scale the weights for the entire set of restraints of this type. Default value 4697 for the weight factor is 1.0.<o:p></o:p></span></p> 4802 4698 4803 4699 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: … … 4821 4717 style='mso-fareast-font-family:"Times New Roman"'>You can examine the table of 4822 4718 restraints and change individual values; grayed out regions cannot be changed. 4823 The ‘calc’ values are determined from the atom positions in your structure, ‘<span4824 class=SpellE>obs</span>’ values are the target values for the restraint and ‘<span 4825 class=SpellE>esd</span>’ is the uncertainty used to weight the restraint inthe4826 refinement (multiplied by theweight factor).<o:p></o:p></span></p>4719 The ‘calc’ values are determined from the atom positions in your structure, 4720 ‘obs’ values are the target values for the restraint and ‘esd’ is the 4721 uncertainty used to weight the restraint in the refinement (multiplied by the 4722 weight factor).<o:p></o:p></span></p> 4827 4723 4828 4724 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: … … 4852 4748 this takes you through a sequence of dialog boxes which ask for the identities 4853 4749 of the atoms involved in the restraint and the value to be assigned to the 4854 restraint. The <span class=SpellE>esd</span> is given a default value which can4855 be changed after therestraints are created.<o:p></o:p></span></p>4750 restraint. The esd is given a default value which can be changed after the 4751 restraints are created.<o:p></o:p></span></p> 4856 4752 4857 4753 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 4863 4759 – if the phase is a ‘macromolecule’ then develop the restraints from a selected 4864 4760 ‘macro’ file based on those used in GSAS for this purpose. A file dialog box is 4865 shown directed to /<span class=SpellE>GSASIImacros</span>; be sure to select 4866 the correct file.<o:p></o:p></span></p> 4761 shown directed to /GSASIImacros; be sure to select the correct file.<o:p></o:p></span></p> 4867 4762 4868 4763 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 4879 4774 case a dialog box will appear asking for the residue types or specific torsion 4880 4775 angles to plot. Each plot will show the observed distribution (blue) obtained 4881 from a wide variety of <span class=GramE>high resolution</span> protein 4882 structures and those found (red dots) for your structure. The restraints are 4883 based on a pseudopotential (red curve or contours – favorable values at the 4884 peaks) which has been developed from the observed distributions for each 4885 residue type.<o:p></o:p></span></p> 4776 from a wide variety of high resolution protein structures and those found (red 4777 dots) for your structure. The restraints are based on a pseudopotential (red 4778 curve or contours – favorable values at the peaks) which has been developed 4779 from the observed distributions for each residue type.<o:p></o:p></span></p> 4886 4780 4887 4781 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 4891 4785 style='mso-bidi-font-weight:normal'><span style='mso-fareast-font-family:"Times New Roman"'>Change 4892 4786 value</span></b><span style='mso-fareast-font-family:"Times New Roman"'> – this 4893 changes the ‘ <span class=SpellE>obsd</span>’ value for selected restraints; a dialog4894 box will appearasking for the new value. <o:p></o:p></span></p>4787 changes the ‘obsd’ value for selected restraints; a dialog box will appear 4788 asking for the new value. <o:p></o:p></span></p> 4895 4789 4896 4790 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 4899 4793 style='font:7.0pt "Times New Roman"'> 4900 4794 </span></span></span><![endif]><b style='mso-bidi-font-weight:normal'><span 4901 style='mso-fareast-font-family:"Times New Roman"'>Change <span class=SpellE>esd</span></span></b><span4902 style='mso-fareast-font-family:"Times New Roman"'> – this changes the ‘ <span4903 class=SpellE>esd</span>’ value for selected restraints; a dialog box will 4904 appear asking for the newvalue.<o:p></o:p></span></p>4795 style='mso-fareast-font-family:"Times New Roman"'>Change esd</span></b><span 4796 style='mso-fareast-font-family:"Times New Roman"'> – this changes the ‘esd’ 4797 value for selected restraints; a dialog box will appear asking for the new 4798 value.<o:p></o:p></span></p> 4905 4799 4906 4800 <p class=MsoListParagraphCxSpLast style='margin-left:1.5in;mso-add-space:auto; … … 4964 4858 XYZ</span></b><span style='mso-fareast-font-family:"Times New Roman"'> – 4965 4859 (Residue rigid bodies) this reads a text file containing a set of Cartesian 4966 coordinates describing a rigid body model. Each line has atom type ( <span4967 class=GramE>e.g.</span> C, Na,etc.) and Cartesian X, Y and Z.<o:p></o:p></span></p>4860 coordinates describing a rigid body model. Each line has atom type (e.g. C, Na, 4861 etc.) and Cartesian X, Y and Z.<o:p></o:p></span></p> 4968 4862 4969 4863 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.5in;mso-add-space: … … 4986 4880 residues</span></b><span style='mso-fareast-font-family:"Times New Roman"'> – 4987 4881 (Residue rigid bodies) this reads a predetermined macro file that contains 4988 standard (<span class=SpellE>Engh</span> & Huber) coordinates for the amino 4989 acids found in natural proteins along with predetermined variable torsion angle 4990 definitions.<o:p></o:p></span></p> 4882 standard (Engh & Huber) coordinates for the amino acids found in natural 4883 proteins along with predetermined variable torsion angle definitions.<o:p></o:p></span></p> 4991 4884 4992 4885 <p class=MsoListParagraphCxSpMiddle style='margin-left:1.0in;mso-add-space: … … 4995 4888 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 4996 4889 style='mso-fareast-font-family:"Times New Roman"'>Once a rigid body is defined 4997 you can plot it, change its <span class=GramE>name</span> or manipulate any4998 torsion angle to see theeffect on the plot.<o:p></o:p></span></p>4890 you can plot it, change its name or manipulate any torsion angle to see the 4891 effect on the plot.<o:p></o:p></span></p> 4999 4892 5000 4893 <p class=MsoListParagraphCxSpLast style='margin-left:1.0in;mso-add-space:auto; … … 5013 4906 use the Calculate/Sequential refine menu command to run the refinement.) When 5014 4907 this is selected, the window tabulates the sequential refinement results. The 5015 columns are the parameter names; the naming convention is ‘<span class=SpellE>p:h:<span 5016 class=GramE>name:n</span></span>’ where ‘p’ is the phase number,’ h’ is the 5017 histogram number, ‘name’ is the parameter name, and ‘n’ (if needed) is the item 5018 number (e.g. atom number). The rows are the data sets used in the sequential 5019 refinement.</p> 4908 columns are the parameter names; the naming convention is ‘p:h:name:n’ where 4909 ‘p’ is the phase number,’ h’ is the histogram number, ‘name’ is the parameter 4910 name, and ‘n’ (if needed) is the item number (e.g. atom number). The rows are 4911 the data sets used in the sequential refinement.</p> 5020 4912 5021 4913 <h5 style='margin-left:.5in'><span style='mso-fareast-font-family:"Times New Roman"'>What … … 5058 4950 style='mso-fareast-font-family:"Times New Roman";color:windowtext;font-weight: 5059 4951 normal;mso-bidi-font-weight:bold'> – this will create a text file of selected 5060 columns with values and corresponding <span class=SpellE>esds</span>. A file 5061 dialog box will appear; give a suitable file name; you may change directory if 5062 desired.<o:p></o:p></span></h5> 4952 columns with values and corresponding esds. A file dialog box will appear; give 4953 a suitable file name; you may change directory if desired.<o:p></o:p></span></h5> 5063 4954 5064 4955 <div class=MsoNormal align=center style='text-align:center'><span … … 5119 5010 <p class=MsoNormal style='margin-left:.5in'><span style='mso-bookmark:PDF'><span 5120 5011 style='mso-fareast-font-family:"Times New Roman"'>By default, the plot will 5121 show a l=0 layer of reflections on a square grid as rings proportional to <span5122 class=SpellE>F<sub>o</sub></span> (blue), F<sub>c</sub> (green) and a central 5123 dot (green or red) proportional to <span class=SpellE>F<sub>o</sub></span>-F<sub>c</sub>.<o:p></o:p></span></span></p>5012 show a l=0 layer of reflections on a square grid as rings proportional to F<sub>o</sub> 5013 (blue), F<sub>c</sub> (green) and a central dot (green or red) proportional to 5014 F<sub>o</sub>-F<sub>c</sub>.<o:p></o:p></span></span></p> 5124 5015 5125 5016 <h5 style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span … … 5127 5018 can I do with the plot?</span></span></h5> 5128 5019 5129 <p class=MsoNormal style='margin-left:.5in'><span style='mso-bookmark:PDF'>The 5130 “K” box in the plot controls shows the 14 keystroke controls for the plot – 5131 theyare generally self-explanatory.</span></p>5020 <p class=MsoNormal style='margin-left:.5in'><span style='mso-bookmark:PDF'>The “K” 5021 box in the plot controls shows the 14 keystroke controls for the plot – they 5022 are generally self-explanatory.</span></p> 5132 5023 5133 5024 <h2 style='margin-left:.25in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span … … 5156 5047 5157 5048 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>The 5158 Optimize PDF button can be used to refine the values of the "Flat <span 5159 class=SpellE>Bkg</span>", "Background ratio" and "Ruland 5160 width" parameters to best agree with the -4*pi*r line that is plotted for 5161 r < <span class=SpellE>Rmin</span>. <span class=SpellE>Rmin</span> should be 5162 set to a distance below the shortest expected interatomic distance for the 5163 material. </p> 5049 Optimize PDF button can be used to refine the values of the "Flat 5050 Bkg", "Background ratio" and "Ruland width" parameters 5051 to best agree with the -4*pi*r line that is plotted for r < Rmin. Rmin 5052 should be set to a distance below the shortest expected interatomic distance 5053 for the material. </p> 5164 5054 5165 5055 <h5 style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>What … … 5167 5057 5168 5058 <p style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>The 5169 PDF parameters can be changed, triggering <span class=SpellE>recomputation</span> 5170 of the <a href="#PDF_I_Q">I(Q)</a>, <a href="#PDF_S_Q">S(Q)</a>, <a 5171 href="#PDF_F_Q">F(Q)</a> and <a href="#PDF_G_R">G(R) functions</a>. Available 5172 menu commands are: </p> 5059 PDF parameters can be changed, triggering recomputation of the <a 5060 href="#PDF_I_Q">I(Q)</a>, <a href="#PDF_S_Q">S(Q)</a>, <a href="#PDF_F_Q">F(Q)</a> 5061 and <a href="#PDF_G_R">G(R) functions</a>. Available menu commands are: </p> 5173 5062 5174 5063 <p class=MsoNormal style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span … … 5176 5065 5177 5066 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5178 style='mso-fareast-font-family:"Times New Roman"'>Adds a new element to the 5179 chemical formula by clicking on a periodic table. Note that the number of atoms5180 of thistype in the empirical formula must still be entered. <o:p></o:p></span></p>5067 style='mso-fareast-font-family:"Times New Roman"'>Adds a new element to the chemical 5068 formula by clicking on a periodic table. Note that the number of atoms of this 5069 type in the empirical formula must still be entered. <o:p></o:p></span></p> 5181 5070 5182 5071 <p class=MsoNormal style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span … … 5184 5073 5185 5074 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5186 style='mso-fareast-font-family:"Times New Roman"'>Removes a <span class=GramE>previously-entered</span>5075 style='mso-fareast-font-family:"Times New Roman"'>Removes a previously-entered 5187 5076 element from the chemical formula. <o:p></o:p></span></p> 5188 5077 … … 5191 5080 5192 5081 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5193 style='mso-fareast-font-family:"Times New Roman"'>Copies the current PDF control5194 values to other PDF data entries <o:p></o:p></span></p>5082 style='mso-fareast-font-family:"Times New Roman"'>Copies the current PDF 5083 control values to other PDF data entries <o:p></o:p></span></p> 5195 5084 5196 5085 <p class=MsoNormal style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span … … 5214 5103 style='mso-fareast-font-family:"Times New Roman"'>Recomputes the PDF for the 5215 5104 current entry. This is usually done automatically when values are changed, but 5216 if <span class=GramE>not</span>this can be forced with this menu item. <o:p></o:p></span></p>5105 if not this can be forced with this menu item. <o:p></o:p></span></p> 5217 5106 5218 5107 <p class=MsoNormal style='margin-left:1.0in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span … … 5221 5110 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5222 5111 style='mso-fareast-font-family:"Times New Roman"'>Recomputes the PDFs for all 5223 selected PDF entries. This is usually done after Copy Controls is used. By <span5224 class=GramE>default</span> PDFs are optimized to reduce the low G(r) region, 5225 but this can beturned off. <o:p></o:p></span></p>5112 selected PDF entries. This is usually done after Copy Controls is used. By 5113 default PDFs are optimized to reduce the low G(r) region, but this can be 5114 turned off. <o:p></o:p></span></p> 5226 5115 5227 5116 <h5 style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span … … 5276 5165 5277 5166 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5278 style='mso-fareast-font-family:"Times New Roman"'>Allows only some PDFs to be plotted,5279 rather than all. <o:p></o:p></span></p>5167 style='mso-fareast-font-family:"Times New Roman"'>Allows only some PDFs to be 5168 plotted, rather than all. <o:p></o:p></span></p> 5280 5169 5281 5170 <p class=MsoNormal style='margin-left:.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b><span … … 5345 5234 5346 5235 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>This 5347 shows the I(Q) function. See the <a href="#PDF_Controls">PDF Controls</a> for information5348 on menu commands and plot options, </p>5236 shows the I(Q) function. See the <a href="#PDF_Controls">PDF Controls</a> for 5237 information on menu commands and plot options, </p> 5349 5238 5350 5239 <h4 style='margin-left:.25in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><a … … 5373 5262 – type IMG </span></a><span style='mso-fareast-font-family:"Times New Roman"'><o:p></o:p></span></h2> 5374 5263 5264 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 5265 "Times New Roman"'>When a 2D diffraction image (prefix ‘IMG’) is selected from 5266 the data tree, the image is displayed as a color contoured picture. At a 5267 minimum, a small ‘X’ shows the currently defined location of the incident beam on 5268 the image plane (NB: it could off to one side or the other depending on 5269 detector location). Optionally, the integration limits are shown as an interior 5270 arc, an outer arc and green (beginning 2</span><span style='font-family:Symbol; 5271 mso-ascii-font-family:"Times New Roman";mso-fareast-font-family:"Times New Roman"; 5272 mso-hansi-font-family:"Times New Roman";mso-char-type:symbol;mso-symbol-font-family: 5273 Symbol'><span style='mso-char-type:symbol;mso-symbol-font-family:Symbol'>Q</span></span><span 5274 style='mso-fareast-font-family:"Times New Roman"'> limit) and red (ending 2</span><span 5275 style='font-family:Symbol;mso-ascii-font-family:"Times New Roman";mso-fareast-font-family: 5276 "Times New Roman";mso-hansi-font-family:"Times New Roman";mso-char-type:symbol; 5277 mso-symbol-font-family:Symbol'><span style='mso-char-type:symbol;mso-symbol-font-family: 5278 Symbol'>Q</span></span><span style='mso-fareast-font-family:"Times New Roman"'> 5279 limit) as well as “cake” section limits (dashed lines) connecting the two. 5280 These are set in <b>Image Controls</b>. There may be a frame mask (green) that encloses 5281 the area used for subsequent integration or other analysis. Red outlines and 5282 pixels indicated selected areas/pixels that are excluded (masked) from further 5283 use; the settings for these are found in <b>Masks</b>. The data window for IMG 5284 shows some controls, most of which are rarely modified (e.g., pixel dimensions) 5285 and are usually obtained via the image importer from either the image header or 5286 a metadata file associated with the image. It is the user’s/instrument 5287 scientist’s responsibility to ensure the accuracy of these values.<o:p></o:p></span></p> 5288 5289 <h5 style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>What 5290 can I do here?<o:p></o:p></h5> 5291 5292 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 5293 "Times New Roman"'>Apart from changing one of the listed values (caution: you 5294 do need to know what their true value is), you can determine the x-ray bean 5295 polarization and create a gain map for your detector. Both require this image 5296 to from a purely isotropic amorphous sample (a glass slide mounted 5297 perpendicular to the incident beam is recommended) with the detector close to 5298 the sample so that the scattering angle at the edge of the detector is at least 5299 35° 2</span><span style='font-family:Symbol;mso-ascii-font-family:"Times New Roman"; 5300 mso-fareast-font-family:"Times New Roman";mso-hansi-font-family:"Times New Roman"; 5301 mso-char-type:symbol;mso-symbol-font-family:Symbol'><span style='mso-char-type: 5302 symbol;mso-symbol-font-family:Symbol'>Q</span></span><span style='mso-fareast-font-family: 5303 "Times New Roman"'>; better is > 40° 2</span><span style='font-family:Symbol; 5304 mso-ascii-font-family:"Times New Roman";mso-fareast-font-family:"Times New Roman"; 5305 mso-hansi-font-family:"Times New Roman";mso-char-type:symbol;mso-symbol-font-family: 5306 Symbol'><span style='mso-char-type:symbol;mso-symbol-font-family:Symbol'>Q</span></span><span 5307 style='mso-fareast-font-family:"Times New Roman"'>. A frame mask is recommended 5308 to remove detector edge effects. The image should be as free as possible 5309 (except for beam stop) from shadows and obstructions and normal to the incident 5310 beam. The detector orientation should have been previously calibrated with a 5311 known reference material (e.g., LaB<sub>6</sub> or Si).<o:p></o:p></span></p> 5312 5313 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 5314 "Times New Roman"'><o:p> </o:p></span></p> 5315 5316 <p class=MsoNormal style='margin-left:.25in'><b><span style='mso-fareast-font-family: 5317 "Times New Roman"'>Polarization</span></b><span style='mso-fareast-font-family: 5318 "Times New Roman"'> – <b>Calibrate</b>? <o:p></o:p></span></p> 5319 5320 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 5321 "Times New Roman"'>This begins the calibration procedure (<a 5322 href="https://doi.org/10.1107/S1600576720014132">Von Dreele & Xi, 2021</a>) 5323 for the x-ray beam polarization which integrates a 4° 2</span><span 5324 style='font-family:Symbol;mso-ascii-font-family:"Times New Roman";mso-fareast-font-family: 5325 "Times New Roman";mso-hansi-font-family:"Times New Roman";mso-char-type:symbol; 5326 mso-symbol-font-family:Symbol'><span style='mso-char-type:symbol;mso-symbol-font-family: 5327 Symbol'>Q</span></span><span style='mso-fareast-font-family:"Times New Roman"'> 5328 wide ring sampling area with and without an arc mask positioned about 90° 5329 azimuth (top of image) with selected polarization values. The integrations 5330 match with the correct polarization. You will be asked for a 2</span><span 5331 style='font-family:Symbol;mso-ascii-font-family:"Times New Roman";mso-fareast-font-family: 5332 "Times New Roman";mso-hansi-font-family:"Times New Roman";mso-char-type:symbol; 5333 mso-symbol-font-family:Symbol'><span style='mso-char-type:symbol;mso-symbol-font-family: 5334 Symbol'>Q</span></span><span style='mso-fareast-font-family:"Times New Roman"'> 5335 position for the sampling mask; choose a value at least 2° 2</span><span 5336 style='font-family:Symbol;mso-ascii-font-family:"Times New Roman";mso-fareast-font-family: 5337 "Times New Roman";mso-hansi-font-family:"Times New Roman";mso-char-type:symbol; 5338 mso-symbol-font-family:Symbol'><span style='mso-char-type:symbol;mso-symbol-font-family: 5339 Symbol'>Q</span></span><span style='mso-fareast-font-family:"Times New Roman"'> 5340 less than the maximum 2</span><span style='font-family:Symbol;mso-ascii-font-family: 5341 "Times New Roman";mso-fareast-font-family:"Times New Roman";mso-hansi-font-family: 5342 "Times New Roman";mso-char-type:symbol;mso-symbol-font-family:Symbol'><span 5343 style='mso-char-type:symbol;mso-symbol-font-family:Symbol'>Q</span></span><span 5344 style='mso-fareast-font-family:"Times New Roman"'> seen for all edges inside 5345 the frame mask. The process takes about 5min, so be patient.<o:p></o:p></span></p> 5346 5347 <p class=MsoNormal style='margin-left:.25in'><b><span style='mso-fareast-font-family: 5348 "Times New Roman"'>Make gain map …<o:p></o:p></span></b></p> 5349 5350 <p class=MsoNormal style='margin-left:.5in'><span style='mso-fareast-font-family: 5351 "Times New Roman"'>This uses the same image (from a glass slide) used for 5352 polarization analysis to determine a gain map for the detector. The process 5353 uses the result of an integration of the glass pattern to normalize the entire detector 5354 pixel array. The result (~1.0 for all pixels) is the scaled by 1000, converted 5355 to integers and stored as a GSAS-II image file (NB: this is a python pickle 5356 file and thus not usable by other programs) and entered in the GSAS-II data 5357 tree. You can view it to see what the map looks like (select its IMG entry). The 5358 gain map file can be imported into other projects using the same detector. If 5359 selected in Image Controls, the image is immediately corrected for the gain 5360 map.<o:p></o:p></span></p> 5361 5375 5362 <h4 style='margin-left:.25in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><a 5376 5363 name="IMG_Comments"><u>Comments</u></a></h4> … … 5379 5366 window shows whatever comment lines found in a “metadata” file when the image 5380 5367 data file was read by GSAS-II. If you are lucky, there will be useful 5381 information here (<span class=GramE>e.g.</span> sample name, date collected, 5382 wavelength used, etc.). If not, this window will be blank. The text is 5383 read-only.</p> 5368 information here (e.g., sample name, date collected, wavelength used, etc.). If 5369 not, this window will be blank. The text is read-only.</p> 5384 5370 5385 5371 <h4 style='margin-left:.25in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>Image … … 5392 5378 5393 5379 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>Menu 5394 command for this window <span class=GramE>are</span> used to perform 5395 calibration (fitting the calibration values from a diffraction pattern image 5396 taken with a calibrant) and for integration. Other menu commands allow the 5397 values on the window to be saved to a file, read from a <span class=GramE>file</span> 5398 or copied to other images. The "Xfer Angles" menu command scales the 5399 current integration range for other images located at different detector 5400 distances. <span class=MsoHyperlink><span style='color:windowtext;text-decoration: 5401 none;text-underline:none'><o:p></o:p></span></span></p> 5380 commands for this window are used to perform calibration (fitting the 5381 calibration values from a diffraction pattern image taken with a calibrant) and 5382 for integration. Other menu commands allow the values on the window to be saved 5383 to a file, read from a file or copied to other images. The "Xfer 5384 Angles" menu command scales the current integration range for other images 5385 located at different detector distances. <span class=MsoHyperlink><span 5386 style='color:windowtext;text-decoration:none;text-underline:none'><o:p></o:p></span></span></p> 5402 5387 5403 5388 <h4 style='margin-left:.25in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><a … … 5406 5391 <p class=MsoNormal style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><span 5407 5392 style='mso-fareast-font-family:"Times New Roman"'>Image masks are used 5408 designate areas of an image that should not be included in the integration, typically5409 used due to detector irregularities, shadows of the <span class=SpellE>beamstop</span>,5393 designate areas of an image that should not be included in the integration, 5394 typically used due to detector irregularities, shadows of the beam stop, 5410 5395 single-crystal peaks from a mounting, etc. Masks can be created with a menu 5411 5396 command or with keyboard/mouse shortcuts. There are five types of masks:<o:p></o:p></span></p> … … 5422 5407 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>2.<span 5423 5408 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 5424 style='mso-fareast-font-family:"Times New Roman"'>Ring masks: occludes a 5425 specific Bragg reflection (a ring placed relative to the image center). The 5426 location andthickness of the ring are specified in degrees 2-theta. <o:p></o:p></span></p>5409 style='mso-fareast-font-family:"Times New Roman"'>Ring masks: occludes a specific 5410 Bragg reflection (a ring placed relative to the image center). The location and 5411 thickness of the ring are specified in degrees 2-theta. <o:p></o:p></span></p> 5427 5412 5428 5413 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5431 5416 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 5432 5417 style='mso-fareast-font-family:"Times New Roman"'>Arc masks: occlude a section 5433 of a Bragg reflection, <span class=GramE>similar to</span> a ring mask, except5434 that in addition to the location and thickness of the ring, the mask has a 5435 starting and endingazimuthal angle. <o:p></o:p></span></p>5418 of a Bragg reflection, similar to a ring mask, except that in addition to the 5419 location and thickness of the ring, the mask has a starting and ending 5420 azimuthal angle. <o:p></o:p></span></p> 5436 5421 5437 5422 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5439 5424 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>4.<span 5440 5425 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 5441 style='mso-fareast-font-family:"Times New Roman"'>Polygon masks: occlude an <span 5442 class=SpellE>arbitary</span> region created by line segments joining a series 5443 of points specified in image coordinates (mm). Pixels inside the polygon mask 5444 are not used for integration. <o:p></o:p></span></p> 5426 style='mso-fareast-font-family:"Times New Roman"'>Polygon masks: occlude an arbitrary 5427 region created by line segments joining a series of points specified in image 5428 coordinates (mm). Pixels inside the polygon mask are not used for integration. <o:p></o:p></span></p> 5445 5429 5446 5430 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5448 5432 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>5.<span 5449 5433 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 5450 style='mso-fareast-font-family:"Times New Roman"'>The Frame mask: occludes an <span5451 class=SpellE>arbitary</span> region created by line segments joining a series 5452 of points specified in image coordinates (mm). <span class=GramE>Typically</span> 5453 a point is placed near each corner of the image. Only pixels inside the frame 5454 mask are used for integration. Only one frame maskcan be defined. <o:p></o:p></span></p>5434 style='mso-fareast-font-family:"Times New Roman"'>The Frame mask: occludes an arbitrary 5435 region created by line segments joining a series of points specified in image 5436 coordinates (mm). Typically, a point is placed near each corner of the image. 5437 Only pixels inside the frame mask are used for integration. Only one frame mask 5438 can be defined. <o:p></o:p></span></p> 5455 5439 5456 5440 <h5 style='margin-left:.5in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>What … … 5483 5467 5484 5468 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Create 5485 Spot masks</b> after a menu command by clicking on the location on the image that5486 should be masked. There are also two ways to create spot masks with the5469 Spot masks</b> after a menu command by clicking on the location on the image 5470 that should be masked. There are also two ways to create spot masks with the 5487 5471 keyboard: </p> 5488 5472 … … 5492 5476 mso-fareast-font-family:"Courier New"'><span style='mso-list:Ignore'>o<span 5493 5477 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 5494 style='mso-fareast-font-family:"Times New Roman"'>Press the 's' key and then <span 5495 class=GramE>left-click</span> successively on multiple locations for spot 5496 masks. Press the 's' key again or <a href="#Mac_rightclick">right-click*</a> to 5497 stop adding spot masks. <o:p></o:p></span></p> 5478 style='mso-fareast-font-family:"Times New Roman"'>Press the 's' key and then 5479 left-click successively on multiple locations for spot masks. Press the 's' key 5480 again or <a href="#Mac_rightclick">right-click*</a> to stop adding spot masks. <o:p></o:p></span></p> 5498 5481 5499 5482 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5507 5490 5508 5491 <p style='margin-left:1.95in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>The 5509 default size for <span class=GramE>newly-created</span> spot masks is5510 determined by the <span class=SpellE><tt><span style='font-size:10.0pt'>Spot_mask_diameter</span></tt></span> 5511 <a href="#Preferences">configurationvariable</a> or 1.0 mm, if not specified. </p>5492 default size for newly-created spot masks is determined by the <tt><span 5493 style='font-size:10.0pt'>Spot_mask_diameter</span></tt> <a href="#Preferences">configuration 5494 variable</a> or 1.0 mm, if not specified. </p> 5512 5495 5513 5496 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Edit 5514 Spot mask location</b> by <span class=GramE>left-clicking</span> inside or on5515 the edge the of the maskand then drag the spot mask to a new location. </p>5497 Spot mask location</b> by left-clicking inside or on the edge the of the mask 5498 and then drag the spot mask to a new location. </p> 5516 5499 5517 5500 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Edit … … 5526 5509 5527 5510 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Create 5528 Ring masks</b> with a menu command and then by left-clicking on the mask center;5529 Or, by pressing the 'r' key and then left-clicking. (<a href="#Mac_rightclick">Right-click*</a> 5530 to cancel.) </p>5511 Ring masks</b> with a menu command and then by left-clicking on the mask 5512 center; Or, by pressing the 'r' key and then left-clicking. (<a 5513 href="#Mac_rightclick">Right-click*</a> to cancel.) </p> 5531 5514 5532 5515 <p style='margin-left:1.95in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>The 5533 default thickness for <span class=GramE>newly-created</span> ring masks is 5534 determined by the <span class=SpellE><tt><span style='font-size:10.0pt'>Ring_mask_thickness</span></tt></span> 5535 <a href="#Preferences">configuration variable</a> or 0.1 degrees (2theta) if 5536 not specified. </p> 5516 default thickness for newly-created ring masks is determined by the <tt><span 5517 style='font-size:10.0pt'>Ring_mask_thickness</span></tt> <a href="#Preferences">configuration 5518 variable</a> or 0.1 degrees (2theta) if not specified. </p> 5537 5519 5538 5520 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Edit 5539 Ring mask location</b> by <span class=GramE>left-clicking</span> on either the5540 inner or outer circle anddrag the circle to the new radius. </p>5521 Ring mask location</b> by left-clicking on either the inner or outer circle and 5522 drag the circle to the new radius. </p> 5541 5523 5542 5524 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Edit 5543 5525 Ring mask thickness</b> by <a href="#Mac_rightclick">right-clicking*</a> either 5544 on the inner or outer circle and drag the <span class=SpellE>the</span> circle5545 change spacing between theinner and outer circle. </p>5526 on the inner or outer circle and drag the the circle change spacing between the 5527 inner and outer circle. </p> 5546 5528 5547 5529 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5550 5532 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 5551 5533 style='mso-fareast-font-family:"Times New Roman"'>Arc masks: occludes a section 5552 of a Bragg reflection, <span class=GramE>similar to</span> a ring mask, except that5553 in addition to the location and thickness of the ring, the mask has a starting5554 a nd ending azimuthal angle. <o:p></o:p></span></p>5534 of a Bragg reflection, similar to a ring mask, except that in addition to the 5535 location and thickness of the ring, the mask has a starting and ending 5536 azimuthal angle. <o:p></o:p></span></p> 5555 5537 5556 5538 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Create … … 5560 5542 5561 5543 <p style='margin-left:1.95in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'>The 5562 default size for <span class=GramE>newly-created</span> ring masks is5563 determined by <ahref="#Preferences">configuration variables</a><br>5564 thickness: < span class=SpellE><tt><span style='font-size:10.0pt'>Ring_mask_thickness</span></tt></span>5544 default size for newly-created ring masks is determined by <a 5545 href="#Preferences">configuration variables</a><br> 5546 thickness: <tt><span style='font-size:10.0pt'>Ring_mask_thickness</span></tt> 5565 5547 (0.1 degrees 2theta if not specified) and <br> 5566 azimuthal range: < span class=SpellE><tt><span style='font-size:10.0pt'>Arc_mask_azimuth</span></tt></span>5548 azimuthal range: <tt><span style='font-size:10.0pt'>Arc_mask_azimuth</span></tt> 5567 5549 (10.0 degrees if not specified.) </p> 5568 5550 5569 5551 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Edit 5570 Arc mask location</b> by <span class=GramE>left-clicking</span> on either the 5571 inner or outer circle and drag the circle to the new radius. Alternately, <span 5572 class=GramE>left-click</span> on the upper or lower arc limit (the straight 5573 lines) and drag them to rotate the center of the arc azimuthal range to a new 5574 position. </p> 5552 Arc mask location</b> by left-clicking on either the inner or outer circle and 5553 drag the circle to the new radius. Alternately, left-click on the upper or 5554 lower arc limit (the straight lines) and drag them to rotate the center of the 5555 arc azimuthal range to a new position. </p> 5575 5556 5576 5557 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Edit 5577 5558 Arc mask thickness or range</b> by <a href="#Mac_rightclick">right-clicking*</a> 5578 either on the inner or outer circle and drag the <span class=SpellE>the</span>5579 circle change spacing between the inner and outer circle. Alternately, <a 5580 href="#Mac_rightclick">right-click*</a> on the upper or lower arc limit (the5581 straight lines) and drag them to changethe arc azimuthal range. </p>5559 either on the inner or outer circle and drag the the circle change spacing 5560 between the inner and outer circle. Alternately, <a href="#Mac_rightclick">right-click*</a> 5561 on the upper or lower arc limit (the straight lines) and drag them to change 5562 the arc azimuthal range. </p> 5582 5563 5583 5564 <p class=MsoNormal style='mso-margin-top-alt:auto;mso-margin-bottom-alt:auto; … … 5585 5566 style='mso-fareast-font-family:"Times New Roman"'><span style='mso-list:Ignore'>4.<span 5586 5567 style='font:7.0pt "Times New Roman"'> </span></span></span><![endif]><span 5587 style='mso-fareast-font-family:"Times New Roman"'>Polygon masks: occludes an <span 5588 class=SpellE>arbitary</span> region created by line segments joining a series 5589 of points specified in image coordinates (mm). Pixels inside the polygon mask 5590 are not used for integration. <o:p></o:p></span></p> 5568 style='mso-fareast-font-family:"Times New Roman"'>Polygon masks: occludes an arbitrary 5569 region created by line segments joining a series of points specified in image 5570 coordinates (mm). Pixels inside the polygon mask are not used for integration. <o:p></o:p></span></p> 5591 5571 5592 5572 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Create 5593 Polygon masks</b> with a menu command and then by <span class=GramE>left-clicking</span>5594 successively on the vertices of the polygon shape surrounding pixels to be5595 excluded. After the last point is defined, <a href="#Mac_rightclick">right-click*</a> 5596 anywhere to close the mask. Alternately, press the 'p' key and then left-click,5597 as before, to define the mask and <a href="#Mac_rightclick">right-click*</a> 5598 anywhere toclose the mask. </p>5573 Polygon masks</b> with a menu command and then by left-clicking successively on 5574 the vertices of the polygon shape surrounding pixels to be excluded. After the 5575 last point is defined, <a href="#Mac_rightclick">right-click*</a> anywhere to 5576 close the mask. Alternately, press the 'p' key and then left-click, as before, 5577 to define the mask and <a href="#Mac_rightclick">right-click*</a> anywhere to 5578 close the mask. </p> 5599 5579 5600 5580 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Edit 5601 Polygon mask</b> by <span class=GramE>left-clicking</span> on any point at a 5602 vertex in the polygon mask and drag that point to a new position. If the vertex 5603 is dragged to the same position as any other vertex in the mask the dragged 5604 point is deleted. </p> 5581 Polygon mask</b> by left-clicking on any point at a vertex in the polygon mask 5582 and drag that point to a new position. If the vertex is dragged to the same 5583 position as any other vertex in the mask the dragged point is deleted. </p> 5605 5584 5606 5585 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Add … … 5615 5594 style='mso-fareast-font-family:"Times New Roman"'>The Frame mask: occludes an 5616 5595 arbitrary region created by line segments joining a series of points specified 5617 in image coordinates (mm). <span class=GramE>Typically</span> a point is placed5618 near each corner of the image. Only pixels inside the frame mask are used for 5619 integration. Only oneframe mask can be defined. <o:p></o:p></span></p>5596 in image coordinates (mm). Typically a point is placed near each corner of the 5597 image. Only pixels inside the frame mask are used for integration. Only one 5598 frame mask can be defined. <o:p></o:p></span></p> 5620 5599 5621 5600 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Create 5622 a Frame mask</b> with a menu command and then by <span class=GramE>left-clicking</span>5623 successively onthe vertices of a polygon. After the last point is defined, <a5624 href="#Mac_rightclick">right-click*</a> anywhere to close the frame mask. Alternately,5625 press the 'f' key and then left-click, as before, to define the mask and <a 5626 href="#Mac_rightclick">right-click*</a> anywhere to close the mask. Note that 5627 if a Frame mask already exists, using the 'f' key or the "Create5601 a Frame mask</b> with a menu command and then by left-clicking successively on 5602 the vertices of a polygon. After the last point is defined, <a 5603 href="#Mac_rightclick">right-click*</a> anywhere to close the frame mask. 5604 Alternately, press the 'f' key and then left-click, as before, to define the 5605 mask and <a href="#Mac_rightclick">right-click*</a> anywhere to close the mask. 5606 Note that if a Frame mask already exists, using the 'f' key or the "Create 5628 5607 Frame" menu item causes the existing frame mask to be deleted. </p> 5629 5608 5630 5609 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Edit 5631 the Frame mask</b> by <span class=GramE>left-clicking</span> on any point at a 5632 vertex in the frame mask and drag that point to a new position. If the vertex 5633 is dragged to the same position as any other vertex in the mask the dragged 5634 point is deleted. </p> 5610 the Frame mask</b> by left-clicking on any point at a vertex in the frame mask 5611 and drag that point to a new position. If the vertex is dragged to the same 5612 position as any other vertex in the mask the dragged point is deleted. </p> 5635 5613 5636 5614 <p style='margin-left:1.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><b>Add 5637 a point to the Frame mask</b> by <a href="#Mac_rightclick">right-clicking*</a> 5638 on any vertex and dragging. A new point is added to the mask immediately after 5639 theselected point at the position where the mouse is released. </p>5615 a point to the Frame mask</b> by <a href="#Mac_rightclick">right-clicking*</a> on 5616 any vertex and dragging. A new point is added to the mask immediately after the 5617 selected point at the position where the mouse is released. </p> 5640 5618 5641 5619 <p style='margin-left:.75in;tab-stops:45.8pt 91.6pt 137.4pt 183.2pt 229.0pt 274.8pt 320.6pt 366.4pt 412.2pt 458.0pt 503.8pt 549.6pt 595.4pt 641.2pt 687.0pt 732.8pt'><a … … 5677 5655 <p class=MsoNormal style='margin-left:.25in'>This window shows whatever comment 5678 5656 lines (preceded by “#”) found when the peaks data file was read by GSAS-II. If 5679 you are lucky, there will be useful information here ( <span class=GramE>e.g.</span>5680 sample name, date collected, wavelength used, etc.). If not, this window will 5681 be blank. The textis read-only.</p>5657 you are lucky, there will be useful information here (e.g. sample name, date 5658 collected, wavelength used, etc.). If not, this window will be blank. The text 5659 is read-only.</p> 5682 5660 5683 5661 <h4><a name="PKS_Limits">Limits</a></h4> … … 5694 5672 can I do here?<o:p></o:p></span></h5> 5695 5673