Changeset 3635
- Timestamp:
- Oct 1, 2018 1:20:06 PM (5 years ago)
- Location:
- Tutorials
- Files:
-
- 55 added
- 31 deleted
- 3 edited
Legend:
- Unmodified
- Added
- Removed
-
Tutorials/Magnetic-III/Magnetic-III.htm
r3632 r3635 23 23 <o:Author>Von Dreele</o:Author> 24 24 <o:LastAuthor>vondreele</o:LastAuthor> 25 <o:Revision>1 6</o:Revision>26 <o:TotalTime>5 54</o:TotalTime>25 <o:Revision>17</o:Revision> 26 <o:TotalTime>562</o:TotalTime> 27 27 <o:Created>2012-05-05T14:50:00Z</o:Created> 28 <o:LastSaved>2018- 09-30T13:28:00Z</o:LastSaved>28 <o:LastSaved>2018-10-01T13:53:00Z</o:LastSaved> 29 29 <o:Pages>19</o:Pages> 30 <o:Words>21 54</o:Words>31 <o:Characters>12 281</o:Characters>30 <o:Words>2164</o:Words> 31 <o:Characters>12339</o:Characters> 32 32 <o:Lines>102</o:Lines> 33 33 <o:Paragraphs>28</o:Paragraphs> 34 <o:CharactersWithSpaces>144 07</o:CharactersWithSpaces>34 <o:CharactersWithSpaces>14475</o:CharactersWithSpaces> 35 35 <o:Version>16.00</o:Version> 36 36 </o:DocumentProperties> … … 1288 1288 normal'>Magnetic Symmetry and Applications</i> routine k-SUBGROUPSMAG (<a 1289 1289 href="http://iopscience.iop.org/0953-8984/28/28/286001"><span style='font-size: 1290 10.0pt;font-family:"Arial",sans-serif'>Perez-<span class=SpellE>Mato</span>, 1291 JM; <span class=SpellE>Gallego</span>, SV; <span class=SpellE>Elcoro</span>, L; 1292 <span class=SpellE>Tasci</span>, E and <span class=SpellE>Aroyo</span>, MI</span><span 1293 style='font-size:10.0pt;font-family:"Arial",sans-serif;color:windowtext; 1294 text-decoration:none;text-underline:none'><br> 1295 </span><i><span style='font-size:10.0pt;font-family:"Arial",sans-serif'>J. of 1296 Phys.: <span class=SpellE>Condens</span> Matter</span></i><span 1297 style='font-size:10.0pt;font-family:"Arial",sans-serif'> (2016), <b>28</b>:28601</span></a>) 1298 to determine a magnetic crystal structure with a non-zero propagation vector. 1299 If you have not done so already, you may wish to do the Simple Magnetic 1300 Structures tutorial first as it contains some background information that will 1301 not be covered here. It is also helpful to do parts I and II of the series of 1302 Magnetic Structures tutorials. To make this work, your computer must have an 1303 internet connection for GSAS-II to access this site. (We will supply the 1304 project file that results after k-SUBGROUPSMAG is called in case you lack 1305 internet access).</p> 1290 10.0pt;font-family:"Arial",sans-serif'>Perez-Mato, JM; <span class=SpellE>Gallego</span>, 1291 SV; <span class=SpellE>Elcoro</span>, L; <span class=SpellE>Tasci</span>, E and 1292 <span class=SpellE>Aroyo</span>, MI, <i>J. of Phys.: <span class=SpellE>Condens</span> 1293 Matter</i> (2016), <b>28</b>:28601</span></a>) to determine a magnetic crystal 1294 structure with a non-zero propagation vector. If you have not done so already, 1295 you may wish to do the Simple Magnetic Structures tutorial first as it contains 1296 some background information that will not be covered here. It is also helpful 1297 to do parts I and II of the series of Magnetic Structures tutorials. To make 1298 this work, your computer must have an internet connection for GSAS-II to access 1299 this site. (We will supply the project file that results after k-SUBGROUPSMAG 1300 is called in case you lack internet access).</p> 1306 1301 1307 1302 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shapetype … … 1326 1321 <o:lock v:ext="edit" aspectratio="t"/> 1327 1322 </v:shapetype><v:shape id="Picture_x0020_4" o:spid="_x0000_i1055" type="#_x0000_t75" 1328 style='width:359.25pt;height:369 .75pt;visibility:visible;mso-wrap-style:square'>1323 style='width:359.25pt;height:369pt;visibility:visible;mso-wrap-style:square'> 1329 1324 <v:imagedata src="Magnetic-III_files/image001.png" o:title=""/> 1330 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=49 31331 src="Magnetic-III_files/image00 2.gif" v:shapes="Picture_x0020_4"><![endif]></span></p>1325 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=492 1326 src="Magnetic-III_files/image004.gif" v:shapes="Picture_x0020_4"><![endif]></span></p> 1332 1327 1333 1328 <p class=MsoNormal>In this example, we will determine the magnetic structure … … 1350 1345 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1351 1346 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1352 <v:imagedata src="Magnetic-III_files/image03 6.png" o:title="" chromakey="white"/>1347 <v:imagedata src="Magnetic-III_files/image035.png" o:title="" chromakey="white"/> 1353 1348 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1354 src="Magnetic-III_files/image0 04.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m21349 src="Magnetic-III_files/image036.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2 1355 1350 with a= 5.64870 Å and c= 5.64870 Å. From the structure drawing above, you can 1356 1351 see a tetrameric string of face sharing CoO<sub>6</sub> <span class=SpellE>octahedra</span> … … 1433 1428 1434 1429 <p class=MsoListParagraphCxSpLast><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1435 id="Picture_x0020_5" o:spid="_x0000_i1054" type="#_x0000_t75" style='width:324 .75pt;1430 id="Picture_x0020_5" o:spid="_x0000_i1054" type="#_x0000_t75" style='width:324pt; 1436 1431 height:199.5pt;visibility:visible;mso-wrap-style:square'> 1437 1432 <v:imagedata src="Magnetic-III_files/image003.png" o:title=""/> 1438 </v:shape><![endif]--><![if !vml]><img border=0 width=43 3height=2661439 src="Magnetic-III_files/image0 06.gif" v:shapes="Picture_x0020_5"><![endif]></span></p>1433 </v:shape><![endif]--><![if !vml]><img border=0 width=432 height=266 1434 src="Magnetic-III_files/image057.gif" v:shapes="Picture_x0020_5"><![endif]></span></p> 1440 1435 1441 1436 <p class=MsoNormal style='margin-left:.5in'><span class=GramE>and</span> the … … 1444 1439 <p class=MsoNormal style='margin-left:.5in'><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1445 1440 id="Picture_x0020_6" o:spid="_x0000_i1053" type="#_x0000_t75" style='width:324.75pt; 1446 height:33 4.5pt;visibility:visible;mso-wrap-style:square'>1441 height:335.25pt;visibility:visible;mso-wrap-style:square'> 1447 1442 <v:imagedata src="Magnetic-III_files/image005.png" o:title=""/> 1448 </v:shape><![endif]--><![if !vml]><img border=0 width=433 height=44 61449 src="Magnetic-III_files/image0 08.gif" v:shapes="Picture_x0020_6"><![endif]></span></p>1443 </v:shape><![endif]--><![if !vml]><img border=0 width=433 height=447 1444 src="Magnetic-III_files/image058.gif" v:shapes="Picture_x0020_6"><![endif]></span></p> 1450 1445 1451 1446 <p class=MsoNormal style='margin-left:.5in'>We will use the default limits.</p> … … 1507 1502 <v:imagedata src="Magnetic-III_files/image007.png" o:title=""/> 1508 1503 </v:shape><![endif]--><![if !vml]><img border=0 width=430 height=235 1509 src="Magnetic-III_files/image0 10.gif" v:shapes="Picture_x0020_7"><![endif]></span></p>1504 src="Magnetic-III_files/image059.gif" v:shapes="Picture_x0020_7"><![endif]></span></p> 1510 1505 1511 1506 <h3>Step 3. Check powder pattern indexing</h3> 1512 1507 1513 <p class=MsoNormal>Here the objective is to determine how the reflection positions1514 generated from the chemical (nuclear) crystal structure lattice match up with 1515 the peaks observed for this antiferromagnet. </p>1508 <p class=MsoNormal>Here the objective is to determine how the reflection 1509 positions generated from the chemical (nuclear) crystal structure lattice 1510 match up with the peaks observed for this antiferromagnet. </p> 1516 1511 1517 1512 <p class=MsoNormal>Select <b style='mso-bidi-font-weight:normal'><span … … 1525 1520 <v:imagedata src="Magnetic-III_files/image009.png" o:title=""/> 1526 1521 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=162 1527 src="Magnetic-III_files/image0 12.gif" v:shapes="Picture_x0020_8"><![endif]></span></p>1522 src="Magnetic-III_files/image060.gif" v:shapes="Picture_x0020_8"><![endif]></span></p> 1528 1523 1529 1524 <p class=MsoNormal>This can use lattice parameters & space groups to … … 1548 1543 and the Indexing controls will be change<br> 1549 1544 <span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape id="Picture_x0020_9" 1550 o:spid="_x0000_i1050" type="#_x0000_t75" style='width:35 8.5pt;height:114pt;1545 o:spid="_x0000_i1050" type="#_x0000_t75" style='width:357.75pt;height:114pt; 1551 1546 visibility:visible;mso-wrap-style:square'> 1552 1547 <v:imagedata src="Magnetic-III_files/image011.png" o:title=""/> 1553 </v:shape><![endif]--><![if !vml]><img border=0 width=47 8height=1521554 src="Magnetic-III_files/image0 14.gif" v:shapes="Picture_x0020_9"><![endif]></span></p>1548 </v:shape><![endif]--><![if !vml]><img border=0 width=477 height=152 1549 src="Magnetic-III_files/image061.gif" v:shapes="Picture_x0020_9"><![endif]></span></p> 1555 1550 1556 1551 <p class=MsoNormal><span class=GramE>showing</span> the lattice constants for … … 1567 1562 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1568 1563 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1569 <v:imagedata src="Magnetic-III_files/image03 6.png" o:title="" chromakey="white"/>1564 <v:imagedata src="Magnetic-III_files/image035.png" o:title="" chromakey="white"/> 1570 1565 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1571 src="Magnetic-III_files/image0 04.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m21566 src="Magnetic-III_files/image036.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2 1572 1567 and those lattice parameters. </p> 1573 1568 … … 1576 1571 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin;mso-no-proof: 1577 1572 yes'><!--[if gte vml 1]><v:shape id="Picture_x0020_10" o:spid="_x0000_i1049" 1578 type="#_x0000_t75" style='width:35 5.5pt;height:366pt;visibility:visible;1573 type="#_x0000_t75" style='width:354.75pt;height:366pt;visibility:visible; 1579 1574 mso-wrap-style:square'> 1580 1575 <v:imagedata src="Magnetic-III_files/image013.png" o:title=""/> 1581 </v:shape><![endif]--><![if !vml]><img border=0 width=47 4height=4881582 src="Magnetic-III_files/image0 16.gif" v:shapes="Picture_x0020_10"><![endif]></span></b></p>1576 </v:shape><![endif]--><![if !vml]><img border=0 width=473 height=488 1577 src="Magnetic-III_files/image062.gif" v:shapes="Picture_x0020_10"><![endif]></span></b></p> 1583 1578 1584 1579 <p class=MsoNormal>Ive expanded & shifted the plot slightly to see that a … … 1593 1588 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1594 1589 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1595 <v:imagedata src="Magnetic-III_files/image03 6.png" o:title="" chromakey="white"/>1590 <v:imagedata src="Magnetic-III_files/image035.png" o:title="" chromakey="white"/> 1596 1591 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1597 src="Magnetic-III_files/image0 04.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m21592 src="Magnetic-III_files/image036.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2 1598 1593 lacks space group extinctions so there is no need to change it as in previous 1599 1594 tutorials) and lattice. Antiferromagnetic ordering may force an increase in the … … 1612 1607 1613 1608 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1614 id="Picture_x0020_11" o:spid="_x0000_i1048" type="#_x0000_t75" style='width:357 .75pt;1609 id="Picture_x0020_11" o:spid="_x0000_i1048" type="#_x0000_t75" style='width:357pt; 1615 1610 height:114pt;visibility:visible;mso-wrap-style:square'> 1616 1611 <v:imagedata src="Magnetic-III_files/image015.png" o:title=""/> 1617 </v:shape><![endif]--><![if !vml]><img border=0 width=47 7height=1521618 src="Magnetic-III_files/image0 18.gif" v:shapes="Picture_x0020_11"><![endif]></span></p>1612 </v:shape><![endif]--><![if !vml]><img border=0 width=476 height=152 1613 src="Magnetic-III_files/image063.gif" v:shapes="Picture_x0020_11"><![endif]></span></p> 1619 1614 1620 1615 <p class=MsoNormal>Notice that the a-axis (11.2974) is now twice the original … … 1622 1617 1623 1618 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1624 id="Picture_x0020_12" o:spid="_x0000_i1047" type="#_x0000_t75" style='width:35 7pt;1625 height:36 7.5pt;visibility:visible;mso-wrap-style:square'>1619 id="Picture_x0020_12" o:spid="_x0000_i1047" type="#_x0000_t75" style='width:356.25pt; 1620 height:366.75pt;visibility:visible;mso-wrap-style:square'> 1626 1621 <v:imagedata src="Magnetic-III_files/image017.png" o:title=""/> 1627 </v:shape><![endif]--><![if !vml]><img border=0 width=47 6 height=4901628 src="Magnetic-III_files/image0 20.gif" v:shapes="Picture_x0020_12"><![endif]></span></p>1622 </v:shape><![endif]--><![if !vml]><img border=0 width=475 height=489 1623 src="Magnetic-III_files/image064.gif" v:shapes="Picture_x0020_12"><![endif]></span></p> 1629 1624 1630 1625 <p class=MsoNormal>Clearly that did not index all the observed peaks, so we … … 1640 1635 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1641 1636 id="Picture_x0020_13" o:spid="_x0000_i1046" type="#_x0000_t75" style='width:5in; 1642 height:3 70.5pt;visibility:visible;mso-wrap-style:square'>1637 height:369.75pt;visibility:visible;mso-wrap-style:square'> 1643 1638 <v:imagedata src="Magnetic-III_files/image019.png" o:title=""/> 1644 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=49 41645 src="Magnetic-III_files/image0 22.gif" v:shapes="Picture_x0020_13"><![endif]></span></p>1639 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=493 1640 src="Magnetic-III_files/image065.gif" v:shapes="Picture_x0020_13"><![endif]></span></p> 1646 1641 1647 1642 <p class=MsoNormal>In this case every powder peak is indexed so a doubling of … … 1673 1668 <v:imagedata src="Magnetic-III_files/image021.png" o:title=""/> 1674 1669 </v:shape><![endif]--><![if !vml]><img border=0 width=222 height=371 1675 src="Magnetic-III_files/image0 24.gif" v:shapes="Picture_x0020_14"><![endif]></span></p>1670 src="Magnetic-III_files/image066.gif" v:shapes="Picture_x0020_14"><![endif]></span></p> 1676 1671 1677 1672 <p class=MsoNormal>These are the controls for running the Bilbao routine. The … … 1686 1681 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1687 1682 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1688 <v:imagedata src="Magnetic-III_files/image03 6.png" o:title="" chromakey="white"/>1683 <v:imagedata src="Magnetic-III_files/image035.png" o:title="" chromakey="white"/> 1689 1684 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1690 src="Magnetic-III_files/image0 04.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2)1685 src="Magnetic-III_files/image036.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2) 1691 1686 is taken from the Space Group entry on the Unit Cells window. Since we just 1692 1687 discovered the propagation vector as (0<span class=GramE>,0,1</span>/2) change <b … … 1714 1709 <v:imagedata src="Magnetic-III_files/image023.png" o:title=""/> 1715 1710 </v:shape><![endif]--><![if !vml]><img border=0 width=477 height=165 1716 src="Magnetic-III_files/image0 26.gif" v:shapes="Picture_x0020_15"><![endif]></span></p>1711 src="Magnetic-III_files/image067.gif" v:shapes="Picture_x0020_15"><![endif]></span></p> 1717 1712 1718 1713 <p class=MsoNormal>Press <b style='mso-bidi-font-weight:normal'><span … … 1735 1730 Project</span></b> from the main menu to access it as <b style='mso-bidi-font-weight: 1736 1731 normal'><span style='font-family:"Calibri",sans-serif;mso-ascii-theme-font: 1737 minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Ba6Co6.gpx</span></b>). 1732 minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Ba6Co6.gpx</span></b>, 1733 then do <span class=GramE><b style='mso-bidi-font-weight:normal'><span 1734 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1735 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Save</span></b></span><b 1736 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1737 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1738 minor-latin'> as</span></b> to save it immediately in your working directory.). 1738 1739 The Unit Cells List window will show the results</p> 1739 1740 … … 1743 1744 <v:imagedata src="Magnetic-III_files/image025.png" o:title=""/> 1744 1745 </v:shape><![endif]--><![if !vml]><img border=0 width=483 height=256 1745 src="Magnetic-III_files/image0 28.gif" v:shapes="Picture_x0020_16"><![endif]></span></p>1746 src="Magnetic-III_files/image068.gif" v:shapes="Picture_x0020_16"><![endif]></span></p> 1746 1747 1747 1748 <p class=MsoNormal>Use the <b style='mso-bidi-font-weight:normal'><span … … 1757 1758 <v:imagedata src="Magnetic-III_files/image027.png" o:title=""/> 1758 1759 </v:shape><![endif]--><![if !vml]><img border=0 width=406 height=439 1759 src="Magnetic-III_files/image0 30.gif" v:shapes="Picture_x0020_17"><![endif]></span></p>1760 src="Magnetic-III_files/image069.gif" v:shapes="Picture_x0020_17"><![endif]></span></p> 1760 1761 1761 1762 <p class=MsoNormal>These are the magnetic symmetry operations for P<sub>c</sub> … … 1785 1786 <v:imagedata src="Magnetic-III_files/image029.png" o:title=""/> 1786 1787 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=246 1787 src="Magnetic-III_files/image0 32.gif" v:shapes="Picture_x0020_18"><![endif]></span></p>1788 src="Magnetic-III_files/image070.gif" v:shapes="Picture_x0020_18"><![endif]></span></p> 1788 1789 1789 1790 <p class=MsoNormal>Do <b style='mso-bidi-font-weight:normal'><span … … 1797 1798 <v:imagedata src="Magnetic-III_files/image031.png" o:title=""/> 1798 1799 </v:shape><![endif]--><![if !vml]><img border=0 width=297 height=297 1799 src="Magnetic-III_files/image0 34.gif" v:shapes="Picture_x0020_19"><![endif]></span></p>1800 src="Magnetic-III_files/image071.gif" v:shapes="Picture_x0020_19"><![endif]></span></p> 1800 1801 1801 1802 <p class=MsoNormal>This shows all magnetic phases that were marked <span … … 1812 1813 <v:imagedata src="Magnetic-III_files/image033.png" o:title=""/> 1813 1814 </v:shape><![endif]--><![if !vml]><img border=0 width=378 height=165 1814 src="Magnetic-III_files/image0 38.gif" v:shapes="Picture_x0020_20"><![endif]></span></p>1815 src="Magnetic-III_files/image072.gif" v:shapes="Picture_x0020_20"><![endif]></span></p> 1815 1816 1816 1817 <p class=MsoNormal>Since the chemical phase had three Co atoms, having three … … 1837 1838 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1838 1839 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1839 <v:imagedata src="Magnetic-III_files/image03 6.png" o:title="" chromakey="white"/>1840 <v:imagedata src="Magnetic-III_files/image035.png" o:title="" chromakey="white"/> 1840 1841 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1841 src="Magnetic-III_files/image0 04.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m21842 src="Magnetic-III_files/image036.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2 1842 1843 magnetic phase just created.</p> 1843 1844 1844 1845 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1845 id="Picture_x0020_21" o:spid="_x0000_i1038" type="#_x0000_t75" style='width:468 pt;1846 id="Picture_x0020_21" o:spid="_x0000_i1038" type="#_x0000_t75" style='width:468.75pt; 1846 1847 height:247.5pt;visibility:visible;mso-wrap-style:square'> 1847 1848 <v:imagedata src="Magnetic-III_files/image037.png" o:title=""/> 1848 </v:shape><![endif]--><![if !vml]><img border=0 width=62 4height=3301849 src="Magnetic-III_files/image0 40.gif" v:shapes="Picture_x0020_21"><![endif]></span></p>1849 </v:shape><![endif]--><![if !vml]><img border=0 width=625 height=330 1850 src="Magnetic-III_files/image073.gif" v:shapes="Picture_x0020_21"><![endif]></span></p> 1850 1851 1851 1852 <p class=MsoNormal>Select Atoms, enter <b style='mso-bidi-font-weight:normal'><span … … 1866 1867 <v:imagedata src="Magnetic-III_files/image039.png" o:title=""/> 1867 1868 </v:shape><![endif]--><![if !vml]><img border=0 width=454 height=864 1868 src="Magnetic-III_files/image0 42.gif" v:shapes="Picture_x0020_22"><![endif]></span></p>1869 src="Magnetic-III_files/image074.gif" v:shapes="Picture_x0020_22"><![endif]></span></p> 1869 1870 1870 1871 <p class=MsoNormal>Do <b style='mso-bidi-font-weight:normal'><span … … 1878 1879 <v:imagedata src="Magnetic-III_files/image041.png" o:title=""/> 1879 1880 </v:shape><![endif]--><![if !vml]><img border=0 width=485 height=164 1880 src="Magnetic-III_files/image0 44.gif" v:shapes="Picture_x0020_23"><![endif]></span></p>1881 src="Magnetic-III_files/image075.gif" v:shapes="Picture_x0020_23"><![endif]></span></p> 1881 1882 1882 1883 <p class=MsoNormal>This is similar to what happened in the previous tutorial … … 1894 1895 <v:imagedata src="Magnetic-III_files/image043.png" o:title=""/> 1895 1896 </v:shape><![endif]--><![if !vml]><img border=0 width=482 height=359 1896 src="Magnetic-III_files/image0 46.gif" v:shapes="Picture_x0020_24"><![endif]></span></p>1897 src="Magnetic-III_files/image076.gif" v:shapes="Picture_x0020_24"><![endif]></span></p> 1897 1898 1898 1899 <p class=MsoNormal>The actual conflict is the 2<sup>nd</sup> from last one <b … … 1907 1908 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1908 1909 id="Picture_x0020_25" o:spid="_x0000_i1034" type="#_x0000_t75" style='width:359.25pt; 1909 height:267 .75pt;visibility:visible;mso-wrap-style:square'>1910 height:267pt;visibility:visible;mso-wrap-style:square'> 1910 1911 <v:imagedata src="Magnetic-III_files/image045.png" o:title=""/> 1911 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=35 71912 src="Magnetic-III_files/image0 48.gif" v:shapes="Picture_x0020_25"><![endif]></span></p>1912 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=356 1913 src="Magnetic-III_files/image077.gif" v:shapes="Picture_x0020_25"><![endif]></span></p> 1913 1914 1914 1915 <p class=MsoNormal>Now try <b style='mso-bidi-font-weight:normal'><span … … 1958 1959 1959 1960 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1960 id=" Picture_x0020_26" o:spid="_x0000_i1033" type="#_x0000_t75" style='width:356.25pt;1961 height:598.5pt;visibility:visible;mso-wrap-style:square'>1961 id="_x0000_i1033" type="#_x0000_t75" style='width:356.25pt;height:598.5pt; 1962 visibility:visible;mso-wrap-style:square'> 1962 1963 <v:imagedata src="Magnetic-III_files/image047.png" o:title=""/> 1963 1964 </v:shape><![endif]--><![if !vml]><img border=0 width=475 height=798 1964 src="Magnetic-III_files/image0 50.gif" v:shapes="Picture_x0020_26"><![endif]></span></p>1965 src="Magnetic-III_files/image078.gif" v:shapes="_x0000_i1033"><![endif]></span></p> 1965 1966 1966 1967 <p class=MsoNormal>The fit to the powder pattern looks quite good</p> 1967 1968 1968 1969 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1969 id=" Picture_x0020_27" o:spid="_x0000_i1032" type="#_x0000_t75" style='width:5in;1970 height:282.75pt;visibility:visible;mso-wrap-style:square'>1970 id="_x0000_i1032" type="#_x0000_t75" style='width:5in;height:282.75pt; 1971 visibility:visible;mso-wrap-style:square'> 1971 1972 <v:imagedata src="Magnetic-III_files/image049.png" o:title=""/> 1972 1973 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=377 1973 src="Magnetic-III_files/image0 52.gif" v:shapes="Picture_x0020_27"><![endif]></span></p>1974 src="Magnetic-III_files/image079.gif" v:shapes="_x0000_i1032"><![endif]></span></p> 1974 1975 1975 1976 <p class=MsoNormal>But we should try the other solution to see if it is better. … … 1995 1996 1996 1997 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1997 id=" Picture_x0020_28" o:spid="_x0000_i1031" type="#_x0000_t75" style='width:359.25pt;1998 height:184.5pt;visibility:visible;mso-wrap-style:square'>1998 id="_x0000_i1031" type="#_x0000_t75" style='width:359.25pt;height:184.5pt; 1999 visibility:visible;mso-wrap-style:square'> 1999 2000 <v:imagedata src="Magnetic-III_files/image051.png" o:title=""/> 2000 2001 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=246 2001 src="Magnetic-III_files/image0 54.gif" v:shapes="Picture_x0020_28"><![endif]></span></p>2002 src="Magnetic-III_files/image080.gif" v:shapes="_x0000_i1031"><![endif]></span></p> 2002 2003 2003 2004 <p class=MsoNormal>Do <b style='mso-bidi-font-weight:normal'><span … … 2007 2008 2008 2009 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 2009 id=" _x0000_i1030" type="#_x0000_t75" style='width:222.75pt;height:222.75pt;2010 visibility:visible;mso-wrap-style:square'>2010 id="Picture_x0020_26" o:spid="_x0000_i1030" type="#_x0000_t75" style='width:222.75pt; 2011 height:222.75pt;visibility:visible;mso-wrap-style:square'> 2011 2012 <v:imagedata src="Magnetic-III_files/image031.png" o:title=""/> 2012 2013 </v:shape><![endif]--><![if !vml]><img border=0 width=297 height=297 2013 src="Magnetic-III_files/image0 34.gif" v:shapes="_x0000_i1030"><![endif]></span></p>2014 src="Magnetic-III_files/image071.gif" v:shapes="Picture_x0020_26"><![endif]></span></p> 2014 2015 2015 2016 <p class=MsoNormal>We already tried the 1<sup>st</sup> one; now select the 2<sup>nd</sup> … … 2017 2018 2018 2019 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 2019 id=" _x0000_i1029" type="#_x0000_t75" style='width:283.5pt;height:123.75pt;2020 visibility:visible;mso-wrap-style:square'>2020 id="Picture_x0020_27" o:spid="_x0000_i1029" type="#_x0000_t75" style='width:283.5pt; 2021 height:123.75pt;visibility:visible;mso-wrap-style:square'> 2021 2022 <v:imagedata src="Magnetic-III_files/image053.png" o:title=""/> 2022 2023 </v:shape><![endif]--><![if !vml]><img border=0 width=378 height=165 2023 src="Magnetic-III_files/image0 56.gif" v:shapes="_x0000_i1029"><![endif]></span></p>2024 src="Magnetic-III_files/image081.gif" v:shapes="Picture_x0020_27"><![endif]></span></p> 2024 2025 2025 2026 <p class=MsoNormal>It looks very similar to what we had before; close … … 2030 2031 new project <b style='mso-bidi-font-weight:normal'><span style='font-family: 2031 2032 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-hansi-theme-font: 2032 minor-latin;mso-bidi-theme-font:minor-latin'>Ba6Co6 mag_2.gpx</span></b> will 2033 becreated. The General tab for this new phase will be shown</p>2034 2035 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 2036 id=" _x0000_i1028" type="#_x0000_t75" style='width:363.75pt;height:186.75pt;2037 visibility:visible;mso-wrap-style:square'>2033 minor-latin;mso-bidi-theme-font:minor-latin'>Ba6Co6 mag_2.gpx</span></b> will be 2034 created. The General tab for this new phase will be shown</p> 2035 2036 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 2037 id="Picture_x0020_28" o:spid="_x0000_i1028" type="#_x0000_t75" style='width:363.75pt; 2038 height:186.75pt;visibility:visible;mso-wrap-style:square'> 2038 2039 <v:imagedata src="Magnetic-III_files/image055.png" o:title=""/> 2039 2040 </v:shape><![endif]--><![if !vml]><img border=0 width=485 height=249 2040 src="Magnetic-III_files/image0 90.gif" v:shapes="_x0000_i1028"><![endif]></span></p>2041 src="Magnetic-III_files/image082.gif" v:shapes="Picture_x0020_28"><![endif]></span></p> 2041 2042 2042 2043 <p class=MsoNormal>Select the Atoms tab & set <span class=SpellE>Mz</span> … … 2044 2045 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 2045 2046 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>1.0</span></b>. 2046 Then do the refinement steps we outlined for the 1<sup>st</sup> magnetic 2047 structure. Do <b style='mso-bidi-font-weight:normal'><span style='font-family: 2048 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-hansi-theme-font: 2049 minor-latin;mso-bidi-theme-font:minor-latin'>Calculate/Refine</span></b> first 2050 youll again have to correct he constraints by deleting the duplicate one. 2051 Then set the <b style='mso-bidi-font-weight:normal'><span style='font-family: 2052 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-hansi-theme-font: 2053 minor-latin;mso-bidi-theme-font:minor-latin'>M</span></b> refine flags for the 2054 magnetic atoms; do <b style='mso-bidi-font-weight:normal'><span 2047 Then do the refinement steps we outlined for the 1<sup>st</sup> magnetic structure. 2048 Do <b style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 2049 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 2050 minor-latin'>Calculate/Refine</span></b> first youll again have to correct 2051 he constraints by deleting the duplicate one. Then set the <b style='mso-bidi-font-weight: 2052 normal'><span style='font-family:"Calibri",sans-serif;mso-ascii-theme-font: 2053 minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>M</span></b> 2054 refine flags for the magnetic atoms; do <b style='mso-bidi-font-weight:normal'><span 2055 2055 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 2056 2056 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Calculate/Refine</span></b>. … … 2106 2106 <v:imagedata src="Magnetic-III_files/image084.png" o:title=""/> 2107 2107 </v:shape><![endif]--><![if !vml]><img border=0 width=482 height=110 2108 src="Magnetic-III_files/image0 91.gif" v:shapes="Picture_x0020_29"><![endif]></span></p>2108 src="Magnetic-III_files/image083.gif" v:shapes="Picture_x0020_29"><![endif]></span></p> 2109 2109 2110 2110 <p class=MsoNormal><span class=GramE>gives</span> <span class=SpellE>Mz</span>=3.296(35); 2111 2111 the <span class=SpellE>esd</span> is from <b style='mso-bidi-font-weight:normal'><span 2112 2112 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 2113 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Ba6Co6 mag_2.lst</span></b>.2114 The structure is then</p>2113 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Ba6Co6 2114 mag_2.lst</span></b>. The structure is then</p> 2115 2115 2116 2116 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape … … 2119 2119 <v:imagedata src="Magnetic-III_files/image086.png" o:title=""/> 2120 2120 </v:shape><![endif]--><![if !vml]><img border=0 width=237 height=480 2121 src="Magnetic-III_files/image0 92.gif" v:shapes="Picture_x0020_30"><![endif]><!--[if gte vml 1]><v:shape2121 src="Magnetic-III_files/image085.gif" v:shapes="Picture_x0020_30"><![endif]><!--[if gte vml 1]><v:shape 2122 2122 id="Picture_x0020_31" o:spid="_x0000_i1025" type="#_x0000_t75" style='width:187.5pt; 2123 2123 height:358.5pt;visibility:visible;mso-wrap-style:square'> 2124 2124 <v:imagedata src="Magnetic-III_files/image088.png" o:title=""/> 2125 2125 </v:shape><![endif]--><![if !vml]><img border=0 width=250 height=478 2126 src="Magnetic-III_files/image0 93.gif" v:shapes="Picture_x0020_31"><![endif]></span></p>2126 src="Magnetic-III_files/image087.gif" v:shapes="Picture_x0020_31"><![endif]></span></p> 2127 2127 2128 2128 <p class=MsoNormal>Ive placed the doubled c-axis chemical structure so you can 2129 2129 see the relationship between them.</p> 2130 2130 2131 <p class=MsoNormal>If I impose a similar constraint for the 1<sup>st</sup> 2132 model, the final <span class=SpellE>wR</span>=7.524% is slightly higher than for 2133 the 2<sup>nd</sup> model. This concludes this tutorial; you probably want to <span 2134 class=GramE><b style='mso-bidi-font-weight:normal'><span style='font-family: 2135 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-hansi-theme-font: 2136 minor-latin;mso-bidi-theme-font:minor-latin'>Save</span></b></span> both 2137 projects before closing GSAS-II.</p> 2131 <p class=MsoNormal>If I impose a similar constraint for the 1<sup>st</sup> model, 2132 the final <span class=SpellE>wR</span>=7.524% is slightly higher than for the 2<sup>nd</sup> 2133 model. This concludes this tutorial; you probably want to <span class=GramE><b 2134 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 2135 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 2136 minor-latin'>Save</span></b></span> both projects before closing GSAS-II.</p> 2138 2137 2139 2138 </div> -
Tutorials/Magnetic-III/Magnetic-III_files/filelist.xml
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