Changeset 3642
- Timestamp:
- Oct 3, 2018 2:23:00 PM (5 years ago)
- Location:
- Tutorials/Magnetic-III
- Files:
-
- 33 added
- 3 edited
Legend:
- Unmodified
- Added
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Tutorials/Magnetic-III/Magnetic-III.htm
r3635 r3642 23 23 <o:Author>Von Dreele</o:Author> 24 24 <o:LastAuthor>vondreele</o:LastAuthor> 25 <o:Revision> 17</o:Revision>26 <o:TotalTime>5 62</o:TotalTime>25 <o:Revision>20</o:Revision> 26 <o:TotalTime>589</o:TotalTime> 27 27 <o:Created>2012-05-05T14:50:00Z</o:Created> 28 <o:LastSaved>2018-10-0 1T13:53:00Z</o:LastSaved>29 <o:Pages>1 9</o:Pages>30 <o:Words>21 64</o:Words>31 <o:Characters>12 339</o:Characters>32 <o:Lines>10 2</o:Lines>33 <o:Paragraphs>2 8</o:Paragraphs>34 <o:CharactersWithSpaces>14 475</o:CharactersWithSpaces>28 <o:LastSaved>2018-10-03T19:22:00Z</o:LastSaved> 29 <o:Pages>1</o:Pages> 30 <o:Words>2187</o:Words> 31 <o:Characters>12468</o:Characters> 32 <o:Lines>103</o:Lines> 33 <o:Paragraphs>29</o:Paragraphs> 34 <o:CharactersWithSpaces>14626</o:CharactersWithSpaces> 35 35 <o:Version>16.00</o:Version> 36 36 </o:DocumentProperties> … … 40 40 <!--[if gte mso 9]><xml> 41 41 <w:WordDocument> 42 <w:View>Print</w:View> 43 <w:Zoom>95</w:Zoom> 42 <w:Zoom>108</w:Zoom> 44 43 <w:SpellingState>Clean</w:SpellingState> 45 44 <w:GrammarState>Clean</w:GrammarState> … … 1283 1282 <h2>Introduction</h2> 1284 1283 1285 <p class=MsoNormal>In this and subsequent tutorials, we will show how GSAS-II1286 makes use of the Bilbao crystallographic server (<a 1287 href="http://www.cryst.ehu.es/">www.cryst.ehu.es/</a>) <i style='mso-bidi-font-style: 1288 normal'>Magnetic Symmetry and Applications</i> routine k-SUBGROUPSMAG (<a 1289 href="http://iopscience.iop.org/0953-8984/28/28/286001"><span style='font-size: 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 i s called in case you lack internet access).</p>1284 <p class=MsoNormal>In this tutorials, we continue showing how GSAS-II makes use 1285 of the Bilbao crystallographic server (<a href="http://www.cryst.ehu.es/">www.cryst.ehu.es/</a>) 1286 <i style='mso-bidi-font-style:normal'>Magnetic Symmetry and Applications</i> routine 1287 k-SUBGROUPSMAG (<a href="http://iopscience.iop.org/0953-8984/28/28/286001"><span 1288 style='font-size:10.0pt;font-family:"Arial",sans-serif'>Perez-Mato, JM; <span 1289 class=SpellE>Gallego</span>, SV; <span class=SpellE>Elcoro</span>, L; <span 1290 class=SpellE>Tasci</span>, E and <span class=SpellE>Aroyo</span>, MI, <i>J. of 1291 Phys.: <span class=SpellE>Condens</span> Matter</i> (2016), <b>28</b>:28601</span></a>) 1292 while determining a magnetic crystal structure with a non-zero propagation 1293 vector. If you have not done so already, you may wish to do the Simple Magnetic 1294 Structures tutorial first as it contains some background information that will 1295 not be covered here. It is also helpful to do parts I and II of the series of 1296 Magnetic Structures tutorials. To make this work, your computer must have an 1297 internet connection for GSAS-II to access this site. (We will supply the 1298 project file that results after k-SUBGROUPSMAG is called in case you lack 1299 internet access).</p> 1301 1300 1302 1301 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shapetype … … 1327 1326 1328 1327 <p class=MsoNormal>In this example, we will determine the magnetic structure 1329 for Ba<sub>6</sub>Co<sub>6</sub>ClO<sub>1 6</sub> from neutron data taken on the1330 D1b diffractometer (ILL, Grenoble, France) at 1.4K and λ=2.394 Å and is 1331 based on Example 12.2 in the Jana2006 Cookbook (<span class=SpellE>Duek</span>,1328 for Ba<sub>6</sub>Co<sub>6</sub>ClO<sub>15.5</sub> from neutron data taken on 1329 the D1b diffractometer (ILL, Grenoble, France) at 1.4K and λ=2.394 Å and 1330 is based on Example 12.2 in the Jana2006 Cookbook (<span class=SpellE>Duek</span>, 1332 1331 et al., 2017).<span style='mso-spacerun:yes'> </span>Its magnetic structure 1333 1332 was originally determined by <span class=SpellE>Mentré</span>, et al. (<span … … 1345 1344 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1346 1345 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1347 <v:imagedata src="Magnetic-III_files/image0 35.png" o:title="" chromakey="white"/>1346 <v:imagedata src="Magnetic-III_files/image006.png" o:title="" chromakey="white"/> 1348 1347 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1349 src="Magnetic-III_files/image0 36.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m21348 src="Magnetic-III_files/image008.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2 1350 1349 with a= 5.64870 Å and c= 5.64870 Å. From the structure drawing above, you can 1351 1350 see a tetrameric string of face sharing CoO<sub>6</sub> <span class=SpellE>octahedra</span> … … 1432 1431 <v:imagedata src="Magnetic-III_files/image003.png" o:title=""/> 1433 1432 </v:shape><![endif]--><![if !vml]><img border=0 width=432 height=266 1434 src="Magnetic-III_files/image0 57.gif" v:shapes="Picture_x0020_5"><![endif]></span></p>1433 src="Magnetic-III_files/image021.gif" v:shapes="Picture_x0020_5"><![endif]></span></p> 1435 1434 1436 1435 <p class=MsoNormal style='margin-left:.5in'><span class=GramE>and</span> the … … 1442 1441 <v:imagedata src="Magnetic-III_files/image005.png" o:title=""/> 1443 1442 </v:shape><![endif]--><![if !vml]><img border=0 width=433 height=447 1444 src="Magnetic-III_files/image0 58.gif" v:shapes="Picture_x0020_6"><![endif]></span></p>1443 src="Magnetic-III_files/image025.gif" v:shapes="Picture_x0020_6"><![endif]></span></p> 1445 1444 1446 1445 <p class=MsoNormal style='margin-left:.5in'>We will use the default limits.</p> … … 1454 1453 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1455 1454 minor-latin'>Import/Phase/from CIF file</span></b> menu item to read the phase 1456 information for Ba<sub>6</sub>Co<sub>6</sub>ClO<sub>1 6</sub> into the current1455 information for Ba<sub>6</sub>Co<sub>6</sub>ClO<sub>15.5</sub> into the current 1457 1456 GSAS-II project. The file you want is <b style='mso-bidi-font-weight:normal'><span 1458 1457 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; … … 1502 1501 <v:imagedata src="Magnetic-III_files/image007.png" o:title=""/> 1503 1502 </v:shape><![endif]--><![if !vml]><img border=0 width=430 height=235 1504 src="Magnetic-III_files/image05 9.gif" v:shapes="Picture_x0020_7"><![endif]></span></p>1503 src="Magnetic-III_files/image057.gif" v:shapes="Picture_x0020_7"><![endif]></span></p> 1505 1504 1506 1505 <h3>Step 3. Check powder pattern indexing</h3> … … 1508 1507 <p class=MsoNormal>Here the objective is to determine how the reflection 1509 1508 positions generated from the chemical (nuclear) crystal structure lattice 1510 match up with the peaks observed for this antiferromagnet. </p> 1511 1512 <p class=MsoNormal>Select <b style='mso-bidi-font-weight:normal'><span 1513 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1514 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Unit Cells 1515 List</span></b> from the tree entries under the histogram (begins with PWDR); 1516 the Indexing controls will be shown<br> 1509 match up with the peaks observed for this antiferromagnet. Select <b 1510 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1511 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1512 minor-latin'>Unit Cells List</span></b> from the tree entries under the 1513 histogram (begins with PWDR); the Indexing controls will be shown<br> 1517 1514 <span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape id="Picture_x0020_8" 1518 1515 o:spid="_x0000_i1051" type="#_x0000_t75" style='width:359.25pt;height:121.5pt; … … 1520 1517 <v:imagedata src="Magnetic-III_files/image009.png" o:title=""/> 1521 1518 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=162 1522 src="Magnetic-III_files/image0 60.gif" v:shapes="Picture_x0020_8"><![endif]></span></p>1519 src="Magnetic-III_files/image058.gif" v:shapes="Picture_x0020_8"><![endif]></span></p> 1523 1520 1524 1521 <p class=MsoNormal>This can use lattice parameters & space groups to … … 1547 1544 <v:imagedata src="Magnetic-III_files/image011.png" o:title=""/> 1548 1545 </v:shape><![endif]--><![if !vml]><img border=0 width=477 height=152 1549 src="Magnetic-III_files/image0 61.gif" v:shapes="Picture_x0020_9"><![endif]></span></p>1546 src="Magnetic-III_files/image059.gif" v:shapes="Picture_x0020_9"><![endif]></span></p> 1550 1547 1551 1548 <p class=MsoNormal><span class=GramE>showing</span> the lattice constants for 1552 Ba<sub>6</sub>Co<sub>6</sub>ClO<sub>1 6</sub> you had obtained from the <span1549 Ba<sub>6</sub>Co<sub>6</sub>ClO<sub>15.5</sub> you had obtained from the <span 1553 1550 class=SpellE>cif</span> file and the powder pattern will change showing the 1554 1551 lines for P <!--[if gte msEquation 12]><m:oMath><m:acc><m:accPr><m:chr m:val="̅"/><span … … 1562 1559 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1563 1560 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1564 <v:imagedata src="Magnetic-III_files/image0 35.png" o:title="" chromakey="white"/>1561 <v:imagedata src="Magnetic-III_files/image006.png" o:title="" chromakey="white"/> 1565 1562 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1566 src="Magnetic-III_files/image0 36.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m21563 src="Magnetic-III_files/image008.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2 1567 1564 and those lattice parameters. </p> 1568 1565 … … 1575 1572 <v:imagedata src="Magnetic-III_files/image013.png" o:title=""/> 1576 1573 </v:shape><![endif]--><![if !vml]><img border=0 width=473 height=488 1577 src="Magnetic-III_files/image06 2.gif" v:shapes="Picture_x0020_10"><![endif]></span></b></p>1574 src="Magnetic-III_files/image060.gif" v:shapes="Picture_x0020_10"><![endif]></span></b></p> 1578 1575 1579 1576 <p class=MsoNormal>Ive expanded & shifted the plot slightly to see that a … … 1588 1585 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1589 1586 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1590 <v:imagedata src="Magnetic-III_files/image0 35.png" o:title="" chromakey="white"/>1587 <v:imagedata src="Magnetic-III_files/image006.png" o:title="" chromakey="white"/> 1591 1588 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1592 src="Magnetic-III_files/image0 36.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m21589 src="Magnetic-III_files/image008.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2 1593 1590 lacks space group extinctions so there is no need to change it as in previous 1594 1591 tutorials) and lattice. Antiferromagnetic ordering may force an increase in the … … 1599 1596 described by a propagation vector (<span class=SpellE>kx<span class=GramE>,ky,kz</span></span>) 1600 1597 consisting of fractions (1/2, 1/3, etc.). To explore this possibility here, we 1601 need to try doubling either <span class=GramE>a or</span> c axis and see the 1602 effect on the powder pattern indexing. To try a-axis doubling add <b 1603 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1604 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1605 minor-latin'>*2</span></b> to the end of the a-axis value; it will quickly 1606 change to</p> 1598 need to try doubling either a- or c-axis and see the effect on the powder 1599 pattern indexing. To try a-axis doubling add <b style='mso-bidi-font-weight: 1600 normal'><span style='font-family:"Calibri",sans-serif;mso-ascii-theme-font: 1601 minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>*2</span></b> 1602 to the end of the a-axis value; it will quickly change to</p> 1607 1603 1608 1604 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape … … 1611 1607 <v:imagedata src="Magnetic-III_files/image015.png" o:title=""/> 1612 1608 </v:shape><![endif]--><![if !vml]><img border=0 width=476 height=152 1613 src="Magnetic-III_files/image06 3.gif" v:shapes="Picture_x0020_11"><![endif]></span></p>1609 src="Magnetic-III_files/image061.gif" v:shapes="Picture_x0020_11"><![endif]></span></p> 1614 1610 1615 1611 <p class=MsoNormal>Notice that the a-axis (11.2974) is now twice the original … … 1621 1617 <v:imagedata src="Magnetic-III_files/image017.png" o:title=""/> 1622 1618 </v:shape><![endif]--><![if !vml]><img border=0 width=475 height=489 1623 src="Magnetic-III_files/image06 4.gif" v:shapes="Picture_x0020_12"><![endif]></span></p>1619 src="Magnetic-III_files/image062.gif" v:shapes="Picture_x0020_12"><![endif]></span></p> 1624 1620 1625 1621 <p class=MsoNormal>Clearly that did not index all the observed peaks, so we … … 1638 1634 <v:imagedata src="Magnetic-III_files/image019.png" o:title=""/> 1639 1635 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=493 1640 src="Magnetic-III_files/image06 5.gif" v:shapes="Picture_x0020_13"><![endif]></span></p>1636 src="Magnetic-III_files/image063.gif" v:shapes="Picture_x0020_13"><![endif]></span></p> 1641 1637 1642 1638 <p class=MsoNormal>In this case every powder peak is indexed so a doubling of … … 1649 1645 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1650 1646 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Load cell</span></b> 1651 operation, because the next step requires the chemical cell and space group to 1652 be entered here (<b style='mso-bidi-font-weight:normal'><span style='font-family: 1653 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-hansi-theme-font: 1654 minor-latin;mso-bidi-theme-font:minor-latin'>VERY IMPORTANT!</span></b>)</p> 1647 operation, because the next step requires the correct chemical cell and space 1648 group to be entered here (<b style='mso-bidi-font-weight:normal'><span 1649 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1650 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>VERY 1651 IMPORTANT!</span></b>)</p> 1655 1652 1656 1653 <h3>Step 4. Run k-SUBGROUPSMAG</h3> … … 1664 1661 1665 1662 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1666 id="Picture_x0020_ 14" o:spid="_x0000_i1045" type="#_x0000_t75" style='width:166.5pt;1667 height:2 78.25pt;visibility:visible;mso-wrap-style:square'>1668 <v:imagedata src="Magnetic-III_files/image02 1.png" o:title=""/>1669 </v:shape><![endif]--><![if !vml]><img border=0 width=2 22 height=3711670 src="Magnetic-III_files/image06 6.gif" v:shapes="Picture_x0020_14"><![endif]></span></p>1663 id="Picture_x0020_32" o:spid="_x0000_i1045" type="#_x0000_t75" style='width:182.25pt; 1664 height:299.25pt;visibility:visible;mso-wrap-style:square'> 1665 <v:imagedata src="Magnetic-III_files/image028.png" o:title=""/> 1666 </v:shape><![endif]--><![if !vml]><img border=0 width=243 height=399 1667 src="Magnetic-III_files/image064.gif" v:shapes="Picture_x0020_32"><![endif]></span></p> 1671 1668 1672 1669 <p class=MsoNormal>These are the controls for running the Bilbao routine. The … … 1681 1678 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1682 1679 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1683 <v:imagedata src="Magnetic-III_files/image0 35.png" o:title="" chromakey="white"/>1680 <v:imagedata src="Magnetic-III_files/image006.png" o:title="" chromakey="white"/> 1684 1681 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1685 src="Magnetic-III_files/image0 36.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2)1682 src="Magnetic-III_files/image008.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2) 1686 1683 is taken from the Space Group entry on the Unit Cells window. Since we just 1687 discovered the propagation vector as (0<span class=GramE>,0,1</span>/2) change <b1684 discovered the propagation vector is (0<span class=GramE>,0,1</span>/2) change <b 1688 1685 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1689 1686 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: … … 1709 1706 <v:imagedata src="Magnetic-III_files/image023.png" o:title=""/> 1710 1707 </v:shape><![endif]--><![if !vml]><img border=0 width=477 height=165 1711 src="Magnetic-III_files/image06 7.gif" v:shapes="Picture_x0020_15"><![endif]></span></p>1708 src="Magnetic-III_files/image065.gif" v:shapes="Picture_x0020_15"><![endif]></span></p> 1712 1709 1713 1710 <p class=MsoNormal>Press <b style='mso-bidi-font-weight:normal'><span … … 1740 1737 1741 1738 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1742 id="Picture_x0020_16" o:spid="_x0000_i1043" type="#_x0000_t75" style='width:362.25pt; 1743 height:192pt;visibility:visible;mso-wrap-style:square'> 1744 <v:imagedata src="Magnetic-III_files/image025.png" o:title=""/> 1745 </v:shape><![endif]--><![if !vml]><img border=0 width=483 height=256 1746 src="Magnetic-III_files/image068.gif" v:shapes="Picture_x0020_16"><![endif]></span></p> 1747 1748 <p class=MsoNormal>Use the <b style='mso-bidi-font-weight:normal'><span 1749 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1750 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Try</span></b> 1751 on the first two entries; they both index every reflection. The two seem 1752 identical except for the translation vector. Double click the row number for 1753 the 1<sup>st</sup> one; a popup will appear</p> 1739 id="Picture_x0020_33" o:spid="_x0000_i1043" type="#_x0000_t75" style='width:360.75pt; 1740 height:293.25pt;visibility:visible;mso-wrap-style:square'> 1741 <v:imagedata src="Magnetic-III_files/image066.png" o:title=""/> 1742 </v:shape><![endif]--><![if !vml]><img border=0 width=481 height=391 1743 src="Magnetic-III_files/image067.gif" v:shapes="Picture_x0020_33"><![endif]></span></p> 1744 1745 <p class=MsoNormal>Notice that the number of unique magnetic atoms is either 3 1746 or 6; this should be no surprise since the chemical structure has 3 unique Co 1747 atoms. Use the <b style='mso-bidi-font-weight:normal'><span style='font-family: 1748 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-hansi-theme-font: 1749 minor-latin;mso-bidi-theme-font:minor-latin'>Try</span></b> on the first two 1750 entries; they both index every reflection. The two seem identical except for 1751 the translation vector. Double click the row number for the 1<sup>st</sup> one; 1752 a popup will appear</p> 1754 1753 1755 1754 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1756 1755 id="Picture_x0020_17" o:spid="_x0000_i1042" type="#_x0000_t75" style='width:304.5pt; 1757 height:3 29.25pt;visibility:visible;mso-wrap-style:square'>1756 height:330pt;visibility:visible;mso-wrap-style:square'> 1758 1757 <v:imagedata src="Magnetic-III_files/image027.png" o:title=""/> 1759 </v:shape><![endif]--><![if !vml]><img border=0 width=406 height=4 391760 src="Magnetic-III_files/image06 9.gif" v:shapes="Picture_x0020_17"><![endif]></span></p>1758 </v:shape><![endif]--><![if !vml]><img border=0 width=406 height=440 1759 src="Magnetic-III_files/image068.gif" v:shapes="Picture_x0020_17"><![endif]></span></p> 1761 1760 1762 1761 <p class=MsoNormal>These are the magnetic symmetry operations for P<sub>c</sub> … … 1768 1767 in red to indicate the spin inversion is applied for all of them. The Print Ops 1769 1768 button makes a full list on the console; these can be cut & pasted into 1770 other programs is needed. Press <b style='mso-bidi-font-weight:normal'><span1769 other programs as needed. Press <b style='mso-bidi-font-weight:normal'><span 1771 1770 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1772 1771 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>OK</span></b>. … … 1786 1785 <v:imagedata src="Magnetic-III_files/image029.png" o:title=""/> 1787 1786 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=246 1788 src="Magnetic-III_files/image0 70.gif" v:shapes="Picture_x0020_18"><![endif]></span></p>1787 src="Magnetic-III_files/image069.gif" v:shapes="Picture_x0020_18"><![endif]></span></p> 1789 1788 1790 1789 <p class=MsoNormal>Do <b style='mso-bidi-font-weight:normal'><span … … 1798 1797 <v:imagedata src="Magnetic-III_files/image031.png" o:title=""/> 1799 1798 </v:shape><![endif]--><![if !vml]><img border=0 width=297 height=297 1800 src="Magnetic-III_files/image07 1.gif" v:shapes="Picture_x0020_19"><![endif]></span></p>1801 1802 <p class=MsoNormal>This shows all magnetic phases that were marked <span1803 class=GramE>Keep</span> in the Unit Cells List; for each you see the 1804 transformation and vector (the first two results will have the same space group 1805 but are different translations). Select the 1<sup>st</sup> one and press <b 1806 style=' mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif;1807 mso- ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:1808 minor-latin'>OK</span></b>;a new popup dialog will appear.</p>1809 1810 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1811 id=" Picture_x0020_20" o:spid="_x0000_i1039" type="#_x0000_t75" style='width:283.5pt;1812 height:123.75pt;visibility:visible;mso-wrap-style:square'>1799 src="Magnetic-III_files/image070.gif" v:shapes="Picture_x0020_19"><![endif]></span></p> 1800 1801 <p class=MsoNormal>This shows all magnetic phases that were marked Keep in the 1802 Unit Cells List; for each you see the transformation and vector (the first two 1803 results will have the same space group but different translations). Select the 1804 1<sup>st</sup> one and press <b style='mso-bidi-font-weight:normal'><span 1805 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1806 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>OK</span></b>; 1807 a new popup dialog will appear.</p> 1808 1809 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1810 id="_x0000_i1039" type="#_x0000_t75" style='width:283.5pt;height:123.75pt; 1811 visibility:visible;mso-wrap-style:square'> 1813 1812 <v:imagedata src="Magnetic-III_files/image033.png" o:title=""/> 1814 1813 </v:shape><![endif]--><![if !vml]><img border=0 width=378 height=165 1815 src="Magnetic-III_files/image07 2.gif" v:shapes="Picture_x0020_20"><![endif]></span></p>1814 src="Magnetic-III_files/image071.gif" v:shapes="_x0000_i1039"><![endif]></span></p> 1816 1815 1817 1816 <p class=MsoNormal>Since the chemical phase had three Co atoms, having three … … 1824 1823 number from the space group list (<b style='mso-bidi-font-weight:normal'><span 1825 1824 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1826 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Ba6Co6 mag_1.gpx</span></b>);1827 press <b style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1828 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1829 m inor-latin'>Save.</span></b> The new project will be opened to the General tab1830 for the P<sub>c</sub> <!--[if gte msEquation 12]><m:oMath><m:acc><m:accPr><m:chr1825 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Ba6Co6 1826 mag_1.gpx</span></b>); press <b style='mso-bidi-font-weight:normal'><span 1827 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1828 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Save.</span></b> 1829 The new project will be opened to the General tab for the P<sub>c</sub> <!--[if gte msEquation 12]><m:oMath><m:acc><m:accPr><m:chr 1831 1830 m:val="̅"/><span style='font-family:"Cambria Math",serif;mso-ascii-font-family: 1832 1831 "Cambria Math";mso-hansi-font-family:"Cambria Math";font-style:italic; … … 1838 1837 EN-US;mso-bidi-language:AR-SA'><!--[if gte vml 1]><v:shape id="_x0000_i1025" 1839 1838 type="#_x0000_t75" style='width:6.75pt;height:14.25pt'> 1840 <v:imagedata src="Magnetic-III_files/image0 35.png" o:title="" chromakey="white"/>1839 <v:imagedata src="Magnetic-III_files/image006.png" o:title="" chromakey="white"/> 1841 1840 </v:shape><![endif]--><![if !vml]><img width=9 height=19 1842 src="Magnetic-III_files/image0 36.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m21841 src="Magnetic-III_files/image008.gif" v:shapes="_x0000_i1025"><![endif]></span><![endif]>m2 1843 1842 magnetic phase just created.</p> 1844 1843 1845 1844 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1846 id=" Picture_x0020_21" o:spid="_x0000_i1038" type="#_x0000_t75" style='width:468.75pt;1847 height:247.5pt;visibility:visible;mso-wrap-style:square'>1845 id="_x0000_i1038" type="#_x0000_t75" style='width:468.75pt;height:247.5pt; 1846 visibility:visible;mso-wrap-style:square'> 1848 1847 <v:imagedata src="Magnetic-III_files/image037.png" o:title=""/> 1849 1848 </v:shape><![endif]--><![if !vml]><img border=0 width=625 height=330 1850 src="Magnetic-III_files/image07 3.gif" v:shapes="Picture_x0020_21"><![endif]></span></p>1849 src="Magnetic-III_files/image072.gif" v:shapes="_x0000_i1038"><![endif]></span></p> 1851 1850 1852 1851 <p class=MsoNormal>Select Atoms, enter <b style='mso-bidi-font-weight:normal'><span … … 1863 1862 1864 1863 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1865 id=" Picture_x0020_22" o:spid="_x0000_i1037" type="#_x0000_t75" style='width:340.5pt;1866 height:9in;visibility:visible;mso-wrap-style:square'>1864 id="_x0000_i1037" type="#_x0000_t75" style='width:340.5pt;height:9in; 1865 visibility:visible;mso-wrap-style:square'> 1867 1866 <v:imagedata src="Magnetic-III_files/image039.png" o:title=""/> 1868 1867 </v:shape><![endif]--><![if !vml]><img border=0 width=454 height=864 1869 src="Magnetic-III_files/image07 4.gif" v:shapes="Picture_x0020_22"><![endif]></span></p>1868 src="Magnetic-III_files/image073.gif" v:shapes="_x0000_i1037"><![endif]></span></p> 1870 1869 1871 1870 <p class=MsoNormal>Do <b style='mso-bidi-font-weight:normal'><span … … 1875 1874 1876 1875 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1877 id="Picture_x0020_2 3" o:spid="_x0000_i1036" type="#_x0000_t75" style='width:363.75pt;1876 id="Picture_x0020_20" o:spid="_x0000_i1036" type="#_x0000_t75" style='width:363.75pt; 1878 1877 height:123pt;visibility:visible;mso-wrap-style:square'> 1879 1878 <v:imagedata src="Magnetic-III_files/image041.png" o:title=""/> 1880 1879 </v:shape><![endif]--><![if !vml]><img border=0 width=485 height=164 1881 src="Magnetic-III_files/image07 5.gif" v:shapes="Picture_x0020_23"><![endif]></span></p>1880 src="Magnetic-III_files/image074.gif" v:shapes="Picture_x0020_20"><![endif]></span></p> 1882 1881 1883 1882 <p class=MsoNormal>This is similar to what happened in the previous tutorial … … 1891 1890 1892 1891 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1893 id="Picture_x0020_2 4" o:spid="_x0000_i1035" type="#_x0000_t75" style='width:361.5pt;1892 id="Picture_x0020_21" o:spid="_x0000_i1035" type="#_x0000_t75" style='width:361.5pt; 1894 1893 height:269.25pt;visibility:visible;mso-wrap-style:square'> 1895 1894 <v:imagedata src="Magnetic-III_files/image043.png" o:title=""/> 1896 1895 </v:shape><![endif]--><![if !vml]><img border=0 width=482 height=359 1897 src="Magnetic-III_files/image07 6.gif" v:shapes="Picture_x0020_24"><![endif]></span></p>1896 src="Magnetic-III_files/image075.gif" v:shapes="Picture_x0020_21"><![endif]></span></p> 1898 1897 1899 1898 <p class=MsoNormal>The actual conflict is the 2<sup>nd</sup> from last one <b … … 1907 1906 1908 1907 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1909 id="Picture_x0020_2 5" o:spid="_x0000_i1034" type="#_x0000_t75" style='width:359.25pt;1908 id="Picture_x0020_22" o:spid="_x0000_i1034" type="#_x0000_t75" style='width:359.25pt; 1910 1909 height:267pt;visibility:visible;mso-wrap-style:square'> 1911 1910 <v:imagedata src="Magnetic-III_files/image045.png" o:title=""/> 1912 1911 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=356 1913 src="Magnetic-III_files/image07 7.gif" v:shapes="Picture_x0020_25"><![endif]></span></p>1912 src="Magnetic-III_files/image076.gif" v:shapes="Picture_x0020_22"><![endif]></span></p> 1914 1913 1915 1914 <p class=MsoNormal>Now try <b style='mso-bidi-font-weight:normal'><span … … 1959 1958 1960 1959 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1961 id=" _x0000_i1033" type="#_x0000_t75" style='width:356.25pt;height:598.5pt;1962 visibility:visible;mso-wrap-style:square'>1960 id="Picture_x0020_23" o:spid="_x0000_i1033" type="#_x0000_t75" style='width:356.25pt; 1961 height:599.25pt;visibility:visible;mso-wrap-style:square'> 1963 1962 <v:imagedata src="Magnetic-III_files/image047.png" o:title=""/> 1964 </v:shape><![endif]--><![if !vml]><img border=0 width=475 height=79 81965 src="Magnetic-III_files/image07 8.gif" v:shapes="_x0000_i1033"><![endif]></span></p>1963 </v:shape><![endif]--><![if !vml]><img border=0 width=475 height=799 1964 src="Magnetic-III_files/image077.gif" v:shapes="Picture_x0020_23"><![endif]></span></p> 1966 1965 1967 1966 <p class=MsoNormal>The fit to the powder pattern looks quite good</p> 1968 1967 1969 1968 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1970 id=" _x0000_i1032" type="#_x0000_t75" style='width:5in;height:282.75pt;1971 visibility:visible;mso-wrap-style:square'>1969 id="Picture_x0020_24" o:spid="_x0000_i1032" type="#_x0000_t75" style='width:5in; 1970 height:282.75pt;visibility:visible;mso-wrap-style:square'> 1972 1971 <v:imagedata src="Magnetic-III_files/image049.png" o:title=""/> 1973 1972 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=377 1974 src="Magnetic-III_files/image07 9.gif" v:shapes="_x0000_i1032"><![endif]></span></p>1973 src="Magnetic-III_files/image078.gif" v:shapes="Picture_x0020_24"><![endif]></span></p> 1975 1974 1976 1975 <p class=MsoNormal>But we should try the other solution to see if it is better. … … 1996 1995 1997 1996 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1998 id=" _x0000_i1031" type="#_x0000_t75" style='width:359.25pt;height:184.5pt;1999 visibility:visible;mso-wrap-style:square'>1997 id="Picture_x0020_25" o:spid="_x0000_i1031" type="#_x0000_t75" style='width:359.25pt; 1998 height:185.25pt;visibility:visible;mso-wrap-style:square'> 2000 1999 <v:imagedata src="Magnetic-III_files/image051.png" o:title=""/> 2001 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=24 62002 src="Magnetic-III_files/image0 80.gif" v:shapes="_x0000_i1031"><![endif]></span></p>2000 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=247 2001 src="Magnetic-III_files/image079.gif" v:shapes="Picture_x0020_25"><![endif]></span></p> 2003 2002 2004 2003 <p class=MsoNormal>Do <b style='mso-bidi-font-weight:normal'><span … … 2012 2011 <v:imagedata src="Magnetic-III_files/image031.png" o:title=""/> 2013 2012 </v:shape><![endif]--><![if !vml]><img border=0 width=297 height=297 2014 src="Magnetic-III_files/image07 1.gif" v:shapes="Picture_x0020_26"><![endif]></span></p>2013 src="Magnetic-III_files/image070.gif" v:shapes="Picture_x0020_26"><![endif]></span></p> 2015 2014 2016 2015 <p class=MsoNormal>We already tried the 1<sup>st</sup> one; now select the 2<sup>nd</sup> … … 2022 2021 <v:imagedata src="Magnetic-III_files/image053.png" o:title=""/> 2023 2022 </v:shape><![endif]--><![if !vml]><img border=0 width=378 height=165 2024 src="Magnetic-III_files/image08 1.gif" v:shapes="Picture_x0020_27"><![endif]></span></p>2023 src="Magnetic-III_files/image080.gif" v:shapes="Picture_x0020_27"><![endif]></span></p> 2025 2024 2026 2025 <p class=MsoNormal>It looks very similar to what we had before; close … … 2035 2034 2036 2035 <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;2036 id="Picture_x0020_28" o:spid="_x0000_i1028" type="#_x0000_t75" style='width:363pt; 2038 2037 height:186.75pt;visibility:visible;mso-wrap-style:square'> 2039 2038 <v:imagedata src="Magnetic-III_files/image055.png" o:title=""/> 2040 </v:shape><![endif]--><![if !vml]><img border=0 width=48 5height=2492041 src="Magnetic-III_files/image08 2.gif" v:shapes="Picture_x0020_28"><![endif]></span></p>2039 </v:shape><![endif]--><![if !vml]><img border=0 width=484 height=249 2040 src="Magnetic-III_files/image081.gif" v:shapes="Picture_x0020_28"><![endif]></span></p> 2042 2041 2043 2042 <p class=MsoNormal>Select the Atoms tab & set <span class=SpellE>Mz</span> … … 2106 2105 <v:imagedata src="Magnetic-III_files/image084.png" o:title=""/> 2107 2106 </v:shape><![endif]--><![if !vml]><img border=0 width=482 height=110 2108 src="Magnetic-III_files/image08 3.gif" v:shapes="Picture_x0020_29"><![endif]></span></p>2107 src="Magnetic-III_files/image082.gif" v:shapes="Picture_x0020_29"><![endif]></span></p> 2109 2108 2110 2109 <p class=MsoNormal><span class=GramE>gives</span> <span class=SpellE>Mz</span>=3.296(35); … … 2119 2118 <v:imagedata src="Magnetic-III_files/image086.png" o:title=""/> 2120 2119 </v:shape><![endif]--><![if !vml]><img border=0 width=237 height=480 2121 src="Magnetic-III_files/image08 5.gif" v:shapes="Picture_x0020_30"><![endif]><!--[if gte vml 1]><v:shape2120 src="Magnetic-III_files/image083.gif" v:shapes="Picture_x0020_30"><![endif]><!--[if gte vml 1]><v:shape 2122 2121 id="Picture_x0020_31" o:spid="_x0000_i1025" type="#_x0000_t75" style='width:187.5pt; 2123 2122 height:358.5pt;visibility:visible;mso-wrap-style:square'> 2124 2123 <v:imagedata src="Magnetic-III_files/image088.png" o:title=""/> 2125 2124 </v:shape><![endif]--><![if !vml]><img border=0 width=250 height=478 2126 src="Magnetic-III_files/image08 7.gif" v:shapes="Picture_x0020_31"><![endif]></span></p>2125 src="Magnetic-III_files/image085.gif" v:shapes="Picture_x0020_31"><![endif]></span></p> 2127 2126 2128 2127 <p class=MsoNormal>Ive placed the doubled c-axis chemical structure so you can -
Tutorials/Magnetic-III/Magnetic-III_files/filelist.xml
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