Changeset 3723
- Timestamp:
- Nov 7, 2018 10:24:52 AM (4 years ago)
- Location:
- Tutorials/Magnetic-I
- Files:
-
- 46 added
- 57 deleted
- 29 edited
Legend:
- Unmodified
- Added
- Removed
-
Tutorials/Magnetic-I/Magnetic Structures-I.htm
r3688 r3723 23 23 <o:Author>Von Dreele</o:Author> 24 24 <o:LastAuthor>vondreele</o:LastAuthor> 25 <o:Revision>1 1</o:Revision>26 <o:TotalTime> 693</o:TotalTime>25 <o:Revision>13</o:Revision> 26 <o:TotalTime>743</o:TotalTime> 27 27 <o:Created>2018-09-18T19:55:00Z</o:Created> 28 <o:LastSaved>2018-1 0-22T15:38:00Z</o:LastSaved>28 <o:LastSaved>2018-11-07T16:21:00Z</o:LastSaved> 29 29 <o:Pages>1</o:Pages> 30 <o:Words>33 26</o:Words>31 <o:Characters>1 8963</o:Characters>32 <o:Lines>1 58</o:Lines>33 <o:Paragraphs>4 4</o:Paragraphs>34 <o:CharactersWithSpaces>22 245</o:CharactersWithSpaces>30 <o:Words>3398</o:Words> 31 <o:Characters>19373</o:Characters> 32 <o:Lines>161</o:Lines> 33 <o:Paragraphs>45</o:Paragraphs> 34 <o:CharactersWithSpaces>22726</o:CharactersWithSpaces> 35 35 <o:Version>16.00</o:Version> 36 36 </o:DocumentProperties> … … 659 659 {font-family:"Cambria Math"; 660 660 panose-1:2 4 5 3 5 4 6 3 2 4; 661 mso-font-charset: 0;661 mso-font-charset:1; 662 662 mso-generic-font-family:roman; 663 663 mso-font-pitch:variable; 664 mso-font-signature: -536869121 1107305727 33554432 0 4150;}664 mso-font-signature:0 0 0 0 0 0;} 665 665 @font-face 666 666 {font-family:Calibri; … … 1427 1427 text-underline:none'>Perez-Mato, JM; <span class=SpellE>Gallego</span>, SV; <span 1428 1428 class=SpellE>Elcoro</span>, L; <span class=SpellE>Tasci</span>, E and <span 1429 class=SpellE>Aroyo</span>, MI <br>1430 <i>J. of Phys.: <span class=SpellE>Condens</span> Matter</i> (2016), <b>28</b>:28601</span></a>) 1431 to determine magnetic crystal structures. If you have not done so already, you 1432 may wish to do the Simple Magnetic Structures tutorial first as it contains 1433 some background information that will not be covered here. To make this work, 1434 your computer must have an internet connection for GSAS-II to access this site. 1435 (We will supply the project file that results after k-SUBGROUPSMAG is called in 1436 case you lackinternet access)</p>1429 class=SpellE>Aroyo</span>, MI <i>J. of Phys.: <span class=SpellE>Condens</span> 1430 Matter</i> (2016), <b>28</b>:28601</span></a>) to determine magnetic crystal 1431 structures. If you have not done so already, you may wish to do the Simple 1432 Magnetic Structures tutorial first as it contains some background information 1433 that will not be covered here. To make this work, your computer must have an 1434 internet connection for GSAS-II to access this site. (We will supply the 1435 project file that results after k-SUBGROUPSMAG is called in case you lack 1436 internet access)</p> 1437 1437 1438 1438 <p class=MsoNormal><o:p> </o:p></p> 1439 1439 1440 <p class=MsoNormal> <span class=GramE>k-SUBGROUPSMAG</span> operates by starting1441 with the grey group for the parent chemical structure (e.g. Pnma1) and any 1442 propagation vector (k-vector) by removing symmetry operators to generate 1443 magnetic space subgroups. The remaining operators in each case are identified 1444 with a standard setting of the known magnetic BNS space groups (2<sup>nd</sup> 1445 setting with inversion at the origin as needed). It generally doesnt stop 1446 until the lowest possible symmetry (triclinic) is reached; there can be more1447 than 100 of these possible subgroups. For each one, the magnetic space group 1448 symbol, lattice transformation matrix and any required translation of the 1449 original coordinates is returned in a table of the results. In GSAS-II,the1440 <p class=MsoNormal>Starting with the grey group for the parent chemical 1441 structure (e.g. Pnma1) and any propagation vector (k-vector), k-SUBGROUPSMAG 1442 operates by removing symmetry operators to generate magnetic space subgroups. 1443 The remaining operators in each case are identified with a standard setting of 1444 the known magnetic BNS space groups (2<sup>nd</sup> setting with inversion at 1445 the origin as needed). It generally doesnt stop until the lowest possible 1446 symmetry (triclinic) is reached; there can be more than 100 of these possible 1447 subgroups. For each one, the magnetic space group symbol, lattice 1448 transformation matrix and any required translation of the original coordinates is 1449 returned in a table of the results. In GSAS-II, a special version of the 1450 1450 k-SUBGROUPSMAG web page is called with the parent chemical space group 1451 operations, your selected k-vectors and some option flags. The returned web1452 page is parsed by GSAS-II to extract the generated magnetic space groups, 1453 transformation matrices and origin shift vector. If the resulting space group 1454 is orthorhombic, GSAS-II will by default transform the standard setting to a 1455 setting where the unit cell axes orientation is preserved vs the chemical cell. 1456 GSAS-II will also optionally examine the magnetic atom positions to determine 1457 if any or all can carry a nonzero moment, flagging those space groups with 1458 atoms that can. This simplifies the search for a correct description of the 1459 magnetic structure.</p>1451 operations, your selected k-vectors and some option flags. It return an html file 1452 containing a table which is parsed by GSAS-II to extract the generated magnetic 1453 space groups, transformation matrices, origin shift vector, conjugacy classes 1454 (if any) and super group lists. If the resulting space group is orthorhombic, 1455 GSAS-II will by default transform the standard setting to a setting where the 1456 unit cell axes orientation is preserved vs the chemical cell. GSAS-II will also 1457 optionally examine the magnetic atom positions to determine if any or all can 1458 carry a nonzero moment, flagging those space groups with atoms that can. This 1459 simplifies the search for a correct description of the magnetic structure.</p> 1460 1460 1461 1461 <p class=MsoNormal><o:p> </o:p></p> … … 1535 1535 the <b style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1536 1536 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1537 minor-latin'> CaMnO3_50K.gsas</span></b><span style='font-family:"Calibri",sans-serif;1537 minor-latin'>LaMnO3_50K.gsas</span></b><span style='font-family:"Calibri",sans-serif; 1538 1538 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1539 1539 minor-latin'> data</span> file in the first dialog and press <b … … 1559 1559 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1560 1560 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1561 minor-latin'>BT1_Cu3 00.inst</span></b>; you may have to change the file type in1561 minor-latin'>BT1_Cu311.inst</span></b>; you may have to change the file type in 1562 1562 the file selection Dialog box to <b style='mso-bidi-font-weight:normal'><span 1563 1563 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; … … 1592 1592 <v:imagedata src="Magnetic%20Structures-I_files/image001.png" o:title=""/> 1593 1593 </v:shape><![endif]--><![if !vml]><img border=0 width=426 height=289 1594 src="Magnetic%20Structures-I_files/image00 3.gif" v:shapes="Picture_x0020_1"><![endif]></span></h2>1594 src="Magnetic%20Structures-I_files/image002.gif" v:shapes="Picture_x0020_1"><![endif]></span></h2> 1595 1595 1596 1596 <p class=MsoNormal><span class=GramE>and</span> the plot window will show the … … 1600 1600 id="Picture_x0020_2" o:spid="_x0000_i1062" type="#_x0000_t75" style='width:5in; 1601 1601 height:368.25pt;visibility:visible;mso-wrap-style:square'> 1602 <v:imagedata src="Magnetic%20Structures-I_files/image00 4.png" o:title=""/>1602 <v:imagedata src="Magnetic%20Structures-I_files/image003.png" o:title=""/> 1603 1603 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=491 1604 src="Magnetic%20Structures-I_files/image00 5.gif" v:shapes="Picture_x0020_2"><![endif]></span></p>1604 src="Magnetic%20Structures-I_files/image004.gif" v:shapes="Picture_x0020_2"><![endif]></span></p> 1605 1605 1606 1606 <h3>Step 2: Select Limits </h3> … … 1641 1641 id="Picture_x0020_3" o:spid="_x0000_i1061" type="#_x0000_t75" style='width:358.5pt; 1642 1642 height:367.5pt;visibility:visible;mso-wrap-style:square'> 1643 <v:imagedata src="Magnetic%20Structures-I_files/image00 8.png" o:title=""/>1643 <v:imagedata src="Magnetic%20Structures-I_files/image005.png" o:title=""/> 1644 1644 </v:shape><![endif]--><![if !vml]><img border=0 width=478 height=490 1645 src="Magnetic%20Structures-I_files/image00 7.gif" v:shapes="Picture_x0020_3"><![endif]></span></p>1645 src="Magnetic%20Structures-I_files/image006.gif" v:shapes="Picture_x0020_3"><![endif]></span></p> 1646 1646 1647 1647 <h3>Step 3: Read in the chemical structure for LaMnO<sub>3</sub></h3> … … 1662 1662 minor-latin;mso-fareast-font-family:Calibri;mso-fareast-theme-font:minor-latin; 1663 1663 mso-hansi-theme-font:minor-latin'>Help/Download tutorial</span></b><span 1664 style='mso-fareast-font-family:Calibri;mso-fareast-theme-font:minor-latin'> menu1665 entry to open this page and downloaded the exercise files (recommended), then 1666 the </span><b style='mso-bidi-font-weight:normal'><span style='font-family:1664 style='mso-fareast-font-family:Calibri;mso-fareast-theme-font:minor-latin'> 1665 menu entry to open this page and downloaded the exercise files (recommended), 1666 then the </span><b style='mso-bidi-font-weight:normal'><span style='font-family: 1667 1667 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-fareast-font-family: 1668 1668 Calibri;mso-fareast-theme-font:minor-latin;mso-hansi-theme-font:minor-latin'>Magnetic-I/data/...</span></b><span … … 1710 1710 o:spid="_x0000_i1060" type="#_x0000_t75" style='width:283.5pt;height:227.25pt; 1711 1711 visibility:visible;mso-wrap-style:square'> 1712 <v:imagedata src="Magnetic%20Structures-I_files/image0 12.png" o:title=""/>1712 <v:imagedata src="Magnetic%20Structures-I_files/image007.png" o:title=""/> 1713 1713 </v:shape><![endif]--><![if !vml]><img border=0 width=378 height=303 1714 src="Magnetic%20Structures-I_files/image00 9.gif" v:shapes="Picture_x0020_4"><![endif]></span></p>1714 src="Magnetic%20Structures-I_files/image008.gif" v:shapes="Picture_x0020_4"><![endif]></span></p> 1715 1715 1716 1716 <p class=MsoListParagraphCxSpLast style='margin-left:.25in;mso-add-space:auto'>Select … … 1724 1724 o:spid="_x0000_i1059" type="#_x0000_t75" style='width:343.5pt;height:219pt; 1725 1725 visibility:visible;mso-wrap-style:square'> 1726 <v:imagedata src="Magnetic%20Structures-I_files/image0 15.png" o:title=""/>1726 <v:imagedata src="Magnetic%20Structures-I_files/image009.png" o:title=""/> 1727 1727 </v:shape><![endif]--><![if !vml]><img border=0 width=458 height=292 1728 src="Magnetic%20Structures-I_files/image01 3.gif" v:shapes="Picture_x0020_5"><![endif]></span></p>1728 src="Magnetic%20Structures-I_files/image010.gif" v:shapes="Picture_x0020_5"><![endif]></span></p> 1729 1729 1730 1730 <h3>Step 4. Check powder pattern indexing</h3> 1731 1731 1732 1732 <p class=MsoNormal>Here the objective is to determine how the reflection 1733 positions generated from the chemical (nuclear) crystal structure lattice 1734 matchup with the peaks observed for this antiferromagnet. </p>1733 positions generated from the chemical (nuclear) crystal structure lattice match 1734 up with the peaks observed for this antiferromagnet. </p> 1735 1735 1736 1736 <p class=MsoListParagraphCxSpFirst style='margin-left:.25in;mso-add-space:auto; … … 1747 1747 <v:imagedata src="Magnetic%20Structures-I_files/image011.png" o:title=""/> 1748 1748 </v:shape><![endif]--><![if !vml]><img border=0 width=465 height=167 1749 src="Magnetic%20Structures-I_files/image01 9.gif" v:shapes="Picture_x0020_6"><![endif]></span></p>1749 src="Magnetic%20Structures-I_files/image012.gif" v:shapes="Picture_x0020_6"><![endif]></span></p> 1750 1750 1751 1751 <p class=MsoListParagraphCxSpMiddle style='margin-left:.25in;mso-add-space: … … 1779 1779 o:spid="_x0000_i1057" type="#_x0000_t75" style='width:342pt;height:122.25pt; 1780 1780 visibility:visible;mso-wrap-style:square'> 1781 <v:imagedata src="Magnetic%20Structures-I_files/image01 8.png" o:title=""/>1781 <v:imagedata src="Magnetic%20Structures-I_files/image013.png" o:title=""/> 1782 1782 </v:shape><![endif]--><![if !vml]><img border=0 width=456 height=163 1783 src="Magnetic%20Structures-I_files/image0 21.gif" v:shapes="Picture_x0020_7"><![endif]></span><br>1783 src="Magnetic%20Structures-I_files/image014.gif" v:shapes="Picture_x0020_7"><![endif]></span><br> 1784 1784 showing the lattice constants for LaMnO<sub>3</sub> you had obtained from the <span 1785 1785 class=SpellE>cif</span> file and the powder pattern will change showing the … … 1794 1794 o:spid="_x0000_i1056" type="#_x0000_t75" style='width:342pt;height:279.75pt; 1795 1795 visibility:visible;mso-wrap-style:square'> 1796 <v:imagedata src="Magnetic%20Structures-I_files/image0 28.png" o:title=""/>1796 <v:imagedata src="Magnetic%20Structures-I_files/image015.png" o:title=""/> 1797 1797 </v:shape><![endif]--><![if !vml]><img border=0 width=456 height=373 1798 src="Magnetic%20Structures-I_files/image0 22.gif" v:shapes="Picture_x0020_8"><![endif]></span></p>1798 src="Magnetic%20Structures-I_files/image016.gif" v:shapes="Picture_x0020_8"><![endif]></span></p> 1799 1799 1800 1800 <p class=MsoNormal>Notice that every peak is indexed by this cell, therefore … … 1824 1824 1825 1825 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1826 id=" _x0000_i1055" type="#_x0000_t75" style='width:207.75pt;height:225.75pt;1827 visibility:visible;mso-wrap-style:square'>1828 <v:imagedata src="Magnetic%20Structures-I_files/image0 23.png" o:title=""/>1826 id="Picture_x0020_9" o:spid="_x0000_i1055" type="#_x0000_t75" style='width:207.75pt; 1827 height:225.75pt;visibility:visible;mso-wrap-style:square'> 1828 <v:imagedata src="Magnetic%20Structures-I_files/image017.png" o:title=""/> 1829 1829 </v:shape><![endif]--><![if !vml]><img border=0 width=277 height=301 1830 src="Magnetic%20Structures-I_files/image0 24.gif" v:shapes="_x0000_i1055"><![endif]></span></p>1830 src="Magnetic%20Structures-I_files/image018.gif" v:shapes="Picture_x0020_9"><![endif]></span></p> 1831 1831 1832 1832 <p class=MsoNormal>These are the controls for running the Bilbao routine. The … … 1850 1850 id="Picture_x0020_16" o:spid="_x0000_i1054" type="#_x0000_t75" style='width:357.75pt; 1851 1851 height:123.75pt;visibility:visible;mso-wrap-style:square'> 1852 <v:imagedata src="Magnetic%20Structures-I_files/image0 32.png" o:title=""/>1852 <v:imagedata src="Magnetic%20Structures-I_files/image019.png" o:title=""/> 1853 1853 </v:shape><![endif]--><![if !vml]><img border=0 width=477 height=165 1854 src="Magnetic%20Structures-I_files/image02 5.gif" v:shapes="Picture_x0020_16"><![endif]></span></p>1854 src="Magnetic%20Structures-I_files/image020.gif" v:shapes="Picture_x0020_16"><![endif]></span></p> 1855 1855 1856 1856 <p class=MsoNormal>Press <b style='mso-bidi-font-weight:normal'><span … … 1878 1878 1879 1879 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1880 id=" Picture_x0020_11" o:spid="_x0000_i1053" type="#_x0000_t75" style='width:5in;1881 height:212.25pt;visibility:visible;mso-wrap-style:square'>1882 <v:imagedata src="Magnetic%20Structures-I_files/image0 51.png" o:title=""/>1883 </v:shape><![endif]--><![if !vml]><img border=0 width=4 80 height=2831884 src="Magnetic%20Structures-I_files/image02 6.gif" v:shapes="Picture_x0020_11"><![endif]></span></p>1880 id="_x0000_i1053" type="#_x0000_t75" style='width:357.75pt;height:240.75pt; 1881 visibility:visible;mso-wrap-style:square'> 1882 <v:imagedata src="Magnetic%20Structures-I_files/image021.png" o:title=""/> 1883 </v:shape><![endif]--><![if !vml]><img border=0 width=477 height=321 1884 src="Magnetic%20Structures-I_files/image022.gif" v:shapes="_x0000_i1053"><![endif]></span></p> 1885 1885 1886 1886 <p class=MsoNormal>The table shows all the magnetic space groups that are 1887 1887 possible starting with P n m <span class=GramE>a and</span> zero propagation 1888 vector; this is noted in the table heading. Notice that it goes all the way to a1889 triclinic P1 magnetic space group; you probably will never need to go that far 1890 to find a suitable magnetic space group. The ones marked Keep have a possibly 1891 magnetic <span class=SpellE>Mn</span> atom based on the magnetic site1888 vector; this is noted in the table heading. Notice that it goes all the way to 1889 a triclinic P1 magnetic space group; you probably will never need to go that 1890 far to find a suitable magnetic space group. The ones marked Keep have a 1891 possibly magnetic <span class=SpellE>Mn</span> atom based on the magnetic site 1892 1892 symmetries of the transformed atom positions (there may be more than one). The <span 1893 1893 class=SpellE>Uniq</span> column indicates how many unique <span class=SpellE>Mn</span> … … 1895 1895 with the smallest number of magnetic sites. Each entry also shows the 1896 1896 transformation matrix in symbolic form and the necessary origin shift so that 1897 the new structure is properly positioned to satisfy the new space group. The 1898 orthorhombic ones (1-18) are all transformed so the cell matches the parent; 1899 this is the default action. K-SUBGROUPSMAG returned these in the standard 1900 orthorhombic setting; GSAS-II reset these to match the parent. The <b 1901 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1902 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1903 minor-latin'>Try</span></b> box is for you to test the reflection indexing of 1904 each structure to be sure all the magnetic peaks are included. Try each of the 1905 first 3 that are marked Keep (you may recognize these from the Simple Magnetic 1906 tutorial). As you select each one the powder pattern will be replotted showing 1907 the allowed lines. For the 2<sup>nd</sup> <span class=GramE>one ,</span> <span 1908 class=SpellE><b style='mso-bidi-font-weight:normal'><span style='font-family: 1909 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-hansi-theme-font: 1910 minor-latin;mso-bidi-theme-font:minor-latin'>Pnma</span></b></span><b 1897 the new structure is properly positioned to satisfy the new space group. <span 1898 class=SpellE><span class=GramE>nConj</span></span> indicates how many other 1899 magnetic space groups are members of the conjugate class (in this case only 1 1900 for every space group) and <span class=SpellE>nSup</span> shows how many super 1901 groups there are for each space group. Those with only one may have just the 1902 parent space group as their super group; these are the maximal subgroups 1903 resulting from the loss of just a single symmetry generator. The orthorhombic 1904 ones (1-24) are all transformed so the cell matches the parent; this is the 1905 default action. K-SUBGROUPSMAG returned these in the standard orthorhombic 1906 setting; GSAS-II reset these to match the parent. The <b style='mso-bidi-font-weight: 1907 normal'><span style='font-family:"Calibri",sans-serif;mso-ascii-theme-font: 1908 minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Try</span></b> 1909 box is for you to test the reflection indexing of each structure to be sure all 1910 the magnetic peaks are included. Try each of the first 3 that are marked Keep 1911 (you may recognize these from the Simple Magnetic tutorial). As you select each 1912 one the powder pattern will be replotted showing the allowed lines. For the 2<sup>nd</sup> 1913 one, <span class=SpellE><b style='mso-bidi-font-weight:normal'><span 1914 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1915 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Pnma</span></b></span><b 1911 1916 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1912 1917 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: … … 1917 1922 id="Picture_x0020_47" o:spid="_x0000_i1052" type="#_x0000_t75" style='width:359.25pt; 1918 1923 height:367.5pt;visibility:visible;mso-wrap-style:square'> 1919 <v:imagedata src="Magnetic%20Structures-I_files/image0 49.png" o:title=""/>1924 <v:imagedata src="Magnetic%20Structures-I_files/image023.png" o:title=""/> 1920 1925 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=490 1921 src="Magnetic%20Structures-I_files/image02 7.gif" v:shapes="Picture_x0020_47"><![endif]></span></p>1926 src="Magnetic%20Structures-I_files/image024.gif" v:shapes="Picture_x0020_47"><![endif]></span></p> 1922 1927 1923 1928 <p class=MsoNormal>Ive zoomed in on the low angle region for clarity. If you <span … … 1932 1937 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1933 1938 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1934 minor-latin'>Keep</span></b></span> the other choices so they dont appear in1935 a later step where you select the magnetic phase. Now do a <b style='mso-bidi-font-weight: 1936 normal'><span style='font-family:"Calibri",sans-serif;mso-ascii-theme-font: 1937 m inor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Save1938 project</span></b>; that will save your choices for later (there should be at 1939 least two).</p>1939 minor-latin'>Keep</span></b></span> the other 2 choices so they dont appear 1940 in a later step where you select the magnetic phase. Now do a <b 1941 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1942 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: 1943 minor-latin'>Save project</span></b>; that will save your choices for later 1944 (there should be at least two).</p> 1940 1945 1941 1946 <h3>Step 6. Select a magnetic phase</h3> … … 1954 1959 id="Picture_x0020_48" o:spid="_x0000_i1051" type="#_x0000_t75" style='width:5in; 1955 1960 height:217.5pt;visibility:visible;mso-wrap-style:square'> 1956 <v:imagedata src="Magnetic%20Structures-I_files/image0 53.png" o:title=""/>1961 <v:imagedata src="Magnetic%20Structures-I_files/image025.png" o:title=""/> 1957 1962 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=290 1958 src="Magnetic%20Structures-I_files/image02 9.gif" v:shapes="Picture_x0020_48"><![endif]></span></p>1963 src="Magnetic%20Structures-I_files/image026.gif" v:shapes="Picture_x0020_48"><![endif]></span></p> 1959 1964 1960 1965 <p class=MsoNormal>Do <b style='mso-bidi-font-weight:normal'><span … … 1966 1971 id="Picture_x0020_49" o:spid="_x0000_i1050" type="#_x0000_t75" style='width:207.75pt; 1967 1972 height:222.75pt;visibility:visible;mso-wrap-style:square'> 1968 <v:imagedata src="Magnetic%20Structures-I_files/image0 57.png" o:title=""/>1973 <v:imagedata src="Magnetic%20Structures-I_files/image027.png" o:title=""/> 1969 1974 </v:shape><![endif]--><![if !vml]><img border=0 width=277 height=297 1970 src="Magnetic%20Structures-I_files/image0 30.gif" v:shapes="Picture_x0020_49"><![endif]></span></p>1975 src="Magnetic%20Structures-I_files/image028.gif" v:shapes="Picture_x0020_49"><![endif]></span></p> 1971 1976 1972 1977 <p class=MsoNormal>This shows all magnetic phases that were marked Keep in the 1973 Unit Cells ; for each you see the transformation and vector (occasionally two1974 results will have the same space group but are different). Select the 1<sup>st</sup> 1975 one and press <b style='mso-bidi-font-weight:normal'><span style='font-family: 1976 "Calibri",sans-serif;mso-ascii-theme-font:minor-latin;mso-hansi-theme-font: 1977 m inor-latin;mso-bidi-theme-font:minor-latin'>OK</span></b>; a new popup dialog1978 will appear.</p>1978 Unit Cells table; for each you see the transformation and vector (occasionally 1979 two results will have the same space group but have different vectors). Select 1980 the 1<sup>st</sup> one and press <b style='mso-bidi-font-weight:normal'><span 1981 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 1982 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>OK</span></b>; 1983 a new popup dialog will appear.</p> 1979 1984 1980 1985 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 1981 1986 id="Picture_x0020_50" o:spid="_x0000_i1049" type="#_x0000_t75" style='width:262.5pt; 1982 1987 height:92.25pt;visibility:visible;mso-wrap-style:square'> 1983 <v:imagedata src="Magnetic%20Structures-I_files/image0 61.png" o:title=""/>1988 <v:imagedata src="Magnetic%20Structures-I_files/image029.png" o:title=""/> 1984 1989 </v:shape><![endif]--><![if !vml]><img border=0 width=350 height=123 1985 src="Magnetic%20Structures-I_files/image03 1.gif" v:shapes="Picture_x0020_50"><![endif]></span></p>1990 src="Magnetic%20Structures-I_files/image030.gif" v:shapes="Picture_x0020_50"><![endif]></span></p> 1986 1991 1987 1992 <p class=MsoNormal>This shows the magnetic atoms in this structure and allows 1988 one to reject certain ones that are known to not be magnetic. If you press 1989 Delete then this space group will be unmarked Keep in the Unit Cell List and 1990 will not be available for a future selection. If you select No then nothing 1991 will happen and you can find this space group in a subsequent try of Select 1992 magnetic phase.This space group is the desired one; press <span class=GramE><b1993 one to reject certain ones that are known to not be magnetic. If you press Delete 1994 then this space group will be unmarked Keep in the Unit Cell List and will not 1995 be available for a future selection. If you select No then nothing will happen 1996 and you can find this space group in a subsequent try of Select magnetic phase. 1997 This space group is the desired one; press <span class=GramE><b 1993 1998 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; 1994 1999 mso-ascii-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;mso-bidi-theme-font: … … 2008 2013 id="Picture_x0020_17" o:spid="_x0000_i1048" type="#_x0000_t75" style='width:357pt; 2009 2014 height:232.5pt;visibility:visible;mso-wrap-style:square'> 2010 <v:imagedata src="Magnetic%20Structures-I_files/image0 42.png" o:title=""/>2015 <v:imagedata src="Magnetic%20Structures-I_files/image031.png" o:title=""/> 2011 2016 </v:shape><![endif]--><![if !vml]><img border=0 width=476 height=310 2012 src="Magnetic%20Structures-I_files/image03 3.gif" v:shapes="Picture_x0020_17"><![endif]></span></p>2013 2014 <p class=MsoNormal>The phase is named with mag_2 appended to the end, the phase2015 type is magnetic and there are magnetic spin operator selections part way down 2016 the page. These are properly set for the chosen magnetic space group <span2017 src="Magnetic%20Structures-I_files/image032.gif" v:shapes="Picture_x0020_17"><![endif]></span></p> 2018 2019 <p class=MsoNormal>The phase is named with mag_2 appended to the end, the 2020 phase type is magnetic and there are magnetic spin operator selections part way 2021 down the page. These are properly set for the chosen magnetic space group <span 2017 2022 class=SpellE>Pnma</span> as red<span class=GramE>, </span>black, red. 2018 2023 You also can see the <span class=SpellE>Lande</span> g factor can be changed … … 2026 2031 magnetic structure.</p> 2027 2032 2028 <p class=MsoNormal><o:p> </o:p></p>2029 2030 2033 <h3>Step 7. Solving the magnetic structure</h3> 2031 2034 … … 2050 2053 2051 2054 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 2052 id="_x0000_i1047" type="#_x0000_t75" style='width:359.25pt;height:1 80.75pt;2055 id="_x0000_i1047" type="#_x0000_t75" style='width:359.25pt;height:139.5pt; 2053 2056 visibility:visible;mso-wrap-style:square'> 2054 <v:imagedata src="Magnetic%20Structures-I_files/image03 4.png" o:title=""/>2055 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height= 2412056 src="Magnetic%20Structures-I_files/image03 5.gif" v:shapes="_x0000_i1047"><![endif]></span></p>2057 <v:imagedata src="Magnetic%20Structures-I_files/image033.png" o:title=""/> 2058 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=186 2059 src="Magnetic%20Structures-I_files/image034.gif" v:shapes="_x0000_i1047"><![endif]></span></p> 2057 2060 2058 2061 <p class=MsoNormal>Under the <b style='mso-bidi-font-weight:normal'><span … … 2067 2070 id="Picture_x0020_19" o:spid="_x0000_i1046" type="#_x0000_t75" style='width:361.5pt; 2068 2071 height:175.5pt;visibility:visible;mso-wrap-style:square'> 2069 <v:imagedata src="Magnetic%20Structures-I_files/image0 46.png" o:title=""/>2072 <v:imagedata src="Magnetic%20Structures-I_files/image035.png" o:title=""/> 2070 2073 </v:shape><![endif]--><![if !vml]><img border=0 width=482 height=234 2071 2074 src="Magnetic%20Structures-I_files/image036.gif" v:shapes="Picture_x0020_19"><![endif]></span></p> … … 2077 2080 id="Picture_x0020_20" o:spid="_x0000_i1045" type="#_x0000_t75" style='width:361.5pt; 2078 2081 height:175.5pt;visibility:visible;mso-wrap-style:square'> 2079 <v:imagedata src="Magnetic%20Structures-I_files/image0 48.png" o:title=""/>2082 <v:imagedata src="Magnetic%20Structures-I_files/image037.png" o:title=""/> 2080 2083 </v:shape><![endif]--><![if !vml]><img border=0 width=482 height=234 2081 2084 src="Magnetic%20Structures-I_files/image038.gif" v:shapes="Picture_x0020_20"><![endif]></span></p> … … 2085 2088 2086 2089 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 2087 id="_x0000_i1044" type="#_x0000_t75" style='width: 5in;height:180.75pt;2090 id="_x0000_i1044" type="#_x0000_t75" style='width:362.25pt;height:141pt; 2088 2091 visibility:visible;mso-wrap-style:square'> 2089 2092 <v:imagedata src="Magnetic%20Structures-I_files/image039.png" o:title=""/> 2090 </v:shape><![endif]--><![if !vml]><img border=0 width=48 0 height=2412093 </v:shape><![endif]--><![if !vml]><img border=0 width=483 height=188 2091 2094 src="Magnetic%20Structures-I_files/image040.gif" v:shapes="_x0000_i1044"><![endif]></span></p> 2092 2095 … … 2102 2105 id="Picture_x0020_22" o:spid="_x0000_i1043" type="#_x0000_t75" style='width:361.5pt; 2103 2106 height:80.25pt;visibility:visible;mso-wrap-style:square'> 2104 <v:imagedata src="Magnetic%20Structures-I_files/image0 52.png" o:title=""/>2107 <v:imagedata src="Magnetic%20Structures-I_files/image041.png" o:title=""/> 2105 2108 </v:shape><![endif]--><![if !vml]><img border=0 width=482 height=107 2106 src="Magnetic%20Structures-I_files/image04 4.gif" v:shapes="Picture_x0020_22"><![endif]></span></p>2109 src="Magnetic%20Structures-I_files/image042.gif" v:shapes="Picture_x0020_22"><![endif]></span></p> 2107 2110 2108 2111 <p class=MsoNormal>The least squares will not begin a refinement of <span … … 2120 2123 id="Picture_x0020_23" o:spid="_x0000_i1042" type="#_x0000_t75" style='width:360.75pt; 2121 2124 height:294pt;visibility:visible;mso-wrap-style:square'> 2122 <v:imagedata src="Magnetic%20Structures-I_files/image0 54.png" o:title=""/>2125 <v:imagedata src="Magnetic%20Structures-I_files/image043.png" o:title=""/> 2123 2126 </v:shape><![endif]--><![if !vml]><img border=0 width=481 height=392 2124 src="Magnetic%20Structures-I_files/image04 5.gif" v:shapes="Picture_x0020_23"><![endif]></span></p>2127 src="Magnetic%20Structures-I_files/image044.gif" v:shapes="Picture_x0020_23"><![endif]></span></p> 2125 2128 2126 2129 <p class=MsoNormal>There does not appear to be any calculated magnetic … … 2131 2134 id="Picture_x0020_24" o:spid="_x0000_i1041" type="#_x0000_t75" style='width:359.25pt; 2132 2135 height:293.25pt;visibility:visible;mso-wrap-style:square'> 2133 <v:imagedata src="Magnetic%20Structures-I_files/image0 56.png" o:title=""/>2136 <v:imagedata src="Magnetic%20Structures-I_files/image045.png" o:title=""/> 2134 2137 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=391 2135 src="Magnetic%20Structures-I_files/image0 50.gif" v:shapes="Picture_x0020_24"><![endif]></span></p>2138 src="Magnetic%20Structures-I_files/image046.gif" v:shapes="Picture_x0020_24"><![endif]></span></p> 2136 2139 2137 2140 <p class=MsoNormal>The magnetic moment is clearly too small; to let the least … … 2148 2151 id="Picture_x0020_25" o:spid="_x0000_i1040" type="#_x0000_t75" style='width:361.5pt; 2149 2152 height:294.75pt;visibility:visible;mso-wrap-style:square'> 2150 <v:imagedata src="Magnetic%20Structures-I_files/image0 58.png" o:title=""/>2153 <v:imagedata src="Magnetic%20Structures-I_files/image047.png" o:title=""/> 2151 2154 </v:shape><![endif]--><![if !vml]><img border=0 width=482 height=393 2152 src="Magnetic%20Structures-I_files/image0 62.gif" v:shapes="Picture_x0020_25"><![endif]></span></p>2155 src="Magnetic%20Structures-I_files/image048.gif" v:shapes="Picture_x0020_25"><![endif]></span></p> 2153 2156 2154 2157 <p class=MsoNormal>This appears to be a reasonable solution; a more complete … … 2177 2180 id="Picture_x0020_26" o:spid="_x0000_i1039" type="#_x0000_t75" style='width:5in; 2178 2181 height:204.75pt;visibility:visible;mso-wrap-style:square'> 2179 <v:imagedata src="Magnetic%20Structures-I_files/image0 60.png" o:title=""/>2182 <v:imagedata src="Magnetic%20Structures-I_files/image049.png" o:title=""/> 2180 2183 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=273 2181 src="Magnetic%20Structures-I_files/image0 88.gif" v:shapes="Picture_x0020_26"><![endif]></span></p>2184 src="Magnetic%20Structures-I_files/image050.gif" v:shapes="Picture_x0020_26"><![endif]></span></p> 2182 2185 2183 2186 <p class=MsoNormal>Do <b style='mso-bidi-font-weight:normal'><span … … 2189 2192 id="Picture_x0020_54" o:spid="_x0000_i1038" type="#_x0000_t75" style='width:207.75pt; 2190 2193 height:222.75pt;visibility:visible;mso-wrap-style:square'> 2191 <v:imagedata src="Magnetic%20Structures-I_files/image0 57.png" o:title=""/>2194 <v:imagedata src="Magnetic%20Structures-I_files/image027.png" o:title=""/> 2192 2195 </v:shape><![endif]--><![if !vml]><img border=0 width=277 height=297 2193 src="Magnetic%20Structures-I_files/image0 30.gif" v:shapes="Picture_x0020_54"><![endif]></span></p>2196 src="Magnetic%20Structures-I_files/image028.gif" v:shapes="Picture_x0020_54"><![endif]></span></p> 2194 2197 2195 2198 <p class=MsoNormal>This time select the second choice <b style='mso-bidi-font-weight: … … 2205 2208 id="Picture_x0020_55" o:spid="_x0000_i1037" type="#_x0000_t75" style='width:262.5pt; 2206 2209 height:92.25pt;visibility:visible;mso-wrap-style:square'> 2207 <v:imagedata src="Magnetic%20Structures-I_files/image 115.png" o:title=""/>2210 <v:imagedata src="Magnetic%20Structures-I_files/image051.png" o:title=""/> 2208 2211 </v:shape><![endif]--><![if !vml]><img border=0 width=350 height=123 2209 src="Magnetic%20Structures-I_files/image0 89.gif" v:shapes="Picture_x0020_55"><![endif]></span></p>2212 src="Magnetic%20Structures-I_files/image052.gif" v:shapes="Picture_x0020_55"><![endif]></span></p> 2210 2213 2211 2214 <p class=MsoNormal>Press <span class=GramE><b style='mso-bidi-font-weight:normal'><span … … 2225 2228 id="Picture_x0020_30" o:spid="_x0000_i1036" type="#_x0000_t75" style='width:363pt; 2226 2229 height:233.25pt;visibility:visible;mso-wrap-style:square'> 2227 <v:imagedata src="Magnetic%20Structures-I_files/image0 64.png" o:title=""/>2230 <v:imagedata src="Magnetic%20Structures-I_files/image053.png" o:title=""/> 2228 2231 </v:shape><![endif]--><![if !vml]><img border=0 width=484 height=311 2229 src="Magnetic%20Structures-I_files/image0 90.gif" v:shapes="Picture_x0020_30"><![endif]></span></p>2232 src="Magnetic%20Structures-I_files/image054.gif" v:shapes="Picture_x0020_30"><![endif]></span></p> 2230 2233 2231 2234 <p class=MsoNormal>This time all the spin operators are black. Select the … … 2235 2238 id="Picture_x0020_33" o:spid="_x0000_i1035" type="#_x0000_t75" style='width:5in; 2236 2239 height:88.5pt;visibility:visible;mso-wrap-style:square'> 2237 <v:imagedata src="Magnetic%20Structures-I_files/image0 66.png" o:title=""/>2240 <v:imagedata src="Magnetic%20Structures-I_files/image055.png" o:title=""/> 2238 2241 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=118 2239 src="Magnetic%20Structures-I_files/image0 91.gif" v:shapes="Picture_x0020_33"><![endif]></span></p>2242 src="Magnetic%20Structures-I_files/image056.gif" v:shapes="Picture_x0020_33"><![endif]></span></p> 2240 2243 2241 2244 <p class=MsoNormal>Again, one can make the same argument that since the 010 … … 2263 2266 id="Picture_x0020_34" o:spid="_x0000_i1034" type="#_x0000_t75" style='width:358.5pt; 2264 2267 height:292.5pt;visibility:visible;mso-wrap-style:square'> 2265 <v:imagedata src="Magnetic%20Structures-I_files/image0 68.png" o:title=""/>2268 <v:imagedata src="Magnetic%20Structures-I_files/image057.png" o:title=""/> 2266 2269 </v:shape><![endif]--><![if !vml]><img border=0 width=478 height=390 2267 src="Magnetic%20Structures-I_files/image0 92.gif" v:shapes="Picture_x0020_34"><![endif]></span></p>2270 src="Magnetic%20Structures-I_files/image058.gif" v:shapes="Picture_x0020_34"><![endif]></span></p> 2268 2271 2269 2272 <p class=MsoNormal>There is intensity in the lowest angle reflection (the 010) … … 2286 2289 id="Picture_x0020_37" o:spid="_x0000_i1033" type="#_x0000_t75" style='width:5in; 2287 2290 height:123pt;visibility:visible;mso-wrap-style:square'> 2288 <v:imagedata src="Magnetic%20Structures-I_files/image0 70.png" o:title=""/>2291 <v:imagedata src="Magnetic%20Structures-I_files/image059.png" o:title=""/> 2289 2292 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=164 2290 src="Magnetic%20Structures-I_files/image0 93.gif" v:shapes="Picture_x0020_37"><![endif]></span></p>2293 src="Magnetic%20Structures-I_files/image060.gif" v:shapes="Picture_x0020_37"><![endif]></span></p> 2291 2294 2292 2295 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 2293 2296 id="Picture_x0020_38" o:spid="_x0000_i1032" type="#_x0000_t75" style='width:358.5pt; 2294 2297 height:114pt;visibility:visible;mso-wrap-style:square'> 2295 <v:imagedata src="Magnetic%20Structures-I_files/image0 72.png" o:title=""/>2298 <v:imagedata src="Magnetic%20Structures-I_files/image061.png" o:title=""/> 2296 2299 </v:shape><![endif]--><![if !vml]><img border=0 width=478 height=152 2297 src="Magnetic%20Structures-I_files/image0 94.gif" v:shapes="Picture_x0020_38"><![endif]></span></p>2300 src="Magnetic%20Structures-I_files/image062.gif" v:shapes="Picture_x0020_38"><![endif]></span></p> 2298 2301 2299 2302 <p class=MsoNormal>You can see in particular at the pair of peaks at 33.3 and … … 2319 2322 id="Picture_x0020_39" o:spid="_x0000_i1031" type="#_x0000_t75" style='width:359.25pt; 2320 2323 height:282.75pt;visibility:visible;mso-wrap-style:square'> 2321 <v:imagedata src="Magnetic%20Structures-I_files/image0 74.png" o:title=""/>2324 <v:imagedata src="Magnetic%20Structures-I_files/image063.png" o:title=""/> 2322 2325 </v:shape><![endif]--><![if !vml]><img border=0 width=479 height=377 2323 src="Magnetic%20Structures-I_files/image0 95.gif" v:shapes="Picture_x0020_39"><![endif]></span></p>2326 src="Magnetic%20Structures-I_files/image064.gif" v:shapes="Picture_x0020_39"><![endif]></span></p> 2324 2327 2325 2328 <p class=MsoNormal>Looking at the plot, it would seem that the lattice … … 2342 2345 id="Picture_x0020_40" o:spid="_x0000_i1030" type="#_x0000_t75" style='width:358.5pt; 2343 2346 height:225.75pt;visibility:visible;mso-wrap-style:square'> 2344 <v:imagedata src="Magnetic%20Structures-I_files/image0 76.png" o:title=""/>2347 <v:imagedata src="Magnetic%20Structures-I_files/image065.png" o:title=""/> 2345 2348 </v:shape><![endif]--><![if !vml]><img border=0 width=478 height=301 2346 src="Magnetic%20Structures-I_files/image0 96.gif" v:shapes="Picture_x0020_40"><![endif]></span></p>2349 src="Magnetic%20Structures-I_files/image066.gif" v:shapes="Picture_x0020_40"><![endif]></span></p> 2347 2350 2348 2351 <p class=MsoNormal>Since the scan covers a very wide range in 2<span … … 2375 2378 minor-latin;mso-bidi-theme-font:minor-latin'>Calculate/Refine</span></b> until 2376 2379 convergence is achieved (i.e. <span class=SpellE>Rwp</span> doesnt change). 2377 This will be 2-3 times. When done my <span class=SpellE>Rwp</span> was ~6. 6%2380 This will be 2-3 times. When done my <span class=SpellE>Rwp</span> was ~6.2% 2378 2381 with a nice clean plot</p> 2379 2382 … … 2381 2384 id="Picture_x0020_41" o:spid="_x0000_i1029" type="#_x0000_t75" style='width:358.5pt; 2382 2385 height:282pt;visibility:visible;mso-wrap-style:square'> 2383 <v:imagedata src="Magnetic%20Structures-I_files/image0 78.png" o:title=""/>2386 <v:imagedata src="Magnetic%20Structures-I_files/image067.png" o:title=""/> 2384 2387 </v:shape><![endif]--><![if !vml]><img border=0 width=478 height=376 2385 src="Magnetic%20Structures-I_files/image0 97.gif" v:shapes="Picture_x0020_41"><![endif]></span></p>2388 src="Magnetic%20Structures-I_files/image068.gif" v:shapes="Picture_x0020_41"><![endif]></span></p> 2386 2389 2387 2390 <p class=MsoNormal>Now we can add refinement of the atom positions and thermal … … 2422 2425 style='font-family:"Calibri",sans-serif;mso-ascii-theme-font:minor-latin; 2423 2426 mso-hansi-theme-font:minor-latin;mso-bidi-theme-font:minor-latin'>Calculate/Refine</span></b> 2424 until convergence (1-2 times). My <span class=SpellE>Rwp</span> was 6.29% with2427 until convergence (1-2 times). My <span class=SpellE>Rwp</span> was 5.95% with 2425 2428 a plot that is hardly different from the previous one. If you press the <b 2426 2429 style='mso-bidi-font-weight:normal'><span style='font-family:"Calibri",sans-serif; … … 2432 2435 id="Picture_x0020_42" o:spid="_x0000_i1028" type="#_x0000_t75" style='width:357.75pt; 2433 2436 height:281.25pt;visibility:visible;mso-wrap-style:square'> 2434 <v:imagedata src="Magnetic%20Structures-I_files/image0 80.png" o:title=""/>2437 <v:imagedata src="Magnetic%20Structures-I_files/image069.png" o:title=""/> 2435 2438 </v:shape><![endif]--><![if !vml]><img border=0 width=477 height=375 2436 src="Magnetic%20Structures-I_files/image0 98.gif" v:shapes="Picture_x0020_42"><![endif]></span></p>2439 src="Magnetic%20Structures-I_files/image070.gif" v:shapes="Picture_x0020_42"><![endif]></span></p> 2437 2440 2438 2441 <p class=MsoNormal>This curve shows a couple of peaks which are from some … … 2466 2469 id="Picture_x0020_43" o:spid="_x0000_i1027" type="#_x0000_t75" style='width:362.25pt; 2467 2470 height:84.75pt;visibility:visible;mso-wrap-style:square'> 2468 <v:imagedata src="Magnetic%20Structures-I_files/image0 82.png" o:title=""/>2471 <v:imagedata src="Magnetic%20Structures-I_files/image071.png" o:title=""/> 2469 2472 </v:shape><![endif]--><![if !vml]><img border=0 width=483 height=113 2470 src="Magnetic%20Structures-I_files/image0 99.gif" v:shapes="Picture_x0020_43"><![endif]></span></p>2473 src="Magnetic%20Structures-I_files/image072.gif" v:shapes="Picture_x0020_43"><![endif]></span></p> 2471 2474 2472 2475 <p class=MsoNormal>The plot will show one atom with magnetic moment. Select the … … 2482 2485 id="Picture_x0020_44" o:spid="_x0000_i1026" type="#_x0000_t75" style='width:5in; 2483 2486 height:139.5pt;visibility:visible;mso-wrap-style:square'> 2484 <v:imagedata src="Magnetic%20Structures-I_files/image0 84.png" o:title=""/>2487 <v:imagedata src="Magnetic%20Structures-I_files/image073.png" o:title=""/> 2485 2488 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=186 2486 src="Magnetic%20Structures-I_files/image 100.gif" v:shapes="Picture_x0020_44"><![endif]></span></p>2489 src="Magnetic%20Structures-I_files/image074.gif" v:shapes="Picture_x0020_44"><![endif]></span></p> 2487 2490 2488 2491 <p class=MsoNormal>The plot will show the unit cell contents of <span 2489 2492 class=SpellE>Mn</span> atoms each with its magnetic moment; they are arranged 2490 2493 in layers along the b-axis with the <span class=GramE>moments</span> 2491 antiparallel from one layer to the next. Some are red indicating that a spin inversion2492 operation was applied for that atom moment.</p>2494 antiparallel from one layer to the next. Some are red indicating that a spin 2495 inversion operation was applied for that atom moment.</p> 2493 2496 2494 2497 <p class=MsoNormal><span style='mso-no-proof:yes'><!--[if gte vml 1]><v:shape 2495 2498 id="Picture_x0020_45" o:spid="_x0000_i1025" type="#_x0000_t75" style='width:5in; 2496 2499 height:368.25pt;visibility:visible;mso-wrap-style:square'> 2497 <v:imagedata src="Magnetic%20Structures-I_files/image0 86.png" o:title=""/>2500 <v:imagedata src="Magnetic%20Structures-I_files/image075.png" o:title=""/> 2498 2501 </v:shape><![endif]--><![if !vml]><img border=0 width=480 height=491 2499 src="Magnetic%20Structures-I_files/image 117.gif" v:shapes="Picture_x0020_45"><![endif]></span></p>2502 src="Magnetic%20Structures-I_files/image076.gif" v:shapes="Picture_x0020_45"><![endif]></span></p> 2500 2503 2501 2504 <p class=MsoNormal>This completes this tutorial; you can save the project if -
Tutorials/Magnetic-I/Magnetic Structures-I_files/filelist.xml
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Tutorials/Magnetic-I/Magnetic Structures-I_files/props083.xml
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