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	<id>https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?action=history&amp;feed=atom&amp;title=EffectiveSupercell</id>
	<title>EffectiveSupercell - Revision history</title>
	<link rel="self" type="application/atom+xml" href="https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?action=history&amp;feed=atom&amp;title=EffectiveSupercell"/>
	<link rel="alternate" type="text/html" href="https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?title=EffectiveSupercell&amp;action=history"/>
	<updated>2026-04-04T07:55:27Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
	<generator>MediaWiki 1.39.7</generator>
	<entry>
		<id>https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?title=EffectiveSupercell&amp;diff=1819&amp;oldid=prev</id>
		<title>import&gt;Jss43 at 11:41, 5 February 2007</title>
		<link rel="alternate" type="text/html" href="https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?title=EffectiveSupercell&amp;diff=1819&amp;oldid=prev"/>
		<updated>2007-02-05T11:41:32Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;col class=&quot;diff-content&quot; /&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 11:41, 5 February 2007&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 7:&lt;/td&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 7:&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;We can apply (with some care) symmetry operations to our wavefunctions expanded out into the effective supercell.&lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;We can apply (with some care) symmetry operations to our wavefunctions expanded out into the effective supercell.&lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Supercells (both in &amp;lt;math&amp;gt;\Gamma&amp;lt;/math&amp;gt;-point calculations and k-point calculations) have a subtle problem with symmetry in that symmetry operations of the lattice are not necessarily symmetry operations of the supercell (and hence of the wavefunctions), if the supercell is not an &amp;lt;math&amp;gt;n\times n\times n&amp;lt;/math&amp;gt; enlargement of the primitive cell.  --[[User:jss43|james]] &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;14&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;58&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;1&lt;/del&gt; February 2007 (GMT)&lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Supercells (both in &amp;lt;math&amp;gt;\Gamma&amp;lt;/math&amp;gt;-point calculations and k-point calculations) have a subtle problem with symmetry in that symmetry operations of the lattice are not necessarily symmetry operations of the supercell (and hence of the wavefunctions), if the supercell is not an &amp;lt;math&amp;gt;n\times n\times n&amp;lt;/math&amp;gt; enlargement of the primitive&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt; cell.  For a symmetry operation of the lattice to be a symmetry operation of the cell, we require the length of each lattice vector to be unchanged by the operation.  This amounts to considering the effect of the operation on the Cartesian basis vectors.  Hence we require the columns of the rotation matrix to be of unit magnitude in order for the operation to be a symmetry operation of the&lt;/ins&gt; cell.  --[[User:jss43|james]] &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;11&lt;/ins&gt;:&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;41&lt;/ins&gt;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;5&lt;/ins&gt; February 2007 (GMT)&lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>import&gt;Jss43</name></author>
	</entry>
	<entry>
		<id>https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?title=EffectiveSupercell&amp;diff=1818&amp;oldid=prev</id>
		<title>import&gt;Jss43 at 14:58, 1 February 2007</title>
		<link rel="alternate" type="text/html" href="https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?title=EffectiveSupercell&amp;diff=1818&amp;oldid=prev"/>
		<updated>2007-02-01T14:58:08Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 14:58, 1 February 2007&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;To correctly evaluate the Coulomb integrals when dealing with wavefunctions at different k-points, we need to consider the integral over a volume in which the integrals over the exponential factors vanish (the proof of this is attached as a pdf.  The tex file is also around if &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;anyone needs it&lt;/del&gt;).  &lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;To correctly evaluate the Coulomb integrals when dealing with wavefunctions at different k-points, we need to consider the integral over a volume in which the integrals over the exponential factors vanish (the proof of this is attached as a pdf.  The tex file is also around if &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;needed&lt;/ins&gt;).  &lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;This leads us to the concept of an effective supercell, which is the non-primitive cell that is &#039;&#039;&#039;exactly&#039;&#039;&#039; equivalent to the calculation over the k-point mesh.&lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;This leads us to the concept of an effective supercell, which is the non-primitive cell that is &#039;&#039;&#039;exactly&#039;&#039;&#039; equivalent to the calculation over the k-point mesh.&lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-empty diff-side-deleted&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-empty diff-side-deleted&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;As a result, we are restricted in choice of the k-point mesh to those which are physically meaningful: each component of each wavevector must be of the form 1/n, where n is an integer (units: reciprocal lattice basis).  In order to sample each replication of the primitive cell in the effective supercell, the k-point mesh must be regularly spaced, with each k-point separated from the nearest along each axis by &amp;lt;math&amp;gt;1/n_i&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;n_i&amp;lt;/math&amp;gt; is the number of k-points along axis &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt;. We also require the &amp;lt;math&amp;gt;\Gamma&amp;lt;/math&amp;gt;-point to be included.  Such meshes are easy to generate, although somewhat tedious.  A simple python script (~jss43/bin/kpntgen.py) on sword generates the desired mesh for inclusion in CPMD input files.  &lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-empty diff-side-deleted&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-empty diff-side-deleted&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;We can apply (with some care) symmetry operations to our wavefunctions expanded out into the effective supercell.&lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-empty diff-side-deleted&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-empty diff-side-deleted&quot;&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Supercells (both in &amp;lt;math&amp;gt;\Gamma&amp;lt;/math&amp;gt;-point calculations and k-point calculations) have a subtle problem with symmetry in that symmetry operations of the lattice are not necessarily symmetry operations of the supercell (and hence of the wavefunctions), if the supercell is not an &amp;lt;math&amp;gt;n\times n\times n&amp;lt;/math&amp;gt; enlargement of the primitive cell.  --[[User:jss43|james]] 14:58, 1 February 2007 (GMT)&lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>import&gt;Jss43</name></author>
	</entry>
	<entry>
		<id>https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?title=EffectiveSupercell&amp;diff=1817&amp;oldid=prev</id>
		<title>import&gt;Jss43 at 19:39, 31 January 2007</title>
		<link rel="alternate" type="text/html" href="https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?title=EffectiveSupercell&amp;diff=1817&amp;oldid=prev"/>
		<updated>2007-01-31T19:39:17Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;To correctly evaluate the Coulomb integrals when dealing with wavefunctions at different k-points, we need to consider the integral over a volume in which the integrals over the exponential factors vanish (the proof of this is attached as a pdf.  The tex file is also around if anyone needs it).  &lt;br /&gt;
&lt;br /&gt;
This leads us to the concept of an effective supercell, which is the non-primitive cell that is &amp;#039;&amp;#039;&amp;#039;exactly&amp;#039;&amp;#039;&amp;#039; equivalent to the calculation over the k-point mesh.&lt;/div&gt;</summary>
		<author><name>import&gt;Jss43</name></author>
	</entry>
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