<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?action=history&amp;feed=atom&amp;title=Symmetry</id>
	<title>Symmetry - 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=Symmetry"/>
	<link rel="alternate" type="text/html" href="https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?title=Symmetry&amp;action=history"/>
	<updated>2026-04-15T20:56:49Z</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=Symmetry&amp;diff=1816&amp;oldid=prev</id>
		<title>import&gt;Jss43 at 17:49, 23 January 2007</title>
		<link rel="alternate" type="text/html" href="https://wikis.ch.cam.ac.uk/cuc3/wiki/index.php?title=Symmetry&amp;diff=1816&amp;oldid=prev"/>
		<updated>2007-01-23T17:49:48Z</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;A calculation at a &amp;quot;sensible&amp;quot; choice of k-points is entirely analagous to a &amp;lt;math&amp;gt;\Gamma&amp;lt;/math&amp;gt;-point calculation in a non-primitive cell.  This leads us to our concept of effective supercells.  We can efficiently apply symmetry to &amp;lt;math&amp;gt;\Gamma&amp;lt;/math&amp;gt;-point wavefunctions but not (typically) k-point wavefunctions (ref: Tinkham).  The question is, can we use our effective supercell concept to apply space-group symmetry operations.  I think the answer is yes.&lt;br /&gt;
&lt;br /&gt;
Consider a point &amp;lt;math&amp;gt;r&amp;lt;/math&amp;gt; and an operation &amp;lt;math&amp;gt;{R|t}&amp;lt;/math&amp;gt;.  (Bold type left out, but take them as vectors and matrices as appropriate.)&lt;br /&gt;
:&amp;lt;math&amp;gt;r&amp;#039;={R|t}&amp;lt;/math&amp;gt;&lt;br /&gt;
Find the equivalent point inside our effective supercell:&lt;br /&gt;
:&amp;lt;math&amp;gt;r&amp;#039;&amp;#039;=r&amp;#039;+L_s={R|t}r&amp;#039;+L_s&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;L_s&amp;lt;/math&amp;gt; is a lattice vector of the effective supercell.&lt;br /&gt;
Finally, we can map this point back into the primitive cell.&lt;br /&gt;
:&amp;lt;math&amp;gt;r&amp;#039;&amp;#039;&amp;#039;={R|t}r+L_s+L_p&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;L_p&amp;lt;/math&amp;gt; is a primitive lattice vector.&lt;br /&gt;
&lt;br /&gt;
Now, consider the effect of a symmetry operation on the i-th wavefunction at the k-th k-point:&lt;br /&gt;
:&amp;lt;math&amp;gt;{R^{-1}|-R^{-1}t}\psi_{k,i}(r)=\psi_{k,i}(r)&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;=\psi_{k,i}(r&amp;#039;)&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;=\psi_{k,i}(r&amp;#039;&amp;#039;)&amp;lt;/math&amp;gt;  due to the long-range periodicity of the wavefunction.&lt;br /&gt;
:&amp;lt;math&amp;gt;=e^{ik.r&amp;#039;&amp;#039;}u_{k,i}(r&amp;#039;&amp;#039;)&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;=e^{ik.(r&amp;#039;&amp;#039;&amp;#039;-L_p)}u_{k,i}(r&amp;#039;&amp;#039;&amp;#039;)&amp;lt;/math&amp;gt;  due to the periodicity of the Bloch function.&lt;br /&gt;
:&amp;lt;math&amp;gt;=e^{-ik.L_p}psi_{k,i}(r&amp;#039;&amp;#039;&amp;#039;)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Haven&amp;#039;t got time to finish typing this now.&lt;/div&gt;</summary>
		<author><name>import&gt;Jss43</name></author>
	</entry>
</feed>