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	<title>Problem:Scattering from an antiferromagnet - Revision history</title>
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	<updated>2026-05-15T13:06:02Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<title>Wikiadmin: Wikiadmin moved page Problem: Scattering from an antiferromagnet to Problem:Scattering from an antiferromagnet</title>
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		<updated>2020-09-20T15:44:19Z</updated>

		<summary type="html">&lt;p&gt;Wikiadmin moved page &lt;a href=&quot;/wiki/Problem:_Scattering_from_an_antiferromagnet&quot; class=&quot;mw-redirect&quot; title=&quot;Problem: Scattering from an antiferromagnet&quot;&gt;Problem: Scattering from an antiferromagnet&lt;/a&gt; to &lt;a href=&quot;/wiki/Problem:Scattering_from_an_antiferromagnet&quot; title=&quot;Problem:Scattering from an antiferromagnet&quot;&gt;Problem:Scattering from an antiferromagnet&lt;/a&gt;&lt;/p&gt;
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		<author><name>Wikiadmin</name></author>
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		<id>https://e-learning.pan-training.eu/wiki/index.php?title=Problem:Scattering_from_an_antiferromagnet&amp;diff=1020&amp;oldid=prev</id>
		<title>ucph&gt;Tommy at 18:42, 4 September 2019</title>
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		<updated>2019-09-04T18:42:34Z</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;&amp;lt;!--\label{prob:2DAFM_scatt}--&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This problem is a simple illustration of magnetic diffraction,&lt;br /&gt;
as calculated in section [[Magnetic diffraction]].&lt;br /&gt;
&lt;br /&gt;
We consider the two-dimensional square lattice with lattice constant \(d\) and antiferromagnetic interactions&lt;br /&gt;
between nearest neighbours.&lt;br /&gt;
&lt;br /&gt;
In the previous problem, we showed that this system is antiferromagnetic &lt;br /&gt;
with alternating spin directions between nearest neighbours, as illustrated in [[Elastic_magnetic_scattering#label-fig:magnetic_structures|this figure (middle)]] from the [[Elastic magnetic scattering]] page&amp;lt;!--(\ref{fig:magnetic_scattering})--&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
=====Question 1=====&lt;br /&gt;
Argue that the square 4-atom cell with side length \(2 d\) is a valid magnetic unit cell for the system&lt;br /&gt;
and that the reciprocal lattice then becomes a square lattice with side length \(\pi/d\).&lt;br /&gt;
&lt;br /&gt;
=====Question 2=====&lt;br /&gt;
We define as usual the reciprocal lattice coordinates, \((h,k)\), in terms of the nuclear &lt;br /&gt;
reciprocal lattice vectors, \(|{\bf a}^*| = |{\bf b}^*| = 2 \pi/d\). Show that the points of the 4-atom &lt;br /&gt;
magnetic reciprocal lattice can be reached by integer and half-integer values of \(h\) and \(k\).&lt;br /&gt;
&lt;br /&gt;
=====Question 3=====&lt;br /&gt;
In the nuclear Brillouin zone, there are 4 different magnetic reciprocal lattice points: &lt;br /&gt;
\((0,0)\), \((0,1/2)\), \((1/2,0)\), and \((1/2, 1/2)\). Calculate the magnetic scattering structure factor&lt;br /&gt;
for these 4 reflections when the spins are all pointing out of the plane (the \(l\)-direction). Draw a map&lt;br /&gt;
of \(q\)-space, showing the allowed nuclear and magnetic reflections, respectively.&lt;br /&gt;
&lt;br /&gt;
=====Question 4=====&lt;br /&gt;
Compare to the value of the ordering \(Q\)-vector, \({\bf Q} = (1/2 1/2)\), found in the previous problem.&lt;/div&gt;</summary>
		<author><name>ucph&gt;Tommy</name></author>
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