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	<title>Simulation Project tripleaxis: The resolution function - Revision history</title>
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	<updated>2026-04-23T13:37:23Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<title>Wikiadmin: 1 revision imported</title>
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		<updated>2020-02-18T22:15:14Z</updated>

		<summary type="html">&lt;p&gt;1 revision imported&lt;/p&gt;
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		<id>https://e-learning.pan-training.eu/wiki/index.php?title=Simulation_Project_tripleaxis:_The_resolution_function&amp;diff=1142&amp;oldid=prev</id>
		<title>ucph&gt;Tommy: Created page with &quot;You may have noticed that your two phonon peaks are not identical, e.g. for 2.0 meV. The reason for this is hidden in the &quot;resolution function&quot;, which is a measure of the prec...&quot;</title>
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		<updated>2019-07-14T21:44:50Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;You may have noticed that your two phonon peaks are not identical, e.g. for 2.0 meV. The reason for this is hidden in the &amp;quot;resolution function&amp;quot;, which is a measure of the prec...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;You may have noticed that your two phonon peaks are not identical, e.g. for 2.0 meV. The reason for this is hidden in the &amp;quot;resolution function&amp;quot;, which is a measure of the precision of the spectrometer. In more precise terms, it is the distribution \(\hbar \omega\) and \(q\) of the scattered neutrons that actually hit the detector for one particular setting. The &amp;quot;resolution ellipse&amp;quot; is the contour in \((\hbar \omega, q)\)-space, where the transmission has fallen to half the value of the nominal point.&lt;br /&gt;
&lt;br /&gt;
In experiments, the resolution function at \(\hbar \omega = 0\) can be measured by e.g. elastic scattering from single crystals, but direct measurements of the inelastic resolution function cannot be performed. Often, the resolution is calculated from the analytical Popovici approximation, by means of the program RESCAL&amp;lt;ref name=&amp;quot;RESCAL&amp;quot;&amp;gt;See http://xray.physics.ox.ac.uk/rescal/rescal.htm&amp;lt;/ref&amp;gt;&amp;lt;!--\cite{RESCAL}--&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
The resolution function may, however, be calculated by McStas. Replace your sample by component &amp;lt;tt&amp;gt;res_sample&amp;lt;/tt&amp;gt; and replace your detector by &amp;lt;tt&amp;gt;res_monitor&amp;lt;/tt&amp;gt;. The sample then scatteres neutrons inelastically into a focusing direction and energy interval determined by you, and the monitor records the values of \(\hbar \omega\) and \(q\) of the neutrons that hits. After the simulation, the outcome can be shown with the McStas tool &amp;lt;tt&amp;gt;mcresplot&amp;lt;/tt&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Determine your resolution function at both 2.0 meV inelastic peaks and discuss why the peak shapes and peak intensities were not equal.&lt;br /&gt;
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&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>ucph&gt;Tommy</name></author>
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