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	<id>https://wiki.iac.isu.edu/index.php?action=history&amp;feed=atom&amp;title=Relative_efficiency</id>
	<title>Relative efficiency - Revision history</title>
	<link rel="self" type="application/atom+xml" href="https://wiki.iac.isu.edu/index.php?action=history&amp;feed=atom&amp;title=Relative_efficiency"/>
	<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;action=history"/>
	<updated>2026-05-09T06:59:29Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
	<generator>MediaWiki 1.35.2</generator>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94975&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94975&amp;oldid=prev"/>
		<updated>2014-09-22T15:33:09Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&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 15:33, 22 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l327&quot; &gt;Line 327:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 327:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{\bar{n}^n  e^{-\bar{n}}}{n!}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{\bar{n}^n  e^{-\bar{n}&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;}}{n!}=\frac{(2.5)^ne^{-2.5&lt;/ins&gt;}}{n!}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94974&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94974&amp;oldid=prev"/>
		<updated>2014-09-22T15:32:09Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&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 15:32, 22 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l327&quot; &gt;Line 327:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 327:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{\bar{n}^n  e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{\bar{n}^n  e^{-&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;\bar{&lt;/ins&gt;n&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;}&lt;/ins&gt;}}{&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;n!&lt;/ins&gt;}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94973&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94973&amp;oldid=prev"/>
		<updated>2014-09-22T15:31:46Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&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 15:31, 22 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l327&quot; &gt;Line 327:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 327:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{\&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;=&lt;/del&gt;{n}^n  e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{\&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;bar&lt;/ins&gt;{n}^n  e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94970&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94970&amp;oldid=prev"/>
		<updated>2014-09-22T15:30:43Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&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 15:30, 22 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l327&quot; &gt;Line 327:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 327:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{n^n  e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;{\=&lt;/ins&gt;{n&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;}&lt;/ins&gt;^n  e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94969&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94969&amp;oldid=prev"/>
		<updated>2014-09-22T15:30:31Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&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 15:30, 22 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l327&quot; &gt;Line 327:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 327:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;{\=&lt;/del&gt;{n&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;}&lt;/del&gt;^n &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;\cdot &lt;/del&gt;e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{n^n &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/ins&gt;e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94968&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94968&amp;oldid=prev"/>
		<updated>2014-09-22T15:30:11Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&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 15:30, 22 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l327&quot; &gt;Line 327:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 327:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{n^n \&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;cdpt &lt;/del&gt;e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;{\=&lt;/ins&gt;{n&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;}&lt;/ins&gt;^n \&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;cdot &lt;/ins&gt;e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94967&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94967&amp;oldid=prev"/>
		<updated>2014-09-22T15:29:47Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&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 15:29, 22 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l327&quot; &gt;Line 327:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 327:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;{\=&lt;/del&gt;{n&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;}&lt;/del&gt;^n \cdpt e^{-&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;\={&lt;/del&gt;n&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;}&lt;/del&gt;}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Poisson distribution &amp;lt;math&amp;gt;P(n)=\frac{n^n \cdpt e^{-n}}{}&amp;lt;/math&amp;gt; of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94966&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94966&amp;oldid=prev"/>
		<updated>2014-09-22T15:29:27Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&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 15:29, 22 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l327&quot; &gt;Line 327:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 327:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Poisson distribution of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Poisson distribution &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;lt;math&amp;gt;P(n)=\frac{\={n}^n \cdpt e^{-\={n}}}{}&amp;lt;/math&amp;gt; &lt;/ins&gt;of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;[[File:poisson_2_5n_ave.png | 500px]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94964&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94964&amp;oldid=prev"/>
		<updated>2014-09-22T15:27:05Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&quot; data-mw=&quot;interface&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 15:27, 22 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l327&quot; &gt;Line 327:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 327:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt;  and calculated yield of uncorrelated neutrons per pulse &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&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;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Poisson distribution of the number of fission neutrons per fission event if the average number of neutrons emitted in fission event is 2.5 neutrons.&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&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;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&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;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[File:poisson_2_5n_ave.png | 500px]]&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;'''Bin-by-bin subtraction'''&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;'''Bin-by-bin subtraction'''&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94786&amp;oldid=prev</id>
		<title>Kosiolek: /* The ratio of the integrated yields */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Relative_efficiency&amp;diff=94786&amp;oldid=prev"/>
		<updated>2014-09-15T14:12:58Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;The ratio of the integrated yields&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&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 14:12, 15 September 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l325&quot; &gt;Line 325:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 325:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;==The ratio of the integrated yields==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;==The ratio of the integrated yields==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt; &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;per pulse &lt;/del&gt;and calculated yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;per pulse &lt;/del&gt;gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;The ratio of the normalized integrated yields of correlated + uncorrelated neutrons &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;per pulse &lt;/ins&gt;&amp;lt;math&amp;gt;Y^{\text{tot}}=2.2E-5&amp;lt;/math&amp;gt; &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/ins&gt;and calculated yield of uncorrelated neutrons &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;per pulse &lt;/ins&gt;&amp;lt;math&amp;gt;Y^{\text{2n/fisson}}=6.49E-6&amp;lt;/math&amp;gt; gives the following number &amp;lt;math&amp;gt;\frac{Y^{\text{tot}}}{Y^{\text{2 fisson}}}=3.4&amp;lt;/math&amp;gt;. If we want to get the ratio of pure yield of correlated neutrons &amp;lt;math&amp;gt;Y^{\text{1n/fission}}&amp;lt;/math&amp;gt; over the yield of uncorrelated neutrons &amp;lt;math&amp;gt;Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; we should take the difference &amp;lt;math&amp;gt;Y^{\text{1n/fission}}=Y^{\text{tot}}-Y^{\text{2n/fisson}}&amp;lt;/math&amp;gt; and then take the ratio &amp;lt;math&amp;gt;\frac{Y^{\text{1n/fission}}}{Y^{\text{2n/fisson}}} = \frac{(2.2E-5)-(6.49E-6)}{6.49E-6}=2.4&amp;lt;/math&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kosiolek</name></author>
	</entry>
</feed>