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	<id>https://wiki.iac.isu.edu/index.php?action=history&amp;feed=atom&amp;title=TF_NEUP_2011</id>
	<title>TF NEUP 2011 - 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=TF_NEUP_2011"/>
	<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;action=history"/>
	<updated>2026-05-09T12:54:50Z</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=TF_NEUP_2011&amp;diff=68787&amp;oldid=prev</id>
		<title>Foretony: /* Benefits of Collaboration */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68787&amp;oldid=prev"/>
		<updated>2011-10-27T20:55:44Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Benefits of Collaboration&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;
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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 20:55, 27 October 2011&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-l92&quot; &gt;Line 92:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 92:&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;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;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Some additional accelerator facilities at &lt;/del&gt;Idaho State University include &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;another 25 MeV S-band linac&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;a 12 MeV a Pelletron, a 9.5 MeV&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;10kA pulsed&lt;/del&gt;-&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;power machine, &lt;/del&gt;and &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;a 16 MeV High Repetition Rate Linac. If funded&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;the technical experience involved in constructing and maintaining such &lt;/del&gt;accelerator &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;systems will be brought to bear on this project.&lt;/del&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;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;.&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;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;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Both PNNL and IAC/ISU personnel will be involved &lt;/del&gt;in &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;all aspects of this project. PNNL personnel have particular expertise &lt;/del&gt;and &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;experience in photon tagger development&lt;/del&gt;, and &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;will therefore take &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;lead role on this side &lt;/del&gt;of the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;project. Similarly, &lt;/del&gt;IAC &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;personnel will take the lead role &lt;/del&gt;on &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;the accelerator development side&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;The two collaborating institutions will take equally active roles in &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;supervision and mentoring &lt;/del&gt;of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;graduate students, as well as &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;development &lt;/del&gt;and &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;execution &lt;/del&gt;of the physics &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;program that this facility will enable&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;This will entail frequent visits to each others’ facilities for technical exchanges&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;joint seminars&lt;/del&gt;, and &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;coordinated efforts in the recruiting of students&lt;/del&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;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;The &lt;/ins&gt;Idaho State University &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Department of Physics Strategic Plan identifies the use of experimental nuclear physics techniques as its focus area to addressing problems in both fundamental and applied science. The major efforts of the department &lt;/ins&gt;include &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;fundamental nuclear and particle physics&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;nuclear reactor fuel cycle physics&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;nuclear non&lt;/ins&gt;-&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;proliferation &lt;/ins&gt;and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;homeland security&lt;/ins&gt;, accelerator &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;applications, radiation effects &lt;/ins&gt;in &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;materials &lt;/ins&gt;and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;devices&lt;/ins&gt;, and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;biology. One of the key ingredients to the department's success has been &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;completion &lt;/ins&gt;of the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Idaho Accelerator Center (&lt;/ins&gt;IAC&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;) &lt;/ins&gt;on &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;April 30, 1999. A substantial amount of lab space (4000 sq.~ft&lt;/ins&gt;.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;) within &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;department has become available due to a combination &lt;/ins&gt;of the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;IAC &lt;/ins&gt;and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;a remodeling &lt;/ins&gt;of the physics &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;building. The Physics department has recently added a 400 sq.~ft&lt;/ins&gt;., &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;class 10&lt;/ins&gt;,&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;000 clean room that is current;y being used to build large drift chambers that are about 6 feet high &lt;/ins&gt;and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;contain more than 4500 wires&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 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;The PI has created a Laboratory for Detector Science at Idaho State University which houses the infrastructure for detector development projects. The 1200 sq.~ft. Laboratory is equipped with flow hoods, a darkroom, and a laminar flow hood used to provide a clean room environment sufficient to construct small prototype detectors. A CODA based data acquisition system with ADC, TDC, and scaler VME modules has been installed to record detector performance measurements. The PIs also established a student machine shop containing a mill, a lathe, drill press, table saw, and band which occupies its own space for the physics department to share. These facilities have a history of being used to construct detectors, measure detector prototype performance, and design electronic circuits.&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;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;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;The Idaho State University Department of Physics Strategic Plan identifies the use of experimental nuclear physics techniques as its focus area to addressing problems in both fundamental and applied science. The major efforts of the department include fundamental nuclear and particle physics, nuclear reactor fuel cycle physics, nuclear non-proliferation and homeland security, accelerator applications, radiation effects in materials and devices, and biology. One of the key ingredients to the department's success has been the completion of the Idaho Accelerator Center (IAC) on April 30, 1999. A substantial amount of lab space (4000 sq.~ft.) within the department has become available due to a combination of the IAC and a remodeling of the physics building. A 400 sq.~ft., class 10,000 clean room has been constructed at ISU to build the Region I drift chambers for Hall~B's 12 GeV detector upgrade.&lt;/del&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 Idaho Accelerator Center (IAC) is located less than a mile away from campus and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;can &lt;/ins&gt;provide &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;a computer controlled &lt;/ins&gt;a machining facility for detector construction, an electronics shop for installation of instrumentation, and beamtime for detector performance studies. The IAC houses ten operating accelerators as well as a machine and electronics shop with a permanent staff of 8 Ph.D.s and 6 engineers. Among its many accelerator systems, the Center houses a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;16 MeV &lt;/ins&gt;Linac capable of delivering 20~ns to 2~$\mu$s electron pulses with an instantaneous current of 80 mA up to an energy of 25 MeV at pulse rates up to 1~kHz.  &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Some additional &lt;/ins&gt;accelerator &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;facilities at Idaho State University include another 25 MeV S-band linac, a 12 MeV a Pelletron, &lt;/ins&gt;a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;9.5 MeV, and 10kA pulsed-power machine&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/ins&gt;A full description of the facility is available at the web site (www.iac.isu.edu).&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;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; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&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;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;The PI has created a Laboratory for Detector Science at Idaho State University which houses the infrastructure for detector development projects. The 1200 sq.~ft. Laboratory is equipped with flow hoods, a darkroom, and a laminar flow hood used to provide a clean room environment sufficient to construct small prototype detectors. A CODA based data acquisition system with ADC, TDC, and scaler VME modules has been installed to record detector performance measurements. The PIs also established a student machine shop containing a mill, a lathe, drill press, table saw, and band which occupies its own space for the physics department to share. These facilities has a history of being used to construct detectors, measure detector prototype performance, and design electronic circuits.&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&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; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&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 Idaho Accelerator Center (IAC) is located less than a mile away from campus and &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;will &lt;/del&gt;provide a machining facility for detector construction, an electronics shop for installation of instrumentation, and beamtime for detector performance studies. The IAC houses ten operating accelerators as well as a machine and electronics shop with a permanent staff of 8 Ph.D.s and 6 engineers. Among its many accelerator systems, the Center houses a Linac capable of delivering 20~ns to 2~$\mu$s electron pulses with an instantaneous current of 80 mA up to an energy of 25 MeV at pulse rates up to 1~kHz.  &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;The IAC and JLab are currently constructing an &lt;/del&gt;accelerator &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;to test &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;candidate positron source system for JLab&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;  &lt;/del&gt;A full description of the facility is available at the web site (www.iac.isu.edu).&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&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;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;=Neutron fluxes in reactors=&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;=Neutron fluxes in reactors=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68786&amp;oldid=prev</id>
		<title>Foretony: /* Budget */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68786&amp;oldid=prev"/>
		<updated>2011-10-27T20:11:22Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Budget&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 20:11, 27 October 2011&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-l88&quot; &gt;Line 88:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 88:&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;We request total of $290,000 for a period of three years to defray the costs of this Program Supporting development of an improved fission chamber.&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;We request total of $290,000 for a period of three years to defray the costs of this Program Supporting development of an improved fission chamber.&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;div&gt;The main expense will be for a graduate student ($50k) and some faculty mentor time ($20k) per  year.  Equipment construction and beam time expenses are also requested in the amount of $30k per year.&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 main expense will be for a graduate student ($50k) and some faculty mentor time ($20k) per  year.  Equipment construction and beam time expenses are also requested in the amount of $30k per year.&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;=Benefits of Collaboration=&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;&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;Some additional accelerator facilities at Idaho State University include another 25 MeV S-band linac, a 12 MeV a Pelletron, a 9.5 MeV, 10kA pulsed-power machine, and a 16 MeV High Repetition Rate Linac. If funded, the technical experience involved in constructing and maintaining such accelerator systems will be brought to bear on this project.&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;Both PNNL and IAC/ISU personnel will be involved in all aspects of this project. PNNL personnel have particular expertise and experience in photon tagger development, and will therefore take the lead role on this side of the project. Similarly, IAC personnel will take the lead role on the accelerator development side. The two collaborating institutions will take equally active roles in the supervision and mentoring of graduate students, as well as the development and execution of the physics program that this facility will enable. This will entail frequent visits to each others’ facilities for technical exchanges, joint seminars, and coordinated efforts in the recruiting of students.&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;&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;The Idaho State University Department of Physics Strategic Plan identifies the use of experimental nuclear physics techniques as its focus area to addressing problems in both fundamental and applied science. The major efforts of the department include fundamental nuclear and particle physics, nuclear reactor fuel cycle physics, nuclear non-proliferation and homeland security, accelerator applications, radiation effects in materials and devices, and biology. One of the key ingredients to the department's success has been the completion of the Idaho Accelerator Center (IAC) on April 30, 1999. A substantial amount of lab space (4000 sq.~ft.) within the department has become available due to a combination of the IAC and a remodeling of the physics building. A 400 sq.~ft., class 10,000 clean room has been constructed at ISU to build the Region I drift chambers for Hall~B's 12 GeV detector upgrade.&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;The PI has created a Laboratory for Detector Science at Idaho State University which houses the infrastructure for detector development projects. The 1200 sq.~ft. Laboratory is equipped with flow hoods, a darkroom, and a laminar flow hood used to provide a clean room environment sufficient to construct small prototype detectors. A CODA based data acquisition system with ADC, TDC, and scaler VME modules has been installed to record detector performance measurements. The PIs also established a student machine shop containing a mill, a lathe, drill press, table saw, and band which occupies its own space for the physics department to share. These facilities has a history of being used to construct detectors, measure detector prototype performance, and design electronic circuits.&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;The Idaho Accelerator Center (IAC) is located less than a mile away from campus and will provide a machining facility for detector construction, an electronics shop for installation of instrumentation, and beamtime for detector performance studies. The IAC houses ten operating accelerators as well as a machine and electronics shop with a permanent staff of 8 Ph.D.s and 6 engineers. Among its many accelerator systems, the Center houses a Linac capable of delivering 20~ns to 2~$\mu$s electron pulses with an instantaneous current of 80 mA up to an energy of 25 MeV at pulse rates up to 1~kHz.  The IAC and JLab are currently constructing an accelerator to test a candidate positron source system for JLab.   A full description of the facility is available at the web site (www.iac.isu.edu).&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;=Neutron fluxes in reactors=&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;=Neutron fluxes in reactors=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68785&amp;oldid=prev</id>
		<title>Foretony: /* Budget */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68785&amp;oldid=prev"/>
		<updated>2011-10-27T17:53:46Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Budget&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 17:53, 27 October 2011&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-l87&quot; &gt;Line 87:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 87:&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;=Budget=&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;=Budget=&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;div&gt;We request total of $290,000 for a period of three years to defray the costs of this Program Supporting development of an improved fission chamber.&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;We request total of $290,000 for a period of three years to defray the costs of this Program Supporting development of an improved fission chamber.&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;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 main expense will be for a graduate student ($50k) and some faculty mentor time ($20k) per  year.  &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;equipment &lt;/del&gt;construction and beam time expenses are also requested in the amount of $30k per year.&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 main expense will be for a graduate student ($50k) and some faculty mentor time ($20k) per  year.  &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Equipment &lt;/ins&gt;construction and beam time expenses are also requested in the amount of $30k per year.&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;=Neutron fluxes in reactors=&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;=Neutron fluxes in reactors=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68784&amp;oldid=prev</id>
		<title>Foretony: /* Timeline */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68784&amp;oldid=prev"/>
		<updated>2011-10-27T17:53:22Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Timeline&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 17:53, 27 October 2011&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-l83&quot; &gt;Line 83:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 83:&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;=Timeline=&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;=Timeline=&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;This project spans a three year period.  &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;year &lt;/del&gt;one will be devoted to machining the components of a fission chamber equipped with gas electron multipliers.   Assembly of the detector with a fission target will be completed in year 2.  In the final year, the device will be tested using neutrons generated by the bremstrahlung photons from electrons accelerated by a 16 MeV Linac that impinge on a target of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Deuterated &lt;/del&gt;water.&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;This project spans a three year period.  &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Year &lt;/ins&gt;one will be devoted to machining the components of a fission chamber equipped with gas electron multipliers.   Assembly of the detector with a fission target will be completed in year 2.  In the final year, the device will be tested using neutrons generated by the bremstrahlung photons from electrons accelerated by a 16 MeV Linac that impinge on a target of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;deuterated &lt;/ins&gt;water &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;(HDO)&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;=Budget=&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;=Budget=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68783&amp;oldid=prev</id>
		<title>Foretony: /* Logical pathway to work accomplishments */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68783&amp;oldid=prev"/>
		<updated>2011-10-27T17:52:05Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Logical pathway to work accomplishments&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 17:52, 27 October 2011&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-l76&quot; &gt;Line 76:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 76:&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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 next logical step will be to test the proposed instrument response to neutrons.  The figure below illustrates a neutral particle time of flight measurement using the High Rep Rate Linac facility that is managed by the Idaho Accelerator Center and located at Idaho State University's physics department.  A Tungsten radiation was used in conjuction with a 15 MeV electron beam to  create a photon source from Bremstrahlung radiation.  The emmitted photons entered the experimental cell which held either a water or deuterated water (HDO)  target.  A NaI detector was positioned 2 meters away from the target and at the azimuthal angle of 90 degrees to detect neutral particles.  The hatched peaks in the histrogram represent the NaI detector measurement when using a water target.  The un-hatched histogram shows a clear neutron event enhancement when using the HDO target.  We observed an integrated neutron rate of 50 Hz in the 2 cm x 2 cm NaI detector.&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 next logical step will be to test the proposed instrument response to neutrons.  The figure below illustrates a neutral particle time of flight measurement using the High Rep Rate Linac facility that is managed by the Idaho Accelerator Center and located at Idaho State University's physics department.  A Tungsten radiation was used in conjuction with a 15 MeV electron beam to  create a photon source from Bremstrahlung radiation.  The emmitted photons entered the experimental cell which held either a water or deuterated water (HDO)  target.  A NaI detector was positioned 2 meters away from the target and at the azimuthal angle of 90 degrees to detect neutral particles.  The hatched peaks in the histrogram represent the NaI detector measurement when using a water target.  The un-hatched histogram shows a clear neutron event enhancement when using the HDO target.  We observed an integrated neutron rate of 50 Hz in the 2 cm x 2 cm NaI detector&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;.  We propose using this device to test the temporal performance of a gas electron multiplier equipped fission chamber&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;=Deliverables and outcomes=&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;=Deliverables and outcomes=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68782&amp;oldid=prev</id>
		<title>Foretony: /* Logical pathway to work accomplishments */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68782&amp;oldid=prev"/>
		<updated>2011-10-27T17:50:34Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Logical pathway to work accomplishments&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 17:50, 27 October 2011&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-l76&quot; &gt;Line 76:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 76:&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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 next logical step will be to test the proposed instrument response to neutrons.  The figure below illustrates a neutral particle time of flight measurement using the High Rep Rate Linac facility that is managed by the Idaho Accelerator Center and located at Idaho State University's physics department.  A Tungsten radiation was used in conjuction with a 15 MeV electron beam to  create a photon source from Bremstrahlung radiation.  The emmitted photons entered the experimental cell which held either a water or deuterated water target.  A NaI detector was positioned 2 meters away from the target and at the azimuthal angle of 90 degrees to detect neutral particles.  The hatched peaks in the histrogram represent the NaI detector measurement when using a water target.  The un-hatched histogram shows a clear neutron event enhancement when using &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;a heavy water &lt;/del&gt;target.&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 next logical step will be to test the proposed instrument response to neutrons.  The figure below illustrates a neutral particle time of flight measurement using the High Rep Rate Linac facility that is managed by the Idaho Accelerator Center and located at Idaho State University's physics department.  A Tungsten radiation was used in conjuction with a 15 MeV electron beam to  create a photon source from Bremstrahlung radiation.  The emmitted photons entered the experimental cell which held either a water or deuterated water &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;(HDO)  &lt;/ins&gt;target.  A NaI detector was positioned 2 meters away from the target and at the azimuthal angle of 90 degrees to detect neutral particles.  The hatched peaks in the histrogram represent the NaI detector measurement when using a water target.  The un-hatched histogram shows a clear neutron event enhancement when using &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;the HDO &lt;/ins&gt;target&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;.  We observed an integrated neutron rate of 50 Hz in the 2 cm x 2 cm NaI detector&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;=Deliverables and outcomes=&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;=Deliverables and outcomes=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68781&amp;oldid=prev</id>
		<title>Foretony: /* Logical pathway to work accomplishments */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68781&amp;oldid=prev"/>
		<updated>2011-10-27T17:45:29Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Logical pathway to work accomplishments&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 17:45, 27 October 2011&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-l76&quot; &gt;Line 76:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 76:&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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 next logical step will be to test the proposed instrument response to neutrons.  The figure below illustrates a neutral particle time of flight measurement using the High Rep Rate Linac facility that is managed by the Idaho Accelerator Center and located at Idaho State University's physics department.  A Tungsten radiation was used in conjuction with a 15 MeV electron beam to  create a photon source from Bremstrahlung radiation.  The emmitted photons entered the experimental cell which held either a water or deuterated water target.  A NaI detector was positioned 2 meters away from the target and at the azimuthal angle of 90 degrees to detect neutral particles.  The hatched peaks in the histrogram represent the NaI detector measurement when using a water target.  The&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 next logical step will be to test the proposed instrument response to neutrons.  The figure below illustrates a neutral particle time of flight measurement using the High Rep Rate Linac facility that is managed by the Idaho Accelerator Center and located at Idaho State University's physics department.  A Tungsten radiation was used in conjuction with a 15 MeV electron beam to  create a photon source from Bremstrahlung radiation.  The emmitted photons entered the experimental cell which held either a water or deuterated water target.  A NaI detector was positioned 2 meters away from the target and at the azimuthal angle of 90 degrees to detect neutral particles.  The hatched peaks in the histrogram represent the NaI detector measurement when using a water target.  The &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;un-hatched histogram shows a clear neutron event enhancement when using a heavy water target.&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;=Deliverables and outcomes=&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;=Deliverables and outcomes=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68780&amp;oldid=prev</id>
		<title>Foretony: /* Logical pathway to work accomplishments */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68780&amp;oldid=prev"/>
		<updated>2011-10-27T17:44:46Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Logical pathway to work accomplishments&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 17:44, 27 October 2011&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-l76&quot; &gt;Line 76:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 76:&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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 next logical step will be to test the proposed instrument response to neutrons.  The figure below illustrates a neutral particle time of flight measurement using the High Rep Rate Linac facility that is managed by the Idaho Accelerator Center and located at Idaho State University's physics department.  A Tungsten radiation was used in conjuction with a 15 MeV electron beam to  create a photon source from Bremstrahlung radiation.  The emmitted photons entered the experimental cell which held either a water or deuterated water target.  The&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 next logical step will be to test the proposed instrument response to neutrons.  The figure below illustrates a neutral particle time of flight measurement using the High Rep Rate Linac facility that is managed by the Idaho Accelerator Center and located at Idaho State University's physics department.  A Tungsten radiation was used in conjuction with a 15 MeV electron beam to  create a photon source from Bremstrahlung radiation.  The emmitted photons entered the experimental cell which held either a water or deuterated &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;water target.  A NaI detector was positioned 2 meters away from the target and at the azimuthal angle of 90 degrees to detect neutral particles.  The hatched peaks in the histrogram represent the NaI detector measurement when using a &lt;/ins&gt;water target.  The&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;=Deliverables and outcomes=&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;=Deliverables and outcomes=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68779&amp;oldid=prev</id>
		<title>Foretony: /* Logical pathway to work accomplishments */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68779&amp;oldid=prev"/>
		<updated>2011-10-27T17:42:01Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Logical pathway to work accomplishments&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 17:42, 27 October 2011&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-l76&quot; &gt;Line 76:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 76:&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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 next logical step will be to test the proposed instrument response to 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;The next logical step will be to test the proposed instrument response to neutrons. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; The figure below illustrates a neutral particle time of flight measurement using the High Rep Rate Linac facility that is managed by the Idaho Accelerator Center and located at Idaho State University's physics department.  A Tungsten radiation was used in conjuction with a 15 MeV electron beam to  create a photon source from Bremstrahlung radiation.  The emmitted photons entered the experimental cell which held either a water or deuterated water target.  The&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;=Deliverables and outcomes=&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;=Deliverables and outcomes=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68778&amp;oldid=prev</id>
		<title>Foretony: /* Logical pathway to work accomplishments */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=TF_NEUP_2011&amp;diff=68778&amp;oldid=prev"/>
		<updated>2011-10-27T17:38:08Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Logical pathway to work accomplishments&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 17:38, 27 October 2011&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-l76&quot; &gt;Line 76:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 76:&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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;focus on the construction of a fission chamber with gas electron multiplication pre-amplifiers.  The PI of this proposal has produced several ionization chambers equipped with gas electron multipliers that are constructed from copper clad kapton foils.  A comparison of the output signal from an ionization chamber with the gas electron multiplier pre-amplifier is shown in the figure below along with a typical signal from a drift chamber (geiger muller tube) detector.  The duration of the output pulse is at least a factor of two longer for an ionization chamber which does not use gas electron multiplication.   The output pulse of the gas electron multiplier equipped chamber is also more gaussian like.  THis performance occurs because the ionization region within the detector can be reduced in size using the preamplifiers.  The ionized particle in the chamber have a shorter drift distance and result in a faster output signal response.  The objective in this proposal will be to add a fissionable material to an ionization chamber making it neutron sensitive.&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 &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;testing of a&lt;/del&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 &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;next logical step will be to test the proposed instrument response to neutrons.&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;=Deliverables and outcomes=&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;=Deliverables and outcomes=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Foretony</name></author>
	</entry>
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