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	<updated>2026-05-09T01:44:23Z</updated>
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	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49703&amp;oldid=prev</id>
		<title>Oborn: /* Abstract */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49703&amp;oldid=prev"/>
		<updated>2010-04-12T22:33:06Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Abstract&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;
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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 22:33, 12 April 2010&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-l3&quot; &gt;Line 3:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 3:&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 Q-weak experiment at Jefferson Lab will make a precision measurement of the weak mixing angle using parity-violating electron scattering from the proton. The Q-weak apparatus will use a tracking system to measure the electron elastic scattering profile using a set of detectors that are separate from the main detector systems. The Region 1 detector of the Q-weak experiment is the first detector encountered by scattered particles in this tracking system.  The R1 detector uses Gas Electron Multiplication (GEM) to amplify the ionization signal generated by scattered electrons traveling through the detector. The resulting cloud of charge generated by these preamplifiers is directed, by and external electric field, towards a charge collector which allows a determination of the location of the charge deposited on the charge collector.  A signal processing integrated circuit, design at CERN for the TOTEM experiment, amplifies and discriminates the analog charge deposited on the charge collector converting it into a digital yes/no hit signal.  This serialized data is then transferred to permanent data files. Once in this form, these files can then later be parsed to determine position of particles passing through the detector.  &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 Q-weak experiment at Jefferson Lab will make a precision measurement of the weak mixing angle using parity-violating electron scattering from the proton. The Q-weak apparatus will use a tracking system to measure the electron elastic scattering profile using a set of detectors that are separate from the main detector systems. The Region 1 detector of the Q-weak experiment is the first detector encountered by scattered particles in this tracking system.  The R1 detector uses Gas Electron Multiplication (GEM) to amplify the ionization signal generated by scattered electrons traveling through the detector. The resulting cloud of charge generated by these preamplifiers is directed, by and external electric field, towards a charge collector which allows a determination of the location of the charge deposited on the charge collector.  A signal processing integrated circuit, design at CERN for the TOTEM experiment, amplifies and discriminates the analog charge deposited on the charge collector converting it into a digital yes/no hit signal.  This serialized data is then transferred to permanent data files. Once in this form, these files can then later be parsed to determine position of particles passing through the detector.  &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 focus of this thesis is on the process of querying the VFAT2 ICs on the GEM detectors, collecting all of the simultaneous data packets from the VFATs into one large data file using an FPGA (Field Programmable Gate Array), and then transferring this large data file to a Linux-based computer for future parsing.&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 focus of this thesis is on the process of querying the VFAT2 ICs on the GEM detectors, collecting all of the simultaneous data packets from the VFATs into one large data file using an FPGA (Field Programmable Gate Array), and then transferring this large data file to a Linux-based computer for future parsing.&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;&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;[[Warren_Parsons_MS_Thesis]]&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;

&lt;!-- diff cache key iacwikidb-iacwiki_:diff::1.12:old-49702:rev-49703 --&gt;
&lt;/table&gt;</summary>
		<author><name>Oborn</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49702&amp;oldid=prev</id>
		<title>Oborn: /* Abstract */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49702&amp;oldid=prev"/>
		<updated>2010-04-12T22:30:43Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Abstract&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 22:30, 12 April 2010&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-l1&quot; &gt;Line 1:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&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;=Abstract=&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;=Abstract=&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 Q-weak experiment at Jefferson &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Laboratories is &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;multi-collegiate effort to determine weak charges of quarks through &lt;/del&gt;precision measurement of parity-violating electron scattering. The Q-weak apparatus &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;itself contains many sensors &lt;/del&gt;that &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;provide crucial information such as position, time of flight, etc&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;of scattered particles &lt;/del&gt;The Region 1 detector of the Q-weak experiment is the first detector encountered by scattered particles &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;and is used to determine cylindrical position of charged particles using a &lt;/del&gt;Gas Electron Multiplication (GEM) &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;technique via Micro-Pattern Gas Detector (MPGD) technology&lt;/del&gt;. The &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;multiplied &lt;/del&gt;charge &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;from &lt;/del&gt;these &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;very precise detectors &lt;/del&gt;is &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;discriminated from thin&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;individual, parallel conductive lines&lt;/del&gt;, which &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;are subsequently processed and collected into serialized packets using customized &lt;/del&gt;integrated &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;circuits&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;e.g. VFAT2, created and used by &lt;/del&gt;CERN for the TOTEM experiment. This serialized data is then transferred to permanent data files. Once in this form, these files can then later be parsed to determine &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;cylindrical &lt;/del&gt;position of particles passing through the 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 Q-weak experiment at Jefferson &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Lab will make &lt;/ins&gt;a precision measurement of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;the weak mixing angle using &lt;/ins&gt;parity-violating electron scattering &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;from the proton&lt;/ins&gt;. The Q-weak apparatus &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;will use a tracking system to measure the electron elastic scattering profile using a set of detectors &lt;/ins&gt;that &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;are separate from the main detector systems&lt;/ins&gt;. The Region 1 detector of the Q-weak experiment is the first detector encountered by scattered particles &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;in this tracking system.  The R1 detector uses &lt;/ins&gt;Gas Electron Multiplication (GEM) &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;to amplify the ionization signal generated by scattered electrons traveling through the detector&lt;/ins&gt;. The &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;resulting cloud of &lt;/ins&gt;charge &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;generated by &lt;/ins&gt;these &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;preamplifiers &lt;/ins&gt;is &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;directed&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;by and external electric field&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;towards a charge collector &lt;/ins&gt;which &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;allows a determination of the location of the charge deposited on the charge collector.  A signal processing &lt;/ins&gt;integrated &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;circuit&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;design at &lt;/ins&gt;CERN for the TOTEM experiment&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;, amplifies and discriminates the analog charge deposited on the charge collector converting it into a digital yes/no hit signal&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/ins&gt;This serialized data is then transferred to permanent data files. Once in this form, these files can then later be parsed to determine position of particles passing through the detector.  &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;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 focus of this thesis is on the process of querying the VFAT2 ICs on the GEM detectors, collecting all of the simultaneous data packets from the VFATs into one large data file using an FPGA (Field Programmable Gate Array), and then transferring this large data file to a Linux-based computer for future parsing.&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 focus of this thesis is on the process of querying the VFAT2 ICs on the GEM detectors, collecting all of the simultaneous data packets from the VFATs into one large data file using an FPGA (Field Programmable Gate Array), and then transferring this large data file to a Linux-based computer for future parsing.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;

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&lt;/table&gt;</summary>
		<author><name>Oborn</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49701&amp;oldid=prev</id>
		<title>Oborn: /* Abstract */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49701&amp;oldid=prev"/>
		<updated>2010-03-27T19:25:23Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Abstract&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 19:25, 27 March 2010&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-l1&quot; &gt;Line 1:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&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;=Abstract=&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;=Abstract=&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 Q-weak experiment at Jefferson Laboratories is a multi-collegiate effort to determine weak charges of quarks through precision measurement of parity-violating electron scattering. The Q-weak apparatus itself contains many sensors that provide crucial information such as position, time of flight, etc. of scattered particles The Region 1 detector of the Q-weak experiment is the first detector encountered by scattered particles and is used to determine cylindrical position of charged particles using a Gas Electron Multiplication (GEM) technique via Micro-Pattern Gas Detector (MPGD) technology. The multiplied charge from these very precise detectors is discriminated from thin, individual, parallel conductive lines, processed&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;, &lt;/del&gt;and collected into serialized packets using customized integrated circuits, e.g. VFAT2, created and used by CERN for the TOTEM experiment. This serialized data is then transferred to permanent data files. Once in this form, these files can then later be parsed to determine cylindrical position of particles passing through the 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 Q-weak experiment at Jefferson Laboratories is a multi-collegiate effort to determine weak charges of quarks through precision measurement of parity-violating electron scattering. The Q-weak apparatus itself contains many sensors that provide crucial information such as position, time of flight, etc. of scattered particles The Region 1 detector of the Q-weak experiment is the first detector encountered by scattered particles and is used to determine cylindrical position of charged particles using a Gas Electron Multiplication (GEM) technique via Micro-Pattern Gas Detector (MPGD) technology. The multiplied charge from these very precise detectors is discriminated from thin, individual, parallel conductive lines, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;which are subsequently &lt;/ins&gt;processed and collected into serialized packets using customized integrated circuits, e.g. VFAT2, created and used by CERN for the TOTEM experiment. This serialized data is then transferred to permanent data files. Once in this form, these files can then later be parsed to determine cylindrical position of particles passing through the detector.  &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;The focus of this thesis is on the process of querying the VFAT2 ICs on the GEM detectors, collecting all of the simultaneous data packets from the VFATs into one large data file using an FPGA (Field Programmable Gate Array), and then transferring this large data file to a Linux-based computer for future parsing.&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 focus of this thesis is on the process of querying the VFAT2 ICs on the GEM detectors, collecting all of the simultaneous data packets from the VFATs into one large data file using an FPGA (Field Programmable Gate Array), and then transferring this large data file to a Linux-based computer for future parsing.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;

&lt;!-- diff cache key iacwikidb-iacwiki_:diff::1.12:old-49700:rev-49701 --&gt;
&lt;/table&gt;</summary>
		<author><name>Oborn</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49700&amp;oldid=prev</id>
		<title>Oborn: /* Abstract */</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49700&amp;oldid=prev"/>
		<updated>2010-03-27T04:10:45Z</updated>

		<summary type="html">&lt;p&gt;&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Abstract&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 04:10, 27 March 2010&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-l2&quot; &gt;Line 2:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 2:&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;The Q-weak experiment at Jefferson Laboratories is a multi-collegiate effort to determine weak charges of quarks through precision measurement of parity-violating electron scattering. The Q-weak apparatus itself contains many sensors that provide crucial information such as position, time of flight, etc. of scattered particles The Region 1 detector of the Q-weak experiment is the first detector encountered by scattered particles and is used to determine cylindrical position of charged particles using a Gas Electron Multiplication (GEM) technique via Micro-Pattern Gas Detector (MPGD) technology. The multiplied charge from these very precise detectors is discriminated from thin, individual, parallel conductive lines, processed, and collected into serialized packets using customized integrated circuits, e.g. VFAT2, created and used by CERN for the TOTEM experiment. This serialized data is then transferred to permanent data files. Once in this form, these files can then later be parsed to determine cylindrical position of particles passing through the detector.  &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 Q-weak experiment at Jefferson Laboratories is a multi-collegiate effort to determine weak charges of quarks through precision measurement of parity-violating electron scattering. The Q-weak apparatus itself contains many sensors that provide crucial information such as position, time of flight, etc. of scattered particles The Region 1 detector of the Q-weak experiment is the first detector encountered by scattered particles and is used to determine cylindrical position of charged particles using a Gas Electron Multiplication (GEM) technique via Micro-Pattern Gas Detector (MPGD) technology. The multiplied charge from these very precise detectors is discriminated from thin, individual, parallel conductive lines, processed, and collected into serialized packets using customized integrated circuits, e.g. VFAT2, created and used by CERN for the TOTEM experiment. This serialized data is then transferred to permanent data files. Once in this form, these files can then later be parsed to determine cylindrical position of particles passing through the detector.  &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 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 focus of this thesis is on the process of querying the VFAT2 ICs on the GEM detectors, collecting all of the simultaneous data packets from the VFATs into one large data file using an FPGA (Field Programmable Gate Array), and then transferring this large data file to a Linux-based computer for future parsing.&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 focus of this thesis is on the process of querying the VFAT2 ICs on the GEM detectors, collecting all of the simultaneous data packets from the VFATs into one large data file using an FPGA (Field Programmable Gate Array), and then transferring this large data file to a Linux-based computer for future parsing.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;

&lt;!-- diff cache key iacwikidb-iacwiki_:diff::1.12:old-49699:rev-49700 --&gt;
&lt;/table&gt;</summary>
		<author><name>Oborn</name></author>
	</entry>
	<entry>
		<id>https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49699&amp;oldid=prev</id>
		<title>Oborn: Created page with '=Abstract=  The Q-weak experiment at Jefferson Laboratories is a multi-collegiate effort to determine weak charges of quarks through precision measurement of parity-violating ele...'</title>
		<link rel="alternate" type="text/html" href="https://wiki.iac.isu.edu/index.php?title=Abstract&amp;diff=49699&amp;oldid=prev"/>
		<updated>2010-03-27T04:10:33Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;#039;=Abstract=  The Q-weak experiment at Jefferson Laboratories is a multi-collegiate effort to determine weak charges of quarks through precision measurement of parity-violating ele...&amp;#039;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;=Abstract=&lt;br /&gt;
&lt;br /&gt;
The Q-weak experiment at Jefferson Laboratories is a multi-collegiate effort to determine weak charges of quarks through precision measurement of parity-violating electron scattering. The Q-weak apparatus itself contains many sensors that provide crucial information such as position, time of flight, etc. of scattered particles The Region 1 detector of the Q-weak experiment is the first detector encountered by scattered particles and is used to determine cylindrical position of charged particles using a Gas Electron Multiplication (GEM) technique via Micro-Pattern Gas Detector (MPGD) technology. The multiplied charge from these very precise detectors is discriminated from thin, individual, parallel conductive lines, processed, and collected into serialized packets using customized integrated circuits, e.g. VFAT2, created and used by CERN for the TOTEM experiment. This serialized data is then transferred to permanent data files. Once in this form, these files can then later be parsed to determine cylindrical position of particles passing through the detector. &lt;br /&gt;
The focus of this thesis is on the process of querying the VFAT2 ICs on the GEM detectors, collecting all of the simultaneous data packets from the VFATs into one large data file using an FPGA (Field Programmable Gate Array), and then transferring this large data file to a Linux-based computer for future parsing.&lt;/div&gt;</summary>
		<author><name>Oborn</name></author>
	</entry>
</feed>