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	<updated>2026-11-10T20:08:03Z</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 class=&quot;autocomment&quot;&gt;Abstract&lt;/span&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&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 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=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&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; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&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; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&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; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&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;

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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=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 class=&quot;autocomment&quot;&gt;Abstract&lt;/span&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&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 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=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&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;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&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 style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Laboratories is &lt;/del&gt;a &lt;del style=&quot;font-weight: bold; text-decoration: none;&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 style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;itself contains many sensors &lt;/del&gt;that &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;provide crucial information such as position, time of flight, etc&lt;/del&gt;. &lt;del style=&quot;font-weight: bold; text-decoration: none;&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 style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;and is used to determine cylindrical position of charged particles using a &lt;/del&gt;Gas Electron Multiplication (GEM) &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;technique via Micro-Pattern Gas Detector (MPGD) technology&lt;/del&gt;. The &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;multiplied &lt;/del&gt;charge &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;from &lt;/del&gt;these &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;very precise detectors &lt;/del&gt;is &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;discriminated from thin&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;individual, parallel conductive lines&lt;/del&gt;, which &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;are subsequently processed and collected into serialized packets using customized &lt;/del&gt;integrated &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;circuits&lt;/del&gt;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&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 style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;cylindrical &lt;/del&gt;position of particles passing through the detector.  &lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&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 style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Lab will make &lt;/ins&gt;a precision measurement of &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;the weak mixing angle using &lt;/ins&gt;parity-violating electron scattering &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;from the proton&lt;/ins&gt;. The Q-weak apparatus &lt;ins style=&quot;font-weight: bold; text-decoration: none;&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 style=&quot;font-weight: bold; text-decoration: none;&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 style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;in this tracking system.  The R1 detector uses &lt;/ins&gt;Gas Electron Multiplication (GEM) &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;to amplify the ionization signal generated by scattered electrons traveling through the detector&lt;/ins&gt;. The &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;resulting cloud of &lt;/ins&gt;charge &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;generated by &lt;/ins&gt;these &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;preamplifiers &lt;/ins&gt;is &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;directed&lt;/ins&gt;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;by and external electric field&lt;/ins&gt;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;towards a charge collector &lt;/ins&gt;which &lt;ins style=&quot;font-weight: bold; text-decoration: none;&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 style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;circuit&lt;/ins&gt;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;design at &lt;/ins&gt;CERN for the TOTEM experiment&lt;ins style=&quot;font-weight: bold; text-decoration: none;&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 style=&quot;font-weight: bold; text-decoration: none;&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=&quot;diff-marker&quot; data-marker=&quot;−&quot;&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; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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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		<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 class=&quot;autocomment&quot;&gt;Abstract&lt;/span&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&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;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;
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&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&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;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&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 style=&quot;font-weight: bold; text-decoration: none;&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=&quot;diff-marker&quot; data-marker=&quot;+&quot;&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 style=&quot;font-weight: bold; text-decoration: none;&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=&quot;diff-marker&quot;&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;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&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;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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=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 class=&quot;autocomment&quot;&gt;Abstract&lt;/span&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
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				&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=&quot;diff-marker&quot;&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;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&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;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&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=&quot;diff-marker&quot;&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=&quot;diff-marker&quot;&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:1.41:old-49699:rev-49700:php=table --&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 &#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...&#039;</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>