Qweak.QweakIntro History
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March 05, 2011, at 12:31 PM
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The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see Figure above). We continue to now put much of our effort into installation and commissioning, as well as data analysis and DAQ setup related programming. \\
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The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see slide show above). Our team of students, postdocs, and faculty have worked hard during the installation and commissioning period and we continue to now put much of our effort into data analysis and related programming efforts. \\
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The experiment is scheduled to begin production running in the Fall of 2010. \\
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The experiment began production running in the Fall of 2010 and is expected to reach its goal statistical error in May 2012. \\
March 05, 2011, at 12:26 PM
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakPhysics | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=410px height=308px%Attach:ExpStatusSlideShowNonStopCycle.swf \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakPhysics | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently taking data in Hall C at Jefferson Laboratory. ||%width=410px height=308px%Attach:ExpStatusSlideShowNonStopCycle.swf \\
September 08, 2010, at 08:43 AM
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The experiment is scheduled to being production running in the Fall of 2010. \\
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The experiment is scheduled to begin production running in the Fall of 2010. \\
June 24, 2010, at 11:55 AM
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=410px height=308px%Attach:ExpStatusSlideShowNonStopCycle.swf \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakPhysics | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=410px height=308px%Attach:ExpStatusSlideShowNonStopCycle.swf \\
April 02, 2010, at 07:47 PM
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=267px height=200px%Attach:ExpStatusSlideShowNonStopCycle.swf \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=410px height=308px%Attach:ExpStatusSlideShowNonStopCycle.swf \\
April 02, 2010, at 07:44 PM
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=300px height=300px%Attach:ExpStatusSlideShow.swf \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=267px height=200px%Attach:ExpStatusSlideShowNonStopCycle.swf \\
March 03, 2010, at 09:38 PM
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=350px height=350px%Attach:ExpStatusSlideShow.swf \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=300px height=300px%Attach:ExpStatusSlideShow.swf \\
March 03, 2010, at 09:38 PM
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March 03, 2010, at 09:37 PM
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%rfloat width=350px height=350px%Attach:ExpStatusSlideShow.swf \\
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%rfloat width=350px height=350px%Attach:ExpStatusSlideShow.swf \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=350px height=350px%Attach:ExpStatusSlideShow.swf \\
March 03, 2010, at 09:35 PM
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%rfloat width=200px height=200px%Attach:ExpStatusSlideShow.swf \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%rfloat width=350px height=350px%Attach:ExpStatusSlideShow.swf \\
March 03, 2010, at 07:03 PM
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=200px height=200px%Attach:ExpStatusSlideShow.swf \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%rfloat width=200px height=200px%Attach:ExpStatusSlideShow.swf \\
March 03, 2010, at 07:02 PM
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=300px height=300px%Attach:ExpStatusSlideShow.swf \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=200px height=200px%Attach:ExpStatusSlideShow.swf \\
March 03, 2010, at 07:02 PM
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=300px height=300px% Attach:ExpStatusSlideShow.swf \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=300px height=300px%Attach:ExpStatusSlideShow.swf \\
March 03, 2010, at 07:00 PM
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see Figure above). ||%width=300px height=300px% Attach:ExpStatusSlideShow.swf \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. ||%width=300px height=300px% Attach:ExpStatusSlideShow.swf \\
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We continue to now put much of our effort into installation and commissioning, as well as data analysis and DAQ setup related programming. \\
to:
The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see Figure above). We continue to now put much of our effort into installation and commissioning, as well as data analysis and DAQ setup related programming. \\
March 03, 2010, at 06:59 PM
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see Figure above). ||%width=350px height=350px% Attach:ExpStatusSlideShow.swf \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see Figure above). ||%width=300px height=300px% Attach:ExpStatusSlideShow.swf \\
March 03, 2010, at 06:58 PM
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=350px height=350px% Attach:ExpStatusSlideShow.swf \\
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see Figure above). \\
Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see Figure above). \\
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see Figure above). ||%width=350px height=350px% Attach:ExpStatusSlideShow.swf \\
March 03, 2010, at 06:56 PM
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%rfloat text-align=center width=350px height=350px% Attach:ExpStatusSlideShow.swf \\
Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. \\
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=350px height=350px% Attach:ExpStatusSlideShow.swf \\
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March 03, 2010, at 06:50 PM
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%rfloat text-align=center width=350px height=350px% Attach:ExpStatusSlideShow.swf \\ Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
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%rfloat text-align=center width=350px height=350px% Attach:ExpStatusSlideShow.swf \\
Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
March 03, 2010, at 06:50 PM
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%rfloat text-align=center width=350px height=350px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''\\
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Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
\\
Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
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%rfloat text-align=center width=350px height=350px% Attach:ExpStatusSlideShow.swf \\ Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
March 03, 2010, at 06:49 PM
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%rfloat text-align=center width=400px height=400px% Attach:ExpStatusSlideShow.swf |'''Hall C Installation Progress'''
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%rfloat text-align=center width=350px height=350px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''\\
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March 03, 2010, at 06:47 PM
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%rfloat text-align=center width=400px height=400px% Attach:ExpStatusSlideShow.swf| '''Hall C Installation Progress'''
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%rfloat text-align=center width=400px height=400px% Attach:ExpStatusSlideShow.swf |'''Hall C Installation Progress'''
March 03, 2010, at 06:45 PM
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%rfloat text-align=center width=400px height=400px% Attach:ExpStatusSlideShow.swf|'''Hall C Installation Progress'''
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%rfloat text-align=center width=400px height=400px% Attach:ExpStatusSlideShow.swf| '''Hall C Installation Progress'''
March 03, 2010, at 06:45 PM
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%rfloat text-align=center width=400px height=400px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''
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%rfloat text-align=center width=400px height=400px% Attach:ExpStatusSlideShow.swf|'''Hall C Installation Progress'''
March 03, 2010, at 03:55 PM
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%rfloat text-align=center width=550px height=550px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''
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%rfloat text-align=center width=400px height=400px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''
March 03, 2010, at 03:54 PM
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%rfloat text-align=center width=550px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''
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%rfloat text-align=center width=550px height=550px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''
March 03, 2010, at 03:52 PM
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%rfloat text-align=center width=300px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''
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%rfloat text-align=center width=550px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''
March 03, 2010, at 03:51 PM
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%rfloat text-align=center width=300px% Attach:QTORInHall.jpg | '''Q'^P^''_weak_' Spectrometer Installation in Hall C'''
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%rfloat text-align=center width=300px% Attach:ExpStatusSlideShow.swf | '''Hall C Installation Progress'''
February 26, 2010, at 04:45 PM
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February 25, 2010, at 09:55 PM
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning, having contributed to the design, simulation, and construction of the experiment as a whole, and specifically the main detector system and the QTOR spectrometer (see Figure above).
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Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning. We have contributed to the design, simulation, and construction of the experiment as a whole, and specifically to the main detector system and the QTOR spectrometer (see Figure above). \\
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We continue to now put much of our effort into installation and commissioning, as well as data analysis and DAQ setup related programming. \\
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The experiment is scheduled to being production running in the Fall of 2010. \\
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More detailed information about the experiment and our work on it can obtained by following the menu links at the top of the page.
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We continue to now put much of our effort into installation and commissioning, as well as data analysis and DAQ setup related programming. \\
\\
The experiment is scheduled to being production running in the Fall of 2010. \\
\\
More detailed information about the experiment and our work on it can obtained by following the menu links at the top of the page.
February 25, 2010, at 09:51 PM
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model.
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. \\
\\
Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning, having contributed to the design, simulation, and construction of the experiment as a whole, and specifically the main detector system and the QTOR spectrometer (see Figure above).
\\
Q'^P^''_weak_' is currently being installed in Hall C at Jefferson Laboratory. The University of Manitoba subatomic physics group has made large scale contributions to the experiment, from the very beginning, having contributed to the design, simulation, and construction of the experiment as a whole, and specifically the main detector system and the QTOR spectrometer (see Figure above).
February 25, 2010, at 01:07 PM
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model [[qweak/QweakDetectors | Detectors]].
to:
At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model.
February 25, 2010, at 01:07 PM
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model [[qweak/QweakHardware/Detectors]].
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model [[qweak/QweakDetectors | Detectors]].
February 25, 2010, at 01:06 PM
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model [[qweak/QweakHardware/Detectors | Detectors]].
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model [[qweak/QweakHardware/Detectors]].
February 25, 2010, at 01:06 PM
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model.
[[qweak/QweakHardware/Detectors | Detectors]]
[[qweak/QweakHardware/Detectors | Detectors]]
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model [[qweak/QweakHardware/Detectors | Detectors]].
February 25, 2010, at 01:05 PM
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[[qweak/QweakHardware/Detectors | Detectors]]
February 24, 2010, at 08:39 PM
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February 24, 2010, at 08:13 PM
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
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%rfloat text-align=center width=300px% Attach:QTORInHall.jpg | '''Q'^P^''_weak_' Spectrometer Installation in Hall C'''
Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=300px text-align=center% Attach:QTORInHall.jpg"QTOR In the Hall" | '''Q'^P^''_weak_' Spectrometer Installation in Hall C'''
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model.
February 24, 2010, at 08:09 PM
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=300px% Attach:QTORInHall.jpg '''Q'^P^''_weak_' Spectrometer Installation in Hall C'''
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=300px text-align=center% Attach:QTORInHall.jpg"QTOR In the Hall" | '''Q'^P^''_weak_' Spectrometer Installation in Hall C'''
February 24, 2010, at 08:07 PM
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=300px% Attach:QTORInHall.jpg | '''Q'^P^''_weak_' Spectrometer Installation in Hall C'''
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=300px% Attach:QTORInHall.jpg '''Q'^P^''_weak_' Spectrometer Installation in Hall C'''
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=300px% Attach:QTORInHall.jpg
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=300px% Attach:QTORInHall.jpg | '''Q'^P^''_weak_' Spectrometer Installation in Hall C'''
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry to 2% ||%width=300px% Attach:QTORInHall.jpg \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry with an error of 2.5%. \\
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=300px% Attach:QTORInHall.jpg
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At that accuracy, the measurement will determine the so called weak charge of the proton (Q'^P^''_weak_') with an error of 4.1% (see [[qweak/QweakTheory | theory]]), making this a sensitive test of new physics beyond the Standard Model. ||%width=300px% Attach:QTORInHall.jpg
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry to 2\%||%width=300px% Attach:QTORInHall.jpg\\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry to 2% ||%width=300px% Attach:QTORInHall.jpg \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV polarized electrons, scattered at forward angles from protons in a high power liquid hydrogen target. The goal is to measure this asymmetry to 2\%||%width=300px% Attach:QTORInHall.jpg\\
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%center% ! The Q'^P^''_weak_' Experiment: \\
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||Q'^P^''_weak_' will measure the parity violating asymmetry in the number of ~1 GeV electrons, scattered at forward angles from protons in a high power liquid hydrogen target ||%width=300px% Attach:QTORInHall.jpg \\
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