Qweak.QweakIntro History
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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. \\
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. \\
The experiment is scheduled to begin production running in the Fall of 2010. \\
The experiment began production running in the Fall of 2010 and is expected to reach its goal statistical error in May 2012. \\
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShowNonStopCycle.swf Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently taking data in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShowNonStopCycle.swf Δ \\ |
The experiment is scheduled to being production running in the Fall of 2010. \\
The experiment is scheduled to begin production running in the Fall of 2010. \\
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShowNonStopCycle.swf Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShowNonStopCycle.swf Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShowNonStopCycle.swf Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShowNonStopCycle.swf Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShow.swf Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShowNonStopCycle.swf Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShow.swf Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShow.swf Δ \\ |
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| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShow.swf Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. QPweak is currently being installed in Hall C at Jefferson Laboratory. | Attach:ExpStatusSlideShow.swf Δ \\ |
QPweak is currently being installed in Hall C at Jefferson Laboratory. ||Attach:ExpStatusSlideShow.swf Δ \\
QPweak is currently being installed in Hall C at Jefferson Laboratory. ||Attach:ExpStatusSlideShow.swf Δ \\
QPweak is currently being installed in Hall C at Jefferson Laboratory. ||Attach:ExpStatusSlideShow.swf Δ \\
QPweak is currently being installed in Hall C at Jefferson Laboratory. ||Attach:ExpStatusSlideShow.swf Δ \\
QPweak is currently being installed in Hall C at Jefferson Laboratory. ||Attach:ExpStatusSlideShow.swf Δ \\
QPweak is currently being installed in Hall C at Jefferson Laboratory. ||Attach:ExpStatusSlideShow.swf Δ \\
QPweak is currently being installed in Hall C at Jefferson Laboratory. || Attach:ExpStatusSlideShow.swf Δ \\
QPweak is currently being installed in Hall C at Jefferson Laboratory. ||Attach:ExpStatusSlideShow.swf Δ \\
QPweak 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). || Attach:ExpStatusSlideShow.swf Δ \\
QPweak is currently being installed in Hall C at Jefferson Laboratory. || Attach:ExpStatusSlideShow.swf Δ \\
We continue to now put much of our effort into installation and commissioning, as well as data analysis and DAQ setup related programming. \\
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. \\
QPweak 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). || Attach:ExpStatusSlideShow.swf Δ \\
QPweak 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). || Attach:ExpStatusSlideShow.swf Δ \\
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. || Attach:ExpStatusSlideShow.swf Δ \\
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. \\
QPweak 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). \\
QPweak 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). || Attach:ExpStatusSlideShow.swf Δ \\
Attach:ExpStatusSlideShow.swf Δ \\ QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. \\
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. || Attach:ExpStatusSlideShow.swf Δ \\
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Attach:ExpStatusSlideShow.swf Δ \\ QPweak 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%. \\
Attach:ExpStatusSlideShow.swf Δ \\ QPweak 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%. \\
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
QPweak 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%. \\
Attach:ExpStatusSlideShow.swf Δ \\ QPweak 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%. \\
Attach:ExpStatusSlideShow.swf Δ |Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
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Attach:ExpStatusSlideShow.swf Δ| Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ |Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ|Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ| Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ|Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
Attach:QTORInHall.jpg Δ | QPweak Spectrometer Installation in Hall C
Attach:ExpStatusSlideShow.swf Δ | Hall C Installation Progress
QPweak 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).
QPweak 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).
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.
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model.
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model.
QPweak 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).
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model Detectors?.
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model.
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model .
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model .
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model .
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model.
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model .
Attach:QTORInHall.jpg Δ | QPweak Spectrometer Installation in Hall C QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. || Attach:QTORInHall.jpg Δ | QPweak Spectrometer Installation in Hall C
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model.
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. || Attach:QTORInHall.jpg Δ QPweak Spectrometer Installation in Hall C
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. || Attach:QTORInHall.jpg Δ | QPweak Spectrometer Installation in Hall C
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. || Attach:QTORInHall.jpg Δ | QPweak Spectrometer Installation in Hall C
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. || Attach:QTORInHall.jpg Δ QPweak Spectrometer Installation in Hall C
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. || Attach:QTORInHall.jpg Δ
At that accuracy, the measurement will determine the so called weak charge of the proton (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. || Attach:QTORInHall.jpg Δ | QPweak Spectrometer Installation in Hall C
The QPweak Experiment: \\\
The QPweak Experiment: \\\
| QPweak 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% | Attach:QTORInHall.jpg Δ \\ |
| QPweak 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 (QPweak) with an error of 4.1% (see theory), making this a sensitive test of new physics beyond the Standard Model. | Attach:QTORInHall.jpg Δ |
| QPweak 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\% | Attach:QTORInHall.jpg Δ\\ |
| QPweak 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% | Attach:QTORInHall.jpg Δ \\ |
| QPweak 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 | Attach:QTORInHall.jpg Δ \\ |
| QPweak 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\% | Attach:QTORInHall.jpg Δ\\ |
! The QPweak Experiment: \\
The QPweak Experiment: \\\
!!!The QPweak Experiment:
| QPweak 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 | Attach:QTORInHall.jpg Δ |
! The QPweak Experiment:
| QPweak 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 | Attach:QTORInHall.jpg Δ \\ |
The QPweak Experiment:
!!!The QPweak Experiment:
| QPweak 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 | Attach:QTORInHall.jpg Δ |
This is Qweak!
The QPweak Experiment:
This is Qweak!