A Measurement of the Proton's Weak Charge Using an Integration Cerenkov Detector System

The Q-weak experiment at Thomas Jefferson National Accelerator Facility (USA) will make a precision determination of the proton weak charge with approximately 4% combined statistical and systematic uncertainties via a measurement of the parity violating asymmetry in elastic electron-proton scatterin...

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Main Author: Wang, Peiqing
Other Authors: Gericke, Michael (Physics & Astronomy)
Published: 2011
Subjects:
Online Access:http://hdl.handle.net/1993/4835
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spelling ndltd-MANITOBA-oai-mspace.lib.umanitoba.ca-1993-48352014-01-31T03:32:39Z A Measurement of the Proton's Weak Charge Using an Integration Cerenkov Detector System Wang, Peiqing Gericke, Michael (Physics & Astronomy) Gwinner, Gerald (Physics & Astronomy), Martin, Jeffrey (Physics & Astronomy), Goltz, Douglas (Chemistry), Huber, Garth (Physics, U. of Regina) Standard Model weak Interaction weak mixing angle weak charge electron-proton scattering parity violation Cerenkov detector Q-weak momentum transfer cross-section asymmetry hadronic structure form factor The Q-weak experiment at Thomas Jefferson National Accelerator Facility (USA) will make a precision determination of the proton weak charge with approximately 4% combined statistical and systematic uncertainties via a measurement of the parity violating asymmetry in elastic electron-proton scattering at very low momentum transfer and forward angle. This will allow an extraction of the weak mixing angle at Q^2=0.026 (GeV/c)^2 to approximately 0.3%. The weak mixing angle is a fundamental parameter in the Standard Model of electroweak interactions. At the proposed accuracy, a measured deviation of this parameter from the predicted value would indicate new physics beyond what is currently described in the Standard Model. Without deviation from the predicted value, this measurement would place stringent limits on possible extensions to the Standard Model and constitute the most precise measurement of the proton's weak charge to date. The key experimental apparatus include a liquid hydrogen target, a toroidal magnetic spectrometer and a set of eight Cerenkov detectors. The Cerenkov detectors form the main detector system for the Q-weak experiment and are used to measure the parity violating asymmetry during the primary Q-weak production runs. The Cerenkov detectors form the main subject of this thesis. Following a brief introduction to the experiment, the design, development, construction, installation, and testing of this detector system will be discussed in detail. This is followed by a detailed discussion of detector diagnostic data analysis and the corresponding detector performance. The experiment has been successfully constructed and commissioned, and is currently taking data. The thesis will conclude with a discussion of the preliminary analysis of a small portion of the liquid hydrogen data. 2011-09-02T17:35:39Z 2011-09-02T17:35:39Z 2011-09-02 http://hdl.handle.net/1993/4835
collection NDLTD
sources NDLTD
topic Standard Model
weak Interaction
weak mixing angle
weak charge
electron-proton scattering
parity violation
Cerenkov detector
Q-weak
momentum transfer
cross-section asymmetry
hadronic structure
form factor
spellingShingle Standard Model
weak Interaction
weak mixing angle
weak charge
electron-proton scattering
parity violation
Cerenkov detector
Q-weak
momentum transfer
cross-section asymmetry
hadronic structure
form factor
Wang, Peiqing
A Measurement of the Proton's Weak Charge Using an Integration Cerenkov Detector System
description The Q-weak experiment at Thomas Jefferson National Accelerator Facility (USA) will make a precision determination of the proton weak charge with approximately 4% combined statistical and systematic uncertainties via a measurement of the parity violating asymmetry in elastic electron-proton scattering at very low momentum transfer and forward angle. This will allow an extraction of the weak mixing angle at Q^2=0.026 (GeV/c)^2 to approximately 0.3%. The weak mixing angle is a fundamental parameter in the Standard Model of electroweak interactions. At the proposed accuracy, a measured deviation of this parameter from the predicted value would indicate new physics beyond what is currently described in the Standard Model. Without deviation from the predicted value, this measurement would place stringent limits on possible extensions to the Standard Model and constitute the most precise measurement of the proton's weak charge to date. The key experimental apparatus include a liquid hydrogen target, a toroidal magnetic spectrometer and a set of eight Cerenkov detectors. The Cerenkov detectors form the main detector system for the Q-weak experiment and are used to measure the parity violating asymmetry during the primary Q-weak production runs. The Cerenkov detectors form the main subject of this thesis. Following a brief introduction to the experiment, the design, development, construction, installation, and testing of this detector system will be discussed in detail. This is followed by a detailed discussion of detector diagnostic data analysis and the corresponding detector performance. The experiment has been successfully constructed and commissioned, and is currently taking data. The thesis will conclude with a discussion of the preliminary analysis of a small portion of the liquid hydrogen data.
author2 Gericke, Michael (Physics & Astronomy)
author_facet Gericke, Michael (Physics & Astronomy)
Wang, Peiqing
author Wang, Peiqing
author_sort Wang, Peiqing
title A Measurement of the Proton's Weak Charge Using an Integration Cerenkov Detector System
title_short A Measurement of the Proton's Weak Charge Using an Integration Cerenkov Detector System
title_full A Measurement of the Proton's Weak Charge Using an Integration Cerenkov Detector System
title_fullStr A Measurement of the Proton's Weak Charge Using an Integration Cerenkov Detector System
title_full_unstemmed A Measurement of the Proton's Weak Charge Using an Integration Cerenkov Detector System
title_sort measurement of the proton's weak charge using an integration cerenkov detector system
publishDate 2011
url http://hdl.handle.net/1993/4835
work_keys_str_mv AT wangpeiqing ameasurementoftheprotonsweakchargeusinganintegrationcerenkovdetectorsystem
AT wangpeiqing measurementoftheprotonsweakchargeusinganintegrationcerenkovdetectorsystem
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