A Measurement Of The Parity Violating Asymmetry In Aluminum And Its Contribution To A Measurement Of The Protons Weak Charge PDF Download

Are you looking for read ebook online? Search for your book and save it on your Kindle device, PC, phones or tablets. Download A Measurement Of The Parity Violating Asymmetry In Aluminum And Its Contribution To A Measurement Of The Protons Weak Charge PDF full book. Access full book title A Measurement Of The Parity Violating Asymmetry In Aluminum And Its Contribution To A Measurement Of The Protons Weak Charge.

A Measurement of the Parity-Violating Asymmetry in Aluminum and Its Contribution to a Measurement of the Proton's Weak Charge

A Measurement of the Parity-Violating Asymmetry in Aluminum and Its Contribution to a Measurement of the Proton's Weak Charge
Author:
Publisher:
Total Pages:
Release: 2016
Genre:
ISBN:

Download A Measurement of the Parity-Violating Asymmetry in Aluminum and Its Contribution to a Measurement of the Proton's Weak Charge Book in PDF, ePub and Kindle

The Q_weak experiment, which ran at the Thomas Jefferson National Accelerator Facility, made a precision measurement of the proton's weak charge, Q^p_W. The weak charge is extracted via a measurement of the parity-violating asymmetry in elastic electron-proton scattering from hydrogen at low momentum transfer (Q^2=0.025 GeV^2). This result is directly related to the electroweak mixing angle, sin^2(Theta_W), a fundamental parameter in the Standard Model of particle physics. This provides a precision test sensitive to new, as yet unknown, fundamental physics. This dissertation focuses on two central corrections to the Q_weak measurement: the target window contribution and sub-percent determination of the electron beam polarization. The aluminum target windows contribute approximately 30% of the measured asymmetry. Removal of this background requires precise measurements of both the elastic electron-aluminum scattering rate and its parity-violating asymmetry. The results reported here are the most precise measurement of the Q_weak target dilution and asymmetry to date. The parity-violating asymmetry for the aluminum alloy was found to be 1.6174 +/- 0.0704 (stat.) +/- 0.0113 (sys.) parts-per-million. The first sub-percent precision polarization measurements made from the Hall C Moller polarimeter are also reported, with systematic uncertainties of 0.84%.


A Measurement of the Parity-violating Asymmetry in Aluminum and Its Contribution to a Measurement of the Proton's Weak Charge

A Measurement of the Parity-violating Asymmetry in Aluminum and Its Contribution to a Measurement of the Proton's Weak Charge
Author: Joshua Allen Magee (Ph.D.)
Publisher:
Total Pages: 169
Release: 2016
Genre: Aluminum
ISBN:

Download A Measurement of the Parity-violating Asymmetry in Aluminum and Its Contribution to a Measurement of the Proton's Weak Charge Book in PDF, ePub and Kindle

The Qweak experiment, which ran at the Thomas Jefferson National Accelerator Facility, made a precision measurement of the protons weak charge, Q_p^W . The weak charge is extracted via a measurement of the parity-violating asymmetry in elastic electron-proton scattering from hydrogen at low momentum transfer (Q^2=0.025 GeV^2). This result is directly related to the electroweak mixing angle, sin2 (theta_W), a fundamental parameter in the Standard Model of particle physics. This provides a precision test sensitive to new, as yet unknown, fundamental physics. This dissertation focuses on two central corrections to the Qweak measurement: the target window contribution and sub-percent determination of the electron beam polarization. The aluminum target windows contribute approximately 30% of the measured asymmetry. Removal of this background requires precise measurements of both the elastic electron-aluminum scattering rate and its parity-violating asymmetry. The results reported here are the most precise measurement of the Qweak target dilution and asymmetry to date. The parity-violating asymmetry for the aluminum alloy was found to be 1.6174 0.0704 (stat.) 0.0113 (sys.) parts-per-million. The first sub-percent precision polarization measurements made from the Hall C Mller polarimeter are also reported, with systematic uncertainties of 0.84%.


First Measurements of the Parity-violating and Beam-normal Single-spin Asymmetries in Elastic Electron-aluminum Scattering

First Measurements of the Parity-violating and Beam-normal Single-spin Asymmetries in Elastic Electron-aluminum Scattering
Author: Kurtis David Bartlett
Publisher:
Total Pages: 227
Release: 2018
Genre: Particles (Nuclear physics)
ISBN:

Download First Measurements of the Parity-violating and Beam-normal Single-spin Asymmetries in Elastic Electron-aluminum Scattering Book in PDF, ePub and Kindle

The Qweak collaboration has made the first measurements of the elastic parity-violating and beam-normal single-spin asymmetries from the $^{27}$Al nucleus. Both are the result of ancillary measurements conducted during the Qweak experiment at Jefferson Lab. The goal of the experimental was to determine the proton's weak charge, $Q_{W}^{p}$, via a measurement of the elastic parity-violating electron-proton scattering asymmetry. During the experiment, ancillary measurements were made with different beam configurations on a separate aluminum alloy target, in an effort to directly measure the aluminum background coming from the experiment's liquid hydrogen target cell. This dissertation discusses three primary results: the parity-violating $^{27}$Al asymmetry analysis used to correct for the aluminum target background in the final Qweak analysis, its extended analysis leading to the extraction of the pure elastic parity-violating {\aluminum} asymmetry, and the determination of the elastic beam-normal single-spin $^{27}$Al asymmetry. The parity-violating result was also used to make a semi model-independent determination of $^{27}$Al neutron distribution radius, an important test for models used to describe neutron-rich matter. The beam-normal single-spin asymmetry stands to possibly shed light on an observed disagreement between theory and a previous measurement performed on $^{208}$Pb, as $^{27}$Al is the next highest atomic mass nucleus to have this observable measured. The elastic parity-violating $^{27}$Al asymmetry was found to be $1.927 \pm 0.173$ ppm at $\langle Q^{2} \rangle = 0.0236 \pm 0.0001$ GeV$^{2}$. This measured parity-violating asymmetry implies a $^{27}$Al neutron distribution radius of $3.024 \pm 0.104$ fm. Calculating the difference between this radius and the $^{27}$Al proton distribution radius yields the neutron skin, which was found to be $0.092 \pm 0.104$ fm. This skin value is consistent with zero, within its uncertainty, and it confirms the naive expectation for a light nucleus like $^{27}$Al. The beam-normal single-spin $^{27}$Al asymmetry was found to be $-16.322 \pm 2.679$ ppm at $\langle Q \rangle = 0.154$ GeV. This value agrees with the previous observed trend of beam-normal single-spin asymmetries measured from light nuclei, which motivates the need for future measurements of higher atomic mass nuclei.


Determination of the Weak Charge of the Proton Through Parity Violating Asymmetry Measurements in the Elastic E+p Scattering

Determination of the Weak Charge of the Proton Through Parity Violating Asymmetry Measurements in the Elastic E+p Scattering
Author:
Publisher:
Total Pages:
Release: 2014
Genre:
ISBN:

Download Determination of the Weak Charge of the Proton Through Parity Violating Asymmetry Measurements in the Elastic E+p Scattering Book in PDF, ePub and Kindle

The Qweak experiment has taken data to make a 2.5% measurement of parity violating elastic e+p asymmetry in the four momentum transfer region of 0.0250 (GeV/c)^2. This asymmetry is proportional to the weak charge of the proton, which is related to the weak mixing angle, sin^2(theta_W). The final Qweak measurement will provide the most precise measurement of the weak mixing angle below the Z^0 pole to test the Standard Model prediction. A description of the experimental apparatus is provided in this dissertation. The experiment was carried out using a longitudinally polarized electron beam of up to 180 microampere on a 34.5 cm long unpolarized liquid hydrogen target. The Qweak target is not only the world's highest cryogenic target ever built for a parity experiment but also is the least noisy target. This dissertation provides a detailed description of this target and presents a thorough analysis of the target performance. Statistical analysis of Run 1 data, collected between Feb - May 2011, is done to extract a blinded parity violating asymmetry of size -299.7 " 13.4 (stat.) " 17.2 (syst.) " 68 (blinding) parts-per-billion. This resulted in a preliminary proton's weak charge of value 0.0865 " 0.0085, a 9% measurement. Based on this blinded asymmetry, the weak mixing angle was determined to be sin^2(theta_W) = 0.23429 " 0.00211.


Determination of the Weak Charge of the Proton Through Parity Violating Asymmetry Measurements in the Elastic E+p Scattering

Determination of the Weak Charge of the Proton Through Parity Violating Asymmetry Measurements in the Elastic E+p Scattering
Author: Adesh Subedi
Publisher:
Total Pages: 269
Release: 2014
Genre:
ISBN:

Download Determination of the Weak Charge of the Proton Through Parity Violating Asymmetry Measurements in the Elastic E+p Scattering Book in PDF, ePub and Kindle

The Qweak experiment has taken data to make a 2.5 percent measurement of parity violating elastic e + p asymmetry in the four momentum transfer region of 0.0250 (GeV/c)2. This asymmetry is proportional to the weak charge of the proton, which is related to the weak mixing angle, sin2 (thetaW). The final Qweak measurement will provide the most precise measurement of the weak mixing angle below the Z _ pole to test the Standard Model prediction. A description of the experimental apparatus is provided in this dissertation.The experiment was carried out using a longitudinally polarized electron beam of up to 180 microampere on a 34.5 cm long unpolarized liquid hydrogen target. The Qweak target is not only the world's highest cryogenic target ever built for a parity experiment but also is the least noisy target. This dissertation provides a detailed description of this target and presents a thorough analysis of the target performance. Statistical analysis of Run 1 data, collected between Feb - May 2011, is done to extract a blinded parity violating\ asymmetry of size 299.7 +/- 13.4 (stat.) +/- 17.2 (syst.) +/- 68 (blinding) parts-per-billion. This resulted in a preliminary proton's weak charge of value 0.0865 +/- 0.0085, a 9% measurement. Based on this blinded asymmetry, the weak mixing angle was determined to be sin2 (thetaW) = 0.23429 +/- 0.00211.


Measuring the Weak Charge of the Proton and the Hadronic Parity Violation of the N 2![Delta] Transition

Measuring the Weak Charge of the Proton and the Hadronic Parity Violation of the N 2![Delta] Transition
Author:
Publisher:
Total Pages: 217
Release: 2012
Genre:
ISBN:

Download Measuring the Weak Charge of the Proton and the Hadronic Parity Violation of the N 2![Delta] Transition Book in PDF, ePub and Kindle

Qweak will determine the weak charge of the proton, Qp{sub W}, via an asymmetry measurement of parity-violating elastic electron-proton scattering at low four momentum transfer to a precision of 4%. QpW has a firm Standard Model prediction and is related to the weak mixing angle, sin2 [Phi]W, a well-defined Standard Model parameter. Qweak will probe a subset of new physics to the TeV mass scale and test the Standard Model. The details of how this measurement was performed and the analysis of the 25% elastic dataset will be presented in this thesis. Also, an analysis of an auxiliary measurement of the parity-violating asymmetry in the N → [Delta] transition is presented. It is used as a systematic inelastic background correction in the elastic analysis and to extract information about the hadronic parity violation through the low energy constant, d[Delta]. The elastic asymmetry at Q2 = 0.0252 ± 0.0007 GeV2 was measured to be Aep = -265 ± 40 ± 22 ± 68 ppb (stat., sys., and blinding). Extrapolated to Q2 = 0, the value of the proton's weak charge was measured to be QpW = 0.077 ± 0.019 (stat. and sys.) ± 0.026 (blinding). This is within 1 [sigma] of the Standard Model prediction of QpW = 0.0705 ± 0.0008. The N → [Delta] inelastic asymmetry at Q2 = 0.02078 ± 0.0005 GeV2 and W = 1205 MeV was measured to be Ainel = -3.03 ± 0.65 ± 0.73 ± 0.07 ppm (stat., sys., and blinding). This result constrains the low energy constant to be d[Delta] = 5.8 ± 22g[pi], and, if the result of the G0 experiment is included, d[Delta] = 5.8 ± 17g[pi]. This result rules out suggested large values of d[Delta] motivated by radiative hyperon decays. The elastic measurement is the first direct measurement of the weak charge of the proton while the inelastic measurement is only the second measurement of the neutral current excitation of the [Delta]resonance. It is currently the best constraint for the low energy constant, d[Delta].


Measurement of the Proton's Weak Charge at the Qweak Experiment

Measurement of the Proton's Weak Charge at the Qweak Experiment
Author:
Publisher:
Total Pages:
Release: 2011
Genre:
ISBN:

Download Measurement of the Proton's Weak Charge at the Qweak Experiment Book in PDF, ePub and Kindle

The Qweak experiment at Jefferson Laboratory measures the parity violating asymmetry of polarized electrons scattering from a proton target at very low momentum transfer. In the Standard Model, this asymmetry reveals the proton's coupling to the neutral vector current, the weak charge. This value, measured directly for the first time, will provide a precision test of the Standard Model and will constrain the possibility of relevant physics beyond the Standard Model. The planned precision will probe certain classes of new physics at the 2̃ TeV scale. In order to challenge the precise predictions, the asymmetry will be measured with a 2.5 percent accuracy. To achieve such a precision, great care has to be taken on many aspects of the experiment. The very low momentum transfer reduces the hadronic effects to the asymmetry and must be determined to half of a percent accuracy. Beam stability is controlled and monitored constantly and background events are carefully studied.


Determination of the Proton's Weak Charge Via Parity Violating Electron Scattering

Determination of the Proton's Weak Charge Via Parity Violating Electron Scattering
Author:
Publisher:
Total Pages: 202
Release: 2015
Genre:
ISBN:

Download Determination of the Proton's Weak Charge Via Parity Violating Electron Scattering Book in PDF, ePub and Kindle

The Qweak experiment, which completed running in May of 2012 at Jefferson Laboratory, has measured the parity-violating asymmetry in elastic electron-proton scattering at four-momentum transfer Q2=0.025 (GeV/c)2 in order to provide the first direct measurement of the proton's weak charge, Qpw. The Standard Model makes firm predictions for the weak charge; deviations from the predicted value would provide strong evidence of new physics beyond the Standard Model. Using an 89% polarized electron beam at 145 microA scattering from a 34.4 cm long liquid hydrogen target, scattered electrons were detected using an array of eight fused-silica detectors placed symmetric about the beam axis. The parity-violating asymmetry was then measured by reversing the helicity of the incoming electrons and measuring the normalized difference in rate seen in the detectors. The low Q2 enables a theoretically clean measurement; the higher order hadronic corrections are constrained using previous parity-violating electron scattering world data. The experimental method will be discussed, with recent results constituting 4% of our total data and projections of our proposed uncertainties on the full data set.