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A subset of results from the recently completed Jefferson Lab Qweak experiment are reported. This experiment, sensitive to physics beyond the Standard Model, exploits the small parity-violating asymmetry in elastic ep scattering to provide…

We present a new powerful liquid hydrogen target developed for the precise study of parity violating electron scattering on hydrogen and deuterium. This target has been designed to have minimal target density fluctuations under the heat…

The Qweak experiment at Jefferson Lab aims to make a 4% measurement of the parity-violating asymmetry in elastic scattering at very low $Q^2$ of a longitudinally polarized electron beam on a proton target. The experiment will measure the…

High Energy Physics - Experiment · Physics 2019-08-14 Gregory S. Mitchell

Parity-violating electron scattering measurements on hydrogen and deuterium, such as those underway at the Bates and CEBAF laboratories, require luminosities exceeding $10^{38}$cm$^{-2}$s$^{-1}$, resulting in large beam power deposition…

Nuclear Experiment · Physics 2009-10-30 E. J. Beise , D. H. Beck , E. Candell , R. Carr , F. Duncan , T. Forest , W. Korsch , J. W. Mark , R. D. McKeown , B. A. Mueller , S. Wells

A new precision measurement of the parity violating analyzing power in longitudinally polarized electron scattering from the proton at very low Q^2 at an incident energy of 1.16 GeV is in the final stages of preparation for execution at…

Nuclear Experiment · Physics 2008-11-26 Qweak Collaboration , Willem T. H. van Oers

The Jefferson Lab Q_weak experiment determined the weak charge of the proton by measuring the parity-violating elastic scattering asymmetry of longitudinally polarized electrons from an unpolarized liquid hydrogen target at small momentum…

Instrumentation and Detectors · Physics 2015-01-08 Qweak Collaboration , T. Allison , M. Anderson , D. Androic , D. S. Armstrong , A. Asaturyan , T. D. Averett , R. Averill , J. Balewski , J. Beaufait , R. S. Beminiwattha , J. Benesch , F. Benmokhtar , J. Bessuille , J. Birchall , E. Bonnell , J. Bowman , P. Brindza , D. B. Brown , R. D. Carlini , G. D. Cates , B. Cavness , G. Clark , J. C. Cornejo , S. Covrig Dusa , M. M. Dalton , C. A. Davis , D. C. Dean , W. Deconinck , J. Diefenbach , K. Dow , J. F. Dowd , J. A. Dunne , D. Dutta , W. S. Duvall , J. R. Echols , M. Elaasar , W. R. Falk , K. D. Finelli , J. M. Finn , D. Gaskell , M. T. W. Gericke , J. Grames , V. M. Gray , K. Grimm , F. Guo , J. Hansknecht , D. J. Harrison , E. Henderson , J. R. Hoskins , E. Ihloff , K. Johnston , D. Jones , M. Jones , R. Jones , M. Kargiantoulakis , J. Kelsey , N. Khan , P. M. King , E. Korkmaz , S. Kowalski , A. Kubera , J. Leacock , J. P. Leckey , A. R. Lee , J. H. Lee , L. Lee , Y. Liang , S. MacEwan , D. Mack , J. A. Magee , R. Mahurin , J. Mammei , J. W. Martin , A. McCreary , M. H. McDonald , M. J. McHugh , P. Medeiros , D. Meekins , J. Mei , R. Michaels , A. Micherdzinska , A. Mkrtchyan , H. Mkrtchyan , N. Morgan , J. Musson , K. E. Mesick , A. Narayan , L. Z. Ndukum , V. Nelyubin , Nuruzzaman , W. T. H. van Oers , A. K. Opper , S. A. Page , J. Pan , K. D. Paschke , S. K. Phillips , M. L. Pitt , M. Poelker , J. F. Rajotte , W. D. Ramsay , W. R. Roberts , J. Roche , P. W. Rose , B. Sawatzky , T. Seva , M. H. Shabestari , R. Silwal , N. Simicevic , G. R. Smith , S. Sobczynski , P. Solvignon , D. T. Spayde , B. Stokes , D. W. Storey , A. Subedi , R. Subedi , R. Suleiman , V. Tadevosyan , W. A. Tobias , V. Tvaskis , E. Urban , B. Waidyawansa , P. Wang , S. P. Wells , S. A. Wood , S. Yang , S. Zhamkochyan , R. B. Zielinski

A cryogenic horizontal single loop target has been designed, built, tested and operated for the G$^0$ experiment in Hall C at Jefferson Lab. The target cell is 20 cm long, the loop volume is 6.5 l and the target operates with the cryogenic…

The Q-weak experiment at Hall C of Thomas Jefferson National Accelerator Facility has made the first direct measurement of the weak charge of the proton, Qweak(p), through a precision measurement of the parity-violating asymmetry in elastic…

Nuclear Experiment · Physics 2015-06-18 Nuruzzaman

The Qweak experiment has measured the parity-violating asymmetry in polarized e-p elastic scattering at Q^2 = 0.025(GeV/c)^2, employing 145 microamps of 89% longitudinally polarized electrons on a 34.4cm long liquid hydrogen target at…

We propose a new precision measurement of parity-violating electron scattering on the proton at very low Q^2 and forward angles to challenge predictions of the Standard Model and search for new physics. A unique opportunity exists to carry…

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…

High Energy Physics - Experiment · Physics 2019-08-13 Jean-Francois Rajotte

The Qweak experiment which ran at Jefferson Lab in Newport News, VA, measured the weak charge of the proton $Q_W^p$ via elastic electron-proton scattering. Longitudinally polarized electrons were scattered from an unpolarized liquid…

Nuclear Experiment · Physics 2016-01-28 Donald Jones

A 280 ml liquid hydrogen target has been constructed and tested for the MUSE experiment at PSI to investigate the proton charge radius via simultaneous measurement of elastic muon-proton and elastic electron-proton scattering. To control…

The Qweak experiment aims to measure the weak charge of the proton to 4% via the parity-violating asymmetry ($\sim$-200 ppb) in elastic e+p scattering. The scattering rate is largely influenced by five beam parameters: horizontal position…

Accelerator Physics · Physics 2015-06-11 Nuruzzaman

The $Q_{weak}$ Collaboration has completed a challenging measurement of the parity-violating asymmetry in elastic electron-proton ($\vec{e}$p) scattering at the Thomas Jefferson National Accelerator Facility (Jefferson Lab). The initial…

Nuclear Experiment · Physics 2015-10-02 Manolis Kargiantoulakis

From a distance, the proton's weak charge is seen through the distorting effects of clouds of virtual particles. The effective weak charge can be calculated by starting with the measured weak coupling at the Z-pole and "running" the…

High Energy Physics - Phenomenology · Physics 2019-08-14 W. D. Ramsay

A system of modular sealed gas target cells has been developed for use in electron scattering experiments at the Thomas Jefferson National Accelerator Facility (Jefferson Lab). This system was initially developed to complete the MARATHON…

We describe a dynamically polarized target that has been utilized for two electron scattering experiments in Hall A at Jefferson Lab. The primary components of the target are a new, high cooling power 4He evaporation refrigerator, and a…

We report measurements of the parity-conserving beam-normal single-spin elastic scattering asymmetries $B_n$ on $^{12}$C and $^{27}$Al, obtained with an electron beam polarized transverse to its momentum direction. These measurements add an…

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