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Precision measurements of the structure of nucleons and nuclei in the regime of strong interaction QCD are now possible with the availability of high current polarized electron beams, polarized targets, and recoil polarimeters, in…

Nuclear Experiment · Physics 2017-08-23 Elton S. Smith

Positron beams, both polarized and unpolarized, are identified as essential ingredients for the experimental program at the next generation of lepton accelerators. In the context of the Hadronic Physics program at the Jefferson Laboratory…

Nuclear Experiment · Physics 2019-06-25 A. Afanasev , I. Albayrak , S. Ali , M. Amaryan , A. D'Angelo , J. Annand , J. Arrington , A. Asaturyan , H. Avakian , T. Averett , L. Barion , M. Battaglieri , V. Bellini , V. Berdnikov , J. Bernauer , A. Biselli , M. Boer , M. Bondì , K. -T. Brinkmann , B. Briscoe , V. Burkert , A. Camsonne , T. Cao , L. Cardman , M. Carmignotto , L. Causse , A. Celentano , P. Chatagnon , G. Ciullo , M. Contalbrigo , D. Day , M. Defurne , S. Diehl , B. Dongwi , R. Dupré , D. Dutta , M. Ehrhart , L. Elouadrhiri , R. Ent , I. Fernando , A. Filippi , Y. Furletova , H. Gao , A. Gasparian , D. Gaskell , F. Georges , F. -X. Girod , J. Grames , C. Gu , M. Guidal , D. Hamilton , D. Hasell , D. Higinbotham , M. Hoballah , T. Horn , C. Hyde , A. Italiano , N. Kalantarians , G. Kalicy , D. Keller , C. Keppel , M. Kerver , P. King , E. Kinney , H. -S. Ko , M. Kohl , V. Kubarovsky , L. Lanza , P. Lenisa , N. Liyanage , S. Liuti , J. Mamei , D. Marchand , P. Markowitz , L. Marsicano , M. Mazouz , M. McCaughan , B. McKinnon , M. Mihovilovič , R. Milner , A. Mkrtchyan , H. Mkrtchyan , A. Movsisyan , C. Muñoz Camacho , P. Nadel-Turońs , M. De Napoli , J. Nazeer , S. Niccolai , G. Niculescu , R. Novotny , L. Pappalardo , R. Paremuzyan , E. Pasyuk , T. Patel , I. Pegg , D. Perera , A. Puckett , N. Randazzo , M. Rashad , M. Rathnayake , A. Rizzo , J. Roche , O. Rondon , A. Schmidt , M. Shabestari , Y. Sharabian , S. Širca , D. Sokhan , A. Somov , N. Sparveris , S. Stepanyan , I. Strakovsky , V. Tadevosyan , M. Tiefenback , R. Trotta , R. De Vita , H. Voskanyan , E. Voutier , R. Wang , B. Wojtsekhowski , S. Wood , H. -G. Zaunick , S. Zhamkochyan , J. Zhang , S. Zhao , X. Zheng , C. Zorn

Positron beams, both polarized and unpolarized, are identified as essential ingredients for the experimental programs at the next generation of lepton accelerators. In the context of the hadronic physics program at Jefferson Lab (JLab),…

Nuclear Experiment · Physics 2021-09-15 A. Accardi , A. Afanasev , I. Albayrak , S. F. Ali , M. Amaryan , J. R. M. Annand , J. Arrington , A. Asaturyan , H. Atac , H. Avakian , T. Averett , C. Ayerbe Gayoso , X. Bai , L. Barion , M. Battaglieri , V. Bellini , R. Beminiwattha , F. Benmokhtar , V. V. Berdnikov , J. C. Bernauer , V. Bertone , A. Bianconi , A. Biselli , P. Bisio , P. Blunden , M. Boer , M. Bondì , K. -T. Brinkmann , W. J. Briscoe , V. Burkert , T. Cao , A. Camsonne , R. Capobianco , L. Cardman , M. Carmignotto , M. Caudron , L. Causse , A. Celentano , P. Chatagnon , J. -P. Chen , T. Chetry , G. Ciullo , E. Cline , P. L. Cole , M. Contalbrigo , G. Costantini , A. D'Angelo , L. Darmé , D. Day , M. Defurne , M. De Napoli , A. Deur , R. De Vita , N. D'Hose , S. Diehl , M. Diefenthaler , B. Dongwi , R. Dupré , H. Dutrieux , D. Dutta , M. Ehrhart , L. El Fassi , L. Elouadrhiri , R. Ent , J. Erler , I. P. Fernando , A. Filippi , D. Flay , T. Forest , E. Fuchey , S. Fucini , Y. Furletova , H. Gao , D. Gaskell , A. Gasparian , T. Gautam , F. -X. Girod , K. Gnanvo , J. Grames , G. N. Grauvoge , P. Gueye , M. Guidal , S. Habet , T. J. Hague , D. J. Hamilton , O. Hansen , D. Hasell , M. Hattawy , D. W. Higinbotham , A. Hobart , T. Horn , C. E. Hyde , H. Ibrahim , A. Ilyichev , A. Italiano , K. Joo , S. J. Joosten , V. Khachatryan , N. Kalantarians , G. Kalicy , B. Karky , D. Keller , C. Keppel , M. Kerver , M. Khandaker , A. Kim , J. Kim , P. M. King , E. Kinney , V. Klimenko , H. -S. Ko , M. Kohl , V. Kozhuharov , B. T. Kriesten , G. Krnjaic , V. Kubarovsky , T. Kutz , L. Lanza , M. Leali , P. Lenisa , N. Liyanage , Q. Liu , S. Liuti , J. Mammei , S. Mantry , D. Marchand , P. Markowitz , L. Marsicano , V. Mascagna , M. Mazouz , M. McCaughan , B. McKinnon , D. McNulty , W. Melnitchouk , A. Metz , Z. -E. Meziani , S. Migliorati , M. Mihovilovic , R. Milner , A. Mkrtchyan , H. Mkrtchyan , A. Movsisyan , H. Moutarde , M. Muhoza , C. Muñoz Camacho , J. Murphy , P. Nadel-Turonski , E. Nardi , J. Nazeer , S. Niccolai , G. Niculescu , R. Novotny , J. F. Owens , M. Paolone , L. Pappalardo , R. Paremuzyan , B. Pasquini , E. Pasyuk , T. Patel , I. Pegg , C. Peng , D. Perera , M. Poelker , K. Price , A. J. R. Puckett , M. Raggi , N. Randazzo , M. N. H. Rashad , M. Rathnayake , B. Raue , P. E. Reimer , M. Rinaldi , A. Rizzo , Y. Roblin , J. Roche , O. Rondon-Aramayo , F. Sabatié , G. Salmè , E. Santopinto , R. Santos Estrada , B. Sawatzky , A. Schmidt , P. Schweitzer , S. Scopetta , V. Sergeyeva , M. Shabestari , A. Shahinyan , Y. Sharabian , S. Širca , E. S. Smith , D. Sokhan , A. Somov , N. Sparveris , M. Spata , H. Spiesberger , M. Spreafico , S. Stepanyan , P. Stoler , I. Strakovsky , R. Suleiman , M. Suresh , P. Sznajder , H. Szumila-Vance , V. Tadevosyan , A. S. Tadepalli , A. W. Thomas , M. Tiefenback , R. Trotta , M. Ungaro , P. Valente , M. Vanderhaeghen , L. Venturelli , H. Voskanyan , E. Voutier , B. Wojtsekhowski , M. H. Wood , S. Wood , J. Xie , W. Xiong , Z. Ye , M. Yurov , H. -G. Zaunick , S. Zhamkochyan , J. Zhang , S. Zhang , S. Zhao , Z. W. Zhao , X. Zheng , J. Zhou , C. Zorn

Precise proton and neutron form factor measurements at Jefferson Lab, using spin observables, have recently made a significant contribution to the unraveling of the internal structure of the nucleon. Accurate experimental measurements of…

Nuclear Experiment · Physics 2015-06-02 V. Punjabi , C. F. Perdrisat , M. K. Jones , E. J. Brash , C. E. Carlson

Recent results on studies of the structure of nucleons and nuclei in the regime of strong interaction QCD are discussed. Use of high current polarized electron beams, polarized targets, and recoil polarimeters, in conjunction with modern…

Nuclear Theory · Physics 2008-11-26 Volker D. Burkert

In the G0 experiment, performed at Jefferson Lab, the parity-violating elastic scattering of electrons from protons and quasi-elastic scattering from deuterons is measured in order to determine the neutral weak currents of the nucleon.…

Nuclear Experiment · Physics 2011-06-29 G0 Collaboration , D. Androic , D. S. Armstrong , J. Arvieux , R. Asaturyan , T. D. Averett , S. L. Bailey , G. Batigne , D. H. Beck , E. J. Beise , J. Benesch , F. Benmokhtar , L. Bimbot , J. Birchall , A. Biselli , P. Bosted , H. Breuer , P. Brindza , C. L. Capuano , R. D. Carlini , R. Carr , N. Chant , Y. -C. Chao , R. Clark , A. Coppens , S. D. Covrig , A. Cowley , D. Dale , C. A. Davis , C. Ellis , W. R. Falk , H. Fenker , J. M. Finn , T. Forest , G. Franklin , R. Frascaria , C. Furget , D. Gaskell , M. T. W. Gericke , J. Grames , K. A. Griffioen , K. Grimm , G. Guillard , B. Guillon , H. Guler , K. Gustafsson , L. Hannelius , J. Hansknecht , R. D. Hasty , A. M. Hawthorne Allen , T. Horn , T. M. Ito , K. Johnston , M. Jones , P. Kammel , R. Kazimi , P. M. King , A. Kolarkar , E. Korkmaz , W. Korsch , S. Kox , J. Kuhn , J. Lachniet , R. Laszewski , L. Lee , J. Lenoble , E. Liatard , J. Liu , A. Lung , G. A. MacLachlan , J. Mammei , D. Marchand , J. W. Martin , D. J. Mack , K. W. McFarlane , D. W. McKee , R. D. McKeown , F. Merchez , M. Mihovilovic , A. Micherdzinska , H. Mkrtchyan , B. Moffit , M. Morlet , M. Muether , J. Musson , K. Nakahara , R. Neveling , S. Niccolai , D. Nilsson , S. Ong , S. A. Page , V. Papavassiliou , S. F. Pate , S. K. Phillips , P. Pillot , M. L. Pitt , M. Poelker , T. A. Porcelli , G. Quemener , B. P. Quinn , W. D. Ramsay , A. W. Rauf , J. -S. Real , T. Ries , J. Roche P. Roos , G. A. Rutledge , J. Schaub , J. Secrest , T. Seva , N. Simicevic , G. R. Smith , D. T. Spayde , S. Stepanyan , M. Stutzman , R. Suleiman , V. Tadevosyan , R. Tieulent , J. van de Wiele , W. T. H. van Oers , M. Versteegen , E. Voutier , W. F. Vulcan , S. P. Wells , G. Warren , S. E. Williamson , R. J. Woo , S. A. Wood , C. Yan , J. Yun , V. Zeps

The $12~$GeV electron beam energy at Jefferson Laboratory provides ideal electroproduction kinematics for many novel tests of QCD in both the perturbative and nonperturbative domains. These include tests of the quark flavor dependence of…

High Energy Physics - Phenomenology · Physics 2015-11-16 Stanley J. Brodsky

We investigate the potential impact of forthcoming Jefferson Lab semi-inclusive polarized deep inelastic scattering proton measurements in the determination of the sea quark polarization in the nucleon by means of a next to leading order…

High Energy Physics - Phenomenology · Physics 2009-01-07 X. Jiang , G. A. Navarro , R. Sassot

The simplest models might describe the nucleon as 3 light quarks, but this description would be incomplete without inclusion of the sea of glue and q-qbar pairs which binds it. Early indications of a particularly large contribution from…

Nuclear Experiment · Physics 2011-10-18 Kent Paschke , Anthony Thomas , Robert Michaels , David Armstrong

After almost five decades of study of parity violation in hadronic systems, the determination of the seven weak meson-nucleon couplings is still incomplete. Whereas parity violation in nuclear systems is complicated by the intricacies of…

Nuclear Experiment · Physics 2009-11-13 Willem T. H. van Oers

Recently, there has been considerable theoretical interest in determining strange quark contributions to hadronic matrix elements. Such matrix elements can be accessed through the nucleon's neutral weak form factors as determined in parity…

Nuclear Experiment · Physics 2019-08-14 E. J. Beise

The duality between the partonic and hadronic descriptions of electron--nucleon scattering is a remarkable feature of nuclear interactions. When averaged over appropriate energy intervals the cross section at low energy which is dominated…

Nuclear Experiment · Physics 2015-09-28 Ioana Niculescu

Measurement of the neutral weak vector form factors of the nucleon provides unique access to the strange quark content of the nucleon. These form factors can be studied using parity-violating electron scattering. A comprehensive program of…

Nuclear Experiment · Physics 2012-10-29 D. S. Armstrong , R. D. McKeown

Atomic nuclei can be used as spatial analyzers of the hadronization process in semi-inclusive deep inelastic scattering. The study of this process using fully-identified final state hadrons began with the HERMES program in the late 1990s,…

High Energy Physics - Phenomenology · Physics 2015-05-30 Will Brooks , Hayk Hakobyan , Cristian Peña , Miguel Arratia , Constanza Valdés

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

High-energy electron scattering is a clean and precise probe for measurements of hadronic and nuclear structure, with a key role in understanding the role of high-momentum nucleons (and quarks) in nuclei. Jefferson Lab has dramatically…

Nuclear Experiment · Physics 2022-03-08 John Arrington , Nadia Fomin , Axel Schmidt

Baryons are complex systems of confined quarks and gluons and exhibit the characteristic spectra of excited states. The systematics of the baryon excitation spectrum is important to our understanding of the effective degrees of freedom…

Nuclear Experiment · Physics 2019-08-13 Volker Crede

Over the past decade measurements of unpolarized structure functions at Jefferson Lab with unprecedented precision have significantly advanced our knowledge of nucleon structure. These have for the first time allowed quantitative tests of…

Nuclear Experiment · Physics 2015-05-27 M. E. Christy , W. Melnitchouk

Elastic lepton scattering off of a nucleon has proved to be an efficient tool to study the structure of the hadron. Modern cross section and asymmetry measurements at Jefferson Lab require effects beyond the leading order Born approximation…

High Energy Physics - Phenomenology · Physics 2018-07-18 Oleksandr Koshchii , Andrei Afanasev

The ratio of the proton form factors, GEp/GMp, has been measured from Q2 of 0.5 GeV2 to 8.5 GeV2, at the Jefferson Laboratory, using the polarization transfer method. This ratio is extracted directly from the measured ratio of the…

Nuclear Experiment · Physics 2015-06-19 Vina Punjabi , Charles F. Perdrisat
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