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Related papers: Measurements of $d_{2}^{n}$ and $A_{1}^{n}$: Probi…

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Double-spin asymmetries and absolute cross sections were measured at large Bjorken $x$ (0.25 $ \le x \le $ 0.90), in both the deep-inelastic and resonance regions, by scattering longitudinally polarized electrons at beam energies of 4.7 and…

We have measured the neutron structure function g$_{2}^{n}$ and the virtual photon-nucleon asymmetry A$_{2}^{n}$ over the kinematic range $0.014\leq x \leq 0.7$ and $1.0 \leq Q^{2} \leq 17.0$ by scattering 48.3 GeV longitudinally polarized…

High Energy Physics - Experiment · Physics 2008-11-26 K. Abe

The Spin Asymmetries of the Nucleon Experiment (SANE) measured two double spin asymmetries using a polarized proton target and polarized electron beam at two beam energies, 4.7 GeV and 5.9 GeV. A large-acceptance open-configuration detector…

Using lattice QCD, we calculate the twist-2 contribution $a_2$ to the third Mellin moment of the spin structure functions $g_1$ and $g_2$ in the nucleon. In addition we evaluate the twist-3 contribution $d_2$. Our computations make use of…

High Energy Physics - Lattice · Physics 2022-03-23 S. Bürger , T. Wurm , M. Löffler , M. Göckeler , G. Bali , S. Collins , A. Schäfer , A. Sternbeck

The twist-3 transverse spin--dependent nucleon structure function $g_2$ arises in high-energy processes involving a transversely polarized nucleon. Its connection to quark--gluon correlations allows for an interpretation in terms of the…

High Energy Physics - Phenomenology · Physics 2026-03-27 Ziqi Zhang , Chandan Mondal , Siqi Xu , Xingbo Zhao , James P. Vary

Recent precision spin structure data from Jefferson Lab have significantly advanced our knowledge of nucleon structure in the valence quark (high-$x$) region and improved our understanding of higher-twist effects, spin sum rules and…

Nuclear Experiment · Physics 2007-05-23 Jian-ping Chen

The spin structure functions of the proton and the deuteron were measured during the EG4 experiment at Jefferson Lab in 2006. Data were collected for longitudinally polarized electron scattering off longitudinally polarized NH$_3$ and…

Nuclear Experiment · Physics 2026-01-06 A. Deur , S. E. Kuhn , M. Ripani , X. Zheng , A. G. Acar , P. Achenbach , K. P. Adhikari , J. S. Alvarado , M. J. Amaryan , W. R. Armstrong , H. Atac , H. Avakian , L. Baashen , N. A. Baltzell , L. Barion , M. Bashkanov , M. Battaglieri , B. Benkel , F. Benmokhtar , A. Bianconi , A. S. Biselli , W. A. Booth , F. B ossu , P. Bosted , S. Boiarinov , K. Th. Brinkmann , W. J. Briscoe , S. Bueltmann , V. D. Burkert , D. S. Carman , P. Chatagnon , J. P. Chen , G. Ciullo , P. L. Cole , M. Contalbrigo , V. Crede , A. D'Angelo , N. Dashyan , R. De Vita , M. Defurne , S. Diehl , C. Djalali , V. A. Drozdov , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , L. Elouadrhiri , P. Eugenio , J. C. Faggert , S. Fegan , R. Fersch , A. Filippi , K. Gates , G. Gavalian , G. P. Gilfoyle , R. W. Gothe , L. Guo , H. Hakobyan , M. Hattawy , F. Hauenstein , D. Heddle , A. Hobart , M. Holtrop , D. G. Ireland , E. L. Isupov , H. Jiang , H. S. Jo , S. Joosten , H. Kang , C. Keith , M. Khandaker , W. Kim , F. J. Klein , V. Klimenko , P. Konczykowski , K. Kovacs , A. Kripko , V. Kubarovsky , L. Lanza , S. Lee , P. Lenisa , X. Li , E. Long , I. J. D. MacGregor , D. Marchand , V. Mascagna , D. Matamoros , B. McKinnon , D. Meekins , S. Migliorati , T. Mineeva , M. Mirazita , V. Mokeev , C. Munoz-Camacho , P. Nadel-Turonski , T. Nagorna , K. Neupane , S. Niccolai , M. Osipenko , A. I. Ostrovidov , P. Pandey , M. Paolone , L. L. Pappalardo , R. Paremuzyan , E. Pasyuk , S. J. Paul , W. Phelps , S. K. Phillips , J. Pierce , N. Pilleux , M. Pokhrel , J. W. Price , Y. Prok , A. Radic , T. Reed , J. Richards , G. Rosner , P. Rossi , A. A. Rusova , C. Salgado , A. Schmidt , R. A. Schumacher , Y. G. Sharabian , E. V. Shirokov , U. Shrestha , S. Sirca , K. Slifer , N. Sparveris , M. Spreafico , S. Stepanyan , I. I. Strakovsky , S. Strauch , V. Sulkosky , J. A. Tan , M. Tenorio , N. Trotta , R. Tyson , M. Ungaro , D. W. Upton , S. Vallarino , L. Venturelli , H. Voskanyan , E. Voutier , D. P. Watts , X. Wei , M. H. Wood , N. Zachariou , J. Zhang , M. Zurek

The neutron longitudinal and transverse asymmetries $A^n_1$ and $A^n_2$ have been extracted from deep inelastic scattering of polarized electrons by a polarized $^3$He target at incident energies of 19.42, 22.66 and 25.51 GeV. The…

High Energy Physics - Experiment · Physics 2008-11-26 The E142 Collaboration , P. L. Anthony et al

We discuss the implications of a "constituent quark" structure of the nucleon for the leading (1/Q^2-) power corrections to the spin structure functions. Our basic assumption is the presence of quark-gluon correlations in the nucleon wave…

High Energy Physics - Phenomenology · Physics 2017-08-23 A. V. Sidorov , C. Weiss

We determined the electric form factor of the neutron $G_E^n$ via the reaction ${\vec{d}(\vec{e},e'n)p}$ using a longitudinally polarized electron beam and a frozen, polarized $^{15}ND_3$ target at Jefferson Lab. The knocked out neutrons…

Nuclear Experiment · Physics 2009-11-07 N. Savvinov

Recent progress from Jefferson Lab has significantly improved our understanding of the nucleon spin structure in the high-$x$ region. Results of a precision measurement of the neutron spin asymmetry, $A_1^n$, in the high-$x$ (valence quark)…

Nuclear Experiment · Physics 2014-11-18 Jian-ping Chen

Color polarizabilities of the neutron are extracted from data on the lowest moment of the spin-dependent $g_1$ structure function. New data in the resonance region from Jefferson Lab at $Q^2 \alt 1$ GeV$^2$, in combination with world data…

We have measured proton and deuteron virtual photon-nucleon asymmetries A2p and A2d and structure functions g2p and g2d over the range 0.03<x<0.8 and 1.3<Q2<10 (GeV/c)2 by inelastically scattering polarized electrons off polarized ammonia…

High Energy Physics - Experiment · Physics 2008-11-26 The E143 Collaboration , K. Abe et al

The experimental data on F2 structure functions of the proton and deuteron were used to construct their moments. In particular, recent measurements performed with CLAS detector at Jefferson Lab allowed to extend our knowledge of structure…

High Energy Physics - Phenomenology · Physics 2014-11-18 M. Osipenko , S. Simula , S. Kulagin , G. Ricco , CLAS Collaboration

We have measured the spin structure functions g2p and g2d and the virtual photon asymmetries A2p and A2d over the kinematic range 0.02 < x < 0.8 and 1.0 < Q^2 < 30(GeV/c)^2 by scattering 38.8 GeV longitudinally polarized electrons from…

High Energy Physics - Experiment · Physics 2008-11-26 E155 Collaboration , P. L. Anthony , R. G. Arnold

Recent progress from Jefferson Lab has significantly improved our understanding of the nucleon spin structure in the high-$x$ region. Results from two experiments in Hall A are presented. The first experiment is a precision measurement of…

Nuclear Experiment · Physics 2012-08-27 JLab Hall A , E94-010 Collaborations , : , J. P. Chen

We have measured the spin structure functions $g_1$ and $g_2$ of $^3$He in a double-spin experiment by inclusively scattering polarized electrons at energies ranging from 0.862 to 5.07 GeV off a polarized $^3$He target at a 15.5$^{\circ}$…

High Energy Physics - Experiment · Physics 2012-08-27 010 Collaboration , M. Amarian , L. Auerbach , T. Averett , J. Berthot

Jefferson Lab experiment E01-012 measured the He-3 spin-structure functions and virtual photon asymmetries in the resonance region in the momentum transfer range 1.0<Q**2<4.0(GeV/c)**2. Our data, when compared with existing deep inelastic…

Nuclear Experiment · Physics 2014-11-21 Patricia Solvignon

The electric form factor of the neutron was determined from studies of the reaction He3(e,e'n)pp in quasi-elastic kinematics in Hall A at Jefferson Lab. Longitudinally polarized electrons were scattered off a polarized target in which the…

Nuclear Experiment · Physics 2011-01-28 S. Riordan , S. Abrahamyan , B. Craver , A. Kelleher , A. Kolarkar , J. Miller , G. D. Cates , N. Liyanage , B. Wojtsekhowski , A. Acha , K. Allada , B. Anderson , K. A. Aniol , J. R. M. Annand , J. Arrington , T. Averett , A. Beck , M. Bellis , W. Boeglin , H. Breuer , J. R. Calarco , A. Camsonne , J. P. Chen , E. Chudakov , L. Coman , B. Crowe , F. Cusanno , D. Day , P. Degtyarenko , P. A. M. Dolph , C. Dutta , C. Ferdi , C. Fernandez-Ramirez , R. Feuerbach , L. M. Fraile , G. Franklin , S. Frullani , S. Fuchs , F. Garibaldi , N. Gevorgyan , R. Gilman , A. Glamazdin , J. Gomez , K. Grimm , J. O. Hansen , J. L. Herraiz , D. W. Higinbotham , R. Holmes , T. Holmstrom , D. Howell , C. W. deJager , X. Jiang , M. K. Jones , J. Katich , L. J. Kaufman , M. Khandaker , J. J. Kelly , D. Kiselev , W. Korsch , J. LeRose , R. Lindgren , P. Markowitz , D. J. Margaziotis , S. May-Tal Beck , S. Mayilyan , K. McCormick , Z. E. Meziani , R. Michaels , B. Moffit , S. Nanda , V. Nelyubin , T. Ngo , D. M. Nikolenko , B. Norum , L. Pentchev , C. F. Perdrisat , E. Piasetzky , R. Pomatsalyuk , D. Protopopescu , A. J. R. Puckett , V. A. Punjabi , X. Qian , Y. Qiang , B. Quinn , I. Rachek , R. D. Ransome , P. E. Reimer , B. Reitz , J. Roche , G. Ron , O. Rondon , G. Rosner , A. Saha , M. Sargsian , B. Sawatzky , J. Segal , M. Shabestari , A. Shahinyan , Yu. Shestakov , J. Singh , S. Sirca , P. Souder , S. Stepanyan , V. Stibunov , V. Sulkosky , S. Tajima , W. A. Tobias , J. M. Udias , G. M. Urciuoli , B. Vlahovic , H. Voskanyan , K. Wang , F. R. Wesselmann , J. R. Vignote , S. A. Wood , J. Wright , H. Yao , X. Zhu
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