S. Strauch; S. Dieterich; K.A. Aniol; J.R.M. Annand; O.K. Baker; W. Bertozzi; M. Boswell; E.J. Brash; Z. Chai; J.-P. Chen; M.E. Christy; E. Chudakov; A. Cochran; R. De Leo; R. Ent; M.B. Epstein; J.M. Finn; K.G. Fissum; T.A. Forest; S. Frullani; F. Garibaldi; A. Gasparian; O. Gayou; S. Gilad; R. Gilman; C. Glashausser; J. Gomez; V. Gorbenko; P.L.J. Gueye; J.O. Hansen; D.W. Higinbotham; B. Hu; C.E. Hyde-Wright; D.G. Ireland; C. Jackson; C.W. de Jager; X. Jiang; C. Jones; M.K. Jones; J.D. Kellie; J.J. Kelly; Cynthia E. Keppel; G. Kumbartzki; Michael Kuss; J.J. LeRose; K. Livingston; Nilanga Liyanage; R.W. Lourie; S. Malov; D.J. Margaziotis; D. Meekins; R. Michaels; J.H. Mitchell; S.K. Nanda; J. Nappa; C.F. Perdrisat; Vina A. Punjabi; R.D. Ransome; R. Roche; G. Rosner; M. Rvachev; R. Sabatie; A. Saha; A. Sarty; J.M. Udias; P.E. Ulmer; G.M. Urciuoli; J.F.J can den Brand; J.R. Vignote; D.P. Watts; L.B. Weinstein; K. Wijesooriya; B. Wojtsekhowski
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
AbstractAbstract
[en] We have measured the proton recoil polarization in the 4He(polarized-e, e-prime, p)3H reaction at Q2 = 0.5, 1.0, 1.6, and 2.6 (GeV/c)2. The measured ratio of polarization transfer coefficients differs from a fully relativistic calculation, favoring the inclusion of a predicted medium modification of the proton form factors based on a quark-meson coupling model. In contrast, the measured induced polarizations agree reasonably well with the fully relativistic calculation indicating that the treatment of final-state interactions is under control
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Source
1 Nov 2002; 381 Kilobytes; DOE/ER--40150-2318; AC05-84ER40150; Available from PURL: https://www.osti.gov/servlets/purl/804051-ce3Rhe/native/; No Journal information given for this preprint
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Miscellaneous
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High energy angular distribution measurements of the exclusive deuteron photodisintegration reaction
Schulte, E. C.; A. Afanasev; M. Amarian; K. Aniol; S. Becher; K. Benslama; L. Bimbot; P. Bosted; E. Brash; J. Calarco; Z. Chai; C. Chang; T. Chang; J. P. Chen; S. Choi; E. Chudakov; S. Churchwell; D. Crovelli; S. Dieterich; S. Dumalski; D. Dutta; M. Epstein; K. Fissum; B. Fox; S. Frullani; H. Gao; J. Gao; F. Garibaldi; O. Gayou; R. Gilman; A. Glamazdin; C. Glashausser; J. Gomez; V. Gorbenko; J.-O. Hansen; R. J. Holt; J. Hovdebo; G. M. Huber; C. W. de Jager; X. Jiang; C. Jones; M. K. Jones; J. Kelly; E. Kinney; E. Kooijman; G. Kumbartzki; M. Kuss; J. LeRose; M. Liang; R. Lindgren; N. Liyanage; S. Malov; D. Margaziotis; P. Markowitz; K. McCormick; D. Meekins; Z.-E. Meziani; R. Michaels; J. Mitchell; L. Morand; C. Perdrisat; R. Pomatsalyuk; V. Punjabi; A. Radyushkin; R. Ransome; R. Roche; M. Rvachev; A. Saha; A. Sarty; D. Simon; S. Strauch; R. Suleiman; L. Todor; P. Ulmer; G. M. Urciuoli; K. Wijesooriya; B. Wojtsekhowski; F. Xiong; W. Xu
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
AbstractAbstract
[en] The first complete measurements of the angular distributions of the two-body deuteron photodisintegration differential cross section at photon energies above 1.6 GeV were performed at the Thomas Jefferson National Accelerator Facility. The results show a persistent forward-backward asymmetry up to Egamma = 2.4 GeV, the highest-energy measured in this experiment. The Hard Rescattering and the Quark-Gluon string models are in fair agreement with the results
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Secondary Subject
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JLAB-PHY--02-60; DOE/ER--40150-2397; AC05-84ER40150; Phys. Rev. C 66, 042201(R) (2002) (5 pages) (October 2002)
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Journal Article
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Physical Review. C, Nuclear Physics; ISSN 0556-2813; ; v. 66; [5 p.]
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M. Amarian; L. Auerbach; T. Averett; J. Berthot; P. Bertin; B. Bertozzi; T. Black; E. Brash; D. Brown; E. Burtin; J. Calarco; G. Cates; Z. Chai; J.P. Chen; Seon-ho Choi; E. Chudakov; E. Cisbani; C.W. de Jager; A. Deur; R. DiSalvo; S. Dieterich; P. Djawotho; M. Finn; K. Fissum; H. Fonvieille; S. Frullani; H. Gao; J. Gao; F. Garibaldi; A. Gasparian; S. Gilad; R. Gilman; A. Glamazdin; C. Glashausser; E. Goldberg; J. Gomez; V. Gorbenko; J.O. Hansen; B. Hersman; R. Holmes; G.M. Huber; E. Hughes; B. Humensky; S. Incerti; M. Iodice; S. Jensen; X. Jiang; C. Jones; G. Jones; M. Jones; C. Jutier; A. Ketikyan; I. Kominis; W. Korsch; K. Kramer; K. Kumar; G. Kumbartzki; M. Kuss; E. Lakuriqi; G. Laveissiere; J. Lerose; M. Liang; N. Liyanage; G. Lolos; S. Malov; J. Marroncle; K. McCormick; R. Mckeown; Z.E. Meziani; R. Michaels; J. Mitchell; Z. Papandreou; T. Pavlin; G.G. Petratos; D. Pripstein; D. Prout; R. Ransome; Y. Roblin; D. Rowntree; M. Rvachev; F. Sabatie; A. Saha; K. Slifer; P. Souder; T. Saito; S. Strauch; R. Suleiman; K. Takahashi; S. Teijiro; L. Todor; H. Tsubota; H. Ueno; G. Urciuoli; R. Van der Meer; P. Vernin; H. Voskanian; B. Wojtsekhowski; F. Xiong; W. Xu; J.C. Yang; B. Zhang; P. Zolnierczuk
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2004
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2004
AbstractAbstract
[en] We have measured the spin structure functions g1 and g2 of 3He in a double-spin experiment by inclusively scattering polarized electrons at energies ranging from 0.862 to 5.07 GeV off a polarized 3He target at a 15.5o scattering angle. Excitation energies covered the resonance and the onset of the deep inelastic regions. We have determined for the first time the Q2 evolution of Γ1(Q2)=/int01 g1(x,Q2) dx, Γ2(Q2)=/int01 g2(x,Q2) dx and d2 (Q2) = /int01 x 2[2g1(x,Q2) + 3g2(x,Q2)] dx for the neutron in the range 0.1 GeV2 /leq Q2 /leq 0.9 GeV2 with good precision. Γ1(Q2) displays a smooth variation from high to low Q2. The Burkhardt-Cottingham sum rule holds within uncertainties and d2 is non-zero over the measured range
Primary Subject
Source
JLAB-PHY--03-21; DOE/ER--40150-2636; HEP-EX--0310003; AC--05-84ER40150
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Journal Article
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