Tvaskis, V.; Blok, H. P.; Christy, M. E.; Baker, O. K.; Cochran, A.; Cole, L.; Gasparian, A.; Nazaryan, V.; Sato, Y.; Uzzle, A.; Arrington, J.; Jackson, H. E.; Potterveld, D. H.; Asaturyan, R.; Mkrtchyan, H.; Stepanyan, S.; Tadevosian, V.; Bosted, P.; Ent, R.; Fenker, H. C.
arXiv e-print [ PDF ]2007
arXiv e-print [ PDF ]2007
AbstractAbstract
[en] We report on a study of the longitudinal to transverse cross section ratio, R=σL/σT, at low values of x and Q2, as determined from inclusive inelastic electron-hydrogen and electron-deuterium scattering data from Jefferson Laboratory Hall C spanning the four-momentum transfer range 0.06< Q2<2.8 GeV2. Even at the lowest values of Q2, R remains nearly constant and does not disappear with decreasing Q2, as might be expected. We find a nearly identical behavior for hydrogen and deuterium
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(c) 2007 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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ACCELERATORS, BEAMS, ELEMENTS, FUNCTIONS, HYDROGEN ISOTOPES, INELASTIC SCATTERING, INTERACTIONS, ISOTOPES, LEPTON BEAMS, LEPTON-BARYON INTERACTIONS, LEPTON-HADRON INTERACTIONS, LEPTON-NUCLEON INTERACTIONS, LIGHT NUCLEI, LINEAR ACCELERATORS, MOMENTUM TRANSFER, NONMETALS, NUCLEI, ODD-ODD NUCLEI, PARTICLE BEAMS, PARTICLE INTERACTIONS, SCATTERING, STABLE ISOTOPES
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AbstractAbstract
[en] The Λ3,4H and Λ4H hypernuclear bound states have been observed for the first time in kaon electroproduction on 3,4He targets. The production cross sections have been determined at Q2=0.35 GeV2 and W=1.91 GeV. For either hypernucleus the nuclear form factor is determined by comparing the angular distribution of the 3,4He(e,e'K+)Λ3,4H processes to the elementary cross section 1H(e,eK+)Λ on the free proton, measured during the same experiment
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(c) 2004 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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BARYONS, BASIC INTERACTIONS, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, BOSONS, CHARGED-PARTICLE REACTIONS, DISTRIBUTION, ELECTROMAGNETIC INTERACTIONS, ELEMENTARY PARTICLES, ENERGY RANGE, FERMIONS, GEV RANGE, HADRONS, HYDROGEN ISOTOPES, INTERACTIONS, ISOTOPES, KAONS, LEPTON REACTIONS, LIGHT NUCLEI, MESONS, NUCLEAR FRAGMENTS, NUCLEAR REACTIONS, NUCLEI, NUCLEONS, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, PARTICLE INTERACTIONS, PARTICLE PRODUCTION, PARTICLE PROPERTIES, PSEUDOSCALAR MESONS, RADIOISOTOPES, STRANGE MESONS, STRANGE PARTICLES, TARGETS, YEARS LIVING RADIOISOTOPES
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Reichelt, T.; Madey, R.; Semenov, A.Yu.; Taylor, S.; Aghalarian, A.; Crouse, E.; MacLachlan, G.; Plaster, B.; Tajima, S.; Tireman, W.; Yan, C.Y.; Ahmidouch, A.; Anderson, B.D.; Asaturian, R.; Baker, O.; Baldwin, A.R.; Breuer, H.; Carlini, R.; Christy, E.; Churchwell, S.; Cole, L.; Danagulian, S.; Day, D.; Elaasar, M.; Ent, R.; Farkhondeh, M.; Fenker, H.; Finn, J.M.; Gan, L.; Garrow, K.; Gueye, P.; Howell, C.; Hu, B.; Jones, M.K.; Kelly, J.J.; Keppel, C.; Khandaker, M.; Kim, W.Y.; Kowalski, S.; Lung, A.; Mack, D.; Manley, D.M.; Markowitz, P.; Mitchell, J.; Mkrtchian, H.; Opper, H.; Perdrisat, C.; Punjabi, V.; Raue, B.; Reichelt, T.; Reinhold, J.; Roche, J.; Sato, Y.; Seo, W.; Simicevic, N.; Smith, G.; Stepanian, S.; Tadevosian, V.; Tang, L.; Ulmer, P.; Vulcan, W.; Watson, J.W.; Wells, S.; Wesselmann, F.; Wood, S.; Yan, C.; Yang, S.; Yuan, L.; Zhang, W.M.; Zhu, H.; Zhu, X.; Arenhovel, H.
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2003
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2003
AbstractAbstract
[en] The ratio Gcn/Gmn of the electric to the magnetic form factor of the neutron has been measured by analyzing the polarization of the recoiling neutron in quasi-elastic scattering of longitudinally polarized electrons from deuterium at the Q2 values of 0.45, 1.15, and 1.47 (GeV/c)2. The experiment has been performed in Hall C of the Thomas Jefferson National Accelerator Facility. With Gmn being known G can be deduced. The preliminary results show that the lowest Q2 points follow the Galster parameterization and that the 1.47 (GeV/c)2 point rises above this parameterization
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22 Oct 2003; 3 p; QNP 2002; Juelich (Germany); 9-14 Jun 2002; DOE/ER--40150-2638; AC--05-84ER40150; Available from Thomas Jefferson National Accelerator Facility, Newport News, VA (US)
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Report
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Conference
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ACCELERATORS, BARYONS, BEAMS, DIRECT REACTIONS, ELEMENTARY PARTICLES, FERMIONS, HADRONS, HYDROGEN ISOTOPES, ISOTOPES, LEPTON BEAMS, LIGHT NUCLEI, LINEAR ACCELERATORS, NUCLEAR REACTIONS, NUCLEI, NUCLEONS, ODD-ODD NUCLEI, PARTICLE BEAMS, PARTICLE PROPERTIES, QUASI-FREE REACTIONS, SCATTERING, STABLE ISOTOPES
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Tvaskis, V.; Arrington, J.; Potterveld, D. H.; Asaturyan, R.; Mkrtchyan, H.; Stepanyan, S.; Tadevosian, V.; Baker, O. K.; Christy, M. E.; Cochran, A.; Gasparian, A.; Blok, H. P.; Bosted, P.; Ent, R.; Mack, D. J.; Smith, G.; Wood, S. A.; Boswell, M.; Bruell, A.; Filippone, B. W.
arXiv e-print [ PDF ]2010
arXiv e-print [ PDF ]2010
AbstractAbstract
[en] Measurements of the proton and deuteron F2 structure functions are presented. The data, taken at Jefferson Lab Hall C, span the four-momentum transfer range 0.06< Q2<2.8 GeV2 and Bjorken x values from 0.009 to 0.45, thus extending the knowledge of F2 to low values of Q2 at low x. Next-to-next-to-leading-order calculations using recent parton distribution functions start to deviate from the data for Q2<2 GeV2 at the low and high x values. Down to the lowest value of Q2, the structure function is in good agreement with a parametrization of F2 based on data that have been taken at much higher values of Q2 or much lower values of x, and which are constrained by data at the photon point. The ratio of the deuteron and proton structure functions at low x remains well described by a logarithmic dependence on Q2 at low Q2.
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(c) 2010 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA)
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Frolov, V.V.; Adams, G.S.; Davidson, R.M.; Klusman, M.; Mukhopadhyay, N.C.; Napolitano, J.; Nozar, M.; Price, J.W.; Stoler, P.; Witkowski, M.; Bosted, P.; Armstrong, C.S.; Meekins, D.; Assamagan, K.; Avery, S.; Baker, O.K.; Eden, T.; Gaskell, D.; Gueye, P.; Hinton, W.; Keppel, C.; Madey, R.; Niculescu, G.; Niculescu, I.; Tang, L.; Ahmidouch, A.; Madey, R.; Kim, W.; Baker, O.K.; Burkert, V.; Carlini, R.; Dunne, J.; Ent, R.; Keppel, C.; Mack, D.; Mitchell, J.; Tang, L.; Wood, S.; Koltenuk, D.; Minehart, R.; Mkrtchyan, H.; Tadevosian, V.1999
AbstractAbstract
[en] We studied the electroproduction of the Δ(1232) resonance via the reaction p(e,e'p)π0 at four-momentum transfers Q2=2.8 and 4.0 GeV2 . This is the highest Q2 for which exclusive resonance electroproduction has ever been observed. Decay angular distributions for Δ→pπ0 were measured over a wide range of barycentric energies covering the resonance. The N - Δ transition form factor G*M and ratios of resonant multipoles E1+/M1+ and S1+/M1+ were extracted from the decay angular distributions. These ratios remain small, indicating that perturbative QCD is not applicable for this reaction at these momentum transfers. copyright 1998 The American Physical Society
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BARYONS, BASIC INTERACTIONS, BOSONS, DELTA BARYONS, ELECTROMAGNETIC INTERACTIONS, ELECTRON-NUCLEON INTERACTIONS, ELEMENTARY PARTICLES, FERMIONS, FIELD THEORIES, HADRONS, INTERACTIONS, LEPTON-BARYON INTERACTIONS, LEPTON-HADRON INTERACTIONS, LEPTON-NUCLEON INTERACTIONS, MESONS, N*BARYONS, PARTICLE INTERACTIONS, PARTICLE PRODUCTION, PIONS, PSEUDOSCALAR MESONS, QUANTUM FIELD THEORY
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Juerg Reinhold; David Abbott; Abdellah Ahmidouch; Pawel Ambrozewicz; Chris Armstrong; John Arrington; Razmik Asaturyan; Assamagan, K.; Steven Avery; Kevin Bailey; Baker, Oliver K.; Shelton Beedoe; Bitao, H.; Werner Boeglin; Herbert Breuer; Brown, D.S.; Roger Carlini; Jinseok Cha; Nicholas Chant; Christy, E.; Anthony Cochran; Leon Cole; Collins, G.; Cothran, C.; Crowder, J.; Cummings, W.G.; Samuel Danagoulian; Frank Dohrmann; Fraser Duncan; Jim Dunne; Dipangkar Dutta; Tom Eden; Mostafa Elaasar; Rolf Ent; Lars Ewell; Howard Fenker; Fortune, H.T.; Yu Fujii; Liping Gan; Haiyan Gao; Kenneth Garrow; Donald Geesaman; Paul Gueye; Kenneth Gustafsson; Kawtar Hafidi; Jens-Ole Hansen; Wendy Hinton; Hal Jackson; Juengst, H.; Cynthia Keppel; Andi Klein; Doug Koltenuk; Yongguang Liang; Hongxiu Liu, J.; Allison Lung; David Mack; Richard Madey; Markowitz, Pete; Martoff, C.J.; David Meekins; Joseph Mitchell; Miyoshi, T.; Hamlet Mkrtchyan; Mohring, R.; Mtingwa, S.K.; Mueller, B.; Tom O'Neill; Gabriel Niculescu; Ioana Niculescu; Dave Potterveld; John Price; Brian Raue; Reimer, P.E.; Julie Roche; Philip Roos; Murad Sarsour; Yoshinori Sato; Savage, G.; Reyad Sawafta; Schiffer; Segel, Ralph; Andrei Semenov; Stepan Stepanyan; Tadevosian, V.; Tajima, S.; Liguang Tang; Terburg, B.; Uzzle, Alicia J.P.; Stephen Wood; Yamaguchi, H.; Chen Yan; Chen Yan; Lulin Yuan; Ben Zeidman; Marko Zeier; Beni Zihlmann
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research ER (United States)2001
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research ER (United States)2001
AbstractAbstract
No abstract available
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Source
JLAB-PHY--01-38; DOE/ER--40150-2097; AC05-84ER40150; Contr to FB 16, Taipei, Taiwan, China, 6-10 Mar 2000
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Journal Article
Journal
Nuclear Physics. A; ISSN 0375-9474; ; v. 684; [5 p.]
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Niculescu, G.; Gueye, P.; Ahmidouch, A.; Assamagan, K.; Avery, S.; Baker, O.K.; Beard, K.; Cha, J.; Eden, T.; Harvey, M.; Hinton, W.; Keppel, C.; Madey, R.; Niculescu, I.; Savage, G.; Tang, L.; Williams, R.; Mohring, R.M.; Beise, E.; Breuer, H.; Chang, C.C.; Chant, N.; Collins, G.; Duncan, F.; Ewell, L.; Gustafsson, K.K.; Lung, A.; Roos, P.; Abbott, D.; Baker, O.K.; Carlini, R.; Dunne, J.; Ent, R.; Keppel, C.; Mack, D.; Majewski, S.; Mitchell, J.; Tang, L.; Vulcan, W.; Wood, S.; Yan, C.; Ahmidouch, A.; Madey, R.; Amatuni, T.A.; Mkrtchyan, H.; Stepanyan, S.; Tadevosian, V.; Angelescu, T.; Mihul, A.; Teodorescu, L.; Bailey, K.; Cummings, W.; Geesaman, D.F.; Hansen, J.; Potterveld, D.; Reinhold, J.; Zeidman, B.; Beedoe, S.; Danagoulian, S.; Jackson, C.; Mtingwa, S.; Sawafta, R.; Volmer, J.; Eyraud, L.; Furget, C.; Kox, S.; Real, J.1998
AbstractAbstract
[en] The 1H( e,thinspe'K+)Λ reaction was studied as a function of the squared four-momentum transfer, Q2 , and the virtual photon polarization, var-epsilon . For each of four Q2 settings, 0.52, 0.75, 1.00, and 2.00 (GeV/c)2 , the longitudinal and transverse virtual photon cross sections were extracted in measurements at three virtual photon polarizations. The Q2 dependence of the σL/σT ratio differs significantly from current theoretical predictions. This, combined with the precision of the measurement, implies a need for revision of existing calculations. copyright 1998 The American Physical Society
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