Dynamical Relativistic Effects In Quasielastic 1p-Shell Proton Knockout From O-16

J. Gao,B. D. Anderson,K. A. Aniol,L. Auerbach,F. T. Baker,J. Berthot, W. Bertozzi, Y. Bertin,L. Bimbot,W. U. Boeglin,E. J. Brash,V. Breton,H. Breuer,E. Burtin,J. R. Calarco,G. D. Cates,C. Cavata,C. C. Chang,E. Cisbani,D. S. Dale,A. Deur,B. Diederich,P. Djawotho,J. Domingo,B. Doyle,J.-E. Ducret,M. B. Epstein,L. A. Ewell,J. M. Finn,K. G. Fissum,H. Fonvieille,B. Frois,S. Frullani,F. Garibaldi,A. Gasparian,S. Gilad,A. Glamazdin,C. Glashausser,J. Gomez,V. Gorbenko,T. Gorringe,K. Griffioen,F. W. Hersman,R. Holmes,M. Holtrop,N. d'Hose,C. Howell,G. M. Huber,C. E. Hyde-Wright,M. Iodice,C. W. de Jager,S. Jaminion,M. K. Jones,K. Joo,C. Jutier,W. Kahl,S. Kato, J. J. Kelly,S. Kerhoas,M. Khandaker,M. Khayat,K. Kino,W. Korsh,L. Kramer,K. S. Kumar,G. Kumbartzki,A. Leone,J. J. LeRose, L. Levchuk,M. Liang,R. A. Lindgren,N. Liyanage,G. J. Lolos,R. W. Lourie,R. Madey,K. Maeda,S. Malov,D. M. Manley,D. J. Margaziotis,P. Markowitz,J. Martino,J. S. McCarthy,K. McCormick,J. McIntyre,R. L. J. van der Meer,E. Meziani,J. Mougey,S. Nanda,D. Neyret,E. A. J. M. Offermann,Z. Papandreou,C. F. Perdrisat,R. Perrino,G. G. Petratos,S. Platchkov,R. Pomatsalyuk,D. L. Prout,V. A. Punjabi,T. Pussieux,R. D. Ransome,O. Ravel,Y. Roblin,R. Roche,D. Rowntree,G. A. Rutledge,P. M. Rutt,A. Saha,T. Saito,A. J. Sarty,A. Serdarevic-Offermann,T. P. Smith,A. Soldi,P. Sorokin, P. Souder,R. Suleiman,J. A. Templon,T. Terasawa,L. Todor,H. Tsubota,H. Ueno,G. M. Urciuoli,P. Vernin,S. van Verst,H. Voskanyan,J. W. Watson,L. B. Weinstein,K. Wijesooriya,R. Wilson,D. G. Zainea,V. Zeps, J. Zhao,Z.-L. Zhou,H. Voskanyan,J. Watson,L. Weinstein,K. Wijesooriya,R. Wilson,B. Wojtsekhowski,D. Zainea, V. Zeps, J. Zhao,Z.-L. Zhou

PHYSICAL REVIEW LETTERS(2000)

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摘要
We have measured the cross section for quasielastic 1p-shell proton knockout in the O-16(e,e'p) reaction at omega = 0.439 GeV and Q(2) = 0.8 (GeV/c)(2) for missing momentum P-miss less than or equal to 355 MeV/c. We have extracted the response functions RL+TT, R-T, R-LT, and the left-right asymmetry, A(LT), for the 1p(1/2) and the 1p(3/2) states. The data are well described by relativistic distorted wave impulse approximation calculations. At large P-miss, the structure observed in A(LT) indicates the existence of dynamical relativistic effects.
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关键词
relativistic effects,cross section
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