Di ractive production of 0 ( 770 ) mesons in muon-protoninteractions at 470 GeVE 665

CollaborationM,. R. Adams,M. Aderholz,P. L. Anthony, D. A. Averill,M. D. Baker, B. R. Baller,A. Banerjee,A. A. Bhatti, U. Bratzler,H. M. Braun,T. J. Carroll,H. L. Clark, M. J., Conrad,R. Davisson, I. Derado, F. S. Dietrich,W. Dougherty,T. Dreyer, V. Eckardt, U., Ecker,M. Erdmann, G. Y. Fang,J. Figiel, R. W. Finlay, H. J. Gebauer, D. F. Geesaman, R. S. Guo,J. Haas,C. Halliwell,D. Hantke,K. H. Hicks, H. E. Jackson, D. E. Ja, G. Jancso,D. M. Jansen,Z. Jin,K. Kadija,S. Kaufmann, R. D. Kennedy, R. E., Kinney, H. G. E. Kobrak,A. V. Kotwal,S. Kunori, J. J. Lord,H. J. Lubatti, D. McLeod,P. Madden,S. Magill,A. Manz, H. Melanson, D. G. Michael, H. E. Montgomery, G. J., Mor, R. B. Nickerson,J. Novak, K. Olkiewicz,L. Osborne,R. Otten, V. Papavassiliou,B. Pawlik, F. M. Pipkin, D. H. Potterveld, A. R oser,J. J. Ryan,C. W. Salgado, H., Schellman,M. Schmitt,N. Schmitz,K. P. Sch uler, G. Siegert,A. Skuja, G. A. Snow,S. S oldner-Rembold,P. Spentzouris,P. Stopa, R. A. Swanson, H. Venkataramania, M., Wilhelm,Richard Wilson,W. Wittek,S. A. Wolbers, G. P. Zeller,A. Zghiche,T. Zhao

semanticscholar(2007)

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摘要
The diiractive production of 0 (770) mesons in muon-proton interactions is studied in the kinematic region 0.15 GeV 2 < Q 2 < 20 GeV 2 and 20 GeV < < 420 GeV. The data were obtained in the Fermilab xed-target experiment E665 with primary muons of 470 GeV energy. Results are presented on the Q 2 , x and dependence of the cross section, on the shape of the + ? mass spectrum, on the slope of the diiraction peak and on the production and decay angular distributions of the 0 (770). The cross section for diiractive production of 0 by virtual photons on protons depends mainly on Q 2. At xed Q 2 , no signiicant dependence on x or is observed. The extrapolation to Q 2 = 0 yields a photoproduction cross section of (10:30 0:33) b. The slope of the t 0 distribution has a value of (7:00:2) GeV ?2 , with a tendency to decrease as Q 2 increases. The production and decay angular distributions of the 0 depend strongly on Q 2 and are consistent with s-channel helicity conservation. The ratio R = L == T deduced from the decay angular distributions rises strongly with Q 2 , passing the value of 1 at Q 2 2 GeV 2 .
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