Leading and Next-to-Leading Order Gluon Polarisation in the Nucleon and Longitudinal Double Spin Asymmetries from Open Charm Muoproduction

C. Adolph,M. G. Alekseev,V. Yu. Alexakhin,Yu. Alexandrov,G. D. Alexeev,A. Amoroso,A. A. Antonov,A. Austregesilo,B. Badelek,F. Balestra,J. Barth,G. Baum,Y. Bedfer,A. Berlin,J. Bernhard,R. Bertini,M. Bettinelli,K. Bicker,J. Bieling,R. Birsa,J. Bisplinghoff,P. Bordalo,F. Bradamante,C. Braun,A. Bravar,A. Bressan,M. Buechele,E. Burtin,L. Capozza,M. Chiosso,S. U. Chung,A. Cicuttin,M. L. Crespo,S. Dalla Torre,S. Das,S. S. Dasgupta,S. Dasgupta,O. Yu. Denisov,L. Dhara,S. V. Donskov,N. Doshita,V. Duic,W. Duennweber,M. Dziewiecki,A. Efremov,C. Elia,P. D. Eversheim,W. Eyrich,M. Faessler,A. Ferrero,A. Filin,M. Finger,M. Finger Jr,H. Fischer,C. Franco,N. du Fresne von Hohenesche,J. M. Friedrich,V. Frolov,R. Garfagnini,F. Gautheron,O. P. Gavrichtchouk,S. Gerassimov,R. Geyer,M. Giorgi,I. Gnesi,B. Gobbo,S. Goertz,S. Grabmueller,A. Grasso,B. Grube,R. Gushterski,A. Guskov,T. Guthoerl,F. Haas,D. von Harrach,F. H. Heinsius,F. Herrmann,C. Hess,F. Hinterberger,N. Horikawa,Ch. Hoeppner,N. d'Hose,S. Huber,S. Ishimoto,O. Ivanov,Yu. Ivanshin,T. Iwata,R. Jahn,V. Jary,P. Jasinski,R. Joosten,E. Kabuss,D. Kang,B. Ketzer,G. V. Khaustov,Yu. A. Khokhlov,Yu. Kisselev,F. Klein,K. Klimaszewski,S. Koblitz,J. H. Koivuniemi,V. N. Kolosov,K. Kondo,K. Koenigsmann,I. Konorov,V. F. Konstantinov,A. Korzenev,A. M. Kotzinian,O. Kouznetsov,M. Kraemer,Z. V. Kroumchtein,F. Kunne,K. Kurek,L. Lauser,A. A. Lednev,A. Lehmann,S. Levorato,J. Lichtenstadt,T. Liska,A. Maggiora,A. Magnon,N. Makke,G. K. Mallot,A. Mann,C. Marchand,A. Martin,J. Marzec,T. Matsuda,G. Meshcheryakov,W. Meyer,T. Michigami,Yu. V. Mikhailov,A. Morreale,A. Mutter,A. Nagaytsev,T. Nagel,F. Nerling,S. Neubert,D. Neyret,V. I. Nikolaenko,W. -D. Nowak,A. S. Nunes,A. G. Olshevsky,M. Ostrick,A. Padee,R. Panknin,D. Panzieri,B. Parsamyan,S. Paul,E. Perevalova,G. Pesaro,D. V. Peshekhonov,G. Piragino,S. Platchkov,J. Pochodzalla,J. Polak,V. A. Polyakov,J. Pretz,M. Quaresma,C. Quintans,J. -F. Rajotte,S. Ramos,V. Rapatsky,G. Reicherz,E. Rocco,E. Rondio,N. S. Rossiyskaya,D. I. Ryabchikov,V. D. Samoylenko,A. Sandacz,M. G. Sapozhnikov,S. Sarkar,I. A. Savin,G. Sbrizzai,P. Schiavon,C. Schill,T. Schlueter,A. Schmidt,K. Schmidt,L. Schmitt,H. Schmieden,K. Schoenning,S. Schopferer,M. Schott,O. Yu. Shevchenko,L. Silva,L. Sinha,A. N. Sissakian,M. Slunecka,G. I. Smirnov,S. Sosio,F. Sozzi,A. Srnka,L. Steiger,M. Stolarski,M. Sulc,R. Sulej,H. Suzuki,P. Sznajder,S. Takekawa,J. Ter Wolbeek,S. Tessaro,F. Tessarotto,L. G. Tkatchev,S. Uhl,I. Uman,M. Vandenbroucke,M. Virius,N. V. Vlassov,L. Wang,T. Weisrock,M. Wilfert,R. Windmolders,W. Wislicki,H. Wollny,K. Zaremba,M. Zavertyaev,E. Zemlyanichkina,M. Ziembicki,N. Zhuravlev,A. Zvyagin

Physical Review D(2013)

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摘要
The gluon polarization in the nucleon was measured using open charm production by scattering 160 GeV/c polarized muons off longitudinally polarized protons or deuterons. The data were taken by the COMPASS Collaboration between 2002 and 2007. A detailed account is given of the analysis method that includes the application of neural networks. Several decay channels of D-0 mesons are investigated. Longitudinal spin asymmetries of the D meson production cross sections are extracted in bins of D-0 transverse momentum and energy. At leading order QCD accuracy, the average gluon polarization is determined as Delta g/g (LO) = -0.06 +/- 0: 21(stat.) +/- 0. 08(syst.) at the scale mu(2) approximate to 13 (GeV/c)(2) and an average gluon momentum fraction x approximate to 0.11. The average gluon polarization is also obtained at next-to-leading order QCD accuracy as Delta g/g NLO = -0.13 +/- 0.15(stat.).+/- 0.15(syst.) at the scale mu(2) approximate to 13 (GeV/c)(2) and x approximate to 0.20. DOI:10.1103/PhysRevD.87.052018
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neural network,compass
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