Measurement of the longitudinal spin transfer to Λ and $\bar{\varLambda}$ hyperons in polarised muon DIS

M. Alekseev,V. Yu. Alexakhin,Yu. Alexandrov,G. D. Alexeev,A. Amoroso,A. Austregesilo,B. Badełek,F. Balestra,J. Ball,J. Barth,G. Baum,Y. Bedfer,J. Bernhard,R. Bertini, M. Bettinelli,R. Birsa,J. Bisplinghoff,P. Bordalo,F. Bradamante,A. Bravar,A. Bressan,G. Brona,E. Burtin,M. P. Bussa,A. Chapiro,M. Chiosso,S. U. Chung,A. Cicuttin,M. Colantoni,M. L. Crespo,S. Dalla Torre,T. Dafni,S. Das,S. S. Dasgupta,O. Yu. Denisov,L. Dhara,V. Diaz,A. M. Dinkelbach,S. V. Donskov,N. Doshita,V. Duic,W. Dünnweber,A. Efremov,P. D. Eversheim,W. Eyrich,M. Faessler,A. Ferrero,M. Finger,H. Fischer,C. Franco,J. M. Friedrich,R. Garfagnini,F. Gautheron,O. P. Gavrichtchouk,R. Gazda,S. Gerassimov,R. Geyer,M. Giorgi,B. Gobbo,S. Goertz,S. Grabmüller,O. A. Grajek,A. Grasso,B. Grube,R. Gushterski,A. Guskov,F. Haas,D. Harrach,T. Hasegawa,J. Heckmann,F. H. Heinsius,M. Hermann,R. Hermann,F. Herrmann,C. Heß,F. Hinterberger,N. Horikawa,Ch. Höppner,N. d’Hose,C. Ilgner,S. Ishimoto,O. Ivanov,Yu. Ivanshin,B. Iven, T. Iwata,R. Jahn,P. Jasinski,G. Jegou,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,E. V. Komissarov,K. Kondo,K. Königsmann,R. Konopka,I. Konorov,V. F. Konstantinov,A. Korzenev,A. M. Kotzinian,O. Kouznetsov,K. Kowalik,M. Krämer, A. Kral,Z. V. Kroumchtein,R. Kuhn,F. Kunne,K. Kurek,J. M. Le Goff,A. A. Lednev,A. Lehmann,S. Levorato,J. Lichtenstadt,T. Liska,A. Maggiora,M. Maggiora,A. Magnon,G. K. Mallot,A. Mann,C. Marchand,J. Marroncle,A. Martin,J. Marzec,F. Massmann,T. Matsuda,A. N. Maximov,W. Meyer,T. Michigami,Yu. V. Mikhailov,M. A. Moinester,A. Mutter,A. Nagaytsev,T. Nagel,J. Nassalski,S. Negrini,F. Nerling,S. Neubert,D. Neyret,V. I. Nikolaenko,A. G. Olshevsky,M. Ostrick,A. Padee,R. Panknin,D. Panzieri,B. Parsamyan,S. Paul,B. Pawlukiewicz-Kaminska,E. Perevalova,G. Pesaro,D. V. Peshekhonov,G. Piragino,S. Platchkov, J. Pochodzalla,J. Polak,V. A. Polyakov,G. Pontecorvo,J. Pretz,C. Quintans,J.-F. Rajotte,S. Ramos,V. Rapatsky,G. Reicherz,D. Reggiani, A. Richter,F. Robinet,E. Rocco,E. Rondio,D. I. Ryabchikov,V. D. Samoylenko,A. Sandacz,H. Santos,M. G. Sapozhnikov,S. Sarkar,G. Sbrizzai,P. Schiavon,C. Schill,L. Schmitt,W. Schröder,O. Yu. Shevchenko,H.-W. Siebert,L. Silva,L. Sinha,A. N. Sissakian,M. Slunecka,G. I. Smirnov,S. Sosio,F. Sozzi,A. Srnka,M. Stolarski,M. Sulc,R. Sulej,S. Takekawa,S. Tessaro,F. Tessarotto,A. Teufel,L. G. Tkatchev,G. Venugopal,M. Virius,N. V. Vlassov,A. Vossen,Q. Weitzel,R. Windmolders,W. Wiślicki,H. Wollny,K. Zaremba,E. Zemlyanichkina,M. Ziembicki,J. Zhao,N. Zhuravlev,A. Zvyagin

European Physical Journal C(2009)

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摘要
The longitudinal polarisation transfer from muons to Λ and \(\bar{\varLambda}\)  hyperons, \(D_{LL}^{\varLambda(\bar{\varLambda})}\) , has been studied in deep-inelastic scattering off an unpolarised isoscalar target at the COMPASS experiment at CERN. The spin transfers to Λ and \(\bar{\varLambda}\)  produced in the current fragmentation region exhibit different behaviours as a function of x and x F . The measured x and x F dependences of D LL Λ are compatible with zero, while \(D_{LL}^{\bar{\varLambda}}\) tends to increase with x F , reaching values of 0.4–0.5. The resulting average values are D LL Λ = −0.012±0.047±0.024 and \(D_{LL}^{\bar{\varLambda}}\) = 0.249±0.056±0.049. These results are discussed in the frame of recent model calculations.
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13.60.Rj, 13.87.Fh, 13.88.+e, 14.20.Jn
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