Measurement of the e+e-→J/ψcc̄ cross section at s 10.6GeV

P. Pakhlov,H. Aihara,K. Arinstein,T. Aushev, A. M. Bakich,Vladislav Balagura,E. L. Barberio, A. Bay,K. Belous,V. Bhardwaj, A.E. Bondar, M. Bračko,Jolanta Brodzicka,T. E. Browder,M. C. Chang,P. Chang,A. Chen, B. G. Cheon, R. Chistov,S. K. Choi, Y. Choi, M. Danilov,M. Dash, A. Drutskoy, W. Dungel,S.I. Eidelman,D. Epifanov, N. Gabyshev, P. Goldenzweig, B. Golob, H. Ha, B. Y. Han,K. Hayasaka, H. Hayashii,Masashi Hazumi,Yasuyuki Horii,Y. Hoshi, W. S. Hou,Y. B. Hsiung, H. J. Hyun,T. Iijima,K. Inami, A. Ishikawa,Hirokazu Ishino, Y. Iwasaki,N. J. Joshi,D. H. Kah,H. Kaji, H. Kawai, T. Kawasai,H. Kichimi, H. O. Kim, Y. I. Kim,K. Kinoshita,B. R. Ko, S. Korpar,P. Krian,P. Krokovny,A. Kuzmin,Y. J. Kwon,S. H. Kyeong, J. S. Lange,M. J. Lee, S. E. Lee,T. Lesiak,S. W. Lin,Yang Liu,D. Liventsev, R. Louvot, F. Mandl, A. Matyja, S. McOnie, H. Miyata, Y. Miyazaki,R. Mizuk,Yasushi Nagasaka, M. Nakao,H. Nakazawa,K. Nishimura,O. Nitoh, S. Ogawa, T. Ohshima, S. Okuno, H. Ozaki,G. Pakhlova, H. Palka,C. W. Park,H. Park,H. K. Park,K. S. Park, R. Pestotnik,L. E. Piilonen,Anton Poluektov,H. Sahoo,Y. Sakai,O. Schneider, C. Schwanda, K. Senyo,M. E. Sevior, M. Shapkin

Physical Review D(2009)

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摘要
We present a new measurement of the e(+)e(-)-> J/psi c(c)over bar cross section where the c(c)over bar pair can fragment either into charmed hadrons or a charmonium state. In the former case the J/psi and a charmed hadron are reconstructed, while the latter process is measured using the recoil mass technique, which allows the identification of two-body final states without reconstruction of one of the charmonia. The measured e(+)e(-)-> J/psi c(c)over bar cross section is (0.74 +/- 0.08(-0.08)(+0.09)) pb, and the e(+)e(-)-> J/psi Xnon-c(c)over bar cross section is (0.43 +/- 0.09 +/- 0.09) pb. We note that the measured cross sections are obtained from a data sample with the multiplicity of charged tracks in the event larger than 4; corrections for the effect of this requirement are not performed as this cannot be done in a model-independent way. The analysis is based on a data sample with an integrated luminosity of 673 fb(-1) recorded near the Upsilon(4S) resonance with the Belle detector at the KEKB e(+)e(-) asymmetric-energy collider.
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