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Search for double charmonium decays of the P-wave spin-triplet bottomonium statesopen access

Authors
Shen, CP[Shen, C. P.]Yuan, CZ[Yuan, C. Z.]Iijima, T[Iijima, T.]Adachi, I[Adachi, I.]Aihara, H[Aihara, H.]Arinstein, K[Arinstein, K.]Asner, DM[Asner, D. M.]Aushev, T[Aushev, T.]Bakich, AM[Bakich, A. M.]Bhuyan, B[Bhuyan, B.]Bischofberger, M[Bischofberger, M.]Bozek, A[Bozek, A.]Bracko, M[Bracko, M.]Browder, TE[Browder, T. E.]Chang, MC[Chang, M. -C.]Chen, A[Chen, A.]Cheon, BG[Cheon, B. G.]Chilikin, K[Chilikin, K.]Chistov, R[Chistov, R.]Cho, IS[Cho, I. -S.]Cho, K[Cho, K.]Choi, SK[Choi, S. -K.]Choi, Y[Choi, Y.]Dalseno, J[Dalseno, J.]Drasal, Z[Drasal, Z.]Drutskoy, A[Drutskoy, A.]Eidelman, S[Eidelman, S.]Fast, JE[Fast, J. E.]Gaur, V[Gaur, V.]Gabyshev, N[Gabyshev, N.]Garmash, A[Garmash, A.]Goh, YM[Goh, Y. M.]Haba, J[Haba, J.]Hara, T[Hara, T.]Hayasaka, K[Hayasaka, K.]Hayashii, H[Hayashii, H.]Horii, Y[Horii, Y.]Hoshi, Y[Hoshi, Y.]Hou, WS[Hou, W. -S.]Hyun, HJ[Hyun, H. J.]Ishikawa, A[Ishikawa, A.]Itoh, R[Itoh, R.]Iwabuchi, M[Iwabuchi, M.]Iwashita, T[Iwashita, T.]Julius, T[Julius, T.]Kang, JH[Kang, J. H.]Kawasaki, T[Kawasaki, T.]Kim, HJ[Kim, H. J.]Kim, HO[Kim, H. O.]Kim, JB[Kim, J. B.]Kim, KT[Kim, K. T.]Kim, MJ[Kim, M. J.]Kim, YJ[Kim, Y. J.]Ko, BR[Ko, B. R.]Koblitz, S[Koblitz, S.]Kodys, P[Kodys, P.]Korpar, S[Korpar, S.]Krizan, P[Krizan, P.]Krokovny, P[Krokovny, P.]Kumita, T[Kumita, T.]Kwon, YJ[Kwon, Y. -J.]Lange, JS[Lange, J. S.]Lee, SH[Lee, S. -H.]Li, J[Li, J.]Libby, J[Libby, J.]Lim, CL[Lim, C. -L.]Liu, C[Liu, C.]Liu, ZQ[Liu, Z. Q.]Liventsev, D[Liventsev, D.]Louvot, R[Louvot, R.]McOnie, S[McOnie, S.]Miyabayashi, K[Miyabayashi, K.]Miyata, H[Miyata, H.]Miyazaki, Y[Miyazaki, Y.]Mizuk, R[Mizuk, R.]Mohanty, GB[Mohanty, G. B.]Moll, A[Moll, A.]Mori, T[Mori, T.]Muramatsu, N[Muramatsu, N.]Mussa, R[Mussa, R.]Nakano, E[Nakano, E.]Nakao, M[Nakao, M.]Nakazawa, H[Nakazawa, H.]Nishida, S[Nishida, S.]Nishimura, K[Nishimura, K.]Nitoh, O[Nitoh, O.]Ogawa, S[Ogawa, S.]Ohshima, T[Ohshima, T.]Okuno, S[Okuno, S.]Olsen, SL[Olsen, S. L.]Onuki, Y[Onuki, Y.]Pakhlova, G[Pakhlova, G.]Park, CW[Park, C. W.]Park, HK[Park, H. K.]Pedlar, TK[Pedlar, T. K.]Petric, M[Petric, M.]Piilonen, LE[Piilonen, L. E.]Poluektov, A[Poluektov, A.]Ritter, M[Ritter, M.]Rohrken, M[Roehrken, M.]Sahoo, H[Sahoo, H.]Sakai, Y[Sakai, Y.]Sanuki, T[Sanuki, T.]Sato, Y[Sato, Y.]Schneider, O[Schneider, O.]Schwanda, C[Schwanda, C.]Senyo, K[Senyo, K.]Seon, O[Seon, O.]Shapkin, M[Shapkin, M.]Shibata, TA[Shibata, T. -A.]Shiu, JG[Shiu, J. -G.]Sibidanov, A[Sibidanov, A.]Simon, F[Simon, F.]Singh, JB[Singh, J. B.]Smerkol, P[Smerkol, P.]Sohn, YS[Sohn, Y. -S.]Solovieva, E[Solovieva, E.]Stanic, S[Stanic, S.]Staric, M[Staric, M.]Sumiyoshi, T[Sumiyoshi, T.]Tatishvili, G[Tatishvili, G.]Teramoto, Y[Teramoto, Y.]Tsuboyama, T[Tsuboyama, T.]Uchida, M[Uchida, M.]Uehara, S[Uehara, S.]Unno, Y[Unno, Y.]Uno, S[Uno, S.]Urquijo, P[Urquijo, P.]Varner, G[Varner, G.]Varvell, KE[Varvell, K. E.]Wang, CH[Wang, C. H.]Wang, P[Wang, P.]Wang, XL[Wang, X. L.]Watanabe, M[Watanabe, M.]Watanabe, Y[Watanabe, Y.]Won, E[Won, E.]Yamashita, Y[Yamashita, Y.]Yusa, Y[Yusa, Y.]Zhang, ZP[Zhang, Z. P.]Zhilich, V[Zhilich, V.]Zhulanov, V[Zhulanov, V.]Zupanc, A[Zupanc, A.]
Issue Date
18-Apr-2012
Publisher
AMER PHYSICAL SOC
Citation
PHYSICAL REVIEW D, v.85, no.7
Indexed
SCIE
SCOPUS
Journal Title
PHYSICAL REVIEW D
Volume
85
Number
7
URI
https://scholarworks.bwise.kr/skku/handle/2021.sw.skku/65702
DOI
10.1103/PhysRevD.85.071102
ISSN
1550-7998
Abstract
Using a sample of 158 x 10(6) Y(2S) events collected with the Belle detector, we search for the first time for double-charmonium decays of the P-wave spin-triplet bottomonium states (Y(2S) -> gamma chi(bJ), chi(bJ) -> J/psi J/psi, J/psi psi', psi'psi' for J 0, 1, and 2). No significant chi(bJ) signal is observed in the double-charmonium mass spectra, and we obtain the following upper limits: B(chi(bJ) -> J/psi J/psi) < 7.1 x 10(-5), 2.7 x 10(-5), 4.5 x 10(-5), B(chi(bJ) -> J/psi psi') < 1.2 x 10(-4), 1. 7 x 10(-5), 4.9 x 10(-5), B(chi(bJ) -> psi'psi') < 3.1 x 10(-5), 6.2 x 10(-5), 1.6 x 10(-5) for J = 0, 1, and 2, respectively, at the 90% confidence level. These limits are significantly lower than the central values (with uncertainties of 50% to 70%) predicted using the light cone formalism but are consistent with calculations using the nonrelativistic QCD (NRQCD) factorization approach.
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