Bai, JZ; Bian, JG; Blum, I; Chai, ZW; Chen, GP; Chen, HF; Chen, J; Chen, JC; Chen, Y; Chen, YB; Chen, YQ; Cheng, BS; Cui, XZ; Ding, HL; Ding, LY; Dong, LY; Du, ZZ; Dunwoodie, W; Feng, S; Gao, CS; Gao, ML; Gao, SQ; Gratton, P; Gu, JH; Gu, SD; Gu, WX; Gu, YF; Guo, YN; Han, SW; Han, Y; Harris, FA; He, J; He, JT; He, M; Hitlin, DG; Hu, GY; Hu, HM; Hu, JL; Hu, QH; Hu, T; Hu, XQ; Huang, JD; Huang, YZ; Izen, JM; Jiang, CH; Jin, Y; Ke, ZJ; Kelsey, MH; Kim, BK; Kong, D; Lai, YF; Lang, PF; Lankford, A; Li, CG; Li, D; Li, HB; Li, J; Li, PQ; Li, RB; Li, W; Li, WD; Li, WG; Li, XH; Li, XN; Liu, HM; Liu, J; Liu, JH; Liu, RG; Liu, Y; Lou, XC; Lowery, B; Lu, F; Lu, JG; Lu, JY; Lu, LC; Luo, CH; M., A; C., E; M., J; Malchow, R; Mao, HS; Mao, ZP; Meng, XC; Nie, J; Olsen, SL

doi:10.1103/physrevlett.81.5080

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ψ(2S) Hadronic Decays to Vector-Tensor Final States

1998

Bai, JZ;
Bian, JG;
Blum, I;
Chai, ZW;
Chen, GP;
Chen, HF;
Chen, J;
Chen, JC;
Chen, Y;
Chen, YB;
Chen, YQ;
Cheng, BS;
Cui, XZ;
Ding, HL;
Ding, LY;
Dong, LY;
Du, ZZ;
Dunwoodie, W;
Feng, S;
Gao, CS;
Gao, ML;
Gao, SQ;
Gratton, P;
Gu, JH;
Gu, SD;
Gu, WX;
Gu, YF;
Guo, YN;
Han, SW;
Han, Y;
Harris, FA;
He, J;
He, JT;
He, M;
Hitlin, DG;
Hu, GY;
Hu, HM;
Hu, JL;
Hu, QH;
Hu, T;
Hu, XQ;
Huang, JD;
Huang, YZ;
Izen, JM;
Jiang, CH;
Jin, Y;
Ke, ZJ;
Kelsey, MH;
Kim, BK;
Kong, D;
Lai, YF;
Lang, PF;
Lankford, A;
Li, CG;
Li, D;
Li, HB;
Li, J;
Li, PQ;
Li, RB;
Li, W;
Li, WD;
Li, WG;
Li, XH;
Li, XN;
Liu, HM;
Liu, J;
Liu, JH;
Liu, RG;
Liu, Y;
Lou, XC;
Lowery, B;
Lu, F;
Lu, JG;
Lu, JY;
Lu, LC;
Luo, CH;
M., A;
C., E;
M., J;
Malchow, R;
Mao, HS;
Mao, ZP;
Meng, XC;
Nie, J;
Olsen, SL;
Oyang, J;
Paluselli, D;
Pan, LJ;
Panetta, J;
Porter, F;
Qi, ND;
Qi, XR;
Qian, CD;
Qiu, JF;
Qu, YH;
Que, YK;
Rong, G;
Schernau, M;
Shao, YY;
Shen, BW;
Shen, DL;
Shen, H;
Shen, XY;
Sheng, HY;
Shi, HZ;
Song, XF;
Standifird, J;
Sun, F;
Sun, HS;
Tang, SQ;
Toki, W;
Tong, GL;
Wang, F;
Wang, LS;
Wang, LZ;
Wang, M;
Wang, Meng;
Wang, P;
Wang, PL;
Wang, SM;
Wang, TJ;
Wang, YY;
Weaver, M;
Wei, CL;
Wu, YG;
Xi, DM;
Xia, XM;
Xie, PP;
Xie, Y;
Xie, YH;
Xiong, WJ;
Xu, CC;
Xu, GF;
Xue, ST;
Yan, J;
Yan, WG;
Yang, CM;
Yang, CY;
Yang, J;
Yang, W;
Yang, XF;
Ye, MH;
Ye, SW;
Ye, YX;
Yi, K;
Yu, CS;
Yu, CX;
Yu, YH;
Yu, ZQ;
Yu, ZT;
Yuan, CZ;
Yuan, Y;
Zhang, BY;
Zhang, CC;
Zhang, DH;
Zhang, Dehong;
Zhang, HL;
Zhang, J;
Zhang, JL;
Zhang, JW;
Zhang, LS;
Zhang, QJ;
Zhang, SQ;
Zhang, XY;
Zhang, Y;
Zhang, YY;
Zhao, DX;
Zhao, HW;
Zhao, JW;
Zhao, M;
Zhao, WR;
Zhao, ZG;
Zheng, JP;
Zheng, LS;
Zheng, ZP;
Zhou, GP;
Zhou, HS;
Zhou, L;
Zhu, QM;
Zhu, YC;
Zhu, YS;
Zhuang, BA
et al.

Published Web Location

https://doi.org/10.1103/physrevlett.81.5080

Creative Commons 'BY' version 4.0 license

Abstract

The decays of the ψ(2S) into vector plus tensor meson final states have been studied for the first time using the BES detector. We determine upper limits on branching fractions for ψ(2S) decays into ωf2, ρa2, K*0K*02 + c.c., and φf'2(1525) that are, in each case, significantly smaller than the corresponding branching fractions for the J/ψ meson, scaled according to the expectations of perturbative QCD. © 1998 The American Physical Society.

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ψ(2S) Hadronic Decays to Vector-Tensor Final States

Published Web Location