- Bai, JZ;
- Ban, Y;
- Bian, JG;
- Blum, I;
- Chen, GP;
- Chen, HF;
- Chen, J;
- Chen, JC;
- Chen, Y;
- Chen, YB;
- Chen, YQ;
- Cheng, BS;
- Cui, XZ;
- Ding, HL;
- Dong, LY;
- Du, ZZ;
- Dunwoodie, W;
- Gao, CS;
- Gao, ML;
- Gao, SQ;
- Gratton, P;
- Gu, JH;
- Gu, SD;
- Gu, WX;
- Gu, YF;
- Guo, ZJ;
- Guo, YN;
- Han, SW;
- Han, Y;
- Harris, FA;
- He, J;
- He, JT;
- He, KL;
- He, M;
- Heng, YK;
- Hitlin, DG;
- Hu, GY;
- Hu, HM;
- Hu, JL;
- Hu, QH;
- Hu, T;
- Hu, XQ;
- Huang, GS;
- Huang, YZ;
- Izen, JM;
- Jiang, CH;
- Jin, Y;
- Jones, BD;
- Ju, X;
- Ke, ZJ;
- Kelsey, MH;
- Kim, BK;
- Kong, D;
- Lai, YF;
- Lang, PF;
- Lankford, A;
- Li, CG;
- Li, D;
- Li, HB;
- Li, J;
- Li, JC;
- Li, PQ;
- Li, RB;
- Li, W;
- Li, WG;
- Li, XH;
- Li, XN;
- Liu, HM;
- Liu, J;
- Liu, RG;
- Liu, Y;
- Lou, XC;
- Lowery, B;
- Lu, F;
- Lu, JG;
- Luo, XL;
- Ma, EC;
- Ma, JM;
- 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
Using a sample of 3.8 M ψ(2S) events accumulated with the BES detector, the process ψ(2S) →π+π-J/ψ is studied. The angular distributions are compared with the general decay amplitude analysis of Cahn. We find that the dipion system requires some D wave amplitude, as well as S wave. On the other hand, the J/ψ-(π+π-) relative angular momentum is consistent with being pure S wave. The decay distributions have been fit to heavy quarkonium models, including the Novikov-Shifman model. This model, which is written in terms of the parameter κ, predicts that D wave pions should be present. We determine κ=0.183 ±0.002±0.003 based on the joint mππ-cos θπ* distribution. The fraction of D wave amplitude as a function of mππ is found to decrease with increasing mππ, in agreement with the model. We have also fit the Mannel-Yan model, which is another model that allows D wave pions. ©2000 The American Physical Society.