- Main
Study of dynamics of D0→K-e+νe and D0→π-e+νe decays
- Ablikim, M;
- Achasov, MN;
- Ai, XC;
- Albayrak, O;
- Albrecht, M;
- Ambrose, DJ;
- Amoroso, A;
- An, FF;
- An, Q;
- Bai, JZ;
- Ferroli, R Baldini;
- Ban, Y;
- Bennett, DW;
- Bennett, JV;
- Bertani, M;
- Bettoni, D;
- Bian, JM;
- Bianchi, F;
- Boger, E;
- Boyko, I;
- Briere, RA;
- Cai, H;
- Cai, X;
- Cakir, O;
- Calcaterra, A;
- Cao, GF;
- Cetin, SA;
- Chang, JF;
- Chelkov, G;
- Chen, G;
- Chen, HS;
- Chen, HY;
- Chen, JC;
- Chen, ML;
- Chen, SJ;
- Chen, X;
- Chen, XR;
- Chen, YB;
- Cheng, HP;
- Chu, XK;
- Cibinetto, G;
- Dai, HL;
- Dai, JP;
- Dbeyssi, A;
- Dedovich, D;
- Deng, ZY;
- Denig, A;
- Denysenko, I;
- Destefanis, M;
- De Mori, F;
- Ding, Y;
- Dong, C;
- Dong, J;
- Dong, LY;
- Dong, MY;
- Du, SX;
- Duan, PF;
- Eren, EE;
- Fan, JZ;
- Fang, J;
- Fang, SS;
- Fang, X;
- Fang, Y;
- Fava, L;
- Feldbauer, F;
- Felici, G;
- Feng, CQ;
- Fioravanti, E;
- Fritsch, M;
- Fu, CD;
- Gao, Q;
- Gao, XY;
- Gao, Y;
- Gao, Z;
- Garzia, I;
- Goetzen, K;
- Gong, WX;
- Gradl, W;
- Greco, M;
- Gu, MH;
- Gu, YT;
- Guan, YH;
- Guo, AQ;
- Guo, LB;
- Guo, Y;
- Guo, YP;
- Haddadi, Z;
- Hafner, A;
- Han, S;
- Hao, XQ;
- Harris, FA;
- He, KL;
- He, XQ;
- Held, T;
- Heng, YK;
- Hou, ZL;
- Hu, C;
- Hu, HM;
- Hu, JF;
- Hu, T;
- Hu, Y;
- Huang, GM;
- Huang, GS;
- Huang, JS;
- Huang, XT;
- Huang, Y;
- Hussain, T;
- Ji, Q;
- Ji, QP;
- Ji, XB;
- Ji, XL;
- Jiang, LL;
- Jiang, LW;
- Jiang, XS;
- Jiang, XY;
- Jiao, JB;
- Jiao, Z;
- Jin, DP;
- Jin, S;
- Johansson, T;
- Julin, A;
- Kalantar-Nayestanaki, N;
- Kang, XL;
- Kang, XS;
- Kavatsyuk, M;
- Ke, BC;
- Kiese, P;
- Kliemt, R;
- Kloss, B;
- Kolcu, OB;
- Kopf, B;
- Kornicer, M;
- Kuehn, W;
- Kupsc, A;
- Lange, JS;
- Lara, M;
- Larin, P;
- Leng, C;
- Li, C;
- Li, Cheng;
- Li, DM;
- Li, F;
- Li, FY;
- Li, G;
- Li, HB;
- Li, JC;
- Li, Jin;
- Li, K;
- Li, K;
- Li, Lei;
- Li, PR;
- Li, T;
- Li, WD;
- Li, WG;
- Li, XL;
- Li, XM;
- Li, XN;
- Li, XQ;
- Li, ZB;
- Liang, H;
- Liang, YF;
- Liang, YT;
- Liao, GR;
- Lin, DX;
- Liu, BJ;
- Liu, CL;
- Liu, CX;
- Liu, FH;
- Liu, Fang;
- Liu, Feng;
- Liu, HB;
- Liu, HH;
- Liu, HH;
- Liu, HM;
- Liu, J;
- Liu, JB;
- Liu, JP;
- Liu, JY;
- Liu, K;
- Liu, KY;
- Liu, LD;
- Liu, PL;
- Liu, Q;
- Liu, SB;
- Liu, X;
- Liu, YB;
- Liu, ZA;
- Liu, Zhiqing;
- Loehner, H;
- Lou, XC;
- Lu, HJ;
- Lu, JG;
- Lu, Y;
- Lu, YP;
- Luo, CL;
- Luo, MX;
- Luo, T;
- Luo, XL;
- Lyu, XR;
- C., F;
- L., H;
- L., L;
- M., Q;
- Ma, T;
- N., X;
- Y., X;
- Maas, FE;
- Maggiora, M;
- Mao, YJ;
- Mao, ZP;
- Marcello, S;
- Messchendorp, JG;
- Min, J;
- Mitchell, RE;
- Mo, XH;
- Mo, YJ;
- Morales, C Morales;
- Moriya, K;
- Muchnoi, N Yu;
- Muramatsu, H;
- Nefedov, Y;
- Nerling, F;
- Nikolaev, IB;
- Ning, Z;
- Nisar, S;
- Niu, SL;
- Niu, XY;
- Olsen, SL;
- Ouyang, Q;
- Pacetti, S;
- Patteri, P;
- Pelizaeus, M;
- Peng, HP;
- Peters, K;
- Pettersson, J;
- Ping, JL;
- Ping, RG;
- Poling, R;
- Prasad, V;
- Qi, M;
- Qian, S;
- Qiao, CF;
- Qin, LQ;
- Qin, N;
- Qin, XS;
- Qin, ZH;
- Qiu, JF;
- Rashid, KH;
- Redmer, CF;
- Ripka, M;
- Rong, G;
- Rosner, Ch;
- Ruan, XD;
- Santoro, V;
- Sarantsev, A;
- Savrié, M;
- Schoenning, K;
- Schumann, S;
- Shan, W;
- Shao, M;
- Shen, CP;
- Shen, PX;
- Shen, XY;
- Sheng, HY;
- Song, WM;
- Song, XY;
- Sosio, S;
- Spataro, S;
- Sun, GX;
- Sun, JF;
- Sun, SS;
- Sun, YJ;
- Sun, YZ;
- Sun, ZJ;
- Sun, ZT;
- Tang, CJ;
- Tang, X;
- Tapan, I;
- Thorndike, EH;
- Tiemens, M;
- Ullrich, M;
- Uman, I;
- Varner, GS;
- Wang, B;
- Wang, D;
- Wang, DY;
- Wang, K;
- Wang, LL;
- Wang, LS;
- Wang, M;
- Wang, P;
- Wang, PL;
- Wang, SG;
- Wang, W;
- Wang, XF;
- Wang, YD;
- Wang, YF;
- Wang, YQ;
- Wang, Z;
- Wang, ZG;
- Wang, ZH;
- Wang, ZY;
- Weber, T;
- Wei, DH;
- Wei, JB;
- Weidenkaff, P;
- Wen, SP;
- Wiedner, U;
- Wolke, M;
- Wu, LH;
- Wu, Z;
- Xia, LG;
- Xia, Y;
- Xiao, D;
- Xiao, H;
- Xiao, ZJ;
- Xie, YG;
- Xiu, QL;
- Xu, GF;
- Xu, L;
- Xu, QJ;
- Xu, XP;
- Yan, L;
- Yan, WB;
- Yan, WC;
- Yan, YH;
- Yang, HJ;
- Yang, HX;
- Yang, L;
- Yang, Y;
- Yang, YX;
- Ye, M;
- Ye, MH;
- Yin, JH;
- Yu, BX;
- Yu, CX;
- Yu, JS;
- Yuan, CZ;
- Yuan, WL;
- Yuan, Y;
- Yuncu, A;
- Zafar, AA;
- Zallo, A;
- Zeng, Y;
- Zhang, BX;
- Zhang, BY;
- Zhang, C;
- Zhang, CC;
- Zhang, DH;
- Zhang, HH;
- Zhang, HY;
- Zhang, JJ;
- Zhang, JL;
- Zhang, JQ;
- Zhang, JW;
- Zhang, JY;
- Zhang, JZ;
- Zhang, K;
- Zhang, L;
- Zhang, XY;
- Zhang, Y;
- Zhang, YN;
- Zhang, YH;
- Zhang, YT;
- Zhang, Yu;
- Zhang, ZH;
- Zhang, ZP;
- Zhang, ZY;
- Zhao, G;
- Zhao, JW;
- Zhao, JY;
- Zhao, JZ;
- Zhao, Lei;
- Zhao, Ling;
- Zhao, MG;
- Zhao, Q;
- Zhao, QW;
- Zhao, SJ;
- Zhao, TC;
- Zhao, YB;
- Zhao, ZG;
- Zhemchugov, A;
- Zheng, B;
- Zheng, JP;
- Zheng, WJ;
- Zheng, YH;
- Zhong, B;
- Zhou, L;
- Zhou, X;
- Zhou, XK;
- Zhou, XR;
- Zhou, XY;
- Zhu, K;
- Zhu, KJ;
- Zhu, S;
- Zhu, SH;
- Zhu, XL;
- Zhu, YC;
- Zhu, YS;
- Zhu, ZA;
- Zhuang, J;
- Zotti, L;
- Zou, BS;
- Zou, JH
- et al.
Abstract
In an analysis of a 2.92 fb-1 data sample taken at 3.773 GeV with the BESIII detector operated at the BEPCII collider, we measure the absolute decay branching fractions B(D0→K-e+νe)=(3.505±0.014±0.033)% and B(D0→π-e+νe)=(0.295±0.004±0.003)%. From a study of the differential decay rates we obtain the products of hadronic form factor and the magnitude of the Cabibbo-Kobayashi- Maskawa (CKM) matrix element f+K(0)|Vcs|=0.7172±0.0025±0.0035 and f+π(0)|Vcd|=0.1435±0.0018±0.0009. Combining these products with the values of |Vcs(d)| from the SM constraint fit, we extract the hadronic form factors f+K(0)=0.7368±0.0026±0.0036 and f+π(0)=0.6372±0.0080±0.0044, and their ratio f+π(0)/f+K(0)=0.8649±0.0112±0.0073. These form factors and their ratio are used to test unquenched lattice QCD calculations of the form factors and a light cone sum rule (LCSR) calculation of their ratio. The measured value of f+K(π)(0)|Vcs(d)| and the lattice QCD value for f+K(π)(0) are used to extract values of the CKM matrix elements of |Vcs|=0.9601±0.0033±0.0047±0.0239 and |Vcd|=0.2155±0.0027±0.0014±0.0094, where the third errors are due to the uncertainties in lattice QCD calculations of the form factors. Using the LCSR value for f+π(0)/f+K(0), we determine the ratio |Vcd|/|Vcs|=0.238±0.004±0.002±0.011, where the third error is from the uncertainty in the LCSR normalization. In addition, we measure form factor parameters for three different theoretical models that describe the weak hadronic charged currents for these two semileptonic decays. All of these measurements are the most precise to date.
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