Analysis of $D$+ → $K¯$0$e$+$ν$$e$ and $D$+ → $π$0$e$+$ν$$e$ semileptonic decays

Using 2.93 fb–1 of data taken at 3.773 GeV with the BESIII detector operated at the BEPCII collider, we study the semileptonic decays D+ → K¯0e+νe and D+ → π0e+νe. Here, we measure the absolute decay branching fractions B(D+ → K¯0e+νe) = (8.60 ± 0.06 ± 0.15) × 10–2 and B(D+ → π0e+νe) = (3.63 ± 0.08...

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Veröffentlicht in:Physical review. D 2017-07, Vol.96 (1)
Hauptverfasser: An, Q., Bakina, O., Baldini Ferroli, R., Bennett, J.  V., Bettoni, D., Briere, R.  A., Cai, X., Chelkov, G., Chen, G., Chen, J.  C., Chu, X.  K., Dbeyssi, A., Du, S.  X., Fan, J.  Z., Fang, S.  S., Fava, L., Fioravanti, E., Gu, M.  H., Guo, A.  Q., Guo, Y., Hu, T., Huang, J.  S., Ji, Q.  P., Jiang, L.  W., Jiang, X.  Y., Johansson, T., Julin, A., Kloss, B., Kopf, B., Lara, M., Li, F., Li, G., Li, J.  C., Li, Jin, Li, K., Li, Y.  B., Liu, B., Liu, F.  H., Liu, J.  P., Liu, X., Liu, Y.  B., Liu, Zhiqing, Lu, Y., Luo, X.  L., Lyu, X.  R., Ma, M.  M., Ma, Q.  M., Ma, T., Min, J., Mo, Y.  J., Morello, G., Nefedov, Y., Niu, X.  Y., Ouyang, Q., Pacetti, S., Pan, Y., Patteri, P., Ping, R.  G., Prasad, V., Qi, H.  R., Qi, M., Qin, L.  Q., Ripka, M., Schnier, C., Shan, W., Shao, M., Shen, C.  P., Shen, P.  X., Song, X.  Y., Sun, S.  S., Sun, Z.  J., Sun, Z.  T., Thorndike, E.  H., Wang, B.  L., Wang, P., Wang, W., Wang, Z.  H., Xia, L., Xia, Y., Xie, Y.  G., Xu, L., Ye, M.  H., Yin, J.  H., You, Z.  Y., Yu, C.  X., Yuncu, A., Zafar, A.  A., Zhang, J.  L., Zhang, Y.  H., Zhang, Y.  N., Zhang, Z.  H., Zhao, J.  Y., Zhao, Z.  G., Zheng, J.  P., Zheng, W.  J., Zhong, B., Zhou, L., Zhou, X.  R., Zhou, X.  Y., Zou, J.  H.
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Zusammenfassung:Using 2.93 fb–1 of data taken at 3.773 GeV with the BESIII detector operated at the BEPCII collider, we study the semileptonic decays D+ → K¯0e+νe and D+ → π0e+νe. Here, we measure the absolute decay branching fractions B(D+ → K¯0e+νe) = (8.60 ± 0.06 ± 0.15) × 10–2 and B(D+ → π0e+νe) = (3.63 ± 0.08 ± 0.05) × 10–3, where the first uncertainties are statistical and the second systematic. We also measure the differential decay rates and study the form factors of these two decays. With the values of |Vcs| and |Vcd| from Particle Data Group fits assuming CKM unitarity, we obtain the values of the form factors at q2 = 0, $f$ $^{K}_{+}$(0) = 0.725 ± 0.004 ± 0.012 and $f$ $^{π}_{+}$(0) = 0.622 ± 0.012 ± 0.003. Taking input from recent lattice QCD calculations of these form factors, we determine values of the CKM matrix elements |Vcs| = 0.944 ± 0.005 ± 0.015 ± 0.024 and |Vcd| = 0.210 ± 0.004 ± 0.001 ± 0.009, where the third uncertainties are theoretical.
ISSN:2470-0010
2470-0029