×
近期发现有不法分子冒充我刊与作者联系,借此进行欺诈等不法行为,请广大作者加以鉴别,如遇诈骗行为,请第一时间与我刊编辑部联系确认(《中国物理C》(英文)编辑部电话:010-88235947,010-88236950),并作报警处理。
本刊再次郑重声明:
(1)本刊官方网址为cpc.ihep.ac.cn和https://iopscience.iop.org/journal/1674-1137
(2)本刊采编系统作者中心是投稿的唯一路径,该系统为ScholarOne远程稿件采编系统,仅在本刊投稿网网址(https://mc03.manuscriptcentral.com/cpc)设有登录入口。本刊不接受其他方式的投稿,如打印稿投稿、E-mail信箱投稿等,若以此种方式接收投稿均为假冒。
(3)所有投稿均需经过严格的同行评议、编辑加工后方可发表,本刊不存在所谓的“编辑部内部征稿”。如果有人以“编辑部内部人员”名义帮助作者发稿,并收取发表费用,均为假冒。
                  
《中国物理C》(英文)编辑部
2024年10月30日

Semileptonic decays Bc→(ηc,J/Ψ)lv in the perturbative QCD approach

  • In this paper we study the semileptonic decays of Bc-→(ηc,J/Ψ)l-vl. We first evaluate the Bc→(ηc,J/Ψ) transition form factors F0(q2), F+(q2), V(q2) and A0,1,2(q2) by employing the pQCD factorization approach, and then we calculate the branching ratios for all considered semileptonic decays. Based on the numerical results and the phenomenological analysis, we find that: (a) the pQCD predictions for the values of the Bc→ηc and Bc→J/Ψ transition form factors agree well with those obtained by using other methods; (b) the pQCD predictions for the branching ratios of the considered decays are Br(Bc-→ηc e-ve-vμ)=(4.41-1.09+1.22)×10-3, Br(Bc-→ηcτ-vτ) =(1.37-0.34+0.37)×10-3, Br(Bc-→J/Ψ e-ve-vμ)) =(10.03-1.18+1.33)×10-3, and Br(Bc-→J/Ψτ-vτ) =(2.92-0.34+0.40)×10-3; and (c) we also define and calculate two ratios of the branching ratios Rηc and RJ/Ψ, which will be tested by LHCb and the forthcoming Super-B experiments.
      PCAS:
  • 加载中
  • [1] Abe F et al. (CDF collaboration). Phys. Rev. D, 1998, 58: 112004[2] Gouz I P, Kiselev V V, Likhoded A K, Romanovsky V I, Yushchenko O P. Phys. At. Nucl., 2004, 67: 1559[3] Quarkonium Working Group, Brambilla N et al. Report No: CERN-2005-005; Altarelli M P, Teubert F. Int. J. Mod. Phys. A, 2008, 23: 5117[4] Dhir R, Verma R C. Phys. Rev. D, 2009, 79: 034004[5] Hernandez E, Nieves J, Verde-Velasco J M. Phys. Rev. D, 2006, 74: 074008[6] Ivanov M A, Korner J G, Santorelli P. Phys. Rev. D, 2005, 71: 094006; 2007, 75: 019901(E)[7] Ebert D, Faustov R N, Galkin V O. Phys. Rev. D, 2003, 68: 094020; Eur. Phys. J. C, 2003, 32: 29[8] SUN J F, YANG Y L, DU W J, MA H L. Phys. Rev. D, 2008, 77: 114004[9] WANG W, SHEN Y L, L C D. Phys. Rev. D, 2009, 79: 054012[10] QIAO C F, ZHU R L. Phys. Rev. D, 2013, 87: 014009[11] XIAO Z J, LIU X. Phys. Rev. D, 2011, 84: 074033; LIU X, XIAO Z J, L C D. Phys. Rev. D, 2010, 81: 014022[12] CHENG J F, DU D S, L C D. Eur. Phys. J. C, 2006, 45: 711[13] SUN J F, DU D S, YANG Y L. Eur. Phys. J. C, 2009, 60: 107[14] Yeh T W, LI H N. Phys. Rev. D, 1997, 56: 1615; LI H N, YU H L. Phys. Rev. Lett., 1995, 74: 4388; Phys. Lett. B, 1995, 353: 301; Phys. Rev. D, 1996, 53: 2480.[15] L C D, Ukai K, YANG M Z. Phys. Rev. D, 2001, 63: 074009[16] Kurimoto T, LI H N, Sanda A I. Phys. Rev. D, 2003, 67, 054028[17] LI Y, L C D. Phys. Rev. D, 2006, 73: 094006[18] LIU X, ZHANG Z Q, XIAO Z J. Chin. Phys. C, 2010, 34:937; Bondar A E, Chernyak V L. Phys. Lett. B, 2005, 612: 215[19] Kurimoto T, LI H N, Sanda A I. Phys. Rev. D, 2001, 65: 014007[20] WEI Z T, YANG M Z. pb, 2002, 642: 263; L C D, YANG M Z. Eur. Phys. J. C, 2002, 23: 275; Eur. Phys. J. C, 2003, 28: 515; LI R H, L C D, WANG W, WANG X X. Phys. Rev. D, 2009, 79: 014013; HUANG T, WU X G. Phys. Rev. D, 2005, 71: 034018[21] Wirbel M, Stech B, Bauerm. Z. Phys. C, 1985, 29: 637; Colangelo P, de Fazio F, Santorelli P, Scrimieri E. Phys. Lett. B, 1997, 395: 339[22] Beneke M, Feldmann T. pb, 2001, 592: 3[23] Buchalla G, Buras A J, Lautenbacher M E. Rev. Mod. Phys., 1996, 68: 1125[24] Colangelo P, de Fazio F, Ferrandes R, Pham T N. Phys. Rev. D, 2006, 73: 115006[25] LI H N, SHEN Y L, WANG Y M. Phys. Rev. D, 2012, 85: 074004[26] WANG W F, XIAO Z J. Phys. Rev. D, 2012, 86: 114025[27] CHEN C H, GENG C Q. JHEP, 2006, 10: 053; Ball P, Braun V M. Phys. Rev. D, 1997, 55: 5561[28] del Amo Sanchez P et al. (BABAR collaboration). Phys. Rev. D, 2011, 83: 032007[29] Beringer J et al. (Particle Data Group). Phys. Rev. D, 2012, 86: 010001[30] WANG Z G. arXiv:1209.1157v1[hep-ph]
  • 加载中

Get Citation
WANG Wen-Fei, FAN Ying-Ying and XIAO Zhen-Jun. Semileptonic decays Bc→(ηc,J/Ψ)lv in the perturbative QCD approach[J]. Chinese Physics C, 2013, 37(9): 093102. doi: 10.1088/1674-1137/37/9/093102
WANG Wen-Fei, FAN Ying-Ying and XIAO Zhen-Jun. Semileptonic decays Bc→(ηc,J/Ψ)lv in the perturbative QCD approach[J]. Chinese Physics C, 2013, 37(9): 093102.  doi: 10.1088/1674-1137/37/9/093102 shu
Milestone
Received: 2012-12-14
Revised: 2013-01-22
Article Metric

Article Views(2151)
PDF Downloads(509)
Cited by(0)
Policy on re-use
To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.
通讯作者: 陈斌, [email protected]
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Email This Article

Title:
Email:

Semileptonic decays Bc→(ηc,J/Ψ)lv in the perturbative QCD approach

    Corresponding author: XIAO Zhen-Jun,

Abstract: In this paper we study the semileptonic decays of Bc-→(ηc,J/Ψ)l-vl. We first evaluate the Bc→(ηc,J/Ψ) transition form factors F0(q2), F+(q2), V(q2) and A0,1,2(q2) by employing the pQCD factorization approach, and then we calculate the branching ratios for all considered semileptonic decays. Based on the numerical results and the phenomenological analysis, we find that: (a) the pQCD predictions for the values of the Bc→ηc and Bc→J/Ψ transition form factors agree well with those obtained by using other methods; (b) the pQCD predictions for the branching ratios of the considered decays are Br(Bc-→ηc e-ve-vμ)=(4.41-1.09+1.22)×10-3, Br(Bc-→ηcτ-vτ) =(1.37-0.34+0.37)×10-3, Br(Bc-→J/Ψ e-ve-vμ)) =(10.03-1.18+1.33)×10-3, and Br(Bc-→J/Ψτ-vτ) =(2.92-0.34+0.40)×10-3; and (c) we also define and calculate two ratios of the branching ratios Rηc and RJ/Ψ, which will be tested by LHCb and the forthcoming Super-B experiments.

    HTML

Reference (1)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return