×
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

Study of singlet-triplet mixing via semileptonic decays

  • The singlet-triplet mixing of 1P1-3P1 is studied via calculating the branching ratios of semileptonic decay Bs→Ds1lν and B→D1lν by means of the instantaneous Bethe-Salpeter method. Special attention is paid to the relativistic corrections, since they are large for the P-wave states. Using the Mandelstam Formalism, we compute the transition form factors not only in the high-energy lepton end-point region but also in the full Q2 region. And the non-perturbative QCD effects are taken care of in the overlapping integral over the relativistic wave functions of the initial and nial states.
      PCAS:
  • 加载中
  • [1] Rosner J. Comm. Nucl. Part. Phys., 1986, 16: 109[2] Isgur N, Wise M B. Phys. Rev. D, 1991, 43: 819[3] Godfrey S, Kokoski R. Phys. Rev. D, 1981, 43: 1679[4] Isgur N, Wise M B. Phys. Lett. B, 1989, 232: 113; 1990, 237: 527[5] Voloshin M B, Shifman M A. Sov. J. Nucl. Phys. 1987, 45: 292; 1988, 47: 511[6] Aliev T M, Azizi K, Ozpineci A. Eur. Phys. J. C, 2007, 51: 593[7] ZHAO Shu-Min, LIU Xiang, LI Shuang-Jiu. Eur. Phys. J. C, 2007, 51: 601[8] Segovia J et al. Phys. Rev. D, 84: 094029[9] HUANG Ming-Qiu. Phys. Rev. D, 2004, 69: 114015[10] Scora D, Isgur N. Phys. Rev. D, 1995, 52: 2783[11] Salpeter E E, Bethe H A. Phys. Rev., 1951, 84: 1232[12] Salpeter E E. Phys. Rev. 1952, 87: 328[13] Mandelstam S. Proc. R. Soc. London, 1955, 233: 248[14] Isgur N, Scora D, Grinstein B, Wise M B. Phys. Rev. D, 1989, 39: 799[15] CHANG Chao-Hsi, CHEN Jiao-Kai, WANG Guo-Li. Commun. Theor. Phys., 2006, 46: 467[16] Kim C S, WANG Guo-Li. Phys. Lett. B, 2004, 584: 285[17] WANG Guo-Li. Phys. Lett. B, 2007, 650: 15[18] Ebert D, Faustov R N, Galkin V O. Eur. Phys. J. C, 2010, 66: 197[19] Particle Data Group. J. Phys. G, 2010, 37: 1[20] Ebert D, Faustov R N, Galkin V O. Phys. Rev. D, 2000, 61: 014016[21] Mayorga H B, Briceno A Moreno, Munoz J H. J. Phys. G, 2003, 29: 2059[22] Abazov V M et al. (D0 collaboration). Phys. Rev. Lett., 2009, 102: 051801[23] Abe K et al. (Belle collaboration). Phys. Rev. D, 2004, 69: 112002[24] Liventsev D et al. (Belle collaboration). Phys. Rev. D, 2008, 77: 091503[25] Aubert B et al. (BABAR collaboration). Phys. Rev. Lett., 2008, 101: 261802[26] Aubert B et al. (BABAR collaboration). Phys. Rev. Lett., 2009, 103: 051803
  • 加载中

Get Citation
JIANG Yue, WANG Guo-Li, WANG Tian-Hong and JU Wan-Li. Study of singlet-triplet mixing via semileptonic decays[J]. Chinese Physics C, 2013, 37(1): 013101. doi: 10.1088/1674-1137/37/1/013101
JIANG Yue, WANG Guo-Li, WANG Tian-Hong and JU Wan-Li. Study of singlet-triplet mixing via semileptonic decays[J]. Chinese Physics C, 2013, 37(1): 013101.  doi: 10.1088/1674-1137/37/1/013101 shu
Milestone
Received: 2012-03-02
Revised: 2012-04-05
Article Metric

Article Views(2064)
PDF Downloads(289)
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, bchen63@163.com
  • 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:

Study of singlet-triplet mixing via semileptonic decays

Abstract: The singlet-triplet mixing of 1P1-3P1 is studied via calculating the branching ratios of semileptonic decay Bs→Ds1lν and B→D1lν by means of the instantaneous Bethe-Salpeter method. Special attention is paid to the relativistic corrections, since they are large for the P-wave states. Using the Mandelstam Formalism, we compute the transition form factors not only in the high-energy lepton end-point region but also in the full Q2 region. And the non-perturbative QCD effects are taken care of in the overlapping integral over the relativistic wave functions of the initial and nial states.

    HTML

Reference (1)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return