×
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

General scan in flavor parameter space in models with vector quark doublets and an enhancement in the B→Xsγ process

  • In models with vector-like quark doublets, the mass matrices of up and down type quarks are related. Precise diagonalization of the mass matrices has become an obstacle in numerical studies. In this work we first propose a diagonalization method. As its application, in the Standard Model with one vector-like quark doublet we present the quark mass spectrum and Feynman rules for the calculation of B→Xsγ. We find that i) under the constraints of the CKM matrix measurements, the mass parameters in the bilinear term are constrained to a small value by the small deviation from unitarity; ii) compared with the fourth generation extension of the Standard Model, there is an enhancement to the B→Xsγ process in the contribution of vector-like quarks, resulting in a non-decoupling effect in such models.
      PCAS:
  • 加载中
  • [1] G. Cvetic, Rev. Mod. Phys., 71:513(1999)[hep-ph/9702381]; H. J. He, T. M. P. Tait, and C. P. Yuan, Phys. Rev. D, 62:011702(2000)[hep-ph/9911266]; H. J. He, C. T. Hill, and T. M. P. Tait, Phys. Rev. D, 65:055006(2002)[hep-ph/0108041]. J. Cao, L. Shang, W. Su, F. Wang, and Y. Zhang, arXiv:1512.08392[hep-ph]. F. Wang, W. Wang, L. Wu, J. M. Yang, and M. Zhang, arXiv:1512.08434[hep-ph]
    [2] J. Jiang, T. Li, D. V. Nanopoulos, and D. Xie, Phys. Lett. B, 677:322(2009); Nucl. Phys. B, 830:195(2010)
    [3] J. Jiang, T. Li, and D. V. Nanopoulos, Nucl. Phys. B, 772:49(2007)
    [4] I. Antoniadis, J. R. Ellis, J. S. Hagelin, and D. V. Nanopoulos, Phys. Lett. B, 208:209(1988)[Addendum-ibid. B, 213:562(1988)]; Phys. Lett. B, 231:65(1989)
    [5] J. L. Lopez, D. V. Nanopoulos, and K. J. Yuan, Nucl. Phys. B, 399:654(1993)
    [6] C. Beasley, J. J. Heckman, and C. Vafa, JHEP, 0901:058(2009); JHEP, 0901:059(2009); R. Donagi and M. Wijnholt, Adv. Theor. Math. Phys., 15 (5):1237(2011)[arXiv:0802.2969[hep-th]]; Adv. Theor. Math. Phys., 15(6):1523(2011)[arXiv:0808.2223[hep-th]]
    [7] T. Li, D. V. Nanopoulos, W. Y. Wang, X. C. Wang, and Z. H. Xiong, JHEP, 1207:190(2012)[arXiv:1204.5326[hep-ph]]
    [8] T. Li, W. Wang, X. C. Wang, and Z. H. Xiong, arXiv:1506.04987[hep-ph]
    [9] A. J. Buras, M. Misiak, M. Mnz, and S. Pokorski, Nucl. Phys. B, 424:374(1994)
    [10] J. Beringer et al (Particle Data Group Collaboration), Phys. Rev. D, 86:010001(2012)
    [11] O. Eberhardt, A. Lenz, and J. Rohrwild, Phys. Rev. D, 82:095006(2010)[arXiv:1005.3505[hep-ph]]
    [12] L. Wolfenstein, Phys. Rev. Lett., 51:1945(1983); A. J. Buras, M. E. Lautenbacher, and G. Ostermaier, Phys. Rev. D, 50:3433(1994)[hep-ph/9403384]; J. Charles et al (CKMfitter Group Collaboration), Eur. Phys. J. C, 41:1(2005)[hep-ph/0406184]
    [13] P. Langacker and D. London, Phys. Rev. D, 38:886(1988)
    [14] F. del Aguila and M. Bowick, Nucl. Phys. B, 224:107(1983)
    [15] F. del Aguila, E. Laermann, and P. Zerwas, Nucl. Phys. B, 297:1(1988)
    [16] T. Cheng and L.-F. Li, Phys. Rev. D, 45:1708-1710(1992)
    [17] F. J. Botella, G. C. Branco, and M. Nebot, JHEP, 1212:040(2012)[arXiv:1207.4440[hep-ph]]; A. K. Alok, S. Banerjee, D. Kumar, S. U. Sankar, and D. London, Phys. Rev. D, 92(1):013002(2015)[arXiv:1504.00517[hep-ph]]; A. K. Alok, S. Banerjee, D. Kumar and S. Uma Sankar, Nucl. Phys. B, 906:321(2016)[arXiv:1402.1023[hep-ph]]
    [18] B. Grinstein, R. P. Springer, and M. B. Wise, Nucl. Phys. B, 339:269(1990)
    [19] W. Altmannshofer, A. J. Buras, S. Gori, P. Paradisi, and D. M. Straub, Nucl. Phys. B, 830:17(2010)[arXiv:0909.1333[hep-ph]]
  • 加载中

Get Citation
Wenyu Wang, Zhao-Hua Xiong and Xin-Yan Zhao. General scan in flavor parameter space in models with vector quark doublets and an enhancement in the B→Xsγ process[J]. Chinese Physics C, 2016, 40(9): 093102. doi: 10.1088/1674-1137/40/9/093102
Wenyu Wang, Zhao-Hua Xiong and Xin-Yan Zhao. General scan in flavor parameter space in models with vector quark doublets and an enhancement in the B→Xsγ process[J]. Chinese Physics C, 2016, 40(9): 093102.  doi: 10.1088/1674-1137/40/9/093102 shu
Milestone
Received: 2016-03-30
Revised: 2016-05-13
Fund

    Supported by Natural Science Foundation of China (11375001) and Talents Foundation of Education Department of Beijing

Article Metric

Article Views(1943)
PDF Downloads(161)
Cited by(0)
Policy on re-use
To reuse of Open Access content published by CPC, for content published under the terms of the Creative Commons Attribution 3.0 license (“CC CY”), the users don’t need to request permission to copy, distribute and display the final published version of the article and to create derivative works, subject to appropriate attribution.
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:

General scan in flavor parameter space in models with vector quark doublets and an enhancement in the B→Xsγ process

    Corresponding author: Wenyu Wang,
    Corresponding author: Zhao-Hua Xiong,
    Corresponding author: Xin-Yan Zhao,
Fund Project:  Supported by Natural Science Foundation of China (11375001) and Talents Foundation of Education Department of Beijing

Abstract: In models with vector-like quark doublets, the mass matrices of up and down type quarks are related. Precise diagonalization of the mass matrices has become an obstacle in numerical studies. In this work we first propose a diagonalization method. As its application, in the Standard Model with one vector-like quark doublet we present the quark mass spectrum and Feynman rules for the calculation of B→Xsγ. We find that i) under the constraints of the CKM matrix measurements, the mass parameters in the bilinear term are constrained to a small value by the small deviation from unitarity; ii) compared with the fourth generation extension of the Standard Model, there is an enhancement to the B→Xsγ process in the contribution of vector-like quarks, resulting in a non-decoupling effect in such models.

    HTML

Reference (19)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return