Impact factor of Chinese Physics C is 3.6 in 2023 Impact factor of Chinese Physics C is 3.6 in 2022 2021 Impact Factor 2.944
Advanced Search
×
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
Chinese Physics C> 2016, Vol. 40> Issue(12) : 123103 DOI: 10.1088/1674-1137/40/12/123103

Flavor violating Higgs signals in the Texturized Two-Higgs Doublet Model (THDM-Tx)

  • Flavor violating Higgs signals, such as the top FCNC decay t→ch0 and the LFV Higgs decay h0→τμ, have been studied at the LHC. These signals can arise within the general Two-Higgs Doublet Model (THDM), where each Higgs doublet couples to all fermion types through Yukawa matrices Y1f and Y2f. The Yukawa matrices can be assumed to have the same form or they could have different structures. In this paper we study the case when both Y1f and Y2f have completely different forms, but in such a way that they complement to produce a specific hermitian mass matrix. We find that for specific four-zero textures, the flavor violating Higgs couplings depend only on the free parameters tan β, γf and the fermion masses. We use the current bounds on the low energy processes to derive constraints on the heavy Higgs boson mass, tan β and γf. Then, we use these constraints to evaluate the LFV Higgs decays, which reach branching ratios that could be tested at the LHC.
      PCAS:
  • 加载中

  • References

    [1] G. Aad et al.[ATLAS and CMS Collaborations], Phys. Rev. Lett., 114:191803(2015)[arXiv:1503.07589]
    [2] J. F. Gunion, H. E. Haber, G. L. Kane and S. Dawson, Front. Phys., 80:1(2000)
    [3] J. L. Diaz-Cruz and D. A. Lopez-Falcon, Phys. Lett. B, 568:245(2003)[hep-ph/0304212]
    [4] N. G. Deshpande and E. Ma, Phys. Rev. D, 18:2574(1978)
    [5] S. P. Martin, in Perspectives on supersymmetry Ⅱ, edired by C. L. Kane, 1-153[hep-ph/9709356]
    [6] M. Quiros, arxiv:hep-ph/0606153
    [7] A. Pomarol, CERN Yellow Report CERN-2012-001, 115-151[arXiv:1202.1391[hep-ph]]
    [8] A. Aranda, J. L. Diaz-Cruz, J. Hernandez-Sanchez and R. Noriega-Papaqui, Phys. Lett. B, 658:57(2007)[arXiv:0708.3821]
    [9] G. C. Branco, P. M. Ferreira, L. Lavoura, M. N. Rebelo, M. Sher and J. P. Silva, Phys. Rept., 516:1(2012)[arXiv:1106.0034]
    [10] E. Ma, Mod. Phys. Lett. A, 21:1777(2006)[hep-ph/0605180];R. Barbieri, L. J. Hall and V. S. Rychkov, Phys. Rev. D, 74:015007(2006)[hep-ph/0603188]; L. Lopez Honorez, E. Nezri, J. F. Oliver and M. H. G. Tytgat, JCAP, 0702:028(2007)[hep-ph/0612275]; I. F. Ginzburg, K. A. Kanishev, M. Krawczyk and D. Sokolowska, Phys. Rev. D, 82:123533(2010)[arXiv:1009.4593]
    [11] I. F. Ginzburg and M. Krawczyk, Phys. Rev. D, 72:115013(2005)[hep-ph/0408011]
    [12] S. L. Glashow and S. Weinberg, Phys. Rev. D, 15:1958(1977)
    [13] J. F. Gunion and H. E. Haber, Nucl. Phys. B, 307:445(1988)[Erratum-ibid. B 402, 569(1993)]
    [14] H. Fritzsch and Z.-Z. Xing, Phys. Lett. B, 353:114(1995)[hep-ph/9502297]
    [15] G. C. Branco, D. Emmanuel-Costa and R. Gonzalez Felipe, Phys. Lett. B, 477:147(2000)[hep-ph/9911418]
    [16] L. J. Hall and S. Weinberg, Phys. Rev. D, 48:979(1993)[hep-ph/9303241]
    [17] W. Altmannshofer, S. Gori and G. D. Kribs, Phys. Rev. D, 86:115009(2012)[arXiv:1210.2465]
    [18] A. J. Buras, M. V. Carlucci, S. Gori and G. Isidori, JHEP, 1010:009(2010)[arXiv:1005.5310]
    [19] G. D'Ambrosio, G. F. Giudice, G. Isidori and A. Strumia, Nucl. Phys. B, 645:155(2002)[hep-ph/0207036]
    [20] A. Aranda, C. Bonilla and J. L. Diaz-Cruz, Phys. Lett. B, 717:248(2012)[arXiv:1204.5558]
    [21] A. Pich and P. Tuzon, Phys. Rev. D, 80:091702(2009)[arXiv:0908.1554]
    [22] T. P. Cheng and M. Sher, Phys. Rev. D, 35:3484(1987)
    [23] Y.-F. Zhou, J. Phys. G, 30:783(2004)[hep-ph/0307240]
    [24] J. L. Diaz-Cruz, R. Noriega-Papaqui and A. Rosado, Phys. Rev. D, 69:095002(2004),[hep-ph/0401194]
    [25] J. L. Diaz-Cruz, R. Noriega-Papaqui and A. Rosado, Phys. Rev. D, 71:015014(2005)[hep-ph/0410391]
    [26] Y.-L. Wu and Y.-F. Zhou, Eur. Phys. J. C, 36:89(2004)[hep-ph/0403252]
    [27] W.-J. Li, Y.-D. Yang and X.-D. Zhang, Phys. Rev. D, 73:073005(2006)[hep-ph/0511273]
    [28] A. E. Carcamo Hernandez, R. Martinez and J. A. Rodriguez, Eur. Phys. J. C, 50:935(2007)[hep-ph/0606190]
    [29] D. Atwood, S. Bar-Shalom and A. Soni, Phys. Lett. B, 635:112(2006)[hep-ph/0502234]
    [30] K.A. Olive et al. (Particle Data Group), Chin. Phys. C, 38:090001(2014) and 2015 update
    [31] T. P. Cheng and M. Sher, Phys. Rev. D, 35:3484(1987)
    [32] M. Gomez-Bock and R. Noriega-Papaqui, J. Phys. G, 32:761(2006)[hep-ph/0509353]
    [33] Dean Carmi, Adam Falkowski, Eric Kuflik, Tomer Volansky, Jure Zupan, JHEP, 10:196(2012),[arXiv:1207.1718v3]
    [34] G. Bennett et al. (Muon G-2 Collaboration), Phys.Rev. D, 73:072003(2006),[arXiv:hep-ex/0602035]
    [35] D. Chang, W.-F. Chang, C.-H. Chou, and W.-Y. Keung, Phys.Rev. D, 63:091301(R)(2001)
    [36] V. Khachatryan et al.,[CMS and LHCb Collaborations],[arXiv:1411.4413]
    [37] C. Bobeth et al., Phys. Rev. Lett, 112:101801(2014)
    [38] A. Dedes and A. Pilaftsis, Phys. Rev. D, 67:015012(2003)
    [39] B. Aubert et al.[BaBar Collaboration], Phys. Rev. D, 79:092002(2009),[arXiv:0902.2660[hep-ex]]
    [40] A. Matyja et al.[Belle Collaboration], Phys. Rev. Lett., 99:191807(2007),[arXiv:0706.4429[hep-ex]]
    [41] A. Crivellin, C. Greub and A. Kokulu, Phys. Rev. D, 86:054014(2012),[arXiv:1206.2634[hep-ph]]
    [42] J. Adam et al.[MEG Collaboration], Phys. Rev. Lett., 110(20):201801(2013)[arXiv:1303.0754]
    [43] B. Aubert et al.[BaBar Collaboration], Phys. Rev. Lett., 104:021802(2010)[arXiv:0908.2381]
    [44] A. Pilaftsis, Phys. Lett. B, 285:68(1992)
    [45] J. L. Diaz-Cruz and J. J. Toscano, Phys. Rev. D, 62:116005(2000)[hep-ph/9910233]
    [46] T. Han and D. Marfatia, Phys. Rev. Lett., 86:1442(2001)[hep-ph/0008141]; K. A. Assamagan, A. Deandrea and P.-A. Delsart, Phys. Rev. D, 67:035001(2003)[hep-ph/0207302]; D. McKeen, M. Pospelov and A. Ritz, Phys. Rev. D, 86:113004(2012)[arXiv:1208.4597]
    [47] J. L. Diaz-Cruz, JHEP, 0305:036(2003)[hep-ph/0207030]; A. Brignole and A. Rossi, Nucl. Phys. B, 701:3(2004)[hep-ph/0404211]; E. Arganda, A. M. Curiel, M. J. Herrero and D. Temes, Phys. Rev. D, 71:035011(2005)[hep-ph/0407302]; S. Kanemura, T. Ota and K. Tsumura, Phys. Rev. D, 73:016006(2006)[hep-ph/0505191]
    [48] J. L. Diaz-Cruz, D. K. Ghosh and S. Moretti, Phys. Lett. B, 679:376(2009)[arXiv:0809.5158]; M. Arana-Catania, E. Arganda and M. J. Herrero,[arXiv:1304.3371]; A. Arhrib, Y. Cheng and O. C. W. Kong, Phys. Rev. D, 87:015025(2013)[arXiv:1210.8241]; R. Harnik, J. Kopp and J. Zupan, JHEP, 1303:026(2013)[arXiv:1209.1397]; A. Goudelis, O. Lebedev and J.-H. Park, Phys. Lett. B, 707:369(2012)[arXiv:1111.1715]
    [49] G. Eilam, J. L. Hewett and A. Soni, Phys. Rev. D, 44:1473(1991)[Erratum-ibid. D 59, 039901(1999)]
    [50] B. Mele, S. Petrarca and A. Soddu, Phys. Lett. B, 435:401(1998)[hep-ph/9805498]
    [51] S. Bejar, J. Guasch and J. Sola, arxiv:hep-ph/0101294
    [52] B. Mele, arxiv:hep-ph/0003064
    [53] J. L. Diaz-Cruz, R. Martinez, M. A. Perez and A. Rosado, Phys. Rev. D, 41:891(1990)
    [54] J. L. Diaz-Cruz, H.-J. He and C. P. Yuan, Phys. Lett. B, 530:179(2002)[hep-ph/0103178]
    [55] J. A. Aguilar-Saavedra and G. C. Branco, Phys. Lett. B, 495:347(2000)[hep-ph/0004190]
    [56] V. Khachatryan et al.[CMS Collaboration], arXiv:1502.07400
    [57] Aad, Georges et al (ATLAS Collaboration), arXiv:1604.07730

  • Access

    加载中

Get Citation
M. A. Arroyo-Ureña, J. Lorenzo Diaz-Cruz, Enrique Díaz and Javier A. Orduz-Ducuara. Flavor violating Higgs signals in the Texturized Two-Higgs Doublet Model (THDM-Tx)[J]. Chinese Physics C, 2016, 40(12): 123103. doi: 10.1088/1674-1137/40/12/123103
M. A. Arroyo-Ureña, J. Lorenzo Diaz-Cruz, Enrique Díaz and Javier A. Orduz-Ducuara. Flavor violating Higgs signals in the Texturized Two-Higgs Doublet Model (THDM-Tx)[J]. Chinese Physics C, 2016, 40(12): 123103.  doi: 10.1088/1674-1137/40/12/123103 shu
Milestone
Received: 2016-04-20
Revised: 2016-08-04
Article Metric

Article Views(1739)
PDF Downloads(63)
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:

Flavor violating Higgs signals in the Texturized Two-Higgs Doublet Model (THDM-Tx)

  • Received Date: 2016-04-20
  • Accepted Date: 2016-08-04
  • Available Online: 2016-12-05

Abstract: Flavor violating Higgs signals, such as the top FCNC decay t→ch0 and the LFV Higgs decay h0→τμ, have been studied at the LHC. These signals can arise within the general Two-Higgs Doublet Model (THDM), where each Higgs doublet couples to all fermion types through Yukawa matrices Y1f and Y2f. The Yukawa matrices can be assumed to have the same form or they could have different structures. In this paper we study the case when both Y1f and Y2f have completely different forms, but in such a way that they complement to produce a specific hermitian mass matrix. We find that for specific four-zero textures, the flavor violating Higgs couplings depend only on the free parameters tan β, γf and the fermion masses. We use the current bounds on the low energy processes to derive constraints on the heavy Higgs boson mass, tan β and γf. Then, we use these constraints to evaluate the LFV Higgs decays, which reach branching ratios that could be tested at the LHC.

    HTML

Reference (57)

目录

Link
IOPScience
SCOAP3
arXiv
Chinese Physical Society
Journal information
Introduction
Editorial Board
Others
Subscribe
Contact us
QQ: 1307685413
Tel: +86-010-88235947
Fax: +86-010-88233126
E-mail: cpc@ihep.ac.cn

  • CPC Website

  • IOP Website

  • CPC WeChat

Copyright © Institute of High Energy Physics, Chinese Academy of Sciences, 19B Yuquan Road, Beijing 100049, China 京ICP备05002789号-1

Supported by: Beijing Renhe Information Technology Co. Ltd  E-mail: info@rhhz.net

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return