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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.
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  • 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

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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
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Received: 2016-04-20
Revised: 2016-08-04
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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.

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