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《中国物理C》（英文）编辑部
2024年10月30日
Chinese Physics C> 2018, Vol. 42> Issue(12) : 123107 DOI: 10.1088/1674-1137/42/12/123107

Probing top-quark couplings indirectly at Higgs factories

  • 1.

      DESY Notkestraß

  • 2.

      PRISMA Cluster of Excellence, Institut fü

  • 3.

      Theoretical Physics Department, CERN, 1211 Geneva 23, Switzerland

  • 4.

      Institute of High Energy Physics, and School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China

  • We perform a global effective-field-theory analysis to assess the combined precision of Higgs couplings, triple gauge-boson couplings, and top-quark couplings, at future circular e+e- colliders, with a focus on runs below the tt production threshold. Deviations in the top-quark sector entering as one-loop corrections are consistently taken into account in the Higgs and diboson processes. We find that future lepton colliders running at center-of-mass energies below the tt production threshold can still provide useful information on top-quark couplings, by measuring virtual top-quark effects. With rate and differential measurements, the indirect individual sensitivity achievable is better than at the high-luminosity LHC. However, strong correlations between the extracted top-quark and Higgs couplings are also present and lead to much weaker global constraints on top-quark couplings. This implies that a direct probe of top-quark couplings above the tt production threshold is also helpful for the determination of Higgs and triple-gauge-boson couplings. In addition, we find that below the e+e-→tth production threshold, the top-quark Yukawa coupling can be determined by its loop corrections to all Higgs production and decay channels. Degeneracy with the ggh coupling can be resolved, and even a global limit is competitive with the prospects of a linear collider above the threshold. This provides an additional means of determining the top-quark Yukawa coupling indirectly at lepton colliders.
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  • References

    [1] G. Aad et al (ATLAS), Phys. Lett. B, 716:1 (2012), arXiv:1207.7214[hep-ex]
    [2] S. Chatrchyan et al (CMS), Phys. Lett. B, 716:30 (2012), arXiv:1207.7235[hep-ex]
    [3] J. Ellis and T. You, JHEP, 03:089 (2016), arXiv:1510.04561 [hep-ph]
    [4] J. Ellis, P. Roloff, V. Sanz, and T. You, JHEP, 05:096 (2017), arXiv:1701.04804[hep-ph]
    [5] G. Durieux, C. Grojean, J. Gu, and K. Wang, JHEP, 09:014 (2017), arXiv:1704.02333[hep-ph]
    [6] T. Barklow, K. Fujii, S. Jung, R. Karl, J. List, T. Ogawa, M. E. Peskin, and J. Tian, Phys. Rev. D, 97:053003 (2018), arXiv:1708.08912[hep-ph]
    [7] T. Barklow, K. Fujii, S. Jung, M. E. Peskin, and J. Tian, Phys. Rev. D, 97:053004 (2018), arXiv:1708.09079[hep-ph]
    [8] S. Di Vita, G. Durieux, C. Grojean, J. Gu, Z. Liu, G. Panico, M. Riembau, and T. Vantalon, JHEP, 02:178 (2018), arXiv:1711.03978[hep-ph]
    [9] W. H. Chiu, S. C. Leung, T. Liu, K.-F. Lyu, and L.-T. Wang, JHEP, 05:081 (2018), arXiv:1711.04046[hep-ph]
    [10] M. McCullough, Phys. Rev. D, 90:015001 (2014); Erratum: Phys. Rev. D, 92(3):039903 (2015), arXiv:1312.3322[hep-ph]
    [11] G. Durieux, M. Perell, M. Vos, and C. Zhang, arXiv:1807.02121[hep-ph]
    [12] E. Vryonidou and C. Zhang, JHEP, 08:036 (2018), arXiv:1804.09766[hep-ph]
    [13] C. Hartmann and M. Trott, JHEP, 07:151 (2015), arXiv:1505.02646[hep-ph]
    [14] M. Ghezzi, R. Gomez-Ambrosio, G. Passarino, and S. Uccirati, JHEP, 07:175 (2015), arXiv:1505.03706[hep-ph]
    [15] C. Hartmann and M. Trott, Phys. Rev. Lett., 115:191801 (2015), arXiv:1507.03568[hep-ph]
    [16] R. Gauld, B. D. Pecjak, and D. J. Scott, JHEP, 05:080 (2016), arXiv:1512.02508[hep-ph]
    [17] R. Gauld, B. D. Pecjak, and D. J. Scott, Phys. Rev. D, 94:074045 (2016), arXiv:1607.06354[hep-ph]
    [18] S. Dawson and P. P. Giardino, Phys. Rev. D, 97:093003 (2018), arXiv:1801.01136[hep-ph]
    [19] A. Dedes, M. Paraskevas, J. Rosiek, K. Suxho, and L. Trifyllis, JHEP, 08:103 (2018), arXiv:1805.00302[hep-ph]
    [20] S. Dawson and P. P. Giardino, arXiv:1807.11504[hep-ph]
    [21] S. Dawson and A. Ismail, SMEFT Corrections to Z Boson Decays, (2018), arXiv:1808.05948[hep-ph]
    [22] S. Weinberg, Phenomenological Lagrangians, Proceedings, Symposium Honoring Julian Schwinger on the Occasion of his 60th Birthday:Los Angeles, California, February 18-19, 1978, Physica A, 96:327 (1979)
    [23] C. N. Leung, S. T. Love, and S. Rao, Z. Phys. C, 31:433 (1986)
    [24] W. Buchmuller and D. Wyler, Nucl. Phys. B, 268:621 (1986)
    [25] C. Degrande, N. Greiner, W. Kilian, O. Mattelaer, H. Mebane, T. Stelzer, S. Willenbrock, and C. Zhang, Annals Phys., 335:21 (2013), arXiv:1205.4231[hep-ph]
    [26] S. Weinberg, Effective Field Theory, Past and Future, PoS, CD09:001 (2009), arXiv:0908.1964[hep-th]
    [27] A. Kobakhidze, N. Liu, L. Wu, and J. Yue, Phys. Rev. D, 95:015016 (2017), arXiv:1610.06676[hep-ph]
    [28] Z. Liu, I. Low, and L.-T. Wang, Higgs-top interactions at future circular e+e- colliders, (2018), arXiv:2018.xxxxx
    [29] ATLAS Collaboration, ATL-PHYS-PUB-2017-001 (2017)
    [30] C. Zhang, N. Greiner, and S. Willenbrock, Phys. Rev. D, 86:014024 (2012), arXiv:1201.6670[hep-ph]
    [31] M. E. Peskin and T. Takeuchi, Phys. Rev. D, 46:381 (1992)
    [32] J. Alwall, R. Frederix, S. Frixione, V. Hirschi, F. Maltoni, O. Mattelaer, H. S. Shao, T. Stelzer, P. Torrielli, and M. Zaro, JHEP, 07:079 (2014), arXiv:1405.0301[hep-ph]
    [33] O. Mattelaer, Eur. Phys. J. C, 76:674 (2016), arXiv:1607.00763[hep-ph]
    [34] D. Kreimer, Phys. Lett. B, 237:59 (1990)
    [35] J. G. Korner, D. Kreimer, and K. Schilcher, Z. Phys. C, 54:503 (1992)
    [36] D. Kreimer, The Role of 5 in dimensional regularization, (1993), arXiv:hep-ph/9401354
    [37] A. Pomarol and F. Riva, JHEP, 01:151 (2014), arXiv:1308.2803[hep-ph]
    [38] T. Corbett, O. J. P. Eboli, J. Gonzalez-Fraile, and M. C. Gonzalez-Garcia, Phys. Rev. Lett., 111:011801 (2013), arXiv:1304.1151[hep-ph]
    [39] A. Falkowski, M. Gonzalez-Alonso, A. Greljo, and D. Marzocca, Phys. Rev. Lett., 116:011801 (2016), arXiv:1508.00581 [hep-ph]
    [40] J. Wess and B. Zumino, Phys. Lett. B, 37:95 (1971)
    [41] C. Patrignani et al (Particle Data Group), Chin. Phys. C, 40:100001 (2016)
    [42] J. D. Wells and Z. Zhang, JHEP, 01:123 (2016), arXiv:1510.08462[hep-ph]
    [43] C. Degrande, J. M. Gerard, C. Grojean, F. Maltoni, and G. Servant, JHEP, 07:036 (2012); Erratum:JHEP, 03:032 (2013), arXiv:1205.1065[hep-ph]
    [44] F. Maltoni, E. Vryonidou, and C. Zhang, JHEP, 10:123 (2016), arXiv:1607.05330[hep-ph]
    [45] CEPC-SPPC Study Group, CEPC-SPPC Preliminary Conceptual Design Report. 1. Physics and Detector (2015)
    [46] M. Bicer et al (TLEP Design Study Working Group), First Look at the Physics Case of TLEP, Proceedings, 2013 Community Summer Study on the Future of U.S. Particle Physics: Snowmass on the Mississippi (CSS2013):Minneapolis, MN, USA, July 29-August 6, 2013, JHEP, 01:164 (2014), arXiv:1308.6176[hep-ex]
    [47] M. Benedikt and F. Zimmerman, FCC Week, Amsterdam, 9 Apr 2018
    [48] M. J. Boland et al (CLICdp, CLIC), Updated baseline for a staged Compact Linear Collider, 10.5170/CERN-2016-004, arXiv:1608.07537[physics.acc-ph]
    [49] H. Baer, T. Barklow, K. Fujii, Y. Gao, A. Hoang, S. Kanemura, J. List, H. E. Logan, A. Nomerotski, M. Perelstein, et al, The International Linear Collider Technical Design Report - Volume 2:Physics, arXiv:1306.6352[hep-ph]
    [50] A. M. Sirunyan et al (CMS), JHEP, 09:051 (2017), arXiv:1701.06228[hep-ex]
    [51] B. Schoenrock, E. Drueke, B. Alvarez Gonzalez, and R. Schwienhorst, Proceedings, 2013 Community Summer Study on the Future of U.S. Particle Physics:Snowmass on the Mississippi (CSS2013):Minneapolis, MN, USA, July 29- August 6, 2013, arXiv:1308.6307[hep-ex]
    [52] M. Aaboud et al (ATLAS), Eur. Phys. J. C, 77:264 (2017), arXiv:1612.02577[hep-ex]
    [53] ATLAS Collaboration, Projections for measurements of Higgs boson signal strengths and coupling parameters with the ATLAS detector at a HL-LHC, ATL-PHYS-PUB-2014-016 (2014)
    [54] E. L. Berger, J. Gao, C. P. Yuan, and H. X. Zhu, Phys. Rev. D, 94:071501 (2016), arXiv:1606.08463[hep-ph]
    [55] A. Czarnecki, J. G. Korner, and J. H. Piclum, Phys. Rev. D, 81:111503 (2010), arXiv:1005.2625[hep-ph]
    [56] S. Di Vita, C. Grojean, G. Panico, M. Riembau, and T. Vantalon, JHEP, 09:069 (2017), arXiv:1704.01953[hep-ph]
    [57] A. Azatov, R. Contino, G. Panico, and M. Son, Phys. Rev. D, 92:035001 (2015), arXiv:1502.00539[hep-ph]
    [58] M. Beneke, D. Boito, and Y.-M. Wang, JHEP, 11:028 (2014), arXiv:1406.1361[hep-ph]
    [59] N. Craig, J. Gu, Z. Liu, and K. Wang, JHEP, 03:050 (2016), arXiv:1512.06877[hep-ph]
    [60] O. Bessidskaia Bylund, F. Maltoni, I. Tsinikos, E. Vryonidou, and C. Zhang, JHEP, 05:052 (2016), arXiv:1601.08193[hepph]
    [61] S. Boselli, R. Hunter, and A. Mitov, Prospects for the determination of the top-quark Yukawa coupling at future e+e- colliders, (2018), arXiv:1805.12027[hep-ph]
    [62] C. Shen and S.-h. Zhu, Phys. Rev. D, 92:094001 (2015), arXiv:1504.05626[hep-ph]
    [63] H. Abramowicz et al (CLICdp), Top-Quark Physics at the CLIC Electron-Positron Linear Collider, arXiv:1807.02441 [hep-ex]
    [64] R. Yonamine, K. Ikematsu, T. Tanabe, K. Fujii, Y. Kiyo, Y. Sumino, and H. Yokoya, Phys. Rev. D, 84:014033 (2011), arXiv:1104.5132[hep-ph]
    [65] W. A. Bardeen and B. Zumino, Nucl. Phys. B, 244:421 (1984)

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Gauthier Durieux, Jiayin Gu, Eleni Vryonidou and Cen Zhang. Probing top-quark couplings indirectly at Higgs factories[J]. Chinese Physics C, 2018, 42(12): 123107. doi: 10.1088/1674-1137/42/12/123107
Gauthier Durieux, Jiayin Gu, Eleni Vryonidou and Cen Zhang. Probing top-quark couplings indirectly at Higgs factories[J]. Chinese Physics C, 2018, 42(12): 123107.  doi: 10.1088/1674-1137/42/12/123107 shu
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Received: 2018-08-21
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    CZ is supported by IHEP (Y7515540U1)

    EV is supported by a Marie Sklodowska-Curie Individual Fellowship of the European Commission's Horizon 2020 Programme (704187)

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Probing top-quark couplings indirectly at Higgs factories

    Corresponding author: Gauthier Durieux,
    Corresponding author: Jiayin Gu,
    Corresponding author: Eleni Vryonidou,
    Corresponding author: Cen Zhang,
  • 1.  DESY Notkestraß
  • 2.  PRISMA Cluster of Excellence, Institut fü
  • 3.  Theoretical Physics Department, CERN, 1211 Geneva 23, Switzerland
  • 4.  Institute of High Energy Physics, and School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
  • Received Date: 2018-08-21
  • Available Online: 2018-12-05
Fund Project:  CZ is supported by IHEP (Y7515540U1) EV is supported by a Marie Sklodowska-Curie Individual Fellowship of the European Commission's Horizon 2020 Programme (704187)

Abstract: We perform a global effective-field-theory analysis to assess the combined precision of Higgs couplings, triple gauge-boson couplings, and top-quark couplings, at future circular e+e- colliders, with a focus on runs below the tt production threshold. Deviations in the top-quark sector entering as one-loop corrections are consistently taken into account in the Higgs and diboson processes. We find that future lepton colliders running at center-of-mass energies below the tt production threshold can still provide useful information on top-quark couplings, by measuring virtual top-quark effects. With rate and differential measurements, the indirect individual sensitivity achievable is better than at the high-luminosity LHC. However, strong correlations between the extracted top-quark and Higgs couplings are also present and lead to much weaker global constraints on top-quark couplings. This implies that a direct probe of top-quark couplings above the tt production threshold is also helpful for the determination of Higgs and triple-gauge-boson couplings. In addition, we find that below the e+e-→tth production threshold, the top-quark Yukawa coupling can be determined by its loop corrections to all Higgs production and decay channels. Degeneracy with the ggh coupling can be resolved, and even a global limit is competitive with the prospects of a linear collider above the threshold. This provides an additional means of determining the top-quark Yukawa coupling indirectly at lepton colliders.

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