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> 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.
      PCAS:
  • 加载中

  • 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)

  • Access

    加载中

Get Citation
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
Milestone
Received: 2018-08-21
Fund

    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)

Article Metric

Article Views(1731)
PDF Downloads(10)
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:

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.

    HTML

Reference (65)

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