×
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

T-odd top partner pair production in the dilepton final states at the LHC in the littlest Higgs Model with T-parity

  • In the littlest Higgs model with T-parity, we discuss the pair production of the T-odd top partner (T_) that decays almost 100% into the top quark and the lightest T-odd particle (AH). Considering the current constraints, we investigate the observability of the T-odd top partner pair production through the process ppT_T_→ttAHAH in the final states with two leptons at 14 TeV LHC. We analyze the signal significance and found that the lower limits on the T-odd top partner mass are approximately 1.2 TeV, 1.3 TeV, and 1.4 TeV at the 2σ confidence level at 14 TeV LHC with an integrated luminosities of 30 fb-1, 100 fb-1, and 300 fb-1, respectively. This lower limit can be increased to approximately 1.5(1.6) TeV if we used 1000(3000) fb-1 of the integrated luminosity.
      PCAS:
  • 加载中
  • [1] G. Aad et al (ATLAS Collaboration), Phys. Lett. B,, 716:1 (2012)
    [2] S. Chatrchyan et al (CMS Collaboration), Phys. Lett. B, 716:30 (2012)
    [3] L. Susskind, Phys. Rev. D, 20:2619 (1979)
    [4] see examples:J. Li, Z. G. Si, L. Wu, and J. Yue, Phys. Lett. B, 779:72 (2018); J. Cao, L. Wang, L. Wu, and J. M. Yang, Phys. Rev. D, 84:074001 (2011); A. Kobakhidze, L. Wu, and J. Yue, JHEP, 1410:100 (2014)
    [5] H. C. Cheng and I. Low, JHEP, 0309:051 (2003); JHEP, 0408:061 (2004); I. Low, JHEP, 0410:067 (2004)
    [6] N. Liu, L. Wu, B. F. Yang, and M. C. Zhang, Phys. Lett. B, 753:664-669 (2016); H. Y. Wang and B. F. Yang, Adv. High Energy Phys., 2017, 5463128 (2017); B. F. Yang, B. F. Hou, and H. Y. Zhang, Nucl. Phys. B, 929:207 (2018)
    [7] G. Aad et al (ATLAS Collaboration), ATLAS-CONF-2016-013; ATLAS-CONF-2016-101; ATLAS-CONF-2016-102; ATLAS-CONF-2017-015; S. Chatrchyan et al (CMS Collaboration), CMS PAS B2G-15-008; CMS PAS B2G-16-001; CMS PAS SUS-16-029, CMS PAS SUS-16-049; CMS PAS SUS-16-028; CMS PAS SUS-16-051
    [8] G. Aad et al (ATLAS Collaboration), ATLAS-CONF-2017-034, CERN-EP-2017-150
    [9] S. Chatrchyan et al (CMS Collaboration), CMS PAS SUS-16-027
    [10] C. C. Han, A. Kobakhidze, N. Liu, L. Wu, and B. F. Yang, Nucl. Phys. B, 890:388 (2015); Lorenzo Basso, Jeremy Andrea, JHEP, 1502:032 (2015); J. Reuter, M. Tonini, JHEP, 1501:088 (2015); Y. B. Liu, Phys. Rev. D, 95:035013 (2017); Y. B. Liu, Y. Q. Li, Eur. Phys. J. C, 77:654 (2017); M. Chala, Phys.Rev. D, 96:015028 (2017)
    [11] J. Reuter, M. Tonini, and M. de Vries, JHEP, 1402:053 (2014); B. F. Yang, G. F. Mi, and N. Liu, JHEP, 1410:47 (2014)
    [12] G. Aad et al (ATLAS Collaboration), Phys. Rev. Lett., 108:041805 (2012); G. Aad et al (ATLAS Collaboration), JHEP, 1211:094 (2012)
    [13] H. C. Cheng, I. Low, and L. T. Wang, Phys. Rev. D, 74:055001 (2006); A. Anandakrishnan, J. H. Collins, M. Farina, E. Kuflik, and M. Perelstein, Phys. Rev. D, 93:075009 (2016)
    [14] P. Meade and M. Reece, Phys. Rev. D, 74:015010 (2006)
    [15] T. Han, R. Mahbubani, D. G. E. Walker, and L. T. Wang, JHEP, 0905:117 (2009)
    [16] L. Wu, B. F. Yang, and M. C. Zhang, JHEP, 12:152 (2016); B. F. Yang, J. Z. Han, and N. Liu, Phys. Rev. D, 95:035010 (2017); B. F. Yang, Z. Y. Liu and N. Liu, Chin. Phys. C, 41(4):043103 (2017)
    [17] P. Bechtle, S. Heinemeyer, O. Stl, T. Stefaniak, and G. Weiglein, Eur. Phys. J. C, 74:2711 (2014); O. Stl, T. Stefaniak, PoS EPS-HEP, 2013:314 (2013); P. Bechtle, S. Heinemeyer, O. Stl, T. Stefaniak, and G. Weiglein, JHEP, 1411:039 (2014)
    [18] P. Bechtle, O. Brein, S. Heinemeyer, G. Weiglein, and K. E. Williams, Comput. Phys. Commun., 181:138-167 (2010); Comput. Phys. Commun., 182:2605-2631 (2011); P. Bechtle, O. Brein, S. Heinemeyer, O. Stl, T. Stefaniak, G. Weiglein, and K. Williams, PoS CHARGED 2012, 024 (2012); Eur. Phys. J. C, 74:2693 (2014); P. Bechtle, S. Heinemeyer, O. Stl, T. Stefaniak, and G. Weiglein, Eur. Phys. J. C, 75:421 (2015)
    [19] C. R. Chen, K. Tobe, and C.-P. Yuan, Phys. Lett. B, 640:263 (2006)
    [20] L. Wu, B. F. Yang and M. C. Zhang, JHEP, 12:152 (2016)
    [21] D. Dercks, G. Moortgat-Pick, J. Reuter, S. Y. Shim, arXiv:1801.06499
    [22] J. Alwall et al, JHEP, 07:079 (2014)
    [23] M. Czakon, P. Fiedler and A. Mitov, Phys. Rev. Lett., 110:252004 (2013); M. Czakon and A. Mitov, JHEP, 01:080 (2013); M. Czakon and A. Mitov, JHEP, 12:054 (2012); P. Brnreuther, M. Czakon and A. Mitov, Phys. Rev. Lett., 109:132001 (2012); M. Cacciari, M. Czakon, M. Mangano, A. Mitov and P. Nason, Phys. Lett. B, 710:612 (2012); M. Czakon and A. Mitov, Comput. Phys. Commun., 185:2930 (2014); N. Kidonakis, Phys. Rev. D, 82:054018 (2010)
    [24] T. Sjostrand, S. Mrenna, and P. Z. Skands, JHEP, 0605:026 (2006)
    [25] J. de Favereau et al, JHEP, 1402:057 (2014)
    [26] M. Cacciari, G. P. Salam, and G. Soyez, Eur. Phys. J. C, 72:1896 (2012)
    [27] M. Cacciari, G. P. Salam, and G. Soyez, JHEP, 04:063 (2008)
    [28] C. Patrignani et al (Particle Data Group), Chin. Phys. C, 40(10):100001 (2016)
    [29] C. G. Lester and D. J. Summers, Phys. Lett. B, 463:99 (1999); A. Barr, C. Lester, and P. Stephens, J. Phys. G 29:2343 (2003)
    [30] M. Drees et al, Comput. Phys. Commun., 187:227 (2014) J. S. Kim, D. Schmeier, J. Tattersall and K. Rolbiecki, Comput. Phys. Commun., 196:535-562 (2015)
    [31] G. Cowan, K. Cranmer, E. Gross, and O. Vitells, Eur. Phys. J. C, 71:1554 (2011)
  • 加载中

Get Citation
Bingfang Yang, Huaying Zhang, Biaofeng Hou and Ning Liu. T-odd top partner pair production in the dilepton final states at the LHC in the littlest Higgs Model with T-parity[J]. Chinese Physics C, 2018, 42(10): 103102. doi: 10.1088/1674-1137/42/10/103102
Bingfang Yang, Huaying Zhang, Biaofeng Hou and Ning Liu. T-odd top partner pair production in the dilepton final states at the LHC in the littlest Higgs Model with T-parity[J]. Chinese Physics C, 2018, 42(10): 103102.  doi: 10.1088/1674-1137/42/10/103102 shu
Milestone
Received: 2018-05-18
Fund

    Supported by National Natural Science Foundation of China (NNSFC) (11405047, 11305049) and the Startup Foundation for Doctors of Henan Normal University (qd15207).

Article Metric

Article Views(1687)
PDF Downloads(31)
Cited by(0)
Policy on re-use
To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.
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:

T-odd top partner pair production in the dilepton final states at the LHC in the littlest Higgs Model with T-parity

  • 1.  College of Physics and Materials Science, Henan Normal University, Xinxiang 453007, China
  • 2.  Department of Physics and Institute of Theoretical Physics, Nanjing Normal University, Nanjing 210023, China
Fund Project:  Supported by National Natural Science Foundation of China (NNSFC) (11405047, 11305049) and the Startup Foundation for Doctors of Henan Normal University (qd15207).

Abstract: In the littlest Higgs model with T-parity, we discuss the pair production of the T-odd top partner (T_) that decays almost 100% into the top quark and the lightest T-odd particle (AH). Considering the current constraints, we investigate the observability of the T-odd top partner pair production through the process ppT_T_→ttAHAH in the final states with two leptons at 14 TeV LHC. We analyze the signal significance and found that the lower limits on the T-odd top partner mass are approximately 1.2 TeV, 1.3 TeV, and 1.4 TeV at the 2σ confidence level at 14 TeV LHC with an integrated luminosities of 30 fb-1, 100 fb-1, and 300 fb-1, respectively. This lower limit can be increased to approximately 1.5(1.6) TeV if we used 1000(3000) fb-1 of the integrated luminosity.

    HTML

Reference (31)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return