×
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

An optimal scheme for top quark mass measurement near the tt threshold at future e+e- colliders

  • A top quark mass measurement scheme near the tt production threshold in future e+e- colliders, e.g.the Circular Electron Positron Collider (CEPC), is simulated. A χ2 fitting method is adopted to determine the number of energy points to be taken and their locations. Our results show that the optimal energy point is located near the largest slope of the cross section v. beam energy plot, and the most efficient scheme is to concentrate all luminosity on this single energy point in the case of one-parameter top mass fitting. This suggests that the so-called data-driven method could be the best choice for future real experimental measurements. Conveniently, the top mass statistical uncertainty can also be calculated directly by the error matrix even without any sampling and fitting. The agreement of the above two optimization methods has been checked. Our conclusion is that by taking 50 fb-1 total effective integrated luminosity data, the statistical uncertainty of the top potential subtracted mass can be suppressed to about 7 MeV and the total uncertainty is about 30 MeV. This precision will help to identify the stability of the electroweak vacuum at the Planck scale.
      PCAS:
  • 加载中
  • [1] Particle Data Group, C. Patrignani et al, Chin. Phys. C, 40:100001(2016)
    [2] A. H. Hoang, M. C. Smith, T. Stelzer, and S. Willenbrock, Phys. Rev. D, 59:114014(1999), arXiv:hep-ph/9804227
    [3] M. C. Smith and S. S. Willenbrock, Phys. Rev. Lett., 79:3825(1997), arXiv:hep-ph/9612329
    [4] M. Beneke and V. M. Braun, Nucl. Phys. B, 426:301(1994), arXiv:hep-ph/9402364
    [5] P. Nason, arXiv:1712.02796
    [6] M. Beneke, Phys. Lett. B, 434:115(1998), arXiv:hep-ph/9804241
    [7] Y. Kiyo and Y. Sumino, Phys. Rev. D, 67:071501(2003), arXiv:hep-ph/0211299
    [8] A. H. Hoang and T. Teubner, Phys. Rev. D, 58:114023(1998), arXiv:hep-ph/9801397
    [9] U. Husemann, Prog. Part. Nucl. Phys., 95:48(2017), arXiv:1704.01356
    [10] J. Fuster, A. Irles, D. Melini, P. Uwer, and M. Vos, (2017), arXiv:1704.00540
    [11] G. Cortiana, Rev. Phys., 1:60(2016), arXiv:1510.04483
    [12] CMS, S. Chatrchyan et al, Phys. Lett. B, 728:496(2014), arXiv:1307.1907; Phys. Lett.B, 738:526(2014)
    [13] D0, V. M. Abazov et al, Phys. Lett., B703:422(2011), arXiv:1104.2887.
    [14] M. Martinez and R. Miquel, Eur. Phys. J. C, 27:49(2003), arXiv:hep-ph/0207315
    [15] K. Seidel, F. Simon, M. Tesar, and S. Poss, Eur. Phys. J. C, 73:2530(2013), arXiv:1303.3758
    [16] F. Simon, PoS, ICHEP2016:872(2017), arXiv:1611.03399
    [17] F. James, Comput. Phys. Commun., 20:29(1980)
    [18] B. A. Thacker and G. P. Lepage, Phys. Rev. D, 43:196(1991)
    [19] G. P. Lepage, L. Magnea, C. Nakhleh, U. Magnea, and K. Hornbostel, Phys. Rev. D, 46:4052(1992), arXiv:hep-lat/9205007
    [20] A. Pineda and J. Soto, Nucl. Phys. Proc. Suppl., 64:428(1998), arXiv:hep-ph/9707481
    [21] M. Beneke et al, Phys. Rev. Lett., 115:192001(2015), arXiv:1506.06864
    [22] A. Pineda, Phys. Rev. D, 66:054022(2002), arXiv:hep-ph/0110216
    [23] A. H. Hoang, A. V. Manohar, I. W. Stewart, and T. Teubner, Phys. Rev. Lett., 86:1951(2001), arXiv:hep-ph/0011254
    [24] A. H. Hoang, A. V. Manohar, I. W. Stewart, and T. Teubner, Phys. Rev. D, 65:014014(2002), arXiv:hep-ph/0107144
    [25] A. Pineda, Phys. Rev. D, 65:074007(2002), arXiv:hep-ph/0109117
    [26] A. Pineda and A. Signer, Nucl. Phys. B, 762:67(2007), arXiv:hep-ph/0607239
    [27] A. H. Hoang and M. Stahlhofen, JHEP, 1405:121(2014), arXiv:1309.6323
    [28] W. Kilian, T. Ohl, and J. Reuter, Eur. Phys. J. C, 71:1742(2011), arXiv:0708.4233
    [29] J. Reuter et al, Top Physics in WHIZARD:in Proceedings, International Workshop on Future Linear Colliders (LCWS15):Whistler, B.C., Canada, November 02-06, 2015, 2016, arXiv:1602.08035
    [30] J. Reuter et al, PoS, RADCOR2015:088(2015), arXiv:1601.02459
    [31] F. Bach and M. Stahlhofen, Top pair threshold production at a linear collider with WHIZARD:in Proceedings, 7th International Workshop on Top Quark Physics (TOP2014):Cannes, France, September 28-October 3, 2014, arXiv:1411.7318
    [32] A. H. Hoang and M. Stahlhofen, JHEP, 05:121(2014), arXiv:1309.6323
    [33] A. H. Hoang, C. J. Reisser, and P. Ruiz-Femenia, Phys. Rev. D, 82:014005(2010), arXiv:1002.3223
    [34] M. Beneke, J. Piclum, and T. Rauh, Nucl. Phys. B, 880:414(2014), arXiv:1312.4792
    [35] M. Beneke, Y. Kiyo, and K. Schuller, (2013), arXiv:1312.4791
    [36] M. Beneke, Y. Kiyo, A. Maier, and J. Piclum, Comput. Phys. Commun., 209:96(2016), arXiv:1605.03010
    [37] X. Mo, G. Li, M.-Q. Ruan, and X.-C. Lou, Chin. Phys. C, 40:033001(2016), arXiv:1505.01008
    [38] CEPC-SPPC Study Group, CEPC-SPPC Preliminary Conceptual Design Report. 2. Accelerator, 2015
    [39] M. Koratzinos, CEPC design performance considerations:in Proceedings, 55th ICFA Advanced Beam Dynamics Workshop on High Luminosity Circular e+e-Colliders-Higgs Factory (HF2014):Beijing, China, October 9-12, 2014:p. THT4A2, 2015, arXiv:1501.06854
    [40] E. A. Kuraev and V. S. Fadin, Sov. J. Nucl. Phys., 41:466(1985),[Yad. Fiz. 41:733(1985)]
    [41] X. H. Mo, Int. J. Mod. Phys. A, 30:1550149(2015), arXiv:1505.00059
    [42] T. Horiguchi et al, (2013), arXiv:1310.0563.
    [43] A. H. Hoang and C. J. Reisser, Phys. Rev. D, 71:074022(2005), arXiv:hep-ph/0412258
    [44] TLEP Design Study Working Group, M. Bicer et al, JHEP, 01:164(2014), arXiv:1308.6176
    [45] M. Beneke, P. Marquard, P. Nason, and M. Steinhauser, Phys. Lett. B, 775:63(2017), arXiv:1605.03609
    [46] A. H. Hoang, C. Lepenik, and M. Preisser, JHEP, 1709:099(2017), arXiv:1706.08526
    [47] P. Marquard, A. V. Smirnov, V. A. Smirnov, M. Steinhauser, and D. Wellmann, Phys. Rev. D, 94(7):074025(2016) arXiv:1606.06754
    [48] M. Beneke, Y. Kiyo, and K. Schuller, Nucl. Phys. B, 714:67(2005), arXiv:hep-ph/0501289
    [49] S. A. Larin and J. A. M. Vermaseren, Phys. Lett. B, 303:334(1993), arXiv:hep-ph/9302208
    [50] Y. Schroder, Phys. Lett. B, 447:321(1999), arXiv:hep-ph/9812205
    [51] A. Djouadi, Phys. Rept., 457:1(2008), arXiv:hep-ph/0503172
    [52] CMS Collaboration, (2012), CMS-PAS-TOP-11-015
    [53] G. Degrassi et al, JHEP, 08:098(2012), arXiv:1205.6497
    [54] S. Alekhin, A. Djouadi, and S. Moch, Phys. Lett. B, 716:214(2012), arXiv:1207.0980
    [55] Z. Chen et al, Chin. Phys. C, 41:023003(2017), arXiv:1601.05352
  • 加载中

Get Citation
Wei-Guo Chen, Xia Wan and You-Kai Wang. An optimal scheme for top quark mass measurement near the tt threshold at future e+e- colliders[J]. Chinese Physics C, 2018, 42(5): 053002. doi: 10.1088/1674-1137/42/5/053002
Wei-Guo Chen, Xia Wan and You-Kai Wang. An optimal scheme for top quark mass measurement near the tt threshold at future e+e- colliders[J]. Chinese Physics C, 2018, 42(5): 053002.  doi: 10.1088/1674-1137/42/5/053002 shu
Milestone
Received: 2018-01-05
Revised: 2018-03-04
Fund

    Supported by National Science Foundation of China (11405102) and the Fundamental Research Funds for the Central Universities of China (GK201603027, GK201803019)

Article Metric

Article Views(1612)
PDF Downloads(19)
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:

An optimal scheme for top quark mass measurement near the tt threshold at future e+e- colliders

    Corresponding author: Wei-Guo Chen,
    Corresponding author: Xia Wan,
    Corresponding author: You-Kai Wang,
Fund Project:  Supported by National Science Foundation of China (11405102) and the Fundamental Research Funds for the Central Universities of China (GK201603027, GK201803019)

Abstract: A top quark mass measurement scheme near the tt production threshold in future e+e- colliders, e.g.the Circular Electron Positron Collider (CEPC), is simulated. A χ2 fitting method is adopted to determine the number of energy points to be taken and their locations. Our results show that the optimal energy point is located near the largest slope of the cross section v. beam energy plot, and the most efficient scheme is to concentrate all luminosity on this single energy point in the case of one-parameter top mass fitting. This suggests that the so-called data-driven method could be the best choice for future real experimental measurements. Conveniently, the top mass statistical uncertainty can also be calculated directly by the error matrix even without any sampling and fitting. The agreement of the above two optimization methods has been checked. Our conclusion is that by taking 50 fb-1 total effective integrated luminosity data, the statistical uncertainty of the top potential subtracted mass can be suppressed to about 7 MeV and the total uncertainty is about 30 MeV. This precision will help to identify the stability of the electroweak vacuum at the Planck scale.

    HTML

Reference (55)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return