×
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

Production of the new gauge boson BH via e collision in the littlest Higgs model

  • The lightest new gauge boson BH with mass of hundreds GeV is predicted in the littlest Higgs model. BH should be accessible in the planned ILC and the observation of such particle can strongly support the littlest Higgs model. The realization of γγ and eγ collisions would open a wider window to probe BH. In this paper, we study the new gauge boson BH production processes e-γ→e-γ
    BH and e-γ→e-ZBH at the ILC. Our results show that the production cross section of the process e-γ→e-ZBH is less than 0.1fb in most parameter spaces allowed by the electroweak precision data while the cross section of the process e-γ→e-γBH can be over one fb in the favorable parameter spaces. With the high luminosity, the enough typical signals could be produced via ee-γ→e-γBH.
    Because the final electron and photon beams can be easily identified and the signal can be easily distinguished from the backgrounds produced by Z and H decaying, e-γ→e-γBH is a promising process to probe BH.

  • 加载中
  • [1] . Schmaltz M, Tucker-Smith D. Ann. Rev. Nucl. Part. Sci.,2005, 55: 229; HAN T, Logen H E, McElrath B et al.JHEP, 2006, 0601: 0992. Arkani-Hamed N, Cohen A G, Gregoire T et al. JHEP,2002, 0208: 020; Arkani-Hamed N, Cohen A G, Katz E et al. JHEP, 2002, 0208: 0213. Low I, Skiba W, Smith D. Phys. Rev. D, 2002, 66: 072001;Skiba W, Terning J. Phys. Rev. D, 2003, 68: 075001; Kaplan D E, Schmaltz M. JHEP, 2003, 0310: 0394. CHANG S, Wacker J G. Phys. Rev. D, 2004, 69: 035002;CHANG S. JHEP, 2003, 0312: 0575. Arkani-Hamed N, Cohen A G, Katz E et al. JHEP, 2002,0207: 0346. Perelstein M. Prog. Part. Nucl. Phys., 2007, 58: 2477. Badelek B et al. Inter. Jour. Mod. Phys. A, 2004, 30: 50978. Thlnov V I. Acta Phys. Polon. B, 2006, 37: 1049; Telnov V I. Acta Phys. Polon. B, 2006, 37: 633; Battaglia M,Barklow T, Peskin M E et al. hep-ex/06030109. Boos E et al. Nucl. Instrum. Methods Phys.Res., Sect. A, 2001, 472: 100; Brodsky S J. Int. J. Mod. Phys. A, 2003,18: 287110. WANG X L, CHEN J H, LIU Y B et al. Phys. Rev. D,2006, 74: 01500611. YUE C X, WANG W. Phys. Rev. D, 2005, 71: 01500212. HAN T, Logan H E, McElrath B et al. Phys. Rev. D, 2003,67: 09500413. Logan H E. Phys. Rev. D, 2004, 70: 11500314. Buras A J, Poschenrieder A, Uhlig S. Nucl. Phys. B, 2005,716: 173; Choudhury S R, Gaur N, Joshi G C et al. hep-ph/0408125; Choudhury S R, Gaur N, Goyal A et al. Phys.Lett. B, 2004, 601: 16415. Park S C, SONG J. Phys. Rev. D, 2004, 69: 115010; Hubisz J, Meade P. Phys. Rev. D, 2005, 71: 035016; Schmaltz M, Tucker-Smith D. Ann. Rev. Nucl. Part. Sci., 2005, 55:229; Kilian W, Reuter J. Phys. Rev. D, 2004, 70: 015004;Blanke M, Buras A J et al. JHEP, 2007, 0701: 066; CHEN M C, Dawson S. Phys. Rev. D, 2004, 70: 015003; CHEN M C. Mod. Phys. Lett. A, 2006, 21: 621; Casalbuoni R, Deandrea A, Oertel M. JHEP, 2004, 0402: 03216. Conley J A, Hewett J, Le M P. Phys. Rev. D, 2005, 72:11501417. Hewett J L, Petriello F J et al. JHEP, 2003, 0310: 062;Csaki C, Hubisz J, Kribs G D et al. Phys. Rev. D, 2003,67: 11500218. Csaki C, Hubisz J, Kribs G D et al. Phys. Rev. D, 2003,68: 035009; Gregoire T, Smith D R, Wacker J G. Phys.Rev. D, 2004, 69: 11500819. Buras A J, Poschenrieder A et al. JHEP, 2006, 0611: 06220. Jikia G. Nucl. Phys. B, 1992, 374: 83; Eboli O J P et al.Phys. Rev. D, 1993, 47: 1889; Cheung K M. ibid., 1993,47: 375021. Donoghue J F, Golowich E, Holstein B R. Dynamics of the Standard Model. Cambridge: Cambridge Univiversity Press, 1992. 3422. Dittmaier S, Bohm M. Nucl. Phys. B, 1994, 412: 3923. Eboli O J P, Gonzaléz-García M C, Novaes S F. Nucl. Phys.B, 1994, 411: 381; Cheung K. Nucl. Phys. B, 1993, 403:572
  • 加载中

Get Citation
WANG Xue-Lei, JIN Zhen-Lan and ZENG Qing-Guo. Production of the new gauge boson BH via e collision in the littlest Higgs model[J]. Chinese Physics C, 2008, 32(3): 165-171. doi: 10.1088/1674-1137/32/3/001
WANG Xue-Lei, JIN Zhen-Lan and ZENG Qing-Guo. Production of the new gauge boson BH via e collision in the littlest Higgs model[J]. Chinese Physics C, 2008, 32(3): 165-171.  doi: 10.1088/1674-1137/32/3/001 shu
Milestone
Received: 2007-04-23
Revised: 2007-07-17
Article Metric

Article Views(4140)
PDF Downloads(728)
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:

Production of the new gauge boson BH via e collision in the littlest Higgs model

    Corresponding author: WANG Xue-Lei,

Abstract: 

The lightest new gauge boson BH with mass of hundreds GeV is predicted in the littlest Higgs model. BH should be accessible in the planned ILC and the observation of such particle can strongly support the littlest Higgs model. The realization of γγ and eγ collisions would open a wider window to probe BH. In this paper, we study the new gauge boson BH production processes e-γ→e-γ
BH and e-γ→e-ZBH at the ILC. Our results show that the production cross section of the process e-γ→e-ZBH is less than 0.1fb in most parameter spaces allowed by the electroweak precision data while the cross section of the process e-γ→e-γBH can be over one fb in the favorable parameter spaces. With the high luminosity, the enough typical signals could be produced via ee-γ→e-γBH.
Because the final electron and photon beams can be easily identified and the signal can be easily distinguished from the backgrounds produced by Z and H decaying, e-γ→e-γBH is a promising process to probe BH.

    HTML

Reference (1)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return