簡易檢索 / 詳目顯示

研究生: 粟星輔
論文名稱: 在強子對撞機中找尋頂夸克與膠子間的異常耦合
Probing the Anomalous Top-gluon Coupling at Hadron Colliders
指導教授: 張敬民
口試委員: 耿朝強
張維甫
阮自強
學位類別: 碩士
Master
系所名稱: 理學院 - 物理學系
Department of Physics
論文出版年: 2014
畢業學年度: 102
語文別: 英文
論文頁數: 31
中文關鍵詞: 對撞機頂夸克兆電子伏特加速器大型強子對撞機
外文關鍵詞: top quark, CEDM, CMDM
相關次數: 點閱:3下載:0
分享至:
查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報
  • 藉由對撞機中所產生的正反頂夸克對,我們用以研究由電偶極矩及磁偶極矩所引起頂夸克與膠子之間的異常耦合。並藉由等效場論的方法,我們得以計算頂夸克的電偶極矩及磁偶極矩如何影響在對撞機中正反頂夸克對產生的散射截面。並將其理論計算的結果與兆電子伏特加速器(Tevatron)以及大型強子對撞機(LHC)最新的實驗結果進行對比,以了解偶極矩數值的許可範圍。接下來,我們利用兩種與頂夸克自旋數有關的不對稱值來觀察頂夸克的衰變產物。藉由此一方法我們可以觀察異常耦合的影響並給出偶極矩數值的限制。


    Through top quark-pair production at hadron collider, we study the possible effects of nonstandard top-gluon couplings are composed of chromomagnetic dipole moments and chrmoelectric dipole moments, CMDM and CEDM, of top quarks. And using the effective operators, which produces anomalous coupling of top quark to calculate the total cross section for the top-pair production process pp/p¯p → t¯tX. By comparing the latest result of the total cross section at Tevatron and LHC, can us describe these anomalous coupling parameters as an allowed region on the coordinate plane. And
    we found that there is a common space consist in all the region, which made by different experiment. Next we offer another method to give constraint on nonstandard top-gluon couplings by analysing the different type of asymmetries, and these asymmetries are related to the t¯t spin correlation. Then we compared to the LHC measurement result at 7 TeV to find out the possible values of anomalous top-gluon coupling parameters.

    1 Introduction 1 2 Framework 4 2.1 Effective Lagrangian . . . . . . . . . . . . . . . . . . . . . . . 4 2.2 Set-up of the computation . . . . . . . . . . . . . . . . . . . . 5 3 Numerical analysis 11 3.1 Analysis of Tevatron data . . . . . . . . . . . . . . . . . . . . 11 3.2 Total cross section of top-pair production at LHC . . . . . . . 14 3.3 Asymmetry in top-pair production . . . . . . . . . . . . . . . 18 4 Conclusion 26 Bibliography 28

    [1] CDF Collaboration, F. Abe et al., Phys. Rev. Lett. 74, 2626 (1995)
    [2] D∅ Collaboration, S. Abachi et al., Phys. Rev. Lett. 74, 2632 (1995)
    [3] D. Atwood, A. Aeppli, and A. Soni, Phys. Rev. Lett. 69, 2754 (1992).
    [4] D. Atwood, A. Kagan, and T. G. Rizzo. Phys. Rev. D 52, 6264 (1995).
    [5] P. Haberl, O. Nachtmann, A. Wilch. Phys.Rev. D53 (1996) 487
    arXiv:hep-ph/9505409
    [6] K. -m. Cheung, Phys. Rev. D 53, 3604 (1996) [hep-ph/9511260];
    K. Cheung, Phys. Rev. D 55, 4430 (1997).
    [7] R. Mart´ınz, M.A. P´erez, N. Poveda. Phys. J. C 53, 211 (2008)
    [8] T. Ibrahim, P, Nath Phys.Rev.D 84:015003,(2011) arXiv:1104.3851v2
    [hep-ph]
    [9] R. Mart´ınez, J.A. Rod´riguez,Phys. Rev. D 65,057301(2002)
    [10] W. Buchm¨uller and D. Wyler, Nucl. Phys. B433. 41 (1995).
    [11] B. Grazadkowski, M Iskrzynski, M Misiak and J.Rosiek, J. High Energy
    Phys. 10 (2010) 085.
    [12] Z. Hioki and K. Ohkuma, Eur. Phys. J. C65 127(2010)
    [13] Z. Hioki and K. Ohkuma, Phys. Rev. D 88,017503, (2013)
    [14] I. B. Khriplovich Phys. Lett. B 173(1986) 193; A. Czarnecki and B.
    Krause,Acta Phys. Polon. B 28(1997) 829.
    [15] J.A.M. Vermaseren, Symbolic Manipulation with FORM, Version 2, Tu-
    torial and Reference Manual (CAN, Amsterdam 1991). ISBN 90-74116-
    01-9
    [16] M. Glu¨ck, J.F. Owens, E.Reya, Phys. Rev. D 17, 2324 (1978)
    [17] B.L. Combridge, Nuc.l Phys. B 151, 429 (1979)
    [18] Johan Alwall, Michel Herquet, Fabio Maltoni, Olivier Mattelaer,
    Tim Stelzer “MadGraph 5: going beyond”, JHEP 06(2011) 128,
    doi:10.1007/JHEP06(2011)128, arXiv:1106.0522.
    [19] Neil D. Christensen, Claude Duhr “FeynRules - Feynman
    rules made easy” Comput. Phys. Commun. 180 (2009) 1614,
    doi:10.1016/j.cpc.2009.02.018, arXiv::0806.4194.
    [20] A. Alloul, N. D. Christensen, C. Degrande, C. Duhr, B. Fuks “FeynRules
    2.0 - A complete toolbox for tree-level phenomenology” arXiv:1310.1921.
    [21] J. M. Campbell, J. W. Huston and W. J. Stirling, Rept. Prog. Phys. 70,
    89(2007) arXiv: hep-ph/0611148.
    [22] Tevatron Electroweak Working Group, CDF Note 10926 and D∅ Note
    6363 arXiv: 13097570
    [23] M. Cacciari, S. Frixione, M. L. Mangano, P. Nason, and G. Ridolofi J.
    High Energy Phys. 04 (2004); 06809 (2008) 127.
    [24] N. Kidonakis, R. Vogt, Phys. Rev. D 78, 074005 (2008).
    arXiv:0805.3844 [hep-ph]
    [25] S. Moch, P. Uwer, Phys. Rev. D 78, 034003 (2008).
    arXiv:0804.1476 [hep-ph]
    [26] ATLAS and CMS Collaborations, Reports No. ATLAS-CONF-2012-134
    and No. CMS-PAS-TOP-12-003, 2012.
    [27] CMS Collaboration, Report No. CMS-TOP-12-007, 2013
    arXiv:1312.7582
    [28] ATLAS Collaboration, Report No. ATLAS-CONF-2013-097, 2013
    [29] U. Langenfeld, S. Moch, and P. Uwer, Phys. Rev. D 80,054009 (2009).
    [30] N. Kidonakis, Phys. Rev. D 82, 114030 (2010).
    [31] R. Martinez, M. A. Perez, and N. Poveda, Eur. Phys. J. C 53, 221
    (2008).
    [32] P. Artoisenet, R. Frederix, O. Mattelaer, R. Rietkerk arXiv:1212.3460
    [33] G. Mahlon, S.J.Parke, Phys. Lett. B 411, 173 (1997).
    arXiv:hep-ph/9706304
    [34] G. Mahlon, S.J.Parke arXiv:1001.3422v2
    [35] S.J.Parke arXiv:1005.0347v1
    [36] W. Bernreuther, A. Brandenburg, Z.G. Si and P. Uwer, Phys. Rev. Lett.
    87 (2001) 242002 arXiv:hep-ph/0107086
    [37] T. Stelzer and S. Willenbrock, Phys.Lett.B 374, 169(1996)
    arXiv:hep-ph/9512292
    [38] ATLAS Collaboration, Report No. CERN-PH-EP-2012-074
    Phys. Rev. Lett. 108 (2012) 212001 arXiv:1203.4081v3 [hep-ex]
    [39] CMS Collaboration, Report No. CMS-TOP-13-003
    Phys. Rev. Lett. 112 (2004) 182001 arXiv:1311.3924

    無法下載圖示 全文公開日期 本全文未授權公開 (校內網路)
    全文公開日期 本全文未授權公開 (校外網路)

    QR CODE