Constraints on composite quark partners from higgs searches

Journal of High Energy Physics

Volumn 2014, Issue 5, 2014, Pages

  Flacke, Thomas ^a   Han Kim, Jeong ^a,b   Lee, Seung J ^a,c   Hak Lim, Sung ^a,b  

^a Korea Advanced Institute of Science and Technology (KAIST)   (South Korea)

^b Institute for Basic Science   (South Korea)

^c Korea Institute for Advanced Study   (South Korea)

Author keywords

Beyond Standard Model; Higgs Physics; Technicolor and Composite Models

Indexed keywords

EID: 84924091568     PISSN: 11266708     EISSN: 10298479     Source Type: Journal    
DOI: 10.1007/JHEP05(2014)123     Document Type: Article

References (78)

1. [1] ATLAS collaboration, Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC, Phys. Lett. B 716 (2012) 1 [arXiv:1207.7214][INSPIRE].
2. [2] CMS collaboration, Observation of a new boson at a mass of 125GeV with the CMS experiment at the LHC, Phys. Lett. B 716 (2012) 30 [arXiv:1207.7235][INSPIRE].
3. [3] G. ’t Hooft, Naturalness, chiral symmetry, and spontaneous chiral symmetry breaking, in Proc. of 1979 Cargese institute on Recent developments in gauge theories, Plenum Press, New York U.S.A. (1980), pg. 135[INSPIRE].
4. [4] K.G. Wilson, The renormalization group and strong interactions, Phys. Rev. D 3 (1971) 1818[INSPIRE].
5. [5] E. Gildener, Gauge symmetry hierarchies, Phys. Rev. D 14 (1976) 1667[INSPIRE].
6. [6] S. Weinberg, Gauge hierarchies, Phys. Lett. B 82 (1979) 387[INSPIRE].
7. [7] D.B. Kaplan and H. Georgi, SU(2) × U(1) breaking by vacuum misalignment, Phys. Lett. B 136 (1984) 183[INSPIRE].
8. [8] D.B. Kaplan, H. Georgi and S. Dimopoulos, Composite Higgs scalars, Phys. Lett. B 136 (1984) 187[INSPIRE].
9. [9] H. Georgi, D.B. Kaplan and P. Galison, Calculation of the composite Higgs mass, Phys. Lett. B 143 (1984) 152[INSPIRE].
10. [10] T. Banks, Constraints on SU(2) × U(1) breaking by vacuum misalignment, Nucl. Phys. B 243 (1984) 125[INSPIRE].
11. [11] H. Georgi and D.B. Kaplan, Composite Higgs and custodial SU(2), Phys. Lett. B 145 (1984) 216[INSPIRE].
12. [12] M.J. Dugan, H. Georgi and D.B. Kaplan, Anatomy of a composite Higgs model, Nucl. Phys. B 254 (1985) 299[INSPIRE].
13. [13] N. Arkani-Hamed, A.G. Cohen, E. Katz and A.E. Nelson, The littlest Higgs, JHEP 07 (2002) 034 [hep-ph/0206021][INSPIRE].
14. [14] R. Contino, Y. Nomura and A. Pomarol, Higgs as a holographic pseudo-Goldstone boson, Nucl. Phys. B 671 (2003) 148 [hep-ph/0306259][INSPIRE].
15. [15] K. Agashe, R. Contino and A. Pomarol, The minimal composite Higgs model, Nucl. Phys. B 719 (2005) 165 [hep-ph/0412089][INSPIRE].
16. [16] O. Matsedonskyi, G. Panico and A. Wulzer, Light top partners for a light composite Higgs, JHEP 01 (2013) 164 [arXiv:1204.6333][INSPIRE].
17. [17] M. Redi and A. Tesi, Implications of a light Higgs in composite models, JHEP 10 (2012) 166 [arXiv:1205.0232][INSPIRE].
18. [18] D. Marzocca, M. Serone and J. Shu, General composite Higgs models, JHEP 08 (2012) 013 [arXiv:1205.0770][INSPIRE].
19. [19] A. Pomarol and F. Riva, The composite Higgs and light resonance connection, JHEP 08 (2012) 135 [arXiv:1205.6434][INSPIRE].
20. [20] G. Panico, M. Redi, A. Tesi and A. Wulzer, On the tuning and the mass of the composite Higgs, JHEP 03 (2013) 051 [arXiv:1210.7114][INSPIRE].
21. [21] C. Grojean, O. Matsedonskyi and G. Panico, Light top partners and precision physics, JHEP 10 (2013) 160 [arXiv:1306.4655][INSPIRE].
22. [22] M. Gillioz, R. Gröber, A. Kapuvari and M. Mühlleitner, Vector-like bottom quarks in composite Higgs models, JHEP 03 (2014) 037 [arXiv:1311.4453][INSPIRE].
23. [23] A. De Simone, O. Matsedonskyi, R. Rattazzi and A. Wulzer, A first top partner hunter’s guide, JHEP 04 (2013) 004 [arXiv:1211.5663][INSPIRE].
24. [24] M. Buchkremer, G. Cacciapaglia, A. Deandrea and L. Panizzi, Model independent framework for searches of top partners, Nucl. Phys. B 876 (2013) 376 [arXiv:1305.4172][INSPIRE].
25. [25] CMS collaboration, Inclusive search for a vector-like T quark by CMS, CMS-PAS-B2G-12-015, CERN, Geneva Switzerland (2012).
26. [26] N. Vignaroli, Early discovery of top partners and test of the Higgs nature, Phys. Rev. D 86 (2012) 075017 [arXiv:1207.0830][INSPIRE].
27. [27] A. Azatov, M. Salvarezza, M. Son and M. Spannowsky, Boosting top partner searches in composite Higgs models, Phys. Rev. D 89 (2014) 075001 [arXiv:1308.6601][INSPIRE].
28. [28] N. Vignaroli, Discovering the composite Higgs through the decay of a heavy fermion, JHEP 07 (2012) 158 [arXiv:1204.0468][INSPIRE].
29. [29] C. Delaunay et al., Light non-degenerate composite partners at the LHC, JHEP 02 (2014) 055 [arXiv:1311.2072][INSPIRE].
30. [30] M. Redi and A. Weiler, Flavor and CP invariant composite Higgs models, JHEP 11 (2011) 108 [arXiv:1106.6357][INSPIRE].
31. [31] O. Gedalia, J.F. Kamenik, Z. Ligeti and G. Perez, On the universality of CP-violation in_F = 1 processes, Phys. Lett. B 714 (2012) 55 [arXiv:1202.5038][INSPIRE].
32. [32] G. Cacciapaglia et al., A GIM mechanism from extra dimensions, JHEP 04 (2008) 006 [arXiv:0709.1714][INSPIRE].
33. [33] A.L. Fitzpatrick, G. Perez and L. Randall, Flavor anarchy in a Randall-Sundrum model with 5D minimal flavor violation and a low Kaluza-Klein scale, Phys. Rev. Lett. 100 (2008) 171604 [arXiv:0710.1869][INSPIRE].
34. [34] C. Csaki, G. Perez, Z. Surujon and A. Weiler, Flavor alignment via shining in RS, Phys. Rev. D 81 (2010) 075025 [arXiv:0907.0474][INSPIRE].
35. [35] C. Delaunay, O. Gedalia, S.J. Lee, G. Perez and E. Ponton, Ultra visible warped model from flavor triviality and improved naturalness, Phys. Rev. D 83 (2011) 115003 [arXiv:1007.0243][INSPIRE].
36. [36] K. Agashe, R. Contino, L. Da Rold and A. Pomarol, A custodial symmetry for Zbb, Phys. Lett. B 641 (2006) 62 [hep-ph/0605341][INSPIRE].
37. [37] R. Contino, L. Da Rold and A. Pomarol, Light custodians in natural composite Higgs models, Phys. Rev. D 75 (2007) 055014 [hep-ph/0612048][INSPIRE].
38. [38] A. Pomarol and J. Serra, Top quark compositeness: feasibility and implications, Phys. Rev. D 78 (2008) 074026 [arXiv:0806.3247][INSPIRE].
39. [39] D. Pappadopulo, A. Thamm and R. Torre, A minimally tuned composite Higgs model from an extra dimension, JHEP 07 (2013) 058 [arXiv:1303.3062][INSPIRE].
40. [40] M. Montull, F. Riva, E. Salvioni and R. Torre, Higgs couplings in composite models, Phys. Rev. D 88 (2013) 095006 [arXiv:1308.0559][INSPIRE].
41. [41] A. Azatov and J. Galloway, Light custodians and Higgs physics in composite models, Phys. Rev. D 85 (2012) 055013 [arXiv:1110.5646][INSPIRE].
42. [42] S.R. Coleman, J. Wess and B. Zumino, Structure of phenomenological Lagrangians. 1, Phys. Rev. 177 (1969) 2239[INSPIRE].
43. [43] C.G. Callan Jr., S.R. Coleman, J. Wess and B. Zumino, Structure of phenomenological Lagrangians. 2, Phys. Rev. 177 (1969) 2247[INSPIRE].
44. [44] M. Redi, V. Sanz, M. de Vries and A. Weiler, Strong signatures of right-handed compositeness, JHEP 08 (2013) 008 [arXiv:1305.3818][INSPIRE].
45. [45] A. Atre, M. Chala and J. Santiago, Searches for new vector like quarks: Higgs channels, JHEP 05 (2013) 099 [arXiv:1302.0270][INSPIRE].
46. [46] C. Delaunay, T. Golling, G. Perez and Y. Soreq, Charming the Higgs, arXiv:1310.7029[INSPIRE].
47. [47] J.M. Butterworth, A.R. Davison, M. Rubin and G.P. Salam, Jet substructure as a new Higgs search channel at the LHC, Phys. Rev. Lett. 100 (2008) 242001 [arXiv:0802.2470][INSPIRE].
48. [48] L.G. Almeida et al., Substructure of high-pT jets at the LHC, Phys. Rev. D 79 (2009) 074017 [arXiv:0807.0234][INSPIRE].
49. [49] L.G. Almeida, S.J. Lee, G. Perez, G. Sterman and I. Sung, Template overlap method for massive jets, Phys. Rev. D 82 (2010) 054034 [arXiv:1006.2035][INSPIRE].
50. [50] T. Plehn, G.P. Salam and M. Spannowsky, Fat jets for a light Higgs, Phys. Rev. Lett. 104 (2010) 111801 [arXiv:0910.5472][INSPIRE].
51. [51] D.E. Soper and M. Spannowsky, Combining subjet algorithms to enhance ZH detection at the LHC, JHEP 08 (2010) 029 [arXiv:1005.0417][INSPIRE].
52. [52] J.-H. Kim, Rest frame subjet algorithm with SISCone jet for fully hadronic decaying Higgs search, Phys. Rev. D 83 (2011) 011502 [arXiv:1011.1493][INSPIRE].
53. [53] L.G. Almeida et al., Three-particle templates for a boosted Higgs boson, Phys. Rev. D 85 (2012) 114046 [arXiv:1112.1957][INSPIRE].
54. [54] M. Backovic, J. Juknevich and G. Perez, Boosting the Standard Model Higgs signal with the template overlap method, JHEP 07 (2013) 114 [arXiv:1212.2977][INSPIRE].
55. [55] ATLAS collaboration, Search for pair production of heavy top-like quarks decaying to a high-pT W boson and a b quark in the lepton plus jets final state at √s = 7TeV with the ATLAS detector, Phys. Lett. B 718 (2013) 1284 [arXiv:1210.5468][INSPIRE].
56. [56] CMS collaboration, Search for pair-production of second generation leptoquarks in 8TeV proton-proton collisions, CMS-PAS-EXO-12-042, CERN, Geneva Switzerland (2012).
57. [57] CMS collaboration, Searches for light-and heavy-flavour three-jet resonances in pp collisions at √s = 8TeV, Phys. Lett. B 730 (2014) 193 [arXiv:1311.1799][INSPIRE].
58. [58] ATLAS collaboration, Search for pair production of new heavy quarks that decay to a Z boson and a third generation quark in pp collisions at √s = 8TeV with the ATLAS detector, ATLAS-CONF-2013-056, CERN, Geneva Switzerland (2013).
59. [59] CMS collaboration, Search for pair-produced vector-like quarks of charge −1/3 in lepton+jets final state in pp collisions at √s = 8TeV, CMS-PAS-B2G-12-019, CERN, Geneva Switzerland (2012).
60. [60] CMS collaboration, Search for pair-produced vector-like quarks of charge −1/3 in dilepton+jets final state in pp collisions at √s = 8TeV, CMS-PAS-B2G-12-021, CERN, Geneva Switzerland (2012).
61. [61] J.R. Espinosa, C. Grojean, M. Muhlleitner and M. Trott, Fingerprinting Higgs suspects at the LHC, JHEP 05 (2012) 097 [arXiv:1202.3697][INSPIRE].
62. [62] D. Carmi, A. Falkowski, E. Kuflik, T. Volansky and J. Zupan, Higgs after the discovery: a status report, JHEP 10 (2012) 196 [arXiv:1207.1718][INSPIRE].
63. [63] G. Moreau, Constraining extra-fermion(s) from the Higgs boson data, Phys. Rev. D 87 (2013) 015027 [arXiv:1210.3977][INSPIRE].
64. [64] C. Delaunay, C. Grojean and G. Perez, Modified Higgs physics from composite light flavors, JHEP 09 (2013) 090 [arXiv:1303.5701][INSPIRE].
65. [65] ATLAS collaboration, Differential cross sections of the Higgs boson measured in the diphoton decay channel using 8TeV pp collisions, ATLAS-CONF-2013-072, CERN, Geneva Switzerland (2013).
66. [66] A. Alloul, N.D. Christensen, C. Degrande, C. Duhr and B. Fuks, FeynRules 2.0 — a complete toolbox for tree-level phenomenology, arXiv:1310.1921[INSPIRE].
67. [67] C. Degrande et al., UFO — the Universal FeynRules Output, Comput. Phys. Commun. 183 (2012) 1201 [arXiv:1108.2040][INSPIRE].
68. [68] N. Christensen, B. Fuks and C. Duhr, The Standard Model Feynrules wiki webpage, http://feynrules.irmp.ucl.ac.be/wiki/StandardModel.
69. [69] C. Duhr, The Higgs effective theory Feynrules wiki webpage, http://feynrules.irmp.ucl.ac.be/wiki/HiggsEffectiveTheory.
70. [70] LHC Higgs Cross section Working Group collaboration, S. Heinemeyer et al., Handbook of LHC Higgs cross sections: 3. Higgs properties, arXiv:1307.1347[INSPIRE].
71. [71] J. Alwall, M. Herquet, F. Maltoni, O. Mattelaer and T. Stelzer, MadGraph 5: going beyond, JHEP 06 (2011) 128 [arXiv:1106.0522][INSPIRE].
72. [72] J. Pumplin et al., New generation of parton distributions with uncertainties from global QCD analysis, JHEP 07 (2002) 012 [hep-ph/0201195][INSPIRE].
73. [73] T. Sjöstrand, S. Mrenna and P.Z. Skands, PYTHIA 6.4 physics and manual, JHEP 05 (2006) 026 [hep-ph/0603175][INSPIRE].
74. [74] DELPHES 3 collaboration, J. de Favereau et al., DELPHES 3, a modular framework for fast simulation of a generic collider experiment, JHEP 02 (2014) 057 [arXiv:1307.6346][INSPIRE].
75. [75] M. Cacciari and G.P. Salam, Dispelling the N3 myth for the kt jet-finder, Phys. Lett. B 641 (2006) 57 [hep-ph/0512210][INSPIRE].
76. [76] M. Cacciari, G.P. Salam and G. Soyez, FastJet user manual, Eur. Phys. J. C 72 (2012) 1896 [arXiv:1111.6097][INSPIRE].
77. [77] M. Cacciari, G.P. Salam and G. Soyez, The anti-kt jet clustering algorithm, JHEP 04 (2008) 063 [arXiv:0802.1189][INSPIRE].
78. [78] CMS collaboration, 2HDM scenario, H → hh and A → Zh, CMS-PAS-HIG-13-025, CERN, Geneva Switzerland (2013).