2010
DOI: 10.1007/jhep11(2010)159
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Bounds and decays of new heavy vector-like top partners

Abstract: Abstract:We study the phenomenology of new heavy vector-like fermions that couple to the third generation quarks via Yukawa interactions, covering all the allowed representations under the standard model gauge groups. We first review tree and loop level bounds on these states. We then discuss tree level decays and loop-induced decays to photon or gluon plus top. The main decays at tree level are to W b and/or Z and Higgs plus top via the new Yukawa couplings. The radiative loop decays turn out to be quite clos… Show more

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Cited by 89 publications
(120 citation statements)
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“…The minimal set of VL multiplets that can mix with SM quarks and a SM (or SM-like) Higgs boson have been extensively studied in literature [23,28,32,[34][35][36]40].…”
Section: Vector-like Multipletsmentioning
confidence: 99%
See 1 more Smart Citation
“…The minimal set of VL multiplets that can mix with SM quarks and a SM (or SM-like) Higgs boson have been extensively studied in literature [23,28,32,[34][35][36]40].…”
Section: Vector-like Multipletsmentioning
confidence: 99%
“…Both CMS [21] and ATLAS [22] have recently devoted a considerable effort in the analyses apt to setting bounds on this type of new particles. Initially, simplifying assumptions were considered (mixing only with the third generation of SM quark family or specific decay modes) [23][24][25][26][27][28][29][30][31][32][33]. However the most recent analyses, due to larger data samples, allow exploring more general situations with mixing of VL quarks with the first two generation of SM quarks [34][35][36][37][38].…”
Section: Introductionmentioning
confidence: 99%
“…Refs. [45][46][47][48] evaluates precision electroweak and flavor constraints on top-partner vector-like quarks, and studies direct LHC signatures.…”
Section: Jhep09(2014)130mentioning
confidence: 99%
“…By simply requiring the presence of a Yukawa-type coupling with the standard quarks, the allowed representations can contain both a top and bottom partner (t ′ and b ′ ), but also two exotic quarks with charges + 5 3 (X 5/3 ) and − 4 3 (Y −4/3 ) 1 . In [12] a complete list of the possible representations is presented, including the relevant bounds from precisely measured quantities in the Standard Model (SM). For earlier bounds see for example [13,14].…”
Section: Introductionmentioning
confidence: 99%