Abstract

Theories which provide a dynamical explanation for the large top-quark mass often include TeV-scale vector-like top-quark and bottom-quark partner states which can be potentially discovered at the LHC. These states are currently probed through model-independent searches for pair-production via gluon fusion, as well as through model-dependent complementary electroweak single production. In this paper we study the potential to extend those searches for the partners of the third-generation Standard Model quarks on the basis of their expected chromomagnetic interactions. We discuss how current searches for "excited" bottom-quarks produced via $b$-gluon fusion through chromomagnetic interactions are relevant, and provide significant constraints. We then explore the region of the parameter space in which the bottom-quark partner is heavier than the top-quark partner, in which case the top-partner can be primarily produced via the decay of the bottom-partner. Next, we probe the potential of the production of a single top-quark partner in association with an ordinary top-quark by gluon-fusion. Kinematically these two new processes are similar, and they yield the production of a heavy top partner and a lighter Standard Model state, a pattern which allows for the rejection of the associated dominant Standard Model backgrounds. We examine the sensitivity of these modes in the case where the top-partner subsequently decays to a Higgs boson and an ordinary top-quark, and we demonstrate that these new channels have the potential of extending and complementing the conventional strategies at LHC run III and at the high-luminosity phase of the LHC. In this last case, we find that partner masses that range up to about 3 TeV can be reached. This substantially expands the expected mass reach for these new states, including regions of parameter space that are inaccessible by traditional searches.

Highlights

  • Theories which provide a dynamical explanation for the large top quark mass often include TeV-scale vectorlike top quark (T) and bottom quark (B) partner states which can be discovered at the LHC [1,2,3,4,5]

  • For the high-luminosity phase of the LHC (HL-LHC), that top partner masses ranging up to about 3 TeV could be reached, which substantially improves the LHC expectations for the considered new states, including in regions of parameter space that are inaccessible by traditional searches

  • In this paper we have investigated the potential for the LHC to discover top quark partner states produced via their chromomagnetic moment interaction, either via single production of a bottom quark partner state which subsequently decays to a top quark partner and a top quark, or through the direct production of a top partner in association with a top quark

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Summary

INTRODUCTION

Theories which provide a dynamical explanation for the large top quark mass often include TeV-scale vectorlike top quark (T) and bottom quark (B) partner states which can be discovered at the LHC [1,2,3,4,5] (see [6,7] for recent works). It becomes possible to combine the fat top jet and the fat Higgs jet (assuming an h → bbdecay) to seek evidence for an invariant mass peak corresponding to the vectorlike T quark, without worrying about any combinatorial issues originating from the presence of two final-state top quarks This specific signature allows us, by its peculiar kinematic properties, to unravel the heavy quark signal from the associated key backgrounds. The production of a top-antitop pair, together with an extra hard radiation, leads to the same final state (two top quarks and a jet) and may have a large cross section, only radiation of an unusually hard gluon would enable one of the top quarks to be as near-threshold as in the signal case This background, has very different properties than the signal events. II B, we introduce the model parameter space and investigate the mass spectrum of the new states, as well as predictions for the associated decay patterns

Field content and fermion eigenstates
SEARCHES AT THE LHC
Vectorlike quark single and pair production
Single production of the B1 partner
Single production of the T1 partner
CONCLUSIONS
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