Probing bottom-associated production of a TeV scale scalar decaying to a top quark and dark matter at the LHC

A bstract A minimal non-thermal dark matter model that can explain both the existence of dark matter and the baryon asymmetry in the universe is studied. It requires two color-triplet, iso-singlet scalars with $$ \mathcal{O}\left(\textrm{TeV}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:mi>TeV</mml:mi> </mml:mfenced> </mml:math> masses and a singlet Majorana fermion with a mass of $$ \mathcal{O}\left(\textrm{GeV}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:mi>GeV</mml:mi> </mml:mfenced> </mml:math> . The fermion becomes stable and can play the role of the dark matter candidate. We consider the fermion to interact with a top quark via the exchange of QCD-charged scalar fields coupled dominantly to third generation fermions. The signature of a single top quark production associated with a bottom quark and large missing transverse momentum opens up the possibility to search for this type of model at the LHC in a way complementary to existing monotop searches.

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Publication Details

Journal
Journal of High Energy Physics
Published
2024-09-27
DOI
https://doi.org/10.1007/jhep09(2024)203
Citations
2
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
1.32

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article

Probing bottom-associated production of a TeV scale scalar decaying to a top quark and dark matter at the LHC

T. Kamon, A. Thompson, J. S. H. Lee, D. Rathjens et al.
2 citations
Journal of High Energy Physics
Particle physics theoretical and experimental studies
1.32
article

Probing bottom-associated production of a TeV scale scalar decaying to a top quark and dark matter at the LHC

T. Kamon, A. Thompson, J. S. H. Lee, D. Rathjens, Seulgi Kim, Youn Jung Roh, I. J. Watson, A. K. Kalsi
article en
2 citations

Abstract

A bstract A minimal non-thermal dark matter model that can explain both the existence of dark matter and the baryon asymmetry in the universe is studied. It requires two color-triplet, iso-singlet scalars with $$ \mathcal{O}\left(\textrm{TeV}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:mi>TeV</mml:mi> </mml:mfenced> </mml:math> masses and a singlet Majorana fermion with a mass of $$ \mathcal{O}\left(\textrm{GeV}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:mi>GeV</mml:mi> </mml:mfenced> </mml:math> . The fermion becomes stable and can play the role of the dark matter candidate. We consider the fermion to interact with a top quark via the exchange of QCD-charged scalar fields coupled dominantly to third generation fermions. The signature of a single top quark production associated with a bottom quark and large missing transverse momentum opens up the possibility to search for this type of model at the LHC in a way complementary to existing monotop searches.

Journal of High Energy PhysicsVol. 2024(9)
University of Seoul (KR), Mitchell Institute (US), Punjab Agricultural University (IN), Texas A&M University (US)
U.S. Department of Energy, National Research Foundation, National Research Foundation of Korea
Openalex Percentile: Top 11%
Particle physics theoretical and experimental studies
1.32
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