Shedding light on top partner at the LHC

Abstract We investigate the sensitivity of the 14 TeV LHC to pair-produced top partners (T) decaying into the Standard Model top quark (t) plus either a gluon (g) or a photon (γ). The decays T → tg and T → tγ can be dominant when the mixing between the top partner and top quark are negligible. In th...

Full description

Bibliographic Details
Main Authors: Haider Alhazmi, Jeong Han Kim, Kyoungchul Kong, Ian M. Lewis
Format: Article
Language:English
Published: SpringerOpen 2019-01-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP01(2019)139
_version_ 1818887431284326400
author Haider Alhazmi
Jeong Han Kim
Kyoungchul Kong
Ian M. Lewis
author_facet Haider Alhazmi
Jeong Han Kim
Kyoungchul Kong
Ian M. Lewis
author_sort Haider Alhazmi
collection DOAJ
description Abstract We investigate the sensitivity of the 14 TeV LHC to pair-produced top partners (T) decaying into the Standard Model top quark (t) plus either a gluon (g) or a photon (γ). The decays T → tg and T → tγ can be dominant when the mixing between the top partner and top quark are negligible. In this case, the conventional decays T → bW , T → tZ, and T → th are highly suppressed and can be neglected. We take a model-independent approach using effective operators for the T -t-g and T -t-γ interactions, considering both spin- 1 2 $$ \frac{1}{2} $$ and spin- 3 2 $$ \frac{3}{2} $$ top partners. We perform a semi-realistic simulation with boosted top quark tagging and an appropriate implementation of a jet-faking-photon rate. Despite a simple dimensional analysis indicating that the branching ratios BR(T → tγ) ≪ BR(T → tg) due to the electric-magnetic coupling being much smaller than the strong force coupling, our study shows that the LHC sensitivity to T T ¯ → t t ¯ γ g $$ T\overline{T}\to t\overline{t}\gamma g $$ is more significant than the sensitivity to T T ¯ → t t ¯ gg $$ T\overline{T}\to t\overline{t} gg $$ . This is due to much smaller backgrounds attributed to the isolated high-p T photon. We find that with these decay channels and 3 ab−1 of data, the LHC is sensitive to top partner masses m T ≲ 1.4-1.8 TeV for spin- 1 2 $$ \frac{1}{2} $$ and spin- 3 2 $$ \frac{3}{2} $$ top partners, respectively.
first_indexed 2024-12-19T16:37:07Z
format Article
id doaj.art-c7ded35c36b94cf9a7522e65c4b46060
institution Directory Open Access Journal
issn 1029-8479
language English
last_indexed 2024-12-19T16:37:07Z
publishDate 2019-01-01
publisher SpringerOpen
record_format Article
series Journal of High Energy Physics
spelling doaj.art-c7ded35c36b94cf9a7522e65c4b460602022-12-21T20:13:56ZengSpringerOpenJournal of High Energy Physics1029-84792019-01-012019113010.1007/JHEP01(2019)139Shedding light on top partner at the LHCHaider Alhazmi0Jeong Han Kim1Kyoungchul Kong2Ian M. Lewis3Department of Physics and Astronomy, University of KansasDepartment of Physics and Astronomy, University of KansasDepartment of Physics and Astronomy, University of KansasDepartment of Physics and Astronomy, University of KansasAbstract We investigate the sensitivity of the 14 TeV LHC to pair-produced top partners (T) decaying into the Standard Model top quark (t) plus either a gluon (g) or a photon (γ). The decays T → tg and T → tγ can be dominant when the mixing between the top partner and top quark are negligible. In this case, the conventional decays T → bW , T → tZ, and T → th are highly suppressed and can be neglected. We take a model-independent approach using effective operators for the T -t-g and T -t-γ interactions, considering both spin- 1 2 $$ \frac{1}{2} $$ and spin- 3 2 $$ \frac{3}{2} $$ top partners. We perform a semi-realistic simulation with boosted top quark tagging and an appropriate implementation of a jet-faking-photon rate. Despite a simple dimensional analysis indicating that the branching ratios BR(T → tγ) ≪ BR(T → tg) due to the electric-magnetic coupling being much smaller than the strong force coupling, our study shows that the LHC sensitivity to T T ¯ → t t ¯ γ g $$ T\overline{T}\to t\overline{t}\gamma g $$ is more significant than the sensitivity to T T ¯ → t t ¯ gg $$ T\overline{T}\to t\overline{t} gg $$ . This is due to much smaller backgrounds attributed to the isolated high-p T photon. We find that with these decay channels and 3 ab−1 of data, the LHC is sensitive to top partner masses m T ≲ 1.4-1.8 TeV for spin- 1 2 $$ \frac{1}{2} $$ and spin- 3 2 $$ \frac{3}{2} $$ top partners, respectively.http://link.springer.com/article/10.1007/JHEP01(2019)139Beyond Standard ModelHiggs Physics
spellingShingle Haider Alhazmi
Jeong Han Kim
Kyoungchul Kong
Ian M. Lewis
Shedding light on top partner at the LHC
Journal of High Energy Physics
Beyond Standard Model
Higgs Physics
title Shedding light on top partner at the LHC
title_full Shedding light on top partner at the LHC
title_fullStr Shedding light on top partner at the LHC
title_full_unstemmed Shedding light on top partner at the LHC
title_short Shedding light on top partner at the LHC
title_sort shedding light on top partner at the lhc
topic Beyond Standard Model
Higgs Physics
url http://link.springer.com/article/10.1007/JHEP01(2019)139
work_keys_str_mv AT haideralhazmi sheddinglightontoppartneratthelhc
AT jeonghankim sheddinglightontoppartneratthelhc
AT kyoungchulkong sheddinglightontoppartneratthelhc
AT ianmlewis sheddinglightontoppartneratthelhc