# Loop Induced Single Top Partner Production and Decay at the LHC

## TL;DR

This paper explores a novel loop-induced single top partner production mechanism at the LHC, which can dominate over pair production at high masses, and discusses new decay modes and search strategies for these particles.

## Contribution

It introduces a new loop-mediated production channel for top partners and analyzes its significance and detection prospects at the LHC.

## Key findings

- Loop-induced production can dominate at masses above 1.5 TeV.
- Exotic decay modes like T→tg are significant and lead to long-lived top partners.
- High luminosity LHC can probe top partner masses up to 2 TeV.

## Abstract

Most searches for top partners, $T$, are concerned with top partner pair production. However, as these bounds become increasingly stringent, the LHC energy will saturate and single top partner production will become more important. In this paper we study the novel signature of the top partner produced in association with the SM top, $pp\rightarrow T\overline{t}+t\overline{T}$, in a model where the Standard Model (SM) is extended by a vector-like $SU(2)_L$ singlet fermion top partner and a real, SM gauge singlet scalar, $S$. In this model, $pp\rightarrow T\overline{t}+t\overline{T}$ production is possible through loops mediated by the scalar singlet. We find that, with reasonable coupling strengths, the production rate of this channel can dominate top partner pair production at top partner masses of $m_T\gtrsim 1.5$ TeV. In addition, this model allows for the exotic decay modes $T\rightarrow tg$, $T\rightarrow t \gamma$, and $T\rightarrow t S$. In much of the parameter space the loop induced decay $T\rightarrow tg$ dominates and the top partner is quite long lived. New search strategies are necessary to cover these decay modes. We project the the sensitivity of the high luminosity LHC to $pp\rightarrow T\overline{t}+t\overline{T}$ via a realistic collider study. We find with 3 ab$^{-1}$, the LHC is sensitive to this process for masses $m_T\lesssim2$ TeV. In addition, we provide appendices detailing the renormalization of this model.