Abstract

We investigate the production of fermionic dark matter $\chi$ via $pp \to p\gamma p \to p j \chi \bar{\chi}X$ mediated by a leptophobic spin-1 particle, where one of the protons remains intact and is tagged by forward proton detectors. We find that the masses of $\chi$ and the mediator $Z'$ are severely constrained when $Z'$ interacts with $\chi$ and quarks through the vector couplings. We show that dark matter searches in this production channel are sensitive to a mediator mass $m_{Z'} \lesssim 1.4~\mathrm{TeV}$ at 14 TeV at the LHC with an integrated luminosity $L_{\rm{int}} = 3000~\rm{fb}^{-1}$. The lower mass bound on the dark matter is $m_\chi \simeq 550~\mathrm{GeV}$ at the mediator mass $m_{Z'}=1.2~\mathrm{TeV}$.

Highlights

  • The existence of dark matter (DM) motivates us to explore physics beyond the Standard Model (SM)

  • We investigate the production of fermionic dark matter χ via pp → pγp → pjχχX mediated by a leptophobic spin-1 particle, where one of the protons remains intact and is tagged by forward proton detectors

  • There are lots of new physics models that explain the origin of DM, simplified models of dark matter have been adopted as benchmark scenarios to study the DM search strategies at the LHC [1]

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Summary

INTRODUCTION

The existence of dark matter (DM) motivates us to explore physics beyond the Standard Model (SM). These forward proton detectors enable us to study processes with photons in the initial state that are induced from initial protons Such non-QCD processes might give us new strategies to look for DM at the LHC, the feasibility of searching for DM candidates of simplified DM models. We study the feasibility of looking for signatures or constraints on the simplified DM model with fermionic DM and a spin-1 mediator using the forward proton detectors. The production process of the DM (3) could be studied quantitatively using the following model parameters: the dark matter mass mχ, the mediator mass mZ0, and the couplings of fermions gVψ and gAψ. Where the values of the couplings in Eqs. (6) and (7) are adopted from benchmark scenarios by the LHC Dark Matter Working Group [5]

NUMERICAL ANALYSIS
CONSTRAINTS USING PROTON TAGGING AT THE FORWARD PROTON DETECTORS
Findings
SUMMARY
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