Gluino Coannihilation and Observability of Gluinos at LHC RUN II

TL;DR

This paper investigates the detectability of gluinos in the gluino-neutralino coannihilation region at LHC RUN II, considering dark matter constraints, and predicts the required luminosity for discovery at various gluino masses.

Contribution

It provides an analysis of gluino observability in the coannihilation region under current dark matter constraints, optimizing signal regions for potential discovery at LHC RUN II.

Findings

Gluinos with masses around 700 GeV could be discovered with 14 fb$^{-1}$ of data.

Gluinos with masses around 1250 GeV require about 3400 fb$^{-1}$ for discovery.

The neutralino mass is within 100 GeV of the gluino mass, aiding mass determination.

Abstract

The observability of a gluino at LHC RUN II is analyzed for the case where the gluino lies in the gluino-neutralino coannihilation region and the mass gap between the gluino and the neutralino is small. The analysis is carried out under the Higgs boson mass constraint and the constraint of dark matter relic density consistent with the WMAP and Planck experiment. It is shown that in this case a gluino with mass much smaller than the current lower limit of $\sim 1500$ GeV as given by LHC RUN II at 3.2 fb$^{-1}$ of integrated luminosity would have escaped detection. The analysis is done using the signal regions used by the ATLAS Collaboration where an optimization of signal regions was carried out to determine the best regions for gluino discovery in the gluino-neutralino coannihilation region. It is shown that under the Higgs boson mass constraint and the relic density constraint, a gluino mass of $\sim 700$ GeV would require 14 fb$^{-1}$ of integrated luminosity for discovery and a gluino of mass $\sim 1250$ GeV would require 3400 fb$^{-1}$ of integrated luminosity for discovery at LHC RUN II. An analysis of dark matter for this case is also given. It is found that for the range of gluino masses considered, the neutralino mass lies within less than 100 GeV of the gluino mass. Thus a measurement of the gluino mass in the gluino-neutralino coannihilation region will provide a determination of the neutralino mass. In this region the neutralino is dominantly a gaugino and the spin-independent proton-neutralino cross section is small but much larger than the neutrino floor lying in the range $\sim (1-10)\times 10^{-47}$ cm$^{2}$. Thus a significant part of the parameter space of the model will lie within the reach of the next generation LUX-ZEPLIN dark matter experiment.