Abstract

We develop a method to forecast the outcome of the LHC Run 3 based on the hypothetical detection of $\mathcal{O}(100)$ signal events at XENONnT. Our method relies on a systematic classification of renormalisable single-mediator models for dark matter-quark interactions, and is valid for dark matter candidates of spin less than or equal to one. Applying our method to simulated data, we find that at the end of the LHC Run 3 only two mutually exclusive scenarios would be compatible with the detection of $\mathcal{O}(100)$ signal events at XENONnT. In a first scenario, the energy distribution of the signal events is featureless, as for canonical spin-independent interactions. In this case, if a mono-jet signal is detected at the LHC, dark matter must have spin 1/2 and interact with nucleons through a unique velocity-dependent operator. If a mono-jet signal is not detected, dark matter interacts with nucleons through canonical spin-independent interactions. In a second scenario, the spectral distribution of the signal events exhibits a bump at non zero recoil energies. In this second case, a mono-jet signal can be detected at the LHC Run 3, dark matter must have spin 1/2 and interact with nucleons through a unique momentum-dependent operator. We therefore conclude that the observation of $\mathcal{O}(100)$ signal events at XENONnT combined with the detection, or the lack of detection, of a mono-jet signal at the LHC Run 3 would significantly narrow the range of possible dark matter-nucleon interactions. As we argued above, it can also provide key information on the dark matter particle spin.

Highlights

  • Compelling evidence shows that significant amounts of dark matter (DM) are present in the Universe [1]

  • (2) In the second stage, we identify the correct DM-nucleon interaction(s) and possibly the DM particle spin based upon the observation, or the lack of observation, of a monojet signal at the end of the Large Hadron Collider (LHC) Run 3

  • We conclude that the observation of Oð100Þ signal events at XENONnT combined with the detection or the lack of detection of a monojet signal at the LHC Run 3 would significantly narrow the range of possible DMnucleon interactions

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Summary

Introduction

Compelling evidence shows that significant amounts of dark matter (DM) are present in the Universe [1]. This conclusion is supported by increasingly accurate cosmological and astrophysical observations performed on extremely different physical scales, ranging from the solar neighborhood [2] up to the largest scales we can probe in the cosmos [3]. The search for DM has successfully been pushed forward on several frontiers, and further

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