Abstract

A search is performed for events consistent with the pair production of a new heavy particle that acts as a mediator between a dark sector and normal matter, and that decays to a light quark and a new fermion called a dark quark. The search is based on data corresponding to an integrated luminosity of 16.1 fb−1 from proton-proton collisions at sqrt{s}=13 TeV collected by the CMS experiment at the LHC in 2016. The dark quark is charged only under a new quantum-chromodynamics-like force, and forms an “emerging jet” via a parton shower, containing long-lived dark hadrons that give rise to displaced vertices when decaying to standard model hadrons. The data are consistent with the expectation from standard model processes. Limits are set at 95% confidence level excluding dark pion decay lengths between 5 and 225 mm for dark mediators with masses between 400 and 1250 GeV. Decay lengths smaller than 5 and greater than 225 mm are also excluded in the lower part of this mass range. The dependence of the limit on the dark pion mass is weak for masses between 1 and 10 GeV. This analysis is the first dedicated search for the pair production of a new particle that decays to a jet and an emerging jet.

Highlights

  • Background estimationThe production of events containing four SM jets can mimic the signal when two of the jets pass the emerging jet criteria, or when one passes and jet mismeasurement results in artificial pmTiss

  • A search is performed for events consistent with the pair production of a new heavy particle that acts as a mediator between a dark sector and normal matter, and that decays to a light quark and a new fermion called a dark quark

  • The dark quark is charged only under a new quantum-chromodynamics-like force, and forms an “emerging jet” via a parton shower, containing long-lived dark hadrons that give rise to displaced vertices when decaying to standard model hadrons

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Summary

GeV 2 100 MeV 2 2 GeV fπDK mdown mπDK mXDK

Where κ is the appropriate element of the NCDK×3 matrix of Yukawa couplings between the mediator particle, the quarks, and the dark quarks; fπDK is the dark pion decay constant; and mdown, mπDK, and mXDK are the masses of the down quark, the dark pion, and the mediator particle, respectively. The signature for this search consists of four high transverse momentum (pT).

The CMS detector and event reconstruction
Simulated samples
Event selection
10 Simulation
Background estimation
Systematic uncertainties
Results
Summary
Full Text
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