Abstract

A search for new particles has been conducted using events with two high transverse momentum τ leptons that decay hadronically and at least two energetic jets. The analysis is performed using data from proton-proton collisions at sqrt{s}=13 TeV, collected by the CMS experiment at the LHC in 2016 and corresponding to an integrated luminosity of 35.9 fb−1. The observed data are consistent with standard model expectations. The results are interpreted in the context of two physics models. The first model involves right-handed charged bosons, WR, that decay to heavy right-handed Majorana neutrinos, Nℓ (ℓ = e, μ, τ), arising in a left-right symmetric extension of the standard model. The model considers that Ne and Nμ are too heavy to be detected at the LHC. Assuming that the Nτ mass is half of the WR mass, masses of the WR boson below 3.50 TeV are excluded at 95% confidence level. Exclusion limits are also presented considering different scenarios for the mass ratio between Nτ and WR, as a function of WR mass. In the second model, pair production of third-generation scalar leptoquarks that decay into ττbb is considered, resulting in an observed exclusion region with leptoquark masses below 1.02 TeV, assuming a 100% branching fraction for the leptoquark decay to a τ lepton and a bottom quark. These results represent the most stringent limits to date on these models.

Highlights

  • Background estimationThe tt, quantum chromodynamics (QCD) multijet, and Z+jets processes are expected to account for 84% of the total background

  • The heavy neutrino model with m(WR) = 3.0 TeV and m(Nτ ) = 1.5 TeV is used as a benchmark in figure 5, while the leptoquark model with m(LQ) = 1.0 TeV is used as a benchmark in figure 5

  • A search is performed for physics beyond the standard model in events with two energetic τ of leptons and two energetic 35.9 fb−1 collected in 2016 jets, with using data corresponding to an integrated luminosity √

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Summary

The CMS detector

A detailed description of the CMS detector, together with a definition of the coordinate system used and the relevant kinematic variables, can be found in [56]. The central feature of the CMS apparatus is a superconducting solenoid of 6 m inner diameter, providing a field of 3.8 T. Within the field volume are the silicon pixel and strip tracker, the crystal electromagnetic calorimeter (ECAL), which includes a silicon sensor preshower detector in front of the ECAL endcaps, and the brass and scintillator hadron calorimeter. The inner tracker measures charged particles within pseudorapidity range |η| < 2.5 and provides an impact parameter resolution of ∼15 μm and a transverse momentum resolution of about 1.5% for 100 GeV particles. Collision events of interest are selected using a two-tiered trigger system. The first level, composed of custom hardware processors, selects events at a rate of around 100 kHz. The second level, based on an array of microprocessors running a version of the full event reconstruction software optimized for fast processing, reduces the event rate to around 1 kHz before data storage

Event reconstruction and particle identification
Signal and background samples
Event selection
Background estimation
Systematic uncertainties
Results
Summary
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