Abstract

A search is presented for new high-mass resonances decaying into electron or muon pairs. The search uses proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the CMS experiment at the LHC in 2016, corresponding to an integrated luminosity of 36 fb−1. Observations are in agreement with standard model expectations. Upper limits on the product of a new resonance production cross section and branching fraction to dileptons are calculated in a model-independent manner. This permits the interpretation of the limits in models predicting a narrow dielectron or dimuon resonance. A scan of different intrinsic width hypotheses is performed. Limits are set on the masses of various hypothetical particles. For the {Z}_{mathrm{SSM}}^{prime}left({Z}_{{}^{psi}}^{prime}right) particle, which arises in the sequential standard model (superstring-inspired model), a lower mass limit of 4.50 (3.90) TeV is set at 95% confidence level. The lightest Kaluza-Klein graviton arising in the Randall-Sundrum model of extra dimensions, with coupling parameters k/MPl of 0.01, 0.05, and 0.10, is excluded at 95% confidence level below 2.10, 3.65, and 4.25 TeV, respectively. In a simplified model of dark matter production via a vector or axial vector mediator, limits at 95% confidence level are obtained on the masses of the dark matter particle and its mediator.

Highlights

  • Model-dependent Z boson couplings to the up-type quarks, while wu depends on the up-type quark parton distribution functions (PDFs)

  • For the ZSSM (Zψ) particle, which arises in the sequential standard model, a lower mass limit of 4.50 (3.90) TeV is set at 95% confidence level

  • Considered models are the generalized sequential model (GSM) [6], containing the ZSSM boson that has SM-like couplings to SM fermions [7]; GUT models based on the E6 gauge group, containing the Zψ boson [1, 8]; and high-mass neutral bosons of the left (L)-right (R) symmetric extensions of the SM based on the SU(2)L ⊗ SU(2)R ⊗ U(1)B-L gauge group, where B-L refers to the difference between baryon and lepton numbers

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Summary

The CMS detector

The central feature of the CMS detector is a superconducting solenoid providing an axial magnetic field of 3.8 T and enclosing an inner tracker, an electromagnetic calorimeter (ECAL), and a hadron calorimeter (HCAL). Additional detectors and upgrades of electronics were installed before the beginning of the 13 TeV data collection period in 2015, yielding improved reconstruction performance. The level-1 (L1) trigger [30], composed of custom hardware processors, selects events of interest using information from the calorimeters and muon detectors and reduces the readout rate from the 40 MHz bunch crossing frequency to a maximum of 100 kHz. The software based high-level trigger (HLT) [30] uses the full event information, including that from the inner tracker, to reduce the event rate to around the 1 kHz that is retained for further processing

Simulated data samples
Lepton reconstruction and event selection
Backgrounds
Findings
Summary
Full Text
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