Abstract

Events containing one or more top quarks produced with additional prompt leptons are used to search for new physics within the framework of an effective field theory (EFT). The data correspond to an integrated luminosity of 41.5 fb−1 of proton-proton collisions at a center-of-mass energy of 13 TeV at the LHC, collected by the CMS experiment in 2017. The selected events are required to have either two leptons with the same charge or more than two leptons; jets, including identified bottom quark jets, are also required, and the selected events are divided into categories based on the multiplicities of these objects. Sixteen dimension-six operators that can affect processes involving top quarks produced with additional charged leptons are considered in this analysis. Constructed to target EFT effects directly, the analysis applies a novel approach in which the observed yields are parameterized in terms of the Wilson coefficients (WCs) of the EFT operators. A simultaneous fit of the 16 WCs to the data is performed and two standard deviation confidence intervals for the WCs are extracted; the standard model expectations for the WC values are within these intervals for all of the WCs probed.

Highlights

  • The CMS detectorThe central feature of the CMS apparatus is a superconducting solenoid of 6 m internal diameter, providing a magnetic field of 3.8 T

  • Background estimationContributions to the selected event yields arise from a variety of background processes, which can be categorized as reducible or irreducible and are either estimated from data control regions or modeled using simulation

  • The number of events selected in different categories is compared to the expected contributions of the signal processes and of the different background processes before and after simultaneously fitting all 16 Wilson coefficients (WCs), and the nuisance parameters (NPs), to minimize the negative loglikelihood in figure 3

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Summary

The CMS detector

The central feature of the CMS apparatus is a superconducting solenoid of 6 m internal diameter, providing a magnetic field of 3.8 T. Forward calorimeters extend the pseudorapidity coverage provided by the barrel and endcap detectors. Events of interest are selected using a two-tiered trigger system [29]. The first level, composed of custom hardware processors, uses information from the calorimeters and muon detectors to select events at a rate of around 100 kHz within a fixed time interval of about 4 μs. The second level, known as the high-level trigger, consists of a farm of processors running a version of the full event reconstruction software optimized for fast processing, and reduces the event rate to around 1 kHz before data storage

Data samples and simulation
Simulation of the signal processes
Parameterization of the yields in terms of the WCs
Event reconstruction
Event selection
Separation into subcategories
Background estimation
Background from misidentified leptons
Background from lepton charge mismeasurement
Signal extraction
Systematic uncertainties
Results
10 Summary
Full Text
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