Abstract
The observation of single top quark production in association with a Z boson and a quark (tZq) is reported. Events from proton-proton collisions at a center-of-mass energy of 13TeV containing three charged leptons (either electrons or muons) and at least two jets are analyzed. The data were collected with the CMS detector in 2016 and 2017 and correspond to an integrated luminosity of 77.4fb^{-1}. The increased integrated luminosity, a multivariate lepton identification, and a redesigned analysis strategy improve significantly the sensitivity of the analysis compared to previous searches for tZq production. The tZq signal is observed with a significance well over 5 standard deviations. The measured tZq production cross section is σ(pp→tZq→tℓ^{+}ℓ^{-}q)=111±13(stat)_{-9}^{+11}(syst) fb, for dilepton invariant masses above 30GeV, in agreement with the standard model expectation.
Highlights
Compared to the non-boosted decision trees (BDTs)-based lepton identification used in the previous analysis [7], the selection efficiency for prompt electrons improves by up to 12% (8%), while rejecting more nonprompt leptons by a factor of approximately 2 (8) in simulated events
The ZZ background normalization is constrained via a control data sample of four-lepton events, in which there are two opposite sign and same flavor (OSSF) pairs with invariant masses close to that of the Z boson
The probability for a loose nonprompt lepton to pass the tight selection requirements is measured as a function of its pT and jηj in a control data sample of quantum chromodynamics (QCD) multijet events, rich in nonprompt leptons
Summary
A stringent requirement is placed on the BDT output, resulting in a selection efficiency of 85% (92%) per prompt electron (muon) with pT > 25 GeV passing the prerequisite selection criteria, as measured in simulated tZq events. Compared to the non-BDT-based lepton identification used in the previous analysis [7], the selection efficiency for prompt electrons (muons) improves by up to 12% (8%), while rejecting more nonprompt leptons by a factor of approximately 2 (8) in simulated events.
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