Abstract

Abstract The first measurement of the electroweak production cross section of a Z boson with two jets (Zjj) in pp collisions at $ \sqrt{s}=7 $ TeV is presented, based on a data sample recorded by the CMS experiment at the LHC with an integrated luminosity of 5 fb−1. The cross section is measured for the ℓℓjj (ℓ = e, μ) final state in the kinematic region m ℓℓ > 50 GeV, m jj > 120 GeV, transverse momenta $ p_{\mathrm{T}}^{\mathrm{j}}>25 $ GeV and pseudorapidity |η j| < 4.0. The measurement, combining the muon and electron channels, yields σ = 154 ± 24 (stat.) ± 46 (exp. syst.) ± 27 (th. syst.) ± 3 (lum.) fb, in agreement with the theoretical cross section. The hadronic activity, in the rapidity interval between the jets, is also measured. These results establish an important foundation for the more general study of vector boson fusion processes, of relevance for Higgs boson searches and for measurements of electroweak gauge couplings and vector boson scattering.

Highlights

  • BackgroundGraph via a matrix element (ME) calculation that includes up to four jets at parton level

  • Z+jets and ditop processes are generated with Mad-Graph via a matrix element (ME) calculation that includes up to four jets at parton level.The ME and parton shower (ME-parton showering (PS)) matching is performed following the ktMLM prescription [26]

  • The plan of the paper is as follows: in section 2 we describe the Compact Muon Solenoid (CMS) detector, reconstruction, and event simulation; in section 3 we discuss the event selections; sections 4 and 5 are devoted to the study of the hadronic activity in Drell-Yan events; in section 6 we present the measurement of the cross section for the EW Zjj production; in section 7 we summarize our main results

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Summary

Background

Graph via a matrix element (ME) calculation that includes up to four jets at parton level. PiT with n final state particles (partons, not jets; n = 4, 5) is used with the QCD factorization and renormalization scales set equal, μF = μR = μ0. Generated events are processed through the full CMS detector simulation based on. The calculation is carried out with the vbfnlo program [33] with the factorization and renormalization scales set to μR = μF = 90 GeV and with CT10 parton distribution functions [34]. The kinematic distributions for the signal generated by vbfnlo at leading order agree with those produced by the MadGraph generator. The interference effects between EW and DY jj production processes are evaluated with the MadGraph, sherpa [35], CompHEP [36], and vbfnlo programs by the authors of these programs and were found to be negligible

Event selection
40 JE5S0 U6p0 70 80 100
Hadronic activity in the rapidity interval between tagging jets
20 JES3U0p 40 50 60 70
Central hadronic activity measurement using jets
Central hadronic activity measurement with track jets
Signal extraction using the dijet mass fit
Systematic uncertainties
Background modeling
Results
Summary
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