Abstract

We present the measurements of the differential cross-sections for inclusive electron and muon production in proton–proton collisions at a centre-of-mass energy of $\sqrt{s} = $ 7 TeV, using ∼1.4 pb − 1 of data collected by the ATLAS detector at the Large Hadron Collider. The muon cross-section is measured as a function of muon transverse momentum p T in the range 4 < p T < 100 GeV and within pseudorapidity |η| < 2.5. In addition, the electron and muon cross-sections are measured in the range 7 < p T < 26 GeV and within |η| < 2.0, excluding 1.37 < |η| < 1.52. After subtraction of the W/Z/γ ∗ contribution, the differential cross-sections are found to be in good agreement with theoretical predictions for heavy-flavour production obtained from fixed order NLO calculations with NLL high-p T resummation, and to be sensitive to the effects of NLL resummation.

Highlights

  • The inclusive production of electrons and muons is dominated by decays of charm and beauty hadrons after subtraction of the W/Z /γ ∗ components and may be used to constrain theoretical predictions for heavy-flavour (HF) production

  • We present the measurements of the differential cross-sections for√inclusive electron and muon production in proton–proton collisions at a centre-of-mass energy of s = 7 TeV, using ∼1.4 pb−1 of data collected by the ATLAS detector at the Large Hadron Collider

  • The overall systematic uncertainty of the electron measurement is dominated by the uncertainties of the signal-extraction method and the material uncertainty in the detector volume upstream of the ECAL

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Summary

Introduction

The inclusive production of electrons and muons is dominated by decays of charm and beauty hadrons after subtraction of the W/Z /γ ∗ components and may be used to constrain theoretical predictions for heavy-flavour (HF) production. In this analysis [1], the inclusive muon cross-section is measured as a function of muon transverse momentum pT in the range 4 < pT < 100 GeV and within pseudorapidity |η| < 2.5. The main components of the ATLAS detector [2] are the inner detector (ID), the electromagnetic (ECAL) and hadronic calorimeters, and the muon spectrometer (MS). Cmigrationi is the bin-migration correction factor, defined as the ratio of the number of charged leptons in bin i of true pT and the number in the same bin of reconstructed pT

Signal selection and efficiency determination
Findings
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