Repository logo
Log in(current)
Repository logoMIT Open ScholarshipDSpace@MIT
  1. Home
  2. MIT Open Access Articles
  3. MIT Open Access Articles
  4. Measurement of the Transverse Momentum and ϕ[subscript η]* Distributions of Drell–Yan Lepton Pairs in Proton–proton Collisions at √s = 8 TeV with the ATLAS Detector

Measurement of the Transverse Momentum and ϕ[subscript η]* Distributions of Drell–Yan Lepton Pairs in Proton–proton Collisions at √s = 8 TeV with the ATLAS Detector

Thumbnail Image
Download
Name

s10052-016-4070-4.pdf

Size

3.32 MB

Format

Adobe PDF

Checksum (MD5)

495bc119fcc87dd1459e1666e3f61902

Download all files submitted through automated deposit
sword-2018-02-09.original.zip (1.74 MB)
Author(s)
ATLAS Collaboration
•
Taylor, Frank E
Date Issued
May 2016
Journal
European Physical Journal C: Particles and Fields
Publisher
Springer Berlin Heidelberg
Citation
Aad, G. et al. “Measurement of the Transverse Momentum and ϕ[subscript η]* Distributions of Drell–Yan Lepton Pairs in Proton–proton Collisions at √s = 8 TeV with the ATLAS Detector.” The European Physical Journal C 76, 5 (May 2016): 291 © 2016 CERN for the benefit of the ATLAS collaboration
Version
Final published version
Abstract
Distributions of transverse momentum p[subscript T][superscript ℓℓ] and the related angular variable ϕ[subscript η]* of Drell–Yan lepton pairs are measured in 20.3fb ⁻¹ of proton–proton collisions at √ s = 8 TeV with the ATLAS detector at the LHC. Measurements in electron-pair and muon-pair final states are corrected for detector effects and combined. Compared to previous measurements in proton–proton collisions at √ s = 7 TeV, these new measurements benefit from a larger data sample and improved control of systematic uncertainties. Measurements are performed in bins of lepton-pair mass above, around and below the Z-boson mass peak. The data are compared to predictions from perturbative and resummed QCD calculations. For values of ϕ[subscript η]* < 1 the predictions from the Monte Carlo generator ResBos are generally consistent with the data within the theoretical uncertainties. However, at larger values of ϕ[subscript η]* this is not the case. Monte Carlo generators based on the parton-shower approach are unable to describe the data over the full range of p[subscript T][superscript ℓℓ] while the fixed-order prediction of Dynnlo falls below the data at high values of p[subscript T][superscript ℓℓ] . ResBos and the parton-shower Monte Carlo generators provide a much better description of the evolution of the ϕ[subscript η]* and p[subscript T][superscript ℓℓ] distributions as a function of lepton-pair mass and rapidity than the basic shape of the data.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution 4.0 International License
http://creativecommons.org/licenses/by/4.0/
Persistent DSpace Link
http://hdl.handle.net/1721.1/117331
DOI of Published Version
https://doi.org/10.1140/epjc/s10052-016-4070-4
Repository logo
PrivacyPermissionsAccessibilityContact us
Repository logo
Notify us about copyright concerns.