Determination of the strong coupling constant αs\alpha _\mathrm {s} from transverse energy–energy correlations in multijet events at s=8 TeV\sqrt{s} = 8~\hbox {TeV} using the ATLAS detector

Collaboration
Jul 9, 2017
49 pages
Published in:
  • Eur.Phys.J.C 77 (2017) 12, 872
  • Published: Dec 15, 2017
e-Print:
Report number:
  • CERN-EP-2017-093
Experiments:

Citations per year

20172019202120232025051015
Abstract: (Springer)
Measurements of transverse energy–energy correlations and their associated asymmetries in multi-jet events using the ATLAS detector at the LHC are presented. The data used correspond to s=8 TeV\sqrt{s} = 8~\hbox {TeV} proton–proton collisions with an integrated luminosity of 20.2  fb1~\hbox {fb}^{-1} . The results are presented in bins of the scalar sum of the transverse momenta of the two leading jets, unfolded to the particle level and compared to the predictions from Monte Carlo simulations. A comparison with next-to-leading-order perturbative QCD is also performed, showing excellent agreement within the uncertainties. From this comparison, the value of the strong coupling constant is extracted for different energy regimes, thus testing the running of αs(μ)\alpha _{\mathrm {s}}(\mu ) predicted in QCD up to scales over 1 TeV1~\hbox {TeV} . A global fit to the transverse energy–energy correlation distributions yields αs(mZ)=0.1162±0.0011(exp.) +0.00840.0070(theo.) \alpha _{\mathrm {s}}(m_Z) = 0.1162 \pm 0.0011 \text{(exp.) }^{+0.0084-0.0070} \text{(theo.) } , while a global fit to the asymmetry distributions yields a value of αs(mZ)=0.1196±0.0013(exp.) +0.00750.0045(theo.) \alpha _{\mathrm {s}}(m_Z) = 0.1196 \pm 0.0013 \text{(exp.) }^{+0.0075-0.0045} \text{(theo.) } .
Note:
  • p p: colliding beams
  • strong interaction: coupling constant
  • quantum chromodynamics: perturbation theory
  • perturbation theory: higher-order
  • numerical calculations: Monte Carlo
  • jet: multiple production
  • p p: scattering
  • higher-order: 1
  • correlation
  • transverse energy