Measurement of the polarisation of W bosons produced with large transverse momentum in pp collisions at √𝑠 = 7 with the ATLAS experiment TeV
Author(s)
Aad, G.; Abbott, B.; Abdallah, J.; Abdelalim, A. A.; Abdesselam, A.; Abdinov, O.; Abi, B.; Abolins, M.; AbouZeid, O. S.; Abramowicz, H.; Abreu, H.; Acerbi, E.; Acharya, B. S.; Adamczyk, L.; Adams, D. L.; Addy, T. N.; Adelman, J.; Aderholz, M.; Adomeit, S.; Adragna, P.; ... Show more Show less
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This paper describes an analysis of the angular distribution of W→eν and W→μν decays, using data from pp collisions at
$\sqrt{s} = 7\ \mbox{TeV}$
recorded with the ATLAS detector at the LHC in 2010, corresponding to an integrated luminosity of about 35 pb−1. Using the decay lepton transverse momentum and the missing transverse momentum, the W decay angular distribution projected onto the transverse plane is obtained and analysed in terms of helicity fractions f
0, f
L and f
R over two ranges of W transverse momentum
$(p_{\mathrm{T}}^{W} ): 35 < p_{\mathrm{T}}^{W}< 50\ \mbox{GeV}$
and
$p_{\mathrm{T}}^{W}> 50\ \mbox{GeV}$
. Good agreement is found with theoretical predictions. For
$p_{\mathrm{T}}^{W}> 50\ \mbox{GeV}$
, the values of f
0 and f
L−f
R, averaged over charge and lepton flavour, are measured to be: f
0=0.127±0.030±0.108 and f
L−f
R=0.252±0.017±0.030, where the first uncertainties are statistical, and the second include all systematic effects.
Date issued
2012-05-08Department
Massachusetts Institute of Technology. Department of PhysicsPublisher
Springer Berlin Heidelberg
Citation
The European Physical Journal C. 2012 May 08;72(5):2001
Version: Final published version