Measurement of the τ lepton polarization in Z boson decays in proton-proton collisions at √𝑠 = 13 TeV
Name
13130_2024_Article_22610.pdf
Size
1.68 MB
Format
Adobe PDF
Checksum (MD5)
2131ed43ff07e14abb47add01b3e0feb
Author(s) • • • • • • • • •
Hayrapetyan, A.
Tumasyan, A.
Adam, W.
Andrejkovic, J. W.
Bergauer, T.
Chatterjee, S.
Damanakis, K.
Dragicevic, M.
Escalante Del Valle, A.
Hussain, P. S.
Date Issued
January 19, 2024
Publisher
Springer Berlin Heidelberg
Citation
Journal of High Energy Physics. 2024 Jan 19;2024(1):101
Version
Final published version
Abstract
The polarization of τ leptons is measured using leptonic and hadronic τ lepton decays in Z → τ+τ− events in proton-proton collisions at
s
$$ \sqrt{s} $$
= 13 TeV recorded by CMS at the CERN LHC with an integrated luminosity of 36.3 fb−1. The measured τ− lepton polarization at the Z boson mass pole is
P
τ
Z
$$ {\mathcal{P}}_{\tau}\left(\textrm{Z}\right) $$
= −0.144 ± 0.006 (stat) ± 0.014 (syst) = −0.144 ± 0.015, in good agreement with the measurement of the τ lepton asymmetry parameter of Aτ = 0.1439 ± 0.0043 =
−
P
τ
Z
$$ -{\mathcal{P}}_{\tau}\left(\textrm{Z}\right) $$
at LEP. The τ lepton polarization depends on the ratio of the vector to axial-vector couplings of the τ leptons in the neutral current expression, and thus on the effective weak mixing angle sin2
θ
W
eff
$$ {\theta}_{\textrm{W}}^{\textrm{eff}} $$
, independently of the Z boson production mechanism. The obtained value sin2
θ
W
eff
$$ {\theta}_{\textrm{W}}^{\textrm{eff}} $$
= 0.2319 ± 0.0008(stat) ± 0.0018(syst) = 0.2319 ± 0.0019 is in good agreement with measurements at e+e− colliders.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution
Persistent DSpace Link
DOI of Published Version
https://doi.org/10.1007/JHEP01(2024)101