Abstract

A measurement of the parity-violating decay asymmetry parameter, alpha_b, and the helicity amplitudes for the decay Lambda_b->J/psi(mu mu)+Lambda(p pi) is reported. The analysis is based on 1400 Lambda_b and anti-Lambda_b baryons selected in 4.6/fb of proton-proton collision data with a center-of-mass energy of 7 TeV recorded by the ATLAS experiment at the LHC. By combining the Lambda_b and anti-Lambda_b samples under the assumption of CP conservation, the value of alpha_b is measured to be 0.30+/-0.16(stat)+/-0.06(syst). This measurement provides a test of theoretical models based on perturbative QCD or heavy-quark effective theory.

Highlights

  • Parity violation, a well-known feature of weak interactions [1,2,3,4], is exhibited in its maximal form in decays of muons and τ leptons

  • Several models have been employed to predict the value of the parity-violating decay asymmetry parameter αb for the weak decay Λ0b → J=ψΛ0

  • This paper provides a measurement of comparable precision using 4.6 fb−1 pp collision data recorded by the ATLAS detector with a center-of-mass energy of 7 TeV

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Summary

INTRODUCTION

A well-known feature of weak interactions [1,2,3,4], is exhibited in its maximal form in decays of muons and τ leptons. Several models have been employed to predict the value of the parity-violating decay asymmetry parameter αb for the weak decay Λ0b → J=ψΛ0. The decay asymmetry parameter αb is related to the helicity amplitudes as follows [15]: αb 1⁄4 jaþj2 − ja−j2 þ jbþj2 − jb−j2:. Only six out of the eight helicity amplitude parameters are independent, taking into account the normalization constraint [Eq (2)] and, due to the arbitrary value of the common phase, only differences between the four phases are relevant. Assuming CP conservation, the Λ0b and Λ 0b samples are combined to measure αb and the helicity amplitudes

DATA SAMPLES AND TRIGGER SELECTION
MONTE CARLO SAMPLES
Muon reconstruction
PARAMETER EXTRACTION
Background subtraction
Detector effects correction
Fit results
SYSTEMATIC UNCERTAINTIES
Background
VIII. CONCLUSIONS
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