Abstract
Abstract
We propose a new strategy to probe the Z boson couplings to bottom and charm quarks at the LHC. In this work we mainly focus on the case of bottom quarks. Here, the Z boson is produced in association with two b-jets and decays to electrons or muons. In this final state, tagging the charge of the b-jets allows us to measure the charge asymmetry and thus to directly probe the $$ Zb\overline{b} $$
Zb
b
¯
couplings. The leptonic final state not only allows us to cleanly reconstruct the Z boson but also to mitigate the otherwise overwhelming backgrounds. Furthermore, while LEP could only scan a limited range of dilepton invariant masses, there is no such limitation at the LHC. Consequently, this allows us to make full use of the interference between the amplitudes mediated by a Z boson and a photon. Using the full high-luminosity LHC dataset of 3 ab−1 and with the current flavor and charge-tagging capabilities would allow us to reject the wrong-sign right-handed coupling solution by 4σ. Further improving the charge-tagging efficiency would disfavor it by 6σ.
Publisher
Springer Science and Business Media LLC
Subject
Nuclear and High Energy Physics
Reference65 articles.
1. ALEPH collaboration, Measurement of $$ {A}_{FB}^b $$ using inclusive b hadron decays, Eur. Phys. J. C 22 (2001) 201 [hep-ex/0107033] [INSPIRE].
2. ALEPH et al. collaborations, Precision electroweak measurements on the Z resonance, Phys. Rept. 427 (2006) 257 [hep-ex/0509008] [INSPIRE].
3. ALEPH et al. collaborations, Precision Electroweak Measurements and Constraints on the Standard Model, arXiv:0911.2604 [INSPIRE].
4. ALEPH et al. collaborations, Precision Electroweak Measurements and Constraints on the Standard Model, arXiv:1012.2367 [INSPIRE].
5. W. Bernreuther et al., The forward-backward asymmetry for massive bottom quarks at the Z peak at next-to-next-to-leading order QCD, JHEP 01 (2017) 053 [arXiv:1611.07942] [INSPIRE].