Abstract

We investigate how precisely the CP nature of the 125 GeV Higgs-boson resonance $$h$$ can be unraveled at the LHC in its decays to $$\tau $$ pairs, $$h \rightarrow \tau ^-\tau ^+$$ . We use a method which allows one to determine the scalar–pseudoscalar Higgs mixing angle $$\phi _\tau $$ in this decay mode. This mixing angle can be extracted from the distribution of a signed angle, denoted by $$\varphi _\mathrm{CP}^{*}$$ , which we analyze for the major charged-prong $$\tau $$ decays. For definiteness, we consider Higgs-boson production by gluon fusion at NLO QCD. We take into account also the irreducible background from Drell–Yan production, $$Z^*/\gamma ^*\rightarrow \tau \tau $$ , at NLO QCD. We compute, for the signal and background reactions, angular and energy correlations of the charged prongs and analyze which type of cuts suppress the Drell–Yan background. An important feature of this background is that its contribution to the distribution of our observable $$\varphi _\mathrm{CP}^{*}$$ is a flat line, also at NLO QCD. By separating the Drell–Yan $$\tau $$ events into two different sets, two different non-trivial $$\varphi _\mathrm{CP}^{*}$$ distributions are obtained. Based on this observation we propose to use these sets for calibration purposes. By Monte Carlo simulation we study also the effect of measurement uncertainties on this distribution. We estimate that the Higgs mixing angle $$\phi _\tau $$ can be determined with our method to a precision of $$\Delta \phi _\tau \simeq 14^\circ $$ $$(5^\circ )$$ at the high-luminosity LHC (14 TeV) with an integrated luminosity of $$500$$ fb $$^{-1}$$ (3 ab $$^{-1}$$ ).

Highlights

  • IntroductionMuch more experimental analysis is required for completely unraveling the properties of this resonance

  • We have investigated how precisely the CP nature of the 125 GeV Higgs-boson resonance h can be determined at the Large Hadron Collider (LHC) (14 TeV) in its decay to τ leptons

  • As to the subsequent τ decays, we have taken into account all the major decay modes (3)–(7)

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Summary

Introduction

Much more experimental analysis is required for completely unraveling the properties of this resonance. Our approach is based on the distribution of a signed angle φC∗P between the decay planes of the charged-prong decays τ − → a− and τ + → a + in the a−a + zero-momentum frame. We apply this method to the 125 GeV resonance h. While the signal contribution to this distribution shows a characteristic dependence on cos(φC∗P −2φτ ), where the angle φτ describes the mixing of the scalar and pseudoscalar Higgs component which couple to τ leptons We analyze how appropriate cuts on the polar angle distributions of the charged prongs, respectively, associated cuts on their energies can reduce the irreducible background.

Higgs-boson production and decay to τ τ
Distributions for Higgs production and decay to τ τ at the LHC
Observables
Numerical results for the LHC
Other τ decay modes
Impact of measurement uncertainties
Estimate of φτ
Findings
Summary
Full Text
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