Abstract

With the goal of increasing the precision of NLO QCD predictions for the ppto toverline{t}gamma process in the di-lepton top quark decay channel we present theoretical predictions for the mathrm{mathcal{R}}={sigma}_{toverline{t}gamma }/{sigma}_{toverline{t}} cross section ratio. Results for the latter together with various differential cross section ratios are given for the LHC with the Run II energy of sqrt{s}=13 TeV. Fully realistic NLO computations for toverline{t} and toverline{t}gamma production are employed. They are based on matrix elements for {e}^{+}{nu}_e{mu}^{-}{overline{nu}}_{mu }boverline{b} and {e}^{+}{nu}_e{mu}^{-}{overline{nu}}_{mu }boverline{b}gamma processes and include all resonant and non-resonant diagrams, interferences, and off-shell effects of the top quarks and the W gauge bosons. Various renormalisation and factorisation scale choices and parton density functions are examined to assess their impact on the cross section ratio. Depending on the transverse momentum cut on the hard photon a judicious choice of a dynamical scale allows us to obtain 1%–3% percent precision on mathrm{mathcal{R}} . Moreover, for differential cross section ratios theoretical uncertainties in the range of 1%-6% have been estimated. Until now such high precision predictions have only been reserved for the top quark pair production at NNLO QCD. Thus, mathrm{mathcal{R}} at NLO in QCD represents a very precise observable to be measured at the LHC for example to study the top quark charge asymmetry or to probe the strength and the structure of the t- overline{t} -γ vertex. The latter can shed some light on possible new physics that can reveal itself only once sufficiently precise theoretical predictions are available.

Highlights

  • JHEP01(2019)188 ttγ production process at the LHC is much smaller than the cross section for the production of the top quark pair alone, the former can provide key information on the strength and the structure of the top quark coupling to the photon

  • With the goal of increasing the precision of NLO QCD predictions for the pp → ttγ process in the di-lepton top quark decay channel we present theoretical predictions for the R = σttγ/σttcross section ratio

  • Realistic NLO computations for ttand ttγ production are employed. They are based on matrix elements for e+νeμ−νμbb and e+νeμ−νμbbγ processes and include all resonant and non-resonant diagrams, interferences, and off-shell effects of the top quarks and the W gauge bosons

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Summary

Computational framework and input parameters

All the LO and NLO results for e+νe μ−νμ bb γ and e+νe μ−νμ bb production, which are presented in this paper, have been obtained with the help of the Helac-NLO MC framework [10]. At the one loop level the appearance of Γt = 0 in the propagator requires the evaluation of scalar integrals with complex masses, which is supported by the OneLOop program [20] Further details of these calculations can be found in our earlier work on pp → tt [8], pp → ttj [21, 22] and pp → ttγ [6] where complete top quark off-shell effects have been consistently taken into account at the NLO level in QCD. For the central value of the scale, μ0, we consider the fixed scale (the phase-space independent scale choice) μ0 = mt/2 and the dynamic scale (the phase-space dependent scale choice) μ0 = HT /4 The latter is defined on an event-by-event basis according to HT = pT, e+ + pT, μ− + pmT iss + pT, b1 + pT, b2 ,. We set no restriction on the kinematics of the extra (non b-)jet

Differential cross sections at NLO in QCD
Absolute cross sections at NLO in QCD
Cross section ratios at NLO in QCD
Differential cross section ratios at NLO in QCD
Findings
Conclusions
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