Abstract

We construct predictions for top quark pair differential distributions at hadron colliders that combine state-of-the-art NNLO QCD calculations with double resummation at NNLL′ accuracy of threshold logarithms arising from soft gluon emissions and of small mass logarithms. This is the first time a resummed calculation at full NNLO+NNLL′ accuracy in QCD for a process with non-trivial color structure has been completed at the differential level. Of main interest to us is the stability of the {M}_{toverline{t}} and top-quark pT distributions in the boosted regime where fixed order calculations may become strongly dependent on the choice of dynamic scales. With the help of numeric and analytic arguments we confirm that the choice for the factorization and renormalization scales advocated recently by some of the authors is indeed optimal. We further derive a set of optimized kinematics-dependent scales for the matching functions which appear in the resummed calculations. Our NNLO+NNLL′ prediction for the top-pair invariant mass is significantly less sensitive to the choice of factorization scale than the fixed order prediction, even at NNLO. Notably, the resummed and fixed order calculations are in nearly perfect agreement with each other in the full {M}_{toverline{t}} range when the optimal dynamic scale is used. For the top-quark pT distribution the resummation performed here has less of an impact and instead we find that upgrading the matching with fixed-order from NLO+NNLL′ to NNLO+NNLL′ to be an important effect, a point to be kept in mind when using NLO-based Monte Carlo event generators to calculate this distribution.

Highlights

  • Kinematic regime where the energies of the produced top quarks are much larger than the top-quark mass

  • For the top-quark pT distribution the resummation performed here has less of an impact and instead we find that upgrading the matching with fixed-order from next-to-leading order (NLO)+next-to-next-to-leading logarithmic (NNLL) to NNLO+NNLL to be an important effect, a point to be kept in mind when using NLO-based Monte Carlo event generators to calculate this distribution

  • We give our main results for the top-pair invariant mass and top-quark pT distributions, as well as the total cross section, with a focus on comparing NNLO results with NNLO+NNLL ones

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Summary

Introduction

Kinematic regime where the energies of the produced top quarks are much larger than the top-quark mass. The second is that, due to the shape of the parton distribution functions (PDFs), the effective partonic center-of-mass energies in most events with boosted top quarks are not much larger than the invariant masses of the top quark pairs This can lead to enhanced corrections from so-called soft logarithms or threshold logarithms, and in general the two types of logarithms multiply each other at a given order in perturbation theory, due to emissions which are simultaneously soft and collinear. While the focus of that phenomenological study was the boosted regime, a matching procedure with standard soft-gluon resummation results (i.e. without the simultaneous resummation of small-mass logarithms) at next-to-next-to-leading logarithmic (NNLL) accuracy [32] and to NLO fixedorder calculations was performed in order to expand the validity of the results to the full phase space

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