0000000000147931

AUTHOR

Ze Long Liu

0000-0001-7735-3451

showing 4 related works from this author

Three-Loop Quark Jet Function.

2018

We calculate the massless quark jet function to three-loop order. The quark jet function is a universal ingredient in SCET factorization for many collider and decay processes with quark initiated final state jets. Our three-loop result contributes to the resummation for observables probing the invariant mass of final state quark jets at primed next-to-next-to-next-to-leading-logarithmic accuracy. It represents the first complete three-loop result for a factorization ingredient describing collinear radiation. Furthermore it constitutes a major component of the N-jettiness subtraction method at next-to-next-to-next-to-leading order accuracy, which eventually may enable the calculation of full…

QuarkPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyObservableJet (particle physics)01 natural scienceslaw.inventionMassless particleFactorizationlaw0103 physical sciencesInvariant massHigh Energy Physics::ExperimentResummation010306 general physicsColliderPhysical review letters
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Factorization at Subleading Power, Sudakov Resummation and Endpoint Divergences in Soft-Collinear Effective Theory

2020

Starting from the first renormalized factorization theorem for a process described at subleading power in soft-collinear effective theory, we discuss the resummation of Sudakov logarithms for such processes in renormalization-group improved perturbation theory. Endpoint divergences in convolution integrals, which arise generically beyond leading power, are regularized and removed by systematically rearranging the factorization formula. We study in detail the example of the $b$-quark induced $h\to\gamma\gamma$ decay of the Higgs boson, for which we resum large logarithms of the ratio $M_h/m_b$ at next-to-leading logarithmic order. We also briefly discuss the related $gg\to h$ amplitude.

High Energy Physics - TheoryPhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciencesHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Soft-collinear effective theoryFactorizationHigh Energy Physics - Theory (hep-th)Weierstrass factorization theoremsymbolsHiggs bosonEffective field theoryPerturbation theoryResummationMathematical physics
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s-channel single top quark production and decay at next-to-next-to-leading-order in QCD

2018

We report on a fully differential next-to-next-to-leading order (NNLO) calculation of s-channel single top (anti)quark production with a semileptonic decay at the LHC, neglecting the color correlation between the light and heavy quark lines and in the narrow width approximation. The NNLO corrections can increase the cross section by about 10% in the low transverse momentum region of the top quark and reduce scale variation uncertainty. In order to compare with experimental results without unfolding procedures, we also present theoretical predictions with fiducial cuts, including total cross sections and distributions of observables used in the experimental multivariate analysis. The NNLO co…

QuarkSemileptonic decayQuantum chromodynamicsPhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear TheoryOrder (ring theory)Observable01 natural sciencesCross section (physics)0103 physical sciences010306 general physicsPhysical Review
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Renormalization and Scale Evolution of the Soft-Quark Soft Function

2020

Soft functions defined in terms of matrix elements of soft fields dressed by Wilson lines are central components of factorization theorems for cross sections and decay rates in collider and heavy-quark physics. While in many cases the relevant soft functions are defined in terms of gluon operators, at subleading order in power counting soft functions containing quark fields appear. We present a detailed discussion of the properties of the soft-quark soft function consisting of a quark propagator dressed by two finite-length Wilson lines connecting at one point. This function enters in the factorization theorem for the Higgs-boson decay amplitude of the $h\to\gamma\gamma$ process mediated by…

QuarkHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::LatticeFOS: Physical sciencesPosition and momentum spaceRenormalizationsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)FactorizationPerturbative QCDRenormalization Grouplcsh:Nuclear and particle physics. Atomic energy. RadioactivityResummationMathematical physicsPhysicsHigh Energy Physics::PhenomenologyPropagatorEffective Field TheoriesRenormalization groupHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Weierstrass factorization theoremsymbolslcsh:QC770-798High Energy Physics::ExperimentResummation
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