0000000000004426

AUTHOR

Iain W. Stewart

showing 2 related works from this author

Precision thrust cumulant moments atN3LL

2012

We consider cumulant moments (cumulants) of the thrust distribution using predictions of the full spectrum for thrust including O(alpha_s^3) fixed order results, resummation of singular N^3LL logarithmic contributions, and a class of leading power corrections in a renormalon-free scheme. From a global fit to the first thrust moment we extract the strong coupling and the leading power correction matrix element Omega_1. We obtain alpha_s(m_Z) = 0.1141 \pm (0.0004)_exp \pm (0.0014)_hadr \pm (0.0007)_pert, where the 1-sigma uncertainties are experimental, from hadronization (related to Omega_1) and perturbative, respectively, and Omega_1 = 0.372 \pm (0.044)_exp \pm (0.039)_pert GeV. The n-th th…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsElectron–positron annihilationFOS: Physical sciencesOrder (ring theory)01 natural sciencesOmegaHigh Energy Physics - ExperimentNuclear Theory (nucl-th)CombinatoricsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Power correctionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesStrong couplingHigh Energy Physics::ExperimentMatrix element010306 general physicsNuclear theoryPhysical Review D
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Power Corrections to Event Shapes with Mass-Dependent Operators

2013

We introduce an operator depending on the "transverse velocity'' r that describes the effect of hadron masses on the leading 1/Q power correction to event-shape observables. Here, Q is the scale of the hard collision. This work builds on earlier studies of mass effects by Salam and Wicke [J. High Energy Phys. 05 (2001) 061] and of operators by Lee and Sterman [Phys. Rev. D 75, 014022 (2007)]. Despite the fact that different event shapes have different hadron mass dependence, we provide a simple method to identify universality classes of event shapes whose power corrections depend on a common nonperturbative parameter. We also develop an operator basis to show that at a fixed value of Q, the…

Nuclear and High Energy PhysicsParticle physicsExponentiationFOS: Physical sciences01 natural sciencesOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesRenormalonsResummationFactorization010306 general physicsMathematical physicsPhysicsQuantum chromodynamics010308 nuclear & particles physicsMultiplicative functionObservableUniversality (dynamical systems)HadronizationHigh Energy Physics - PhenomenologyQCD correctionsE&E-annihilationDistributionsResummationJet cross-sectionsQuantum chromodynamics
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