Search results for "Laurent series"

showing 6 items of 16 documents

Four-gluon scattering at three loops, infrared structure and Regge limit

2016

We compute the three-loop four-gluon scattering amplitude in maximally supersymmetric Yang-Mills theory, including its full color dependence. Our result is the first complete computation of a non-planar four-particle scattering amplitude to three loops in four-dimensional gauge theory and consequently provides highly non-trivial data for the study of non-planar scattering amplitudes. We present the amplitude as a Laurent expansion in the dimensional regulator to finite order, with coefficients composed of harmonic poly-logarithms of uniform transcendental weight, and simple rational prefactors. Our computation provides an independent check of a recent result for three-loop corrections to th…

PhysicsHigh Energy Physics - Theory010308 nuclear & particles physicsScatteringLaurent seriesHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesGluonScattering amplitudeMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryAmplitudeSingularityHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum electrodynamics0103 physical sciencesGauge theory010306 general physicsParticle Physics - Theory
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Pole positions and residues from pion photoproduction using the Laurent-Pietarinen expansion method

2014

We have applied a new approach to determine the pole positions and residues from pion photoproduction multipoles. The method is based on a Laurent expansion of the partial wave T-matrices, with a Pietarinen series representing the regular part of energy-dependent and single-energy photoproduction solutions. The method has been applied to multipole fits generated by the MAID and GWU/SAID groups. We show that the number and properties of poles extracted from photoproduction data correspond very well to results from $\pi$N elastic data and values cited by Particle Data Group (PDG). The photoproduction residues provide new information for the electromagnetic current at the pole position, which …

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theorybaryon resonances ; poles ; Laurent+Pietarinen expansionSeries (mathematics)Laurent seriesNuclear TheoryFOS: Physical sciencesParticle Data GroupNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionAmplitudePosition (vector)High Energy Physics::ExperimentNuclear ExperimentNucleonMultipole expansionPhysical Review C
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Introducing the Pietarinen expansion method into the single-channel pole extraction problem

2013

We present a new approach to quantifying pole parameters of single-channel processes based on a Laurent expansion of partial-wave T matrices in the vicinity of the real axis. Instead of using the conventional power-series description of the nonsingular part of the Laurent expansion, we represent this part by a convergent series of Pietarinen functions. As the analytic structure of the nonsingular part is usually very well known (physical cuts with branch points at inelastic thresholds, and unphysical cuts in the negative energy plane), we find that one Pietarinen series per cut represents the analytic structure fairly reliably. The number of terms in each Pietarinen series is determined by …

PhysicsNuclear and High Energy PhysicsToy modelSeries (mathematics)Plane (geometry)Quantum mechanicsLaurent seriesMathematical analysisNegative energynucleon resonances; poles; new pole extraction methodComplex planeConvergent seriesBranch point
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Towards a NNLO Calculation in Hadronic Heavy Hadron Production

2005

We calculate the Laurent series expansion up to ${\cal O}(\epsilon^2)$ for all scalar one-loop one-, two-, three- and four-point integrals that are needed in the calculation of hadronic heavy flavour production. The Laurent series up to ${\cal O}(\epsilon^2)$ is needed as input to that part of the NNLO corrections to heavy hadron production at hadron colliders where the one-loop integrals appear in the loop-by-loop contributions. The four-point integrals are the most complicated. The ${\cal O}(\epsilon^2)$ expansion of the four-point integrals contains polylogarithms up to $ Li_4$ and the multiple polylogarithms.

PhysicsParticle physicsLaurent seriesHigh Energy Physics::PhenomenologyFlavourHadronScalar (mathematics)High Energy Physics::ExperimentNuclear Experiment
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On the nonarchimedean quadratic Lagrange spectra

2018

We study Diophantine approximation in completions of functions fields over finite fields, and in particular in fields of formal Laurent series over finite fields. We introduce a Lagrange spectrum for the approximation by orbits of quadratic irrationals under the modular group. We give nonarchimedean analogs of various well known results in the real case: the closedness and boundedness of the Lagrange spectrum, the existence of a Hall ray, as well as computations of various Hurwitz constants. We use geometric methods of group actions on Bruhat-Tits trees. peerReviewed

Pure mathematicscontinued fraction expansionGeneral MathematicsLaurent seriesLagrange spectrumDiophantine approximationalgebra01 natural sciences[MATH.MATH-GR]Mathematics [math]/Group Theory [math.GR]Group actionQuadratic equationModular group0103 physical sciences0101 mathematicsquadratic irrationalContinued fractionMathematicslukuteoriaMathematics - Number TheoryHall ray010102 general mathematicsSpectrum (functional analysis)ryhmäteoriapositive characteristicformal Laurent series[MATH.MATH-NT]Mathematics [math]/Number Theory [math.NT]Finite fieldHurwitz constantAMS codes: 11J06 11J70 11R11 20E08 20G25010307 mathematical physics11J06 11J70 11R11 20E08 20G25
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Laurent series expansion of a class of massive scalar one-loop integrals toO(ε2)

2005

We use dimensional regularization to calculate the O({epsilon}{sup 2}) expansion of all scalar one-loop one-, two-, three-, and four-point integrals that are needed in the calculation of hadronic heavy quark production. The Laurent series up to O({epsilon}{sup 2}) is needed as input to that part of the next-to-next-to-leading order corrections to heavy flavor production at hadron colliders where the one-loop integrals appear in the loop-by-loop contributions. The four-point integrals are the most complicated. The O({epsilon}{sup 2}) expansion of the three- and four-point integrals contains in general polylogarithms up to Li{sub 4} and functions related to multiple polylogarithms of maximal …

QuarkQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsDimensional regularizationQuantum electrodynamicsLaurent seriesHigh Energy Physics::PhenomenologyHadronScalar (mathematics)Series expansionMathematical physicsPhysical Review D
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