Search results for "evolution equation"

showing 10 items of 26 documents

Next-to-leading order Balitsky-Kovchegov equation with resummation

2016

We solve the Balitsky-Kovchegov evolution equation at next-to-leading order accuracy including a resummation of large single and double transverse momentum logarithms to all orders. We numerically determine an optimal value for the constant under the large transverse momentum logarithm that enables including a maximal amount of the full NLO result in the resummation. When this value is used the contribution from the $\alpha_s^2$ terms without large logarithms is found to be small at large saturation scales and at small dipoles. Close to initial conditions relevant for phenomenological applications these fixed order corrections are shown to be numerically important.

PhysicsLogarithmta114Nuclear Theory010308 nuclear & particles physicsFOS: Physical sciencesBalitsky-Kovchegov equation01 natural sciencesgluonsNuclear Theory (nucl-th)DipoleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamics0103 physical sciencesEvolution equationquantum chromodynamicscolor glass condensateOrder (group theory)Boundary value problemResummation010306 general physicsConstant (mathematics)Saturation (chemistry)next-to-leading order corrections
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The effect of random matter density perturbations on the MSW solution to the solar neutrino problem

1996

We consider the implications of solar matter density random noise upon resonant neutrino conversion. The evolution equation describing MSW-like conversion is derived in the framework of the Schr\"odinger approach. We study quantitatively their effect upon both large and small mixing angle MSW solutions to the solar neutrino problem. This is carried out both for the active-active $\nu_e \ra \nu_{\mu,\tau}$ as well as active-sterile $\nu_e \ra \nu_s$ conversion channels. We find that the small mixing MSW solution is much more stable (especially in $\Delta m^2$) than the large mixing solution. The possible existence of solar matter density noise at the few percent level could be tested at futu…

PhysicsNuclear and High Energy PhysicsParticle physicsSolar neutrinoAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSolar neutrino problemAstrophysicsNoise (electronics)symbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Evolution equationsymbolsHigh Energy Physics::ExperimentNeutrinoBorexinoSchrödinger's catMixing (physics)
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Hydrodynamic equations of anisotropic, polarized and inhomogeneous superfluid vortex tangles

2008

We include the effects of anisotropy and polarization in the hydrodynamics of inhomogeneous vortex tangles, thus generalizing the well known Hall-Vinen-Bekarevich-Khalatnikov equations, which do not take them in consideration. These effects contribute to the mutual friction force ${\bf F}_{ns}$ between normal and superfluid components and to the vortex tension force $\rho_s{\bf T}$. These equations are complemented by an evolution equation for the vortex line density $L$, which takes into account these contributions. These equations are expected to be more suitable than the usual ones for rotating counterflows, or turbulence behind a cylinder, or turbulence produced by a grid of parallel th…

PhysicsTurbulenceCondensed Matter::OtherFOS: Physical sciencesStatistical and Nonlinear PhysicsTourbillonCondensed Matter PhysicsPolarization (waves)VortexCylinder (engine)law.inventionSuperfluidityPhysics::Fluid DynamicsCondensed Matter - Other Condensed MatterClassical mechanicslawEvolution equationAnisotropySettore MAT/07 - Fisica MatematicaSuperfluid turbulence Liquid helium II Hydrodynamic equationsOther Condensed Matter (cond-mat.other)
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Color glass condensate at next-to-leading order meets HERA data

2020

We perform the first dipole picture fit to HERA inclusive cross section data using the full next-to-leading order (NLO) impact factor combined with an improved Balitsky-Kovchegov evolution including the dominant effects beyond leading logarithmic accuracy at low $x$. We find that three different formulations of the evolution equation that have been proposed in the recent literature result in a very similar description of HERA data, and robust predictions for future deep inelastic scattering experiments. We find evidence pointing towards a significant nonperturbative contribution to the structure function for light quarks, which stresses the need to extend the NLO impact factor calculation t…

QuarkParticle physicsLogarithmNuclear TheoryFOS: Physical scienceshiukkasfysiikka01 natural sciences114 Physical sciencesperturbative QCDColor-glass condensateNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)HERADeep inelastic scatteringDipoleHigh Energy Physics - PhenomenologyQCD in nuclear reactionsEvolution equationHigh Energy Physics::Experimentydinfysiikka
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Single inclusive forward hadron production at next-to-leading order

2016

We discuss single inclusive hadron production from a high energy quark scattering off a strong target color field in the Color Glass Condensate formalism. Recent calculations of this process at the next-to-leading order accuracy have led to negative cross sections at large transverse momenta. We identify the origin of this problem as an oversubtraction of the rapidity divergence into the Balitsky-Kovchegov evolution equation for the target. We propose a new way to implement the kinematical restriction on the emitted gluons to overcome this difficulty.

QuarkParticle physicssingle inclusive hardon productionNuclear TheoryHadronFOS: Physical sciencescolor glass condensate formalism01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Balitsky-Kovchegov evolution0103 physical sciencesRapidityfysiikka010306 general physicsPhysicsta114010308 nuclear & particles physicsScatteringGluonTransverse planeHigh Energy Physics - PhenomenologyEvolution equationphysics
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JIMWLK evolution of the odderon

2016

We study the effects of a parity-odd "odderon" correlation in JIMWLK renormalization group evolution at high energy. Firstly we show that in the eikonal picture where the scattering is described by Wilson lines, one obtains a strict mathematical upper limit for the magnitude of the odderon amplitude compared to the parity even pomeron one. This limit increases with N_c, approaching infinity in the infinite N_c limit. We use a systematic extension of the Gaussian approximation including both 2- and 3-point correlations which enables us to close the system of equations even at finite N_c. In the large-N_c limit we recover an evolution equation derived earlier. By solving this equation numeric…

SMALL-X EVOLUTIONWilson loopNuclear TheoryLARGE NUCLEIWilson linesFOS: Physical sciencesField (mathematics)114 Physical sciences01 natural sciencesHIGH-ENERGY SCATTERINGColor-glass condensateRENORMALIZATION-GROUPNuclear Theory (nucl-th)GLUON DISTRIBUTION-FUNCTIONSPomeronHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsquantum chromodynamics0103 physical sciencesEQUATION010306 general physicsPhysicsta114evolution equations010308 nuclear & particles physicsScatteringEikonal equationHERA-DATAHigh Energy Physics::PhenomenologyCOLOR GLASS CONDENSATEodderonRenormalization groupHigh Energy Physics - PhenomenologyAmplitudeJIMWLKPA-COLLISIONSBK EVOLUTION
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The generalized Kadomtsev-Petviashvili equation I

1997

Sobolev spaceApplied MathematicsMathematical analysisEvolution equationKadomtsev–Petviashvili equationAnalysisMathematical physicsMathematicsNonlinear Analysis: Theory, Methods & Applications
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Decay estimates in the supremum norm for the solutions to a nonlinear evolution equation

2014

We study the asymptotic behaviour, as t → ∞, of the solutions to the nonlinear evolution equationwhere ΔpNu = Δu + (p−2) (D2u(Du/∣Du∣)) · (Du/∣Du∣) is the normalized p-Laplace equation and p ≥ 2. We show that if u(x,t) is a viscosity solution to the above equation in a cylinder Ω × (0, ∞) with time-independent lateral boundary values, then it converges to the unique stationary solution h as t → ∞. Moreover, we provide an estimate for the decay rate of maxx∈Ω∣u(x,t) − h(x)∣.

Uniform normGeneral MathematicsMathematical analysista111CylinderViscosity solutionNonlinear evolutionStationary solutionnonlinear evolution equationBoundary valuesMathematicsProceedings of the Royal Society of Edinburgh, Section: A Mathematics
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Well-posedness of a nonlinear evolution equation arising in growing cell population

2011

We prove that a nonlinear evolution equation which comes from a model of an age-structured cell population endowed with general reproduction laws is well-posed. Copyright © 2011 John Wiley & Sons, Ltd.

Well-posed problemeducation.field_of_studyGeneral MathematicsReproduction (economics)PopulationMathematical analysisGeneral EngineeringPhysics::History of PhysicsEvolution equationQuantitative Biology::Populations and EvolutioneducationNonlinear evolutionWell posednessMathematicsMathematical Methods in the Applied Sciences
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Effective charge from lattice QCD

2020

Using lattice configurations for quantum chromodynamics (QCD) generated with three domain-wall fermions at a physical pion mass, we obtain a parameter-free prediction of QCD's renormalisation-group-invariant process-independent effective charge, $\hat\alpha(k^2)$. Owing to the dynamical breaking of scale invariance, evident in the emergence of a gluon mass-scale, this coupling saturates at infrared momenta: $\hat\alpha(0)/\pi=0.97(4)$. Amongst other things: $\hat\alpha(k^2)$ is almost identical to the process-dependent (PD) effective charge defined via the Bjorken sum rule; and also that PD charge which, employed in the one-loop evolution equations, delivers agreement between pion parton di…

dimension: 4Nuclear TheoryHigh Energy Physics::Latticesum rule: Bjorkenparton: distribution function01 natural sciencespi: massHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentInstrumentationQuantum chromodynamicsPhysicsHigh Energy Physics - Lattice (hep-lat)scalingdynamical symmetry breakinglattice field theoryLattice QCDDyson-Schwinger equationsEmergence of massHigh Energy Physics - Phenomenologyinfraredfermion: domain wallSum rule in quantum mechanicsRunning couplingNuclear and High Energy PhysicsParticle physicsLattice field theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Lattice field theoryFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Theory (nucl-th)High Energy Physics - Lattice0103 physical sciencesquantum chromodynamicsQuantum field theory010306 general physicsCoupling constant010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics::Phenomenologycoupling constantAstronomy and AstrophysicsgluonGluonDistribution functionevolution equation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentQuantum chromodynamicsConfinement
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