Search results for "LESS"

showing 10 items of 2452 documents

Reexamination of the Power Spectrum in De Sitter Inflation

2008

4 pages, 1 table.-- PACS nrs.: 98.80.Cq, 04.62.+v.-- PMID: 18999735 [PubMed].

PhysicsQuantum field theory in curved spacetime010308 nuclear & particles physicsVacuum stateGeneral Physics and AstronomySpectral densityAstrophysics::Cosmology and Extragalactic AstrophysicsInflaton01 natural sciences[PACS] Quantum fields in curved spacetimeMassless particleGeneral Relativity and Quantum CosmologyAmplitude[PACS] Particle-theory and field-theory models of the early UniverseDe Sitter universeQuantum mechanicsQuantum electrodynamics0103 physical sciences010306 general physicsQuantum fluctuationPhysical Review Letters
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Phase transition in liquid 4HE by a mean field model

2013

In this work the transition of 4He at the lambda line in presence of a Cattaneo- Maxwell heat flux is studied. A hydrodynamical model is formulated, which chooses as fundamental fields the velocity, the temperature, the heat flux and a phase field function f, for which a time dependent Ginzburg-Landau equation is proposed. Using this model we are able to describe the phase transition and to obtain the pressure-temperature phase diagram which represents the transition, the thermodynamic restrictions and a maximum theorem for the phase field.

PhysicsQuantum phase transitionLiquid heliumPhase transitionField (physics)ThermodynamicsCondensed Matter PhysicsKosterlitz–Thouless transitionMean field theoryHeat fluxMean phase-field modelPhase (matter)Quantum critical pointGeneral Materials ScienceSettore MAT/07 - Fisica MatematicaPhase transition
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Parton showers from the dipole formalism

2007

We present an implementation of a parton shower algorithm for hadron colliders and electron-positron colliders based on the dipole factorisation formulae. The algorithm treats initial-state partons on equal footing with final-state partons. We implemented the algorithm for massless and massive partons.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFOS: Physical sciencesPartonGluonNuclear physicsMassless particleHigh Energy Physics - PhenomenologyDipoleHigh Energy Physics - Phenomenology (hep-ph)FactorizationPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentInvariant massNuclear ExperimentParton showerPhysical Review D
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Neutrinoless double β decay with small neutrino masses

2013

Proceedings of the Corfu Summer Institute 2012 "School and Workshops on Elementary Particle Physicsand Gravity", September 8-27, 2012, Corfu (Greece). PoS(Cofu2012)028.

PhysicsQuarkParticle physicsPhysics beyond the Standard ModelDouble betaHigh Energy Physics::PhenomenologyFísicaNeutrinolessLepton numberPartícules (Física nuclear)Operator (computer programming)Neutrino massDouble beta decayHigh Energy Physics::ExperimentNeutrinoPhenomenology (particle physics)LeptonDouble β
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Infrared singularities of scattering amplitudes in perturbative QCD

2009

An exact formula is derived for the infrared singularities of dimensionally regularized scattering amplitudes in massless QCD with an arbitrary number of legs, valid at any number of loops. It is based on the conjecture that the anomalous-dimension matrix of n-jet operators in soft-collinear effective theory contains only a single non-trivial color structure, whose coefficient is the cusp anomalous dimension of Wilson loops with light-like segments. Its color-diagonal part is characterized by two anomalous dimensions, which are extracted to three-loop order from known perturbative results for the quark and gluon form factors. This allows us to predict the three-loop coefficients of all 1/ep…

PhysicsQuarkQuantum chromodynamicsHigh Energy Physics - TheoryHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyPerturbative QCDFOS: Physical sciencesJet (particle physics)Massless particleScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Soft-collinear effective theoryHigh Energy Physics - Theory (hep-th)Quantum mechanicsEffective field theoryHigh Energy Physics::ExperimentMathematical physics
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The baryonic spectrum of QCD 2 in the chiral limit

1991

Abstract A description of the baryonic spectrum of quantum chromodynamics in one-space-one-time dimensions for massless quarks is presented. The theory has been studied in the equivalent non-abelian bosonic representation, and four-point functions of the colored meson fields under the simplifying assumption of two colors have been calculated. The crucial role of the chiral sector in providing baryon number has been unveiled. Excited baryon states appear as pseudomesonic excitations on top of the massless baryons associated with the chiral fields.

PhysicsQuarkQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyAstrophysics::Cosmology and Extragalactic Astrophysicslcsh:QC1-999Massless particleBaryonExcited stateBaryon numberNuclear Experimentlcsh:PhysicsBosonPhysics Letters B
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The forward-backward asymmetry at NNLO revisited

2006

I reconsider the forward-backward asymmetry for flavoured quarks in electron-positron annihilation. I suggest an infrared-safe definition of this observable, such that the asymmetry may be computed in perturbative QCD with massless quarks. With this definition, the first and second order QCD corrections are computed.

PhysicsQuarkQuantum chromodynamicsParticle physicsNuclear and High Energy PhysicsAnnihilationmedia_common.quotation_subjectHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesObservableForward backwardAsymmetryMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::Experimentmedia_common
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About the realization of chiral symmetry in QCD2

1992

Two dimensional massless Quantum Chromodynamics presents many features which resemble those of the true theory. In particular the spectrum consists of mesons and baryons arranged in flavor multiplets without parity doubling. We analyze the implications of chiral symmetry, which is not spontaneously broken in two dimensions, in the spectrum and in the quark condensate. We study how parity doubling, an awaited consequence of Coleman's theorem, is avoided due to the dimensionality of space-time and confinement. We prove that a chiral phase transition is not possible in the theory.

PhysicsQuarkQuantum chromodynamicsParticle physicsPhysics and Astronomy (miscellaneous)MesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologySpectrum (functional analysis)FOS: Physical sciencesFísicaParity (physics)BaryonMassless particleHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Engineering (miscellaneous)Realization (systems)Zeitschrift f�r Physik C Particles and Fields
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A 3D Meshless Approach for Transient Electromagnetic PDEs

2012

A full wave three dimensional meshless approach for electromagnetic transient simulations is presented. The smoothed particle hydrodynamic (SPH) method is used by considering the particles as interpolation points, arbitrarily placed in the computational domain. Maxwell’s equations in time domain with the assigned boundary and initial conditions are numerically solved by means of the proposed method. The computational tool is assessed and, for the first time, a 3D test problem is simulated in order to validate the proposed approach.

PhysicsRegularized meshless methodPartial differential equationBoundary (topology)Meshless methodPartial differential equationsDomain (mathematical analysis)Settore MAT/08 - Analisi NumericaSettore ING-IND/31 - ElettrotecnicaParticleApplied mathematicsTime domainTransient (oscillation)Interpolation
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Renormalization-scheme ambiguity and perturbation theory near a fixed point

1984

We consider the perturbative calculation of critical exponents in massless, renormalizable theories having a nontrivial fixed point. In conventional perturbation theory, all results depend on the arbitrary renormalization scheme used. We show how to resolve this problem, following the "principle of minimal sensitivity" approach. At least three orders of perturbation theory are required for quantitative results. We give scheme-independent criteria for determining the presence or absence of a fixed point in $n\mathrm{th}$ order, and discuss the conditions under which perturbative results might be reliable. As illustrations we discuss QED with many flavors, and ${({\ensuremath{\varphi}}^{4})}_…

PhysicsRenormalizationMassless particleScheme (mathematics)Quantum electrodynamicsOrder (ring theory)Perturbation theory (quantum mechanics)Sensitivity (control systems)Fixed pointCritical exponentMathematical physicsPhysical Review D
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