Search results for "PERTURBATION"

showing 10 items of 811 documents

Chiral perturbation theory: Introduction and recent results in the one-nucleon sector

2009

We provide an introduction to the basic concepts of chiral perturbation theory and discuss some recent developments in the manifestly Lorentz-invariant formulation of the one-nucleon sector.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryMesonSpontaneous symmetry breakingHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesNuclear Theory (nucl-th)RenormalizationHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosonBibliographyNucleonProgress in Particle and Nuclear Physics
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QCD condensates from tau-decay data: A functional approach

2004

We study a functional method to extract the V − A condensate of dimension 6 from a comparison of τ -decay data with the asymptotic space-like QCD prediction. Our result is in agreement within errors with that from conventional analyses based on finite energy sum rules.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsFunctional approachFOS: Physical sciencesPerturbation (Mathematics)Mathematical analysisRenormalization (Physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Quantum mechanics[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quantum chromodynamics -- Mathematical modelsSum rule in quantum mechanicsEnergy (signal processing)
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τ hadronic spectral function moments in a nonpower QCD perturbation theory

2016

Abstract The moments of the hadronic spectral functions are of interest for the extraction of the strong coupling and other QCD parameters from the hadronic decays of the τ lepton. We consider the perturbative behavior of these moments in the framework of a QCD nonpower perturbation theory, defined by the technique of series acceleration by conformal mappings, which simultaneously implements renormalization-group summation and has a tame large-order behavior. Two recently proposed models of the Adler function are employed to generate the higher order coefficients of the perturbation series and to predict the exact values of the moments, required for testing the properties of the perturbativ…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHadronPerturbation (astronomy)Conformal map01 natural sciencesSeries accelerationstrong coupling0103 physical sciencesCentre for High Energy PhysicsPerturbation theory (quantum mechanics)010306 general physicsReference modeltau decaysLeptonNuclear and Particle Physics Proceedings
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Comparison study of medium-modified QCD shower evolution scenarios

2009

The computation of hard processes in hadronic collisions is a major success of perturbative Quantum Chromodynamics (pQCD). In such processes, pQCD not only predicts the hard reaction itself, but also the subsequent evolution in terms of parton branching and radiation, leading to a parton shower and ultimately to an observable jet of hadrons. If the hard process occurs in a heavy-ion collision, a large part of this evolution takes place in the soft medium created along with the hard reaction. An observation of jets in heavy-ion collision thus allows a study of medium-modified QCD shower evolution. In vacuum, Monte-Carlo (MC) simulations are well established tools to describe such showers. Fo…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyHadronMonte Carlo methodFOS: Physical sciencesObservablePartonCollisionNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPerturbation theory (quantum mechanics)Nuclear ExperimentParton showerPhysical Review C
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Towards a determination of the chiral couplings at NLO in 1/N-C: L-8(r)(μ) and C-38(r)(μ)

2007

14 pages.-- ISI Article Identifier: 000244120200039.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0610290

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeScalar (mathematics)ResonanceOrder (ring theory)FísicaFOS: Physical sciences1/N ExpansionRenormalizationPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum Chromodynamics (QCD)High Energy Physics::ExperimentPion decay constantChiral lagrangians
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Chiral extrapolation and finite-volume dependence of the hyperon vector couplings

2014

The hyperon vector form factors at zero momentum transfer, $f_1(0)$, play an important role in a precise determination of the Cabibbo-Kobayashi-Maskawa matrix element $V_{us}$. Recent studies based on lattice chromodynamics (LQCD) simulations and covariant baryon chiral perturbation theory yield contradicting results. In this work, we study chiral extrapolation of and finite-volume corrections to the latest $n_f=2+1$ LQCD simulations. Our results show that finite-volume corrections are relatively small and can be safely ignored at the present LQCD setup of $m_\pi L=4.6$ but chiral extrapolation needs to be performed more carefully. Nevertheless, the discrepancy remains and further studies a…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeMomentum transferHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)ExtrapolationHyperonFOS: Physical sciences16. Peace & justiceHigh Energy Physics - ExperimentBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Covariant transformation
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The lowest-lying baryon masses in covariant SU(3)-flavor chiral perturbation theory

2010

We present an analysis of the baryon-octet and -decuplet masses using covariant SU(3)-flavor chiral perturbation theory up to next-to-leading order. Besides the description of the physical masses we address the problem of the lattice QCD extrapolation. Using the PACS-CS Collaboration data we show that a good description of the lattice points can be achieved at next-to-leading order with the covariant loop amplitudes and phenomenologically determined values for the meson-baryon couplings. Moreover, the extrapolation to the physical point up to this order is found to be better than the linear one given at leading-order by the Gell-Mann-Okubo approach. The importance that a reliable combinatio…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryHigh Energy Physics::LatticeLattice field theoryQuark modelNuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesLattice QCDBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Covariant transformationHigh Energy Physics::ExperimentQuantum field theoryNuclear Experiment
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Confronting QCD with the experimental hadronic spectral functions from tau-decay

2009

The (non-strange) vector and axial-vector spectral functions extracted from $\tau $-decay by the ALEPH collaboration are confronted with QCD in the framework of a Finite Energy QCD sum rule (FESR) involving a polynomial kernel tuned to suppress the region beyond the kinematical end point where there is no longer data. This effectively allows for a QCD FESR analysis to be performed beyond the region of the existing data. Results show excellent agreement between data and perturbative QCD in the remarkably wide energy range $s = 3 - 10 {GeV}^2$, leaving room for a dimension $d$ =4 vacuum condensate consistent with values in the literature. A hypothetical dimension $d$=2 term in the Operator Pr…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsDimension (graph theory)Order (ring theory)Perturbative QCDFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Perturbation theory (quantum mechanics)Sum rule in quantum mechanicsOperator product expansionEnergy (signal processing)
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Parton shower evolution in a 3-d hydrodynamical medium

2008

We present a Monte Carlo simulation of the perturbative Quantum Chromodynamics (pQCD) shower developing after a hard process embedded in a heavy-ion collision. The main assumption is that the cascade of branching partons traverses a medium which (consistent with standard radiative energy loss pictures) is characterized by a local transport coefficient qhat which measures the virtuality per unit length transferred to a parton which propagates in this medium. This increase in parton virtuality alters the development of the shower and in essence leads to extra induced radiation and hence a softening of the momentum distribution in the shower. After hadronization, this leads to the concept of a…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsTransport coefficientHadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservablePartonHadronizationNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPerturbation theory (quantum mechanics)Parton showerNuclear Experiment
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anQCD: Fortran programs for couplings at complex momenta in various analytic QCD models

2015

We provide three Fortran programs which evaluate the QCD analytic (holomorphic) couplings $\mathcal{A}_{\nu}(Q^2)$ for complex or real squared momenta $Q^2$. These couplings are holomorphic analogs of the powers $a(Q^2)^{\nu}$ of the underlying perturbative QCD (pQCD) coupling $a(Q^2) \equiv \alpha_s(Q^2)/\pi$, in three analytic QCD models (anQCD): Fractional Analytic Perturbation Theory (FAPT), Two-delta analytic QCD (2$\delta$anQCD), and Massive Perturbation Theory (MPT). The index $\nu$ can be noninteger. The provided programs do basically the same job as the Mathematica package anQCD.m in Mathematica published by us previously, Ref.[1], but are now written in Fortran.

PhysicsQuantum chromodynamicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsHolomorphic functionGeneral Physics and AstronomyPerturbative QCDFOS: Physical sciences01 natural sciencesRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Hardware and Architecture0103 physical sciencesHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Invariant (mathematics)010306 general physicsComplex planeMathematical physics
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