Search results for "TRANSFORMATION"

showing 10 items of 1634 documents

Effective Boost and 'Point Form' Approach

2002

Triangle Feynman diagrams can be considered as describing form factors of states bound by a zero-range interaction. These form factors are calculated for scalar particles and compared to point-form and non-relativistic results. By examining the expressions of the complete calculation in different frames, we obtain an effective boost transformation which can be compared to the relativistic kinematical one underlying the present point-form calculations, as well as to the Galilean boost. The analytic expressions obtained in this simple model allow a qualitative check of certain results obtained in similar studies. In particular, a mismatch is pointed out between recent practical applications o…

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Dirac (software)Scalar (physics)FOS: Physical sciences01 natural sciencesGalileanNuclear Theory (nucl-th)symbols.namesakeTheoretical physicsTransformation (function)Simple (abstract algebra)Quantum mechanics0103 physical sciencessymbolsFeynman diagramPoint (geometry)Física nuclear010306 general physicsNuclear theory
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Lorentz Multiplet Structure of Baryon Spectra and Relativistic Description

1997

The pole positions of the various baryon resonances are known to reveal well-pronounced clustering, so-called Hoehler clusters. For nonstrange baryons the Hoehler clusters are shown to be identical to Lorentz multiplets of the type (j,j)*[(1/2,0)+(0,1/2)] with j being a half-integer. For the Lambda hyperons below 1800 MeV these clusters are shown to be of the type [(1,0)+ (0,1)]*[(1/2,0)+(0,1/2)] while above 1800 MeV they are parity duplicated (J,0)+(0,J) (Weinberg-Ahluwalia) states. Therefore, for Lambda hyperons the restoration of chiral symmetry takes place above 1800 MeV. Finally, it is demonstrated that the description of spin-3/2 particles in terms of a 2nd rank antisymmetric Lorentz …

PhysicsNuclear and High Energy PhysicsNuclear TheoryAntisymmetric relationLorentz transformationNuclear TheoryHyperonFOS: Physical sciencesGeneral Physics and AstronomyAstronomy and AstrophysicsParity (physics)Spectral lineNuclear Theory (nucl-th)BaryonHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Dirac spinorsymbolsMultipletMathematical physicsModern Physics Letters A
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Matching stages of heavy-ion collision models

2010

Heavy-ion reactions and other collective dynamical processes are frequently described by different theoretical approaches for the different stages of the process, like initial equilibration stage, intermediate locally equilibrated fluid dynamical stage, and final freeze-out stage. For the last stage, the best known is the Cooper-Frye description used to generate the phase space distribution of emitted, noninteracting particles from a fluid dynamical expansion or explosion, assuming a final ideal gas distribution, or (less frequently) an out-of-equilibrium distribution. In this work we do not want to replace the Cooper-Frye description, but rather clarify the ways of using it and how to choo…

PhysicsNuclear and High Energy PhysicsNuclear TheoryHeavy ion collisionNuclear physicsFOS: Physical sciencesCol·lisions d'ions pesatsHadronsMolecular dynamicsSpace (mathematics)Ideal gasHadronizationNuclear Theory (nucl-th)Model descriptionClassical mechanicsDistribution (mathematics)HypersurfaceCollisions (Nuclear physics)Phase spaceCol·lisions (Física nuclear)Covariant transformationFísica nuclearStatistical physicsDinàmica molecularNuclear Experiment
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Covariant description of kinetic freeze out through a finite space-like layer

2005

The problem of Freeze Out (FO) in relativistic heavy ion reactions is addressed. We develop and analyze an idealized one-dimensional model of FO in a finite layer, based on the covariant FO probability. The resulting post FO phase-space distributions are discussed for different FO probabilities and layer thicknesses.

PhysicsNuclear and High Energy PhysicsNuclear TheoryReaccions nuclearsFOS: Physical sciencesKinetic energyThermodynamic modelNuclear Theory (nucl-th)Distribution (mathematics)Classical mechanicsCollisions (Nuclear physics)Phase spaceCol·lisions (Física nuclear)Covariant transformationNuclear reactionsLayer (object-oriented design)Nuclear ExperimentNuclear theoryMathematical physics
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Exploring the intrinsic Lorentz-violating parameters at DUNE

2018

Neutrinos can push our search for new physics to a whole new level. What makes them so hard to be detected, what allows them to travel humongous distances without being stopped or deflected allows to amplify Planck suppressed effects (or effects of comparable size) to a level that we can measure or bound in DUNE. In this work we analyze the sensitivity of DUNE to CPT and Lorentz-violating interactions in a framework that allows a straightforward extrapolation of the bounds obtained to any phenomenological modification of the dispersion relation of neutrinos.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelLorentz transformationExtrapolationFOS: Physical sciences01 natural sciencesMeasure (mathematics)Partícules (Física nuclear)lcsh:QC1-999High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Dispersion relation0103 physical sciencessymbolsSensitivity (control systems)NeutrinoPlanck010306 general physicslcsh:PhysicsPhysics Letters B
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Pinch technique self-energies and vertices to all orders in perturbation theory

2003

The all-order construction of the pinch technique gluon self-energy and quark-gluon vertex is presented in detail within the class of linear covariant gauges. The main ingredients in our analysis are the identification of a special Green's function, which serves as a common kernel to all self-energy and vertex diagrams, and the judicious use of the Slavnov-Taylor identity it satisfies. In particular, it is shown that the ghost-Green's functions appearing in this identity capture precisely the result of the pinching action at arbitrary order. By virtue of this observation the construction of the quark-gluon vertex becomes particularly compact. It turns out that the aforementioned ghost-Green…

PhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaFunction (mathematics)Vertex (geometry)RenormalizationHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Kernel (statistics)Covariant transformationUniquenessPerturbation theory (quantum mechanics)
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Hyperon forward spin polarizability gamma0 in baryon chiral perturbation theory

2015

We present the calculation of the hyperon forward spin polarizability gamma0 using manifestly Lorentz covariant baryon chiral perturbation theory including the intermediate contribution of the spin 3/2 states. As at the considered order the extraction of gamma0 is a pure prediction of chiral perturbation theory, the obtained values are a good test for this theory. After including explicitly the decuplet states, our SU(2) results have a very good agreement with the experimental data and we extend our framework to SU(3) to give predictions to the hyperons' gamma0 values. Prominent are the Sigma^- and Xi^- baryons as their photon transition to the decuplet is forbidden in SU(3) symmetry and th…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryLorentz transformationгипероныNuclear TheoryHigh Energy Physics::PhenomenologyHyperonFOS: Physical sciencesSymmetry (physics)Baryonsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PolarizabilityQuantum electrodynamicssymbolsCovariant transformationSpin-½Proceedings of The 8th International Workshop on Chiral Dynamics — PoS(CD15)
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Leading-order decuplet contributions to the baryon magnetic moments in chiral perturbation theory

2009

We extend an earlier study of the baryon magnetic moments in chiral perturbation theory by the explicit inclusion of the spin-3/2 decuplet resonances. We find that the corrections induced by these heavier degrees of freedom are relatively small in a covariant framework where unphysical spin-1/2 modes are removed. Consequently, implementing the leading SU(3)-breaking corrections given by both the baryon and decuplet contributions, we obtain a description of the baryon-octet magnetic moments that is better than the Coleman-Glashow relations. Finally, we discuss the uncertainties and compare between heavy baryon and covariant approaches. (C) 2009 Elsevier B.V. All rights reserved.

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryMagnetic momentHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryHigh Energy Physics::PhenomenologyDegrees of freedom (physics and chemistry)HyperonFOS: Physical sciencesCovarianceNuclear Theory (nucl-th)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Covariant transformationPerturbation theory (quantum mechanics)Nuclear ExperimentPhysics Letters B
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Polarized parton distributions and light-front dynamics

1998

We present a consistent calculation of the structure functions within a light-front constituent quark model of the nucleon. Relativistic effects and the relevance of the covariance constraints are analyzed for both polarized and unpolarized parton distributions. Various models, which differ in their gluonic structure at the hadronic scale, are investigated. The results of the full covariant calculation are compared with those of a non-relativistic approximation to show the structure and magnitude of the differences.

PhysicsNuclear and High Energy PhysicsParticle physicsCovarianceStructure functionsScale (ratio)Light-frontHadronNuclear TheoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesConstituent quarkPartonCovarianceGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quark modelCovariant transformationHigh Energy Physics::ExperimentNucleonRelativistic quantum chemistryNuclear Experiment
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Covariant foundation of heavy hadron decays

1991

Abstract I present a covariant formulation of heavy hadron decays in the formal limit of MQ → ∞. This allows for an elegant way to implement the symmeteries found by Isgur and Wise in this limit. I also discuss a Bloch-Nordsieck formulation of this limit and leading log corrections.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyHadronFoundation (engineering)Covariant transformationLimit (mathematics)Atomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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