Search results for "Covariant transformation"

showing 10 items of 100 documents

On the chiral covariant approach to ρρ scattering

2017

We examine in detail a recent work (D.~G\"ulmez, U.-G.~Mei\ss ner and J.~A.~Oller, Eur. Phys. J. C 77:460 (2017)), where improvements to make $\rho\rho$ scattering relativistically covariant are made. The paper has the remarkable conclusion that the $J=2$ state disappears with a potential which is much more attractive than for $J=0$, where a bound state is found. We trace this abnormal conclusion to the fact that an "on-shell" factorization of the potential is done in a region where this potential is singular and develops a large discontinuous and unphysical imaginary part. A method is developed, evaluating the loops with full $\rho$ propagators, and we show that they do not develop singula…

PhysicsNuclear and High Energy PhysicsBethe–Salpeter equationNuclear TheoryMeson010308 nuclear & particles physicsPropagatorAstronomy and AstrophysicsState (functional analysis)01 natural sciencesHigh Energy Physics - PhenomenologySingularityFactorization0103 physical sciencesBound stateCovariant transformation010306 general physicsInstrumentationMathematical physicsChinese Physics C
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Locality properties of Neuberger's lattice Dirac operator

1998

The gauge covariant lattice Dirac operator D which has recently been proposed by Neuberger satisfies the Ginsparg-Wilson relation and thus preserves chiral symmetry. The operator also avoids a doubling of fermion species, but its locality properties are not obvious. We now prove that D is local (with exponentially decaying tails) if the gauge field is sufficiently smooth at the scale of the cutoff. Further analytic and numerical studies moreover suggest that the locality of the operator is in fact guaranteed under far more general conditions.

PhysicsNuclear and High Energy PhysicsChiral symmetryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)LocalityFOS: Physical sciencesFísicaParticle Physics - LatticeFermionDirac operatorsymbols.namesakeHigh Energy Physics - LatticeLattice (order)symbolsCutoffCovariant transformationGauge theoryMathematical physics
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Fully covariant and conformal formulation of the Z4 system in a reference-metric approach: Comparison with the BSSN formulation in spherical symmetry

2014

We adopt a reference-metric approach to generalize a covariant and conformal version of the Z4 system of the Einstein equations. We refer to the resulting system as ``fully covariant and conformal", or fCCZ4 for short, since it is well suited for curvilinear as well as Cartesian coordinates. We implement this fCCZ4 formalism in spherical polar coordinates under the assumption of spherical symmetry using a partially-implicit Runge-Kutta (PIRK) method and show that our code can evolve both vacuum and non-vacuum spacetimes without encountering instabilities. Our method does not require regularization of the equations to handle coordinate singularities, nor does it depend on constraint-preservi…

PhysicsNuclear and High Energy PhysicsCurvilinear coordinates010308 nuclear & particles physicsFOS: Physical sciencesSpherical coordinate systemGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum Cosmologylaw.inventionGeneral Relativity and Quantum CosmologyNumerical relativityClassical mechanicsHamiltonian constraintlaw0103 physical sciencesGravitational singularityCartesian coordinate systemCovariant transformationCircular symmetry010306 general physicsPhysical Review D
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Covariant approximation averaging

2015

We present a new class of statistical error reduction techniques for Monte-Carlo simulations. Using covariant symmetries, we show that correlation functions can be constructed from inexpensive approximations without introducing any systematic bias in the final result. We introduce a new class of covariant approximation averaging techniques, known as all-mode averaging (AMA), in which the approximation takes account of contributions of all eigenmodes through the inverse of the Dirac operator computed from the conjugate gradient method with a relaxed stopping condition. In this paper we compare the performance and computational cost of our new method with traditional methods using correlation…

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeMonte Carlo methodLattice field theoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCDDirac operatorsymbols.namesakeHigh Energy Physics - LatticeConjugate gradient methodLattice gauge theoryQuantum mechanicssymbolsCovariant transformationVector mesonMathematical physics
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Covariant phase space quantization of the Jackiw-Teitelboim model of two-dimensional gravity

1992

Abstract On the basis of the covariant phase space formulation of field theory we analyze the Jackiw-Teitelboim model of two-dimensional gravity on a cylinder. We compute explicitly the symplectic structure showing that the (reduced) phase space is the cotangent bundle of the space of conjugacy classes of the PSL(2, R ) group. This makes it possible to quantize the theory exactly. The Hilbert space is given by the character functions of the PSL (2, R ) group. As a byproduct, this implies the complete equivalence with the PSL (2, R )-topological gravity model.

PhysicsNuclear and High Energy PhysicsHilbert spaceCotangent spaceSpace (mathematics)symbols.namesakeConjugacy classPhase spaceQuantum mechanicssymbolsCotangent bundlePhase space formulationCovariant transformationMathematical physicsPhysics Letters B
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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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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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