Search results for "Diagram"

showing 10 items of 795 documents

Temperatures and chemical potentials at kinetic freeze-out in relativistic heavy ion collisions from coarse grained transport simulations

2019

Using the UrQMD/coarse graining approach we explore the kinetic freeze-out stage in central Au + Au collisions at various energies. These studies allow us to obtain detailed information on the thermodynamic properties (e.g. temperature and chemical potential) of the system during the kinetic decoupling stage. We explore five relevant collision energies in detail, ranging from $\sqrt{s_{NN}}=2.4\,\mathrm{GeV}$ (GSI-SIS) to $\sqrt{s_{NN}}=200\,\mathrm{GeV}$ (RHIC). By adopting a standard Hadron Resonance Gas equation of state, we determine the average temperature $\langle T \rangle$ and the average baryon chemical potential $\langle\mu_{\mathrm{B}}\rangle$ on the space-time hyper-surface of l…

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsEquation of state (cosmology)HadronFOS: Physical sciencesDecoupling (cosmology)hiukkasfysiikkaKinetic energy01 natural sciencesResonance (particle physics)Nuclear physicsBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)13. Climate action0103 physical sciencesQuark–gluon plasmaNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhase diagram
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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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Helicity Amplitudes of the Lambda(1670) and two Lambda(1405) as dynamically generated resonances

2010

We determine the helicity amplitudes A(1/2) and radiative decay widths in the transition Lambda(1670) -> gamma Y (Y = Lambda or Sigma(0)). The Lambda(1670) is treated as a dynamically generated resonance in meson-baryon chiral dynamics. We obtain the radiative decay widths of the Lambda(1670) to gamma Lambda as 2 +/- 1 keV and to -gamma Sigma(0) as 120 +/- 50 keV. Also, the Q(2)-dependence of the helicity amplitudes A(1/2) is calculated. We find that the K Xi component in the Lambda(1670) structure, mainly responsible for the dynamical generation of this resonance, is also responsible for the significant suppression of the decay ratio Gamma(gamma A)/Gamma(gamma Sigma 0). A measurement of th…

PhysicsNuclear and High Energy PhysicsNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaAnalytic continuationFísicaResonanceFOS: Physical sciencesLambdaHelicityLoop (topology)Nuclear Theory (nucl-th)symbols.namesakeAmplitudesymbolsFeynman diagramddc:530Atomic physicsComplex plane
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New Schwinger-Dyson equations for non-Abelian gauge theories

2008

We show that the application of the pinch technique to the conventional Schwinger-Dyson equations for the gluon propagator, gluon-quark vertex, and three-gluon vertex, gives rise to new equations endowed with special properties. The new series coincides with the one obtained in the Feynman gauge of the background field method, thus capturing the extensive gauge cancellations implemented by the pinch technique at the level of individual Green's functions. Its building blocks are the fully dressed pinch technique Green's functions obeying Abelian all-order Ward identities instead of the Slavnov-Taylor identites satisfied by their conventional counterparts. As a result, and contrary to the sta…

PhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaPropagatorFOS: Physical sciencesGluonsymbols.namesakeFormalism (philosophy of mathematics)High Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)PinchsymbolsFeynman diagramGauge theoryAbelian groupMathematical physics
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The sunset diagram in SU(3) chiral perturbation theory

1996

A general procedure for the calculation of a class of two-loop Feynman diagrams is described. These are two-point functions containing three massive propagators, raised to integer powers, in the denominator, and arbitrary polynomials of the loop momenta in the numerator. The ultraviolet divergent parts are calculated analytically, while the remaining finite parts are obtained by a one-dimensional numerical integration, both below and above the threshold. Integrals of this type occur, for example, in chiral perturbation theory at order p^6.

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryDiagramFOS: Physical sciencesGeneral Physics and AstronomyPropagatorAstronomy and AstrophysicsNumerical integrationLoop (topology)symbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)IntegersymbolsOrder (group theory)Feynman diagramMathematical physics
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Hadron structure in the description of electromagnetic reactions

2002

The description of electromagnetic reactions at intermediate energies, such as pion electroproduction or (virtual) Compton scattering, traditionally starts from covariant tree-level Feynman diagrams (Born or pole terms). Internal hadron structure is included by means of (on-shell) form factors in the vertices while free propagators are used. To overcome problems with gauge invariance, simple prescriptions, such as, choosing ${F}_{1}^{V}{(q}^{2}{)=F}_{\ensuremath{\pi}}{(q}^{2})$ in pion electroproduction or the ``minimal substitution,'' are used. We discuss the inherent assumptions of such approaches and study the general structure of electromagnetic vertices and propagators for pions and nu…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryHadronCompton scatteringPropagatorVertex (geometry)symbols.namesakePionsymbolsFeynman diagramGauge theoryNuclear ExperimentMathematical physicsPhysical Review C
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Neutrinoless double beta decay in supersymmetry with bilinear R-parity breaking

1998

We reanalyze the contributions to neutrinoless double beta ($\znbb$) decay from supersymmetry with explicit breaking of R-parity. Although we keep both bilinear and trilinear terms, our emphasis is put on bilinear R-parity breaking terms, because these mimic more closely the models where the breaking of R-parity is spontaneous. Comparing the relevant Feynman diagrams we conclude that the usual mass mechanism of double beta decay is the dominant one. From the non-observation of $\znbb$ decay we set limits on the bilinear R-parity breaking parameters of typically a (few) 100 $keV$. Despite such stringent bounds, we stress that the magnitude of R-parity violating phenomena that can be expected…

PhysicsNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesBilinear interpolationFísicaSupersymmetryFirst generationThird generationHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Double beta decayR-paritysymbolsFeynman diagramBeta (velocity)High Energy Physics::Experiment
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The effective neutrino charge radius in the presence of fermion masses

2005

Abstract We show how the crucial gauge cancellations leading to a physical definition of an effective neutrino charge radius persist in the presence of non-vanishing fermion masses. An explicit one-loop calculation demonstrates that, as happens in the massless case, the pinch technique rearrangement of the Feynman amplitudes, together with the judicious exploitation of the fundamental current relation J α ( 3 ) = 2 ( J Z + sin θ w 2 J γ ) α , leads to a completely gauge independent definition of the effective neutrino charge radius. Using the formalism of the Nielsen identities it is further proved that the same cancellation mechanism operates unaltered to all orders in perturbation theory.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyVertex functionFísicaFermionMassless particlesymbols.namesakeAmplitudeCharge radiusQuantum electrodynamicssymbolsPinchFeynman diagramNeutrino
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On the evaluation of sunset-type Feynman diagrams

1999

We introduce an efficient configuration space technique which allows one to compute a class of Feynman diagrams which generalize the scalar sunset topology to any number of massive internal lines. General tensor vertex structures and modifications of the propagators due to particle emission with vanishing momenta can be included with only a little change of the basic technique described for the scalar case. We discuss applications to the computation of $n$-body phase space in $D$-dimensional space-time. Substantial simplifications occur for odd space-time dimensions where the final results can be expressed in closed form through rational functions. We present explicit analytical formulas fo…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryComputationScalar (mathematics)FOS: Physical sciencesPropagatorRational functionSunsetNuclear Theory (nucl-th)High Energy Physics - Phenomenologysymbols.namesakeTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Phase spacesymbolsFeynman diagramConfiguration spaceNuclear Physics B
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Mesonic and binding contributions to the EMC effect in a relativistic many-body approach

1996

We revise the conventional nuclear effects of Fermi motion, binding and pionic effects in deep inelastic lepton scattering using a relativistic formalism for an interacting Fermi sea and the local density approximation to translate results from nuclear matter to finite nuclei. In addition we also consider effects from rho-meson renormalization in the nucleus. The use of nucleon Green's functions in terms of their spectral functions offers a precise way to account for Fermi motion and binding. On the other hand the use of many body Feynman diagrams in a relativistic framework allows one to avoid using prescriptions given in the past to introduce relativistic corrections in a non relativistic…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryMesonHigh Energy Physics::PhenomenologyEMC effectNuclear TheoryFOS: Physical sciencesFísicaNuclear matterNuclear Theory (nucl-th)RenormalizationHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)symbolsFeynman diagramNucleonNuclear ExperimentFermi Gamma-ray Space TelescopeLepton
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