Search results for "existence."

showing 10 items of 189 documents

Yang-Mills two-point functions in linear covariant gauges

2015

In this work we use two different but complementary approaches in order to study the ghost propagator of a pure SU(3) Yang-Mills theory quantized in the linear covariant gauges, focusing on its dependence on the gauge-fixing parameter $\xi$ in the deep infrared. In particular, we first solve the Schwinger-Dyson equation that governs the dynamics of the ghost propagator, using a set of simplifying approximations, and under the crucial assumption that the gluon propagators for $\xi>0$ are infrared finite, as is the case in the Landau gauge $(\xi=0)$. Then we appeal to the Nielsen identities, and express the derivative of the ghost propagator with respect to $\xi$ in terms of certain auxiliary…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)PropagatorFOS: Physical sciencesFísicaYang–Mills existence and mass gapRotation formalisms in three dimensionsGluonHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum mechanicsCovariant transformationMathematical physicsGauge fixingAnsatz
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Charge radii of odd-A 191–211Po isotopes

2013

Isotope shifts have been measured for the odd-A polonium isotopes 191–211Po and changes in the nuclear mean square charge radii δr2 have been deduced. The measurements were performed at CERN-ISOLDE using the in-source resonance-ionization spectroscopy technique. The combined analysis of these data and our recent results for even-A polonium isotopes indicates an onset of deformation already at 197,198Po, when going away from stability. This is significantly earlier than was suggested by previous theoretical and experimental studies of the polonium isotopes. Moreover and in contrast to the mercury isotopes, where a strong odd–even staggering of the charge radii of the ground states was observ…

PhysicsMean squareNuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsShape coexistencechemistry.chemical_elementMercury IsotopesCharge (physics)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesIsotopes of nitrogenNuclear physicsIsotope shiftchemistry0103 physical sciencesNeutronPhysics::Atomic PhysicsAtomic physicsNuclear charge radiusNuclear Experiment010306 general physicsSpectroscopyPoloniumPhysics Letters B
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On the gluon spectrum in the glasma

2010

We study the gluon distribution in nucleus-nucleus collisions in the framework of the Color-Glass-Condensate. Approximate analytical solutions are compared to numerical solutions of the non-linear Yang-Mills equations. We find that the full numerical solution can be well approximated by taking the full initial condition of the fields in Coulomb gauge and using a linearized solution for the time evolution. We also compare kt-factorized approximations to the full solution.

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsTime evolutionFOS: Physical sciencesYang–Mills existence and mass gap01 natural sciencesGluonColor-glass condensateNuclear Theory (nucl-th)High Energy Physics - PhenomenologyNonlinear systemDistribution (mathematics)High Energy Physics - Phenomenology (hep-ph)Quantum electrodynamics0103 physical sciencesInitial value problemComputer Science::Symbolic Computation010306 general physicsNuclear ExperimentGauge fixing
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Gluon spectrum in the glasma from JIMWLK evolution

2011

The JIMWLK equation with a "daughter dipole" running coupling is solved numerically starting from an initial condition given by the McLerran-Venugopalan model. The resulting Wilson line configurations are then used to compute the spectrum of gluons comprising the glasma inital state of a high energy heavy ion collision. The development of a geometrical scaling region makes the spectrum of produced gluons harder. Thus the ratio of the mean gluon transverse momentum to the saturation scale grows with energy. Also the total gluon multiplicity increases with energy slightly faster than the saturation scale squared.

PhysicsNuclear and High Energy PhysicsParticle physicsWilson loopta114Nuclear Theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesYang–Mills existence and mass gapRenormalization group01 natural sciencesGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyDipoleHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamics0103 physical sciencesInitial value problemBoundary value problem010306 general physicsNuclear ExperimentScaling
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Pinch technique at two loops: The case of massless Yang-Mills theories

2000

The generalization of the pinch technique beyond one loop is presented. It is shown that the crucial physical principles of gauge-invariance, unitarity, and gauge-fixing-parameter independence single out at two loops exactly the same algorithm which has been used to define the pinch technique at one loop, without any additional assumptions. The two-loop construction of the pinch technique gluon self-energy, and quark-gluon vertex are carried out in detail for the case of mass-less Yang-Mills theories, such as perturbative QCD. We present two different but complementary derivations. First we carry out the construction by directly rearranging two-loop diagrams. The analysis reveals that, quit…

PhysicsNuclear and High Energy PhysicsUnitarityBackground field methodFOS: Physical sciencesFísicaYang–Mills existence and mass gapSymmetry (physics)RenormalizationHigh Energy Physics - PhenomenologyDimensional regularizationsymbols.namesakeTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicssymbolsFeynman diagramGauge theoryPhysical Review D
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Perturbative BF-Yang–Mills theory on noncommutative

2000

A U(1) BF-Yang-Mills theory on noncommutative ${\mathbb{R}}^4$ is presented and in this formulation the U(1) Yang-Mills theory on noncommutative ${\mathbb{R}}^4$ is seen as a deformation of the pure BF theory. Quantization using BRST symmetry formalism is discussed and Feynman rules are given. Computations at one-loop order have been performed and their renormalization studied. It is shown that the U(1) BFYM on noncommutative ${\mathbb{R}}^4$ is asymptotically free and its UV-behaviour in the computation of the $\beta$-function is like the usual SU(N) commutative BFYM and Yang Mills theories.

PhysicsNuclear and High Energy PhysicsYang–Mills existence and mass gapYang–Mills theoryNoncommutative geometryBRST quantizationRenormalizationHigh Energy Physics::Theorysymbols.namesakeFormalism (philosophy of mathematics)Mathematics::Quantum AlgebrasymbolsFeynman diagramCommutative propertyMathematical physicsNuclear Physics B
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In-beam spectroscopic studies of shape coexistence and collectivity in the neutron-deficientZ≈ 82 nuclei

2016

In the present paper we focus on studies of shape coexistence in even-mass nuclei in the neutron-deficient Pb region. They are based on experiments carried out using tagging techniques in the Accelerator Laboratory of the University of Jyväskylä, Finland. Excited states in many of these nuclei can only be accessed via fusion-evaporation reactions employing high-intensity stable-ion beams. The key features in these experiments are high selectivity, clean spectra and instrumentation that enables high count rates. We review three spectroscopic highlights in this region. peerReviewed

PhysicsNuclear and High Energy Physicsquadrupole momentrecoil distance Doppler-shift method010308 nuclear & particles physicsHigh selectivitydeformationshape coexistenceKey features01 natural sciencesSpectral lineNuclear physicsJUROGAMydinreaktiotExcited state0103 physical sciencesNeutronin-beam γ-ray spectroscopyAtomic physicsNuclear Experiment010306 general physicsBeam (structure)Journal of Physics G: Nuclear and Particle Physics
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Large Time Behavior for Inhomogeneous Damped Wave Equations with Nonlinear Memory

2020

We investigate the large time behavior for the inhomogeneous damped wave equation with nonlinear memory ϕtt(t,&omega

PhysicsPhysics and Astronomy (miscellaneous)General MathematicsNonlinear memoryWeak solutionlcsh:Mathematics010102 general mathematicsnonexistence resultglobal weak solutionDamped wavenonlinear memorylcsh:QA1-93901 natural sciencesinhomogeneous term010101 applied mathematicsChemistry (miscellaneous)Settore MAT/05 - Analisi MatematicaComputer Science (miscellaneous)damped wave equation0101 mathematicsMathematical physicsSymmetry
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Interpolating between low and high energy QCD via a 5D Yang-Mills model

2005

We describe the Goldstone bosons of massless QCD together with an infinite number of spin-1 mesons. The field content of the model is SU(Nf)xSU(Nf) Yang-Mills in a compact extra-dimension. Electroweak interactions reside on one brane. Breaking of chiral symmetry occurs due to the boundary conditions on the other brane, away from our world, and is therefore spontaneous. Our implementation of the holographic recipe maintains chiral symmetry explicit throughout. For intermediate energies, we extract resonance couplings. These satisfy sum rules due to the 5D nature of the model. These sum rules imply, when taking the high energy limit, that perturbative QCD constraints are satisfied. We also il…

PhysicsQuantum chromodynamicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesYang–Mills existence and mass gapMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Goldstone bosonBraneMathematical physics
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An existence result for a Neumann problem

2015

The main result of this paper deals with the existence of at least one positive solution for a second order Neumann boundary value problem. Such a result is obtained by using an abstract coincidence point theorem that allows to get our conclusion under non standard conditions on the nonlinearity.

Positive solutionSecond-order Neumann problemApplied MathematicsAnalysiFixed pointExistence resultCoincidence pointDiscrete Mathematics and Combinatoric
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