Search results for "Particle physics"

showing 10 items of 6826 documents

Horizon geometry, duality and fixed scalars in six dimensions

1998

We consider the problem of extremizing the tension for BPS strings in D=6 supergravities with different number of supersymmetries. General formulae for fixed scalars and a discussion of degenerate directions is given. Quantized moduli, according to recent analysis, are supposed to be related to conformal field theories which are the boundary of three dimensional anti-de Sitter space time.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsHorizonSpace timeDegenerate energy levelsFOS: Physical sciencesBoundary (topology)Duality (optimization)FísicaField (mathematics)Conformal mapModuliGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Particle Physics - TheoryMathematical physics
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Coordinate space calculation of two- and three-loop sunrise-type diagrams, elliptic functions and truncated Bessel integral identities

2019

We integrate three-loop sunrise-type vacuum diagrams in $D_0=4$ dimensions with four different masses using configuration space techniques. The finite parts of our results are in numerical agreement with corresponding three-loop calculations in momentum space. Using some of the closed form results of the momentum space calculation we arrive at new integral identities involving truncated integrals of products of Bessel functions. For the non-degenerate finite two-loop sunrise-type vacuum diagram in $D_0=2$ dimensions we make use of the known closed form $p$-space result to express the moment of a product of three Bessel functions in terms of a sum of Claussen polylogarithms. Using results fo…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsMathematical analysisElliptic functionFOS: Physical sciencesPosition and momentum spaceLoop (topology)High Energy Physics - Phenomenologysymbols.namesakeIdentity (mathematics)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Product (mathematics)symbolslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityConfiguration spaceCoordinate spaceBessel function
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Causal representation of multi-loop Feynman integrands within the loop-tree duality

2021

The numerical evaluation of multi-loop scattering amplitudes in the Feynman representation usually requires to deal with both physical (causal) and unphysical (non-causal) singularities. The loop-tree duality (LTD) offers a powerful framework to easily characterise and distinguish these two types of singularities, and then simplify analytically the underling expressions. In this paper, we work explicitly on the dual representation of multi-loop Feynman integrals generated from three parent topologies, which we refer to as Maximal, Next-to-Maximal and Next-to-Next-to-Maximal loop topologies. In particular, we aim at expressing these dual contributions, independently of the number of loops an…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDuality (mathematics)PropagatorDual representation01 natural sciencesAlgebraHigh Energy Physics - Phenomenologysymbols.namesakeIntegerSimple (abstract algebra)Perturbative QCD0103 physical sciencessymbolslcsh:QC770-798Feynman diagramlcsh:Nuclear and particle physics. Atomic energy. RadioactivityGravitational singularityScattering Amplitudes010306 general physicsRepresentation (mathematics)Duality in Gauge Field TheoriesJournal of High Energy Physics
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Gluon mass generation in the PT-BFM scheme

2006

In this article we study the general structure and special properties of the Schwinger-Dyson equation for the gluon propagator constructed with the pinch technique, together with the question of how to obtain infrared finite solutions, associated with the generation of an effective gluon mass. Exploiting the known all-order correspondence between the pinch technique and the background field method, we demonstrate that, contrary to the standard formulation, the non-perturbative gluon self-energy is transverse order-by-order in the dressed loop expansion, and separately for gluonic and ghost contributions. We next present a comprehensive review of several subtle issues relevant to the search …

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodLorentz transformationHigh Energy Physics::LatticeMass generationHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyPropagatorFOS: Physical sciencesFísicaRenormalization groupIntegral equationMassless particleHigh Energy Physics - Phenomenologysymbols.namesakeTheoretical physicsDimensional regularizationHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)symbols
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Threshold expansion of the sunset diagram

1999

By use of the threshold expansion we develop an algorithm for analytical evaluation, within dimensional regularization, of arbitrary terms in the expansion of the (two-loop) sunset diagram with general masses m_1, m_2 and m_3 near its threshold, i.e. in any given order in the difference between the external momentum squared and its threshold value, (m_1+m_2+m_3)^2. In particular, this algorithm includes an explicit recurrence procedure to analytically calculate sunset diagrams with arbitrary integer powers of propagators at the threshold.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsDiagramMathematical analysisFOS: Physical sciencesPropagatorSunsetMomentumHigh Energy Physics - PhenomenologyDimensional regularizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)IntegerOrder (group theory)Nuclear Physics B
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Non-abelian gauge structure in neutrino mixing

2010

We discuss the existence of a non-abelian gauge structure associated with flavor mixing. In the specific case of two flavor mixing of Dirac neutrino fields, we show that this reformulation allows to define flavor neutrino states which preserve the Poincar\'e structure. Phenomenological consequences of our analysis are explored.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsDirac (video compression format)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particleLorentz covarianceMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)High Energy Physics::ExperimentGauge theoryNeutrinoNeutrino oscillationMixing (physics)
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Limits on the parameters of the equation of state for interacting dark energy

2010

Under the assumption that cold dark matter and dark energy interact with each other through a small coupling term, $Q$, we constrain the parameter space of the equation of state $w$ of those dark energy fields whose variation of the field since last scattering do not exceed Planck's mass. We use three parameterizations of $w$ and two different expressions for $Q$. Our work extends previous ones.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsEquation of stateCosmology and Nongalactic Astrophysics (astro-ph.CO)Hot dark matterScalar field dark matterFOS: Physical sciencesLambda-CDM modelAstrophysics::Cosmology and Extragalactic AstrophysicsGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyThermodynamics of the universeHigh Energy Physics - Theory (hep-th)Quantum mechanicsQuantum electrodynamicsMixed dark matterWarm dark matterDark energyLight dark matterDark fluidAstrophysics - Cosmology and Nongalactic Astrophysics
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N-quantum approach to quantum field theory at finite T and mu: the NJL model

1999

We extend the N-quantum approach to quantum field theory to finite temperature ($T$) and chemical potential ($\mu$) and apply it to the NJL model. In this approach the Heisenberg fields are expressed using the Haag expansion while temperature and chemical potential are introduced simultaneously through a generalized Bogoliubov transformation. Known mean field results are recovered using only the first term in the Haag expansion. In addition, we find that at finite T and in the broken symmetry phase of the model the mean field approximation can not diagonalize the Hamiltonian. Inclusion of scalar and axial vector diquark channels in the SU(2)$_{rm f}$ $otimes$ SU(3)$_{\rm c}$ version of the …

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryScalar (mathematics)Order (ring theory)FísicaHigh Energy Physics - Phenomenologysymbols.namesakeBogoliubov transformationVacuum energyMean field theorysymbolsQuantum field theoryHamiltonian (quantum mechanics)PseudovectorMathematical physics
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Inverse symmetry breaking and the exact renormalization group

1996

We discuss the question of inverse symmetry breaking at non-zero temperature using the exact renormalization group. We study a two-scalar theory and concentrate on the nature of the phase transition during which the symmetry is broken. We also examine the persistence of symmetry breaking at temperatures higher than the critical one.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsPhase transitionFOS: Physical sciencesInverseFísicaRenormalization groupSymmetry (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Symmetry breakingPersistence (discontinuity)Particle Physics - PhenomenologyMathematical physics
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Orientifold theory dynamics and symmetry breaking

2004

We show that it is possible to construct explicit models of electroweak symmetry breaking in which the number of techniflavors needed to enter the conformal phase of the theory is small and weakly dependent on the number of technicolors. Surprisingly, the minimal model with {\it just} two (techni)flavors, together with a suitable gauge dynamics, can be made almost conformal. The theories we consider are generalizations of orientifold type gauge theories, in which the fermions are in either two index symmetric or antisymmetric representation of the gauge group, as the underlying dynamics responsible for the spontaneous breaking of the electroweak symmetry. We first study their phase diagram,…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsSpontaneous symmetry breakingHigh Energy Physics::LatticeElectroweak interactionLattice field theoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorSupersymmetryYang–Mills theoryHigh Energy Physics - PhenomenologyExplicit symmetry breakingTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Symmetry breaking
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