Search results for "High Energy Physics::Theory"

showing 10 items of 291 documents

Finite Braid Groups for the SU(2) Knizhnik Zamolodchikov Equation

1995

We consider the monodromy representations of the mapping class group B 4 of the 2-sphere with 4 punctures acting in the solutions space of the zu(2) Knizhnik-Zamolodchikov equation [3] (note that the monodromy representations of the braid group have a more general geometric definition [4]).

AlgebraHigh Energy Physics::TheoryMonodromyMathematics::Quantum AlgebraBraid groupSpace (mathematics)Special unitary groupMapping class groupMathematicsKnizhnik–Zamolodchikov equations
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Simple connections between generalized hypergeometric series and dilogarithms

1997

AbstractConnections between generalized hypergeometric series and dilogarithms are investigated. Some simple relations of an Appell's function and dilogarithms are found.

Appell functionDilogarithmBasic hypergeometric seriesConfluent hypergeometric functionAppell seriesBilateral hypergeometric seriesApplied MathematicsMathematics::Classical Analysis and ODEsGeneralized hypergeometric functionMathematics::Geometric TopologyHypergeometric seriesAlgebraHigh Energy Physics::TheoryComputational MathematicsHypergeometric identityMathematics::K-Theory and HomologyMathematics::Quantum AlgebraLauricella hypergeometric seriesHypergeometric functionMathematicsJournal of Computational and Applied Mathematics
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Free Fields for Chiral 2D Dilaton Gravity

1998

We give an explicit canonical transformation which transforms a generic chiral 2D dilaton gravity model into a free field theory.

AstrofísicaPhysicsGravitacióNuclear and High Energy PhysicsGravity (chemistry)Canonical quantizationHigh Energy Physics::LatticeFOS: Physical sciencesCanonical transformationGeneral Relativity and Quantum Cosmology (gr-qc)Free fieldGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheoryGeneral Relativity and Quantum CosmologyGravity model of tradeQuantum gravityDilatonMathematical physics
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Chiral anomalies in even and odd dimensions

1985

Odd dimensional Yang-Mills theories with an extra ‘topological mass” term, defined by the Chern-Simons secondary characteristic, are discussed. It is shown in detail how the topological mass affects the equal time charge commutation relations and how the modified commutation relations are related to non-abelian chiral anomalies in even dimensions. We also study the SU(3) chiral model (Wess-Zumino model) in four dimensions and we show how a gauge invariant interaction with an external SU(3) vector potential can be defined with the help of the Chern-Simons characteristic in five dimensions.

Chiral anomalyPhysicsHigh Energy Physics::Lattice53C80Statistical and Nonlinear PhysicsCharge (physics)Gauge (firearms)58G25Wess–Zumino modelHigh Energy Physics::TheoryChiral modelInvariant (mathematics)81E20Mathematical PhysicsGauge anomalyMathematical physicsVector potential
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Structure of Kac-Moody groups

2008

For a phys ic i s t , a Kac-Moody algebra is the current algebra of a quantum f i e l d theory model in I + I space-time dimensions with an in terna l symmetry group G [ I ] . A More p rec ise ly , l e t ~ be the Lie algebra of G . The Kac-Moody algebra g is a one-dimensional central extension of the loop algebra Map(S I , g ) . I f f l ' f2 C Map(S I ,~ ) , then the commutator is defined point -wise,

CombinatoricsPhysicsHigh Energy Physics::TheoryCommutatorLoop algebraLine bundleMathematics::Quantum AlgebraLoop groupLie algebraStructure (category theory)Current algebraSymmetry groupMathematics::Representation Theory
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New expressions for string loop amplitudes leading to an ultrasimple conception of string dynamics

1991

New expressions are derived for string loop amplitudes as overlap integrals of string wave functionals. They are shown to take the form of exchange terms coming from the Bose-Einstein symmetrization between string segments. One is thus led to the ultrasimple conception that string theory is basically free, and that ``string interactions'' are merely due to the fact that strings are composite objects with Bose-Einstein segments as constituents.

Condensed Matter::Quantum GasesPhysicsFísicaString field theoryType I string theoryString theoryRelationship between string theory and quantum field theoryHigh Energy Physics::TheoryDomain wall (string theory)Non-critical string theoryClassical mechanicsSymmetrizationString dualityPhysical Review D
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Interference-assisted resonant detection of axions

2018

Detection schemes for the quantum chromodynamics axions and other axion-like particles in light-shining-through-a-wall (LSW) experiments are based on the conversion of these particles into photons in a magnetic field. An alternative scheme may involve the detection via a resonant atomic or molecular transition induced by resonant axion absorption. The signal obtained in this process is second order in the axion-electron interaction constant but may become first order if we allow interference between the axion-induced transition amplitude and the transition amplitude induced by the electromagnetic radiation that produces the axions.

Cosmology and Nongalactic Astrophysics (astro-ph.CO)PhotonAtomic Physics (physics.atom-ph)Physics::Instrumentation and DetectorsFOS: Physical sciencesInterference (wave propagation)01 natural sciencesSignalElectromagnetic radiationPhysics - Atomic PhysicsHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesAbsorption (electromagnetic radiation)010303 astronomy & astrophysicsAxionPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyAstronomy and AstrophysicsComputational physicsMagnetic fieldHigh Energy Physics - PhenomenologyAmplitudeSpace and Planetary ScienceAstrophysics - Cosmology and Nongalactic AstrophysicsPhysics of the Dark Universe
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Axion star nucleation in dark minihalos around primordial black holes

2020

We consider a general class of axion models, including the QCD and string axion, in which the PQ symmetry is broken before or during inflation. Assuming the axion is the dominant component of the dark matter, we discuss axion star formation in virialized dark minihalos around primordial black holes through gravitational Bose-Einstein condensation. We determine the conditions for minihalos to kinetically produce axion stars before galaxy formation. Today, we expect up to $\sim 10^{17}$ ($\sim 10^9$) axion stars in a radius of 100 parsecs around the Sun for the case of the QCD (string) axion.

Cosmology and Nongalactic Astrophysics (astro-ph.CO)Physics::Instrumentation and DetectorsDark matterFOS: Physical sciencesmustat aukotPrimordial black holeGeneral Relativity and Quantum Cosmology (gr-qc)Astrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicshiukkasfysiikka01 natural sciencesGeneral Relativity and Quantum CosmologyGravitationHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesGalaxy formation and evolution010306 general physicsAxionAstrophysics::Galaxy AstrophysicsPhysicsInflation (cosmology)010308 nuclear & particles physicsStar formationHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyStarsydinfysiikkaAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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Radio signatures from encounters between Neutron Stars and QCD-Axion Minihalos around Primordial Black Holes

2021

Probing the QCD axion dark matter (DM) hypothesis is extremely challenging as the axion interacts very weakly with Standard Model particles. We propose a new avenue to test the QCD axion DM via transient radio signatures coming from encounters between neutron stars (NSs) and axion minihalos around primordial black holes (PBHs). We consider a general QCD axion scenario in which the PQ symmetry breaking occurs before (or during) inflation coexisting with a small fraction of DM in the form of PBHs. The PBHs will unavoidably acquire around them axion minihalos with the typical length scale of parsecs. The axion density in the minihalos may be much higher than the local DM density, and the prese…

Cosmology and Nongalactic Astrophysics (astro-ph.CO)Physics::Instrumentation and DetectorsMilky WayAstrophysics::High Energy Astrophysical PhenomenaDark matterFOS: Physical sciencesPrimordial black holeAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyRadio telescopeHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010303 astronomy & astrophysicsAxionPhysicsQuantum chromodynamicsHigh Energy Astrophysical Phenomena (astro-ph.HE)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyAstronomy and AstrophysicsAstrophysics - Astrophysics of GalaxiesGalaxyHigh Energy Physics - PhenomenologyNeutron star13. Climate actionAstrophysics of Galaxies (astro-ph.GA)Astrophysics - High Energy Astrophysical PhenomenaAstrophysics - Cosmology and Nongalactic Astrophysics
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Small neutrino masses and gauge coupling unification

2014

The physics responsible for gauge coupling unification may also induce small neutrino masses. We propose a novel gauge mediated radiative seesaw mechanism for calculable neutrino masses. These arise from quantum corrections mediated by new $SU(3)_c \times SU(2)_L \times U(1)_X$ (3-3-1) gauge bosons and the physics driving gauge coupling unification. Gauge couplings unify for a 3-3-1 scale in the TeV range, making the model directly testable at the LHC.

CouplingPhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaYang–Mills theoryGauge (firearms)High Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSupersymmetric gauge theoryNeutrinoGauge anomaly
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