Search results for "Particle Physics - Theory"

showing 10 items of 48 documents

The role of resonances in chiral perturbation theory

1989

32 páginas, 2 figuras, 5 tablas.-- BUTP-88-18 ; CERN-TH-5185-88 ; CPT-2158 ; UWTHPH-1988-29.

Chiral anomalyPhysicsNuclear and High Energy PhysicsChiral perturbation theoryMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFísicaVector meson dominancePseudoscalar mesonPionQuantum electrodynamicsNambu–Jona-Lasinio modelHigh Energy Physics::ExperimentChiral symmetry breakingParticle Physics - Theory
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Non-Leptonic Kaon Decays and the Chiral Anomaly

1994

32 páginas, 3 figuras, 4 tablas.-- El PDF es el artículo publicado en el CERN en Junio de 1993.

Chiral anomalyPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaPhoton energyHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)Radiative transferHigh Energy Physics::ExperimentPhenomenology (particle physics)Particle Physics - Theory
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Unitarity and K$_{L}$ --> $\pi^{0}\gamma\gamma$

1993

We discuss the rare decay K(L) --> pi0gammagamma. Although the recently measured 2gamma-invariant-mass distribution is in quite good agreement with the lowest-order chiral perturbation theory prediction, there seems to be a discrepancy with the calculated branching ratio. We extend the previous computations to next-to-leading order, O(p6). The two dominant mechanisms at this order are emphasized: the two-pion intermediate state and vector meson exchange.

FísicaHigh Energy Physics::ExperimentParticle Physics - Theory
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Real symplectic formulation of local special geometry

2006

We consider a formulation of local special geometry in terms of Darboux special coordinates $P^I=(p^i,q_i)$, $I=1,...,2n$. A general formula for the metric is obtained which is manifestly $\mathbf{Sp}(2n,\mathbb{R})$ covariant. Unlike the rigid case the metric is not given by the Hessian of the real function $S(P)$ which is the Legendre transform of the imaginary part of the holomorphic prepotential. Rather it is given by an expression that contains $S$, its Hessian and the conjugate momenta $S_I=\frac{\partial S}{\partial P^I}$. Only in the one-dimensional case ($n=1$) is the real (two-dimensional) metric proportional to the Hessian with an appropriate conformal factor.

High Energy Physics - TheoryHessian matrixPhysicsPure mathematicsNuclear and High Energy PhysicsHolomorphic functionFOS: Physical sciencesLegendre functionLegendre transformationsymbols.namesakeAssociated Legendre polynomialsHigh Energy Physics - Theory (hep-th)Real-valued functionMetric (mathematics)symbolsParticle Physics - TheorySymplectic geometryPhysics Letters B
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Swampland Bounds on the Abelian Gauge Sector

2019

We derive bounds on the number of abelian gauge group factors in six-dimensional gravitational theories with minimal supersymmetry and in their F-theoretic realisations. These bounds follow by requiring consistency of certain BPS strings in the spectrum of the theory, as recently proposed in the literature. Under certain assumptions this approach constrains the number of abelian gauge group factors in six-dimensional supergravity theories with at least one tensor multiplet to be $N \leq 20$ (or $N \leq 22$ in absence of charged matter). For any geometric F-theory realisation with at least one tensor multiplet we establish the bound $N \leq 16$ by demanding unitarity of a heterotic solitonic…

High Energy Physics - TheoryHeterotic string theoryPhysics010308 nuclear & particles physicsSupergravityhep-thFibered knotFOS: Physical sciencesSupersymmetry01 natural sciencesString (physics)High Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Gauge group0103 physical sciencesAbelian group010306 general physicsMultipletParticle Physics - TheoryMathematical physics
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On the Embedding of Space-Time Symmetries into Simple Superalgebras

2001

We explore the embedding of Spin groups of arbitrary dimension and signature into simple superalgebras in the case of extended supersymmetry. The R-symmetry, which generically is not compact, can be chosen compact for all the cases that are congruent mod 8 to the physical conformal algebra so($D-2$,2), $D\geq 3$. An $\rm{so}(1,1)$ grading of the superalgebra is found in all cases. Central extensions of super translation algebras are studied in this framework.

High Energy Physics - TheoryHigh Energy Physics - Theory (hep-th)FOS: Physical sciencesÀlgebraLie Grups deParticle Physics - Theory
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Quantum transport and the phase space structure of the Wightman functions

2019

We study the phase space structure of exact quantum Wightman functions in spatially homogeneous, temporally varying systems. In addition to the usual mass shells, the Wightman functions display additional coherence shells around zero frequency $k_0=0$, which carry the information of the local quantum coherence of particle-antiparticle pairs. We find also other structures, which encode non-local correlations in time, and discuss their role and decoherence. We give a simple derivation of the cQPA formalism, a set of quantum transport equations, that can be used to study interacting systems including the local quantum coherence. We compute quantum currents created by a temporal change in a par…

High Energy Physics - TheoryNuclear and High Energy PhysicsAstrophysics and AstronomyLEPTOGENESISCosmology and Nongalactic Astrophysics (astro-ph.CO)Quantum decoherencegr-qcFOS: Physical sciencesSemiclassical physicsGeneral Relativity and Quantum Cosmology (gr-qc)114 Physical sciences01 natural sciencesGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityThermal Field Theory010306 general physicsQuantumELECTROWEAK BARYOGENESISParticle Physics - PhenomenologyPhysicsThermal quantum field theory010308 nuclear & particles physicsGeneral Relativity and Cosmologyhep-thhep-phFermionFERMIONSBaryogenesisHigh Energy Physics - PhenomenologyCP violationClassical mechanicsHigh Energy Physics - Theory (hep-th)Phase spaceastro-ph.COlcsh:QC770-798Quantum Dissipative SystemsParticle Physics - TheoryAstrophysics - Cosmology and Nongalactic AstrophysicsCoherence (physics)
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Implications of nonplanar dual conformal symmetry

2018

Recently, Bern et al observed that a certain class of next-to-planar Feynman integrals possess a bonus symmetry that is closely related to dual conformal symmetry. It corresponds to a projection of the latter along a certain lightlike direction. Previous studies were performed at the level of the loop integrand, and a Ward identity for the integral was formulated. We investigate the implications of the symmetry at the level of the integrated quantities. In particular, we focus on the phenomenologically important case of five-particle scattering. The symmetry simplifies the four-variable problem to a three-variable one. In the context of the recently proposed space of pentagon functions, the…

High Energy Physics - TheoryNuclear and High Energy PhysicsFunction spaceFeynman graphFOS: Physical sciencesanomalyContext (language use)Ward identitySpace (mathematics)Conformal and W Symmetry01 natural sciencesProjection (linear algebra)Identity (mathematics)High Energy Physics - Phenomenology (hep-ph)Conformal symmetry0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityAnomalies in Field and String Theories010306 general physicsScattering AmplitudesParticle Physics - PhenomenologyMathematical physicsPhysicsloop integral010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]hep-thscattering amplitudehep-phSymmetry (physics)Loop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)symmetry: conformalsupersymmetry: 4[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]lcsh:QC770-798dualityParticle Physics - Theoryinfrared problem
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Modular fluxes, elliptic genera, and weak gravity conjectures in four dimensions

2019

We analyse the Weak Gravity Conjecture for chiral four-dimensional F-theory compactifications with N=1 supersymmetry. Extending our previous work on nearly tensionless heterotic strings in six dimensions, we show that under certain assumptions a tower of asymptotically massless states arises in the limit of vanishing coupling of a U(1) gauge symmetry coupled to gravity. This tower contains super-extremal states whose charge-to-mass ratios are larger than those of certain extremal dilatonic Reissner-Nordstrom black holes, precisely as required by the Weak Gravity Conjecture. Unlike in six dimensions, the tower of super-extremal states does not always populate a charge sub-lattice. The main t…

High Energy Physics - TheoryNuclear and High Energy PhysicsGravity (chemistry)FOS: Physical sciencesF-TheoryTopological Strings01 natural sciencesTheoretical physicsGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheorySuperstrings and Heterotic Strings0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsGauge symmetryPhysicsHeterotic string theory010308 nuclear & particles physicshep-thCharge (physics)SupersymmetryF-theoryHigh Energy Physics - Theory (hep-th)lcsh:QC770-798String DualityMirror symmetryParticle Physics - TheoryString dualityJournal of High Energy Physics
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Limits on neutrino Lorentz violation from multimessenger observations of TXS 0506+056

2019

The observation by the IceCube Collaboration of a high-energy ($E \gtrsim 200$ TeV) neutrino from the direction of the blazar TXS 0506+056 and the coincident observations of enhanced $\gamma$-ray emissions from the same object by MAGIC and other experiments can be used to set stringent constraints on Lorentz violation in the propagation of neutrinos that is linear in the neutrino energy: $\Delta v = - E/M_1$, where $\Delta v$ is the deviation from the velocity of light, and $M_1$ is an unknown high energy scale to be constrained by experiment. Allowing for a difference in neutrino and photon propagation times of $\sim 10$ days, we find that $M_1 \gtrsim 3 \times 10^{16}$ GeV. This improves …

High Energy Physics - TheoryNuclear and High Energy PhysicsHigh energyParticle physicsAstrophysics and AstronomyCosmology and Nongalactic Astrophysics (astro-ph.CO)Lorentz transformationgr-qcAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesComputer Science::Digital LibrariesGeneral Relativity and Quantum CosmologyIceCubesymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Coincident0103 physical sciences010306 general physicsBlazarParticle Physics - PhenomenologyHigh Energy Astrophysical Phenomena (astro-ph.HE)Physicsastro-ph.HEMultimessenger010308 nuclear & particles physicsGeneral Relativity and Cosmologyhep-thHigh Energy Physics::PhenomenologyLorentz violationGamma rayhep-phlcsh:QC1-999High Energy Physics - PhenomenologyPhoton propagationHigh Energy Physics - Theory (hep-th)Astrophysical neutrinosVelocity of lightsymbolsastro-ph.COHigh Energy Physics::ExperimentNeutrinoTXS 0506+056Astrophysics - High Energy Astrophysical PhenomenaParticle Physics - Theorylcsh:PhysicsBlazarsAstrophysics - Cosmology and Nongalactic AstrophysicsPhysics Letters
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