Search results for "meson"

showing 10 items of 1548 documents

Quantum loops in radiative decays of the a(1) and b(1) axial-vector mesons

2007

10 pages, 4 figures.-- ISI Article Identifier: 000251895400004.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0611075

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Scalar mesonsChiral perturbation theoryFOS: Physical sciencesFísicaUnitary approach
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Scalar, axial-vector, and tensor resonances from the rho D-*, omega D-* interaction in the hidden gauge formalism

2009

13 pages, 15 figures.-- PACS nrs.: 13.75.Lb, 12.40.Vv, 12.40.Yx, 14.40.Cs.-- ArXiv pre-print available at: http://arxiv.org/abs/0903.3823

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)[PACS] Meson-meson interactions (energy ≤ 10 GeV)[PACS] Vector-meson dominanceHigh Energy Physics::Phenomenology0202 electrical engineering electronic engineering information engineeringFOS: Physical sciences[PACS] Other mesons with S=C=0 mass < 2.5 GeVFísica020206 networking & telecommunications020201 artificial intelligence & image processing02 engineering and technology[PACS] Hadron mass models and calculations
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The rho-omega splitting in constituent quark models

2009

PACS: 12.39.Jh; 14.40.-n.--ArXiv pre-print avaible at: http://arxiv.org/abs/0903.2949v1

High Energy Physics - PhenomenologyMeson spectraHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFísicaConstituent quark modelsHigh Energy Physics::Experiment
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Scalar contributions to b→c(u)τν transitions

2017

Abstract We perform a comprehensive analysis of scalar contributions in b → c τ ν transitions including the latest measurements of R ( D ( ⁎ ) ) , the q 2 differential distributions in B → D ( ⁎ ) τ ν , the τ polarization asymmetry for B → D ⁎ τ ν , and the bound derived from the total width of the B c meson. We find that scalar contributions with the simultaneous presence of both left- and right-handed couplings to quarks can explain the available data, specifically R ( D ( ⁎ ) ) together with the measured differential distributions. However, the constraints from the total B c width present a slight tension with the current data on B → D ⁎ τ ν in this scenario, preferring smaller values fo…

High Energy Physics - Phenomenology; High Energy Physics - Phenomenology; High Energy Physics - Experiment; Nuclear and High Energy PhysicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsPhysics beyond the Standard Modelmedia_common.quotation_subjectObservablePolarization (waves)01 natural sciences7. Clean energyAsymmetrylcsh:QC1-999High Energy Physics - ExperimentBaryonHigh Energy Physics - Phenomenology0103 physical sciencesCurrent vector010306 general physicslcsh:Physicsmedia_commonPhysics Letters B
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Heavy quarkonium: progress, puzzles, and opportunities

2011

A golden age for heavy quarkonium physics dawned a decade ago, initiated by the confluence of exciting advances in quantum chromodynamics (QCD) and an explosion of related experimental activity. The early years of this period were chronicled in the Quarkonium Working Group (QWG) CERN Yellow Report (YR) in 2004, which presented a comprehensive review of the status of the field at that time and provided specific recommendations for further progress. However, the broad spectrum of subsequent breakthroughs, surprises, and continuing puzzles could only be partially anticipated. Since the release of the YR, the BESII program concluded only to give birth to BESIII; the $B$-factories and CLEO-c flo…

High Energy Physics - TheoryNuclear TheoryPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeTevatronB-C MESON; QCD SUM-RULES; NUCLEUS COLLISIONSAtomic01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Broad spectrumHigh Energy Physics - Phenomenology (hep-ph)Particle and Plasma Physicseffective field theoryBatavia TEVATRON CollNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentBrookhaven RHIC CollQuantum chromodynamicsPhysicsQuantum PhysicsLarge Hadron ColliderHigh Energy Physics - Lattice (hep-lat)lattice field theoryHERAQuarkoniumNuclear & Particles PhysicsCLEOB-C MESONHigh Energy Physics - PhenomenologyDESY HERA Stordecay [quarkonium]Jefferson LabParticle physicsFOS: Physical sciencesnonrelativistic [quantum chromodynamics]DeconfinementB-factoryNuclear Theory (nucl-th)High Energy Physics - Latticescattering [heavy ion]QCD SUM-RULES0103 physical sciencesNuclearddc:530010306 general physicsEngineering (miscellaneous)Particle Physics - Phenomenologyproduction [quarkonium]BES010308 nuclear & particles physicsHigh Energy Physics::Phenomenologyplasma [quark gluon]FísicaMoleculartetraquarkHigh Energy Physics - Theory (hep-th)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]hadron spectroscopy [meson]hadron spectroscopy [quarkonium]High Energy Physics::Experimentheavy [quarkonium]NUCLEUS COLLISIONSThe European Physical Journal C
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Confinement, the gluon propagator and the interquark potential for heavy mesons

2012

The interquark static potential for heavy mesons described by a massive one-gluon exchange interaction obtained from the propagator of the truncated Dyson-Schwinger equations does not reproduced the expected Cornell potential. I show that no formulation based on a finite propagator will lead to confinement of quenched QCD. I propose a mechanism based on a singular nonperturbative coupling constant which has the virtue of giving rise to a finite gluon propagator and (almost) linear confinement. The mechanism can be slightly modified to produce the screened potentials of unquenched QCD.

High Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeFOS: Physical sciencesMechanism based01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsPhysicsCoupling constantQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyExchange interactionPropagatorGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Quark ConfinementChiral-Symmetry BreakingFísica nuclearHigh Energy Physics::ExperimentThe European Physical Journal A
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T and CPT Symmetries in Entangled Neutral Meson Systems

2011

Genuine tests of an asymmetry under T and/or CPT transformations imply the interchange between in-states and out-states. I explain a methodology to perform model-indepedent separate measurements of the three CP, T and CPT symmetry violations for transitions involving the decay of the neutral meson systems in B- and {\Phi}-factories. It makes use of the quantum-mechanical entanglement only, for which the individual state of each neutral meson is not defined before the decay of its orthogonal partner. The final proof of the independence of the three asymmetries is that no other theoretical ingredient is involved and that the event sample corresponding to each case is different from the other …

High Energy Physics - TheoryPhysicsHistoryParticle physicsMesonCPT symmetrymedia_common.quotation_subjectFOS: Physical sciencesQuantum entanglementState (functional analysis)Function (mathematics)AsymmetryOmegaComputer Science ApplicationsEducationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum gravityHigh Energy Physics::Experimentmedia_common
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Intrinsic CPT violation and decoherence for entangled neutral mesons

2005

We present a combined treatment of quantum-gravity-induced effects and intrinsic CPT violation in entangled neutral-Kaon states. Our analysis takes into consideration two types of effects: first, those associated with the loss of particle-antiparticle identity, as a result of the ill-defined nature of the CPT operator, and second, effects due to the non-unitary evolution of the Kaons in the space-time foam. By studying a variety of phi-factory observables, involving identical as well as general final states, we derive analytical expressions, to leading order in the associated CPT violating parameters, for double-decay rates and their time-integrated counterparts. Our analysis shows that the…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsQuantum decoherenceAnalytical expressionsMesonOperator (physics)FísicaFOS: Physical sciencesObservableHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Experiment (hep-ex)Combined treatmentHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum mechanicsHigh Energy Physics::Experiment
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Sum rules for light-by-light scattering

2010

We derive a set of sum rules for the light-by-light scattering and fusion: $\gamma\gamma \to all$, and verify them in lowest order QED calculations. A prominent implication of these sum rules is the superconvergence of the helicity-difference total cross-section for photon fusion, which in the hadron sector reveals an intricate cancellation between the pseudoscalar and tensor mesons. An experimental verification of superconvergence of the polarized photon fusion into hadrons is called for, but will only be possible at $e^+ e^-$ and $\gamma\gamma$ colliders with both beams polarized. We also show how the sum rules can be used to measure various contributions to the low-energy light-by-light …

High Energy Physics - TheoryPhysicsQuantum PhysicsParticle physicsPhotonNuclear TheoryMesonScatteringHadronHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyOrder (ring theory)FOS: Physical sciencesElementary particleLight scatteringNuclear physicsPseudoscalarNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum Physics (quant-ph)
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The QCD analytic effective charge and its dependence on the pion mass

2004

A new model for the QCD analytic running coupling, which incorporates the effects due to the $\pi$ meson mass, is proposed. The properties of this invariant charge in spacelike and timelike regions are examined. Its main distinctive features are a finite infrared limiting value, which depends on the pion mass, and the "plateau-like" behavior in the deep infrared domain of the timelike region.

High Energy Physics - TheoryPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsMesonInfraredHigh Energy Physics::LatticeFísicaFOS: Physical sciencesAstronomy and AstrophysicsLimitingInvariant (physics)Atomic and Molecular Physics and OpticsEffective nuclear chargeHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Dispersion relationHigh Energy Physics::ExperimentMathematics::Differential Geometry
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