Search results for "Particle physics"

showing 10 items of 6826 documents

Large-NCproperties of theρandf0(600)mesons from unitary resonance chiral dynamics

2011

We construct $\ensuremath{\pi}\ensuremath{\pi}$ amplitudes that fulfill exact elastic unitarity, account for one-loop chiral perturbation theory contributions and include all $1/{N}_{C}$ leading terms, with the only limitation of considering just the lowest-lying nonet of exchanged resonances. Within such a scheme, the ${N}_{C}$ dependence of $\ensuremath{\sigma}$ and $\ensuremath{\rho}$ masses and widths is discussed. Robust conclusions are drawn in the case of the $\ensuremath{\rho}$ resonance, confirming that it is a stable meson in the limit of a large number of QCD colors, ${N}_{C}$. Less definitive conclusions are reached in the scalar-isoscalar sector. With the present quality of dat…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryUnitarityMeson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronElementary particleFermion01 natural sciences0103 physical sciences010306 general physicsPhysical Review D
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QCD isospin breaking in meson masses, decay constants and quark mass ratios

2001

The procedure to calculate masses and matrix-elements in the presence of mixing of the basis states is explained in detail. We then apply this procedure to the two-loop calculation in Chiral Perturbation Theory of pseudoscalar masses and decay constants including quark mass isospin breaking. These results are used to update our analysis of $K_{\ell4}$ done previously and obtain a value of $m_u/m_d$ in addition to values for the low-energy-constants $L_i^r$.

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theory[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]MesonBasis (linear algebra)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Isospin0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsMixing (physics)
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Nucleon and delta masses in QCD

1992

Using the positivity of the path integral measure of $QCD$ and defining a structure for the quark propagator in a background field according to the fluxon scenario for confinement, we calculate and compare the correlators for nucleon and delta. From their shape we elucidate about the origin of their mass difference, which in our simplified scenario is due to the tensor structure in the propagator. This term arises due to a dynamical mechanism which is responsible simultaneously for confinement and spontaneous chiral symmetry breaking. Finally we discuss, by comparing the calculated correlators with the Lehmann representation, the possibility that a strong CP and/or P violation occurs as a c…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsField (physics)PropagatorFOS: Physical sciencesCromodinàmica quànticaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Violació CP (Física nuclear)Path integral formulationTensorChiral symmetry breakingNucleon
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Δ-baryon electromagnetic form factors in lattice QCD

2008

We develop techniques to calculate the four Delta electromagnetic form factors using lattice QCD, with particular emphasis on the sub-dominant electric quadrupole form factor that probes deformation of the Delta. Results are presented for pion masses down to approximately 350 MeV for three cases: quenched QCD, two flavors of dynamical Wilson quarks, and three flavors of quarks described by a mixed action combining domain wall valence quarks and dynamical staggered sea quarks. The magnetic moment of the Delta is chirally extrapolated to the physical point and the Delta charge density distributions are discussed.

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDDelta baryonBaryonHigh Energy Physics - LatticePionLattice gauge theoryHigh Energy Physics::Experiment
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Semileptonic decays of theBcmeson

2001

We study the semileptonic transitions ${B}_{c}\ensuremath{\rightarrow}{\ensuremath{\eta}}_{c},$ $J/\ensuremath{\psi},$ D, ${D}^{*},$ B, ${B}^{*},$ ${B}_{s},$ ${B}_{s}^{*}$ in the framework of a relativistic constituent quark model. We use experimental data on leptonic $J/\ensuremath{\psi}$ decay, lattice and QCD sum rule results on leptonic ${B}_{c}$ decay, and experimental data on radiative ${\ensuremath{\eta}}_{c}$ transitions to adjust the quark model parameters. We compute all form factors of the above semileptonic ${B}_{c}$ transitions and give predictions for various semileptonic ${B}_{c}$ decay modes including their $\ensuremath{\tau}$ modes when they are kinematically accessible. Th…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyQuark modelConstituent quarkBottom quarkLattice (order)High Energy Physics::ExperimentSum rule in quantum mechanicsPhysical Review D
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Quark degrees of freedom in hadronic systems

2000

Quantum Chromodynamics (QCD) is the theory of the strong interactions. We review descriptions of hadronic systems motivated by QCD, analyzing the recent controversy between gluonic and bosonic degrees of freedom under the prism of the Cheshire Cat Principle. Our analysis leads to an optimal scheme to study hadronic properties. We proceed to extend this low energy descriptions to the deep inelastic regime.

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeDegrees of freedomNuclear TheoryHadronHigh Energy Physics::PhenomenologyDegrees of freedom (physics and chemistry)FísicaConstituent quarkFOS: Physical sciencesGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyLow energyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNon-perturbativeNuclear ExperimentNucleon
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The role of the dilaton in dense skyrmion matter

2008

In this note, we report on a remarkable and surprising interplay between the omega meson and the dilaton chi in the structure of a single skyrmion as well as in the phase structure of dense skyrmion matter which may have a potentially important consequence on the properties of compact stars. In our continuing effort to understand hadronic matter at high density, we have developed a unified field theoretic formalism for dense skyrmion matter using a single Lagrangian to describe simultaneously both matter and meson fluctuations and studied in-medium properties of hadrons. The effective theory used is the Skyrme model Lagrangian gauged with the vector mesons rho and omega, implemented with th…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsNuclear TheorySkyrmionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaScale invarianceNuclear Theory (nucl-th)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Local symmetryEffective field theoryDilatonUnified field theory
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Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD

2007

We simulate two variants of quenched twisted mass QCD (tmQCD), with degenerate Wilson quarks of masses equal to or heavier than half the strange quark mass. We use Ward identities in order to measure the twist angles of the theory and thus check the quality of the tuning of mass parameters to a physics condition which stays constant as the lattice spacing is varied. Flavour symmetry breaking in tmQCD is studied in a framework of two fully twisted and two standard Wilson quark flavours, tuned to be degenerate in the continuum. Comparing pseudoscalar masses, obtained from connected quark diagrams made of tmQCD and/or standard Wilson quark propagators, we confirm that flavour symmetry breaking…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsStrange quarkHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Degenerate energy levelsLattice field theoryFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesParticle Physics - LatticePseudoscalarHigh Energy Physics - LatticeHigh Energy Physics::ExperimentSymmetry breaking
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Massive Yang-Mills model and diffractive scattering

1998

We argue that the massive Yang-Mills model of Kunimasa and Goto, Slavnov, and Cornwall, in which massive gauge vector bosons are introduced in a gauge-invariant way without resorting to the Higgs mechanism, may be useful for studying diffractive scattering of strongly interacting particles. We perform in this model explicit calculations of S-matrix elements between quark states, at tree level, one loop, and two loops, and discuss issues of renormalisability and unitarity. In particular, it is shown that the S-matrix element for quark scattering is renormalisable at one-loop order and is only logarithmically non-renormalisable at two loops. The discrepancies in the ultraviolet regime between…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsUnitarityHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGluonsymbols.namesakePomeronHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)symbolsHigh Energy Physics::ExperimentHiggs mechanismParticle Physics - PhenomenologyS-matrixBoson
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Combining heavy quark spin and local hidden gauge symmetries in the dynamical generation of hidden charm baryons

2013

We present a coupled channel unitary approach to obtain states dynamically generated from the meson-baryon interaction with hidden charm, using constraints of heavy quark spin symmetry. As a basis of states, we use (D) over barB, (D) over bar *B states, with B baryon charmed states belonging to the 20 representations of SU(4) with J(P) = 1/2(+), 3/2(+). In addition we also include the eta N-c and J/psi N states. The inclusion of these coupled channels is demanded by heavy quark spin symmetry, since in the large m(Q) limit the D and D* states are degenerate and are obtained from each other by means of a spin rotation, under which QCD is invariant. The novelty in the work is that we use dynam…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsQCD sum rulesParticle physicsChiral perturbation theoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesQCD sum-rulesBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)IsospinChiral perturbation theoryBound stateHigh Energy Physics::ExperimentSpin-½
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