Search results for "RESONANCES"

showing 10 items of 67 documents

Structure of pion photoproduction amplitudes

2018

We derive and apply the finite energy sum rules to pion photoproduction. We evaluate the low energy part of the sum rules using several state-of-the-art models. We show how the differences in the low energy side of the sum rules might originate from different quantum number assignments of baryon resonances. We interpret the observed features in the low energy side of the sum rules with the expectation from Regge theory. Finally, we present a model, in terms of a Regge-pole expansion, that matches the sum rules and the high-energy observables.

Particle physicsStructure (category theory)FOS: Physical sciences01 natural sciencesPOLARIZED PHOTONSCHARGED PIONSPionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesT DISPERSION-RELATIONSPhysics and Astronomy (miscellaneous); high energy; pion photoproduction010306 general physicsCOMPTON-SCATTERINGPhysicsREGGE-POLES010308 nuclear & particles physicsObservablePI0 PHOTOPRODUCTIONQuantum numberBaryonRegge theoryHigh Energy Physics - PhenomenologyAmplitudeBARYON RESONANCESPhysics and AstronomyPI-0 PHOTOPRODUCTIONMESON PHOTOPRODUCTIONENERGY SUM-RULESEnergy (signal processing)
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Studies of Inelastic Scattering of Fast Heavy Ions

2003

In the present experiment 250A MeV O-17 ions were melastically scattered front xenon and argon in the cluster-jet target of the CELSIUS storage ring. The magnetic lattice of the ring is such that the quadrant following the target can be used as a magnetic spectrometer with an acceptance cone of +/-0.6degrees, centred at 0degrees. A focal plane telescope, placed in the injection straight section. determined the excitation energy of the residual target nuclei. Data were taken for excitation energies between 15 and 35 MeV. The neutron decay was studied by the EDEN detector array positioned around the target, covering an angular range of 7-110degrees. In order to investigate a previously observ…

PhysicsArgonNUCLEISpectrometerchemistry.chemical_elementInelastic scatteringCondensed Matter PhysicsAtomic and Molecular Physics and OpticsNeutron temperatureNuclear physicsXenonchemistryNeutronAtomic physicsNuclear ExperimentRESONANCESMathematical PhysicsExcitationStorage ringPhysica Scripta
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Vacuum field correlations and three-body Casimir-Polder potential with one excited atom

2004

The three-body Casimir-Polder potential between one excited and two ground-state atoms is evaluated. A physical model based on the dressed field correlations of vacuum fluctuations is used, generalizing a model previously introduced for three ground-state atoms. Although the three-body potential with one excited atom is already known in the literature, our model gives new insights on the nature of non-additive Casimir-Polder forces with one or more excited atoms.

PhysicsCondensed Matter::Quantum GasesQuantum PhysicsField (physics)resonancesdispersion forceFOS: Physical sciencesAtomic and Molecular Physics and OpticsCasimir effectExcited statePhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsAtomic physicsVacuum fluctuationQuantum Physics (quant-ph)Quantum fluctuation
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A finite difference time domain model for the Titan ionosphere Schumann resonances

2007

[1] This paper presents a numerical approach to model the electrical properties of Titan's atmosphere. The finite difference time domain technique is applied to model the atmosphere of Saturn's satellite in order to determine Schumann resonant frequencies and electromagnetic field distributions at the extremely low frequency range. Spherical coordinates are employed, and periodic boundary conditions are implemented in order to exploit the symmetry in rotation of the celestial body. Results are compared with a previous model using the transmission line matrix method up to 180 km altitude. For the first time a numerical FDTD model up to 800 km altitude is carried out, and we report lower freq…

PhysicsMeteorologySchumann resonancesFinite-difference time-domain methodSpherical coordinate systemTransmission-line matrix methodCondensed Matter PhysicsComputational physicssymbols.namesakePhysics::Space PhysicssymbolsGeneral Earth and Planetary SciencesPeriodic boundary conditionsExtremely low frequencyAstrophysics::Earth and Planetary AstrophysicsElectrical and Electronic EngineeringIonosphereTitan (rocket family)Radio Science
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Nuclear symmetry energy and neutron skins derived from pygmy dipole resonances

2007

By exploiting Coulomb dissociation of high-energy radioactive beams of the neutron-rich nuclei $^{129\ensuremath{-}132}\mathrm{Sn}$ and $^{133,134}\mathrm{Sb}$, their dipole-strength distributions have been measured. A sizable fraction of ``pygmy'' dipole strength, energetically located below the giant dipole resonance, is observed in all of these nuclei. A comparison with available pygmy resonance data in stable nuclei ($^{208}\mathrm{Pb}$ and $N=82$ isotones) indicates a trend of strength increasing with the proton-to-neutron asymmetry. On theoretical grounds, employing the RQRPA approach, a one-to-one correlation is found between the pygmy strength and parameters describing the density d…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryHadronNuclear structureElementary particlereactions induced by unstable nucleiCoulomb excitation01 natural sciencesNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Dipole0103 physical sciencesIsotopes of tinNeutronAtomic physicsCoulomb excitation by heavy ionsNuclear Experiment010306 general physicsNucleonnuclear giant resonancesPhysical Review C
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Predictions for η→ηπ+π− producing f0(500), f0(980) and a0(980)

2017

Abstract We perform calculations for the η c → η π + π − decay using elements of SU(3) symmetry to see the weight of different trios of pseudoscalars produced in this decay, prior to the final state interaction of the mesons. After that, the interaction of pairs of mesons, leading finally to η π + π − , is done using the chiral unitary approach. We evaluate the π + π − and πη mass distributions and find large and clear signals for f 0 ( 500 ) , f 0 ( 980 ) and a 0 ( 980 ) excitation. The reaction is similar to the χ c 1 → η π + π − , which has been recently measured at BESIII and its implementation and comparison with these predictions will be very valuable to shed light on the nature of th…

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsScalar (mathematics)Scalar meson statesState (functional analysis)01 natural scienceslcsh:QC1-999Symmetry (physics)Dynamically generated resonances0103 physical sciencesCharmonium decays010306 general physicsLow Masslcsh:PhysicsExcitationPhysics Letters B
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Pole positions and residues from pion photoproduction using the Laurent-Pietarinen expansion method

2014

We have applied a new approach to determine the pole positions and residues from pion photoproduction multipoles. The method is based on a Laurent expansion of the partial wave T-matrices, with a Pietarinen series representing the regular part of energy-dependent and single-energy photoproduction solutions. The method has been applied to multipole fits generated by the MAID and GWU/SAID groups. We show that the number and properties of poles extracted from photoproduction data correspond very well to results from $\pi$N elastic data and values cited by Particle Data Group (PDG). The photoproduction residues provide new information for the electromagnetic current at the pole position, which …

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theorybaryon resonances ; poles ; Laurent+Pietarinen expansionSeries (mathematics)Laurent seriesNuclear TheoryFOS: Physical sciencesParticle Data GroupNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionAmplitudePosition (vector)High Energy Physics::ExperimentNuclear ExperimentNucleonMultipole expansionPhysical Review C
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V P gamma radiative decay of resonances dynamically generated from the vector meson-vector meson interaction

2010

We evaluate the radiative decay into a vector, a pseudoscalar and a photon of several resonances dynamically generated from the vector-vector interaction. The process proceeds via the decay of one of the vector components into a pseudoscalar and a photon, which have an invariant mass distribution very different from phase space as a consequence of the two vector structure of the resonances. Experimental work along these lines should provide useful information on the nature of these resonances.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonMass distribution010308 nuclear & particles physicsFísicaResonanceLocal hidden gauge01 natural sciencesDynamically generated resonancesPseudoscalarHigh Energy Physics - PhenomenologyDistribution (mathematics)Phase spaceQuantum electrodynamics0103 physical sciencesInvariant massVector meson010306 general physicsVector mesonsRadiative decays
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Axial resonances in the open and hidden charm sectors

2007

13 pages, 2 figures.-- PACS nrs.: 11.10.St, 11.80.Gw, 12.39.Hg, 12.39.Fe.-- ISI Article Identifier: 000249271600001.-- ArXiv pre-print available at: http://arxiv.org/abs/0704.2314

PhysicsNuclear and High Energy PhysicsParticle physics[PACS] Chiral LagrangiansChiral-symmetryMeson resonancesHeavy mesons[PACS] Heavy quark effective theoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísica[PACS] Bound and unstable states; Bethe-Salpeter equationsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)[PACS] Multichannel scatteringBethe-Salpeter equationsHigh Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment[PACS] Bound and unstable states
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Invariant mass spectrum and α-n correlation function studied in the fragmentation of 6He on a carbon target

1998

13 pags, 5 figures.-- PACS nrs.: 24.60.−t; 25.70.Ef; 27.20.+n.

PhysicsNuclear and High Energy PhysicsReaction mechanismMomentum distributionsBreakupSpectral lineIon[PACS] Reactions induced by unstable nucleiBreakup reactions6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)Halo nucleiFragmentation mechanism[PACS] ResonancesSecondary radioactive beamsInvariant massNeutronHe-5He-6Invariant mass spectra[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physicsGround stateExotic nucleiNuclear Physics A
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