Search results for "scattering [hadron]"

showing 10 items of 232 documents

Chiral Dynamics of the two Lambda(1405) States

2004

Using a chiral unitary approach for the meson--baryon interactions, we show that two octets of J^{\pi}=1/2^- baryon states, which are degenerate in the limit of exact SU(3) symmetry, and a singlet are generated dynamically. The SU(3) breaking produces the splitting of the two octets, resulting in the case of strangeness S=-1 in two poles of the scattering matrix close to the nominal \Lambda(1405) resonance. These poles are combinations of the singlet state and the octets. We show how actual experiments see just one effective resonance shape, but with properties which change from one reaction to another.

Nuclear TheoryLambda(1405)High Energy Physics::Latticeinelastic scattering [meson baryon]Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSU(3) [symmetry]singlet [baryon]symmetry breakingcoupled channelHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Phenomenologyddc:530elastic scattering [meson baryon]chiral [effective Lagrangian]numerical calculationsNuclear Experimentoctet [baryon]analytic properties [scattering amplitude]
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Transition form factors of the N(*()1535) as a dynamically generated resonance

2007

We discuss how electromagnetic properties provide useful tests of the nature of resonances, and we study these properties for the N*(1535) which appears dynamically generated from the strong interaction of mesons and baryons. Within this coupled channel chiral unitary approach, we evaluate the A_1/2 and S_1/2 helicity amplitudes as a function of Q^2 for the electromagnetic N*(1535) to gamma* N transition. Within the same formalism we evaluate the cross section for the reactions gamma N to eta N. We find a fair agreement for the absolute values of the transition amplitudes, as well as for the Q^2 dependence of the amplitudes, within theoretical and experimental uncertainties discussed in the…

Nuclear Theorydispersion relationamplitude analysis [helicity]Nuclear Theoryform factor [N(1535)]FOS: Physical sciencesscattering amplitude [meson baryon]Nuclear Theory (nucl-th)nonrelativistictransition [form factor]ddc:530higher-order [Feynman graph]ratio [channel cross section]numerical calculationsNuclear Experimentphotoproduction [eta]chiral [symmetry]effective LagrangianFísicaenergy dependence [channel cross section]coupled channelradiative decay [N(1535)]relativisticinelastic scattering [electron nucleon]inelastic scattering [photon nucleon]
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Meson Resonances at large Nc: Complex Poles vs Breit-Wigner Masses

2009

The rigorous quantum mechanical definition of a resonance requires determining the pole position in the second Riemann sheet of the analytically continued partial wave scattering amplitude in the complex Mandelstam s variable plane. For meson resonances we investigate the alternative Breit–Wigner (BW) definition within the large NC expansion. By assuming that the pole position is View the MathML source and exploiting unitarity, we show that the BW determination of the resonance mass differs from the pole position by View the MathML source terms, which can be extracted from ππ scattering data. For the case of the σ (f0(600)) pole, the BW scalar mass is predicted to occur at not, vert, simila…

Nuclear and High Energy PhysicsMesonScalar (mathematics)FOS: Physical sciences01 natural sciencesUnitarizationHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciences010306 general physicsScalar mesonChiral symmetriesScalar mesonPhysicsUnitarity010308 nuclear & particles physicsPlane (geometry)ScatteringLarge N-CResonanceFísicaScattering amplitudeHigh Energy Physics - PhenomenologyResonancesQuantum electrodynamics
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Implementing the three-particle quantization condition including higher partial waves

2019

We present an implementation of the relativistic three-particle quantization condition including both $s$- and $d$-wave two-particle channels. For this, we develop a systematic expansion about threshold of the three-particle divergence-free K matrix, $\mathcal{K}_{\mathrm{df,3}}$, which is a generalization of the effective range expansion of the two-particle K matrix, $\mathcal{K}_2$. Relativistic invariance plays an important role in this expansion. We find that $d$-wave two-particle channels enter first at quadratic order. We explain how to implement the resulting multichannel quantization condition, and present several examples of its application. We derive the leading dependence of the …

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)Relativistic invarianceFOS: Physical sciencesLattice QCD01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)Quantization (physics)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuadratic orderScattering Amplitudes010306 general physicsNuclear theoryCondensed Matter - Statistical MechanicsK matrixMathematical physicsPhysicsLattice Quantum Field TheoryStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Lattice QCDScattering amplitudeHigh Energy Physics - Phenomenologylcsh:QC770-798Journal of High Energy Physics
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Complete calculation of exclusive heavy vector meson production at next-to-leading order in the dipole picture

2022

Exclusive production of transversely polarized heavy vector mesons in deep inelastic scattering at high energy is calculated at next-to-leading order accuracy in the Color Glass Condensate framework. In addition to the first QCD correction proportional to the strong coupling constant $\alpha_s$, we systematically also include the first relativistic correction proportional to the heavy quark velocity squared $v^2$. When combined with our previously published results for longitudinal vector meson production at next-to-leading order accuracy, these results make phenomenological calculations of heavy vector meson production possible at the order $\mathcal{O}(\alpha_s v^0, \alpha_s^0 v^2)$. When…

Nuclear and High Energy PhysicsNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical scienceshiukkasfysiikka114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenologydeep inelastic scattering or small-x physicsHigh Energy Physics - Phenomenology (hep-ph)higher-order perturbative calculationskvanttiväridynamiikkaHigh Energy Physics::Experimentquarkonium
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Chiral unitary approach to eta'N scattering at low energies

2010

We study the \eta' N interaction within a chiral unitary approach which includes \pi N, \eta N and related pseudoscalar meson-baryon coupled channels. Since the SU(3) singlet does not contribute to the standard interaction and the \eta' is mostly a singlet, the resulting scattering amplitude is very small and inconsistent with experimental estimations of the \eta' N scattering length. The additional consideration of vector meson-baryon states into the coupled channel scheme, via normal and anomalous couplings of pseudoscalar to vector mesons, enhances substantially the \eta' N amplitude. We also exploit the freedom of adding to the Lagrangian a new term, allowed by the symmetries of QCD, wh…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeNuclear Theory01 natural sciencesQuantum mechanics0103 physical sciencesMesons (Nuclear physics)Mesons (Física nuclear)010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsUnitarityReaccions nuclears010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaCromodinàmica quàntica Partícules (Física nuclear)Scattering lengthBaryonPseudoscalarScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNuclear reactionsQuantum chromodynamics
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Dynamically generated resonances from the vector octet-baryon octet interaction

2010

We study the interaction of vector mesons with the octet of stable baryons in the framework of the local hidden gauge formalism using a coupled-channels unitary approach. We examine the scattering amplitudes and their poles, which can be associated to known J(P) = 1/2(-), 3/2(-) baryon resonances, in some cases, or give predictions in other ones. The formalism employed produces doublets of degenerate J(P) = 1/2(-), 3/2(-) states, a pattern which is observed experimentally in several cases. The findings of this work should also be useful to guide present experimental programs searching for new resonances, in particular in the strange sector where the current information is very poor.

Nuclear and High Energy PhysicsParticle physicsOctetMesonNuclear TheoryNuclear TheoryFOS: Physical sciences01 natural sciencesUnitary stateNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBaryonsMesons (Nuclear physics)Mesons (Física nuclear)010306 general physicsBarionsPhysicsWeak interactions (Nuclear physics)010308 nuclear & particles physicsDegenerate energy levelsHigh Energy Physics::PhenomenologyInteraccions febles (Física nuclear)FísicaScattering amplitudeBaryonFormalism (philosophy of mathematics)High Energy Physics - PhenomenologyProjecte 227431
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Study of the f(2)(1270) , f(2)'(1525) , f(0)(1370) and f(0)(1710) in the J/psi radiative decays

2009

In this paper we present an approach to study the radiative decay modes of the J/psi into a photon and one of the tensor mesons f (2)(1270) , f' (2)(1525) , as well as the scalar ones f (0)(1370) and f (0)(1710) . Especially, we compare predictions that emerge from a scheme where the states appear dynamically in the solution of vector meson-vector meson scattering amplitudes to those from a (admittedly naive) quark model. We provide evidence that it might be possible to distinguish amongst the two scenarios, once improved data are available.

Nuclear and High Energy PhysicsParticle physicsPhotonMesonScalar (mathematics)Radiative decayhadronic decay [J/psi(3100)]01 natural sciencesf0(1710)bound state [vector meson]radiative decay [J/psi(3100)]0103 physical sciencesRadiative transferddc:530f0(1370)Tensor010306 general physicsnumerical calculationsdecay modes [J/psi(3100)]Physicsquark modelf2(1525)ratio [width]010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyQuark modelFísicascalar meson3. Good healthScattering amplitudef2(1270)tensor mesonHigh Energy Physics - Phenomenologywidth [J/psi(3100)]High Energy Physics::Experiment
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s-wave pion-nucleus optical potential

2007

We calculate the s-wave part of the pion-nucleus optical potential using a unitarized chiral approach that has been previously used to simultaneously describe pionic hydrogen and deuterium data as well as low energy pi N scattering in the vacuum. This energy dependent model allows for additional isoscalar parts in the potential from multiple rescattering. We consider Pauli blocking and pion polarization in an asymmetric nuclear matter environment. Also, higher order corrections of the pi N amplitude are included. The model can accommodate the repulsion required by phenomenological fits, though the theoretical uncertainties are bigger than previously thought. At the same time, we also find a…

Nuclear and High Energy PhysicsParticle physicsscattering amplitude [pi nucleon]Nuclear Theorymedia_common.quotation_subjectIsoscalarpartial waveNuclear TheoryFOS: Physical sciencesAsymmetryrenormalizationNuclear physicsNuclear Theory (nucl-th)symbols.namesakePionPauli exclusion principlemesic atom [deuterium]unitarityddc:530higher-order [Feynman graph]nuclear reaction [pi nucleus]numerical calculationsNuclear Experimentmedia_commonPhysicschiral [symmetry]UnitarityIsovectorN(1440)FísicaNuclear mattermesic atom [hydrogen]propagator [pi]Scattering amplitudenuclear mattersymbolsoptical [potential]correction [vertex function]
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Numerical exploration of three relativistic particles in a finite volume including two-particle resonances and bound states

2019

In this work, we use an extension of the quantization condition, given in Ref. [1], to numerically explore the finite-volume spectrum of three relativistic particles, in the case that two-particle subsets are either resonant or bound. The original form of the relativistic three-particle quantization condition was derived under a technical assumption on the two-particle K matrix that required the absence of two-particle bound states or narrow two-particle resonances. Here we describe how this restriction can be lifted in a simple way using the freedom in the definition of the K-matrix-like quantity that enters the quantization condition. With this in hand, we extend previous numerical studie…

Nuclear and High Energy Physicsnucl-thNuclear TheoryAtomic Physics (physics.atom-ph)Other Fields of Physicshep-latFOS: Physical sciencesLattice QCDphysics.atom-ph01 natural sciencesPhysics - Atomic PhysicsRelativistic particleNuclear Theory (nucl-th)Quantization (physics)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. Radioactivitycond-mat.stat-mech010306 general physicsScattering AmplitudesCondensed Matter - Statistical MechanicsParticle Physics - PhenomenologyPhysicsFinite volume methodStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsScatteringHigh Energy Physics - Lattice (hep-lat)hep-phParticle Physics - LatticeLattice QCDScattering amplitudeHigh Energy Physics - PhenomenologyAmplitudeNuclear Physics - Theorylcsh:QC770-798
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