Search results for "scattering [hadron hadron]"

showing 10 items of 232 documents

Multi-hadron spectroscopy in a large physical volume

2017

We demonstrate the efficacy of the stochastic LapH method to treat all-to-all quark propagation on a $N_f = 2+1$ CLS ensemble with large linear spatial extent $L = 5.5$ fm, allowing us to obtain the benchmark elastic isovector p-wave pion-pion scattering amplitude to good precision already on a relatively small number of gauge configurations. These results hold promise for multi-hadron spectroscopy at close-to-physical pion mass with exponential finite-volume effects under control.

PhysicsQuarkParticle physicsIsovector010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::LatticeComputer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryFOS: Physical sciencesGauge (firearms)01 natural sciencesExponential functionScattering amplitudeHigh Energy Physics - LatticePionHadron spectroscopy0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsSpectroscopyEPJ Web of Conferences
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Exotic hyperons: Theoretical status and search perspectives in hyperon beam facilities

1992

The theoretical models that predict the existence of exotic hyperons made of more than three quarks are reviewed. We present the properties of exotic hyperons with strangenessS=−1 (quark contents $$sqqq\bar q$$ ),S=−2 ( $$ssqq\bar q$$ ) andS=−3 ( $$sssq\bar q$$ ) predicted by the sum rules for reggeon-particle scattering amplitudes. The inclusive cross sections for the production of these hyperons in hyperon-proton interactions are calculated. The cross sections turn out to be of the order of millibarns, thus opening a good perspective to encounter such exotic hyperons in the available hyperon beam facilities at CERN and FNAL. We also propose to study the Regge trajectories corresponding to…

PhysicsQuarkParticle physicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)MesonBar (music)Nuclear TheoryHigh Energy Physics::PhenomenologyTheoretical modelsHyperonNuclear physicsScattering amplitudeHigh Energy Physics::ExperimentNuclear ExperimentEngineering (miscellaneous)Beam (structure)Zeitschrift f�r Physik C Particles and Fields
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Infrared singularities of scattering amplitudes in perturbative QCD

2009

An exact formula is derived for the infrared singularities of dimensionally regularized scattering amplitudes in massless QCD with an arbitrary number of legs, valid at any number of loops. It is based on the conjecture that the anomalous-dimension matrix of n-jet operators in soft-collinear effective theory contains only a single non-trivial color structure, whose coefficient is the cusp anomalous dimension of Wilson loops with light-like segments. Its color-diagonal part is characterized by two anomalous dimensions, which are extracted to three-loop order from known perturbative results for the quark and gluon form factors. This allows us to predict the three-loop coefficients of all 1/ep…

PhysicsQuarkQuantum chromodynamicsHigh Energy Physics - TheoryHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyPerturbative QCDFOS: Physical sciencesJet (particle physics)Massless particleScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Soft-collinear effective theoryHigh Energy Physics - Theory (hep-th)Quantum mechanicsEffective field theoryHigh Energy Physics::ExperimentMathematical physics
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The Crossing Symmetric Bethe-Salpeter Equation

1972

As you may recall from the lectures of Prof. Sand-has [1], in non-relativistic quantum theory,the scattering amplitude satisfies the Lippmann-Schwinger equation, $$T = V + V{G_o}T$$ (1) It can be explicitly shown that if V=V+, T satisfies the elastic unitarity relation, Im T=TT+.

PhysicsScattering amplitudeBethe–Salpeter equationUnitarityQuantum mechanicsCrossingQuantum gravity
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Low Energy Behaviour of the Phase Shifts for Velocity-Dependent Potentials

1973

PhysicsScattering amplitudeElastic scatteringLow energyPhysics and Astronomy (miscellaneous)Phonon scatteringPhase (waves)Scattering lengthInelastic scatteringAtomic physicsProgress of Theoretical Physics
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Study of thepd→pdηreaction

2007

A study of the pd{yields}pd{eta} reaction in the energy range where the recent data from Uppsala are available is done in the two-step model of {eta} production including the final state interaction. The {eta}-d final state interaction is incorporated through the solution of the Lippmann Schwinger equation using an elastic scattering matrix element, T{sub {eta}}{sub d{yields}}{sub {eta}}{sub d}, which is required to be half off-shell. It is written in a factorized form, with an off-shell form factor multiplying an on-shell part given by an effective range expansion up to the fourth power in momentum. The parameters of this expansion have been taken from an existing recent relativistic Fadde…

PhysicsScattering amplitudeElastic scatteringNuclear and High Energy PhysicsFaddeev equationsFourth powerQuantum electrodynamicsForm factor (quantum field theory)InverseProduction (computer science)Atomic physicsNuclear ExperimentEnergy (signal processing)Physical Review C
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Description of thef2(1270),ρ3(1690),f4(2050),ρ5(2350), andf6(2510)resonances as multi-ρ(770)states

2010

In a previous work regarding the interaction of two $\ensuremath{\rho}(770)$ resonances, the ${f}_{2}(1270)$ (${J}^{PC}={2}^{++}$) resonance was obtained dynamically as a two-$\ensuremath{\rho}$ molecule with a very strong binding energy, 135 MeV per $\ensuremath{\rho}$ particle. In the present work we use the $\ensuremath{\rho}\ensuremath{\rho}$ interaction in spin 2 and isospin 0 channel to show that the resonances ${\ensuremath{\rho}}_{3}(1690)$ (${3}^{--}$), ${f}_{4}(2050)$ (${4}^{++}$), ${\ensuremath{\rho}}_{5}(2350)$ (${5}^{--}$), and ${f}_{6}(2510)$ (${6}^{++}$) are basically molecules of increasing number of $\ensuremath{\rho}(770)$ particles. We use the fixed center approximation o…

PhysicsScattering amplitudeNuclear and High Energy PhysicsFaddeev equationsParticle physicsMesonIsospinBinding energyCenter (category theory)Energy (signal processing)Spin-½Physical Review D
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Scattering of unstable particles in a finite volume: The case ofπρscattering and thea1(1260)resonance

2012

We present a way to evaluate the scattering of unstable particles quantized in a finite volume with the aim of extracting physical observables for infinite volume from lattice data. We illustrate the method with the $\ensuremath{\pi}\ensuremath{\rho}$ scattering which generates dynamically the axial-vector ${a}_{1}(1260)$ resonance. Energy levels in a finite box are evaluated both considering the $\ensuremath{\rho}$ as a stable and unstable resonance and we find significant differences between both cases. We discuss how to solve the problem to get the physical scattering amplitudes in the infinite volume, and hence phase shifts, from possible lattice results on energy levels quantized insid…

PhysicsScattering amplitudeNuclear and High Energy PhysicsFinite volume methodBethe–Salpeter equationScatteringLattice gauge theoryQuantum mechanicsLattice (order)Phase (waves)ObservablePhysical Review D
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Expressing the three-particle finite-volume spectrum in terms of the three-to-three scattering amplitude

2015

In this article we complete our formalism relating the finite-volume energy spectrum of a scalar quantum field theory to the three-to-three scattering amplitude, ${\cal M}_3$. In previous work we found a quantization condition relating the spectrum to a non-standard infinite-volume quantity, denoted ${\cal K}_{{\rm df},3}$. Here we present the relation between ${\cal K}_{{\rm df},3}$ and ${\cal M}_3$. We then discuss briefly how our now completed formalism can be practically implemented to extract ${\cal M}_3$ from the finite-volume energy spectrum.

PhysicsScattering amplitudeNuclear and High Energy PhysicsFormalism (philosophy of mathematics)Quantization (physics)Finite volume methodHigh Energy Physics - LatticeQuantum mechanicsHigh Energy Physics - Lattice (hep-lat)Energy spectrumFOS: Physical sciencesQuantum field theory
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Inverse amplitude method in pi pi scattering in chiral perturbation theory to two loops

2002

The inverse amplitude method is used to unitarize the two loop $\pi\pi$ scattering amplitudes of SU(2) Chiral Perturbation Theory in the $I=0,J=0$, $I=1,J=1$ and $I=2,J=0$ channels. An error analysis in terms of the low energy one-loop parameters $\bar l_{1,2,3,4,}$ and existing experimental data is undertaken. A comparison to standard resonance saturation values for the two loop coefficients $\bar b_{1,2,3,4,5,6} $ is also carried out. Crossing violations are quantified and the convergence of the expansion is discussed.

PhysicsScattering amplitudeNuclear and High Energy PhysicsHigh Energy Physics - PhenomenologyChiral perturbation theoryAmplitudeScatteringQuantum mechanicsPartial wave analysisSaturation (graph theory)InverseFísicaResonance (particle physics)
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