Search results for "Bound state"

showing 10 items of 235 documents

Distribution Amplitudes of Heavy-Light Mesons

2019

A symmetry-preserving approach to the continuum bound-state problem in quantum field theory is used to calculate the masses, leptonic decay constants and light-front distribution amplitudes of empirically accessible heavy-light mesons. The inverse moment of the $B$-meson distribution is particularly important in treatments of exclusive $B$-decays using effective field theory and the factorisation formalism; and its value is therefore computed: $\lambda_B(\zeta = 2\,{\rm GeV}) = 0.54(3)\,$GeV. As an example and in anticipation of precision measurements at new-generation $B$-factories, the branching fraction for the rare $B\to \gamma(E_\gamma) \ell \nu_\ell$ radiative decay is also calculated…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaInverseFOS: Physical sciencesHeavy-light mesons01 natural sciencesParton distribution amplitudesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBound stateNonperturbative continuum methods in quantum field theoryEffective field theoryQuantum field theory010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsBranching fractionHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyB-meson decayslcsh:QC1-999High Energy Physics - PhenomenologyAmplitudeHigh Energy Physics::Experimentlcsh:PhysicsQuantum chromodynamics
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Neutral baryonic systems with strangeness

2020

We review the status as regards the existence of three- and four-body bound states made of neutrons and $\Lambda$ hyperons. For interesting cases, the coupling to neutral baryonic systems made of charged particles of different strangeness has been addressed. There are strong arguments showing that the $\Lambda nn$ system has no bound states. $\Lambda\Lambda nn$ strong stable states are not favored by our current knowledge of the strangeness $-1$ and $-2$ baryon-baryon interactions. However, a possible $\Xi^- t$ quasibound state decaying to $\Lambda\Lambda nn$ might exist in nature. Similarly, there is a broad agreement about the nonexistence of $\Lambda\Lambda n$ bound states. However, the …

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryFOS: Physical sciencesGeneral Physics and AstronomyStrangenessFew-body systems01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound stateComputer Science::General LiteratureNeutronNuclear Experiment010306 general physicsPhysics010308 nuclear & particles physicsComputer Science::Information RetrievalAstrophysics::Instrumentation and Methods for AstrophysicsHyperonComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)Charge (physics)BaryonHigh Energy Physics - PhenomenologyCoupling (physics)International Journal of Modern Physics E
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Quark-model based study of the triton binding energy

2001

The three-nucleon bound state problem is studied employing a nucleon-nucleon potential obtained from a basic quark-quark interaction in a five-channel Faddeev calculation. The obtained triton binding energy is comparable to those predicted by conventional models of the $NN$ force.

Nuclear and High Energy PhysicsParticle physicsNuclear Theorycoupled channel [partial wave analysis]Nuclear TheoryBinding energyFOS: Physical scienceselastic scattering [nucleon nucleon]Few-body systemsinteraction [quark quark]Nuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Bound stateddc:530numerical calculationsNuclear ExperimentNuclear theoryPhysicsQuark modelbinding energy [tritium]Three-body problemHigh Energy Physics - Phenomenologynonrelativistic [quark]three-body problempotential [nucleon nucleon]Physical Review C
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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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Pion-photon transition distribution amplitudes in the Nambu-Jona-Lasinio model

2007

12 pages, 6 figures.-- PACS nrs.: 13.60.-r; 11.10.St; 12.38.Lg; 24.10.Jv.-- ISI Article Identifier: 000251327200049.-- ArXiv pre-print available at: http://arxiv.org/abs/0707.3366

Nuclear and High Energy PhysicsPhotonBethe–Salpeter equationHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences[PACS] Relativistic models of nucleiPartícules (Física nuclear)PionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio modelBound stateVirtual Compton-scatteringCovariant transformation[PACS] Photon and charged-lepton interactions with hadrons[PACS] Bound and unstable statesMathematical physicsQuantum chromodynamicsPhysicsHigh Energy Physics::PhenomenologyGeneralized Parton distributions[PACS] Bound and unstable states; Bethe-Salpeter equations[PACS] Other nonperturbative calculations in QCDHigh Energy Physics - PhenomenologyAmplitudeQuantum electrodynamicsBethe-Salpeter equationsFísica nuclear
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White paper: from bound states to the continuum

2020

This white paper reports on the discussions of the 2018 Facility for Rare Isotope Beams Theory Alliance (FRIB-TA) topical program ‘From bound states to the continuum: Connecting bound state calculations with scattering and reaction theory’. One of the biggest and most important frontiers in nuclear theory today is to construct better and stronger bridges between bound state calculations and calculations in the continuum, especially scattering and reaction theory, as well as teasing out the influence of the continuum on states near threshold. This is particularly challenging as many-body structure calculations typically use a bound state basis, while reaction calculations more commonly utili…

Nuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Structure (category theory)nucleus: structure functionFew-body systems[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesMany-body problemTheoretical physicsFew-body systems0103 physical sciencesBound stateReactionsNuclear structure010306 general physicsPhysicsBasis (linear algebra)010308 nuclear & particles physicsContinuum (topology)ScatteringscatteringNuclear structurePhysique atomique et nucléairebound statefew-body problemmany-body problem
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The nuclear magnetic moment of 208Bi and its relevance for a test of bound-state strong-field QED

2018

Physics letters / B 779, 324 - 330 (2018). doi:10.1016/j.physletb.2018.02.024

Nuclear and High Energy Physicschemistry.chemical_elementHyperfine anomaly53001 natural sciencesBismuth0103 physical sciencesBound stateNuclear Physics - Experimentddc:530Physics::Atomic PhysicsLaser spectroscopy010306 general physicsSpectroscopyHyperfine structureQuantum electrodynamicsPhysicsSpecific difference010308 nuclear & particles physicsNuclear structurelcsh:QC1-999chemistryNuclear magnetic momentNuclear magnetic momentPräzisionsexperimente - Abteilung BlaumAtomic physicsAnomaly (physics)Bismuthlcsh:PhysicsOrder of magnitudePhysics Letters B
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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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Further Theoretical Analysis on the $K^{-} {}^{3} \text{He} \to \Lambda p n$ Reaction for the $\bar{K} N N$ Bound-State Search in the J-PARC E15 Expe…

2019

Based on the scenario that a $\bar{K} N N$ bound state is generated and it eventually decays into $\Lambda p$, we calculate the cross section of the $K^{-} {}^{3} \text{He} \to \Lambda p n$ reaction, which was recently measured in the J-PARC E15 experiment. We find that the behavior of the calculated differential cross section $d ^{2} \sigma / d M_{\Lambda p} d q_{\Lambda p}$, where $M_{\Lambda p}$ and $q_{\Lambda p}$ are the $\Lambda p$ invariant mass and momentum transfer in the $(K^{-} , \, n)$ reaction in the laboratory frame, respectively, is consistent with the experiment. Furthermore, we can reproduce almost quantitatively the experimental data of the $\Lambda p$ invariant mass spect…

Nuclear physicsPhysicsHigh Energy Physics - PhenomenologyNuclear TheoryMomentum transferBound stateMass spectrumJ-PARCLambdaNuclear theoryNuclear ExperimentBar (unit)
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RECENT DEVELOPMENTS INVOLVING ISOBARS IN NUCLEAR SYSTEMS — Workshop D

1977

Developments of the last year or two concerning the role of isobar resonances in nuclear systems are reviewed. Special attention is given to the influence of the A isobar in the nucleon-nucleon force and to the possibility of the existence of NA or AA bound states. Also mentioned are the effects of the A in polarized pp scattering, in proton-nucleus scattering and in nuclear matter and the ground states of finite nuclei. Recent experiments intended to observe preexisting isobar configurations in nuclei are briefly surveyed. Approaches to pion-nucleus scattering based on NA interactions are discussed.

Nuclear physicsPhysicsScatteringNuclear TheoryBound stateIsobarNuclear ExperimentNuclear matter
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