0000000000040071

AUTHOR

Wolfram Weise

showing 8 related works from this author

Low-energy interactions of Nambu-Goldstone bosons with D mesons in covariant chiral perturbation theory

2010

We calculate the scattering lengths of Nambu-Goldstone bosons interacting with D mesons in a covariant formulation of chiral perturbation theory, which satisfies heavy-quark spin symmetry and analytical properties of loop amplitudes. We compare our results with previous studies performed using heavy-meson chiral perturbation theory and show that recoil corrections are sizable in most cases.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particleRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosonHigh Energy Physics::ExperimentPerturbation theoryChiral symmetry breakingNuclear ExperimentBoson
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Resonances in QCD

2015

We report on the EMMI Rapid Reaction Task Force meeting 'Resonances in QCD', which took place at GSI October 12-14, 2015. A group of 26 people met to discuss the physics of resonances in QCD. The aim of the meeting was defined by the following three key questions: What is needed to understand the physics of resonances in QCD? Where does QCD lead us to expect resonances with exotic quantum numbers? What experimental efforts are required to arrive at a coherent picture? For light mesons and baryons only those with ${\it up}$, ${\it down}$ and ${\it strange}$ quark content were considered. For heavy-light and heavy-heavy meson systems, those with ${\it charm}$ quarks were the focus. This docum…

PhysicsQuarkQuantum chromodynamicsNuclear and High Energy PhysicsStrange quarkParticle physicsMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHadron01 natural sciencesCharm quarkBaryonHigh Energy Physics - Phenomenology0103 physical sciencesHadrons; Mini review; QCD; Resonancesddc:530High Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment010306 general physicsNuclear Physics A
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Nuclear Quark and Gluon Distributions in Coordinate Space

1998

In coordinate space, quark and gluon distributions of the nucleon are defined as correlation functions involving two field operators separated by a light-cone distance $y^+ = 2l$. We study the nuclear modifications of these distributions. The largest effect is a strong depletion of parton distributions (shadowing) at large longitudinal distances, which starts for all parton species at $l=2$ fm, i.e. at the average nucleon-nucleon separation in nuclei. On the other hand, the nuclear radius does not play a significant role. At $l \lsim 1$ fm, nuclear modifications of parton distributions are small. The intrinsic structure of individual nucleons is evidently not very much affected by nuclear b…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsField (physics)High Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesPartonGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentCoordinate spaceNucleonNuclear ExperimentNuclear radius
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Nuclear parton distributions in coordinate space

2000

PhysicsNuclear and High Energy PhysicsParticle physicsPartonCoordinate spaceNuclear Physics A
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Antikaon-nucleon interaction and Lambda(1405) in chiral SU(3) dynamics

2016

The properties of the Lambda(1405) resonance are key ingredients for determining the antikaon-nucleon interaction in strangeness nuclear physics, and the novel internal structure of the Lambda(1405) is of great interest in hadron physics, as a prototype case of a baryon that does not fit into the simple three-quark picture. We show that a quantitative description of the antikaon-nucleon interaction with the Lambda(1405) is achieved in the framework of chiral SU(3) dynamics, with the help of recent experimental progress. Further constraints on the Kbar N subthreshold interaction are provided by analyzing pi Sigma spectra in various processes, such as the K-d -> pi Sigma n reaction and the…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsHadronNuclear TheoryFOS: Physical sciencesMolecular configurationStrangeness16. Peace & justice01 natural sciencesResonance (particle physics)Spectral lineBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNucleonWave functionNuclear Experiment
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Multi-nucleon mechanism for subthreshold antiproton production in proton-nucleus reactions

1995

We study a many-body (multipion) mechanism for ¯p subthreshold production in proton-nucleus collisions. The incoming proton and the interacting nucleons in the target act as sources of pions that merge to produce a nucleon-antiproton pair. The calculation takes fully into account the initial state interaction and antiproton absorption in the final state. The cooperation of several nucleons in the initial state reduces the threshold for the reaction allowing for production rates that may account for 15–50% of the total ¯p production. We point out that this contribution should be added to the primary ¯p production mechanism due toΔ formation and rescattering, as found by other groups, and sho…

PhysicsNuclear and High Energy PhysicsParticle physicsProtonSubthreshold conductionNuclear TheoryNuclear physicsPionmedicine.anatomical_structureAntiprotonmedicineNuclear fusionProduction (economics)Nuclear ExperimentNucleonNucleusZeitschrift f�r Physik A Hadrons and Nuclei
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Peripheral nucleon-nucleon phase shifts and chiral symmetry

1997

Within the one-loop approximation of baryon chiral perturbation theory we calculate all one-pion and two-pion exchange contributions to the nucleon-nucleon interaction. In fact we construct the elastic NN-scattering amplitude up to and including third order in small momenta. The phase shifts with orbital angular momentum $L\geq2 $ and the mixing angles with $J\geq2$ are given parameterfree and thus allow for a detailed test of chiral symmetry in the two-nucleon system. We find that for the D-waves the $2\pi$-exchange corrections are too large as compared with empirical phase shifts, signaling the increasing importance of shorter range effects in lower partial waves. For higher partial waves…

PhysicsNuclear and High Energy PhysicsAngular momentumChiral perturbation theoryNuclear TheoryNuclear TheoryPhase (waves)FOS: Physical sciencesNuclear Theory (nucl-th)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AmplitudeQuantum electrodynamicsCoordinate spaceNuclear ExperimentNucleonMixing (physics)Nuclear Physics A
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Physics with Antiprotons at the Future GSI Facility

2003

Recently GSI presented the plans for a major new international research facility (http://www.gsi.de/GSI-future/). Highly luminous secondary beams with excellent quality encompassing the production of antiprotons will be delivered. In a High Energy Storage Ring (HESR) with a bending power of 50 Tm antiprotons will be cooled either stochastically or by electrons. The envisaged limits are a momentum range of 1.5 to 15 GeV/c and a luminosity of 2 × 1032 cm-2 s-1. Four major physical research goals can be addressed: high precision charmonium spectroscopy, medium effects of open and hidden charm, the search for glueballs and hybrids, and the production of hypernuclei.

MomentumPhysicsNuclear physicsInternational researchLuminosity (scattering theory)AntiprotonElectronCharm (quantum number)Condensed Matter PhysicsMathematical PhysicsAtomic and Molecular Physics and OpticsPhysica Scripta
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