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NSR database version of May 24, 2024.

Search: Author = W.Plessas

Found 38 matches.

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2010CH04      Phys.Rev. C 81, 028201 (2010)

K.-S.Choi, W.Plessas, R.F.Wagenbrunn

Axial charges of the nucleon and N* resonances

doi: 10.1103/PhysRevC.81.028201
Citations: PlumX Metrics


2008ME08      Eur.Phys.J. A 35, 329 (2008)

T.Melde, W.Plessas

Baryon resonances and strong decays

doi: 10.1140/epja/i2007-10556-5
Citations: PlumX Metrics


2007ME10      Few-Body Systems 40, 165 (2007)

J.Zs.Mezei, J.Darai, Z.Papp, W.Plessas

Faddeev-Noble Versus Sasakawa-Sawada Equations for the Nuclear Three-Body Coulomb Problem

doi: 10.1007/S00601-006-0170-2
Citations: PlumX Metrics


2007ME15      Phys.Rev. C 76, 025204 (2007)

T.Melde, W.Plessas, B.Sengl

Covariant calculation of nonstrange decays of strange baryon resonances

doi: 10.1103/PhysRevC.76.025204
Citations: PlumX Metrics


2005GL02      Eur.Phys.J. A 23, 507 (2005)

K.Glantschnig, R.Kainhofer, W.Plessas, B.Sengl, R.F.Wagenbrunn

Extended Goldstone-boson-exchange constituent-quark model

doi: 10.1140/epja/i2004-10106-9
Citations: PlumX Metrics


2005ME15      Eur.Phys.J. A 25, 97 (2005)

T.Melde, L.Canton, W.Plessas, R.F.Wagenbrunn

Spectator-model operators in point-form relativistic quantum mechanics

doi: 10.1140/epja/i2004-10276-4
Citations: PlumX Metrics


2005ME16      Phys.Rev. C 72, 015207 (2005); Erratum Phys.Rev. C 74, 069901 (2006)

T.Melde, W.Plessas, R.F.Wagenbrunn

Covariant calculation of mesonic baryon decays

doi: 10.1103/PhysRevC.72.015207
Citations: PlumX Metrics


2003DO05      Phys.Rev. C 67, 064005 (2003)

P.Doleschall, I.Borbely, Z.Papp, W.Plessas

Nonlocality in the nucleon-nucleon interaction and three-nucleon bound states

NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, effect of nonlocal nucleon-nucleon interaction. Comparison with data.

doi: 10.1103/PhysRevC.67.064005
Citations: PlumX Metrics


2003WA30      Eur.Phys.J. A 18, 155 (2003)

R.F.Wagenbrunn, S.Boffi, L.Ya.Glozman, W.Klink, W.Plessas, M.Radici

Relativistic study of nucleon electroweak properties in a constituent-quark model

NUCLEAR STRUCTURE 1n, 1H; calculated form factors, radii, μ. Constituent-quark model.

doi: 10.1140/epja/i2002-10291-5
Citations: PlumX Metrics


2002BO23      Eur.Phys.J. A 14, 17 (2002)

S.Boffi, L.Ya.Glozman, W.Klink, W.Plessas, M.Radici, R.F.Wagenbrunn

Covariant Electroweak Nucleon Form Factors in a Chiral Constituent-Quark Model

NUCLEAR STRUCTURE 1n, 1H; calculated electric, magnetic and pseudoscalar form factors, charge radii. Chiral constituent-quark model.

doi: 10.1007/s10050-002-8784-3
Citations: PlumX Metrics


2002PL01      Nucl.Phys. A699, 312c (2002)

W.Plessas, S.Boffi, L.Ya.Glozman, W.Klink, M.Radici, R.F.Wagenbrunn

Nucleon Properties in a Semirelativistic Chiral Quark Model

NUCLEAR STRUCTURE 1n, 1H; calculated form factors, radii, μ. Goldstone-boson-exchange constituent quark model, comparison with data.

doi: 10.1016/S0375-9474(01)01509-3
Citations: PlumX Metrics


2001GL08      Phys.Lett. 516B, 183 (2001)

L.Ya.Glozman, M.Radici, R.F.Wagenbrunn, S.Boffi, W.Klink, W.Plessas

Covariant Axial Form Factor of the Nucleon in a Chiral Constituent Quark Model

NUCLEAR STRUCTURE 1n, 1H; calculated axial form factor. Chiral constituent quark model.

doi: 10.1016/S0370-2693(01)00915-7
Citations: PlumX Metrics


2001TH13      Nucl.Phys. A689, 394c (2001)

L.Theussl, R.F.Wagenbrunn, B.Desplanques, W.Plessas

Hadronic Decay of N and Δ Resonances in a Chiral Quark Model

doi: 10.1016/S0375-9474(01)00863-6
Citations: PlumX Metrics


2001TH20      Eur.Phys.J. A 12, 91 (2001)

L.Theussl, R.F.Wagenbrunn, B.Desplanques, W.Plessas

Hadronic Decays of N and Δ Resonances in a Chiral Quark Model

doi: 10.1007/s100500170042
Citations: PlumX Metrics


2001WA12      Nucl.Phys. A684, 284c (2001)

R.F.Wagenbrunn, L.Ya.Glozman, W.Plessas, K.Varga

Extended Goldstone-Boson-Exchange Chiral Quark Model

doi: 10.1016/S0375-9474(01)00422-5
Citations: PlumX Metrics


2001WA30      Phys.Lett. 511B, 33 (2001)

R.F.Wagenbrunn, S.Boffi, W.Klink, W.Plessas, M.Radici

Covariant Nucleon Electromagnetic Form Factors from the Goldstone-Boson-Exchange Quark Model

NUCLEAR STRUCTURE 1n, 1H; calculated electric and magnetic form factors. Constituent quark model, point-form approach, comparison with data.

doi: 10.1016/S0370-2693(01)00622-0
Citations: PlumX Metrics


2000PA52      Phys.Rev. C62, 044004 (2000)

Z.Papp, A.Krassnigg, W.Plessas

Faddeev Approach to Confined Three-Quark Problems

doi: 10.1103/PhysRevC.62.044004
Citations: PlumX Metrics


2000WA08      Nucl.Phys. A666-667, 29c (2000)

R.F.Wagenbrunn, L.Ya.Glozman, W.Plessas, K.Varga

Extension of the GBE Chiral Constituent Quark Model

doi: 10.1016/S0375-9474(00)00006-3
Citations: PlumX Metrics


2000WA11      Nucl.Phys. A663-664, 703c (2000)

R.F.Wagenbrunn, L.Ya.Glozman, W.Plessas, K.Varga

Extended Goldstone-Boson-Exchange Constituent Quark Model

doi: 10.1016/S0375-9474(99)00726-5
Citations: PlumX Metrics


1998GL04      Nucl.Phys. A631, 469c (1998)

L.Ya.Glozman, W.Plessas, K.Varga, R.F.Wagenbrunn

Light and Strange Baryons in a Chiral Quark Model with Goldstone-Boson-Exchange Interactions

doi: 10.1016/S0375-9474(98)00049-9
Citations: PlumX Metrics


1998GL05      Phys.Rev. C57, 3406 (1998); Comments Phys.Rev. C61, 019803 (1999)

L.Ya.Glozman, Z.Papp, W.Plessas, K.Varga, R.F.Wagenbrunn

Effective Q-Q Interactions in Constituent Quark Models

doi: 10.1103/PhysRevC.57.3406
Citations: PlumX Metrics


1997GL04      Nucl.Phys. A623, 90c (1997)

L.Ya.Glozman, Z.Papp, W.Plessas, K.Varga, R.F.Wagenbrunn

Light and Strange Baryons in a Chiral Constituent-Quark Model

doi: 10.1016/S0375-9474(97)00426-0
Citations: PlumX Metrics


1996PA15      Phys.Rev. C54, 50 (1996)

Z.Papp, W.Plessas

Coulomb-Sturmian Separable Expansion Approach: Three-body Faddeev calculations for Coulomb-like interactions

doi: 10.1103/PhysRevC.54.50
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1990CO13      Phys.Rev. C41, 2538 (1990)

T.Cornelius, W.Glockle, J.Haidenbauer, Y.Koike, W.Plessas, H.Witala

Predictions of the Paris N-N Potential for Three-Nucleon Continuum Observables: Comparison of two approaches

NUCLEAR REACTIONS 2H(n, n), (polarized n, n), E=10 MeV; calculated σ(θ), polarization observables. Two approaches comparison.

doi: 10.1103/PhysRevC.41.2538
Citations: PlumX Metrics


1990PA06      Nucl.Phys. A508, 253c (1990)

J.Pauschenwein, L.Mathelitsch, W.Plessas

Several Versions of the Bonn N-N Potential Tested in Elastic e-d Scattering

NUCLEAR REACTIONS 2H(e, e), E not given; calculated electric, magnetic form factors. New Bonn potential.

doi: 10.1016/0375-9474(90)90481-Z
Citations: PlumX Metrics


1987KO02      Phys.Rev. C35, 396 (1987)

Y.Koike, J.Haidenbauer, W.Plessas

Nucleon-Deuteron Elastic Scattering with the Paris Nucleon-Nucleon Potential

NUCLEAR REACTIONS, MECPD 2H(n, n), E=5-20 MeV; calculated σ(E), σ(θ); 2H(polarized p, d), E=10 MeV; calculated vector-to-vector spin transfer coefficients. Paris potential.

doi: 10.1103/PhysRevC.35.396
Citations: PlumX Metrics


1986HA01      Phys.Rev. C33, 439 (1986)

J.Haidenbauer, Y.Koike, W.Plessas

Separable Respresentation of the Bonn Nucleon-Nucleon Potential

NUCLEAR REACTIONS 1n, 1H(p, p), E=0-450 MeV; calculated phase shifts. Bonn nucleon-nucleon potential, separable representation.

doi: 10.1103/PhysRevC.33.439
Citations: PlumX Metrics


1985HA26      Phys.Rev. C32, 1424 (1985)

J.Haidenbauer, W.Plessas

Modified Separable Representation of the Paris Nucleon-Nucleon Potential in the 1S0 and 3P0 States

NUCLEAR REACTIONS 1n, 1H(p, p), E ≈ 0-500 MeV; analyzed phase shifts; deduced potentials parameters. Paris potentials, modified separable representation.

doi: 10.1103/PhysRevC.32.1424
Citations: PlumX Metrics


1985KO31      Phys.Rev. C32, 1796 (1985)

Y.Koike, W.Plessas, H.Zankel

Nucleon-Deuteron Scattering Based on Meson-Exchange Nucleon-Nucleon Dynamics

NUCLEAR REACTIONS 2H(n, n), E=8, 10, 10.25, 12 MeV; calculated σ(θ). 2H(polarized n, n), E=10 MeV; calculated polarization spin-transfer coefficient. Comparison to 2H(d, d) data, meson exchange effects.

doi: 10.1103/PhysRevC.32.1796
Citations: PlumX Metrics


1985LO14      Phys.Rev. C32, 2165 (1985)

B.Loiseau, L.Mathelitsch, W.Plessas, K.Schwarz

Off-Shell Properties of the Paris Nucleon-Nucleon Potential and Implications for Few-Body Systems

NUCLEAR REACTIONS 2H(e, e), E not given; calculated deuteron tensor polarization, θ=70°. 2H(polarized p, p), (polarized n, n), E=10 MeV; calculated spin transfer coefficient.

doi: 10.1103/PhysRevC.32.2165
Citations: PlumX Metrics


1985SC20      Phys.Rev. C32, 1261 (1985)

W.Schweiger, J.Haidenbauer, W.Plessas

Separable Model for the Antinucleon-Nucleon Elastic and Annihilation Interaction

NUCLEAR REACTIONS 1H(p-bar, p-bar), E ≈ 10-100 MeV; calculated elastic, compound elastic, total σ(E). Separable model.

doi: 10.1103/PhysRevC.32.1261
Citations: PlumX Metrics


1984HA51      Phys.Rev. C30, 1822 (1984)

J.Haidenbauer, W.Plessas

Separable Representation of the Paris Nucleon-Nucleon Potential

NUCLEAR STRUCTURE 2H; calculated binding energies, D-state probability, quadrupole moment. Paris potential, separable representation.

NUCLEAR REACTIONS 1H(p, p), (n, n), E=0-450 MeV; calculated phase shifts, mixing parameters. 2H(polarized p, p), (polarized n, n), E=10 MeV; calculated spin transfer coefficient vs θ. Paris potential, separable interaction.

doi: 10.1103/PhysRevC.30.1822
Citations: PlumX Metrics


1984ZA06      Z.Phys. A317, 45 (1984)

H.Zankel, W.Plessas

Off-Shell Effects in Nucleon-Deuteron Polarization Observables

NUCLEAR REACTIONS 1H(polarized d, d), E=10 MeV; calculated spin correlation parameter. Vector polarized beam. 2H(polarized p, p), E=10 MeV; calculated spin transfer coefficients, polarized outgoing proton; deduced intermediate range repulsion, off-shell effect roles. Separable representation, S-wave Paris potential.

doi: 10.1007/BF01420447
Citations: PlumX Metrics


1983SC04      Phys.Rev. C27, 515 (1983)

W.Schweiger, W.Plessas, L.P.Kok, H.van Haeringen

Separable Representation of the Nuclear Proton-Proton Interaction

NUCLEAR REACTIONS 1H(p, p), E=50-500 MeV; analyzed phase shift data. Separable representation, Coulomb distortion effects.

doi: 10.1103/PhysRevC.27.515
Citations: PlumX Metrics


1983SC30      Phys.Rev. C28, 1414 (1983)

W.Schweiger, W.Plessas, L.P.Kok, H.van Haeringen

Coulomb Plus Separable Potential in Coupled Channels

NUCLEAR REACTIONS 1H(p, p), E=0-500 MeV; calculated Coulomb modified phase shifts. Coupled-channels, separable potentials.

doi: 10.1103/PhysRevC.28.1414
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1983SC35      Nuovo Cim. 76A, 322 (1983)

K.Schwarz, W.Plessas, L.Mathelitsch

Deuteron Form Factors and e-d Polarization Observables for the Paris and Graz-II Potentials

NUCLEAR REACTIONS 2H(e, e), E not given; calculated electric, magnetic form factors, deuteron vector, tensor polarizations; deduced potential off-shell features. Paris, Graz potentials.

doi: 10.1007/BF02833729
Citations: PlumX Metrics


1982PL07      Acta Phys.Austr. 54, 305 (1982)

W.Plessas

On-Shell and Off-Shell Behaviour of Separable Nucleon-Nucleon Potentials

NUCLEAR REACTIONS 1H(p, p), E < 500 MeV; calculated phase shifts; deduced potential on-shell, off-shell behavior. Separable potentials.


1981PL02      Phys.Rev. C23, 1340 (1981)

W.Plessas, L.Mathelitsch, F.Pauss

Influence of the Coulomb-Distortion Effect on Proton-Proton Observables

NUCLEAR REACTIONS 1H(p, p), (polarized p, p), 1n(n, n), (polarized n, n), E=10, 20, 50 MeV; calculated σ(θ), polarization, spin-correlation parameters, spin-transfer coefficients; deduced Coulomb distortion effects. Different potentials.

doi: 10.1103/PhysRevC.23.1340
Citations: PlumX Metrics


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