NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = W.Plessas Found 38 matches. 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
2008ME08 Eur.Phys.J. A 35, 329 (2008) Baryon resonances and strong decays
doi: 10.1140/epja/i2007-10556-5
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
2007ME15 Phys.Rev. C 76, 025204 (2007) Covariant calculation of nonstrange decays of strange baryon resonances
doi: 10.1103/PhysRevC.76.025204
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1996PA15 Phys.Rev. C54, 50 (1996) Coulomb-Sturmian Separable Expansion Approach: Three-body Faddeev calculations for Coulomb-like interactions
doi: 10.1103/PhysRevC.54.50
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
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
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
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
1985HA26 Phys.Rev. C32, 1424 (1985) 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
1985KO31 Phys.Rev. C32, 1796 (1985) 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
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
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
1984HA51 Phys.Rev. C30, 1822 (1984) 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
1984ZA06 Z.Phys. A317, 45 (1984) 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
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
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
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
1982PL07 Acta Phys.Austr. 54, 305 (1982) 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
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