NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = H.Weigel Found 47 matches. 2019TA16 Eur.Phys.J. A 55, 128 (2019) Nucleon structure functions from the NJL-model chiral soliton
doi: 10.1140/epja/i2019-12806-3
2008KU20 Eur.Phys.J. A 38, 295 (2008) Two-photon contributions to the Rosenbluth cross-section in the Skyrme model
doi: 10.1140/epja/i2008-10672-8
2007WE06 Eur.Phys.J. A 31, 495 (2007) Collective resonances in the soliton model approach to meson-baryon scattering
doi: 10.1140/epja/i2006-10191-8
2005WA37 Eur.Phys.J. A 26, 361 (2005) Bound-state versus collective-coordinate approaches in chiral soliton models and the width of the Θ+ pentaquark
doi: 10.1140/epja/i2005-10180-5
2004SC12 Nucl.Phys. A735, 163 (2004) Magnetic moments of baryons with a single heavy quark
doi: 10.1016/j.nuclphysa.2004.01.132
2004WE07 Eur.Phys.J. A 21, 133 (2004) Exotic baryons and monopole excitations in a chiral soliton model
doi: 10.1140/epja/i2004-10022-0
2003WE15 Eur.Phys.J. A 18, 559 (2003) Flavor symmetry breaking and strangeness in the nucleon
doi: 10.1140/epja/i2002-10283-5
2001WE01 Nucl.Phys. A680, 48c (2001) Hadron Structure Functions within a Chiral Quark Model
doi: 10.1016/S0375-9474(00)00386-9
2001WE10 Nucl.Phys. A690, 595 (2001) Hyperon Beta-Decay and Axial Charges of the Lambda in View of Strongly Distorted Baryon Wave-Functions
doi: 10.1016/S0375-9474(01)00347-5
2000DA13 Nucl.Phys. A671, 547 (2000) J.da Providencia, H.Walliser, H.Weigel Soliton Formation in the Nambu-Jona-Lasinio Model
doi: 10.1016/S0375-9474(99)00849-0
2000WE05 Nucl.Phys. A670, 92c (2000) Nucleon Structure Functions in a Chiral Soliton Model NUCLEAR STRUCTURE 1n, 1H; calculated structure functions. Chiral soliton model.
doi: 10.1016/S0375-9474(00)00077-4
1999ME03 Phys.Lett. 447B, 1 (1999) The Parity-Violating Pion-Nucleon Coupling Constant from a Realistic Three Flavor Skyrme Model
doi: 10.1016/S0370-2693(98)01569-X
1999SC15 Nucl.Phys. A651, 174 (1999) O.Schroder, H.Reinhardt, H.Weigel Nucleon Structure Functions in the Three-Flavor NJL Soliton Model NUCLEAR STRUCTURE 1n, 1H; calculated structure functions. Three-flavor chiral soliton model. Comparisons with data.
doi: 10.1016/S0375-9474(99)00131-1
1999WE11 Nucl.Phys. B(Proc.Supp.) S74, 125 (1999) H.Weigel, L.Gamberg, H.Reinhardt, O.Schroder Nucleon Structure Functions from a Chiral Soliton
doi: 10.1016/S0920-5632(99)00147-4
1998GA49 Int.J.Mod.Phys. A32, 5519 (1998) L.Gamberg, H.Reinhardt, H.Weigel Nucleon Structure Functions from a Chiral Soliton in the Infinite Momentum Frame NUCLEAR STRUCTURE 1H, 1n; calculated structure functions for deep inelastic scattering.
doi: 10.1142/S0217751X98002511
1998SC39 Phys.Lett. 439B, 398 (1998) O.Schroder, H.Reinhardt, H.Weigel Strangeness Contribution to the Polarized Nucleon Structure Function g1(x) NUCLEAR STRUCTURE 1n, 1H; calculated polarized structure function g1(x); deduced strange quark contribution. Valence quark approximation to chiral soliton model.
doi: 10.1016/S0370-2693(98)01038-7
1998WE15 Eur.Phys.J. A 2, 391 (1998) Radial Excitations of Low-Lying Baryons and the Z+ Penta-Quark
doi: 10.1007/s100500050136
1997HA10 Nucl.Phys. A615, 291 (1997) T.Haberichter, H.Reinhardt, N.N.Scoccola, H.Weigel Strangeness Dependence in Radiative Hyperon Decay Amplitudes
doi: 10.1016/S0375-9474(96)00485-X
1997HA52 Nucl.Phys. A625, 789 (1997) M.Harada, A.Qamar, F.Sannino, J.Schechter, H.Weigel Hyperfine Splitting of Low-Lying Heavy Baryons
doi: 10.1016/S0375-9474(97)00400-4
1997KO38 Z.Phys. A358, 445 (1997) Strangeness in the Nucleon and the Ratio of Proton-to-Neutron Neutrino-Induced Quasi-Elastic Yield NUCLEAR REACTIONS 12C(ν, ν'), (ν-bar, ν-bar'), E not given; calculated proton-to-neutron yield ratio. Nucleon electroweak form factors from three flavor pseudoscalar vector meson soliton model.
doi: 10.1007/s002180050353
1997WE02 Phys.Lett. 399B, 287 (1997) H.Weigel, L.Gamberg, H.Reinhardt Nucleon Structure Functions from a Chiral Soliton NUCLEAR REACTIONS 1H(ν, ν), (ν-bar, ν-bar), (e, e), E not given; analyzed scattering associated unpolarized structure functions. Chiral soliton approach, bosonized Nambu-Jona-Lasinio model.
doi: 10.1016/S0370-2693(97)00296-7
1997WE11 Phys.Rev. D55, 6910 (1997) H.Weigel, L.Gamberg, H.Reinhardt Polarized Nucleon Structure Functions within a Chiral Soliton Model NUCLEAR STRUCTURE 1n, 1H; calculated polarized-spin structure functions. Bosonized Nambu-Jona-Lasinio model.
doi: 10.1103/PhysRevD.55.6910
1997ZU01 Phys.Rev. C55, 2030 (1997) U.Zuckert, R.Alkofer, H.Weigel, H.Reinhardt Baryons as Hybrids of Solitons and Three Quark Bound States
doi: 10.1103/PhysRevC.55.2030
1996AB06 Phys.Lett. 366B, 26 (1996) A.Abada, H.Weigel, H.Reinhardt Radiative Decays of Hyperons in the Skyrme Model: E2/M1 transitions ratios
doi: 10.1016/0370-2693(95)01353-9
1996AL04 Z.Phys. A354, 181 (1996) R.Alkofer, H.Reinhardt, J.Schlienz, H.Weigel Topologically Non-Trivial Chiral Transformations. The Chiral Invariant Elimination of the Axial Vector Meson
doi: 10.1007/s002180050031
1996HA33 Phys.Lett. 384B, 5 (1996) M.Harada, F.Sannino, J.Schechter, H.Weigel Scaling Behavior in Soliton Models
doi: 10.1016/0370-2693(96)00801-5
1996SC36 Phys.Lett. 389B, 433 (1996) N.N.Scoccola, H.Weigel, B.Schwesinger SU(3) Symmetry Breaking and Octet Baryon Polarizabilities NUCLEAR STRUCTURE 1n, 1H; calculated magnetic, electric polarizabilities. Collective coordinate approach to three flavor generalization of the Skyrme model.
doi: 10.1016/S0370-2693(96)01300-7
1995AB16 Nucl.Phys. A593, 488 (1995) A.Abada, R.Alkofer, H.Reinhardt, H.Weigel Monopole Excitations of Baryons in the Nambu-Jona-Lasinio Soliton Model
doi: 10.1016/0375-9474(95)00342-X
1995SC35 Nucl.Phys. A590, 655 (1995); Erratum Nucl.Phys. A598, 583 (1996) J.Schechter, A.Subbaraman, S.Vaidya, H.Weigel Heavy-Quark Solitons: Towards realistic masses
doi: 10.1016/0375-9474(95)00182-Z
1995WE01 Nucl.Phys. A582, 484 (1995) H.Weigel, R.Alkofer, H.Reinhardt Estimate of Quantum Corrections to the Mass of the Chiral Soliton in the Nambu-Jona-Lasinio Model
doi: 10.1016/0375-9474(94)00480-B
1995WE04 Nucl.Phys. A585, 513 (1995) H.Weigel, U.Zuckert, R.Alkofer, H.Reinhardt On the Analytic Properties of Chiral Solitons in the Presence of the (Omega)-Meson
doi: 10.1016/0375-9474(94)00625-W
1995WE07 Phys.Lett. 353B, 20 (1995) H.Weigel, A.Abada, R.Alkofer, H.Reinhardt On the Strange Vector Form Factors of the Nucleon in the NJL Soliton Model NUCLEAR STRUCTURE 1H, 1n; calculated μ, strange electric, magnetic form factor. Nambu-Jona-Lasinio model.
doi: 10.1016/0370-2693(95)00534-R
1995ZU03 Phys.Lett. 362B, 1 (1995) U.Zuckert, R.Alkofer, H.Weigel, H.Reinhardt Diquarks in a Chiral Soliton Field
doi: 10.1016/0370-2693(95)01206-6
1994WE12 Nucl.Phys. A576, 477 (1994) H.Weigel, R.Alkofer, H.Reinhardt Hyperons in the Bound-State Approach to the Nambu-Jona-Lasinio Chiral Soliton
doi: 10.1016/0375-9474(94)90742-0
1994ZU02 Nucl.Phys. A570, 445 (1994) U.Zuckert, R.Alkofer, H.Reinhardt, H.Weigel The Chiral Soliton of the Nambu-Jona-Lasinio Model with Vector and Axial-Vector Mesons
doi: 10.1016/0375-9474(94)90068-X
1992JA19 Phys.Rev. D45, 1470 (1992) Approach to Color Transparency in the Soliton Picture of the Nucleon NUCLEAR STRUCTURE A=5-50; calculated nucleon-nucleon noninteraction probability vs nucleon number. Soliton picture of nucleon approach to color transparency.
doi: 10.1103/PhysRevD.45.1470
1992PA13 Nucl.Phys. A541, 453 (1992) Static Properties of Baryons from an SU(3) Pseudoscalar Vector Meson Lagrangian NUCLEAR STRUCTURE 1H, 1n; calculated μ, magnetic radii, magnetic, electric form factors. Skyrme model with vector mesons, collective treatment of the SU(3).
doi: 10.1016/0375-9474(92)90187-O
1992SC11 Nucl.Phys. A540, 461 (1992) SU(3) Symmetry Breaking for Masses, Magnetic moments and Sizes of Baryons RADIOACTIVITY 1n(β-); calculated β-decay matrix element.
doi: 10.1016/0375-9474(92)90169-K
1991ME08 Phys.Lett. 267B, 167 (1991) Chiral Symmetry and the Neutron-Proton Mass Difference in the Medium NUCLEAR STRUCTURE 1n, 1H; calculated mass difference. Nonlinear chiral meson theory.
doi: 10.1016/0370-2693(91)91242-N
1991SC29 Phys.Lett. 261B, 235 (1991) Breathing Mode Quantization in an Extended SU(3) Skyrme Model NUCLEAR STRUCTURE 1n, 1H; calculated μ. Extended SU(3) Skyrme model, breathing mode quantization.
doi: 10.1016/0370-2693(91)90320-P
1991SC30 Phys.Lett. 267B, 438 (1991) Slowly Rotating Skyrmions in Broken SU(3) NUCLEAR STRUCTURE 1n, 1H; calculated μ ratio. Broken SU(3), rotating skyrmions.
doi: 10.1016/0370-2693(91)90890-3
1991SC35 Phys.Rev. D44, 2916 (1991) Breathing Mode in the SU(3) Skyrme Model NUCLEAR STRUCTURE 1H, 1n; calculated μ. SU(3) Skyrme model, breathing mode.
doi: 10.1103/PhysRevD.44.2916
1979MI10 Nucl.Phys. A322, 40 (1979) R.Michel, G.Brinkmann, H.Weigel, W.Herr Measurement and Hybrid-Model Analysis of Proton-Induced Reactions with V, Fe and Co NUCLEAR REACTIONS 50,51V(p, xnyp), 54,56,57,58Fe(p, xnyp), 59Co(p, xnyp), E=12-45 MeV; measured σ(E). Natural targets, stacked foil technique, hybrid-model calculations.
doi: 10.1016/0375-9474(79)90332-4
1978MI08 Z.Phys. A286, 393 (1978) Proton-Induced Reactions on Nickel with Energies between 12 and 45 Mev NUCLEAR REACTIONS Ni(p, X), E=12-45 MeV; measured σ for production of 61Cu, 56,57Ni, 55,56,57,58,58m,60,60mCo, 52,52mMn.
doi: 10.1007/BF01408896
1978MI12 J.Inorg.Nucl.Chem. 40, 1845 (1978) R.Michel, G.Brinkmann, H.Weigel, W.Herr Proton-Induced Reactions on Titanium with Energies between 13 and 45 MeV NUCLEAR REACTIONS Ti(p, xnyp), E=13-45 MeV; measured σ(E) for production of 48V, 43,44,46,47,48Sc, 43K. integral yields.
doi: 10.1016/0022-1902(78)80241-3
1977MI21 Radiochim.Acta 24, 50 (1977) Gamma-Branching in the Decay of 55Co RADIOACTIVITY 55Co(β+), (EC); measured Eγ, Iγ, T1/2. 55Fe deduced levels, γ-branching.
1975WE13 Radiochem.Radioanal.Lett. 21, 293 (1975) H.Weigel, R.Michel, U.Herpers, W.Herr Survey of 600 MeV Proton Cross-Sections for Spallogenic Radionuclides in Quartz-, Fe-, Co-, and Ni-Targets NUCLEAR REACTIONS Fe, Co, Ni, Al, Si, O(p, X), E=600 MeV; measured σ. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0088. Back to query form |