NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Reinhardt Found 35 matches. 2000AL15 Nucl.Phys. A663-664, 683c (2000) R.Alkofer, S.Ahlig, C.Fischer, M.Oettel, H.Reinhardt Octet and Decuplet Baryons in a Confining and Convariant Diquark-Quark Model
doi: 10.1016/S0375-9474(99)00721-6
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
1998OE03 Phys.Rev. C58, 2459 (1998) M.Oettel, G.Hellstern, R.Alkofer, H.Reinhardt Octet and Decuplet Baryons in a Covariant and Confining Diquark-Quark Model
doi: 10.1103/PhysRevC.58.2459
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
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
1997HE21 Nucl.Phys. A625, 697 (1997) G.Hellstern, R.Alkofer, H.Reinhardt Diquark Confinement in an Extended NJL Model
doi: 10.1016/S0375-9474(97)00412-0
1997HE26 Nucl.Phys. A627, 679 (1997) G.Hellstern, R.Alkofer, M.Oettel, H.Reinhardt Nucleon Form Factors in a Covariant Diquark-Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated form factors. Covariant quark-diquark model, Bethe-Salpeter equation.
doi: 10.1016/S0375-9474(97)00514-9
1997LA25 Nucl.Phys. A622, 620 (1997) K.Langfeld, H.Reinhardt, M.Rho A New State of Hadronic Matter at High Density
doi: 10.1016/S0375-9474(97)00364-3
1997MI26 Nucl.Instrum.Methods Phys.Res. B129, 153 (1997) R.Michel, R.Bodemann, H.Busemann, R.Daunke, M.Gloris, H.-J.Lange, B.Klug, A.Krins, I.Leya, M.Lupke, S.Neumann, H.Reinhardt, M.Schnatz-Buttgen, U.Herpers, Th.Schiekel, F.Sudbrock, B.Holmqvist, H.Conde, P.Malmborg, M.Suter, B.Dittrich-Hannen, P.-W.Kubik, H.-A.Synal, D.Filges Cross Sections for the Production of Residual Nuclides by Low- and Medium-Energy Protons from the Target Elements C, N, O, Mg, Al, Si, Ca, Ti, V, Mn, Fe, Co, Ni, Cu, Sr, Y, Zr, Nb, Ba and Au NUCLEAR REACTIONS, ICPND C, N, O, Mg, 27Al, Si, Ca, Ti, V, Mn, Fe, Co, Ni, Cu, Sr, Y, Zr, Nb, Ba, Au(p, X), E ≈ 10-2500 MeV; measured residuals production σ. Activation, accelerator mass spectrometry techniques.
doi: 10.1016/S0168-583X(97)00213-9
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
1996LA25 Nucl.Phys. A608, 331 (1996) K.Langfeld, C.Kettner, H.Reinhardt A Renormalizable Extension of the NJL-Model
doi: 10.1016/S0375-9474(96)00245-X
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
1995BU31 Phys.Lett. 356B, 168 (1995) Octet and Decuplet Baryons in the Hadronized Nambu-Jona-Lasinio Model with Proper Spin Projection NUCLEAR STRUCTURE 1H; calculated mass. Hadronized Nambu-Jona-Lasinio model, proper spin projection, other baryons included.
doi: 10.1016/0370-2693(95)00847-E
1995FR18 Nucl.Phys. A594, 406 (1995) ρω Mixing and the Pion Electromagnetic Form Factor in the Nambu-Jona-Lasinio Model
doi: 10.1016/0375-9474(95)00373-9
1995LA04 Nucl.Phys. A585, 554 (1995) Saddle-Point Approximation of Compact Integrals
doi: 10.1016/0375-9474(94)00533-S
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
1994LA21 Nucl.Phys. A579, 472 (1994) SU(N) Instantons and Their Condensation in the Field-Strength Approach
doi: 10.1016/0375-9474(94)90919-9
1994LA26 Nucl.Phys. A580, 349 (1994) The Field-Strength Approach on a Lattice
doi: 10.1016/0375-9474(94)90902-4
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
1993MA50 Nucl.Phys. A565, 543 (1993) G.Mairle, M.Seeger, H.Reinhardt, T.Kihm, K.T.Knopfle, C.L.Wen The Distribution of Proton-Hole Strengths in the (2s, 1d)-Shell of 35Cl, 37Cl and 39Cl NUCLEAR REACTIONS 36,38,40Ar(polarized d, 3He), E=52 MeV; measured σ(θ), iT11(θ). 35,37,39Cl deduced levels, J, π, spectroscopic factors, proton occupancies, single-particle energies, spreading widths. 39Cl deduced mass excess. Enriched 36,38Ar gas targets. DWBA analysis.
doi: 10.1016/0375-9474(93)90044-X
1993WE07 Phys.Lett. 312B, 6 (1993) C.Weiss, A.Buck, R.Alkofer, H.Reinhardt Diquark Electromagnetic Form Factors in a Nambu-Jona-Lasinio Model NUCLEAR STRUCTURE 1H, 1n; calculated μ. Nambu-Jona-Lasinio model.
doi: 10.1016/0370-2693(93)90477-Y
1988KI07 Phys.Lett. 208B, 79 (1988) On the Meson-Exchange Correction to the Axial-Charge Density for ns1/2 → n'p1/2 n'p1/2 → ns1/2 β-Transitions NUCLEAR STRUCTURE A=16; A=18; A=96; 206Hg, 206Tl(β-); calculated meson-exchange current correction, log ft.
doi: 10.1016/0370-2693(88)91207-5
1985DZ02 Yad.Fiz. 41, 906 (1985) R.V.Dzholos, H.Reinhardt, R.Schmidt, R.Schwengner Microscopic Model of Kinetic Energy Damping in Heavy-Ion Deep Inelastic Collisions NUCLEAR REACTIONS 238U(238U, X), E=1766 MeV; calculated fragment trajectories, kinetic energy loss time dependence.
1980RE01 Nucl.Phys. A337, 176 (1980) Application of the Nuclear Field Theory to Superfluid Nuclei: The Quasiparticle-Phonon Multiplet NUCLEAR STRUCTURE 93Nb; calculated quasiparticle-phonon multiplet energy, B(λ). Nuclear field theory, pairing plus quadrupole force.
doi: 10.1016/0375-9474(80)90085-8
1976RE05 Nucl.Phys. A262, 231 (1976) Investigation of Anharmonic Effects in Nuclear Field Theory: The Influence of the Non-Collective Roots NUCLEAR STRUCTURE 58,60,62Ni; calculated quadrupole moment, B(E2).
doi: 10.1016/0375-9474(76)90617-5
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