NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Muther Found 171 matches. Showing 1 to 100. [Next]2021MU03 Phys.Rev. C 103, 024306 (2021) Spin-orbit term in the nuclear shell model NUCLEAR STRUCTURE 16O, 40Ca; calculated spin-orbit splitting in quasinuclear systems as a function of radius of the nucleon density distribution, radial shape of the spin-orbit potential. 12C, 16O, 28Si, 40Ca, 56Ni; calculated spin-orbit splittings in the nuclear mean field in the transition from infinite nuclear matter to finite nuclei using various approximations. Relativistic as well as non-relativistic mean-field calculations based on realistic models for the nucleon-nucleon (NN) interaction. Discussed results for a realistic interaction model based on chiral effective field theory including contribution of three-nucleon interactions.
doi: 10.1103/PhysRevC.103.024306
2020SU07 Phys.Rev. C 101, 034302 (2020) X.Sun, R.Xu, Y.Tian, Z.Ma, Z.Zhang, Z.Ge, H.Zhang, E.N.E.van Dalen, H.Muther Relativistic mean-field approach in nuclear systems NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,132Sn, 208Pb; calculated binding energy per nucleon, charge radii, charge density distribution, single particle energies, spin-orbit splitting in 16O, scalar and vector potentials for neutrons and protons as a function of isospin asymmetry using both local density approximation (LDA) and improved LDA, based on Dirac-Brueckner-Hartree-Fock (DBHF) approach starting from a realistic nucleon-nucleon interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.034302
2019MU06 Phys.Rev. C 99, 034315 (2019) Pairing in nuclear matter and finite nuclei NUCLEAR STRUCTURE 12C, 16O, 28Si, 40Ca; calculated single-particle energies of low-lying states and depth of Woods-Saxon potentials for 16O and 40Ca, spin-orbit term, pairing gaps of isospin T=0 and T=1 of the nuclear system ranging from infinite nuclear matter to light nuclei using model based on realistic nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.99.034315
2017MU07 Int.J.Mod.Phys. E26, 1730001 (2017) Relativistic effects and three-nucleon forces in nuclear matter and nuclei NUCLEAR STRUCTURE 208Pb, 48Ca, 25O, 40Mg; calculated binding energy. NUCLEAR REACTIONS 12C, 40Ca, 27Al, 56Fe, 98Mo, 208Pb(n, n), E<30 MeV; calculated θ(θ). Comparison with available data.
doi: 10.1142/S0218301317300016
2017RU06 Phys.Rev. C 96, 034327 (2017) O.A.Rubtsova, V.I.Kukulin, V.N.Pomerantsev, H.Muther In-medium bound states and pairing gap
doi: 10.1103/PhysRevC.96.034327
2016MU08 Phys.Rev. C 94, 024328 (2016) H.Muther, O.A.Rubtsova, V.I.Kukulin, V.N.Pomerantsev Discrete wave-packet representation in nuclear matter calculations
doi: 10.1103/PhysRevC.94.024328
2016XU07 Phys.Rev. C 94, 034606 (2016) R.Xu, Z.Ma, Y.Zhang, Y.Tian, E.N.E.van Dalen, H.Muther Global analysis of isospin dependent microscopic nucleon-nucleus optical potentials in a Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 40Ca(n, n), E=2.06-185.0 MeV; 208Pb(n, n), E=1.8-155.0 MeV; 12C(n, n), E=1.04-225.0 MeV; 56Fe(n, n), E=1.8-75.0 MeV; 98Mo(n, n), E=1.5-26.0 MeV; 103Rh(n, n), E=4.51-10.0 MeV; 28Si, 90Zr, 120Sn(n, n), E=65 MeV; 27Al(n, n), E=3.2-26.0 MeV; 40Ca, 56Fe(p, p), E=61.5, 65 MeV; 28Si(p, p), E=14.26-250.0 MeV; 58Ni(p, p), E=7.0-250.0 MeV; 90Zr(p, p), E=9.7-185.0 MeV; 208Pb(p, p), E=16.0-201.0 MeV; calculated σ(θ, E). 12C, 40Ca(polarized n, n), E=10.9 MeV; 58Ni(polarized n, n), E=9.92 MeV; 208Pb(polarized n, n), E=9.97 MeV; 56Fe(polarized p, p), E=16.0-65.0 MeV; 58Ni(polarized p, p), E=16.0-250.0 MeV; 208Pb(polarized p, p), E=80, 200 MeV; calculated analyzing powers Ay(θ, E). 12C, 56Fe, 208Pb(n, X), 40Ca, 120Sn, 208Pb(p, X), E<200 MeV; calculated reaction σ(E). Global analysis of the isospin dependent nucleon-nucleus microscopic optical potential (MOP) based on the DBHF calculation in symmetric and asymmetric nuclear matter; deduced relativistic MOP for nucleon-nucleus scattering. Comparisons with experimental data, and with results from phenomenological Koning-Delaroche global potential. Compiled bibliographic information for experimental (n, n) data for 12C, 14N, 16O, 23Na, 24Mg, 27Al, 28Si, 31P, 32S, 39K, 40Ca, 48Ti, 52Cr, 55Mn, 56Fe, 59Co, 58Ni, 63Cu, 80Se, 88Sr, 89Y, 90Zr, 93Nb, 98Mo, 103Rh, 115In, 120Sn, 197Au, 208Pb, 209Bi targets, and experimental (p, p) data for 12C, 27Al, 28Si, 40Ca, 56Fe, 58Ni, 90Zr, 120Sn, 208Pb targets.
doi: 10.1103/PhysRevC.94.034606
2015LI35 Phys.Rev. C 92, 034312 (2015) Relativistic effects in three-nucleon forces for nuclear matter and finite nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated single-particle energies, binding energies, occupation probabilities, and radius of the charge distribution. Relativistic Dirac-Brueckner-Hartree-Fock (DBHF) approach using realistic NN interaction plus Urbana three-nucleon (3N) force, and rearrangement terms for nuclear matter and finite nuclei.
doi: 10.1103/PhysRevC.92.034312
2014VA13 Phys.Rev. C 90, 034312 (2014) Triaxial deformation in nuclei with realistic NN interactions NUCLEAR STRUCTURE 18,20,22,24,26,28,30,32,34Ne; calculated binding energies, neutron and proton single-particle energies, Fermi energies and rms radii, energy gaps, deformations, S(2n). Transition to pasta phase. 24,42Ne; calculated neutron and proton density distribution contours. Realistic NN interaction and Hartree-Fock approach. Comparison with experimental results.
doi: 10.1103/PhysRevC.90.034312
2013VA04 Phys.Rev. C 87, 024317 (2013) Spinodal instabilities in asymmetric nuclear matter based on realistic NN interactions
doi: 10.1103/PhysRevC.87.024317
2012XU03 Phys.Rev. C 85, 034613 (2012) R.Xu, Z.Ma, E.N.E.van Dalen, H.Muther Relativistic nucleon optical potentials with isospin dependence in a Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 27Al(n, n), (p, p), E=0.1-250 MeV; calculated Schrodinger equivalent central potential, spin-orbit, and Darwin potentials as function of incident energy and deformation parameter, σ(θ, E), vector analyzing powers. Relativistic microscopical optical potential (RMOP) method in the framework of Dirac-Brueckner-Hartree-Fock (DBHF). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.034613
2011DU21 Phys.Rev. C 84, 044319 (2011) H.Dussan, S.J.Waldecker, W.H.Dickhoff, H.Muther, A.Polls Microscopic self-energy of 40Ca from the charge-dependent Bonn potential NUCLEAR STRUCTURE 40Ca; calculated spectral functions, single-particle levels, spectroscopic factors, natural orbits; comparison of microscopic CD Bonn Self-Energy and Dispersive Optical Model fit. 40Ca(n, n), E=0-100 MeV; calculated total and differential cross sections. Comparison with experimental data; analyzed non-locality of the imaginary part of the CD Bonn Self-energy.
doi: 10.1103/PhysRevC.84.044319
2011VA10 Phys.Rev. C 84, 024320 (2011) Relativistic description of finite nuclei based on realistic NN interactions NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr; calculated binding energies per nucleon, charge radii, spin-orbit splittings, proton density distribution for 16O. Density-dependent relativistic Hartree (DDRH), and density-dependent relativistic HF (DDRHF) theories. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.024320
2010GR05 Phys.Rev. C 82, 014315 (2010) P.Grygorov, E.N.E.van Dalen, H.Muther, J.Margueron Separable form of a low-momentum realistic NN interaction
doi: 10.1103/PhysRevC.82.014315
2010VA09 Phys.Rev. C 82, 014319 (2010) Off-shell behavior of nucleon self-energy in asymmetric nuclear matter
doi: 10.1103/PhysRevC.82.014319
2010VA15 Int.J.Mod.Phys. E19, 2077 (2010) Relativistic effects in nuclear matter and nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated binding energies, radii. Dirac-Brueckner-Hartee-Fock approach, comparison with experimental data.
doi: 10.1142/S0218301310016533
2009GO04 Phys.Rev. C 79, 024308 (2009) P.Gogelein, E.N.E.van Dalen, Kh.Gad, Kh.S.A.Hassaneen, H.Muther Properties of asymmetric nuclear matter in different approaches
doi: 10.1103/PhysRevC.79.024308
2009SI11 Phys.Rev. C 79, 055501 (2009) F.Simkovic, A.Faessler, H.Muther, V.Rodin, M.Stauf 0ν ΒΒ-decay nuclear matrix elements with self-consistent short-range correlations RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128Te, 130Te, 136Xe(2β-); calculated nucleon wave function, ratio of neutrino potentials and nuclear matrix elements for neutrinoless double beta decay using renormalized quasiparticle random phase approximation (RQRPA) and standard QRPA methods.
doi: 10.1103/PhysRevC.79.055501
2009VA11 Phys.Rev. C 80, 037303 (2009) Nuclear saturation with low momentum interactions
doi: 10.1103/PhysRevC.80.037303
2009VA12 Phys.Rev. C 80, 044312 (2009) E.N.E.van Dalen, P.Gogelein, H.Muther Bulk properties of nuclei and realistic NN interactions NUCLEAR STRUCTURE 16O, 40,48,60Ca, 208Pb; calculated density distributions, binding energy, rms radii, single-particle energies, and neutron and proton wave functions using Hartree-Fock approach with realistic nucleon-nucleon interaction, interaction model and unitary-model operator method.
doi: 10.1103/PhysRevC.80.044312
2008GO04 Phys.Rev. C 77, 025802 (2008) P.Gogelein, E.N.E.van Dalen, C.Fuchs, H.Muther Nuclear matter in the crust of neutron stars derived from realistic NN interaction
doi: 10.1103/PhysRevC.77.025802
2008RI06 Phys.Rev. C 78, 044314 (2008) A.Rios, A.Polls, A.Ramos, H.Muther Liquid-gas phase transition in nuclear matter from realistic many-body approaches
doi: 10.1103/PhysRevC.78.044314
2007GO25 Phys.Rev. C 76, 024312 (2007) Nuclear matter in the crust of neutron stars
doi: 10.1103/PhysRevC.76.024312
2007RI04 Nucl.Phys. A782, 346c (2007) A.Rios, A.Polls, A.Ramos, H.Muther The entropy of a correlated system of nucleons
doi: 10.1016/j.nuclphysa.2006.10.066
2007RI06 Prog.Part.Nucl.Phys. 59, 311 (2007) A.Rios, A.Polls, A.Ramos, H.Muther The entropy of a correlated system of nucleons
doi: 10.1016/j.ppnp.2006.12.031
2007SE16 Phys.Rev. C 76, 055805 (2007) A.Sedrakian, H.Muther, P.Schuck Vertex renormalization of weak interactions and Cooper-pair breaking in cooling compact stars
doi: 10.1103/PhysRevC.76.055805
2006BO17 Phys.Rev. C 74, 014303 (2006) Correlations and effective interactions in nuclear matter
doi: 10.1103/PhysRevC.74.014303
2006RI02 Phys.Rev. C 73, 024305 (2006) Sum rules and correlations in asymmetric nuclear matter
doi: 10.1103/PhysRevC.73.024305
2006RI12 Phys.Rev. C 74, 054317 (2006) A.Rios, A.Polls, A.Ramos, H.Muther Entropy of a correlated system of nucleons
doi: 10.1103/PhysRevC.74.054317
2006SE01 Nucl.Phys. A766, 97 (2006) A.Sedrakian, H.Muther, P.Schuck Alpha matter on a lattice
doi: 10.1016/j.nuclphysa.2005.11.025
2005BO17 Ann.Phys.(New York) 318, 245 (2005) P.Bozek, J.Margueron, H.Muther Dynamical response functions in correlated fermionic systems
doi: 10.1016/j.aop.2005.01.001
2005FR01 Phys.Rev. C 71, 014313 (2005) T.Frick, H.Muther, A.Rios, A.Polls, A.Ramos Correlations in hot asymmetric nuclear matter
doi: 10.1103/PhysRevC.71.014313
2005MU29 Phys.Rev. C 72, 054313 (2005) Pairing properties of nucleonic matter employing dressed nucleons
doi: 10.1103/PhysRevC.72.054313
2004FR15 Phys.Rev. C 69, 054305 (2004) Sum rules and short-range correlations in nuclear matter at finite temperature
doi: 10.1103/PhysRevC.69.054305
2004FR27 Phys.Rev. C 70, 024309 (2004) T.Frick, Kh.S.A.Hassaneen, D.Rohe, H.Muther Spectral function at high missing energies and momenta NUCLEAR REACTIONS 12C(e, e'p), E not given; calculated spectral function.
doi: 10.1103/PhysRevC.70.024309
2004HA52 Phys.Rev. C 70, 054308 (2004) Correlations and spectral functions in asymmetric nuclear matter
doi: 10.1103/PhysRevC.70.054308
2004MO25 Phys.Rev. C 69, 065801 (2004) Mean field and pairing properties in the crust of neutron stars
doi: 10.1103/PhysRevC.69.065801
2004MU29 Phys.Rev. C 70, 041301 (2004) Correlated nucleons in configuration space NUCLEAR REACTIONS 12C(e, e), (e, e'p), E not given; analyzed data. 12C deduced quasiparticle densities, short-range correlation effects.
doi: 10.1103/PhysRevC.70.041301
2003FR21 Phys.Rev. C 68, 034310 (2003) Self-consistent solution to the nuclear many-body problem at finite temperature
doi: 10.1103/PhysRevC.68.034310
2003KU16 Nucl.Phys. A723, 32 (2003) J.Kuckei, F.Montani, H.Muther, A.Sedrakian The structure of nuclear systems derived from low momentum nucleon-nucleon potentials NUCLEAR STRUCTURE 16O; calculated single-particle energies, occupation probabilities, related features. Effective interactions, low-momentum nucleon-nucleon potential.
doi: 10.1016/S0375-9474(03)01229-6
2003MU01 Phys.Rev. C 67, 015802 (2003) Phases of asymmetric nuclear matter with broken space symmetries
doi: 10.1103/PhysRevC.67.015802
2003SE09 Phys.Lett. B 576, 68 (2003) A.Sedrakian, T.T.S.Kuo, H.Muther, P.Schuck Pairing in nuclear systems with effective Gogny and Vlow-k interactions
doi: 10.1016/j.physletb.2003.09.090
2002FR06 Phys.Rev. C65, 034316 (2002) T.Frick, S.Kaiser, H.Muther, A.Polls, D.R.Entem, R.Machleidt Δ(1232) Isobar Excitations and the Ground State of Nuclei NUCLEAR STRUCTURE 16O; calculated ground-state binding energy, radius, Δ probability.
doi: 10.1103/PhysRevC.65.034316
2002FR07 Phys.Rev. C65, 034321 (2002) T.Frick, Kh.Gad, H.Muther, P.Czerski Nuclear Self-Energy and Realistic Interactions
doi: 10.1103/PhysRevC.65.034321
2002FR09 Phys.Rev. C65, 061303 (2002); Comment Phys.Rev. C 69, 049801 (2004) T.Frick, H.Muther, A.Sedrakian Interaction Induced Deformation of the Momentum Distribution of Spin Polarized Nuclear Matter
doi: 10.1103/PhysRevC.65.061303
2002GA42 Phys.Rev. C66, 044301 (2002) Ground state of finite nuclei evaluated from realistic interactions NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energies, single-particle energies, spectral functions. Brueckner-Hartree-Fock approximation.
doi: 10.1103/PhysRevC.66.044301
2002MU08 Phys.Rev.Lett. 88, 252503 (2002) Spontaneous Breaking of Rotational Symmetry in Superconductors
doi: 10.1103/PhysRevLett.88.252503
2001FR15 Phys.Rev. C64, 014309 (2001) T.Frick, S.Kaiser, H.Muther, A.Polls Δ(1232) Isobar Excitations in Nuclear Many-Body Systems Derived from Various NN Interactions NUCLEAR STRUCTURE 2H, 16O; calculated Δ isobar contributions to wave functions. Coupled-cluster theory.
doi: 10.1103/PhysRevC.64.014309
2001KN01 Phys.Rev. C63, 044602 (2001) Final State Interaction in Exclusive (e, e'NN) Reactions
doi: 10.1103/PhysRevC.63.044602
2001MA16 Phys.Rev. C63, 034005 (2001) Charge Symmetry Breaking of the Nucleon-Nucleon Interaction: ρ-ω Mixing versus nucleon mass splitting NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference, role of charge symmetry breaking. 16O calculated Coulomb displacement energies. Comparison of three charge symmetry breaking models.
doi: 10.1103/PhysRevC.63.034005
2001SC32 Eur.Phys.J. A 11, 15 (2001) Correlations and the Dirac Structure of the Nucleon Self-Energy
doi: 10.1007/s100500170092
2001SH01 Phys.Rev. C63, 014303 (2001) Y.Y.Sharon, M.S.Fayache, Y.D.Devi, L.Zamick, H.Muther Dependence of the Shell-Model Single-Particle Energies on Different Components of the Nucleon-Nucleon Interaction NUCLEAR STRUCTURE A=5; A=15; A=17; calculated levels spin-orbit splitting; deduced role of nucleon-nucleon interactions. Shell model.
doi: 10.1103/PhysRevC.63.014303
2000GA42 Trans.Bulg.Nucl.Soc. 5, 188 (2000) M.K.Gaidarov, K.A.Pavlova, A.N.Antonov, S.S.Dimitrova, M.V.Stoitsov, C.Giusti, D.Van Neck, H.Muther New Theoretical Treatment of One-Nucleon Transfer Reactions NUCLEAR REACTIONS 16O(p, d), E=31.8, 45.3, 65 MeV; 16O(e, e'p), E=520.6 MeV; 16O(γ, p), E=60 MeV; calculated single-particle overlap functions, σ(θ). comparisons with data.
2000KN01 Phys.Rev. C61, 064603 (2000) D.Knodler, H.Muther, P.Czerski Nucleon-Nucleon Correlations and Two-Nucleon Currents in Exclusive (e, e'NN) Reactions
doi: 10.1103/PhysRevC.61.064603
2000MU01 Phys.Rev. C61, 014304 (2000) Correlations Derived from Modern Nucleon-Nucleon Potentials
doi: 10.1103/PhysRevC.61.014304
2000MU15 Prog.Part.Nucl.Phys. 45, 243 (2000) Two-Body Correlations in Nuclear Systems
doi: 10.1016/S0146-6410(00)00105-8
1999FA15 Phys.Rev. C60, 067305 (1999) M.S.Fayache, L.Zamick, H.Muther Vanishing Gamow-Teller Transition Rate for A = 14 and the Nucleon-Nucleon Interaction in the Medium NUCLEAR STRUCTURE 14C, 14N, 14O; calculated Gamow-Teller transition rate; deduced effective nucleon-nucleon interaction features.
doi: 10.1103/PhysRevC.60.067305
1999GA27 Phys.Rev. C60, 024312 (1999) M.K.Gaidarov, K.A.Pavlova, S.S.Dimitrova, M.V.Stoitsov, A.N.Antonov, D.Van Neck, H.Muther Correlation Effects in Single-Particle Overlap Functions and One-Nucleon Removal Reactions NUCLEAR STRUCTURE 16O; calculated single-particle overlap functions, spectroscopic factors, separation energies. NUCLEAR REACTIONS 16O(p, d), E=31.8, 45.3, 65 MeV; calculated σ(θ). Single-particle overlap functions, comparison with data.
doi: 10.1103/PhysRevC.60.024312
1999GI15 Phys.Rev. C60, 054608 (1999) C.Giusti, H.Muther, F.D.Pacati, M.Stauf Short-Range and Tensor Correlations in the 16O(e, e'pn) Reaction NUCLEAR REACTIONS 16O(e, e'np), E=855 MeV; calculated σ(E, θ) vs recoil momentum; deduced role of nucleon-nucleon correlations, two-body meson exchange currents.
doi: 10.1103/PhysRevC.60.054608
1999HA33 Phys.Lett. 459B, 1 (1999) C.Harzer, H.Muther, R.Machleidt Modern Nucleon-Nucleon Interactions and Charge-Symmetry Breaking in Nuclei NUCLEAR STRUCTURE 16O; calculated single-particle levels binding energies, spectroscopic factors; deduced correlation, charge-symmetry breaking effects. Several NN potentials compared.
doi: 10.1016/S0370-2693(99)00670-X
1999MU02 Phys.Lett. 445B, 259 (1999) H.Muther, A.Polls, R.Machleidt Isospin Symmetry Breaking Nucleon-Nucleon Potentials and Nuclear Structure
doi: 10.1016/S0370-2693(98)01499-3
1999MU11 Int.J.Mod.Phys. E8, 179 (1999) Correlations and the Relativistic Structure of the Nucleon Self-Energy
doi: 10.1142/S0218301399000148
1999SC09 Phys.Rev. C59, 2934 (1999); Erratum Phys.Rev. C60, 059901 (1999) E.Schiller, H.Muther, P.Czerski Pauli Exclusion Operator and Binding Energy of Nuclear Matter
doi: 10.1103/PhysRevC.59.2934
1998GI05 Phys.Rev. C57, 1691 (1998) C.Giusti, F.D.Pacati, K.Allaart, W.J.W.Geurts, W.H.Dickhoff, H.Muther Selectivity of the 16O(e, e'pp) Reaction to Discrete Final States NUCLEAR REACTIONS 16O(e, e'2p), E=475, 584, 855 MeV; calculated σ(E, θ); deduced final state selectivity.
doi: 10.1103/PhysRevC.57.1691
1998ON02 Phys.Rev.Lett. 81, 2213 (1998) C.J.G.Onderwater, K.Allaart, E.C.Aschenauer, Th.S.Bauer, D.J.Boersma, E.Cisbani, W.H.Dickhoff, S.Frullani, F.Garibaldi, W.J.W.Geurts, C.Giusti, D.L.Groep, W.H.A.Hesselink, M.Iodice, E.Jans, N.Kalantar-Nayestanaki, W.-J.Kasdorp, C.Kormanyos, L.Lapikas, J.J.van Leeuwe, R.De Leo, A.Misiejuk, H.Muther, F.D.Pacati, A.R.Pellegrino, R.Perrino, R.Starink, M.Steenbakkers, G.van der Steenhoven, J.J.M.Steijger, M.A.van Uden, G.M.Urciuoli, L.B.Weinstein, H.W.Willering Signatures for Short-Range Correlations in 16O Observed in the Reaction 16O(e, e'pp)14C NUCLEAR REACTIONS 16O(e, e'2p), E=584 MeV; measured σ(Ee, θ(e), Ep, θ(p)), missing momentum; deduced short-range correlations role.
doi: 10.1103/PhysRevLett.81.2213
1998PO12 Phys.Lett. 432B, 1 (1998) A.Polls, H.Muther, R.Machleidt, M.Hjorth-Jensen Phaseshift Equivalent NN Potentials and the Deuteron NUCLEAR STRUCTURE 2H; calculated S-wave, D-wave momentum distributions; deduced one-pion exchange contribution effect. Several NN potentials compared.
doi: 10.1016/S0370-2693(98)00628-5
1998TR09 Nucl.Phys. A640, 471 (1998) A.Trasobares, A.Polls, A.Ramos, H.Muther On the Dirac Structure of the Nucleon Self-Energy in Nuclear Matter
doi: 10.1016/S0375-9474(98)00471-0
1998UL01 Nucl.Phys. A641, 499 (1998) Study of Relativistic Bound State Wave Functions in Quasielastic (e, e'p) Reactions NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated response functions vs missing momentum; deduced sensitivity to bound-state wave functions. Relativistic Hartree, relativistic Hartree-Fock, density-dependent relativistic Hartree calculations. NUCLEAR STRUCTURE 16O; calculated single-particle energies, radius. Relativistic Hartree, relativistic Hartree-Fock, density-dependent relativistic Hartree calculations.
doi: 10.1016/S0375-9474(98)00537-5
1997AM08 Nucl.Phys. A625, 633 (1997) K.Amir-Azimi-Nili, J.M.Udias, H.Muther, L.D.Skouras, A.Polls Correlations and the Cross Section of Exclusive (e, e'p) Reactions for 16O NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated reduced σ vs missing momentum; deduced long-range correlations role. DWIA analysis. Comparison with data.
doi: 10.1016/S0375-9474(97)00595-2
1997EN07 Nucl.Phys. A627, 85 (1997) L.Engvik, M.Hjorth-Jensen, R.Machleidt, H.Muther, A.Polls Modern Nucleon-Nucleon Potentials and Symmetry Energy in Infinite Matter
doi: 10.1016/S0375-9474(97)00496-X
1997PO01 Phys.Rev. C55, 810 (1997) A.Polls, M.Radici, S.Boffi, W.H.Dickhoff, H.Muther High-Momentum Proton Removal from 16O and the (e, e'p) Cross Section NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated reduced σ vs missing momentum. Single-hole spectral function evaluated with short-range, tensor correlations.
doi: 10.1103/PhysRevC.55.810
1997UL01 Phys.Rev. C56, 1788 (1997) Relativistic Structure of the Nucleon Self-Energy in Asymmetric Nuclei NUCLEAR STRUCTURE 16,22O; calculated nucleon energy, charge distribution. Dirac-Hartree approach, density dependent coupling constants.
doi: 10.1103/PhysRevC.56.1788
1996AM05 Nucl.Phys. A604, 245 (1996) K.Amir-Azimi-Nili, H.Muther, L.D.Skouras, A.Polls Long-Range Correlations and the Momentum Distribution in Nuclei NUCLEAR STRUCTURE 16O; calculated binding energy per nucleon, nucleon distribution radius, particle number. Green's function approach, long-range correlations.
doi: 10.1016/0375-9474(96)00142-X
1996BA71 Phys.Lett. 386B, 7 (1996) G.Bartnitzky, H.Clement, P.Czerski, H.Muther, F.Nuoffer, J.Siegler A Microscopic Energy- and Density-Dependent Effective Interaction and Its Test by Nucleus-Nucleus Scattering NUCLEAR REACTIONS 16O(16O, 16O), E=704 MeV; calculated real potential. 40Ca, 208Pb(p, p), 208Pb(α, α), 16O(16O, 16O), E=22-44 MeV/nucleon; calculated real central scattering potentials. Microscopic energy-, density-dependent effective interaction.
doi: 10.1016/0370-2693(96)00969-0
1996FE12 Nucl.Phys. A611, 514 (1996) P.Fernandez de Cordoba, E.Marco, H.Muther, E.Oset, A.Faessler Deep Inelastic Lepton Scattering in Nuclei at x > 1 and the Nucleon Spectral Function NUCLEAR STRUCTURE 12C, 56Fe, 40Ca, 16O, 6Li; calculated structure functions, also per nucleon in some cases.
doi: 10.1016/S0375-9474(96)00249-7
1996GE01 Phys.Rev. C53, 2207 (1996) W.J.W.Geurts, K.Allaart, W.H.Dickhoff, H.Muther Spectroscopic Factors for Nucleon Knock-Out from 16O at Small Missing Energy NUCLEAR STRUCTURE 16O; calculated one-nucleon knock-out spectroscopic factors. Green's function formalism.
doi: 10.1103/PhysRevC.53.2207
1996GE03 Phys.Rev. C54, 1144 (1996) W.J.W.Geurts, K.Allaart, W.H.Dickhoff, H.Muther Two-Nucleon Spectral Function of 16O at High Momenta NUCLEAR STRUCTURE 16O; calculated two-nucleon spectral functions. NUCLEAR REACTIONS 16O(e, e'X), E=700 MeV; calculated longitudinal differential σ for 2p knockout. Plane wave approximation.
doi: 10.1103/PhysRevC.54.1144
1996HJ02 J.Phys.(London) G22, 321 (1996) M.Hjorth-Jensen, H.Muther, E.Osnes, A.Polls Comparison of the Effective Interaction to Various Orders in Different Mass Regions NUCLEAR STRUCTURE 4He, 16O, 40Ca, 100Sn, 208Pb; calculated diagonal, nondiagonal matrix elements, mean value ratios; deduced higher-order terms contributions stability mass dependence. Effective interaction to various orders, shell model.
doi: 10.1088/0954-3899/22/3/006
1996HJ03 Nucl.Phys. A605, 458 (1996) M.Hjorth-Jensen, A.Polls, A.Ramos, H.Muther Self-Energy of Λ in Finite Nuclei NUCLEAR STRUCTURE 17O; calculated strange baryon (Λ) self-energy. Microscopic many-body approach.
doi: 10.1016/0375-9474(96)00190-X
1996KU20 Nucl.Phys. A606, 15 (1996); Erratum Nucl.Phys. A611, 587 (1996) T.T.S.Kuo, H.Muther, K.Amir-Azimi-Nili Realistic Effective Interactions for Halo Nuclei NUCLEAR STRUCTURE 6He, 6Li; calculated valence energies. Two-frequency shell model.
doi: 10.1016/0375-9474(96)00205-9
1995GI04 Nucl.Phys. A584, 621 (1995) A.Gil, M.Kleinmann, H.Muther, E.Oset The Axial Charge Renormalization in a Relativistic Description of Finite Nuclei NUCLEAR STRUCTURE 16O; calculated axial charge form factor, relativistic to nonrelativistic matrix elements ratio for 0+ → 0- transition. 40Ca; calculated relativistic to nonrelativistic matrix elements ratio for 0+ → 0- transition. One-boson-exchange model, Dirac-Brueckner-Hartree-Fock approach based relativistic mean field.
doi: 10.1016/0375-9474(94)00517-Q
1995HE10 Nucl.Phys. A587, 77 (1995) E.Heinz, H.Muther, H.A.Mavromatis Collective Excitations and Ground State Correlations NUCLEAR STRUCTURE 16O; calculated correlation energies, single particle orbit occupation probabilities, radius. Generalized RPA.
doi: 10.1016/0375-9474(94)00807-Y
1995MU02 Nucl.Phys. A581, 247 (1995) Long-Range Correlations in Closed-Shell Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energy/nucleon. Large model space, long range correlations.
doi: 10.1016/0375-9474(94)00438-S
1995MU09 Phys.Rev. C51, 3040 (1995) H.Muther, A.Polls, W.H.Dickhoff Momentum and Energy Distributions of Nucleons in Finite Nuclei Due to Short-Range Correlations NUCLEAR STRUCTURE 16O; calculated nucleon momentum, energy distributions. Short range correlations, realistic meson-exchange potential.
doi: 10.1103/PhysRevC.51.3040
1995MU19 Phys.Rev. C52, 2955 (1995) Momentum Distribution in Nuclear Matter and Finite Nuclei
doi: 10.1103/PhysRevC.52.2955
1995PO13 Nucl.Phys. A594, 117 (1995) Short-Range Correlations and the One-Body Density Matrix in Finite Nuclei NUCLEAR STRUCTURE 16O; calculated nucleons momentum distributions. Quasihole approximation, continuum part included.
doi: 10.1016/0375-9474(95)00380-J
1995ZH11 Phys.Rev. C51, 2471 (1995) D.C.Zheng, B.R.Barrett, J.P.Vary, H.Muther Auxiliary Potential in No-Core Shell-Model Calculations NUCLEAR STRUCTURE 4He; calculated ground state energy. No-core shell model, Lee-Suzuki iteration method.
doi: 10.1103/PhysRevC.51.2471
1994CZ01 J.Phys.(London) G20, 425 (1994) P.Czerski, H.Muther, W.H.Dickhoff Effective Local Interactions and the Equation of State for Nuclear Matter and Finite Nuclei NUCLEAR STRUCTURE 16O; calculated binding energy per nucleon, two-nucleon density. Equation of state, effective nuclear interactions.
doi: 10.1088/0954-3899/20/3/004
1994DO25 J.Phys.(London) G20, 1885 (1994) On the Analytic Structure of the Quark Self-Energy in Nambu-Jona-Lasinio Models
doi: 10.1088/0954-3899/20/12/005
1994FR02 Phys.Rev. C49, 633 (1994) NN Correlations and Relativistic Hartree-Fock in Finite Nuclei NUCLEAR STRUCTURE 16O, 48,40Ca; calculated proton single particle state energy, binding energy per nucleon; deduced NN-correlations role. Relativistic Brueckner Hartree-Fock equation, effective meson exchange parametrization.
doi: 10.1103/PhysRevC.49.633
1994HJ02 Phys.Rev. C50, 501 (1994) M.Hjorth-Jensen, H.Muther, A.Polls Width of the Δ Resonance in Nuclei NUCLEAR STRUCTURE 40Ca, 16O, 100Sn; calculated two-body absorption component of Δ self-energy vs distance from center of nucleus, imaginary part vs deposited energy.
doi: 10.1103/PhysRevC.50.501
1994KL05 Nucl.Phys. A579, 85 (1994) M.Kleinmann, R.Fritz, H.Muther, A.Ramos On the Momentum Dependence of the Nucleon-Nucleus Optical Potential NUCLEAR STRUCTURE 40Ca, 16O; calculated optical potential, density distribution. Relativistic, non-relativistic approach. NUCLEAR REACTIONS 40Ca, 16O(n, n), (p, p), E ≤ 150 MeV; calculated phase shift. Relativistic, non-relativistic approach.
doi: 10.1016/0375-9474(94)90795-1
1994MU01 Phys.Rev. C49, R17 (1994) Single-Particle Spectral Function of 16O NUCLEAR STRUCTURE 16O; calculated single particle spectral function; deduced short range correlations role.
doi: 10.1103/PhysRevC.49.R17
1994ZH13 Ann.Phys.(New York) 230, 118 (1994) D.C.Zheng, L.Zamick, M.S.Fayache, H.Muther Medium Corrections to the Tensor Interaction in Nuclei: Energy difference of T = 1 and T = 0 J(π) = 0- states in 16O NUCLEAR STRUCTURE 16O; calculated levels; deduced 0- level isospin splitting sensitivity to T=1 tensor force. Realistic G-matrices, medium corrections, shell model.
doi: 10.1006/aphy.1994.1019
1993CE01 Phys.Rev. C47, 1091 (1993) M.Centelles, X.Vinas, M.Barranco, N.Ohtsuka, A.Faessler, D.T.Khoa, H.Muther Relativistic Extended Thomas-Fermi Calculations of Finite Nuclei with Realistic Nucleon-Nucleon Interactions NUCLEAR STRUCTURE 12C, 16O, 40,48Ca, 56Ni, 90Zr, 114,118Sn, 140Ce, 208Pb; calculated binding energy, charge radius. 52Fe, 118Sn, 152Dy, 186Os, 207Bi, 240Pu; calculated fission barrier, saddle point quadrupole moment, critical angular momentum, equidensity lines. Relativistic extended Thomas-Fermi calculations, realistic interactions. NUCLEAR REACTIONS 12C(12C, 12C), E=2.4 GeV; 28Si, 12C(16O, 16O), E=1.503 GeV; calculated σ(θ). Relativistic extended Thomas-Fermi calculations, realistic interactions.
doi: 10.1103/PhysRevC.47.1091
1993FR08 Phys.Rev.Lett. 71, 46 (1993) R.Fritz, H.Muther, R.Machleidt Dirac Effects in the Hartree-Fock Description of Finite Nuclei Employing Realistic Forces NUCLEAR STRUCTURE 16O, 40Ca; calculated total energy per nucleon, charge radius, proton single particle energies. Relativistic Brueckner-Hartree-Fock equation.
doi: 10.1103/PhysRevLett.71.46
1993LI36 Phys.Rev. C48, 2443 (1993) G.Q.Li, R.Machleidt, R.Fritz, H.Muther, Y.Z.Zhuo Relativistic Microscopic Description of Proton-Nucleus Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=150-450 MeV; calculated σ(θ), analyzing power vs θ. Relativistic, microscopic approach.
doi: 10.1103/PhysRevC.48.2443
1993MU04 Nucl.Phys. A555, 541 (1993) Low-Energy Excitations and Occupation Probabilities NUCLEAR STRUCTURE 16O; calculated single particle strength distribution; deduced fragmentation. Green function, shell model approaches comparison, realistic nucleon-nucleon interaction.
doi: 10.1016/0375-9474(93)90487-I
1993MU07 Phys.Lett. 306B, 201 (1993) Correlations in Nuclei. Self-Consistent Treatment and the BAGEL Approach NUCLEAR STRUCTURE 16O; calculated single particle energies, occupation probabilities, strengths. Self-consistent treatment.
doi: 10.1016/0370-2693(93)90068-S
1993SK05 Nucl.Phys. A561, 157 (1993) L.D.Skouras, H.Muther, M.A.Nagarajan Determination of Dipole Polarization Effects in 7Li and 11Li NUCLEAR STRUCTURE 6,7Li; calculated μ, quadrupole moment, rms radii, B(λ). 11Li; calculated μ, quadrupole moment, rms radii. Shell model.
doi: 10.1016/0375-9474(93)90148-Q
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