NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.Machleidt Found 90 matches. 2023MA52 Few-Body Systems 64, 77 (2023) What is ab initio? NUCLEAR STRUCTURE 16,24O, 36,40,48,52,60Ca, 48,56,68,78Ni; analyzed available data; deduced ground-state energies per nucleon and point-proton rms radii in the "Huther" case.
doi: 10.1007/s00601-023-01857-2
2023SA11 Phys.Rev. C 107, 034002 (2023) S.K.Saha, D.R.Entem, R.Machleidt, Y.Nosyk Local position-space two-nucleon potentials from leading to fourth order of chiral effective field theory NUCLEAR REACTIONS 1H(p, X), (n, X), E<290 MeV; calculated phase shifts, cutoff variations for phase shifts, scattering lengths, effective ranges. Local, position-space chiral NN potential through four orders of chiral effective field theory ranging from LO to N3LO. Comparison with phenomenological Argonne ν18 (AV18) potential. NUCLEAR STRUCTURE 2H; calculated binding energy, asymptotic S state, asymptotic D/S state, quadrupole moment, D-state probability from the nucleon-nucleon potentials of the present study. 3H; calculated binding energy.
doi: 10.1103/PhysRevC.107.034002
2022VO02 Phys.Rev. C 105, 014621 (2022) M.Vorabbi, M.Gennari, P.Finelli, C.Giusti, P.Navratil, R.Machleidt Elastic proton scattering off nonzero spin nuclei NUCLEAR REACTIONS 6,7Li, 13C(polarized p, p), E=200 MeV; 10B(polarized p, p), E=197 MeV; 1H(9C, p), E=290 MeV; calculated σ(θ) and analyzing powers Ay(θ) using microscopic optical potential (OP) and chiral theories for the nucleon-nucleon (NN) interaction, extended to include the spin of the target nucleus. Comparison with experimental data.
doi: 10.1103/PhysRevC.105.014621
2021NO12 Phys.Rev. C 104, 054001 (2021) Y.Nosyk, D.R.Entem, R.Machleidt Nucleon-nucleon potentials from Δ-full chiral effective-field-theory and implications NUCLEAR REACTIONS 1H(n, X), E<200 MeV; calculated neutron-proton scattering phase parameters predicted by Goteborg-Oak Ridge (GO) potentials: NNLO(450)GO, NNLO(394)GO, NNLO(450)Rf and NNLO(394)Rf with fits in the present work, scattering lengths and effective ranges, energy per nucleon in symmetric nuclear matter; investigated chiral nucleon-nucleon potentials at NNLO including Δ-isobar degrees. 2H; predicted binding energy, asymptotic S state, asymptotic D/S state, structure radius, quadrupole moment, D-state probability from the nucleon-nucleon potentials of the present study.
doi: 10.1103/PhysRevC.104.054001
2021VO03 Phys.Rev. C 103, 024604 (2021) M.Vorabbi, M.Gennari, P.Finelli, C.Giusti, P.Navratil, R.Machleidt Impact of three-body forces on elastic nucleon-nucleus scattering observables NUCLEAR REACTIONS 12C(polarized p, p), E=122, 160, 200, 300 MeV; 16O(p, p), (polarized p, p), E=100, 135, 200, 318 MeV; 12C(n, n), E=108, 128, 155, 185, 225 MeV; calculated differential σ(E, θ), and analyzing power Ay(Ε, θ) using nonrelativistic optical model potentials obtained from the no-core shell model densities using two- and three-nucleon chiral interactions; deduced that contribution of the 3N force in the tNN matrix is small for the differential cross section and sizable for the spin observables such as analyzing power. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.024604
2020MA13 Eur.Phys.J. A 56, 95 (2020) Can chiral EFT give us satisfaction?
doi: 10.1140/epja/s10050-020-00101-3
2019MA22 Phys.Rev. C 99, 034003 (2019) L.E.Marcucci, F.Sammarruca, M.Viviani, R.Machleidt Momentum distributions and short-range correlations in the deuteron and 3He with modern chiral potentials NUCLEAR STRUCTURE 2H, 3He; calculated single neutron and proton, neutron-proton, and proton-proton momentum distributions, short-range correlation probabilities using two-nucleon (2N) and 2N+3N chiral potentials (LO, NLO, N2LO, N3LO, N4LO) with and without leading chiral three-nucleon force; deduced model dependence of one- and two-body momentum distributions and the impact of three body forces. Comparison with previous theoretical predictions.
doi: 10.1103/PhysRevC.99.034003
2017EN03 Phys.Rev. C 96, 024004 (2017) D.R.Entem, R.Machleidt, Y.Nosyk High-quality two-nucleon potentials up to fifth order of the chiral expansion
doi: 10.1103/PhysRevC.96.024004
2015EN01 Phys.Rev. C 91, 014002 (2015) D.R.Entem, N.Kaiser, R.Machleidt, Y.Nosyk Peripheral nucleon-nucleon scattering at fifth order of chiral perturbation theory
doi: 10.1103/PhysRevC.91.014002
2015EN05 Phys.Rev. C 92, 064001 (2015) D.R.Entem, N.Kaiser, R.Machleidt, Y.Nosyk Dominant contributions to the nucleon-nucleon interaction at sixth order of chiral perturbation theory
doi: 10.1103/PhysRevC.92.064001
2015SA22 Phys.Rev. C 91, 054311 (2015) F.Sammarruca, L.Coraggio, J.W.Holt, N.Itaco, R.Machleidt, L.E.Marcucci Toward order-by-order calculations of the nuclear and neutron matter equations of state in chiral effective field theory
doi: 10.1103/PhysRevC.91.054311
2015SA44 Phys.Rev. C 92, 054327 (2015) F.Sammarruca, R.Machleidt, N.Kaiser Spin-polarized neutron-rich matter at different orders of chiral effective field theory
doi: 10.1103/PhysRevC.92.054327
2014CO09 Phys.Rev. C 89, 044321 (2014) L.Coraggio, J.W.Holt, N.Itaco, R.Machleidt, L.E.Marcucci, F.Sammarruca Nuclear-matter equation of state with consistent two- and three-body perturbative chiral interactions NUCLEAR STRUCTURE 3H, 3He; calculated neutron-proton phase shifts, binding energy, Gamow-Teller transition matrix element, nuclear matter energy per particle. Equation of state (EOS) for two- and three-body perturbative chiral interactions in the framework of the perturbative Goldstone expansion and regulator functions. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.044321
2014MA89 Phys.Rev. C 90, 054001 (2014) Muon capture on the deuteron and the neutron-neutron scattering length NUCLEAR REACTIONS 2H(μ-, ν)2n, E not given; 3He(μ-, ν)3H, E not given; calculated muon capture rates μ-2 and μ-3 with nuclear potentials and charge-changing weak currents derived within chiral EFT. Relevance to MuSun experimental collaboration at PSI.
doi: 10.1103/PhysRevC.90.054001
2013CO02 Phys.Rev. C 87, 014322 (2013) L.Coraggio, J.W.Holt, N.Itaco, R.Machleidt, F.Sammarruca Reduced regulator dependence of neutron-matter predictions with perturbative chiral interactions
doi: 10.1103/PhysRevC.87.014322
2013DO05 Phys.Rev. C 87, 054332 (2013) H.Dong, T.T.S.Kuo, H.K.Lee, R.Machleidt, M.Rho Half-Skyrmions and the equation of state for compact-star matter
doi: 10.1103/PhysRevC.87.054332
2013EK01 Phys.Rev.Lett. 110, 192502 (2013) A.Ekstrom, G.Baardsen, C.Forssen, G.Hagen, M.Hjorth-Jensen, G.R.Jansen, R.Machleidt, W.Nazarewicz, T.Papenbrock, J.Sarich, S.M.Wild Optimized Chiral Nucleon-Nucleon Interaction at Next-to-Next-to-Leading Order NUCLEAR STRUCTURE 3H, 3,4He, 10B, 17,22,24O, 40,48,50,52,54,56Ca; calculated energy of the first 2+ state, energy per nucleon for neutron matter, phase shifts. The nucleon-nucleon interaction from chiral effective field theory at next-to-next-to-leading order (NNLO).
doi: 10.1103/PhysRevLett.110.192502
2013MA80 Phys.Rev. C 88, 054002 (2013) E.Marji, A.Canul, Q.MacPherson, R.Winzer, Ch.Zeoli, D.R.Entem, R.Machleidt Nonperturbative renormalization of the chiral nucleon-nucleon interaction up to next-to-next-to-leading order
doi: 10.1103/PhysRevC.88.054002
2012HA19 Phys.Rev.Lett. 108, 242501 (2012) G.Hagen, M.Hjorth-Jensen, G.R.Jansen, R.Machleidt, T.Papenbrock Continuum Effects and Three-Nucleon Forces in Neutron-Rich Oxygen Isotopes NUCLEAR STRUCTURE 18,22,23,24O; calculated level energies, J, π, point matter and charge radii, 24O long-lived resonances. Chiral effective field interaction, comparison with available data.
doi: 10.1103/PhysRevLett.108.242501
2012HA26 Phys.Rev.Lett. 109, 032502 (2012) G.Hagen, M.Hjorth-Jensen, G.R.Jansen, R.Machleidt, T.Papenbrock Evolution of Shell Structure in Neutron-Rich Calcium Isotopes NUCLEAR STRUCTURE 42,48,50,52,53,54,55,56,61Ca, 50,54,56Ti; calculated ground state energies, J, π. Chiral effective field theory, comparison with available data.
doi: 10.1103/PhysRevLett.109.032502
2012SA51 Phys.Rev. C 86, 054317 (2012) F.Sammarruca, B.Chen, L.Coraggio, N.Itaco, R.Machleidt Dirac-Brueckner-Hartree-Fock versus chiral effective field theory
doi: 10.1103/PhysRevC.86.054317
2011DO07 Phys.Rev. C 83, 054002 (2011) H.Dong, T.T.S.Kuo, R.Machleidt Low-momentum interactions with Brown-Rho-Ericson scalings, and the density dependence of the nuclear symmetry energy
doi: 10.1103/PhysRevC.83.054002
2011MA28 Phys.Rep. 503, 1 (2011) Chiral effective field theory and nuclear forces
doi: 10.1016/j.physrep.2011.02.001
2010DO04 Phys.Rev. C 81, 034003 (2010) H.Dong, L.-W.Siu, T.T.S.Kuo, R.Machleidt Unitarity potentials and neutron matter at the unitary limit
doi: 10.1103/PhysRevC.81.034003
2010MA07 Phys.Rev. C 81, 024001 (2010) R.Machleidt, P.Liu, D.R.Entem, E.R.Arriola Renormalization of the leading-order chiral nucleon-nucleon interaction and bulk properties of nuclear matter
doi: 10.1103/PhysRevC.81.024001
2009DO17 Phys.Rev. C 80, 065803 (2009) H.Dong, T.T.S.Kuo, R.Machleidt Neutron stars, β-stable ring-diagram equation of state, and Brown-Rho scaling
doi: 10.1103/PhysRevC.80.065803
2009FO06 Phys.Rev. C 80, 027001 (2009) A.C.Fonseca, R.Machleidt, G.A.Miller Nucleon-nucleon charge symmetry breaking and the dd → απ0 reaction
doi: 10.1103/PhysRevC.80.027001
2008EN01 Phys.Rev. C 77, 044006 (2008) D.R.Entem, E.Ruiz Arriola, M.Pavon Valderrama, R.Machleidt Renormalization of chiral two-pion exchange NN interactions: Momentum space versus coordinate space
doi: 10.1103/PhysRevC.77.044006
2008HO01 Phys.Rev.Lett. 100, 062501 (2008) J.W.Holt, G.E.Brown, T.T.S.Kuo, J.D.Holt, R.Machleidt Shell Model Description of the 14C Dating β Decay with Brown-Rho-Scaled NN Interactions RADIOACTIVITY 14C(β-); calculated Gamow-Teller matrix elements and β-decay half life using the shell model and medium modified Bonn-B potential.
doi: 10.1103/PhysRevLett.100.062501
2008SI08 Phys.Rev. C 77, 034001 (2008) L.-W.Siu, T.T.S.Kuo, R.Machleidt Low-momentum ring diagrams of neutron matter at and near the unitary limit
doi: 10.1103/PhysRevC.77.034001
2007CO04 Phys.Rev. C 75, 024311 (2007) L.Coraggio, A.Covello, A.Gargano, N.Itaco, D.R.Entem, T.T.S.Kuo, R.Machleidt Low-momentum nucleon-nucleon interactions and shell-model calculations NUCLEAR STRUCTURE 18,20,22,24,26O; calculated ground and excited states energies. Low-momentum potential.
doi: 10.1103/PhysRevC.75.024311
2007MA50 Nucl.Phys. A790, 17c (2007) The theory of nuclear forces: Is the never-ending story coming to an end?
doi: 10.1016/j.nuclphysa.2007.03.051
2005CO01 Phys.Rev. C 71, 014307 (2005) L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo, R.Machleidt Nuclear structure calculations and modern nucleon-nucleon potentials NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated binding energies, radii. Several nucleon-nucleon potentials compared.
doi: 10.1103/PhysRevC.71.014307
2005MA58 J.Phys.(London) G31, S1235 (2005) Towards a consistent approach to nuclear structure: EFT of two- and many-body forces
doi: 10.1088/0954-3899/31/8/001
2004EY01 Eur.Phys.J. A 22, 105 (2004) K.O.Eyser, R.Machleidt, W.Scobel Modelling nucleon-nucleon scattering above 1 GeV NUCLEAR REACTIONS 1H(p, p), (p, X), E=0.4-2.5 GeV; calculated phase shifts, σ, analyzing powers. Comparisons with data.
doi: 10.1140/epja/i2004-10014-0
2004MA43 Nucl.Phys. A737, 223 (2004) The nuclear force problem: Are we seeing the end of the tunnel?
doi: 10.1016/j.nuclphysa.2004.03.080
2003BO37 Phys.Lett. B 576, 265 (2003) S.K.Bogner, T.T.S.Kuo, A.Schwenk, D.R.Entem, R.Machleidt Towards a model-independent low momentum nucleon-nucleon interactions
doi: 10.1016/j.physletb.2003.10.012
2003DE19 Phys.Rev. C 68, 024005 (2003) A.Deltuva, R.Machleidt, P.U.Sauer Realistic two-baryon potential coupling two-nucleon and nucleon-Δ-isobar states: Fit and applications to three-nucleon system NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, Δ-isobar effect, nucleon and Δ momentum distributions. NUCLEAR REACTIONS 2H(n, n), (p, p), E=108-190 MeV; 2H(n, np), (p, np), E=65 MeV; calculated σ(θ), analyzing powers. Two-baryon coupled-channels potential.
doi: 10.1103/PhysRevC.68.024005
2003EN09 Phys.Rev. C 68, 041001 (2003) Accurate charge-dependent nucleon-nucleon potential at fourth order of chiral perturbation theory NUCLEAR REACTIONS 1H(n, n), E=0-300 MeV; calculated phase shift parameters, scattering lengths. Fourth-order chiral perturbation theory. NUCLEAR STRUCTURE 2H; calculated binding energy, radius, quadrupole moment, D-state probability. 3H; calculated binding energy. Fourth-order chiral perturbation theory.
doi: 10.1103/PhysRevC.68.041001
2002CO20 Phys.Rev. C66, 021303 (2002) L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo, D.R.Entem, R.Machleidt Microscopic nuclear structure based upon a chiral NN potential NUCLEAR STRUCTURE 18O, 134Te, 210Po; calculated levels, J, π, binding energies. Shell model, chiral effective field theory, comparison with data.
doi: 10.1103/PhysRevC.66.021303
2002EN01 Phys.Lett. 524B, 93 (2002) Accurate Nucleon-Nucleon Potential Based Upon Chiral Perturbation Theory NUCLEAR REACTIONS 1H(n, n), E < 300 MeV; calculated phase shifts. Chiral effective Lagrangians, comparison with data. NUCLEAR STRUCTURE 2,3H; calculated binding energy. 2H calculated radius, quadrupole moment. Chiral effective Lagrangians, comparison with data.
doi: 10.1016/S0370-2693(01)01363-6
2002EN04 Phys.Rev. C65, 064005 (2002) D.R.Entem, R.Machleidt, H.Witala Chiral NN Model and Ay Puzzle NUCLEAR REACTIONS 2H(n, n), (p, p), E=3, 10, 65 MeV; calculated σ(θ), Ay(θ), other polarization observables. Chiral NN model, comparison with data.
doi: 10.1103/PhysRevC.65.064005
2002EN08 Phys.Rev. C66, 014002 (2002) Chiral 2π Exchange at Fourth Order and Peripheral NN Scattering NUCLEAR REACTIONS 1H(n, X), E<300 MeV; calculated phase shifts, two-pion exchange contributions. Effective chiral Lagrangians, fourth-order contributions.
doi: 10.1103/PhysRevC.66.014002
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
2001MA07 Phys.Rev. C63, 024001 (2001) High-Precision, Charge-Dependent Bonn Nucleon-Nucleon Potential NUCLEAR REACTIONS 1H(p, X), (n, X), E=1-350 MeV; calculated scattering potentials, phase shifts. Charge-dependent one-boson-exchange potential, comparison with data.
doi: 10.1103/PhysRevC.63.024001
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
2001MA38 J.Phys.(London) G27, R69 (2001) The Nucleon-Nucleon Interaction
doi: 10.1088/0954-3899/27/5/201
2001MA57 Nucl.Phys. A689, 11c (2001) The Nuclear Force in the Third Millennium
doi: 10.1016/S0375-9474(01)00814-4
2000MA52 Few-Body Systems 28, 139 (2000) Charge Dependence of the πNN Coupling Constant and Charge Dependence of the Nucleon-Nucleon Interaction
2000MA55 Phys.Scr. T87, 47 (2000) How Sensitive are Various NN Observables to Changes in the πNN Coupling Constant ?
doi: 10.1238/Physica.Topical.087a00047
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
1999MI15 Phys.Lett. 455B, 19 (1999) Light Front Theory of Nuclear Matter
doi: 10.1016/S0370-2693(99)90042-4
1999MI25 Phys.Rev. C60, 035202 (1999) Infinite Nuclear Matter on the Light Front: Nucleon-nucleon correlations
doi: 10.1103/PhysRevC.60.035202
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
1999RA06 Phys.Rev.Lett. 82, 1827 (1999) R.Rapp, R.Machleidt, J.W.Durso, G.E.Brown Nuclear Saturation with In-Medium Meson Exchange Interactions
doi: 10.1103/PhysRevLett.82.1827
1998LI34 Phys.Rev. C58, 1393 (1998) Charge Asymmetry of the Nucleon-Nucleon Interaction
doi: 10.1103/PhysRevC.58.1393
1998LI52 Phys.Rev. C58, 3153 (1998) Charge Dependence of the Nucleon-Nucleon Interaction NUCLEAR REACTIONS 1H(n, n), (n, p), (p, p), E < 300 MeV; calculated phase shifts; deduced charge-independence breaking contribution.
doi: 10.1103/PhysRevC.58.3153
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
1998SA37 Few-Body Systems 24, 87 (1998) Triton Binding Energy and Minimal Relativity NUCLEAR STRUCTURE 3H; calculated binding energy correction; deduced invariant two-body amplitude contribution, relativistic effects.
doi: 10.1007/s006010050078
1998SC31 Phys.Rev. C58, 1263 (1998) R.Schiavilla, V.G.J.Stoks, W.Glockle, H.Kamada, A.Nogga, J.Carlson, R.Machleidt, V.R.Pandharipande, R.B.Wiringa, A.Kievsky, S.Rosati, M.Viviani Weak Capture of Protons by Protons NUCLEAR REACTIONS 1H(p, e+ν), E not given; calculated weak capture σ, axial matrix elements.
doi: 10.1103/PhysRevC.58.1263
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
1997HO02 Phys.Rev. C55, 1088 (1997) Skyrme-Model πNN Form Factor and Nucleon-Nucleon Interaction NUCLEAR REACTIONS 1H(n, n), E ≤ 300 MeV; analyzed phase shifts data. Skyrme model πNN form factor, one-boson exchange NN-interaction. NUCLEAR STRUCTURE 2H; calculated binding energy, D-state probability, quadrupole moment, asymptotic D/S state ratio.
doi: 10.1103/PhysRevC.55.1088
1996MA09 Phys.Rev. C53, R1483 (1996) R.Machleidt, F.Sammarruca, Y.Song Nonlocal Nature of the Nuclear Force and Its Impact on Nuclear Structure NUCLEAR STRUCTURE 3H; calculated binding energy; deduced nonlocal potential off-shell behavior role. Relativistic meson field theory based nonlocality.
doi: 10.1103/PhysRevC.53.R1483
1995BU22 Phys.Rev. C52, 1203 (1995) πNN Coupling Constants from NN Elastic Data between 210 and 800 MeV NUCLEAR REACTIONS 1H(p, p), (n, n), E=210-800 MeV; analyzed data; deduced πNN coupling constants.
doi: 10.1103/PhysRevC.52.1203
1994BR23 Phys.Rev. C50, 1731 (1994) Strength of the ρ Meson Coupling to Nucleons NUCLEAR REACTIONS 1H(p, p), E= ≤ 400 MeV; calculated phase shifts vs E; deduced ρNN coupling dependence of NN-interactions.
doi: 10.1103/PhysRevC.50.1731
1994LI01 Phys.Rev. C49, 566 (1994) Microscopic Calculation of In-Medium Proton-Proton Cross Sections NUCLEAR REACTIONS 1H(p, p), E=50-350 MeV; calculated in-medium σ(θ), σ. 1H(n, n), E=50-350 MeV; calculated in-medium σ.
doi: 10.1103/PhysRevC.49.566
1994MA24 Phys.Rev.Lett. 72, 2664 (1994) Comment on ' Neutron-Proton Spin-Correlation Parameter A(zz) at 68 MeV ' NUCLEAR REACTIONS 1H(polarized n, n), E=67.5 MeV; analyzed spin-correlation, phase shifts data; deduced 3S1-3D1 mixing parameter value implications.
doi: 10.1103/PhysRevLett.72.2664
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
1993LI27 Phys.Rev. C48, 1062 (1993); Erratum Phys.Rev. C49, 570 (1994) Self-Consistent Relativistic Calculation of Nucleon Mean Free Path NUCLEAR REACTIONS 40Ca(p, p), E=150-450 MeV; calculated nucleon mean free path vs radial distance. Self-consistent relativistic calculation.
doi: 10.1103/PhysRevC.48.1062
1993LI33 Phys.Rev. C48, 1702 (1993) Microscopic Calculation of In-Medium Nucleon-Nucleon Cross Sections NUCLEAR REACTIONS 1H(n, n), E=50-300 MeV; calculated σ(E), σ(θ). In medium estimates, Dirac-Brueckner approach.
doi: 10.1103/PhysRevC.48.1702
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
1992JI04 Phys.Rev. C46, 910 (1992) M.F.Jiang, R.Machleidt, D.B.Stout, T.T.S.Kuo Bonn Potential and sd-Shell Nuclei NUCLEAR STRUCTURE 18,20,19O, 18,19,21,20F, 20,21Ne; calculated levels. G-matrix folded diagram method, effective interaction from Bonn nucleon-nucleon potential.
doi: 10.1103/PhysRevC.46.910
1992SA17 Phys.Rev. C46, 1636 (1992) F.Sammarruca, D.P.Xu, R.Machleidt Relativistic Corrections to the Triton Binding Energy NUCLEAR STRUCTURE 3H; calculated binding energy. Bethe-Salpeter equation, relativistic three dimensional version, Faddeev calculation.
doi: 10.1103/PhysRevC.46.1636
1991MA12 Phys.Rev.Lett. 66, 564 (1991) Recent Determinations of the πNN Coupling Constants and Deuteron Properties NUCLEAR STRUCTURE 2H; calculated quadrupole moment, D-state probability, asymptotic (D/S)-state ratio. New value of πNN coupling constant.
doi: 10.1103/PhysRevLett.66.564
1991SC26 Nucl.Phys. A530, 14 (1991) K.W.Schmid, H.Muther, R.Machleidt Meson Exchange Potentials and the Problem of Saturation in Finite Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energy per nucleon, charge distribution radius.
doi: 10.1016/0375-9474(91)90753-S
1990JI03 Phys.Rev. C41, 2346 (1990) M.F.Jiang, R.Machleidt, T.T.S.Kuo Uncertainties in the Two-Nucleon Potential and Nuclear Matter Predictions NUCLEAR REACTIONS 1H(n, n), E=50 MeV; calculated phase shifts. Ring diagram method. NUCLEAR STRUCTURE 2H; calculated binding energy, D-state probability, quadrupole moment. Ring diagram method.
doi: 10.1103/PhysRevC.41.2346
1990MU15 Phys.Rev. C42, 1981 (1990) H.Muther, R.Machleidt, R.Brockmann Relativistic Nuclear Structure. II. Finite Nuclei NUCLEAR STRUCTURE 16O; calculated energy per particle, charge radius. Dirac-Brueckner-Hartree-Fock approximation.
doi: 10.1103/PhysRevC.42.1981
1988BR03 Phys.Rev. C37, 781 (1988) R.A.Brandenburg, G.S.Chulick, Y.E.Kim, D.J.Klepacki, R.Machleidt, A.Picklesimer, R.M.Thaler Nuclear Charge Symmetry Breaking and the 3H-3He Binding Energy Difference NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference; deduced charge asymmetric contributions.
doi: 10.1103/PhysRevC.37.781
1988BR05 Phys.Rev. C37, 1245 (1988) R.A.Brandenburg, G.S.Chulick, R.Machleidt, A.Picklesimer, R.M.Thaler Essential Mechanisms in the Triton Binding NUCLEAR STRUCTURE 3H; calculated binding energy. Effective energy dependent central potential.
doi: 10.1103/PhysRevC.37.1245
1988BR22 Phys.Rev. C38, 1397 (1988) R.A.Brandenburg, G.S.Chulick, R.Machleidt, A.Picklesimer, R.M.Thaler Mesic Retardation and the Triton Binding Energy NUCLEAR STRUCTURE 3H; analyzed binding energy estimates; deduced mesic retardation role.
doi: 10.1103/PhysRevC.38.1397
1988CH12 Phys.Rev. C37, 1549 (1988) G.S.Chulick, Ch.Elster, R.Machleidt, A.Picklesimer, R.M.Thaler Neutron-Proton Scattering Observables at 325 MeV, the ϵ1 Parameter, and the Tensor Force NUCLEAR REACTIONS 1H(polarized n, n), E=325 MeV; calculated polarization observables; deduced tensor force role.
doi: 10.1103/PhysRevC.37.1549
1988EL04 Phys.Rev. C38, 1828 (1988) Ch.Elster, K.Holinde, D.Schutte, R.Machleidt Extension of the Bonn Meson Exchange NN Potential above Pion Production Threshold: Role of the delta isobar NUCLEAR REACTIONS 1H(p, p), 1H(n, n), 1H(p, p), E=0.4-1 GeV; calculated phase shifts σ vs E. Bonn meson exchange potential.
doi: 10.1103/PhysRevC.38.1828
1988KI10 Phys.Rev. C38, 2366 (1988) Kr.T.Kim, Y.E.Kim, D.J.Klepacki, R.A.Brandenburg, E.P.Harper, R.Machleidt Charge Form Factors and Root Mean Square Radii of 3He and 3H with the New Bonn Potential NUCLEAR STRUCTURE 3He, 3H; calculated charge form factor, rms radii. New Bonn potential.
doi: 10.1103/PhysRevC.38.2366
1988MU04 Phys.Lett. 202B, 483 (1988) H.Muther, R.Machleidt, R.Brockmann Dirac-Brueckner-Hartree-Fock Approach in Finite Nuclei NUCLEAR STRUCTURE 16O; calculated binding energy per nucleon, charge distribution radius. Dirac-Brueckner-Hartree-Fock approach.
doi: 10.1016/0370-2693(88)91848-5
1987MU16 Phys.Lett. 198B, 45 (1987) H.Muther, R.Machleidt, R.Brockmann On Relativistic Effects in the Low-Energy Spectra of Nuclei NUCLEAR STRUCTURE A=18; calculated T=0, 1 levels. Relativistic meson exchange potential.
doi: 10.1016/0370-2693(87)90155-9
1979AN09 Nucl.Phys. A322, 369 (1979) M.R.Anastasio, A.Faessler, H.Muther, K.Holinde, R.Machleidt The Δ(1236) Probability in the Ground State of the Nuclear Many-Body System NUCLEAR STRUCTURE 2H, 16O; calculated probability of Δ-isobar configuration in ground states.
doi: 10.1016/0375-9474(79)90432-9
1978AN16 Phys.Rev. C18, 2416 (1978) M.R.Anastasio, A.Faessler, H.Muther, K.Holinde, R.Machleidt Mesonic and Isobar Degrees of Freedom in the Ground State of the Nuclear Many-Body System NUCLEAR STRUCTURE 16O; calculated radius; deduced modification of nn interaction due to nuclear medium. Brueckner-Hartree-Fock with mesonic, isobar effects.
doi: 10.1103/PhysRevC.18.2416
1977BR04 Z.Phys. A280, 93 (1977) R.A.Brandenburg, P.U.Sauer, R.Machleidt Trinucleon Properties with One-Boson-Exchange Potentials NUCLEAR STRUCTURE 3He; calculated charge form factors.
doi: 10.1007/BF01438113
1976FA08 Nucl.Phys. A262, 389 (1976) A.Faessler, H.Muther, R.Machleidt, D.Schutte Mesonic Degrees of Freedom and Ground-State Properties of Nuclei NUCLEAR REACTIONS 16O(e, e), E=374.5, 750 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(76)90505-4
1975MA33 Nucl.Phys. A251, 93 (1975) R.Machleidt, K.Holinde, J.Nemeth One-Boson-Exchange Potential and Structure of Finite Nuclei in the Local-Density Approximation NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated levels.
doi: 10.1016/0375-9474(75)90703-4
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