NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = T.A.Rijken Found 60 matches. 2023NA21 Phys.Rev. C 108, 024003 (2023) M.M.Nagels, Th.A.Rijken, Y.Yamamoto Extended-soft-core baryon-baryon model ESC16. IV. S = -3 and S = -4 hyperon-hyperon interactions
doi: 10.1103/PhysRevC.108.024003
2023YA27 Phys.Rev. C 108, 035811 (2023) Y.Yamamoto, N.Yasutake, Th.A.Rijken Quark phases in neutron stars consistent with implications from NICER observations
doi: 10.1103/PhysRevC.108.035811
2022YA06 Phys.Rev. C 105, 015804 (2022) Y.Yamamoto, N.Yasutake, Th.A.Rijken Quark-quark interaction and quark matter in neutron stars
doi: 10.1103/PhysRevC.105.015804
2020HI05 Phys.Rev.Lett. 124, 092501 (2020) E.Hiyama, K.Sasaki, T.Miyamoto, T.Doi, T.Hatsuda, Y.Yamamoto, T.A.Rijken Possible Lightest Ξ Hypernucleus with Modern ΞN Interactions NUCLEAR STRUCTURE 3H, 3He, 4H, 4He, 5H, 5He; calculated binding energies by a high precision variational approach, the Gaussian expansion method.
doi: 10.1103/PhysRevLett.124.092501
2020HI06 Phys.Rev.Lett. 124, 092501 (2020) E.Hiyama, K.Sasaki, T.Miyamoto, T.Doi, T.Hatsuda, Y.Yamamoto, T.A.Rijken Possible Lightest Ξ Hypernucleus with Modern ΞN Interactions NUCLEAR STRUCTURE 3H, 3He; calculated properties of hypernuclei, binding energies of the three-body and four-body systems.
doi: 10.1103/PhysRevLett.124.092501
2020NA37 Phys.Rev. C 102, 054003 (2020) M.M.Nagels, Th.A.Rijken, Y.Yamamoto Extended-soft-core baryon-baryon model ESC16. III. S= -2 hyperon-hyperon/nucleon interactions
doi: 10.1103/PhysRevC.102.054003
2019NA05 Phys.Rev. C 99, 044002 (2019) M.M.Nagels, Th.A.Rijken, Y.Yamamoto Extended-soft-core baryon-baryon model ESC16. I. Nucleon-nucleon scattering
doi: 10.1103/PhysRevC.99.044002
2019NA06 Phys.Rev. C 99, 044003 (2019) M.M.Nagels, Th.A.Rijken, Y.Yamamoto Extended-soft-core baryon-baryon model ESC16. II. Hyperon-nucleon interactions NUCLEAR STRUCTURE 13C, 16O, 28Si, 51V, 89Y, 139La, 208Pb; calculated energy spectra of hypernuclei by the G-matrix folding model derived from ESC16+, and compared with experimental data.
doi: 10.1103/PhysRevC.99.044003
2018IT08 Prog.Theor.Exp.Phys. 2018, 113D01 (2018) K.Itonaga, T.Motoba, T.A.Rijken Hypernuclear non-mesonic weak decays in the extended meson exchange model NUCLEAR STRUCTURE 4H, 4,5He, 7Li, 9Be, 11B, 12,13C, 15N, 16O, 27Al, 28Si, 56Fe, 89Y, 139La, 209Bi; analyzed available data; deduced calculated decay rates, resonance parameter widths, intrinsic asymmetry parameter medium-to-heavy hypernuclei.
doi: 10.1093/ptep/pty110
2017IS05 Phys.Rev. C 95, 044308 (2017) M.Isaka, Y.Yamamoto, Th.A.Rijken Effects of a hyperonic many-body force on BΛ values of hypernuclei NUCLEAR STRUCTURE 9Li, 9,10Be, 9,10,11,12B, 12,13,14C, 15N, 16,19O, 21Ne, 25,27Mg, 28Si, 32S, 40,48K, 40,41Ca, 51V, 59Fe; calculated mass dependence of binding energies of hypernuclei by adding strongly repulsive many-body effects (MBE) to the strongly repulsive multi-Pomeron exchange potential (MPP). Equation of state (EoS) of hyperon-mixed neutron-star matter. Antisymmetrized molecular dynamics for hypernuclei (HyperAMD) framework using ΛN G-matrix interactions from ESC14 and ESC12.
doi: 10.1103/PhysRevC.95.044308
2017YA29 Phys.Rev. C 96, 065804 (2017) Y.Yamamoto, H.Togashi, T.Tamagawa, T.Furumoto, N.Yasutake, Th.A.Rijken Neutron-star radii based on realistic nuclear interactions
doi: 10.1103/PhysRevC.96.065804
2016IS11 Phys.Rev. C 94, 044310 (2016) M.Isaka, Y.Yamamoto, Th.A.Rijken Competing effects of nuclear deformation and density dependence of the ΛN interaction in BΛ values of hypernuclei NUCLEAR STRUCTURE 9Li, 9,10Be, 9,10,11,12B, 12,13,14C, 15N, 16,19O, 21Ne, 25,27Mg, 28Si, 32S, 40,48K, 40,41Ca, 51V, 59Fe; calculated binding energies and quadrupole deformation parameters for hypernuclei, effect of deformation. Microscopic calculations based on baryon-baryon interaction extended soft core (ESC) model including many-body effects, and using G-matrix interaction. Comparison with experimental binding energies for hypernuclei.
doi: 10.1103/PhysRevC.94.044310
2016RI01 Eur.Phys.J. A 52, 21 (2016) Hyperon-hyperon interactions with the Nijmegen ESC08 model
doi: 10.1140/epja/i2016-16021-6
2016YA01 Eur.Phys.J. A 52, 19 (2016) Y.Yamamoto, T.Furumoto, N.Yasutake, Th.A.Rijken Hyperon-mixed neutron star with universal many-body repulsion NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; calculated σ(θ) using G-matrix folding potentials.
doi: 10.1140/epja/i2016-16019-0
2014HI03 Phys.Rev. C 89, 061302 (2014) E.Hiyama, S.Ohnishi, B.F.Gibson, Th.A.Rijken Three-body structure of the nnΛ system with ΛN - ΣN coupling NUCLEAR STRUCTURE 3,4H, 3n, 4He; calculated binding energies, and Λ-separation energies of hypernuclei taking into account ΛN-ΣN coupling explicitly and using simulated NSC97f YN and AV8 NN potentials. No bound state found for 3Ln system contradicting the interpretation of experimental data reported by the HypHI Collaboration.
doi: 10.1103/PhysRevC.89.061302
2014YA26 Phys.Rev. C 90, 045805 (2014) Y.Yamamoto, T.Furumoto, N.Yasutake, Th.A.Rijken Hyperon mixing and universal many-body repulsion in neutron stars NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; analyzed differential elastic σ(θ) data with the G-matrix folding potentials; deduced multi-Pomeron exchange potential (MPPs) and used as input to hyperon mixing in neutron stars. NUCLEAR STRUCTURE 13C, 28Si, 51V, 89Y, 139La, 208Pb; calculated energy spectra of hypernuclei using MPPs deduced from analysis of 16O(16O, 16O) reaction, composition of hyperonic neutron-star matter in the case of extended soft core (ESC) baryon-baryon interaction, equation of state (EoS) in neutron matter with hyperon mixing; derived mass-radius relations of neutron stars. Comparison with experimental data for energy spectra of hypernuclei.
doi: 10.1103/PhysRevC.90.045805
2013SC15 Phys.Rev. C 88, 024322 (2013) Hypernuclear structure with the Nijmegen ESC08 potentials NUCLEAR STRUCTURE 12,13,16C, 28Si, 32S, 40Ca, 51V, 89Y, 139La, 208Pb; calculated single particle energies in single-hypernuclei. 6He, 10Be, 14C, 18O, 30Si, 42Ca, 92Zr, 142Ce, 240Pb; calculated bond energies of double-hypernuclei. Brueckner-Hartree-Fock calculations of hypernuclear matter using several potentials. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.024322
2013YA15 Phys.Rev. C 88, 022801 (2013) Y.Yamamoto, T.Furumoto, N.Yasutake, Th.A.Rijken Multi-Pomeron repulsion and the neutron-star mass NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; analyzed σ(θ) data using G-matrix folding potential derived from extended soft core (ESC) model with three-nucleon interaction (TNA) and multi-Pomeron exchange potential (MPP); deduced fitting parameters for the neutron matter equation of state (EoS); calculated neutron-star mass by solving the Tolmann-Oppenheimer-Volkof equation.
doi: 10.1103/PhysRevC.88.022801
2011SC24 Phys.Rev. C 84, 035801 (2011) Maximum mass of hyperon stars with the Nijmegen ESC08 model
doi: 10.1103/PhysRevC.84.035801
2010HI06 Prog.Theor.Phys.(Kyoto), Suppl. 185, 1 (2010) E.Hiyama, T.Motoba, T.A.Rijken, Y.Yamamoto Baryon-Baryon Interactions and Hypernuclei
doi: 10.1143/PTPS.185.1
2010HI07 Prog.Theor.Phys.(Kyoto), Suppl. 185, 106 (2010) E.Hiyama, M.Kamimura, Y.Yamamoto, T.Motoba, T.A.Rijken S = -1 Hypernuclear Structure NUCLEAR STRUCTURE 4H, 4,6,7He, 7Li, 7,9Be, 12,13C; calculated hypernucleus excitation energies, splittings, n-p relative and probability densities, B(E2). Comparison with experimental data.
doi: 10.1143/PTPS.185.106
2010HI08 Prog.Theor.Phys.(Kyoto), Suppl. 185, 152 (2010) E.Hiyama, M.Kamimura, Y.Yamamoto, T.Motoba, T.A.Rijken S = -2 Hypernuclear Structure NUCLEAR STRUCTURE 5,7H, 7He, 7,8,9,10Li, 9,10,11,12Be; calculated double hypernucleus energy levels and ground state J, π, rms radii, density distribution, binding energies. Cluster model and the Gaussian Expansion Method (GEM).
doi: 10.1143/PTPS.185.152
2010IT04 Int.J.Mod.Phys. E19, 2579 (2010) K.Itonaga, T.Motoba, Th.A.Rijken, T.Ueda Meson exchange model with the axial vector a1-meson exchange and hypernuclear nonmesonic decay asymmetries NUCLEAR STRUCTURE 5He, 7Li, 9Be, 10,11B, 12,13C, 16O; calculated asymmetry parameters for s- and p-shell hypernuclei.
doi: 10.1142/S0218301310017113
2010RI07 Prog.Theor.Phys.(Kyoto), Suppl. 185, 14 (2010) T.A.Rijken, M.M.Nagels, Y.Yamamoto Baryon-Baryon Interactions -Nijmegen Extended-Soft-Core Models-
doi: 10.1143/PTPS.185.14
2010RI09 Nucl.Phys. A835, 160c (2010) Th.A.Rijken, M.M.Nagels, Y.Yamamoto Status of understanding the YN/YY-interactions Meson-exchange viewpoint
doi: 10.1016/j.nuclphysa.2010.01.189
2010YA18 Prog.Theor.Phys.(Kyoto), Suppl. 185, 72 (2010) Y.Yamamoto, T.Motoba, T.A.Rijken G-Matrix Approach to Hyperon-Nucleus Systems NUCLEAR STRUCTURE 11B, 12C, 16O, 28Si, 40Ca, 90Zr; calculated hypernucleus single-particle energies, conversion widths, Coulomb force contribution. ESC08 interaction model, comparison with experimental data.
doi: 10.1143/PTPS.185.72
2010YA25 Nucl.Phys. A835, 350c (2010) Y.Yamamoto, E.Hiyama, Th.A.Rijken Hypernuclear properties derived from the new interaction model ESC08 NUCLEAR STRUCTURE 7H; calculated Ξ- hypernucleus levels, J, π using G-matrix models ESC08 (Extended Soft-Core Model) and ESC04.
doi: 10.1016/j.nuclphysa.2010.01.216
2009MO40 Nucl.Phys. A827, 318c (2009) T.Motoba, S.Sugimoto, E.Hiyama, Y.Yamamoto, Th.A.Rijken, M.Kamimura Structure and production of p-shell Ξ-hypernuclei predicted with realistic interactions
doi: 10.1016/j.nuclphysa.2009.05.065
2009WA20 Phys.Rev. C 80, 055204 (2009) Pion-nucleon scattering in Kadyshevsky formalism. I. Meson exchange sector
doi: 10.1103/PhysRevC.80.055204
2009WA21 Phys.Rev. C 80, 055205 (2009) Pion-nucleon scattering in Kadyshevsky formalism. II. Baryon exchange sector
doi: 10.1103/PhysRevC.80.055205
2008HI16 Phys.Rev. C 78, 054316 (2008) E.Hiyama, Y.Yamamoto, T.Motoba, Th.A.Rijken, M.Kamimura Light Ξ hypernuclei in four-body cluster models NUCLEAR STRUCTURE 5,7H, 9,10Li, 12Be; calculated level energies, density distributions, binding energies, rms radii. Gaussian expansion method. Hypernuclei.
doi: 10.1103/PhysRevC.78.054316
2008IT02 Phys.Rev. C 77, 044605 (2008) K.Itonaga, T.Motoba, T.Ueda, Th.A.Rijken Role of the axial vector a1-meson exchange in hypernuclear nonmesonic weak decays NUCLEAR STRUCTURE 5He, 11B, 12C; calculated decay rates, neutron/proton width ratios, asymmetry parameters of hypernuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.044605
2008RI01 Nucl.Phys. A804, 51 (2008) Recent soft-core baryon-baryon interactions
doi: 10.1016/j.nuclphysa.2007.12.016
2008YA11 Nucl.Phys. A804, 139 (2008) S = -2 hypernuclei based on the ESC04 model
doi: 10.1016/j.nuclphysa.2007.12.005
2007HI09 Nucl.Phys. A790, 646c (2007) E.Hiyama, Y.Yamamoto, Th.A.Rijken, T.Motoba Few-body aspects of hypernuclear physics NUCLEAR STRUCTURE 7Li; calculated hypernucleus level energies, J, π. Spin-dependent ΛN interaction features. Four-body model.
doi: 10.1016/j.nuclphysa.2007.03.110
2006ER02 Phys.Rev. C 73, 044009 (2006) G.Erkol, R.G.E.Timmermans, M.Oka, Th.A.Rijken Scalar-meson-baryon coupling constants in QCD sum rules
doi: 10.1103/PhysRevC.73.044009
2006ER07 Phys.Rev. C 74, 045201 (2006) G.Erkol, R.G.E.Timmermans, Th.A.Rijken Vector-meson-baryon coupling constants in QCD sum rules
doi: 10.1103/PhysRevC.74.045201
2006HI11 Phys.Rev. C 74, 054312 (2006) E.Hiyama, Y.Yamamoto, Th.A.Rijken, T.Motoba Four-body structure of 7ΛLi and Λn spin-dependent interaction NUCLEAR STRUCTURE 7Li; calculated hypernucleus level energies, spin-dependent ΛN interaction features. Four-body model.
doi: 10.1103/PhysRevC.74.054312
2006RI04 Phys.Rev. C 73, 044007 (2006) Extended-soft-core baryon-baryon model. I. Nucleon-nucleon scattering with the ESC04 interaction NUCLEAR REACTIONS 1H(p, p), (n, n), E=0-350 MeV; analyzed phase shifts, related data; deduced parameters. Extended-soft-core baryon-baryon model.
doi: 10.1103/PhysRevC.73.044007
2006RI05 Phys.Rev. C 73, 044008 (2006) Extended-soft-core baryon-baryon model. II. Hyperon-nucleon interaction
doi: 10.1103/PhysRevC.73.044008
2005ER04 Phys.Rev. C 72, 035209 (2005) G.Erkol, R.G.E.Timmermans, Th.A.Rijken Nucleon-sigma coupling constant in QCD sum rules
doi: 10.1103/PhysRevC.72.035209
2005PO25 Phys.Rev. C 72, 065210 (2005) Soft-core meson-baryon interactions. I. One-hadron-exchange potentials
doi: 10.1103/PhysRevC.72.065210
2005PO26 Phys.Rev. C 72, 065211 (2005) Soft-core meson-baryon interactions. II πN and K+N scattering NUCLEAR REACTIONS 1n, 1H(K+, K+), E ≈ 300-600 MeV; calculated σ(θ), polarization observables, resonance features. Soft-core approach.
doi: 10.1103/PhysRevC.72.065211
2005RI08 Nucl.Phys. A754, 27c (2005) Recent soft-core baryon-baryon interactions
doi: 10.1016/j.nuclphysa.2005.01.012
2002RI11 Phys.Rev. C66, 044008 (2002) Th.A.Rijken, H.Polinder, J.Nagata Extended-soft-core NN potentials in momentum space. I. Pseudoscalar-pseudoscalar exchange potentials
doi: 10.1103/PhysRevC.66.044008
2002RI12 Phys.Rev. C66, 044009 (2002) Th.A.Rijken, H.Polinder, J.Nagata Extended-soft-core NN potentials in momentum space. II. Meson-pair exchange potentials NUCLEAR REACTIONS 1H(p, p), (n, n), E=0-350 MeV; calculated phase shifts. Meson-pair exchange potentials, comparison with data.
doi: 10.1103/PhysRevC.66.044009
2001RI21 Nucl.Phys. A691, 322c (2001) Recent Nijmegen Soft-Core Hyperon-Nucleon and Hyperon-Hyperon Interactions
doi: 10.1016/S0375-9474(01)01052-1
1999RI01 Phys.Rev. C59, 21 (1999) Th.A.Rijken, V.G.J.Stoks, Y.Yamamoto Soft-Core Hyperon-Nucleon Potentials
doi: 10.1103/PhysRevC.59.21
1999ST11 Phys.Rev. C59, 3009 (1999) Soft-Core Baryon-Baryon Potentials for the Complete Baryon Octet
doi: 10.1103/PhysRevC.59.3009
1998RI08 Nucl.Phys. A639, 29c (1998) The Nijmegen Hyperon-Nucleon and Hyperon-Hyperon Interactions
doi: 10.1016/S0375-9474(98)00249-8
1998ST09 Nucl.Phys. A631, 452c (1998) NN Potential from Chiral SU(3) Lagrangian
doi: 10.1016/S0375-9474(98)00046-3
1997ST05 Nucl.Phys. A613, 311 (1997) Meson-Baryon Coupling Constants from a Chiral-Invariant SU(3) Lagrangian and Application to NN Scattering
doi: 10.1016/S0375-9474(96)00462-9
1996RI15 Phys.Rev. C54, 2851 (1996) Soft Two-Meson-Exchange Nucleon-Nucleon Potentials. I. Planar and Crossed-Box Diagrams
doi: 10.1103/PhysRevC.54.2851
1996RI16 Phys.Rev. C54, 2869 (1996) Soft Two-Meson-Exchange Nucleon-Nucleon Potentials. II. One-Pair and Two-Pair Diagrams
doi: 10.1103/PhysRevC.54.2869
1995TI03 Nucl.Phys. A585, 143c (1995) R.G.E.Timmermans, Th.A.Rijken, J.J.de Swart (Lambda)NK and ΣNK Couplings from LEAR PS185 Data NUCLEAR REACTIONS 1H(p-bar, X), E at 1435, 1546 MeV/c; compiled, reviewed this, other data analyses; deduced Goldberger-Treiman relations violation features.
doi: 10.1016/0375-9474(94)00557-4
1995TI05 Phys.Rev. C52, 1145 (1995) R.Timmermans, Th.A.Rijken, J.J.de Swart Reply to ' Comment on ' Antiproton-Proton Partial-Wave Analysis Below 925 MeV/c ' ' NUCLEAR REACTIONS 1H(p-bar, p-bar), E at < 925 MeV/c; analyzed partial wave analyses; deduced parameter extraction justifications.
doi: 10.1103/PhysRevC.52.1145
1994DE42 Yad.Fiz. 57, No 9, 1621 (1994); Phys.Atomic Nuclei 57, 1547 (1994) J.J.De Swart, Th.A.Rijken, R.Timmermans (p-bar)p Partial-Wave Analysis and (N-bar)N Potentials NUCLEAR REACTIONS 1H(p-bar, p-bar), E at 790 MeV/c; compiled, reviewed this, other data, analyses; deduced (N-bar)(N)-potential model.
1994TI04 Phys.Rev. C50, 48 (1994) R.Timmermans, Th.A.Rijken, J.J.de Swart Antiproton-Proton Partial-Wave Analysis Below 925 MeV/c NUCLEAR REACTIONS 1H(p-bar, p-bar), E at ≤ 925 MeV/c; analyzed σ(θ), total, annihilation σ vs momentum. 1H(polarized p-bar, p-bar), E at 544-886 MeV/c; 1H(polarized p-bar, n-bar), E at 546-875 MeV/c; analyzed analyzing power data; deduced Nijmegen potential validity.
doi: 10.1103/PhysRevC.50.48
1990BE10 Phys.Rev. C41, 1435 (1990) J.R.Bergervoet, P.C.van Campen, R.A.M.Klomp, J.-L.de Kok, T.A.Rijken, V.G.J.Stoks, J.J.de Swart Phase Shift Analysis of All Proton-Proton Scattering Data Below T(lab) = 350 MeV NUCLEAR REACTIONS 1H(p, p), E=0-350 MeV; analyzed data; deduced phase shifts. P-matrix method.
doi: 10.1103/PhysRevC.41.1435
1988BE28 Phys.Rev. C38, 770 (1988) J.R.Bergervoet, P.C.van Campen, T.A.Rijken, J.J.de Swart Optimal Polynomial Theory Applied to 0-350 MeV pp Scattering NUCLEAR REACTIONS 1H(p, p), E=0-350 MeV; calculated phase parameters. Optimal polynomial theory.
doi: 10.1103/PhysRevC.38.770
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