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NSR database version of May 24, 2024.

Search: Author = T.A.Rijken

Found 59 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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2016RI01      Eur.Phys.J. A 52, 21 (2016)

Th.A.Rijken, H.-J.Schulze

Hyperon-hyperon interactions with the Nijmegen ESC08 model

doi: 10.1140/epja/i2016-16021-6
Citations: PlumX Metrics


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
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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
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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
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2013SC15      Phys.Rev. C 88, 024322 (2013)

H.-J.Schulze, T.Rijken

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
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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
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2011SC24      Phys.Rev. C 84, 035801 (2011)

H.-J.Schulze, T.Rijken

Maximum mass of hyperon stars with the Nijmegen ESC08 model

doi: 10.1103/PhysRevC.84.035801
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2009WA20      Phys.Rev. C 80, 055204 (2009)

J.W.Wagenaar, T.A.Rijken

Pion-nucleon scattering in Kadyshevsky formalism. I. Meson exchange sector

doi: 10.1103/PhysRevC.80.055204
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2009WA21      Phys.Rev. C 80, 055205 (2009)

J.W.Wagenaar, T.A.Rijken

Pion-nucleon scattering in Kadyshevsky formalism. II. Baryon exchange sector

doi: 10.1103/PhysRevC.80.055205
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2008RI01      Nucl.Phys. A804, 51 (2008)

Th.A.Rijken, Y.Yamamoto

Recent soft-core baryon-baryon interactions

doi: 10.1016/j.nuclphysa.2007.12.016
Citations: PlumX Metrics


2008YA11      Nucl.Phys. A804, 139 (2008)

Y.Yamamoto, Th.A.Rijken

S = -2 hypernuclei based on the ESC04 model

doi: 10.1016/j.nuclphysa.2007.12.005
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2006RI04      Phys.Rev. C 73, 044007 (2006)

Th.A.Rijken

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
Citations: PlumX Metrics


2006RI05      Phys.Rev. C 73, 044008 (2006)

Th.A.Rijken, Y.Yamamoto

Extended-soft-core baryon-baryon model. II. Hyperon-nucleon interaction

doi: 10.1103/PhysRevC.73.044008
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2005PO25      Phys.Rev. C 72, 065210 (2005)

H.Polinder, Th.A.Rijken

Soft-core meson-baryon interactions. I. One-hadron-exchange potentials

doi: 10.1103/PhysRevC.72.065210
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2005PO26      Phys.Rev. C 72, 065211 (2005)

H.Polinder, Th.A.Rijken

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
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2005RI08      Nucl.Phys. A754, 27c (2005)

Th.A.Rijken, Y.Yamamoto

Recent soft-core baryon-baryon interactions

doi: 10.1016/j.nuclphysa.2005.01.012
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


2001RI21      Nucl.Phys. A691, 322c (2001)

Th.A.Rijken

Recent Nijmegen Soft-Core Hyperon-Nucleon and Hyperon-Hyperon Interactions

doi: 10.1016/S0375-9474(01)01052-1
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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
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1999ST11      Phys.Rev. C59, 3009 (1999)

V.G.J.Stoks, Th.A.Rijken

Soft-Core Baryon-Baryon Potentials for the Complete Baryon Octet

doi: 10.1103/PhysRevC.59.3009
Citations: PlumX Metrics


1998RI08      Nucl.Phys. A639, 29c (1998)

Th.A.Rijken

The Nijmegen Hyperon-Nucleon and Hyperon-Hyperon Interactions

doi: 10.1016/S0375-9474(98)00249-8
Citations: PlumX Metrics


1998ST09      Nucl.Phys. A631, 452c (1998)

V.G.J.Stoks, Th.A.Rijken

NN Potential from Chiral SU(3) Lagrangian

doi: 10.1016/S0375-9474(98)00046-3
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1997ST05      Nucl.Phys. A613, 311 (1997)

V.G.J.Stoks, Th.A.Rijken

Meson-Baryon Coupling Constants from a Chiral-Invariant SU(3) Lagrangian and Application to NN Scattering

doi: 10.1016/S0375-9474(96)00462-9
Citations: PlumX Metrics


1996RI15      Phys.Rev. C54, 2851 (1996)

Th.A.Rijken, V.G.J.Stoks

Soft Two-Meson-Exchange Nucleon-Nucleon Potentials. I. Planar and Crossed-Box Diagrams

doi: 10.1103/PhysRevC.54.2851
Citations: PlumX Metrics


1996RI16      Phys.Rev. C54, 2869 (1996)

Th.A.Rijken, V.G.J.Stoks

Soft Two-Meson-Exchange Nucleon-Nucleon Potentials. II. One-Pair and Two-Pair Diagrams

doi: 10.1103/PhysRevC.54.2869
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter T.A.Rijken: , T.A.RIJKEN