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NSR database version of April 27, 2024.

Search: Author = S.Tamenaga

Found 12 matches.

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2009NO11      Prog.Theor.Phys.(Kyoto) 122, 1501 (2009)

N.Nose-Togawa, H.Toki, A.Haga, S.Tamenaga

Relativistic Description of Semi-Infinite Nuclear Matter with Vacuum Polarization

doi: 10.1143/PTP.122.1501
Citations: PlumX Metrics

2008TA26      Nucl.Phys. A811, 306 (2008)

S.Tamenaga, H.Toki, A.Haga, Y.Ogawa

Spontaneous chiral symmetry breaking in the massless linear sigma model by fermion and boson loop corrections

NUCLEAR STRUCTURE ¹⁶O; calculated baryon density using the (massless) chiral sigma models.

doi: 10.1016/j.nuclphysa.2008.07.015
Citations: PlumX Metrics

2007OG03      Phys.Rev. C 76, 014305 (2007)

Y.Ogawa, H.Toki, S.Tamenaga

Relativistic chiral mean-field model with parity and charge projection for finite nuclei

NUCLEAR STRUCTURE A=12, 16, 28, 0, 56; calculated ground state properties using the CPPCMF chiral mean field model.

doi: 10.1103/PhysRevC.76.014305
Citations: PlumX Metrics

2007SC23      Phys.Rev. C 75, 055203 (2007)

O.Scholten, S.Tamenaga, H.Toki

Loop corrections and the K-matrix formalism

doi: 10.1103/PhysRevC.75.055203
Citations: PlumX Metrics

2007TO12      Prog.Part.Nucl.Phys. 59, 209 (2007)

H.Toki, Y.Ogawa, S.Tamenaga, A.Haga

Relativistic chiral mean field model for finite nuclei

doi: 10.1016/j.ppnp.2006.12.011
Citations: PlumX Metrics

2006OG02      Phys.Rev. C 73, 034301 (2006)

Y.Ogawa, H.Toki, S.Tamenaga, S.Sugimoto, K.Ikeda

Charge and parity projected relativistic mean field model with pion for finite nuclei

NUCLEAR STRUCTURE ⁴He; calculated ground-state energy, matter density distribution, dependence on meson-nucleon potential. Charge and parity projected relativistic mean field model.

doi: 10.1103/PhysRevC.73.034301
Citations: PlumX Metrics

2005HA53      Phys.Rev. C 72, 034301 (2005)

A.Haga, H.Toki, S.Tamenaga, Y.Horikawa, H.L.Yadav

Self-consistent relativistic random-phase approximation with vacuum polarization

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca; calculated isoscalar-dipole strength distributions. Self-consistent relativistic RPA.

doi: 10.1103/PhysRevC.72.034301
Citations: PlumX Metrics

2005SC03      Phys.Rev. C 71, 034005 (2005)

O.Scholten, J.G.O.Ojwang, S.Tamenaga

Dibaryon resonance and two-photon bremsstrahlung in pp scattering

NUCLEAR REACTIONS ¹H(p, 2γX), E=216 MeV; calculated two-photon bremsstrahlung σ(E, θ), dibaryon state contribution.

doi: 10.1103/PhysRevC.71.034005
Citations: PlumX Metrics

2004HA60      Phys.Rev. C 70, 064322 (2004)

A.Haga, S.Tamenaga, H.Toki, Y.Horikawa

Relativistic Hartree approach with exact treatment of vacuum polarization for finite nuclei

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca; calculated binding energies, charge radii, single-particle energies. Relativistic Hartree approach with exact treatment of vacuum polarization.

doi: 10.1103/PhysRevC.70.064322
Citations: PlumX Metrics

2004OG04      Prog.Theor.Phys.(Kyoto) 111, 75 (2004)

Y.Ogawa, H.Toki, S.Tamenaga, H.Shen, A.Hosaka, S.Sugimoto, K.Ikeda

Chiral Sigma Model with Pion Mean Field in Finite Nuclei

NUCLEAR STRUCTURE ³²S, ³⁶Ar, ⁴⁰Ca, ⁴⁴Ti, ⁴⁸Cr, ⁵²Fe, ⁵⁶Ni, ⁶⁰Zn, ⁶⁴Ge, ⁶⁸Se; calculated single-particle level energies, pion mean-field features.

doi: 10.1143/PTP.111.75
Citations: PlumX Metrics

2004SH44      Nucl.Phys. A745, 121 (2004)

H.Shen, S.Tamenaga, H.Toki

Variation of hadron masses in nuclear matter in the relativistic Hartree approximation

doi: 10.1016/j.nuclphysa.2004.09.006
Citations: PlumX Metrics

2004TO13      Nucl.Phys. A738, 87 (2004)

H.Toki, Y.Ogawa, S.Tamenaga, S.Sugimoto, K.Ikeda

Chiral Symmetry and Finite Pion Mean Field in Nuclei

NUCLEAR STRUCTURE ³²S, ³⁶Ar, ⁴⁰Ca, ⁴⁴Ti, ⁴⁸Cr, ⁵²Fe, ⁵⁶Ni, ⁶⁰Zn, ⁶⁴Ge, ⁶⁸Se; calculated proton single-particle levels, binding energy per nucleon; deduced role of chiral symmetry. Chiral sigma model with finite pion mean field.

doi: 10.1016/j.nuclphysa.2004.04.016
Citations: PlumX Metrics