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NSR database version of April 24, 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


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