NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = K.Iida Found 34 matches. 2022TA18 Phys.Rev. C 106, 045807 (2022) H.Tajima, H.Moriya, W.Horiuchi, K.Iida, E.Nakano Resonance-to-bound transition of 5He in neutron matter and its analogy with heteronuclear Feshbach molecules NUCLEAR STRUCTURE 5He; calculated ground-state energy using p-wave neutron-alpha scattering amplitude, 5He spectral function in dilute neutron matter at T=0. Described resonance-to-bound transition using two-channel model developed for the description of a cold atomic gas near the narrow Feshbach resonance.
doi: 10.1103/PhysRevC.106.045807
2021MO30 Phys.Rev. C 104, 065801 (2021) H.Moriya, H.Tajima, W.Horiuchi, K.Iida, E.Nakano Binding two and three α particles in cold neutron matter NUCLEAR STRUCTURE 8Be, 12C; calculated two-α ground state (8Be) and three-α first excited state (Hoyle state in 12C), energies and pair density distributions of the three-α system in neutron matter as a function of the neutron Fermi momentum with Ali-Bodmer (AB) and orthogonality condition model (OCM) potentials. Numerical solution of the few-body Schrodinger equation of α particles within standard α-cluster models, combined with in-medium properties of α particles.
doi: 10.1103/PhysRevC.104.065801
2020NA38 Phys.Rev. C 102, 055802 (2020) Quasiparticle properties of a single α particle in cold neutron matter
doi: 10.1103/PhysRevC.102.055802
2017HO20 Phys.Rev. C 96, 035804 (2017) Neutron-skin thickness determines the surface tension of a compressible nuclear droplet NUCLEAR STRUCTURE Z=50, N=50-90; Z=82, N=100-164; calculated charge radii, and compared with experimental data. Z=50, N=50-90; Z=82, N=100-164; Z=20, N=20-40; Z=28, N=28-58; Z=40, N=38-80; Z=50, N=50-90; Z=70, N=80-120; Z=82, N=100-164; calculated surface widths from the neutron and proton density distributions using SkM*, SLy4, and SkI3 interactions, neutron-skin thicknesses as a function of the asymmetry parameter using SkM*, SLy4, and SkI3 interactions for HF+BCS theory. 116,118,120,122,124Sn, 204,206,208Pb; calculated neutron-skin thicknesses within the compressible droplet model using empirical density distributions. Equation of state (EOS) parameters deduced from nine Skyrme-EDF models.
doi: 10.1103/PhysRevC.96.035804
2015SC04 Phys.Rev. C 91, 025801 (2015) B.Schuetrumpf, M.A.Klatt, K.Iida, G.E.Schroder-Turk, J.A.Maruhn, K.Mecke, P.-G.Reinhard Appearance of the single gyroid network phase in "nuclear pasta" matter
doi: 10.1103/PhysRevC.91.025801
2015SO03 Phys.Rev. C 91, 015805 (2015) Constraining the density dependence of the nuclear symmetry energy from an x-ray bursting neutron star
doi: 10.1103/PhysRevC.91.015805
2014II01 Eur.Phys.J. A 50, 42 (2014) Symmetry energy, unstable nuclei and neutron star crusts
doi: 10.1140/epja/i2014-14042-9
2014SC25 Phys.Rev. C 90, 055802 (2014) B.Schuetrumpf, K.Iida, J.A.Maruhn, P.-G.Reinhard Nuclear ``pasta matter" for different proton fractions
doi: 10.1103/PhysRevC.90.055802
2013IW01 Phys.Rev. C 87, 014609 (2013) Synthesis of thin, long heavy nuclei in ternary collisions
doi: 10.1103/PhysRevC.87.014609
2013KL03 J.Phys.:Conf.Ser. 445, 012036 (2013) M.A.Klatt, T.Ichikawa, K.Iida, N.Itagaki, J.A.Maruhn, K.Matsuyanagi, K.Mecke, S.Ohkubo, P.-G.Reinhard, B.Schuetrumpf Exotic cluster structures in the mean-field theory NUCLEAR STRUCTURE 16O, 40Ca; calculated deformation, exotic shapes using Skyrme Hartree-Fock, TDHF.
doi: 10.1088/1742-6596/445/1/012036
2013SC09 Phys.Rev. C 87, 055805 (2013) B.Schuetrumpf, M.A.Klatt, K.Iida, J.A.Maruhn, K.Mecke, P.-G.Reinhard Time-dependent Hartree-Fock approach to nuclear "pasta" at finite temperature
doi: 10.1103/PhysRevC.87.055805
2011II01 Prog.Theor.Phys.(Kyoto) 126, 1091 (2011) K.Iida, K.Oyamatsu, B.Abu-Ibrahim, A.Kohama Proton-Nucleus Total Reaction Cross Sections in the Optical Limit Glauber Theory -Subtle Dependence on the Equation of State of Nuclear Matter - NUCLEAR REACTIONS 112,124Sn, 80Ni(p, X), E=40, 300, 800 MeV; calculated total σ. Glauber theory.
doi: 10.1143/PTP.126.1091
2011NA22 Phys.Rev. C 83, 065811 (2011) K.Nakazato, K.Iida, K.Oyamatsu Curvature effect on nuclear "pasta": Is it helpful for gyroid appearance?
doi: 10.1103/PhysRevC.83.065811
2010OY01 Phys.Rev. C 81, 054302 (2010) Symmetry energy at subnuclear densities deduced from nuclear masses NUCLEAR STRUCTURE Z=8, A=11-28; Z=12, A=17-43; Z=20, A=30-72; Z=28, A=45-100; Z=50, A=90-180; Z=82, A=175-285; calculated two proton separation energies, δVnp, influence of the density dependence of the symmetry energy on nuclear masses using a macroscopic nuclear model. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.054302
2010OY02 Phys.Rev. C 82, 027301 (2010) Neutron drip line and the equation of state of nuclear matter
doi: 10.1103/PhysRevC.82.027301
2008KO29 Phys.Rev. C 78, 061601 (2008) Difference between interaction cross sections and reaction cross sections NUCLEAR REACTIONS 12C(3He, X), (α, X), (6Li, X), (7Li, X), (9Be, X), (10B, X), (11B, X), (12C, X), (13C, X), (14N, X), (15N, X), (16O, X), (17O, X), (18O, X), (19F, X), (20Ne, X), (21Ne, X), (23Na, X), (24Mg, X), (25Mg, X), (27Al, X), (35Cl, X), (37Cl, X), (36Ar, X), (38Ar, X), (40Ar, X), (80Kr, X), E>800 MeV; calculated reaction σ. Comparisons with data.
doi: 10.1103/PhysRevC.78.061601
2007II01 Nucl.Phys. A785, 118c (2007) Instability of a gapless color superconductor with respect to inhomogeneous fluctuations
doi: 10.1016/j.nuclphysa.2006.11.055
2007OY01 Phys.Rev. C 75, 015801 (2007) Symmetry energy at subnuclear densities and nuclei in neutron star crusts
doi: 10.1103/PhysRevC.75.015801
2005KO28 Phys.Rev. C 72, 024602 (2005) Reaction cross section described by a black sphere approximation of nuclei NUCLEAR REACTIONS 4He, 12,13C, 14N, 16O, 20,22Ne, 24,26Mg, 28Si, 32,34S, 39K, 40,42,44,48Ca, 46,48Ti, 120Sn, 208Pb(p, p), E ≈ 800-1100 MeV; analyzed σ(θ); deduced black-sphere radius parameters. 12C, 120Sn, 208Pb(p, X), E ≈ 800 MeV; analyzed reaction, interaction σ.
doi: 10.1103/PhysRevC.72.024602
2004II01 Phys.Rev. C 69, 037301 (2004) Surface tension in a compressible liquid-drop model: Effects on nuclear density and neutron skin thickness NUCLEAR STRUCTURE 56,64Ni, 90Zr, 116,124Sn, 208Pb; calculated neutron and proton radii, role of surface tension. Compressible liquid-drop model.
doi: 10.1103/PhysRevC.69.037301
2004II02 Prog.Theor.Phys.(Kyoto), Suppl. 156, 139 (2004) K.Iida, K.Oyamatsu, B.Abu-Ibrahim Deducing the Density Dependence of the Symmetry Energy from Unstable Nuclei NUCLEAR REACTIONS 58Ni(p, p), E=400, 1047 MeV; 58,80Ni, 124Sn, 208Pb(p, p), E=800 MeV; calculated σ(θ), density dependence features. Glauber model.
doi: 10.1143/PTPS.156.139
2004KO34 Phys.Rev. C 69, 064316 (2004) Nuclear radius deduced from proton diffraction by a black nucleus NUCLEAR REACTIONS 58,60,62,64Ni(p, p), E ≈ 800-1050 MeV; 90,92Zr, 120Sn, 144,154Sm, 176Yb, 208Pb(p, p), E=800 MeV; analyzed σ(θ); deduced radii. Black-sphere approach.
doi: 10.1103/PhysRevC.69.064316
2004OY01 Prog.Theor.Phys.(Kyoto), Suppl. 156, 137 (2004) Equation of State of Nuclear Matter, Neutron Rich Nuclei in Laboratories and Pasta Nuclei in Neutron Star Crusts NUCLEAR STRUCTURE 80Ni; calculated matter radius.
doi: 10.1143/PTPS.156.137
2003II01 Nucl.Phys. A718, 697c (2003) Magnetic and rotational vortices in superfluid quark matter
doi: 10.1016/S0375-9474(03)00892-3
2003II02 Phys.Lett. B 576, 273 (2003) K.Iida, K.Oyamatsu, B.Abu-Ibrahim Proton-nucleus elastic scattering and the equation of state of nuclear matter NUCLEAR REACTIONS 58Ni(p, p), E=400, 1047 MeV; 58,80Ni, 116,124Sn, 208Pb(p, p), E=800 MeV; calculated σ(θ); deduced dependence on nuclear matter density parameter. Glauber model.
doi: 10.1016/j.physletb.2003.10.019
2003OY01 Nucl.Phys. A718, 363c (2003) Empirical properties of asymmetric nuclear matter to be obtained from unstable nuclei NUCLEAR STRUCTURE 80Ni; calculated matter radius vs density symmetry coefficient. Ni; calculated matter radii for N=18-64.
doi: 10.1016/S0375-9474(03)00740-1
2003OY02 Prog.Theor.Phys.(Kyoto) 109, 631 (2003) Saturation of Nuclear Matter and Radii of Unstable Nuclei NUCLEAR STRUCTURE 90Zr, 208Pb; calculated matter density distributions. 58,80Ni, 116,142Sn; calculated radii, parameter dependences, saturation properties.
doi: 10.1143/PTP.109.631
2003WA25 Phys.Rev. C 68, 045801 (2003) Electron screening in the liquid-gas mixed phases of nuclear matter
doi: 10.1103/PhysRevC.68.045801
2002II01 Prog.Theor.Phys.(Kyoto), Suppl. 146, 514 (2002) Formation of Nuclear "Pasta" in Cold Neutron Star Matter
doi: 10.1143/PTPS.146.514
2001II01 Prog.Theor.Phys.(Kyoto) 106, 551 (2001); Erratum Prog.Theor.Phys.(Kyoto) 110, 847 (2003) Formation of Nuclear ' Pasta ' in Cold Neutron Star Matter
doi: 10.1143/PTP.106.551
2001WA15 Nucl.Phys. A687, 512 (2001); Erratum Nucl.Phys. A726, 357 (2003) Effects of Neutrino Trapping on Thermodynamic Properties of Nuclear ' Pasta '
doi: 10.1016/S0375-9474(00)00585-6
2000WA27 Nucl.Phys. A676, 455 (2000); Erratum Nucl.Phys. A726, 357 (2003) Thermodynamic Properties of Nuclear ' Pasta ' in Neutron Star Crusts
doi: 10.1016/S0375-9474(00)00197-4
1999II01 Phys.Rev. C60, 024905 (1999) Color Plasma Oscillation in Strangelets
doi: 10.1103/PhysRevC.60.024905
1998II01 Phys.Rev. C58, 2538 (1998) Effects of Hyperons on the Dynamical Deconfinement Transition in Cold Neutron Star Matter
doi: 10.1103/PhysRevC.58.2538
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