NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = K.Tanabe Found 56 matches. 2018TA15 Phys.Rev. C 97, 069802 (2018) Reply to "Comment on 'Stability of the wobbling motion in an odd-mass nucleus and the analysis of 135Pr'" NUCLEAR STRUCTURE 163Lu; calculated root-mean-square values of the alignments for triaxial, strongly deformed (TSD) bands using HFB formalism; deduced absence of stable transverse wobbling mode, refuting the comment on their 2017Ta14 paper by 2018Fr02.
doi: 10.1103/PhysRevC.97.069802
2017SU20 Phys.Scr. 92, 094005 (2017) Application of the top-on-top model to 135Pr
doi: 10.1088/1402-4896/aa81eb
2017TA14 Phys.Rev. C 95, 064315 (2017) Stability of the wobbling motion in an odd-mass nucleus and the analysis of 135Pr NUCLEAR STRUCTURE 135Pr; calculated levels, J, π, B(E2) ratios, B(M1)/B(E2) ratios, mixing ratios, moment of inertia and backbending plots, stability of the wobbling motion. Particle-rotor model with Holstein-Primakoff boson expansion. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.064315
2017TA32 Phys.Scr. 92, 124003 (2017) Stability of the wobbling motion in the triaxially deformed odd-A nucleus
doi: 10.1088/1402-4896/aa923f
2015TA09 Phys.Rev. C 91, 034328 (2015) Nuclear moment of inertia as an indicator of the phase transition in a finite system
doi: 10.1103/PhysRevC.91.034328
2014SU14 Prog.Theor.Exp.Phys. 2014, 063D01 (2014) K.Sugawara-Tanabe, K.Tanabe, N.Yoshinaga Analysis of the triaxial, strongly deformed bands in odd-odd nucleus 164Lu with the tops-on-top model NUCLEAR STRUCTURE 164Lu; calculated energy levels, J, π, B(E2), B(M1), moment of inertia; deduced triaxial strongly-deformed bands. Comparison with available data.
doi: 10.1093/ptep/ptu088
2012SU27 J.Phys.:Conf.Ser. 381, 012069 (2012) Tops-on-top model for triaxial, strongly deformed bands in 164Lu NUCLEAR STRUCTURE 164Lu; calculated triaxial strongly deformed rotational bands, energy, alignments, B(E2), B(M1) using tops-on-top model. 163Lu; calculated B(E2), B(M1); compared with data.
doi: 10.1088/1742-6596/381/1/012069
2010SU27 Phys.Rev. C 82, 051303 (2010) Properties of triaxial, strongly deformed bands in 167Ta and 167Lu and the top-on-top model NUCLEAR STRUCTURE 167Ta, 167Lu; calculated levels, J, triaxial strongly deformed (TSD) bands, B(M1)/B(E2) and in-band, out-of-band B(E2) ratios based on particle-rotor model with one particle coupled to a triaxially deformed rotor, . Comparison with experimental data.
doi: 10.1103/PhysRevC.82.051303
2009SU16 Phys.Rev. C 80, 044307 (2009) K.Sugawara-Tanabe, K.Tanabe, A.Arima, B.Gruber SU(3) symmetry in the triaxially deformed harmonic oscillator
doi: 10.1103/PhysRevC.80.044307
2008TA14 Phys.Rev. C 77, 064318 (2008) Selection rules for electromagnetic transitions in triaxially deformed odd-A nuclei NUCLEAR STRUCTURE 161,163,165,167Lu; calculated level energies of triaxial strongly-deformed bands, B(M1), B(E2) values, transition schemes. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.064318
2006DA23 Phys.Rev. C 74, 034326 (2006) Self-consistent random-phase approximation at finite temperature within the Richardson model
doi: 10.1103/PhysRevC.74.034326
2006NA40 Phys.Rev.C 74, 061301 (2006) New Bardeen-Cooper-Schrieffer-type theory at finite temperature with particle-number conservation
doi: 10.1103/PhysRevC.74.061301
2006NA41 Int.J.Mod.Phys. E15, 1761 (2006) BCS-type theory in canonical ensembles
doi: 10.1142/S0218301306005290
2006TA11 Phys.Rev. C 73, 034305 (2006); Erratum Phys.Rev. C 75, 059903 (2007) Algebraic description of triaxially deformed rotational bands in odd mass nuclei NUCLEAR STRUCTURE 163,165,167Lu; calculated triaxial deformed rotational bands energies, B(M1), B(E2), selection rules. Algebraic approach.
doi: 10.1103/PhysRevC.73.034305
2005ES09 Phys.Rev. C 72, 044303 (2005) K.Esashika, H.Nakada, K.Tanabe Effects of particle-number conservation on heat capacity of nuclei NUCLEAR STRUCTURE 161,162Dy; calculated heat capacities, other thermal properties. Finite-temperature BCS theory with particle number projection.
doi: 10.1103/PhysRevC.72.044303
2005HI17 Phys.Rev. C 72, 024315 (2005) K.Higashiyama, N.Yoshinaga, K.Tanabe New band mechanism of doubly-odd nuclei around mass 130 NUCLEAR STRUCTURE 130,132Xe, 132,134Ba, 130,132Cs, 132,134La; calculated levels, J, π, B(M1), B(E2), g factors, rotational bands. Pair-truncated shell model, comparison with data.
doi: 10.1103/PhysRevC.72.024315
2005TA05 Phys.Rev. C 71, 024314 (2005) Quantum number projection at finite temperature via thermofield dynamics
doi: 10.1103/PhysRevC.71.024314
2003HI04 Phys.Rev. C 67, 044305 (2003) K.Higashiyama, N.Yoshinaga, K.Tanabe Pair-truncated shell-model approach to backbending and low-lying states in 132Ba NUCLEAR STRUCTURE 132Ba; calculated rotational bands structure, J, π, transitions B(E2), backbending features. Pair-truncated shell model, comparison with data.
doi: 10.1103/PhysRevC.67.044305
2002EN05 Phys.Rev. C65, 064308 (2002) K.Enami, K.Tanabe, N.Yoshinaga Quantum-Number-Projected Generator Coordinate Method and the Shell Model NUCLEAR STRUCTURE 12C, 14,20Ne; calculated levels, J, π, deformation effects, B(E2), B(M1). Quantum-number-projected generator coordinate method, comparison with exact shell model results.
doi: 10.1103/PhysRevC.65.064308
2002EN09 Phys.Rev. C66, 047301 (2002) K.Enami, K.Higashiyama, K.Tanabe, N.Yoshinaga Quantum-number-projected generator coordinate method analysis of low-lying states in 130, 132Xe NUCLEAR STRUCTURE 130,132Xe; calculated low- and high-spin states energies, J, π, rotational bands; deduced role of triaxial deformation. Quantum-number-projected generator coordinate method, comparison with data and shell-model results.
doi: 10.1103/PhysRevC.66.047301
2002HI08 Phys.Rev. C65, 054317 (2002) K.Higashiyama, N.Yoshinaga, K.Tanabe Shell Model Study of Backbending Phenomena in Xe Isotopes NUCLEAR STRUCTURE 130,131,132,133,134,135,136Xe; calculated levels, J, π, rotational bands features. Shell model, comparison with data.
doi: 10.1103/PhysRevC.65.054317
2002HI22 Prog.Theor.Phys.(Kyoto), Suppl. 146, 563 (2002) K.Higashiyama, N.Yoshinaga, K.Tanabe Shell Model Study of Even-Even Xe Isotopes NUCLEAR STRUCTURE 132Xe; calculated levels, J, π, B(E2). Shell model, comparison with data.
doi: 10.1143/PTPS.146.563
2002SU32 Prog.Theor.Phys.(Kyoto), Suppl. 146, 621 (2002) The Triaxial Superdeformed Bands in 163Lu NUCLEAR STRUCTURE 163Lu; analyzed triaxial superdeformed bands energies, B(M1), B(E2), configurations.
doi: 10.1143/PTPS.146.621
2001EN01 Phys.Rev. C63, 044322 (2001) K.Enami, K.Tanabe, N.Yoshinaga Generator Coordinate Method Combined with Exact Triaxial Spin Projection: Application to the single-j shell model
doi: 10.1103/PhysRevC.63.044322
2001EN03 Prog.Part.Nucl.Phys. 46, 177 (2001) K.Enami, K.Tanabe, N.Yoshinaga Capability of the GCM Calculation with Spin and Particle Number Projections for Single j-Shell Model
doi: 10.1016/S0146-6410(01)00122-3
2001EN06 Phys.Rev. C64, 044305 (2001) K.Enami, K.Tanabe, N.Yoshinaga Quantum-Number-Projected Generator Coordinate Method: Pairing plus quadrupole model within a single-j shell
doi: 10.1103/PhysRevC.64.044305
2000EN03 Phys.Rev. C61, 027301 (2000) K.Enami, K.Tanabe, N.Yoshinaga Calculation of E2-Transition Probabilities Based on Angular Momentum-Projected Cranked Hartree-Fock-Bogoliubov Theory NUCLEAR STRUCTURE 160,164,168Yb; calculated high-spin states B(E2). Cranked HFB approach with angular momentum projection.
doi: 10.1103/PhysRevC.61.027301
2000EN13 Prog.Theor.Phys.(Kyoto) 104, 757 (2000) K.-I.Enami, K.Tanabe, N.Yoshinaga, K.Higashiyama Triaxiality-Driving Effect Extracted by Spin Projection NUCLEAR STRUCTURE 142Nd, 168Er, 188Os; calculated potential energy surfaces, effect of triaxial spin projection as a function of deformation. Deformed mean-field approach.
doi: 10.1143/PTP.104.757
2000NG02 Nucl.Phys. A675, 531 (2000) Damping of Multiphonon Giant Resonances NUCLEAR STRUCTURE 90Zr, 120Sn, 208Pb; calculated GDR, double GDR, triple GDR strength functions and energy weighted strength functions, GDR parameters.
doi: 10.1016/S0375-9474(00)00186-X
2000NG04 Phys.Scr. T88, 189 (2000) Microscopic Description of the Hot Giant Dipole Resonances's Shape Evolution NUCLEAR STRUCTURE 120Sn, 208Pb; calculated GDR strength functions, width vs excitation energy. Phonon damping model.
2000TA25 Phys.Rev. C62, 024310 (2000) Exact Form of the Random Phase Approximation Equation at Finite Temperature Including the Entropy Effect
doi: 10.1103/PhysRevC.62.024310
1999EN01 Phys.Rev. C59, 135 (1999) K.Enami, K.Tanabe, N.Yoshinaga Microscopic Description of High-Spin States: Quantum-number projections of the cranked Hartree-Fock-Bogoliubov Self-Consistent Solution NUCLEAR STRUCTURE 132Ce, 158,164,168Er; calculated high-spin levels configurations, deformations. Self-consistent cranked HFB, angular momentum and particle number projection.
doi: 10.1103/PhysRevC.59.135
1999NG01 Nucl.Phys. A645, 536 (1999) Shape Evolution of the Hot Giant Dipole Resonance NUCLEAR STRUCTURE 120Sn, 208Pb; calculated GDR widths, strength functions vs temperature, integrated γ yields vs excitation energy. Phonon damping model.
doi: 10.1016/S0375-9474(98)00621-6
1999NG02 Phys.Rev. C59, 3128 (1999) Damping of the Double Giant Dipole Resonance NUCLEAR STRUCTURE 90Zr, 120Sn, 208Pb; calculated double GDR energy, Γ, strength distributions vs temperature. Phonon damping model.
doi: 10.1103/PhysRevC.59.3128
1999NG04 Nucl.Phys. A649, 201c (1999) Quantal and Thermal Dampings of the Hot Giant Dipole Resonance Due to Complex Configuration Mixing NUCLEAR STRUCTURE 120Sn, 208Pb; calculated GDR width vs temperature; deduced pp, ph, hh coupling effects.
doi: 10.1016/S0375-9474(99)00061-5
1999NG05 Phys.Rev. C60, 034306 (1999) Evolution of the Hot Giant Dipole Resonance as a Manifestation of the Order-and-Chaos Coexistence NUCLEAR STRUCTURE 120Sn; calculated GDR strength functions, correlation functions vs temperature, time; deduced order-to-chaos transition features. Phonon-damping model.
doi: 10.1103/PhysRevC.60.034306
1999TA12 Phys.Rev. C59, 2494 (1999) K.Tanabe, K.Enami, N.Yoshinaga Extension of Wick's Theorem for Many-Particle Matrix Elements
doi: 10.1103/PhysRevC.59.2494
1999TA19 Nucl.Phys. A649, 205c (1999) Stability of Thermal HFB and Dissipative Thermal RPA
doi: 10.1016/S0375-9474(99)00062-7
1998NG06 Phys.Rev. C58, 3374 (1998) Contribution of Higher-Order Processes to the Damping of Hot Giant Dipole Resonance NUCLEAR STRUCTURE 120Sn, 208Pb; calculated GDR width, strength functions, γ-ray yields vs temperature. Double-time Green's function method.
doi: 10.1103/PhysRevC.58.3374
1998NG07 Phys.Lett. 445B, 1 (1998) Damping of Hot Giant Dipole Resonance Due to Complex Configuration Mixing NUCLEAR STRUCTURE 120Sn, 208Pb; calculated GDR width vs temperature; deduced contributions. Comparison with experiment.
doi: 10.1016/S0370-2693(98)01454-3
1994TA03 Nucl.Phys. A569, 27c (1994) Temperature-Dependence of the GDR Width in the Second Thermal RPA
doi: 10.1016/0375-9474(94)90093-0
1993SU10 Nucl.Phys. A559, 42 (1993) The Angular Distribution of Gamma-Rays from Thermal High-Spin Giant-Dipole-Resonances on Superdeformed States NUCLEAR STRUCTURE 132Ce; calculated levels, transition γ(θ), absorption σ(Eγ), thermal high spin GDR, superdeformed states. Microscopic approach, thermal RPA, thermal cranked HFB ensemble.
doi: 10.1016/0375-9474(93)90179-2
1991TA14 Phys.Lett. 259B, 12 (1991) Microscopic Properties of the Superdeformed Rotational States in Light Rare-Earth Nuclei 132Ce and 134,136Nd NUCLEAR STRUCTURE 132Ce, 134,136Nd; calculated levels, g-factors, yrast sequence electric quadrupole moment, dynamical moments of inertia; deduced superdeformed to yrast transition. Particle number, angular momentum constrained HFB.
doi: 10.1016/0370-2693(91)90125-A
1990SU05 Phys.Lett. 238B, 15 (1990) The Nuclear Meissner Effect and Superdeformation in the Number-Projected Constrained-Cranked HFB Approach NUCLEAR STRUCTURE 132Ce; calculated levels, superdeformed band structure. Self-consistent constrained-cranked HFB approach.
doi: 10.1016/0370-2693(90)92092-W
1990TA29 Prog.Theor.Phys.(Kyoto) 83, 1148 (1990) Microscopic Structure of the Superdeformed Rotational Band in 132Ce NUCLEAR STRUCTURE 132Ce; calculated levels, average pairing gaps, g, intrinsic quadrupole moments; deduced superdeformed band structure. Self-consistent cranked HFB.
doi: 10.1143/PTP.83.1148
1988SU07 Phys.Lett. 207B, 243 (1988) g-Factors and Backbending Along the Yrast in Er Isotopes from A = 158 to 170 NUCLEAR STRUCTURE 158,160,162,164,166,168,170Er; calculated levels, g. Self-consistent cranked HFB.
doi: 10.1016/0370-2693(88)90568-0
1987SU10 Phys.Lett. 192B, 268 (1987) Thermal High Spin Giant Dipole Resonance in Er Isotopes NUCLEAR REACTIONS 162,166Er(γ, n), E=5-20 MeV; calculated dipole absorption σ, strength function. RPA. NUCLEAR STRUCTURE 162,166Er; calculated angular momentum vs rotational frequency, quasiparticle pair number. RPA.
doi: 10.1016/0370-2693(87)90103-1
1986SU19 Prog.Theor.Phys.(Kyoto) 76, 1272 (1986) Thermal and Rotational Effect on Giant Dipole Resonances in Rotating Nuclei at High Temperature NUCLEAR REACTIONS 162,166Er(γ, X), E ≤ 20 MeV; calculated absorption σ(E) vs temperature, angular momentum. 162,166Er deduced GDR characteristics. Thermal linear response theory.
doi: 10.1143/PTP.76.1272
1984TA01 Phys.Lett. 135B, 353 (1984) Shape Coexistence at High Spins in 158Er and 160Yb Predicted by the Self-Consistent Calculation NUCLEAR STRUCTURE 158Er, 160Yb; calculated high-spin state moment of inertia vs angular frequency, yrast state behavior in (β-γ) plane. 160Yb; calculated proton, neutron gap energies; deduced prolate, oblate deformation coexistence.
doi: 10.1016/0370-2693(84)90292-2
1982TA22 Nucl.Phys. A390, 385 (1982) Phase Transitions Along and Off the Yrast Line NUCLEAR STRUCTURE 164Er; analyzed level scheme; deduced phase transition along, off yrast line.
doi: 10.1016/0375-9474(82)90276-7
1981SU02 Nucl.Phys. A357, 45 (1981) K.Sugawara-Tanabe, K.Tanabe, H.J.Mang Application of the Cranked Temperature-Dependent Hartree-Fock-Bogoliubov Theory to the Excited States in the Deformed Nucleus NUCLEAR STRUCTURE 154Er; calculated excitation energy vs temperature, spin-dependent, total level densities, deformation parameter vs excitation energy; deduced thermal effect on nucleon pairs, proton, neutron gap differences. Temperature-dependent HFB.
doi: 10.1016/0375-9474(81)90625-4
1979HA57 Nucl.Phys. A332, 69 (1979) On the Quantum Number Projection (II). Projection of Particle Number NUCLEAR STRUCTURE 108,110,112,114,116,118,120,122,124,126,128Sn; calculated energy levels, occupation probabilities. General quantum number projection model.
doi: 10.1016/0375-9474(79)90095-2
1979SU03 Phys.Rev. C19, 545 (1979) Effective Coriolis Coupling and Nuclear Kondo Effect NUCLEAR STRUCTURE 156,164,172Er; calculated effective coupling constant of Coriolis term treating interaction of intruder nucleon with nucleons of rotor by renormalization group method.
doi: 10.1103/PhysRevC.19.545
1975TA14 Phys.Rev. C12, 1346 (1975) Photon Propagation in Nuclear Matter and the Correction to the Theoretical Nuclear Charge Density NUCLEAR REACTIONS 90Zr, 208Pb(μ-, X); calculated charge density in muonic atoms. Nucleon Compton scattering on photon propagator.
doi: 10.1103/PhysRevC.12.1346
1973SU06 Nucl.Phys. A208, 317 (1973) The Yrast States on the Asymmetric Rotor Model NUCLEAR STRUCTURE 158,161,162,163,165Er; calculated yrast levels, J.
doi: 10.1016/0375-9474(73)90379-5
1972KO44 Progr.Theor.Phys. 48, 182 (1972) T.Kohmura, K.Tanabe, Y.Futami, A.Fujii Forward Deuteron Emission in High Energy Proton-Nucleus Collision and Nuclear Correlations
doi: 10.1143/PTP.48.182
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