NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = N.Hinohara Found 41 matches. 2024HI03 Phys.Rev. C 109, 034302 (2024) N.Hinohara, T.Oishi, K.Yoshida Triplet-odd pairing in finite nuclear systems: Even-even singly closed nuclei
doi: 10.1103/PhysRevC.109.034302
2023GI09 Phys.Rev. C 108, 044316 (2023) H.Gil, N.Hinohara, C.H.Hyun, K.Yoshida Nuclear mass table in density functional approach inspired by neutron-star observations
doi: 10.1103/PhysRevC.108.044316
2023NA20 Phys.Rev. C 108, 014318 (2023) Local α-removal strength in the mean-field approximation NUCLEAR STRUCTURE 112,116,120,124Sn; calculated nucleon density distributions for neutrons and protons, local α-removal strengths, integrated local α-removal strength, local α probabilities for excited residual nuclei, localization functions for neutrons and protons. Hartree-Fock+BCS method used for mean-field calculation. Defined "local α-removal strength" to quantify the possibility to form an α particle at a specific location inside the nucleus.
doi: 10.1103/PhysRevC.108.014318
2022HI02 Phys.Rev. C 105, 044314 (2022) Global calculation of two-neutrino double-β decay within the finite amplitude method in nuclear density functional theory NUCLEAR STRUCTURE 76Ge, 76Se, 130Te, 130Xe, 136Xe, 136Ba, 150Nd, 150Sm; calculated ground state properties, quadrupole deformation, neutron and proton pairing gaps, total energies. 48Ca, 48Ti, 82Se, 82Kr, 96Zr, 96Mo, 100Mo, 100Ru, 116Cd, 116Sn, 128Te, 128Xe, 238U, 238Pu; calculated quadrupole deformation, neutron and proton pairing gaps. Proton-neutron version of the finite amplitude method (pnFAM) with SkM* functional. Comparison to experimental data. RADIOACTIVITY 46,48Ca, 70Zn, 76Ge, 80,82Se, 86Kr, 94,96Zr, 98,100Mo, 104Ru, 110Pd, 114,116Cd, 122,124Sn, 128,130Te, 134,136Xe, 142Ce, 146,148,150Nd, 154Sm, 160Gd, 170Er, 176Yb, 186W, 192Os, 198Pt, 204Hg, 226Ra, 232Th, 238U, 244Pu, 248Cm(2β-); calculated matrix elements. 76Ge, 76Se, 130Te, 130Xe, 136Xe, 136Ba, 150Nd, 150Sm(2β-); calculated summed Fermi- and Gamow-Teller transitions. Proton-neutron version of the finite amplitude method (pnFAM) within time-dependent DFT. Used functional are fit globally to single-beta-decay half-lives and charge-exchange giant-resonance energies. Comparison to available experimental data.
doi: 10.1103/PhysRevC.105.044314
2022KA44 Phys.Rev. C 106, 054312 (2022) Collective model for cluster motion in 8Be, 12C, and 16O systems based on microscopic 2α, 3α, and 4α models NUCLEAR STRUCTURE 8Be, 12C, 16O; calculated levels, J, π, energies, rms radii. Generator coordinate method (GCM) calculations in restricted model space of nα systems within highly symmetric configurations. Description of radial cluster motion in the ground and excited states with collective model in one-dimensional coordinate by utilizing inputs from the parity-projected microscopic nα wave functions. Comparison to microscopic calculations and experimental data.
doi: 10.1103/PhysRevC.106.054312
2021WA03 Phys.Rev. C 103, 014306 (2021) K.Washiyama, N.Hinohara, T.Nakatsukasa Finite-amplitude method for collective inertia in spontaneous fission RADIOACTIVITY 240Pu, 256Fm(SF); calculated collective inertia for fission dynamics, potential energy and pairing gaps for neutrons and protons as a function of quadrupole moment using the local quasiparticle random-phase approximation (LQRPA) with fission path obtained from constrained Hartree-Fock-Bogoliubov method with Skyrme energy density functional (EDF), and the finite-amplitude method (FAM) with a contour integration technique. Relevance to fission dynamics in heavy and superheavy nuclei to microscopically describe large-amplitude nuclear collective motion.
doi: 10.1103/PhysRevC.103.014306
2020HA14 Phys.Rev. C 101, 044311 (2020) J.Ha, T.Sumikama, F.Browne, N.Hinohara, A.M.Bruce, S.Choi, I.Nishizuka, S.Nishimura, P.Doornenbal, G.Lorusso, P.-A.Soderstrom, H.Watanabe, R.Daido, Z.Patel, S.Rice, L.Sinclair, J.Wu, Z.Y.Xu, A.Yagi, H.Baba, N.Chiga, R.Carroll, F.Didierjean, Y.Fang, N.Fukuda, G.Gey, E.Ideguchi, N.Inabe, T.Isobe, D.Kameda, I.Kojouharov, N.Kurz, T.Kubo, S.Lalkovski, Z.Li, R.Lozeva, H.Nishibata, A.Odahara, Zs.Podolyak, P.H.Regan, O.J.Roberts, H.Sakurai, H.Schaffner, G.S.Simpson, H.Suzuki, H.Takeda, M.Tanaka, J.Taprogge, V.Werner, O.Wieland Shape evolution of neutron-rich 106, 108, 110Mo isotopes in the triaxial degree of freedom RADIOACTIVITY 106,108,110Nb, 106,108,110Zr(β-); 108,110Nb(β-n)[from 9Be(238U, F), E=345 MeV/nucleon, followed by separation of ions using BigRIPS fragment separator and transported through the ZeroDegree spectrometer at RIBF-RIKEN facility]; measured Eγ, Iγ, β-, β-γγ-coin, and half-lives of decays of 106Nb, 108Nb, 110Nb and 110Zr from β-delayed γ-decay curves, half-lives of the first 2+ states in 106Mo, 108Mo and 110Mo using WAS3ABi system for ion and β- detection, EURICA array for γ detection, and fast-timing array for level half-lives. 106,108,110Mo; deduced levels, J, π, bands, configurations, β feedings, logft, B(E2) ratios, quadrupole deformation, kinematic moment of inertia for the ground bands, staggering pattern. 108,110Nb; deduced %β-n or Pn from the β-delayed γ rays emitted from the daughter nuclei, two β-decaying states or an isomer in 110Nb. 106,108,110Nb; deduced J, π; discussed Nilsson configurations. Comparison with theoretical calculations. Systematics of E(4+)/E(first 2+) ratios in N(even)=56-72, Zr, Mo, Ru and Pd isotopes, and level energy staggering pattern relative to the first 2+ states in N=64, 66, 68 Mo, Ru, and Pd isotopes. NUCLEAR STRUCTURE 106,108,110Mo; calculated levels, J, π, potential-energy surface (PES) contours and the collective-wave functions for low-lying positive-parity states. Comparison with beyond-meanfield calculations using the constrained Hartree-Fock-Bogoliubov and local quasiparticle-random-phase approximation with SLy5+T interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.044311
2020SH26 Phys.Rev. C 102, 044325 (2020) Y.Shi, N.Hinohara, B.Schuetrumpf Implementation of nuclear time-dependent density-functional theory and its application to the nuclear isovector electric dipole resonance NUCLEAR STRUCTURE 16O, 24,34Mg, 40Ca, 92,94,96,98,100Mo, 90,92,94Zr; calculated isovector electric dipole resonance response functions, cross sections, photoabsorption σ(E), ground-state energies decomposed into various terms, root-mean-square radii, time evolution of the isovector density, E1 strength functions, EWSR values of the isovector dipole (IVD) operator, isovector E1 σ(E). 98,100,102,104,106,108Zr, 100,102,104,106,108,110Mo, 102,104,106,108,110,112Ru; calculated potential energy surfaces in (Q20, Q22) plane, photoabsorption σ(E), pairing energies, quadrupole moments, and triaxial parameters γ. Time-dependent density functional theory (TDDFT) with BCS pairing for isovector (IV) electric dipole (E1) observables, and finite-amplitude method for quasiparticle random phase approximation (FAM-QRPA) calculations for 16O, 24,34Mg, 40Ca for benchmarking.
doi: 10.1103/PhysRevC.102.044325
2019HI07 Phys.Rev. C 100, 024310 (2019) Energy-weighted sum rule for nuclear density functional theory NUCLEAR STRUCTURE 166Dy, 208Pb; calculated energy-weighted sum rule (EWSR) for the isoscalar and isovector multipole operators up to L=3 for selected spherical and axially deformed nuclei using nuclear density functional theory (DFT), without using EDF Hamiltonian.
doi: 10.1103/PhysRevC.100.024310
2018HI01 J.Phys.(London) G45, 024004 (2018) Extending pairing energy density functional using pairing rotational moments of inertia NUCLEAR STRUCTURE Sn, Pb; calculated neutron pairing gap, neutron pairing rotational moment of inertia, neutron pair density and kinetic energy. The pairing energy density functionals (EDFs).
doi: 10.1088/1361-6471/aa9f8b
2018NI17 Phys.Rev. C 98, 064327 (2018) F.Ni, N.Hinohara, T.Nakatsukasa Low-lying collective excited states in nonintegrable pairing models based on the stationary-phase approximation to the path integral NUCLEAR STRUCTURE 186,188,190,192,194Pb; calculated eigenvalues of moving-frame quasi-random phase approximation equation as a function of collective coordinate, occupation numbers in each single-particle level, collective potentials, energies of first and second excited states, strength of pair-addition transitions, and pairing gap using stationary-phase approximation (SPA) to the path integral, combined with the adiabatic self-consistent collective coordinate method (ASCC+SPA). Description of low-lying excited 0+ states in nonintegrable pairing systems.
doi: 10.1103/PhysRevC.98.064327
2016HI02 Phys.Rev.Lett. 116, 152502 (2016) Pairing Nambu-Goldstone Modes within Nuclear Density Functional Theory NUCLEAR STRUCTURE 116Sn, Ca, Sn, Er, Pb; calculated neutron pairing-rotational energy, chemical potential and pairing-rotational moment of inertia, pairing-rotational moments of inertia; deduced T=1 pairing-rotational moments of inertia of semimagic and doubly-open-shell nuclei within the NG formalism of the broken gauge symmetry.
doi: 10.1103/PhysRevLett.116.152502
2016MA10 J.Phys.(London) G43, 024006 (2016) K.Matsuyanagi, M.Matsuo, T.Nakatsukasa, K.Yoshida, N.Hinohara, K.Sato Microscopic derivation of the quadrupole collective Hamiltonian for shape coexistence/mixing dynamics NUCLEAR STRUCTURE 72Kr, 30,32,34Mg; calculated potential energy surfaces, J, π, energy levels. Large-amplitude collective motions (LACM).
doi: 10.1088/0954-3899/43/2/024006
2016MA71 Phys.Scr. 91, 063014 (2016) K.Matsuyanagi, M.Matsuo, T.Nakatsukasa, K.Yoshida, N.Hinohara, K.Sato Microscopic derivation of the Bohr-Mottelson collective Hamiltonian and its application to quadrupole shape dynamics
doi: 10.1088/0031-8949/91/6/063014
2016ME02 Phys.Rev. C 93, 014305 (2016) J.Menendez, No.Hinohara, J.Engel, G.Martinez-Pinedo, T.R.Rodriguez Testing the importance of collective correlations in neutrinoless ββ decay RADIOACTIVITY 42,44,46,48,50,52,54,56,58,60Ca, 44,46,48,50,52,54,56,58Ti, 46,48,50,52,54,56,58,60Cr(2β-); calculated Gamow-Teller part of the 0νββ decay matrix elements, percentage of ground state in daughter nuclei belonging to SU(4) irreducible representations using shell model with KB3G interaction, full collective interaction Hcoll, Hcoll with the quadrupole-quadrupole term removed, Hcoll with the isoscalar pairing term removed, and Hcoll with both the isoscalar-pairing and spin-isospin removed. 48Ca, 76Ge, 82Se, 124Sn, 130Te, 136Xe(2β-); calculated Gamow-Teller matrix elements for 0νββ decay and estimated effect of isoscalar pairing. Role of collective correlations in 0νββ decay. Comparison of GCM calculations for fp shell nuclei with full shell-model calculations. NUCLEAR STRUCTURE 46,48,50,52,54,56,58,60Cr; calculated B(E2) for first 2+ states using shell model with KB3G interaction, full collective interaction Hcoll, and by Hcoll without the quadrupole-quadrupole part. Comparison with experimental values.
doi: 10.1103/PhysRevC.93.014305
2016OI01 Phys.Rev. C 93, 034329 (2016) T.Oishi, M.Kortelainen, N.Hinohara Finite amplitude method applied to the giant dipole resonance in heavy rare-earth nuclei NUCLEAR STRUCTURE 152,154,156,158,160,162,164Gd, 156,160,162,164,166,168Dy, 162,164,166,168,170,172,174Er, 168,170,172,174,176,178Yb, 174,176,178,180,182,184Hf, 180,182,184,186,188,190W; calculated axial deformation β, pairing gaps for neutrons and protons, energy-weighted sum rule, and its enhancement factor from the Thomas-Reiche-Kuhn (TRK) sum rule for ground states. Hartree-Fock-Bogoliubov (HFB) calculation with Skyrme EDF framework (SkM* parameterization). NUCLEAR REACTIONS 144,145Sm, 152,154,156,158,160,162,164Gd, 156,160,162,164,166,168Dy, 162,164,166,168,170,172,174Er, 168,170,172,174,176,178Yb, 174,176,178,180,182,184Hf, 180,182,184,186,188,190W(γ, X), E not given; calculated E1 photoabsorption σ as function of excitation energy, mean giant dipole resonance (GDR) frequencies and widths within a parallelized finite amplitude method, and quasiparticle random phase approximation (FAM-QRPA) scheme, with the Skyrme energy density functional in the nuclear density functional theory (DFT) applied for ground states and FAM-QRPA for excitations. Comparison with experimental data. Discussed role of role of the Thomas-Reiche-Kuhn (TRK) sum rule enhancement factor, connected to the isovector effective mass.
doi: 10.1103/PhysRevC.93.034329
2015HI03 Phys.Rev. C 91, 044323 (2015) No.Hinohara, M.Kortelainen, W.Nazarewicz, E.Olsen Complex-energy approach to sum rules within nuclear density functional theory NUCLEAR STRUCTURE 24Mg; calculated energy weighted Kπ=0+ sum rule for the oblate minimum. 142,144,146,148,150,152Nd, 144,146,148,150,152,154Sm; calculated isoscalar monopole and quadrupole energy-weighted Kπ=0+ sum rules, quadrupole deformation β, neutron and proton pairing gaps, total rms radius. Complex-energy finite-amplitude method (FAM) based on quasiparticle random-phase approximation (QRPA), and Hartree-Fock-Bogoliubov (HFB) techniques.
doi: 10.1103/PhysRevC.91.044323
2015HI07 Phys.Rev. C 92, 034321 (2015) Collective inertia of the Nambu-Goldstone mode from linear response theory NUCLEAR STRUCTURE 26Mg; calculated Thouless-Valatin inertia, FAM strength function for the proton pairing-rotational angle operator. 110,112,114,116,118,120,122,124,126Sn; 120,122,124,126,128,130,132,134,136Xe; 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er; 126Sn, 128Te, 130Xe, 132Ba, 134Ce, 136Nd, 138Sm, 140Gd; 130Sm, 130Nd, 130Ce, 130Ba, 130Xe, 130Te, 130Sn, 130Cd; 122Sn, 126Te, 130Xe, 134Ba, 138Ce, 142Nd; calculated neutron and proton pairing rotational energies with the Thouless-Valatin collective inertias. Spurious zero-energy Nambu-Goldstone (NG) mode. Finite amplitude method (FAM) for response function of superfluid nuclei with SLy4+volume pairing nuclear density functional theory. Comparison with other theoretical approaches, and with experimental data.
doi: 10.1103/PhysRevC.92.034321
2015KO18 Phys.Rev. C 92, 051302 (2015) M.Kortelainen, N.Hinohara, W.Nazarewicz Multipole modes in deformed nuclei within the finite amplitude method NUCLEAR STRUCTURE 154Sm; calculated levels, B(E3). 240Pu; calculated isoscalar and isovector quadrupole and isovector octupole strength of giant resonances. Finite amplitude method (FAM) quasiparticle random phase approximation (QRPA).
doi: 10.1103/PhysRevC.92.051302
2014HI06 Phys.Rev. C 90, 031301 (2014) Proton-neutron pairing amplitude as a generator coordinate for double-β decay RADIOACTIVITY 76Ge(2β-); calculated matrix elements for neutrinoless double β decay (0νββ), and square of the collective wave functions using generator coordinate method (GCM) and larger single-particle spaces than the shell model.
doi: 10.1103/PhysRevC.90.031301
2014MA98 Phys.Scr. 89, 054020 (2014) M.Matsuo, N.Hinohara, K.Sato, K.Matsuyanagi, T.Nakatsukasa, K.Yoshida Quadrupole shape dynamics from the viewpoint of a theory of large-amplitude collective motion NUCLEAR STRUCTURE 58,60,62,64,66Cr; calculated low-lying quadrupole shape dynamics using large-scale collective motion; deduced deformation, shape-coexistence, shape-mixing, shape-transitional behavior, B(E2). Partially compared with data.
doi: 10.1088/0031-8949/89/5/054020
2014SH11 Phys.Rev. C 89, 054317 (2014) J.A.Sheikh, N.Hinohara, J.Dobaczewski, T.Nakatsukasa, W.Nazarewicz, K.Sato Isospin-invariant Skyrme energy-density-functional approach with axial symmetry NUCLEAR STRUCTURE A=78, 48, 40; calculated total Hartree-Fock (HF) energy, single-particle energies and Routhians with and without isospin-symmetry-breaking Coulomb term, neutron and proton rms radii for isobaric analog chains. 78Ni, 78Zn, 78Ge, 78Se, 78Kr, 78Sr, 78Zr, 78Mo, 78Ru, 78Pd, 78Cd, 78Sn; calculated g9/2 proton effective HF potential, rms radii, single-particle energies. binding energy. Extension of existing axial DFT solver HFBTHO to isospin-invariant Skyrme EDF approach with all possible p-n (isospin) mixing terms. Comparison between HFODD and HFBTHO results.
doi: 10.1103/PhysRevC.89.054317
2013HI05 Phys.Rev. C 87, 064309 (2013) N.Hinohara, M.Kortelainen, W.Nazarewicz Low-energy collective modes of deformed superfluid nuclei within the finite-amplitude method NUCLEAR STRUCTURE 24Mg; calculated low-lying QRPA energies of K=0 states, isoscalar and isovector monopole strengths. 166,168,172Yb, 170Er; calculated FAM-QRPA energies, B(E2), isoscalar and isovector quadrupole strength for low-lying K=0 states. Superfluid nuclear density functional theory with Skyrme energy density functionals, the FAM-QRPA approach, and the conventional matrix formulation of the QRPA.
doi: 10.1103/PhysRevC.87.064309
2012HI02 Phys.Rev. C 85, 024323 (2012) N.Hinohara, Z.P.Li, T.Nakatsukasa, T.Niksic, D.Vretenar Effect of time-odd mean fields on inertial parameters of the quadrupole collective Hamiltonian NUCLEAR STRUCTURE 128,130,132Xe, 130,132,134Ba; calculated triaxial quadrupole binding energy maps, and quadrupole energy surfaces in β-γ plane, ratios of moments of inertia, ratios of vibrational mass parameters, cranking mass parameters, low-lying levels, J, π. Hybrid model based on microscopic collective Hamiltonian and CHFB+LQRPA method to estimate the contribution of time-odd mean fields (Thouless-Valatin contribution). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.024323
2012HI08 Prog.Theor.Phys.(Kyoto), Suppl. 196, 328 (2012) N.Hinohara, K.Sato, K.Yoshida, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Microscopic Analysis of Shape Coexistence/Mixing and Shape Phase Transition in Neutron-Rich Nuclei around 32Mg NUCLEAR STRUCTURE 30,32,34,36Mg; analyzed quadrupole dynamics data; deduced enhancement of the quadrupole collectivity using collective Hamiltonian approach.
doi: 10.1143/PTPS.196.328
2012SA33 Phys.Rev. C 86, 024316 (2012) K.Sato, N.Hinohara, K.Yoshida, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Shape transition and fluctuations in neutron-rich Cr isotopes around N=40 NUCLEAR STRUCTURE 58,60,62,64,66Cr; calculated potential energy surface contours in β-γ plane, levels, B(E2), vibrational wave functions contours, E0 transition strengths. Solution of Schrodinger equation for five-dimensional quadrupole collective Hamiltonian, with constrained Hartree-Fock-Bogoliubov plus local quasiparticle random-phase approximation (CHFB+LQRPA) method. Large-amplitude shape fluctuations in low-lying states. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.024316
2012SA63 J.Phys.:Conf.Ser. 381, 012103 (2012) K.Sato, N.Hinohara, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Microscopic approach to large-amplitude deformation dynamics with local QRPA inertial masses NUCLEAR STRUCTURE 72Kr; calculated levels, J, π, deformation, B(E2) using CHFB (constrained HFB) + LQRPA (local QRPA). 58,60,62,64Cr; calculated levels, J, π, deformation, spectroscopic quadrupole moment, B(E2) using CHFB.
doi: 10.1088/1742-6596/381/1/012103
2011HI01 Phys.Rev. C 83, 014321 (2011) Triaxial quadrupole deformation dynamics in sd-shell nuclei around 26Mg NUCLEAR STRUCTURE 24Ne, 24,26Mg, 28Si; calculated collective potential contours in β-γ plane, neutron and proton pairing gaps, levels, J, π, B(E2) values, and spectroscopic quadrupole moments for ground-state bands, β-, and γ-vibrational states, vibrational wave functions, rotational moments of inertia, and E2 transition density contour plots in β-γ plane. Calculations based on quadrupole collective Hamiltonian constructed with the use of the constrained Hartree-Fock-Bogoliubov plus the local quasiparticle random-phase approximation (CHB+LQRPA) method. Large-amplitude quadrupole dynamics of axial and triaxial deformation. Comparison with experimental data for sd-shell nuclei.
doi: 10.1103/PhysRevC.83.014321
2011HI03 Acta Phys.Pol. B42, 443 (2011) N.Hinohara, K.Sato, T.Nakatsukasa, M.Matsuo Local QRPA Vibrational and Rotational Inertial Functions for Large-amplitude Quadrupole Collective Dynamics NUCLEAR STRUCTURE 68,76Se; calculated collective potential, energies, J, π. Comparison with experimental data.
doi: 10.5506/APhysPolB.42.443
2011HI18 Phys.Rev. C 84, 061302 (2011) N.Hinohara, K.Sato, K.Yoshida, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Shape fluctuations in the ground and excited 0+ states of 30, 32, 34Mg NUCLEAR STRUCTURE 30,32,34,36Mg; calculated collective potential surfaces, levels, J, π, B(E2) values for low-lying positive-parity states, vibrational wave functions. Five-dimensional (5D) quadrupole collective Schrodinger equation, constrained Hartree-Fock-Bogoliubov plus local quasiparticle random phase approximation. Ground and excited 0+ states. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.061302
2011SA09 Nucl.Phys. A849, 53 (2011) Shape mixing dynamics in the low-lying states of proton-rich Kr isotopes NUCLEAR STRUCTURE 72,74,76Kr; calculated levels, J, π, B(E2), deformation parameters and related properties using a 5-D quadrupole collective Hamiltonian. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.11.003
2011SA69 J.Phys.:Conf.Ser. 312, 092054 (2011) Microscopic analysis of shape mixing in low-lying states of proton-rich nuclei in the Se-Kr region NUCLEAR STRUCTURE 72,74,76Kr; calculated deformation, potential energy, moment of inertia, quadrupole moment. 72Kr; calculated levels, J, π, γ transitions, B(E2). CHFB (constrained HFB) + LQRPA (local QRPA). Compared to available data.
doi: 10.1088/1742-6596/312/9/092054
2011WA26 Phys.Lett. B 704, 270 (2011) H.Watanabe, K.Yamaguchi, A.Odahara, T.Sumikama, S.Nishimura, K.Yoshinaga, Z.Li, Y.Miyashita, K.Sato, L.Prochniak, H.Baba, J.S.Berryman, N.Blasi, A.Bracco, F.Camera, J.Chiba, P.Doornenbal, S.Go, T.Hashimoto, S.Hayakawa, C.Hinke, N.Hinohara, E.Ideguchi, T.Isobe, Y.Ito, D.G.Jenkins, Y.Kawada, N.Kobayashi, Y.Kondo, R.Krucken, S.Kubono, G.Lorusso, T.Nakano, T.Nakatsukasa, M.Kurata-Nishimura, H.J.Ong, S.Ota, Zs.Podolyak, H.Sakurai, H.Scheit, K.Steiger, D.Steppenbeck, K.Sugimoto, K.Tajiri, S.Takano, A.Takashima, T.Teranishi, Y.Wakabayashi, P.M.Walker, O.Wieland, H.Yamaguchi Development of axial asymmetry in the neutron-rich nucleus 110Mo RADIOACTIVITY 110Nb(β-) [from Be(238U, X), E=345 MeV/nucleon]; measured decay products, Eγ, Iγ, X-rays. 110Mo; deduced energy levels, J, π, quasi-γ-band state, B(e2) ratio. Comparison with general Bohr Hamiltonian method calculations, systematics of low-lying levels of even-even Mo nuclei. NUCLEAR STRUCTURE 104,106,108,110Mo; calculated moments of inertia, potential energy surface, the nuclear landscape. General Bohr Hamiltonian method calculations.
doi: 10.1016/j.physletb.2011.09.050
2011YO04 Phys.Rev. C 83, 061302 (2011) Shape changes and large-amplitude collective dynamics in neutron-rich Cr isotopes NUCLEAR STRUCTURE 58,60,62,64,66,68Cr; calculated total energy curves, energies of first 2+ and 4+ states, B(E2) and spectroscopic quadrupole moment of first 2+ states, rms radii, quadrupole masses, and collective wave functions of ground states. Microscopic model for the collective motion based on the Skyrme and the pairing energy density functionals (EDF). Comparison with experimental data.
doi: 10.1103/PhysRevC.83.061302
2010HI09 Phys.Rev. C 82, 064313 (2010) N.Hinohara, K.Sato, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Microscopic description of large-amplitude shape-mixing dynamics with inertial functions derived in local quasiparticle random-phase approximation NUCLEAR STRUCTURE 68,70,72Se; calculated, in β-γ plane, collective potential surfaces, monopole and quadrupole pairing gaps, vibrational masses, rotational masses, vibrational wave functions, B(E2), excitation energies, and spectroscopic quadrupole moments using constrained Hartree-Fock-Bogoliubov (CHFB) and local quasiparticle random-phase approximation (LQRPA) based on adiabatic self-consistent collective coordinate (ASCC) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.064313
2010SA01 Prog.Theor.Phys.(Kyoto) 123, 129 (2010) K.Sato, N.Hinohara, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi A Model Analysis of Triaxial Deformation Dynamics in Oblate-Prolate Shape Coexistence Phenomena
doi: 10.1143/PTP.123.129
2009HI07 Phys.Rev. C 80, 014305 (2009) N.Hinohara, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Microscopic description of oblate-prolate shape mixing in proton-rich Se isotopes NUCLEAR STRUCTURE 68,70,72Se; calculated levels, J, π, B(E2), quadrupole deformation, collective paths, monopole and quadrupole pairing gaps, collective potential and mass, frequencies at Hartree-Bogoliubov (HB) equilibrium, vibrational wave functions and spectroscopic quadrupole moments using adiabatic self-consistent collective coordinate (ASCC) method.
doi: 10.1103/PhysRevC.80.014305
2009KA17 Phys.Rev. C 79, 054305 (2009) Y.Kanada-Enyo, N.Hinohara, T.Suhara, P.Schuck Dineutron correlations in quasi-two-dimensional systems in a simplified model, and possible relation to neutron-rich nuclei
doi: 10.1103/PhysRevC.79.054305
2008HI02 Prog.Theor.Phys.(Kyoto) 119, 59 (2008) N.Hinohara, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Microscopic Derivation of Collective Hamiltonian by Means of the Adiabatic Self-Consistent Collective Coordinate Method -Shape Mixing in Low-Lying States of 68Se and 72Kr- NUCLEAR STRUCTURE 68Se, 72Kr; calculated level energies, B(E2), quadrupole deformation parameters, and pairing gaps using the ASCC method in conjunction with P+Q hamiltonian.
doi: 10.1143/PTP.119.59
2007HI03 Prog.Theor.Phys.(Kyoto) 117, 451 (2007) N.Hinohara, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Gauge-Invariant Formulation of the Adiabatic Self-Consistent Collective Coordinate Method
doi: 10.1143/PTP.117.451
2006HI03 Prog.Theor.Phys.(Kyoto) 115, 567 (2006) N.Hinohara, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Effects of Time-Odd Components in Mean Field on Large Amplitude Collective Dynamics
doi: 10.1143/PTP.115.567
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