NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = T.Mizusaki Found 106 matches. Showing 1 to 100. [Next]2023KA05 Phys.Rev.Lett. 130, 052501 (2023) K.Kaneko, Y.Sun, N.Shimizu, T.Mizusaki Quasi-SU(3) Coupling Induced Oblate-Prolate Shape Phase Transition in the Casten Triangle NUCLEAR STRUCTURE 122,124,126,128,130,132Te, 124,126,128,130,132,134Xe, 126,128,130,132,134,136Ba; calculated energy levels, J, π, B(E2), quadrupole moments, potential energy surfaces using HFB+GCM with the PMMU Hamiltonian; deduced hidden symmetries from the vast shell-model configurations, microscopical insights into the empirical symmetry triangle.
doi: 10.1103/PhysRevLett.130.052501
2022KI17 Phys.Rev. C 106, 034311 (2022) S.Kisyov, C.Y.Wu, J.Henderson, A.Gade, K.Kaneko, Y.Sun, N.Shimizu, T.Mizusaki, D.Rhodes, S.Biswas, A.Chester, M.Devlin, P.Farris, A.M.Hill, J.Li, E.Rubino, D.Weisshaar Structure of 126, 128Xe studied in Coulomb excitation measurements NUCLEAR REACTIONS 196Pt, 208Pb(126Xe, 126Xe'), (128Xe, 128Xe'), E(126Xe)=3.74 MeV/nucleon, E(128Xe)=3.81 MeV/nucleon; measured reaction products, Eγ, Iγ, (126Xe)γ-coin, (128Xe)γ-coin using JANUS array consisting of a pair of segmented double-sided Si detectors for particles, and SeGA array with sixteen 32-fold segmented HPGe detector for γ radiation at the NSCL-MSU facility. 126,128Xe; deduced levels, J, π, E2 matrix elements, B(E2), static quadrupole moments. GOSIA + GOSIA2 analyses; calculated Potential-energy surfaces (PES) in (Q0, Q2) plane. Comparison with PMMU shell model calculations, and with previous experimental results.
doi: 10.1103/PhysRevC.106.034311
2021KA15 Phys.Rev. C 103, L021301 (2021) K.Kaneko, N.Shimizu, T.Mizusaki, Y.Sun Quasi-SU(3) coupling of (1h11/2, 2f7/2) across the N=82 shell gap: Enhanced E2 collectivity and shape evolution in Nd isotopes NUCLEAR STRUCTURE 56Ni; calculated levels, J, π using HFB+gcm and exact shell-model, and compared with experimental data. 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130Sn, 108,110,112,114,116,118,120,122,124,126,128,130,132,134Te, 110,112,114,116,118,120,122,124,126,128,130,132,134,136Xe, 118,120,122,124,126,128,130,132,134,136,138Ba, 126,128,130,132,134,136,138,140Ce, 128,130,132,134,136,138,140,142Nd, 130,132,134,136,138,140,142,144Nd; calculated energies of the first 2+ and 4+ levels, B(E2) for the first 2+ states, and compared with experimental data. 128,130,132,134,136,138,140,142Nd; calculated energies of levels in the g.s. yrast band up to 12+, Qs and B(E2) for the first 2+ states in the gdshf model space, potential energy surfaces for 130,138,142Nd. Comparison with experimental data. Projected Hartree-Fock-Bogolyubov plus generator coordinate method using the PMMU model in the model space of 1g9/2, 1g7/2, 2d5/2, 2d3/2, 3s1/2, and 1h11/2 orbitals.
doi: 10.1103/PhysRevC.103.L021301
2021MI14 Phys.Rev. C 104, L031305 (2021) Symmetry projection to coupled-cluster singles plus doubles wave function through the Monte Carlo method
doi: 10.1103/PhysRevC.104.L031305
2021SH24 Phys.Rev. C 103, 064302 (2021) N.Shimizu, T.Mizusaki, K.Kaneko, Y.Tsunoda Generator-coordinate methods with symmetry-restored Hartree-Fock-Bogoliubov wave functions for large-scale shell-model calculations NUCLEAR STRUCTURE 48Ca, 56Ni, 132,133Ba; calculated levels, J, π, B(E2), quadrupole moments, and total energy surface contours in (Q0, Q2) plane using generator HFB-based coordinate method (GCM) combined with the projection method for large-scale shell model calculations. Benchmark tests of the axial HF+GCM, HF+GCM, axial HFB+GCM, and HFB+GCM methods for 48Ca and 132Ba. Possible relevance to proton-neutron mixing of the quasiparticle vacuum for precise estimation of nuclear matrix element (NMEs) for neutrinoless double-β decay.
doi: 10.1103/PhysRevC.103.064302
2019KA19 Nucl.Phys. A986, 107 (2019) K.Kaneko, Y.Sun, T.Mizusaki, D.G.Jenkins, S.K.Ghorui, S.Tazaki Large mirror asymmetry in Gamow-Teller β-decay in the A=26 isobaric multiplet RADIOACTIVITY 26Na, 27Mg, 28Al(β-), 26,27,28P(β+), (EC); compiled experimental mirror asymmetry δ from the ft data for mirror nuclei of A=17-35; deduced large mirror asymmetry between 26P and 26Na; calculated ft, mirror asymmetry in GT β-decay using large-scale shell model including Isospin-NonConserving (INC) forces with introduced T=1, J NOT= 0 INC forces deduced good agreement to the data, whereas usual J=0 INC force does not work. Calculations compared with available data.
doi: 10.1016/j.nuclphysa.2019.03.002
2018KA24 Phys.Rev. C 97, 054326 (2018) Isoscalar neutron-proton pairing and SU(4)-symmetry breaking in Gamow-Teller transitions NUCLEAR STRUCTURE 42Sc, 46V, 50Mn, 54Co; calculated cumulative sums of Gamow-Teller transition strengths B(GT) of lowest 1+ states, with separate contributions from each interaction, level energies, B(GT) and overlap between wave functions for the first 0+ and 1+ states. Large-scale shell-model calculations with realistic PMMU Hamiltonian; deduced role of isoscalar T=0, Jπ=1+ np-pairing interaction and SU(4)-symmetry breaking in GT transitions. Comparison with experimental values.
doi: 10.1103/PhysRevC.97.054326
2018SH37 Phys.Rev. C 98, 054309 (2018) Variational Monte Carlo method for shell-model calculations in odd-mass nuclei and restoration of symmetry NUCLEAR STRUCTURE 48Cr; calculated energies of the ground-state band members up to 12+ using variation after and before angular momentum projection (J-VAP and J-VBP), and with the GXPF1A interaction. 49Cr; calculated energies of the 5/2-, 7/2-, 9/2- and 11/2- states with J-VAP approach and GXPF1A interaction. Variational Monte Carlo (VMC) method with and without variation after angular-momentum projection. Comparison with shell-model calculations.
doi: 10.1103/PhysRevC.98.054309
2016WA07 Phys.Rev. C 93, 034322 (2016) L.-J.Wang, Y.Sun, T.Mizusaki, M.Oi, S.K.Ghorui Reduction of collectivity at very high spins in 134Nd: Expanding the projected-shell-model basis up to 10-quasiparticle states NUCLEAR STRUCTURE 134Nd; calculated levels, J, K, π, bands, B(E2), configurations, moment of inertia of yrast band using projected shell model expanded to include up to 10-qp states. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.034322
2015KA46 Phys.Rev. C 92, 044331 (2015) K.Kaneko, T.Mizusaki, Y.Sun, S.Tazaki Systematical shell-model calculation in the pairing-plus-multipole Hamiltonian with a monopole interaction for the pf5/2g9/2 shell NUCLEAR STRUCTURE 64,65,66,67,68,69,70,71,72,73,74,75,76Ni, 64,65,66,67,68,69,70,71,72,73,74,75,76,77,78Cu, 65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80Zn, 66,67,68,69,70,71,72,73,74,75,76,77,78,79,80Ga, 69,70,71,72,73,74,75,76,77,78,79,80Ge, 67,68,69,70,71,72,73,74,75,76,77,78As, 73,74,75,76,77,78,79,80Se; calculated binding energies, effective single-particle energies of proton orbits for Cu isotopes, level energies of low-lying, low spin states and B(E2) values in even- and odd-A isotopes, neutron g9/2 and proton p3/2 occupancies for low lying states in Ge isotopes, magnetic moments and electric quadrupole moments of Cu, Ga, and Ge isotopes. 64,66,68,69,70,71,72,73,74,75,76Ge, 68,69,70,71,72,73,74Se; calculated low- and high-spin levels, J, π, B(E2). Shell-model calculations with a pairing-plus-multipole Hamiltonian and monopole-based universal force interaction (PMMU model) for the pf5/2g9/2 shell nuclei. Comparison with experimental and evaluated data.
doi: 10.1103/PhysRevC.92.044331
2015WA13 Acta Phys.Pol. B46, 497 (2015) L.-J.Wang, F.-Q.Chen, Y.Sun, T.Mizusaki, M.Oi Application of the Pfaffian Algorithm in the Nuclear Structure Study at High Spins NUCLEAR STRUCTURE 166Hf; calculated yrast band at high spin; deduced anomalies. Projected shell model, the Pfaffian algorithm.
doi: 10.5506/APhysPolB.46.497
2014KA03 Phys.Rev. C 89, 011302 (2014) K.Kaneko, T.Mizusaki, Y.Sun, S.Tazaki Toward a unified realistic shell-model Hamiltonian with the monopole-based universal force NUCLEAR STRUCTURE Z=20-28, A=42-64; calculated binding energies and fitted with experimental values for 95 nuclides. 42,44,46,48,50,52,54,56,58Ca, 44,46,48,50,52,54,56,58,60Ti, 48,50,52,54,56,58,60,62Cr, 52,54,56,58,60,62,64Fe, 56,58,60,62,64,66,68,70,72,74Ni, 60,62,64,66,68,70,72,74,76,78,80Zn, 64,66,68,70,72,74,76,78,80,82Ge, 68,70,72,74,76,78,80,82,84Se; calculated energies and B(E2) for first 2+ levels. 55Co, 56Ni, 69,72Ge; calculated levels, J, π. Unified realistic shell-model Hamiltonian employing pairing plus multipole Hamiltonian combined with monopole interaction (PMMU model). Comparison with experimental data.
doi: 10.1103/PhysRevC.89.011302
2014KA08 Phys.Rev. C 89, 031302 (2014) K.Kaneko, Y.Sun, T.Mizusaki, S.Tazaki Isospin nonconserving interaction in the T=1 analogue states of the mass-70 region NUCLEAR STRUCTURE A=66-78; calculated mirror energy differences (MEDs) and triplet energy differences (TEDs) for even-even nuclei in the T=1 analog states; calculated Coulomb energy differences for N=Z nuclei 66As-66Ge, 70Br-70Se, 74Rb-74Kr, and 78Y-78Sr. Large-scale shell-model calculations. Effect of isospin nonconserving (INC) nuclear force for the upper fp-shell region. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.031302
2014MI17 Prog.Theor.Exp.Phys. 2014, 091D01 (2014) A new approach for many-body resonance spectroscopy with the complex scaling method NUCLEAR STRUCTURE 8C; calculated resonance and continuum energies of many-body states. Sakurai-Sugiura method with the complex scaling.
doi: 10.1093/ptep/ptu124
2014WA29 Phys.Rev. C 90, 011303 (2014) L.-J.Wang, F.-Q.Chen, T.Mizusaki, M.Oi, Y.Sun Toward extremes of angular momentum: Application of the Pfaffian algorithm in realistic calculations NUCLEAR STRUCTURE 166Hf; calculated back-bending plot, and level-energy versus spin plot for high-spin band structure. 176Hf; calculated levels, J, π for yrast, 2-qp, 4-qp and 6-qp bands with quantum number K=6, 8, 14, 15, 19, 20, 22, B(E2) values using Pfaffian algorithm to calculate matrix elements for Hartree-Fock-Bogoliubov states for high-spin and multi-qp states. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.011303
2013KA15 Phys.Rev.Lett. 110, 172505 (2013) K.Kaneko, Y.Sun, T.Mizusaki, S.Tazaki Variation in Displacement Energies Due to Isospin-Nonconserving Forces NUCLEAR STRUCTURE A=42-95; calculated Coulomb and triplet displacement energies, one- and two-proton separation energies; deduced importance of isospin-nonconserving forces. Large scale shell model calculation, GXPF1A and JUN45 effective interactions.
doi: 10.1103/PhysRevLett.110.172505
2013SH28 J.Phys.:Conf.Ser. 445, 012004 (2013) N.Shimizu, T.Otsuka, Y.Utsuno, T.Mizusaki, M.Honma, T.Abe History and future perspectives of the Monte Carlo shell model -from Alphleet to K computer-
doi: 10.1088/1742-6596/445/1/012004
2012KA26 Phys.Rev.Lett. 109, 092504 (2012) K.Kaneko, T.Mizusaki, Y.Sun, S.Tazaki, G.de Angelis Coulomb Energy Difference as a Probe of Isospin-Symmetry Breaking in the Upper fp-Shell Nuclei NUCLEAR STRUCTURE 66As, 66Ge, 70Br, 70Se, 74Rb, 74Kr, 78Y, 78Sr; calculated Coulomb energy differences; deduced isospin-symmetry breaking. Shell model calculations, Sakurai-Sugiura algorithm, comparison with available data.
doi: 10.1103/PhysRevLett.109.092504
2012MI02 Phys.Rev. C 85, 021301 (2012) New variational Monte Carlo method with energy variance extrapolation for large-scale shell-model calculations NUCLEAR STRUCTURE 56Ni; calculated levels energy patterns for J=0, 2, 4 states, exact shell-model energies. New variational Monte Carlo (VMC) method with energy variance extrapolation for large scale shell-model calculations.
doi: 10.1103/PhysRevC.85.021301
2012SH13 Phys.Rev. C 85, 054301 (2012) N.Shimizu, Y.Utsuno, T.Mizusaki, M.Honma, Y.Tsunoda, T.Otsuka Variational procedure for nuclear shell-model calculations and energy-variance extrapolation NUCLEAR STRUCTURE 64,72Ge; calculated energy vs. energy variance plot for 0+ ground state and first excited 0+ state. 72Ge; calculated total energy surface contours. Shell-model calculations with energy-variance extrapolation (EVE) method and wavefunctions from linear combinations of the parity, angular-momentum projected Slater determinants.
doi: 10.1103/PhysRevC.85.054301
2012UT01 Prog.Theor.Phys.(Kyoto), Suppl. 196, 304 (2012) Y.Utsuno, T.Otsuka, B.A.Brown, M.Honma, T.Mizusaki, N.Shimizu Shell Evolution around and beyond N=28 Studied with Large-Scale Shell-Model Calculations NUCLEAR STRUCTURE 40,42,44,46,48,50,52Ca; calculated energy levels, distribution of spectroscopic factors; deduced evolution of shell structure. Comparison with experimental data.
doi: 10.1143/PTPS.196.304
2012UT02 Phys.Rev. C 86, 051301 (2012) Y.Utsuno, T.Otsuka, B.A.Brown, M.Honma, T.Mizusaki, N.Shimizu Shape transitions in exotic Si and S isotopes and tensor-force-driven Jahn-Teller effect NUCLEAR STRUCTURE 36,38,40,42Si, 38,40,42,44S; calculated levels, J, π, B(E2), S(2n), potential-energy surfaces. 40,42,44,46Ar, 42,44,46,48Ca; calculated S(2n). 48Ca(e, e'p); calculated spectroscopic factors. Shell-model calculations with tensor-force component of the Hamiltonian. Jahn-Teller type effect. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.051301
2011HA03 Phys.Lett. B 696, 197 (2011) M.Hasegawa, Y.Sun, S.Tazaki, K.Kaneko, T.Mizusaki Characteristics of the 2 1/2+ isomer in 93Mo: Toward the possibility of enhanced nuclear isomer decay NUCLEAR STRUCTURE 93Mo, 93Tc, 95Ru; calculated excitation energy, structure of yrast states, B(E4), B(E2), B(M1). Microscopic shell model calculations, comparison with experimental data.
doi: 10.1016/j.physletb.2010.10.065
2011KA03 Phys.Rev. C 83, 014320 (2011) K.Kaneko, Y.Sun, T.Mizusaki, M.Hasegawa Shell-model study for neutron-rich sd-shell nuclei NUCLEAR STRUCTURE 35Si, 36,37,38,40,42,43,44,46S, 38,39,40,42,43,44,45,46,47,48Ar, 41,49Ca, 47K; calculated levels, J, π. 40Mg, 34,36,38,40,42,44,46,48,50,52Si, 36,38,40,42,44,46,48,50,52,54S, 38,40,42,44,46,48,50,52,54,56Ar, 40,42,44,46,48,50,52,54,56,58Ca; calculated energies of first 2+ states. Z=20, N=20-40; calculated effective proton single-particle energies. Z=8-20, N=20; calculated effective neutron single-particle energies. 36,38,40,42Si, 36,38,40,42,44S, 38,40,42,44,46Ar; calculated B(E2) values for first 2+ states. 40Mg, 42Si, 44S, 44,46Ar, 48Ca; calculated spectroscopic quadrupole moments of first 2+ states. 35,37,39,41,43P, 37,39,41,43,45Cl, 39,41,43,45,47,49K; calculated 3/2+ to 1/2+ splittings. 41Si, 43S, 45Ar, 47Ca; calculated 7/2- to 3/2- splittings. Spherical shell model in the sd-pf valence space with the extended pairing plus quadrupole-quadrupole forces accompanied by the monopole interaction (EPQQM). Comparison with experimental data for sd-shell nuclei.
doi: 10.1103/PhysRevC.83.014320
2011KA07 Acta Phys.Pol. B42, 439 (2011) K.Kaneko, S.Tazaki, T.Mizusaki, Y.Sun, M.Hasegawa, G.de Angelis Mirror Energy Difference at High Spins in the Mirror Pair 67Se and 67As NUCLEAR STRUCTURE 67Se, 67As; calculated mirror energy difference for high-spin states. Comparison with all available data.
doi: 10.5506/APhysPolB.42.439
2011MI01 Acta Phys.Pol. B42, 447 (2011) T.Mizusaki, K.Kaneko, M.Honma, T.Sakurai Filter Diagonalization: A New Method for Large-scale Shell-model Calculations NUCLEAR STRUCTURE 48Cr, 66As, 66Ge; calculated mirror energy differences due to small isospin breaking. Filter diagonalization method.
doi: 10.5506/APhysPolB.42.447
2010KA32 Phys.Rev. C 82, 061301 (2010) K.Kaneko, S.Tazaki, T.Mizusaki, Y.Sun, M.Hasegawa, G.de Angelis Isospin symmetry breaking at high spins in the mirror pair 67Se and 67As NUCLEAR STRUCTURE 67Se, 67As; calculated levels, J, π, mirror energy differences (MED), occupation numbers for proton and neutron orbits, spin distribution in each and spectroscopic quadrupole moments at high spins using large-scale shell-model approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.061301
2010MI16 Phys.Rev. C 82, 024310 (2010) T.Mizusaki, K.Kaneko, M.Honma, T.Sakurai Filter diagonalization of shell-model calculations NUCLEAR STRUCTURE 48Cr; calculated yrast state energies and M1 strength functions using Sakurai and Sugiura (SS)+shifted complex orthogonal conjugate gradient (COCG) method of filter diagonalization for shell-model calculations.
doi: 10.1103/PhysRevC.82.024310
2010SH30 Phys.Rev. C 82, 061305 (2010) N.Shimizu, Y.Utsuno, T.Mizusaki, T.Otsuka, T.Abe, M.Honma Novel extrapolation method in the Monte Carlo shell model NUCLEAR STRUCTURE 56Ni, 64Ge; calculated ground and excited state energies and quadrupole moments using Monte-Carlo shell-model (MCSM).
doi: 10.1103/PhysRevC.82.061305
2009HO14 Phys.Rev. C 80, 064323 (2009) M.Honma, T.Otsuka, T.Mizusaki, M.Hjorth-Jensen New effective interaction for f5pg9-shell nuclei NUCLEAR STRUCTURE Z=28-50, N=28-50; calculated two-body matrix elements, monopole matrix elements, single-particle proton and neutron energies, binding energies, magnetic dipole moments, electric quadrupole moments, levels, and B(E2) using shell-model in f5pg9 model space with a new JUN45 effective interaction based on realistic Bonn-C potential. 64,69,70,71,72,73,74,75Ge, 66,82As, 68Se, 70,84Br, 80Ga, 86Rb, 88Y; calculated levels, J, π, and transition matrix elements using shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.064323
2009SU20 Phys.Rev. C 80, 054306 (2009) Y.Sun, Y.-C.Yang, H.-L.Liu, K.Kaneko, M.Hasegawa, T.Mizusaki Projected shell model description for high-spin states in neutron-rich Fe isotopes NUCLEAR STRUCTURE 58,60,62,64,66,68Fe; calculated levels, J, moment of inertia, B(E2), deformation parameters, yrast band structures using projected shell-model calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.054306
2008KA19 Phys.Rev. C 77, 064304 (2008); Erratum Phys.Rev. C 78, 049903 (2008) K.Kaneko, Y.Sun, M.Hasegawa, T.Mizusaki Structure of upper-g9/2-shell nuclei and shape effect in the 94Ag isomeric states NUCLEAR STRUCTURE 94Ag; calculated levels, J, π, spectroscopic quadrupole moments, expectation values of proton and neutron numbers, B(E2). 90,91,92,93,94Ru, 91,92,93Tc, 90,92,93,94,95Rh, 92,93,94,95,96Pd, 95Ag, 96,98Cd; calculated level energies, J, π. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.064304
2008KA41 Phys.Rev. C 78, 064312 (2008) K.Kaneko, Y.Sun, M.Hasegawa, T.Mizusaki Shell model study of single-particle and collective structure in neutron-rich Cr isotopes NUCLEAR STRUCTURE 52,53,54,55,56,57,58,59,60,62Cr; calculated B(E2), levels, single-particle energies. Spherical shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.064312
2007AD27 Nucl.Phys. A788, 70c (2007) T.Adachi, Y.Fujita, P.von Brentano, G.P.A.Berg, C.Fransen, D.De Frenne, H.Fujita, K.Fujita, K.Hatanaka, M.Honma, E.Jacobs, J.Kamiya, K.Kawase, T.Mizusaki, K.Nakanishi, A.Negret, T.Otsuka, N.Pietralla, L.Popescu, Y.Sakemi, Y.Shimbara, Y.Shimizu, Y.Tameshige, A.Tamii, M.Uchida, T.Wakasa, M.Yosoi, K.O.Zell Gamow-Teller transitions in pf-shell nuclei studied in (3He, t) reactions NUCLEAR REACTIONS 42Ca, 46Ti, 50Cr, 54Fe(3He, t), E=140 MeV/nucleon; measured excitation energy spectra. 42Sc, 46V, 50Mn, 54Co deduced Gamow-Teller strength distribution. Comparison with shell model.
doi: 10.1016/j.nuclphysa.2007.01.050
2007FU14 Phys.Lett. B 650, 9 (2007) S.Fujii, T.Mizusaki, T.Otsuka, T.Sebe, A.Arima Microscopic shell-model description of the exotic nucleus 16C NUCLEAR STRUCTURE 16O; calculated levels, J, π, B(E2), configurations. Shell model, spin-orbit splitting. Comparison with data.
doi: 10.1016/j.physletb.2007.04.067
2007HA35 Nucl.Phys. A789, 46 (2007) M.Hasegawa, T.Mizusaki, K.Kaneko, Y.Sun Enhancement of B(E2)↑ and low excitation of the second 0+ state near N = 40 in Ge isotopes NUCLEAR STRUCTURE 70,72,74Ge; calculated B(E2) using large scale shell model calculations. Compared results to available data.
doi: 10.1016/j.nuclphysa.2007.02.012
2007HA48 Phys.Lett. B 656, 51 (2007) M.Hasegawa, K.Kaneko, T.Mizusaki, Y.Sun Phase transition in exotic nuclei along the N = Z line NUCLEAR STRUCTURE 64Ge, 66As, 68Se, 70Br, 72,74,76Kr, 74Rb, 76Sr; calculated levels, J, π, B(E2); deduced configurations, shape co-existence. Large-scale shell model calculations and comparison with data.
doi: 10.1016/j.physletb.2007.09.017
2007LI84 Eur.Phys.J. Special Topics 150, 135 (2007) S.N.Liddick, P.F.Mantica, R.V.F.Janssens, B.A.Brown, M.P.Carpenter, A.D.Davies, M.Honma, M.Horoi, T.Mizusaki, A.C.Morton, W.F.Mueller, T.Otsuka, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking Beta-delayed γ-ray studies of πf7/2 - νpf shell nuclei
doi: 10.1140/epjst/e2007-00286-4
2007MI19 Acta Phys.Pol. B38, 1363 (2007) T.Mizusaki, K.Kaneko, M.Hasegawa Shell Model Approach to Proton - Neutron Alignment in N ∼ Z Ge - As Nuclei NUCLEAR STRUCTURE 66Ge, 62,63Ga; calculated level energies, J, π using the nuclear shell model.
2007UT02 Eur.Phys.J. Special Topics 150, 187 (2007) Y.Utsuno, T.Otsuka, T.Mizusaki, M.Honma Structure of unstable nuclei in the sd-pf shell region by shell model with proper tensor force
doi: 10.1140/epjst/e2007-00300-y
2006AD05 Phys.Rev. C 73, 024311 (2006) T.Adachi, Y.Fujita, P.von Brentano, A.F.Lisetskiy, G.P.A.Berg, C.Fransen, D.De Frenne, H.Fujita, K.Fujita, K.Hatanaka, M.Honma, E.Jacobs, J.Kamiya, K.Kawase, T.Mizusaki, K.Nakanishi, A.Negret, T.Otsuka, N.Pietralla, L.Popescu, Y.Sakemi, Y.Shimbara, Y.Shimizu, Y.Tameshige, A.Tamii, M.Uchida, T.Wakasa, M.Yosoi, K.O.Zell High-resolution study of Gamow-Teller transitions from the Tz = 1 nucleus 46Ti to the Tz = 0 nucleus 46V NUCLEAR REACTIONS 46Ti(3He, t), E=140 MeV; measured triton spectra, σ(E, θ=0°); deduced Gamow-Teller transition strengths. 46Ti(e, e'), (γ, γ'), E not given; analyzed B(M1).
doi: 10.1103/PhysRevC.73.024311
2006HO07 Phys.Rev. C 73, 061305 (2006); Erratum Phys.Rev. C 74, 059904 (2006) M.Horoi, B.A.Brown, T.Otsuka, M.Honma, T.Mizusaki Shell model analysis of the 56Ni spectrum in the full pf model space NUCLEAR STRUCTURE 56Ni; calculated levels, J, π, B(E2), rotational bands. Shell model, comparison with data.
doi: 10.1103/PhysRevC.73.061305
2006KA39 Phys.Rev. C 74, 024321 (2006); Erratum Phys.Rev. C 74, 049901 (2006) K.Kaneko, M.Hasegawa, T.Mizusaki, Y.Sun Magicity and occurrence of a band with enhanced B(E2) in neutron-rich nuclei 68Ni and 90Zr NUCLEAR STRUCTURE 64,66,68Ni, 86Kr, 88Sr, 90Zr; calculated levels, J, π, B(E2), configurations; deduced shell closure features.
doi: 10.1103/PhysRevC.74.024321
2006SI37 Phys.Rev.C 74, 064312 (2006) M.A.G.Silveira, N.H.Medina, J.R.B.Oliveira, J.A.Alcantara-Nunez, E.W.Cybulska, H.Dias, M.N.Rao, R.V.Ribas, W.A.Seale, K.T.Wiedemann, B.A.Brown, M.Honma, T.Mizusaki, T.Otsuka 58Co: Structure of an odd-odd nucleus in the pf shell NUCLEAR REACTIONS 51V(10B, 2np), E=33, 36 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin, DSA. 58Co deduced high-spin levels, J, π, T1/2, configurations, B(M1), B(E2). Shell-model calculations.
doi: 10.1103/PhysRevC.74.064312
2005FO14 Phys.Rev. C 72, 044315 (2005) B.Fornal, S.Zhu, R.V.F.Janssens, M.Honma, R.Broda, B.A.Brown, M.P.Carpenter, S.J.Freeman, N.Hammond, F.G.Kondev, W.Krolas, T.Lauritsen, S.N.Liddick, C.J.Lister, S.Lunardi, P.F.Mantica, N.Marginean, T.Mizusaki, E.F.Moore, T.Otsuka, T.Pawlat, D.Seweryniak, B.E.Tomlin, C.A.Ur, I.Wiedenhover, J.Wrzesinski Yrast structure of neutron-rich 53Ti NUCLEAR REACTIONS 208Pb(48Ca, X), E=305 MeV; 238U(48Ca, X), E=330 MeV; measured Eγ, Iγ, γγ-coin. 53Ti deduced levels, J, π. Gammasphere array, cross-coincidence with reaction partners. Comparison with model predictions.
doi: 10.1103/PhysRevC.72.044315
2005GA15 Acta Phys.Pol. B36, 1227 (2005) A.Gade, D.Bazin, B.A.Brown, C.M.Campbell, J.A.Church, D.-C.Dinca, J.Enders, T.Glasmacher, P.G.Hansen, M.Honma, T.Mizusaki, W.F.Mueller, H.Olliver, T.Otsuka, L.A.Riley, J.R.Terry, J.A.Tostevin, K.L.Yurkewicz Nuclear spectroscopy with fast exotic beams NUCLEAR REACTIONS 197Au(52Fe, 52Fe'), (54Ni, 54Ni'), (56Ni, 56Ni'), (58Ni, 58Ni'), E not given; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 52Fe, 54,56,58Ni transitions deduced B(E2). 9Be(32S, 31SX), (33Cl, 32ClX), (34Ar, 33ArX), E not given; measured one-neutron removal σ.
2005HA19 Phys.Rev. C 71, 044301 (2005) M.Hasegawa, K.Kaneko, T.Mizusaki Particle alignments and shape change in 66Ge and 68Ge NUCLEAR STRUCTURE 66,68Ge; calculated levels, J, π, rotational bands, B(E2), B(M1), configurations, deformation. Shell model.
doi: 10.1103/PhysRevC.71.044301
2005HA30 Phys.Lett. B 617, 150 (2005) M.Hasegawa, Y.Sun, K.Kaneko, T.Mizusaki Structure of isomeric states in 66As and 67As NUCLEAR STRUCTURE 66,67As; calculated levels, J, π, isomeric states, shape coexistence features. Spherical shell model.
doi: 10.1016/j.physletb.2005.05.027
2005HA70 Phys.Rev. C 72, 064320 (2005) M.Hasegawa, K.Kaneko, T.Mizusaki Unique features of structure in an odd-proton N ≈ Z nucleus 69As NUCLEAR STRUCTURE 69As; calculated levels, J, π, configurations, deformation. Large-scale shell model approach, comparison with data.
doi: 10.1103/PhysRevC.72.064320
2005HO32 Eur.Phys.J. A 25, Supplement 1, 499 (2005) M.Honma, T.Otsuka, B.A.Brown, T.Mizusaki Shell-model description of neutron-rich pf-shell nuclei with a new effective interaction GXPF1 NUCLEAR STRUCTURE 42,44,46,48,50,52,54,56,58Ca, 44,46,48,50,52,54,56,58,60Ti, 48,50,52,54,56,58,60,62Cr; calculated 2+ excited states energies, single-particle level energies. 53,54,55,56Ti; calculated levels, J, π. Shell model, modified effective interaction, comparisons with data.
doi: 10.1140/epjad/i2005-06-032-2
2005KA04 Phys.Rev. C 71, 014319 (2005) K.Kaneko, R.F.Casten, M.Hasegawa, T.Mizusaki, J.-y.Zhang, E.A.McCutchan, N.V.Zamfir, R.Krucken Anomalous behavior of the first excited 0+ state in N ≈ Z nuclei NUCLEAR STRUCTURE Ne, Mg, Ti, Cr, Fe; analyzed excited states energies; deduced role of proton-neutron correlations in anomalous behavior.
doi: 10.1103/PhysRevC.71.014319
2005SI28 J.Phys.(London) G31, S1577 (2005) M.A.G.Silveira, N.H.Medina, J.A.Alcantara-Nunez, E.W.Cybulska, H.Dias, J.R.B.Oliveira, M.N.Rao, R.V.Ribas, W.A.Seale, K.T.Wiedemann, B.A.Brown, M.Honma, T.Mizusaki, T.Otsuka Nuclear structure of the odd-odd nucleus 58Co NUCLEAR REACTIONS 51V(10B, 2np), E=33, 36 MeV; measured Eγ, Iγ, γγ-coin, DSA. 58Co deduced levels, J, π, T1/2, B(M1). Comparison with shell model predictions.
doi: 10.1088/0954-3899/31/10/036
2004HA15 Phys.Rev. C 69, 034324 (2004) M.Hasegawa, K.Kaneko, T.Mizusaki, S.Tazaki Different particle alignments in N ≈ Z Ru isotopes studied by the shell model NUCLEAR STRUCTURE 88,89,90,91,92,93,94Ru; calculated levels, J, π, B(E2), rotational bands features. Shell model, pairing-plus-quadrupole-quadrupole interaction. Comparison with data.
doi: 10.1103/PhysRevC.69.034324
2004HA43 Phys.Rev. C 70, 031301 (2004) M.Hasegawa, K.Kaneko, T.Mizusaki Proton-neutron alignment in the yrast states of 66Ge and 68Ge NUCLEAR STRUCTURE 66,68Ge; calculated levels, J, π, rotational bands, particle alignment features. Comparison with data.
doi: 10.1103/PhysRevC.70.031301
2004HO08 Phys.Rev. C 69, 034335 (2004) M.Honma, T.Otsuka, B.A.Brown, T.Mizusaki New effective interaction for pf-shell nuclei and its implications for the stability of the N = Z = 28 closed core NUCLEAR STRUCTURE 53Mn, 54Fe, 54,55Co, 56,57,58,59Ni, 58Cu; calculated levels, J, π, B(M1), B(E2). Shell model, new effective interaction, comparison with data. NUCLEAR MOMENTS 47,49Ca, 47Sc, 47,48,49,50Ti, 48,49,50,51V, 49,50,51,52,53,54Cr, 51,52,53,54,55,56Mn, 53,54,55,56,57,58,59Fe, 55,56,57,58,59,60Co, 57,58,59,60,61,62,63,64,65,67Ni, 60,61,62,63,64,65,66Cu, 62,63,64,65,66,67,68,70Zn, 66,67,68,69,71Ga, 69,70,71,72Ge; calculated μ, quadrupole moments. Comparison with data.
doi: 10.1103/PhysRevC.69.034335
2004KA57 Phys.Rev. C 70, 051301 (2004) K.Kaneko, M.Hasegawa, T.Mizusaki Shape transition and oblate-prolate coexistence in N=Z fpg-shell nuclei NUCLEAR STRUCTURE 60Zn, 64Ge, 68Se, 72Kr; calculated levels, J, π, quadrupole moments, configurations, potential energy surfaces, shape coexistence features. Shell-model and constrained Hartree-Fock model calculations, comparison with data.
doi: 10.1103/PhysRevC.70.051301
2004LI12 Phys.Rev.Lett. 92, 072502 (2004) S.N.Liddick, P.F.Mantica, R.V.F.Janssens, R.Broda, B.A.Brown, M.P.Carpenter, B.Fornal, M.Honma, T.Mizusaki, A.C.Morton, W.F.Mueller, T.Otsuka, J.Pavan, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking Lowest Excitations in 56Ti and the Predicted N = 34 Shell Closure RADIOACTIVITY 56Sc(β-) [from 9Be(86Kr, X)]; measured β-delayed Eγ, Iγ, βγ-coin. 56Ti deduced levels, J, π, configurations, shell closure features. Mass-separated source. Comparison with shell model predictions.
doi: 10.1103/PhysRevLett.92.072502
2004LI75 Phys.Rev. C 70, 064303 (2004) S.N.Liddick, P.F.Mantica, R.Broda, B.A.Brown, M.P.Carpenter, A.D.Davies, B.Fornal, T.Glasmacher, D.E.Groh, M.Honma, M.Horoi, R.V.F.Janssens, T.Mizusaki, D.J.Morrissey, A.C.Morton, W.F.Mueller, T.Otsuka, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking Development of shell closures at N = 32, 34. I. β decay of neutron-rich Sc isotopes RADIOACTIVITY 54,55,56Sc(β-) [from Be(86Kr, X)]; measured Eβ, Eγ, βγ-coin, T1/2. 54,55,56Ti deduced levels, J, π, configurations. Comparison with model predictions.
doi: 10.1103/PhysRevC.70.064303
2004MI44 Phys.Rev. C 70, 044316 (2004) Extrapolation method in shell model calculations with a deformed basis NUCLEAR STRUCTURE 48Cr, 60Zn; calculated level energies, effects of extrapolation method.
doi: 10.1103/PhysRevC.70.044316
2004SH46 Phys.Rev. C 70, 054313 (2004); Erratum Phys.Rev. C 74, 059903 (2006) N.Shimizu, T.Otsuka, T.Mizusaki, M.Honma Anomalous properties of quadrupole collective states in 136Te and beyond NUCLEAR STRUCTURE 134,136,138,140Te, 134,136,138Sn; calculated level energies, B(E2), quadrupole matrix elements, g factors. 136Te levels calculated quadrupole moments, μ. Monte Carlo shell model.
doi: 10.1103/PhysRevC.70.054313
2004UT03 Phys.Rev. C 70, 044307 (2004) Y.Utsuno, T.Otsuka, T.Glasmacher, T.Mizusaki, M.Honma Onset of intruder ground state in exotic Na isotopes and evolution of the N = 20 shell gap NUCLEAR STRUCTURE 27,28,29,30,31Na; analyzed quadrupole moments, μ, two-neutron separation energies, excited levels J, configurations; deduced onset of intruder ground state. Monte Carlo shell model approach.
doi: 10.1103/PhysRevC.70.044307
2004YU07 Phys.Rev. C 70, 034301 (2004) K.L.Yurkewicz, D.Bazin, B.A.Brown, C.M.Campbell, J.A.Church, D.-C.Dinca, A.Gade, T.Glasmacher, M.Honma, T.Mizusaki, W.F.Mueller, H.Olliver, T.Otsuka, L.A.Riley, J.R.Terry Intermediate-energy Coulomb excitation of 52Fe NUCLEAR REACTIONS 197Au(52Fe, 52Fe'), E=56.9 MeV/nucleon; measured σ(θ), Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 52Fe transition deduced B(E2). Comparisons with neighboring nuclides.
doi: 10.1103/PhysRevC.70.034301
2004YU10 Phys.Rev. C 70, 054319 (2004) K.L.Yurkewicz, D.Bazin, B.A.Brown, C.M.Campbell, J.A.Church, D.C.Dinca, A.Gade, T.Glasmacher, M.Honma, T.Mizusaki, W.F.Mueller, H.Olliver, T.Otsuka, L.A.Riley, J.R.Terry Nuclear structure in the vicinity of N=Z=28 56Ni NUCLEAR REACTIONS 197Au(58Ni, 58Ni'), E=77.8 MeV/nucleon; 197Au(56Ni, 56Ni'), E=85.8 MeV/nucleon; 197Au(54Ni, 54Ni'), E=70.3 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 54,56,58Ni levels deduced excitation B(E2). Comparison with model predictions.
doi: 10.1103/PhysRevC.70.054319
2004YU11 Phys.Rev. C 70, 064321 (2004) K.L.Yurkewicz, D.Bazin, B.A.Brown, C.M.Campbell, J.A.Church, D.-C.Dinca, A.Gade, T.Glasmacher, M.Honma, T.Mizusaki, W.F.Mueller, H.Olliver, T.Otsuka, L.A.Riley, J.R.Terry E2 excitation strength in 55Ni: Coupling of the 56Ni 2+1 collective core vibration to the f7/2 odd neutron hole NUCLEAR REACTIONS 197Au(55Ni, 55Ni'), E=84.8 MeV; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 55Ni deduced level, transition B(E2). Comparison with model predictions.
doi: 10.1103/PhysRevC.70.064321
2003LI38 Phys.Rev. C 68, 034316 (2003) A.F.Lisetskiy, N.Pietralla, M.Honma, A.Schmidt, I.Schneider, A.Gade, P.von Brentano, T.Otsuka, T.Mizusaki, B.A.Brown Experimental evidence for 56Ni-core breaking from the low-spin structure of the N = Z nucleus 5829Cu29 NUCLEAR REACTIONS 58Ni(p, nγ), E=14 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 58Cu deduced levels, J, π, δ, B(E2), B(M1), analog states features. Comparison with model predictions.
doi: 10.1103/PhysRevC.68.034316
2003MI07 Phys.Rev. C 67, 041301 (2003) Precise estimation of shell model energy by second-order extrapolation method NUCLEAR STRUCTURE 48,49Cr; calculated ground-state energies. 64Zn; calculated level energy, transition B(E2). Truncated spaces, second-order extrapolation method, comparison with exact results.
doi: 10.1103/PhysRevC.67.041301
2002HO08 Phys.Rev. C65, 061301 (2002) M.Honma, T.Otsuka, B.A.Brown, T.Mizusaki Effective Interaction for pf-Shell Nuclei NUCLEAR STRUCTURE Ca, Ti, Cr, Fe, Ni; calculated 2+ energy levels, single-particle energies. 56,57,58,59,61,63,65Ni; calculated levels, J, π. Unified effective interaction, comparisons with data.
doi: 10.1103/PhysRevC.65.061301
2002HO12 Nucl.Phys. A704, 134c (2002) M.Honma, B.A.Brown, T.Mizusaki, T.Otsuka Full pf-Shell Calculations with a New Effective Interaction NUCLEAR STRUCTURE Z=20-32; calculated binding energies. 56Ni; calculated single-particle energies. 48Ca, 50Ti, 52Cr, 54Fe, 56,58,60,62,64,66Ni; calculated level energies, B(E2), quadrupole moments. Shell model, comparison with data.
doi: 10.1016/S0375-9474(02)00774-1
2002JA16 Phys.Lett. 546B, 55 (2002) R.V.F.Janssens, B.Fornal, P.F.Mantica, B.A.Brown, R.Broda, P.Bhattacharyya, M.P.Carpenter, M.Cinausero, P.J.Daly, A.D.Davies, T.Glasmacher, Z.W.Grabowski, D.E.Groh, M.Honma, F.G.Kondev, W.Krolas, T.Lauritsen, S.N.Liddick, S.Lunardi, N.Marginean, T.Mizusaki, D.J.Morrissey, A.C.Morton, W.F.Mueller, T.Otsuka, T.Pawlat, D.Seweryniak, H.Schatz, A.Stolz, S.L.Tabor, C.A.Ur, G.Viesti, I.Wiedenhover, J.Wrzesinski Structure of 52, 54Ti and shell closures in neutron-rich nuclei above 48Ca RADIOACTIVITY 54Sc(β-) [from 9Be(86Kr, X)]; measured Eγ, Iγ, βγ-coin, T1/2. 54Ti deduced levels, possible J, π, shell features. Mass separator, comparisons with model predictions. NUCLEAR REACTIONS 208Pb(48Ca, X)50Ti/51Ti/52Ti/53Ti/54Ti/196Hg, E=305 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin following deep-inelastic reactions. 52,54Ti deduced levels, J, π, configurations, shell features. Gammasphere array, comparison with model predictions.
doi: 10.1016/S0370-2693(02)02682-5
2002KA60 Phys.Rev. C 66, 051306 (2002) K.Kaneko, M.Hasegawa, T.Mizusaki Quadrupole and octupole softness in the N=Z nucleus 64Ge NUCLEAR STRUCTURE 64Ge; calculated levels, J, π, quadrupole and octupole correlations. Shell model.
doi: 10.1103/PhysRevC.66.051306
2002MI23 Phys.Rev. C65, 064319 (2002) Extrapolation Method for Shell Model Calculations NUCLEAR STRUCTURE 48Cr, 54Fe, 56Ni; calculated shell-model energy. 48Cr; calculated quadrupole moments, B(E2). Extrapolation method.
doi: 10.1103/PhysRevC.65.064319
2002MI26 Nucl.Phys. A704, 190c (2002) T.Mizusaki, T.Otsuka, M.Honma, B.A.Brown Normal and Superdeformation in 56Ni NUCLEAR STRUCTURE 56Ni, 58Cu, 64Ge; calculated levels, J, π, rotational bands, shape coexistance features.
doi: 10.1016/S0375-9474(02)00779-0
2002OS07 Phys.Lett. 546B, 48 (2002) A.Osa, T.Czosnyka, Y.Utsuno, T.Mizusaki, Y.Toh, M.Oshima, M.Koizumi, Y.Hatsukawa, J.Katakura, T.Hayakawa, M.Matsuda, T.Shizuma, M.Sugawara, T.Morikawa, H.Kusakari First measurement of the quadrupole moment in the 2+1 state of 84Kr NUCLEAR REACTIONS 98Mo, Ta(84Kr, 84Kr'), E=250 MeV; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 84Kr level deduced quadrupole moment, B(E2). Comparisons with large-scale shell model predictions.
doi: 10.1016/S0370-2693(02)02660-6
2002OT01 Eur.Phys.J. A 13, 69 (2002) T.Otsuka, Y.Utsuno, R.Fujimoto, B.A.Brown, M.Honma, T.Mizusaki Frontiers and Challenges of the Nuclear Shell Model NUCLEAR STRUCTURE Z=8-20; calculated levels, shell features far from stability. Monte Carlo shell model.
doi: 10.1007/s10050-002-8721-5
2002OT03 Eur.Phys.J. A 15, 151 (2002) T.Otsuka, Y.Utsuno, R.Fujimoto, B.A.Brown, M.Honma, T.Mizusaki Frontiers and challenges of nuclear shell model
doi: 10.1140/epja/i2001-10244-6
2002SH27 Nucl.Phys. A704, 244c (2002) N.Shimizu, T.Otsuka, T.Mizusaki, M.Honma Collective Excitations of Nuclei in the Monte-Carlo Shell Model NUCLEAR STRUCTURE 138,140,142,144,146,148,150Ba; calculated levels, J, π, B(E2). 132Xe; calculated levels, J, π, B(E2), triaxial deformation. Monte Carlo shell model.
doi: 10.1016/S0375-9474(02)00784-4
2002UT01 Nucl.Phys. A704, 50c (2002) Y.Utsuno, T.Otsuka, T.Mizusaki, M.Honma Monte Carlo Shell Model Calculation for Unstable Nuclei Around N = 20 NUCLEAR STRUCTURE O, Ne, Mg, Si; calculated two-neutron separation energies, level energies for neutron-rich nuclides. 31Na, 34Si; calculated levels, J, π. Monte Carlo shell model.
doi: 10.1016/S0375-9474(02)00765-0
2002UT02 Prog.Theor.Phys.(Kyoto), Suppl. 146, 488 (2002) Y.Utsuno, T.Otsuka, T.Mizusaki, M.Honma Electromagnetic Moments of Exotic Na Isotopes and Their Relation to the N = 20 Shell Gap NUCLEAR STRUCTURE 27,28,29,30,31Na; calculated μ, quadrupole moments, configurations; deduced role of shell gap. Monte Carlo shell model, comparison with data.
doi: 10.1143/PTPS.146.488
2001MI11 Phys.Rev. C63, 044306 (2001) T.Mizusaki, T.Otsuka, M.Honma, B.A.Brown Spherical-Deformed Shape Coexistence for the pf Shell in the Nuclear Shell Model NUCLEAR STRUCTURE 48Ca, 50Ti, 52Cr, 54Fe, 56Ni; calculated levels, J, π, deformation, shape coexistence features. Shell model, several methods compared.
doi: 10.1103/PhysRevC.63.044306
2001OT01 Nucl.Phys. A682, 155c (2001) T.Otsuka, Y.Utsuno, T.Mizusaki, M.Honma Shell Model Results for Neutron-Rich Nuclei NUCLEAR STRUCTURE 26,28,30,32,34Ne, 28,30,32,34,36Mg; calculated level energies, transitions B(E2), g factors. Monte Carlo shell model.
doi: 10.1016/S0375-9474(00)00634-5
2001OT02 Nucl.Phys. A685, 100c (2001) T.Otsuka, Y.Utsuno, T.Mizusaki, M.Honma Exotic Nuclei in the Monte Carlo Shell Model Calculations NUCLEAR STRUCTURE 56Ni; calculated levels, J, π, rotational bands. 26,28,30,32,34Ne, 28,30,32,34,36Mg; calculated level energies, B(E2). Monte Carlo shell model, comparisons with data.
doi: 10.1016/S0375-9474(01)00532-2
2001OT03 Prog.Part.Nucl.Phys. 46, 155 (2001) T.Otsuka, Y.Utsuno, M.Honma, T.Mizusaki Structure of Unstable Nuclei NUCLEAR STRUCTURE 48Cr, 56Ni, 26,28,30,32,34Ne, 28,30,32,34,36,38Mg; calculated levels, J, π. Monte Carlo shell model, comparison with data.
doi: 10.1016/S0146-6410(01)00119-3
2001OT04 Phys.Rev.Lett. 87, 082502 (2001) T.Otsuka, R.Fujimoto, Y.Utsuno, B.A.Brown, M.Honma, T.Mizusaki Magic Numbers in Exotic Nuclei and Spin-Isospin Properties of the NN Interaction NUCLEAR STRUCTURE 24O, 30Si; calculated effective single-particle energy levels. 9He, 11Be, 13C; calculated levels, J, π. 24O, 26Ne, 28Mg, 30Si, 32S, 34Ar, 36Ca; calculated effective shell gap. Shell-model magic numbers in exotic nuclides, role of spin-isospin contribution discussed.
doi: 10.1103/PhysRevLett.87.082502
2001OT06 Prog.Part.Nucl.Phys. 47, 319 (2001) T.Otsuka, M.Honma, T.Mizusaki, N.Shimizu, Y.Utsuno Monte Carlo Shell Model for Atomic Nuclei
doi: 10.1016/S0146-6410(01)00157-0
2001SH06 Phys.Rev.Lett. 86, 1171 (2001) N.Shimizu, T.Otsuka, T.Mizusaki, M.Honma Transition from Spherical to Deformed Shapes of Nuclei in the Monte Carlo Shell Model NUCLEAR STRUCTURE 138,140,142,144,146,148,150Ba; calculated energy levels, transitions B(E2), deformation features. Monte Carlo shell model.
doi: 10.1103/PhysRevLett.86.1171
2001UT02 Phys.Rev. C64, 011301 (2001) Y.Utsuno, T.Otsuka, T.Mizusaki, M.Honma Extreme Location of F Drip Line and Disappearance of the N = 20 Magic Structure NUCLEAR STRUCTURE 25Mg, 31Na, 34Si; calculated levels, J, π. 29F, 30Ne, 31Na, 32Mg, 33Al, 34Si; calculated two-neutron separation energies. Monte Carlo shell model, comparisons with data and other calculations.
doi: 10.1103/PhysRevC.64.011301
2000MI25 Phys.Scr. T88, 107 (2000) T.Mizusaki, T.Otsuka, M.Honma, B.A.Brown Doubly-Deformed Bands in Doubly-Magic 56Ni NUCLEAR STRUCTURE 56Ni; calculated levels, J, π, potential energy surfaces, configurations. Monte Carlo shell model.
doi: 10.1238/Physica.Topical.088a00107
2000OT01 Prog.Theor.Phys.(Kyoto), Suppl. 138, 24 (2000) T.Otsuka, N.Shimizu, S.Haruyama, M.Honma, T.Mizusaki, A.Taketani, Y.Utsuno, Y.Watanabe Monte Carlo Shell Model Calculations for Atomic Nuclei and Their Parallel Computing NUCLEAR STRUCTURE 48Cr; calculated levels, J, π. Quantum Monte Carlo diagonalization method.
doi: 10.1143/PTPS.138.24
2000SM11 Nucl.Phys. A678, 235 (2000) N.A.Smirnova, N.Pietralla, T.Mizusaki, P.Van Isacker Interrelation between the Isoscalar Octupole Phonon and the Proton-Neutron Mixed-Symmetry Quadrupole Phonon in Near-Spherical Nuclei
doi: 10.1016/S0375-9474(00)00331-6
2000WA24 Prog.Theor.Phys.(Kyoto), Suppl. 138, 43 (2000) Y.Watanabe, N.Shimizu, S.Haruyama, M.Honma, T.Mizusaki, A.Taketani, Y.Utsuno, T.Otsuka A Workstation Farm Optimized for Monte Carlo Shell Model Calculations: Alphleet
doi: 10.1143/PTPS.138.43
1999HA40 Phys.Rev.Lett. 83, 1922 (1999) Backbending Mechanism of 48Cr NUCLEAR STRUCTURE 48Cr; calculated rotational bands transition energies, B(E2); deduced backbending mechanism. Projected shell model, generator coordinate methods.
doi: 10.1103/PhysRevLett.83.1922
1999MI07 Phys.Rev. C59, R1846 (1999) T.Mizusaki, T.Otsuka, Y.Utsuno, M.Honma, T.Sebe Shape Coexistence in Doubly-Magic 56Ni by the Monte Carlo Shell Model NUCLEAR STRUCTURE 56Ni; calculated levels, J, π, B(E2). Monte Carlo shell model.
doi: 10.1103/PhysRevC.59.R1846
1999OT01 J.Phys.(London) G25, 699 (1999) Monte Carlo Shell-Model Calculations NUCLEAR STRUCTURE 48Cr, 64Ge, 56Ni; calculated levels, J, π. Quantum Monte Carlo diagonalization method, several two-body interactions compared.
doi: 10.1088/0954-3899/25/4/023
1999UT02 Phys.Rev. C60, 054315 (1999) Y.Utsuno, T.Otsuka, T.Mizusaki, M.Honma Varying Shell Gap and Deformation in N ∼ 20 Unstable Nuclei Studied by the Monte Carlo Shell Model NUCLEAR STRUCTURE 28Ne, 32Mg, 34Si; calculated potential energy surfaces. O, Ne, Mg, Si; calculated two-neutron separation energies, level energies, B(E2), related features; deduced shell gap, deformation roles. Shell model Monte Carlo approach.
doi: 10.1103/PhysRevC.60.054315
1998OT01 Phys.Rev.Lett. 81, 1588 (1998) Structure of the N = Z = 28 Closed Shell Studied by Monte Carlo Shell Model Calculation NUCLEAR STRUCTURE 56Ni; calculated levels, J, π, doubly closed shell configuration probability. Quantum Monte Carlo approach.
doi: 10.1103/PhysRevLett.81.1588
1998PI01 Phys.Rev. C57, 150 (1998) N.Pietralla, T.Mizusaki, P.von Brentano, R.V.Jolos, T.Otsuka, V.Werner 21+ and 22+ States in Collective Nuclei as Multiple Q-Phonon Excitations
doi: 10.1103/PhysRevC.57.150
1997MI14 Acta Phys.Pol. B28, 91 (1997) Quantum Monte Carlo Diagonalization Method for Realistic Shell Model Calculations NUCLEAR STRUCTURE 48Cr, 54Fe; calculated levels vs basis dimension. Quantum Monte Carlo Diagonalization method.
1996HO20 Phys.Rev.Lett. 77, 3315 (1996) Nuclear Shell Model by the Quantum Monte Carlo Diagonalization Method NUCLEAR STRUCTURE 24Mg, 64Ge; calculated levels, E2 properties. Shell model, quantum Monte Carlo diagonalization method.
doi: 10.1103/PhysRevLett.77.3315
1996KI08 Nucl.Phys. A604, 163 (1996) K.-H.Kim, A.Gelberg, T.Mizusaki, T.Otsuka, P.von Brentano IBM-2 Calculations of Even-Even Pd Nuclei NUCLEAR STRUCTURE 102,104,106,108,110,112,118,120,122,124,126Pd; calculated levels, B(λ). Proton-neutron interacting boson model.
doi: 10.1016/0375-9474(96)00128-5
1996MI02 Nucl.Phys. A598, 47 (1996) T.Mizusaki, T.Otsuka, P.von Brentano IBM Approach to the Rotational Damping
doi: 10.1016/0375-9474(95)00493-9
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