NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = T.Abe Found 19 matches. 2024KO04 Phys.Rev. C 109, L031301 (2024) S.Koyama, D.Suzuki, M.Assie, L.Lalanne, O.Sorlin, T.Abe, D.Beaumel, Y.Blumenfeld, L.Caceres, F.De Oliveira Santos, F.Delaunay, F.Flavigny, S.Franchoo, J.Gibelin, V.Girard-Alcindor, J.Guillot, F.Hammache, O.Kamalou, A.Kamenyero, N.Kitamura, V.Lapoux, A.Lemasson, A.Matta, B.Mauss, P.Morfouace, M.Niikura, H.Otsu, J.Pancin, T.Roger, T.Y.Saito, H.Sakurai, C.Stodel, J-C.Thomas Mirror symmetry at far edges of stability: The cases of 8C and 8He
doi: 10.1103/PhysRevC.109.L031301
2023IS02 Phys.Rev. C 107, 024306 (2023) Y.Ishibashi, A.Gladkov, Y.Ichikawa, A.Takamine, H.Nishibata, T.Sato, H.Yamazaki, T.Abe, J.M.Daugas, T.Egami, T.Fujita, G.Georgiev, K.Imamura, T.Kawaguchi, W.Kobayashi, Y.Nakamura, A.Ozawa, M.Sanjo, N.Shimizu, D.Tominaga, L.C.Tao, K.Asahi, H.Ueno Nuclear magnetic moment of the neutron-rich nucleus 21O NUCLEAR MOMENTS 21O; measured Iβ, b(θ), β-NMR spectra; deduced g-factor, J and π of the ground state as 5/2+ based on comparison to single-particle g-factors, configuration, magnetic moment for the 5/2+ ground state. Comparison to shell-model predictions using the USD, YSOX, and SDPF-M interactions and to random phase approximation (RPA) based calculations. Measured with β-ray detected nuclear magnetic resonance (β-NMR) spectroscopy. Spin-polarized 21O beam produced in 9Be(22Ne, X), E=70 MeV/nucleon reaction, followed by separation of 21O fragments using RIPS separator at RIKEN.
doi: 10.1103/PhysRevC.107.024306
2021AB03 Phys.Lett. B 815, 136174 (2021) Atomic form factors and inverse Primakoff scattering of axion
doi: 10.1016/j.physletb.2021.136174
2021AB10 Phys.Rev. C 104, 054315 (2021) T.Abe, P.Maris, T.Otsuka, N.Shimizu, Y.Utsuno, J.P.Vary Ground-state properties of light 4n self-conjugate nuclei in ab initio no-core Monte Carlo shell model calculations with nonlocal NN interactions NUCLEAR STRUCTURE 4He, 8Be, 12C, 16O, 20Ne; calculated ground-state energies and point-proton rms radii using ab initio no-core Monte Carlo shell model (MCSM), with the JISP16 and Daejeon16 nonlocal nucleon-nucleon interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.054315
2019MI17 Phys.Rev. C 100, 034310 (2019) T.Miyagi, T.Abe, M.Kohno, P.Navratil, R.Okamoto, T.Otsuka, N.Shimizu, S.R.Stroberg Ground-state properties of doubly magic nuclei from the unitary-model-operator approach with chiral two- and three-nucleon forces NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground-state energies, root-mean square (rms) radii, charge radii. Unitary-model-operator approach (UMOA), with similarity renormalization group (SRG) evolved nucleon-nucleon (NN) and three-nucleon (3N) interactions based on chiral effective field theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.034310
2019OT01 Phys.Rev.Lett. 123, 222502 (2019) T.Otsuka, Y.Tsunoda, T.Abe, N.Shimizu, P.Van Duppen Underlying Structure of Collective Bands and Self-Organization in Quantum Systems NUCLEAR STRUCTURE 154Sm, 166Er; calculated energy levels, J, π, spectroscopic electric quadrupole moments; deduced formation of collective bands.
doi: 10.1103/PhysRevLett.123.222502
2017MI18 Phys.Rev. C 96, 054312 (2017) T.Miyagi, T.Abe, R.Okamoto, T.Otsuka Introduction of the one-body correlation operator in the unitary-model-operator approach NUCLEAR STRUCTURE 4He; calculated ground-state energy, point-nucleon rms matter radii, total, one-body, two-body, and three-body energies, One-body density matrix using nucleon-nucleon (NN) interactions from Argonne (AV18) and chiral effective field theory (χEFT) up to the next-to-next-to-next leading order (N3LO), and Unitary-model-operator approach (UMOA) with one-body correlations, and diagonalization of unitary-transformed Hamiltonians in the 0p0h and 1p1h space.
doi: 10.1103/PhysRevC.96.054312
2016IW02 Phys.Rev.Lett. 116, 112502 (2016) Y.Iwata, N.Shimizu, T.Otsuka, Y.Utsuno, J.Menendez, M.Honma, T.Abe Large-Scale Shell-Model Analysis of the Neutrinoless ββ Decay of 48Ca RADIOACTIVITY 48Ca(2β-); calculated nuclear matrix element for the neutrinoless double-beta decay using large-scale shell-model calculations.
doi: 10.1103/PhysRevLett.116.112502
2015MI09 Prog.Theor.Exp.Phys. 2015, 041D01 (2015) T.Miyagi, T.Abe, Ry.Okamoto, T.Otsuka Ground-state energies and charge radii of 4He, 16O, 40Ca, and 56Ni in the unitary-model-operator approach NUCLEAR STRUCTURE 4He, 16O, 40Ca, 56Ni; calculated ground state energies, charge radii. Unitary-model-operator approach, comparison with experimental data.
doi: 10.1093/ptep/ptv042
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
2013YO06 J.Phys.:Conf.Ser. 445, 012038 (2013) T.Yoshida, N.Shimizu, T.Abe, T.Otsuka Density profiles in the intrinsic frame of light nuclei obtained from Monte Carlo shell model calculation NUCLEAR STRUCTURE 8,10Be; calculated wavefunctions, proton density profiles, radius using Monte Carlo shell model. 8Be deduced 2α-cluster.
doi: 10.1088/1742-6596/445/1/012038
2012AB14 Phys.Rev. C 86, 054301 (2012) T.Abe, P.Maris, T.Otsuka, N.Shimizu, Y.Utsuno, J.P.Vary Benchmarks of the full configuration interaction, Monte Carlo shell model, and no-core full configuration methods NUCLEAR STRUCTURE 4,6He, 6,7Li, 8Be, 10B, 12C, 16O; calculated levels, point-particle rms radii, electromagnetic moments using the full configuration interaction (FCI), Monte Carlo shell model (MCSM), and no core full configuration (NCFC) approaches using realistic JISP16 nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.86.054301
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
2009AB11 Phys.Rev. C 79, 054002 (2009) Lattice calculation of thermal properties of low-density neutron matter with pionless NN effective field theory
doi: 10.1103/PhysRevC.79.054002
2009AB12 Phys.Rev. C 79, 054003 (2009) From low-density neutron matter to the unitary limit
doi: 10.1103/PhysRevC.79.054003
2009NA21 Nucl.Technology 168, 519 (2009) Monte Carlo Calculations for the Shielding Design of Beam Injection and Extraction Areas at the 3-GeV Synchrotron in J-PARC
doi: 10.13182/NT09-A9236
2006KA36 Astrophys.J. 647, 692 (2006); Erratum Astrophys.J. 662, 779 (2007) T.Kamae, N.Karlsson, T.Mizuno, T.Abe, T.Koi Parameterization of γ, e±, and neutrino spectra produced by p-p interaction in astronomical environments NUCLEAR REACTIONS 1H(p, X), E=high; analyzed pion, γ, electron, neutrino spectra, yields; deduced parameters.
doi: 10.1086/505189
2005KA38 Astrophys.J. 620, 244 (2005) Diffractive interaction and scaling violation in pp → π0 interaction and GeV excess in Galactic diffuse gamma-ray spectrum of EGRET NUCLEAR REACTIONS 1H(p, π0X), E=high; calculated γ spectra in astrophysical environment.
doi: 10.1086/426935
2004AB14 Phys.Rev. C 70, 014315 (2004); Erratum Phys.Rev. C71, 059902 (2005) Mean field calculation of thermal properties of simple nucleon matter on a lattice
doi: 10.1103/PhysRevC.70.014315
Back to query form |