NSR Query Results
Output year order : Descending NSR database version of March 18, 2024. Search: Author = H.Toki Found 315 matches. Showing 1 to 100. [Next]2023TA08 Phys.Rev. C 107, 044304 (2023) H.Takemoto, T.Myo, H.Horiuchi, H.Toki, M.Isaka, M.Lyu, Q.Zhao, N.Wan Appearance of the Hoyle state and its breathing mode in 12C despite strong short-range repulsion of the nucleon-nucleon potential NUCLEAR STRUCTURE 8Be; calculated trajectories of the eigenstates of 0+ and 2+, energy and rms radius of the ground state. 12C; calculated levels, J, π, rms radii and energies of the monopole transition of the nine lowest eigenstates, monopole transition matrix elements, trajectories of the eigenstates of 0+. Calculations using 3α cluster model (Bloch–Brink wave function) using the AV4P potential, which has a strong repulsive core. Comparison to experimental data and other theoretical calculations.
doi: 10.1103/PhysRevC.107.044304
2022IS08 Phys.Rev. C 106, 044310 (2022) M.Isaka, Q.Zhao, T.Myo, M.Lyu, H.Toki, H.Horiuchi, H.Takemoto, N.Wan Role of spatially compact nucleon wave packets in an ab initio description of 3H within high-momentum antisymmetrized molecular dynamics NUCLEAR STRUCTURE 3H; calculated total energy, rms radii. Calculations describing the nucleon correlations by utilizing high-momentum antisymmetrized molecular dynamics (HM-AMD) with Argonne V8' potential. Comparison of the results with and without the spinparallel configuration. Comparison to other theoretical calculations.
doi: 10.1103/PhysRevC.106.044310
2022MY01 Phys.Rev. C 105, 014317 (2022) T.Myo, M.Lyu, H.Toki, H.Horiuchi, Q.Zhao, M.Isaka, H.Takemoto, N.Wan New many-body method using cluster expansion diagrams with tensor-optimized antisymmetrized molecular dynamics NUCLEAR STRUCTURE 3H, 4He; calculated total energy and Hamiltonian components of the kinetic energy, central force, and tensor force using a new variational method of tensor optimized antisymmetrized molecular dynamics (New-TOAMD) with AV6' potential. Comparison with other theoretical calculations such as TOAMD, Green's function Monte Carlo (GFMC) and Faddeev-Yakubovsky (FY).
doi: 10.1103/PhysRevC.105.014317
2022WA32 Phys.Rev. C 106, 034308 (2022) N.Wan, T.Myo, H.Takemoto, H.Toki, C.Xu, H.Horiuchi, M.Isaka, M.Lyu, Q.Zhao Finite particle-number description of symmetric nuclear matter with spin excitations of high-momentum pairs induced by the tensor force
doi: 10.1103/PhysRevC.106.034308
2021ZH34 Prog.Theor.Exp.Phys. 2021, 063D02 (2021) Q.Zhao, M.Isaka, T.Myo, M.Lyu, H.Toki, H.Horiuchi, H.Takemoto, N.Wan Role of the unitary correlation operator on high-momentum antisymmetrized molecular dynamics using the bare NN interaction for 3H and 4He NUCLEAR STRUCTURE 3H, 4He; calculated binding energies using high-momentum antisymmetrized molecular dynamics (HMAMD) by incorporating the short-range part of the unitary correlation operator method (UCOM) as the variational method.
doi: 10.1093/ptep/ptab058
2020LI20 Phys.Rev. C 101, 064307 (2020) S.Li, T.Myo, Q.Zhao, H.Toki, H.Horiuchi, C.Xu, J.Liu, M.Lyu, Z.Ren Evolution of clustering structure through the momentum distributions in 8-10B isotopes NUCLEAR STRUCTURE 8,9,10Be; calculated intrinsic and total nucleon momentum distributions of the α-α clusters, and components of the deformation parameter β using Brink type α-α and Tohsaki-Horiuchi-Schuck-Ropke wavefunctions.
doi: 10.1103/PhysRevC.101.064307
2020LY01 Phys.Lett. B 805, 135421 (2020) M.Lyu, T.Myo, H.Toki, H.Horiuchi, C.Xu, N.Wan High-momentum components in the 4He nucleus caused by inter-nucleoncorrelations NUCLEAR STRUCTURE 4He; calculated momentum distributions using two-kinds of the wave functions of TO-HMAMD and TOAMD, Probabilities of each orthogonal component of AMD, central, tensor, and many-body in the TO-HMAMD wave function, decomposition of the high momentum component of the 4He nucleus.
doi: 10.1016/j.physletb.2020.135421
2020WA32 Chin.Phys.C 44, 124104 (2020) N.Wan, T.Myo, C.Xu, H.Toki, H.Horiuchi, M.Lyu Finite particle number description of neutron matter using the unitary correlation operator and high-momentum pair method NUCLEAR STRUCTURE N=66; calculated the nuclear equation of state (EOS) using bare Argonne nucleon-nucleon (NN) interactions.
doi: 10.1088/1674-1137/abb4d1
2019MY01 Phys.Rev. C 99, 024312 (2019) T.Myo, H.Takemoto, M.Lyu, N.Wan, C.Xu, H.Toki, H.Horiuchi, T.Yamada, K.Ikeda Variational calculation of nuclear matter in a finite particle number approach using the unitary correlation operator and high-momentum pair methods NUCLEAR STRUCTURE A=28, 76, 108, 132, 228, 324, 0-1500; N=14, 38, 54, 66, 114, 162, 0-800; calculated numbers of 2p2h configurations, total, kinetic, and potential energy per particle in symmetric nuclear matter and neutron matter using the unitary correlation operator method for central correlations, and two-particle two-hole (2p2h) excitations involving a large relative and high-momentum pair (UCOM+HM). Comparison with Brueckner-Hartree-Fock and auxiliary field diffusion Monte Carlo calculations.
doi: 10.1103/PhysRevC.99.024312
2019YA19 Prog.Theor.Exp.Phys. 2019, 113D03 (2019) T.Yamada, T.Myo, H.Toki, H.Horiuchi, K.Ikeda A nuclear matter calculation with the tensor-optimized Fermi sphere method with central interaction
doi: 10.1093/ptep/ptz117
2019ZH14 Phys.Rev. C 99, 034311 (2019) Q.Zhao, M.Lyu, Z.Ren, T.Myo, H.Toki, K.Ikeda, H.Horiuchi, M.Isaka, T.Yamada Contact representation of short-range correlation in light nuclei studied by the high-momentum antisymmetrized molecular dynamics NUCLEAR STRUCTURE 3H; calculated total energy and Hamiltonian components of the total energy using high-momentum antisymmetrized molecular dynamics (HMAMD) with AV4' central potential; deduced a contact representation of high momentum components of short-range correlation between nucleons. Comparison with authors' previous theoretical approaches.
doi: 10.1103/PhysRevC.99.034311
2018LY08 Phys.Rev. C 98, 064002 (2018) M.Lyu, T.Myo, M.Isaka, H.Toki, K.Ikeda, H.Horiuchi, T.Suhara, T.Yamada Tensor-optimized high-momentum antisymmetrized molecular dynamics with a bare interaction, and its application to the 4He nucleus NUCLEAR STRUCTURE 3H, 4He; calculated nucleon-nucleon correlations, total energy, Hamiltonian components, rms radius of 4He, and energy convergence of 3H, and 4He using tensor-optimized high-momentum antisymmetrized molecular dynamics (TO-HMAMD) framework. Comparison with other AMD-based theoretical calculations.
doi: 10.1103/PhysRevC.98.064002
2017HU02 Phys.Rev. C 95, 025804 (2017) Neutron stars within a relativistic central variational method
doi: 10.1103/PhysRevC.95.025804
2017MY01 Phys.Rev. C 95, 044314 (2017) T.Myo, H.Toki, K.Ikeda, H.Horiuchi, T.Suhara Successive variational method of the tensor-optimized antisymmetrized molecular dynamics for central interaction in finite nuclei NUCLEAR STRUCTURE 3H, 4He; calculated energy surfaces and radii as function of range parameter, energies of 1/2+ g.s. in 3H and 0+ g.s. in 4He. New variational theory, tensor optimized antisymmetrized molecular dynamics (TOAMD), to describe nuclei from the nucleon-nucleon (NN) interaction, and nuclear clustering. Comparison of results with those from the unitary correlation operator method (UCOM).
doi: 10.1103/PhysRevC.95.044314
2017MY02 Prog.Theor.Exp.Phys. 2017, 073D01 (2017) T.Myo, H.Toki, K.Ikeda, H.Horiuchi, T.Suhara New successive variational method of tensor-optimized antisymmetrized molecular dynamics for nuclear many-body systems NUCLEAR STRUCTURE 3H, 4He; calculated total energy and the Hamiltonian components, short-range correlation and tensor functions, energy surface.
doi: 10.1093/ptep/ptx089
2017MY03 Phys.Rev. C 96, 034309 (2017) T.Myo, H.Toki, K.Ikeda, H.Horiuchi, T.Suhara Power series expansion method in tensor-optimized antisymmetrized molecular dynamics beyond the Jastrow correlation method NUCLEAR STRUCTURE 3H, 4He; calculated energies of 1/2+ state in 3H and 0+ in 4He using MT-V and AV6 potentials, Hamiltonian components using AV6 potential. New variational method for the tensor optimized antisymmetrized molecular dynamics (TOAMD), introducing correlation functions for the tensor force and short-range repulsion in strong interactions. Comparison with other theoretical approaches.
doi: 10.1103/PhysRevC.96.034309
2016TA07 Prog.Theor.Exp.Phys. 2016, 043D05 (2016) I.Tanihata, S.Terashima, R.Kanungo, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, R.Knoebel, J.Kurcewicz, Yu.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, H.Toki, J.Vargas, J.S.Winfield, H.Weick Observation of large enhancements of charge exchange cross sections with neutron-rich carbon isotopes NUCLEAR REACTIONS C, H(C, X)12N/13N/14N/15N/16N/17N/18N/19N, E∼950 MeV/nucleon; measured reaction products; deduced σ, Gamow-Teller and/or Fermi transition strengths.
doi: 10.1093/ptep/ptw034
2015MY01 Prog.Theor.Exp.Phys. 2015, 063D03 (2015) T.Myo, A.Umeya, H.Toki, K.Ikeda Structures in 9, 10Be and 10B studied with the tensor-optimized shell model NUCLEAR STRUCTURE 8,9,10Be, 10B; calculated excitation energies, J, π, rms radii, nucleon occupation numbers. Comparison with experimental data.
doi: 10.1093/ptep/ptv077
2015MY02 Prog.Theor.Exp.Phys. 2015, 073D02 (2015) T.Myo, H.Toki, K.Ikeda, H.Horiuchi, T.Suhara Tensor-optimized antisymmetrized molecular dynamics in nuclear physics
doi: 10.1093/ptep/ptv087
2014HU01 Prog.Theor.Exp.Phys. 2014, 013D02 (2014) Quark mean-field model for single and double Λ and Ξ hypernuclei NUCLEAR STRUCTURE 40Ca, 89Y, 208Pb; calculated hypernuclei single-particle, binding and bond energies.
doi: 10.1093/ptep/ptt119
2014HU03 Phys.Rev. C 89, 025802 (2014) Extended quark mean-field model for neutron stars
doi: 10.1103/PhysRevC.89.025802
2014HU13 Phys.Rev. C 90, 014309 (2014) Effective ΛN potential from relativistic Brueckner-Hartree-Fock theory NUCLEAR STRUCTURE 16O, 28Si, 40Ca, 51V, 89Y, 139La, 208Pb; calculated total and single binding energies of hypernuclei, effective ΛN potentials. Density-dependent relativistic mean-field (DDRMF) approach through the relativistic Brueckner-Hartree-Fock (RBHF) theory with Jul94 potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.014309
2014MY02 Prog.Theor.Exp.Phys. 2014, 033D01 (2014) T.Myo, A.Umeya, K.Horii, H.Toki, K.Ikeda Shell and alpha cluster structures in 8Be with tensor-optimized shell model NUCLEAR STRUCTURE 8Be; calculated occupation numbers, J, π, energy levels. Tensor-optimized shell model (TOSM).
doi: 10.1093/ptep/ptu012
2013IM01 Nucl.Phys. A913, 71 (2013) Quark-hadron matter at finite temperature and density in a two-color PNJL model
doi: 10.1016/j.nuclphysa.2013.06.001
2013ON02 Phys.Lett. B 725, 277 (2013) H.J.Ong, I.Tanihata, A.Tamii, T.Myo, K.Ogata, M.Fukuda, K.Hirota, K.Ikeda, D.Ishikawa, T.Kawabata, H.Matsubara, K.Matsuta, M.Mihara, T.Naito, D.Nishimura, Y.Ogawa, H.Okamura, A.Ozawa, D.Y.Pang, H.Sakaguchi, K.Sekiguchi, T.Suzuki, M.Taniguchi, M.Takashina, H.Toki, Y.Yasuda, M.Yosoi, J.Zenihiro Probing effect of tensor interactions in 16O via (p, d) reaction NUCLEAR REACTIONS 16O(p, d), E=198, 295, 392 MeV; measured reaction products; deduced σ(θ), tensor interaction in one-nucleon transfer reactions.
doi: 10.1016/j.physletb.2013.07.038
2013TO11 Phys.Rev. C 88, 015806 (2013) H.Toki, T.Suzuki, K.Nomoto, S.Jones, R.Hirschi Detailed β-transition rates for URCA nuclear pairs in 8-10 solar-mass stars RADIOACTIVITY 23Ne, 25Na, 27Mg(β-); 23Na, 25Mg, 27Al(EC); calculated β-transition rates for 23Ne - 23Na, 25Na - 25Mg, 27Mg - 27Al URCA nuclear pairs. Shell-model calculations in sd-orbital. Discussed impact on the evolution and cooling process in stars of 810 times the solar mass.
doi: 10.1103/PhysRevC.88.015806
2013UM01 Few-Body Systems 54, 99 (2013) A.Umeya, T.Myo, E.Hiyama, H.Toki, K.Ikeda s-Shell Λ-Hypernuclei Taking into Account ΛN - ΛN Coupling Explicitly with TOSM NUCLEAR STRUCTURE 4H, 5He; calculated hypernuclei energy levels, J, π, Λ separation energies. Comparison with available data.
doi: 10.1007/s00601-012-0336-z
2012HO13 Prog.Theor.Phys.(Kyoto) 127, 1019 (2012) K.Horii, H.Toki, T.Myo, K.Ikeda Tensor Optimized Few-Body Model for s-Shell Nuclei NUCLEAR STRUCTURE 2,3H, 4He; calculated correlation and wave functions; deduced deuteron-like configurations.
doi: 10.1143/PTP.127.1019
2012MY03 Phys.Rev. C 86, 024318 (2012) T.Myo, A.Umeya, H.Toki, K.Ikeda Tensor-optimized shell model for the Li isotopes with a bare nucleon-nucleon interaction NUCLEAR STRUCTURE 4,5,6,7,8He, 5,6,7,8,9Li; calculated levels, J, π, matter radius, energy components, configurations, occupation numbers. Tensor-optimized shell-model using AV8' interaction and unitary correlation operator method (TOSM+UCOM). The jj coupling character in the ground states of 7,8,9Li. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.024318
2012OG08 J.Phys.:Conf.Ser. 381, 012111 (2012) Extended Brueckner-Hartree-Fock theory with pionic correlation in finite nuclei
doi: 10.1088/1742-6596/381/1/012111
2012WA11 Prog.Theor.Phys.(Kyoto) 127, 739 (2012) Skyrme-Hartree-Fock plus Tensor Correction for Nuclear Matter
doi: 10.1143/PTP.127.739
2011MY02 Phys.Rev. C 84, 034315 (2011) T.Myo, A.Umeya, H.Toki, K.Ikeda Role of the tensor interaction in He isotopes with a tensor-optimized shell model NUCLEAR STRUCTURE 4,5,6,7,8He; calculated levels, J, π, configurations, matter radii, kinetic, central, tensor, and LS energy components in the configurations. Tensor-optimized shell model (TOSM) with AV8' interaction, unitary correlation operator method (UCOM). Comparison with experimental data.
doi: 10.1103/PhysRevC.84.034315
2011OG05 Nucl.Phys. A860, 22 (2011) Relativistic chiral mean field model for finite nuclei NUCLEAR STRUCTURE 12C, 16O; calculated mass excess, pion energy using RCMF (Relativistic Chiral Mean Field) with pionic correlations.
doi: 10.1016/j.nuclphysa.2011.04.015
2010HO08 Phys.Rev. C 81, 061602 (2010) K.Horii, M.Takashina, T.Furumoto, Y.Sakuragi, H.Toki Elastic scattering of 8B from 12C with internal three-cluster structure of 8B NUCLEAR REACTIONS 12C(8B, 8B), E=95 MeV; calculated σ, σ(θ) using adiabatic recoil and cluster folding calculations. 12C, 14N(7Be, 7Be), E=87 MeV; calculated σ(θ). Comparison with experimental data.
doi: 10.1103/PhysRevC.81.061602
2010HU10 Eur.Phys.J. A 43, 323 (2010) The role of the form factor and short-range correlation in the relativistic Hartree-Fock model for nuclear matter
doi: 10.1140/epja/i2010-10917-y
2010TO13 Int.J.Mod.Phys. E19, 2531 (2010) Tensor optimized shell model and hypernuclei NUCLEAR STRUCTURE 4He; calculated hypernuclear energy components. Tensor optimized shell model (TOSM).
doi: 10.1142/S0218301310017046
2010WE03 Prog.Theor.Phys.(Kyoto) 123, 811 (2010) Role of Form Factor in Relativistic Hartree-Fock Approach for Finite Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated binding energy per nucleon, single-particle energies. Relativistic Hartree-Fock (RHF) approach.
doi: 10.1143/PTP.123.811
2009HU02 Phys.Rev. C 79, 024305 (2009) J.Hu, Y.Ogawa, H.Toki, A.Hosaka, H.Shen Extended relativistic chiral mean field model for nuclear matter
doi: 10.1103/PhysRevC.79.024305
2009MY01 Prog.Theor.Phys.(Kyoto) 121, 511 (2009) Tensor-Optimized Shell Model with Bare Nucleon-Nucleon Interaction for 4He
doi: 10.1143/PTP.121.511
2009NO11 Prog.Theor.Phys.(Kyoto) 122, 1501 (2009) N.Nose-Togawa, H.Toki, A.Haga, S.Tamenaga Relativistic Description of Semi-Infinite Nuclear Matter with Vacuum Polarization
doi: 10.1143/PTP.122.1501
2009TO07 Int.J.Mod.Phys. E18, 2040 (2009) Tensor optimized shell model and the role of pion in finite nuclei NUCLEAR STRUCTURE 4He; calculated 4He wave functions, nuclear ground state.
doi: 10.1142/S0218301309014251
2008MY02 Prog.Theor.Phys.(Kyoto) 119, 561 (2008) T.Myo, Y.Kikuchi, K.Kato, H.Toki, K.Ikeda Systematic Study of 9, 10, 11Li with the Tensor and Pairing Correlations
doi: 10.1143/PTP.119.561
2008RA10 Nucl.Phys. A804, 219 (2008) A.Ramos, V.K.Magas, E.Oset, H.Toki The antikaon - nucleus interaction and alternative views to deeply bound antikaonic nuclear systems NUCLEAR REACTIONS 6,7Li, 9Be, 12,13C, 16O, 27Al, 51V(K-, p), E at rest; analyzed invariant mass spectra including final state interactions; deduced no evidence for deeply bound kaonic state.
doi: 10.1016/j.nuclphysa.2008.01.019
2008TA26 Nucl.Phys. A811, 306 (2008) S.Tamenaga, H.Toki, A.Haga, Y.Ogawa Spontaneous chiral symmetry breaking in the massless linear sigma model by fermion and boson loop corrections NUCLEAR STRUCTURE 16O; calculated baryon density using the (massless) chiral sigma models.
doi: 10.1016/j.nuclphysa.2008.07.015
2007GE08 Chin.Phys.Lett. 24, 1865 (2007) Reflection Asymmetric Relativistic Mean Field Approach and Its Application to the Octupole Deformed Nucleus 226Ra NUCLEAR STRUCTURE 226Ra; calculated binding energy, neutron and proton density distributions, deformation parameters using a reflection asymmetric relativistic mean field approach.
doi: 10.1088/0256-307X/24/7/021
2007HA14 Phys.Rev. C 75, 044315 (2007) Reanalysis of muonic 90Zr and 208Pb atoms ATOMIC PHYSICS 90Zr, 208Pb; analyzed muonic atoms transition energies, fine structure splitting.
doi: 10.1103/PhysRevC.75.044315
2007MY01 Prog.Theor.Phys.(Kyoto) 117, 257 (2007) T.Myo, S.Sugimoto, K.Kato, H.Toki, K.Ikeda Tensor Correlation in 4He with the Tensor-Optimized Shell Model NUCLEAR STRUCTURE 4He; calculated binding energy, radius, wave functions, role of tensor correlation. Tensor-optimized shell model.
doi: 10.1143/PTP.117.257
2007MY03 Nucl.Phys. A790, 311c (2007) T.Myo, K.Kato, H.Toki, K.Ikeda Properties of the tensor correlation in neutron halo nuclei NUCLEAR STRUCTURE 9,11Li; calculated binding energy, matter radius, configurations, role of pairing and Pauli blocking. Coupled 3-body calculations. Comparison with shell model calculations.
doi: 10.1016/j.nuclphysa.2007.03.056
2007MY04 Phys.Rev. C 76, 024305 (2007) T.Myo, K.Kato, H.Toki, K.Ikeda Roles of tensor and pairing correlations on halo formation in 11Li NUCLEAR STRUCTURE 11Li; calculated coulomb breakup cross section.
doi: 10.1103/PhysRevC.76.024305
2007OG03 Phys.Rev. C 76, 014305 (2007) Relativistic chiral mean-field model with parity and charge projection for finite nuclei NUCLEAR STRUCTURE A=12, 16, 28, 0, 56; calculated ground state properties using the CPPCMF chiral mean field model.
doi: 10.1103/PhysRevC.76.014305
2007OS01 Nucl.Phys. A782, 259c (2007) E.Oset, S.Sarkar, M.J.Vicente Vacas, M.Kaskulov, L.Roca, V.K.Magas, A.Ramos, H.Toki Recent developments in chiral dynamics of hadrons and hadrons in a nuclear medium
doi: 10.1016/j.nuclphysa.2006.10.026
2007RA06 Eur.Phys.J. A 31, 684 (2007) A.Ramos, V.K.Magas, E.Oset, H.Toki Conventional view versus FINUDA claims of a deeply bound K-pp state NUCLEAR REACTIONS 6,7Li, 9Be, 12,13C, 16O, 27Al, 51V(K-, pX), E at rest; calculated hyperon-proton invariant mass distributions, role of two-nucleon absorption process.
doi: 10.1140/epja/i2006-10264-8
2007SC23 Phys.Rev. C 75, 055203 (2007) O.Scholten, S.Tamenaga, H.Toki Loop corrections and the K-matrix formalism
doi: 10.1103/PhysRevC.75.055203
2007SU01 Phys.Rev. C 75, 014317 (2007) Study of the effect of the tensor correlation in oxygen isotopes with the charge- and parity-projected Hartree-Fock method NUCLEAR STRUCTURE 14,16,22,24,28O; calculated binding energies, radii, form factors, role of tensor correlation. Mean-field framework.
doi: 10.1103/PhysRevC.75.014317
2007SU16 Nucl.Phys. A789, 155 (2007) Study of the effect of the tensor correlation on the alpha-alpha interaction in 8Be with the charge- and parity-projected Hartree-Fock method NUCLEAR STRUCTURE 8Be; calculated binding energy using the charge and parity projected HF method and the effect of the tensor correlation on the α-α interaction in 8Be using the α cluster model.
doi: 10.1016/j.nuclphysa.2007.04.004
2007SU24 Phys.Rev. C 76, 054310 (2007) Effect of the tensor force in the exchange channel on the spin-orbit splitting in 23F in the Hartree-Fock framework NUCLEAR STRUCTURE 15,16,17,22O, 23F; calculated kinetic and potential energies, charge and matter radii. 23F; calculated ls-splitting.
doi: 10.1103/PhysRevC.76.054310
2007TO12 Prog.Part.Nucl.Phys. 59, 209 (2007) H.Toki, Y.Ogawa, S.Tamenaga, A.Haga Relativistic chiral mean field model for finite nuclei
doi: 10.1016/j.ppnp.2006.12.011
2006BA82 Nucl.Phys. A774, 769 (2006) S.Banerjee, A.Bhattacharyya, S.K.Ghosh, E.-M.Ilgenfritz, S.Raha, B.Sinha, E.Takasugi, H.Toki Colour entangled orphan quarks and dark energy from cosmic QCD phase transition
doi: 10.1016/j.nuclphysa.2006.06.133
2006GE03 J.Phys.(London) G32, 573 (2006) The stability and the shape of the heaviest nuclei NUCLEAR STRUCTURE Z=101-120; calculated binding energies, deformation parameters. Relativistic mean-field model, comparison with other models.
doi: 10.1088/0954-3899/32/4/013
2006GE07 Chin.Phys.Lett. 23, 1139 (2006) L.-S.Geng, J.Meng, H.Toki, W.-H.Long, G.Shen Spurious Shell Closures in the Relativistic Mean Field Model NUCLEAR STRUCTURE 132Sn, 140Ce, 208Pb, 218U; analyzed binding energies, related data; deduced spurious shell closures in relativistic mean field model.
doi: 10.1088/0256-307X/23/5/021
2006HI05 Few-Body Systems 38, 91 (2006) E.Hiyama, M.Kamimura, A.Hosaka, H.Toki, M.Yahiro Five-Body Calculation of Resonance and Scattering States of the uudd(s-bar) System
doi: 10.1007/s00601-005-0143-x
2006MA53 Phys.Rev. C 74, 025206 (2006) V.K.Magas, E.Oset, A.Ramos, H.Toki Critical view on the deeply bound K-pp system NUCLEAR REACTIONS 6,7Li, 12C(K-, pX), E at rest; analyzed proton-hyperon invariant mass spectra; deduced deeply bound kaonic states features.
doi: 10.1103/PhysRevC.74.025206
2006ME11 Prog.Part.Nucl.Phys. 57, 470 (2006) J.Meng, H.Toki, S.G.Zhou, S.Q.Zhang, W.H.Long, L.S.Geng Relativistic continuum Hartree Bogoliubov theory for ground-state properties of exotic nuclei
doi: 10.1016/j.ppnp.2005.06.001
2006OG02 Phys.Rev. C 73, 034301 (2006) Y.Ogawa, H.Toki, S.Tamenaga, S.Sugimoto, K.Ikeda Charge and parity projected relativistic mean field model with pion for finite nuclei NUCLEAR STRUCTURE 4He; calculated ground-state energy, matter density distribution, dependence on meson-nucleon potential. Charge and parity projected relativistic mean field model.
doi: 10.1103/PhysRevC.73.034301
2006OS04 Phys.Rev. C 74, 015207 (2006) Critical analysis on deeply bound kaonic states in nuclei
doi: 10.1103/PhysRevC.74.015207
2006SH04 Prog.Theor.Phys.(Kyoto) 115, 325 (2006) Double-Λ Hypernuclei in the Relativistic Mean-Field Theory NUCLEAR STRUCTURE 9Be, 12,13C, 16O, 28Si, 40Ca, 51V, 89Y, 139La, 208Pb; calculated hyperon binding energies for single-Λ hypernuclei. 6He, 10Be, 13B, 18O, 42Ca, 92Zr, 210Pb; calculated binding energies for two-Λ hypernuclei. 4,5,6He, 16,17,18O, 40,41,42Ca, 208,209,210Pb; calculated binding energies and radii for normal nuclei and one- and two-Λ hypernuclei. Relativistic mean-field theory.
doi: 10.1143/PTP.115.325
2005BO41 Part. and Nucl., Lett. 128, 9 (2005) S.G.Bondarenko, V.V.Burov, N.Hamamoto, A.Hosaka, Y.Manabe, H.Toki One- and two-rank separable kernels of the two-nucleon system in the Bethe-Salpeter approach
2005BO42 Part. and Nucl., Lett. 128, 17 (2005) S.G.Bondarenko, V.V.Burov, N.Hamamoto, A.Hosaka, Y.Manabe, H.Toki Elastic eD scattering in the Bethe-Salpeter approach for the deuteron with the positive- and negative-energy states NUCLEAR REACTIONS 2H(e, e), E not given; analyzed form factors, tensor polarization vs momentum transfer. Bethe-Salpeter approach.
2005GE04 Prog.Theor.Phys.(Kyoto) 113, 785 (2005) Masses, Deformations and Charge Radii -- Nuclear Ground-State Properties in the Relativistic Mean Field Model NUCLEAR STRUCTURE Z=8-100; calculated binding energies, radii, deformations. Relativistic mean field model.
doi: 10.1143/PTP.113.785
2005HA02 Nucl.Phys. B(Proc.Supp.) S139, 234 (2005) A.Haga, Y.Horikawa, Y.Tanaka, H.Toki Relativistic and nonrelativistic descriptions of nuclear polarization in electronic and muonic atoms ATOMIC PHYSICS, Mesic-atoms 208Pb; calculated polarization energy shifts for muonic and electronic atoms.
doi: 10.1016/j.nuclphysbps.2004.11.228
2005HA29 Nucl.Instrum.Methods Phys.Res. B235, 71 (2005) A.Haga, Y.Horikawa, H.Toki, Y.Tanaka Full-relativistic calculation of nuclear polarization in atomic and muonic levels ATOMIC PHYSICS 208Pb; calculated nuclear polarization effects in atomic and muonic levels.
doi: 10.1016/j.nimb.2005.03.148
2005HA53 Phys.Rev. C 72, 034301 (2005) A.Haga, H.Toki, S.Tamenaga, Y.Horikawa, H.L.Yadav Self-consistent relativistic random-phase approximation with vacuum polarization NUCLEAR STRUCTURE 16O, 40Ca; calculated isoscalar-dipole strength distributions. Self-consistent relativistic RPA.
doi: 10.1103/PhysRevC.72.034301
2005HI14 Nucl.Phys. A755, 411c (2005) E.Hiyama, M.Kamimura, A.Hosaka, H.Toki, M.Yahiro Five-body calculation of resonance and continuum states of pentaquark baryons with quark-quark correlations
doi: 10.1016/j.nuclphysa.2005.03.047
2005MA79 J.Phys.(London) G31, 1183 (2005) Relationship between the separable and one-boson-exchange potential for the covariant Bethe-Salpeter equation
doi: 10.1088/0954-3899/31/11/005
2005ME14 Eur.Phys.J. A 25, 23 (2005) J.Meng, W.Zhang, S.G.Zhou, H.Toki, L.S.Geng Shape evolution for Sm isotopes in relativistic mean-field theory NUCLEAR STRUCTURE 144,146,148,150,152,154,156,158Sm; calculated potential energy vs deformation, single-particle level energies. Relativistic mean-field theory, several effective interactions compared.
doi: 10.1140/epja/i2005-10066-6
2005MY02 J.Phys.(London) G31, S1681 (2005) T.Myo, K.Kato, H.Toki, K.Ikeda Tensor correlation in He isotopes NUCLEAR STRUCTURE 4,5,6He; calculated levels, wave functions, role of tensor correlations.
doi: 10.1088/0954-3899/31/10/053
2005SH25 Phys.Rev. C 71, 065208 (2005) Pentaquark Θ+ in nuclear matter and Θ+ hypernuclei NUCLEAR STRUCTURE 17O, 41Ca, 209Pb; calculated Λ and pentaquark hypernuclei single-particle energies.
doi: 10.1103/PhysRevC.71.065208
2005SM03 Nucl.Phys. A755, 337c (2005) G.Smirnov, V.V.Burov, A.V.Molochkov, H.Toki Relating Fp2(x), Fn2(x) and FD2(x) using a relativistic description of the deuteron structure NUCLEAR STRUCTURE 1n, 1,2H; analyzed structure functions; deduced parameters.
doi: 10.1016/j.nuclphysa.2005.03.094
2005SU17 Nucl.Phys. A758, 63c (2005) K.Sumiyoshi, S.Yamada, H.Suzuki, H.Shen, H.Toki An approach toward the successful supernova explosion by physics of unstable nuclei
doi: 10.1016/j.nuclphysa.2005.05.017
2005ZH12 Nucl.Phys. A753, 106 (2005) W.Zhang, J.Meng, S.Q.Zhang, L.S.Geng, H.Toki Magic numbers for superheavy nuclei in relativistic continuum Hartree-Bogoliubov theory NUCLEAR STRUCTURE Z=100-140; calculated two-particle separation energies, pair gap energies, α-decay T1/2; deduced shell closure features. 292,304,318,348,358,378120; calculated binding energy and shell correction energy vs deformation. Relativistic continuum Hartree-Bogoliubov theory.
doi: 10.1016/j.nuclphysa.2005.02.086
2004BU11 Phys.Lett. B 587, 175 (2004) V.V.Burov, A.V.Molochkov, G.I.Smirnov, H.Toki Relating the proton, neutron and deuteron structure functions in the covariant Bethe-Salpeter formalism NUCLEAR STRUCTURE 1n, 1,2H; analyzed proton and deuteron structure function data; deduced neutron structure function. Covariant Bethe-Salpeter formalism.
doi: 10.1016/j.physletb.2004.01.011
2004CA06 Nucl.Phys. A733, 130 (2004) D.Cabrera, L.Roca, E.Oset, H.Toki, M.J.Vicente Vacas Mass dependence of inclusive nuclear φ photoproduction NUCLEAR REACTIONS 12C, 64Cu(γ, X), E not given; calculated φ meson production σ vs momentum; deduced target mass dependences.
doi: 10.1016/j.nuclphysa.2003.12.012
2004GE02 Nucl.Phys. A730, 80 (2004) L.S.Geng, H.Toki, A.Ozawa, J.Meng Proton and neutron skins of light nuclei within the relativistic mean field theory NUCLEAR STRUCTURE 16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34Ne, 18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37Na, 28,29,30,31,32,33,34,35,36,37,38,39,40,41Cl, 29,30,31,32,33,34,35,36,37,38,39,40,41Ar; calculated binding energies, radii, deformation parameters, neutron and proton separation energies. Deformed relativistic mean field.
doi: 10.1016/j.nuclphysa.2003.10.014
2004GE16 Prog.Theor.Phys.(Kyoto) 112, 603 (2004) Proton-Rich Nuclei at and beyond the Proton Drip Line in the Relativistic Mean Field Theory NUCLEAR STRUCTURE 149,150,151,152,153,154Lu, 155,156,157,158Ta, 140,141Ho, 145,146,147Tm, 130,131Eu, 135,136Tb, 119,120Pr, 124,125Pm, 111,112,113Cs, 115,116,117La; calculated proton separation energy, deformation. Relativistic mean-field approach, comparisons with data.
doi: 10.1143/PTP.112.603
2004GE17 J.Phys.(London) G30, 1915 (2004) A systematic study of neutron magic nuclei with N = 8, 20, 28, 50, 82 and 126 in the relativistic mean-field theory NUCLEAR STRUCTURE Z=2-98; calculated binding energies, one- and two-proton separation energies, radii, deformation parameters for N=8, 20, 28, 50, 82, 126 nuclides. Relativistic mean-field approach, comparisons with data.
doi: 10.1088/0954-3899/30/12/011
2004HA24 Phys.Rev. C 69, 044308 (2004) A.Haga, Y.Horikawa, Y.Tanaka, H.Toki Relativistic random-phase approximation calculation with negative energy states of nuclear polarization in muonic atoms ATOMIC PHYSICS, Mesic-atoms 16O; calculated muonic atom energy levels, nuclear-polarization corrections. Relativistic RPA approach.
doi: 10.1103/PhysRevC.69.044308
2004HA60 Phys.Rev. C 70, 064322 (2004) A.Haga, S.Tamenaga, H.Toki, Y.Horikawa Relativistic Hartree approach with exact treatment of vacuum polarization for finite nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energies, charge radii, single-particle energies. Relativistic Hartree approach with exact treatment of vacuum polarization.
doi: 10.1103/PhysRevC.70.064322
2004HI14 Prog.Theor.Phys.(Kyoto) 112, 99 (2004) E.Hiyama, K.Suzuki, H.Toki, M.Kamimura Role of the Quark-Quark Correlation in Baryon Structure and Non-Leptonic Weak Transitions of Hyperons
doi: 10.1143/PTP.112.99
2004IK02 Nucl.Phys. A738, 73 (2004) New mean field theory with the parity and charge mixing for the pion in nuclei NUCLEAR STRUCTURE 12C, 16O, 40Ca, 56Ni, 80Zr, 100Sn, 164Pb; calculated pion energy per nucleon as a function of pion-nucleon coupling constant.
doi: 10.1016/j.nuclphysa.2004.04.014
2004OG04 Prog.Theor.Phys.(Kyoto) 111, 75 (2004) Y.Ogawa, H.Toki, S.Tamenaga, H.Shen, A.Hosaka, S.Sugimoto, K.Ikeda Chiral Sigma Model with Pion Mean Field in Finite Nuclei NUCLEAR STRUCTURE 32S, 36Ar, 40Ca, 44Ti, 48Cr, 52Fe, 56Ni, 60Zn, 64Ge, 68Se; calculated single-particle level energies, pion mean-field features.
doi: 10.1143/PTP.111.75
2004SH44 Nucl.Phys. A745, 121 (2004) Variation of hadron masses in nuclear matter in the relativistic Hartree approximation
doi: 10.1016/j.nuclphysa.2004.09.006
2004SU03 Nucl.Phys. A730, 227 (2004) K.Sumiyoshi, H.Suzuki, S.Yamada, H.Toki Properties of a relativistic equation of state for collapse-driven supernovae
doi: 10.1016/j.nuclphysa.2003.10.007
2004SU16 Nucl.Phys. A738, 240 (2004) Charge- and parity-projected Hartree-Fock study with the tensor force of light nuclei NUCLEAR STRUCTURE 4He; calculated binding energy, radius, parity- and charge-mixing effects. Charge- and parity-projected Hartree-Fock approach.
doi: 10.1016/j.nuclphysa.2004.04.038
2004SU17 Nucl.Phys. A740, 77 (2004) Charge- and parity-projected Hartree-Fock method for the strong tensor correlation and its application to the alpha particle NUCLEAR STRUCTURE 4He; calculated ground and excited states energies, radii, related features. Charge- and parity-projected Hartree-Fock method, tensor force.
doi: 10.1016/j.nuclphysa.2004.05.009
2004TO13 Nucl.Phys. A738, 87 (2004) H.Toki, Y.Ogawa, S.Tamenaga, S.Sugimoto, K.Ikeda Chiral Symmetry and Finite Pion Mean Field in Nuclei NUCLEAR STRUCTURE 32S, 36Ar, 40Ca, 44Ti, 48Cr, 52Fe, 56Ni, 60Zn, 64Ge, 68Se; calculated proton single-particle levels, binding energy per nucleon; deduced role of chiral symmetry. Chiral sigma model with finite pion mean field.
doi: 10.1016/j.nuclphysa.2004.04.016
2004YA23 Int.J.Mod.Phys. E13, 647 (2004) Description of drip-line nuclei within the relativistic mean field plus BCS approach NUCLEAR STRUCTURE 20O, 62Ca, 84Ni, 138Zr, 150Sn, 250Pb; calculated neutron single-particle energies, configurations. O, Ca, Ni, Zr, Sn, Pb; calculated pairing energies, two-neutron separation energies, density distributions, radii. Relativistic mean field plus BCS approach.
doi: 10.1142/S0218301304002375
2003BA30 Nucl.Phys. A715, 827c (2003) S.Banerjee, A.Bhattacharyya, S.K.Ghosh, S.Raha, B.Sinha, H.Toki Relics of Cosmic Quark-Hadron Phase Transition and Massive Compact Halo Objects
doi: 10.1016/S0375-9474(02)01508-7
2003BA96 Nucl.Phys. A721, 1028c (2003) S.Banerjee, A.Bhattacharyya, S.K.Ghosh, S.Raha, B.Sinha, H.Toki Some aspects of strangeness in astrophysics and cosmology
doi: 10.1016/S0375-9474(03)01277-6
2003BO34 Nucl.Phys. A721, 413c (2003) S.G.Bondarenko, V.V.Burov, N.Hamamoto, A.Hosaka, Y.Manabe, H.Toki Separable kernel of nucleon-nucleon interaction in the Bethe-Salpeter approach for J = 0, 1
doi: 10.1016/S0375-9474(03)01085-6
2003GE09 Phys.Rev. C 68, 061303 (2003) α-decay chains of 288173115 and 287172115 in the relativistic mean field theory NUCLEAR STRUCTURE 287,288Mc, 283,284Nh, 279,280Rg, 275,276Mt, 271,272Bh, 267,268Db; calculated binding energies, deformations, Qα, α-decay T1/2. Relativistic mean-field theory, comparison with data.
doi: 10.1103/PhysRevC.68.061303
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