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NSR database version of April 24, 2024.

Search: Author = K.Ikeda

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2020SA51      Sci. Rep. 10, 10674 (2020)

S.Sasaki, T.Miura, K.Ikeda, M.Sakai, T.Sekikawa, M.Saito, T.Yuge, Y.Hirayama

1/f2 spectra of decoherence noise on 75As nuclear spins in bulk GaAs

NUCLEAR MOMENTS 75As; measured frequencies; deduced spectra of decoherence noise on 75As nuclear spins in GaAs substrate, the decoherence noise spectrum from a multiple spin-echo decay, nuclear spins exhibit 1/f2 dependences over two orders of magnitude in all the substrates of un-doped, Cr-doped semi-insulating and Si-doped metallic GaAs at 297 K.

doi: 10.1038/s41598-020-67636-9
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2017FU10      Phys.Lett. B 773, 336 (2017)

Y.Funaki, M.Isaka, E.Hiyama, T.Yamada, K.Ikeda

Multi-cluster dynamics in 13ΛC and analogy to clustering in 12C

NUCLEAR STRUCTURE 12,13C; calculated hypernuclei level energies, J, π, rms radii, parameters. Comparison with available data.

doi: 10.1016/j.physletb.2017.08.048
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2014FU10      Prog.Theor.Exp.Phys. 2014, 113D01 (2014)

Ya.Funaki, T.Yamada, E.Hiyama, B.Zhou, K.Ikeda

Container structure of alpha-alpha-Lambda clusters in 9-Lambda-Berylium

NUCLEAR STRUCTURE 9Be; calculated cluster hypernuclei structures, energy levels, J, π. Comparison with available data.

doi: 10.1093/ptep/ptu143
Citations: PlumX Metrics


2014IT02      Rep.Prog.Phys. 77, 096301 (2014)

M.Ito, K.Ikeda

Unified studies of chemical bonding structures and resonant scattering in light neutron-excess systems, 10, 12Be

NUCLEAR STRUCTURE 8,9,10,11,12Be; calculated energy levels of single-particle states, covalent and ionic configurations, J, π in 10,12Be.

doi: 10.1088/0034-4885/77/9/096301
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2013FU11      Nucl.Phys. A914, 194c (2013)

Y.Funaki, T.Yamada, E.Hiyama, K.Ikeda

Alpha-particle condensation in light hypernuclei

NUCLEAR STRUCTURE 12C, 13C. 13C hypernucleus calculated α-particle occupation probability for specified hypernucleus single-α-orbits vs radius using α-condensate-type microscopic model.

doi: 10.1016/j.nuclphysa.2013.05.012
Citations: PlumX Metrics


2013KI01      Phys.Rev. C 87, 011301 (2013)

M.Kimura, Y.Taniguchi, Y.Kanada-Enyo, H.Horiuchi, K.Ikeda

Prolate, oblate, and triaxial shape coexistence, and the lost magicity of N=28 in 43S

NUCLEAR STRUCTURE 43S; calculated levels, J, π, deformation parameters, B(E2), B(M1), neutron single-particle energies, magnetic-dipole moment, electric quadrupole moment, negative-parity energy surface contours in β-γ plane using triaxial and axial generator coordinate methods (GCM). 47Ca; calculated levels, J, π, Antisymmetrized molecular dynamics (AMD). Coexistence of prolate-deformed, triaxially deformed, and oblate-deformed states, quenching of N=28 shell gap. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.011301
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2013KI05      Phys.Rev. C 87, 034606 (2013)

Y.Kikuchi, T.Myo, K.Kato, K.Ikeda

Coulomb breakup reactions of 11Li in the coupled-channel 9Li+n+n model

NUCLEAR REACTIONS Pb(11Li, X), E=70 MeV/nucleon; calculated breakup cross section using coupled channel three-body (9Li+n+n) Coulomb breakup model of 11Li, a two-neutron halo nucleus. Complex-scaled solutions of the Lippmann-Schwinger equation (CSLS). Comparison with experimental data and previous studies. Mixing of s state in the halo ground state of 11Li.

doi: 10.1103/PhysRevC.87.034606
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2436. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2012IT01      Phys.Rev. C 85, 014302 (2012)

M.Ito, N.Itagaki, K.Ikeda

Cluster correlations for low-lying intruder states of 12Be

NUCLEAR STRUCTURE 12Be; calculated lowest two molecular orbit configurations, energy surfaces for 0+ states, yrast and first excited rotational bands. Generalized two-center cluster model.

doi: 10.1103/PhysRevC.85.014302
Citations: PlumX Metrics


2012MA50      Nucl.Phys. A895, 1 (2012)

H.Masui, K.Kato, K.Ikeda

Expansion of the 16O-core in neutron drip-line nuclei: 23O and 24O

NUCLEAR STRUCTURE 16,17,18,19,20,22,23,24,25,26O; calculated neutron binding energy, Q, rms nuclear radii, first excited state energy, nuclear core, matter density distribution using m-scheme of extended COSM (cluster-orbitting shell model) with various parameters, rms radii also with coupled-channel model. Compared with available data.

doi: 10.1016/j.nuclphysa.2012.09.004
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2012YA02      Phys.Rev. C 85, 034315 (2012)

T.Yamada, Y.Funaki, T.Myo, H.Horiuchi, K.Ikeda, G.Ropke, P.Schuck, A.Tohsaki

Isoscalar monopole excitations in 16O: α-cluster states at low energy and mean-field-type states at higher energy

NUCLEAR STRUCTURE 16O; calculated energies of 0+ levels, rms charge radii, E0 transition matrix elements, particle decay widths, spectroscopic factors, isoscalar monopole strength functions using four α cluster model and α+12C orthogonality condition model (OCM) model. Discussed dual nature of 16O ground state. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.034315
Citations: PlumX Metrics


2011KI11      Int.J.Mod.Phys. E20, 843 (2011)

Y.Kikuchi, K.Kato, T.Myo, M.Takashina, K.Ikeda

Two-neutron correlations in halo nuclei via Coulomb breakup reactions

doi: 10.1142/S0218301311018812
Citations: PlumX Metrics


2011MA87      J.Phys.:Conf.Ser. 312, 092038 (2011)

H.Masui, K.Kato, K.Ikeda

Properties of drip-line nuclei with an m-scheme cluster-orbital shell model approach

NUCLEAR STRUCTURE 18,19,20,21,22,23,24,25,26O; calculated rms radius, mass excess using m-scheme of COSM (cluster-orbital shell model). Compared with available data.

doi: 10.1088/1742-6596/312/9/092038
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2010KI06      Phys.Rev. C 81, 044308 (2010)

Y.Kikuchi, K.Kato, T.Myo, M.Takashina, K.Ikeda

Two-neutron correlations in 6He in a Coulomb breakup reaction

NUCLEAR STRUCTURE 6He; calculated two-neutron density distribution, coulomb breakup cross-section of halo nucleus via α+n+n channel, E1 strength distributions, invariant mass spectra using Complex Scaling Lippmann-Schwinger method. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.044308
Citations: PlumX Metrics


2010TA11      Phys.Rev. C 82, 011302 (2010)

Y.Taniguchi, Y.Kanada-Enyo, M.Kimura, K.Ikeda, H.Horiuchi, E.Ideguchi

Triaxial superdeformation in 40Ar

NUCLEAR STRUCTURE 40Ar; calculated levels, J, π, single-particle energies, triaxial superdeformed band, B(E2) using deformed-basis antisymmetrized molecular dynamics. Comparison with experimental data.

doi: 10.1103/PhysRevC.82.011302
Citations: PlumX Metrics


2010TO13      Int.J.Mod.Phys. E19, 2531 (2010)

H.Toki, T.Myo, K.Ikeda

Tensor optimized shell model and hypernuclei

NUCLEAR STRUCTURE 4He; calculated hypernuclear energy components. Tensor optimized shell model (TOSM).

doi: 10.1142/S0218301310017046
Citations: PlumX Metrics


2009MA76      Eur.Phys.J. A 42, 535 (2009)

H.Masui, K.Kato, K.Ikeda

Study of neutron-rich nuclei with an m -scheme cluster-orbital shell model approach

NUCLEAR STRUCTURE 16,17,18,19,20,21,22,23,24,25,26O; calculated single-neutron separation energies, radii using cluster-orbital shell model. Comparison with data.

doi: 10.1140/epja/i2009-10839-9
Citations: PlumX Metrics


2009MY01      Prog.Theor.Phys.(Kyoto) 121, 511 (2009)

T.Myo, H.Toki, K.Ikeda

Tensor-Optimized Shell Model with Bare Nucleon-Nucleon Interaction for 4He

doi: 10.1143/PTP.121.511
Citations: PlumX Metrics


2009TO07      Int.J.Mod.Phys. E18, 2040 (2009)

H.Toki, T.Myo, K.Ikeda

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
Citations: PlumX Metrics


2008IT03      Phys.Rev.Lett. 100, 182502 (2008)

M.Ito, N.Itagaki, H.Sakurai, K.Ikeda

Coexistence of Covalent Superdeformation and Molecular Resonances in an Unbound Region of 12Be

doi: 10.1103/PhysRevLett.100.182502
Citations: PlumX Metrics


2008KI22      Int.J.Mod.Phys. E17, 2368 (2008)

Y.Kikuchi, K.Kato, T.Myo, M.Takashina, K.Ikeda

Analysis on two-neutron correlation through Dalitz plot of Coulomb breakup reaction for 6He

NUCLEAR STRUCTURE 6He; calculated the energy and Dalitz distributions of E1 transition strength; deduced dominance of sequential decay process. Lippmann-Schwinger equation.

doi: 10.1142/S021830130801163X
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2007MA17      Phys.Rev. C 75, 034316 (2007)

H.Masui, K.Kato, K.Ikeda

Comparison between the Gamow shell model and the cluster-orbital shell model for weakly bound systems

NUCLEAR STRUCTURE 18,19,20O; calculated levels, J, π, configurations. 5,6,7,8He; calculated ground-state energies. 6,8He; calculated radii. Gamow and cluster-orbital shell models.

doi: 10.1103/PhysRevC.75.034316
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2007MY05      Phys.Rev. C 76, 054309 (2007)

T.Myo, K.Kato, K.Ikeda

Resonances of 7He using the complex scaling method

NUCLEAR STRUCTURE 5,6,7He; calculated excitation energies, J, π, spectroscopic factors using complex scaling model.

doi: 10.1103/PhysRevC.76.054309
Citations: PlumX Metrics


2007SU01      Phys.Rev. C 75, 014317 (2007)

S.Sugimoto, K.Ikeda, H.Toki

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
Citations: PlumX Metrics


2007SU16      Nucl.Phys. A789, 155 (2007)

S.Sugimoto, K.Ikeda, H.Toki

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
Citations: PlumX Metrics


2007SU24      Phys.Rev. C 76, 054310 (2007)

S.Sugimoto, H.Toki, K.Ikeda

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
Citations: PlumX Metrics


2006AO02      Phys.Scr. T125, 100 (2006)

S.Aoyama, T.Myo, K.Kato, K.Ikeda

Coulomb breakup and pairing excitation of the two-neutron halo nucleus 11Li

NUCLEAR STRUCTURE 11Li; calculated Coulomb breakup σ(E), pairing excitation, excited state J, π.

doi: 10.1088/0031-8949/2006/T125/023
Citations: PlumX Metrics


2006DO12      Prog.Theor.Phys.(Kyoto) 115, 1069 (2006)

A.Dote, Y.Kanada-En'yo, H.Horiuchi, Y.Akaishi, K.Ikeda

Explicit Treatment of the Tensor Force with the Method of Antisymmetrized Molecular Dynamics

NUCLEAR STRUCTURE 2,3H, 4He; calculated binding energies, radii, tensor force contribution. 4He; calculated single-particle energies. Antisymmetrized molecular dynamics.

doi: 10.1143/PTP.115.1069
Citations: PlumX Metrics


2006IT02      Phys.Rev. C 73, 034310 (2006)

N.Itagaki, H.Masui, M.Ito, S.Aoyama, K.Ikeda

Simplified method to include the tensor contribution in α-cluster model

NUCLEAR STRUCTURE 8Be, 12C; calculated 0+ α-cluster states energies, role of tensor interaction, spin-orbit contribution.

doi: 10.1103/PhysRevC.73.034310
Citations: PlumX Metrics


2006MA17      Phys.Rev. C 73, 034318 (2006)

H.Masui, K.Kato, K.Ikeda

Study of oxygen isotopes and N=8 isotones with an extended cluster-orbital shell model

NUCLEAR STRUCTURE 16,17,18,19,20O, 17F, 18Ne, 20Mg; calculated radii, ground-state energies. Extended cluster-orbital shell model.

doi: 10.1103/PhysRevC.73.034318
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2005KI14      Phys.Rev. C 72, 014606 (2005); Erratum Phys.Rev. C 72, 069901 (2005)

T.Kin, F.Saiho, S.Hohara, K.Ikeda, K.Ichikawa, Y.Yamashita, M.Imamura, G.Wakabayashi, N.Ikeda, Y.Uozumi, M.Matoba, M.Nakano, N.Koori

Proton production cross sections for reactions by 300- and 392-MeV protons on carbon, aluminum, and niobium

NUCLEAR REACTIONS 12C, 27Al, 93Nb(p, p'X), E=300, 392 MeV; measured Ep, σ(E, θ). Comparison with intranuclear cascade and quantum molecular dynamics model predictions.

doi: 10.1103/PhysRevC.72.014606
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1936.


2005MA98      Eur.Phys.J. A 25, Supplement 1, 505 (2005)

H.Masui, T.Myo, K.Kato, K.Ikeda

Study of drip-line nuclei with a core plus multi-valence nucleon model

NUCLEAR STRUCTURE 15N, 16,17,18,19,20,21,22,23,24O, 17F, 18Ne, 19Na, 20Mg; calculated radii. Extended cluster-orbital shell model.

doi: 10.1140/epjad/i2005-06-135-8
Citations: PlumX Metrics


2005MY01      Prog.Theor.Phys.(Kyoto) 113, 763 (2005)

T.Myo, K.Kato, K.Ikeda

Tensor Correlation in 4He and Its Effect on the Doublet Splitting in 5He

NUCLEAR STRUCTURE 4He; calculated tensor correlation. 5He; calculated doublet splitting, role of 4He tensor correlation.

doi: 10.1143/PTP.113.763
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2004IK02      Nucl.Phys. A738, 73 (2004)

K.Ikeda, S.Sugimoto, H.Toki

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
Citations: PlumX Metrics


2004IT04      Phys.Rev.Lett. 92, 142501 (2004)

N.Itagaki, T.Otsuka, K.Ikeda, S.Okabe

Equilateral-Triangular Shape in 14C

NUCLEAR STRUCTURE 14C; calculated levels, deformation, molecular states features; deduced equilateral-triangular shape, rotational bands. Microscopic five-body model.

doi: 10.1103/PhysRevLett.92.142501
Citations: PlumX Metrics


2004IT06      Phys.Lett. B 588, 43 (2004)

M.Ito, K.Kato, K.Ikeda

Application of the generalized two-center cluster model to 10Be

NUCLEAR STRUCTURE 10Be; calculated levels, J, π, molecular orbitals, cluster states. Generalized two-center cluster model.

doi: 10.1016/j.physletb.2004.01.090
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2004IT08      Nucl.Phys. A738, 17 (2004)

N.Itagaki, S.Aoyama, T.Otsuka, T.Yoshida, S.Okabe, K.Ikeda

Exotic cluster structure in light neutron-rich nuclei

NUCLEAR STRUCTURE 10,12Be, 21,22,23,24,25,26,27Ne; calculated binding energies, cluster features. Antisymmetrized molecular dynamics.

doi: 10.1016/j.nuclphysa.2004.04.006
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2004IT13      Phys.Rev. C 70, 054307 (2004)

N.Itagaki, S.Aoyama, S.Okabe, K.Ikeda

Cluster-shell competition in light nuclei

NUCLEAR STRUCTURE 8,10Be, 10B, 12C, 16O; calculated binding energies, contributions from cluster structure. 12C calculated transition probabilities. Antisymmetrized molecular dynamics, cluster-shell competition discussed.

doi: 10.1103/PhysRevC.70.054307
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2004MI17      Nucl.Instrum.Methods Phys.Res. A523, 96 (2004)

H.Miyahara, K.Katoh, N.Marnada, K.Ikeda, K.Fujiki, I.Nishinaka, K.Tsukada, Y.Nagame, M.Asai, S.-I.Ichikawa, H.Haba

Emission probability measurement of principal γ-rays of 147Eu

RADIOACTIVITY 147Eu(β+), (EC) [from 147Sm(p, n)]; measured Eγ, Iγ, βγ-coin; deduced γ-ray emission probabilities, electron capture branching ratio. 147Sm levels deduced feeding intensities.

doi: 10.1016/j.nima.2003.12.029
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2004MI43      Nucl.Instrum.Methods Phys.Res. A533, 404 (2004)

H.Miyahara, K.Katoh, K.Ikeda, K.Fujiki, I.Nishinaka, K.Tsukada, Y.Nagame, M.Asai, S.Ichikawa, H.Haba

Gamma-ray emission probability measurement of 149Eu

RADIOACTIVITY 149Eu(EC) [from 149Sm(p, n)]; measured Eγ, Iγ; deduced branching ratios, emission probabilities. 149Sm deduced transition intensities, internal conversion probabilities.

doi: 10.1016/j.nima.2004.06.171
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2004MY01      Nucl.Phys. A738, 298 (2004)

T.Myo, S.Aoyama, K.Kato, K.Ikeda

Resonances and continuum states in the breakup of halo nuclei

NUCLEAR STRUCTURE 11Li; calculated Coulomb breakup strengths, continuum states contributions. Complex scaling method.

doi: 10.1016/j.nuclphysa.2004.04.049
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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
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2004SU16      Nucl.Phys. A738, 240 (2004)

S.Sugimoto, K.Ikeda, H.Toki

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
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2004SU17      Nucl.Phys. A740, 77 (2004)

S.Sugimoto, K.Ikeda, H.Toki

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
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2004TH11      Eur.Phys.J. A 22, 461 (2004)

G.Thiamova, N.Itagaki, T.Otsuka, K.Ikeda

Systematic study of structure of carbon isotopes with the antisymmetrized molecular dynamics plus generator coordinate method

NUCLEAR STRUCTURE 12,14,16,18,20,22C; calculated binding energies, radii, excited states energies, B(E2), quadrupole moments. 13,15,17,19,21C; calculated binding energies, radii, levels J, π. Antisymmetrized molecular dynamics, comparisons with data.

doi: 10.1140/epja/i2004-10053-5
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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
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2003IK03      Nucl.Phys. A722, 335c (2003)

K.Ikeda, T.Myo, K.Kato

Beyond the core + n + n model for the neutron halo nucleus 11Li

NUCLEAR STRUCTURE 11Li; calculated binding energy, matter radius, configurations, role of pairing and Pauli blocking.

doi: 10.1016/S0375-9474(03)01386-1
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2003IT06      Nucl.Phys. A719, 205c (2003)

N.Itagaki, K.Hagino, T.Otsuka, S.Okabe, K.Ikeda

Importance of clustering in light neutron-rich nuclei

NUCLEAR REACTIONS 9Be(γ, X), E ≈ 0.5-4.5 MeV; calculated photodisintegration σ. Molecular orbital model, comparison with data.

NUCLEAR STRUCTURE 12C; calculated transitions B(E2). Cluster model.

doi: 10.1016/S0375-9474(03)00918-7
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2003IT12      Acta Phys.Hung.N.S. 18, 173 (2003)

N.Itagaki, T.Otsuka, S.Okabe, K.Ikeda

Exotic Cluster Structure in Light Neutron-Rich Nuclei

NUCLEAR STRUCTURE 14C; calculated levels, J, π, cluster configurations. Molecular orbit model.

doi: 10.1556/APH.18.2003.2-4.9
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2003IT14      Mod.Phys.Lett. A 18, 178 (2003)

K.Ito, K.Kato, K.Ikeda

New cluster model based on the Generator Coordinate Method

NUCLEAR STRUCTURE 10Be; calculated potential energy surface for α-6He cluster configuration. Generator coordinate method.

doi: 10.1142/S021773230301020X
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2003MA70      Nucl.Phys. A722, 469c (2003)

H.Masui, T.Myo, K.Kato, K.Ikeda

Coupled-channel study for O-isotopes with the core plus valence neutrons model

NUCLEAR STRUCTURE 17,18O; calculated level energies, configurations. Core plus neutron model, complex scaling method, Jost function method.

doi: 10.1016/S0375-9474(03)01410-6
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2003MB05      Mod.Phys.Lett. A 18, 186 (2003)

H.Masui, T.Myo, K.Kato, K.Ikeda

Coupled-channel study for O-isotopes with the core plus valence neutrons model

NUCLEAR STRUCTURE 17,18O; calculated level energies, configurations. Coupled-channels and resonating group method approach.

doi: 10.1142/S0217732303010223
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2003MY03      Phys.Lett. B 576, 281 (2003)

T.Myo, S.Aoyama, K.Kato, K.Ikeda

Three-body Coulomb breakup of 11Li in the complex scaling method

NUCLEAR STRUCTURE 11Li; calculated Coulomb breakup strengths. Complex scaling method, comparison with data.

doi: 10.1016/j.physletb.2003.10.011
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2003MY04      Nucl.Phys. A722, 449c (2003)

T.Myo, S.Aoyama, K.Kato, K.Ikeda

Resonances and continuums in the three-body breakup of halo nuclei

NUCLEAR STRUCTURE 11Li; calculated excited states energies, dipole strength distribution, Coulomb breakup σ. Three-body model, complex scaling method.

doi: 10.1016/S0375-9474(03)01406-4
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2003MY05      Mod.Phys.Lett. A 18, 166 (2003)

T.Myo, K.Kato, S.Aoyama, K.Ikeda

Resonances and continuums in the three-body breakup of halo nuclei with the complex scaling method

NUCLEAR STRUCTURE 11Li; calculated excited states energies, dipole strength distribution, Coulomb breakup σ. Three-body model, complex scaling method.

doi: 10.1142/S021773230301017X
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2003SU22      Nucl.Phys. A721, 669c (2003)

S.Sugimoto, H.Toki, K.Ikeda

Surface pion condensation in finite nuclei

NUCLEAR STRUCTURE 12C, 16O, 40Ca, 56Ni, 80Zr, 100Sn, 164Pb; calculated pion mean field, pion energy per nucleon. Relativistic mean field approach.

doi: 10.1016/S0375-9474(03)01149-7
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2003SU27      Nucl.Phys. A722, 360c (2003)

S.Sugimoto, H.Toki, K.Ikeda, N.Minkov

Relativistic mean field theory with the pion of finite nuclei

NUCLEAR STRUCTURE 12C, 16O, 40Ca, 56Ni, 80Zr, 100Sn, 164Pb; calculated pion mean field, pion energy per nucleon. Relativistic mean field approach.

doi: 10.1016/S0375-9474(03)01390-3
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2003TH06      Nucl.Phys. A719, 312c (2003)

G.Thiamova, N.Itagaki, T.Otsuka, K.Ikeda

Systematic analysis of neutron-rich carbon isotopes

NUCLEAR STRUCTURE 12,14,16,18,20,22C; calculated ground and excited states energies, radii. 13,15,17,19,21C; calculated binding energies, ground state J, π. Comparisons with data.

doi: 10.1016/S0375-9474(03)00939-4
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2003TO16      J.Korean Phys.Soc. 43, S6 (2003)

H.Toki, K.Ikeda, S.Sugimoto

Surface Pion Condensation of Finite Nuclei in Relativistic Mean Field Theory

NUCLEAR STRUCTURE 12C, 16O, 40Ca, 56Ni, 80Zr, 100Sn, 164Pb; calculated pion mean-field potential energy. Relativistic mean field theory.


2003TO24      Eur.Phys.J. A 18, 363 (2003)

H.Toki, K.Ikeda, S.Sugimoto

Surface pion condensation in finite nuclei

NUCLEAR STRUCTURE 12C, 16O, 40Ca, 56Ni, 80Zr, 100Sn, 164Pb; calculated pion mean-field potential energy. Relativistic mean field theory.

doi: 10.1140/epja/i2002-10238-x
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2002AO02      Prog.Theor.Phys.(Kyoto) 107, 543 (2002)

S.Aoyama, K.Kato, T.Myo, K.Ikeda

The Binding Mechanism and a Low-Lying Resonance in 11Li

NUCLEAR STRUCTURE 11Li; calculated level energies, configurations, resonance features.

doi: 10.1143/PTP.107.543
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2002AO04      Prog.Theor.Phys.(Kyoto), Suppl. 146, 540 (2002)

S.Aoyama, K.Kato, K.Ikeda

Three-Body Cluster Resonances in 11Li and 10He

NUCLEAR STRUCTURE 11Li; calculated levels, J, π, configurations, resonance features. 10He; calculated possible ground-state configuration. Complex scaling method.

doi: 10.1143/PTPS.146.540
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2002HI23      Prog.Theor.Phys.(Kyoto), Suppl. 146, 565 (2002)

S.Hirose, N.Itagaki, T.Otsuka, S.Okabe, K.Ikeda

The Exotic Clustering and Nucleon-Nucleon Correlations in Light Neutron-Rich Nuclei

NUCLEAR STRUCTURE 10Be; calculated levels, J, π, B(E2). Cluster model.

doi: 10.1143/PTPS.146.565
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2002IT02      Eur.Phys.J. A 13, 43 (2002)

N.Itagaki, S.Okabe, K.Ikeda, I.Tanihata

Molecular-Orbital Structure in Neutron-Rich Be and C Isotopes

NUCLEAR STRUCTURE 10,12Be, 12,14,16C; analyzed cluster configurations. Molecular-orbit model.

doi: 10.1140/epja1339-07
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2002IT03      Phys.Rev. C65, 044302 (2002)

N.Itagaki, S.Hirose, T.Otsuka, S.Okabe, K.Ikeda

Triaxial Deformation in 10Be

NUCLEAR STRUCTURE 10Be; calculated rotational bands features, triaxial deformation, transitions B(E2). Molecular-orbit model.

doi: 10.1103/PhysRevC.65.044302
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2002IT08      Prog.Theor.Phys.(Kyoto), Suppl. 146, 207 (2002)

N.Itagaki, K.Ikeda, S.Okabe, T.Otsuka

Exotic Cluster Shapes in Neutron-Rich Be and C Isotopes

NUCLEAR STRUCTURE 12,14,16C; calculated level energies, cluster configurations.

doi: 10.1143/PTPS.146.207
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2002KA28      J.Nucl.Sci.Technol.(Tokyo) 39, 329 (2002)

K.Katoh, H.Miyahara, N.Marnada, N.Ueda, K.Ikeda, K.Fujiki, H.Haba, I.Nishinaka, K.Tsukada, Y.Nagame, M.Asai, S.-I.Ichikawa

Production of 147Eu for Gamma-Ray Emission Probability Measurement

NUCLEAR REACTIONS 147Sm(p, n), (p, 2n), E=6.7-18.0 MeV; measured production σ. Activation technique, comparison with model predictions.

doi: 10.1080/18811248.2002.9715197
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2172.


2002KA76      Prog.Theor.Phys.(Kyoto), Suppl. 146, 179 (2002)

K.Kato, T.Myo, S.Aoyama, K.Ikeda

Beyond the Core+n+n Model Based on the Complex Scaling Method

NUCLEAR STRUCTURE 6He, 10,11Li; calculated levels, J, π; deduced role of dynamical coupling. 11Li; calculated E1 strength distribution. Complex scaling method, comparison with data.

NUCLEAR REACTIONS Pb(6He, 2nα), E=240 MeV/nucleon; calculated Coulomb dissociation σ. Complex scaling method, comparison with data.


2002MA18      Nucl.Instrum.Methods Phys.Res. A480, 591 (2002)

N.Marnada, H.Miyahara, N.Ueda, K.Ikeda, N.Hayashi

γ-Ray Emission Probabilities of 193Os

RADIOACTIVITY 193Os(β-) [from 192Os(n, γ)]; measured Eγ, Iγ, βγ-coin; deduced β-branching ratios, γ-ray emission probabilities. 193Ir deduced transition intensities.

doi: 10.1016/S0168-9002(01)01107-X
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2002MA77      Prog.Theor.Phys.(Kyoto), Suppl. 146, 589 (2002)

H.Masui, S.Aoyama, T.Myo, K.Kato, K.Ikeda

Study of the s-Wave Properties for 10Li through the Analysis of the Break-Up Reaction

NUCLEAR STRUCTURE 10Li; analyzed break-up reaction data; deduced neutron-core potential features.

doi: 10.1143/PTPS.146.589
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2002MY01      Prog.Theor.Phys.(Kyoto) 108, 133 (2002)

T.Myo, S.Aoyama, K.Kato, K.Ikeda

Extended 9Li+n+n Three-Body Model of 11Li with a Pairing Correlation in 9Li

NUCLEAR STRUCTURE 11Li; calculated binding energy, radius. 9,10,11Li; calculated pairing correlations, blocking effects, related features. Extended three-body model.

doi: 10.1143/PTP.108.133
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2002MY03      Prog.Theor.Phys.(Kyoto), Suppl. 146, 601 (2002)

T.Myo, S.Aoyama, K.Kato, K.Ikeda

Coupled Channel 9Li+n+n Model of 11Li

NUCLEAR STRUCTURE 10,11Li; calculated levels, J, π, widths, configurations, radii. Coupled channel three-body model.

doi: 10.1143/PTPS.146.601
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2002SU31      Prog.Theor.Phys.(Kyoto), Suppl. 146, 437 (2002)

S.Sugimoto, K.Ikeda, H.Toki

Relativistic Mean Field Theory with Pion Field for Finite Nuclei

NUCLEAR STRUCTURE 12C, 16O, 40Ca, 56Ni, 80Zr, 100Sn, 164Pb; calculated pion energies. Relativistic mean field theory.

doi: 10.1143/PTPS.146.437
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2002SU34      Prog.Theor.Phys.(Kyoto), Suppl. 146, 626 (2002)

R.Suzuki, T.Myo, K.Kato, K.Ikeda

Analysis of 11Be in the 10Be + n Model

NUCLEAR STRUCTURE 11Be; calculated levels, J, π, B(E1), B(E2), resonance contribution.

NUCLEAR REACTIONS Pb(11Be, n10Be), E=0-4 MeV; calculated Coulomb dissociation σ.

doi: 10.1143/PTPS.146.626
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2002TO22      Prog.Theor.Phys.(Kyoto) 108, 903 (2002)

H.Toki, S.Sugimoto, K.Ikeda

Relativistic mean-field theory with the pion in finite nuclei

NUCLEAR STRUCTURE 12C, 16O, 40Ca, 56Ni, 80Zr, 100Sn, 164Pb; calculated binding energy, effect of pion mean field.

doi: 10.1143/PTP.108.903
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2001AO04      Prog.Theor.Phys.(Kyoto), Suppl. 142, 35 (2001)

S.Aoyama, K.Kato, K.Ikeda

Three-Body Binding and Resonant Mechanisms in Neutron-Rich Light Nuclei Far from Stability Line - Pairing Correlation in Borromean Nuclei -

NUCLEAR STRUCTURE 6,10He, 10,11Li, 10N; calculated level energies, widths, resonance states, pairing correlation effects. Core-plus-neutrons model, complex scaling method.

doi: 10.1143/PTPS.142.35
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2001IT03      Phys.Rev. C64, 014301 (2001)

N.Itagaki, S.Okabe, K.Ikeda, I.Tanihata

Molecular-Orbital Structure in Neutron-Rich C Isotopes

NUCLEAR STRUCTURE 12,14,16C; calculated molecular configurations. Three-α-plus-neutrons approach.

doi: 10.1103/PhysRevC.64.014301
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2001IT04      Acta Phys.Hung.N.S. 13, 153 (2001)

N.Itagaki, S.Okabe, K.Ikeda

Molecular-Orbital Structure in Be Isotopes

NUCLEAR STRUCTURE 14Be, 12,14,16C; calculated cluster-structure related features.

doi: 10.1556/APH.13.2001.1-3.18
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2001IT08      Prog.Theor.Phys.(Kyoto), Suppl. 142, 297 (2001)

N.Itagaki, S.Okabe, K.Ikeda

Molecular-Orbital Structure in Light Neutron-Rich Nuclei

NUCLEAR STRUCTURE 10,12Be, 14,16C; calculated level energies, configurations. Molecular orbit model.

doi: 10.1143/PTPS.142.297
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2001MA01      Appl.Radiat.Isot. 54, 695 (2001)

N.Marnada, H.Miyahara, N.Ueda, N.Hayashi, K.Ikeda

Precise Emission Probabilities of Gamma-Rays of 159Gd

RADIOACTIVITY 159Gd(β-) [from 158Gd(n, γ)]; measured Eγ, Iγ; deduced γ-ray emission probabilities, β-branching. 159Tb levels deduced β-feeding intensities.

doi: 10.1016/S0969-8043(00)00317-1
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