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NSR database version of February 19, 2024.

Search: Author = H.Toki

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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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
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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
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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
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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


2017HU02      Phys.Rev. C 95, 025804 (2017)

J.Hu, H.Shen, H.Toki

Neutron stars within a relativistic central variational method

doi: 10.1103/PhysRevC.95.025804
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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2358.


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
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2014HU01      Prog.Theor.Exp.Phys. 2014, 013D02 (2014)

J.N.Hu, A.Li, H.Shen, H.Toki

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
Citations: PlumX Metrics


2014HU03      Phys.Rev. C 89, 025802 (2014)

J.N.Hu, A.Li, H.Toki, W.Zuo

Extended quark mean-field model for neutron stars

doi: 10.1103/PhysRevC.89.025802
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2014HU13      Phys.Rev. C 90, 014309 (2014)

J.Hu, E.Hiyama, H.Toki

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
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


2013IM01      Nucl.Phys. A913, 71 (2013)

S.Imai, H.Toki, W.Weise

Quark-hadron matter at finite temperature and density in a two-color PNJL model

doi: 10.1016/j.nuclphysa.2013.06.001
Citations: PlumX Metrics


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.


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 810 times the solar mass.

doi: 10.1103/PhysRevC.88.015806
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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


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
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2012OG08      J.Phys.:Conf.Ser. 381, 012111 (2012)

Y.Ogawa, H.Toki

Extended Brueckner-Hartree-Fock theory with pionic correlation in finite nuclei

doi: 10.1088/1742-6596/381/1/012111
Citations: PlumX Metrics


2012WA11      Prog.Theor.Phys.(Kyoto) 127, 739 (2012)

Y.Wang, J.Hu, H.Toki, H.Shen

Skyrme-Hartree-Fock plus Tensor Correction for Nuclear Matter

doi: 10.1143/PTP.127.739
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


2011OG05      Nucl.Phys. A860, 22 (2011)

Y.Ogawa, H.Toki

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
Citations: PlumX Metrics


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
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2010HU10      Eur.Phys.J. A 43, 323 (2010)

J.Hu, H.Toki, W.Wen, H.Shen

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
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


2010WE03      Prog.Theor.Phys.(Kyoto) 123, 811 (2010)

W.Wen, J.Hu, H.Toki, H.Shen

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
Citations: PlumX Metrics


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
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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


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
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


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


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
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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
Citations: PlumX Metrics


2007GE08      Chin.Phys.Lett. 24, 1865 (2007)

Li.-S.Geng, J.Meng, H.Toki

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
Citations: PlumX Metrics


2007HA14      Phys.Rev. C 75, 044315 (2007)

A.Haga, Y.Horikawa, H.Toki

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
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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
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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


2007OG03      Phys.Rev. C 76, 014305 (2007)

Y.Ogawa, H.Toki, S.Tamenaga

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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


2006GE03      J.Phys.(London) G32, 573 (2006)

L.S.Geng, H.Toki, E.G.Zhao

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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


2006OS04      Phys.Rev. C 74, 015207 (2006)

E.Oset, H.Toki

Critical analysis on deeply bound kaonic states in nuclei

doi: 10.1103/PhysRevC.74.015207
Citations: PlumX Metrics


2006SH04      Prog.Theor.Phys.(Kyoto) 115, 325 (2006)

H.Shen, F.Yang, H.Toki

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
Citations: PlumX Metrics


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)

L.Geng, H.Toki, J.Meng

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2005MA79      J.Phys.(London) G31, 1183 (2005)

Y.Manabe, A.Hosaka, H.Toki

Relationship between the separable and one-boson-exchange potential for the covariant Bethe-Salpeter equation

doi: 10.1088/0954-3899/31/11/005
Citations: PlumX Metrics


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
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


2005SH25      Phys.Rev. C 71, 065208 (2005)

H.Shen, H.Toki

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2004GE16      Prog.Theor.Phys.(Kyoto) 112, 603 (2004)

L.Geng, H.Toki, J.Meng

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
Citations: PlumX Metrics


2004GE17      J.Phys.(London) G30, 1915 (2004)

L.S.Geng, H.Toki, J.Meng

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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


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
Citations: PlumX Metrics


2004SH44      Nucl.Phys. A745, 121 (2004)

H.Shen, S.Tamenaga, H.Toki

Variation of hadron masses in nuclear matter in the relativistic Hartree approximation

doi: 10.1016/j.nuclphysa.2004.09.006
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2004YA23      Int.J.Mod.Phys. E13, 647 (2004)

H.L.Yadav, M.Kaushik, H.Toki

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


2003GE09      Phys.Rev. C 68, 061303 (2003)

L.S.Geng, H.Toki, J.Meng

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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