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NSR database version of May 24, 2024.

Search: Author = F.Minato

Found 33 matches.

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2024SH01      Phys.Rev. C 109, 014302 (2024)

T.Shizuma, M.Omer, T.Hayakawa, F.Minato, S.Matsuba, S.Miyamoto, N.Shimizu, Y.Utsuno

Parity assignment for low-lying dipole states in 58Ni

doi: 10.1103/PhysRevC.109.014302
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2023IW01      J.Nucl.Sci.Technol.(Tokyo) 60, 1 (2023)

O.Iwamoto, N.Iwamoto, S.Kunieda, F.Minato, S.Nakayama, Y.Abe, K.Tsubakihara, S.Okumura, C.Ishizuka, T.Yoshida, S.Chiba, N.Otuka, J.-C.Sublet, H.Iwamoto, K.Yamamoto, Y.Nagaya, K.Tada, C.Konno, N.Matsuda, K.Yokoyama, H.Taninaka, A.Oizumi, M.Fukushima, S.Okita, G.Chiba, S.Sato, M.Ohta, S.Kwon

Japanese evaluated nuclear data library version 5: JENDL-5

NUCLEAR REACTIONS 233,235,238U, 237Np, 238,239,240,242Pu, 241,243Am, 243,244,245,246Cm(n, F), (n, γ), E<20 MeV; analyzed available data; deduced σ, average energies of prompt fission neutrons, prompt neutron multiplicities. Neutron sublibrary for all of stable and unstable isotopes with the half-lives longer than 1 day for Z<101 except 257Es. Comparison with JENDL-4.0, ENDF/B-VIII.0 and EXFOR libraries.

doi: 10.1080/00223131.2022.2141903
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2023MI06      Phys.Rev. C 107, 054314 (2023)

F.Minato, T.Naito, O.Iwamoto

Nuclear many-body effects on particle emission following muon capture on 28Si and 40Ca

NUCLEAR REACTIONS 28Si, 40Ca(μ-, X), (μ-, pX), (μ-, d), (μ-, tX), (μ-, αX), (μ-, nX), E*<100 MeV ; calculated muon capture rate, particle yields after the muon capture, multiplicities of the emitted particles. Tamm-Dancoff approximation combined with the two-component exciton model, describing particle emission from the pre-equilibrium state. Hauser-Feshbach statistical model used for particle evaporation from the compound state. Comparison to available experimental data.

doi: 10.1103/PhysRevC.107.054314
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2023TA23      Phys.Rev. C 108, 054607 (2023)

S.Tanaka, N.Nishimura, F.Minato, Y.Aritomo

Postfission properties of uranium isotopes: A hybrid method with Langevin dynamics and the Hauser-Feshbach statistical model

doi: 10.1103/PhysRevC.108.054607
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2023YO02      Phys.Rev. C 108, 034305 (2023)

K.Yoshida, Y.Niu, F.Minato

β-decay half-lives as an indicator of shape-phase transition in neutron-rich Zr isotopes with particle-vibration coupling effects

doi: 10.1103/PhysRevC.108.034305
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2022MI14      Phys.Rev. C 106, 024306 (2022)

F.Minato, Z.Niu, H.Liang

Calculation of β-decay half-lives within a Skyrme-Hartree-Fock-Bogoliubov energy density functional with the proton-neutron quasiparticle random-phase approximation and isoscalar pairing strengths optimized by a Bayesian method

RADIOACTIVITY 87,88,89,90,91,92,93,94,95,96,97,98,99,100Kr, 88,89,90,91,92,93,94,95,96,97,98,99,100,101Rb, 101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137Mo, 102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138Tc(β-); 113,115,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143Cd, 116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144In(β-); 155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192Sm, 156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193Eu(β-); Z=8-110(β-); A=20-368(β-); calculated β--decay T1/2, partial T1/2 for Gamow-Teller decays, Q values, isoscalar spin-triplet strength for neutron-rich nuclei using proton-neutron quasiparticle random-phase approximation (pnQRPA), proton-neutron quasiparticle Tamm-Dancoff approximation (pnQTDA), with Skryme energy density functional, and Bayesian neural network (BNN), the last for isoscalar spin-triplet strength. Calculated T1/2, Q values, isoscalar spin-triplet strength for 5580 neutron-rich nuclei spanning Z=8-110, N=12-258 and A=20-368 are listed in Supplemental Material of the paper. Comparison with available experimental T1/2 in NUBASE2016.

doi: 10.1103/PhysRevC.106.024306
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2021DI04      Nucl.Data Sheets 173, 144 (2021)

P.Dimitriou, I.Dillmann, B.Singh, V.Piksaikin, K.P.Rykaczewski, J.L.Tain, A.Algora, K.Banerjee, I.N.Borzov, D.Cano-Ott, S.Chiba, M.Fallot, D.Foligno, R.Grzywacz, X.Huang, T.Marketin, F.Minato, G.Mukherjee, B.C.Rasco, A.Sonzogni, M.Verpelli, A.Egorov, M.Estienne, L.Giot, D.Gremyachkin, M.Madurga, E.A.McCutchan, E.Mendoza, K.V.Mitrofanov, M.Narbonne, P.Romojaro, A.Sanchez-Caballero, N.D.Scielzo

Development of a Reference Database for Beta-Delayed Neutron Emission

COMPILATION Z=2-87; compiled β-delayed neutron emission data; deduced total delayed neutron yields, time-dependent group parameters in 6- and 8-group representation, and aggregate delayed neutron spectra.

doi: 10.1016/j.nds.2021.04.006
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2021MI17      Phys.Rev. C 104, 044321 (2021)

F.Minato, T.Marketin, N.Paar

β-delayed neutron-emission and fission calculations within relativistic quasiparticle random-phase approximation and a statistical model

RADIOACTIVITY Z=8-110, N=11-209, A=19-318(β-), (β-n); calculated T1/2, β--delayed neutron emission (BDNE) branching ratios (P0n, P1n, P2n, P3n, P4n, P5n, P6n, P7n, P8n, P9n, P10n), mean number of delayed neutrons per beta-decay, and average delayed neutron kinetic energy, total beta-delayed fission and α emission branching ratios for four fission barrier height models (ETFSI, FRDM, SBM, HFB-14). Z=93-110, N=184-200, A=224-318; calculated T1/2, β--delayed fission (BDF) branching ratios (P0f, P1f, P2f, P3f, P4f, P5f, P6f, P7f, P8f, P9f, P10f), total beta-delayed fission and beta-delayed neutron emission branching ratios for four fission barrier height models 140,162Sn; calculated β strength functions, β--delayed neutron branching ratios from P0n to P10n by pn-RQRPA+HFM and pn-RQRPA methods. 137,138,139,140,156,157,158,159,160,161,162Sb; calculated isotope production ratios as a function of excitation energy. 123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156Pd, 120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159Ag, 200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250Os, 200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255Ir; calculated β-delayed one neutron branching ratio P1n by pn-RQRPA+HFM, pn-RQRPA, and FRDM+QRPA+HFM methods, and compared with available experimental data. 89Br, 138I; calculated β-delayed neutron spectrum by pn-RQRPA+HFM method, and compared with experimental spectra. 260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330Fm; calculated fission barrier heights for HFB-14, FRDM, ETFSI and SBM models, mean numbers and mean energies of emitted β-delayed neutrons by pn-RQRPA+HFM and pn-RQRPA methods. 63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99Ni, 120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,161,162,163,164,165,166,167,168,169,170Sn; calculated mean numbers and mean energies of emitted β-delayed neutrons by pn-RQRPA+HFM and pn-RQRPA methods. Z=70-110, N=120-190; calculated β--delayed α branching ratios Pα (%) for FRDM fission barrier data. Fully self-consistent covariant density-functional theory (CDFT), with the ground states of all the nuclei calculated with the relativistic Hartree-Bogoliubov (RHB) model with the D3C* interaction, and relativistic proton-neutron quasiparticle random-phase approximation (pn-RQRPA) for β strength functions, with particle evaporations and fission from highly excited nuclear states estimated by Hauser-Feshbach statistical model (pn-RQRPA+HFM) for four fission barrier height models (ETFSI, FRDM, SBM, HFB-14). Detailed tables of numerical data for β-delayed neutron emission (BDNE), β-delayed fission (BDF) and β-delayed α-particle emission branching ratios are given in the Supplemental Material of the paper.

doi: 10.1103/PhysRevC.104.044321
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2021SH08      Phys.Rev. C 103, 024309 (2021)

T.Shizuma, F.Minato, M.Omer, T.Hayakawa, H.Ohgaki, S.Miyamoto

Low-lying electric and magnetic dipole strengths in 207Pb

NUCLEAR REACTIONS 207Pb(polarized γ, γ'), E(maximum)=5.8, 6.3, 6.8 MeV quasimonochromatic photon beam generated by laser Compton scattering (LCS) with relativistic electrons circulating in the NewSUBARU storage ring; measured Eγ, Iγ at azimuthal angles of 0° and 90° relative to the polarization plane, azimuthal intensity ratios using two HPGe detectors at the LASTI of the University of Hyogo. 207Pb; deduced levels, J, π, branching ratios Γ0/Γ, integrated scattering cross sections, gΓ02/Γ, B(E1)(up), B(M1)(up), E1 and M1 photoabsorption cross sections, coherent excitations of spin-flip 1p-1h states in the 206Pb core. Nuclear resonance fluorescence (NRF) study. Comparison with particle-vibration coupling (PVC), with the quasiparticle random-phase approximation (QRPA) calculations using SkM*, SGII, and SkP interactions, and with previous experimental results.

doi: 10.1103/PhysRevC.103.024309
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2688. Data from this article have been entered in the XUNDL database. For more information, click here.


2020CI07      Phys.Rev. C 102, 034306 (2020)

M.Ciccarelli, F.Minato, T.Naito

Theoretical study of Nb isotope productions by muon capture reaction on 100Mo

NUCLEAR REACTIONS 100Mo(μ-, ν)100Nb, (μ-, n)99Nb, (μ-, 2n)98Nb, (μ-, 3n)97Nb, (μ-, 4n)96Nb, (μ-, 5n)95Nb, E not given; calculated production rates of Nb isotopes, and compared with experimental data at incident momentum=28 MeV/c for muons; calculated production rates and mean excitation energy of different Jπ states of Nb isotopes, neutron spectrum for 100Mo(μ-, xn) reaction. 92,94,96,98Mo(μ-, ν), (μ-, n), (μ-, 2n), (μ-, 3n), (μ-, 4n), (μ-, 5n), (μ-, X)87Nb/88Nb/89Nb/90Nb/91Nb/92Nb/93Nb/94Nb/95Nb/96Nb/97Nb/98Nb, E not given; calculated production rates of Nb isotopes from neutron emission and also charged-particle emissions; estimated muon intensity to produce enough 99Mo for medical diagnostics applications. Proton-neutron quasiparticle random phase approximation (pn-QRPA) on the basis of Skyrme-Hartree-Fock+BCS model (SHFBCS) for muon capture, and Hauser-Feshbach statistical model for particle evaporation process from the daughter nucleus.

doi: 10.1103/PhysRevC.102.034306
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2020MI02      Eur.Phys.J. A 56, 45 (2020)

F.Minato, Y.Tanimura

Spin-isospin properties of N=Z odd-odd nuclei from a core + pn three-body model including core excitations

doi: 10.1140/epja/s10050-020-00035-w
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2019FU04      J.Nucl.Sci.Technol.(Tokyo) 56, 412 (2019)

N.Furutachi, F.Minato, O.Iwamoto

Phenomenological level density model with hybrid parameterization of deformed and spherical state densities

doi: 10.1080/00223131.2019.1588801
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2019FU05      Phys.Rev. C 100, 014610 (2019)

N.Furutachi, F.Minato, O.Iwamoto

Statistical properties of thermal neutron capture cross sections calculated with randomly generated resonance parameters

NUCLEAR REACTIONS 119,120Sn, 152Eu, 154Gd, 192Ir(n, γ), E=thermal; calculated resonance parameters, probability distribution of thermal neutron capture cross sections deduced stochastically with the resonance parameters randomly sampled from Wigner and Porter-Thomas distributions, distribution of average s-wave resonance spacing D0 and Γγ0 for 193 nuclei. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.014610
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2017FU12      Phys.Rev. C 96, 054608 (2017); Erratum Phys.Rev. C 97, 029901 (2018)

T.Fukui, F.Minato

Theoretical investigation of two-particle two-hole effects on spin-isospin excitations through charge-exchange reactions

NUCLEAR REACTIONS 48Ca(p, n)48Sc, E=25, 35, 45, 295 MeV; calculated σ(θ, E) of the IAS for E(p)=25-45 MeV using TDA and Lane form factors, and σ(θ, E) for GT, low-lying 1+ resonance and giant resonances for E(p)=295 MeV with and without the 2p2h configuration, transition density and σ(θ, E) of low-lying 1+ resonance and giant resonances of 48Sc with the STDA at E(p)=295 MeV; deduced effect of 2p2h configuration mixing on the GT-resonance states. Second Tamm-Dancoff approximation (STDA) and distorted-wave Born approximation (DWBA), with phenomenological one-range Gaussian interaction for obtaining the form factor. Comparison with experimental data.

NUCLEAR STRUCTURE 48Ca; calculated strength functions of Gamow-Teller (GT) and IAS resonances, and that of spin-quadrupole (SQ) 1+ using second Tamm-Dancoff approximation (STDA) and TDA.

doi: 10.1103/PhysRevC.96.054608
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2017SH41      Phys.Rev. C 96, 044316 (2017)

T.Shizuma, T.Hayakawa, I.Daito, H.Ohgaki, S.Miyamoto, F.Minato

Low-lying dipole strength in 52Cr

NUCLEAR REACTIONS 52Cr(polarized γ, γ'), E(max)=8.8, 9.4, 10.1, 11.0, 12.1 MeV quasimonochromatic, linearly polarized photon beam from NewSUBARU synchrotron radiation facility at the University of Hyogo; measured Eγ, Iγ, γγ(θ), polarization asymmetry, multipolarities. 52Cr; deduced levels, J, π, Γ02/Γ, B(E1), B(M1), cumulative M1 and E1 strengths, configurations. Comparison with previous experimental results, and with RPA and SRPA calculations using SGII and SGII+Te1 interactions.

doi: 10.1103/PhysRevC.96.044316
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2555. Data from this article have been entered in the XUNDL database. For more information, click here.


2016IW01      Nucl.Data Sheets 131, 259 (2016)

O.Iwamoto, N.Iwamoto, S.Kunieda, F.Minato, K.Shibata

The CCONE Code System and its Application to Nuclear Data Evaluation for Fission and Other Reactions

doi: 10.1016/j.nds.2015.12.004
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2016MI09      Phys.Rev. C 93, 044319 (2016)

F.Minato

Estimation of a 2p2h effect on Gamow-Teller transitions within the second Tamm-Dancoff approximation

NUCLEAR STRUCTURE 24O, 34Si, 48Ca; calculated Gamow-Teller (GT) strength distributions as function of excitation energy, GT-strength distribution as a function of excitation energy of daughter nuclei, quenching and fragmentation of GT strengths of Gamow-Teller giant resonances (GTGRs); deduced two-particle two-hole (2p2h) effect on Gamow-Teller (GT) transition for neutron-rich nuclei, correlation of the 2p2h configurations. Second Tamm-Dancoff approximation (STDA) with the Skyrme interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.93.044319
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2014SA38      J.Phys.Soc.Jpn. 83, 073201 (2014)

N.Sato, K.Tsukada, S.Watanabe, N.S.Ishioka, M.Kawabata, H.Saeki, Y.Nagai, T.Kin, F.Minato, N.Iwamoto, O.Iwamoto

First Measurement of the Radionuclide Purity of the Therapeutic Isotope 67Cu Produced by 68Zn(n, x) Reaction Using natC(d, n) Neutrons

NUCLEAR REACTIONS 68Zn(n, X)64Cu/67Cu/69Zn/65Zn/65Ni/66Ni, E<40 MeV; measured reaction products, Eγ, Iγ; deduced yields. Comparison with CCONE nuclear model code calculations.

doi: 10.7566/JPSJ.83.073201
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2013HA27      Nucl.Phys. A914, 151c (2013)

K.Hagino, J.M.Yao, F.Minato, Z.P.Li, M.T.Win

Collective excitations of Λ hypernuclei

NUCLEAR STRUCTURE 20,22,24,26,28,30,32,34,36,38Ne, 22,24,26,28,30,32,34,36,38,40,42Si; calculated deformation, deformation of (A+Λ) hypernuclei, binding energy, Q vs deformation using relativistic mean field. 24Mg, 25Mg; calculated 25ΛMg hypernucleus deformation, low-spin levels, J, π, rotational bands, B(E2) using relativistic mean field. 16O, 18O; calculated 18ΛΛO hypernucleus dipole strength distribution vs energy, B(E2), B(E3) using RPA. Compared with data.

doi: 10.1016/j.nuclphysa.2012.12.077
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2013KI03      J.Phys.Soc.Jpn. 82, 034201 (2013)

T.Kin, Y.Nagai, N.Iwamoto, F.Minato, O.Iwamoto, Y.Hatsukawa, M.Segawa, H.Harada, C.Konno, K.Ochiai, K.Takakura

New Production Routes for Medical Isotopes 64Cu and 67Cu Using Accelerator Neutrons

NUCLEAR REACTIONS Zn(n, X)64Cu/67Cu, E=14 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with experimental data.

NUCLEAR REACTIONS Cu(d, n)64Cu/67Cu, E=40 MeV; estimated production yields. 67Zn(n, p)67Cu, 68Zn(n, X)67Cu, E=14.7 MeV; calculated yields. comparison with available data.

doi: 10.7566/JPSJ.82.034201
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2013MI02      Phys.Rev.Lett. 110, 122501 (2013)

F.Minato, C.L.Bai

Impact of Tensor Force on β Decay of Magic and Semimagic Nuclei

RADIOACTIVITY 34Si, 68,78Ni, 132Sn(β-); calculated T1/2, Q-value, log ft values. Comparison with experimental data.

doi: 10.1103/PhysRevLett.110.122501
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2013MI26      Phys.Rev. C 88, 064303 (2013)

F.Minato, K.Hagino

Sum rule approach to a soft dipole mode in Λ hypernuclei

NUCLEAR STRUCTURE 16O, 32S, 40Ca, 51V, 64Ni, 89Y, 120Sn, 139La, 208Pb; calculated hypernucleus ground-state wave function, root-mean-square radii, excitation energy and energy-weighted sum rule for soft dipole mode. 18O, 210Pb; calculated strength distributions for dipole mode for the double-hypernucleus. Hartree-Fock method with several Skyrme-type ΛN interactions.

doi: 10.1103/PhysRevC.88.064303
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2013NA16      J.Phys.Soc.Jpn. 82, 064201 (2013)

Y.Nagai, K.Hashimoto, Y.Hatsukawa, H.Saeki, S.Motoishi, N.Sato, M.Kawabata, H.Harada, T.Kin, K.Tsukada, T.K.Sato, F.Minato, O.Iwamoto, N.Iwamoto, Y.Seki, K.Yokoyama, T.Shiina, A.Ohta, N.Takeuchi, Y.Kawauchi, N.Sato, H.Yamabayashi, Y.Adachi, Y.Kikuchi, T.Mitsumoto, T.Igarashi

Generation of Radioisotopes with Accelerator Neutrons by Deuterons

NUCLEAR REACTIONS 100Mo(n, 2n), E<20 MeV; measured reaction products, Eγ, Iγ; deduced yields. Comparison with available data.

doi: 10.7566/JPSJ.82.064201
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2012MI04      Phys.Rev. C 85, 024316 (2012)

F.Minato, K.Hagino

Application of random-phase approximation to vibrational excitations of double-Λ hypernuclei

NUCLEAR STRUCTURE 18O; calculated single-particle neutron and proton levels, energies of first 2+ and 3- states, B(E2), B(E3), centroid energies and strength distributions for E1, E2 and E3 excitations, transition densities for GDR, GQR and high-lying octupole states for double-Λ hypernuclei. 18O, 208Pb; calculated isoscalar monopole (E0) and GMR strength distributions of double-Λ hypernuclei. Collective vibrational excitations of double-Λ hypernuclei. Hartree-Fock plus random phase approximation (HF+RPA). Comparison with properties of 16O and 208Pb nuclei.

doi: 10.1103/PhysRevC.85.024316
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2012OS04      J.Phys.Soc.Jpn. 81, 084201 (2012)

M.Oshima, T.Kin, S.Nakamura, M.Honma, F.Minato, T.Hayakawa, K.Y.Hara, A.Kimura, M.Koizumi, H.Harada, J.Goto, Y.Murakami

Spectroscopic Study of 63Ni via Cold Neutron Capture Reaction: I. Nuclear Structure of 63Ni

NUCLEAR REACTIONS 62Ni(n, γ), E low; measured reaction products, Eγ, Iγ; deduced energies, J, π, level scheme. Comparison with microscopic calculations.

doi: 10.1143/JPSJ.81.084201
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2011MI05      Nucl.Phys. A856, 55 (2011)

F.Minato, S.Chiba

Fission barrier of actinide nuclei with double-Λ particles within the Skyrme-Hartree-Fock method

NUCLEAR STRUCTURE 13B, 240U double hypernuclei; calculated fission barriers.

doi: 10.1016/j.nuclphysa.2011.02.127
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2011MI12      J.Nucl.Sci.Technol.(Tokyo) 48, 984 (2011)

F.Minato

Nuclear Level Densities with Microscopic Statistical Method Using a Consistent Residual Interaction

NUCLEAR STRUCTURE 60Ni, 98Mo, 142Ce, 184W; calculated nuclear level density. Skyrme-Hartree-Fock and Bardeen-Cooper-Schrieffer method.

NUCLEAR REACTIONS 97Mo, 183W, 235U(n, γ), E<10 MeV; calculated σ. Skyrme-Hartree-Fock and Bardeen-Cooper-Schrieffer method, comparison with experimental data.

doi: 10.3327/jnst.48.984
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2010MI14      J.Phys.Soc.Jpn. 79, 093201 (2010)

F.Minato, Y.Nagai

Estimation of Production Yield of 99Mo for Medical Use using Neutrons from natC(d, n) at Ed=40 MeV

NUCLEAR REACTIONS 100Mo(n, 2n), E=14 MeV; calculated 99Mo yield using JENDL neutron library.

doi: 10.1143/JPSJ.79.093201
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2009HA34      Phys.Rev. C 80, 047301 (2009)

K.Hagino, F.Minato

Test of finite temperature random-phase approximation on a Lipkin model

doi: 10.1103/PhysRevC.80.047301
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2009MI25      Phys.Rev. C 80, 065808 (2009)

F.Minato, K.Hagino

β-decay half-lives at finite temperatures for N=82 isotones

RADIOACTIVITY 120Sr, 122Zr, 124Mo, 126Ru, 128Pd, 130Cd, 132Sn(β-); calculated half-lives, GT strength functions, average proton pairing gap using finite-temperature quasiparticle random phase approximation (FTQRPA) on the basis of the finite temperature Skyrme-HF+BCS method. 122,124,126,128,130,132Cd; calculated half-lives. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.065808
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2009MI28      Nucl.Phys. A831, 150 (2009)

F.Minato, S.Chiba, K.Hagino

Fission of heavy Λ hypernuclei with the Skyrme-Hartree-Fock approach

NUCLEAR STRUCTURE 239U; calculated fission barrier height, single particle levels and associated parameters for bound hypernucleus using Skyrme-Hartree-Fock-BCS method. Comparison with 238U.

doi: 10.1016/j.nuclphysa.2009.09.063
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2008MI05      Phys.Rev. C 77, 044308 (2008)

F.Minato, K.Hagino

Fission barriers in the neutron-proton isospin plane for heavy neutron-rich nuclei

NUCLEAR STRUCTURE 220,236,266U; calculated fission barriers, proton single particle levels, proton and neutron deformation parameters, density distributions. Skyrme-Hartree-Fock-BCS method.

doi: 10.1103/PhysRevC.77.044308
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2007MI13      Phys.Rev. C 75, 045802 (2007)

F.Minato, K.Hagino, N.Takigawa, A.B.Balantekin, Ph.Chomaz

Effect of electronic environment on neutrino-nucleus reactions at r-process sites

NUCLEAR REACTIONS 56Fe, 208Pb(ν, e), E not given; calculated σ(E), electron screening and Pauli blocking effects.

doi: 10.1103/PhysRevC.75.045802
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