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NSR database version of May 24, 2024.

Search: Author = Y.Hashimoto

Found 60 matches.

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2020HI08      Prog.Theor.Exp.Phys. 2020, 033I01 (2020)

A.Higashi, Y.Hashimoto, D.Ohsawa, T.Shirai, K.Noda

Secondary electron emission measurement from Cr and Cu bombarded by an Ne10+ beam at 6 MeV/n

NUCLEAR REACTIONS Cr, Cu, 27Al(Ne, E), E=6 MeV/nucleon; measured reaction products, Eβ, Iβ; deduced backward secondary-electron-emission yield.

doi: 10.1093/ptep/ptaa006
Citations: PlumX Metrics


2019SC14      Phys.Rev. C 100, 024623 (2019)

G.Scamps, Y.Hashimoto

Density-constrained time-dependent Hartree-Fock-Bogoliubov method

NUCLEAR REACTIONS 16O(16O, X), 20O(20O, X), E(cm)=6-15 MeV; 40Ca(40Ca, X), E(cm)=48-65 MeV; 44Ca(44Ca, X), E(cm)=53 MeV; calculated V(r) and fusion σ(E) versus distance between fragments (R) using a density-constrained time-dependent Hartree-Fock (DC-TDHF) method with a Gogny interaction and a DC-TDHF-Bogoliubov method.

doi: 10.1103/PhysRevC.100.024623
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2018RE04      Phys.Rev. C 97, 034627 (2018)

D.Regnier, D.Lacroix, G.Scamps, Y.Hashimoto

Microscopic description of pair transfer between two superfluid Fermi systems: Combining phase-space averaging and combinatorial techniques

NUCLEAR REACTIONS 20O(20O, X), E<Coulomb barrier; calculated probability to transfer one and two pairs in symmetric central collision as function of the closest distance of approach. 20O(14O, X), E(cm)=7.903, 8.903, 9.403 MeV; calculated average drift along with fluctuation of the number of transferred particles, and pair transfer probabilities. Phase-space combinatorial (PSC) technique combined with TDHFB framework to obtain multiple pair transfer probabilities between superfluid systems.

doi: 10.1103/PhysRevC.97.034627
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2017SC15      Phys.Rev. C 96, 031602 (2017)

G.Scamps, Y.Hashimoto

Transfer probabilities for the reactions 14, 20O + 20O in terms of multiple time-dependent Hartree-Fock-Bogoliubov trajectories

NUCLEAR REACTIONS 20O(20O, X), E=8.91, 9.21, 9.31; calculated pair transfer probability as a function of time, neutron pair transfer probability as a function of distance. 14O(20O, X), E not given; calculated transfer probability of one and two neutrons as a function of the distance of closest approach. Time-dependent Hartree-Fock-Bogoliubov (TDHFB) theory.

doi: 10.1103/PhysRevC.96.031602
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2016HA21      Phys.Rev. C 94, 014610 (2016)

Y.Hashimoto, G.Scamps

Gauge angle dependence in time-dependent Hartree-Fock-Bogoliubov calculations of 20O+20O head-on collisions with the Gogny interaction

NUCLEAR REACTIONS 20O(20O, X), E(cm)=9.21, 9.41, 9.61 MeV; calculated density contours in y-z plane, trajectories of head-on collisions, pairing energies, numbers of transferred protons and neutrons. Time-dependent Hartree-Fock-Bogoliubov (TDHFB) calculations using Gogny D1S effective interaction for head-on collision processes.

doi: 10.1103/PhysRevC.94.014610
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2014SA06      Phys.Lett. B 728, 462 (2014)

Y.Satou, J.W.Hwang, S.Kim, K.Tshoo, S.Choi, T.Nakamura, Y.Kondo, N.Matsui, Y.Hashimoto, T.Nakabayashi, T.Okumura, M.Shinohara, N.Fukuda, T.Sugimoto, H.Otsu, Y.Togano, T.Motobayashi, H.Sakurai, Y.Yanagisawa, N.Aoi, S.Takeuchi, T.Gomi, M.Ishihara, S.Kawai, H.J.Ong, T.K.Onishi, S.Shimoura, M.Tamaki, T.Kobayashi, Y.Matsuda, N.Endo, M.Kitayama

One-neutron knockout reaction of 17C on a hydrogen target at 70 MeV/nucleon

NUCLEAR REACTIONS 1H(17C, 16C), E=70 MeV/nucleon; measured reaction products, TOF, Eγ, Iγ. 16C; deduced energy levels, J, π, σ. Comparison with Glauber model calculations, available data.

doi: 10.1016/j.physletb.2013.12.024
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2448. Data from this article have been entered in the XUNDL database. For more information, click here.


2013HA31      Phys.Rev. C 88, 034307 (2013)

Y.Hashimoto

Time-dependent Hartree-Fock-Bogoliubov calculations using a Lagrange mesh with the Gogny interaction

NUCLEAR STRUCTURE 20O, 34Mg; calculated ground-state energies, pairing correlations in the collective motions, strength function S(E) for isoscalar quadrupole vibrations. Hartree-Fock-Bogoliubov (HFB) and time-dependent HFB (TDHFB) method with the Gogny interaction and Lagrange mesh and harmonic oscillator (LMHO).

doi: 10.1103/PhysRevC.88.034307
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2013SU20      Phys.Rev. C 88, 024326 (2013)

H.Suzuki, N.Aoi, E.Takeshita, S.Takeuchi, S.Ota, H.Baba, S.Bishop, T.Fukui, Y.Hashimoto, E.Ideguchi, K.Ieki, N.Imai, M.Ishihara, H.Iwasaki, S.Kanno, Y.Kondo, T.Kubo, K.Kurita, K.Kusaka, T.Minemura, T.Motobayashi, T.Nakabayashi, T.Nakamura, T.Nakao, M.Niikura, T.Okumura, T.K.Ohnishi, H.J.Ong, H.Sakurai, S.Shimoura, R.Sugo, D.Suzuki, M.K.Suzuki, M.Tamaki, K.Tanaka, Y.Togano, K.Yamada

Collectivity of neutron-rich Ti isotopes

NUCLEAR REACTIONS 1H(58Ti, 58Ti'), [secondary 58Ti beam from Be(70Zn, X), E=63 MeV/nucleon primary reaction], E=42.0 MeV/nucleon; measured particle spectra, time-of-flight, Eγ, Iγ, (particle)γ-, γγ-coin, angle-integrated σ using RIPS separator and DALI2 array of NaI(Tl) detectors at RIBF, RIKEN facility. 58Ti; deduced levels, J, π, deformation length of first 2+ state, collectivity. Systematics of energies and deformation lengths of first 2+ states in A=44-62 Ti, Fe and Cr isotopes, comparison with shell-model calculations.

doi: 10.1103/PhysRevC.88.024326
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Data from this article have been entered in the XUNDL database. For more information, click here.


2012HA18      Eur.Phys.J. A 48, 55 (2012)

Y.Hashimoto

Linear responses in time-dependent Hartree-Fock-Bogoliubov method with Gogny interaction

NUCLEAR STRUCTURE 18,20,22,24O, 26Ne, 24,34Mg, 44,50,52,54Ti; calculated quadrupole and dipole strength functions from quadrupole and dipole moments obtained within TDHFB. Compared with data.

doi: 10.1140/epja/i2012-12055-0
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2011SA02      Phys.Lett. B 697, 459 (2011)

Y.Satou, T.Nakamura, Y.Kondo, N.Matsui, Y.Hashimoto, T.Nakabayashi, T.Okumura, M.Shinohara, N.Fukuda, T.Sugimoto, H.Otsu, Y.Togano, T.Motobayashi, H.Sakurai, Y.Yanagisawa, N.Aoi, S.Takeuchi, T.Gomi, M.Ishihara, S.Kawai, H.J.Ong, T.K.Onishi, S.Shimoura, M.Tamaki, T.Kobayashi, Y.Matsuda, N.Endo, M.Kitayama

14Be(p, n)14B reaction at 69 MeV in inverse kinematics

NUCLEAR REACTIONS 1H(14Be, n), E=69 MeV/nucleon; measured reaction fragments, Eγ, Iγ; deduced resonance parameters, energy spectrum, σ(θ), Gamow-Teller transition, J, π. DWBA calculations.

doi: 10.1016/j.physletb.2011.02.045
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2325. Data from this article have been entered in the XUNDL database. For more information, click here.


2011SA39      Phys.Rev. C 84, 024604 (2011)

S.Sakaguchi, Y.Iseri, T.Uesaka, M.Tanifuji, K.Amos, N.Aoi, Y.Hashimoto, E.Hiyama, M.Ichikawa, Y.Ichikawa, S.Ishikawa, K.Itoh, M.Itoh, H.Iwasaki, S.Karataglidis, T.Kawabata, T.Kawahara, H.Kuboki, Y.Maeda, R.Matsuo, T.Nakao, H.Okamura, H.Sakai, Y.Sasamoto, M.Sasano, Y.Satou, K.Sekiguchi, M.Shinohara, K.Suda, D.Suzuki, Y.Takahashi, A.Tamii, T.Wakui, K.Yako, M.Yamaguchi, Y.Yamamoto

Analyzing power in elastic scattering of 6He from a polarized proton target at 71 MeV/nucleon

NUCLEAR REACTIONS 1H(6He, 6He), [6He secondary beam from 9Be(12C, X), E=92 MeV/nucleon primary reaction], E=71 MeV/nucleon; measured 6He and proton spectra, (6He)(p)(q, φ), p(θ), vector analyzing powers, polarized target, σ(θ); deduced optical model parameters. Comparison with semimicroscopic analysis with an α+n+n cluster folding model.

doi: 10.1103/PhysRevC.84.024604
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2287.


2011SA68      J.Phys.:Conf.Ser. 312, 082037 (2011)

S.Sakaguchi, T.Uesaka, T.Kawabata, T.Wakui, N.Aoi, Y.Hashimoto, Y.Ichikawa, K.Itoh, M.Itoh, H.Iwasaki, T.Kawahara, Y.Kondo, H.Kuboki, Y.Maeda, T.Nakamura, T.Nakao, Y.Nakayama, H.Okamura, H.Sakai, Y.Sasamoto, M.Sasano, Y.Satou, K.Sekiguchi, T.Shimamura, Y.Shimizu, M.Shinohara, K.Suda, D.Suzuki, Y.Takahashi, A.Tamii, K.Yako, M.Yamaguchi

Elastic Scattering of Neutron-Rich Helium Isotopes from Polarized Protons at 71 MeV/A

NUCLEAR REACTIONS 1H(6He, 6He), (8He, 8He), E=71 MeV/nucleon; measured polarized target Ep, Ip using SWDCs drift chambers and CsI(Tl), E(He), I(He), (He)p-coin; calculated σ(θ), analyzing power using optical model; deduced σ(θ), analyzing power, optical model parameters. Compared with published data with α and with 6Li.

doi: 10.1088/1742-6596/312/4/082037
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2010EB01      Phys.Rev. C 82, 034306 (2010)

S.Ebata, T.Nakatsukasa, T.Inakura, K.Yoshida, Y.Hashimoto, K.Yabana

Canonical-basis time-dependent Hartree-Fock-Bogoliubov theory and linear-response calculations

NUCLEAR STRUCTURE 20,22,24,26,28,30,32Ne, 24,26,28,30,32,34,36,38,40Mg; calculated quadrupole deformation parameters, pairing gaps, chemical potentials, E1 and isoscalar quadrupole strength distributions, photoabsorption cross sections from equations derived from canonical-basis (Cb) formulation of the time-dependent Hartree-Fock-Bogoliubov (TDHFB) theory.

doi: 10.1103/PhysRevC.82.034306
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2010KO17      Phys.Lett. B 690, 245 (2010)

Y.Kondo, T.Nakamura, Y.Satou, T.Matsumoto, N.Aoi, N.Endo, N.Fukuda, T.Gomi, Y.Hashimoto, M.Ishihara, S.Kawai, M.Kitayama, T.Kobayashi, Y.Matsuda, N.Matsui, T.Motobayashi, T.Nakabayashi, T.Okumura, H.J.Ong, T.K.Onishi, K.Ogata, H.Otsu, H.Sakurai, S.Shimoura, M.Shinohara, T.Sugimoto, S.Takeuchi, M.Tamaki, Y.Togano, Y.Yanagisawa

Low-lying intruder state of the unbound nucleus 13Be

NUCLEAR REACTIONS 1H(14Be, X)13Be, E=69 MeV/nucleon; measured reaction fragments; deduced σ, σ(E), p- and d-wave resonance energies and widths, J, π. Comparison with shell model calculations.

doi: 10.1016/j.physletb.2010.05.031
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2173. Data from this article have been entered in the XUNDL database. For more information, click here.


2010SA25      Nucl.Phys. A834, 404c (2010)

Y.Satou, T.Nakamura, N.Fukuda, T.Sugimoto, Y.Kondo, N.Matsui, Y.Hashimoto, T.Nakabayashi, Y.Okumura, M.Shinohara, T.Motobayashi, Y.Yanagisawa, N.Aoi, S.Takeuchi, T.Gomi, Y.Togano, S.Kawai, H.Sakurai, H.J.Ong, T.K.Onishi, S.Shimoura, M.Tamaki, T.Kobayashi, H.Otsu, N.Endo, M.Kitayama, M.Ishihara

Invariant mass spectroscopy of 19, 17C and 14B using proton inelastic and charge-exchange reactions

NUCLEAR REACTIONS 1H(17C, 17C'), (19C, 19C'), E=70 MeV/nucleon; measured Ep, Ip, fragment-spectra; deduced levels, J, π, σ(θ); calculated levels, J, π using shell model with different forces, σ(θ) using DWBA with WBT shell model wave function. 1H(14Be, 14B), E=70 MeV/nucleon; measured Eβ, Iβ, fragment-spectra; deduced low-lying levels, J, π; calculated levels, J, π using shell model, β-decay strength B(GT). Secondary radioactive beams. Inverse kinematics.

doi: 10.1016/j.nuclphysa.2010.01.050
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2010UE01      Phys.Rev. C 82, 021602 (2010)

T.Uesaka, S.Sakaguchi, Y.Iseri, K.Amos, N.Aoi, Y.Hashimoto, E.Hiyama, M.Ichikawa, Y.Ichikawa, S.Ishikawa, K.Itoh, M.Itoh, H.Iwasaki, S.Karataglidis, T.Kawabata, T.Kawahara, H.Kuboki, Y.Maeda, R.Matsuo, T.Nakao, H.Okamura, H.Sakai, Y.Sasamoto, M.Sasano, Y.Satou, K.Sekiguchi, M.Shinohara, K.Suda, D.Suzuki, Y.Takahashi, M.Tanifuji, A.Tamii, T.Wakui, K.Yako, Y.Yamamoto, M.Yamaguchi

Analyzing power for proton elastic scattering from the neutron-rich 6He nucleus

NUCLEAR REACTIONS 1H(6He, 6He), E=71 MeV/nucleon; measured σ(θ), vector analyzing power, polarized proton solid target. Comparison with t-matrix and g-matrix microscopic folding calculations. Discussed α-core distribution in 6He.

doi: 10.1103/PhysRevC.82.021602
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2287.


2009AO01      Phys.Rev.Lett. 102, 012502 (2009)

N.Aoi, E.Takeshita, H.Suzuki, S.Takeuchi, S.Ota, H.Baba, S.Bishop, T.Fukui, Y.Hashimoto, H.J.Ong, E.Ideguchi, K.Ieki, N.Imai, M.Ishihara, H.Iwasaki, S.Kanno, Y.Kondo, T.Kubo, K.Kurita, K.Kusaka, T.Minemura, T.Motobayashi, T.Nakabayashi, T.Nakamura, T.Nakao, M.Niikura, T.Okumura, T.K.Ohnishi, H.Sakurai, S.Shimoura, R.Sugo, D.Suzuki, M.K.Suzuki, M.Tamaki, K.Tanaka, Y.Togano, K.Yamada

Development of Large Deformation in 62Cr

NUCLEAR REACTIONS 1H(60Cr, 60Cr'), E=42 MeV/nucleon; 1H(62Cr, 62Cr'), E=39 MeV/nucleon; measured Eγ, Iγ, γγ, (particle)γ-coin. 60Cr; deduced deformation length. 62Cr; deduced levels, J, π, deformation length.

doi: 10.1103/PhysRevLett.102.012502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2142. Data from this article have been entered in the XUNDL database. For more information, click here.


2009HA45      Eur.Phys.J. A 42, 571 (2009)

Y.Hashimoto, T.Horibata

Tilted axis rotation and t -band in 182Os with the three-dimensional cranked Hartree-Fock-Bogoliubov method

NUCLEAR STRUCTURE 182Os; calculated tilted axis rotational state energies vs angular momenta and tilt angle using 3D cranked HFB model. Comparison with data.

doi: 10.1140/epja/i2009-10837-y
Citations: PlumX Metrics


2009KO02      Phys.Rev. C 79, 014602 (2009)

Y.Kondo, T.Nakamura, Y.Satou, T.Matsumoto, N.Aoi, N.Endo, N.Fukuda, T.Gomi, Y.Hashimoto, M.Ishihara, S.Kawai, M.Kitayama, T.Kobayashi, Y.Matsuda, N.Matsui, T.Motobayashi, T.Nakabayashi, K.Ogata, T.Okumura, H.J.Ong, T.K.Onishi, H.Otsu, H.Sakurai, S.Shimoura, M.Shinohara, T.Sugimoto, S.Takeuchi, M.Tamaki, Y.Togano, Y.Yanagisawa

One-neutron removal reactions of 18C and 19C on a proton target

NUCLEAR REACTIONS 1H(19C, 18C), E=81 MeV/nucleon; 1H(18C, 17C), E=68 MeV/nucleon; measured Eγ, Iγ, σ, (particle)-γ coin, transverse-momentum distributions. 17,18C; deduced levels, J, π. Comparison with continuum-discretized coupled-channel calculations.

doi: 10.1103/PhysRevC.79.014602
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1665.


2009TA08      Phys.Rev. C 79, 054319 (2009)

S.Takeuchi, N.Aoi, T.Motobayashi, S.Ota, E.Takeshita, H.Suzuki, H.Baba, T.Fukui, Y.Hashimoto, K.Ieki, N.Imai, H.Iwasaki, S.Kanno, Y.Kondo, T.Kubo, K.Kurita, T.Minemura, T.Nakabayashi, T.Nakamura, T.Okumura, T.K.Onishi, H.Sakurai, S.Shimoura, R.Sugou, D.Suzuki, M.K.Suzuki, M.Takashina, M.Tamaki, K.Tanaka, Y.Togano, K.Yamada

Low-lying states in 32Mg studied by proton inelastic scattering

NUCLEAR REACTIONS 1H(32Mg, 32Mg'), E=46.5 MeV/nucleon; measured Eγ, Iγ, scattered particle spectra, σ, σ(θ). 32Mg; deduced levels, J, π, deformation lengths, rms radii.Coupled-channel analysis of angular distribution cross sections. 24,26,28,30,32,34Mg; level systematics.

doi: 10.1103/PhysRevC.79.054319
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2147. Data from this article have been entered in the XUNDL database. For more information, click here.


2009TA31      Int.J.Mod.Phys. E18, 2025 (2009)

S.Takeuchi, N.Aoi, H.Baba, T.Kubo, T.Motobayashi, K.Tanaka, K.Yamada, T.Fukui, S.Ota, Y.Hashimoto, Y.Kondo, T.Nakabayashi, T.Nakamura, T.Okumura, K.Ieki, S.Kanno, K.Kurita, R.Sugou, E.Takeshita, Y.Togano, N.Imai, T.Minemura, H.Iwasaki, T.K.Onishi, H.Sakurai, D.Suzuki, H.Suzuki, M.K.Suzuki, S.Shimoura, M.Tamaki

Study of low-lying states in 32Mg

NUCLEAR REACTIONS 1H(32Mg, 32Mg'), E=45.5 MeV/nucleon; measured Eγ, Iγ, γ-γ-coin.; 32Mg deduced level energies, decay and level scheme, J, π, σ(θ), β2. Secondary beam from 40Ar fragmentation.

doi: 10.1142/S0218301309014226
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2147.


2008AO01      Nucl.Phys. A805, 400c (2008)

N.Aoi, H.Suzuki, E.Takeshita, S.Takeuchi, S.Ota, H.Baba, S.Bishop, T.Fukui, Y.Hashimoto, H.J.Ong, E.Ideguchi, K.Ieki, N.Imai, H.Iwasaki, S.Kanno, Y.Kondo, T.Kubo, K.Kurita, K.Kusaka, T.Minemura, T.Motobayashi, T.Nakabayashi, T.Nakamura, T.Nakao, M.Niikura, T.Okumura, T.K.Ohnishi, H.Sakurai, S.Shimoura, R.Sugo, D.Suzuki, M.K.Suzuki, M.Tamaki, K.Tanaka, Y.Togano, K.Yamada

Shape transition observed in neutron-rich pf-shell isotopes studied via proton inelastic scattering

NUCLEAR REACTIONS 1H(58Ti, 58Ti'), (60Cr, 60Cr'), (62Cr, 62Cr'), E≈40 MeV/nucleon; measured Eγ, Iγ, γγ-coin. 58Ti, 60,62Cr deduced levels, J, π, deformation lengths. Inverse kinematics.

doi: 10.1016/j.nuclphysa.2008.02.280
Citations: PlumX Metrics


2008EL02      J.Phys.(London) G35, 014038 (2008)

Z.Elekes, Z.Dombradi, N.Aoi, H.Baba, S.Bishop, K.Demichi, Z.Fulop, J.Gibelin, T.Gomi, H.Hasegawa, Y.Hashimoto, N.Imai, M.Ishihara, N.Iwasa, H.Iwasaki, G.Kalinka, S.Kanno, S.Kawai, T.Kishida, Y.Kondo, A.A.Korsheninnikov, T.Kubo, K.Kurita, M.Kurokawa, N.Matsui, Y.Matsuyama, S.Michimasa, T.Minemura, T.Motobayashi, T.Nakamura, T.Nakao, E.Y.Nikolskii, M.Notani, T.K.Ohnishi, T.Okumura, H.J.Ong, S.Ota, A.Ozawa, A.Perera, A.Saito, H.K.Sakai, H.Sakurai, Y.Satou, S.Shimoura, D.Sohler, T.Sumikama, D.Suzuki, M.Suzuki, H.Takeda, E.Takeshita, S.Takeuchi, M.Tamaki, Y.Togano, K.Yamada, Y.Yanagisawa, K.Yoneda

The study of shell closures in light neutron-rich nuclei

NUCLEAR REACTIONS 1H(28Ne, 27Ne), E≈51.3 MeV/nucleon; 22O(d, p)23O, E=34 MeV/nucleon; measured Eγ, Iγ, cross sections. 27Ne, 23O; deduced levels, J, π, Spectroscopic factors. Compared results to model calculations.

doi: 10.1088/0954-3899/35/1/014038
Citations: PlumX Metrics


2008GU06      Phys.Rev. C 77, 041301 (2008)

L.Guo, J.A.Maruhn, P.-G.Reinhard, Y.Hashimoto

Conservation properties in the time-dependent Hartree Fock theory

NUCLEAR REACTIONS 16O(16O, X), E(cm)=25, 125 MeV; calculated angular momentum. Hartree-Fock calculations.

doi: 10.1103/PhysRevC.77.041301
Citations: PlumX Metrics


2008SA03      Phys.Lett. B 660, 320 (2008)

Y.Satou, T.Nakamura, N.Fukuda, T.Sugimoto, Y.Kondo, N.Matsui, Y.Hashimoto, T.Nakabayashi, T.Okumura, M.Shinohara, T.Motobayashi, Y.Yanagisawa, N.Aoi, S.Takeuchi, T.Gomi, Y.Togano, S.Kawai, H.Sakurai, H.J.Ong, T.K.Onishi, S.Shimoura, M.Tamaki, T.Kobayashi, H.Otsu, Y.Matsuda, N.Endo, M.Kitayama, M.Ishihara

Unbound excited states in 19, 17C

NUCLEAR REACTIONS 1H(19C, 18C), (19C, 16C), (17C, 16C), E=70 MeV/nucleon; measured σ, σ(θ), relative energy spectra. 17,19C deduced level energies, J, π using DWBA analysis.

doi: 10.1016/j.physletb.2008.01.022
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2096. Data from this article have been entered in the XUNDL database. For more information, click here.


2007EL02      Phys.Rev.Lett. 98, 102502 (2007)

Z.Elekes, Zs.Dombradi, N.Aoi, S.Bishop, Zs.Fulop, J.Gibelin, T.Gomi, Y.Hashimoto, N.Imai, N.Iwasa, H.Iwasaki, G.Kalinka, Y.Kondo, A.A.Korsheninnikov, K.Kurita, M.Kurokawa, N.Matsui, T.Motobayashi, T.Nakamura, T.Nakao, E.Yu.Nikolskii, T.K.Ohnishi, T.Okumura, S.Ota, A.Perera, A.Saito, H.Sakurai, Y.Satou, D.Sohler, T.Sumikama, D.Suzuki, M.Suzuki, H.Takeda, S.Takeuchi, Y.Togano, Y.Yanagisawa

Spectroscopic Study of Neutron Shell Closures via Nucleon Transfer in the Near-Dripline Nucleus 23O

NUCLEAR REACTIONS 2H(22O, 23O), E=34 MeV/nucleon; measured excitation energy spectrum. 23O deduced resonance energies, neutron shell features.

doi: 10.1103/PhysRevLett.98.102502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2020. Data from this article have been entered in the XUNDL database. For more information, click here.


2007PA15      J.Radioanal.Nucl.Chem. 272, 243 (2007)

M.Paul, A.Valenta, I.Ahmad, D.Berkovits, C.Bordeanu, S.Ghelberg, Y.Hashimoto, A.Hershkowitz, S.Jiang, T.Nakanishi, K.Sakamoto

An upper limit to interstellar 244Pu abundance as deduced from radiochemical search in deep-sea sediment: An account

doi: 10.1007/s10967-007-0508-3
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2006EL05      Phys.Rev. C 74, 017306 (2006)

Z.Elekes, Zs.Dombradi, N.Aoi, S.Bishop, Zs.Fulop, J.Gibelin, T.Gomi, Y.Hashimoto, N.Imai, N.Iwasa, H.Iwasaki, G.Kalinka, Y.Kondo, A.A.Korsheninnikov, K.Kurita, M.Kurokawa, N.Matsui, T.Motobayashi, T.Nakamura, T.Nakao, E.Yu.Nikolskii, T.K.Ohnishi, T.Okumura, S.Ota, A.Perera, A.Saito, H.Sakurai, Y.Satou, D.Sohler, T.Sumikama, D.Suzuki, M.Suzuki, H.Takeda, S.Takeuchi, Y.Togano, Y.Yanagisawa

Search for neutron decoupling in 22O via the (d, d'γ) reaction

NUCLEAR REACTIONS 2H(22O, 22O'), E=34 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin, σ(E). 22O deduced excited state energy, neutron and proton deformations.

doi: 10.1103/PhysRevC.74.017306
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2006EL06      Eur.Phys.J. A 27, Supplement 1, 321 (2006)

Z.Elekes, Zs.Dombradi, S.Bishop, Zs.Fulop, J.Gibelin, T.Gomi, Y.Hashimoto, N.Imai, N.Iwasa, H.Iwasaki, G.Kalinka, Y.Kondo, A.A.Korsheninnikov, K.Kurita, M.Kurokawa, N.Matsui, T.Motobayashi, T.Nakamura, T.Nakao, E.Yu.Nikolskii, T.K.Ohnishi, T.Okumura, S.Ota, A.Perera, A.Saito, H.Sakurai, Y.Satou, D.Sohler, T.Sumikama, D.Suzuki, M.Suzuki, H.Takeda, S.Takeuchi, Y.Togano, Y.Yanagisawa

Testing of the RIKEN-ATOMKI CsI(Tl) array in the study of 22, 23O nuclear structure

NUCLEAR REACTIONS 2H, C(22O, 22O'), E=34 MeV/nucleon; measured Eγ, Iγ. 22O deduced transition.

doi: 10.1140/epja/i2006-08-049-x
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2006HA27      Phys.Rev. C 74, 017301 (2006)

Y.Hashimoto, T.Horibata

Stability of s-band states in the tilting calculation of 182Os

NUCLEAR STRUCTURE 182Os; calculated rotational bands energies, configurations, stability. Three-dimensional cranking calculations, HFB framework.

doi: 10.1103/PhysRevC.74.017301
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2006IN01      Nucl.Phys. A768, 61 (2006)

T.Inakura, H.Imagawa, Y.Hashimoto, S.Mizutori, M.Yamagami, K.Matsuyanagi

Mixed representation RPA calculation for octupole excitations on superdeformed states in the 40Ca and neutron-rich sulfur regions

NUCLEAR STRUCTURE 32,36,48,50S, 36Ar, 40Ca, 44Ti; calculated energy, J, octupole transition strengths for low-frequency negative-parity excitations built on superdeformed states. Self-consistent RPA approach, comparison with other models.

doi: 10.1016/j.nuclphysa.2006.01.008
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2006TA31      J.Phys.:Conf.Ser. 49, 153 (2006)

S.Takeuchi, N.Aoi, H.Baba, T.Fukui, Y.Hashimoto, K.Ieki, N.Imai, H.Iwasaki, S.Kanno, Y.Kondo, T.Kubo, K.Kurita, T.Minemura, T.Motobayashi, T.Nakabayashi, T.Nakamura, T.Okumura, T.K.Onishi, S.Ota, H.Sakurai, S.Shimoura, R.Sugou, D.Suzuki, H.Suzuki, M.K.Suzuki, E.Takeshita, M.Tamaki, K.Tanaka, Y.Togano, K.Yamada

Proton inelastic scattering on 32Mg

NUCLEAR REACTIONS H(32Mg, 32Mg'), E=57 MeV/nucleon; measured reaction products, Eγ, Iγ. 32Mg; deduced σ(θ), level energies, J, π, angular momentum. Comparison with DWBA calculations, 40Ar secondary beams.

doi: 10.1088/1742-6596/49/1/033
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2005HA52      Prog.Theor.Phys.(Kyoto) 114, 595 (2005)

Y.Hashimoto, Y.Tsue, H.Fujii

Effective Potential Study of the Chiral Phase Transition in a QCD-Like Theory

doi: 10.1143/PTP.114.595
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2005IN02      Eur.Phys.J. A 25, Supplement 1, 545 (2005)

T.Inakura, H.Imagawa, Y.Hashimoto, M.Yamagami, S.Mizutori, K.Matsuyanagi

Soft octupole vibrations on superdeformed states in nuclei around 40Ca suggested by Skyrme-HF and self-consistent RPA calculations

NUCLEAR STRUCTURE 32S, 36Ar, 40Ca, 44Ti; calculated energy, J for low-frequency negative-parity excitations built on superdeformed states. Self-consistent RPA approach.

doi: 10.1140/epjad/i2005-06-111-4
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2004IN01      Int.J.Mod.Phys. E13, 157 (2004)

T.Inakura, M.Yamagami, K.Matsuyanagi, S.Mizutori, H.Imagawa, Y.Hashimoto

Static and dynamic non-axial octupole deformations suggested by Skyrme-HF and selfconsistent RPA calculations

NUCLEAR STRUCTURE 32,34,36,38,40,42,44,46,48,50S, 36Ar, 40Ca, 44Ti, 48Cr; calculated deformation energy curves. 32,36,48,50S; calculated levels, J, π, transition matrix elements. Skyrme-Hartree-Fock and RPA calculations.

doi: 10.1142/S0218301304001886
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2003IM01      Phys.Rev. C 67, 037302 (2003)

H.Imagawa, Y.Hashimoto

Accurate random-phase approximation calculation of low-lying states on a three-dimensional Cartesian mesh

NUCLEAR STRUCTURE 16O, 208Pb; calculated first 3- states energies, transitions B(E3). Hartree-Fock, RPA, Skyrme interaction.

doi: 10.1103/PhysRevC.67.037302
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2003KO29      Phys.Rev. C 67, 054316 (2003)

T.Kohmura, M.Maruyama, Y.Hashimoto

Nuclear collective tunneling between Hartree states

NUCLEAR STRUCTURE 28Si; calculated collective tunneling probability between Hartree states. Adiabatic collective tunneling approximation.

doi: 10.1103/PhysRevC.67.054316
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2003PA37      Nucl.Phys. A719, 29c (2003)

M.Paul, A.Valenta, I.Ahmad, D.Berkovits, C.Bordeanu, S.Ghelberg, Y.Hashimoto, A.Hershkowitz, S.Jiang, T.Nakanishi, K.Sakamoto

A window on nucleosynthesis through detection of short-lived radionuclides

doi: 10.1016/S0375-9474(03)00954-0
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2002KO03      Prog.Theor.Phys.(Kyoto) 107, 87 (2002)

T.Kohmura, M.Maruyama, H.Ohta, Y.Hashimoto

Projection Operator Method for Collective Tunneling Transitions

doi: 10.1143/PTP.107.87
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2002MU20      Prog.Theor.Phys.(Kyoto) 108, 1065 (2002)

A.Muta, J.-I.Iwata, Y.Hashimoto, K.Yabana

Solving the RPA Eigenvalue Equation in Real-Space

NUCLEAR STRUCTURE 16O, 20Ne; calculated level energies. Computational method for solution of RPA eigenvalue equation.

doi: 10.1143/PTP.108.1065
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2001SA45      Prog.Theor.Phys.(Kyoto), Suppl. 141, 1 (2001)

F.Sakata, T.Marumori, Y.Hashimoto, S.-W.Yan

Nonlinear Dynamics of Nuclear Collective Motion

doi: 10.1143/PTPS.141.1
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2000KO13      Phys.Rev. C61, 034315 (2000)

T.Kohmura, Y.Hashimoto, H.Ohta, M.Maruyama

Adiabatic Mean-Field Model for Dynamical Collective State Transitions of a Nuclear System

doi: 10.1103/PhysRevC.61.034315
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1998TS16      Prog.Theor.Phys.(Kyoto) 100, 1203 (1998)

H.Tsukuma, Y.Hashimoto, F.Sakata, K.Iwasawa

Bifurcation Structure of Eigenstates and Periodic Trajectories in TDHF Phase Space - Weak Nonlinearity Case in SU(3) Model -

doi: 10.1143/PTP.100.1203
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1997KU05      Nucl.Phys. A616, 11c (1997)

S.Kubono, T.Nomura, S.Arai, Y.Arakaki, Y.Hashimoto, A.Imanishi, S.C.Jeong, I.Katayama, T.Katayama, H.Kawakami, H.Masuda, T.Miyachi, K.Niki, M.Okada, M.Oyaizu, Y.Shirakabe, P.Strasser, Y.Takeda, J.Tanaka, M.H.Tanaka, E.Tojyo, N.Tokuda, M.Tomizawa, M.Wada, K.Yoshida, M.Yoshizawa, M.Fujioka, S.Kato, T.Shinozuka, H.Wollnik

New ISOL-Based Radioactive Nuclear Beam Facility at INS

doi: 10.1016/S0375-9474(97)00069-9
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1994IW05      Prog.Theor.Phys.(Kyoto) 92, 1119 (1994)

K.Iwasawa, F.Sakata, Y.Hashimoto, J.Terasaki

New Algorithm for Hartree-Fock Variational Equation

NUCLEAR STRUCTURE 82Sr; calculated single proton level energies. Self-consistent Hartree-Fock, new algorithm.

doi: 10.1143/ptp/92.6.1119
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1994SA22      Phys.Rev. C50, 138 (1994)

F.Sakata, T.Kubo, T.Marumori, K.Iwasawa, Y.Hashimoto

Nonlinear Resonance in the Time-Dependent Hartree-Fock Manifold

doi: 10.1103/PhysRevC.50.138
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1990SH33      J.Phys.Soc.Jpn. 59, 2522 (1990)

K.Shimizu, Y.Hashimoto

159Tb NMR in TbNi3 and Related Compounds

NUCLEAR MOMENTS 159Tb; measured NMR; deduced Tb magnetic moment in TbNi3.

doi: 10.1143/JPSJ.59.2522
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1981TA04      Phys.Rev. C23, 1305 (1981)

N.Takahashi, Y.Hashimoto, Y.Iwasaki, K.Sakurai, F.Soga, K.Sagara, Y.Yano, M.Sekiguchi

Nuclear Structure of 26Al Studied by Two-Nucleon Transfer Reaction 28Si(d, α) and 24Mg(3He, p)

NUCLEAR REACTIONS 28Si(d, α), E=33 MeV; 24Mg(3He, p), E=27.5 MeV; measured σ(Eα, θ), σ(Ep, θ). 26Al deduced levels, L, J, π. Enriched targets. DWBA analysis, Nilsson model, pairing correlations, spherical nucleus, simple pairing.

doi: 10.1103/PhysRevC.23.1305
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1979GI03      Nucl.Phys. A317, 313 (1979)

W.M.Gibson, M.Maruyama, Y.Hashimoto, E.P.Kanter, G.M.Temmer, R.J.Keddy, D.W.Mingay, J.P.F.Sellschop

Application of the Crystal Blocking Technique to the Study of the Highly Excited Nuclear Continuum

NUCLEAR REACTIONS 70,72,74Ge(p, p), (p, p'), E=5.035, 5.110 MeV; measured σ(E;Ep', θ=89-91°). 71,73,75As deduced reaction times, < Γ > , enhancement due to IAS, final-state spin effect, level-density effect on reaction time. Natural single crystal target.

doi: 10.1016/0375-9474(79)90485-8
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1978SA07      Nucl.Phys. A299, 77 (1978)

K.Sagara, T.Motobayashi, N.Takahashi, Y.Hashimoto, M.Hara, Y.Nogami, H.Nakamura, H.Noya

Measurement and Semi-Phenomenological Analysis of the 2H(α, pα)n Reaction at 18 MeV

NUCLEAR REACTIONS 2H(α, pα), E=18 MeV; measured σ(Ep, θ(p), θ(α)). Enriched target.

doi: 10.1016/0375-9474(78)90209-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0078.


1977SO10      Nucl.Phys. A288, 504 (1977)

F.Soga, Y.Hashimoto, N.Takahashi, Y.Iwasaki, K.Sakurai, S.Kohmoto, Y.Nogami

Proton Inelastic Scattering from 110Cd and 112Cd at Isobaric Analog Resonances and Analysis with the Quasiparticle Random-Phase Approximation

NUCLEAR REACTIONS 110Cd(p, p), (p, p'), E=5.8-8.1 MeV; 112Cd(p, p), (p, p'), E=6.1-8.4 MeV; measured σ(θ). 111,113In deduced IAS, L, Γ, Γp, S, spectroscopic amplitudes. RPA analysis. Enriched targets.

doi: 10.1016/0375-9474(77)90347-5
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1976SA29      Nucl.Phys. A273, 493 (1976)

K.Sagara, T.Motobayashi, N.Takahashi, Y.Hashimoto, M.Hara, Y.Nogami, H.Noya, H.Nakamura

A Study of the n-p Final State Interaction in the 2H(α, pα)n Reaction at 18 MeV

NUCLEAR REACTIONS 2H(α, pα), E=18 MeV; measured σ(Ep, θ(p), θ(α)); deduced n-p final state interaction. Enriched target.

doi: 10.1016/0375-9474(76)90606-0
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1972GI08      Phys.Rev.Lett. 29, 74 (1972)

M.W.Gibson, Y.Hashimoto, R.J.Keddy, M.Maruyama, G.M.Temmer

Effects of Isobaric-Analog Resonances on the Mean Lifetimes of Compound-Nucleus Fine Structure by Crystal Blocking in Germanium

NUCLEAR REACTIONS Ge(p, p), (p, p'), E=5.005, 5.110 MeV; measured crystal blocking effect; deduced compound-nucleus T1/2. 72Ge(p, p'), E=4.9-5.2 MeV; measured σ(E). 73As deduced isobaric analog resonance, L, J, π.

doi: 10.1103/PhysRevLett.29.74
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2710.


1965OH01      Nucl.Phys. 66, 337 (1965)

H.Ohnuma, Y.Hashimoto, I.Tomita

Nuclear Levels of 56Co from the Decay of 56Ni

RADIOACTIVITY 56Ni, 57Ni[from Fe(α, 2n)]; measured Iγ, Eγ, γγ-coin, γγ(θ), I(ce), E(ce), ICC. 56Co deduced levels, J, π, γ-multipolarities. Natural target.

doi: 10.1016/0029-5582(65)90181-1
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1964EJ02      Nucl.Phys. 52, 561 (1964)

H.Ejiri, H.Ohmura, Y.Nakajima, K.Horie, Y.Hashimoto, K.Etoh, S.Matsumoto, Y.Nogami

Excited States in 29P by the Reaction 28Si(p, γ)29P

NUCLEAR STRUCTURE 29P; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(64)90716-3
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1963NO05      INSJ-60 (1963)

I.Nonaka, T.Mikumo, H.Yamaguchi, M.Odera, Y.Hashimoto, M.Kondo, T.Maki

Numerical Differential Cross Sections of the Scattering of Alpha Particles

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.


1962YA02      J.Phys.Soc.Japan 17, 1223 (1962)

T.Yamazaki, H.Ohnuma, Y.Hashimoto, M.Fujioka, E.Takekoshi, A.Hashizume, H.Ikegami, M.Sakai

New Radioactivity 43-min Yttrium-84

NUCLEAR STRUCTURE 85Y, 84Y; measured not abstracted; deduced nuclear properties.

doi: 10.1143/JPSJ.17.1223
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1962YA03      J.Phys.Soc.Japan 17, 595 (1962)

K.Yagi, K.Katori, H.Ohnuma, Y.Hashimoto, Y.Nogami

NUCLEAR REACTIONS 18O(p, p), E=600-1450 keV; measured reaction products. 19F; deduced levels, J, π, nuclear properties, σ(θ).

doi: 10.1143/JPSJ.17.595
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1976.


1960MI03      J.Phys.Soc.Japan 15, 1158 (1960)

T.Mikumo, H.Yamaguchi, I.Nonaka, M.Odera, Y.Hashimoto, M.Kondo, T.Maki

Elastic and Inelastic Scattering of Alpha Particles by Carbon

NUCLEAR STRUCTURE 12C, 16O; measured not abstracted; deduced nuclear properties.

doi: 10.1143/JPSJ.15.1158
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1944.


1959HA17      Phys.Rev. 116, 981 (1959)

Y.Hashimoto, W.P.Alford

Violation of the Isotopic Spin Selection Rule in the Ca40(d, α)K38 Reaction

doi: 10.1103/PhysRev.116.981
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