NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = K.Sato Found 104 matches. Showing 1 to 100. [Next]2022AB17 Phys.Lett. B 833, 137355 (2022) K.Abe, K.Hiraide, K.Ichimura, N.Kato, Y.Kishimoto, K.Kobayashi, M.Kobayashi, S.Moriyama, M.Nakahata, K.Sato, H.Sekiya, T.Suzuki, A.Takeda, S.Tasaka, M.Yamashita, B.S.Yang, N.Y.Kim, Y.D.Kim, Y.H.Kim, R.Ishii, Y.Itow, K.Kanzawa, K.Masuda, K.Martens, A.Mason, Y.Suzuki, K.Miuchi, Y.Takeuchi, K.B.Lee, M.K.Lee, Y.Fukuda, H.Ogawa, K.Nishijima, K.Fushimi, B.D.Xu, S.Nakamura, for the XMASS Collaboration Search for neutrinoless quadruple beta decay of 136Xe in XMASS-I RADIOACTIVITY 136Xe(4β-); measured decay products, Eβ, Iβ, Eγ, Iγ; deduced T1/2 lower limit. The liquid-xenon detector XMASS-I.
doi: 10.1016/j.physletb.2022.137355
2020KI05 Phys.Rev.Lett. 124, 252501 (2020) M.H.Kim, O.Adriani, E.Berti, L.Bonechi, R.D'Alessandro, Y.Goto, B.Hong, Y.Itow, K.Kasahara, J.H.Lee, T.Ljubicic, Y.Makino, H.Menjo, I.Nakagawa, A.Ogawa, J.S.Park, T.Sako, N.Sakurai, K.Sato, R.Seidl, K.Tanida, S.Torii, A.Tricomi, M.Ueno, Q.D.Zhou for the RHICf Collaboration Transverse Single-Spin Asymmetry for Very Forward Neutral Pion Production in Polarized p + p Collisions at √ s = 510 GeV NUCLEAR REACTIONS 1H(polarized p, X)π0, E ∼ 510 GeV; measured reaction products, Eγ, Iγ; deduced transverse single-spin asymmetries.
doi: 10.1103/PhysRevLett.124.252501
2019SA48 Prog.Theor.Exp.Phys. 109, 101D01 (2019) K.Sato, T.Furumoto, Y.Kikuchi, K.Ogata, Y.Sakuragi Large-amplitude quadrupole shape mixing probed by the (p, p') reaction: A model analysis NUCLEAR REACTIONS 154Sm(p, p'), E=35, 65, 66.5 MeV; calculated σ(θ). Comparison with experimental results.
doi: 10.1093/ptep/ptz095
2019SU05 Astropart.Phys. 110, 1 (2019) T.Suzuki, K.Abe, K.Hiraide, K.Ichimura, Y.Kishimoto, K.Kobayashi, M.Kobayashi, S.Moriyama, M.Nakahata, H.Ogawa, K.Sato, H.Sekiya, A.Takeda, S.Tasaka, M.Yamashita, B.S.Yang, N.Y.Kim, Y.D.Kim, Y.Itow, K.Kanzawa, K.Masuda, K.Martens, Y.Suzuki, B.D.Xu, K.Miuchi, N.Oka, Y.Takeuchi, Y.H.Kim, K.B.Lee, M.K.Lee, Y.Fukuda, M.Miyasaka, K.Nishijima, K.Fushimi, G.Kanzaki, S.Nakamura, for the XMASS Collaboration Search for WIMP-129Xe inelastic scattering with particle identification in XMASS-I
doi: 10.1016/j.astropartphys.2019.02.007
2017BA09 Acta Phys.Pol. B48, 259 (2017) P.Baczyk, J.Dobaczewski, M.Konieczka, T.Nakatsukasa, K.Sato, W.Satula Mirror and Triplet Displacement Energies Within Nuclear DFT: Numerical Stability
doi: 10.5506/APhysPolB.48.259
2016MA10 J.Phys.(London) G43, 024006 (2016) K.Matsuyanagi, M.Matsuo, T.Nakatsukasa, K.Yoshida, N.Hinohara, K.Sato Microscopic derivation of the quadrupole collective Hamiltonian for shape coexistence/mixing dynamics NUCLEAR STRUCTURE 72Kr, 30,32,34Mg; calculated potential energy surfaces, J, π, energy levels. Large-amplitude collective motions (LACM).
doi: 10.1088/0954-3899/43/2/024006
2016MA71 Phys.Scr. 91, 063014 (2016) K.Matsuyanagi, M.Matsuo, T.Nakatsukasa, K.Yoshida, N.Hinohara, K.Sato Microscopic derivation of the Bohr-Mottelson collective Hamiltonian and its application to quadrupole shape dynamics
doi: 10.1088/0031-8949/91/6/063014
2015SA52 Prog.Theor.Exp.Phys. 2015, 123D01 (2015) Gauge symmetry in the large-amplitude collective motion of superfluid nuclei
doi: 10.1093/ptep/ptv163
2014MA98 Phys.Scr. 89, 054020 (2014) M.Matsuo, N.Hinohara, K.Sato, K.Matsuyanagi, T.Nakatsukasa, K.Yoshida Quadrupole shape dynamics from the viewpoint of a theory of large-amplitude collective motion NUCLEAR STRUCTURE 58,60,62,64,66Cr; calculated low-lying quadrupole shape dynamics using large-scale collective motion; deduced deformation, shape-coexistence, shape-mixing, shape-transitional behavior, B(E2). Partially compared with data.
doi: 10.1088/0031-8949/89/5/054020
2014SH11 Phys.Rev. C 89, 054317 (2014) J.A.Sheikh, N.Hinohara, J.Dobaczewski, T.Nakatsukasa, W.Nazarewicz, K.Sato Isospin-invariant Skyrme energy-density-functional approach with axial symmetry NUCLEAR STRUCTURE A=78, 48, 40; calculated total Hartree-Fock (HF) energy, single-particle energies and Routhians with and without isospin-symmetry-breaking Coulomb term, neutron and proton rms radii for isobaric analog chains. 78Ni, 78Zn, 78Ge, 78Se, 78Kr, 78Sr, 78Zr, 78Mo, 78Ru, 78Pd, 78Cd, 78Sn; calculated g9/2 proton effective HF potential, rms radii, single-particle energies. binding energy. Extension of existing axial DFT solver HFBTHO to isospin-invariant Skyrme EDF approach with all possible p-n (isospin) mixing terms. Comparison between HFODD and HFBTHO results.
doi: 10.1103/PhysRevC.89.054317
2014TA32 Phys.Rev. C 90, 061305 (2014) M.Takechi, S.Suzuki, D.Nishimura, M.Fukuda, T.Ohtsubo, M.Nagashima, T.Suzuki, T.Yamaguchi, A.Ozawa, T.Moriguchi, H.Ohishi, T.Sumikama, H.Geissel, N.Aoi, R.-J.Chen, D.-Q.Fang, N.Fukuda, S.Fukuoka, H.Furuki, N.Inabe, Y.Ishibashi, T.Itoh, T.Izumikawa, D.Kameda, T.Kubo, M.Lantz, C.S.Lee, Y.-G.Ma, K.Matsuta, M.Mihara, S.Momota, D.Nagae, R.Nishikiori, T.Niwa, T.Ohnishi, K.Okumura, M.Ohtake, T.Ogura, H.Sakurai, K.Sato, Y.Shimbara, H.Suzuki, H.Takeda, S.Takeuchi, K.Tanaka, M.Tanaka, H.Uenishi, M.Winkler, Y.Yanagisawa, S.Watanabe, K.Minomo, S.Tagami, M.Shimada, M.Kimura, T.Matsumoto, Y.R.Shimizu, M.Yahiro Evidence of halo structure in 37Mg observed via reaction cross sections and intruder orbitals beyond the island of inversion NUCLEAR REACTIONS 12C(24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), E=240 MeV/nucleon, [secondary Mg beams from 9Be(48Ca, X), E=345 MeV/nucleon primary reaction]; measured spectra and TOF of outgoing particles, precise reaction σ using BigRIPS spectrometer at RIBF-RIKEN facility. Comparison with theoretical deformation parameter β2 versus mass plot using double-folding model (DFM) calculation combined with antisymmetrized molecular dynamics (AMD) calculation. 37Mg; deduced deformed halo effect from observed enhanced cross section, comparison with DFM calculation based on the deformed Woods-Saxon (DWS) model; collapse of N=28 magic shell for neutrons.
doi: 10.1103/PhysRevC.90.061305
2013SA59 Phys.Rev. C 88, 061301 (2013) K.Sato, J.Dobaczewski, T.Nakatsukasa, W.Satula Energy-density-functional calculations including proton-neutron mixing NUCLEAR STRUCTURE A=14, 40-56; 48Cr; calculated single particle Routhians, IAS, isospin states using Skyrme energy density functional including mixing between protons and neutrons, high-isospin states in 48Cr using augmented Lagrange method.
doi: 10.1103/PhysRevC.88.061301
2012HI08 Prog.Theor.Phys.(Kyoto), Suppl. 196, 328 (2012) N.Hinohara, K.Sato, K.Yoshida, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Microscopic Analysis of Shape Coexistence/Mixing and Shape Phase Transition in Neutron-Rich Nuclei around 32Mg NUCLEAR STRUCTURE 30,32,34,36Mg; analyzed quadrupole dynamics data; deduced enhancement of the quadrupole collectivity using collective Hamiltonian approach.
doi: 10.1143/PTPS.196.328
2012SA33 Phys.Rev. C 86, 024316 (2012) K.Sato, N.Hinohara, K.Yoshida, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Shape transition and fluctuations in neutron-rich Cr isotopes around N=40 NUCLEAR STRUCTURE 58,60,62,64,66Cr; calculated potential energy surface contours in β-γ plane, levels, B(E2), vibrational wave functions contours, E0 transition strengths. Solution of Schrodinger equation for five-dimensional quadrupole collective Hamiltonian, with constrained Hartree-Fock-Bogoliubov plus local quasiparticle random-phase approximation (CHFB+LQRPA) method. Large-amplitude shape fluctuations in low-lying states. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.024316
2012SA63 J.Phys.:Conf.Ser. 381, 012103 (2012) K.Sato, N.Hinohara, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Microscopic approach to large-amplitude deformation dynamics with local QRPA inertial masses NUCLEAR STRUCTURE 72Kr; calculated levels, J, π, deformation, B(E2) using CHFB (constrained HFB) + LQRPA (local QRPA). 58,60,62,64Cr; calculated levels, J, π, deformation, spectroscopic quadrupole moment, B(E2) using CHFB.
doi: 10.1088/1742-6596/381/1/012103
2011HI03 Acta Phys.Pol. B42, 443 (2011) N.Hinohara, K.Sato, T.Nakatsukasa, M.Matsuo Local QRPA Vibrational and Rotational Inertial Functions for Large-amplitude Quadrupole Collective Dynamics NUCLEAR STRUCTURE 68,76Se; calculated collective potential, energies, J, π. Comparison with experimental data.
doi: 10.5506/APhysPolB.42.443
2011HI18 Phys.Rev. C 84, 061302 (2011) N.Hinohara, K.Sato, K.Yoshida, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Shape fluctuations in the ground and excited 0+ states of 30, 32, 34Mg NUCLEAR STRUCTURE 30,32,34,36Mg; calculated collective potential surfaces, levels, J, π, B(E2) values for low-lying positive-parity states, vibrational wave functions. Five-dimensional (5D) quadrupole collective Schrodinger equation, constrained Hartree-Fock-Bogoliubov plus local quasiparticle random phase approximation. Ground and excited 0+ states. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.061302
2011KO02 J.Nucl.Sci.Technol.(Tokyo) 48, 227 (2011) K.Kosako, K.Oishi, T.Nakamura, M.Takada, K.Sato, T.Kamiyama, Y.Kiyanagi Angular Distribution of Photoneutrons from Copper and Tungsten Targets Bombarded by 18, 28, and 38 MeV Electrons NUCLEAR REACTIONS Cu, W(γ, n), E=18, 28, 38 MeV; measured reaction activation products, Eγ, Iγ; deduced photoneutron σ(E), σ(θ). Comparison with experimental data, MCNP5 and JENDL-3.3 library.
doi: 10.3327/jnst.48.227
2011SA09 Nucl.Phys. A849, 53 (2011) Shape mixing dynamics in the low-lying states of proton-rich Kr isotopes NUCLEAR STRUCTURE 72,74,76Kr; calculated levels, J, π, B(E2), deformation parameters and related properties using a 5-D quadrupole collective Hamiltonian. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.11.003
2011SA69 J.Phys.:Conf.Ser. 312, 092054 (2011) Microscopic analysis of shape mixing in low-lying states of proton-rich nuclei in the Se-Kr region NUCLEAR STRUCTURE 72,74,76Kr; calculated deformation, potential energy, moment of inertia, quadrupole moment. 72Kr; calculated levels, J, π, γ transitions, B(E2). CHFB (constrained HFB) + LQRPA (local QRPA). Compared to available data.
doi: 10.1088/1742-6596/312/9/092054
2011WA26 Phys.Lett. B 704, 270 (2011) H.Watanabe, K.Yamaguchi, A.Odahara, T.Sumikama, S.Nishimura, K.Yoshinaga, Z.Li, Y.Miyashita, K.Sato, L.Prochniak, H.Baba, J.S.Berryman, N.Blasi, A.Bracco, F.Camera, J.Chiba, P.Doornenbal, S.Go, T.Hashimoto, S.Hayakawa, C.Hinke, N.Hinohara, E.Ideguchi, T.Isobe, Y.Ito, D.G.Jenkins, Y.Kawada, N.Kobayashi, Y.Kondo, R.Krucken, S.Kubono, G.Lorusso, T.Nakano, T.Nakatsukasa, M.Kurata-Nishimura, H.J.Ong, S.Ota, Zs.Podolyak, H.Sakurai, H.Scheit, K.Steiger, D.Steppenbeck, K.Sugimoto, K.Tajiri, S.Takano, A.Takashima, T.Teranishi, Y.Wakabayashi, P.M.Walker, O.Wieland, H.Yamaguchi Development of axial asymmetry in the neutron-rich nucleus 110Mo RADIOACTIVITY 110Nb(β-) [from Be(238U, X), E=345 MeV/nucleon]; measured decay products, Eγ, Iγ, X-rays. 110Mo; deduced energy levels, J, π, quasi-γ-band state, B(e2) ratio. Comparison with general Bohr Hamiltonian method calculations, systematics of low-lying levels of even-even Mo nuclei. NUCLEAR STRUCTURE 104,106,108,110Mo; calculated moments of inertia, potential energy surface, the nuclear landscape. General Bohr Hamiltonian method calculations.
doi: 10.1016/j.physletb.2011.09.050
2010HI09 Phys.Rev. C 82, 064313 (2010) N.Hinohara, K.Sato, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi Microscopic description of large-amplitude shape-mixing dynamics with inertial functions derived in local quasiparticle random-phase approximation NUCLEAR STRUCTURE 68,70,72Se; calculated, in β-γ plane, collective potential surfaces, monopole and quadrupole pairing gaps, vibrational masses, rotational masses, vibrational wave functions, B(E2), excitation energies, and spectroscopic quadrupole moments using constrained Hartree-Fock-Bogoliubov (CHFB) and local quasiparticle random-phase approximation (LQRPA) based on adiabatic self-consistent collective coordinate (ASCC) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.064313
2010SA01 Prog.Theor.Phys.(Kyoto) 123, 129 (2010) K.Sato, N.Hinohara, T.Nakatsukasa, M.Matsuo, K.Matsuyanagi A Model Analysis of Triaxial Deformation Dynamics in Oblate-Prolate Shape Coexistence Phenomena
doi: 10.1143/PTP.123.129
2009SA32 Nucl.Phys. A826, 74 (2009) Spontaneous magnetization in QCD and non-Fermi-liquid effects
doi: 10.1016/j.nuclphysa.2009.05.005
2008SO03 Phys.Rev. C 77, 035806 (2008), Erratum Phys.Rev. C 81, 049902 (2010) H.Sonoda, G.Watanabe, K.Sato, K.Yasuoka, T.Ebisuzaki Phase diagram of nuclear "pasta" and its uncertainties in supernova cores NUCLEAR STRUCTURE 56Fe, 90Zr, 208Pb, 238U; calculated binding energies, central nucleon density, surface diffusiveness parameters, surface tension, nucleon distributions, phase diagrams. Quantum-molecular dynamics (QMD) model.
doi: 10.1103/PhysRevC.77.035806
2007SO08 Phys.Rev. C 75, 042801 (2007) H.Sonoda, G.Watanabe, K.Sato, T.Takiwaki, K.Yasuoka, T.Ebisuzaki Impact of nuclear "pasta" on neutrino transport in collapsing stellar cores
doi: 10.1103/PhysRevC.75.042801
2004WA15 Phys.Rev. C 69, 055805 (2004), Erratum Phys.Rev. C 81, 049901 (2010) G.Watanabe, K.Sato, K.Yasuoka, T.Ebisuzaki Phases of hot nuclear matter at subnuclear densities
doi: 10.1103/PhysRevC.69.055805
2003AN31 Nucl.Phys. A721, 541c (2003) Detectability of the Supernova Relic Neutrinos
doi: 10.1016/S0375-9474(03)01119-9
2003KO48 Nucl.Phys. A718, 629c (2003) K.Kotake, S.Yamada, K.Sato, T.M.Shimizu Gravitational Collapse of Rotating Massive Stars
doi: 10.1016/S0375-9474(03)00906-0
2003NA23 Nucl.Phys. A718, 437c (2003) S.Nagataki, K.Kohri, S.Ando, K.Sato Gamma-ray burst neutrino background and star formation history in the universe
doi: 10.1016/S0375-9474(03)00824-8
2003TA23 Nucl.Phys. A718, 455c (2003) Effects of neutrino oscillation on supernova neutrino: inverted mass hierarchy
doi: 10.1016/S0375-9474(03)00850-9
2003WA17 Phys.Rev. C 68, 035806 (2003) G.Watanabe, K.Sato, K.Yasuoka, T.Ebisuzaki Structure of cold nuclear matter at subnuclear densities by quantum molecular dynamics
doi: 10.1103/PhysRevC.68.035806
2003WA22 Nucl.Phys. A718, 700c (2003) G.Watanabe, K.Sato, K.Yasuoka, T.Ebisuzaki Microscopic study of nuclear "pasta": Quantum molecular dynamics approach
doi: 10.1016/S0375-9474(03)00893-5
2002II01 Prog.Theor.Phys.(Kyoto), Suppl. 146, 514 (2002) Formation of Nuclear "Pasta" in Cold Neutron Star Matter
doi: 10.1143/PTPS.146.514
2002MA41 Nucl.Phys. A701, 383c (2002) K.Matsuta, T.Tsubota, C.Ha, T.Miyake, M.Sasaki, K.Sato, K.Minamisono, K.Tanaka, S.Kaminaka, A.Takemura, T.Sumikama, T.Nagatomo, K.Hashimoto, M.Mihara, M.Fukuda, T.Minamisono, T.Ohtsubo, Y.Nojiri, S.Momota, A.Kitagawa, M.Torikoshi, M.Kanazawa, S.Koda, T.Nishio, M.Suda, J.R.Alonso, G.F.Krebs, T.J.M.Symons Precise Magnetic Moment of Short-Lived Beta Emitter 35Ar RADIOACTIVITY 35Ar(β-); measured β-NMR spectra from oriented nuclei; deduced μ.
doi: 10.1016/S0375-9474(01)01615-3
2002MA43 Nucl.Phys. A704, 98c (2002) K.Matsuta, T.Minamisono, M.Fukuda, M.Mihara, K.Sato, K.Minamisono, T.Yamaguchi, T.Onishi, T.Miyake, M.Sasaki, M.Tanigaki, T.Ohtsubo, S.Momota, Y.Nojiri, K.Yoshida, A.Ozawa, I.Tanihata, A.Kitagawa, M.Torikoshi, M.Kanazawa, S.Koda, T.Nishio, M.Suda, J.R.Alonso, G.F.Krebs, T.J.M.Symons, S.S.Hanna Recent Studies on the Nuclear Moments of Light Mirror Nuclei ( T = 1/2, 3/2) NUCLEAR MOMENTS 9C, 13O, 27Mg, 27Si; measured β-NMR spectra of oriented nuclei; deduced quadrupole moments.
doi: 10.1016/S0375-9474(02)00770-4
2002MI37 Z.Naturforsch. 57a, 595 (2002) T.Minamisono, K.Matsuta, K.Minamisono, S.Kudo, M.Ogura, S.Fukuda, K.Sato, M.Mihara, M.Fukuda, S.Takeda, S.Y.Zhu Quadrupole Moments of the 40Ca Core Plus One Nucleon Nuclei 41Sc and 41Ca NUCLEAR MOMENTS 41Sc, 41Ca; measured NMR and NQR spectra; deduced quadrupole moments, electric field gradients in TiO2 crystals.
2002OG08 Z.Naturforsch. 57a, 599 (2002) M.Ogura, K.Minamisono, T.Sumikama, T.Nagatomo, T.Iwakoshi, T.Miyake, S.Kudo, K.Akutsu, K.Sato, M.Mihara, M.Fukuda, K.Matsuta, H.Akai, T.Minamisono Development of a Nuclear Spin Dewar: Hyperfine Interactions of the Short-Lived β Emitter 12B in TiO2 NUCLEAR MOMENTS 12B(β-); measured β-NMR spectra, asymmetry vs temperature for source implanted in TiO2; deduced polarization.
2002SA64 Prog.Theor.Phys.(Kyoto), Suppl. 146, 212 (2002) Neutrino Burst from Supernovae and Neutrino Oscillation
doi: 10.1143/PTPS.146.212
2002WA21 Phys.Rev. C66, 012801 (2002) G.Watanabe, K.Sato, K.Yasuoka, T.Ebisuzaki Microscopic Study of Slablike and Rodlike Nuclei: Quantum molecular dynamics approach
doi: 10.1103/PhysRevC.66.012801
2002WA30 Prog.Theor.Phys.(Kyoto), Suppl. 146, 638 (2002) G.Watanabe, K.Sato, K.Yasuoka, T.Ebisuzaki Microscopic Study of Nuclear "Pasta" by Quantum Molecular Dynamics
doi: 10.1143/PTPS.146.638
2001II01 Prog.Theor.Phys.(Kyoto) 106, 551 (2001); Erratum Prog.Theor.Phys.(Kyoto) 110, 847 (2003) Formation of Nuclear ' Pasta ' in Cold Neutron Star Matter
doi: 10.1143/PTP.106.551
2001MA42 Phys.Rev.Lett. 86, 3735 (2001) K.Matsuta, T.Miyake, K.Minamisono, A.Morishita, S.Momota, Y.Nojiri, M.Mihara, M.Fukuda, K.Sato, S.Y.Zhu, H.Kitagawa, H.Sagawa, T.Minamisono Electromagnetic Moments of the β-Emitting Nucleus 16N RADIOACTIVITY 16N(β-) [from 15N(d, p)]; measured β-NMR asymmetry in MgO, β-NQR asymmetry in TiO2; deduced μ, quadrupole moment. Comparison with model predictions.
doi: 10.1103/PhysRevLett.86.3735
2001MB06 Hyperfine Interactions 136/137, 189 (2001) K.Matsuta, T.Miyake, K.Minamisono, M.Mihara, M.Fukuda, K.Sato, S.Y.Zhu, T.Minamisono Hyperfine Interactions of N Isotopes in TiO2 and Quadrupole Moment of 16N RADIOACTIVITY 16N(β-) [from 15N(d, p)]; measured β-NMR and β-NQR spectra from oriented source. 16N deduced μ, quadrupole moment.
doi: 10.1023/A:1020517014587
2001MI40 Hyperfine Interactions 136/137, 225 (2001) T.Minamisono, K.Matsuta, K.Minamisono, S.Kudo, M.Ogura, S.Fukuda, K.Sato, M.Mihara, M.Fukuda Precise Quadrupole Moment of the Doubly Closed Shell Plus One Proton Nucleus 41Sc NUCLEAR MOMENTS 45Sc; measured Fourier-transformed pulse-NMR spectrum in TiO2 crystal. 41Sc; analyzed β-NQR data; deduced quadrupole moment. Comparison with model prediction.
doi: 10.1023/A:1020588417313
2001OG12 Hyperfine Interactions 136/137, 195 (2001) M.Ogura, K.Minamisono, T.Sumikama, T.Nagatomo, T.Iwakoshi, T.Miyake, K.Hashimoto, S.Kudo, K.Arimura, M.Ota, K.Akutsu, K.Sato, M.Mihara, M.Fukuda, K.Matsuta, H.Akai, T.Minamisono A Possible Nuclear Spin Dewar. Hyperfine Interactions of Short-Lived β Emitter 8Li and 12B in TiO2 RADIOACTIVITY 8Li, 12B(β-) [from 7Li, 11B(dp)]; measured β-NMR spectra from oriented sources.
doi: 10.1023/A:1020528231425
2001WA15 Nucl.Phys. A687, 512 (2001); Erratum Nucl.Phys. A726, 357 (2003) Effects of Neutrino Trapping on Thermodynamic Properties of Nuclear ' Pasta '
doi: 10.1016/S0375-9474(00)00585-6
2001ZH43 Hyperfine Interactions 136/137, 149 (2001) S.-Y.Zhu, J.Zhu, T.Minamisono, K.Matsuta, Y.Xu, M.Fukuda, M.Mihara, Z.Wang, K.Sato, H.Akai, C.Rong, C.Chu, J.Chen, H.Luo On-line Time Differential Perturbed Angular Correlation with Light Probe Nucleus 19F RADIOACTIVITY 19O(β-); measured Eγ, Iγ(θ, H, t). 19F deduced quadrupole moment. On-line time differential perturbed angular correlation.
doi: 10.1023/A:1020532332334
2000WA27 Nucl.Phys. A676, 455 (2000); Erratum Nucl.Phys. A726, 357 (2003) Thermodynamic Properties of Nuclear ' Pasta ' in Neutron Star Crusts
doi: 10.1016/S0375-9474(00)00197-4
1999HA27 J.Nucl.Sci.Technol.(Tokyo) 36, 313 (1999) M.Harada, Y.Watanabe, A.Yamamoto, S.Yoshioka, K.Sato, T.Nakashima, H.Ijiri, H.Yoshida, Y.Uozumi, N.Koori, S.-I.Meigo, O.Iwamoto, T.Fukahori, S.Chiba The 12C(p, p'3α) Breakup Reaction Induced by 14, 18 and 26 MeV Protons NUCLEAR REACTIONS 12C(p, xp), (p, xα), (p, p'α), (p, p3α), E=14, 18, 26 MeV; measured proton spectra, Eα, σ(E, θ); deduced role of three-body simultaneous breakup. Comparison with Monte Carlo calculations.
doi: 10.1080/18811248.1999.9726214
1999MA46 Phys.Lett. 459B, 81 (1999) K.Matsuta, K.Sato, M.Fukuda, M.Mihara, T.Yamaguchi, M.Sasaki, T.Miyake, K.Minamisono, T.Minamisono, M.Tanigaki, T.Ohtsubo, T.Onishi, Y.Nojiri, S.Momota, S.Fukuda, K.Yoshida, A.Ozawa, T.Kobayashi, I.Tanihata, J.R.Alonso, G.F.Krebs, T.J.M.Symons, H.Kitagawa, H.Sagawa Quadrupole Moment of the Proton Drip-Line Nuclide 13O RADIOACTIVITY 13O(β+) [from Be(16O, X)]; measured β-NQR spectrum; deduced quadrupole moment. Comparison with shell model predictions.
doi: 10.1016/S0370-2693(99)00620-6
1999MB13 Hyperfine Interactions 120/121, 673 (1999) K.Matsuta, T.Onishi, M.Fukuda, T.Minamisono, H.Akai, M.Sasaki, T.Yamaguchi, T.Miyake, K.Sato, K.Minamisono, F.Ohsumi, Y.Muramoto, S.Oui, C.Ha, K.Tanaka, K.Kidera, A.Morishita, A.Kitagawa, M.Torikoshi, M.Kanazawa, T.Nishio, S.Koda, T.Ohtsubo, S.Fukuda, Y.Nojiri, S.Momota, A.Ozawa, K.Yoshida, T.Suzuki, T.Kobayashi, I.Tanihata, S.S.Hanna, J.R.Alonso, G.F.Krebs, T.J.M.Symons Electromagnetic moments of short lived β emitters 21F, 23Mg, 27Si and 39Ca NUCLEAR MOMENTS 21F, 23Mg, 27Si, 39Ca; measured asymmetry change as a function of the frequency; deduced magnetic moments, electrical quadrupole coupling constants. Comparison with OXBASH shell model calculations.
doi: 10.1023/A:1017036009679
1999MI16 Phys.Lett. 457B, 9 (1999) T.Minamisono, Y.Nojiri, K.Matsuta, M.Fukuda, K.Sato, M.Tanigaki, A.Morishita, T.Miyake, Y.Matsumoto, T.Onishi, K.Ishiga, F.Ohsumi, H.Kitagawa, H.Sagawa Electromagnetic Moments of the β-Emitting Nucleus 19O RADIOACTIVITY 19O(β-) [from 18O(d, p)]; measured β-NMR spectra. 19O deduced μ, Q. NUCLEAR MOMENTS 19O; measured β-NMR spectra; deduced μ, Q.
doi: 10.1016/S0370-2693(99)00468-2
1999SA75 Nucl.Phys. (Supplement) A654, 735c (1999) K.Sato, M.Tanigaki, T.Onishi, M.Fukuda, T.Minamisono, M.Mihara, K.Matsuta, S.Takeda, M.Sasaki, T.Yamaguchi, T.Miyake, K.Minamisono, A.Morishita, F.Osumi, Y.Muramoto, S.Oui, T.Fukao, Y.Matsumoto, T.Ohtsubo, S.Fukuda, Y.Nojiri, S.Momota, K.Yoshida, A.Ozawa, T.Kobayashi, I.Tanihata, A.Kitagawa, M.Torikoshi, H.Sagawa, H.Kitagawa, G.F.Krebs, J.R.Alonso, T.J.M.Symons Quadrupole Moments of Short-Lived β-Emitters 13, 19O and 21F RADIOACTIVITY 13O(β+) [from 9Be(16O, X), E=135 MeV/nucleon]; 19O(β-) [from 18O(d, p), E=3.25 MeV]; 21F(β-) [from 9Be(22Ne, X), E=100 MeV/nucleon]; measured β-NQR spectrum in TiO2, MgF2. 13O, 19O, 21F deduced quadrupole moments. Comparison with neighboring nuclei and with theoretical results. Halo effects discussed.
doi: 10.1016/S0375-9474(00)88538-3
1998II01 Phys.Rev. C58, 2538 (1998) Effects of Hyperons on the Dynamical Deconfinement Transition in Cold Neutron Star Matter
doi: 10.1103/PhysRevC.58.2538
1998MI10 Phys.Lett. 420B, 31 (1998) T.Minamisono, T.Ohtsubo, K.Sato, S.Takeda, S.Fukuda, T.Izumikawa, M.Tanigaki, T.Miyake, T.Yamaguchi, N.Nakamura, H.Tanji, K.Matsuta, M.Fukuda, Y.Nojiri Quadrupole Moment of the Proton Rich β-Emitting Nucleus 12N RADIOACTIVITY 12N(β+); measured β-NMR. 12N deduced quadrupole moment. Modified β-NMR technique.
doi: 10.1016/S0370-2693(97)01553-0
1998MI20 Z.Naturforsch. 53a, 293 (1998) T.Minamisono, K.Sato, H.Akai, S.Takeda, Y.Maruyama, K.Matsuta, M.Fukuda, T.Miyake, A.Morishita, T.Izumikawa, Y.Nojiri Electric Quadrupole Interactions of the Short-Lived β-Emitter 12N in Insulator Crystals (12N Implanted in Single Crystal TiO2) RADIOACTIVITY 12N(β+) [from 10B(3He, n)]; measured β-NMR. 12N deduced quadrupole moment, electric field gradiants in TiO2.
1997KU10 Phys.Rev. C55, 2866 (1997) Calculation of Excited-State Properties with an Auxiliary-Field Monte Carlo Method
doi: 10.1103/PhysRevC.55.2866
1996MA37 Hyperfine Interactions 97/98, 501 (1996) K.Matsuta, M.Fukuda, M.Tanigaki, T.Minamisono, Y.Nojiri, H.Akai, T.Izumikawa, M.Nakazato, M.Mihara, T.Yamaguchi, A.Harada, M.Sasaki, T.Miyake, T.Onishi, K.Minamisono, T.Fukao, K.Sato, Y.Matsumoto, T.Ohtsubo, S.Fukuda, K.Yoshida, A.Ozawa, S.Momota, T.Kobayashi, I.Tanihata, J.R.Alonso, G.F.Krebs, T.J.M.Symons Hyperfine Interactions of 13O and 23Mg Implanted in Pt RADIOACTIVITY 13O(β+) [from 9Be(16O, X), E=135 MeV/nucleon]; 23Mg(β+) [from 197Au(24Mg, X), E=100 MeV/nucleon]; measured β time spectra, NMR techniques, implantation in Pt; deduced hyperfine interaction, spin relaxation time, Knight shift.
doi: 10.1007/BF02150192
1996MA38 Hyperfine Interactions 97/98, 519 (1996) K.Matsuta, T.Minamisono, M.Tanigaki, M.Fukuda, Y.Nojiri, M.Mihara, T.Onishi, T.Yamaguchi, A.Harada, M.Sasaki, T.Miyake, K.Minamisono, T.Fukao, K.Sato, Y.Matsumoto, T.Ohtsubo, S.Fukuda, S.Momota, K.Yoshida, A.Ozawa, T.Kobayashi, I.Tanihata, J.R.Alonso, G.F.Krebs, T.J.M.Symons Magnetic Moments of Proton Drip-Line Nuclei 13O and 9C RADIOACTIVITY 13O(β+) [from 9Be(16O, X), E=135 MeV/nucleon]; 9C(β+) [from 12C(12C, X), E=70 MeV/nucleon]; measured β-NMR, polarized sources; deduced μ, spin expectation values.
doi: 10.1007/BF02150194
1996SA25 Nucl.Phys. A606, 118 (1996) Gravitational Collapse of Rotating Stellar Cores and Supernovae
doi: 10.1016/0375-9474(96)00236-9
1996UE08 Czech.J.Phys. B46, 867 (1996) K.-C.Ueda, T.Oda, Y.Iwamoto, T.Kohara, Q.F.Lu, I.Umehara, K.Sato NMR and NQR Studies in Binary Superconductor La7Ni3 NUCLEAR MOMENTS 139La; measured NMR, NQR; deduced spin-lattice relaxation rate vs temperature. Superconductivity features of La7Ni3.
doi: 10.1007/BF02583741
1995AB15 Phys.Rev. C52, 837 (1995) Imaginary Part of the Optical Potential for Finite Temperature and for Preequilibrium Processes NUCLEAR REACTIONS 208Pb(n, n), E not given; calculated imaginary potential, temperature dependence. Many-particle, many-hole states.
doi: 10.1103/PhysRevC.52.837
1995SA13 Phys.Lett. 341B, 257 (1995) Spreading Widths of Nucleons in the Semiclassical Approximation NUCLEAR STRUCTURE 208Pb; calculated nucleon spreading widths. Semi-classical approximation.
doi: 10.1016/0370-2693(94)01373-K
1995SA35 Nucl.Phys. A588, 229c (1995) K.Sato, S.Yamada, H.Ogawa, K.Kawachi, N.Araki, A.Itano, M.Kanazawa, A.Kitagawa, T.Kohno, M.Kumada, T.Murakami, M.Muramatsu, K.Noda, S.Sato, Y.Sato, E.Takada, A.Tanaka, K.Tashiro, M.Torikoshi, J.Yoshizawa, M.Endo, Y.Furusawa, T.Kanai, H.Koyama-Ito, N.Matsufuji, S.Minohara, N.Miyahara, F.Soga, M.Suzuki, H.Tomura, Y.Hirao Performance of HIMAC
doi: 10.1016/0375-9474(95)00144-P
1995SA36 Nucl.Phys. A588, 345c (1995) Explosion Mechanism of Collapse-Driven Supernovae
doi: 10.1016/0375-9474(95)00160-3
1994OD01 At.Data Nucl.Data Tables 56, 231 (1994) T.Oda, M.Hino, K.Muto, M.Takahara, K.Sato Rate Tables for the Weak Processes of sd-Shell Nuclei in Stellar Matter NUCLEAR STRUCTURE A=1-39; calculated weak interaction rates; deduced weak interaction rates in stellar matter.
doi: 10.1006/adnd.1994.1007
1994SA05 Phys.Rev. C49, 1099 (1994) Imaginary Part of the Optical Potential for Preequilibrium Processes NUCLEAR STRUCTURE 93Nb; calculated particle, hole, particle-hole state densities. 40Ca, 208Pb, 93Nb; calculated preequilibrium reaction related optical potential imaginary part. Semi-classical approximation, delta function interaction, microscopic approach.
doi: 10.1103/PhysRevC.49.1099
1993NI17 Hyperfine Interactions 78, 153 (1993) K.Nishimura, I.S.Oliveira, N.J.Stone, Y.Isikawa, K.Shimizu, K.Sato Hyperfine Field and Beta-Decay of 142Pr in PrNi Studied by Low Temperature Nuclear Orientation RADIOACTIVITY 142Pr(β-), (EC); measured Iγ(θ) vs temperature; deduced β-decay matrix element features. Polarized source, low temperature nuclear orientation.
doi: 10.1007/BF00568131
1991SA13 Z.Phys. A339, 129 (1991) K.Sato, Y.Takahashi, S.Yoshida Exciton Level Densities with Spin and Parity Based on Random Matrix Model NUCLEAR STRUCTURE 40Ca, 208Pb; calculated level densities, exciton number. Random matrix model, Woods-Saxon potential.
doi: 10.1007/BF01282942
1989SA12 Z.Phys. A333, 141 (1989) Average Partial Level Density Based on the Random Matrix Model Inclusion of Realistic One-Body Spectrum and Effect of Particle Escape NUCLEAR STRUCTURE 208Pb; calculated partial level densities. Random matrix model.
1989TA26 Nucl.Phys. A504, 167 (1989) M.Takahara, M.Hino, T.Oda, K.Muto, A.A.Wolters, P.W.M.Glaudemans, K.Sato Microscopic Calculation of the Rates of Electron Captures which Induce the Collapse of O + Ne + Mg Cores NUCLEAR STRUCTURE 20Ne, 20F, 24Mg, 24Na; calculated Gamow-Teller transition log ft, electron capture rates; deduced O+Ne+Mg core evolution consequences. Shell model.
doi: 10.1016/0375-9474(89)90288-1
1988SA22 Z.Phys. A330, 265 (1988) Studies of Nuclear Second Moments for Pre-Equilibrium Nuclear Reaction Theories - Extension to Finite-Range Residual Interaction NUCLEAR STRUCTURE 208Pb, 40Ca; calculated second moments, level densities.
1987SA30 Z.Phys. A327, 421 (1987) Studies of Nuclear Second Moments for Pre-Equilibrium Nuclear Reaction Theories NUCLEAR STRUCTURE 40Ca, 208Pb; calculated single particle orbits, binding energies, moment matrix elements, eigen values, level densities. Preequilibrium theories.
1985SA20 Phys.Rev. C32, 647 (1985) Backward Cross Section in the Generalized Exciton Model NUCLEAR REACTIONS 54Fe, 120Sn, 197Au, 209Bi(p, p'), E=62 MeV; calculated σ(E, θ). Generalized exciton model, single nucleon-nucleon scattering kernel, finite nuclear size.
doi: 10.1103/PhysRevC.32.647
1983KU04 Nucl.Phys. A401, 445 (1983) H.Kusakari, K.Kitao, K.Sato, M.Sugawara, H.Katsuragawa High-Spin States in Even-Mass Xe Nuclei and Backbending Phenomena NUCLEAR REACTIONS 122,124,126,128,130Te(α, 4n), E=49-55 MeV; measured relative σ(E, Eγ), σ(Eγ, θ), Iγ, γγα-coin. 122,124,126,128,130Xe deduced levels, J, π, T1/2.
doi: 10.1016/0375-9474(83)90359-7
1983SA27 Phys.Rev. C28, 1527 (1983) Pre-Equilibrium Emission of Light Composite Particles in the Framework of the Exciton Model NUCLEAR REACTIONS 89Y, 120Sn, 197Au, 54Fe(p, p), (p, d), (p, t), (p, 3He), (p, α), E=62 MeV; 58Ni(p, t), (p, α), (p, 3He), E=90 MeV; calculated σ(Ep), σ(Ed), σ(Et), σ(E(3He)), σ(Eα); deduced composite particle emission mechanism. Exciton model.
doi: 10.1103/PhysRevC.28.1527
1983TA08 Nucl.Phys. A399, 241 (1983) T.Tanabe, K.Haga, M.Yasue, K.Sato, K.Ogino, Y.Kadota, M.Tochi, K.Makino, T.Kitahara, T.Shiba (6Li, d) Reactions on 24Mg and 26Mg at 73 MeV NUCLEAR REACTIONS 24,26Mg(6Li, d), E=72.7 MeV; measured σ(Ed, θ). 28,30Si deduced α spectroscopic factors. Enriched targets.
doi: 10.1016/0375-9474(83)90606-1
1981TA06 Phys.Lett. 100B, 241 (1981) T.Tanabe, M.Yasue, K.Sato, K.Ogino, Y.Kadota, Y.Taniguchi, K.Makino, M.Tochi The Reaction 16O(6Li, d)20Ne at 75 MeV NUCLEAR REACTIONS 16O(6Li, d), E=75 MeV; measured σ(Ed, θ). 20Ne levels deduced relative Sα. Finite-range DWBA analysis, α-cluster transfer.
doi: 10.1016/0370-2693(81)90325-7
1981TA23 Phys.Rev. C24, 2556 (1981) T.Tanabe, M.Yasue, K.Sato, K.Ogino, Y.Kadota, Y.Taniguchi, K.Obori, K.Makino, M.Tochi (6Li, d) Reaction on 16O and 28Si at 75 MeV NUCLEAR REACTIONS 16O, 28Si(6Li, d), E=75 MeV; measured σ(θ). 20Ne, 32S levels deduced relative Sα. DWBA analysis.
doi: 10.1103/PhysRevC.24.2556
1979SA10 Z.Phys. A290, 149 (1979) K.Sato, S.Yamaji, K.Harada, S.Yoshida A Numerical Analysis of the Heavy-Ion Reaction Based on the Linear Response Theory NUCLEAR REACTIONS 28Si(20Ne, X), E=120 MeV; calculated σ(θ). Linear response theory with collective variables, deformation δ, relative distance R, two-dimensional coupled equations of motion.
doi: 10.1007/BF01408109
1978TA23 Nucl.Phys. A311, 38 (1978) T.Tanabe, M.Yasue, K.Sato, F.Soga, M.Igarashi, K.Ogino, Y.Kadota, Y.Saito, S.Tanaka, F.Shimokoshi Study of the (3He, t) Reaction on 48Ca at 82 MeV NUCLEAR REACTIONS 48Ca(3He, 3He), (3He, d), (3He, α), (3He, t), E=82 MeV; measured σ(θ). Enriched target. Second-order zero-range, full-finite range. DWBA analysis.
doi: 10.1016/0375-9474(78)90500-6
1976TA12 J.Phys.Soc.Jap. 41, 361 (1976) T.Tanabe, K.Koyama, M.Yasue, H.Yokomizo, K.Sato, J.Kokame, N.Koori, S.Tanaka The (3He, 3He), (3He, 3He') and (3He, α) Reactions on 12C at 82.1 MeV NUCLEAR REACTIONS 12C(3He, 3He), E=82.1 MeV; measured σ(θ); deduced optical potential parameters. 12C(3He, 3He'), (3He, α), E=82.1 MeV; measured σ(θ). 12C levels deduced β.
doi: 10.1143/JPSJ.41.361
1975AD05 J.Phys.Soc.Jap. 38, 81 (1975) K.Adachi, K.Sato, M.Okimori, G.Yamauchi, H.Yasuoka, Y.Nakamura Magnetic Anisotropy of CoS2-Torque and NMR Measurements NUCLEAR MOMENTS 59Co; measured hyperfine field. NMR method.
doi: 10.1143/JPSJ.38.81
1973MA12 Phys.Lett. 44B, 159 (1973) M.Matoba, M.Hyakutake, S.Nakamura, T.Katayama, T.Tonai, K.Yagi, K.Sato, Y.Aoki Splittings of the Octupole Strength in Te Isotopes NUCLEAR REACTIONS 126,128,130Te(p, p'), E=51.91 MeV; measured σ(Ep, θ). 126,128,130Te deduced octupole levels, strengths.
doi: 10.1016/0370-2693(73)90509-1
1973MA29 Phys.Lett. 45B, 463 (1973) M.Matoba, M.Hyakutake, J.Niidome, K.Yagi, Y.Aoki, K.Sato Strong L = 5 Transition in Te(p, p') Reactions NUCLEAR REACTIONS 122,124,126,128,130Te(p, p'), E=51.9 MeV; measured σ(Ep', θ). 122,126,128,130Te deduced levels, J, π, B(EL).
doi: 10.1016/0370-2693(73)90644-8
1972YA07 Phys.Rev.Lett. 29, 1334 (1972) K.Yagi, K.Sato, Y.Aoki, T.Udagawa, T.Tamura (p, t) Excitations of Removal and Addition Types of Quadrupole-Pairing Vibrational States in Even Nd Isotopes NUCLEAR REACTIONS 142,144,146,148,150Nd(p, t), E=52 MeV; analyzed σ(θ). 2-step coupled-channel Born approximation.
doi: 10.1103/PhysRevLett.29.1334
1972YA09 J.Phys.Soc.Jap. 33, 1482 (1972) One-Proton Coupled L = 0 and 2 Transitions in the 141Pr(p, t) Reaction NUCLEAR REACTIONS 141Pr(p, t), E=52 MeV; measured σ(θ). 139Pr deduced levels, L.
doi: 10.1143/JPSJ.33.1482
1971YA05 J.Phys.Soc.Jap. 30, 1500 (1971) The Energy Gap between Two Major Proton Shells in the Z = 82 Region NUCLEAR REACTIONS 208Pb, 209Bi(d, α), E=11 MeV; measured σ(Eα). 206Tl, 207Pb deduced configurations.
doi: 10.1143/JPSJ.30.1500
1971YA10 Phys.Lett. 37B, 369 (1971) Coupled Particle-Pairing Vibrational Excitations in 141Nd and 143Nd by The (p, t) Reaction NUCLEAR REACTIONS 143,145Nd(p, t), E=52 MeV; measured σ(Et, θ), Q. 142,144Nd(p, t), E=52 MeV; measured σ(Et, θ), Q. 141,143Nd deduced coupled particle-pairing vibrational states, L.
doi: 10.1016/0370-2693(71)90205-X
1971YA11 J.Phys.Soc.Jap. 31, 1838 (1971) The (p, t) and (p, d) Reactions on the Nd Isotopes of A = 142-150 NUCLEAR REACTIONS 142,144,146,148,150Nd(p, d), E=52 MeV; measured σ(Ed).
doi: 10.1143/JPSJ.31.1838
1970YA04 J.Phys.Soc.Jap. 28, 1583 (1970) Pairing Vibrational [f7/2(1, 0)] States in 141Nd Obtained from L = 0 and 2 Transitions in a 143Nd(p, t) Reaction NUCLEAR REACTIONS 143Nd(p, t), E=52 MeV; measured σ(Et, θ). 141Nd deduced levels, L, configurations.
doi: 10.1143/JPSJ.28.1583
1970YA05 Nucl.Phys. A149, 45 (1970) Strong L = 0 and 2 Transitions in (p, t) Reactions on Even-Mass Ce Isotopes NUCLEAR REACTIONS 140,142Ce(p, t), E=52.1 MeV; measured σ(Et, θ); deduced Q. 138,140Ce duduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(70)90377-5
1969YA07 Phys.Letters 29B, 647 (1969) K.Yagi, Y.Aoki, J.Kawa, K.Sato Strong L=0 and 2 Transitions in (p, t) Reactions in Even-Mass Nd Isotopes NUCLEAR REACTIONS 142,144,146,150Nd(p, t), E=51.7 MeV; measured σ(Et, θ). 140,142,144,146Nd deduced levels, L. Enriched targets.
doi: 10.1016/0370-2693(69)90098-7
1968YA09 OULNS-69-2, p.13 (1968) (d, α) Reactions on 208Pb and 209Bi NUCLEAR REACTIONS 208Pb, 209Bi(d, α), E=11 MeV; measured σ(Eα, θ). 206Tl, 207Pb deduced levels.
1967KI08 J.Phys.Soc.Jpn. 23, 122 (1967) Gamma Rays from the Decay of 147Nd NUCLEAR STRUCTURE 147Nd; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.23.122
1964SA32 Rept.Chiba Inst.Tech., No.5, 54 (1964); Nucl.Sci.Abstr. 19, 2916, Abstr.23767 (1965) Excited Levels of Ni62 NUCLEAR STRUCTURE 62Cu; measured not abstracted; deduced nuclear properties.
1963SA16 J.Phys.Soc.Japan 18, 1353 (1963) Photo Neutron Cross Sections in Na23 and Si28 NUCLEAR STRUCTURE 22Na, 27Si; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.18.1353
1961KI03 Nuclear Phys. 23, 338 (1961) M.Kimura, K.Shoda, N.Mutsuro, T.Tohei, K.Sato, K.Kuroda, K.Kuriyama, T.Akiba Structure of the Giant Resonance in the Al27(p, γ) Reaction NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90263-2
1960KI08 J.Phys.Soc.Japan 15, 1128 (1960) M.Kimura, K.Shoda, N.Mutsuro, T.Tohei, K.Sato, K.Kuroda, K.Kuriyama, T.Akiba Structure of Giant Resonance in Al27(p, γ) Reaction NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.15.1128
Back to query form [Next] |