NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = M.Wakai Found 31 matches. 1998SA64 Prog.Theor.Phys.(Kyoto) 100, 675 (1998) Polarization of Hypernuclei Produced in High-Energy Nuclear Collisions NUCLEAR STRUCTURE 3H; calculated polarization of hypernucleus formed in heavy-ion collision.
doi: 10.1143/PTP.100.675
1997YA11 Nucl.Phys. A625, 107 (1997) Y.Yamamoto, M.Wakai, T.Motoba, T.Fukuda Production of Double-Λ Hypernuclei at (K-, K+) Reaction Points and Their Pionic Decays NUCLEAR REACTIONS 9Be, 10,11B, 12C(K-, K+), E not given; calculated single-, double-Λ hyperfragment formation probabilities, pionic decay. Statistical model.
doi: 10.1016/S0375-9474(97)00483-1
1994SA74 Prog.Theor.Phys.(Kyoto), Suppl. 117, 99 (1994) Hypernuclear Production in High-Energy Nuclear Collisions NUCLEAR REACTIONS 23Na, 19F(Ne, X), (p, X), E(cm) ≤ 0.8 GeV; Pb(p, X), E=0.8-1 GeV; C(C, X), E at ≤ 16 GeV/nucleon; analyzed hypernuclei production data. 197Au(Si, X), E at 14.5 GeV/nucleon; calculated hypernuclei production data. Four different mechanisms.
doi: 10.1143/PTPS.117.99
1994YA21 Prog.Theor.Phys.(Kyoto), Suppl. 117, 265 (1994) Formation and Fragmentation of Double-Λ Compound Nucleus NUCLEAR STRUCTURE A=10-17; calculated double Λ fragments emission probabilities for hypernuclei. Double-Λ compound nucleus formation.
doi: 10.1143/PTPS.117.265
1992WA34 Nucl.Phys. A547, 89c (1992) Energy Dependence of Hypernucleus Production in High-Energy Nuclear Collision NUCLEAR REACTIONS C(C, X), (α, X), E ≤ 16 GeV/nucleon; calculated A=3, 4, 6 hypernuclear production σ. Coalescence, (fragment)(pion) interaction induced production models.
doi: 10.1016/0375-9474(92)90713-T
1992YA18 Prog.Theor.Phys.(Kyoto) 88, 1163 (1992) Y.Yamamoto, M.Wakai, T.Fukuda, M.Sano Formation of Double-Λ Hypernucleus from Quasi-Free Ξ- Absorption NUCLEAR STRUCTURE 12C; calculated double lambda hypernucleus fragmentation features following absorption of strange particle at (K-, K+) reaction point; deduced 6He(2 lambda) hypernucleus production probability.
doi: 10.1143/ptp/88.6.1163
1989BA93 Nucl.Phys. A501, 900 (1989) H.Bando, M.Sano, J.Zofka, M.Wakai Production of Hypernuclei in Relativistic Ion Beams
doi: 10.1016/0375-9474(89)90168-1
1989SA58 Phys.Lett. 224B, 359 (1989) Possibility of H-Particle Production in High-Energy Nuclear Collisions NUCLEAR REACTIONS 1H, Ne(Ne, X), E=5 GeV/nucleon; calculated H-particle production probability. Coalescence model.
doi: 10.1016/0370-2693(89)91461-5
1989TA17 Phys.Rev. C40, R483 (1989) H.Tamura, T.Yamazaki, M.Sano, Y.Yamamoto, M.Wakai, H.Bando Compound-Hypernucleus Interpretation on 4H(Lambda) Formation Probabilities in Stopped-K- Absorption NUCLEAR REACTIONS 4He, 7Li, 9Be, 40Ca, 12C, 16O(K-, π-), E at rest; calculated lambda energy distribution, hypernuclear formation probabilities. Compound nucleus formation, fragmentation.
doi: 10.1103/PhysRevC.40.R483
1989WA14 Z.Phys. A333, 213 (1989) Mesonic Atom Production in High-Energy Nuclear Collisions NUCLEAR REACTIONS Ne(p, π-X), (Ne, π-X), (Ne, K-X), E=2.1-5 GeV/nucleon; calculated mesic atom production probability. Coalescence model. ATOMIC PHYSICS, Mesic-Atoms Ne(p, π-X), (Ne, π-X), (Ne, K-X), E=2.1-5 GeV/nucleon; calculated mesic atom production probability. Coalescence model.
1988WA16 Phys.Rev. C38, 748 (1988) Hypernucleus Formation in High-Energy Nuclear Collisions NUCLEAR REACTIONS Ne(Ne, K+), (p, K+), E=2.1, 5 GeV/nucleon; calculated energy spectrum, σ. Coalescence model.
doi: 10.1103/PhysRevC.38.748
1986FA10 Nucl.Phys. A458, 381 (1986) A.Faessler, S.Kuyucak, M.Wakai IBA Description of Backbending in Odd-Mass Ce Isotopes NUCLEAR STRUCTURE 129,131Ce; calculated levels, B(E2), g factors. Interacting boson-fermion model.
doi: 10.1016/0375-9474(86)90040-0
1985IN03 Phys.Rev. C32, 1539 (1985) T.Inamura, A.C.Kahler, D.R.Zolnowski, U.Garg, T.T.Sugihara, M.Wakai Gamma-Ray Multiplicity Distribution Associated with Massive Transfer NUCLEAR REACTIONS 154Sm(12C, 2nα), (12C, 3nα), (12C, 4nα), (12C, 5nα), (12C, 6nα), 154Sm(12C, 2n2α), (12C, 2n3α), (12C, 2n4α), (12C, 2n5α), (12C, 2n6α), E=85, 109 MeV; 159Tb(14N, 3nα), (14N, 4nα), (14N, 5nα), (14N, 6nα), E=115 MeV; measured Eγ, Iγ, γα-coin, γ-multplicity; deduced γ-multiplicity, parameter dependences on residue yrast spin, massive transfer evidence. Kinematical, statistical models.
doi: 10.1103/PhysRevC.32.1539
1985KA10 Phys.Rev. C31, 1616 (1985) S.Kato, K.Okada, M.Kondo, K.Hosono, T.Saito, N.Matsuoka, K.Hatanaka, T.Noro, S.Nagamachi, H.Shimizu, K.Ogino, Y.Kadota, S.Matsuki, M.Wakai Inelastic Scattering of 65 MeV Protons from 12C, 24Mg, 28Si, and 32S NUCLEAR REACTIONS 12C, 24Mg, 28Si, 32S(polarized p, p'), E=65 MeV; measured σ(θ), A(θ); deduced deformation lengths, coupling parameters. 12C, 24Mg, 28Si, 32S deduced multipole moments, transition strengths. Optical model, coupled-channels analyses.
doi: 10.1103/PhysRevC.31.1616
1984FA01 J.Phys.(London) G10, L17 (1984) Direction of the Angular Momentum in the Entry State and the Crystal Ball NUCLEAR STRUCTURE 158Er; calculated continuum γ(θ); deduced entry angular momentum direction vs excitation, spin. Monte Carlo simulation.
doi: 10.1088/0305-4616/10/1/004
1984KU08 Nucl.Phys. A420, 83 (1984) S.Kuyucak, A.Faessler, M.Wakai Two-and Three-Quasiparticle States in the Interacting Boson Model and a Unified Description of Even- and Odd-Mass Hg Isotopes NUCLEAR STRUCTURE 189,190,191,192,193,194,195,196,197,198Hg; caluclated levels, B(E2), g. Interacting boson-fermion approximation, two-, three-quasiparticle states.
doi: 10.1016/0375-9474(84)90658-4
1982IN02 J.Phys.Soc.Jpn. 51, 1 (1982) Calculation of Gamma-Ray Multiplicity Moments Associated with Massive-Transfer Reactions NUCLEAR REACTIONS 154Sm(12C, X), E=85, 109 MeV; 159Tb(14N, X), E=115 MeV; 159Tb(10B, X), E=69 MeV; calculated γ-ray multiplicity distribution, moments. 158Dy, 164Yb deduced skewness dependence on massive transfer. Monte Carlo treatment.
doi: 10.1143/JPSJ.51.1
1982TA10 Phys.Rev.Lett. 48, 1791 (1982) M.Tanaka, T.Yamagata, T.Fukuda, T.Shimoda, M.Wakai, S.Nakayama, T.Nojiri, M.Inoue, I.Miura, H.Ogata Gamma Decay of Low-Energy Octupole Resonance in 90Zr NUCLEAR REACTIONS 90Zr(α, α'), E=99.3 MeV; measured σ(Eα'), αγ(θ). 90Zr deduced resonance, octupole character, J, π, γ-branching.
doi: 10.1103/PhysRevLett.48.1791
1982WA25 Prog.Theor.Phys.(Kyoto) 68, 1587 (1982) The Natures of γ-Rays Emitted from 152Dy Formed through 124Sn(32S, 4n)152Dy NUCLEAR REACTIONS 124Sn(32S, 4n), E=145 MeV; analyzed Eγ, Iγ, γ(θ), linear polarization data. Intraband E2 transition paths.
doi: 10.1143/PTP.68.1587
1981NO13 Prog.Theor.Phys.(Kyoto) 66, 1906 (1981) T.Nojiri, M.Kamimura, M.Sano, M.Wakai, K.Yoro Coupled-Channel Study of Proton Inelastic Scattering from the Second 01 State in 12C by use of the 3α Resonating-Group Wave Function NUCLEAR REACTIONS 12C(p, p'), E=65 MeV; calculated σ(θ). Coupled-channel method, three alpha resonating group wave functions.
doi: 10.1143/PTP.66.1906
1981WA30 Z.Phys. A303, 335 (1981) Side Feeding Times to Yrast States of 158Dy in 26Mg(136Xe, 4n)158Dy NUCLEAR REACTIONS 26Mg(136Xe, 4n), E=4.1 MeV/nucleon; analyzed side feeding T1/2, B(E2) for 158Dy. Compound nucleus model, Monte Carlo calculations.
doi: 10.1007/BF01421532
1980WA12 Phys.Lett. 93B, 232 (1980) The Structure of Yrast Isomers and the Nature of γ-Rays from a Compound Nucleus NUCLEAR REACTIONS 124Sn(32S, 4n), E ≈ 145 MeV; calculated yrast state, side feeding populations. 152Dy deduced noncollective nature of yrast isomers. Compound nucleus model, variable collective E2 strength.
doi: 10.1016/0370-2693(80)90501-8
1980WA14 Prog.Theor.Phys.(Kyoto) 63, 176 (1980) Populations of High Spin States in 152Dy NUCLEAR REACTIONS 124Sn(32S, 4n), E=145 MeV; calculated continuum γ-rays with E1, M1, E2 multipolarities. 152Dy transitions deduced decreased E2 collectivity at high spins. Monte Carlo method.
doi: 10.1143/PTP.63.176
1979CI03 Phys.Lett. 84B, 404 (1979) O.Civitarese, A.Faessler, M.Wakai On the Feeding Pattern and γ-Multiplicities in 26Mg(136Xe, 4n)158Dy NUCLEAR REACTIONS 26Mg(136Xe, 4n), E=4.1 MeV/nucleon; calculated entry distribution, γ-multiplicities, side-feeding population of ground state band. Statistical model, Monte Carlo calculation; deduced reaction mechanism.
doi: 10.1016/0370-2693(79)91226-7
1978SA31 Prog.Theor.Phys. 59, 2149 (1978) E2-Transition Rates of the Ground-State Rotational Member NUCLEAR STRUCTURE 158Er; calculated B(E2). Nonadiabatic effects of Coriolis antipairing, centrifugal stretching, angular momentum projection method.
doi: 10.1143/PTP.59.2149
1978WA03 Nucl.Phys. A295, 86 (1978) Influence of Quadrupole Pairing on Backbending NUCLEAR STRUCTURE 162Er; calculated backbending, quadrupole pairing influence.
doi: 10.1016/0375-9474(78)90022-2
1978WA10 Nucl.Phys. A307, 349 (1978) Description of γ-Multiplicities after Fusion Reactions in Deformed Nuclei NUCLEAR REACTIONS 150Nd(16O, 4n), E=65, 71, 77 MeV; 148Nd(18O, 4n); calculated side feeding, γ-multiplicities.
doi: 10.1016/0375-9474(78)90622-X
1977SA25 Progr.Theor.Phys. 58, 1673 (1977) DWBA Analysis of Magnetic Substate Populations of Residual Nucleus In the 11B(d, p)12B Reactions NUCLEAR REACTIONS 11B(d, p), E=1.3-3.0 MeV; calculated magnetic substate populations, optical model parameters. DWBA calculations.
doi: 10.1143/PTP.58.1673
1972SA22 Nucl.Phys. A190, 471 (1972) Stability of Nuclear Rotational States NUCLEAR STRUCTURE 180Hf, 160Dy; analyzed stability of rotational states.
doi: 10.1016/0375-9474(72)90851-2
1972SA35 Progr.Theor.Phys. 48, 160 (1972) Nuclear Level Density and Inertia Parameters NUCLEAR STRUCTURE 68Ge, 242Pu; calculated level density, moments of inertia. Cranking, superconductivity models.
doi: 10.1143/PTP.48.160
1970WA03 Nucl.Phys. A141, 423 (1970) The Nuclear Shape and Rotation NUCLEAR STRUCTURE 154Sm, 154Gd, 160Dy, 164Er, 172Yb, 176,180Hf, 180,182W; calculated equilibrium deformation, energy surfaces, moment of inertia.
doi: 10.1016/0375-9474(70)90857-2
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