NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = M.Sano Found 39 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
1994LI44 J.Phys.(London) G20, 1829 (1994) Further Studies of the Equilibration Process in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS Ca(Ca, X), 20Ne(20Ne, X), 139La(139La, X), E=1-2 GeV/nucleon; calculated average density time evolution, relativistic collision. Relativistic Boltzmann-Uehling-Uhlenbeck model, local equilibration process.
doi: 10.1088/0954-3899/20/11/011
1994MA09 Z.Phys. A347, 173 (1994) G.Mao, Z.Li, Y.Zhuo, Y.Han, Z.Yu, M.Sano Density and Momentum Dependence of the Coupling Strengths for Scalar and Vector Fields
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
1992SO15 Prog.Theor.Phys.(Kyoto) 87, 599 (1992) Coulomb Dissociation of the Weakly-Bound Nucleus 11Li NUCLEAR REACTIONS 9Be, C, 27Al, Cu, Pb(11Li, X), E=0.8 GeV/nucleon; calculated dissociation σ. Two-neutron removal, modified Glauber approximation.
doi: 10.1143/ptp/87.3.599
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
1987KI10 Phys.Rev.Lett. 58, 1508 (1987) Y.Kitazoe, M.Sano, H.Toki, S.Nagamiya Pion-Reabsorption Effect on Pion Spectra in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS Na, F(Ne, p), (Ne, π-), E=0.8 GeV/nucleon; calculated σ(Ep, θp), σ(Eπ, θπ); deduced slope parameters, multiplicities vs mass. Cascade model.
doi: 10.1103/PhysRevLett.58.1508
1986KI02 Phys.Lett. 166B, 35 (1986) Y.Kitazoe, M.Sano, H.Toki, S.Nagamiya Pion Production Mechanism in High Energy Heavy Ion Collisions NUCLEAR REACTIONS K, Cl(Ar, π-), E=800-1600 MeV/nucleon; calculated pion multiplicity vs E. Cascade model. NUCLEAR STRUCTURE A=10-110; calculated charged pion production σ at E=730 MeV. Cascade model.
doi: 10.1016/0370-2693(86)91150-0
1985SA17 Hyperfine Interactions 21, 95 (1985) g-Factors of High-Spin States in the g- and s-Bands NUCLEAR STRUCTURE 162Er; calculated ground state, s-bands, g vs spin. Cranked HFB, number projection.
doi: 10.1007/BF02061980
1984KI02 Phys.Rev. C29, 828 (1984) Y.Kitazoe, M.Sano, Y.Yamamura, H.Furutani, K.Yamamoto Cascade-Model Analysis of Collective Motion in Relativistic Nuclear Reactions NUCLEAR REACTIONS K, Cl(p, pX), E=800 MeV; calculated inclusive σ. New cascade model.
doi: 10.1103/PhysRevC.29.828
1984KI03 Phys.Lett. 138B, 341 (1984) Y.Kitazoe, M.Gyulassy, P.Danielewicz, H.Toki, Y.Yamamura, M.Sano New Cascade Model Calculation of Pion Multiplicity in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS K, Cl(p, pX), E=800 MeV; Na, F(20Ne, pX), E=800 MeV/nucleon; U(20Ne, pX), E=400 MeV/nucleon; calculated inclusive production σ(qp) vs proton momentum. K, Cl(40Ar, π-X), E(cm) ≈ 100-300 MeV/nucleon; calculated average pion multiplicity vs E. New cascade model.
doi: 10.1016/0370-2693(84)91912-9
1984KI10 Prog.Theor.Phys.(Kyoto) 71, 1429 (1984) Y.Kitazoe, O.Hashimoto, H.Toki, Y.Yamamura, M.Sano Primary Projectile Fragmentation Distribution in High Energy Heavy Ion Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=400 MeV/nucleon; 40Ca(12C, X), E=213 MeV/nucleon; measured primary projectile fragmentation distribution; deduced proton-rich nuclei abundance, Coulomb barrier effects. Nuclear cascade model.
doi: 10.1143/PTP.71.1429
1984KI20 Phys.Rev.Lett. 53, 2000 (1984) Y.Kitazoe, H.Furutani, H.Toki, Y.Yamamura, S.Nagamiya, M.Sano Cascade-Model Analysis of the Sideward ' Splash ' in Nb + Nb Collisions with High-Multiplicity Events NUCLEAR REACTIONS Ca(Ca, X), 93Nb(93Nb, X), E=400 MeV/nucleon; calculated high multiplicity event σ(θ); deduced cascade collision development, bounceoff effect. Cascade model.
doi: 10.1103/PhysRevLett.53.2000
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
1981AS01 Phys.Lett. B98, 19 (1981) Kaon Production in the Nuclear Fireball Model NUCLEAR REACTIONS Na, F(Ne, K+), E=2.1 GeV/nucleon; calculated σ(E(K+), θ, inclusive). Fireball model. NaF target.
doi: 10.1016/0370-2693(81)90357-9
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
1980MA24 Prog.Theor.Phys.(Kyoto) 63, 1067 (1980) K.Matsuoka, T.Kammuri, M.Sano, N.Takahashi Spin Alignment of Products 12B in 14N Induced Reactions NUCLEAR REACTIONS 100Mo(14N, 12B), E=90 MeV; calculated 12B polarization vs Q. Semiclassical model, cluster transfer.
doi: 10.1143/PTP.63.1067
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
1978IS01 Phys.Lett. 73B, 281 (1978) M.Ishihara, K.Tanaka, T.Kammuri, K.Matsuoka, M.Sano Semiclassical Analysis of the Spin Polarization of 12B in the 100Mo(14N, 12B)102Ru Reaction NUCLEAR REACTIONS 100Mo(14N, 12B), E=90 MeV; calculated polarization, σ.
doi: 10.1016/0370-2693(78)90514-2
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
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
1975KI20 Lett.Nuovo Cim. 14, 407 (1975) Angular Distributions of Ejected Particles in High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS Ag(16O, X), E=2.1 GeV; Ag(12C, X), E=0.87 GeV; Cl(16O, X), E=0.25 GeV; Cl(12C, X), E=0.11 GeV; analyzed particle distributions.
doi: 10.1007/BF02746866
1975SH22 Nucl.Phys. A254, 7 (1975) Effective E3 Transition Moments for 1h11/2 Single Proton States in N ≈ 82 Nuclei NUCLEAR STRUCTURE 139,141Pr, 143Pm, 147Eu; calculated B(E3), effective coupling constants.
doi: 10.1016/0375-9474(75)90578-3
1974TO09 Lett.Nuovo Cim. 11, 293 (1974) H.Toki, M.Sano, H.Orihara, Y.Ishizaki Energy Dependence of (p, t)-Reaction Cross-Sections NUCLEAR REACTIONS 208Pb(p, t), E=10-80 MeV; calculated σ(E, Et, θ).
doi: 10.1007/BF02813546
1973OH05 Progr.Theor.Phys. 49, 877 (1973) Relativistic Corrections to Nuclear Magnetic Moments and Gamow-Teller Matrix Elements of Beta Decay NUCLEAR STRUCTURE A=11-43; 88Sr, 114Sn, 208Pb; calculated nuclear magnetic moment.
doi: 10.1143/PTP.49.877
1973TO15 Progr.Theor.Phys. 50, 699 (1973) Two-Neutron Transfer Reactions on Nuclei Around N = 82 Closed Shell NUCLEAR REACTIONS 142,144,146,148,150Nd(p, t), E=51.7 MeV; calculated σ(θ).
doi: 10.1143/PTP.50.699
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
1972TA12 Phys.Rev.Lett. 29, 133 (1972) T.Takemasa, M.Sakagami, M.Sano Two-Neutron Transfer Reactions on Rare-Earth Nuclei NUCLEAR REACTIONS 152,154Sm, 158Gd, 164Dy, 168Er, 172Yb, 176Hf, 184W(p, t), calculated σ, spectroscopic amplitudes. 172Yb, 154Sm(p, t), E=52 MeV; calculated σ(θ). Angular-momentum projection method.
doi: 10.1103/PhysRevLett.29.133
1971TA26 Phys.Lett. 37B, 233 (1971) Centrifugal Stretching Effect to Intra-Band E2-Transition Rates NUCLEAR STRUCTURE 156,158,160Er; calculated intra-band B(E2). Centrifugal stretching model.
doi: 10.1016/0370-2693(71)90005-0
1971TA27 Phys.Lett. 37B, 473 (1971) T.Takemasa, M.Sakagami, M.Sano Two-Neutron Transfer Reactions on Nuclei in the Transitional Region NUCLEAR REACTIONS 148,150Sm(t, p), 152Sm(p, t), Ep=52 MeV; calculated σ(θ). 152Sm deduced shape-coexisting wave functions.
doi: 10.1016/0370-2693(71)90348-0
1966IK01 Phys.Lett. 21, 323 (1966) Effect of Collective Vibrational Motion on the Anomalous Coupling States NUCLEAR STRUCTURE 77Se, 79Se, 81Se; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90835-3
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