NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = H.Bando Found 47 matches. 1991MO19 Nucl.Phys. A534, 597 (1991) T.Motoba, H.Bando, T.Fukuda, J.Zofka Continuum Pion Spectra in the Weak Decays of 4H(Lambda), 5He(Lambda) and 6He(Lambda)(Lambda) NUCLEAR STRUCTURE A=4, 5, 6; calculated pionic decay strength function. Kapur-Peierls treatment of continuum, decay rates.
doi: 10.1016/0375-9474(91)90463-G
1990IT02 Prog.Theor.Phys.(Kyoto) 84, 291 (1990) p-Shell Hypernuclei via (K-, π-), (π+, K+) and (Stopped K-, π-) Reactions - A Systematic Calculation with Configuration Mixing - NUCLEAR REACTIONS 14N, 13,12C(K-, π-), E at 800 MeV/c; 12C(π+, K+), E at 1040 MeV/c; calculated σ(θ); 15N, 10B(K-, π-), E at 800 MeV/c; 15N(π+, K+), E at 1040 MeV/c; 15N(K-, π-), E at rest; calculated relative excitation strength vs hypernucleus excitation. Configuration mixed shell model, DWIA.
doi: 10.1143/ptp/84.2.291
1990YA04 Prog.Theor.Phys.(Kyoto) 83, 254 (1990) Hypernuclear Properties Derived from the Nijmegen Soft-Core OBE Potential
doi: 10.1143/PTP.83.254
1989BA06 Phys.Rev. C39, 587 (1989) H.Bando, T.Motoba, M.Sotona, J.Zofka Polarization of Hypernuclei in the (π+, K+) Reaction NUCLEAR REACTIONS 12C, 16O, 28Si, 56Fe(π+, K+), E at 1.04 GeV/c; calculated σ(θ), hypernuclear state polarization.
doi: 10.1103/PhysRevC.39.587
1989BA27 Phys.Rev. C40, 875 (1989) Formation of Deeply Bound π- States from Hypernuclear Decay ATOMIC PHYSICS, Mesic-Atoms 28Si, 90Zr, 208Pb; calculated pion decay rates, atomic orbits, optical potentials. Hypernuclear weak decay, negative pions. NUCLEAR STRUCTURE 28Si, 90Zr, 208Pb; calculated pion decay rates, atomic orbits, optical potentials. Hypernuclear weak decay, negative pions.
doi: 10.1103/PhysRevC.40.875
1989BA39 Czech.J.Phys. B39, 906 (1989) Recent Progress in the Theory of Hypernuclei NUCLEAR REACTIONS 12C(π+, K+), E at 1.04 GeV/c; calculated σ(θ), P(θ).
1989BA92 Nuovo Cim. 102A, 627 (1989) Strangeness Production by Heavy Ions
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
1989KI19 Phys.Lett. 232B, 24 (1989) Production of Polarized Hypernuclei in the (K-, π-) Reaction in the GeV/c Region NUCLEAR REACTIONS 1n(K-, π-), E at ≈ 0.5-1.5 GeV/c; 12C(K-, π-), E at 0.7-1.5 GeV/c; calculated σ(θ), polarization.
doi: 10.1016/0370-2693(89)90552-2
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
1989SO12 Czech.J.Phys. B39, 1273 (1989) M.Sotona, J.Zofka, V.N.Fetisov, H.Bando Hypernuclear Production with a Strong Spin-Flip NUCLEAR REACTIONS 12C(π+, K+), E at 0.95-1.9 GeV/c; calculated σ(θ).
doi: 10.1007/BF01605328
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.
1988BA24 Z.Phys. A330, 203 (1988) Σ-Hypernuclear (π-, K+) Production NUCLEAR REACTIONS 56Fe, 28Si(π-, K+), E at 1-2 GeV/c; calculated σ(θ).
1988BA82 Nucl.Phys. A478, 697c (1988) Production and Decay of Hypernuclei NUCLEAR REACTIONS 56Fe, 208Pb, 9Be(π+, K+), E at 1040 MeV/c; 9Be(K-, π-), E at 720 MeV/c; 9Be(K-, π-), E at rest; calculated kaon, pion spectra.
doi: 10.1016/0375-9474(88)90907-4
1988IT02 Z.Phys. A330, 209 (1988) Pi-Mesonic Decay of Hypernuclei and Pion Wavefunction NUCLEAR REACTIONS 12C, 16O(π+, π+), E=20, 30, 40 MeV; 12C, 16O(π-, π-), E=30 MeV; calculated σ(θ).
1988MA58 Z.Phys. A331, 89 (1988) R.Mach, J.Zofka, K.Itonaga, T.Motoba, H.Bando Pions in Nuclear Interior - Sensitive Test by Hypernuclear Decay
1988MO23 Phys.Rev. C38, 1322 (1988) T.Motoba, H.Bando, R.Wunsch, J.Zofka Hypernuclear Production by the (π+, K+) Reaction NUCLEAR REACTIONS 12C, 16O, 28Si, 40Ca, 56Fe, 90Zr, 208Pb(π+, K+), E at 1040 MeV/c; calculated σ(θ), strength function; deduced effects of resonance and quasifree processes. Kapur-Peierls method, continuum shell model, DWIA analyses.
doi: 10.1103/PhysRevC.38.1322
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
1988YA09 Phys.Rev. C38, 854 (1988) T.Yamada, K.Ikeda, H.Bando, T.Motoba Cluster Model Theory of the (Lambda)9Be Hypernucleus NUCLEAR REACTIONS 9Be(K-, π-), E at 720 MeV/c; 9Be(K-, π-), E at rest; 9Be(π+, K+), E at 1040 MeV/c; calculated reaction σ.
doi: 10.1103/PhysRevC.38.854
1988YA15 Phys.Lett. 214B, 173 (1988) A Nuclear Optical Potential on the (Lambda) Hyperon NUCLEAR STRUCTURE 12C, 16O, 40Ca, 208Pb; calculated Lambda hyperon optical potentials.
doi: 10.1016/0370-2693(88)91463-3
1987EJ02 Phys.Rev. C36, 1435 (1987) H.Ejiri, T.Fukuda, T.Shibata, H.Bando, K.-I.Kubo Spin Polarization and Spin Alignment in Hypernuclei NUCLEAR REACTIONS 12C, 56Fe(π+, K+), E at 1.05 GeV/c; 12C, 56Fe(π+, K+), E at 0.72 GeV/c; calculated spin polarization, spin alignment. DWBA method.
doi: 10.1103/PhysRevC.36.1435
1987WA36 Z.Phys. A327, 59 (1987) Cluster Model Study of Light p-Shell Λ-Hypernuclei with OBE-Based Effective ΛN Interaction
1986BA81 Prog.Theor.Phys.(Kyoto) 76, 1321 (1986) Production of Hypernuclear States by the (π+, K+) Reaction NUCLEAR REACTIONS 12C, 56Fe, 208Pb(π+, K+), E at 720, 1040 MeV/c; calculated σ(θ), excitation spectra. DWIA.
doi: 10.1143/PTP.76.1321
1986YA02 Phys.Lett. 172B, 149 (1986) T.Yamada, K.Ikeda, H.Bando, T.Motoba The 9Be(K-, π-)9Be(Lambda) Hypernuclear Production Reaction with Coupled-Channel Cluster Wave Functions NUCLEAR REACTIONS 9Be(K-, π-), E at 790 MeV/c; calculated reaction strength function vs E; deduced hypernucleus levels.
doi: 10.1016/0370-2693(86)90825-7
1985BA02 Phys.Rev. C31, 265 (1985) Narrow Widths of (Lambda) Single Particle States in Hypernuclei NUCLEAR REACTIONS 40Ca(K-, π-), E at rest; analyzed data; deduced hypernuclear state widths.
doi: 10.1103/PhysRevC.31.265
1985YA05 Prog.Theor.Phys.(Kyoto) 73, 397 (1985) T.Yamada, K.Ikeda, H.Bando, T.Motoba Particle Widths of Excited States in 9Be Hypernucleus NUCLEAR REACTIONS 9Be(K-, π-), E at 790 MeV/c; calculated excitation function; deduced hypernucleus states, Γ.
doi: 10.1143/PTP.73.397
1984MO09 Prog.Theor.Phys.(Kyoto) 71, 222 (1984) (K-, π-) Reaction Cross Sections with Microscopic Cluster-Model Wave Functions for Light p-Shell Hypernuclei NUCLEAR REACTIONS 9Be(K-, π-), E at 720 MeV/c; calculated σ(θ); deduced hypernuclear level excitation possibility. DWIA, cluster model wave functions.
doi: 10.1143/PTP.71.222
1981AN18 Prog.Theor.Phys.(Kyoto) 66, 227 (1981) Single-Particle Spin-Orbit Splittings in Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated single-particle spin-orbit splittings. Reid potential, meson exchange three body forces, Pauli rearrangement effect.
doi: 10.1143/PTP.66.227
1981BA31 Prog.Theor.Phys.(Kyoto) 65, 919 (1981) Four Particle-Two Hole Correlations and the Effective Interaction Two-Level Model for Mass-42 Nuclei NUCLEAR STRUCTURE A=42; calculated levels. Multiple scattering formalism, four particle-two hole correlations, effective interactions.
doi: 10.1143/PTP.65.919
1979AN25 Prog.Theor.Phys.Suppl. No.65, 38 (1979) K.Ando, H.Bando, E.M.Krenciglowa Chapter III. Effective Interactions between Valence Nucleons NUCLEAR STRUCTURE A=14, A=18, A=38, A=42; calculated energy levels. Folded diagrams, double-partitioning, realistic nucleon-nucleon interactions.
1979BA35 Nucl.Phys. A329, 109 (1979) H.Bando, E.M.Krenciglowa, K.Ando Three-Particle One-Hole Multiple Scattering Contribution to the Nuclear Effective Interaction in Mass-18 Nuclei NUCLEAR STRUCTURE A=18; calculated energy levels; three particle-one hole multiple scattering, projection technique, valence-linked effective interaction.
doi: 10.1016/0375-9474(79)90284-7
1979IM03 Prog.Theor.Phys.(Kyoto) 62, 1422 (1979) H.Imada, Y.Kurita, H.Bando, Y.Shono Giant Isoscalar Monopole States of 16O and 40Ca by Reaction Matrix and Generator Coordinate Method NUCLEAR STRUCTURE 16O, 40Ca; calculated giant isoscalar monopole states. Reaction matrix theory, generator coordinate method.
doi: 10.1143/PTP.62.1422
1979KA37 Prog.Theor.Phys.(Kyoto) 62, 644 (1979) A Study of 24Mg by 16O+α+α Cluster Model NUCLEAR STRUCTURE 24Mg; calculated levels, wave functions, electric transition probabilities, Sα, S(8Be). Two alpha plus 16O cluster model, orthogonality condition.
doi: 10.1143/PTP.62.644
1979KR05 Nucl.Phys. A322, 145 (1979) Third-Order Treatment of the One-Body Effective Interaction NUCLEAR STRUCTURE 17O; calculated energy level spectrum. Energy dependent reaction matrix, third order contributions to one-body effective interaction.
doi: 10.1016/0375-9474(79)90338-5
1978KA22 Prog.Theor.Phys. 59, 774 (1978) Alpha- and 8Be-Spectroscopic Factors of 20Ne and 24Mg NUCLEAR STRUCTURE 20Ne, 24Mg; calculated 8Be, α S.
doi: 10.1143/PTP.59.774
1978KR02 Nucl.Phys. A294, 191 (1978) Extended Multiple-Scattering Approach for the 2p1h System and 17O Valence Energies NUCLEAR STRUCTURE 17O; calculated valence energies.
doi: 10.1016/0375-9474(78)90403-7
1976BA11 Nucl.Phys. A261, 269 (1976) Core Polarization and Alpha Clustering in 20Ne NUCLEAR STRUCTURE 20Ne; calculated levels, B(E2), α S. 16O+α-cluster model.
doi: 10.1016/0375-9474(76)90570-4
1976BA55 Nucl.Phys. A273, 95 (1976) Two-Particle One-Hole Multiple-Scattering Contribution to 17O Energies Using an Energy-Dependent Reaction Matrix NUCLEAR STRUCTURE 17O; calculated two-particle one-hole correlations. Multiple scattering theory.
doi: 10.1016/0375-9474(76)90302-X
1975KA39 Progr.Theor.Phys. 54, 1887 (1975) Study of Possible Inversion-Doublet and Other Excited States in 24Mg by a Two Alpha-Cluster Plus 16O-Core Model NUCLEAR STRUCTURE 24Mg; calculated levels in 2α cluster + 16O core model.
doi: 10.1143/PTP.54.1887
1974AN29 Progr.Theor.Phys. 52, 509 (1974) Effective Interactions in Finite Nuclei Based on Reaction Matrix Theory. I. Reaction Matrix Consistent with Model Space NUCLEAR STRUCTURE 42Sc; calculated levels.
doi: 10.1143/PTP.52.509
1974KU07 Nucl.Phys. A224, 573 (1974) Investigation of the 16O(7Li, t)20Ne and 15N(7Li, t)19F Reactions with Microscopic α-Cluster Plus Core Wave Functions NUCLEAR REACTIONS 16O, 15N(7Li, t); calculated σ(θ). 19F, 20Ne levels deduced S.
doi: 10.1016/0375-9474(74)90557-0
1972AK10 Progr.Theor.Phys.Suppl. 52, 339 (1972) Alpha-Like Four-Body Correlations and Molecular Aspects in Nuclei. Chapter VII. Nuclear Forces in Nuclei and Alpha-Clusterization NUCLEAR STRUCTURE 8Be, 12C; calculated structure parameters.
doi: 10.1143/PTPS.52.339
1972HI17 Progr.Theor.Phys.Suppl. 52, 173 (1972) Alpha-Like Four-Body Correlations and Molecular Aspects in Nuclei. Chapter IV. Alpha-Cluster Structure in Neon Region NUCLEAR STRUCTURE 20Ne; calculated levels. Many-body theory.
doi: 10.1143/PTPS.52.173
1971BA85 Progr.Theor.Phys. 45, 1515 (1971) Reaction Matrix Theory for Cluster States in Light Nuclei. II NUCLEAR STRUCTURE 12C; calculated single-particle, total energies. α-cluster model, reaction matrix theory.
1970BA75 Progr.Theor.Phys. 44, 646 (1970) Reaction Matrix Theory for Cluster States in Light Nuclei. I NUCLEAR STRUCTURE 8Be; calculated total, single-particle energies, wave functions. α-cluster model, reaction matrix theory.
1970IT02 Progr.Theoret.Phys. 44, 1232 (1970) On the Contraction of Deuteron Cluster in Li6 NUCLEAR STRUCTURE 6Li; analyzed deuteron cluster contraction.
doi: 10.1143/PTP.44.1232
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