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NSR database version of April 29, 2024.

Search: Author = Y.Kitazoe

Found 10 matches.

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1975KI20      Lett.Nuovo Cim. 14, 407 (1975)

Y.Kitazoe, M.Sano

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
Citations: PlumX Metrics

1973KI14      Atomkernenergie 22, 214 (1973)

Y.Kitazoe, H.Suzuki, T.Sekiya

Intermediate Resonances in the Neutron Total Cross Section of ²³⁵U at Low Energies. II

NUCLEAR REACTIONS ²³⁵U(n, X), E < 100 keV; calculated total σ(E).

1972KI14      Prog.Theor.Phys. 47, 470 (1972)

Y.Kitazoe, T.Sekiya

An Approach to the Unified Theory of Nuclear Reactions

doi: 10.1143/PTP.47.470
Citations: PlumX Metrics

1972KI22      Atomkernenergie 20, 13 (1972)

Y.Kitazoe, H.Suzuki, T.Sekiya

Intermediate Resonances in the Neutron Total Cross Section of ²³⁵U at Low Energies

NUCLEAR REACTIONS ²³⁵U(n, X); calculated σ.