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NSR database version of April 27, 2024.

Search: Author = G.Batko

Found 12 matches.

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1995LE05      Phys.Rev. C51, 2113 (1995)

E.Lehmann, R.K.Puri, A.Faessler, G.Batko, S.W.Huang

Consequences of a Convariant Description of Heavy-Ion Reactions at Intermediate Energies

NUCLEAR REACTIONS C(C, X), E=50 MeV/nucleon; Ca(Ca, X), E=1.5, 2 GeV/nucleon; calculated nucleon flow, directed transverse flow; deduced convariant description importance. Relativistic quantum molecular dynamics approach.

doi: 10.1103/PhysRevC.51.2113
Citations: PlumX Metrics

1994BA19      J.Phys.(London) G20, 461 (1994)

G.Batko, A.Faessler, S.W.Huang, E.Lehmann, R.K.Puri

Does the Reduction of the Mass in the Medium Enhance the Production of Antiprotons in High-Energy Nuclear Reactions ( Question )

NUCLEAR REACTIONS Ni(Ni, X), E=1.93 GeV/nucleon; Cu(C, X), E=3.65 GeV/nucleon; calculated antiproton invariant spectra, σ(θ); deduced medium effects role in anti-proton production.

doi: 10.1088/0954-3899/20/3/007
Citations: PlumX Metrics

1994PU03      Nucl.Phys. A575, 733 (1994)

R.K.Puri, N.Ohtsuka, E.Lehmann, A.Faessler, M.A.Matin, D.T.Khoa, G.Batko, S.W.Huang

Temperature-Dependent Mean Field and Its Effect on Heavy-Ion Reactions

NUCLEAR REACTIONS 40Ca(40Ca, X), 93Nb(93Nb, X), E=400 MeV/nucleon; calculated maximum, average densities, transverse flow time evolution. Temperature dependent mean field nucleon potentials.

doi: 10.1016/0375-9474(94)90164-3
Citations: PlumX Metrics

1993BA51      Nucl.Phys. A563, 97 (1993)

G.Batko, J.Randrup

BUU Dynamics of Unbound Spherical Nuclei

NUCLEAR STRUCTURE 40Ca, 197Au; calculated collective flow, density distribution. Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1016/0375-9474(93)90012-M
Citations: PlumX Metrics

1992BA37      Nucl.Phys. A546, 761 (1992)

G.Batko, J.Randrup, T.Vetter

Effect of N-Body Collisions on Subthreshold Kaon Production in High-Energy Nuclear Reactions

NUCLEAR REACTIONS 93Nb(93Nb, xK+), Ca(Ca, xK+), 197Au(197Au, xK+), E=600-1000 MeV/nucleon; calculated differential K+ multiplicity, energy spectra; deduced N-body collisions play minor role.

doi: 10.1016/0375-9474(92)90006-6
Citations: PlumX Metrics

1991BA13      Phys.Lett. 256B, 331 (1991)

G.Batko, W.Cassing, U.Mosel, K.Niita, Gy.Wolf

Antiproton Production in p-Nucleus and Nucleus-Nucleus Collisions

NUCLEAR REACTIONS 28Si(28Si, X), E=2.1 GeV/nucleon; 63Cu(p, X), E=4-6.1 GeV; calculated p-bar production invariant σ. Vlasov-Uehling-Uhlenbeck transport theory.

doi: 10.1016/0370-2693(91)91771-M
Citations: PlumX Metrics

1991CA20      Z.Phys. A340, 51 (1991)

W.Cassing, G.Batko, T.Vetter, G.Wolf

Eta Production in Proton-Nucleus Reactions

NUCLEAR REACTIONS 12C(p, X), E=0.7-1 GeV; calculated eta production σ(θ). Primary, secondary production, folding model.

doi: 10.1007/BF01284480
Citations: PlumX Metrics

1990CA15      Phys.Lett. 238B, 25 (1990)

W.Cassing, G.Batko, U.Mosel, K.Niita, O.Schult, Gy.Wolf

Subthereshold K+-Production in Proton-Nucleus Reactions

NUCLEAR REACTIONS U, 12C(p, X), E ≈ 1 GeV; calculated K+, π0 differential production probability.

doi: 10.1016/0370-2693(90)92094-Y
Citations: PlumX Metrics

1988BA26      Phys.Rev. C37, 2647 (1988)

G.Batko, O.Civitarese

Nuclear Stratosphere Formation and Its Effects upon Statistical Particle Emission Processes

NUCLEAR STRUCTURE 28Si; calculated p-, α-emission Γ, angle integrated σ. Nuclear stratosphere formation.

doi: 10.1103/PhysRevC.37.2647
Citations: PlumX Metrics

1987BA25      Phys.Rev. C36, 435 (1987)

G.Batko, O.Civitarese, A.L.De Paoli

Compound Nucleus Temperatures from Particle and Gamma Ray Emissions: Effects due to the temperature dependence of the level density parameter

NUCLEAR STRUCTURE 146Sm; calculated level density parameter, particle, γ-ray emission probability vs excitation; deduced temperature dependence.

doi: 10.1103/PhysRevC.36.435
Citations: PlumX Metrics

1987BA36      Z.Phys. A327, 323 (1987)

G.Batko, O.Civitarese, A.L.De Paoli

Temperature Dependent Effects upon Statistical Particle and Gamma Ray Emission from a Compound Nucleus

NUCLEAR REACTIONS 147Sm(n, γ), 147Sm(γ, n), E not given; calculated average γ multiplicity vs excitation energy. Fermi gas model.

NUCLEAR STRUCTURE 147Sm; calculated level density parameter vs nuclear temperature, neutron, γ ray emission probabilities. Fermi gas model.

1987BA37      Z.Phys. A327, 329 (1987)

G.Batko, O.Civitarese, A.L.De Paoli

On the Temperature Dependence of the Level Density Parameter and Its Effect upon Neutron Evaporation Spectra

NUCLEAR STRUCTURE 209Pb; calculated neutron emission probabilities, total decay, widths, level density parameter vs excitation energy, angular momentum. Fermi gas model.

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