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NSR database version of April 27, 2024.

Search: Author = Y.A.Bogila

Found 5 matches.

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1996BO05      Phys.Rev. C53, 855 (1996)

Ye.A.Bogila, V.M.Kolomietz, A.I.Sanzhur, S.Shlomo

Preequilibrium Decay in the Exciton Model for Nuclear Potential with a Finite Depth

NUCLEAR STRUCTURE ⁴⁰Ca; calculated transition, total decay rates for given exciton state, preequilibrium nucleon emission particle spectra. Exciton model, particle-hole level density.

doi: 10.1103/PhysRevC.53.855
Citations: PlumX Metrics

1996BO13      Yad.Fiz. 59, No 5, 808 (1996); Phys.Atomic Nuclei 59, 770 (1996)

Ye.A.Bogila, V.M.Kolomietz, A.I.Sanzhur

Energy Dependence of Transition Rates in the Exciton Model

NUCLEAR REACTIONS, ICPND ¹¹¹Cd(p, n), (p, 2n), (p, 3n), E ≈ threshold-50 MeV; analyzed σ(E). Exciton model, perturbation theory based intermediate state transition rates.

1995BO25      Phys.Rev.Lett. 75, 2284 (1995)

Ye.A.Bogila, V.M.Kolomietz, A.I.Sanzhur, S.Shlomo

Angular Momentum Dependence of Transition Rates in the Exciton Model

NUCLEAR REACTIONS, ICPND ¹¹¹Cd(p, 2n), E ≈ 15-50 MeV; calculated isomeric ratio vs E. Exciton model with angular momentum dependent transition rates.

doi: 10.1103/PhysRevLett.75.2284
Citations: PlumX Metrics

1995SH34      Z.Phys. A353, 27 (1995)

S.Shlomo, Ye.A.Bogila, V.M.Kolomietz, A.I.Sanzhur

Fixed Exciton Number Level Density for a Finite Potential Well

NUCLEAR STRUCTURE ⁴⁰Ca, ²⁰⁸Pb; calculated low number excitons associated level density function relative to that of Ericson-Strutinsky vs E; deduced potential well depth, surface thickness finiteness role.

doi: 10.1007/BF01297723
Citations: PlumX Metrics

1993BO37      Z.Phys. A347, 49 (1993)

Y.A.Bogila, V.M.Kolomietz, A.I.Sanzhur

Relaxation Time of Nonequilibrium Nuclear System

NUCLEAR STRUCTURE A=90; calculated nonequilibrium state relaxation time. Exciton model, equilibrium transition rates used.

doi: 10.1007/BF01301276
Citations: PlumX Metrics