NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = E.Holub Found 13 matches. 1986HO01 Phys.Rev. C33, 143 (1986) E.Holub, D.Hilscher, G.Ingold, U.Jahnke, H.Orf, H.Rossner, W.P.Zank, W.U.Schroder, H.Gemmeke, K.Keller, L.Lassen, W.Lucking Preequilibrium Neutron Emission in Fusion of 165Ho + 12C at 25 MeV per Nucleon NUCLEAR REACTIONS 165Ho(12C, nX), E=300 MeV; measured σ(fragment θ, θn, En), neutron multiplicity; deduced neutron emission mechanism. Fermi-jet model.
doi: 10.1103/PhysRevC.33.143
1984KO22 Nuovo Cim. 81A, 31 (1984) M.Korolija, E.Holub, N.Cindro, D.Hilscher Pre-Equilibrium Emission of Nucleons from Reactions Induced by Medium-Energy Heavy Ions NUCLEAR REACTIONS 165Ho(20Ne, xn), E=220, 292, 402 MeV; 158Gd(12C, xn), E=103, 124, 150 MeV; 157Gd(13C, xn), E=110, 140, 160 MeV; 154Sm(16O, xn), E=151.9 MeV; 238U(16O, xn), E=315 MeV; analyzed fast neutron spectra; deduced initial exciton number, degrees of freedom number near equality. Preequilibrium models.
1983CA23 Z.Phys. A313, 227 (1983) R.Caplar, I.Udovicic, E.Holub, D.Pocanic, N.Cindro Isotopic Effects in the (n, p) Reaction Cross Section on Heavy Targets and the Statistical Preequilibrium Model NUCLEAR REACTIONS 122,124,126,128,130Te(n, p), E=14.6 MeV; 128,130,131,132,134Xe(n, p), E=14.4 MeV; 180,182,183,184,186W, 188,189,190,192Os(n, p), E=14.7 MeV; calculated σ; deduced proton, neutron separation energy role. Statistical preequilibrium model.
1983HO13 Phys.Rev. C28, 252 (1983) E.Holub, D.Hilscher, G.Ingold, U.Jahnke, H.Orf, H.Rossner Neutron Emission in Central Heavy-Ion Collisions of 165Ho + 20Ne at 11, 14.6, and 20.1 MeV/Nucleon NUCLEAR REACTIONS 165Ho(20Ne, nX), E=220, 290, 402 MeV; measured σ(En, θn, fragment θ, fragment E); deduced prefission neutron multiplicity, multiple chance fission probability. Harp-Miller-Berne model.
doi: 10.1103/PhysRevC.28.252
1983HO26 Z.Phys. A314, 347 (1983) Preequilibrium Emission of Nucleons from Reactions Induced by Medium-Energy Heavy Ions NUCLEAR REACTIONS 153Gd(12C, X), E=103, 124, 150 MeV; 157Gd(13C, X), E=110, 140, 160 MeV; 154Sm(16O, X), (16O, F), E=152 MeV; 238U(16O, X), (16O, F), E=315 MeV; 165Ho(20Ne, X), (20Ne, F), E=220, 292, 402 MeV; calculated (evaporation residue)(n)-, fission(fragment)(n)-coin spectra; deduced preequilibrium neutron emission energy dependence. Exciton, equilibration models.
doi: 10.1007/BF01412931
1983RO09 Phys.Rev. C27, 2666 (1983) H.Rossner, D.Hilscher, E.Holub, G.Ingold, U.Jahnke, H.Orf, J.R.Huizenga, J.R.Birkelund, W.U.Schroder, W.W.Wilcke Angular Distributions of Fragments from Fission Induced by 220-MeV 20Ne on Targets of 165Ho, 197Au, and 209Bi NUCLEAR REACTIONS 165Ho, 197Au, 209Bi(20Ne, F), E=220 MeV; measured fission fragment σ(θ). 197Ir, 211Ac, 223Np, 175Re, 207Fr, 219Pa; deduced prefission multi-neutron induced angular momentum dealignment effect. Liquid drop, rotating liquid drop models, incomplete fusion, prefission particle emission mechanisms.
doi: 10.1103/PhysRevC.27.2666
1982JA01 Phys.Rev.Lett. 48, 17 (1982) U.Jahnke, H.H.Rossner, D.Hilscher, E.Holub Global Increase of Near- and Below-Barrier Fusion for Heavier Systems NUCLEAR REACTIONS 12C, 16O, 58,60,62,64Ni, 104,110Pd, 118,124Sn, 130Te(40Ar, xn), E(cm)=90-120 MeV; 154,144Sm, 110Pd(16O, xn), E(cm)=55-70 MeV; 110Pd, 124Sn, 130Te(12C, xn), 58,62,64Ni(86Kr, xn), E not given; measured neutron production σ; deduced σ(fusion, E), barrier dependence, shape distortions.
doi: 10.1103/PhysRevLett.48.17
1981DR01 Phys.Lett. B98, 36 (1981) D.M.Drake, M.Cates, N.Cindro, D.Pocanic, E.Holub Gross Structure and Resonant Behaviour of 14C + 14C Elastic Scattering NUCLEAR REACTIONS 14C(14C, 14C), E=23.4-58.4 MeV; measured σ(θ, E); deduced gross structure, resonant behavior. Optial model analysis.
doi: 10.1016/0370-2693(81)90362-2
1981PO05 J.Phys.(London) G7, 389 (1981) D.Pocanic, G.Vourvopoulos, X.Aslanoglou, E.Holub Possible Evidence for the Existence of Intermediate Resonant Structure in the 9Be + 13C Heavy-Ion System NUCLEAR REACTIONS 13C(9Be, α), E=8-22.75; measured σ(E, θ). 22Ne deduced possible intermediate resonances. Statistical analysis.
doi: 10.1088/0305-4616/7/3/014
1980HO23 Z.Phys. A296, 341 (1980) E.Holub, D.Pocanic, R.Caplar, N.Cindro A Consistent Study of Precompound and Compound-Nucleus Emission Mechanisms in Neutron-Induced Reactions NUCLEAR REACTIONS 45Sc, 55Mn, 56Fe, 59Co, 89Y, 93Nb, 103Rh, 169Tm, 175Lu, 181Ta, 197Au, 209Bi(n, n'), (n, p), (n, 2n), (n, 3n), E=4-24 MeV; calculated σ(E); deduced exciton model parameter K. Weisskopf-Ewing evaporation, precompound exciton models.
doi: 10.1007/BF01438529
1979HO03 Z.Phys. A289, 421 (1979) E.Holub, N.Cindro, O.Bersillon, J.Jary Investigation of (n, 2n) Reactions by the Evaporation Process NUCLEAR REACTIONS 45Sc, 56Fe, 59Co, 89Y, 93Nb, 103Rh, 148,150,152,154Sm, 169Tm, 175Lu, 197Au, 209Bi(n, 2n), E=5-20 MeV; calculated σ. Evaporation model; deduced reaction mechanism.
doi: 10.1007/BF01409395
1977CI01 Phys.Rev.Lett. 39, 1135 (1977) N.Cindro, F.Cocu, J.Uzureau, Z.Basrak, M.Cates, J.M.Fieni, E.Holub, Y.Patin, S.Plattard Evidence for a Rotational Band in 24Mg and its Fragmentation: A Rotation-Vibration Coupling (Question) NUCLEAR REACTIONS 12C(12C, α), E(cm)=6.85-15 MeV; measured σ(Eα, θ). 24Mg deduced resonances, J, π.
doi: 10.1103/PhysRevLett.39.1135
1976HO15 J.Phys.(London) G2, 405 (1976) Study of Some Systematic Trends and Non-Equilibrium Effects in (n, 2n) Reactions for Nuclei Far from the Symmetry Line NUCLEAR REACTIONS 84,86,88Sr, 93Nb, 113In, 134,136Ba(n, 2n), E=14.6 MeV; measured activation σ, isomeric σ ratios. Systematics. Natural targets; enriched, natural In target; Ge(Li) detector.
doi: 10.1088/0305-4616/2/6/009
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