NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = D.Galeriu Found 6 matches. 1987IV05 Rev.Roum.Phys. 32, 937 (1987) M.Ivascu, D.B.Ion, D.Bucurescu, G.Cata, D.Cutoiu, D.Galeriu, R.Ion-Mihai, N.V.Zamfir Search for Spontaneous Emission of Mesons from 252Cf RADIOACTIVITY 252Cf(SF); measured (light particle)(heavy particle)-coin; deduced meson decay branching upper limits.
1986GA04 J.Phys.(London) G12, 329 (1986) D.Galeriu, D.Bucurescu, M.Ivascu Nuclear Deformations in the A ≈ 80-100 Region NUCLEAR STRUCTURE 77,79,81,82,83,84,85,86,90,91,92,93,94,95,96,97,98,99Sr, 99,100,101,102,103,104,105,106,107,108,109,110,111,112Pd; calculated mass excess errors. 92,98,100Zr; calculated mass coefficient vs deformation. 92,93,94,95,96,97,98,99,100Zr; calculated stiffness coefficient. 92,94,96,98Zr; calculated 2+ levels. 92,94,96,98,100,102,104,106Mo; calculated dynamic deformation vs N. 81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102Zr, 93,95,97,99,101Sr, 97,99,101Mo; calculated Fermi energy nucleon number dependence. 100,102,106Mo, 96,98,100,101,102,103Zr, 76,77,78,96,98Sr, 72,73,74,75,76,78Kr; calculated potential energy surfaces. Strutinsky approach, Nilsson type potential.
doi: 10.1088/0305-4616/12/4/006
1983GA05 J.Phys.(London) G9, 309 (1983) The Beta Strength Function of 240Bk and the Fission Barrier of Neutron-Deficient Actinides NUCLEAR STRUCTURE 244,246,248Cf; 248,250Fm; calculated fission barrier heights. Experimental data, β-decay strength function inputs. RADIOACTIVITY 240Bk [from 241Am(3He, 4n), E=33 MeV]; measured β+-delayed fission T1/2; deduced β+-delayed fission probability. 240Cm deduced fission barrier parameters. β-decay strength function input. NUCLEAR REACTIONS, ICPND 241Am(3He, 4n), E=33 MeV; measured production σ for 240Bk.
doi: 10.1088/0305-4616/9/3/011
1983GA20 Rev.Roum.Phys. 28, 477 (1983) Ground State Properties of Actinide Nuclei NUCLEAR STRUCTURE 237U, 247Cm; calculated single-particle E(n). 238U, 241Pu, 246Cm; calculated potential energy surfaces. 230,231,232,233,234,235,236,237,239,240U, 229,230,231,232,233,234,235,236,237,238,239,240,241,242,243Pu, 238,239,240,241,242,243,244,245,246,247,248,249,250Cm, 242,243,244,245,246,247,248,249,250,251,252,253Cf, 244,245,246,247,248,249,250,251,252,253,254,255Fm; calculated mass excess differences. 234,236,238U, 235,237,239,241Pu, 242,244,246Cm; calculated electric quadrupole moment. 230Th; calculated level density energy dependence. A=230-255; calculated level spacing, ratio to data. Macroscopic-microscopic method.
1978CI05 Rev.Roum.Phys. 23, 527 (1978) E.Cincu, D.Galeriu, E.Georgescu, M.Marinescu, I.Vilcov, N.Vilcov Subthreshold Fission Cross-Section Measurements of 236,239U Isotopes. A Comparison with Theoretical Computations Based on the Two-Center Shell Model NUCLEAR REACTIONS 235,238U(d, pF), E=12 MeV; measured subthreshold fission probabilities. 236,239U deduced experimental fission barrier; compared with predictions of two-center shell model.
1975BO54 Rev.Roum.Phys. 20, 985 (1975) E.Bodo, D.Galeriu, M.Marinescu, D.N.Poenaru, I.Vilcov, N.Vilcov Angular Distribution of Recoil Nuclei NUCLEAR REACTIONS 239Pu(α, xn), E=26 MeV; measured angular distribution of recoil nuclei.
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