NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = I.Silisteanu Found 29 matches. 2021SI07 Rom.J.Phys. 66, 303 (2021) Alpha-Decay Half-Lives at the Magic Shell Closures RADIOACTIVITY 104Te, 212Po, 274Ds, 296,308122(α); calculated Q-values, T1/2, proton and neutron single-particle states.
2019ZA04 Rom.J.Phys. 64, 304 (2019) M.Zadehrafi, M.R.Pahlavani, I.Silisteanu, C.I.Anghel A=14 Accompanied Ternary Fission of 242Pu in the Collinear and Equatorial Geometries Using Proximity and Yukawa Potentials NUCLEAR REACTIONS 242Pu(n, F)14C, E cold; analyzed available data; calculated relative fission yields for 14C, fission product yields.
2018SI13 Rom.J.Phys. 63, 302 (2018) A.O.Silisteanu, C.I.Anghel, I.Silisteanu Half-Lives of Nuclei Around the Superheavy Nucleus 304120 RADIOACTIVITY 104Te, 212Po, 274Ds, 302Lv, 293,294,295Og, 294,295119, 298,299,304120, 296,302,303,308122(α); calculated Q-value, T1/2. Comparison with available data.
2017AN02 Phys.Rev. C 95, 034611 (2017) α decay and spontaneous fission half-lives of nuclei around 270Hs RADIOACTIVITY 262,263,264,265,266,267,268,269,270Rf, 263,264,265,266,267,268,269,270,271Db, 264,265,266,267,268,269,270,271,272Sg, 265,266,267,268,269,270,271,272,273Bh, 266,267,268,269,270,271,272,273,274Hs, 267,268,269,270,271,272,273,274,275Mt, 268,269,270,271,272,273,274,275,276Ds, 269,270,271,272,273,274,275,276,277Rg, 270,271,272,273,274,275,276,277,278Cn(α), (SF); calculated Q(α), total α half-lives for ground-state to ground-state α transitions, spontaneous fission half-lives, branching ratios for α and SF decays. Shell model and one-body rate theories for α decay and dynamical approach for spontaneous fission defined by the shape, height of fission barrier, the fissility, and the nuclear deformations. Comparison with available experimental data.
doi: 10.1103/PhysRevC.95.034611
2017SI22 Rom.J.Phys. 62, 303 (2017) Simple Empirical Relations for α-Decay Half Lives of Superheavy Nuclei RADIOACTIVITY Rf, Db, Sg, Bh, Hs, Mt, Ds, Rg, Cn, Nh, Lv, Mc, Ts, Og(α); analyzed available data; deduced T1/2 formula.
2016BU11 Nucl.Phys. A951, 60 (2016) A.I.Budaca, R.Budaca, I.Silisteanu Extended systematics of alpha decay half lives for exotic superheavy nuclei COMPILATION Z=102-118(α); compiled T1/2; deduced Q, T1/2 systematics. Compared to data.
doi: 10.1016/j.nuclphysa.2016.03.048
2015AN04 Rom.J.Phys. 60, 444 (2015) Lifetimes of Superheavy Nuclei Around Double Magic Nucleus 270108Hs162 RADIOACTIVITY 262,263,264,265,266,267,268Rf, 263,264,265,266,267,268,269,270,271Db, 264,265,266,267,268,269,270,271,272Sg, 265,266,267,268,269,270,271,272,273Bh, 266,267,268,269,270,271,272,273,274Hs, 267,268,269,270,271,272,273,274,275Mt, 268,269,270,271,272,273,274,275,276Ds, 269,270,271,272,273,274,275,276,277Rg, 272,274,277,278Cn(SF), (α); calculated T1/2 using the systematics of data and theoretical results. Comparison with available data.
2014SI17 Rom.J.Phys. 59, 724 (2014) Competition between Alpha-Decay and Spontaneous Fission in Rf, Db, and Sg Isotopes RADIOACTIVITY 253,254,255,256,257,258,259,260,261,262,263,264,265,266,267Rf, 255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271Db, 255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,274Sg(α), (SF); calculated T1/2 for α-decay and spontaneous fission.
2013BU19 Phys.Rev. C 88, 044618 (2013) Systematic study of α-decay properties of superheavy nuclei RADIOACTIVITY 251,253,254,255,256,257,259No, 254,255,256,257,258,259,260Lr, 255,257,259,261Rf, 256,257,258,259,260,261,262,263Db, 259,260,261,263,265,266,269,271Sg, 262,264,266,267,270,271,272,274Bh, 263,264,265,266,267,269,270,271,273,275Hs, 266,268,270,274,275,276,278Mt, 267,269,270,271,273,277,279,281Ds, 272,274,278,279,280,282Rg, 277,281,283,285Cn, 278,282,283,284,285,286Nh, 286,287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294,295Og, 298,299120(α); calculated half-lives for superheavy nuclei (SHN). Shell-model rate theory with α clustering and resonance scattering amplitudes given by self-consistent models for nuclear structure and reaction dynamics. Brown relationship for α-decay half-life and Q(α). Simple fit formulas proposed for α-decay half-lives. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.044618
2013SI04 At.Data Nucl.Data Tables 98, 1096 (2013) Structure and α-decay properties of the heaviest nuclei NUCLEAR STRUCTURE Z=102-120; calculated T1/2; deduced Brown systematics. Microscopic shell model.
doi: 10.1016/j.adt.2011.12.007
2013SI27 Rom.J.Phys. 58, 1198 (2013) Study of α-Radioactivity of Superheavy Nuclei RADIOACTIVITY 267,269,270,271,273,277,279,281Ds(α); calculated T1/2. Shell model, comparison with experimental data.
2012BU12 J.Phys.:Conf.Ser. 337, 012022 (2012) Study of α-Decay Properties of Superheavy Nuclei RADIOACTIVITY Z=102-118, 120(α); compiled T1/2; deduced systematics.
doi: 10.1088/1742-6596/337/1/012022
2012SI02 Rom.J.Phys. 57, 493 (2012) Alpha-Decay Data of Superheavy Nuclei as a Source of Information about Nuclear States RADIOACTIVITY 286Fl, 281Cn, 277Ds, 273Hs, 269Sg, 282Nh, 278Rg, 274Mt, 270Bh(α); calculated T1/2. Comparison with experimental data.
2010SI27 Rom.J.Phys. 55, 1088 (2010) I.Silisteanu, A.I.Budaca, A.O.Silisteanu Systematics of α-Decay Half-Lives of the Heaviest Elements RADIOACTIVITY 253,254,255,256,257,259No, 254,255,256,257,258,259,260Lr, 255,256,257,258,259,260,261Rf, 256,257,258,259,260,261,262,263Db, 259,260,261,263,265,266,271Sg, 261,262,264,266,267,272,274Bh, 264,265,266,267,269,270Hs, 266,268,270,275,276,278Mt, 267,269,270,271,273,279Ds, 272,274,279,280,282Rg, 277,283,285Cn, 278,283,284,285,286Nh, 286,287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294,295Og, 298,299120(α); calculated T1/2. Comparison with experimental data.
2007SI32 Rom.J.Phys. 52, 775 (2007) Contributions of Aureliu Sandulescu to the Theory of Alpha Decay
2007SI33 Rom.J.Phys. 52, 807 (2007) I.Silisteanu, A.Sandru, A.O.Silisteanu, B.Popovici, A.Neacsu Theoretical Approaches to Clustering and Fine Structure in Heaviest Elements
2001SI03 Nucl.Phys. A679, 317 (2001) I.Silisteanu, W.Scheid, A.Sandulescu Proton, Alpha and Cluster Decay Rates for Nuclei with 52 ≤ Z ≤ 56 and 52 ≤ N ≤ 60 RADIOACTIVITY 105Sb, 109I, 112,113Cs, 114Ba(p); 114Ba(2p); 106,107,108,109,110Te, 110,111,112,113I, 110,111,112,113Xe, 112,113,114,115Cs, 113,114,115,116Ba(α); 113,114,115,116,117,118Ba(12C); calculated T1/2. comparisons with data. NUCLEAR STRUCTURE Z=52-56; Z=84-88; analyzed decay energies, lifetimes; deduced systematic features.
doi: 10.1016/S0375-9474(00)00336-5
1996SI20 Roum.J.Phys. 41, 43 (1996) Evidence for Similar Alpha and Cluster Decay Properties in the Trans-Tin and Trans-Lead Regions RADIOACTIVITY 106Te, 120Xe, 113I, 115Cs, 114Ba, 214Po, 218Rn, 221At, 227Ra, 221Fr; analyzed, calculated α-decay T1/2. 222,221,223,224,225,226Ra(14C); 114,113,115,116,117,118Ba(12C); calculated cluster decay T1/2. Other nuclei, other decays also considered.
1995SI05 Phys.Rev. C51, 2023 (1995) Half-Lives of Cluster Radioactivity within a Model Including Superfluid Phenomena and Resonance Effects RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 231Pa(23F); 230Th, 231Pa, 232,233,234U(24Ne); 232Th, 234U(26Ne); 233U(25Ne); 234U, 238Pu(28Mg); 238Pu(32Si); 241Am(34Si); calculated cluster decay T1/2. Continuum hopping model, superfluid phenomena, resonance effects.
doi: 10.1103/PhysRevC.51.2023
1993SC38 Roum.J.Phys. 38, 331 (1993) W.Scheid, I.Silisteanu, A.Sandulescu Lifetimes of Cluster Radioactivity of Neutron Deficient Trans-Tin Isotopes RADIOACTIVITY A=114-241; analyzed cluster decay T1/2 vs Q data. 114Ba deduced 12C-decay T1/2, branching ratio relative to α-decay.
1993SI26 Roum.J.Phys. 38, 55 (1993) I.Silisteanu, M.Ivascu, I.Rotter The Excitation of Collective Modes in Heavy Fragment Radioactivity RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 231Pa(23F); 230,232Th, 231Pa, 234,232,233U(24Ne); 233U(25Ne); 234U(26Ne); 234U, 238Pu(28Mg); 237Np, 238Pu(30Mg); 238Pu(32Si); 241Am(34Si); calculated cluster decay resonance width, decay T1/2. Collective mode excitation, microscopic, macroscopic method.
1993SI27 Roum.J.Phys. 38, 329 (1993) I.Silisteanu, W.Scheid, M.Ivascu Alpha and 12C Emission Energies of 114Ba RADIOACTIVITY 114Ba(α), (12C); analyzed Qα data in other Ba, Cs, Xe, I, Te isotopes; deduced α-, 12C-decay Qα, mass excess.
1990IV01 Fiz.Elem.Chastits At.Yadra 21, 1405 (1990); Sov.J.Part.Nucl. 21, 599 (1990) Cluster Radioactivity Half-Lives RADIOACTIVITY A=221-252; compiled, reviewed cluster decay T1/2 data, model results.
1989SI13 J.Phys.(London) G15, 1405 (1989) Estimates of the Influence of Nuclear Deformations on the Lifetimes of Heavy-Fragment Radioactivities RADIOACTIVITY 234,232U(24Ne); 234U, 234Pu(28Mg); 241Am, 237Np(30Mg); 240,246Cm, 240Pu, 241Am(34Si); calculated fragment emission energy, T1/2; deduced deformations role.
doi: 10.1088/0954-3899/15/9/010
1988IV02 Nucl.Phys. A485, 93 (1988) The Microscopic Approach to the Rates of Radioactive Decay by Emission of Heavy Clusters RADIOACTIVITY 222,223,224,226Ra, 231Pa, 232,233U(α), (12C), (24Ne); calculated α-, cluster-decay T1/2, ratios, spectroscopic factor, Γ ratios. Microscopic model.
doi: 10.1016/0375-9474(88)90524-6
1988SI09 Rev.Roum.Phys. 33, 267 (1988) The Instability of Rapidly Rotating Nuclei Towards Emission of α-Particles RADIOACTIVITY 74Kr, 122Xe(α); calculated T1/2, emission rates.
1987IV01 Rev.Roum.Phys. 32, 549 (1987) M.Ivascu, A.Sandulescu, I.Silisteanu On the Rates of Radioactive Decays by Emission of Heavy Clusters RADIOACTIVITY 222,223,224,226Ra(14C), 231Pa, 232,233U(24Ne); calculated T1/2, branching ratios, one-body resonance widths, cluster spectroscopic factors. Microscopic-macroscopic method.
1986NA02 Yad.Fiz. 43, 58 (1986) α Decay of Fast Rotating Nuclei RADIOACTIVITY 122Xe(α); calculated T1/2, α-formation factor. Fast rotating nuclei.
1983SI16 Rev.Roum.Phys. 28, 331 (1983) Alpha Decay Rates of Neutron Deficient Trans-Tin Isotopes RADIOACTIVITY 106,107,108,109,110Te, 108,109,110,111,112,113I, 108,109,110,111,112,113Xe, 109,110,111,112,113,114,115Cs, 110,111,112,113,114,115,116Ba; calculated Eα, T1/2, α-decay rates. Unified theory, one-body, shell model approaches.
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