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NSR database version of April 27, 2024.

Search: Author = S.N.Kuklin

Found 8 matches.

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2016KU10      Physics of Part.and Nuclei 47, 206 (2016)

S.N.Kuklin, G.G.Adamian, N.V.Antonenko

Description of alpha decay and cluster radioactivity in the dinuclear system model

RADIOACTIVITY 184,186,188,190,192,194,196,198,200,202,204,206,208Po, 194,196,198,200,202,204,206,208,210Rn, 233U(α); calculated T1/2, spectroscopic factor as a function of the mass number A. Comparison with available data.

NUCLEAR STRUCTURE 224,226,228,230,232,234,236,238U, 224,226Th; calculated energy levels, J, π. Comparison with available data.

doi: 10.1134/S1063779616020039
Citations: PlumX Metrics


2012KU23      Eur.Phys.J. A 48, 112 (2012)

S.N.Kuklin, T.M.Shneidman, G.G.Adamian, N.V.Antonenko

Alpha-decay fine structures of U isotopes and systematics for isotopic chains of Po and Rn

RADIOACTIVITY 228Th(20O), 222Ra(14C), 232U(24Ne), 234U(26Ne), 236U(30Mg), 236Pu(28Mg), 238Pu(32Si); calculated T1/2. 184,186,188,190,192,194,196,198,200,202,204,206,208Po, 194,196,198,200,202,204,206,208,210Rn, 224,226,228,230,232,234,236,238U(α); calculated α spectroscopic factor for low-lying positive parity states, T1/2. Zero-point vibrations in the charge-asymmetry coordinate; compared to data.

NUCLEAR STRUCTURE 184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn; calculated α cluster spectroscopic factor using zero-point vibrations in the charge-asymmetry coordinate. Compared to data.

doi: 10.1140/epja/i2012-12112-8
Citations: PlumX Metrics


2011AD15      Phys.Rev. C 84, 024324 (2011)

G.G.Adamian, N.V.Antonenko, S.N.Kuklin, B.N.Lu, L.A.Malov, S.G.Zhou

Behavior of one-quasiparticle levels in odd isotonic chains of heavy nuclei

NUCLEAR STRUCTURE 255Fm, 257No, 259Rf, 261Sg, 263Hs; calculated ground state deformation parameters β2 and β4. 239U, 241,243,247Pu, 243,245,247,249Cm, 243,245,247,249,251Cf, 241,243,245,247,249,251,253,255Fm, 245,247,249,251,253,255,257No, 255,257,259Rf, 259,261Sg, 263Hs; calculated one-quasiparticle states in N=147, 149, 151, 153, 155 nuclei. 253No; calculated collective rotational bands. Discussed isomers in odd-A Fm and No nuclei. Two-center shell model (TCSM), quasiparticle-phonon model (QPM), Skyrme-Hartree-Fock-Bogolyubov (SHFB) approach with SLy4 and SkP parameterization. Comparison with experimental data.

RADIOACTIVITY 257,257mRf, 257,257mNo(α); calculated Q(α), decay schemes. 253Fm, 253No; deduced levels.

doi: 10.1103/PhysRevC.84.024324
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2010AD19      Phys.Rev. C 82, 054304 (2010)

G.G.Adamian, N.V.Antonenko, S.N.Kuklin, W.Scheid

One-quasiparticle states in odd-Z heavy nuclei

NUCLEAR STRUCTURE 253Lr, 257Db, 261Bh, 265Mt, 269Rg; calculated β2, β4, β6 deformation parameters. 249Md; calculated potential energy surface in the β2, β4 plane. 237Np, 243,245,247,249,251,253,255Es, 243,245,247,249,251,253,255,257Md, 253,255Lr, 257Db, 261Bh, 265Mt, 269Rg; calculated low-lying one-quasiparticle spectra, rotational bands using two-center shell model (TCSM) approach. 252Md; calculated 2-quasiparticle low-lying states. Comparison with experimental data.

RADIOACTIVITY 257Db, 253,255Lr, 251Md(α); proposed α- and γ-decay schemes based on one-quasiparticle spectra. 247,249,251,253,255,257Md, 265Mt, 269Rg(α); calculated Q(α); proposed decay schemes. Comparison with experimental data. Two-center shell model (TCSM) approach.

doi: 10.1103/PhysRevC.82.054304
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2008KU21      Int.J.Mod.Phys. E17, 2020 (2008)

S.N.Kuklin, G.G.Adamian, N.V.Antonenko, W.Scheid

Cluster features of strongly deformed nuclei shapes

NUCLEAR REACTIONS 58Ni(58Ni, X), 86Kr(86Kr, X), 88Sr(88Sr, X), 48Ca(140Ce, X), (142Nd, X), (144Sm, X), E(cm) = 117, 155, 166, 147, 148, 149 MeV; calculated nucleus-nucleus potentials for high-spin hyperdeformed isomers.

RADIOACTIVITY 234,236,238U, 236,239,240Pu, 240Am, 230,231,233Th(SF); 50Ca, 184,186Hf, 28,30,32Mg, 206Hg, 208,209Pb, 32Al, 50Ca, 181,182,183Yb; calculated cluster decay level energies, rotational parameters, charge quadrupole and octupole moments.

doi: 10.1142/S021830130801101X
Citations: PlumX Metrics


2007AN28      Phys.Atomic Nuclei 70, 1649 (2007)

A.V.Andreev, G.G.Adamian, N.V.Antonenko, S.P.Ivanova, S.N.Kuklin, W.Scheid

Cluster aspects of binary and ternary fission

RADIOACTIVITY 256,258Fm(SF), 256,258,262No(SF); calculated kinetic energy and charge distribution of fission fragments using a statistical model.

doi: 10.1134/S1063778807090268
Citations: PlumX Metrics


2005KU04      Phys.Rev. C 71, 014301 (2005)

S.N.Kuklin, G.G.Adamian, N.V.Antonenko

Spectroscopic factors and cluster decay half-lives of heavy nuclei

RADIOACTIVITY 112,114,116,118Ba, 118Ce, 122Nd, 124,126Sm, 220Ra(12C), (16O); 122Nd(20Ne), (24Mg); 126Sm(24Mg), (28Si); 221Fr(14C); 221,222,223Ra(14C), (15N), (18O); 224,226Ra(14C), (20O), (24Ne); 225Ac(14C), (17N), (18O), (23F), (24Ne), (27Na), (28Mg); 224Th(14C), (15N), (16O), (21F), (24Ne), (28Mg), (29Al), (32Si); 226Th(14C), (15N), (18O), (21F), (24Ne), (27Na), (28Mg), (32Si); 228Th(14C), (20O), (23F), (24Ne), (28Mg); 229Th(14C), (16N), (21O), (23F), (24Ne), (28Mg); 230Th(24Ne); 231Pa(22O), (23F), (24Ne), (27Na), (28Mg), (31Al); 232Pa(25Ne), (27Na), (28Mg); 230U(14C), (20O), (24Ne), (27Na), (28Mg), (32Si); 232U(23F), (24Ne), (27Na), (28Mg), (32Si); 233U(25Ne), (27Na), (28Mg); 234U(26Ne), (27Na), (28Mg); 235U(26Ne), (29Mg); 236U(30Mg); 234,236Pu(24Ne), (27Na), (28Mg), (29Al), (32Si); 237Pu(29Mg), (30Al), (32Si); 238Pu(30Mg), (31Al), (32Si); 242Cm(34Si); calculated cluster decay T1/2, Q-values.

doi: 10.1103/PhysRevC.71.014301
Citations: PlumX Metrics


2005KU32      Yad.Fiz. 68, 1501 (2005); Phys.Atomic Nuclei 68, 1443 (2005)

S.N.Kuklin, G.G.Adamian, N.V.Antonenko

Spectroscopic Factors and Barrier Penetrabilities in Cluster Radioactivity

RADIOACTIVITY 112,114,116,118Ba, 118Ce, 122Nd, 124,126Sm, 220Ra(12C), (16O); 122Nd(20Ne), (24Mg); 126Sm(24Mg), (28Si); 221Fr(14C); 221,222,223Ra(14C), (15N), (18O); 224,226Ra(14C), (20O), (24Ne); 225Ac(14C), (17N), (18O), (23F), (24Ne), (27Na), (28Mg); 224Th(14C), (15N), (16O), (21F), (24Ne), (28Mg), (29Al), (32Si); 226Th(14C), (15N), (18O), (21F), (24Ne), (27Na), (28Mg), (32Si); 228Th(14C), (20O), (23F), (24Ne), (28Mg); 229Th(14C), (16N), (21O), (23F), (24Ne), (28Mg); 230Th(24Ne); 231Pa(22O), (23F), (24Ne), (27Na), (28Mg), (31Al); 232Pa(25Ne), (27Na), (28Mg); 230U(14C), (20O), (24Ne), (27Na), (28Mg), (32Si); 232U(23F), (24Ne), (27Na), (28Mg), (32Si); 233U(25Ne), (27Na), (28Mg); 234U(26Ne), (27Na), (28Mg); 235U(26Ne), (29Mg); 236U(30Mg); 234,236Pu(24Ne), (27Na), (28Mg), (29Al), (32Si); 237Pu(29Mg), (30Al), (32Si); 238Pu(30Mg), (31Al), (32Si); 242Cm(34Si); calculated cluster decay T1/2, Q-values, spectroscopic factors, penetrabilities. Dinuclear system approach.

doi: 10.1134/1.2053330
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