NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = D.D.Ni Found 52 matches. 2020NI01 Phys.Rev. C 101, 044308 (2020) Effects of nuclear collective vibrations on the α-decay fine structure of vibrational nuclei with A ≈ 220 RADIOACTIVITY 204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 220,222,224,226Th, 222,224,226U(α); calculated α-branching ratio to various vibrational states, and α-decay half-lives using multichannel cluster model (MCCM). Comparison with experimental values, and with other theoretical calculations.
doi: 10.1103/PhysRevC.101.044308
2020SH10 Chin.Phys.C 44, 054103 (2020) X.-X.Shi, Q.Liu, D.-D.Ni, J.-Y.Guo, Z.-Z.Ren The first excited single-proton resonance in 15F by complex-scaled Green's function method NUCLEAR STRUCTURE 15F; calculated eigenvalues of resonant states, resonance energies and widths, level densities, phase shifts, σ using the complex-scaled Green's function (CGF) method.
doi: 10.1088/1674-1137/44/5/054103
2019SH37 Phys.Lett. B 797, 134820 (2019) Y.P.Shen, B.Guo, T.L.Ma, D.Y.Pang, D.D.Ni, Z.Z.Ren, Y.J.Li, Z.D.An, J.Su, J.C.Liu, Q.W.Fan, Z.Y.Han, X.Y.Li, Z.H.Li, G.Lian, Y.Su, Y.B.Wang, S.Q.Yan, S.Zeng, W.P.Liu First experimental constraint of the spectroscopic amplitudes for the α-cluster in the 11B ground state NUCLEAR REACTIONS 7Li(6Li, d), E=24 MeV; measured reaction products; deduced spectroscopic amplitudes (SA) for the α-cluster in the 11B ground state. Comparison with available data.
doi: 10.1016/j.physletb.2019.134820
2018DE15 J.Phys.(London) G45, 053001 (2018) D.S.Delion, Z.Ren, A.Dumitrescu, D.Ni Coupled channels description of the α-decay fine structure RADIOACTIVITY 246Cf, 242Cm, 253Fm, 251Cf(α); calculated branching ratios, J, π, deformation parameters. Comparison with available data.
doi: 10.1088/1361-6471/aaac52
2018NI12 Chin.Phys.C 42, 114104 (2018) Theoretical research on proton halos in exotic nuclei NUCLEAR STRUCTURE 17F, 25Al, 26,27,28P; calculated radial density probability distributions of all protons, all neutrons, the last valence proton, and nuclear matter in the Woods-Saxon potential.
doi: 10.1088/1674-1137/41/11/114104
2017NI01 Phys.Rev. C 95, 014323 (2017) Competition between α and β decays for heavy deformed neutron-deficient Pa, U, Np, and Pu isotopes RADIOACTIVITY 219,221,223,225,227Pa, 220,221,222,223,224,225,226,227,228,229U, 221,223,225,227,229,231Np, 228,229,230,231,232,233,234,235Pu(β+), (EC), (α); calculated partial half-lives for β+/EC and α-decay modes; deduced total half-lives. The β+/EC decay rates calculated within the deformed QRPA with residual particle-particle and particle-hole interaction matrix elements from Bruckner G matrix with Reid-93 NN forces. The α-decay half-lives calculated using the generalized density-dependent cluster model (GDDCM) with α-core potential from the double-folding model with M3Y effective interactions based on G matrix of Reid NN potential. Comparison with experimental values.
doi: 10.1103/PhysRevC.95.014323
2017NI16 Chin.Phys.C 41, 114104 (2017) Theoretical research on proton halos in exotic nuclei NUCLEAR STRUCTURE 65As, 17F, 26,27,28P, 56,57Cu; calculated nuclear radii, radial density probability distributions, single-particle energies; deduced halo. Comparison with available data.
doi: 10.1088/1674-1137/41/11/114104
2017TA10 Chin.Phys.C 41, 054103 (2017) Calculations of the β-decay half-lives of neutron-deficient nuclei RADIOACTIVITY 42,44,46Cr, 46,48,50Fe, 48,50,52,54Ni, 56,58,60,62Zn, 60,62,64,66Ge, 64,66,68,70Se(EC), (β+); calculated T1/2. Comparison with available data.
doi: 10.1088/1674-1137/41/5/054103
2016NI08 Phys.Rev. C 93, 054318 (2016) α-decay half-lives of odd-mass nuclei with differences between neutron and proton distributions RADIOACTIVITY 151m,153mHo, 157mLu, 157m,159m,161mTa, 187m,189m,191m,193m,195mBi, 177mTl, 173mAu, 169mIr, 165mRe, 269,271Sg, 271Bh, 273,275Hs, 275Mt, 277,279,281Ds, 279,281Rg, 281,283,285Cn, 283,285Nh, 285,287,289Fl, 287,289Mc, 291,293Lv, 293Ts(α); calculated half-lives of the skin-type and halo-type, differences between neutron and proton distributions using generalized density-dependent cluster model. Comparison with experimental values.
doi: 10.1103/PhysRevC.93.054318
2016QI07 Phys.Rev. C 94, 024315 (2016) Reexamining cluster radioactivity in trans-lead nuclei with consideration of specific density distributions in daughter nuclei and clusters RADIOACTIVITY 221Fr, 221,222,223,224,226Ra(14C); 228Th(20O); 230U(22Ne); 231Pa(23F); 230Th, 231Pa, 232,233,234U(24Ne); 233U(25Ne); 234U(26Ne); 234U, 236,238Pu(28Mg); 238Pu(30Mg); calculated effect of density distributions of daughter nuclei and clusters on cluster decays, ratio of the calculated half-life to that in the spherical case. Preformed cluster model, and double-folding integral of the density distributions of daughter nucleus and the emitted cluster. Comparison with available experimental data.
doi: 10.1103/PhysRevC.94.024315
2015DE17 J.Phys.(London) G42, 075106 (2015) Realistic α preformation factors of odd-A and odd-odd nuclei within the cluster-formation model NUCLEAR STRUCTURE N=116-142; analyzed available data; deduced cluster-formation model extension, α preformation factors. Comparison with available data.
doi: 10.1088/0954-3899/42/7/075106
2015JI07 Phys.Rev. C 91, 054617 (2015) S.L.Jin, J.S.Wang, Y.Y.Yang, P.Ma, M.R.Huang, J.B.Ma, F.Fu, Q.Wang, M.Wang, Z.Y.Sun, Z.G.Hu, R.F.Chen, X.Y.Zhang, X.H.Yuan, X.L.Tu, Z.G.Xu, K.Yue, J.D.Chen, B.Tang, Y.D.Zang, D.P.Wu, Q.Hu, Z.Bai, Y.J.Zhou, W.H.Ma, J.Chen, C.J.Lin, X.X.Xu, Z.Z.Ren, C.Xu, D.D.Ni, Y.H.Zhang, H.S.Xu, G.Q.Xiao Reaction mechanism of 8B breakup at the Fermi energy NUCLEAR REACTIONS 12C(8B, 7Be), E=36 MeV/nucleon, [secondary 8B beam produced in 9Be(12C, X), E=80.1 MeV/nucleon primary reaction]; measured particle spectra, (7Be)p-coin in the breakup reactions from 8B at RIBLL-HIRFL-Lanzhou facility; deduced energy sum spectrum of the one-proton knockout residue, longitudinal momentum distributions of 7Be fragments for stripping and diffraction mechanisms. Comparison with CDCC calculations with Koning and Delaroche global parameterization.
doi: 10.1103/PhysRevC.91.054617
2015NI10 Phys.Rev. C 92, 034324 (2015) β-decay rates of odd-mass neutron-rich isotopes in the deformed quasiparticle random-phase approximation with realistic interactions RADIOACTIVITY 85,87,89,91,93,95,97,99,101Kr, 89,91,93,95,97,99,101,103,105,107Sr, 95,97,99,101,103,105,107,109,111,113Zr, 99,101,103,105,107,109,111,113,115,117Mo(β-); calculated half-lives. 91,93,101,105Sr(β-); calculated GT transition strength. Deformed quasiparticle random-phase approximation with realistic nucleon-nucleon interactions including both the GT and first-forbidden (FF) β transitions. Comparison with other theoretical calculations and with experimental values.
doi: 10.1103/PhysRevC.92.034324
2015NI12 Phys.Rev. C 92, 054322 (2015) Effects of differences between neutron and proton density distributions on α-decay half-lives RADIOACTIVITY 204,206,208,210,212,214,216,218,220,222,224,226Ra, 208,210,212,214,216,218,220,222,224,226,228,230,232Th, 218,220,222,224,226,228,230,232,234,236,238U, 246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 260Sg, 264,266,268,270Hs, 270Ds, 286,288Fl, 290,292Lv, 294Og, 298120(α); calculated α-decay half-lives for neutron skin-type and neutron halo-type distributions; investigated effects of differences between neutron and proton distributions on α decay. Generalized density-dependent cluster model (GDDCM) with double-folding model for α-core potential. Comparison with available experimental data.
doi: 10.1103/PhysRevC.92.054322
2015XU15 Sci. Rep. 5, 18350 (2015) L.-Q.Xu, Y.-W.Liu, X.Kang, D.-D.Ni, K.Yang, No.Hiraoka, K.-D.Tsuei, L.-F.Zhu The realization of the dipole (γ, γ) method and its application to determine the absolute optical oscillator strengths of helium NUCLEAR REACTIONS He(γ, γ), E<100 eV; measured reaction products; deduced absolute dipole oscillator strengths, absolute optical oscillator strength (OOS). Comparison with available data. The Taiwan beamline BL12XU of SPring-8.
doi: 10.1038/srep18350
2014NI01 J.Phys.(London) G41, 025107 (2014) β-decay rates of r-process waiting-point nuclei in the extended quasiparticle random-phase approximation RADIOACTIVITY 62,64,66,68,70Fe, 68,70,72,74,76,78Ni, 74,76,78,80,82Zn, 122,124,126,128,130,132Cd(β-); calculated T1/2, proton-proton, neutron-neutron, neutron-proton strengths. QRPA, HFB, Bruckner G-matrix, comparison with available data.
doi: 10.1088/0954-3899/41/2/025107
2014NI12 Phys.Rev. C 89, 064320 (2014) β-decay rates of neutron-rich Zr and Mo isotopes in the deformed quasiparticle random-phase approximation with realistic interactions RADIOACTIVITY 112Mo(β-); calculated spins and excitation energies of the daughter nucleus, half-life, logft values for Gamow-Teller (GT) and first-forbidden (FF) transitions. 106Zr(β-); calculated shape factors of GT and FF transitions for oblate, spherical and prolate nuclear shapes. 104,106,108,110,112,114,116,118,120,122Mo, 98,100,102,104,106,108,110,112,114,116,118,120Zr(β-); calculated half-lives for GT and FF transitions. Deformed quasiparticle random-phase approximation (QRPA) method. Comparison with other theoretical calculations, and with experimental data.
doi: 10.1103/PhysRevC.89.064320
2014NI17 J.Phys.(London) G41, 125102 (2014) β-decay rates of neutron-rich Kr and Sr isotopes in the deformed QRPA with realistic interactions RADIOACTIVITY 92,94,98Kr, 98Sr(β-n); calculated T1/2, low-lying average shape factors for Gamow-Teller and first-forbidden transitions, β-delayed neutron emission probability. Comparison with experimental data.
doi: 10.1088/0954-3899/41/12/125102
2014QI03 Phys.Rev. C 89, 024318 (2014) Tentative probe into the nuclear charge radii of superheavy odd-mass and odd-odd nuclei NUCLEAR STRUCTURE 187Hg, 191Tl, 189,191,193,195,197,201,203,209,211Pb, 203,205,209Bi, 213Fr, 147,148,149,150Tb, 151Ho, 153Tm; analyzed experimental α-decay half-life data; deduced rms nuclear charge radii using density-dependent cluster model (DDCM) combined with the two-potential approach, and the double-folding model. 257No, 255Lr, 267Rf, 262,266,268,270Db, 259,261,269Sg, 266,271,272,274Bh, 263,265,269,275Hs, 268,274,275,276,278Mt, 277,279,281Ds, 278,279,280,281,282Rg, 285Cn, 283,284,285,286Nh, 289,290Mc; deduced rms charge radii based on above formulation. Comparison with a previously proposed formula based on experimental Eα and α-decay half-life data.
doi: 10.1103/PhysRevC.89.024318
2013NI01 Chin.Phys.Lett. 30, 022101 (2013) Alpha-Decay Study of Unfavored Transitions in Bismuth Isotopes RADIOACTIVITY 187,188,189,190,191,192,193,194,195,197,199,201,203,209,210,211,212,213,214Bi(α); calculated T1/2. Generalized density-dependent cluster model (GDDCM), comparison with experimental data.
doi: 10.1088/0256-307X/30/2/022101
2013NI02 Phys.Rev. C 87, 024310 (2013) Nuclear charge radii of heavy and superheavy nuclei from the experimental α-decay energies and half-lives NUCLEAR STRUCTURE 140Ce, 142,144Nd, 144,146,148Sm, 146Gd, 148,150,152Dy, 150,152,154Er, 152,154,156,158Yb, 182W, 184,186Os, 178,180,182,184Pt, 182,184,186,188,190,206Hg, 190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 200,202,204,206,208,210Po, 202,204,206,208,210,212,218,220,222Rn, 208,210,212,214,220,222,224,226,228Ra, 228,230,232Th, 234,236,238U, 238,240,242,244Pu, 242,244,246,248Cm, 242,244,246,248,250,252Cf, 248,250,252Fm, 252,254No, 256Rf, 260,262,264,266Sg, 266Hs, 282,284Cn, 286,288Fl, 290Lv; calculated rms charge radii, charge distribution using the generalized density dependent cluster model (GDDCM). A formula derived from Wentzel-Kramers-Brillouin (WKB) barrier penetration probability is proposed to calculate nuclear charge radii from the experimental α-decay energies and half-lives. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.024310
2013NI03 Phys.Rev. C 87, 027602 (2013) Theoretical description of fine structure in the α decay of heavy odd-odd nuclei RADIOACTIVITY 240,242Am, 254Es(α); calculated α-decay branching ratios, fine structure to rotational bands in daughter nuclei using multichannel cluster model (MCCM), and WKB barrier penetration formula. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.027602
2013NI13 Phys.Rev. C 88, 014325 (2013) Coupled-channel representation to describe fine structure in the α decay of odd-mass Bk isotopes RADIOACTIVITY 243,245,247,249Bk(α); calculated half-lives, α decay branching ratios or fine structure to rotational band members in 239,241,243,245Am using the multichannel cluster model (MCCM). Comparison with experimental data.
doi: 10.1103/PhysRevC.88.014325
2013QI04 Phys.Rev. C 87, 054323 (2013) Attempt to probe nuclear charge radii by cluster and proton emissions RADIOACTIVITY 222,224,226Ra(14C); 228Th(20O); 230U(22Ne); 231Pa(23F); 230Th, 232,234U(24Ne); 233U(25Ne); 234U(26Ne); 234U, 236,238Pu(28Mg); 238Pu(30Mg), (32Si); 144,146Er, 149,150Yb, 155,156Hf, 159,160W, 163,165,166Os, 170Pt, 176Hg, 184Pb(p); calculated rms nuclear charge radii of parent nuclei from cluster and proton decay half-lives. Density-dependent cluster model. Comparison with experimental data. NUCLEAR STRUCTURE 144,146Er, 149,150Yb, 155,156Hf, 159,160W, 163,165,166Os, 170Pt, 176Hg, 184Pb, 222,224,226Ra, 228,230Th, 230,232,233,234U, 231Pa, 238Pu; calculated rms nuclear charge radii from half-lives of cluster and proton decay of nuclei. Density-dependent cluster model. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.054323
2012CH48 J.Phys.(London) G39, 125105 (2012) Calculations of the b-decay half-lives of neutron-rich nuclei RADIOACTIVITY 16,18,20,22C, 22,24,26,28O, 26,28,30,32,34Ne, 30,32,34,36,38,40Mg, 34,36,38,40,42,44Si, 40,42,44,46,48S, 46,48,50,52Ar, 52,54,56,58Ca, 54,56,58,60,62Ti, 58,60,62,64,66,68Cr, 64,66,68,70,72Fe, 70,72,74,76,78Ni, 76,78,80,82Zn, 82,84,86,88Ge, 88,90,92,94Se, 92,94,96,98,100Kr, 96,98,100,102,104Sr, 100,102,104,106,108,110Zr, 106,108,110,112,114Mo, 112,114,116,118,120Ru, 118,120,122,124Pd, 122,124,126,128,130,132Cd, 134,136Sn, 138,140,142Te, 142,144,146Xe, 146,148,150,152Ba, 150,152,154,156Ce(β-); calculated T1/2. pnQRPA with δ-form Gamow-Teller residual interaction, comparison with experimental data.
doi: 10.1088/0954-3899/39/12/125105
2012NI02 Rom.J.Phys. 57, 407 (2012) New Formula of Half-Lives for Proton Emission from Spherical and Deformed Nuclei RADIOACTIVITY 105Sb, 109I, 112,113Cs, 117La, 121Pr, 130,131Eu, 135Tb, 140,141Ho, 145,146,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated T1/2; deduced new formula.
2012NI13 Prog.Theor.Phys.(Kyoto), Suppl. 196, 445 (2012) Alpha-Decay Studies of Rf, Sg, and Hs Isotopes within the Multi-Channel Cluster Model RADIOACTIVITY 252,254,256,258,260,262,264,266,268,270Rf, 256,258,260,262,264,266,268,270,272,274Sg, 260,262,264,266,268,270,272,274,276Hs(α); calculated T1/2, branching ratios. Multi-channel cluster model.
doi: 10.1143/PTPS.196.445
2012NI14 Nucl.Phys. A893, 13 (2012) Binding energies, α-decay energies, and α-decay half-lives for heavy and superheavy nuclei COMPILATION Z=106-120; evaluated nuclear mass, mass excess, Qα using AME2011; deduced new formula parameters from the fit to superheavy nuclei, calculated α-decay T1/2. Compared with KTYU05, FRDM95.
doi: 10.1016/j.nuclphysa.2012.08.006
2012NI16 Phys.Rev. C 86, 054608 (2012) Systematic calculation of fine structure in the α decay of heavy odd-mass nuclei RADIOACTIVITY 237Np, 239,241Pu, 239,241,243Am, 241,243,245,247Cm, 243,245,247,249Bk, 245Cf, 247,249,251,253Cf, 245,247,249,251,253,255Es, 251,253,255,257Fm, 255,257Md, 257No(α); calculated half-lives, branching ratios. Multichannel cluster model (MCCM). Comparison with experimental data.
doi: 10.1103/PhysRevC.86.054608
2012NI17 J.Phys.:Conf.Ser. 381, 012055 (2012) Systematic calculation of fine structure in the α decay of deformed nuclei RADIOACTIVITY 244Cm(α); calculated T1/2, branching ratio to 0+, 2+, 4+, 6+, 8+ 240Pu states. 252,254No, 256,258Rf(α); calculated T1/2 from 0+, 2+, 4+, 6+, 8+ states. Z=92-106(α); calculated T1/2, branching ratio to excited 4+, 6+ states. CC Schroedinger equation with outgoing wave boundary conditions. Compared to data.
doi: 10.1088/1742-6596/381/1/012055
2011LI23 Eur.Phys.J. A 47, 78 (2011) X.J.Liu, X.P.Zhang, D.D.Ni, Z.Z.Ren Benford's law and cross-sections of A(n, α)B reactions
doi: 10.1140/epja/i2011-11078-3
2011NI02 Phys.Rev. C 83, 014310 (2011) α-cluster structure above doubly closed shells in a generalized density-dependent cluster model NUCLEAR STRUCTURE 20Ne, 44Ti, 94Mo, 212Po; calculated B(E2) transition strengths, α-decay widths of cluster states in the 16O+α system, α-decay half-lives and branching ratios in the 208Pb+α system. Generalized density-dependent cluster model (GDDCM). Double-folding potentials with density- and energy-dependent CDM3Y6 nucleon-nucleon interactions for α-core potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.014310
2011NI12 Phys.Rev. C 83, 067302 (2011) Coupled-channels study of fine structure in the α decay of well deformed nuclei RADIOACTIVITY 246Cf, 242Cm, 238Pu(α); A=234-260(α); calculated α-decay branching ratios to low-lying members of the ground-state rotational band up to 8+ band. Five-channel microscopic calculations using Schrodinger equation. Comparison with experimental data, and with calculations based on Boltzmann distribution (BD) hypothesis.
doi: 10.1103/PhysRevC.83.067302
2011NI13 Phys.Rev. C 84, 037301 (2011) Coupled-channels study of fine structure in the α decay of platinum isotopes RADIOACTIVITY 172,174,176,178,180,182,184,186,188,190,192,194Pt(α); calculated Q(α), branching ratio, half-lives. Coupled-channel Schrodinger equation. Predictions for α decay of neutron-rich nuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.037301
2011QI01 J.Phys.(London) G38, 015102 (2011) α-decay half-lives in medium mass nuclei RADIOACTIVITY 144Nd, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154,156Er, 154,156,158Yb, 156,158,160,162Hf, 158,160,162,164,166,168W, 162,164,166,168,170,172,174,186Os, 166,168,170,172,174,176,178,180,182,184,186,188,190Pt(α); calculated T1/2. Comparison with experimental data.
doi: 10.1088/0954-3899/38/1/015102
2011QI06 Phys.Rev. C 83, 044317 (2011) Calculations of α-decay half-lives for heavy and superheavy nuclei RADIOACTIVITY 210Pb, 212,214,216,218Po, 214,216,218,220,222Rn, 216,218,220,222,224,226Ra, 218,220,222,224,226,228,230,232Th, 222,224,226,228,230,232,234,236,238U, 232,234,236,238,240,242,244Pu, 240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 260,266Sg, 274Bh, 264,266,270Hs, 278Mt, 270,281Ds, 278,279,280,282Rg, 284,285Cn, 282,283,284,285,286Nh, 286,288,289Fl, 287,288,289,290Mc, 290,292,293Lv, 293,294Ts, 294Og(α); calculated half-lives using deformed version of the cluster model with modified two-potential approach and Woods-Saxon potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.044317
2011QI10 Nucl.Phys. A866, 1 (2011) α-Decay near the shell closure from ground and isomeric states RADIOACTIVITY 151,153Dy, 151,152,153,154Ho, 153,155Er, 153,154,155,156Tm, 155,157Yb, 155,156,157,158Lu, 157,159Hf, 157,158,159,160Ta, 159,161W, 160,162Re, 163Os, 177,179,181,183Tl, 179,180,181,183,185,187,191Pb, 186,187,188,189,190,191,192,193,194,195,196,209,210,211,213Bi, 187,188,191,192,193,195,197,199,201,203,205,207,213,215Po, 191,192,193,194,195,197,197,198,199,200,201,202,203,204,205,206,207,208,209,213,214,215,216At, 195,197,199,201,203,205,207,215,217Rn, 199,200,201,202,203,204,205,206,207,208,215,216,217,218Fr, 217,219Ra, 217,218,219Ac, 219,221Th, 219,221Pa(α); calculated T1/2, isomeric states T1/2 using two-potential approach with deformed cluster model. Comparison with data.
doi: 10.1016/j.nuclphysa.2011.07.002
2011SH13 J.Phys.(London) G38, 055103 (2011) Systematic calculations on cluster radioactivity half-lives RADIOACTIVITY 112,113,114,115,116,117Cs, 114,115,116,117,118,119,120Ba, 117,118,119,120,121,122La, 120Ce, 219Fr, 219,220,227Ra, 219,220,221,222,228Ac, 220,221,221,222,223Th, 221,223,231,232,233,234Pa, 222,223,224,225,226U, 225,226,227,228Np, 228,229,230Pu(12C), 114,115,116,117,118,119Ba, 117,118,119,120,122La, 119,120,121,122,123,124Ce, 121,122,123,124,125,126Pr, 124,125,126Nd, 224,225Th, 224,225,226,227U, 225,226,227,228,229Np, 228,229,230Pu(16O), 126Pm(24Mg), 220Fr, 224Pa(13C), 227Th, 227,228Pa, 228U(18O), 227,228Ac(20O), 229,230Ac(22O), 232,233,234Pu, 233,234,235Am(26Mg), 236Am, 233,235Pu(27Mg), 237Pu(29Mg), 128,129,130,131,132Sm, 130,131,132,133,134,135Eu, 134,135Gd, 136,137Tb, 138Dy(28Si), 131Sm(29Si), 132Eu, 135Gd(29Si), 136Tb, 138Dy, 140,141Ho(32S), 143Er(36Ar), 239Pu, 239,241Cm(33Si), 225Ac, 221,222,223,224,226Ra, 226Th, 220,222,224,226,223,225Fr, 220,228Ra, 221,222,224,226,227Ac, 224,225,227,223Th, 225,226,227,228Pa, 227,228U(14C), 226Th(18O), 228,229Th(20O), 229,231Pa(23F), 229,230U, 230,231Np, 231,232Pu(22Ne), 231U(23Ne), 229Ac, 230,231,232,233Pa, 229,230,231,232Th, 230,231,232,233,234,235,236U, 231,232,233Np(24Ne), 234Pa, 235U(25Ne), 232Th, 236U(26Ne), 127Pm(24Mg), 232,233,234,235U, 234,235,236Np, 234,235,236,237,238Pu, 235Am(28Mg), 235U, 235Np(29Mg), 236,238Pu, 237Np(30Mg), 238Pu, 236,238Am(32Si), 238Np, 239,240,241,242Am, 238,239,240,241,242,243Cm, 240,241Bk(34Si); calculated T1/2.
doi: 10.1088/0954-3899/38/5/055103
2010NI01 J.Phys.(London) G37, 035104 (2010) α-decay calculations of ground and isomeric states within a generalized density-dependent cluster model NUCLEAR STRUCTURE Z=67-89; calculated ground and isomeric states in neutron-deficient isotopes, α-decay T1/2. Comparison with experimental data.
doi: 10.1088/0954-3899/37/3/035104
2010NI02 Phys.Rev. C 81, 024315 (2010) Systematic calculation of α decay within a generalized density-dependent cluster model RADIOACTIVITY 229Th, 225,227Pa, 225,229,233,235U, 235,237Np, 237,239,241Pu, 239,240,241,242,243Am, 241,242,243,245,247Cm, 245,247,249Bk, 245,247,249,253Cf, 245,247,249,251,253,255Es, 251,255,257Fm(α); Z=52-104, N=84-156(α); Z=52, N=54-58(α); Z=91-100, N=133-157(α); calculated half-lives and branching ratios for even-even, odd-A and odd-odd α emitters using generalized density-dependent cluster model. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.024315
2010NI09 Phys.Rev. C 81, 064318 (2010) New approach for α-decay calculations of deformed nuclei RADIOACTIVITY 244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 260Sg(α); calculated half-lives and branching ratios using multichannel cluster model (MCCM) based on an axially deformed Woods-Saxon potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.064318
2010NI12 J.Phys.(London) G37, 105107 (2010) Calculations of new α-decay data within the generalized density-dependent cluster model RADIOACTIVITY 179Tl, 175Au, 171Ir, 179,180,181Pb, 176,177Hg, 172Pt, 187,188,192Po, 271Sg, 272Bh, 275Hs, 275Mt, 279Ds, 278,279,282Rg, 283,285Cn, 282,283,285,286Nh, 286,287,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294,295Og, 295,298,299120(α); calculated α-decay T1/2. Comparison with experiment.
doi: 10.1088/0954-3899/37/10/105107
2010NI13 Phys.Rev. C 82, 024311 (2010) Half-lives and cluster preformation factors for various cluster emissions in trans-lead nuclei RADIOACTIVITY 210Pb, 211Bi, 211,212,213,214Po(α); 219,220Rn, 221Fr, 221,222,223,224,225,226Ra, 223,225Ac, 226Th(14C); 221Fr, 223Ac(15N); 223Ra, 226,227Th, 227Pa(18O); 225,226Ra, 227Ac, 228,229Th(20O); 228Th, 229Pa, 230U, 231Np(22Ne); 229Ac, 231Pa(23F); 229,230,231,232Th, 231Pa, 230,232,233,234,235,236U, 233Np(24Ne); 231Th, 233,235U(25Ne); 232Th, 234,236U(26Ne); 232,233,234,235,236U, 235Np, 236,237,238Pu, 237Am(28Mg); 235U, 237Pu(29Mg); 236,238U, 237Np, 238,239Pu(30Mg); 237,238Pu, 239Am, 240,241Cm(32Si); 239Pu, 241Am, 242,243,244Cm(34Si); calculated half-lives and cluster preformation factors using generalized density-dependent cluster model (GDDCM). Comparison with experimental data.
doi: 10.1103/PhysRevC.82.024311
2010NI15 Nucl.Phys. A834, 370c (2010) α-decay calculations of light mass nuclei above doubly magic 100Sn RADIOACTIVITY 104,105,106,107,108,109,110Te, 106,107,108,109,110,111,112,113I, 108,109,110,111,112,113Xe, 111,112,113,114Cs, 112,113,114Ba(α); analyzed Q-value; calculated T1/2 using a generalized density-dependent cluster model. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.042
2010QI03 Chin.Phys.Lett. 27, 072301 (2010) Theoretical Calculation for Half-Lives of Spherical Proton Emitters RADIOACTIVITY 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated proton radioactivity T1/2 for spherical emitters. Comparison with experimental data.
doi: 10.1088/0256-307X/27/7/072301
2010QI09 Chin.Phys.Lett. 27, 112301 (2010) Y.-B.Qian, Z.-Z.Ren, D.-D.Ni, Z.-Q.Sheng Half-Lives of Proton Emitters With a Deformed Density-Dependent Model RADIOACTIVITY 105Sb, 145,146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi, 109I, 112,113Cs, 117La, 121Pr, 130,131Eu, 135Tb, 140,141Ho(p); calculated T1/2 for semi-spherical and well-deformed proton emitters.
doi: 10.1088/0256-307X/27/11/112301
2009NI06 Nucl.Phys. A825, 145 (2009) Microscopic calculation of α-decay half-lives within the cluster model RADIOACTIVITY 210Pb, 212,214,216,218Po, 214,216,218,220,222Rn, 216,218,220,222,224,226Ra, 218,220,222,224,226,228,230,232Th, 222,224,226,228,230,232,234,236,238U, 232,234,236,238,240,242,244Pu, 240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 260,266Sg, 264,266,270Hs, 270Ds, 278,279,280Rg, 283,284,285Cn, 282,283,284Nh, 286,287,288,289Fl, 287,288Mc, 290,291,292,293Lv, 294Og(α); calculated α-decay half-lives using a cluster model. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.04.010
2009NI08 Phys.Rev. C 80, 014314 (2009) Exotic α decays around the N=126 magic shell RADIOACTIVITY 209Bi, 209,210,211Po, 211At, 211,212,213Rn, 213Fr, 213,214,215Ra, 215Ac, 215,216,217Th, 217Pa, 217,218,219U(α); calculated half-lives, decay widths, Q-values and α preformation factors using generalized density-dependent cluster model (GDDCM) combined with microscopic two-level model. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.014314
2009NI11 Nucl.Phys. A828, 348 (2009) α-Decay calculations of medium mass nuclei within generalized density-dependent cluster model RADIOACTIVITY 144Nd, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154,156Er, 154,156,158Yb, 156,158,160,162Hf, 158,160,162,164,166,168W, 162,164,166,168,170,172,174,186Os, 166,168,170,172,174,176,178,180,182,184,186,188,190Pt, 172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194Pb, 190,192,194,196,198,200,202,204,206,208,210Po, 196,198,200,202,204,206,208,210,212Rn, 202,204,206,208,210,212Ra, 212,214,216Th, 218U(α); calculated α-decay T1/2 using generalized density-dependent cluster model with double-folded or Woods-Saxon potentials. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.07.014
2009NI12 Phys.Rev. C 80, 051303 (2009) Microscopic calculation of α-decay half-lives with a deformed potential RADIOACTIVITY Z=52-104(α); calculate half-lives, branching ratios of 0+ to 0+ transitions for even-even nuclei using generalized density dependent cluster model (GDDCM). Comparison with experimental data.
doi: 10.1103/PhysRevC.80.051303
2008NI12 Phys.Rev. C 78, 044310 (2008) Unified formula of half-lives for α decay and cluster radioactivity RADIOACTIVITY Po, Rn, Ra, Th, U, Pu, Cm, Cf, Fm, No, Rf, Sg, Hs, Ds; Z=114, 116, 118; 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 228Th(20O); 231Pa, 230,232,233U(24Ne); 231Pa(23F); 234U, 236Pu(28Mg); 238Pu(32Si); 242Cm(34Si); calculated half-lives of α and cluster decays. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.044310
2008NI14 Eur.Phys.J. A 38, 251 (2008) Benford's law and half-lives of unstable nuclei
doi: 10.1140/epja/i2008-10680-8
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