NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.M.Dong Found 59 matches. 2024DO01 Eur.Phys.J. A 60, 34 (2024) Nucleon–nucleon short-range correlation, superfluidity and neutron star cooling
doi: 10.1140/epja/s10050-024-01242-5
2023DO01 Appl.Radiat.Isot. 193, 110647 (2023) J.Dong, T.Bai, Y.Hu, X.Zhang, J.Fan, Y.Dai, L.Miao, X.Yu, Z.Li Determination of the half-life of 161Tb RADIOACTIVITY 161Tb(β-); measured decay products, Eγ, Iγ; deduced T1/2 and uncertainties. Comparison with available data.
doi: 10.1016/j.apradiso.2022.110647
2023DO04 Appl.Radiat.Isot. 194, 110689 (2023) J.Dong, T.Bai, Y.Dai, X.Zhang, J.Fan, Y.Hu, X.Song, Y.Ma, L.Miao, Q.Shi, Z.Li Half-life determination of 111Ag RADIOACTIVITY 111Ag(β-) [from 110Pd(n, γ), E thermal]; measured decay products, Eγ, Iγ; deduced T1/2 by power moderated method. Comparison with available data. Xi'an pulse reactor.
doi: 10.1016/j.apradiso.2023.110689
2021DO01 Phys.Lett. B 813, 136063 (2021) J.M.Dong, Q.Zhao, L.J.Wang, W.Zuo, J.Z.Gu α-Cluster formation in heavy α-emitters within a multistep model RADIOACTIVITY 202,204,206,208,210,212,214,216,218Po, 204,206,208,210,212,214,216,218,220Rn, 206,208,210,212,214,216,218,220,222Ra(α); calculated formation probability values, contour plots within a multistep model.
doi: 10.1016/j.physletb.2021.136063
2021SH15 Phys.Rev. C 103, 034316 (2021) X.-L.Shang, J.-M.Dong, W.Zuo, P.Yin, U.Lombardo Exact solution of the Brueckner-Bethe-Goldstone equation with three-body forces in nuclear matter
doi: 10.1103/PhysRevC.103.034316
2020DO03 Phys.Rev. C 101, 014305 (2020) Breakdown of the tensor component in the Skyrme energy density functional NUCLEAR STRUCTURE 116,118,120,122,124,126,128,130,132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er; calculated energy differences between the 1h11/2 and 1g7/2 single proton states for Sn isotopes, and between 1h9/2 and 1i13/2 single neutron states for N=82 isotones using Skyrme IMP1 and IMP2 central interactions, and the tensor force derived in momentum space via partial-wave expansion; deduced no role of tensor force in Skyrme density functionals, and improvement in the description of shell evolution in Sn isotopes and N=82 isotones, in comparison with experimental data.
doi: 10.1103/PhysRevC.101.014305
2019DO01 Phys.Rev. C 99, 014319 (2019) J.M.Dong, J.Z.Gu, Y.H.Zhang, W.Zuo, L.J.Wang, Yu.A.Litvinov, Y.Sun Beyond Wigner's isobaric multiplet mass equation: Effect of charge-symmetry-breaking interaction and Coulomb polarization NUCLEAR STRUCTURE A=13, 15, 17, 19, 21, 23, 25, 27, 29, 31, 33, 35, 37, 39, 41, 43, 45, 47, 49, 51, 53, 55, 57, 59, 61; calculated coefficient of the added cubic term to the isobaric multiplet mass equation (IMME) for T=3/2 isobaric quartets, and density differences between neutron and proton for A=37 and 43 isobaric doublets. A=12, 16, 20, 24, 28, 32, 36; calculated coefficients of the added cubic and quartic terms to the isobaric multiplet mass equation (IMME) for T=2 isobaric quintets. Deduced general deviation from the original IMME, and the magnitude of the deviation exhibiting an oscillation-like behavior with mass number, modulated by the shell effect. Comparison with available experimental values.
doi: 10.1103/PhysRevC.99.014319
2019DO03 Nucl.Phys. A983, 133 (2019) J.M.Dong, X.L.Shang, W.Zuo, Y.F.Niu, Y.Sun An effective Coulomb interaction in nuclear energy density functionals
doi: 10.1016/j.nuclphysa.2019.01.003
2019FA03 Phys.Rev. C 99, 065804 (2019) X.-H.Fan, X.-l.Shang, J.-M.Dong, W.Zuo Neutron-proton pairing in nuclear matter
doi: 10.1103/PhysRevC.99.065804
2019GU09 Nucl.Phys. A986, 18 (2019) W.Guo, J.M.Dong, X.Shang, H.F.Zhang, W.Zuo, M.Colonna, U.Lombardo Proton-proton 1S0 pairing in neutron stars
doi: 10.1016/j.nuclphysa.2019.02.008
2019WA35 J.Phys.(London) G46, 105102 (2019) L.-J.Wang, J.Dong, F.-Q.Chen, Y.Sun Projected shell model analysis of structural evolution and chaoticity in fast-rotating nuclei NUCLEAR STRUCTURE 164Yb; calculated d energies and moment of inertia of the yrast band, B(E2), branching number; deduced rotationally-induced evolution from order to chaos infinite quantum many-body systems-nuclei.
doi: 10.1088/1361-6471/ab33be
2018DO02 Phys.Rev. C 97, 021301 (2018) J.M.Dong, Y.H.Zhang, W.Zuo, J.Z.Gu, L.J.Wang, Y.Sun Generalized isobaric multiplet mass equation and its application to the Nolen-Schiffer anomaly ATOMIC MASSES 20O, 53Ni, 208Pb; calculated first-order symmetry energy coefficient for charge symmetry breaking (CSB) and second-order charge-independent breaking (CIB) components using SLy4, SLy5 and KBD interactions. Derived a generalized isobaric mass multiplet equation (GIMME), and applied to the study of Nolen-Schiffer anomaly (NSA) in the Coulomb displacement energy of mirror nuclei. A=10-60; calculated contributions of the CSB and CIB effects to coefficients of Tz and Tz2 using SLy4 interaction. 15O, 15N; 17F, 17O; 39Ca, 39K; 41Sc, 41Ca; calculated ΔNSA for T=1/2 mirror pairs due to CSB effects using SLy4, SLy5 and KBD interactions. A=18-42; calculated Coulomb displacement energy (CDE) of the T=1 mirror pairs using SLy4 interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.97.021301
2018DO04 Phys.Rev. C 97, 034318 (2018) J.M.Dong, L.J.Wang, W.Zuo, J.Z.Gu Constraints on Coulomb energy, neutron skin thickness in 208Pb, and symmetry energy NUCLEAR STRUCTURE 208Pb; calculated neutron skin thickness, density-dependent symmetry energy coefficient of nuclear matter by constraining the Coulomb energy with the mirror nuclei. A=17-65; calculated Coulomb displacement energies (CDEs) for T=1/2 mirror pairs, and compared with experimental data. 48Ca, 68Ni, 132Sn, 208Pb, 298Fl; calculated symmetry energy using self-consistent Skyrme-Hartree-Fock approach with SLy4 interaction. Discussed charge-symmetry-breaking (CSB) effect.
doi: 10.1103/PhysRevC.97.034318
2018DO09 Phys.Atomic Nuclei 81, 283 (2018) The Fourth-Order Symmetry Energy of Finite Nuclei NUCLEAR STRUCTURE 208Pb; compiled published calculations of Fourth-Order Symmetry Energy using a large set of Skyrme interactions.
doi: 10.1134/S1063778818030109
2018YI05 Chin.Phys.C 42, 114102 (2018) Effect of tensor correlations on the depletion of nuclear Fermi sea within the extended BHF approach
doi: 10.1088/1674-1137/41/11/114102
2018ZH02 Chin.Phys.C 42, 014104 (2018) A formula for half-life of proton radioactivity RADIOACTIVITY 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 171Au, 177Tl(p); calculated T1/2; deduced formula. Comparison with available data.
doi: 10.1088/1674-1137/42/1/014104
2017YI01 Nucl.Phys. A961, 200 (2017) P.Yin, X.Fan, J.Dong, W.Guo, W.Zuo Model-dependence of neutrino emissivities and neutrino luminosities of neutron stars from the direct Urca processes and the modified Urca processes
doi: 10.1016/j.nuclphysa.2017.03.001
2017YI06 Chin.Phys.C 41, 114102 (2017) Effect of tensor correlations on the depletion of nuclear Fermi sea within the extended BHF approach
doi: 10.1088/1674-1137/41/11/114102
2016DO08 Chin.Phys.Lett. 33, 102101 (2016) First-Order Symmetry Energy Induced by Neutron-Proton Mass Difference NUCLEAR STRUCTURE 208Pb; calculated symmetry energy. Skyrme energy density functionals.
doi: 10.1088/0256-307X/33/10/102101
2015BA24 J.Phys.(London) G42, 085101 (2015) X.J.Bao, S.Q.Guo, H.F.Zhang, Y.Z.Xing, J.M.Dong, J.Q.Li Competition between α-decay and spontaneous fission for superheavy nuclei RADIOACTIVITY 232Th, 234,236,238U, 236,238,240,242,244Pu, 240,242,244,246,248,250Cm, 242,244,246,248,250,252,254Cf, 246,248Fm, 256,258,260Rf, 264,266,270Hs, 270Ds, 284Cn, 286,288Fl, 290,292Lv, 294Og, 235U, 239Pu, 243,245Cm, 237,249Cf, 255,257,259Fm, 253,255,259Rf, 293,294Ts, 287,289,290Mc, 282,283,285,286Nh, 275,278Mt, 271,274Bh, 291,293Lv, 287,289Fl, 283,285Cn, 278,279,280,281,282Rg, 279,281Ds, 274,275,276Mt, 275Hs, 270,272Bh, 266,267,268,270Db(α); calculated T1/2. Comparison with experimental data.
doi: 10.1088/0954-3899/42/8/085101
2015DO02 Phys.Rev. C 91, 034315 (2015) Constraints on neutron skin thickness in 208Pb and density-dependent symmetry energy NUCLEAR STRUCTURE 208Pb; calculated neutron skin thickness and density dependence of symmetry energy based on a high linear correlation between skin thickness and the symmetry energy coefficient of nuclear matter at saturation density. Discussed measurement issues of skin thickness using novel Pb radius experiment (PREX).
doi: 10.1103/PhysRevC.91.034315
2015JI02 Phys.Rev. C 91, 025802 (2015) L.Jiang, S.Yang, J.M.Dong, W.H.Long Self-consistent tensor effects on nuclear matter systems within a relativistic Hartree-Fock approach
doi: 10.1103/PhysRevC.91.025802
2015MA45 J.Phys.(London) G42, 095107 (2015) N.N.Ma, H.F.Zhang, X.J.Bao, P.H.Chen, J.M.Dong, J.Q.Li, H.F.Zhang Weizsacker-Skyrme-type mass formula by considering radial basis function correction NUCLEAR STRUCTURE N<180; calculated nuclear masses, α-decay Q-values and T1/2. Comparison with experimental data.
doi: 10.1088/0954-3899/42/9/095107
2014BA23 Phys.Rev. C 89, 067301 (2014) X.-J.Bao, H.-F.Zhang, J.-M.Dong, J.-Q.Li, H.-F.Zhang Competition between α decay and cluster radioactivity for superheavy nuclei with a universal decay-law formula RADIOACTIVITY Z=104-120, N=140-202(α); 222,224,226Ra, 228,230Th, 230,232,234U, 236Ra, 240,242Cm, 256,258Rf, 260,262Sg, 264,266Hs, 270Ds(α); calculated branching ratios for α-decay and cluster radioactivity. Comparison with available experimental data. 282Ds(76Zn); 284Ds(78Zn); 286Ds(82Ge); 288Ds(84Ge); 284Cn(76Zn), (80Zn); 286Cn(80Ge), (82Ge); 288Cn(82Ge); 290Cn(82Ge), (84Ge), (86Se); 292Cn(84Se), (88Se); 286Fl(78Ge), (80Ge), (84Se); 288Fl(80Ge), (84Se); 290Fl(82Ge), (84Se); 292Fl(86Se); 294Fl(88Se); 294Fl(88Se); 296Fl(88Se), (92Kr); 298Fl(94Kr); 288Lv(82Se); 288,290,292Lv(84Se); 294Lv(86Se); 288,290,292,294Og(86Kr); 296Og(88Kr); 298Og(90Kr); 290,292,294120(88Sr); 296,298120(90Sr); 300120(92Sr); calculated branching ratios and half-lives for the most probable cluster decay using Universal Decay Law formalism, and AME-2012, FRDM95, KTUV05, and WS2011 mass tables.
doi: 10.1103/PhysRevC.89.067301
2014FA03 Phys.Rev. C 89, 017305 (2014) Density-dependent symmetry energy at subsaturation densities from nuclear mass differences
doi: 10.1103/PhysRevC.89.017305
2014WA51 Phys.Rev. C 90, 055801 (2014) Neutron star properties in density-dependent relativistic mean field theory with consideration of an isovector scalar meson
doi: 10.1103/PhysRevC.90.055801
2014ZH28 Nucl.Phys. A929, 38 (2014) H.Zhang, J.Dong, N.Ma, G.Royer, J.Li, H.Zhang An improved nuclear mass formula with a unified prescription for the shell and pairing corrections NUCLEAR STRUCTURE A=16-270; calculated binding energy, mass excess, separation energy; deduced coefficients of modified macroscopic-microscopic nuclear mass formula. Compared with other calculations and data.
doi: 10.1016/j.nuclphysa.2014.05.019
2014ZH39 Phys.Rev. C 90, 054326 (2014) Q.Zhao, J.M.Dong, J.L.Song, W.H.Long Proton radioactivity described by covariant density functional theory with the similarity renormalization group method RADIOACTIVITY 146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 170,171Au, 176,177Tl(p); calculated half-lives and spectroscopic factors for spherical nuclei. Covariant density functional (CDF) theory, combined with the WKB approximation, and the similarity renormalization group (SRG) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.054326
2013DO01 Phys.Rev. C 87, 014303 (2013) Origin of symmetry energy in finite nuclei and density dependence of nuclear matter symmetry energy from measured α-decay energies NUCLEAR STRUCTURE 208Pb; symmetry energy distribution, isospin asymmetry distribution function, polarizations of neutron and proton densities using the Skyrme-energy density functional and Hartree-Fock approach; deduced neutron skin thickness from experimental α-energies, and compared with other methods.
doi: 10.1103/PhysRevC.87.014303
2013DO02 Nucl.Phys. A898, 32 (2013) J.Dong, U.Lombardo, W.Zuo, H.Zhang Dense nuclear matter and symmetry energy in strong magnetic fields
doi: 10.1016/j.nuclphysa.2012.11.011
2013DO13 Phys.Rev. C 87, 062801 (2013) 3PF2 pairing in high-density neutron matter
doi: 10.1103/PhysRevC.87.062801
2013DO15 Phys.Rev. C 88, 014302 (2013) J.Dong, H.Zhang, L.Wang, W.Zuo Density dependence of the symmetry energy probed by β--decay energies of odd-A nuclei NUCLEAR STRUCTURE 208Pb; analyzed symmetry energy coefficient from experimental Q(β-) values; deduced slope parameter of symmetry energy and compared with previous studies, density dependence of nuclear matter symmetry energy, neutron skin thickness.
doi: 10.1103/PhysRevC.88.014302
2013WA12 Phys.Rev. C 87, 047301 (2013) Tensor effects on the evolution of the N=40 shell gap from nonrelativistic and relativistic mean-field theory NUCLEAR STRUCTURE 60Ca, 62Ti, 64Cr, 66Fe, 68Ni, 70Zn; calculated neutron gap, contributions of the neutron gap from the isovector and tensor couplings. Nonrelativistic Skyrme-Hartree-Fock-Bogoliubov (SHFB) and relativistic Hartree-Fock-Bogoliubov (RHFB) theory with the inclusion of tensor force, and using PKA1 and PKO3 interactions.
doi: 10.1103/PhysRevC.87.047301
2013WA15 Phys.Rev. C 87, 054331 (2013) L.J.Wang, B.Y.Sun, J.M.Dong, W.H.Long Odd-even staggering of the nuclear binding energy described by covariant density functional theory with calculations for spherical nuclei NUCLEAR STRUCTURE Z=6, N=3-13; Z=8, N=5-15; Z=20, N=17-31; Z=28, N=27-45; Z=40, N=45-63; Z=50, N=53-83; Z=58, N=69-91; Z=64, N=77-97; Z=82, N=99-131; N=50, Z=29-49; N=82, Z=51-71; calculated neutron and proton odd-even staggering of binding energies. N=50, Z=30-48; N=82, Z=50-70; calculated average pairing gap. 112,114,118,124Sn; calculated occupation numbers of valence neutron orbits. 196,198,200,202,204,206,208,210,212,214,216Pb; calculated pairing energy. Analyzed effects of the optimized pairing force on the pairing energy and binding energy. Spherical covariant density functional (CDF) theory using relativistic Hartree-Fock-Bogoliubov (RHFB) and relativistic Hartree-Bogoliubov (RHB) methods with Gogny D1S pairing force. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.054331
2012DO02 Phys.Rev. C 85, 034308 (2012) J.Dong, W.Zuo, J.Gu, U.Lombardo Density dependence of the nuclear symmetry energy constrained by mean-field calculations NUCLEAR STRUCTURE 208Pb; calculated neutron skin thickness relation to saturation density, slope parameter, curvature parameter, properties of neutron stars, based on mean-field interactions. Comparison with previous studies.
doi: 10.1103/PhysRevC.85.034308
2011DO10 Nucl.Phys. A861, 1 (2011) New approach for alpha decay half-lives of superheavy nuclei and applicability of WKB approximation RADIOACTIVITY 270,272,274Bh, 274,275,276,278Mt, 278,279,280,282Rg, 283,285Cn, 282,283,284,286Nh, 287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 294Og(α); calculated T1/2, potential barrier, proton-, α- and cluster-penetrability. Comparison with available data.
doi: 10.1016/j.nuclphysa.2011.06.016
2011DO11 Phys.Rev.Lett. 107, 012501 (2011) Correlation between α-Decay Energies of Superheavy Nuclei Involving the Effects of Symmetry Energy RADIOACTIVITY 280,282Rg, 283,285Cn, 282,283,284,285,286Nh, 286,297,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294Og(α); calculated Q-values; deduced symmetry dependent formula. Liquid-drop model.
doi: 10.1103/PhysRevLett.107.012501
2011DO12 Phys.Rev. C 84, 014303 (2011) J.M.Dong, W.Zuo, J.Z.Gu, Y.Z.Wang, L.G.Cao, X.Z.Zhang Effects of tensor interaction on pseudospin energy splitting and shell correction NUCLEAR STRUCTURE 106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn; calculated proton and neutron pseudospin orbit splittings. 132Sn, 298Fl; calculated neutron and proton shell correction energies, single particle spectra. Skyrme-Hartree-Fock approach with the SLy5+TF and T31+TF parameter sets combined with the BCS method.
doi: 10.1103/PhysRevC.84.014303
2011WA04 Int.J.Mod.Phys. E20, 127 (2011) Y.Z.Wang, Q.F.Gu, J.M.Dong, B.B.Peng Alpha decay half-lives of exotic nuclei around shell closures RADIOACTIVITY 177,179,183,185,187Tl, 181,183,185,187,191Pb, 186,187,188,189,191,193,194,195,209Bi, 209,210,211,212Po, 211,213Rn, 213,214,215Ra, 215,216,217Th, 217,218,219U, 211,212At, 213,214Fr, 215,216Ac, 217,218Pa, 210,211,212Po(α); calculated T1/2. Generalized liquid drop model, comparison with experimental and other data.
doi: 10.1142/S0218301311017375
2011WA10 Phys.Rev. C 83, 054305 (2011) Y.Z.Wang, J.Z.Gu, J.M.Dong, X.Z.Zhang Systematic study of tensor effects in shell evolution NUCLEAR STRUCTURE Z=8, 20, 28, N=8-50 (even N); N=8, 20, 28, Z=6-32 (even Z); calculated evolution of magic gaps with and without tensor forces, proton spin-orbit potentials and radial wave function square, energy differences between the 1d5/2 and 1d3/2 single proton states in Ca isotopes. Hartree-Fock-Bogliubov approach with several Skyrme interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.054305
2011WA28 Chin.Phys.Lett. 28, 102101 (2011) Y.-Z.Wang, J.-Z.Gu, X.-Z.Zhang, J.-M.Dong Tensor Effect on Bubble Nuclei NUCLEAR STRUCTURE 34Si, 46Ar; calculated proton density distributions, single-particle spectra and proton spin-orbit potential. Hartree-Fock-Bogoliubov (HFB) approach.
doi: 10.1088/0256-307X/28/10/102101
2011WA29 Phys.Rev. C 84, 044333 (2011) Y.Z.Wang, J.Z.Gu, X.Z.Zhang, J.M.Dong Tensor effects on the proton sd states in neutron-rich Ca isotopes and bubble structure of exotic nuclei NUCLEAR STRUCTURE 40,42,44,46,48,50,52,54,56,58,60,62,64,66,68Ca; calculated energy differences of the proton single-particle states with and without tensor force. 48,64Ca; calculated proton spin-orbit potentials and squared radial wave functions, proton single-particle energies. 46Ar, 206Hg; calculated proton single-particle spectrum, proton density distributions. Hartree-Fock-Bogoliubov (HFB) approach with Skyrme interactions SLy5+T, SLy5+Tw and several sets of the TIJ parameterizations. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.044333
2010DO08 Nucl.Phys. A832, 198 (2010) J.Dong, H.Zhang, Y.Wang, W.Zuo, J.Li Alpha-decay for heavy nuclei in the ground and isomeric states RADIOACTIVITY 154Ho, 154Tm, 155Lu, 156Hf, 157,158,160,161Ta, 158W, 161,162,164Re, 166,167,169,174Ir, 173,176Au, 187Hg, 177,181Tl, 185,187Pb, 186,188,191,193,194,195Bi, 193,195,197,199,201Po, 195,197,198,202,212,214At, 195,197,199,201,203Rn, 200,202,204,206Fr, 205,207Ra, 206,208,216Ac, 216Th, 217Pa, 245Md, 253Lr, 257Db, 263Sg(α); calculated T1/2 using generalized liquid drop model (GLDM) for ground-state and isomers. Comparison with experimental data.
doi: 10.1016/j.nuclphysa.2009.10.082
2010DO09 Chin.Phys.C 34, 182 (2010) J.-M.Dong, H.-F.Zhang, W.Zuo, J.-Q.Li Unified fission model for proton emission NUCLEAR STRUCTURE 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,176Ir, 171Au, 177Tl, 185Bi; calculated proton radioactivity T1/2 for spherical emitters. Comparison with experimental data.
doi: 10.1088/1674-1137/34/2/005
2010DO10 Phys.Rev. C 81, 064309 (2010) J.Dong, W.Zuo, J.Gu, Y.Wang, B.Peng α-decay half-lives and Qα values of superheavy nuclei RADIOACTIVITY 271Sg, 270,272,274Bh, 275Hs, 274,275,276,278Mt, 279Ds, 278,279,280,282Rg, 281,283,284,285,287Cn, 281,282,283,284,286,288Nh, 285,286,287,288,289,291Fl, 286,287,288,289,290,292Mc, 289,290,291,292,293,295Lv, 293,294,295Ts, 294,295Og(α); calculated Q(α) and half-lives using Unified Fission Model (UFM). Comparison with experimental data.
doi: 10.1103/PhysRevC.81.064309
2010WA23 Phys.Rev. C 81, 067301 (2010) Y.Z.Wang, J.M.Dong, B.B.Peng, H.F.Zhang Fine structure of α decay to rotational states of heavy nuclei RADIOACTIVITY 172,174,186Os, 180,182,184,186,188,190Pt, 186,188Hg, 228,230,232Th, 230,232,234,236,238U, 232,234,236,238,240,242,244Pu, 238,240,242,244,246,248,250,252,254Cm, 246,248,250,252,254,256Fm, 252,254,256No, 256Rf, 260Sg(α); calculated Q-values, α branches to 2+ and 4+ states using generalized liquid drop model and improved Royer's formula calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.067301
2010WA31 Eur.Phys.J. A 44, 287 (2010) Y.Z.Wang, J.Z.Gu, J.M.Dong, B.B.Peng Properties of α-decay to ground and excited states of heavy nuclei RADIOACTIVITY 222,224,226Ra, 226,228,230,232Th, 228,230,232,234,236,238U, 234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 244,246,248,250,252Cf, 248,250,252Fm, 252No(α); calculated branching ratios, T1/2 using generalized liquid drop model and Royer's formula. Comparison with data and other models.
doi: 10.1140/epja/i2010-10948-4
2010WA35 Int.J.Mod.Phys. E19, 1961 (2010) Y.Z.Wang, J.Z.Gu, J.M.Dong, B.B.Peng Properties of alpha decay to rotational bands of heavy nuclei RADIOACTIVITY 254,256,258No, 256,258,260Rf(α); calculated branching ratios, T1/2 of α-decays of the ground and rotational bands. Generalized Liquid Drop Model (GLDM).
doi: 10.1142/S0218301310016442
2010ZH16 J.Phys.(London) G37, 085107 (2010) H.F.Zhang, Y.J.Wang, J.M.Dong, J.Q.Li, W.Scheid Concise methods for proton radioactivity RADIOACTIVITY 103,104,105Sb, 155,156,109I, 112,113Cs, 117La, 121Pr, 130,131,132Eu, 135Tb, 140,141Ho, 145,146,147Tm, 150,151Lu, 157Ta, 159,160,161,162,163Re, 164,165,166,167Ir, 169,170,171Au, 176,177Tl, 184,185Bi(p); calculated proton radioactivity T1/2, spectroscopic factors for deformed and microscopic factors for spherical emitters. Comparison with other calculations.
doi: 10.1088/0954-3899/37/8/085107
2009DO06 Phys.Rev. C 79, 054330 (2009) Proton radioactivity within a generalized liquid drop model RADIOACTIVITY 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated proton decay half-lives and penetration probabilities using generalized liquid drop model (GLDM) calculations and WKB approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.054330
2009DO16 Eur.Phys.J. A 41, 197 (2009) J.M.Dong, H.F.Zhang, J.Q.Li, W.Scheid Cluster preformation in heavy nuclei and radioactivity half-lives RADIOACTIVITY 226Th(14C), 226Th(18O), 230U(22Ne), (24Ne), 232Th(24Ne), (26Ne), 236U(26Ne), 232U, 233U, 235U(28Mg), 237Np(30Mg), 240Pu, 241Am(34Si); calculated T1/2 for cluster decay using unified fission model; deduced cluster preformation factors. Comparison with data. A=114-124(12C), (16O); A=215-252(8Be), (12C), (14C), (15N), (16O), (17O), (18O), (20O), (22O), (22Ne), (24Ne), (25Ne), (26Ne), (23F), (28Mg), (29Mg), (30Mg), (32Si), (33Si), (34Si), (36S), (38S), (42S), (46Ar), (48Ca), (50Ca); calculated T1/2 for cluster decay using unified fission model.
doi: 10.1140/epja/i2009-10819-1
2009DO21 Chin.Phys.C 33, 633 (2009) J.-M.Dong, H.-F.Zhang, Y-Z.Wang, W.Zuo, X.-N.Su, J.-Q.Li α-decay half-lives of superheavy nuclei and general predictions NUCLEAR STRUCTURE Z=105-118; calculated α-decay T1/2. Generalized liquid drop model (GLDM).
doi: 10.1088/1674-1137/33/8/007
2009GA43 Chin.Phys.C 33, 848 (2009) Y.Gao, J.-M.Dong, H.-F.Zhang, W.Zuo, J.-Q.Li Properties and structure of N = Z nuclei within relativistic mean field theory NUCLEAR STRUCTURE 84Mo; calculated proton and neutron density distributions, single-particle spectra, Fermi energy levels, binding energy, one and two nucleon separation energy, quadrupole deformation, rms radii. Axially deformed RMF.
doi: 10.1088/1674-1137/33/10/006
2009WA01 Phys.Rev. C 79, 014316 (2009) Y.Z.Wang, H.F.Zhang, J.M.Dong, G.Royer Branching ratios of α decay to excited states of even-even nuclei RADIOACTIVITY 180,182,184Hg(α), 186,188Pb(α), 190,194,196,198Po(α), 202Rn(α), 226,228,230,232Th(α), 230,232,234,236U(α), 236,238,240,242Pu(α), 242,244Cm(α), 246Cf(α); calculated branching ratios for decays to ground excited states in the framework of generalized liquid-drop model. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.014316
2009WA08 Chin.Phys.Lett. 26, 062101 (2009) Y-Z.Wang, H.-F.Zhang, J.-M.Dong, X.-N.Su, W.Zuo, J.-Q.Li Branching Ratios of α Decay for Nuclei near Deformed Shell Closures RADIOACTIVITY 270Hs(α); Z=102-112; Calculated α-branching. Generalized Liquid Drop Model (GLDM).
doi: 10.1088/0256-307X/26/6/062101
2009ZH18 Chin.Phys.Lett. 26, 072301 (2009) H.-F.Zhang, J.-M.Dong, Y.-Z.Wang, X.-N.Su, Y.-J.Wang, L.-Z.Cai, T.-B.Zhu, B.-T.Hu, W.Zuo, J.-Q.Li Theoretical Analysis and New Formulae for Half-Lives of Proton Emission NUCLEAR STRUCTURE 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi; calculated proton radioactivity T1/2; deduced formulae for T1/2. comparison with experiment.
doi: 10.1088/0256-307X/26/7/072301
2009ZH28 Phys.Rev. C 80, 037307 (2009) H.F.Zhang, J.M.Dong, G.Royer, W.Zuo, J.Q.Li Preformation of clusters in heavy nuclei and cluster radioactivity RADIOACTIVITY 212,213,214Po, 215At, 238Pu(α), 221Fr, 221,222,223,224Ra, 225Ac, 226Ra(14C), 228Th(20O), 230U(22Ne), 230Th, 231Pa, 232,233,234U(24Ne), 233U(25Ne), 234U(26Ne), 234U, 236,238Pu(28Mg), 238Pu(30Mg), 238Pu(32Si), 242Cm(34Si); calculated preformation factor P0 of cluster decay. 223Ac, 224,226Th(14C), 223Ac(15N), 224Th(16O), 226Th(16O), 232Th, 236U(24Ne), 232Th(26Ne), 233U(28Mg), 237Np(30Mg), 240Pu, 241Am(34Si); calculated half-lives. 114,115,116,117,118,119Ba, 121La(12C), 114,115,116,117,118Ba, 119,120,121,122,124Ce, 125Pr(16O); calculated half-lives. Preformed cluster approach and generalized liquid drop model (GLDM). Comparison with experimental data.
doi: 10.1103/PhysRevC.80.037307
2009ZH38 Phys.Rev. C 80, 057301 (2009) H.F.Zhang, G.Royer, Y.J.Wang, J.M.Dong, W.Zuo, J.Q.Li Analytic expressions for α particle preformation in heavy nuclei RADIOACTIVITY N=82-178(α); analyzed α particle preformation factors from experimental Eα and half-lives; deduced analytical expressions for preformation factors.
doi: 10.1103/PhysRevC.80.057301
2008DO27 Chin.Phys.Lett. 25, 4230 (2008) J.-M.Dong, H.-F.Zhang, W.Zuo, J.Q.Li Half-Lives of Superheavy Nuclei in Z = 113 Alpha Decay Chain RADIOACTIVITY 284,283,282,278Nh; 280,279,278,274Rg;276,275,274Mt;272,270,266Bh; calculated α-decay half-lives using a generalized liquid drop model.
doi: 10.1088/0256-307X/25/12/012
Back to query form Note: The following list of authors and aliases matches the search parameter J.M.Dong: , J.M.DONG |