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NSR database version of April 27, 2024.

Search: Author = Y.Z.Wang

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2023WA23      Chin.Phys.C 47, 084101 (2023)

Y.-Z.Wang, F.-Z.Xing, J.-P.Cui, Y.-H.Gao, J.-Z.Gu

Roles of tensor force and pairing correlation in two-proton radioactivity of halo nuclei

RADIOACTIVITY ¹⁸Mg, ²⁰Si(2p); calculated T_1/2 using different Skyrme interactions, Q-values; deduced small effect of tensor force. The framework of spherical Skyrme-Hartree-Fock-Bogoliubov theory.

doi: 10.1088/1674-1137/acd680
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2022CU01      Nucl.Phys. A1017, 122341 (2022)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Improved effective liquid drop model for α-decay half-lives

RADIOACTIVITY ^{255,256,258,259,261,263}Rf, ^{256,257,258,259}Db, ²⁷⁰Db, ^259,260,261Sg, ²⁶³Sg, ^267,269,271Sg, ²⁶³Sg, ^267,269,271Sg, ^260,261Bh, ^265,266,267Bh, ^270,272,274Bh, ^264,265,266Hs, ^268,269,270Hs, ^273,275Hs, ²⁷⁰Mt, ^274,275,276Mt, ²⁷⁸Mt, ²⁶⁷Ds, ^269,270,271Ds, ²⁷³Ds, ^277,279,281Ds, ²⁷²Rg, ^{278,279,280,281,282}Rg, ²⁷⁷Cn, ^281,283Cn, ^284,285Cn, ²⁷⁸Nh, ^{282,283,284,285,286}Nh, ^{285,286,287,288,289}Fl, ²⁸⁷Mc, ^289,290Mc, ^{290,291,292,293}Lv, ^293,294Ts, ²⁹⁴Og(α); calculated T_1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122341
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2022CU02      Nucl.Phys. A1017, 122341 (2022)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Improved effective liquid drop model for α-decay half-lives

RADIOACTIVITY ^{255,256,258,259,261,263}Rf, ^{256,257,258,259,270}Db, ^{259,260,261,263,267,269,271}Sg, ^{260,261,265,266,267,270,272,274}Bh, ^{264,265,266,268,269,270,273,275}Hs, ^{270,274,275,276,278}Mt, ^{267,269,270,271,273,277,279,281}Ds, ^{272,278,279,280,281,282}Rg, ^{277,281,283,284,285}Cn, ^{278,282,284,285,286}Nh, ^{285,286,287,288,289}Fl, ^{287,288,289,290}Mc, ^{290,291,292,293}Lv, ^293,294Ts, ^{278,282,286,290,294,298,302,306}Og, ^{281,285,289,293,297,301,305,309}119, ^{286,290,294,298,302,306,310,289,293,297,301,305,309}120(α); calculated T_1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122341
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2022WA18      Phys.Lett. B 831, 137198 (2022)

Y.-Z.Wang, S.Zhang, Y.-G.Ma

System dependence of away-side broadening and α-clustering light nuclei structure effect in dihadron azimuthal correlations

NUCLEAR REACTIONS ¹⁶O(¹⁶O, X), ¹⁰B(¹⁰B, X), ⁴⁰Ca(⁴⁰Ca, X), ⁹⁶Zr(⁹⁶Zr, X), ¹⁹⁷Au(¹⁹⁷Au, X), E=6.73 TeV; analyzed available data; deduced dihadron azimuthal correlation, the momentum dependence of away-side broadening parameters.

doi: 10.1016/j.physletb.2022.137198
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2020CU01      Phys.Rev. C 101, 014301 (2020), Erratum Phys.Rev. C 104, 029902 (2021)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Two-proton radioactivity within a generalized liquid drop model

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); calculated half-lives for 2p decay mode using generalized liquid drop model (GLDM) and compared with experimental half-lives, and other theoretical calculations. ²²Si, ²⁶S, ³⁴Ca, ^38,39Ti, ⁴²Cr, ⁴⁹Ni, ⁵⁵Zn, ^58,59,60Ge, ⁶⁴Se(2p); predicted half-lives using GLDM for 2p radioactivity.

doi: 10.1103/PhysRevC.101.014301
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2019CU01      Nucl.Phys. A987, 99 (2019)

J.P.Cui, Y.Xiao, Y.H.Gao, Y.Z.Wang

α-decay half-lives of neutron-deficient nuclei

RADIOACTIVITY Z=80-118(α); calculated α-decay T_1/2 of neutron-deficient nuclei using Effective Liquid Drop Model (ELDM), generalized Liquid Drop Model (GLDM) within fission-like and cluster-like modes and using Royer and Denisov formulae; T_1/2 compared to data; deduced that GLDM gives higher values than calculations using other approaches; calculated, predicted T_1/2 n-deficient nuclei not measured using GLDM with WS4 Q_α values.

doi: 10.1016/j.nuclphysa.2019.04.008
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2019WA10      Chin.Phys.Lett. 36, 32101 (2019)

Y.-Z.Wang, Y.Li, C.Qi, J.-Z.Gu

Pairing Effects on Bubble Nuclei

NUCLEAR STRUCTURE ⁴⁶Ar, ²⁰⁶Hg; calculated proton density distributions, occupation probabilities of the proton s states; deduced the difference between the bubble structure with the surface pairing and those with the volume and mixed pairings.

doi: 10.1088/0256-307x/36/3/032101
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2019WA30      Chin.Phys.C 43, 114101 (2019)

Y.-Z.Wang, X.-D.Su, C.Qi, J.-Z.Gu

Tensor force effect on the exotic structure of neutron-rich Ca isotopes*

NUCLEAR STRUCTURE ^{56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74}Ca; calculated two neutron separation energy, radii, neutron density distributions using spherical Skyrme-Hartree-Fock-Bogoliubov (SHFB) approach.

doi: 10.1088/1674-1137/43/11/114101
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2018CU01      Phys.Rev. C 97, 014316 (2018)

J.P.Cui, Y.L.Zhang, S.Zhang, Y.Z.Wang

α-decay half-lives of superheavy nuclei

RADIOACTIVITY ^{255,256,258,259,261,263}Rf, ^{256,257,258,259,270}Db, ^{259,260,261,263,267,269,271}Sg, ^{260,261,265,266,267,270,272,274}Bh, ^{264,265,266,268,269,270,273,275}Hs, ^{270,274,275,276,278}Mt, ^{267,269,270,271,273,277,279,281}Ds, ^{272,278,279,280,281,282}Rg, ^{277,281,283,284,285}Cn, ^{278,282,283,284,285,286}Nh, ^{285,286,287,288,289}Fl, ^{287,288,289,290}Mc, ^{290,291,292,293}Lv, ^293,294Ts, ²⁹⁴Og(α); calculated α-decay half-lives of superheavy nuclei, and compared with experimental values; deduced hindrance factors. ^{289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304}Og, ^{290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305}119, ^{291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306}120(α); calculated Q(α) and corresponding half-lives using theoretical WS4, FRDM, KTUY and GHFB mass tables. Effective liquid drop model (ELDM).

doi: 10.1103/PhysRevC.97.014316
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2018ZH04      Phys.Rev. C 97, 014318 (2018)

Y.L.Zhang, Y.Z.Wang

Systematic study of cluster radioactivity of superheavy nuclei

RADIOACTIVITY ²⁹⁴Og(α), (⁸Be), (¹²C), (¹⁶O), (²⁸Mg), (³²Si), (⁶⁸Ni), (⁷⁶Zn), (⁷⁹Ga), (⁸⁰Ge), (⁸³As), (⁸⁴Se), (⁸⁵Br), (⁸⁶Kr), (⁸⁹Rb), (⁹⁰Sr), (⁹⁶Y), (⁹⁶Zr), (⁹⁹Nb), (¹⁰²Mo); ²⁹⁶120(α), (⁸Be), (¹²C), (¹⁶O), (³²Si), ⁴⁸Ca, (⁶⁸Ni), (⁷⁴Zn), (⁷⁷Ga), (⁸⁰Ge), (⁸³As), (⁸⁴Se), (⁸⁵Br), (⁸⁶Kr), (⁸⁷Rb), (⁹⁰Sr), (⁹³Y), (⁹⁶Zr), (¹⁰³Nb), (¹⁰⁰Mo); ²⁹⁸122(α), (⁸Be), (¹²C), (¹⁶O), (³⁰Si), ⁴⁸Ca, (⁶⁶Ni), (⁷²Zn), (⁷⁵Ga), (⁸⁰Ge), (⁸¹As), (⁸⁴Se), (⁸⁵Br), (⁸⁶Kr), (⁸⁷Rb), (⁹⁰Sr), (⁸⁹Y), (⁹⁴Zr), (⁹⁷Nb), (⁹⁸Mo); calculated probable half-lives of cluster radioactive (CR) decay modes using unified description (UD) formula, universal (UNIV) curve, Horoi formula, and universal decay law (UDL). ^{286,288,290,292,294}Og(α), (⁸⁶Kr); ²⁹⁶Og(α), (⁸⁸Kr); ²⁹⁸Og(α), (⁹⁰Kr); ³⁰⁰Og(α), (⁹⁴Sr); ³⁰²Og(α), (⁹⁶Sr); ³⁰⁴Og(α), (⁹⁸Sr); ³⁰⁶Og(α), (¹⁰²Zr); ³⁰⁸Og(α), (¹⁰⁴Zr); ^310,312Og(α), (¹⁰⁶Zr); ^314,316Og(α), (¹¹¹Nb); ^318,320Og(α), (¹¹³Nb); ^{284,286,288,290,294}120(α), (⁸⁸Sr); ^292,296120(α), (⁹⁰Sr); ²⁹⁸120(α), (⁹²Sr); ^300,302120(α), (⁹⁴Sr); ³⁰⁴120(α), (⁹⁶Sr); ³⁰⁶120(α), (¹⁰⁰Zr); ³⁰⁸120(α), (¹⁰²Zr); ³¹⁰120(α), (¹⁰⁴Zr); ^312,314,316120(α), (¹⁰⁶Zr); ^318,320,322120(α), (¹¹¹Nb); ^324,326120(α), (¹¹³Nb); ³²⁸120(α), (¹¹⁵Nb); ^290,292,294122(α), (⁹²Zr); ²⁹⁶122(α), (⁸⁸Sr); ^298,300122(α), (⁹⁴Zr); ^302,304122(α), (⁹⁶Zr); ³⁰⁶122(α), (⁹⁸Zr); ³⁰⁸122(α), (¹⁰⁰Zr); ³¹⁰122(α), (¹⁰²Zr); ^312,314,316122(α), (¹⁰⁴Zr); ^318,320,322122(α), (¹⁰⁶Zr); ³²⁴122(α), (¹¹¹Nb); calculated α-decay half-lives, and half-lives of most probable cluster decays using the universal decay law (UDL).

doi: 10.1103/PhysRevC.97.014318
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2017WA04      Phys.Rev. C 95, 014302 (2017)

Y.Z.Wang, J.P.Cui, Y.L.Zhang, S.Zhang, J.Z.Gu

Competition between α decay and proton radioactivity of neutron-deficient nuclei

RADIOACTIVITY ¹⁰⁹I, ¹¹²Cs, ¹⁵⁷Ta, ^{160,161,161m,162,163}Re, ^{164m,165,165m,166,166m,167,167m}Ir, ^{169,170,170m,171m,173}Au, ^{177,177m,178,179}Tl, ^185,185mBi(p), (α); calculated half-lives, and compared with available experimental values, penetration probabilities. ¹⁰⁵Sb, ¹⁰⁸I, ¹¹³Cs, ¹¹⁷La, ¹²¹Pr, ^130,131,132Eu, ^135,136Tb, ^140,141,141mHo, ^{144,145,146,147,147m}Tm, ^{150,150m,151,151m}Lu, ^155,156,156mTa, ¹⁵⁹Re, ¹⁶⁴Ir, ^171,172,172mAu, ¹⁷⁶Tl(α); calculated α-decay half-lives, and compared with experimental proton-decay half-lives. ¹¹⁶La, ^157mTa, ^159mRe, ^168,169,169mIr, ^184,186,187Bi(p); calculated proton-decay half-lives, and compared with experimental α-decay half-lives. ^155,156Ta, ^159,160,161Re, ^164,165Ir, ^169,170,171Au, ¹⁷⁶Tl, ¹⁸⁵Bi; predicted dominant proton decay mode. ¹⁵⁷Ta, ^162,163Re, ^{165,166,167,168,169}Ir, ^172,173Au, ^177,178,179Tl, ^184,186,187Bi; predicted dominant α decay mode. Effective liquid drop model (ELDM). Comparison with predictions of microscopic model (MM) and with available experimental values.

doi: 10.1103/PhysRevC.95.014302
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2017ZH31      Nucl.Phys. A966, 102 (2017)

Y.L.Zhang, Y.Z.Wang

Systematic study on the competition between α-decay and spontaneous fission of superheavy nuclei

RADIOACTIVITY Z=104, 106, 108, 110, 112, 114, 116, 118, 120(α), (SF); calculated separately spontaneous fission T_1/2 and that for α-decay for nuclei with even number of neutrons, the ratio of the two T_1/2.

doi: 10.1016/j.nuclphysa.2017.06.005
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2016CU01      Int.J.Mod.Phys. E25, 1650056(2016)

J.P.Cui, Y.L.Zhang, S.Zhang, Y.Z.Wang

Systematic study on α-decay half-lives of Bi isotopes

RADIOACTIVITY ^{184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214}Bi(α); calculated T_1/2. The generalized liquid drop model (GLDM) and several sets of Royer's analytic formulas, comparison with experimental data.

doi: 10.1142/S0218301316500567
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2015WA05      Phys.Rev. C 91, 017302 (2015)

Y.Z.Wang, Z.Y.Hou, Q.L.Zhang, R.L.Tian, J.Z.Gu

Effect of a tensor force on the proton bubble structure of ²⁰⁶Hg

NUCLEAR STRUCTURE ²⁰⁶Hg; calculated proton density distribution by Skyrme-Hartree-Fock approach with the SLy5, SLy5+T, and SLy5+T_w interactions. Unlikely scenario for proton bubble structure in ²⁰⁶Hg because of the pairing correlation. Discussed antibubble effect from the pairing interaction based on Skyrme-Hartree-Fock-Bogoliubov approach.

doi: 10.1103/PhysRevC.91.017302
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2015WA35      Phys.Rev. C 92, 064301 (2015)

Y.Z.Wang, S.J.Wang, Z.Y.Hou, J.Z.Gu

Systematic study of α-decay energies and half-lives of superheavy nuclei

RADIOACTIVITY ^{270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302}Ds, ^{272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304}Cn, ^{274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306}Fl, ^{276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308}Lv, ^{278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310}Og, ^{284,286,288,290,292,294,296,298,300,302,304,306,308,310,312}120(α); calculated α-decay energies Q(α) and α-decay half-lives of the superheavy nuclei (SHN) using 20 models and 18 empirical formulas. Comparison with the calculated values, and available experimental data.

doi: 10.1103/PhysRevC.92.064301
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2014WA08      J.Phys.(London) G41, 055102 (2014); Erratum J.Phys.(London) G41, 079501 (2014)

Y.Z.Wang, Z.Y.Li, G.L.Yu, Z.Y.Hou

α-decay half-lives around N = Z isotopes

RADIOACTIVITY ^{104,105,106,107,108,109,110,111}Te, ^{106,107,108,109,110,111,112,113}I, ^{108,109,110,111,112,113,114,115}Xe, ^{110,111,112,113,114}Cs, ^112,113,114Ba(α); calculated T_1/2. Liquid drop model, comparison with available data.

doi: 10.1088/0954-3899/41/5/055102
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2014WA15      Phys.Rev. C 89, 047301 (2014)

Y.Z.Wang, J.Z.Gu, Z.Y.Hou

Preformation factor for α particles in isotopes near N = Z

RADIOACTIVITY ^{105,106,107,108,109,110}Te, ^{108,109,110,111,112}I, ^{109,110,111,112,113}Xe, ^112,114Cs(α); calculated α-particle preformation factors using the generalized liquid drop model, and experimental data for Q values and half-lives. Discussion of odd-even effect on preformation factor.

doi: 10.1103/PhysRevC.89.047301
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2014WA37      Chin.Phys.Lett. 31, 102102 (2014)

Y.-Z.Wang, J.-Z.Gu, G.-L.Yu, Z.-Y.Hou

Tensor Force Effect on Shape Coexistence of N = 28 Neutron-Rich Isotones

NUCLEAR STRUCTURE ⁴⁰Mg, ⁴⁶Ar, ⁴²Si, ⁴⁴S; calculated potential energy surfaces, shell correction energies; deduced impact of tensor force. Skyrme-Hartree-Fock-Bogoliubov approach.

doi: 10.1088/0256-307X/31/10/102102
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2013WA05      Eur.Phys.J. A 49, 15 (2013)

Y.Z.Wang, J.Z.Gu, Z.Y.Li, G.L.Yu, Z.Y.Hou

The effect of the tensor force on the bubble structure in Ar isotopes

NUCLEAR STRUCTURE ^{32,34,36,38,40,42,44,46,48,50,52,54,56}Ar; calculated single-particle levels, J, π, occupational probabilities, proton density distributions using Skyrme-Hartree-Fock approach with different tensor forces; deduced bubble possibility.

doi: 10.1140/epja/i2013-13015-x
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2013WA08      J.Phys.(London) G40, 045105 (2013)

Y.Z.Wang, G.L.Yu, Z.Y.Li, J.Z.Gu

Systematic study of tensor force effect on pseudospin orbital splittings in Sn isotopes

NUCLEAR STRUCTURE Z=50; calculated proton pseudospin orbital splittings. SHFB approach, tensor force.

doi: 10.1088/0954-3899/40/4/045105
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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 ^{106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn; 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
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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 ^{177,179,183,185,187}Tl, ^{181,183,185,187,191}Pb, ^{186,187,188,189,191,193,194,195,209}Bi, ^{209,210,211,212}Po, ^211,213Rn, ^213,214,215Ra, ^215,216,217Th, ^217,218,219U, ^211,212At, ^213,214Fr, ^215,216Ac, ^217,218Pa, ^210,211,212Po(α); calculated T_1/2. Generalized liquid drop model, comparison with experimental and other data.

doi: 10.1142/S0218301311017375
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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 1d_5/2 and 1d_3/2 single proton states in Ca isotopes. Hartree-Fock-Bogliubov approach with several Skyrme interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.054305
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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
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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 ^{40,42,44,46,48,50,52,54,56,58,60,62,64,66,68}Ca; 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
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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, ^{180,182,184,186,188,190}Pt, ^186,188Hg, ^228,230,232Th, ^{230,232,234,236,238}U, ^{232,234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248,250,252,254}Cm, ^{246,248,250,252,254,256}Fm, ^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
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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, ^{226,228,230,232}Th, ^{228,230,232,234,236,238}U, ^{234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{244,246,248,250,252}Cf, ^248,250,252Fm, ²⁵²No(α); calculated branching ratios, T_1/2 using generalized liquid drop model and Royer's formula. Comparison with data and other models.

doi: 10.1140/epja/i2010-10948-4
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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, T_1/2 of α-decays of the ground and rotational bands. Generalized Liquid Drop Model (GLDM).

doi: 10.1142/S0218301310016442
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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), ^{190,194,196,198}Po(α), ²⁰²Rn(α), ^{226,228,230,232}Th(α), ^{230,232,234,236}U(α), ^{236,238,240,242}Pu(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
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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, ^{164,165,166,167}Ir, ¹⁷¹Au, ¹⁷⁷Tl, ¹⁸⁵Bi; calculated proton radioactivity T_1/2; deduced formulae for T_1/2. comparison with experiment.

doi: 10.1088/0256-307X/26/7/072301
Citations: PlumX Metrics

2005LI67      High Energy Phys. and Nucl.Phys. (China) 29, 1 (2005)

R.-J.Li, Y.-J.Ma, X.-G.Wu, Y.-H.Zhang, L.-H.Zhu, S.-Y.Wang, M.-F.Li, G.-D.Liang, X.-Z.Cui, X.-F.Li, G.-Y.Zhao, J.-B.Lu, Y.-Z.Liu Z.-M.Wang, G.-S.Li, S.-X.Wen, C.-X.Yang, T.Komatsubara, K.Furuno

Identification of High-Spin States in Odd-Odd ¹²⁶I