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NSR database version of April 27, 2024.

Search: Author = Z.Q.Sheng

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2016FA13      Chin.Phys.C 40, 124101 (2016)

G.-W.Fan, J.-B.Ma, Z.-Q.Sheng, G.-Z.Shi, F.Tian, J.Wang, C.Zhang

Capture cross sections of ¹⁵N(n, γ)¹⁶N at astrophysical energies

NUCLEAR REACTIONS ¹²C(¹⁶N, X), E<1000 MeV/nucleon; ¹⁵N(n, γ)¹⁶N, E(cm)<0.5 MeV; analyzed available ¹²C data; ¹⁶N deduced σ, nuclear radii. Glauber model, comparison with available data.

doi: 10.1088/1674-1137/40/12/124101
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2015FA03      Phys.Rev. C 91, 014614 (2015)

G.W.Fan, M.Fukuda, D.Nishimura, X.L.Cai, S.Fukuda, I.Hachiuma, C.Ichikawa, T.Izumikawa, M.Kanazawa, A.Kitagawa, T.Kuboki, M.Lantz, M.Mihara, M.Nagashima, K.Namihira, Y.Ohkuma, T.Ohtsubo, Z.z.Ren, S.Sato, Z.Q.Sheng, M.Sugiyama, S.Suzuki, T.Suzuki, M.Takechi, T.Yamaguchi, W.Xu

Density distribution of ⁸Li and ⁸B and capture reaction at low energy

NUCLEAR REACTIONS ⁹Be, ¹²C, ²⁷Al(⁸Li, X), E=30-110 MeV, [⁸Li secondary beam produced in ⁹Be(¹³C, X), E=130 MeV/nucleon primary reaction]; measured reaction products, reaction σ(E) at HIMAC synchrotron and fragment-separator facility of NIRS, Japan; deduced density distributions of ⁸B and ⁸Li using modified Glauber model, halo structure of ⁸B. ⁷Li(n, γ)⁸Li, E=0.01 eV-1 MeV; ⁷Be(p, γ)⁸B, E=0-0.5 MeV; calculated capture σ(E) for (n, γ) and S(E) factor for (p, γ) reactions using density distributions determined in present work, comparison with experimental data.

doi: 10.1103/PhysRevC.91.014614
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2479.

2015SH03      Chin.Phys.C 39, 024102 (2015)

Z.-Q.Sheng, L.-P.Shu, G.-W.Fan, Y.Meng, J.-F.Qian

Investigation of proton radioactivity with the effective liquid drop model

RADIOACTIVITY ¹⁰⁵Sb, ¹⁰⁹I, ^112,113Cs, ^145,147Tm, ^150,151Lu, ^155,156,157Ta, ^160,161Re, ^164,166,167Ir, ¹⁷¹Au, ¹⁷⁷Tl, ¹⁸⁵Bi, ⁴²V, ⁵⁰Co, ^54,55Cu, ^68,69Br, ⁷³Rb, ⁷⁶Y, ⁸¹Nb, ⁸⁵Tc, ⁸⁹Rh, ¹⁰⁴Sb, ¹⁰⁸I, ¹¹⁸La, ¹²²Pr, ^126,127Pm, ^130,133Eu, ^136,137Tb, ¹⁴²Ho, ¹⁴⁸Tm, ^152,153Lu, ^162,163Re, ¹⁶⁹Ir, ^{169,170,172,173}Au, ^176,178,179Tl, ^184,186,187Bi(p); calculated T_1/2. Comparison with available data.

doi: 10.1088/1674-1137/39/2/024102
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2011SH13      J.Phys.(London) G38, 055103 (2011)

Z.-q.Sheng, D.-d.Ni, Z.-z.Ren

Systematic calculations on cluster radioactivity half-lives

RADIOACTIVITY ^{112,113,114,115,116,117}Cs, ^{114,115,116,117,118,119,120}Ba, ^{117,118,119,120,121,122}La, ¹²⁰Ce, ²¹⁹Fr, ^219,220,227Ra, ^{219,220,221,222,228}Ac, ^{220,221,221,222,223}Th, ^{221,223,231,232,233,234}Pa, ^{222,223,224,225,226}U, ^{225,226,227,228}Np, ^228,229,230Pu(¹²C), ^{114,115,116,117,118,119}Ba, ^{117,118,119,120,122}La, ^{119,120,121,122,123,124}Ce, ^{121,122,123,124,125,126}Pr, ^124,125,126Nd, ^224,225Th, ^{224,225,226,227}U, ^{225,226,227,228,229}Np, ^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), ^{128,129,130,131,132}Sm, ^{130,131,132,133,134,135}Eu, ^134,135Gd, ^136,137Tb, ¹³⁸Dy(²⁸Si), ¹³¹Sm(²⁹Si), ¹³²Eu, ¹³⁵Gd(²⁹Si), ¹³⁶Tb, ¹³⁸Dy, ^140,141Ho(³²S), ¹⁴³Er(³⁶Ar), ²³⁹Pu, ^239,241Cm(³³Si), ²²⁵Ac, ^{221,222,223,224,226}Ra, ²²⁶Th, ^{220,222,224,226,223,225}Fr, ^220,228Ra, ^{221,222,224,226,227}Ac, ^{224,225,227,223}Th, ^{225,226,227,228}Pa, ^227,228U(¹⁴C), ²²⁶Th(¹⁸O), ^228,229Th(²⁰O), ^229,231Pa(²³F), ^229,230U, ^230,231Np, ^231,232Pu(²²Ne), ²³¹U(²³Ne), ²²⁹Ac, ^{230,231,232,233}Pa, ^{229,230,231,232}Th, ^{230,231,232,233,234,235,236}U, ^231,232,233Np(²⁴Ne), ²³⁴Pa, ²³⁵U(²⁵Ne), ²³²Th, ²³⁶U(²⁶Ne), ¹²⁷Pm(²⁴Mg), ^{232,233,234,235}U, ^234,235,236Np, ^{234,235,236,237,238}Pu, ²³⁵Am(²⁸Mg), ²³⁵U, ²³⁵Np(²⁹Mg), ^236,238Pu, ²³⁷Np(³⁰Mg), ²³⁸Pu, ^236,238Am(³²Si), ²³⁸Np, ^{239,240,241,242}Am, ^{238,239,240,241,242,243}Cm, ^240,241Bk(³⁴Si); calculated T_1/2.

doi: 10.1088/0954-3899/38/5/055103
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2010JI15      Eur.Phys.J. A 44, 465 (2010)

W.Z.Jiang, Z.Z.Ren, Z.Q.Sheng, Z.Y.Zhu

Sensitivity of de-excitation energies of superdeformed secondary minima to the density dependence of symmetry energy with the relativistic mean-field theory

NUCLEAR STRUCTURE ^191,192,194Hg, ^{194,196,198,200}Au; calculated ground state and superdeformed secondary minima properties, radii, deformation, neutron skin thickness using relativistic mean field model.

doi: 10.1140/epja/i2010-10962-6
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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, ^{164,165,166,167}Ir, ¹⁷¹Au, ¹⁷⁷Tl, ¹⁸⁵Bi, ¹⁰⁹I, ^112,113Cs, ¹¹⁷La, ¹²¹Pr, ^130,131Eu, ¹³⁵Tb, ^140,141Ho(p); calculated T_1/2 for semi-spherical and well-deformed proton emitters.

doi: 10.1088/0256-307X/27/11/112301
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2010SH32      Eur.Phys.J. A 46, 241 (2010)

Z.-q.Sheng, Z.-z.Ren

Deformed relativistic mean-field calculations on nuclei near Z = 50 with FSUGold

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136}Sn, ^{108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138}Te, ^{110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,138,140,142}Xe, ^{112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148}Ba; calculated binding energies, quadrupole deformation parameters, hexadecupole moments, charge radii, two-neutron separation energies. Deformed relativistic mean-field theory, comparison with experimental data.

doi: 10.1140/epja/i2010-11038-5
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2008GU03      Int.J.Mod.Phys. E17, 539 (2008)

J.Y.Guo, X.Z.Fang, Z.Q.Sheng

Shape phase transitions and possible E(5) symmetry nuclei for Ti isotopes

NUCLEAR STRUCTURE ^{42,44,46,48,50,52,54,56,58,60,62,64}Ti; calculated potential energy surfaces and ground state deformations using relativistic mean field theory.

doi: 10.1142/S0218301308009860
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