NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = S.Luo Found 12 matches. 2024LU07 Chin.Phys.C 48, 044105 (2024) S.Luo, D.-M.Zhang, L.-J.Qi, X.Chen, P.-Ch.Chu, X.-H.Li α-particle preformation factors in heavy and superheavy nuclei RADIOACTIVITY 220,222,224,226,228,230,232Th, 222,224,226,228,230,232,234,236,238U, 230,232,234,236,238,240,242,244Pu, 234,236,238,240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254Cf, 244,246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 260Sg, 266,268,270Hs, 270Ds, 282Ds, 286Cn, 286,288Fl, 290,292Lv, 294Og(α); calculated T1/2 using the Two-Potential Approach (TPA); deduced preformation factors. Comparison with available data.
doi: 10.1088/1674-1137/ad21e9
2023LU06 Eur.Phys.J. A 59, 125 (2023) S.Luo, L.-J.Qi, D.-M.Zhang, B.He, P.-C.Chu, X.-H.Li An improved empirical formula of α decay half-lives for superheavy nuclei RADIOACTIVITY 234,236,238Cm, 242Cm, 246Cm, 238Cf, 242Cf, 246Cf, 250Cf, 254Cf, 246Fm, 250Fm, 254Fm, 252No, 256No, 258Rf, 266Hs, 270Hs, 282Ds, 286Fl, 290Lv, 294Og(α); calculated T1/2; deduced formula. Comparison with available data.
doi: 10.1140/epja/s10050-023-01040-5
2023QI01 Chin.Phys.C 47, 014101 (2023) L.-J.Qi, D.-M.Zhang, S.Luo, X.-H.Li, X.-J.Wu, C.-T.Liang Systematic calculations of cluster radioactivity half-lives in trans-lead nuclei RADIOACTIVITY 221Fr, 221,222,223,224Ra, 226Ra, 223Ac(14C), 228Th(20O), 231Pa(23F), 230Th, 231Pa, 232,233,234U(24Ne), 233U(25Ne), 234U(26Ne), (28Mg), 236,238Pu(28Mg), 238Pu(30Mg), (32Si), 242Cm(34Si), 219,220Rn(14C), 221Fr(15N), 223Ra(18O), 225Ra(14C), 225,226Ra(20O), 223Ac(15N), 227Ac(20O), 229Ac(23F), 226Th(18O), (14C), 227Th(18O), 228Th(22Ne), (24Ne), 229Th(20O), 231Th(24Ne), (25Ne), 232Th(26Ne), 227Pa(18O), 229Pa(22Ne), 230U(22Ne), (24Ne), 232,233U(28Mg), 235U(24Ne), (25Ne), (28Mg), (29Mg), 236U(24Ne), (25Ne), (28Mg), (30Mg), 238U(30Mg), 231Np(22Ne), 233Np(24Ne), 235Np(28Mg), 237Np(30Mg), 237Pu(28Mg), 239Pu(29Mg), (34Si), (32Si), (30Mg), 237Am(28Mg), 239Am(32Si), 241Am(34Si), 240,241Cm(32Si), 243,244Cm(34Si); calculated T1/2. Comparison with available data.
doi: 10.1088/1674-1137/ac94bd
2023QI05 Chin.Phys.C 47, 064107 (2023) L.-J.Qi, D.-M.Zhang, S.Luo, B.He, X.-J.Wu, X.Chen, X.-H.Li New Geiger-Nuttall law for cluster radioactivity half-lives RADIOACTIVITY 221Fr, 221,222,223,224Ra, 226Ra, 223,225Ac(14C), 228Th(20O), 231Pa(23F), 230Th, 231Pa, 232,233,234,235U(24Ne), 233U(25Ne), 234U(26Ne), 234,236U, 236,238Pu(28Mg), 236U(30Mg), 238Pu(30Mg), (32Si), 242Cm(34Si); calculated T1/2 from Balasubramaniam's formula and further considering the effect of the parent nucleus mass, blocking effect, and effect of reduced mass on cluster radioactivity half-lives; deduced a new Geiger-Nuttall law that is model-independent. Comparison with available data.
doi: 10.1088/1674-1137/accc78
2023QI06 Phys.Rev. C 108, 014325 (2023) L.-J.Qi, D.-M.Zhang, S.Luo, G.-Q.Zhang, P.-C.Chu, X.-J.Wu, X.-H.Li Cluster radioactivity preformation probability of trans-lead nuclei in the NpNn scheme RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 223Ac(14C);228Th(20O);231Pa(23F);230Th, 231Pa, 232,233,234U(24Ne);233U(25Ne);234U(26Ne);234U, 236,238Pu(28Mg), 238Pu(30Mg);238Pu(32Si);242Cm(34Si); calculated cluster preformation probability. Comparison of results obtained with unified fission model (model dependent approach), cluster formation model (microscopic approach) and Wei model (analytical formula).
doi: 10.1103/PhysRevC.108.014325
2023QI07 Eur.Phys.J. A 59, 255 (2023) L.-J.Qi, D.-M.Zhang, S.Luo, X.-H.Li, B.He, P.C.Chu Cluster radioactivity half-lives of trans-lead nuclei with a statistical physical preformation factor RADIOACTIVITY 221Fr, 221,222,223Ra, 223Ac, 224,226Ra(14C), 228Th(20O), 230Th(24Ne), 231Pa(23F), 231Pa, 232,233U(24Ne), 233U(25Ne), 234U(24Ne), 236Pu(26Ne), 238Pu(28Mg); calculated T1/2 using the cluster preformation probability in statistical physical way and Wentzel-Kramers-Brillouin (WKB) theory. Comparison with available data.
doi: 10.1140/epja/s10050-023-01162-w
2023ZH40 Phys.Rev. C 108, 024318 (2023) D.-M.Zhang, L.-J.Qi, H.-F.Gui, S.Luo, B.He, X.-J.Wu, X.-H.Li Analytic formula for the proton radioactivity spectroscopic factor RADIOACTIVITY 108,109I, 111,112,113Cs, 116,117La, 121Pr, 130,131Eu, 135Tb, 140,141mHo, 144,145,146m,147mTm, 150,150m,151,151mLu, 155,156,156m,157Ta, 159,159m,160,161,161mRe, 164,165,165m,166,166m,167,167m,169mIr, 169,170,170m,171,171m,172Au, 176,177,177mTl, 184,185,185mBi, 103Sb, 127Pm, 159,162Re(p); calculated T1/2, spectrosocopic factors of proton radioactivity. Deformed two-potential approach (D-TPA). Established link between the quadrupole deformation parameter of proton emitter and spectroscopic factor of proton radioactivity. Comparison to available experimental data and theoretical results obtained with universal decay law for proton radioactivity (UDLP) and the new Geiger-Nuttall law (NG-N).
doi: 10.1103/PhysRevC.108.024318
2023ZH52 Chin.Phys.C 47, 114103 (2023) X.-Y.Zhu, S.Luo, L.-J.Qi, D.-M.Zhang, X.-H.Li, W.-B.Lin Simple model for cluster radioactivity half-lives in trans-lead nuclei RADIOACTIVITY 212,214Po, 238Pu(α), 222,224,226Ra(14C), 228Th(20O), 230U(22Ne), 230Th, 232,234U(24Ne), 234U(26Ne), 234,236U, 236,238Pu(28Mg), 236U, 238Pu(30Mg), 238Pu(32Si), 242Cm(34Si), 213Po, 215At(α), 221Fr, 221,223Ra, 225Ac(14C), 231Pa(23F), 231Pa, 233,235U(24Ne), 233,235U(25Ne), 235U(26Ne); calculated T1/2. Comparison with available data.
doi: 10.1088/1674-1137/acf48a
2022LU11 Eur.Phys.J. A 58, 244 (2022) S.Luo, Y.-Y.Xu, D.-X.Zhu, B.He, P.-C.Chu, X.-H.Li Improved Geiger-Nuttall law for α-decay half-lives of heavy and superheavy nuclei RADIOACTIVITY 220,222,224,226,228,230,232Th, 222,224,226,228,230,232,234,236,238U, 230,232,234,236,238,240,242,244Pu, 234,236,238,240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254Cf, 244,246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 260Sg, 266,268,270Hs, 270Ds, 282Ds, 286Cn, 286,288Fl, 292Lv, 294Og, 221,223,225,227,229Th, 221,223,225,227,229,231Pa, 223,225,227,229,231,233U, 233,235,237Np, 229,231,233,235Pu, 245,247,249,251,253,255Es, 241,243,245,247,249,251,253,255,257Fm, 245,247,249,251,253,255,257Md, 251,253,255,257,259No, 224,226,228,230Pa, 224,226,228,230,232,234,236Np, 234,236,238,240,242Am, 234Bk, 240,242,244,246Es, 281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317Ts, 282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318Og, 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319119, 287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320120(α); calculated T1/2. Comparison with available data.
doi: 10.1140/epja/s10050-022-00898-1
2009DI02 Nucl.Instrum.Methods Phys.Res. B267, 2341 (2009) W.Ding, L.Q.Shi, X.G.Long, S.Z.Luo, S.M.Peng, B.Zhang, X.J.Xia Cross-section for D(p, p)D elastic scattering from 1.8 to 3.2 MeV at the laboratory angles of 155 degrees and 165 degrees NUCLEAR REACTIONS 2H(p, p), E=1.8-3.2 MeV; measured Eπ, Iπ, s(θ).
doi: 10.1016/j.nimb.2009.03.108
2008XI03 Nucl.Instrum.Methods Phys.Res. B266, 705 (2008) X.J.Xia, W.Ding, B.Zhang, X.G.Long, S.Z.Luo, S.M.Peng, R.Hutton, L.Q.Shi Cross-section for proton-tritium scattering from 1.4 to 3.4 MeV at the laboratory angle of 165 degrees NUCLEAR REACTIONS 3H(p, p), E=1.4-3.4 MeV; measured proton energies, yields, σ at backward angle.
doi: 10.1016/j.nimb.2008.01.005
2000PE21 Phys.Rev. C62, 025801 (2000) G.X.Peng, H.C.Chiang, B.S.Zou, P.Z.Ning, S.J.Luo Thermodynamics, Strange Quark Matter, and Strange Stars
doi: 10.1103/PhysRevC.62.025801
Back to query form Note: The following list of authors and aliases matches the search parameter S.Luo: , S.C.LUO, S.J.LUO, S.Z.LUO |