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NSR database version of April 11, 2024.

Search: Author = X.H.Li

Found 61 matches.

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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 ^{220,222,224,226,228,230,232}Th, ^{222,224,226,228,230,232,234,236,238}U, ^{230,232,234,236,238,240,242,244}Pu, ^{234,236,238,240,242,244,246,248}Cm, ^{238,240,242,244,246,248,250,252,254}Cf, ^{244,246,248,250,252,254,256}Fm, ^252,254,256No, ^256,258Rf, ²⁶⁰Sg, ^266,268,270Hs, ²⁷⁰Ds, ²⁸²Ds, ²⁸⁶Cn, ^286,288Fl, ^290,292Lv, ²⁹⁴Og(α); calculated T_1/2 using the Two-Potential Approach (TPA); deduced preformation factors. Comparison with available data.

doi: 10.1088/1674-1137/ad21e9
Citations: PlumX Metrics

2024ZH20      Chin.Phys.C 48, 044102 (2024)

D.-M.Zhang, X.-Y.Hu, L.-J.Qi, H.-M.Liu, M.Li, X.-H.Li

Theoretical calculations of proton emission half-lives based on a deformed Gamow-like model

RADIOACTIVITY ^108,109I, ^112,113Cs, ¹¹⁷La, ¹²¹Pr, ¹³⁵Tb, ¹⁴¹Ho(p); calculated proton emission T_1/2 with deformed Gamow-like model, where the deformation effect was included in the Coulomb potential. Comparison with available data.

doi: 10.1088/1674-1137/ad243d
Citations: PlumX Metrics

2023CH40      Phys.Rev. C 108, 025808 (2023)

P.-C.Chu, X.-H.Li, H.Liu, M.Ju, Y.Zhou

Properties of isospin asymmetric quark matter in quark stars

doi: 10.1103/PhysRevC.108.025808
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2023LI45      Chin.Phys.C 47, 094103 (2023)

X.Liu, J.-D.Jiang, L.-J.Qi, Y.-Y.Xu, X.-J.Wu, X.-H.Li

Systematic calculations of cluster radioactivity half-lives with a screened electrostatic barrier

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224}Ra, ²²⁶Ra, ²²³Ac(¹⁴C), ²²⁸Th(²⁰O), ²³¹Pa(²³F), ²³⁰Th, ²³¹Pa, ^232,233,234U(²⁴Ne), ²³⁴U, ²³³U(²⁵Ne), ²³⁴U(²⁶Ne), (²⁸Mg), ^236,238Pu(²⁸Mg), ²³⁸Pu(³⁰Mg), (³²Si), ²⁴²Cm(³⁴Si); calculated T_1/2. Comparison with available data.

doi: 10.1088/1674-1137/ace351
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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 T_1/2; deduced formula. Comparison with available data.

doi: 10.1140/epja/s10050-023-01040-5
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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, ^{221,222,223,224}Ra, 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 T_1/2. Comparison with available data.

doi: 10.1088/1674-1137/ac94bd
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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, ^{221,222,223,224}Ra, ²²⁶Ra, ^223,225Ac(¹⁴C), ²²⁸Th(²⁰O), ²³¹Pa(²³F), ²³⁰Th, ²³¹Pa, ^{232,233,234,235}U(²⁴Ne), ²³³U(²⁵Ne), ²³⁴U(²⁶Ne), ^234,236U, ^236,238Pu(²⁸Mg), ²³⁶U(³⁰Mg), ²³⁸Pu(³⁰Mg), (³²Si), ²⁴²Cm(³⁴Si); calculated T_1/2 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
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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 N_pN_n scheme

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224,226}Ra, 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
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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 T_1/2 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
Citations: PlumX Metrics

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,147m}Tm, ^{150,150m,151,151m}Lu, ^{155,156,156m,157}Ta, ^{159,159m,160,161,161m}Re, ^{164,165,165m,166,166m,167,167m,169m}Ir, ^{169,170,170m,171,171m,172}Au, ^176,177,177mTl, ^184,185,185mBi, ¹⁰³Sb, ¹²⁷Pm, ^159,162Re(p); calculated T_1/2, 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
Citations: PlumX Metrics

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 T_1/2. Comparison with available data.

doi: 10.1088/1674-1137/acf48a
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2022CH21      Phys.Rev. C 105, 045806 (2022)

P.-C.Chu, Y.-N.Wang, X.-H.Li, H.Liu, J.-W.Zhang

Strange quark matter at finite temperature under magnetic fields with a quasiparticle model

doi: 10.1103/PhysRevC.105.045806
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2022CH48      Chin.Phys.C 46, 104104 (2022)

J.-H.Cheng, Z.Zhang, X.-J.Wu, P.-C.Chu, X.-H.Li

Systematic study of proton radioactivity half-lives based on the relationship between Skyrme-Hartree-Fock and the macroscopic quantities of nuclear matter

RADIOACTIVITY ^{144,145,146,147}Tm, ^150,151Lu, ^156,157Ta, ^159,160,161Re, ^{164,165,166,167}Ir, ^170,171Au, ^176,177Tl(p); calculated the spherical proton radioactivity using the relationship between Skyrme parameters and the macroscopic quantities of nuclear matter. Comparison with available data.

doi: 10.1088/1674-1137/ac7a99
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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 ^{220,222,224,226,228,230,232}Th, ^{222,224,226,228,230,232,234,236,238}U, ^{230,232,234,236,238,240,242,244}Pu, ^{234,236,238,240,242,244,246,248}Cm, ^{238,240,242,244,246,248,250,252,254}Cf, ^{244,246,248,250,252,254,256}Fm, ^252,254,256No, ^256,258Rf, ²⁶⁰Sg, ^266,268,270Hs, ²⁷⁰Ds, ²⁸²Ds, ²⁸⁶Cn, ^286,288Fl, ²⁹²Lv, ²⁹⁴Og, ^{221,223,225,227,229}Th, ^{221,223,225,227,229,231}Pa, ^{223,225,227,229,231,233}U, ^233,235,237Np, ^{229,231,233,235}Pu, ^{245,247,249,251,253,255}Es, ^{241,243,245,247,249,251,253,255,257}Fm, ^{245,247,249,251,253,255,257}Md, ^{251,253,255,257,259}No, ^{224,226,228,230}Pa, ^{224,226,228,230,232,234,236}Np, ^{234,236,238,240,242}Am, ²³⁴Bk, ^{240,242,244,246}Es, ^{281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317}Ts, ^{282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318}Og, ^{284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319}119, ^{287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320}120(α); calculated T_1/2. Comparison with available data.

doi: 10.1140/epja/s10050-022-00898-1
Citations: PlumX Metrics

2022PA24      Int.J.Mod.Phys. E31, 2250051 (2022)

X.Pan, Y.-T.Zou, B.He, X.-H.Li, X.-J.Wu, Z.Zhang

Systematic study of two-proton radioactivity half-lives using two-potential approach with different Skyrme interactions

RADIOACTIVITY ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr, ¹⁵Ne, ¹⁷Na, ²²Si, ²⁴P, ²⁶S, ²⁸Cl, ^29,30Ar, ^31,32K, ^33,34Ca, ^35,37Sc, ^37,38,39Ti, ^39,40V, ^41,42Cr, ^43,44Mn, ⁴⁷Co, ⁴⁹Ni, ⁵²Cu, ⁵⁵Zn, ^56,57,58Ga, ^58,59Ge, ^60,61,62As, ^63,64Se, ^65,66Br, ⁶⁸Kr, ⁸¹Mo, ⁸⁵Ru(2p); analyzed available data; calculated T_1/2 using Skyrme energy density functional theory.

doi: 10.1142/S0218301322500513
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2022XU04      Eur.Phys.J. A 58, 16 (2022)

Y.-Y.Xu, H.-M.Liu, D.-X.Zhu, X.Pan, Y.-T.Zou, X.-H.Li, P.-C.Chu

An improved formula for the favored α decay half-lives

RADIOACTIVITY ^146,148Sm, ^148,150,152Gd, ^150,152,154Dy, ^152,154,156Er, ^154,156Yb, ^{156,158,160,162}Hf, ¹⁷⁴Hf, ^{158,160,162,164,166,168}W, ¹⁸⁰W, ^{162,164,166,168,170,172,174}Os, ¹⁸⁶Os, ^{166,168,170,172,174,176,178,180,182,184,186,188,190}Pt, ^{170,172,174,176,178,180,182,184,186,188}Hg, ^{178,180,182,184,186,188,190,192,194}Pb, ²¹⁰Pb, ^{186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^{194,196,198,200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^{202,204,206,208,210,212,214,216,218,220,222,224,226}Ra, ^{208,210,212,214,216,218,220,222,224,226,228,230,232}Th, ^{218,220,222,224,226,228,230,232,234,236,238}U, ^{230,232,234,236,238,240,242,244}Pu, ^{234,236,238,240,242,244,246,248}Cm, ^{238,240,242,244,246,248,250,252,254}Cf, ^244,246Fm, ^252,254,256No, ^256,258Rf, ²⁶⁰Sg, ^266,268,270Hs, ²⁷⁰Ds, ²⁸²Ds, ²⁸⁶Cn, ^286,288Fl, ^290,292Lv, ²⁹⁴Og, ^105,107,109Te, ¹¹³I, ^109,111Xe, ¹⁴⁵Pm, ¹⁴⁷Sm, ¹⁴⁷Eu, ^149,151Gd, ^151,153Dy, ^151,153Ho, ^153,155Er, ^153,155,157Tm, ¹⁵⁵Yb, ^155,157Lu, ^157,159,161Hf, ^157,159,161Ta, ^{159,161,163,165,167}W, ^{159,161,163,165}Re, ^{161,163,165,167,169,171,173}Os, ^{165,167,169,171,173}Ir, ¹⁷⁷Ir, ^{165,167,169,171,173}Pt, ¹⁷⁷Pt, ^181,183,185Pt, ^{171,173,175,177,179,181,183,185}Au, ^173,175Hg, ¹⁷⁹Hg, ¹⁸³Hg, ¹⁸⁵Hg, ^177,179,181Tl, ^{185,187,189,191}Pb, ^{185,187,189,191,193,195,197}Bi, ^{191,193,195,197,199,201}Po, ^205,207,209Po, ^{213,215,217,219}Po, ¹⁸⁷Po, ^{191,193,195,197,199,201,203,205,207,209,211,213,215,217,219}At, ^{195,197,199,201,203,205,207,209}Rn, ^215,217Rn, ^{197,199,201,203,205,207,209,211,213,215,217,219}Fr, ^201,203,205Ra, ^209,211Ra, ²¹⁷Ra, ^{207,209,211,213,215,217,219,221}Ac, ²²⁷Ac, ^209,211,213Th, ²¹⁹Th, ^{211,213,215,217,219,221,223,225,227,229,231}Pa, ²²¹U, ²²⁹U, ²³³U, ²¹⁹Np, ^223,225Np, ²³³Np, ²³¹Pu, ²³⁵Pu, ²³⁹Pu, ²³³Cm, ^239,241Cf, ²⁴⁵Cf, ²⁵³Cf, ^{241,243,245,247}Es, ^251,253,255Es, ²⁴¹Fm, ²⁴⁷Fm, ²⁵¹No, ^253,255Lr, ²⁵⁹Lr, ²⁶¹Rf, ²⁵⁷Db, ²⁶³Sg, ^263,265Hs, ²⁶⁷Ds, ¹⁴⁸Eu, ^152,154Ho, ^154,156Tm, ^156,158Lu, ¹⁵⁸Ta, ^162,164Re, ^{164,166,168,170,172}Ir, ^{170,172,174,176,178}Au, ¹⁸⁴Au, ¹⁸⁸Bi, ¹⁹⁶Bi, ^{192,194,196,198,200,202}At, ^214,216At, ^256,258,260Rf, ²⁶⁰Sg, ^262,264Hs, ^268,270,272Hs, ²⁶⁶Ds, ²⁷⁰Ds, ^276,278Ds, ²⁷⁰Cn, ^280,282Cn, ^284,286,288Fl, ^{288,290,292,294,296}Lv, ^{294,296,298,300,302,304}Og, ^{296,298,300,302,304,306,308}120, ^{302,304,306,308,310,312}122, ^{308,310,312,314,316,318}124, ^{314,316,318,320,322,324,326}126, ^{320,322,324,326,328,330,332}128(α); calculated T_1/2 using the modified Hatsukawa formula. Comparison with available data.

doi: 10.1140/epja/s10050-022-00666-1
Citations: PlumX Metrics

2022XU10      Eur.Phys.J. A 58, 163 (2022)

Y.-Y.Xu, D.-X.Zhu, X.Chen, X.-J.Wu, B.He, X.-H.Li

A unified formula for α decay half-lives

RADIOACTIVITY ¹⁰⁹I, ¹⁵¹Eu, ^149,151Tb, ¹⁵⁵Lu, ¹⁵⁷Ta, ¹⁶⁹Re, ^171,173,175Ir, ¹⁷⁵Pt, ¹⁷⁹Pt, ¹⁸⁵Hg, ¹⁷¹Hg, ¹⁷⁷Hg, ¹⁸¹Hg, ^181,183Tl, ¹⁸⁷Tl, ^{179,181,183,185,187,189}Pb, ^187,189Bi, ^209,211,213Bi, ²¹¹Po, ^187,189Po, ²⁰³Po, ^191,193,195At, ¹⁹³Rn, ²⁰⁵Rn, ^211,213Rn, ^219,221Rn, ^221,223Fr, ²¹³Ra, ^{215,217,219,221,223}Ra, ²⁰⁷Ra, ^223,225Ac, ²¹⁷Th, ^{221,223,225,227,229}Th, ²¹⁷Pa, ²²⁵Pa, ²²⁹Pa, ²¹⁹U, ^223,225,227U, ²³¹U, ^227,229,231Np, ^235,237Np, ²²⁹Pu, ²³³Pu, ²⁴¹Pu, ²²⁹Am, ^{233,235,237,239,241,243}Am, ²³⁵Cm, ^{241,243,245,247}Cm, ^245,247,249Bk, ²³⁷Cf, ²⁴³Cf, ^247,249,251Cf, ²⁴⁹Es, ^243,245,247Fm, ^251,253Fm, ²⁵⁷Fm, ^{245,247,249,251,253,255,257}Md, ^{253,255,257,259}No, ²⁵⁵Lr, ^{255,257,259,261}Rf, ^257,259Db, ²⁶³Db, ^{259,261,263,265}Sg, ²⁶¹Bh, ²⁶³Hs, ²⁶⁹Hs, ²⁰⁵Ac, ²¹⁷Ac, ²⁵⁷Lr, ¹⁵⁴Ho, ¹⁵⁶Lu, ¹⁶²Ta, ¹⁵⁸Ta, ¹⁶⁰Re, ¹⁶⁸Re, ^170,172,174Ir, ^{180,182,184,186}Au, ¹⁷⁸Tl, ^184,186Tl, ^{186,188,190,192,194}Bi, ^212,214Bi, ²⁰⁶At, ^210,212At, ²¹⁸At, ¹⁹²At, ²⁰⁰At, ¹⁹⁸Fr, ^212,214Fr, ^218,220Fr, ^214,216At, ²²⁰At, ²⁰⁸At, ^222,224,226At, ^216,218Pa, ^228,230Pa, ²²⁴Np, ^228,230Np, ²³⁶Np, ²³⁴Am, ²⁴²Am, ^{242,244,246,248}Es, ^252,254Es, ^244,246Md, ²⁵⁰Md, ^256,258Md, ^254,256Lr, ²⁵⁶Db, ^{281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317}Ts, ^{282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318}Og, ^{284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319}119, ^{287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320}120, ²⁵⁴No, ^256,258Rf(α); calculated T_1/2; deduced formula. Comparison with NUBASE2020 values.

doi: 10.1140/epja/s10050-022-00812-9
Citations: PlumX Metrics

2022XU13      Chin.Phys.C 46, 114103 (2022)

Y.-Y.Xu, D.-X.Zhu, Y.-T.Zou, X.-J.Wu, B.He, X.-H.Li

Systematic study on α-decay half-lives of uranium isotopes with a screened electrostatic barrier

RADIOACTIVITY ^216,217,218U, ²²¹U, ^{222,223,224,225,226,227,228}U, ²²⁹U, ^230,231,232U, ²³³U, ^{234,235,236,237,238,239,240,241,242,243}U(α); calculated T_1/2 using the Gamow model with a screened electrostatic barrier. Comparison with available data.

doi: 10.1088/1674-1137/ac7fe8
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2022ZH39      Chin.Phys.C 46, 044106 (2022)

D.-X.Zhu, H.-M.Liu, Y.-Y.Xu, Y.-T.Zou, X.-J.Wu, P.-C.Chu, X.-H.Li

Two-proton radioactivity within Coulomb and proximity potential model

RADIOACTIVITY ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); calculated T_1/2 using the Coulomb and proximity potential model (CPPM). Comparison with available data.

doi: 10.1088/1674-1137/ac45ef
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2021CH52      Phys.Rev. C 104, 045805 (2021)

P.-C.Chu, X.-H.Li, H.Liu, J.-W.Zhang

Quark matter and quark stars within the quasiparticle model under magnetic fields

doi: 10.1103/PhysRevC.104.045805
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2021CH57      Eur.Phys.J. A 57, 305 (2021)

J.-L.Chen, X.-H.Li, X.-J.Wu, P.-C.Chu, B.He

Systematic study on proton radioactivity of spherical proton emitters within two-potential approach

RADIOACTIVITY ^{144,145,146,147}Tm, ^150,151Lu, ^155,156,157Ta, ^159,160,161Re, ^{164,165,166,167}Ir, ^170,171Au, ^176,177Tl(p); calculated T_1/2. Comparison with available data.

doi: 10.1140/epja/s10050-021-00618-1
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2021LI16      Chin.Phys.C 45, 024108 (2021)

H.-M.Liu, Y.-T.Zou, X.Pan, J.-L.Chen, B.He, X.-H.Li

New Geiger-Nuttall law for two-proton radioactivity

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr, ²²Si, ²⁶S, ³⁴Ca, ³⁶Sc, ^38,39Ti, ⁴⁰V, ⁴²Cr, ⁴⁷Co, ⁴⁹Ni, ⁵⁶Ga, ^58,59,60Ge, ⁶¹As, ¹⁰N, ²⁸Cl, ³²K, ⁵⁷Ga, ⁶²As, ⁵²Cu, ⁶⁰As(2p); calculated T_1/2 using GLDM, ELDM, the four-parameter empirical formula. Comparison with experimental data.

doi: 10.1088/1674-1137/abd01e
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2021LI45      Int.J.Mod.Phys. E30, 2150074 (2021)

H.-M.Liu, Y.-T.Zou, X.Pan, B.He, X.-H.Li

Systematic study of two-proton radioactivity half-lives based on a modified Gamow-like model

RADIOACTIVITY ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr, ²²Si, ²⁶S, ³⁴Ca, ³⁶Sc, ^38,39Ti, ⁴⁰V, ⁴²Cr, ⁴⁷Co, ⁴⁹Ni, ⁵⁸Ga, ^58,59Ge, ⁶¹As, ¹⁰N, ²⁸Cl, ³²K, ⁵⁷Ga, ⁶²As, ⁵²Cu, ⁶⁰As(2p); calculated T_1/2; deduced T_1/2 and Q-values reaction. Comparison with available data.

doi: 10.1142/S0218301321500749
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2021LI67      Phys.Scr. 96, 12522 (2021)

H.-M.Liu, Y.-T.Zou, X.Pan, X.-H.Li, X.-J.Wu, B.He

Systematic study of cluster radioactivity half-lives based on a modified Gamow-like model

RADIOACTIVITY ^222,224,226Ra(¹⁴C), ^230,232,234U(²⁴Ne), ^234,236U, ^236,238Pu(²⁸Mg), ²²¹Fr, ^221,223Ra, ²²⁵Ac(¹⁴C), ²³¹Pa, ^233,235U(²⁴Ne), ^233,235U(²⁵Ne); calculated T_1/2. Comparison with available data.

doi: 10.1088/1402-4896/ac3dbc
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2021ZO01      Chin.Phys.C 45, 104101 (2021)

Y.-T.Zou, X.Pan, X.-H.Li, H.-M.Liu, X.-J.Wu, B.He

Systematic study of two-proton radioactivity with a screened electrostatic barrier

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); analyzed available data; calculated T_1/2 using five different theoretical models and/or formulas.

doi: 10.1088/1674-1137/ac1b96
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2021ZO02      Phys.Scr. 96, 075301 (2021)

Y.-T.Zou, X.Pan, H.-M.Liu, X.-J.Wu, B.He, X.-H.Li

Systematic studies on a decay half-lives of neptunium isotopes

RADIOACTIVITY ^{219,223,224,225,233,221,222,229,231,235,237,239,220,226,227,228,232,236}Np(α); calculated T_1/2. Comparison with available data.

doi: 10.1088/1402-4896/abf795
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2020CH12      Nucl.Phys. A997, 121717(2020)

J.-Ha.Cheng, J.-L.Chen, J.-G.Deng, X.-H.Li, Z.Zhang, P.-C.Chu

Systematic study of proton emission half-lives within the two-potential approach with Skyrme-Hartree-Fock

doi: 10.1016/j.nuclphysa.2020.121717
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2020CH43      Eur.Phys.J. A 56, 273 (2020)

J.-H.Cheng, X.Pan, Y.-T.Zou, X.-H.Li, Z.Zhang, P.-C.Chu

Systematic study of proton radioactivity of spherical proton emitters with Skyrme interactions

RADIOACTIVITY ^{144,145,146,147}Tm, ^150,151Lu, ^155,156,157Ta, ^159,160,161Re, ^{164,165,166,167}Ir, ^170,171Au, ^176,177Tl(p); calculated T_1/2. Comparison with experimental data.

doi: 10.1140/epja/s10050-020-00280-z
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2020LI27      Chin.Phys.C 44, 094106 (2020)

H.-M.Liu, Y.-T.Zou, X.Pan, X.-J.Bao, X.-H.Li

Systematic study of the α decay preformation factors of the nuclei around the Z = 82, N = 126 shell closures within the generalized liquid drop model

RADIOACTIVITY ^{186,188,190,192,194}Po, ^{196,198,200,202,204,206,208}Po, ^{200,202,204,206,208,210,212}Rn, ²⁰⁴Ra, ²⁰⁸Ra, ²¹²Th, ²¹⁴Th, ²¹⁶U, ^178,180Pb, ^{184,186,188,190,192,194}Pb, ²¹⁰Pb, ^{212,214,216,218}Po, ^{214,216,218,220}Rn, ²¹⁶Ra, ²¹⁸Ra, ^216,218,220Th, ²¹⁸U, ^{195,197,199,201,203,205,207}Po, ^{197,199,201,203,205,207,209,211}At, ^195,197Rn, ²⁰³Rn, ^207,209Rn, ^{199,201,203,205,207,209,211,213}Fr, ²⁰³Ra, ²⁰⁹Ra, ^205,207Ac, ²¹¹Ac, ^213,215Pa, ^177,179Tl, ^213,215Po, ²¹⁹Po, ^{213,215,217,219}At, ^215,217Rn, ^215,217,219Fr, ²¹⁷Ra, ^215,217Ac, ²¹⁹Th, ²¹⁹Pa, ²²¹Pa, ²²¹U, ²⁰⁹Bi, ¹⁸⁹Po, ²⁰³Po, ^{205,207,209,211,213}Ra, ²¹⁵Th, ^187,189Pb, ²¹³Bi, ²¹³Rn, ^219,221Rn, ²¹⁵Ra, ²¹⁹Ra, ²¹⁷Th, ¹⁹²At, ^{200,202,204,206,208}At, ²⁰⁰Fr, ^204,206,208Fr, ²⁰⁶Ac, ^214,216,218At, ^216,218Fr, ²¹⁸Ac, ²²⁰Pa, ¹⁸⁶Bi, ^190,192,194Bi, ²¹⁰At, ^210,212Fr, ²¹²Pa, ^210,212,214Bi, ²¹²At, ²¹⁴Fr, ²¹⁶Ac(α); calculated T_1/2. Comparison with available data.

doi: 10.1088/1674-1137/44/9/094106
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2019CH14      Phys.Rev. C 99, 035802 (2019)

P.-C.Chu, Y.Zhou, X.Qi, X.-H.Li, Z.Zhang, Y.Zhou

Isospin properties in quark matter and quark stars within isospin-dependent quark mass models

doi: 10.1103/PhysRevC.99.035802
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2019CH27      Nucl.Phys. A987, 350 (2019)

J.-H.Cheng, J.-L.Chen, J.G.Deng, X.-J.Wu, X.-H.Li, P.-C.Chu

Systematic study of α decay half-lives based on Gamow-like model with a screened electrostatic barrier

RADIOACTIVITY Z>51(α); calculated even-even nuclei T_1/2 using modified Gamow-like model including centrifugal potential and electrostatic shielding with two parameters, radius constant r₀ and a parameter for the screened electrostatic potential; Z=120; calculated T_1/2 for 7 even-even nuclei and for some of their not yet synthesized α-decay chain. Halflives compared with those calculated using different approaches and with available data.

doi: 10.1016/j.nuclphysa.2019.05.002
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2019CH41      J.Phys.(London) G46, 065107 (2019)

J.-L.Chen, X.-H.Li, J.-H.Cheng, J.-G.Deng, X.-J.Wu

Systematic study of proton radioactivity based on Gamow-like model with a screened electrostatic barrier

RADIOACTIVITY ¹⁰⁵Sb, ¹⁰⁹I, ^112,113Cs, ¹²¹Pr, ^130,131Eu, ¹³⁵Tb, ^140,141Ho, ^145,146,147Tm, ^150,151Lu, ^155,156,157Ta, ^159,160,161Re, ^{164,165,166,167}Ir, ^170,171Au, ^176,177Tl, ¹⁸⁵Bi(p); calculated T_1/2. Comparison with experimental data.

doi: 10.1088/1361-6471/ab1a56
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2019CH45      Eur.Phys.J. A 55, 214 (2019)

J.-L.Chen, J.-Y.Xu, J.-G.Deng, X.-H.Li, B.He, P.-C.Chu

New Geiger-Nuttall law for proton radioactivity

doi: 10.1140/epja/i2019-12927-7
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2019DE17      Eur.Phys.J. A 55, 58 (2019)

J.-G.Deng, X.-H.Li, J.L.Chen, J.-H.Cheng, X.-J.Wu

Systematic study of proton radioactivity of spherical proton emitters within various versions of proximity potential formalisms

RADIOACTIVITY ^145,146,147Tm, ^150,151Lu, ^155,156,157Ta, ^160,161Re, ^165,166,167Ir, ^170,171Au, ^176,177Tl, ¹⁸⁵Bi(p); calculated proton radioactivity T_1/2; compared with published calculations using different proximity potentials and with data.

doi: 10.1140/epja/i2019-12728-0
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2019LI58      Int.J.Mod.Phys. E28, 1950089 (2019)

H.-M.Liu, J.-Y.Xu, J.-G.Deng, B.He, X.-H.Li

Predictions of α decay half-lives for even-even superheavy nuclei with 104≤ Z ≤ 128 based on two-potential approach within cluster-formation model

RADIOACTIVITY ¹⁴⁴Nd, ^146,148Sm, ^148,150,152Gd, ^150,152,154Dy, ^152,154,156Er, ^154,156,158Yb, ^{156,158,160,162,164,166,168,170,172,174}Hf, ^{158,160,162,164,166,168}W, ¹⁸⁰W, ^{162,164,166,168,170,172,174}Os, ¹⁸⁶Os, ^{166,168,170,172,174,176,178,180,182,184,186,188,190}Pt, ^{172,174,176,178,180,182,184,186,188}Hg, ¹⁸⁰Pb, ^{184,186,188,190,192,194}Pb, ²¹⁰Pb, ¹⁹⁰Po, ^{194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^194,196Rn, ^{200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^202,204Ra, ²⁰⁸Ra, ^{214,216,218,220,222,224,226}Ra, ^{212,214,216,218,220,222,224,226,228,230,232}Th, ^{216,218,220,222,224,226,228,230,232,234,236,238}U, ^{228,230,232,234,236,238,240,242,244}Pu, ^{234,236,238,240,242,244,246,248,250}Cm, ^{238,240,242,244,246,248,250,252,254,256}Cf, ²⁴⁴Fm, ²⁴⁸Fm, ^252,254,256Fm, ^254,256,258No, ^256,258,260Rf, ²⁶⁰Sg, ²⁶⁴Hs, ^268,270Hs, ²⁷⁰Ds, ^286,288Fl, ^290,292Lv, ²⁹⁴Og(α); calculated T_1/2. Comparison with available data.

doi: 10.1142/S0218301319500897
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2019YU04      Phys.Rev. C 100, 054609 (2019); Erratum Phys.Rev. C 102, 049901 (2020)

K.Yue, J.T.Zhang, X.L.Tu, C.J.Shao, H.X.Li, P.Ma, B.Mei, X.C.Chen, Y.Y.Yang, X.Q.Liu, Y.M.Xing, K.H.Fang, X.H.Li, Z.Y.Sun, M.Wang, P.Egelhof, Yu.A.Litvinov, K.Blaum, Y.H.Zhang, X.H.Zhou

Measurement of ⁵⁸Ni(p, p)⁵⁸Ni elastic scattering at low momentum transfer by using the HIRFL-CSR heavy-ion storage ring

NUCLEAR REACTIONS ¹H(⁵⁸Ni, p), E=95 MeV/nucleon; measured Ep, Ip, E(x-ray), I(x-ray), absolute differential σ(θ) using a single-sided silicon detector (SSSD) detector at the Cooler Storage Ring (CSRe) at the Heavy Ion Research Facility in Lanzhou (HIRFL-CSR); deduced nuclear matter rms value. Comparison with KDO3 and LC08 optical model calculations, and with previous experimental results.

doi: 10.1103/PhysRevC.100.054609
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0223.

2018DE14      Chin.Phys.C 42, 044102 (2018)

J.-G.Deng, J.-C.Zhao, J.-L.Chen, X.-J.Wu, X.-H.Li

α decay properties of ²⁹⁶Og within the two-potential approach

RADIOACTIVITY ^{250,252,254,256}Cf, ^254,256Fm, ^256,258No, ^258,260Rf, ²⁶⁰Sg, ^264,268,270Hs, ²⁷⁰Ds, ^294,296Og, ^290,292Lv, ^286,288Fl(α); calculated T_1/2. Comparison with experimental data.

doi: 10.1088/1674-1137/42/4/044102
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2018DE17      Phys.Rev. C 97, 044322 (2018)

J.-G.Deng, J.-C.Zhao, P.-C.Chu, X.-H.Li

Systematic study of α decay of nuclei around the Z=82, N=126 shell closures within the cluster-formation model and proximity potential 1977 formalism

RADIOACTIVITY ^{189,190,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,210,212,213,214,215,216,218,219}Po, ^{194,195,196,197,200,202,203,204,205,206,207,208,209,210,212,213,214,215,216,217,218,219,220,221,222}Rn, ^{202,203,204,207,208,209,213,214,215,216,217,218,219,220}Ra, ^{212,214,215,216,217,218,219,220,221}Th, ^{216,217,218,221,222}U, ^186,188Hg, ^{187,188,189,190,191,192,194,210}Pb, ^{190,192,194,209,210,212,213,214}Bi, ^{192,197,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,223}At, ^{199,200,201,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221}Fr, ^{212,213,214,215,217,219,220,221,222}Pa, ^{205,206,207,211,215,216,217,218,219,220}Ac(α); calculated α-decay preformation factors using cluster-formation model (CFM) and T_1/2 using proximity potential 1977 formalism (Prox.1977). Comparison with experimental data.

doi: 10.1103/PhysRevC.97.044322
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2017DE21      Phys.Rev. C 96, 024318 (2017)

J.-G.Deng, J.-C.Zhao, D.Xiang, X.-H.Li

Systematic study of unfavored α-decay half-lives of closed-shell nuclei related to ground and isomeric states

RADIOACTIVITY ^154mHo, ^161,163Hf, ¹⁶⁵W, ¹⁶⁸Re, ¹⁷¹Os, ^{170m,171m,172,173m,175}Ir, ^175,179Pt, ^177,181Hg, ^179,181Au, ^180,181mTl, ^187,189Pb, ^{190,192,192m,194m,209,212m,213,214}Bi, ^{189,203,211,211m}Po, ^{191m,193m,210,212}At, ^{193,205,211,213,219,221}Rn, ^{210,212,214,220}Fr, ^{207,213,215,219}Ra, ^214,216,216mAc, ^215,217Th, ²²⁴Pa(α), ²¹⁹U(α); calculated Q(α), half-lives, α-preformation probabilities for unfavored α decays of closed-shell nuclei related to ground and isomeric states around Z=82, N=82 and 126 closed shells. Two-potential approach for the valence nucleon (hole) and isospin asymmetry of the parent nuclei; deduced linear dependence on N_pN_n or N_pN_nI. Comparison with experimental data.

doi: 10.1103/PhysRevC.96.024318
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2017DE37      Chin.Phys.C 41, 124109 (2017)

J.-G.Deng, J.-H.Cheng, B.Zheng, X.-H.Li

α decay properties of ²⁹⁷Og within the two-potential approach

RADIOACTIVITY ^251,253,255Cf, ^253,255Es, ^253,257Fm, ^255,257,259Md, ^255,259No, ^257,259Lr, ^{257,259,261,263}Rf, ²⁵⁹Db, ^{259,261,263,265,271}Sg, ^261,271Bh, ^{265,267,269,273,275}Hs, ²⁷⁵Mt, ^{267,269,271,273,277,279,281}Ds, ²⁷⁹Rg, ^277,281,285Cn, ^283,285Nh, ^285,287,289Fl, ^287,289Mc, ^291,293Lv, ²⁹³Ts, ^293,295,297Og(α); calculated T_1/2, transitions J, π, preformation probabilities. Comparison with available data.

doi: 10.1088/1674-1137/41/12/124109
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2017SU02      Chin.Phys.C 41, 014102 (2017)

X.-D.Sun, X.-J.Wu, B.Zheng, D.Xiang, P.Guo, X.-H.Li

Systematic study of α preformation probability of nuclear isomeric and ground states

RADIOACTIVITY ^177,175,173Au, ^{173,171,169,167}Ir, ^169,167,163Re, ¹⁷⁷Tl, ¹⁵⁹Ta, ¹⁵⁵Lu, ^153,151Ho, ¹⁴⁹Tb, ¹⁵³Tm, ¹⁸⁵Hg, ^{185,187,189,191}Pb, ^{195,197,199,201,203}Po, ^195,197,203Rn, ^203,209Ra, ^{187,189,191,193,195,197}Bi, ^191,193,197At, ²⁰¹Fr(α); calculated T_1/2 and the α-particle preformation probabilities. Comparison with available data.

doi: 10.1088/1674-1137/41/1/014102
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2017SU06      Phys.Rev. C 95, 014319 (2017)

X.-D.Sun, C.Duan, J.-G.Deng, P.Guo, X.-H.Li

Systematic study of α decay for odd-A nuclei within a two-potential approach

RADIOACTIVITY ¹⁴⁵Pm, ¹⁴⁷Sm, ¹⁴⁷Eu, ¹⁴⁹Gd, ^149,149m,151Tb, ^151,153Dy, ^{151,151m,153,153m}Ho, ^153,155Er, ^153,153m,155Tm, ^155,157Yb, ^{155,155m,157m}Lu, ¹⁵⁷Hf, ^159,159mTa, ^159,161,163W, ^{159m,161m,163,163m,165m,167m,169m}Re, ^{161,163,165,167,169}Os, ^{165m,167,167m,169,169m,171m,173m,175,177}Ir, ^{167,171,173,175,177,179,181,183}Pt, ^{173,175,177,179,181,183,185}Au, ^{173,177,179,183,185}Hg, ^177,183,187mTl, ^{179,185,185m,187,187m,189,191m}Pb, ^{185m,187m,189m,191m,193m,195m,209,211,213}Bi, ^{187,189,195,195m,197,199,201,203,205,207,211,213,215,217}Po, ^{191m,193m,197,199,201,203,205,207,209,211,213,215,217}At, ^{193,195,195m,197,203,205,207,209,213,215,217,219,221,223}Rn, ^{199,201,203,205,207,209,211,213,215,219,221,223}Fr, ^{203,207,209,211,213,215,217,219,221,223}Ra, ^{207,211,215,217,219,221,223,225,227}Ac, ^{215,217,219,221,223,225,227,229,231}Th, ^{213,215,217,217m,219,221,223,227,229,231}Pa, ^{219,225,227,229,231,235}U, ^{225,227,229,231,235,237,239}Np, ^{229,231,233,235,237,241}Pu, ^{233,235,237,239,241,243}Am, ^{233,237,239,243,245,247}Cm, ^{243,245,247,249}Bk, ^247,249,255Cf, ^243,251,253Es, ^{243,247,247m,251,255,257}Fm, ^{247,247m,251,253,255,257}Md, ²⁵¹No, ^253,255mLr, ^{255m,257m,261,263}Rf, ²⁵⁷Db, ^{259m,261,263,265}Sg, ^265,267Hs, ^{267,269,271,271m,273,273m,277,281}Ds, ^281,285Cn, ²⁸⁹Fl(α); calculated α-decay half-lives for odd-A nuclei, preformation probabilities, and compared with experimental values. Two-potential approach based on isospin dependent nuclear potential.

doi: 10.1103/PhysRevC.95.014319
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2017SU11      Phys.Rev. C 95, 044303 (2017)

X.-D.Sun, J.-G.Deng, D.Xiang, P.Guo, X.-H.Li

Systematic study of α decay half-lives of doubly odd nuclei within the two-potential approach

RADIOACTIVITY ^{105,106,107,108,109,110}Te, ^{108,109,110,111,112,113}I, ^{109,110,111,112,113,115}Xe, ^112,114Cs, ¹¹⁴Ba, ¹⁴⁸Eu, ^152,154Ho, ^154,156Tm, ¹⁵⁶Lu, ¹⁵⁸Ta, ^{160,162,164,166}Re, ^{166,168,170,172,174}Ir, ^170,186Au, ^180,186Tl, ^{190,192,194,196,212,214}Bi, ^{192,194,198,200,202,204,206,208,210,212,214,216,218}At, ^{202,204,208,210,212,214,216,218,220}Fr, ^{212,220,224,228}Pa, ^{214,216,218,220,222,226}Ac, ^232,236Np, ^236,238,242Am, ^246,248Bk, ^{244,246,248,252,254}Es, ^{246,248,250,256,258,260}Md, ^254,258,260Lr, ^{272,274,278,280,282}Rg, ^{258,260,262,268}Db, ^{260,264,266,270,272,274}Bh, ^{268,270,274,276,278}Mt, ^{278,282,284,286}Nh, ^288,290Mc, ^292,294Ts, ²⁹⁶119(α); calculated α-decay half-lives, and α preformation probabilities for odd-odd nuclei using a two-potential approach, and compared with experimental values.

doi: 10.1103/PhysRevC.95.044303
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2016SU09      Phys.Rev. C 93, 034316 (2016)

X.-D.Sun, P.Guo, X.-H.Li

Systematic study of α decay half-lives for even-even nuclei within a two-potential approach

RADIOACTIVITY ¹⁴⁶Sm, ^148,150Gd, ^150,152,154Dy, ^152,154,156Er, ^154,156,158Yb, ^{156,158,160,162}Hf, ^{158,160,162,164,166,168}W, ^{166,168,170,172,174,186}Os, ^{166,168,170,172,174,176,178,180,182,184,186,188,190}Pt, ^{172,174,176,178,180,182,184,186,188}Hg, ^{178,180,182,184,186,188,190,192,194,210}Pb, ^{190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^{198,200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^{206,208,210,212,214,216,218,220,222,224,226}Ra, ^{214,216,218,220,222,224,226,228,230,232}Th, ^{224,226,228,230,232,234,236,238}U, ^{228,230,232,234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248,250}Cm, ^{240,242,244,246,248,250,252,254}Cf, ^{248,250,252,254,256}Fm, ^252,254,256No, ^254,256,258Rf, ^260,266Sg, ^264,266Hs, ²⁷⁰Ds, ^286,288Fl, ^290,292Lv, ²⁹⁴Og(α); calculated half-lives for α decay of Z=62-118 even-even nuclei using two-potential approach based on isospin-dependent nuclear potential taking into account hindrance factors; deduced parameters of isospin-dependent nuclear potentials and analytic expression of hindrance factors. Comparison with experimental half-lives, and with results from density-dependent cluster model (DDCM) and the generalized liquid drop model (GLDM).

doi: 10.1103/PhysRevC.93.034316
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2016SU19      Phys.Rev. C 94, 024338 (2016)

X.-D.Sun, P.Guo, X.-H.Li

Systematic study of favored α-decay half-lives of closed shell odd-A and doubly-odd nuclei related to ground and isomeric states

RADIOACTIVITY ¹⁵¹Dy, ^151,151mHo, ¹⁵³Er, ^{153,153m,154,154m,155}Tm, ^155,157Yb, ^{155,155m,156m,157m}Lu, ¹⁵⁷Hf, ^{158,158m,159,159m}Ta, ^159,161,163W, ^{159m,161m,162m,162m,163,163m,165m}Re, ^{161,163,165,167,169}Os, ^{165m,166,166m,167,167m,169,169m}Ir, ^167,171,173Pt, ^{170,170m,173,175,177}Au, ^177,183Tl, ^179,183Hg, ^{185m,187m,191m}Pb, ^{187m,189m,191m,193m,195m}Bi, ^{195,195m,197,199,201,205,207}Po, ^{197,198,199,200,201,202,203,204,205,206,207,208,209,211,214,214m,218}At, ^{203,207,209,215,217}Rn, ^{204,205,207,208,209,211,213,215,216,216m,217,218,219}Fr, ^209,211,217Ra, ^{213,215,217,219,220,221}Pa, ^{211,213,217,218,219}Ac, ²¹⁹Th(α); calculated half-lives for favored α decays of ground and isomeric states of closed shell odd-A and doubly-odd nuclei using the semiclassical WKB method with the isospin dependent nuclear potential; evaluated α preformation probabilities by the linear relationships of N_pN_n and N_pN_nI, where I=asymmetry parameter between neutrons and protons in parent nuclei. Comparison with experimental data taken from NUBASE-2012.

doi: 10.1103/PhysRevC.94.024338
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2012CH08      Phys.Rev. C 85, 024305 (2012)

R.Chen, B.-J.Cai, L.-W.Chen, B.-A.Li, X.-H.Li, C.Xu

Single-nucleon potential decomposition of the nuclear symmetry energy

doi: 10.1103/PhysRevC.85.024305
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2012LI01      Nucl.Phys. A874, 62 (2012)

X.-H.Li, L.-W.Chen

Isospin dependent global neutron-nucleus optical model potential

NUCLEAR REACTIONS A=24-242(n, n'), (n, n), E=0.05-225 MeV; calculated, analyzed σ(θ) using optical model; deduced optical model parameters.

doi: 10.1016/j.nuclphysa.2011.10.008
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2009LI01      J.Phys.(London) G36, 015102 (2009)

C.-T.Liang, Y.-A.Luo, X.-H.Li, C.-H.Cai

Systematic analysis of the reaction cross section for d, ³He and ⁴He as projectiles

NUCLEAR REACTIONS ⁹Be, ¹²C, ¹⁶O, ²⁸Si, ^40,48Ca, ^58,60Ni, ^{112,116,120,124}Sn, ²⁰⁸Pb(d, X), (³He, X), (α, X), E < 100 MeV/nucleon; calculated total reaction cross sections.

doi: 10.1088/0954-3899/36/1/015102
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2009LI26      J.Phys.(London) G36, 085104 (2009)

C.-T.Liang, X.-H.Li, C.-H.Cai

Global ³He optical model potential below 270 MeV

NUCLEAR REACTIONS ⁹Be, ^10,11B, ^12,13C, ¹⁴N, ^16,17,18O, ^20,22Ne, ²³Na, ^24,25,26Mg, ²⁷Al, ²⁸Si, ³¹P, ⁴⁰Ar, ^40,44,48Ca, ⁵¹V, ⁵²Cr, ^54,56Fe, ⁵⁹Co, ^{58,60,61,62,64}Ni, ⁸⁹Y, ^90,92,94Zr, ¹⁰⁵Pd, ¹¹⁴Cd, ¹¹⁵In, ^116,118,120Sn, ^{144,148,150,152,154}Sm, ¹⁹⁷Au, ²⁰⁵Tl, ²⁰⁸Pb(N, N), E ≤ 270 MeV; calculated σ, σ(θ); deduced ³He optical model potential parameters. Code CAPMN, comparison with experiment.

doi: 10.1088/0954-3899/36/8/085104
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2009LI60      Chin.Phys.C 33, 415 (2009)

X.-H.Li, C.-T.Liang, C.-H.Cai

Comparison between global phenomenological and microscopic optical potentials for proton as projectile below 100 MeV

NUCLEAR REACTIONS Mg, Al, Si, P, S, Cl, Ar, K, Ca, Sc, Ti, V, Cr, Fe, Co, Ni, Cu, Zn, Ge, Se, Sr, Y, Zr, Mo, Rh, Pd, Cd, In, Sn, Te, Ba, La, Ce, Nd, Sm, Gd, Tb, Dy, Ho, Er, Tm, Yb, Hf, Ta, W, Os, Pt, Au, Pb, Bi, Th, U(p, p), E<100MeV; calculated incoming proton σ, elastic scattering σ(θ). Optical model potentials.

doi: 10.1088/1674-1137/33/6/003
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2006LI18      Chin.Phys.Lett. 23, 1142 (2006)

Yu.-J.Liang, X.-H.Li, F.-G.Deng, Z.-H.Liu, H.Yu.Zhou

Theoretical Investigation of the Exotic Structure of the Mirror Nuclei ¹⁷Ne and ¹⁷N

NUCLEAR STRUCTURE ¹⁷N, ¹⁷Ne; calculated radii, halo features. Asymptotic normalization coefficient method.

doi: 10.1088/0256-307X/23/5/022
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2005LI18      Chin.Phys.Lett. 22, 1086 (2005)

Yu.-J.Liang, X.-H.Li, H.-Y.Zhou, Z.-H.Liu, F.G.Deng

Theoretical Analysis of the Exotic Structure of ¹⁷F

NUCLEAR STRUCTURE ¹⁷F; analyzed data; deduced ground and excited state configurations, particle density distributions. Asymptotic normalization coefficient method.

doi: 10.1088/0256-307X/22/5/016
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2001ZH37      Chin.Phys.Lett. 18, 1568 (2001)

J.-B.Zhang, L.Huo, W.-N.Zhang, X.-H.Li, N.Xu, Y.-M.Liu

HBT Parameters and Space-Momentum Correlations in Relativistic Heavy-Ion Collisions

NUCLEAR REACTIONS ¹H(p, X), Si(Si, X), ¹⁹⁷Au(¹⁹⁷Au, X), E(cm)=200 GeV/nucleon; calculated two-pion correlation functions, Hanbury-Brown-Twiss size parameters vs transverse momentum.

doi: 10.1088/0256-307X/18/12/308
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1999RO26      Nucl.Phys. A661, 669c (1999)

M.Rosati, K.Barish, S.Botelho, W.C.Chang, A.L.de Gogoi, O.Dietzsch, T.Ferdousi, A.Franz, S.Y.Fung, J.Gannon, J.Harder, A.Kandasamy, A.Khomutnikov, D.Kotchekov, A.Lebedev, X.H.Li, J.Mahon, M.Munirtassimann, J.Negrin, E.O'Brien, P.O'Connor, R.Pisani, S.Rankowitz, R.Seto, E.M.Takagui, H.Q.Wang

The PHENIX Time Expansion Chamber

doi: 10.1016/S0375-9474(99)85114-8
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1988UD01      Phys.Rev. C37, 429 (1988)

T.Udagawa, X.-H.Li, T.Tamura

Breakup-Fusion Analysis of Continuum Spectra of α- and h-Induced Reactions

NUCLEAR REACTIONS, MECPD ⁵⁸Ni(α, p), (α, d), (α, t), E=80, 160 MeV; ⁹⁰Zr(α, p), (α, 2p), E=140 MeV; ¹⁶⁵Ho(³He, p), (³He, d), E=100 MeV; calculated σ(θp, Ep), σ(θ(t), E(t)), σ(θd, Ed). Break-up fusion model.

doi: 10.1103/PhysRevC.37.429
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1986LI05      Phys.Lett. 174B, 1 (1986)

X.-H.Li, T.Udagawa, T.Tamura

Breakup-Pickup and Breakup-Pickup-Fusion Contributions to the Continuum Spectra of (α, d) Reactions

NUCLEAR REACTIONS ⁵⁸Ni(α, d), E=160 MeV; calculated σ(θd, Ed); deduced breakup reaction mechanism.

doi: 10.1016/0370-2693(86)91116-0
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1984LI17      Phys.Rev. C30, 1349 (1984)

X.-H.Li, T.Udagawa, T.Tamura

Breakup-Fusion Calculations of Continuum Spectra of (h, p) and (h, d) Reactions at E(h) = 100 MeV

NUCLEAR REACTIONS ¹⁶⁵Ho(³He, p), (³He, d), E=100 MeV; calculated σ(θp, Ep), σ(θd, Ed); deduced breakup fusion, elastic breakup σ relative contribution, dominant process radial extension.

doi: 10.1103/PhysRevC.30.1349
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1984LI22      Phys.Rev. C30, 1895 (1984)

X.-H.Li, T.Udagawa, T.Tamura

Assessment of Approximations Made in Breakup-Fusion Descriptions

NUCLEAR REACTIONS ⁹³Nb(d, p), E=25.5 MeV; ⁵⁸Ni(α, t), E=160 MeV; ⁵⁸Ni(α, p), E=80, 160 MeV; calculated σ(Ep, θ); deduced approximation accuracies. Different breakup-fusion models.

doi: 10.1103/PhysRevC.30.1895
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1984UD01      Phys.Lett. 135B, 333 (1984)

T.Udagawa, X.-H.Li, T.Tamura

Breakup-Fusion Description of Nonequilibrium Protons from (α, p) Reactions

NUCLEAR REACTIONS ⁵⁸Ni(α, pX), E=80 MeV; ¹⁶⁵Ho(α, pX), E=110 MeV; calculated inclusive σ(θp, Ep); deduced reaction mechanism. Breakup-fusion description.

doi: 10.1016/0370-2693(84)90287-9
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1984UD03      Phys.Lett. 143B, 15 (1984)

T.Udagawa, X.-H.Li, T.Tamura

Breakup-Fusion Description of the (α, d) and (α, t) Reactions

NUCLEAR REACTIONS ⁵⁸Ni(α, d), (α, t), E=80, 160 MeV; calculated σ(Ed, θd), σ(Et, θt); deduced breakup-fusion role. DWBA analysis.

doi: 10.1016/0370-2693(84)90795-0
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1979CH42      Chin.J.Nucl.Phys. 1, 31 (1979)

Chu Yung-Tai, Fan Guo-Ying, Wu Zhong-Li, Feng En-Pu, Liang Guo-Zhao, Li Fa-Wei, Jiao Dun-Long, Li Xian-Hui, Guo Ying-Xiang, Xia Guo-Zhong, Su Ying-Quan, Xiao Qin-Pian

The Research of Scattering and Transfer Reaction of ¹²C with ¹²C

NUCLEAR REACTIONS ¹²C(¹²C, ¹²C), (¹²C, ¹²C'), (¹²C, ¹¹C), (¹²C, ¹³N), E=49, 60, 72.5 MeV; measured σ(θ). Optical model, zero-range DWBA analyses.

Note: The following list of authors and aliases matches the search parameter X.H.Li: , X.H.LI