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NSR database version of April 27, 2024.

Search: Author = Y.T.Zou

Found 13 matches.

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2024ZO01      J.Phys.(London) G51, 045103 (2024)

Y.-T.Zou, J.-H.Cheng, Y.-Y.Xu, Q.Xiao, S.-M.Liu, F.-Q.Shao, T.-P.Yu

Laser-assisted two-proton radioactivity

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); calculated the two-proton radioactivity assisted by an ultra-intense laser field within a deformed one-parameter model (OPM); deduced the lasers characterized by shorter wavelengths and higher intensities exert a more significant influence on the rate of the average change in pulse duration, T_1/2.

doi: 10.1088/1361-6471/ad2691
Citations: PlumX Metrics

2023XI06      J.Phys.(London) G50, 085102 (2023)

Q.Xiao, J.-H.Cheng, B.-L.Wang, Y.-Y.Xu, Y.-T.Zou, T.-P.Yu

Half-lives for proton emission and α decay within the deformed Gamow-like model

RADIOACTIVITY ¹⁰⁹I, ^112,113Cs, ¹¹⁷La, ¹²¹Pr, ¹³¹Eu, ¹³⁵Tb, ^140,141Ho, ^{144,145,146,147}Tm, ^150,151Lu, ^155,156,157Ta, ^159,160,161Re, ^{164,165,166,167}Ir, ^170,171Au, ^176,177Tl, ¹⁸⁵Bi, ¹¹¹Cs, ¹²⁷Pm, ¹³⁷Tb(p), ^106,108Te, ^108,110,112Xe, ¹¹⁴Ba, ¹⁴⁴Nd, ^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, ^{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}Ra, ^{214,216,218,220,222,224,226}Ra, ^{210,212,214,216,218,220,222,224,226,228,230,232}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}Cm, ^{238,240,242,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^252,254,256No, ^256,258Rf, ^266,268,270Hs, ²⁷⁰Ds, ²⁸²Ds, ²⁸⁶Cn, ^286,288,290Fl, ^290,292Lv, ²⁹⁴Og, ¹⁰⁵Te, ¹⁰⁹Te, ¹⁰⁹Xe, ¹⁴⁷Sm, ^149,151Gd, ^151,153Dy, ^153,155Er, ¹⁵⁵Yb, ^157,159Hf, ^161,163W, ¹⁶⁷W, ¹⁶¹Os, ^{167,169,171,173}Os, ^{171,173,175,177,179,181,183,185}Pt, ^{175,177,179,181,183,185}Hg, ^{183,185,187,189}Pb, ^{187,189,191,193,195,197,199,201,203,205,207,209,211,213,215,217,219}Po, ^{193,195,197,199}Rn, ^{203,205,207,209,211,213,215,217,219,221}Rn, ^{201,203,205,207,209,211,213,215,217,219,221,223}Ra, ^{211,213,215,217,219,221,223,225,227}Th, ^{221,223,225,227,229,231,233,235}U, ^{229,231,233,235,237,239,241}Pu, ²³³Cm, ^{239,241,243,245,247}Cm, ²³⁷Cf, ^{245,247,249,251,253}Cf, ^{249,251,253,255,257}Fm, ^255,257,259No, ²⁵⁷Rf, ²⁶¹Rf, ²⁶¹Sg, ²⁶⁵Hs, ¹⁰⁹I, ¹¹³I, ¹⁴⁵Pm, ¹⁴⁷Eu, ¹⁵¹Tb, ^151,153Ho, ^155,157Tm, ¹⁵⁵Lu, ^157,159Ta, ^163,165Re, ^{167,169,171,173,175,177}Ir, ^{173,175,177,179,181,183,185}Au, ^177,179,181Tl, ^{187,189,191,193,195}Bi, ^{193,195,197,199,201,203,205,207,209,211,213,215,217,219,221,223,225,227}Ac, ^{211,213,215,217,219,221,223,225,227,229,231}Pa, ²¹⁹Np, ^{223,225,227,229,231,233,235,237}Np, ²²⁹Am, ²³⁵Am, ^239,241,243Am, ^{243,245,247,249}Bk, ²⁴⁷Es, ^251,253Es, ^249,251Md, ^255,257Md, ^253,255Lr, ²⁵⁹Lr, ²⁵⁹Db, ²⁶¹Bh, ^110,112I, ¹¹⁴Cs, ^152,154Ho, ^154,156Tm, ¹⁵⁸Lu, ¹⁵⁸Ta, ¹⁶²Ta, ^160,162Re, ¹⁶⁸Re, ^166,168Ir, ^172,174Ir, ¹⁷⁰Au, ¹⁷⁶Au, ¹⁸⁰Tl, ¹⁸⁶Bi, ^192,194Bi, ^212,214Bi, ¹⁹²At, ^{200,202,204,206,208,210,212,214,216,218}At, ²⁰⁰Fr, ^{204,206,208,210,212,214,216,218,220}Fr, ^{216,218,220,222,224,226}Ac, ²¹²Pa, ²²⁴Pa, ^228,230Pa, ²³⁶Np, ²³⁶Am, ²⁴⁴Bk, ²⁴⁸Es, ²⁵⁸Md, ²⁷²Rg(α); calculated T_1/2 with the deformed Gamow-like model, which introduces the effects of nucleus deformation; deduced the deformed model follows the Geiger-Nuttall law. Comparison with available data.

doi: 10.1088/1361-6471/acdfeb
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
Citations: PlumX Metrics

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

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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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
Citations: PlumX Metrics

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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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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