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NSR database version of April 27, 2024.

Search: Author = X.Pan

Found 30 matches.

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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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2022WE05      Eur.Phys.J. A 58, 222 (2022)

Y.Wei, C.Lan, Y.Ge, X.Yang, L.Jiang, Y.Nie, X.Li, J.Wang, G.Jiang, X.Ruan, X.Huang, X.Pan

Measurement of the half-life of ^95mTc and the ⁹⁶Ru(n, x)^95mTc reaction cross-section induced by D-T neutron with covariance analysis

RADIOACTIVITY ⁹⁵Tc(IT); measured decay products, Eγ, Iγ; deduced T_1/2. Comparison with available data.

NUCLEAR REACTIONS ⁹⁶Ru(n, X)⁹⁵Tc, E=13.85, 14.30, 14.72 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with the EXFOR database and TALYS-1.95 and EMPIRE-3.2.3 codes calculations. The K-400 neutron generator at the Chinese Academy of Engineering Physics (CAEP).

doi: 10.1140/epja/s10050-022-00879-4
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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
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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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2021ZH27      Nucl.Phys. A1011, 122201 (2021)

D.Zhang, Y.Zhao, M.Xu, X.Pan, Y.Wu

Rapidity window dependence of ridge correlations in the glasma

doi: 10.1016/j.nuclphysa.2021.122201
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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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2017CH56      Chin.Phys.C 41, 104103 (2017)

L.-Z.Chen, Y.-Y.Zhao, X.Pan, Z.-M.Li, Y.-F.Wu

High cumulants of conserved charges and their statistical uncertainties

doi: 10.1088/1674-1137/41/10/104103
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2015PA01      J.Phys.(London) G42, 15104 (2015)

X.Pan, M.Xu, Y.Wu

Generalized susceptibilities along the phase boundary of the three-dimensional, three-state Potts model

doi: 10.1088/0954-3899/42/1/015104
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2014PA03      Phys.Rev. C 89, 014904 (2014)

X.Pan, F.Zhang, Z.Li, L.Chen, M.Xu, Y.Wu

Statistical and dynamical parts of the cumulants of conserved charges in relativistic heavy ion collisions

doi: 10.1103/PhysRevC.89.014904
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2014XU05      Nucl.Phys. A927, 69 (2014)

M.Xu, X.Pan, Y.Wu

Inflection point as a characteristic of the QCD critical point

doi: 10.1016/j.nuclphysa.2014.03.019
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2013PA22      Nucl.Phys. A913, 206 (2013)

X.Pan, L.Chen, X.S.Chen, Y.Wu

High-order cumulants from the 3-dimensional O(1, 2, 4) spin models

doi: 10.1016/j.nuclphysa.2013.06.010
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1996GU10      J.Phys.(London) G22, 425 (1996)

M.W.Guidry, D.H.Feng, X.-W.Pan, C.-L.Wu

Solution of the Nuclear Shell Model by Symmetry-Dictated Truncation

doi: 10.1088/0954-3899/22/4/004
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1996PA03      Phys.Rev. C53, 715 (1996)

X.-W.Pan, J.-L.Ping, D.H.Feng, J.-Q.Chen, C.-L.Wu, M.W.Guidry

Fermion Dynamical Symmetry Model for the Even-Even and Even-Odd Nuclei in the Xe-Ba Region

NUCLEAR STRUCTURE ^{120,122,124,127,129,131,133,126,128,130,132}Xe, ^{131,133,135,137}Ba; calculated levels, B(λ), relative B(λ) in some cases. Fermion dynamical symmetry.

doi: 10.1103/PhysRevC.53.715
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1996PA28      Phys.Rep. 264, 311 (1996)

X.-W.Pan, T.T.S.Kuo, M.Vallieres, D.H.Feng, A.Novoselsky

Nuclear Shell-Model Calculations with Fundamental Nucleon-Nucleon Interactions

NUCLEAR STRUCTURE ¹⁸O, ¹⁸F, ¹⁸Ne; calculated levels, binding energies, single particle energies in some cases. Shell model, fundamental NN-interaction.

doi: 10.1016/0370-1573(95)00045-3
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1995SM07      Phys.Rev.Lett. 75, 3086 (1995)

B.H.Smith, X.-W.Pan, D.H.Feng, M.Guidry

Universality of Symmetry and Mixed-Symmetry Collective Nuclear States

NUCLEAR STRUCTURE ¹⁶⁸Er, ^160,162,164Dy, ^{154,156,158,160}Gd, ^{144,148,150,152,154}Sm, ^{142,146,148,150}Nd; analyzed B(λ), level energy ratio; deduced symmetry universality evidence. Fermion dynamical symmetry model.

doi: 10.1103/PhysRevLett.75.3086
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1995WA25      Phys.Rev. C52, 1792 (1995)

J.C.Walpe, B.F.Davis, S.Naguleswaran, W.Reviol, U.Garg, X.-W.Pan, D.H.Feng, J.X.Saladin

Lifetime Measurements in ¹²⁰Xe

NUCLEAR REACTIONS ¹⁰⁶Pd(¹⁸O, 4n), E=70 MeV; measured Eγ, Iγ, recoil distance method spectra. ¹²⁰Xe levels deduced T_1/2, B(λ), quadrupole moments.

doi: 10.1103/PhysRevC.52.1792
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1995WU03      Phys.Rev. C51, R1086 (1995)

C.-L.Wu, D.H.Feng, M.W.Guidry, H.-T.Chen, X.-W.Pan

Single-Particle Nondegeneracy and SU(3) Fermion Dynamical Symmetry

doi: 10.1103/PhysRevC.51.R1086
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1994FE08      Nucl.Phys. A570, 77c (1994)

D.H.Feng, X.-W.Pan

Dynamical Symmetry in Heavy Nuclei and Complementarity of Bosons and Fermions

NUCLEAR STRUCTURE ¹⁹⁶Pt; compiled, reviewed level predictions; deduced models complementarity features. Interacting boson, dynamical supersymmetry models, other nuclei discussed.

doi: 10.1016/0375-9474(94)90271-2
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1994PA08      Nucl.Phys. A570, 273c (1994)

X.-W.Pan, D.H.Feng, J.-Q.Chen, M.W.Guidry

The Mottelson-Valatin Effect in the SO(5) Scheme

NUCLEAR STRUCTURE ¹²⁸Xe, ¹³²Ba; calculated SO(5) level spectra; deduced τ-bunching, SO(6) symmetry properties violation in γ-soft nuclei.

doi: 10.1016/0375-9474(94)90292-5
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1994PA09      Phys.Rev. C49, 2493 (1994)

X.-W.Pan, D.H.Feng, J.-Q.Chen, M.W.Guidry

τ Compression in the SO(5) Scheme

NUCLEAR STRUCTURE ¹³²Ba; calculated levels. ¹²⁸Xe; calculated levels, B(λ); deduced τ-compression features, origin. SO(6)+ pairing model.

doi: 10.1103/PhysRevC.49.2493
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1994PA24      Phys.Rev. C50, 818 (1994)

X.-W.Pan, D.H.Feng

Normal and Exotic Collective States in the Fermion Dynamical Symmetry Model

NUCLEAR STRUCTURE ¹³⁴Ba; calculated levels, B(λ); deduced normal, exotic states unification, n-p quadrupole interaction role. Fermion dynamical symmetry model.

doi: 10.1103/PhysRevC.50.818
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1994PA38      Phys.Lett. 336B, 285 (1994)

X.-W.Pan, D.H.Feng

A Revisit of SO(6) Dynamical Symmetry in Nuclear Structure

NUCLEAR STRUCTURE ^126,130Xe; analyzed γ-branching ratios. ¹²⁸Xe, ¹⁹⁶Pt; analyzed γ-branching ratios, B(λ) data; deduced similarity to SO(7), SO(6) symmetries transitional nuclei. Fermion dynamical symmetry model.

doi: 10.1016/0370-2693(94)90533-9
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1993FE07      Phys.Rev. C48, R1488 (1993)

D.H.Feng, M.W.Guidry, X.-W.Pan, C.-L.Wu, I.Zlatev

Effective Fermion SO(6) Dynamical Symmetry in the Platinum Nuclei

NUCLEAR STRUCTURE ¹⁹⁶Pt; calculated levels; deduced fermion SO(6) dynamical symmetry evidence.

doi: 10.1103/PhysRevC.48.R1488
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1992PA18      Phys.Lett. 287B, 1 (1992)

X.-W.Pan, T.Otsuka, J.-Q.Chen, A.Arima

A Pairing Effect in γ-Soft Nuclei

NUCLEAR STRUCTURE ^126,128,130Xe; calculated levels; deduced (γ)-soft nuclei level regularities features. Interacting boson model, O(6) limit.

doi: 10.1016/0370-2693(92)91866-8
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1990OT03      Phys.Lett. 247B, 191 (1990)

T.Otsuka, X.-W.Pan, A.Arima

Saturation of E2 Transition and Pauli Factors in the Interacting Boson Model

NUCLEAR STRUCTURE ^{120,122,124,126,128,130,132,134}Xe, ^{120,122,124,126,128,130,132,134,136}Ba; calculated levels, B(E2). Interacting boson model, other isotopes included.

doi: 10.1016/0370-2693(90)90879-B
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Note: The following list of authors and aliases matches the search parameter X.Pan: , X.W.PAN