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NSR database version of May 1, 2024.

Search: Author = P.Guo

Found 12 matches.

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2023DU07      Chin.Phys.C 47, 074108 (2023)

X.-K.Du, P.Guo, X.-H.Wu, S.-Q.Zhang

Examination of machine learning for assessing physical effects: Learning the relativistic continuum mass table with kernel ridge regression

NUCLEAR STRUCTURE N<300; analyzed available data; deduced empirical proton-neutron interactions, odd-even mass differences, one- and two-neutron separation and binding energies extracted from the nuclear mass table obtained by the relativistic continuum Hartree-Bogoliubov theory. Comparison with available data.

doi: 10.1088/1674-1137/acc791
Citations: PlumX Metrics


2023GU12      Phys.Rev. C 108, 014319 (2023)

P.Guo, C.Pan, Y.C.Zhao, X.K.Du, S.Q.Zhang

Prolate-shape dominance in atomic nuclei within the deformed relativistic Hartree-Bogoliubov theory in continuum

NUCLEAR STRUCTURE 134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,178Te, 136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,178,180Xe, 138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,178,180,182Ba; calculated quadrupole deformation, potential-energy curves, single-neutron energies, pairing correlations. Calculations with deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc).

doi: 10.1103/PhysRevC.108.014319
Citations: PlumX Metrics


2022GU06      J.Phys.(London) G49, 055104 (2022)

P.Guo, B.Long

Nuclear reactions in artificial traps

doi: 10.1088/1361-6471/ac59d5
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2021GU17      Phys.Rev. C 103, 064611 (2021)

P.Guo

Coulomb corrections to two-particle interactions in artificial traps

doi: 10.1103/PhysRevC.103.064611
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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, 173,171,169,167Ir, 169,167,163Re, 177Tl, 159Ta, 155Lu, 153,151Ho, 149Tb, 153Tm, 185Hg, 185,187,189,191Pb, 195,197,199,201,203Po, 195,197,203Rn, 203,209Ra, 187,189,191,193,195,197Bi, 191,193,197At, 201Fr(α); calculated T1/2 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,153,153mHo, 153,155Er, 153,153m,155Tm, 155,157Yb, 155,155m,157mLu, 157Hf, 159,159mTa, 159,161,163W, 159m,161m,163,163m,165m,167m,169mRe, 161,163,165,167,169Os, 165m,167,167m,169,169m,171m,173m,175,177Ir, 167,171,173,175,177,179,181,183Pt, 173,175,177,179,181,183,185Au, 173,177,179,183,185Hg, 177,183,187mTl, 179,185,185m,187,187m,189,191mPb, 185m,187m,189m,191m,193m,195m,209,211,213Bi, 187,189,195,195m,197,199,201,203,205,207,211,213,215,217Po, 191m,193m,197,199,201,203,205,207,209,211,213,215,217At, 193,195,195m,197,203,205,207,209,213,215,217,219,221,223Rn, 199,201,203,205,207,209,211,213,215,219,221,223Fr, 203,207,209,211,213,215,217,219,221,223Ra, 207,211,215,217,219,221,223,225,227Ac, 215,217,219,221,223,225,227,229,231Th, 213,215,217,217m,219,221,223,227,229,231Pa, 219,225,227,229,231,235U, 225,227,229,231,235,237,239Np, 229,231,233,235,237,241Pu, 233,235,237,239,241,243Am, 233,237,239,243,245,247Cm, 243,245,247,249Bk, 247,249,255Cf, 243,251,253Es, 243,247,247m,251,255,257Fm, 247,247m,251,253,255,257Md, 251No, 253,255mLr, 255m,257m,261,263Rf, 257Db, 259m,261,263,265Sg, 265,267Hs, 267,269,271,271m,273,273m,277,281Ds, 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 105,106,107,108,109,110Te, 108,109,110,111,112,113I, 109,110,111,112,113,115Xe, 112,114Cs, 114Ba, 148Eu, 152,154Ho, 154,156Tm, 156Lu, 158Ta, 160,162,164,166Re, 166,168,170,172,174Ir, 170,186Au, 180,186Tl, 190,192,194,196,212,214Bi, 192,194,198,200,202,204,206,208,210,212,214,216,218At, 202,204,208,210,212,214,216,218,220Fr, 212,220,224,228Pa, 214,216,218,220,222,226Ac, 232,236Np, 236,238,242Am, 246,248Bk, 244,246,248,252,254Es, 246,248,250,256,258,260Md, 254,258,260Lr, 272,274,278,280,282Rg, 258,260,262,268Db, 260,264,266,270,272,274Bh, 268,270,274,276,278Mt, 278,282,284,286Nh, 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, 156,158,160,162Hf, 158,160,162,164,166,168W, 166,168,170,172,174,186Os, 166,168,170,172,174,176,178,180,182,184,186,188,190Pt, 172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194,210Pb, 190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 206,208,210,212,214,216,218,220,222,224,226Ra, 214,216,218,220,222,224,226,228,230,232Th, 224,226,228,230,232,234,236,238U, 228,230,232,234,236,238,240,242,244Pu, 238,240,242,244,246,248,250Cm, 240,242,244,246,248,250,252,254Cf, 248,250,252,254,256Fm, 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,155Tm, 155,157Yb, 155,155m,156m,157mLu, 157Hf, 158,158m,159,159mTa, 159,161,163W, 159m,161m,162m,162m,163,163m,165mRe, 161,163,165,167,169Os, 165m,166,166m,167,167m,169,169mIr, 167,171,173Pt, 170,170m,173,175,177Au, 177,183Tl, 179,183Hg, 185m,187m,191mPb, 187m,189m,191m,193m,195mBi, 195,195m,197,199,201,205,207Po, 197,198,199,200,201,202,203,204,205,206,207,208,209,211,214,214m,218At, 203,207,209,215,217Rn, 204,205,207,208,209,211,213,215,216,216m,217,218,219Fr, 209,211,217Ra, 213,215,217,219,220,221Pa, 211,213,217,218,219Ac, 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 NpNn and NpNnI, 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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2015GU21      Eur.Phys.J. A 51, 135 (2015)

P.Guo, I.V.Danilkin, A.P.Szczepaniak

Dispersive approaches for three-particle final state interaction

doi: 10.1140/epja/i2015-15135-7
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2012GO08      Phys.Rev. C 86, 015205 (2012)

M.Gorchtein, P.Guo, A.P.Szczepaniak

Form factors of pseudoscalar mesons

doi: 10.1103/PhysRevC.86.015205
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2007JI13      Eur.Phys.J. A 34, 41 (2007)

C.-S.Jia, P.Guo, Y.-F.Diao, L.-Z.Yi, X.-J.Xie

Solutions of Dirac equations with the Poschl-Teller potential

doi: 10.1140/epja/i2007-10486-2
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