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NSR database version of May 3, 2024.

Search: Author = B.L.Wang

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2024WA15      Phys.Lett. B 850, 138515 (2024)

B.-L.Wang, L.-J.Wang

First-forbidden transition of nuclear β decay by projected shell model

RADIOACTIVITY ⁸⁹Br, ^90,92,93,95Rb, ⁹¹Kr, ^94,96,97,98Y, ⁹⁵Sr, ¹³³Sn, ¹³⁵Te, ¹³⁵Sb, ^136,137I, ¹⁴²Cs, ⁸⁶Br, ⁸⁷Se, ¹³⁶Te, ¹³⁸I, ¹⁴⁰Xe, ^140,143Cs, ⁸⁸Rb, ¹³⁹Xe(β^-); calculated dominant first-forbidden transitions for the reactor anti-neutrino spectral shoulder, log ft, the coefficients in the shape factor, parameters. Comparison with available data.

doi: 10.1016/j.physletb.2024.138515
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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
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2022WA42      Phys.Rev. C 106, 054320 (2022)

B.-L.Wang, F.Gao, L.-J.Wang, Y.Sun

Effective and efficient algorithm for the Wigner rotation matrix at high angular momenta

NUCLEAR STRUCTURE ¹⁵⁶Dy; calculated levels, energies of the yrast band, high-spin states. Method for evaluation of the Wigner d function based on the Jacobi polynomials. Comparison to other theoretical methods.

doi: 10.1103/PhysRevC.106.054320
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1997WA22      Chin.Phys.Lett. 14, 503 (1997)

B.-L.Wang

Systematics of β and γ Parameters of O(6)-Like Nuclei in the Interacting Boson Model

NUCLEAR STRUCTURE ^{120,122,124,126,128,130,132}Xe, ^{124,126,128,130,132,134}Ba, ^{126,128,130,132,134,136}Ce; calculated quadrupole moments, reduced transition probabilities; deduced proton, neutron boson numbers dependence. Interacting boson model, comparision with collective model.

1996ZH29      Chin.Phys.Lett. 13, 809 (1996)

Q.-Y.Zhang, M.Feng, X.-L.Chen, B.-L.Wang

Spectra of ^230-238U by 1/N Expansion with Consistent Q Framework

NUCLEAR STRUCTURE ^{230,232,234,236,238}U; calculated levels, B(E2). Interacting boson model, consistent Q framework, 1/N expansion technique.

doi: 10.1088/0256-307X/13/11/003
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