Phys.Rev. C 85, 044324 (2012)

A.Coban, O.Bayrak, A.Soylu, I.Boztosun

Effect of nuclear deformation on α-decay half-lives

RADIOACTIVITY ^{106,107,108,109}Te, ¹¹³I, ^112,113Xe, ¹¹⁴Ba, ¹⁴⁴Nd, ¹⁴⁵Pm, ^146,147Sm, ^147,148Eu, ^148,151,152Gd, ^151,152Dy, ^152,154Ho, ^152,153Er, ^153,155Tm, ^154,155Yb, ^157,158Hf, ^160,162W, ^160,162Re, ^162,166Os, ^166,169Ir, ^{168,170,172,174,176,178,180,182,184,186,188,190,192,194}Pt, ^170,183Au, ^174,177Hg, ^177,179Tl, ^186,188Pb, ^190,192Po, ^196,198At, ^198,201Rn, ^201,203Fr, ^205,206Ra, ^206,208Ac, ^213,216Th, ^217,219Pa, ^226,228U, ^232,234Pu, ^238,246Cm, ^240,245Cf, ^251,253Es, ^248,250Fm, ^252,254No, ²⁶⁰Sg, ²⁶¹Bh, ^{269,270,271,273}Ds, ²⁶⁸Mt, ^{264,265,266,267,269}Hs, ^{264,265,266,267}Bh, ^{261,263,265,266}Sg (α); calculated Q(α), T_1/2. Wentzel-Kramers-Brillouin (WKB) method and Bohr-Sommerfeld quantization condition. Deformed phenomenological Wood-Saxon form and deformed Coulomb potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.044324