Phys.Rev. C 86, 044316 (2012)

A.Bhagwat, X.Vinas, M.Centelles, P.Schuck, R.Wyss

Microscopic-macroscopic approach for binding energies with the Wigner-Kirkwood method. II. Deformed nuclei

NUCLEAR STRUCTURE ⁶³Ge, ⁶⁵As, ⁶⁷Se, ^{71,80,82,84,86,88,90,92,94,96,98,100,102,104}Kr, ^{76,78,80,82,84,86,88,90,92,94,96,98,100,102}Sr, ^{84,86,88,90,92,94,96,98,100,102,104,106,108}Zr, ^{86,88,90,92,94,96,98,100,102,104,106,108,110}Mo, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn, ^{140,142,144,146,148,150,152,154,156,158,160,162}Gd, ^{186,188,190,192,194,196,198,200,202,204,206,208,210,212,214}Po; calculated S_2n, β₂, S_p, binding energy using Microscopic-macroscopic model with Wigner-Kirkwood expansion. Comparison with experimental data. Z, N>7; deduced difference between the calculated and the corresponding experimental binding energies for 561 nuclides.

RADIOACTIVITY ^279,280Rg, ^282,283Nh, ^287,288,289Fl, ^287,288Mc, ^291,292,293Lv, ²⁹⁴Og(α); calculated Q values and half-lives. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.044316