J.Phys.:Conf.Ser. 205, 012020 (2010)

D.Bonatsos, I.Boztosun, I.Inci

A long sought result: Closed analytical solutions of the Bohr Hamiltonian with the Morse potential

NUCLEAR STRUCTURE ^{98,100,102,104}Ru, ^{102,104,106,108,110,112,114,116}Pd, ^{106,108,110,112,114,116,118,120}Cd, ^{118,120,122,124,126,128,130,132,134}Xe, ^{130,132,134,136,142}Ba, ^134,136,138Ce, ^140,148,150Nd, ^{140,142,152,154}Sm, ^{142,144,152,154,156,158,160,162}Gd, ^{158,160,162,164,166}Dy, ^{156,160,162,164,166,168,170}Er, ^{164,166,168,170,172,174,176,178}Yb, ^{168,170,172,174,176,178,180}Hf, ^{176,178,180,182,184,186}W, ^{178,180,184,186,188}Os, ^{186,188,190,192,194,196,198,200}Pt, ²²⁸Ra, ^228,230,232Th, ^{232,234,236,238}U, ^{238,240,242,248}Cm, ²⁵⁰Cf; calculated low-lying 0⁺, 2⁺, 4⁺ states, β and γ bandheads, deformation using Bohr Hamiltonian with Morse potential; deduced Morse potential shapes. Compared with data.

doi: 10.1088/1742-6596/205/1/012020