6533b7dcfe1ef96bd1271d2d

RESEARCH PRODUCT

Octupole correlations in the structure of02+bands in theN=88nuclei150Sm and152Gd

Catherine ScholeyP. VymersD. CurienPaul GreenleesS. M. MullinsA. MinkovaA. KorichiL. L. RiedingerL. BiancoJ. HirvonenD. M. CullenE. A. LawrieS. N. T. MajolaJános TimárP. E. GarrettK. JuhászPanu RuotsalainenPaivi NieminenSteffen KetelhutJan SarénJuha UusitaloRauno JulinP. MainePanu RahkilaS. P. BvumbiJ. KauSanna StolzeMatti LeinoJ.f. Sharpey-schaferUlrika JakobssonJ. J. LawrieRobert BarkThandinkosi E. MadibaF. KomatiPeter M. JonesJuha SorriB. M. NyakóN.j. NcapayiSakari JuutinenPauli Peura

subject

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsExcited state0103 physical sciencesStructure (category theory)Parity (physics)State (functional analysis)Atomic physics010306 general physicsGround stateSpectroscopy01 natural sciences

description

Knowledge of the exact microscopic structure of the 0${}_{1}$${}^{+}$ ground state and first excited 0${}_{2}$${}^{+}$ state in ${}^{150}$Sm is required to understand the branching of double \ensuremath{\beta} decay to these states from ${}^{150}$Nd. The detailed spectroscopy of ${}^{150}$Sm and ${}^{152}$Gd has been studied using (\ensuremath{\alpha},xn) reactions and the \ensuremath{\gamma}-ray arrays AFRODITE and JUROGAM II. Consistently strong $E$1 transitions are observed between the excited ${K}^{\ensuremath{\pi}}$ $=$ 0${}_{2}$${}^{+}$ bands and the lowest negative parity bands in both nuclei. These results are discussed in terms of the possible permanent octupole deformation in the first excited ${K}^{\ensuremath{\pi}}$ $=$ 0${}_{2}$${}^{+}$ band and also in terms of the ``tidal wave'' model of Frauendorf.

https://doi.org/10.1103/physrevc.87.044333