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Low-spin states in $^{80}$Ge populated in the $\beta$ decay of the $^{80}$Ga $3^-$ isomer

The structure of  $^{80}$Ge has been investigated at the ISOLDE facility at CERN. A previous study reported for the first time a low-lying $0^+_2$ intruder state at 639 keV, based on the coincidence with a previously unobserved 1764-keV $γ$ ray, and suggested it as evidence for shape coexistence in...

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Detalles Bibliográficos
Autores principales: Sekal, S, Fraile, L M, Lică, R, Borge, M J G, Walters, W B, Aprahamian, A, Benchouk, C, Bernards, C, Briz, J A, Bucher, B, Chiara, C J, Dlouhý, Z, Gheorghe, I, Ghiţă, D G, Hoff, P, Jolie, J, Köster, U, Kurcewicz, W, Mach, H, Mărginean, N, Mărginean, R, Meliani, Z, Olaizola, B, Paziy, V, Régis, J M, Rudigier, M, Sava, T, Simpson, G S, Stănoiu, M, Stroe, L
Lenguaje:eng
Publicado: 2021
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevC.104.024317
http://cds.cern.ch/record/2778805
Descripción
Sumario:The structure of  $^{80}$Ge has been investigated at the ISOLDE facility at CERN. A previous study reported for the first time a low-lying $0^+_2$ intruder state at 639 keV, based on the coincidence with a previously unobserved 1764-keV $γ$ ray, and suggested it as evidence for shape coexistence in $^{80}$Ge. We used the $\beta$ decay from the $3^-$ 22.4-keV state in $^{80}$Ga to enhance the population of low-spin states in $^{80}$Ge, including any excited $0^+$ level, and $\gamma \gamma$ coincidences to investigate it. We observed a 1764-keV $\gamma$ ray in coincidence with strong transitions in $^{80}$Ge, thus not feeding the proposed 639-keV $0^+_2$. No connecting transitions from previously known levels to the 639-keV and 2403-keV $2^+_3$ states could be established either. Shell-model calculations for Ge isotopes and $N=48$ isotones were performed. They succeed to explain most of the experimental levels, but fail to reproduce the presence of a $0^+_2$ state below $≈1200$ keV in $^{80}$Ge. Our experimental findings and shell-model calculations are difficult to reconcile with a very low-lying $0^+_2$ state in  $^{80}$Ge.