The decay-out process of the yrast superdeformed band in Cu-59 has been investigated. The firm determination of spin, parity, excitation energy, and configuration of the states involved in this process constitutes a unique situation for a detailed understanding of the decay-out mechanism. A theoretical model is introduced that includes a residual interaction and tunneling matrix element between bands, calculated in the configuration-dependent cranked Nilsson-Strutinsky model. This interaction causes the decay to occur via a small number of observed doorway states
Different treatments of the decay-out of superdeformed bands are reviewed, focusing on the role of t...
Exact and approximate quantum numbers of the cranked Nilsson-Strutinsky (CNS) formalism are exploite...
High-spin states in $\chem{^{59}Cu}$ were populated using the fusion-evaporation reaction $\chem{^{2...
This contribution reports on the decay-out of the yrast superdeformed band in 59Cu. It decays by mul...
An extensive high-spin level scheme has been established in 59Cu using a heavy-ion fusion evaporatio...
High-spin states in the mass A~60 region were populated using the state-of-art gamma-ray spectromete...
High-spin states in Cu-59 were populated using the fusion-evaporation reactions Si-28+ Ca-40 at a be...
High-spin states in Cu-59 were populated using the fusion-evaporation reaction Si-28 + Ca-40 at a be...
Five prompt proton decay lines have been identified between deformed states in Cu-59 and three spher...
Some consequences of chaos in the nucleus are discussed. The decay-out from superdeformed band occur...
A systematic study of the depopulation of superdeformed rotational bands in neutron-deficient $A\app...
Exact and approximate quantum numbers of the cranked Nilsson-Strutinsky (CNS) formalism are exploite...
The individual lifetimes of three low-lying states in the proton-decaying well-deformed rotational b...
An excited minimum, or false vacuum, gives rise to a highly elongated superdeformed (SD) nucleus. A ...
One of the major challenges in the study of superdeformation is to directly connect the large number...
Different treatments of the decay-out of superdeformed bands are reviewed, focusing on the role of t...
Exact and approximate quantum numbers of the cranked Nilsson-Strutinsky (CNS) formalism are exploite...
High-spin states in $\chem{^{59}Cu}$ were populated using the fusion-evaporation reaction $\chem{^{2...
This contribution reports on the decay-out of the yrast superdeformed band in 59Cu. It decays by mul...
An extensive high-spin level scheme has been established in 59Cu using a heavy-ion fusion evaporatio...
High-spin states in the mass A~60 region were populated using the state-of-art gamma-ray spectromete...
High-spin states in Cu-59 were populated using the fusion-evaporation reactions Si-28+ Ca-40 at a be...
High-spin states in Cu-59 were populated using the fusion-evaporation reaction Si-28 + Ca-40 at a be...
Five prompt proton decay lines have been identified between deformed states in Cu-59 and three spher...
Some consequences of chaos in the nucleus are discussed. The decay-out from superdeformed band occur...
A systematic study of the depopulation of superdeformed rotational bands in neutron-deficient $A\app...
Exact and approximate quantum numbers of the cranked Nilsson-Strutinsky (CNS) formalism are exploite...
The individual lifetimes of three low-lying states in the proton-decaying well-deformed rotational b...
An excited minimum, or false vacuum, gives rise to a highly elongated superdeformed (SD) nucleus. A ...
One of the major challenges in the study of superdeformation is to directly connect the large number...
Different treatments of the decay-out of superdeformed bands are reviewed, focusing on the role of t...
Exact and approximate quantum numbers of the cranked Nilsson-Strutinsky (CNS) formalism are exploite...
High-spin states in $\chem{^{59}Cu}$ were populated using the fusion-evaporation reaction $\chem{^{2...