6533b823fe1ef96bd127f494

RESEARCH PRODUCT

Neutron-rich isotopesTi54−57

Karl-ludwig KratzF. PougheonA.c. MuellerS. GrévyM. LewitowiczW.-d. Schmidt-ottThomas RauscherD. Guillemaud-muellerA. OstrowskyP. MöllerM. RobinsonO. SorlinB. PfeifferT. DörflerT. MehrenM. G. Saint-laurentT. HildV. BorrelW. BöhmerR. Anne

subject

PhysicsNuclear and High Energy PhysicsDecay schemeIsotopes of germanium010308 nuclear & particles physics01 natural sciences7. Clean energyParticle identificationDouble beta decayIsotopes of protactinium0103 physical sciencesNeutronAtomic physics010306 general physicsNucleonRadioactive decay

description

The neutron-rich isotopes $^{54\mathrm{\ensuremath{-}}57}\mathrm{Ti}$ and $^{58\mathrm{\ensuremath{-}}60}\mathrm{Cr}$ are produced by fragmentation of a 64.5 MeV/nucleon $^{65}\mathrm{Cu}^{26+}$ beam in a 90 mg/${\mathrm{cm}}^{2}$ $^{9}\mathrm{Be}$ target. Following particle identification by energy loss and time of flight, the radioactive decay was observed by \ensuremath{\beta} singles and \ensuremath{\beta}\ensuremath{\gamma}-coincidence measurements. The results obtained for $^{58\mathrm{\ensuremath{-}}60}\mathrm{Cr}$ are compared to previous results, whereas the decay of the $^{54\mathrm{\ensuremath{-}}57}\mathrm{Ti}$ isotopes is studied here. \ensuremath{\gamma}-ray intensities and energies are estimated. The new experimental results are compared to quasi-random-phase-approximation predictions. \textcopyright{} 1996 The American Physical Society.

https://doi.org/10.1103/physrevc.54.2894