6533b872fe1ef96bd12d37ea
RESEARCH PRODUCT
Deformation of the proton emitterCs113from electromagnetic transition and proton-emission rates
M. SmolenCatherine ScholeyJan SarénMikael SandzeliusJoonas KonkiO. NefodovRauno JulinThomas BraunrothSanna StolzePhilippos PapadakisD. M. CullenA. GirkaD. HodgePaul GreenleesTuomas GrahnPanu RuotsalainenJuha SorriJuha UusitaloMichael TaylorM. J. MallaburnJari PartanenJanne PakarinenJ. F. SmithH. BadranL. CapponiG. G. O'neillB. S. Nara SinghPanu RahkilaL. S. FerreiraEnrico Maglionesubject
PhysicsProton010308 nuclear & particles physicsDeformation (meteorology)Transition rate matrix01 natural sciencesNuclear magnetic resonance0103 physical sciencesQuadrupoleQuasiparticleAtomic physicsProton emission010306 general physicsWave functionExcitationdescription
The lifetime of the $(11/{2}^{+})$ state in the band above the proton-emitting $(3/{2}^{+})$ state in $^{113}\mathrm{Cs}$ has been measured to be $\ensuremath{\tau}=24(6)$ ps from a recoil-decay-tagged differential-plunger experiment. The measured lifetime was used to deduce the deformation of the states using wave functions from a nonadiabatic quasiparticle model to independently calculate both proton-emission and electromagnetic $\ensuremath{\gamma}$-ray transition rates as a function of deformation. The only quadrupole deformation, which was able to reproduce the experimental excitation energies of the states, the electromagnetic decay rate of the $(11/{2}^{+})$ state and the proton-emission rate of the $(3/{2}^{+})$ state, was found to be ${\ensuremath{\beta}}_{2}=0.22(6)$. This deformation is in agreement with the earlier proton emission studies which concluded that $^{113}\mathrm{Cs}$ was best described as a deformed proton emitter, however, it is now more firmly supported by the present measurement of the electromagnetic transition rate.
year | journal | country | edition | language |
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2016-09-21 | Physical Review C |