6533b856fe1ef96bd12b256e

RESEARCH PRODUCT

Production cross section and decay study of Es243 and Md249

J. RubertPhilippos PapadakisPauli PeuraCatherine ScholeyM. AiriauRauno JulinJan SarénMikael SandzeliusJari PartanenT. GoigouxA. DrouartJanne PakarinenA. MarchixR.-d. HerzbergTuomas GrahnT. CalverleyM. ZielińskaB. SulignanoA. Lopez-martensUlrika JakobssonPanu RuotsalainenH. BadranPaul GreenleesPaivi NieminenCh. TheisenJuha SorriSakari JuutinenJuha UusitaloAndrej HerzanF. DecheryM. VandebrouckA. LightfootA. WardKalle AuranenDavid BoilleySanna StolzeMatti LeinoB. J. P. GallR. BriseletK. HauschildJoonas KonkiF. Defranchi BissoA. K. MistryPanu RahkilaDaniel Cox

subject

Nuclear reactionPhysicsRecoil010308 nuclear & particles physicsBranching fraction0103 physical sciencesCorrelation analysisAtomic physics010306 general physics01 natural sciences

description

In the study of the odd-$Z$, even-$N$ nuclei $^{243}$Es and $^{249}$Md, performed at the University of Jyv\"askyl\"a, the fusion-evaporation reactions $^{197}$Au($^{48}$Ca,2$n$)$^{243}$Es and $^{203}$Tl($^{48}$Ca,2$n$)$^{249}$Md have been used for the first time. Fusion-evaporation residues were selected and detected using the RITU gas-filled separator coupled with the focal-plane spectrometer GREAT. For $^{243}$Es, the recoil decay correlation analysis yielded a half-life of $24 \pm 3$s, and a maximum production cross section of $37 \pm 10$ nb. In the same way, a half-life of $26 \pm 1$ s, an $\alpha$ branching ratio of 75 $\pm$ 5%, and a maximum production cross section of 300 $\pm$ 80 nb were determined for $^{249}$Md. The decay properties of $^{245}$Es, the daughter of $^{249}$Md, were also measured: an $\alpha$ branching ratio of 54 $\pm$ 7% and a half-life of 65 $\pm$ 6 s. Experimental cross sections were compared to the results of calculations performed using the KEWPIE2 statistical fusion-evaporation code.

https://doi.org/10.1103/physrevc.99.024614