6533b830fe1ef96bd1297aaa
RESEARCH PRODUCT
Production cross section and decay study of $^{243}$Es and $^{249}$Md
R. BriseletCh. TheisenM. VandebrouckA. MarchixM. AiriauK. AuranenH. BadranD. BoilleyT. CalverleyD. CoxF. DécheryF. Defranchi BissoA. DrouartB. GallT. GoigouxT. GrahnP.t. GreenleesK. HauschildA. HerzanR.d. HerzbergU. JakobssonR. JulinS. JuutinenJ. KonkiM. LeinoA. LightfootA. Lopez-martensA. MistryP. NieminenJ. PakarinenP. PapadakisJ. PartanenP. PeuraP. RahkilaJ. RubertP. RuotsalainenM. SandzeliusJ. SarenC. ScholeyJ. SorriS. StolzeB. SulignanoJ. UusitaloA. WardM. Zielińskasubject
ydinreaktiotalpha decayNuclear ReactionsFOS: Physical scienceslow and intermediate energy heavy-ion reactionsNuclear Experiment (nucl-ex)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experimentdescription
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.
year | journal | country | edition | language |
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2019-01-01 |