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RESEARCH PRODUCT
Spectroscopy along Flerovium Decay Chains: Discovery ofDs280and an Excited State inCn282
J. LoukoA. Såmark-rothH. M. AlbersMichael BlockJ. M. GatesS. GötzDirk RudolphDaniel CoxJ. L. EgidoE. ParrM. AlbertssonH. BrandD. A. ShaughnessyR-d HerzbergPhilippos PapadakisI. KojouharovJ. KrierNorbert TrautmannB. G. CarlssonIngemar RagnarssonC.-c. MeyerJ. KhuyagbaatarCh. E. DüllmannM. GötzR. CantemirF. GiacoppoC. MokryBirgit KindlerJörg RunkeJ. HeeryL. LensN. KurzU. ForsbergJ. EberthD. S. JudsonY. HrabarPetra Thörle-pospiechJ. L. PoreSven ÅBergH. SchaffnerMatthias SchädelT. CalverleyA. K. MistryBettina LommelEgon JägerPavel GolubevJ. LjungbergAlexander YakushevJ. V. KratzClaes FahlanderR. M. ClarkB. SchaustenLuis SarmientoJuha Uusitalosubject
PhysicsGeneral Physics and Astronomychemistry.chemical_elementIsotopes of flerovium7. Clean energy01 natural sciencesIsland of stabilityFleroviumchemistryExcited state0103 physical sciencesDecay chainAlpha decayAtomic numberAtomic physics010306 general physicsSpectroscopydescription
A nuclear spectroscopy experiment was conducted to study α-decay chains stemming from isotopes of flerovium (element Z=114). An upgraded TASISpec decay station was placed behind the gas-filled separator TASCA at the GSI Helmholtzzentrum fur Schwerionenforschung in Darmstadt, Germany. The fusion-evaporation reactions ^{48}Ca+^{242}Pu and ^{48}Ca+^{244}Pu provided a total of 32 flerovium-candidate decay chains, of which two and eleven were firmly assigned to ^{286}Fl and ^{288}Fl, respectively. A prompt coincidence between a 9.60(1)-MeV α particle event and a 0.36(1)-MeV conversion electron marked the first observation of an excited state in an even-even isotope of the heaviest man-made elements, namely ^{282}Cn. Spectroscopy of ^{288}Fl decay chains fixed Q_{α}=10.06(1) MeV. In one case, a Q_{α}=9.46(1)-MeV decay from ^{284}Cn into ^{280}Ds was observed, with ^{280}Ds fissioning after only 518 μs. The impact of these findings, aggregated with existing data on decay chains of ^{286,288}Fl, on the size of an anticipated shell gap at proton number Z=114 is discussed in light of predictions from two beyond-mean-field calculations, which take into account triaxial deformation.
year | journal | country | edition | language |
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2021-01-22 | Physical Review Letters |