256RF 260SG A DECAY (4.95 MS) 2009HE20,1985MU11 17NDS 201704
256RF H TYP=FUL$AUT=BALRAJ SINGH$CIT=NDS 141, 327 (2017)$CUT=22-Mar-2017$
256RF c {+260}Sg assignment: {+207}Pb({+54}Cr,n), {+208}Pb({+54}Cr,2n); parent
256RF2c of {+256}Rf (1984De07,1984Og03,1985Mu11)
256RF c 1985Mu11: measured E|a, I|a, half-life
256RF c 2009He20: {+260}Sg produced in the {+208}Pb({+54}Cr,2n) and
256RF2c {+207}Pb({+54}Cr,n) reactions with the {+54}Cr beam delivered by the
256RF3c charge state injector of the UNILAC accelerator at GSI Darmstadt.
256RF4c Evaporation residues were separated by the velocity filter SHIP and
256RF5c implanted into a 16-strip Si PIPS detector. A box of six Si-wafers was
256RF6c used to measure escaping |a-particles. A Ge clover detector consisting
256RF7c of four crystals was used to measure |g rays in coincidence with
256RF8c particles. Measured E|a, E|g, half-lives, |s.
256RF cA IA$|a intensity per 100 |a decays, measured by 1985Mu11.
256RF cA $r{-0}({+256}Rf)=1.456 fm {I8} from assumption of HF=1.0 for
256RF2cA g.s. to g.s. |a transition
256RF cL J,T$From Adopted Levels
260SG P 0.0 0+ 4.95 MS 33 9901 10
260SG cP T$Measured by 2009He20. Others: 3.6 ms {I+9-6} (1985Mu11,from
260SG2cP |a decay curves); 2.5 ms {I15} was deduced by 1984De07
260SG3cP from fission counts (T{-1/2}(SF)=6 ms {I+2-1} was measured from SF
260SG4cP activities, and the time distribution of fission fragments were
260SG5cP utilized in calculation of the half-life by subtracting the SF
260SG6cP activities of {+256}Rf, the |a daughter; %|a>80 was assumed).
260SG cP QP$From 2017Wa10
256RF N 0.29 3
256RF cN BR$%|a=29 {I3}, %SF=71 {I3} (2009He20). Other: %|a=50 {I+20-30}
256RF2cN (1985Mu11)
256RF L 0.0 0+ 6.67 MS 10
256RF A 9750 10 83 10 1.0
256RF cA E$weighted average of 9770 {I30} (1985Mu11) and 9748 {I10} (2009He20)
256RF L 51 35 (2+)
256RF A 9720 30 17 10 3.6 22
256RF cA HF$deduced using r{-0}({+256}Rf)=1.456 fm {I8}
256RF cA E$from 1985Mu11.