236CM    240CF A DECAY                 2010Kh06                  22NDS    202205
236CM  H TYP=FUL$AUT=Shaofei Zhu$CIT=NDS 182, 2 (2022).$CUT=1-Apr-2022$
236CM c  2010Kh06: {+240}Cf produced in reactions {+206}Pb({+36}S,2n) E=163.6,
236CM2c  172.6 MeV and {+207}Pb({+36}S,3n) E=165.5, 170.3 MeV using
236CM3c  isotopically enriched PbS target with beams delivered by UNILAC at
236CM4c  GSI. Evaporation residues (ERs) separated by the velocity filter SHIP
236CM5c  and implanted on a position-sensitive 16 strip Si detector (stop
236CM6c  detector). A Ge clover detector behind the Si detector for detecting
236CM7c  x rays and/or |g-rays. Measured E(|a), ER-|a correlations, T{-1/2},
236CM8c  decay modes
236CM cA IA$Estimated from the systematics of hindrance factors
236CM2cA HF(2+)/HF(0+)=1.5 {I1}. It is consistent with the peak height as
236CM3cA shown in 2010AsZX.
236CM cA HF$r{-0}({+236}Cm)=1.5185 {I25} is calculated from HF(7582|a)=1.0
236CM2cA assuming I|a(to g.s.)=69% {I2} and I|a(to 2+)=31% {I2}.
240CF  P 0.0                            40.3 S    9              7711     4
240CF cP T$from 2010AsZX; others: 0.9 min {I2} (1995La09); 0.8 min {I+3-2}
240CF2cP (1995La09) and 1.06 min {I15} (1970Si19)
240CF cP QP$from 2021Wa16.
236CM  N 1                      0.985  2
236CM cN BR$from 2010Kh06 with %SF=1.5 {I2} and %|e negligible.
236CM  L 0.0          0+                6.8 M     8
236CM cL T$from 2010Kh06 based on |a|a(t) measurement.
236CM  A 7582      4 69      2 1.000
236CM cA E$weighted average of 7590 {I10} (1970Si19), 7585 {I20} (2010Kh06)
236CM2cA and 7581 {I4} (2010AsZX).
236CM  L 47.4      4  2+
236CM cL E$from 2010AsZX.
236CM cL J$from K=0+ g.s. band.
236CM  A 7535      4 31      2 1.51    11
236CM cA E$from 2010AsZX.