182HG 186PB A DECAY (4.82 S) 1980SC09,1994WA23,1999AN2215NDS 201512
182HG H TYP=FUL$AUT=BALRAJ SINGH$CIT=NDS 130, 21 (2015)$CUT=15-Jul-2015$
182HG c Measured E|a, ce, half-lives
182HG d Theory: 2000Va34
182HG cA IA |a intensity per 100 |a decays.
182HG cA HF r{-0}({+182}Hg)=1.50 {I2} is obtained from the systematics of
182HG2cA r{-0} parameters.
182HG cL J$From Adopted Levels
186PB P 0.0 0+ 4.82 S 3 6470 6
186PB cP T$From {+186}Pb Adopted Levels in ENSDF database
186PB cP QP$From 2012Wa38
182HG N 0.40 8
182HG cN BR$%|a from 2003Ba44 deduced from %|a=38 {I9} (1999An22), 45 {I20}
182HG2cN (1997Ba25), 50 {I25} (1997An09). 1972Ga27 and 1974Le02 report %|a=5
182HG3cN and 2.4, respectively, but T{-1/2} in each of these studies
182HG4cN differs from the adopted value. Only the |a decay of {+186}Pb has been
182HG6cN observed and the %|a branch has been measured from |a-|a correlations.
182HG7cN The |b decay of {+186}Pb has not been studied, and |a/|b branchings
182HG8cN have not been determined experimentally.
182HG cN BR$theoretical estimates of %|a: 52-84% from partial half-life of
182HG2cN |?10-30 s for |e decay, estimated from gross |b-decay calculations
182HG3cN of 1973Ta30; 52 from calculated T{-1/2}(|b{++})=10.03 s (1997Mo25);
182HG4cN 54 {I20} from calculations of radius parameters as a function of |a
182HG5cN branching, for r{-0}=1.50 {I2}
182HG L 0.0 0+
182HG A 6331 6 99.6 2 1.0
182HG cA E$measured energies are 6337 {I15} (1997Ba25), 6320 {I15} (1997An09),
182HG2cA 6331 (1980Sc09), 6319 {I20} (1974Le02), 6335 {I10} (1984To09) and
182HG3cA 6320 {I10} (1972Ga27). The E|a values given by 1974Le02 and 1980Sc09
182HG4cA are adjusted for calibration as recommended by 1991Ry01.
182HG5cA Q(|a)({+186}Pb)=6470 {I6} (2012Wa38) yields E|a=6331 {I6}. E|a=6328
182HGxcA {I6} is recommended in 1991Ry01.
182HG cA IA$intensity of 6332-keV |a is from I|a(5988|a) and I|a(6014|a).
182HG L 328 12(0+)
182HG G 328 (E0)
182HG cG E,M$very weak electron line seen in 1994Wa23
182HG A 6014 13 0.20 5 23 5
182HG cA E$from 1994Wa23.
182HG cA IA$obtained by 1994Wa13; the authors list the absolute I|a values as:
182HG2cA I|a(6332|a)<100 and I|a(6014|a)<0.20%. The uncertainty is deduced from
182HG3cA the uncertainty in HF calculated by 1994Wa13.
182HG L 351.8 3 2+
182HG A 5988 8 0.16 LT 23 GT S
182HG cA E$this |a transition has not been observed; its energy
182HG2cA is calculated from E(level)=351.8 {I3} and Q(|a)=6470 {I6}.
182HG cA IA$1994Wa23 calculate HF for this |a branch
182HG2cA (the |a hindrance factors were calculated by using the Rasmussen
182HG3cA formalism from their experimental upper limit for I|a). Their hindrance
182HG4cA factor corresponds to I|a(5988|a)<0.16 per 100 |a decays.
182HG cA $An upper limit of 3.6 per 100 |a decays is deduced for an
182HG2cA |a transition to the 2+ state by requiring its hindrance factor
182HG3cA to be greater than 1.