140CE    144ND A DECAY                                           18NDS    201812
140CE  H TYP=FUL$AUT=N. NICA$CIT=NDS 154, 1 (2018)$CUT=20-Nov-2018$
140CE c  T{-1/2}({+144}Nd)=2.29|*10{+15} y {I16}, adopted by 2001So16, is used
140CE2c  in calculations of r{-0}. This half-life is the unweighted average of
140CE3c  the measured half-lives: 2.65|*10{+15} y {I37} (1987Al28),
140CE4c  2.4|*10{+15} y {I3} (1961Ma05), 2.2|*10{+15} y (1956Po16) and
140CE5c  1.9|*10{+15} y (1965Is01).
140CE c  %|a=100. The nucleus {+144}Nd is stable against |b decay.
140CE cA IA        |a intensity per 100 |a decays.
140CE cA HF        r{-0}({+140}Ce)=1.594 {I6} is computed from HF(1853.4|a)=1.0.
144ND  P 0.0         0+                2.29E+15 Y 16            1903.2    16
144ND cP E,J,T$From 2001So16
144ND cP QP$From 2017Wa10
140CE  N                       1.0
140CE  L 0.0         0+
140CE  A 1830      15 100      1.0
140CE DA E$Source of EA=1830 15 (1989Tu02) cited by 1998Ak04 appears to be a
140CE2DA typographical error. 1987Pe07 cite this value giving 1975Bu19 as the
140CE2DA source. 1975Bu19 do not adopt any value for EA
140CE cA IA$only |a to g.s. observed (1987Al28)