125IN 125CD B- DECAY (0.68 S) 1989HU03,1986HO24 11NDS 201102
125IN H TYP=FUL$AUT=J. KATAKURA$CIT=NDS 112, 495 (2011)$CUT=1-Jan-2010$
125IN c Sources: U(n,F), E=fast, on-line mass (1989Hu03)
125IN2c {+235}U(n,F), E=th; on-line mass (1986Ho24)
125IN c Measured: |g singles, |g|g coin (1989Hu03,1986Ho24); T{-1/2} (1989Hu03)
125IN c The decay scheme is that proposed by 1989Hu03.
125IN2c 1986Ho24 report decay only of the (3/2+), 0.65-s g.s.
125IN cG E,RI From 1989Hu03, unless otherwise noted
125IN cG E(B) Not given in 1986Ho24
125IN cL E$From a least-squares fit to E|g's by evaluators
125IN cL T,J From adopted levels
125IN cL E(H)$From energy difference of g.s. transitions (1099|g, 2147|g and
125IN2cL 2947|g) and those competing |g cascades to 796 level, with E|g=436.25
125IN3cL for the transition from 796 to 360. However, this
125IN3cL is a different value, 287 keV {I31}, from |b|g-coin experiments
125IN4cL (1987Sp09)
125CD P 0.0 (3/2+) 0.68 S 4 7.12E+3 6
125IN N 0.97 4 1.0 1.0
125IN PN 3
125IN cN NR |S(I(|g+ce) to g.s. and 360 level)=97 {I3}, assuming
125IN2cN I|b{+-}<6.0 to 360 level for expected log| {Ift}>5.9. No |b{+-}
125IN3cN transition, involving |DJ=2 is expected to the g.s.
125IN G 267.88 251.5 5 B
125IN G 294.38 151.4 3 B
125IN G 361.10 250.69 19 B
125IN G 389.45 152.3 5 B
125IN G 445.32 201.4 4 B
125IN G 551.46 250.51 21
125IN G 799.0 4 1.8 4
125IN G 1256.7 5 0.48 22 B
125IN G 1275.15 5 0.9 4 B
125IN G 2115.58 152.5 7 B
125IN G 2133.25 153.9 6 B
125IN G 2290.26 153.3 4
125IN cG $ 1986Ho24 placed the |g from 2290-keV level to ground state.
125IN G 2380.24 251.6 3
125IN G 2938.7 4 0.76 21 B
125IN L 0.0 9/2+ 2.36 S 4
125IN2 L %B-=100
125IN L 360.12 91/2(-) 12.2 S 2 HM
125IN DL E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT
125IN2 L %B-=100
125IN B 6.0 LT 5.9 GT
125INS B EAV=3028 29
125IN cB IB From assumption that log| {Ift}>5.9 from (3/2+) parent
125IN L 796.46 10(3/2-)
125IN B 4 LT 6.0 GT
125INS B EAV=2821 29
125IN G 436.29 3 43 3 C
125IN cG RI 1986Ho24 and 1986Go10 report absolute intensity of this
125IN2cG transition as 12% {I2}. But their results seem to include both
125IN3cG components of 0.65 s and 0.47 s decays.
125IN L 1099.49 3(5/2+)
125IN B 24.5 24 5.09 6
125INS B EAV=2677 29
125IN G 302.96 151.90 16 C
125IN G 1099.48 3 25.6 21
125IN L 1219.72 10(1/2,3/2,5/2-)
125IN B 4.7 7 5.77 8
125INS B EAV=2620 29
125IN G 422.91 103.2 4 C
125IN G 859.71 5 6.79 6 C
125IN L 1588.54 14
125IN G 369.23 150.85 18 B
125IN G 792.43 203.3 13 C
125IN L 1810.40 13
125IN G 1013.97 103.9 10 C
125IN L 2147.18 10(5/2+)
125IN B 23.0 17 4.75 5
125INS B EAV=2179 29
125IN G 1349.9 5 1.8 5 C
125IN G 2147.19 1021.9 13
125IN cG $According to 1986Ho24 and 1989Hu03, 2147-keV |g-ray decays directly
125IN2cG to the ground state, but 1987Sp09 suggest the |g-ray as that decaying
125IN3cG from 2507-keV level from Q{-|b} measurement. The 2507-keV level,
125IN4cG however, is not reported in 1989Hu03.
125IN L 2349.45 14(1/2,3/2,5/2)
125IN B 7.1 7 5.18 6
125INS B EAV=2083 29
125IN G 538.9 4 0.33 8 B
125IN G 1249.75 252.2 4 B
125IN G 1552.88 152.9 4 C
125IN G 1989.50 151.9 3
125IN L 2381.30 11(1/2,3/2,5/2)
125IN B 9.3 9 5.05 6
125INS B EAV=2068 29
125IN G 1584.83 5 8.3 7 C
125IN G 2021.16 151.3 3
125IN cG E 2020.4 (1986Ho24)
125IN L 2497.46 11(1/2+,3/2+)
125IN B 14.9 12 4.80 5
125INS B EAV=2013 29
125IN cB E$4357 {I38} (1987Sp09)
125IN G 687.28 153.0 4 B
125IN G 1700.96 5 12.4 9 C
125IN L 2585.06 14(1/2+,3/2+,5/2+)
125IN B 9.4 9 4.96 6
125INS B EAV=1971 29
125IN G 774.46 201.2 3
125IN G 996.78 104.8 7
125IN cG E 996.0 (1986Ho24)
125IN G 1364.64 202.76 20 C
125IN G 1788.38 200.95 25 C
125IN L 2641.22 16(1/2,3/2,5/2)
125IN B 3.4 6 5.38 9
125INS B EAV=1945 29
125IN G 1421.67 151.5 4 BC
125IN G 1844.43 202.0 4 C
125IN cG E$deexciting |g from 2641.7 level in 0.57-s decay in 1986Ho24