123IN 123CD B- DECAY (2.10 S) 1989HU03,1986HO24 21NDS 202105
123IN H TYP=FUL$AUT=Jun Chen$CIT=NDS 174, 1 (2021)$CUT=15-Apr-2021$
123IN c 1989Hu03: source of {+123}Cd was produced via the U(n,F) reaction with
123IN2c fast neutrons produced from the Be(d,n) reaction at the TANDAR
123IN3c Laboratory. Fission products were separated by an electro-magnetic
123IN4c mass separator. |g rays were detected with two HPGe detectors
123IN5c (FWHM=1.95 keV at 1.33 MeV). Measured E|g, I|g, |g|g-coin, |g(t).
123IN6c Deduced levels, J, |p, parent T{-1/2}, |b-decay branching ratios,
123IN7c log {Ift}. Systematics of neighboring odd-mass In isotopes.
123IN8c Comparisons with theoretical calculations.
123IN c 1986Ho24: source of {+123}Cd was produced via {+235}U(n,F) with
123IN2c neutrons provided by the R2-0 reactor at Studvik. Fission products were
123IN3c separated by the mass separator OSIRIS. |g rays were detected with
123IN4c Ge detectors. Conversion electrons were detected with a small
123IN5c high-resolution Si detector. Measured E|g, I|g, |g|g-coin, |g(t).
123IN6c Deduced levels, J, |p, parent T{-1/2}, |b-decay branching ratios,
123IN7c log {Ift}. Systematics of neighboring odd-mass In isotopes.
123IN c Others: 1973BaUR, 1981Ru07, 1983Re05, 1986Go10, 1986Ma42, 1987Sp09,
123IN2c 2014TeZY
123IN c The decay scheme is that proposed by 1989Hu03. Fast-neutron fission
123IN2c favors high-spin isomer. |g-rays were distinguished by comparing the
123IN3c results from 1986Ho24. Decay scheme from 1986Ho24 is mixed from decays
123IN4c of g.s. and isomer. There are some discrepancies between the level
123IN5c scheme from 1989Hu03 and from 1986Ho24. The evaluator has adopted
123IN6c the g.s. decay scheme from 1989Hu03. However, there are many unplaced
123IN7c |g rays, as well as a large gap between the highest level and Q-value,
123IN8c therefore, the decay scheme is considered as incomplete and the deduced
123IN9c |b-feedings and log {Ift} as approximate.
123IN cB IB$From |g+ce intensity imbalance at each level. Quoted values should
123IN2cB be considered as approximate due to incomplete decay scheme.
123IN cG E,RI$From 1989Hu03, unless otherwise noted. Values are also available
123IN2cG in the decay schemes in 1986Ho24 but no tabulated data are given.
123IN cG E(X)$Poor fit. Uncertainty are increased to 0.2 keV in the fitting
123IN2cG procedure.
123IN cG M(A)$As given in the decay scheme in 1986Ho24 based on ce data. The
123IN2cG same values are adopted in Adopted Gammas. No ce data is explicitly
123IN3cG given by 1986Ho24
123IN cL E$From a least-squares fit to |g-ray energies
123IN cL J,T$From Adopted Levels
123CD P 0.0 3/2(+) 2.10 S 3 6015 20
123CD cP J,T$From Adopted Levels of {+123}Cd
123CD cP QP$From 2021Wa16
123IN N 1.0 1.0 1.0
123IN cN NR$From |SI(|g+ce to g.s.+327)=100. No |b feeding is expected to g.s.
123IN2cN (2nd forbidden) and feeding to 327 level is assumed to be negligible
123IN3cN (|<1 from log {Ift}=6.9 for 1st forbidden in this mass region)
123IN PN 3
123IN G 244.0 3 0.37 22
123IN G 525.20 201.01 14
123IN G 545.4 3 2.64 22
123IN G 714.00 250.46 14
123IN G 913.41 152.0 4
123IN G 1044.88 121.7 3
123IN G 1519.48 101.09 16
123IN G 1594.8 7 0.63 6
123IN G 1641.86 200.63 13
123IN G 1976.00 102.2 3
123IN L 0.0 9/2+ 6.15 S 27
123IN L 327.21 5 1/2- 47.4 S 8 M
123IN L 698.51 4(3/2)-
123IN B 2 LE 6.5 GE
123INS B EAV=2390 16
123IN G 371.32 352 3 M1 0.0153 AC
123IN cG E$other: 371.2 {I2} (1981Ru07)
123INS G KC=0.0133$LC=0.00161$MC=0.00031
123IN L 1052.29 3(5/2+)
123IN B 15.2 18 5.5 1
123INS B EAV=2222 16
123IN G 353.63 73.6 4 C
123IN G 1052.28 325.1 16 C
123IN cG E$other: 1052.3 {I2} (1981Ru07)
123IN L 1137.55 5(3/2-,5/2-)
123IN B 3.9 8 6.0 1
123INS B EAV=2182 16
123IN G 438.68 5 2.32 25 XC
123INF G FL=698.51
123IN G 810.29 36.3 6 C
123IN L 1512.12 47/2+,9/2+
123IN G 1512.09 54.28 25 C
123IN L 1566.24 4(9/2+)
123IN G 1566.09 50.33 2 C
123IN L 1615.72 7(1/2,3/2,5/2-)
123IN B 2.9 6 6.0 1
123INS B EAV=1955 16
123IN G 917.16 64.4 5 C
123IN G 1288.35 200.38 7
123IN L 1926.55 6(1/2,3/2,5/2-)
123IN B 1.0 4 6.3 2
123INS B EAV=1807 16
123IN G 1227.50 5 2.48 24 XC
123INF G FL=698.51
123IN G 1599.23 121.17 19
123IN L 2020.63 4(7/2-)
123IN B 1.21 11 6.2 1
123INS B EAV=1763 16
123IN G 454.25 50.25 3 C
123IN G 883.0 9 0.25 6 C
123IN G 2020.71 40.71 5
123IN L 2029.91 6(1/2+,3/2+)
123IN B 5.1 9 5.5 1
123INS B EAV=1758 16
123IN G 1331.44 56.6 6 C
123IN G 1702.37 7 2.2 3 X
123IN L 2136.63 4(1/2+,3/2+)
123IN B 13.7 10 5.0 1
123INS B EAV=1708 16
123IN G 999.12 151.4 3 C
123IN G 1084.32 35.0 4 C
123IN G 1438.13 58.4 7 C
123IN G 1809.50 91.72 18
123IN L 2158.59 7(1/2+,3/2+,5/2+)
123IN B 4.1 3 5.6 1
123INS B EAV=1697 16
123IN G 1460.07 54.1 3 C
123IN L 2377.32 9(1/2+,3/2+,5/2+)
123IN B 4.4 6 5.4 1
123INS B EAV=1594 16
123IN G 347.48 83.0 5 C
123IN G 1324.77 151.4 3
123IN L 2393.31 4(5/2+)
123IN B 21.2 12 4.7 1
123INS B EAV=1587 16
123IN G 256.69 52.8 4
123IN G 363.7 6 0.25 2
123IN G 827.23 250.33 15
123IN G 881.17 54.4 9 C
123IN G 1255.65 52.62 21 C
123IN G 1341.06 53.1 3 C
123IN G 1694.81 57.1 5 C
123IN G 2393.46 150.71 2
123IN L 2429.48 6(1/2+,3/2+,5/2+)
123IN B 5.3 4 5.3 1
123INS B EAV=1570 16
123IN G 813.63 91.9 3 C
123IN G 1377.36 101.39 20
123IN G 1730.95 61.99 19 C
123IN L 2529.30 6(1/2+,3/2+)
123IN B 10.5 5 5.0 1
123INS B EAV=1523 16
123IN G 602.73 31.22 2 C
123IN G 1830.78 56.1 4 C
123IN G 2202.14 73.2 3
123IN L 2541.31 5(1/2+,3/2+)
123IN B 14.3 7 4.8 1
123INS B EAV=1517 16
123IN G 512.0 50.41 8 C
123IN G 615.1 9 1.39 13 C
123IN G 1403.37 150.44 11
123IN G 1488.91 52.6 3 C
123IN G 1842.86 57.8 5 C
123IN G 2214.33 101.61 21