116CD 116AG B- DECAY (20 S) 2009BA52,2005BA94 10NDS 201004
116CD H TYP=FUL$AUT=Jean Blachot$CIT=NDS 111, 717 (2010)$CUT=1-Dec-2009$
116CD C 2009Ba52: {+116}Ag activity was produced by the 40-MeV protons
116CDaC bombarding a {+238}UC{-x} target installed at the On-Line Test
116CDaC Facility (OLTF) at the Holifield Radioactive Ion Beam Facility
116CDaC (HRIBF). Fission products was separated and deposited on a moving
116CDaC tape collector (MTC).
116CD C Measured E|g, I|g, |g|g, conversion electron-|g with the (CARDS)
116CDaC detector array, composed of the three segmented-clover Ge detectors,
116CDaC plastic scintillators and a high-resolution Si conversion-electron
116CDaC spectrometer (BESCA).
116CD C Transitions arising from the respective short-lived isomers were
116CDaC separated by their half-lives.
116CD C The |g-|g and conversion electron-|g coincidences were used to
116CDaC construct the decay scheme in {+116}Cd after the |b decay of the
116CDaC isomer 20 s {+116}Ag.
116CD CB LOGFT$The values are nearly the same as in Table IV of 2009Ba52, the
116CDaCB authors state that log {Ift} values should be considered as lower
116CDaCB limits, especially, for weak |b feedings, due to "pandemonium" effect.
116CD CG $Unplaced |g rays are from the decay of 20-s or the 9.3-s isomer
116CD CG RI$From singles |g and |g|g coin spectra, unless otherwise stated
116CD CG RI(A)$From |g singles spectra.
116CD CG RI(B)$From |g|g coincidence spectra.
116CD CG RI(D)$From {+116}Ag{-gs} decay data.
116CD CL E$From least-squares fit to E|g's
116CD CL J$From Table IV of 2009Ba52.
116AG P 47.9 1 (3+) 20 S 1 6176 4
116AG CP E,J,T$From 2005Ba94. This isomer decays |?7 {I4} % by an isomeric E3
116AGaCP transition of 47.9 keV to g.s., (0-) of {+116}Ag. Likely
116AGaCP configuration=|p1/2[301]~#|n7/2[523]
116AG CP QP$From 2009AuZZ
116CD N 2.76 AP 0.93 4 1.075
116CD CN BR$%IT=7 {I4} from 2005Ba94.
116CD PN 3
116CD G 152.8 3 0.06 1
116CD G 198.7 3 0.21 4
116CD G 204.2 3 0.14 3
116CD G 315.1 3 0.11 2
116CD G 374.3 3 0.04 3
116CD G 552.1 3 0.03 1
116CD G 689.0 3 0.05 1
116CD G 738.7 3 0.02 1
116CD G 754.0 3 0.07 2
116CD G 784.8 3 0.07 3
116CD G 862.4 5 0.2 1
116CD G 873.9 3 0.07 1
116CD G 896.5 3 0.14 7
116CD G 930.0 3 0.014 10
116CD G 953.6 3 0.03 2
116CD G 977.3 3 0.03 1
116CD G 1180.6 4 0.03 1
116CD G 1269.5 5 0.014 9
116CD G 1250.5 4 0.03 1
116CD G 1422.2 5 0.02 1
116CD G 1517.2 3 0.13 3
116CD G 1549.5 5 0.03 1
116CD G 1630.9 5 0.008 6
116CD G 1676.8 4 0.04 1
116CD G 1858.2 4 0.04 1
116CD G 1918.0 5 0.02 1
116CD G 1922.4 5 0.03 1
116CD G 2012.8 5 0.04 1
116CD L 0.0 0+
116CD L 513.50 7 2+
116CD G 513.5 1 36 3 E2 0.006179
116CDX G FLAG=A$EKC=5.3E-3 1
116CDS G KC=0.00532 8$LC=0.000693 10$MC=0.0001335 19$NC=2.35E-5 4$
116CDS G OC=1.210E-6 17$NC+=2.47E-5 4
116CD CG EKC$Uncertainty of 0.00001 in Table I of 2009Ba52 seems unrealistic,
116CDaCG the compilers have increased the uncertainty by a factor of 10
116CD L 1213.11 7 2+
116CD G 699.6 2 8.5 6 M1,E2 0.0028417
116CDX G EKC=2.4E-3 4
116CDS G KC=0.00247 16$LC=0.000300 11$MC=5.75E-5 21$NC=1.02E-5 4$OC=5.8E-7 5$
116CDS G NC+=1.08E-5 5
116CD G 1213.1 1 4.2 3
116CD L 1219.48 9 4+
116CD G 706.0 1 10 1 E2 0.002614
116CDX G EKC=2.2E-3 2
116CDS G KC=0.00227 4$LC=0.000283 4$MC=5.43E-5 8$NC=9.61E-6 14$OC=5.24E-7 8$
116CDS G NC+=1.013E-5 15
116CD L 1642.60 102+
116CD G 423.1 2 0.012 5
116CD G 1129.1 1 0.22 2
116CD G 1642.6 2 0.15 2
116CD B 1.1 2 7.37 9
116CDX B EAV=1996.9 19
116CD L 1869.78 144+
116CD G 650.2 2 0.31 2 M1,E2 0.0034017
116CDX G EKC=2.9E-3 4
116CDS G KC=0.00295 16$LC=0.000361 10$MC=6.92E-5 18$NC=1.23E-5 4$OC=6.9E-7 5$
116CDS G NC+=1.30E-5 4
116CD G 656.7 2 0.65 5 M1,E2 0.0033117
116CDX G EKC=3.0E-3 3
116CDS G KC=0.00288 16$LC=0.000352 10$MC=6.75E-5 18$NC=1.20E-5 4$OC=6.8E-7 5$
116CDS G NC+=1.27E-5 5
116CD G 1356.4 3 0.11 2
116CD B 2.6 17 6.9 3
116CDX B EAV=1889.0 19
116CD L 1915.99 103+
116CD G 696.5 2 0.46 3
116CD G 702.9 3 1.0 1
116CDX G FLAG=B
116CD G 1402.5 1 1.4 2
116CD B 5.2 5 6.57 5
116CDX B EAV=1867.0 19
116CD L 1921.68 103-
116CD G 708.6 2 0.8 2
116CDX G FLAG=B
116CD G 1408.2 1 2.8 2
116CD B 4.8 5 6.61 5
116CDX B EAV=1864.3 19
116CD L 1951.41 8 2+
116CD G 1437.9 1 0.8 2
116CD G 1951.4 1 0.13 3
116CD B 2.1 6 6.95 13
116CDX B EAV=1850.2 19
116CD L 2302.98 22
116CD G 1083.5 2 0.15 1
116CD B 0.36 17 7.56 21
116CDX B EAV=1683.5 19
116CD L 2340.11 12(4-)
116CD CL J$4- in figure 5 and Table I of 2009Ba52; but this assignment is
116CDaCL inconsistent with multipolarities assigned to 418 and 424 |g rays
116CD G 418.3 3 0.03 1
116CDX G FLAG=A
116CD CG M$E1 proposed by 2009Ba52 based on K/L ratio is inconsistent with
116CDaCG |DJ|p
116CD G 423.9 2 0.14 2
116CDX G EKC=7E-3 3
116CD CG M$M1 proposed by 2009Ba52 is inconsistent with |DJ|p
116CD CG $|a(K)exp=8|*10{+-3} {I2} is also listed in the text on page 9 of
116CDaCG 2009Ba52
116CD G 1120.7 1 0.34 3
116CD B 1.3 1 6.98 4
116CDX B EAV=1666.0 19
116CD L 2377.31 18
116CD CL J$(3+) in figure 5; not listed in Table I of 2009Ba52.
116CD G 1157.8 3 0.8 2
116CD G 1164.1 3 0.16 3
116CDX G FLAG=A
116CD G 1863.9 3 0.36 7
116CDX G FLAG=A
116CD B 2.8 4 6.63 7
116CDX B EAV=1648.4 19
116CD L 2392.14 22(3-)
116CD CL J$from table IV of 2009Ba52 and discussion in text; 2+ in figure 5,
116CDaCL not listed in Table I of 2009Ba52.
116CD G 470.5 3 0.04 3
116CDX G FLAG=D
116CD G 1179.0 4 0.18 2
116CDX G FLAG=A
116CD G 1878.6 4 0.52 7
116CD B 1.8 2 6.81 6
116CDX B EAV=1641.3 19
116CD L 2493.69 22
116CD G 1274.2 2 0.18 5
116CDX G FLAG=B
116CD B 0.4 2 7.42 22
116CDX B EAV=1593.3 19
116CD L 2518.38 9 (2-)
116CD CL J$J=2- in Table I of 2009Ba52.
116CD CL $Compilers' note: there seems problem with the inventory of |g rays
116CDaCL from this level as listed in table I of 2009Ba52. Strong transitions
116CDaCL as seen in the decay of the ground state are not listed here. It is
116CDaCL not clear how the |b feeding of 2.2 has been obtained.
116CD G 567.0 2 0.16 3
116CDX G FLAG=D
116CD G 596.6 3 0.15 3
116CDX G FLAG=D
116CD G 602.7 2 0.20 6
116CDX G FLAG=D
116CD B 2.2 9 6.66 18
116CDX B EAV=1581.6 19
116CD L 2784.2 3
116CD G 2270.7 3 0.4 2
116CD B 1.0 5 6.87 22
116CDX B EAV=1456.1 19
116CD L 2822.42 14
116CD G 901.0 2 0.45 6
116CD G 1603.0 3 1.5 2
116CD G 1609.3 5 0.7 1
116CD G 2308.6 2 1.5 2
116CD B 10.5 8 5.83 4
116CDX B EAV=1438.1 19
116CD L 2844.0 3
116CD G 2330.6 3 1.3 2
116CD G 2843.8 5 0.7 1
116CD B 5.2 5 6.12 5
116CDX B EAV=1427.9 19
116CD L 2915.41 22
116CD G 1696.0 3 0.23 3
116CD G 1702.2 3 0.23 3
116CDX G FLAG=A
116CD B 0.6 2 7.02 15
116CDX B EAV=1394.3 19
116CD L 3124.7 3
116CD G 1911.6 3 0.7 1
116CD B 1.6 4 6.47 11
116CDX B EAV=1295.9 19
116CD L 3228.06 16
116CD G 2008.4 2 1.0 2
116CDX G FLAG=B
116CD G 2015.1 2 0.39 7
116CDX G FLAG=B
116CD B 3.5 5 6.07 7
116CDX B EAV=1247.4 19
116CD L 3294.41 16
116CD G 1378.4 3 0.7 1
116CDX G FLAG=A
116CD G 2075.0 4 1.1 2
116CDX G FLAG=B
116CD G 2081.5 4 4.4 4
116CDX G FLAG=B
116CD G 2780.8 2 2.0 2
116CDX G FLAG=B
116CD B 20 1 5.27 3
116CDX B EAV=1216.4 19
116CD L 3303.2 3
116CD G 1381.5 3 1.3 1
116CD B 3.0 3 6.09 5
116CDX B EAV=1212.2 19
116CD L 3304.18 18
116CD G 2084.7 2 2.1 2
116CDX G FLAG=B
116CD G 2091.0 3 1.3 2
116CD B 8.5 5 5.64 4
116CDX B EAV=1211.8 19
116CD L 3354.90 20
116CD G 2135.4 2 1.4 2
116CD G 2841.4 5 6.8 8
116CD B 21 2 5.21 5
116CDX B EAV=1188.1 19