116CD 116AG B- DECAY (9.3 S) 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 First measurements : 1973FOZF,1974BJ01,1975BRYN
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 9.8-s
116CDaC isomer of {+116}Ag.
116CD CB LOGFT$The values are nearly the same as in Table IV of 2009Ba52,
116CDaCB unless otherwise stated. 2009Ba52 state that log {Ift} values should
116CDaCB be considered as lower limits, especially, for weak |b feedings, due
116CDaCB to "pandemonium" effect.
116CD CG $Unplaced |g rays are from the decay of 20-s or the 9.8-s isomer
116CD CG RI$From singles |g and |g|g coin spectra, unless otherwise stated
116CD CG RI(A)$From singles |g spectra.
116CD CG RI(B)$From |g|g coin spectra.
116CD CL E$From least-squares fit to E|g's
116CD CL J$From Table IV (2009Ba52).
116AG P 128.8 1 (6-) 9.3 S 1 6176 4
116AG CP E,J,T$From 2005Ba94. This isomer decays |?8 {I4} % by an isomeric E3
116AGaCP transition of 80.9 keV to 47.9, (3+) level of {+116}Ag. Likely
116AGaCP configuration=|p5/2[422]~#|n7/2[523] or |p3/2[431]~#|n9/2[514]
116AG CP QP$From 2009AuZZ
116CD N 4.4 AP 0.92 4 1.087
116CD CN BR$%IT=8 {I4} from 2005Ba94.
116CD PN 3
116CD G 152.8 3 0.06 1
116CD G 198.7 3 0.21 4
116CD G 204.2 3 0.14 3
116CD G 315.1 3 0.11 2
116CD G 374.3 3 0.04 3
116CD G 552.1 3 0.03 1
116CD G 689.0 3 0.05 1
116CD G 738.7 3 0.02 1
116CD G 754.0 3 0.07 2
116CD G 784.8 3 0.07 3
116CD G 862.4 5 0.2 1
116CD G 873.9 3 0.07 1
116CD G 896.5 3 0.14 7
116CD G 930.0 3 0.014 10
116CD G 953.6 3 0.03 2
116CD G 977.3 3 0.03 1
116CD G 1180.6 4 0.03 1
116CD G 1269.5 5 0.014 9
116CD G 1250.5 4 0.03 1
116CD G 1422.2 5 0.02 1
116CD G 1517.2 3 0.13 3
116CD G 1549.5 5 0.03 1
116CD G 1630.9 5 0.008 6
116CD G 1676.8 4 0.04 1
116CD G 1858.2 4 0.04 1
116CD G 1918.0 5 0.02 1
116CD G 1922.4 5 0.03 1
116CD G 2012.8 5 0.04 1
116CD L 0.0 0+
116CD L 513.50 8 2+
116CD G 513.5 1 24 2 E2
116CDX G FLAG=A$EKC=5.3E-3 1
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 8 2+
116CD G 699.6 2 1.4 1 M1,E2
116CDX G EKC=2.4E-3 4
116CD G 1213.1 1 0.70 5
116CD L 1219.50 104+
116CD G 706.0 1 22 2 E2
116CDX G EKC=2.2E-3 2
116CD L 1642.61 102+
116CD G 423.1 2 0.002 1
116CD G 1129.1 1 0.05 1
116CD G 1642.6 2 0.03 1
116CD L 1869.82 134+
116CD G 650.2 2 0.69 5 M1,E2
116CDX G EKC=3.3E-3 9
116CD G 656.7 2 1.5 1 M1,E2
116CDX G EKC=2.9E-3 5
116CD G 1356.4 3 0.23 2
116CD B 3.9 6 8.1 1 1U
116CDX B EAV=1927.4 19
116CD L 1916.04 113+
116CD G 696.5 2 0.10 1
116CDX G FLAG=B
116CD G 702.9 3 0.24 5
116CDX G FLAG=B
116CD G 1402.5 1 0.33 2
116CD L 1921.70 113-
116CD G 708.6 2 0.05 2
116CD G 1408.2 1 0.16 3
116CD L 2026.72 126+
116CD G 807.1 1 6.5 6 E2
116CDX G EKC=1.6E-3 1
116CD L 2042.29 124+
116CD G 399.5 4 0.06 1
116CDX G FLAG=B
116CD G 822.6 4 0.06 1
116CDX G FLAG=B
116CD G 1528.8 1 0.23 3
116CD B 1.4 1 8.5 1 1U
116CDX B EAV=1845.5 19
116CD L 2249.11 115-
116CD G 327.6 3 0.08 2
116CDX G EKC=2.4E-2 12
116CD G 379.4 2 0.6 1 E1
116CDX G EKC=4E-3 1
116CD G 1029.7 1 13 2 E1
116CDX G EKC=3.6E-4 9
116CD B 15 9 5.7 3
116CDX B EAV=1747.4 19
116CD L 2303.00 22
116CD G 1083.5 2 0.20 2
116CDX G FLAG=B
116CD B 0.81 6 6.93 4
116CDX B EAV=1721.9 19
116CD L 2340.12 12(4-)
116CD CL J$4- from Fig.5 and Table II (2009Ba52).
116CD G 418.3 3 0.06 1
116CDX G FLAG=A
116CD G 423.9 2 0.32 3
116CDX G EKC=7E-3 3
116CD G 1120.7 1 0.77 6
116CD B 0.3 2 7.3 3 ?
116CDX B EAV=1704.3 19
116CD CB LOGFT$8.9 {I3} from Table iv of 2009Ba52, assuming first-forbidden
116CDaCB unique transition. Compilers note that 6- to 4- is not a transition
116CDaCB of this nature. log| {Ift}=7.3 is too low to be realistic for a
116CDaCB |DJ=2, No |b transition
116CD L 2493.71 22
116CD G 1274.2 2 0.04 1
116CDX G FLAG=B
116CD B 0.17 7 7.52 18
116CDX B EAV=1631.6 19
116CD L 2504.04 13(5-)
116CD CL J$5- in Fig.5 and Table II (2009Ba52).
116CD G 254.9 1 2.3 2 M1,E2
116CDX G EKC=3.5E-2 5
116CD G 634.0 2 0.78 7
116CD G 1284.6 2 0.20 2
116CD B 5.9 9 5.97 7
116CDX B EAV=1626.7 19
116CD L 2565.0 3
116CD G 538.3 3 0.035 7
116CDX G FLAG=B
116CD B 0.13 3 7.60 10
116CDX B EAV=1597.8 19
116CD L 2691.16 14(5-)
116CD G 351.2 2 0.09 1 M1
116CDX G FLAG=B$EKC=1.5E-2 3
116CD G 442.0 1 0.23 5
116CDX G FLAG=B
116CD G 664.6 3 1.3 3
116CDX G FLAG=B
116CD B 2.5 5 6.25 9
116CDX B EAV=1538.2 19
116CD L 2693.23 14(7-)
116CD G 443.8 3 1.8 3
116CDX G FLAG=B
116CD G 666.4 2 3.8 6
116CDX G FLAG=B
116CD B 10 5 5.65 22
116CDX B EAV=1537.2 19
116CD L 2699.30 23(5-)
116CD G 450.0 5 0.4 1 M1,E2
116CDX G EKC=7E-3 2
116CD B 1.7 4 6.41 11
116CDX B EAV=1534.4 19
116CD L 2828.91 23(6-)
116CD G 579.8 2 0.3 2
116CDX G EKC=4E-3 2
116CD B 1.1 7 6.5 3
116CDX B EAV=1473.2 19
116CD L 2865.70 16(5-)
116CD G 1646.1 2 0.24 2
116CD B 0.8 3 6.65 17
116CDX B EAV=1455.8 19
116CD L 2877.74 16(6-)
116CD G 186.6 4 0.12 2 M1
116CDX G EKC=8E-2 2
116CD G 373.6 4 0.09 1
116CDX G FLAG=B
116CD G 537.6 6 0.29 3
116CDX G FLAG=B
116CD G 628.6 2 0.67 6
116CDX G EKC=3E-3 1
116CD B 3.9 3 5.96 4
116CDX B EAV=1450.1 19
116CD L 2920.5 10
116CD CL E$from Fig.7 and listed in Table IV ( {+116}Ag{+m1,m2}) not in Table
116CDaCL II ({+116}Ag{+m2} (2009Ba52).
116CD G 1701.0
116CD CG E$from Fig.7 (2009Ba52).
116CD B 0.17 5 7.3 2
116CDX B EAV=1430.0 20
116CD CB IB$from Table IV (2009Ba52).
116CD L 2958.63 14(6-)
116CD G 93.0 2 0.03 1 M1
116CDX G EKC=8E-1 3
116CD G 259.3 2 0.20 8
116CDX G EKC=2E-2 1
116CD G 265.4 1 2.0 1 M1
116CDX G EKC=3.1E-2 3
116CD G 454.1 3 0.54 4
116CDX G FLAG=A$EKC=6E-3 2
116CD G 618.3 3 0.09 1
116CD G 709.7 5 2.6 5
116CDX G FLAG=B
116CD G 932.1 2 0.8 1
116CD B 25 1 5.108 18
116CDX B EAV=1412.0 19
116CD L 3013.55 14(5-,6-)
116CD G 135.6 2 0.05 2 M1
116CDX G FLAG=B$EKC=1.2E-1 3
116CD G 147.7 2 0.012 3 M1,E2
116CDX G EKC=2.3E-1 9
116CD G 320.2 2 0.50 5 M1,E2
116CDX G EKC=1.9E-2 3
116CD G 673.5 2 0.6 1
116CD G 764.7 2 0.27 3
116CDX G FLAG=B
116CD G 987.0 2 0.14 2
116CD B 6.3 7 5.68 5
116CDX B EAV=1386.2 19
116CD L 3088.00 13(7-)
116CD G 129.3 3 0.16 2 M1
116CDX G EKC=1.5E-1 7
116CD G 210.6 3 0.14 3 M1
116CDX G EKC=5E-2 1
116CD G 394.6 2 0.56 5 M1,E2
116CDX G EKC=1.1E-2 2
116CD G 583.9 2 0.86 8 E2
116CDX G EKC=3.8E-3 8
116CD G 839.1 1 0.32 3
116CD G 1061.1 1 0.13 1
116CD B 8.6 7 5.50 4
116CDX B EAV=1351.1 19
116CD L 3130.36 25
116CD G 881.1 3 0.12 2
116CD B 0.4 1 6.81 11
116CDX B EAV=1331.2 19
116CD L 3162.52 23
116CD G 1135.8 2 0.06 1
116CD B 0.25 6 6.99 11
116CDX B EAV=1316.1 19
116CD L 3212.72 23
116CD G 1186.0 2 0.10 2
116CD B 0.40 9 6.76 10
116CDX B EAV=1292.6 19
116CD L 3213.70 22(6+)
116CD G 522.5 5 0.62 7 E1
116CDX G FLAG=B$EKC=2.1E-3 7
116CD G 964.6 2 0.5 1
116CD B 4.6 5 5.70 5
116CDX B EAV=1292.1 19
116CD L 3360.11 17
116CD G 229.6 3 0.03 1
116CDX G FLAG=B$EKC=4E-2 1
116CD G 667.1 5 0.20 7
116CDX G FLAG=B
116CD G 669.0 5 0.3 1
116CDX G FLAG=B
116CD G 1111.1 2 0.45 6
116CD G 1333.3 2 0.11 1
116CD B 4.2 2 5.647 22
116CDX B EAV=1223.5 19
116CD L 3372.0 3
116CD G 1345.3 3 0.07 1
116CDX G FLAG=A
116CD B 0.28 7 6.82 11
116CDX B EAV=1217.9 19
116CD L 3373.3 5
116CD G 1124.2 5 0.11 3
116CDX G FLAG=B
116CD B 0.4 2 6.66 22
116CDX B EAV=1217.3 19
116CD L 3388.0 3
116CD G 559.1 2 0.06 1
116CD B 0.24 5 6.87 9
116CDX B EAV=1210.4 19
116CD L 3486.22 24
116CD CL E$3468.1 listed in Table ii of 2009Ba52 is a misprint
116CD G 1237.1 3 0.05 1
116CD G 1459.5 3 0.08 1
116CDX G FLAG=B
116CD B 0.5 1 6.49 9
116CDX B EAV=1164.5 19
116CD L 3549.75 24
116CD G 1045.7 2 0.29 7
116CD B 1.2 3 6.07 11
116CDX B EAV=1134.8 19
116CD L 3632.7 5
116CD G 1606.0 5 0.06 2
116CDX G FLAG=B
116CD B 0.23 8 6.73 16
116CDX B EAV=1096.2 19
116CD L 3665.02 23
116CD G 1415.9 2 0.16 2
116CDX G FLAG=B
116CD B 0.65 9 6.26 6
116CDX B EAV=1081.2 19