88RB 88KR B- DECAY 1976BU05 14NDS 201401
88RB H TYP=FUL$AUT=E.A. McCutchan and A.A. Sonzogni$CIT=NDS 115, 135 (2014)$
88RB2 H CUT=1-Nov-2013$
88RB c 1976Bu05: {+88}Kr activity from {+235}U(n,F) and subsequent
88RB2c mass-separation and gas-chromatographic-isolation. Measured E|g,
88RB3c I|g, and |g|g using two coaxial Ge(Li) detectors (FWHM=2.5 keV), a
88RB4c Compton-suppressed Ge(Li) detector, and a planar Ge(Li) low-energy
88RB5c photon spectrometer.
88RB c 1976Wo05: {+88}Kr activity from {+235}U(n,f) and subsequent
88RB2c separation by the TRISTAN on-line separator. Measured absolute I|b
88RB3c and I|g using a Ge(Li) detector and plastic scintillator.
88RB c Shapes of |b spectra measured by 1986HeZY.
88RB c Others: 1974WoZO, 1973BlZH, 1973GeZZ, 1970Ly01.
88RB c Total energy release of 2930 keV {I100} is calculated using the
88RB2c RADLST code, in good agreement with the decay Q value of 2918 keV
88RB3c {I3}.
88RB cG $|a(K)exp: from magnetic spectrometer measurement (1973HaZW), except
88RB2cG where noted.
88RB cG E$From 1976Bu05, except where noted
88RB cG RI$From 1976Bu05, normalized to I|g(2392|g)=100.
88RB cL E$From a least-squares fit to E|g by evaluators.
88RB cL J$From the Adopted Levels.
88RB cL E(a)$Level is not adopted
88RB cB IB$From an intensity balance at each level.
88RB D CC$FROM BrIcc v2.3a (30-Jun-2013) 2008Ki07, "Frozen Orbitals" appr.
88KR P 0.0 0+ 2.825 H 19 2918 3
88RB N 0.346 16 0.346 16 1.0 1.0
88RB cN NR$from |S(I(|g+ce) to g.s.)=86 {I4} determined by absolute |b and |g
88RB2cN counting (1976Wo05).
88RB PN 3
88RB G 176.71 17 0.07 2
88RB G 603.21 13 0.12 3
88RB G 1054.54 20 0.09 3
88RB G 1608.01 20 0.20 5
88RB G 1789.14 22 0.13 5
88RB G 1801.3 3 0.11 4
88RB G 2535.52 11 0.12 1
88RB L 0 2-
88RB B 14 4 9.32 13 1U
88RBS B EAV=1235.4 14
88RB L 27.515 9 (3)-
88RB G 27.513 14 5.6 4 M1(+E2) 0.07 +3-7 6.3 5 41.4 4
88RBX G ECC=6.4 5$K/T=0.74 5$L/T=0.106 24$M/T=0.018 5$N/T=0.0019 4$
88RBX G O/T=6.5E-5 5
88RBS G KC=5.4 3$LC=0.78 19$MC=0.13 3$NC=0.014 3$OC=0.000476 18
88RB cG M,MR$from |a(exp).
88RB cG CC,TI$|a(exp) from intensity balance since |b feeding is negligible
88RB2cG for a third-forbidden transition.
88RB L 196.292 8 (1)-
88RB G 168.5 2 0.02 LE
88RB G 196.301 10 75.1 5 M1+E2 0.92 15 0.050 5 C
88RBX G EKC=0.044 4$ELC=0.005 1
88RBS G KC=0.044 5$LC=0.0053 6$MC=0.00088 10$NC=9.7E-5 10$OC=3.6E-6 4
88RB cG E$weighted average of 196.320 {i15} (1976Bu05), 196.288 {i15}
88RB2cG (1973GeZZ), both from Ge(Li), and 196.292 {i17} from curved-crystal
88RB3cG spectrometer (1979Bo26).
88RB cG M,MR$from |a(K)exp.
88RB B 2.0 3 8.67 7
88RBS B EAV=1138.5 15
88RB L 268.24 3 4-
88RB G 240.71 4 0.73 2 C
88RB G 268.24 [E2] 0.0268 0.09 4 S
88RBX G K/T=0.0228 4$L/T=0.00272 4$M/T=0.000448 7$N/T=4.92E-5 7$O/T=1.88E-6 3
88RBS G KC=0.0234 4$LC=0.00279 4$MC=0.000460 7$NC=5.05E-5 7$OC=1.93E-6 3
88RB cG E$from level energy difference.
88RB cG TI$from intensity balance since |b feeding is negligible for
88RB2cG third-unique forbidden transition.
88RB L 362.240 10 (2)-
88RB G 165.98 4 8.97 40 M1+E2 0.74 10 0.077 8 C
88RBX G EKC=0.067 7
88RBS G KC=0.067 7$LC=0.0084 9$MC=0.00138 14$NC=0.000150 15$OC=5.5E-6 5
88RB cG M,MR$from |a(K)exp.
88RB cG EKC$from 1974WoZO (also quoted in 1976Bu05).
88RB cG EKC$Other: 0.029 {I3} (1973HaZW); results in a small negative feeding
88RB2cG of the level.
88RB G 334.71 3 0.42 2 C
88RB G 362.226 13 6.50 16 C
88RB L 390.547 10 (2-)
88RB G 28.26 11 0.08 3 [M1] 5.42 10
88RBS G KC=4.77 9$LC=0.551 10$MC=0.0911 17$NC=0.01022 19$OC=0.000426 8
88RB cG M,CC$|d probably small since a larger |a would result in a large
88RB2cG negative feeding of the 362 level.
88RB G 122.27 6 0.57 2 [E2] 0.463 C
88RBS G KC=0.396 6$LC=0.0566 8$MC=0.00934 14$NC=0.000980 14$OC=3.04E-5 5
88RB G 363.5 5 0.14 9
88RB G 390.543 11 1.86 12 C
88RB B 0.26 10 10.68 17 1U
88RBS B EAV=1053.8 14
88RB L 862.349 9 2-
88RB G 471.80 3 2.10 4 C
88RB G 500.02 6 0.28 2 C
88RB G 665.94 6 0.25 4 C
88RB G 834.83 1 37.5 4 C
88RB G 862.327 19 1.94 5 C
88RB B 1.3 3 9.44 10 1U
88RBS B EAV=837.8 14
88RB L 1141.360 22 1-,2-
88RB G 779.12 8 0.28 6 C
88RB G 944.92 4 0.85 4 C
88RB G 1141.33 6 3.71 9 C
88RB B 0.10 6 9.2 3
88RBS B EAV=698.8 14
88RB L 1182.090 17 (0,1,2)
88RB G 985.780 16 3.80 7 C
88RB B 1.02 7 9.12 3 1U
88RBS B EAV=694.1 14
88RB L 1212.578 21 (1,2)-
88RB G 350.04 19 0.05 2
88RB G 822.01 12 0.26 3 C
88RB G 850.34 5 0.50 3 C
88RB G 1184.95 4 1.99 8 C
88RB G 1212.73 17 0.40 14 C
88RB L 1245.24 4 (2)- ?
88RB G 883.06 14 0.12 2 ? ?
88RB G 1245.22 4 * ?
88RB L 1352.494 22 1-,2-
88RB G 961.83 6 0.24 3 C
88RB G 990.09 9 0.41 5 C
88RB G 1324.98 4 0.46 10 C
88RB G 1352.32 11 0.46 6 C
88RB L 1441.51 3 (1,2-)
88RB G 579.04 14 0.07 3
88RB G 1245.22 4 1.05 5 *C
88RB B 0.22 3 8.54 6
88RBS B EAV=563.4 14
88RB L 1603.83 3 (0-,1-,2-)
88RB G 391.20 10 0.23 12 C
88RB G 421.70 18 0.03 1
88RB G 1603.79 5 1.32 8 C
88RB L 1661.15 4 1-,2-
88RB G 798.65 21 0.08 3
88RB G 1298.78 15 0.27 6
88RB G 1464.84 9 0.33 4
88RB G 1661.3 3 0.26 6
88RB B 0.23 4 8.24 8
88RBS B EAV=466.5 13
88RB L 1714.714 24 0-,1-
88RB G 573.27 6 0.21 2 C
88RB G 1518.39 3 6.22 16 C
88RB B 1.92 12 7.25 3
88RBS B EAV=443.2 13
88RB L 1793.3 3 0-,1-,2- ?
88RB G 1793.3 3 0.10 4 ?
88RB B 0.035 14 8.87 18 ?
88RBS B EAV=409.3 13
88RB L 1915.52 4 (1,2)-
88RB G 311.69 3 0.31 2 C
88RB G 774.14 6 0.28 4
88RB B 0.204 17 8.48 4 1U
88RBS B EAV=378.4 13
88RB L 2089.07 13 a ?
88RB G 1892.76 13 0.40 7 ?
88RB B 0.14 3 7.78 10 ?
88RBS B EAV=285.6 13
88RB L 2231.761 14 1+
88RB G 517.00 8 0.10 3
88RB G 570.57 7 0.18 2
88RB G 790.32 7 0.36 3 C
88RB G 879.51 19 0.07 2
88RB G 1049.48 12 0.41 3 C
88RB G 1090.53 12 0.18 4
88RB G 1369.5 2 4.27 17 C
88RB G 2035.411 18 10.8 3 C
88RB G 2231.772 21 9.80 19
88RB B 9.1 5 5.665 25
88RBS B EAV=228.5 12
88RB L 2392.147 9 1+
88RB G 677.34 5 0.68 4 C
88RB G 731.01 9 0.10 3
88RB G 788.28 4 1.54 4 C
88RB G 950.49 12 0.11 3 C
88RB G 1039.59 3 1.40 5 C
88RB G 1179.51 3 2.88 6 C
88RB G 1209.84 8 0.41 7
88RB G 1250.67 4 3.24 6 C
88RB G 1529.77 3 31.6 5 C
88RB G 2029.84 3 13.09 25 C
88RB G 2195.84 1 38.1 3 C
88RB G 2364.7 3 0.09 4
88RB G 2392.11 4 100.0 3
88RB B 67 4 4.39 3
88RBS B EAV=167.3 12
88RB L 2456.00 16 (0-,1-) ?
88RB G 741.34 18 0.10 3 ?
88RB G 2259.5 3 0.09 4 ?
88RB B 0.066 17 7.20 12 ?
88RBS B EAV=143.9 11
88RB L 2548.420 23 1+
88RB G 1303.09 24 0.19 7
88RB G 1335.81 14 0.19 3 C
88RB G 1406.94 10 0.63 5 C
88RB G 1685.6 4 1.92 21 C
88RB G 2186.5 3 0.83 17 C
88RB G 2352.08 4 2.11 6 C
88RB G 2548.40 3 1.80 3
88RB B 2.65 16 5.27 3
88RBS B EAV=111.2 11
88RB L 2771.11 4 1+
88RB G 1908.7 4 0.29 4 C
88RB G 2408.91 7 0.30 3 C
88RB G 2771.02 5 0.43 2
88RB B 0.353 25 4.85 5
88RBS B EAV=39.79 88