83BR 83SE B- DECAY (22.25 M) 2015Kr02,1974KR27,1973FE0815NDS 201503
83BR H TYP=FUL$AUT=E.A. MCCUTCHAN$CIT=NDS 125, 201 (2015)$CUT=31-Dec-2014$
83BR c 2015Kr02: {+83}Se activity from {+82}Se(n,|g), E=thermal. Measured
83BR2c E|g, I|g, and |g(t) using two HPGe detectors; deduced T{-1/2}.
83BR c 1974Kr27: {+83}Se activity from {+82}Se(n,|g), E=thermal. Measured
83BR2c E|g, I|g, |g|g using two coaxial Ge(Li) detectors
83BR c 1973Fe08: {+83}Se activity from {+82}Se(n,|g), E=thermal. Measured
83BR2c E|g, I|g, |g|g using two Ge(Li) detectors.
83BR c All of the gamma rays observed in 1974Kr27 and 1973Fe08 have been
83BR2c confirmed by 2015Kr02 with the exception of two transitions: a
83BR3c 581.9-keV transition reported by 1973Fe08 was determined to be due to
83BR4c coincidence summing and a 2167-keV transition reported by 1973Fe08
83BR5c was found to be associated with the decay of {+38}Cl.
83BR c Others: 1973BeXW, 1967Ma35, 1962Ba27, 1960Yt03, 1959Co51
83BR c A total energy release of 3770 keV {I30} is calculated for this decay
83BR2c scheme using the RADLST code, compared with the Q value of 3673 keV
83BR3c {I5}. Non-physical negative |b feedings and a large reduced |h{+2}
83BR4c for least-squares fit to |g-ray energies suggests that some aspects
83BR5c of the decay scheme remain unsettled.
83BR cB IB$From |g-ray transition intensity balance
83BR cG E,RI$From 2015Kr02. Intensities from 1974Kr27 and 1973Fe08 are
83BR2cG included in the comments.
83BR cG M,MR$From the Adopted Gammas.
83BR cL E$From a least-squares fit to E|g, by evaluator. Large reduced |h{+2}
83BR2cL suggests incorrect placements in the level scheme or that the
83BR3cL uncertainties are underestimated.
83BR cL J$From the Adopted Levels.
83BR cL T$From the Adopted Levels, except where noted.
83BR cB $Levels at 1352.8, 1701.9, and 2073.4 keV have negative |b{+-}
83BR2cB feedings of -0.53 {I11}, -1.16 {I2}, and -0.73 {I5}, respectively.
83BR D CC$FROM BrIcc v2.3 (29-Mar-2013) 2008Ki07, "Frozen Orbitals" appr.
83SE P 0.0 9/2+ 22.25 M 4 3673 5
83BR N 0.694 5 1.0 1.0 1.0
83BR cN NR$|SI(|g+ce) to g.s.=100. Direct g.s. feeding is not expected with
83BR2cN |DJ=3 and |D|p=yes.
83BR PN 3
83BR G 260.584 22 0.352 13
83BR G 263.68 4 0.295 18
83BR G 502.27 6 0.178 14
83BR G 600.97 3 0.302 13
83BR G 688.32 5 0.172 17
83BR G 708.03 6 0.218 14
83BR G 723.01 3 0.433 18
83BR G 1148.75 5 0.253 12
83BR G 1179.36 5 0.194 11
83BR G 1345.74 5 0.318 15
83BR G 1383.26 6 0.194 15
83BR G 1475.58 2 1.21 2
83BR G 1565.25 6 0.276 11
83BR G 1973.45 3 0.874 17
83BR G 2084.99 3 1.07 2
83BR L 0.0 3/2- 2.374 H 4
83BR L 356.733 6 5/2-
83BR G 356.73 1 100 1 M1(+E2) +0.02 16 0.0042816 C
83BRS G KC=0.00381 14$LC=0.000407 16$MC=6.47E-5 25$NC=6.05E-6 22
83BR B 1.2 9 9.8 4 1U
83BRS B EAV=1428.1 24
83BR L 799.223 7 (5/2,7/2)-
83BR G 442.494 14 1.55 2 C
83BR cG E$1974Kr27 doubly place a 442|g as depopulating the 779- and 3137-keV
83BR2cG levels. The level energy difference from the 779-keV level is 442.5
83BR3cG keV whereas it is 443.5 keV from the 3137-keV level. 2015Kr02 find
83BR4cG that the transition is well fit as a singlet and thus conclude that
83BR5cG its contribution to the placement from the 3137-keV level is
83BR6cG negligible.
83BR G 799.225 10 21.1 2 C
83BR cG RI$others: 19.0 {I5} (1974Kr27), 23.3 {I10} (1973Fe08).
83BR B 1.7 2 9.3 1 1U
83BRS B EAV=1219.9 24
83BR L 866.930 7 7/2-
83BR G 510.204 14 61.7 6 M1(+E2) -0.04 12 0.001844 C
83BRS G KC=0.00164 3$LC=0.000174 4$MC=2.76E-5 6$NC=2.59E-6 5
83BR cG RI$others: 56 {I3} (1974Kr27), 64.6 {I25} (1973Fe08).
83BR G 866.912 17 11.9 1 [E2] 6.45E-4 C
83BRS G KC=0.000574 8$LC=6.10E-5 9$MC=9.68E-6 14$NC=9.01E-7 13
83BR cG RI$others: 10.5 {I2} (1974Kr27), 12.9 {I5} (1973Fe08).
83BR B 1.9 7 7.83 16 ?
83BRS B EAV=1181.7 24
83BR L 988.171 14 1/2-,3/2-
83BR G 988.200 17 1.12 1
83BR cG RI$others: 1.03 {I12} (1974Kr27), 0.9 {I1} (1973Fe08).
83BR L 1030.797 20 (3/2)-
83BR G 673.99 5 0.257 10
83BR cG E$1973Fe08 placed this |g ray in {+83}Se |b{+-} decay (70.1 s) only.
83BR G 1030.80 5 0.321 12
83BR cG E$1973Fe08 placed this |g ray in {+83}Se |b{+-} decay (70.1 s) only.
83BR cG RI$other: 0.32 {I12} (1974Kr27)
83BR L 1092.138 7 9/2+ 4.1 NS 1
83BR cL T$from |g|g(t) in 1967Ma35. Other: 3.65 ns {I9} from |b|g(t) in
83BR2cL 1973BeXW.
83BR G 225.22 1 42.5 8 E1(+M2) -0.07 7 0.008010 C
83BRS G KC=0.0072 9$LC=0.00076 10$MC=0.000120 16$NC=1.11E-5 15
83BR cG RI$others: 48 {I4} (1974Kr27), 46.5 {I20} (1973Fe08).
83BR G 735.375 14 0.90 1 C
83BR cG RI$others: 1.00 {I9} (1974Kr27), 1.2 {I1} (1973Fe08).
83BR B 4.1 6 7.4 1
83BRS B EAV=1075.3 24
83BR L 1238.625 10 (5/2,7/2-)
83BR G 371.671 14 0.858 13
83BR cG RI$others: 0.88 {I8} (1974Kr27), 0.8 {I1} (1973Fe08).
83BR cG E$placed by 1973Fe08 and 1974Kr27 as depopulating the 1810-keV level.
83BR2cG However, E|g differs by more than 12|s from the level energy
83BR3cG difference and thus, 2015Kr02 propose a placement as depopulating the
83BR4cG 1239-keV level.
83BR G 439.39 3 0.265 13
83BR G 881.957 21 1.06 1
83BR G 1238.72 5 0.271 12
83BR cG E,RI$unplaced transition with E|g=1239 {I1} and I|g=0.31 {I6}
83BR2cG observed in 1974Kr27.
83BR B 0.50 3 8.2 1
83BRS B EAV=1006.4 24
83BR L 1352.815 6 (5/2)+
83BR G 322.07 4 0.221 15
83BR cG E,RI$unplaced transition with E|g=322.2 {I3}, I|g=0.10 {I5} observed
83BR2cG in 1973Fe08
83BR cG RI$other: 0.28 {I5} (1974Kr27)
83BR G 485.894 14 3.37 3 C
83BR cG RI$others: 3.5 {I3} (1974Kr27), 3.3 {I2} (1973Fe08).
83BR G 553.608 17 5.14 5 C
83BR cG RI$others: 4.8 {I3} (1974Kr27), 6.2 {I15} (1973Fe08).
83BR G 996.054 14 2.23 2 C
83BR cG RI$others: 1.85 {I15} (1974Kr27), 1.9 {I2} (1973Fe08).
83BR G 1352.799 10 6.80 7 C
83BR cG RI$others: 6.3 {I2} (1974Kr27), 7.0 {I4} (1973Fe08).
83BR L 1421.078 8 (7/2-,5/2+)
83BR G 329.599 18 0.640 14 ?
83BRL G FL=1092.138
83BR cG RI$other: 0.86 {I11} (1974Kr27).
83BR cG E$questionable placement as measured energy disagrees significantly
83BR2cG with level energy difference=328.94 keV; not included in
83BR3cG least-squares fitting.
83BR G 433.03 5 0.237 12
83BR cG RI$other: 0.23 {I6} (1974Kr27).
83BR G 621.796 14 0.905 14 C
83BR cG RI$others: 0.90 {I6} (1974Kr27), 0.6 {I1} (1973Fe08).
83BR G 1064.336 14 7.89 8 C
83BR cG RI$others: 7.3 {I3} (1974Kr27), 8.6 {I4} (1973Fe08).
83BR G 1421.014 20 1.67 2
83BR cG RI$others: 1.64 {I9} (1974Kr27), 1.6 {I1} (1973Fe08).
83BR B 0.44 8 8.1 1
83BRS B EAV=920.9 24
83BR L 1438.972 9 9/2-
83BR G 572.015 10 6.42 6 M1(+E2) -0.07 13 0.001423 C
83BRS G KC=0.001264 25$LC=0.000134 3$MC=2.12E-5 5$NC=1.99E-6 4
83BR cG RI$others: 5.7 {I3} (1974Kr27), 6.5 {I3} (1973Fe08).
83BR G 1082.247 14 4.11 4 E2 3.81E-4 C
83BRS G KC=0.000339 5$LC=3.57E-5 5$MC=5.67E-6 8$NC=5.30E-7 8
83BR cG RI$others: 3.77 {I14} (1974Kr27), 3.9 {I3} (1973Fe08).
83BR B 0.60 8 7.9 1
83BRS B EAV=912.6 24
83BR L 1701.726 17 13/2+
83BR cL E$energy sums involving this level group into two values which differ
83BR2cL by 0.4 keV suggesting this level is possibly a closely spaced doublet
83BR3cL (2015Kr02). Further support for a doublet comes from the negative
83BR4cL |b{+-} feeding intensity derived for this level and the fact that the
83BR5cL 671- and 1702-keV transitions would correspond to E5 or M6
83BR6cL multipolarities given the adopted J|p's of the levels.
83BR G 609.369 14 4.34 4 E2 1.65E-3 C ?
83BRL G FL=1092.138
83BRS G KC=0.001467 21$LC=0.0001585 23$MC=2.51E-5 4$NC=2.33E-6 4
83BR cG RI$others: 4.00 {I15} (1974Kr27), 4.5 {I3} (1973Fe08).
83BR cG E$questionable placement as measured energy disagrees with level
83BR2cG energy difference=609.59 keV; not included in least-squares fitting.
83BR G 670.899 22 0.512 14
83BRL G FL=1030.797
83BR cG RI$other: 0.48 {I9} (1974Kr27).
83BR cG E$adopted J|p's suggest an E5 or M6 multipolarity for this
83BR2cG transition; not included in the adopted levels.
83BR G 1701.79 7 0.251 12 ?
83BR cG E$adopted J|p's suggest an E5 or M6 multipolarity for this
83BR2cG transition; not included in the adopted levels.
83BR cG RI$other: 0.31 {I8} (1974Kr27).
83BR L 1804.485 8 (7/2)
83BR G 451.666 10 1.47 2 C
83BR cG RI$others: 1.42 {I11} (1974Kr27), 1.2 {I1} (1973Fe08).
83BR G 712.344 10 4.63 5 C
83BR cG RI$others: 4.63 {I15} (1974Kr27), 3.9 {I2} (1973Fe08).
83BR G 1447.73 3 0.788 15
83BR cG RI$others: 0.68 {I11} (1974Kr27), 0.7 {I1} (1973Fe08).
83BR B 2.98 5 6.9 1
83BRS B EAV=743.3 23
83BR L 1810.398 7 (7/2+)
83BR G 389.293 15 0.945 13 C
83BR cG RI$others: 0.94 {I8} (1974Kr27), 0.9 {I1} (1973Fe08).
83BR G 457.592 10 5.08 5 C
83BR cG RI$others: 4.8 {I3} (1974Kr27), 5.1 {I3} (1973Fe08).
83BR G 718.253 10 21.2 2 M1+E2 -0.12 10 8.56E-414 C
83BRS G KC=0.000762 12$LC=8.03E-5 13$MC=1.275E-5 21$NC=1.196E-6 19
83BR cG RI$others: 19.0 {I6} (1974Kr27), 23.8 {I10} (1973Fe08).
83BR G 943.480 15 1.09 1 C
83BR cG RI$others: 1.22 {I6} (1974Kr27), 1.3 {I1} (1973Fe08).
83BR B 0.4 2 7.77 22
83BRS B EAV=740.6 23
83BR L 2058.787 9 (5/2+,7/2,9/2+)
83BR G 705.94 3 0.453 15
83BR cG RI$others: 0.60 {I6} (1974Kr27), 0.3 {I1} (1973Fe08).
83BR G 966.74 5 0.251 13
83BR cG RI$other: 0.39 {I11} (1974Kr27)
83BR G 1191.861 14 6.30 6 C
83BR cG RI$others: 5.7 {I2} (1974Kr27), 6.1 {I3} (1973Fe08).
83BR G 1259.603 14 1.43 1 C
83BR cG RI$others: 1.30 {I9} (1974Kr27), 1.3 {I1} (1973Fe08).
83BR B 0.56 7 7.4 1
83BRS B EAV=627.5 23
83BR L 2073.408 10 (5/2-,7/2-)
83BR G 634.55 4 0.187 14
83BR G 652.26 5 0.195 11
83BR G 834.789 14 1.21 2
83BR G 1085.264 22 0.890 15
83BR G 1206.46 4 0.707 18
83BR cG E,RI$unplaced transition with E|g=1206.9 {I2} and I|g=1.3 {I1}
83BR2cG observed in 1973Fe08.
83BR G 1274.20 4 0.261 12
83BR G 2073.35 5 0.490 14
83BR cG E,RI$unplaced transition with E|g=2072.4 {I7} and I|g=0.4 {I1}
83BR2cG observed in 1973Fe08; unplaced transition with E|g=2075 {I2} and
83BR3cG I|g=0.5 {I1} observed in 1974Kr27.
83BR L 2134.502 13 11/2+
83BR cL E$level included by the evaluator since placement of the 1042|g is
83BR2cL known from ({+7}Li,|a2n|g).
83BR G 1042.392 14 1.89 2
83BR cG E$placement by evaluator based on data in ({+7}Li,|a2n|g). Placement
83BR2cG is supported by observed coincidences with 225|g and 356|g in
83BR3cG 1974Kr27. The 1042|g is unplaced in both 1974Kr27 and 1973Fe08.
83BR cG RI$others: 1.82 {I8} (1974Kr27), 1.5 {I1} (1973Fe08).
83BR B 0.60 2 7.3 2
83BRS B EAV=593.3 23
83BR L 2398.068 11 9/2+,7/2+
83BR G 593.580 14 1.09 1
83BR cG RI$others: 1.03 {I6} (1974Kr27), 1.1 {I1} (1973Fe08).
83BR G 1305.930 23 1.07 2 C
83BR cG RI$others: 0.97 {I11} (1974Kr27), 0.8 {I1} (1973Fe08).
83BR G 1531.09 6 0.290 12
83BR cG RI$other: 0.311 {I12} (1974Kr27)
83BR B 0.94 2 6.7 1
83BRS B EAV=476.3 22
83BR L 2531.592 11
83BR G 472.82 4 0.243 12
83BR cG E,RI$unplaced transition with E|g=473 {I1}, I|g=0.25 {I5} observed in
83BR2cG 1974Kr27.
83BR cG RI$other: 0.21 {I5} (1973Fe08).
83BR G 1092.538 14 0.491 18
83BR cG E$1974Kr27 place a 1093 {I1} transition with I|g=0.39 {I12} from the
83BR2cG 1091.9-keV level. This, however, results in an energy mismatch of
83BR3cG 10|s.
83BR G 1110.44 3 0.739 18
83BR cG E,RI$unplaced transition with E|g=1110.2 {I9}, I|g=0.71 {I5} observed
83BR2cG in 1974Kr27.
83BR cG RI$other: 0.6 {I1} (1973Fe08).
83BR G 1664.66 3 0.732 17
83BR cG E,RI$unplaced transition with E|g=1665 {I2}, I|g=0.80 {I9} observed
83BR2cG in 1974Kr27.
83BR cG RI$other: 0.8 {I1} (1973Fe08).
83BR G 2174.95 7 0.157 10
83BR B 0.05 LT 7.8 GT ?
83BRS B EAV=418.2 22
83BR L 2647.187 8 (7/2)+
83BR G 573.71 7 0.187 14
83BR G 836.797 10 16.6 2 C
83BR cG RI$others: 15.4 (1974Kr27), 23.2 {I10} (1973Fe08).
83BR G 1208.22 4 0.681 18 C
83BR cG E,RI$other: unresolved doublet (I|g=1.1) with an unplaced 1206.9|g
83BR2cG (1974Kr27).
83BR G 1226.124 14 1.94 2 C
83BR cG RI$others: 1.87 {I9} (1974Kr27), 1.8 {I2} (1973Fe08).
83BR G 1294.324 14 3.31 5
83BR cG RI$other: 2.4 {I5} (1973Fe08).
83BR G 1408.73 9 0.124 12
83BR G 1555.019 14 3.71 4 C
83BR cG RI$others: 3.4 {I3} (1974Kr27), 3.7 {I2} (1973Fe08).
83BR G 1780.218 21 3.65 4 C
83BR cG RI$others: 3.1 {I3} (1974Kr27), 2.8 {I4} (1973Fe08).
83BR G 1847.970 18 1.48 2
83BR cG RI$others: 1.57 {I14} (1974Kr27), 1.0 {I1} (1973Fe08).
83BR G 2290.398 18 12.6 1 C
83BR cG RI$others: 12.0 {I12} (1974Kr27), 13.5 {I5} (1973Fe08).
83BR B 30.7 3 4.8 1
83BRS B EAV=368.8 22
83BR L 2694.305 8 (7/2)+
83BR G 296.232 23 0.412 15
83BR cG RI$others: 0.5 {I3} (1974Kr27), 0.4 {I1} (1973Fe08).
83BR G 559.99 5 0.220 12
83BR G 636.57 3 0.561 14 ?
83BRL G FL=2058.787
83BR cG RI$other: 0.6 {I3} (1974Kr27)
83BR cG E$questionable placement as measured energy disagrees significantly
83BR2cG with level energy difference=635.52 keV; not included in
83BR3cG least-squares fitting.
83BR G 883.897 10 10.7 1 C
83BR cG RI$others: 10.2 {I2} (1974Kr27), 11.3 {I5} (1973Fe08).
83BR G 889.85 3 0.427 15
83BR G 992.37 4 0.311 13
83BR cG RI$other: 0.5 {I3} (1974Kr27)
83BR G 1341.498 10 7.84 8 C
83BR cG RI$others: 7.1 {I2} (1974Kr27), 8.3 {I4} (1973Fe08).
83BR G 1455.66 5 0.395 15
83BR cG E,RI$unplaced transition with E|g=1456 {I2} and I|g=0.43 {I11}
83BR2cG observed in 1974Kr27.
83BR G 1827.318 23 2.21 2
83BR cG RI$others: 1.85 {I15} (1974Kr27), 2.0 {I2} (1973Fe08).
83BR G 1895.053 17 10.7 1 C
83BR cG RI$others: 10.5 {I9} (1974Kr27), 11.3 {I5} (1973Fe08).
83BR G 2337.529 19 4.69 5 C
83BR cG RI$others: 4.6 {I5} (1974Kr27), 5.0 {I3} (1973Fe08).
83BR B 26.3 2 4.9 1
83BRS B EAV=348.9 21
83BR L 2738.382 8 (9/2)+
83BR G 340.316 16 0.684 14 C
83BR cG RI$others: 0.69 {I9} (1974Kr27), 0.6 {I1} (1973Fe08).
83BR G 603.91 6 0.169 12
83BR G 665.007 14 4.80 5
83BR cG E,RI$unplaced transitions with E|g=665.0 {I3} and I|g=4.3 {I2}
83BR2cG observed in 1974Kr27. 1973Fe08 place a transition with E|g=664.8 {I1}
83BR3cG and I|g=4.7 {I3} as depopulating a level at 1021 keV.
83BR G 679.578 14 1.70 2 C
83BR cG RI$others: 1.39 {I8} (1974Kr27), 1.6 {I1} (1973Fe08).
83BR G 928.02 8 0.211 12
83BR cG RI$other: 0.31 {I11} (1974Kr27)
83BR G 933.878 15 1.08 1
83BR cG RI$others: 1.03 {I8} (1974Kr27), 1.0 {I1} (1973Fe08).
83BR G 1036.45 4 0.495 15
83BR cG RI$others: 0.54 {I11} (1974Kr27), 0.3 {I1} (1973Fe08).
83BR G 1299.419 14 7.63 8 C
83BR cG RI$others: 6.9 {I2} (1974Kr27), 8.5 {I4} (1973Fe08).
83BR G 1317.259 14 6.25 6 C
83BR cG RI$others: 5.6 {I2} (1974Kr27), 6.0 {I6} (1973Fe08).
83BR G 1385.35 6 0.377 15
83BR cG RI$other: 0.54 {I14} (1974Kr27)
83BR G 1646.17 5 0.319 10
83BR cG RI$other: 0.65 {I11} (1974Kr27)
83BR G 1871.493 19 2.49 2 C
83BR cG RI$others: 2.3 {I2} (1974Kr27), 2.1 {I2} (1973Fe08).
83BR B 16.4 2 5.0 1
83BRS B EAV=330.5 21
83BR L 2777.114 22 (7/2,9/2)
83BR G 1684.94 3 0.657 15 C
83BR cG E,RI$unplaced transition with E|g=1684.2 {I10}, I|g=0.3 {I1} observed
83BR2cG in 1973Fe08.
83BR cG RI$other: 0.65 {I8} (1974Kr27)
83BR G 2420.36 3 0.641 10 C
83BR cG E,RI$unplaced transition with E|g=2419.9 {I4}, I|g=0.6 {I1} observed
83BR2cG in 1973Fe08.
83BR cG RI$other: 0.60 {I8} (1974Kr27)
83BR B 0.90 1 6.2 1
83BRS B EAV=314.4 21
83BR L 2946.784 9 9/2+,11/2+
83BR G 208.40 1 2.54 5 C
83BR cG RI$others: 2.9 {I3} (1974Kr27), 2.7 {I2} (1973Fe08).
83BR G 415.112 14 2.33 2
83BR cG RI$other: unplaced transition with E|g= 415.2 {I5} and I|g=2.32 {I15}
83BR2cG observed in 1974Kr27
83BR G 812.311 19 0.641 13
83BR cG E$placed by evaluator after introducing the 2134-keV level found in
83BR2cG ({+7}Li,|a2n|g). |g not placed by 1974Kr27.
83BR cG RI$other: 0.54 {I6} (1974Kr27)
83BR G 888.031 10 5.68 6 C
83BR cG RI$others: 5.2 {I2} (1974Kr27), 6.9 {I3} (1973Fe08).
83BR G 1136.21 6 0.199 10
83BR G 1245.38 2 1.06 1 C ?
83BRL G FL=1701.726
83BR cG RI$others: 0.96 {I6} (1974Kr27), 1.0 {I1} (1973Fe08).
83BR cG E$questionable placement as measured energy disagrees with level
83BR2cG energy difference=1245.06 keV; not included in least-squares fitting.
83BR G 1507.81 3 0.685 16
83BR cG RI$other: 0.73 {I8} (1974Kr27)
83BR G 1854.607 23 2.78 3 C
83BR cG RI$others: 2.8 {I3} (1974Kr27), 2.2 {I2} (1973Fe08).
83BR B 10.3 1 4.8 1
83BRS B EAV=245.4 20
83BR L 3137.825 16 9/2+,11/2+
83BR G 1436.179 21 1.38 2 C
83BRL G FL=1701.726
83BR cG E,RI$unplaced transition with E|g=1435.8 {I3}, I|g=1.2 {I1} observed
83BR2cG in 1973Fe08
83BR cG RI$other: 1.28 {I9} (1974Kr27)
83BR G 1716.61 3 0.965 16 ?
83BRL G FL=1421.078
83BR cG E$placement from 1974Kr27. Alternate placement by 1973Fe08 is from
83BR2cG the 2737-keV level, however, this results in population of a 1021-keV
83BR3cG level, the existence of which could not be confirmed by 2015Kr02.
83BR4cG Thus, the placement of 1974Kr27 is adopted here.
83BR cG RI$others: 0.94 {I9} (1974Kr27), 0.9 {I3} (1973Fe08).
83BR G 2045.624 21 1.37 2 C
83BR cG E,RI$unplaced transition with E|g=2045.2 {I5}, I|g=1.0 {I1} observed
83BR2cG in 1973Fe08
83BR cG RI$other: 1.39 {I15} (1974Kr27)
83BR B 1.91 2 5.0 1
83BRS B EAV=171.5 19