86SR 86Y EC DECAY (14.74 H) 2020GU18 25NDS 202507
86SR H TYP=FUL$AUT=A. Negret and B. Singh$CIT=NDS 203, 283 (2025)$
86SR2 H CUT=20-Jan-2025$
86SR c 2020Gu18: {+86}Y produced in (p,n) reaction by irradiating 96.4%
86SR2c enriched {+86}Sr (as {+86}SrCO{-3}) with 16-MeV protons from the
86SR3c University of Wisconsin Medical Physics cyclotron, followed by
86SR4c a chemical procedure to extract {+86}Y radionuclide with a purity of
86SR5c 98.3%. The |g-ray measurement started at the Argonne National
86SR6c Laboratory, 24 hours after the irradiation and follow up chemistry.
86SR7c Measured E|g, I|g, |g|g- and |g|g|g-coin, |g|g(|q) using the
86SR8c Gammasphere array with 32 HPGe detectors at ANL. A total of
86SR9c 206 |g rays were reported, placed among 53 levels, with 20 new levels.
86SR c 2022Ud01 (also 2023UdZZ): {+86}Y produced in (p,n) reaction by
86SR2c irradiating {+86}SrCO{-3} powder at E{-p}=7, 8 MeV using the BC 1710
86SR3c cyclotron of FZJ, Germany. Measured |g and X rays and deduced
86SR4c %|e=72.8 {i20} and %|b{++}=27.2 {i20} using %I|g data from 2020Gu18.
86SR c 1984Ak02: measured |g|g(|q) for 15 |g|g cascades using Ge(Li)-NaI(Tl)
86SR2c detectors.
86SR c 1975Be59: measured |g|g(|q) for two |g|g cascades using NaI(Tl)
86SR2c detectors.
86SR c 1970Ra06 (also 1969Ra08): {+86}Y source prepared in {+86}Sr(p,n),E=12
86SR2c MeV reaction at ORNL lab cyclotron using 96.7% enriched {+86}Sr (as
86SR3c {+86}SrCO{-3}), followed by a chemical procedure to extract {+86}Y
86SR4c activity. Measured E|g, I|g using several Ge(Li) detectors, |g|g-coin
86SR5c using Ge(Li)-Ge(Li) and Ge(Li)-NaI(Tl) combinations, and conversion
86SR6c electrons using Vanderbilt iron-free double-focusing |b-ray
86SR7c spectrometer. A total of 105 |g rays reported, placed among 31 levels
86SR8c up to 4954 keV, based on extensive |g|g-coin data. The decay scheme
86SR9c was significantly modified from the one proposed by 1969Ar25. Only one
86SRAc level at 3942 keV was not confirmed by 2020Gu18.
86SR c 1970Ar03: measured |g|g(|q) for five |g|g cascades using
86SR2c Ge(Li)-NaI(Tl) detectors.
86SR c 1969Ar25: measured E|g, I|g. Total of 85 |g rays reported. Strong
86SR2c |g rays agree in energy and intensity with those from 2020Gu18
86SR c 1965Va02: measured E|g, I|g, ce, E|b, I|b, |b|g- and |g|g-coin,
86SR2c |g|g(|q), |b-shape factors. A total of 25 |g rays from 189 to 2583
86SR3c keV reported from internal conversion measurements. Gamma-ray data
86SR4c in singles and coincidence were obtained using NaI(Tl) detectors
86SR c 1962Ya01: measured E|b, I|b, internal and external conversion
86SR2c electrons using sector-type double-focusing |b-ray spectrometer,
86SR3c |b shape factor, |g rays in singles, coincidence and |g|g(|q) using
86SR4c NaI(Tl) detectors. A total of 21 |g rays reported from 181 to 2580
86SR5c placed among 13 excited states up to 4932 keV. The |g|g(|q)
86SR6c measurements were made for seven |g|g cascades using NaI(Tl) detectors
86SR c T{-1/2}({+86}Y decay): 1972Em01, 1951Ca46, 1951Hy24
86SR c Theory for {+86}Y decay: 2017Ko05
86SR cE TI,IE$From 2020Gu18, based on in-out transition intensity balances.
86SR cG $A 702.2 {I6} unplaced |g with I|g=0.3 {I1} in 1970Ra06 is omitted
86SR2cG as it is not reported in 2020Gu18
86SR cG $Following 16 weak |g rays were reported by 1969Ar25 only:
86SR2cG 241.7 {I5} (1.01 {I16}), 815.5 {I15} (1.5 {I5}), 909.7 {I5} (2.0 {I5}),
86SR3cG 928 {I1} (1.6 {I4}), 1782 {I1} (0.1), 2043 {I2} (0.1), 2164 {I2}
86SR4cG (0.10 {I5}), 2190 {I3} (0.10 {I3}), 2228 {I3} (|<0.1), 2298 {I2} (0.1),
86SR5cG 2558 {I2} (0.10 {I7}), 2859 {I3} (0.3 {I1}), 3025 {I5} (0.09),
86SR6cG 3795 {I5} (0.10 {I3}) and 3918 {I5} (0.56). Some of these |g rays were
86SR7cG placed in a level scheme proposed by 1969Ar25, but none has been
86SR7cG confirmed from the detailed |g|g-coin data of 2020Gu18, thus
86SR8cG omitted here.
86SR cG $Although not explicitly specified, evaluators assume that all the
86SR2cG |g-ray placements in 2020Gu18 are from their |g|g-coin data,
86SR2cG except for a few g.s. transitions from levels with no feeding from
86SR3cG higher levels
86SR cG E,RI$From 2020Gu18. A minimum systematic uncertainty of 2% was
86SR2cG considered by the authors and added in quadrature to the statistical
86SR3cG uncertainties
86SR cG M,MR$From |g|g(|q) data in 2020Gu18, unless specified otherwise.
86SR cL $A level at 4339 keV proposed by 1970Ra06 was not confirmed by 2020Gu18
86SR2cL as the authors did not observe in singles or coincidences a very weak
86SR3cL 1154.0 {I15} |g in 1970Ra06 from this level
86SR cL $Levels at 2558, 3507, 4871 and 4994 keV proposed in a level scheme by
86SR2cL 1969Ar25 are omitted here, as none is confirmed in later studies by
86SR3cL 1970Ra06 and 2020Gu18 using detailed |g|g-coin data. |g rays
86SR4cL from these levels have either been reassigned to other levels or
86SR5cL their existence not confirmed. In addition, placements of many other
86SR6cL |g rays in the decay scheme of 1969Ar25 have been reassigned by
86SR7cL 1970Ra06 and 2020Gu18.
86SR cL E$From 2020Gu18, deduced by authors from least-squares fit to E|g data.
86SR2cL Evaluators deduce reduced |h{+2}=0.96 from the same least-squares fit
86SR3cL as in 2020Gu18, with only four |g rays deviating between 2 and 3
86SR4cL sigmas.
86SR cL J,T$From the Adopted Levels
86SR N 0.827 14 1.0
86SR cN NR$|S(I(|g+ce) of |g rays to g.s.)=100. Direct feeding to g.s.
86SR2cN is highly forbidden.
86SR PN 3
86Y P 0.0 4- 14.74 H 2 5240 14
86Y cP J,T$From {+86}Y Adopted Levels
86Y cP QP$from 2021Wa16
86Y cP $%|e=72.8 {i20} %|b{++}=27.2 {i20} (2022Ud01)
86SR L 0.0 0+ STABLE
86SR L 1076.63 5 2+ 1.46 PS +9-8
86SR E 0.5 LT0.08 LT10.9 GT 0.6 LT 1U
86SRS E EAV=1428 6$CK=0.1127 31$CL=0.01348 37$CM+=0.00305 7
86SR cE TI$0.6 {I20} from |g-transition intensity balance.
86SR cE $Measured E|b=3153 {I40} (1965Va02), 3130 {I30} (1962Ya01); I|b=0.6
86SR2cE (1965Va02,1962Ya01). Shape=2, yes (1965Va02,1962Ya01)
86SR G 1076.66 9 100 2 E2 4.89E-4 C
86SR2 G EKC=0.00041 4 (1970Ra06) $
86SR cG $K/LM=7.1 {I5} (1962Ya01)
86SR2 G %IG=82.7 4
86SR cG $E|g=1076.63 {I10}, I|g=100, Ice(K)=100 (1970Ra06)
86SR cG $E|g=1076 {I1}, I|g=100 (1969Ar25)
86SR cG $Ice(K)=100, Ice(L+M)=14.0 {I10} (1962Ya01)
86SRS G KC=0.000433 6$LC=4.70E-5 7$MC=7.89E-6 11
86SRS G NC=9.90E-7 14$OC=6.41E-8 9
86SR L 1853.90 5 2+ 193 FS 30
86SR E 0.4 LT0.2 LT10.1 GT 0.8 LT 1U
86SRS E EAV=1072 6$CK=0.242 7$CL=0.0290 8$CM+=0.00657 15
86SR cE TI$from |g-transition intensity balance in 2020Gu18. From |b{++}
86SR2cE spectra in 1965Va02 and 1962Ya01 , the |b{++} feeding of 0.6% to the
86SR3cE g.s. is definite.
86SR cE $Measured E|b=2335 {I40} (1965Va02), 2320 {I50} (1962Ya01); I|b=1.3
86SRxcE (1965Va02), 0.6 (1962Ya01)
86SR G 777.14 8 26.2 7 M1+E2 +0.33 5 9.75E-414 C
86SR2 G %IG=21.7 7
86SR2 G EKC=0.00093 8 (1970Ra06)$ EKC=0.00101 16 (1970Ra06)$
86SR cG $K/LM=9.2 {I16} (1962Ya01)
86SRS G KC=0.000864 12$LC=9.36E-5 14$MC=1.572E-5 23
86SRS G NC=1.977E-6 28$OC=1.295E-7 18
86SR cG MR$from |g|g(|q) (2020Gu18). Other: +0.251 {I17} (1984Ak02)
86SR cG $E|g=777.37 {I10}, I|g=27.2 {I7}, Ice(K)=59 {I5} (1970Ra06)
86SR cG $E|g=778.5 {I5}, I|g=26.0 {I15} (1969Ar25)
86SR cG $Ice(K)=53 {I3}, Ice(L+M)=5.7 {I10} (1962Ya01)
86SR cG $(777|g)(1077|g)(|q): A{-2}=+0.065 {I15}, A{-4}=+0.02 {I3} (1984Ak02)
86SR cG $(777|g)(1077|g)(|q): A{-2}=+0.040 {I23}, A4=+0.017 {I37} (1970Ar03)
86SR cG $(777|g)(1077|g)(|q): A{-2}=+0.007 {I21}, A4=+0.039 {I39} (1962Ya01)
86SR G 1853.82 8 20.4 4 E2 3.98E-4 6 C
86SR2 G %IG=16.9 4
86SR2 G EKC=0.000147 23 (1970Ra06)
86SRS G KC=0.0001423 20$LC=1.522E-5 21$MC=2.55E-6 4
86SRS G NC=3.21E-7 4$OC=2.114E-8 30$IPC=0.0002379 33
86SR cG $E|g=1854.38 {I13}, I|g=20.8 {I6}, Ice(K)=7.1 {I11} (1970Ra06)
86SR cG $E|g=1854.5 {I15}, I|g=22.4 {I16} (1969Ar25)
86SR cG $Ice(K)=8.0 {I5} (1962Ya01)
86SR L 2229.50 5 4+ 1.73 PS 21
86SR E 3.7 70.9 5 7.74 9 4.6 9
86SRS E EAV=881 6$CK=0.167 5$CL=0.0199 6$CM+=0.00450 12
86SR cE $Measured E|b=2019 {I20} (1965Va02), 1960 {I20} (1962Ya01); I|b=4.6
86SR2cE (1965Va02), 3.9 (1962Ya01)
86SR G 1152.82 8 37.0 9 E2(+M3) 0.00016LT 4.23E-4 6 C
86SR2 G %IG=30.6 9
86SR2 G EKC=0.000373 26 (1970Ra06)$
86SR cG $K/LM=9.5 {I3} (1962Ya01)
86SR cG MR$|d(M3/E2)=-0.034 {I8} (2020Gu18) gives too large a B(M3)(W.u.)
86SR2cG value; For B(M3)(W.u.)<10 from RUL, |d(M3/E2)<0.00016
86SRS G KC=0.000373 5$LC=4.05E-5 6$MC=6.79E-6 10
86SRS G NC=8.52E-7 12$OC=5.54E-8 8$IPC=3.02E-6 4
86SR cG $E|g=1153.05 {I10}, I|g=37.0 {I11}, Ice(K)=32 {I2} (1970Ra06)
86SR cG $E|g=1153.0 {I15}, I|g=37 {I1} (1969Ar25)
86SR cG $Ice(K)=33 {I3}, Ice(L+M)=4.0 {I10} (1962Ya01)
86SR cG $(1153|g)(1077|g)(|q) measured in 2020Gu18 agrees with 4|)2|)0
86SR2cG spin sequence, with mult=Q (or E2) for both the transitions
86SR cG $(1153|g)(1077|g)(|q): A{-2}=+0.089 {I15}, A{-4}=+0.01 {I3} (1984Ak02)
86SR cG $(1153|g)(1077|g)(|q): A{-2}=+0.107 {I13}, A{-4}=+0.006 {I20}
86SR2cG (1970Ar03)
86SR cG $(1153|g)(1077|g)(|q): A{-2}=+0.093 {I13}, A{-4}=+0.154 {I24}
86SR2cG (1965Va02)
86SR cG $(1153|g)(1077|g)(|q): A{-2}=+0.097 {I17}, A{-4}=+0.005 {I40}
86SR2cG (1962Ya01)
86SR L 2481.48 5 3- 0.90 PS 7
86SR E 2.8 71.0 6 7.60 10 3.8 9
86SRS E EAV=766 6$CK=0.231 7$CL=0.0276 9$CM+=0.00624 17
86SR G 251.86 8 0.482 12 E1 0.0069210 C
86SR2 G %IG=0.398 12
86SR2 G EKC=0.0040 8 (1970Ra06)
86SRS G KC=0.00612 9$LC=0.000667 9$MC=0.0001115 16
86SRS G NC=1.389E-5 19$OC=8.75E-7 12
86SR cG $E|g=252.05 {I13}, I|g=0.45 {I2}, Ice(K)=4.2 {I8} (1970Ra06)
86SR cG $E|g=251.5 {I15}, I|g=0.31 {I3} (1969Ar25)
86SR cG M$from |a(K) data in 1970Ra06.
86SR G 627.50 8 39.8 9 E1(+M2) 0.0076 LT 6.60E-410 C
86SR2 G %IG=32.9 9
86SR2 G EKC=0.00061 4 (1970Ra06) $ EKC=0.00058 8 (1970Ra06)
86SR cG MR$|d(M2/E1)=+0.017 {I6} (2020Gu18) results in B(M2)(W.u.) too large;
86SR2cG From B(M2)(W.u.)<1 from RUL, |d(M2/E1)<0.0076.
86SRS G KC=0.000586 8$LC=6.31E-5 9$MC=1.057E-5 15
86SRS G NC=1.326E-6 19$OC=8.60E-8 12
86SR cG $E|g=627.72 {I10}, I|g=39.5 {I12}, Ice(K)=56 {I3} (1970Ra06)
86SR cG $E|g=627.7 {I15}, I|g=35.1 {I22} (1969Ar25)
86SR cG $Ice(K)=42 {I2} (1962Ya01)
86SR cG $(628|g)(1854|g)(|q): A{-2}=-0.123 {I10}, A{-4}=+0.02 {I1} (1984Ak02)
86SR cG $(628|g)(777|g)(|q): A{-2}=-0.129 {I5}, A{-4}=-0.041 {I9} (1984Ak02)
86SR cG $(628|g)[777|g](1077|g)(|q): A{-2}=-0.049 {I21}, A{-4}=+0.005 {I20}
86SRxcG (1984Ak02)
86SR cG $(628|g)[777|g](1077|g)(|q): A{-2}=-0.004 {I24}, A{-4}=+0.044 {I38}
86SR2cG (1970Ar03)
86SR G 1405.01 11 0.310 10 C
86SR2 G %IG=0.256 9
86SR cG $E|g=1404.8 {I4}, I|g=0.22 {I6} (1970Ra06)
86SR G 2481.30 10 0.179 6 [E3] 4.95E-4 7 C
86SR2 G %IG=0.148 6
86SRS G KC=0.0001327 19$LC=1.424E-5 20$MC=2.390E-6 33
86SRS G NC=3.01E-7 4$OC=1.981E-8 28$IPC=0.000345 5
86SR cG $E|g=2482.08 {I17}, I|g=0.14 {I1} (1970Ra06)
86SR cG $E|g=2485 {I2}, I|g=0.2 {I1} (1969Ar25)
86SR L 2641.15 5 2+ 87 FS 19
86SR E 0.004 LT0.006 LT11.2 GT 0.01 LT 1U?
86SRS E EAV=718 6$CK=0.535 10$CL=0.0645 12$CM+=0.01463 25
86SR G 1564.48 8 0.140 15 M1+E2 -0.49 22 3.19E-4 5 C
86SR2 G %IG=0.116 13
86SRS G KC=0.0001992 28$LC=2.131E-5 30$MC=3.57E-6 5
86SRS G NC=4.50E-7 6$OC=2.97E-8 4$IPC=9.39E-5 31
86SR cG $E|g=1564.4 {I5}, I|g=0.22 {I6} (1970Ra06, uncertain assignment to
86SR2cG {+86}Y decay)
86SR cG MR$From Adopted Levels, Gammas, based on |g|g(|q) in {+87}Rb(p,2n|g)
86SR2cG (2017Du08).
86SR G 2641.15 8 0.226 25 E2 7.01E-410 C
86SR2 G %IG=0.187 21
86SRS G KC=7.57E-5 11$LC=8.04E-6 11$MC=1.348E-6 19
86SR cG $E|g=2641.9 {I4}, I|g=0.20 {I5} (1970Ra06)
86SR cG $E|g=2643 {I2}, I|g=0.26 {I8} (1969Ar25)
86SRS G NC=1.698E-7 24$OC=1.123E-8 16$IPC=0.000616 9
86SR L 2672.44 5 5- 5 NS LT
86SR E 3.42 40 1.78 45 7.29 5 5.2 6
86SRS E EAV=679 6$CK=0.299 9$CL=0.0356 11$CM+=0.00806 21
86SR cE $Measured E|b=1603 {I20} (1965Va02), 1600 {I50} (1962Ya01).
86SR2cE I|b=6.3 (1965Va02), 5.8 (1962Ya01)
86SR G 190.81 11 1.074 25 E2 0.0957 14 C
86SR2 G %IG=0.888 26
86SR2 G EKC=0.098 7 (1970Ra06)
86SRS G KC=0.0829 12$LC=0.01071 15$MC=0.001800 26
86SRS G NC=0.0002162 31$OC=1.134E-5 16
86SR cG $E|g=190.80 {I13}, I|g=1.23 {I4}, Ice(K)=280 {I20} (1970Ra06)
86SR cG $E|g=190.0 {I5}, I|g=1.6 {I3} (1969Ar25)
86SR cG M$from |a(K) data in 1970Ra06.
86SR G 442.84 8 18.7 6 E1+M2 +0.019 10 1.53E-3 2 C
86SR2 G %IG=15.5 6
86SR2 G EKC=0.00129 8 (1970Ra06)$
86SR cG $K/LM=9.1 {I15} (1962Ya01)
86SRS G KC=0.001352 19$LC=0.0001462 21$MC=2.450E-5 35
86SRS G NC=3.07E-6 4$OC=1.971E-7 28
86SR cG $E|g=443.13 {I10}, I|g=20.48 {I59}, Ice(K)=61.5 {I35} (1970Ra06)
86SR cG $E|g=442 {I1}, I|g=21.8 {I12} (1969Ar25)
86SR cG $Ice(K)=54 {I5}, Ice(L+M)=5.9 {I10} (1962Ya01)
86SR cG $(443|g)(1153|g)(|q): A{-2}=-0.017 {I9}, A{-4}=+0.008 {I16} (1984Ak02)
86SR cG $(443|g)[1153|g](1077|g)(|q): A{-2}=-0.016 {I13}, A{-4}=+0.001 {I22}
86SR2cG (1984Ak02)
86SR cG $(443|g)[1153|g](1077|g)(|q): A{-2}=-0.012 {I18}, A{-4}=-0.005 {I29}
86SR2cG (1970Ar03)
86SR G 1595.93 12 0.322 10 E3 4.33E-4 6 C
86SR2 G %IG=0.266 9
86SRS G KC=0.000336 5$LC=3.67E-5 5$MC=6.16E-6 9
86SRS G NC=7.74E-7 11$OC=5.02E-8 7$IPC=5.29E-5 7
86SR L 2787.30 8 2+ 25 FS 12
86SR E 0.0349 30 0.079 8 9.957 38 0.114 9 1U
86SRS E EAV=653 6$CK=0.605 10$CL=0.0731 12$CM+=0.01656 24
86SR G 1710.7 2 0.181 6 M1+E2 -0.26 13 3.36E-4 5 C
86SR2 G %IG=0.150 6
86SRS G KC=0.0001678 24$LC=1.791E-5 25$MC=3.00E-6 4
86SRS G NC=3.79E-7 5$OC=2.506E-8 35$IPC=0.0001469 28
86SR cG $E|g=1711.6 {I7}, I|g=0.21 {I4} (1970Ra06)
86SR cG $E|g=1710 {I1}, I|g=0.20 {I5} (1969Ar25)
86SR cG MR$From Adopted Levels, Gammas, based on |g|g(|q) in {+87}Rb(p,2n|g)
86SR2cG (2017Du08).
86SR G 2787.3 2 0.070 7 E2 7.60E-411 C
86SR2 G %IG=0.058 6
86SRS G KC=6.91E-5 10$LC=7.33E-6 10$MC=1.229E-6 17
86SRS G NC=1.549E-7 22$OC=1.025E-8 14$IPC=0.000683 10
86SR cG $E|g=2790.0 {I10}, I|g=0.013 {I7} (1970Ra06)
86SR L 2856.62 8 6+ 5 NS LT
86SR E 0.013 13 0.037 48 10.2 GT 0.05 5 1U?
86SRS E EAV=622 6$CK=0.637 10$CL=0.0771 12$CM+=0.01747 23
86SR G 627.23 15 0.78 5 E2 1.90E-3 3 C
86SR2 G %IG=0.64 4
86SRS G KC=0.001678 24$LC=0.0001874 26$MC=3.15E-5 4
86SRS G NC=3.92E-6 5$OC=2.461E-7 34
86SR L 2877.90 5 3+ 110 FS +53-49
86SR cL J$|g|g(|q) (2020Gu18) gives J=3 and rejects J=4
86SR E 0.44 17 0.36 25 7.91 16 0.80 30
86SRS E EAV=587 6$CK=0.393 11$CL=0.0469 13$CM+=0.01062 26
86SR G 648.53 8 0.424 12 C
86SR2 G %IG=0.350 12
86SR cG $E|g=648.6 {I10}, I|g: very weak (1970Ra06)
86SR G 1023.94 8 4.7 3 M1+E2 +0.42 3 5.35E-4 7 C
86SR2 G %IG=3.88 26
86SR2 G EKC=0.00041 4 (1970Ra06)
86SRS G KC=0.000474 7$LC=5.11E-5 7$MC=8.58E-6 12
86SRS G NC=1.080E-6 15$OC=7.10E-8 10
86SR cG $E|g=1024.04 {I10}, I|g=4.6 {I2}, Ice(K)=4.4 {I4} (1970Ra06)
86SR cG $E|g=1024 {I1}, I|g=4.9 {I11} (1969Ar25)
86SR cG $Ice(K)=5.2 {I10} (1962Ya01)
86SR cG $(1023|g)(1854|g)(|q) measured in 2020Gu18 agrees with 3|)2|)0
86SR2cG spin sequence, not with 4|)2|)0
86SR G 1801.23 8 2.15 6 M1+E2 +7.2 13 3.82E-4 5 C
86SR2 G %IG=1.78 6
86SR2 G EKC=0.00013 4 (1970Ra06)
86SRS G KC=0.0001503 21$LC=1.608E-5 23$MC=2.70E-6 4
86SRS G NC=3.39E-7 5$OC=2.232E-8 31$IPC=0.0002130 30
86SR cG $E|g=1801.70 {I10}, I|g=2.00 {I6}, Ice(K)=0.6 {I2} (1970Ra06)
86SR cG $E|g=1801 {I2}, I|g=1.8 {I6} (1969Ar25)
86SR cG $(1801|g)(1077|g)(|q) measured in 2020Gu18 agrees with 3|)2|)0
86SR2cG spin sequence, not with 4|)2|)0
86SR L 2996.81 5 3-
86SR cL $An 1142.3 {I10} |g with I|g=0.12 {I4} in 1970Ra06 with uncertain
86SR2cL assignment to {+86}Y decay and placed tentatively from 2997 level is
86SR3cL not confirmed by 2020Gu18 from |g|g-coin data, with an upper limit of
86SR4cL intensity stated as <0.0083.
86SR E 10.39 45 11.5 5 6.361 19 21.9 7
86SRS E EAV=534 6$CK=0.458 12$CL=0.0547 14$CM+=0.01239 28
86SR cE $Measured E|b=1248 {I15} (1965Va02), 1180 {I60} (1962Ya01);
86SR2cE I|b=14.0 (1965Va02), 18 (1962Ya01)
86SR G 355.67 8 0.315 10 [E1] 0.00269 4 C
86SR2 G %IG=0.260 9
86SR cG $E|g=355.07 {I26}, I|g=0.12 {I3} (1970Ra06)
86SR G 515.3 1 3.78 12 M1,E2 0.0029 5 C
86SR2 G %IG=3.12 11
86SR2 G EKC=0.0026 5 (1970Ra06)$
86SR cG $K/LM=8.6 {I20} (1962Ya01)
86SRS G KC=0.0026 4$LC=0.00029 5$MC=4.8E-5 8
86SRS G NC=6.0E-6 10$OC=3.8E-7 5
86SR cG $E|g=515.18 {I20}, I|g=5.93 {I17}, Ice(K)=36 {I7} (1970Ra06)
86SR cG $Ice(K)=36 {I3}, Ice(L+M)=4.2 {I10} (1962Ya01)
86SR cG M$from |a(K)exp in 1970Ra06.
86SR G 767.20 10 1.85 6 C
86SR2 G %IG=1.53 6
86SR cG $E|g=767.63 {I13}, I|g=2.9 {I4} from |g|g-coin (1970Ra06)
86SR cG $E|g=769 {I1}, I|g=3.4 {I14} (1969Ar25)
86SR G 1920.12 8 26.4 6 E1+M2 +0.035 4 6.47E-4 9 C
86SR2 G %IG=21.8 6
86SR2 G EKC=0.000072 14 (1970Ra06)
86SRS G KC=7.26E-5 10$LC=7.69E-6 11$MC=1.288E-6 18
86SR cG $E|g=1920.72 {I13}, I|g=25.2 {I8}, Ice(K)=4.2 {I8} (1970Ra06)
86SR cG $E|g=1920 {I1}, I|g=30 {I2} (1969Ar25)
86SR cG $Ice(K)=6.5 {I5} (1962Ya01)
86SR cG $(1921|g)(1077|g)(|q): A{-2}=-0.120 {I23}, A{-4}=+0.03 {I5} (1984Ak02)
86SR cG $(1921|g)(1077|g)(|q): A{-2}=+0.041 {I8}, A{-4}=+0.019 {I20} (1975Be59)
86SR cG $(1921|g)(1077|g)(|q): A{-2}=-0.008 {I32}, A{-4}=-0.046 {I50}
86SR2cG (1970Ar03)
86SR cG $(1921|g)(1077|g)(|q): A{-2}=-0.073 {I11}, A{-4}=+0.005 {I21}
86SR2cG (1965Va02)
86SR cG $(1921|g)(1077|g)(|q): A{-2}=-0.074 {I13}, A{-4}=+0.05 {I3} (1962Ya01)
86SRS G NC=1.622E-7 23$OC=1.071E-8 15$IPC=0.000566 8
86SR G 2997.02 20 0.0457 28 E3 6.42E-4 9 C
86SR2 G %IG=0.0378 24
86SRS G KC=9.23E-5 13$LC=9.86E-6 14$MC=1.653E-6 23
86SRS G NC=2.083E-7 29$OC=1.376E-8 19$IPC=0.000538 8
86SR cG $E|g=2997.6 {I5}, I|g=0.010 {I5} (1970Ra06)
86SR L 3055.45 6 5- 5 NS LT
86SR E 0.40 7 0.52 14 7.68 8 0.92 16
86SRS E EAV=508 6$CK=0.493 12$CL=0.0589 15$CM+=0.01334 29
86SR G 382.76 14 3.03 10 M1+E2 -0.09 6 0.00498 9 C
86SR2 G %IG=2.50 9
86SRS G KC=0.00440 8$LC=0.000485 9$MC=8.15E-5 15
86SR cG $E|g=382.86 {I23}, I|g=4.40 {I14} (1970Ra06)
86SRS G NC=1.023E-5 18$OC=6.65E-7 11
86SR G 825.83 13 4.40 12 E1(+M2) -0.01 3 3.64E-4 6 C
86SR2 G %IG=3.64 12
86SR2 G EKC=0.00032 11 (1970Ra06)
86SRS G KC=0.000323 5$LC=3.46E-5 6$MC=5.81E-6 9
86SR cG $E|g=826.02 {I13}, I|g=4.0 {I1}, Ice(K)=3 {I1} (1970Ra06)
86SR cG $E|g=827.0 {I5}, I|g=4.1 {I18} (1969Ar25)
86SR cG $(826|g)(1153|g)(|q): A{-2}=-0.060 {I16}, A{-4}=+0.11 {I27} (1984Ak02)
86SR cG $(826|g)[1153|g](1077|g)(|q): A{-2}=-0.066 {I21}, A{-4}=+0.01 {I4}
86SRxcG (1984Ak02)
86SRS G NC=7.29E-7 12$OC=4.76E-8 8
86SR L 3133.50 10 (3,4+)
86SR E 0.0429 22 0.0701 33 8.520 20 0.1130 40
86SRS E EAV=474 6$CK=0.541 12$CL=0.0646 15$CM+=0.01464 29
86SR G 2056.84 8 0.137 4 C
86SR2 G %IG=0.113 4
86SR cG $E|g=2058 {I12}, I|g=0.37 {I13} (1969Ar25)
86SR L 3175.50 10 (3,4+)
86SR E 0.0241 14 0.0449 26 8.696 23 0.0690 30
86SRS E EAV=456 6$CK=0.567 12$CL=0.0678 15$CM+=0.01536 29
86SR G 2098.84 8 0.083 3 C
86SR2 G %IG=0.0686 27
86SR L 3184.75 6 3- 5 NS LT
86SR cL J$previous assignment of J=3 confirmed in |g|g(|q) data (2020Gu18)
86SR E 3.22 25 6.3 5 6.548 31 9.5 6
86SRS E EAV=451 6$CK=0.573 12$CL=0.0685 15$CM+=0.01551 29
86SR cE $Measured E|b=1043 {I20}, I|b=4.6 (1965Va02)
86SR G 129.1 2 0.0428 12 [E2] 0.399 6 C
86SR2 G %IG=0.0354 12
86SR G 187.79 14 1.58 5 (M1) 0.0297 4 C
86SR2 G %IG=1.31 5
86SR2 G EKC=0.021 4 (1970Ra06)$
86SR cG $K/LM=5.7 {I6} (1962Ya01)
86SRS G KC=0.0262 4$LC=0.00295 4$MC=0.000496 7
86SR cG $E|g=187.87 {I13}, I|g=1.53 {I5}, Ice(K)=73 {I15} (1970Ra06)
86SR cG $E|g=187.8 {I5}, I|g=1.2 {I4} (1969Ar25)
86SR cG $Ice(K)=113 {I10}, Ice(L+M)=20 {I2} (1962Ya01) for 181-keV transition
86SRS G NC=6.21E-5 9$OC=3.99E-6 6
86SR cG M$E1 or M1 from |a(K) data in 1970Ra06; |DJ|p requires M1.
86SR G 306.76 8 4.04 12 E1+M2 -0.08 3 0.0042120 C
86SR2 G %IG=3.34 11
86SR2 G EKC=0.0040 4 (1970Ra06)
86SRS G KC=0.00373 17$LC=0.000407 21$MC=6.82E-5 35
86SRS G NC=8.5E-6 4$OC=5.40E-7 27
86SR cG $E|g=307.00 {I10}, I|g=4.2 {I1}, Ice(K)=39.5 {I35} (1970Ra06)
86SR cG $E|g=306.5 {I5}, I|g=3.4 {I5} (1969Ar25)
86SR G 512.42 8 2.56 8 C
86SR2 G %IG=2.12 8
86SR cG $E|g=512.42 {I16} (from level-energy difference), I|g: very weak
86SR2cG (1970Ra06)
86SR G 703.12 8 18.9 5 M1+E2 +0.54 21 1.25E-3 3 C
86SR2 G %IG=15.6 5
86SR2 G EKC=0.00099 5 (1970Ra06)$
86SR cG $K/LM=8.9 {I16} (1962Ya02)
86SRS G KC=0.001104 27$LC=0.0001203 33$MC=2.02E-5 5
86SR cG $E|g=703.33 {I10}, I|g=18.7 {I5}, Ice(K)=43 {I2} (1970Ra06)
86SR cG $E|g=703.8 {I5}, I|g=18.7 {I43} (1969Ar25)
86SR cG $Ice(K)=49 {I2}, Ice(L+M)=5.5 {I10} (1962Ya01)
86SR cG $(703|g)(628|g)(|q): A{-2}=-0.088 {I4}, A{-4}=-0.024 {I9} (1984Ak02)
86SRS G NC=2.54E-6 7$OC=1.65E-7 4
86SR cG MR$Others: 0.14, from |a(K)=0.00107 (1965Va02). From |a(K)=0.00099
86SR2cG {i5} (1970Ra06) and K/LM=8.9 {i16} (1962Ya02), |d |? 0.
86SR G 955.22 9 1.42 5 C
86SR2 G %IG=1.17 5
86SR cG $E|g=955.35 {I20}, I|g=1.26 {I5} (1970Ra06)
86SR cG $E|g=955.3 {I5}, I|g=1.0 {I7} (1969Ar25)
86SR G 2108.22 12 0.090 4 C
86SR2 G %IG=0.0744 35
86SR cG $E|g=2108.87 {I33}, I|g=0.06 {I1} (1970Ra06)
86SR cG $E|g=2110 {I2}, I|g=0.05 {I2} (1969Ar25)
86SR L 3290.88 6 6- 5 NS LT
86SR cL $An 503.0 {I4} |g with I|g=0.11 {I4} in 1970Ra06, placed from
86SR2cL 3291 level is not confirmed by 2020Gu18 from |g|g-coin data
86SR E 0.0046 39 0.06 5 9.7 GT 0.06 5 1U?
86SR cE $This |e decay branch is highly unlikely for |DJ=2, |D|p=no
86SRS E EAV=430 6$CK=0.8027 49$CL=0.0976 6$CM+=0.02215 16
86SR G 235.23 10 0.49 3 M1+E2 0.031 14 C
86SR2 G %IG=0.405 26
86SRS G KC=0.027 12$LC=0.0033 16$MC=5.5E-4 27
86SRS G NC=6.7E-5 32$OC=3.9E-6 16
86SR cG $E|g=235.37 {I23}, I|g=0.48 {I2} (1970Ra06)
86SR cG $E|g=234.0 {I5}, I|g=0.35 {I5} (1969Ar25)
86SR G 434.21 8 0.147 22 E1+M2 -0.39 +26-320.0031 23 C
86SR2 G %IG=0.122 18
86SRS G KC=0.0027 20$LC=3.1E-4 24$MC=5.E-5 4
86SRS G NC=6.E-6 5$OC=4.1E-7 32
86SR cG MR$From Adopted Levels, Gammas, based on |g|g(|q) in {+87}Rb(p,2n|g)
86SR2cG (2017Du08).
86SR G 618.45 8 0.225 20M1+E2 0.0017919 C
86SR2 G %IG=0.186 17
86SRS G KC=0.00158 16$LC=0.000175 20$MC=2.94E-5 34
86SR cG $E|g=618.24 {I40}, I|g=0.26 {I4} (1970Ra06)
86SRS G NC=3.7E-6 4$OC=2.35E-7 21
86SR L 3317.54 6 4-
86SR cL J$from |g|g(|q) data (2020Gu18) which agree with J=4 not J=5
86SR E 1.52 9 4.70 15 6.613 18 6.22 18
86SRS E EAV=393 6$CK=0.656 12$CL=0.0785 14$CM+=0.01779 28
86SR G 132.6 2 0.262 10 [M1+E2] 0.22 15 C
86SR2 G %IG=0.217 9
86SR cG $E|g=132.34 {I10}, I|g=0.20 {I1} (1970Ra06)
86SR G 439.59 12 1.03 3 C
86SR2 G %IG=0.851 29
86SR cG $E|g=439.5 {I3}, I|g=0.24 {I8} (1970Ra06)
86SR G 644.98 9 3.14 10(M1+E2) 0.27 6 1.48E-3 2 C
86SR2 G %IG=2.60 9
86SR cG $K/LM=9.0 {I22} (1962Ya01)
86SRS G KC=0.001312 20$LC=0.0001428 22$MC=2.40E-5 4
86SRS G NC=3.01E-6 5$OC=1.970E-7 29
86SR cG $E|g=644.82 {I24} from level-energy difference, I|g=2.65 {I40} from
86SR2cG |g|g-coin, Ice(K)=37.5 {I25} for 644.82|g+645.87|g, the latter being
86SR3cG about four times more intense than the 644.82|g, |a(K)exp=0.00117 {I8}
86SR4cG for the doublet (1970Ra06)
86SR cG $Ice(K)=34 {I2}, Ice(L+M)=3.8 {I10} (1962Ya01)
86SR cG M,MR$+0.27 {I6} or -1.2 {I3} from |g|g(|q) data in 1984Ak02.
86SR cG $(645|g)(443|g)(|q): A{-2}=+0.146 {I10}, A{-4}=-0.021 {I17} (1984Ak02)
86SR cG $(645|g)[443|g](1153|g)(|q): A{-2}=+0.103 {I20}, A{-4}=+0.005 {I33}
86SR2cG (1984Ak02)
86SR G 835.94 8 5.01 15 M1+E2 +1.0 4 8.57E-420 C
86SR2 G %IG=4.14 14
86SR2 G EKC=0.00064 5 (1970Ra06)
86SRS G KC=0.000758 17$LC=8.26E-5 22$MC=1.39E-5 4
86SRS G NC=1.74E-6 4$OC=1.129E-7 23
86SR cG $E|g=835.67 {I22} from level-energy difference, I|g=5.3 {I7} from
86SR2cG |g|g-coin, Ice(K)=10.5 {I7} for 833.7|g+835.6|g (1970Ra06)
86SR cG $E|g=837.0 {I5}, I|g=5 {I1} (1969Ar25)
86SR cG $Ice(K)=14 {I2} (1962Ya01)
86SR cG $(836|g)(627|g)(|q) measured in 2020Gu18 agrees with 4|)3|)2
86SR2cG spin sequence, not with 5|)3|)2
86SR G 1088.08 16 0.163 6 C
86SR2 G %IG=0.135 5
86SR cG $E|g=1087.6 {I5}, I|g=0.05 {I1} (1970Ra06)
86SR L 3361.39 6 4+
86SR E 0.097 6 0.350 12 7.719 19 0.447 14
86SRS E EAV=374 6$CK=0.683 11$CL=0.0817 13$CM+=0.01851 27
86SR G 688.76 11 0.120 4 E1 5.36E-4 8 C
86SR2 G %IG=0.099 4
86SRS G KC=0.000475 7$LC=5.11E-5 7$MC=8.56E-6 12
86SRS G NC=1.074E-6 15$OC=6.98E-8 10
86SR cG $E|g=689.29 {I25}, I|g=0.21 {I4} (1970Ra06)
86SR G 1131.85 15 0.171 5 M1+E2 +0.22 11 4.34E-4 6 C
86SR2 G %IG=0.141 5
86SRS G KC=0.000383 5$LC=4.12E-5 6$MC=6.91E-6 10
86SRS G NC=8.71E-7 12$OC=5.74E-8 8$IPC=1.348E-6 30
86SR cG $E|g=1133.3 {I10}, I|g=0.36 {I3} (1970Ra06)
86SR G 1507.48 8 0.438 13 E2(+M3) -0.03 15 3.27E-418 C
86SR2 G %IG=0.362 12
86SRS G KC=0.000213 18$LC=2.29E-5 20$MC=3.84E-6 33
86SRS G NC=4.8E-7 4$OC=3.16E-8 27$IPC=8.71E-5 26
86SR cG $E|g=1507.86 {I10}, I|g=0.43 {I5} (1970Ra06)
86SR cG $E|g=1510 {I1}, I|g=0.3 {I1} (1969Ar25)
86SR cG MR$From Adopted Levels, Gammas, based on |g|g(|q) in {+87}Rb(p,2n|g)
86SR2cG (2017Du08).
86SR G 2284.61 18 0.0279 11 C
86SR2 G %IG=0.0231 10
86SR L 3389.62 8 (2+,3,4+)
86SR cL J$no assignment in 2020Gu18
86SR E 0.00274 40 0.0111 18 9.21 6 0.0138 18
86SRS E EAV=362 6$CK=0.699 11$CL=0.0837 13$CM+=0.01896 26
86SR G 1535.81 15 0.0247 8 C
86SR2 G %IG=0.0204 7
86SR G 2312.87 12 0.0493 15 C
86SR2 G %IG=0.0408 14
86SR cG $E|g=2314 {I3}, I|g=0.4 {I3} (1969Ar25, intensity in disagreement)
86SR L 3430.12 10 2+
86SR E 0.00176 17 0.0402 13 9.715 24 0.0420 13 1U
86SRS E EAV=369 6$CK=0.8334 33$CL=0.10162 43$CM+=0.02307 14
86SR G 2353.7 2 0.0533 15 C
86SR2 G %IG=0.0441 14
86SR G 3429.94 20 0.0008910 E2 1.01E-3 1 C
86SR2 G %IG=0.00074 8
86SRS G KC=4.92E-5 7$LC=5.20E-6 7$MC=8.72E-7 12
86SRS G NC=1.099E-7 15$OC=7.29E-9 10$IPC=0.000954 13
86SR L 3490.86 10 (3,4+)
86SR E 0.0125 11 0.0795 38 8.299 23 0.0920 40
86SRS E EAV=318 6$CK=0.753 9$CL=0.0902 11$CM+=0.02044 23
86SR G 1261.09 18 0.0555 15 D+Q -0.26 24 C
86SR2 G %IG=0.0459 15
86SR cG MR$From Adopted Levels, Gammas, based on |g|g(|q) in {+87}Rb(p,2n|g)
86SR2cG (2017Du08).
86SR G 1636.9 2 0.0602 15 C
86SR2 G %IG=0.0498 15
86SR G 2414.17 14 0.041 2 C
86SR2 G %IG=0.0339 17
86SR L 3499.53 6 4-
86SR cL J$from |g|g(|q) (2020Gu18)
86SR E 0.042 6 0.286 40 7.74 6 0.328 40
86SRS E EAV=314 6$CK=0.757 9$CL=0.0907 11$CM+=0.02055 22
86SR G 181.77 11 0.118 4 [M1+E2] 0.07 4 C
86SR2 G %IG=0.098 4
86SR cG $E|g=182.34 {I20}, I|g=0.13 {I4} (1970Ra06, uncertain assignment to
86SR2cG {+86}Y decay)
86SR G 443.70 25 0.977 25 C
86SR2 G %IG=0.808 25
86SR cG $E|g=444.18 {I23}, I|g=0.78 {I20} from |g|g-coin (1970Ra06)
86SR G 1018.05 12 0.256 10 C
86SR2 G %IG=0.212 9
86SR cG $E|g=1017.93 {I23}, I|g=0.22 {I14} (1970Ra06)
86SR G 1270.05 10 0.780 20 E1(+M2) -0.05 9 2.51E-4 9 C
86SR2 G %IG=0.645 24
86SRS G KC=0.000144 9$LC=1.53E-5 10$MC=2.57E-6 16
86SRS G NC=3.23E-7 20$OC=2.12E-8 13$IPC=8.93E-5 19
86SR cG $E|g=1270.16 {I13}, I|g=0.79 {I12} (1970Ra06)
86SR cG $E|g=1273 {I1}, I|g=0.56 {I21} (1969Ar25)
86SR cG $(1270|g)(1153|g)(|q) measured in 2020Gu18 agrees with 4|)4|)2
86SR2cG spin sequence
86SR L 3555.40 6 (5+)
86SR cL J$(5) in 2020Gu18
86SR E 0.133 12 1.171 38 7.097 19 1.304 40
86SRS E EAV=291 6$CK=0.783 8$CL=0.0938 9$CM+=0.02126 20
86SR cE $Measured E|b=650 {I60}, I|b=2.4 (1962Ya01)
86SR G 237.68 10 0.154 5 [E1] 0.0081512 C
86SR2 G %IG=0.127 5
86SR cG $E|g=237.9 {I3}, I|g=0.16 {I3} (1970Ra06)
86SR G 264.29 10 0.54 3 [E1] 0.0064 9 C
86SR2 G %IG=0.446 26
86SR cG $E|g=264.53 {I13}, I|g=0.65 {I3} (1970Ra06)
86SR cG $E|g=263.0 {I6}, I|g=0.63 {I21} (1969Ar25)
86SR G 698.84 8 0.575 16 C
86SR2 G %IG=0.475 15
86SR G 882.93 8 0.497 15 3.18E-4 C
86SR2 G %IG=0.411 14
86SR cG $E|g=882.96 {I17}, I|g=0.3 {I1} (1970Ra06)
86SRS G KC=0.000282 4$LC=3.02E-5 5$MC=5.06E-6 7
86SRS G NC=6.36E-7 9$OC=4.15E-8 6
86SR G 1325.93 15 0.0115 5 C
86SR2 G %IG=0.0095 4
86SR L 3644.44 6 3-
86SR cL J$(3-) in 2020Gu18
86SR E 0.334 35 4.92 9 6.426 17 5.25 10
86SRS E EAV=252 6$CK=0.816 6$CL=0.0979 7$CM+=0.02219 17
86SR G 144.8 1 0.0155 10 [M1+E2] 0.16 11 C
86SR2 G %IG=0.0128 9
86SR cG $E|g=144.5 {I3}, I|g=0.038 {I4} (1970Ra06)
86SR G 214.37 12 0.0034012 [E1] 0.0109316 C
86SR2 G %IG=0.00281 11
86SR G 857.11 8 0.103 4 C
86SR2 G %IG=0.085 4
86SR G 1163.03 8 1.56 5 M1+E2(+E0) 4.14E-4 6 C
86SR2 G %IG=1.29 5
86SR2 G EKC=0.0014 8 (1970Ra06)
86SRS G KC=0.000364 5$LC=3.92E-5 6$MC=6.58E-6 11
86SRS G NC=8.27E-7 13$OC=5.42E-8 8$IPC=3.4E-6 5
86SR cG $E|g=1163.03 {I10}, I|g=1.43 {I5}, Ice(K)=4.7 {I25} (1970Ra06)
86SR cG $E|g=1164 {I1}, I|g=1.6 {I5} (1969Ar25)
86SR cG $Ice(K)=4 {I2} (1962Ya01)
86SR G 1414.95 15 0.382 12 C
86SR2 G %IG=0.316 11
86SR cG $E|g=1415.20 {I23}, I|g=0.40 {I11} (1970Ra06)
86SR cG $E|g=1416.5 {I15}, I|g=0.5 {I2} (1969Ar25)
86SR cG $Ice(K)=0.7 {I5} (1962Ya01) for a 1428 line
86SR G 1790.57 12 1.45 4 E1+M2 -0.16 7 5.58E-4 9 C
86SR2 G %IG=1.20 4
86SRS G KC=8.6E-5 6$LC=9.1E-6 6$MC=1.53E-6 10
86SRS G NC=1.93E-7 13$OC=1.27E-8 8$IPC=0.000461 12
86SR cG $E|g=1790.90 {I10}, I|g=1.21 {I5} (1970Ra06)
86SR cG $E|g=1791 {I2}, I|g=1.6 {I5} (1969Ar25)
86SR cG M,MR$from |g|g(|q) in 1984Ak02.
86SR cG $(1791|g)(1854|g)(|q): A{-2}=-0.20 {I5}, A{-4}=+0.06 {I9} (1984Ak02)
86SR G 2567.85 15 2.86 10 (E1+M2) +0.187 14 1.03E-3 2 C
86SR2 G %IG=2.36 9
86SRS G KC=5.02E-5 8$LC=5.31E-6 9$MC=8.90E-7 15
86SRS G NC=1.121E-7 19$OC=7.42E-9 12$IPC=0.000972 14
86SR cG $E|g=2567.97 {I18}, I|g=2.73 {I13} (1970Ra06)
86SR cG $E|g=2568 {I1}, I|g=3.2 {I4} (1969Ar25)
86SR cG $Ice(K)=0.6 {I5} (1962Ya01) for 2580 keV
86SR cG M,MR$from |g|g(|q) in 1984Ak02.
86SR cG $(2568|g)(1077|g)(|q): A{-2}=+0.08 {I4}, A{-4}=-0.03 {I7} (1984Ak02)
86SR cG $(2568|g)(1077|g)(|q): A{-2}=+0.065 {I9}, A{-4}=+0.002 {I10} (1975Be59)
86SR L 3686.41 6 3-
86SR E 0.083 10 1.62 6 6.885 22 1.70 6
86SRS E EAV=234 6$CK=0.8289 49$CL=0.0995 6$CM+=0.02255 16
86SR G 1204.87 10 0.084 9 C
86SR2 G %IG=0.069 8
86SR G 1457.02 10 0.113 4 C
86SR2 G %IG=0.093 4
86SR cG $E|g=1460 {I1}, I|g=0.3 (1969Ar25)
86SR G 1832.27 14 0.183 8 C
86SR2 G %IG=0.151 7
86SR G 2609.76 8 1.69 6 E1+M2 +0.040 18 1.07E-3 2 C
86SR2 G %IG=1.40 5
86SRS G KC=4.63E-5 7$LC=4.88E-6 7$MC=8.18E-7 12
86SRS G NC=1.031E-7 15$OC=6.82E-9 10$IPC=0.001018 14
86SR cG $E|g=2610.11 {I20}, I|g=1.50 {I9} (1970Ra06)
86SR cG $E|g=2611 {I1}, I|g=2.1 {I2} (1969Ar25)
86SR G 3686.5 3 0.0018010 [E3] 8.53E-412 C
86SR2 G %IG=0.00149 9
86SRS G KC=6.31E-5 9$LC=6.72E-6 9$MC=1.127E-6 16
86SRS G NC=1.420E-7 20$OC=9.41E-9 13$IPC=0.000782 11
86SR L 3765.15 6 (4)- 5 NS LT
86SR E 0.301 42 10.55 16 6.023 18 10.85 17
86SRS E EAV=201 6$CK=0.8473 34$CL=0.10182 43$CM+=0.02307 13
86SR G 121.0 2 0.00180 9 [M1+E2] 0.30 21 C
86SR2 G %IG=0.00149 8
86SR G 209.68 11 0.0902 24 [E1] 0.0116517 C
86SR2 G %IG=0.0746 23
86SR cG $E|g=209.80 {I23}, I|g=0.48 {I2} (1970Ra06, uncertain assignment to
86SR2cG {+86}Y decay)
86SR cG $E|g=209.0 {I5}, I|g=0.17 {I2} (1969Ar25)
86SR G 265.59 11 0.130 4 [M1+E2] 0.021 9 C
86SR2 G %IG=0.107 4
86SR G 375.52 10 0.0387 12 C
86SR2 G %IG=0.0320 11
86SR G 403.75 10 0.0645 19 C
86SR2 G %IG=0.0533 18
86SR G 447.61 8 0.206 8 C
86SR2 G %IG=0.170 7
86SR cG $E|g=448.10 {I2}, uncertainty is probably 0.20, I|g=0.09 {I3}
86SR2cG (1970Ra06, uncertain assignment to {+86}Y decay)
86SR G 474.32 12 0.017 4 C
86SR G 580.32 8 5.81 15(M1) 1.86E-3 3 C
86SR2 G %IG=4.80 15
86SR2 G EKC=0.00134 19 (1970Ra06)$
86SR cG $K/LM=7.1 {I28} (1962Ya01)
86SRS G KC=0.001646 23$LC=0.0001791 25$MC=3.01E-5 4
86SRS G NC=3.78E-6 5$OC=2.477E-7 35
86SR cG $E|g=580.57 {I10}, I|g=5.80 {I17}, Ice(K)=18.0 {I25} (1970Ra06)
86SR cG $E|g=581.5 {I5}, I|g=5.90 {I55} (1969Ar25)
86SR cG $Ice(K)=19 {I2}, Ice(L+M)=2.7 {I10} (1962Ya01)
86SR cG M$from |a(K)exp (1970Ra06).
86SR G 709.69 8 3.54 10M1,E2 0.001279 C
86SR2 G %IG=2.93 10
86SR2 G EKC=0.00102 27 (1970Ra06)
86SR cG $E|g=709.90 {I10}, I|g=3.18 {I9}, Ice(K)=7.5 {I20} (1970Ra06)
86SR cG $E|g=711.0 {I5}, I|g=1.8 {I12} (1969Ar25)
86SR cG $Ice(K)=5.3 {I10} (1962Ya01)
86SRS G KC=0.00112 8$LC=0.000123 10$MC=2.07E-5 17
86SRS G NC=2.59E-6 20$OC=1.67E-7 10
86SR cG M$from |a(K)exp (1970Ra06).
86SR G 768.15 15 0.997 25 C
86SR2 G %IG=0.824 25
86SR cG $E|g=768.25 {I16} from level-energy difference, I|g=0.39 {I13} from
86SR2cG |g|g-coin (1970Ra06)
86SR G 887.33 8 0.698 21 C
86SR2 G %IG=0.577 20
86SR cG $E|g=887.40 {I17}, I|g=0.53 {I5} (1970Ra06)
86SR cG $E|g=888, I|g=1.2 {I8} (1969Ar25)
86SR G 1092.61 8 1.06 3 C
86SR2 G %IG=0.876 29
86SR cG $E|g=1092.68 {I13}, I|g=0.84 {I5} (1970Ra06)
86SR cG $E|g=1092 {I1}, I|g=0.99 {I26} (1969Ar25)
86SR G 1283.78 10 0.327 10 C
86SR2 G %IG=0.270 9
86SR cG $E|g=1283.96 {I13}, I|g=0.35 {I13} (1970Ra06)
86SR cG $E|g=1283 {I1}, I|g=0.2 {I1} (1969Ar25)
86SR G 1535.70 10 0.120 4 C
86SR2 G %IG=0.099 4
86SR cG $E|g=1535.67 {I13}, I|g=0.14 {I4} (1970Ra06)
86SR cG $E|g=1536 {I2}, I|g=0.3 {I1} (1969Ar25)
86SR L 3774.50 7 (4)+
86SR cL J$(4) in 2020Gu18
86SR E 0.0180 26 0.682 15 7.208 19 0.700 15
86SRS E EAV=197 6$CK=0.8491 32$CL=0.10204 41$CM+=0.02313 13
86SR G 718.95 15 0.231 9 C
86SR2 G %IG=0.191 8
86SR cG $E|g=719.17 {I23}, I|g=0.27 {I4} (1970Ra06)
86SR G 1102.13 10 0.194 8 C
86SR2 G %IG=0.160 7
86SR cG $E|g=1102.02 {I23}, I|g=0.24 {I3} (1970Ra06)
86SR G 1293.01 8 0.396 12 C
86SR2 G %IG=0.327 11
86SR cG $E|g=1294.9 {I3}, I|g=0.35 {I10} (1970Ra06, unplaced). Due to energy
86SR2cG difference of ~2 keV, it could be different line in 1970Ra06
86SR G 1544.96 11 0.0294 10 C
86SR2 G %IG=0.0243 9
86SR L 3806.24 7 (3-,4,5-)
86SR cL J$no assignment in 2020Gu18
86SR E 0.0061 10 0.304 16 7.540 27 0.310 16
86SRS E EAV=183 6$CK=0.8544 27$CL=0.10272 36$CM+=0.02328 13
86SR G 488.64 12 0.1084 26 C
86SR2 G %IG=0.0896 26
86SR G 750.70 12 0.145 8 C
86SR2 G %IG=0.120 7
86SR G 1133.72 12 0.201 8 C
86SR2 G %IG=0.166 7
86SR G 1324.75 8 0.129 9 C
86SR2 G %IG=0.107 8
86SR G 1576.75 11 0.0230 10 C
86SR2 G %IG=0.0190 9
86SR L 3830.57 6 (3)-
86SR cL J$(3-) in 2020Gu18
86SR E 0.231 39 14.58 30 5.844 18 14.81 30
86SRS E EAV=173 6$CK=0.8579 23$CL=0.10317 32$CM+=0.02339 12
86SR cE $Measured E|b=400 {I40}, I|b=2.9 (1962Ya01, tentative)
86SR G 186.2 2 0.0360 12 [M1+E2] 0.07 4 C
86SR2 G %IG=0.0298 11
86SR G 275.05 12 0.0554 15 [M2] 0.0526 8 C
86SR2 G %IG=0.0458 15
86SR G 330.85 12 1.011 25 M1(+E2) 0.7 LT 0.0082 11 C
86SR2 G %IG=0.836 25
86SR2 G EKC=0.0068 13 (1970Ra06)
86SRS G KC=0.0072 10$LC=0.00081 12$MC=0.000136 21
86SR cG $E|g=331.08 {I23}, I|g=1.01 {I3}, Ice(K)=16 {I3} (1970Ra06)
86SR cG $E|g=329 {I1}, I|g=0.72 {I17} (1969Ar25)
86SRS G NC=1.70E-5 25$OC=1.07E-6 13
86SR cG M,MR$from |a(K)exp (1970Ra06).
86SR G 469.04 10 0.1120 25 C
86SR2 G %IG=0.0926 26
86SR cG $E|g=469.24 {I25}, I|g=0.36 {I3} (1970Ra06)
86SR G 645.87 8 9.80 25(M1) 1.46E-3 2 C
86SR2 G %IG=8.10 25
86SR2 G EKC=0.00117 8 (1970Ra06)$
86SR cG $K/LM=9.0 {I22} (1962Ya01)
86SRS G KC=0.001291 18$LC=0.0001401 20$MC=2.353E-5 33
86SRS G NC=2.96E-6 4$OC=1.941E-7 27
86SR cG $E|g=645.87 {I17} from level-energy difference, I|g=11.1 {I13} from
86SR2cG |g|g-coin, Ice(K)=37.5 {I25} for 644.8|g+645.9|g (1970Ra06)
86SR cG $E|g=645 {I1}, I|g=13.4 {I24} (1969Ar25)
86SR cG $Ice(K)=34 {I2}, Ice(L+M)=3.8 {I10} (1962Ya01) for 644.8+645.9 doublet
86SR G 833.72 8 2.51 9 C
86SR2 G %IG=2.07 8
86SR cG $E|g=833.72 {I18} from level-energy difference, I|g=1.8 {I4} from
86SR2cG |g|g-coin, Ice(K)=10.5 {I7} for 833.72|g+835.67|g, the latter being
86SR3cG about three times more intense than the 833.72|g, |a(K)exp=0.00064 {I5}
86SR4cG for the doublet (1970Ra06)
86SR G 952.71 8 0.254 10 C
86SR2 G %IG=0.210 9
86SR G 1349.15 8 3.64 9 M1,E2 3.36E-4 6 C
86SR2 G %IG=3.01 9
86SR2 G EKC=0.00024 4 (1970Ra06)
86SRS G KC=0.000267 4$LC=2.87E-5 4$MC=4.81E-6 7
86SRS G NC=6.05E-7 9$OC=3.98E-8 6$IPC=3.5E-5 4
86SR cG $E|g=1349.15 {I10}, I|g=3.57 {I11}, Ice(K)=2.0 {I3} (1970Ra06)
86SR cG $E|g=1350 {I2}, I|g=3.6 {I5} (1969Ar25)
86SR cG $Ice(K)=3.4 {I5} (1962Ya01)
86SR cG M$from |a(K)exp (1970Ra06).
86SR G 1601.05 8 0.339 10 C
86SR2 G %IG=0.280 10
86SR cG $E|g=1603 {I2}, I|g=0.5 (1969Ar25, uncertain assignment to {+86}Y
86SR2cG decay)
86SR G 1976.71 8 0.0101 5 C
86SR2 G %IG=0.0083 4
86SR G 2754.0 2 0.0404 20 C
86SR2 G %IG=0.0334 17
86SR L 3870.98 7 3-
86SR E 0.0045 9 0.434 10 7.345 19 0.438 10
86SRS E EAV=156 6$CK=0.8625 17$CL=0.10378 26$CM+=0.02353 12
86SR G 184.8 2 0.0053514 [M1+E2] 0.07 4 C
86SR2 G %IG=0.00442 14
86SR G 481.32 14 0.0092 5 C
86SR2 G %IG=0.0076 4
86SR G 1229.88 10 0.0272 11E1 2.32E-4 3 C
86SR2 G %IG=0.0225 10
86SRS G KC=0.0001508 21$LC=1.607E-5 22$MC=2.69E-6 4
86SRS G NC=3.39E-7 5$OC=2.224E-8 31$IPC=6.24E-5 9
86SR G 1641.62 15 0.0259 9 C
86SR2 G %IG=0.0214 8
86SR G 2016.83 11 0.165 6 E1 7.12E-410 C
86SR2 G %IG=0.136 5
86SRS G KC=6.72E-5 9$LC=7.11E-6 10$MC=1.191E-6 17
86SR cG $E|g=2017.1 {I6}, I|g=0.16 {I2} (1970Ra06)
86SR cG $E|g=2017 {I1}, I|g=0.10 {I4} (1969Ar25)
86SRS G NC=1.500E-7 21$OC=9.91E-9 14$IPC=0.000636 9
86SR G 2794.29 12 0.296 9 E1 1.17E-3 2 C
86SR2 G %IG=0.245 9
86SRS G KC=4.19E-5 6$LC=4.42E-6 6$MC=7.41E-7 10
86SR cG $E|g=2794.9 {I4}, I|g=0.25 {I2} (1970Ra06)
86SR cG $E|g=2797 {I2}, I|g=0.3 {I1} (1969Ar25)
86SRS G NC=9.34E-8 13$OC=6.18E-9 9$IPC=0.001119 16
86SR G 3871.2 5 0.0014 LT[E3] 9.08E-413
86SR2 G %IG<0.0012
86SRS G KC=5.79E-5 8$LC=6.15E-6 9$MC=1.032E-6 14
86SRS G NC=1.301E-7 18$OC=8.62E-9 12$IPC=0.000843 12
86SR cG $E|g=3868 {I5}, I|g|?0.15 (1969Ar25, uncertain assignment to {+86}Y
86SR2cG decay, intensity is in disagreement with that from 2020Gu18)
86SR L 3898.28 21 (2+,3,4+)
86SR cL J$no assignment in 2020Gu18
86SR E 1.52E-4 32 0.0202 8 8.658 24 0.0204 8
86SRS E EAV=144 6$CK=0.8648 14$CL=0.10411 23$CM+=0.02360 12
86SR G 2821.6 2 0.0247 8 C
86SR2 G %IG=0.0204 7
86SR L 3904.00 7 (3,4+)
86SR cL J$no assignment in 2020Gu18
86SR E 5.0E-4 11 0.0718 18 8.105 21 0.0723 18
86SRS E EAV=142 6$CK=0.8653 13$CL=0.10417 23$CM+=0.02361 12
86SR G 1674.55 8 0.0244 8 C
86SR2 G %IG=0.0202 7
86SR G 2049.9 2 0.0098 10 C
86SR2 G %IG=0.0081 8
86SR G 2827.28 8 0.0533 15 C
86SR2 G %IG=0.0441 14
86SR cG $E|g=2827.7 {I8}, I|g=0.07 {I2} (1970Ra06, unplaced |g)
86SR cG $E|g=2827 {I3}, I|g=0.1 {I1} (1969Ar25)
86SR L 3925.41 6 (4-,5-)
86SR cL J$(4-) in 2020Gu18
86SR E 0.031 7 5.85 10 6.182 20 5.88 10
86SRS E EAV=133 6$CK=0.8667 11$CL=0.10438 21$CM+=0.02366 11
86SR G 118.96 12 0.231 9 [D,E2] 0.30 24 C
86SR2 G %IG=0.191 8
86SR cG $E|g=118.7 {I5}, I|g=0.25 {I9} (1969Ar25)
86SR G 369.90 8 0.480 15 C
86SR2 G %IG=0.397 14
86SR cG $E|g=370.28 {I17}, I|g=1.00 {I5} (1970Ra06)
86SR cG $E|g=369 {I1}, I|g=0.48 {I9} (1969Ar25)
86SR G 425.83 10 0.291 10 C
86SR2 G %IG=0.241 9
86SR cG $E|g=425.97 {I23}, I|g=0.37 {I2} (1970Ra06)
86SR G 607.87 8 1.62 5 0.0008719 C
86SR2 G %IG=1.34 5
86SR2 G EKC=0.00079 9 (1970Ra06)
86SR cG $E|g=608.29 {I10}, I|g=2.44 {I18}, Ice(K)=4.5 {I5} (1970Ra06)
86SR cG $E|g=609.3 {I5}, I|g=1.5 {I2} (1969Ar25)
86SR cG $Ice(K)=6.2 {I10} (1962Ya01)
86SRS G KC=0.00077 17$LC=8.4E-5 19$MC=1.4E-5 4
86SRS G NC=1.8E-6 4$OC=1.1E-7 3
86SR G 634.52 8 0.220 17 C
86SR2 G %IG=0.182 14
86SR cG $E|g=634.78 {I2}, uncertainty is probably 0.20, I|g=0.11 {I3}
86SR2cG (1970Ra06, uncertain assignment to {+86}Y decay)
86SR G 740.57 9 1.15 3 C
86SR2 G %IG=0.951 30
86SR cG $E|g=740.81 {I13}, I|g=1.65 {I6} (1970Ra06)
86SR G 869.99 11 0.448 12 C
86SR2 G %IG=0.370 12
86SR G 929.0 3 0.173 6 C
86SR2 G %IG=0.143 6
86SR G 1253.04 8 1.86 8 0.000266 C
86SR2 G %IG=1.54 7
86SR2 G EKC=0.00018 5 (1970Ra06)
86SR cG $E|g=1253.11 {I10}, I|g=1.86 {I6}, Ice(K)=0.8 {I2} (1970Ra06)
86SR cG $E|g=1253 {I1}, I|g=1.6 {I5} (1969Ar25)
86SR cG $Ice(K)=1.4 {I5} (1962Ya01)
86SRS G KC=1.66E-4 53$LC=1.78E-5 58$MC=2.98E-6 97
86SRS G NC=3.7E-7 13$OC=2.46E-8 80$IPC=7.5E-5 8
86SR G 1444.03 9 0.0678 20 C
86SR2 G %IG=0.0560 19
86SR G 1696.00 8 0.911 25 C
86SR2 G %IG=0.753 24
86SR cG $E|g=1696.25 {I13}, I|g=0.77 {I2} (1970Ra06)
86SR L 3941.98 6 3-
86SR cL $A 256.38 {I40} |g with I|g=0.09 {I3} in 1970Ra06 with uncertain
86SR2cL assignment to {+86}Y decay and placed from 3942 level is not given
86SR3cL by 2020Gu18
86SR E 0.0041 10 0.978 16 6.945 18 0.982 16
86SRS E EAV=126 6$CK=0.8676 10$CL=0.10452 20$CM+=0.02370 11
86SR G 450.89 15 0.0457 20 C
86SR2 G %IG=0.0378 18
86SR G 945.08 9 0.0772 18 C
86SR2 G %IG=0.0638 18
86SR G 1064.13 9 0.0757 18 C
86SR2 G %IG=0.0626 18
86SR cG $E|g=1064 {I1}, I|g=0.9 {I4} (1969Ar25, intensity is in disagreement)
86SR G 1300.82 10 0.0434 24 C
86SR2 G %IG=0.0359 21
86SR cG $E|g=1300 {I1}, I|g=0.5 {I2} (1969Ar25)
86SR G 1712.46 9 0.0715 18 C
86SR2 G %IG=0.0591 18
86SR G 2088.10 8 0.343 11E1 7.58E-411 C
86SR2 G %IG=0.284 10
86SRS G KC=6.38E-5 9$LC=6.74E-6 9$MC=1.130E-6 16
86SRS G NC=1.423E-7 20$OC=9.40E-9 13$IPC=0.000686 10
86SR cG $E|g=2088.09 {I25}, I|g=0.30 {I3} (1970Ra06)
86SR cG $E|g=2089 {I1}, I|g=0.46 {I16} (1969Ar25)
86SR G 2865.36 8 0.531 15 E1(+M2) -0.003 14 1.20E-3 2 C
86SR2 G %IG=0.439 14
86SRS G KC=4.05E-5 6$LC=4.27E-6 6$MC=7.16E-7 10
86SRS G NC=9.02E-8 13$OC=5.97E-9 8$IPC=0.001155 16
86SR cG $E|g=2865.9 {I3}, I|g=0.46 {I8} (1970Ra06, placed from 4714 level)
86SR cG $E|g=2866 {I4}, I|g=0.66 {I30} (1969Ar25)
86SR L 3968.32 6 4-
86SR cL J$from |g|g(|q) (2020Gu18), but no supporting data given in the
86SR2cL paper, and no discussion of spin of this level in the text.
86SR E 0.0037 10 1.316 30 6.797 19 1.320 30
86SRS E EAV=114 6$CK=0.8688 8$CL=0.10470 19$CM+=0.02374 11
86SR G 468.73 10 0.175 7 C
86SR2 G %IG=0.145 6
86SR cG $E|g=469.24 {I25}, I|g=0.36 {I3} (1970Ra06)
86SR G 578.7 2 0.0059423 C
86SR2 G %IG=0.00491 21
86SR G 606.90 8 0.0394 15 C
86SR2 G %IG=0.0326 14
86SR G 783.48 12 0.320 12 C
86SR2 G %IG=0.265 11
86SR cG $E|g=783.56 {I26}, I|g=0.32 {I4} (1970Ra06)
86SR G 912.9 2 0.0773 22 C
86SR2 G %IG=0.0639 21
86SR G 971.56 8 0.327 14 M1+E2 -0.59 23 6.02E-4 9 C
86SR2 G %IG=0.270 12
86SRS G KC=0.000533 8$LC=5.76E-5 9$MC=9.67E-6 15
86SRS G NC=1.216E-6 19$OC=7.97E-8 11
86SR cG $E|g=971.43 {I18}, I|g=0.33 {I4} (1970Ra06)
86SR cG $E|g=974 {I1}, I|g=0.45 {I5} (1969Ar25)
86SR G 1296.03 12 0.575 15 C
86SR2 G %IG=0.475 15
86SR cG $E|g=1296.03 {I23}, I|g=0.66 {I4} (1970Ra06)
86SR G 1486.83 8 0.0223 8 C
86SR2 G %IG=0.0184 7
86SR G 1738.65 20 0.051 3 C
86SR2 G %IG=0.0422 26
86SR L 4144.67 8 (3,4+)
86SR cL $A 380.4 {I3} |g with I|g=0.55 {I4} in 1970Ra06 placed from 4145 level
86SR2cL is not confirmed by 2020Gu18 from |g|g-coin data
86SR E 3E-6 5 0.232 7 7.420 23 0.232 7
86SRS E EAV=37 7$CK=0.87079 33$CL=0.10531 18$CM+=0.02389 11
86SR G 1503.40 12 0.0067 5 C
86SR2 G %IG=0.0055 4
86SR G 2290.78 12 0.0405 12 C
86SR2 G %IG=0.0335 11
86SR cG $E|g=2291.8 {I5}, I|g=0.15 {I1} (1970Ra06)
86SR cG $E|g=2290 {I2}, I|g=0.1 (1969Ar25)
86SR G 3068.04 20 0.234 7 C
86SR2 G %IG=0.193 7
86SR cG $E|g=3069.7 {I4}, I|g=0.14 {I2} (1970Ra06)
86SR cG $E|g=3071 {I4}, I|g=0.78 {I20} (1969Ar25)
86SR G 4144.7 20 0.0001 LT ?
86SR2 G %IG LT 8.27E-5
86SR cG $Mult=E3, M3 or E4 required for 4145|g to 0+. This |g is treated as
86SR2cG uncertain by the evaluators.
86SR L 4203.40 21 (3,4+)
86SR cL J$no assignment in 2020Gu18
86SR E 0.00450 30 6.772 21 0.00450 30
86SRS E CK=0.871 13$CL=0.1054 16$CM+=0.02392 33
86SR G 3126.71 20 0.0054 3 C
86SR2 G %IG=0.00446 26
86SR L 4205.41 7 (3-,4)
86SR cL $A very weak 1150.34 {I18} |g in 1970Ra06 placed from 4205 level
86SR2cL is not confirmed by 2020Gu18 from |g|g-coin data
86SR E 0.919 17 6.772 21 0.919 17
86SRS E CK=0.87063 33$CL=0.10545 18$CM+=0.02392 12
86SR G 1327.54 8 0.171 9 C
86SR2 G %IG=0.141 8
86SR cG $E|g=1327.5 {I5}, I|g=0.11 {I5} (1970Ra06)
86SR cG $E|g=1330 {I1}, I|g=0.4 {I1} (1969Ar25)
86SR G 1532.99 8 0.250 7 C
86SR2 G %IG=0.207 7
86SR cG $E|g=1533.19 {I13}, I|g=0.27 {I4} (1970Ra06)
86SR G 1723.76 11 0.691 16 C
86SR2 G %IG=0.571 16
86SR cG $E|g=1724.15 {I10}, I|g=0.67 {I5} (1970Ra06)
86SR cG $E|g=1723 {I1}, I|g=0.9 {I3} (1969Ar25)
86SR L 4224.93 11
86SR E 0.0003 LT 10.241 GT
86SRS E CK=0.87057 34$CL=0.10550 18$CM+=0.02393 12
86SR G 1995.3 2 0.0053 4 C
86SR2 G %IG=0.00438 34
86SR L 4394.63 9 (4-,5)
86SR cL J$no assignment in 2020Gu18
86SR E 0.167 6 7.334 27
86SRS E CK=0.86993 36$CL=0.10600 20$CM+=0.02406 12
86SR G 169.7 2 0.0026111 [D,E2] 0.08 6 C
86SR2 G %IG=0.00216 10
86SR G 895.07 12 0.0866 22 C
86SR2 G %IG=0.0716 22
86SR G 1103.69 12 0.033 4 C
86SR2 G %IG=0.0273 33
86SR G 1339.25 12 0.0802 24 C
86SR2 G %IG=0.0663 23
86SR L 4408.81 12 3-
86SR cL $A 2555.3 {I17} |g with I|g=0.033 {I10} in 1970Ra06 placed from 4409
86SR3cL level is not reported by 2020Gu18
86SR E 0.199 8 7.243 29
86SRS E CK=0.86987 36$CL=0.10605 20$CM+=0.02409 12
86SR G 1621.60 15 0.0061 4 C
86SR2 G %IG=0.00504 34
86SR G 2179.2 2 0.0295 10 C
86SR2 G %IG=0.0244 9
86SR cG $E|g=2180.8 {I10}, I|g=0.04 {I1} (1970Ra06)
86SR G 3332.0 2 0.205 8 E1+M2 +0.15 2 1.41E-3 2 C
86SR2 G %IG=0.169 7
86SRS G KC=3.41E-5 6$LC=3.59E-6 6$MC=6.02E-7 10
86SRS G NC=7.59E-8 13$OC=5.03E-9 8$IPC=0.001371 20
86SR cG $E|g=3334.0 {I5}, I|g=0.15 {I2} (1970Ra06)
86SR cG $E|g=3336 {I5}, I|g=0.4 {I3} (1969Ar25)
86SR G 4409 2 0.00014LT [E3] 1.06E-3 2
86SR2 G %IG LT 1.157E-4
86SRS G KC=4.61E-5 6$LC=4.90E-6 7$MC=8.21E-7 12
86SRS G NC=1.035E-7 15$OC=6.87E-9 10$IPC=0.001013 14
86SR L 4441.09 8 (3-,4,5-)
86SR E 0.158 4 7.309 26
86SRS E CK=0.86971 37$CL=0.10618 21$CM+=0.02411 12
86SR G 216.0 3 0.00032 4 [D,E2] 0.003630 C
86SR2 G %IG=0.000265 33
86SR G 666.59 8 0.0044 3 C
86SR2 G %IG=0.00364 26
86SR G 1385.70 12 0.0824 22 C
86SR2 G %IG=0.0681 22
86SR cG $E|g=1390 {I2}, I|g|?0.3 (1969Ar25, uncertain assignment to
86SR2cG {+86}Y decay)
86SR G 1768.62 10 0.0949 25 C
86SR2 G %IG=0.0784 25
86SR G 1959.5 2 0.0089 6 C
86SR2 G %IG=0.0074 5
86SR L 4445.54 21 (2+,3,4+)
86SR cL J$no assignment in 2020Gu18
86SR E 0.0053 5 8.778 47
86SRS E CK=0.86969 37$CL=0.10619 21$CM+=0.02412 12
86SR G 3368.84 20 0.0064 5 C
86SR2 G %IG=0.0053 4
86SR L 4448.97 6 (3-,4)
86SR E 0.173 3 7.260 25
86SRS E CK=0.86967 37$CL=0.10621 21$CM+=0.02412 12
86SR G 223.9 2 0.00076 5 [D,E2] 0.032 22 C
86SR2 G %IG=0.00063 4
86SR G 949.55 8 0.0134 5 C
86SR2 G %IG=0.0111 5
86SR G 1393.6 2 0.0209 10 C
86SR2 G %IG=0.0173 9
86SR G 1452.21 8 0.0473 12 C
86SR2 G %IG=0.0391 12
86SR G 1570.96 11 0.0152 6 C
86SR2 G %IG=0.0126 5
86SR G 1776.6 2 0.0101 5 C
86SR2 G %IG=0.0083 4
86SR G 1967.41 8 0.0492 14 C
86SR2 G %IG=0.0407 13
86SR cG $E|g=1969.1 {I7}, I|g=0.06 {I1} (1970Ra06, unplaced). Due to energy
86SR2cG difference of 1.7 keV, it could be different line in 1970Ra06
86SR G 2219.35 8 0.0523 15 C
86SR2 G %IG=0.0432 14
86SR L 4465.82 7 (3-,4)
86SR E 0.161 4 7.273 26
86SRS E CK=0.86958 37$CL=0.10628 21$CM+=0.02415 12
86SR G 240.9 2 0.00054 4 [D,E2] 0.025 17 C
86SR2 G %IG=0.000446 34
86SR G 966.24 12 0.0138 4 C
86SR2 G %IG=0.0114 4
86SR G 1410.3 2 0.0879 22 C
86SR2 G %IG=0.0727 22
86SR G 1469.1 2 0.0141 4 C
86SR2 G %IG=0.0117 4
86SR G 1587.87 8 0.0309 12 C
86SR2 G %IG=0.0255 11
86SR G 1984.37 8 0.0481 16 C
86SR2 G %IG=0.0398 15
86SR L 4497.75 7 (3,4+)
86SR E 0.0817 16 7.530 26
86SRS E CK=0.86940 38$CL=0.10642 22$CM+=0.02418 12
86SR G 1500.92 8 0.0528 15 C
86SR2 G %IG=0.0436 14
86SR G 1619.82 8 0.0270 8 C
86SR2 G %IG=0.0223 8
86SR G 1710.6 3 0.0043215 C
86SR2 G %IG=0.00357 14
86SR G 2268.24 12 0.0147 7 C
86SR2 G %IG=0.0122 6
86SR L 4580.20 21 (3,4+)
86SR cL J$no assignment in 2020Gu18
86SR E 0.0138 10 8.198 41
86SRS E CK=0.86885 40$CL=0.10686 24$CM+=0.02429 13
86SR G 3503.49 20 0.0167 11 C
86SR2 G %IG=0.0138 9
86SR L 4608.46 8 (4,5-)
86SR cL J$no assignment in 2020Gu18
86SR E 0.0635 20 7.496 31
86SRS E CK=0.86863 41$CL=0.10703 24$CM+=0.02434 13
86SR G 1053.2 3 0.0122 4 C
86SR2 G %IG=0.0101 4
86SR G 1935.97 8 0.0043114 C
86SR2 G %IG=0.00356 13
86SR cG $E|g=1940 {I3}, I|g=0.15 {I5} (1969Ar25, intensity in disagreement)
86SR G 2126.97 8 0.0603 22 C
86SR2 G %IG=0.0498 20
86SR cG $E|g=2130 {I2}, I|g=0.15 {I7} (1969Ar25)
86SR L 4691.13 8 (3-,4,5-)
86SR E 0.094 3 7.201 34
86SRS E CK=0.86784 46$CL=0.10766 28$CM+=0.02450 14
86SR G 466.4 3 0.00170 9 C
86SR2 G %IG=0.00141 8
86SR G 1004.67 12 0.0075 3 C
86SR2 G %IG=0.00620 27
86SR G 1635.73 8 0.0674 23 C
86SR2 G %IG=0.0557 21
86SR G 2018.48 15 0.0262 15 C
86SR2 G %IG=0.0217 13
86SR G 2209.6 2 0.0102 5 C
86SR2 G %IG=0.0084 4
86SR L 4713.58 18 (3,4+)
86SR cL J$no assignment in 2020Gu18
86SR cL $A 2862 {I3} |g with I|g=0.011 {I5} in 1970Ra06 placed from 4714 level
86SR3cL is placed from 3941 level by 2020Gu18 from |g|g-coin data
86SR E 0.0569 17 7.382 35
86SRS E CK=0.86758 47$CL=0.10786 29$CM+=0.02456 14
86SR G 2484.2 3 0.0118 5 D+Q +0.05 1 C
86SR cG $|d=+0.05 {I1} from |g|g(|q) data (2020Gu18), but no spin is
86SR2cG given for the 4713 level
86SR2 G %IG=0.0098 4
86SR G 3636.80 20 0.057 2 C
86SR2 G %IG=0.0471 18
86SR cG $E|g=3642 {I2}, I|g=0.05 {I1} (1970Ra06)
86SR cG $E|g=3640 {I4}, I|g=0.4 {I3} (1969Ar25)
86SR L 4751.27 11
86SR E 0.0029020 8.608 45
86SRS E CK=0.8671 5$CL=0.10825 31$CM+=0.02466 15
86SR G 1361.63 8 0.0035123 C
86SR2 G %IG=0.00290 20
86SR L 4848.80 22 (3,4,5-)
86SR cL J$no assignment in 2020Gu18
86SR E 0.0094 4 7.897 45
86SRS E CK=0.8654 6$CL=0.10962 41$CM+=0.02501 17
86SR G 1663.9 3 0.0028415 C
86SR2 G %IG=0.00235 13
86SR cG $E|g=1661 {I12}, I|g=0.5 {I2} (1969Ar25, intensity in disagreement)
86SR G 2619.4 3 0.0085 3 C
86SR2 G %IG=0.00703 27
86SR cG $E|g=2617 {I2}, I|g=0.20 {I8} (1969Ar25, intensity in disagreement)
86SR L 4894.54 21 (3,4,5)
86SR cL J$no assignment in 2020Gu18
86SR E 0.0033317 8.24 5
86SRS E CK=0.8642 7$CL=0.11054 49$CM+=0.02526 19
86SR G 2665.0 2 0.0040319 C
86SR2 G %IG=0.00333 17
86SR L 4956.08 24 (3)
86SR cL J$no assignment in 2020Gu18
86SR E 0.0530 13 6.86 6
86SRS E CK=0.8620 10$CL=0.1123 7$CM+=0.02573 23
86SR G 2314.9 4 0.0033 3 C
86SR2 G %IG=0.00273 25
86SR G 2726.4 4 0.0055123 C
86SR2 G %IG=0.00455 21
86SR G 3879.5 4 0.0553 15 D+Q +0.06 5 C
86SR cG $|d(Q/D)=+0.06 {I5} from |g|g(|q) data (2020Gu18), but no spin is
86SR2cG given for the 4956 level
86SR2 G %IG=0.0457 15
86SR cG $E|g=3877 {I6}, I|g=0.06 {I5} (1970Ra06)
86SR cG $E|g=3888 {I5}, I|g|?0.37 (1970Ra06, intensity in disagreement)