32S 32CL EC DECAY (298 MS) 2018AB06,2012ME03,1979HO2725NDS 202503
32S H TYP=FUL$AUT=Jun Chen$CIT=NDS 201, 1 (2025)$CUT=31-Oct-2024$
32S c 2018Ab06: {+32}Cl source was produced by fragmentation of 150
32S 2c MeV/nucleon {+36}Ar beam on a {+9}Be target at NSCL, purified using the
32S 3c A1900 separator and the Radio Frequency Fragment Separator (RFFS), and
32S 4c implanted into a plastic scintillator. |g rays were detected with the
32S 5c Yale Clovershare Array of nine HPGe detectors with four clover crystals
32S 6c each. Measured E|g, I|g, |b|g-coin, |b|g|g-con. Deduced levels, J, |p,
32S 7c |b-decay and |g emission probabilities, log {Ift}, B(>). Comparisons
32S 8c with shell-model calculations.
32S c 2012Me03 (also 2011Me15): {+32}Cl source was produced by the reaction
32S 2c {+1}H({+32}S,n) with a beam energy of 24.8 MeV/nucleon incident on a
32S 3c Liquid N-cooled H{-2} gas target at the Cyclotron Institute at Texas
32S 4c A&M University, and implanted into an aluminized Mylar tape. |g
32S 5c particles were detected with a scintillator detector and |g rays were
32S 6c detected with a HPGe detector. Measured E|g, I|g, E|b, I|b, |g|b-coin.
32S 7c Deduced levels, |b-decay branching ratios, log {Ift} values, B(>) and
32S 8c B(F) values, isospin symmetry breaking term. Comparison with
32S 9c shell-model calculations.
32S c 1979Ho27: {+32}Cl source was produced via {+32}S(p,n) with 20 MeV
32S 2c protons from the University of Jyvaskyla |a(M)-20 cyclotron on a
32S 3c natural sulphur target. Charged particles were detected with a Si
32S 4c detector and |g rays were detected with a Ge detector. Measured E(p),
32S 5c I(p), E(|a), I(|a). Deduced proton and |a emission probabilities,
32S 6c |b-decay branching ratios, log {Ift} of particle-unbound levels.
32S c 1973De08: {+32}Cl source was produce via {+32}S(p,n) with 27 MeV
32S 2c protons from the University of Colorado cyclotron. |g rays were
32S 3c detected with a Ge(Li) detector. Measured E|g, I|g. Deduced levels,
32S 4c |b-decay branching ratios, |g-ray emission probabilities and branching
32S 5c ratios. Comparisons with available data.
32S c 1968Ar03: {+32}Cl source was produced via {+32}S(p,n) with 25 MeV
32S 2c protons from the UCLA sector focused cyclotron. Rabbit system for
32S 3c target transfer to counting area. |b particles were detected with a
32S 4c magnetic spectrometer and |g rays were detected with a Ge detector.
32S 5c Measured E|g, I|g, decay curve, Kurie plot. Deuced levels, parent
32S 6c T{-1/2}, |b-decay branching ratios and energies, |g-ray emission
32S 7c probabilities.
32S c Others: 1971Go18, 1969St14, 1966An01
32S c From RADLIST code, the total released energy is 12700 keV {I110} as
32S 2c compared to 12680.8 keV {I6} from Q(|b{+-})value (2021Wa16), indicating
32S 3c completeness of this decay scheme
32S cE $M(>) given under comments are experimental Gamow-Teller matrix
32S 2cE element from 2012Me03. It is related to the experimental > strength
32S 3cE B(>){-exp} by B(>){-exp}=g{+2}{-A,eff}|*M(>){+2}, where
32S 4cE g{+2}{-A,eff}=1 is taken in 2012Me03
32S cE E$From 1968Ar03
32S cE IE$From |g intensity balance at each level for excited levels, also
32S 2cE including %I(p) and %I(|a) from 1979Ho27 as given under comments for
32S 3cE particle-unbound levels above 8407 level, unless otherwise noted
32S cG E,RI$From 2018Ab06, unless otherwise noted.
32S cL $Isospins are from 2012Me03
32S cL $E(p) and E(|a) under comments of particle-unbound levels are from
32S 2cL 1979Ho27
32S cL E$From a least-squares fit to |g-ray energies for levels connected
32S 2cL with |g transitions and from E(|a) or E(p) for particle-unbound
32S 3cL levels (above 8407 level).
32S cL J$From Adopted Levels
32CL P 0 1+ 298 MS 1 12680.8 6
32CL cP J,T$From Adopted Levels of {+32}Cl
32CL cP QP$From 2021Wa16
32S N 1.0 1 1 1
32S cN BR$%|e|a=0.054 {I8}, %|ep=0.026 {I5} (1979Ho27)
32S PN 3
32S L 0 0+
32S 2 L ISPIN=0
32S E 1.0 4 6.7 2 1.0 4
32S S E EAV=5604.77 30
32S cE E$measured value: 11600 {I300} (1968Ar03)
32S cE IB$from 1968Ar03
32S cE $M(>)=0.035 {I+3-10}
32S L 2230.92 29 2+
32S 2 L ISPIN=0
32S E 59.4 6 5.15E-3 7 4.520 5 59.4 6
32S S E EAV=4496.58 33$CK=7.8480E-5 17$CL=7.3818E-6 16$CM+=9.0189E-7 19
32S cE $M(>)=0.423 {I1}
32S G 2230.2 4 91.9 5
32S cG E$from 2012Me03. Others: 2230.4 {I16} (1968Ar03) and 2230.5 {I15}
32S 2cG (1973De08)
32S cG RI$from 2012Me03. Others: 96 {I4} (1966An01), 89 {I6} (1968Ar03), and
32S 2cG 92 {I4} (1973De08)
32S dG RI$ 2012Me03 quote uncertainty of +0.6-0.4.
32S L 3778.55 32 0+
32S 2 L ISPIN=0
32S E 1.09 8 1.6E-4 1 5.89 3 1.09 8
32S S E EAV=3729.85 34$CK=1.33598E-4 34$CL=1.25672E-5 32$CM+=1.53544E-6 39
32S cE E$measured value: 9470 {I30} (1968Ar03)
32S cE $M(>)=0.083 {I3}
32S G 1547.1 4 3.16 4
32S cG E$from 2012Me03. Others: 1545.9 {I20} (1968Ar03) and 1548 {I2}
32S 2cG (1973De08)
32S cG RI$from 2012Me03. Others: 5.1 {I26} (1966An01), 5 {I3} (1968Ar03), and
32S 2cG 3.6 {I6} (1973De08)
32S dG RI$ 2012Me03 quote uncertainty of +0.040-0.036.
32S G 3779.5 8 [E0] 0.044 18
32S cG E$weighted average of 3777 {I4} (2012Me03) and 3779.6 {I8} (2018Ab06)
32S cG TI$other: 0.044 {I25} (2012Me03)
32S L 4282.12 33 2+
32S 2 L ISPIN=0
32S E 2.30 7 4.1E-4 1 5.43 1 2.30 7
32S S E EAV=3479.34 34$CK=1.62435E-4 45$CL=1.52802E-5 42$CM+=1.86692E-6 51
32S cE E$measured value: 7480 {I260} for decays to 4282 and 4697 (1968Ar03)
32S cE $M(>)=0.145 {I3}
32S G 2050.9 4 0.433 24
32S cG E$weighted average of 2050.7 {I4} (2012Me03) and 2051.0 {I4} (2018Ab06)
32S cG RI$weighted average of 0.47 {I4} (2012Me03) and 0.419 {I24} (2018Ab06)
32S G 4281.7 7 2.47 6
32S cG E$weighted average of 4279.6 {I20} (1968Ar03), 4281.5 {I15} (1973De08),
32S 2cG and 4282.0 {I7} (2012Me03)
32S cG RI$weighted average of 2.1 {I11} (1966An01), 4 {I2} (1968Ar03), 2.6
32S 2cG {I1} (1973De08), and 2.42 {I6} (2012Me03)
32S cG RI$ 2012Me03 give branching ratio of 83.5 {I11}; 1.1 (stat),
32S 2cG +0.3-0.1 (syst).
32S L 4695.66 33 1+
32S 2 L ISPIN=0
32S E 6.03 9 1.29E-3 2 4.89 1 6.03 9
32S S E EAV=3275.13 34$CK=1.92735E-4 56$CL=1.81310E-5 53$CM+=2.21524E-6 65
32S cE $M(>)=0.281 {I2}
32S G 916.0 5 0.024 7
32S cG E$weighted average of 915.8 {I5} (2012Me03) and 916.8 {I10} (2018Ab06)
32S cG RI$weighted average of 0.034 {I9} (2012Me03) and 0.019 {I6} (2018Ab06)
32S G 2464.3 5 4.19 7
32S cG E$weighted average of 2464.1 {I17} (1968Ar03), 2463.8 {I10} (1973De08),
32S 2cG and 2464.4 {I5} (2012Me03)
32S cG RI$weighted average of 6.9 {I21} (1966An01), 5.0 {I25} (1968Ar03), 4.0
32S 2cG {I4} (1973De08), 4.24 {I5} (2012Me03), and 3.92 {I12} (2018Ab06)
32S G 4695.3 8 2.42 5
32S cG E$weighted average of 4694.3 {I20} (1968Ar03), 4694 {I2} (1973De08),
32S 2cG and 4695.6 {I8} (2012Me03)
32S cG RI$from 2012Me03. Others: 4 {I3} (1968Ar03) and 2.8 {I6} (1973De08)
32S L 5006.1 5 3-
32S E 0.041 14 7.0 2 0.041 14
32S S E EAV=3122.00 39
32S G 726 0.012 LT ?
32S G 1229 0.015 LT ?
32S G 2775.2 5 0.081 9
32S L 5548.59 34 2+
32S 2 L ISPIN=0
32S E 3.94 16 1.24E-3 5 4.81 2 3.94 16
32S S E EAV=2854.82 34$CK=2.83906E-4 95$CL=2.67095E-5 89$CM+=3.2634E-6 11
32S cE E$measured value: 6180 {I580} (1968Ar03)
32S G 542 0.009 LT ?
32S G 852.3 6 0.019 7
32S cG E$weighted average of 851.8 {I5} (2012Me03) and 852.9 {I6} (2018Ab06)
32S cG RI$weighted average of 0.027 {I8} (2012Me03) and 0.014 {I6} (2018Ab06)
32S G 1266.2 6 0.022 9
32S cG E$weighted average of 1265.7 {I6} (2012Me03) and 1266.9 {I7} (2018Ab06)
32S cG RI$other: <0.036 {I13} (2012Me03).
32S G 1769.7 4 0.127 13
32S cG E$weighted average of 1769.6 {I4} (2012Me03) and 1769.8 {I4} (2018Ab06)
32S cG RI$weighted average of 0.136 {I26} (2012Me03) and 0.125 {I13}
32S 2cG (2018Ab06)
32S G 3317.9 6 2.47 5
32S cG E$from 2012Me03. Others: 3319 {I2} (1968Ar03) and 3317.5 {I15}
32S 2cG (1973De08)
32S cG RI$weighted average of 4.1 {I18} (1966An01), 4 {I1} (1968Ar03), 2.5
32S 2cG {I4} (1973De08), and 2.46 {I5} (2012Me03)
32S G 5548.9 9 1.55 15
32S cG E$from 2012Me03. Others: 5548 {I2} (1968Ar03) and 5549.5 {I20}
32S 2cG (1973De08)
32S cG RI$weighted average of 1.5 {I10} (1966An01), 3.0 {I5} (1968Ar03), 1.6
32S 2cG {I3} (1973De08), and 1.50 {I9} (2012Me03)
32S dG RI$ quoted uncertainty=+0.08-0.09 (2012Me03).
32S L 5799.0 13 1-
32S E 0.028 7 6.9 1 0.028 7
32S S E EAV=2731.69 70
32S G 5798.4 13 0.028 7
32S L 6665.8 4 2+
32S 2 L ISPIN=0
32S E 2.00 5 1.14E-3 3 4.70 1 2.00 5
32S S E EAV=2306.68 35$CK=5.1660E-4 22$CL=4.8606E-5 21$CM+=5.9388E-6 26
32S cE $M(>)=0.353 {I6}
32S G 1659.9 5 0.040 11
32S G 1970.1 5 0.137 19
32S cG E$weighted average of 1969.3 {I6} (2012Me03) and 1970.4 {I4} (2018Ab06)
32S cG RI$weighted average of 0.15 {I4} (2012Me03) and 0.134 {I19} (2018Ab06)
32S G 2383.5 5 0.060 7
32S cG E$weighted average of 2383.3 {I5} (2012Me03) and 2383.6 {I5} (2018Ab06)
32S cG RI$weighted average of 0.077 {I20} (2012Me03) and 0.058 {I7} (2018Ab06)
32S dG RI$ quoted uncertainty=+0.019-0.021 (2012Me03)
32S G 2886.9 5 0.976 27
32S cG E$weighted average of 2885 {I2} (1973De08) and 2887.0 {I5} (2012Me03)
32S cG RI$from 2012Me03. Other: 1.0 {I4} (1973De08)
32S dG RI$ quoted uncertainty=+0.028-0.025 (2012Me03)
32S G 4435.0 8 0.75 3
32S cG E$weighted average of 4433 {I2} (1973De08), 4435.5 {I8} (2012Me03), and
32S 2cG 4434.8 {I8} (2018Ab06)
32S cG RI$weighted average of 0.8 {I2} (1973De08), 0.83 {I6} (2012Me03), and
32S 2cG 0.73 {I3} (2018Ab06)
32S G 6665.2 16 0.037 7
32S cG E$weighted average of 6665.8 {I21} (2012Me03) and 6664.9 {I16}
32S 2cG (2018Ab06)
32S cG RI$weighted average of 0.048 {I19} (2012Me03) and 0.036 {I7} (2018Ab06)
32S dG RI$ quoted uncertainty=+0.018-0.019 (2012Me03)
32S L 7000.9 4 1+
32S 2 L ISPIN=1
32S E 22.4 2 0.0157 2 3.506 4 22.4 2
32S S E EAV=2142.99 35$CK=6.3480E-4 29$CL=5.9731E-5 28$CM+=7.2981E-6 34
32S cE E$measured value: 4750 {I240} (1968Ar03)
32S G 1452.0 4 0.249 20
32S cG E$weighted average of 1451.8 {I4} (2012Me03) and 1452.2 {I4} (2018Ab06)
32S cG RI$weighted average of 0.276 {I19} (2012Me03) and 0.235 {I14}
32S 2cG (2018Ab06)
32S G 2305.2 5 0.154 9
32S cG E$from 2012Me03. Other: 2305.2 {I5} (2018Ab06)
32S cG RI$weighted average of 0.137 {I23} (2012Me03) and 0.157 {I9} (2018Ab06)
32S G 2718.9 5 0.502 31
32S cG E$weighted average of 2719.0 {I5} (2012Me03) and 2718.8 {I5} (2018Ab06)
32S cG RI$unweighted average of 0.533 {I22} (2012Me03) and 0.471 {I17}
32S 2cG (2018Ab06)
32S dG RI$ quoted uncertainty=+0.019-0.024 (2012Me03)
32S G 3222.3 6 0.823 59
32S cG E$weighted average of 3222.4 {I6} (2012Me03) and 3222.1 {I6} (2018Ab06)
32S cG RI$unweighted average of 0.881 {I28} (2012Me03) and 0.764 {I25}
32S 2cG (2018Ab06)
32S dG RI$ quoted uncertainty=+0.029-0.027 (2012Me03)
32S G 4770.0 8 20.62 19
32S cG E$weighted average of 4767.6 {I16} (1968Ar03), 4770.0 {I15} (1973De08),
32S 2cG 4770.8 {I8} (2012Me03), and 4769.8 {I9} (2018Ab06)
32S cG RI$from 2012Me03. Others: 20.5 {I23} (1966An01), 25 {I4} (1968Ar03),
32S 2cG and 20.5 {I20} (1973De08)
32S dG RI$ quoted uncertainty=+0.20-0.17 (2012Me03)
32S G 7001.0 15 0.055 7
32S cG E$weighted average of 7001.4 {I16} (2012Me03) and 7000.6 {I15}
32S 2cG (2018Ab06)
32S cG RI$weighted average of 0.057 {I16} (2012Me03) and 0.054 {I7} (2018Ab06)
32S L 7114.7 5 2+
32S 2 L ISPIN=1
32S E 0.595 25 4.49E-420 5.03 2 0.595 25
32S S E EAV=2087.49 38$CK=6.8314E-4 35$CL=6.4280E-5 33$CM+=7.8539E-6 40
32S cE $M(>)=0.238 {I8}
32S G 2107 0.010 LT ?
32S G 2418.1 5 0.062 9
32S cG E$weighted average of 2417.7 {I6} (2012Me03) and 2418.3 {I5} (2018Ab06)
32S cG RI$weighted average of 0.057 {I14} (2012Me03) and 0.064 {I9} (2018Ab06)
32S dG RI$ quoted uncertainty=+0.013-0.015 (2012Me03)
32S G 2831.4 9 0.021 8
32S cG E$weighted average of 2832.4 {I15} (2012Me03) and 2831.0 {I9}
32S 2cG (2018Ab06)
32S cG RI$weighted average of 0.019 {I13} (2012Me03) and 0.022 {I8} (2018Ab06)
32S G 3339.2 8 0.027 9
32S F G FL=3778.55
32S cG E$weighted average of 3339.7 {I12} (2012Me03) and 3339.0 {I8}
32S 2cG (2018Ab06)
32S cG RI$weighted average of 0.037 {I15} (2012Me03) and 0.024 {I9} (2018Ab06)
32S G 4883.2 8 0.485 20
32S cG E$weighted average of 4881 {I4} (1973De08), 4883.7 {I8} (2012Me03), and
32S 2cG 4882.7 {I9} (2018Ab06)
32S cG RI$weighted average of 0.504 {I32} (2012Me03) and 0.477 {I20}
32S 2cG (2018Ab06). Other: 0.45 {I20} (1973De08)
32S dG RI$ quoted uncertainty=+0.031-0.032 (2012Me03)
32S G 7115 0.020 LT ?
32S L 7190.8 5 1+
32S 2 L ISPIN=0
32S E 0.71 12 5.6E-4 10 4.9 1 0.71 12
32S S E EAV=2050.41 38$CK=7.1825E-4 37$CL=6.7585E-5 35$CM+=8.2576E-6 43
32S cE $M(>)+M(F)=0.250 {I10} for this nonanalog transition, contribution
32S 2cE from Fermi transition is expected to be significant.
32S G 2183 0.010 LT ?
32S G 2494.5 9 0.011 7
32S cG E$weighted average of 2495.2 {I23} (2012Me03) and 2494.4 {I9}
32S 2cG (2018Ab06)
32S cG RI$weighted average of 0.016 {I14} (2012Me03) and 0.010 {I7} (2018Ab06)
32S G 2911 0.030 LT ?
32S cG RI$ 2012Me03 give branching ratio<3.4.
32S G 3412.4 7 0.141 12
32S cG E$weighted average of 3412.2 {I7} (2012Me03) and 3412.5 {I7} (2018Ab06)
32S cG RI$weighted average of 0.122 {I19} (2012Me03) and 0.148 {I12}
32S 2cG (2018Ab06)
32S G 4959.2 8 0.268 18
32S cG E$weighted average of 4959.6 {I8} (2012Me03) and 4958.7 {I9} (2018Ab06)
32S cG RI$weighted average of 0.32 {I4} (2012Me03) and 0.262 {I14} (2018Ab06)
32S G 7190.4 15 0.169 22
32S cG E$weighted average of 7194 {I3} (1973De08) and 7189.8 {I12} (2012Me03)
32S cG RI$from 2012Me03. Other: 0.41 {I10} (1973De08) is discrepant
32S dG RI$ quoted uncertainty=+0.024-0.020 (2012Me03)
32S L 7484.6 15 2+
32S E 0.064 6 5.83 4 0.064 6
32S S E EAV=1907.47 79
32S G 2480 0.070 LT ?
32S G 3203 0.006 LT ?
32S G 7483.7 15 0.064 6
32S L 7535.5 6 0+
32S 2 L ISPIN=1
32S E 0.183 11 1.8E-4 1 5.35 3 0.183 11
32S S E EAV=1882.75 41$CK=9.1154E-4 56$CL=8.5778E-5 53$CM+=1.04806E-5 64
32S cE $M(>)=0.164 {I9}
32S G 2839.7 5 0.183 11
32S cG E$from 2012Me03. Other: 2839.7 {I5} (2018Ab06)
32S cG RI$from 2018Ab06. Other: 0.185 {I18} (2012Me03)
32S G 5304 0.031 LT ?
32S G 7534 0.042 LT ?
32S L 7637 0+
32S DL E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT
32S cL E$rounded value from Adopted Levels
32S cL J$2012Me03 also propose 0+ based on shell-model calculation
32S 2 L ISPIN=0
32S E 0.028 LT 3.04E-5LT 6.12 GT 0.028 LT ?
32S S E EAV=1833.49 29$CK=9.8157E-4 44$CL=9.2369E-5 41$CM+=1.12860E-5 50
32S cE $M(>)<0.05.
32S G 3355 0.028 LT ?
32S L 7923.8 11 0+
32S 2 L ISPIN=0
32S cL J$2012Me03 also propose 0+ based on shell-model calculation
32S E 0.036 77 0.0000511 6.2 3 0.036 77
32S S E EAV=1694.59 61$CK=1.2229E-3 12$CL=1.1509E-4 12$CM+=1.4062E-5 14
32S cE $M(>)=0.087 {I19}
32S G 5692.3 11 0.036 7
32S cG E$weighted average of 5693.3 {I13} (2012Me03) and 5691.6 {I11}
32S 2cG (2018Ab06)
32S cG RI$weighted average of 0.033 {I14} (2012Me03) and 0.037 {I7} (2018Ab06)
32S dG RI$ quoted uncertainty=+0.014-0.013 (2012Me03)
32S L 8126.5 16 1+
32S 2 L ISPIN=1
32S E 0.045 6 7E-5 1 5.66 6 0.045 6
32S S E EAV=1596.71 83$CK=1.4436E-3 21$CL=1.3586E-4 20$CM+=1.6600E-5 24
32S cE $M(>)<0.20.
32S G 3120 0.015 LT ?
32S G 5895 0.015 LT ?
32S G 8125.4 16 0.045 6
32S L 8407.9 15 2+
32S E 0.033 5 7E-5 1 5.6 1 0.033 5
32S S E EAV=1461.29 78$CK=1.8483E-3 27$CL=1.7396E-4 26$CM+=2.1256E-5 32
32S G 3400 0.012 LT ?
32S G 3714 0.045 LT ?
32S G 4126 0.016 LT ?
32S G 4625 0.052 LT ?
32S G 8406.7 15 0.033 5
32S L 8692 5 2+
32S cL $E(|a)=1526 {I5}
32S E 0.0011 2 3.0E-6 5 6.9 1 0.0011 2
32S S E EAV=1325.2 24$CK=2.428E-3 12$CL=2.285E-4 12$CM+=2.792E-5 14
32S cE TI$from %I(|a)=0.0011 {I2} (1979Ho27).
32S L 8861.1 16 2+
32S cL $E(|a)=1673 {I5}
32S E 0.061 11 2.0E-4 4 5.1 1 0.061 11
32S S E EAV=1244.55 81$CK=2.8924E-3 53$CL=2.7226E-4 50$CM+=3.3266E-5 61
32S cE TI$from 2018Ab06, including %I(|a)=0.0146 {I20} (1979Ho27),
32S 2cE %I|g(8859.8|g)=0.024 {I5} from their work, and adopted branching
32S 3cE ratios of 3858|g and 6630|g
32S G 3858 0.013 LT ?
32S G 6630 0.012 LT ?
32S G 8859.8 16 0.024 5
32S L 9206.4 11 1+
32S 2 L ISPIN=1
32S E 0.047 7 2.2E-4 3 4.9 1 0.047 7
32S S E EAV=1080.81 59$CK=4.2892E-3 66$CL=4.0379E-4 62$CM+=4.9338E-5 76
32S cE $M(>)=0.58 {I+5-15}
32S cE TI$from 2018Ab06, also including all other adopted |g transitions that
32S 2cE are not observed in their work. Other: 0.22 {I7} from 2012Me03 is
32S 3cE discrepant
32S G 6973.5 13 0.057 42
32S cG E$from 2012Me03. Other: 6973.3 {I15} (2018Ab06)
32S cG RI$unweighted average of 0.098 {I18} (2012Me03) and 0.015 {I4}
32S 2cG (2018Ab06)
32S G 9207.3 19 0.016 5
32S L 9231 5 1-
32S cL $E(|a)=2201 {I5}
32S E 2E-4 1 1.0E-6 5 7.3 +2-3 0.0002 1
32S S E EAV=1069.2 24$CK=4.421E-3 28$CL=4.162E-4 26$CM+=5.085E-5 32
32S cE TI$from %I(p)<0.001, %I(|a)=2|*10{+-4} {I1} (1979Ho27).
32S L 9463 5 2+
32S cL $E(|a)=2201 {I5}
32S E 0.030 4 2.0E-4 3 4.91 6 0.030 4
32S S E EAV=960.1 24$CK=5.975E-3 41$CL=5.625E-4 39$CM+=6.874E-5 47
32S cE TI$from %I(p)<5.0|*10{+-4}, %I(|a)=0.030 {I4} (1979Ho27).
32S L 9650.3 12 2+
32S cL $E(p)=762 {I5}
32S E 0.101 15 0.0008813 4.2 1 0.102 15
32S S E EAV=872.83 63$CK=7.812E-3 16$CL=7.355E-4 15$CM+=8.987E-5 18
32S cE TI$from 2018Ab06, also including %I(p)=0.0052 {I8} and
32S 2cE %I(|a)<2.0|*10{+-4} (1979Ho27), and all other adopted |g transitions
32S 3cE that are not observed in their work.
32S G 4101 0.038 LT ?
32S G 4643 0.015 LT ?
32S G 4954.2 11 0.038 8
32S G 5368 0.018 LT ?
32S G 5871 0.004 LT ?
32S G 7419 ?
32S L 9710 5 2+
32S cL $E(|a)=2417 {I5}
32S E 0.0040 7 3.8E-5 7 5.6 1 0.0040 7
32S S E EAV=845.1 23$CK=8.554E-3 67$CL=8.055E-4 63$CM+=9.842E-5 77
32S cE TI$from %I(p)<0.0015, %I(|a)=0.0040 {I7} (1979Ho27).
32S L 9887 5 (2)+
32S cL $E(p)=991 {I5}
32S E 0.0112 17 1.4E-4 2 4.9 1 0.0113 17
32S S E EAV=763.2 23$CK=1.1398E-2 98$CL=1.0733E-3 92$CM+=1.312E-4 11
32S cE TI$from %I(p)=0.0113 {I17}, %I(|a)<8.0|*10{+-5} (1979Ho27).
32S L 9949 5 0+,1+,2+
32S cL $E(p)=1051 {I5}
32S E 0.0019 4 2.7E-5 6 5.6 1 0.0019 4
32S S E EAV=734.6 23$CK=0.01269 11$CL=1.195E-3 11$CM+=1.460E-4 13
32S cE TI$from %I(p)=0.0019 {I4}, %I(|a)<1.0|*10{+-4} (1979Ho27).
32S L 9983 5 2
32S cL $E(|a)=2656 {I5}
32S E 0.00068 20 1.0E-5 3 6.0 1 0.00069 20
32S S E EAV=719.0 23$CK=0.01349 12$CL=1.270E-3 12$CM+=1.552E-4 14
32S cE TI$from %I(p)<3.0|*10{+-4}, %I(|a)=0.00069 {I20} (1979Ho27).
32S L 10231 5 1+
32S cL $E(p)=1324 {I5}
32S E 0.0051 8 1.3E-4 2 4.9 1 0.0052 8
32S S E EAV=606.0 23$CK=0.02188 23$CL=2.061E-3 22$CM+=2.518E-4 27
32S cE TI$from %I(p)=0.0052 {I8}, %I(|a)<6.0|*10{+-5} (1979Ho27).
32S L 10291 5 2+
32S cL $E(p)=1381 {I5}, E(|a)=2927 {I5}
32S E 0.0024 3 6.9E-5 8 5.11 5 0.0025 3
32S S E EAV=578.9 23$CK=0.02491 28$CL=2.346E-3 26$CM+=2.867E-4 32
32S cE TI$from %I(p)=0.00078 {I20}, %I(|a)=0.0017 {I3} (1979Ho27).
32S L 10459 5 0+
32S cL $E(|a)=3072 {I5}
32S E 2.3E-4 10 1.0E-5 4 5.9 2 0.00024 10
32S S E EAV=503.6 23$CK=0.03698 47$CL=3.484E-3 44$CM+=4.257E-4 54
32S cE TI$from %I(p)<2.0|*10{+-4}, %I(|a)=2.4|*10{+-4} {I10} (1979Ho27).
32S L 10531 5 2+
32S cL $E(|a)=3135 {I5}
32S E 0.00080 19 4.1E-5 10 5.2 1 0.00084 20
32S S E EAV=471.6 22$CK=0.04453 60$CL=4.195E-3 56$CM+=5.126E-4 69
32S cE TI$from %I(p)<2.0|*10{+-4}, %I(|a)=0.00084 {I20} (1979Ho27).
32S L 10780 5 2+
32S cL $E(p)=1856 {I5}
32S E 0.0014 3 1.7E-4 3 4.5 1 0.0016 3
32S S E EAV=362.5 22$CK=0.0930 16$CL=0.00876 15$CM+=1.071E-3 18
32S cE TI$from %I(p)=0.0016 {I3}, %I(|a)<2.0|*10{+-4} (1979Ho27).
32S L 10792 5 (2)+
32S cL $E(|a)=3364 {I5}
32S E 4.6E-4 9 6E-5 1 5.0 1 0.00051 10
32S S E EAV=357.3 22$CK=0.0968 16$CL=0.00912 15$CM+=1.114E-3 19
32S cE TI$from %I(p)<2.0|*10{+-4}, %I(|a)=0.00051 {I10} (1979Ho27).
32S L 11063 5 0+,2+
32S cL $E(|a)=3601 {I5}
32S E 4E-5 2 1.7E-5 9 5.4 +2-3 0.00006 3
32S S E EAV=241.6 21$CK=0.2625 53$CL=0.02475 50$CM+=3.024E-3 61
32S cE TI$from %I(p)<2.0|*10{+-4}, %I(|a)=6|*10{+-5} {I3} (1979Ho27).