123TE 123I EC DECAY (13.2230 H) 1976WA13,2012Ko47 21NDS 202105 123TE H TYP=ERR$AUT=Jun Chen$CUT=27-Aug-2021$ 123TE2 H COM=added missing EC fractions by running log| {Ift} 123TE H TYP=FUL$AUT=Jun Chen$CIT=NDS 174, 1 (2021)$CUT=15-Apr-2021$ 123TE DG CC$FROM BrIcc v2.3 (29-Mar-2013) 2008Ki07, "Frozen Orbitals" appr. 123TE c 2012Ko47: radionuclide {+123}I was produced at the IPEN Cyclone-30 123TE2c cyclotron at the Nuclear Metrology Laboratory (LMN) at the Nuclear and 123TE3c Energy Research Institute (IPEN) , by means of {+124}Xe(p,2n){+123}Cs 123TE4c reaction, followed by {+123}Cs decay. |g and X rays were detected by 123TE5c NaI(Tl) and HPGe detectors and electrons were detected by a gas-flow or 123TE6c pressured 4|p proportional counter in 4|p|b-|g coincidence systems. 123TE7c Measured E|g, I|g, E(X-ray), I(X-ray), E|b, I|b. Deduced |g-ray 123TE8c emission probabilities, 159|g conversion coefficient from the 123TE9c experimental extrapolation curve. Comparisons with available data. 123TE c 1976Wa13: {+123}I source was produced via {+123}Te(p,n) on isotopically 123TE2c enriched targets at Lawrence Livermore Laboratory. |g rays were 123TE3c detected with ordinary and Compton-suppressed Ge(Li) spectrometers. 123TE4c Measured E|g, I|g. Deduced levels, J, |p, |b branching ratios, 123TE5c log {Ift}. Comparisons with theoretical calculations. Systematics of 123TE6c neighboring Te isotopes. 123TE c 1979Sc13: {+123}I activity was obtained from the decay of {+123}Xe 123TE2c produced by proton bombardment of iodine. |g rays were detected with 123TE3c a NaI detector. Measured E|g, |g(|q,t). Deduced levels, J, |p, |g-ray 123TE4c mixing ratios. Deduced magnetic moment of {+123}I g.s. using the 123TE5c technique of nuclear magnetic resonance of oriented nuclei (NMR/ON). 123TE c 1970Sp03: source of {+123}I was produced by high-energy spallation 123TE2c of 3 GeV proton from the Princeton-Pennsylvania Accelerator on a 123TE3c natural lanthanum target. |g rays were detected with four Ge(Li) 123TE4c detectors. Measured E|g, I|g, |g|g-coin. Deduced levels. Comparisons 123TE5c with available data. 123TE c 1968Ra11: source of {+123}I was produced by {+121}Sb({+4}He,2n) with 123TE2c 30 MeV {+4}He beam from the MIT cyclotron on Sb metal (98.4% in 123TE3c {+121}Sb). |g rays were detected with a Ge(Li) detector and a NaI(Tl) 123TE4c crystal. Measured E|g, I|g, |g|g-coin. Deduced levels, J, |p, |b 123TE5c branching ratios, log {Ift}. Comparisons with theoretical calculations. 123TE6c Systematics of neighboring Te isotopes. 123TE c 1969Se09: {+123}I source was produced via Te(p,xn) with 80 MeV proton 123TE2c beam from the synchrocyclotron at Orsay. |g rays were detected with a 123TE3c Ge(Li) detector and a NaI detector. Measured E|g, I|g, |g|g-coin, 123TE4c |g|g(|q). Deduced |g-ray mixing ratios. See 1967Se05 for deduced 123TE5c levels, J, |p, |b-decay branching ratios, log {Ift}. 123TE c Others: 123TE c I|g: 1960Gu02, 1986AgZW, 1986Fl03, 1987Ja13, 1990Ma24 123TE c Parent T{-1/2}: 2012Re25, 2018Bo02, 2004Da05, 1973Ka45 123TE cE TI$From |g+ce intensity balance at each level 123TE cG E,RI$From 1976Wa13, unless otherwise noted. 123TE2cG Intensities quoted as from 2012Ko47 are deduced by the evaluator 123TE3cG by normalizing their absolute intensities to I(159|g)=100. For values 123TE4cG from 1976Wa13, a 3% uncertainty has been added in quadruture by the 123TE5cG evaluator to the quoted uncertainties in 1976Wa13 to account for the 123TE6cG uncertainty in efficiency calibration, which is normally 2%-3% and is 123TE7cG considered not included by 1976Wa13, since some of their uncertainties 123TE8cG are unrealistically small (<1%). 123TE cG E(A)$From energy difference of E(levels). 123TE cG M,MR$From Adopted Gammas. Values from this study are given in comments. 123TE cG MR(X)$Adopted value is deduced (by the evaluator) from A{-4}=0 and 123TE2cG A{-2} (given in comments) of |g-159|g(|q) in 1969Se09 with adopted 123TE3cG |d(E2/M1)=+0.079 {I11} for 159|g. 123TE cL E$From a least-squares fit to |g-ray energies, assuming |DE|g=0.3 keV 123TE2cL where not given. 123TE cL J,T$From Adopted Levels. 123I P 0.0 5/2+ 13.2230 H 19 1228 3 123I cP J,T$From Adopted Levels of {+123}I 123I cP QP$From 2021Wa16 123TE N 0.8360 19 1.00 123TE cN NR$From |SI(|g+ce to g.s.+247.5 levels)=100. No direct |e decay to 123TE2cN g.s. and 247.5 level is expected. 123TE PN 3 123TE G 190.7 1 0.0006 2 123TE2 G %IG=0.00050 17 123TE G 259.0 2 0.0011 5 123TE2 G %IG=0.0009 5 123TE G 574 1 0.007 ? 123TE2 G %IG=0.005852 13 123TE cG E,RI$from 1967Se05 only 123TE G 760.85 200.00075 25 123TE2 G %IG=0.00063 21 123TE G 898.2 2 0.0007 4 123TE2 G %IG=0.0006 4 123TE L 0.0 1/2+ 123TE L 159.00 33/2+ 196 PS 10 123TE E 97.0 5 5.255 4 97.0 5 123TES E CK=0.8534$CL=0.11590 2$CM+=0.030717 5 123TE G 159.00 5 100 M1+E2 +0.079 11 0.187 C 123TE2 G %IG=83.60 19 123TES G KC=0.1611 23$LC=0.0209 3$MC=0.00417 6 123TES G NC=0.000824 12$OC=8.91E-5 13 123TEB G BM1W=0.0234 11$BE2W=2.5 5 123TE cG E$weighted average of 159.1 {I1} (1968Ra11), 159.0 {I3} (1970Sp03), and 123TE2cG 158.97 {I5} (1976Wa13). Other: 159 {I1} (1967Se05) 123TE cG MR$0.18 {I+8-14} from |a(exp)=0.1905 {I32} (2012Ko47), using the 123TE2cG BrIccMixing program 123TE L 247.5 11/2- 119.2 D 3 M 123TE DL E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 123TE cL E$rounded value from Adopted Levels 123TE L 440.01 43/2+ 22 PS 4 123TE cL J$spin=3/2 from |g|g(|q) in 1969Se09 123TE E 0.424 13 7.34 2 0.424 13 123TES E CK=0.8510$CL=0.11775 3$CM+=0.031290 9 123TE cE IE$0.015 {I16} with a 95% confidence level from a direct measurement by 123TE2cE 1990Ma24 123TE G 281.03 5 0.086 3 M1+E2 -0.24 +10-140.0409 8 XC 123TE2 G %IG=0.072 3 123TES G KC=0.0352 6$LC=0.00454 17$MC=0.00091 4 123TES G NC=0.000179 7$OC=1.93E-5 6 123TE cG E$others: 281.0 {I5} (1968Ra11), 281.3 {I5} (1970Sp03), 282 {I1} 123TE2cG (1967Se05). Other: 282 {I1} (1967Se05), 275 {I10} (1960Gu02) 123TE cG RI$weighted average of 0.08 {I1} (1968Ra11), 0.08 {I3} (1970Sp03), 123TE2cG 0.095 {I3} (1976Wa13), and 0.0841 {I16} (2012Ko47). Other: 0.053 123TE3cG (1967Se05), 0.14 {I3} (1960Gu02) 123TE cG MR$from A{-2}=-0.26 {I3} of 281|g-159|g(|q) (1969Se09), also giving 123TE2cG other possible |d=-1.9 {I5} which is less likely since it would 123TE3cG require a much larger B(E2)(W.u.). Others: -0.08 to 0, or +3.4 to +4.9 123TE4cG from |d{+2}/(1+|d{+2})<0.007 (|d<0) or 0.92 to 0.96 (|d>0), 123TE5cG respectively, from |g(|q) anisotropy in 1979Sc13 123TE G 440.02 5 0.464 12M1+E2 -2.1 1 0.01199 C 123TE2 G %IG=0.388 10 123TES G KC=0.01021 15$LC=0.001432 20$MC=0.000287 4 123TES G NC=5.62E-5 8$OC=5.83E-6 9 123TE cG E$weighted average of 440.4 {I5} (1968Ra11), 440.2 {I4} (1970Sp03), and 123TE2cG 440.02 {I5} (1976Wa13). Others: 440 {I1} (1967Se05), 439.2 (1969Se09), 123TE3cG 440.0 (1987Ja13), 435 {I10} (1960Gu02) 123TE cG RI$weighted average of 0.42 {I2} (1968Ra11), 0.42 {I8} (1970Sp03), 123TE2cG 0.514 {I17} (1976Wa13), 0.464 {I9} (2012Ko47), 0.450 {I15} (1987Ja13), 123TE3cG and 0.44 {I9} (1960Gu02). Other: 0.255 (1967Se05) 123TE cG MR$+0.14 to +0.20, or -4.9 to -2.5 from |d{+2}/(1+|d{+2})=0.02 to 0.04 123TE2cG (|d>0) or 0.86 to 0.96 (|d<0), respectively, from |g(|q) anisotropy in 123TE3cG 1979Sc13 123TE L 489.73 8 7/2+ 30.7 NS 4 123TE E 0.0026 14 9.5 3 0.0026 14 123TES E CK=0.8503$CL=0.11824 4$CM+=0.03144 1 123TE G 330.70 8 0.0139 7 [E2] 0.0282 123TE2 G %IG=0.0116 6 123TES G KC=0.0236 4$LC=0.00370 6$MC=0.000748 11 123TES G NC=0.0001450 21$OC=1.447E-5 21 123TE cG RI$other: 0.0149 {I6} for 330.7|g+329.4|g (2012Ko47) 123TE L 505.34 4 5/2+ 13 PS 3 123TE cL J$spin=5/2 from |g|g(|q) in 1969Se09 123TE E 0.405 11 7.28 1 0.405 11 123TES E CK=0.8501$CL=0.11840 4$CM+=0.03149 1 123TE G 346.36 5 0.144 3 M1+E2 +0.07 8 0.0236 XC 123TE2 G %IG=0.120 3 123TES G KC=0.0204 3$LC=0.00257 4$MC=0.000511 8 123TES G NC=0.0001012 15$OC=1.102E-5 16 123TE cG E$weighted average of 346.6 {I5} (1968Ra11), 347.0 {I5} (1970Sp03), and 123TE2cG 346.35 {I5} (1976Wa13). Others: 346 {I1} (1967Se05), 340 {I10} 123TE3cG (1960Gu02) 123TE cG RI$weighted average of 0.16 {I3} (1960Gu02), 0.12 {I2} (1968Ra11), 0.11 123TE2cG {I3} (1970Sp03), 0.151 {I5} (1976Wa13), and 0.142 {I3} (2012Ko47). 123TE3cG Other: 0.087 (1967Se05) 123TE cG MR$from A{-2}=+0.006 {I30} of 346|g-159|g(|q) in 1969Se09, also giving 123TE2cG other possible |d=+3.4 {I+13-8} which is less likely since it would 123TE3cG require a much larger B(E2)(W.u.). Others: +0.20 to +0.29 from 123TE4cG |d{+2}/(1+|d{+2})=0.04 to 0.08 (|d>0) from |g(|q) anisotropy in 123TE5cG 1979Sc13, with J(688)=5/2 123TE G 505.33 5 0.344 9 (E2) C 123TE2 G %IG=0.288 8 123TE cG E$others: 505.6 {I6} (1968Ra11), 505.6 {I5} (1970Sp03), 505 {I1} 123TE2cG (1967Se05), 500 {I10} (1960Gu02) 123TE cG RI$weighted average of 0.31 {I5} (1968Ra11), 0.32 {I8} (1970Sp03), 123TE2cG 0.379 {I12} (1976Wa13), 0.337 {I6} (2012Ko47), and 0.28 {I6} 123TE3cG (1960Gu02). Other: 0.193 (1967Se05) 123TE cG M$Q from |g(|q) anisotropy in 1979Sc13 123TE L 532.82 11(7/2-) 123TE E 0.0044 5 9.21 5 0.0044 5 123TES E CK=0.8497$CL=0.11871 4$CM+=0.03159 2 123TE G 285.32 110.0051 5 123TE2 G %IG=0.0043 5 123TE L 599.57151/2+ 123TE G 599.69 160.0031 4 123TE2 G %IG=0.0026 4 123TE cG RI$from 2012Ko47. Other: 0.0031 {I11} (1976Wa13) 123TE L 687.97 43/2+ 123TE cL J$spin=3/2 from |g|g(|q) in 1969Se09; 5/2 from |g(|q) anisotropy in 123TE2cL 1979Sc13 123TE E 1.51 5 6.45 2 1.51 5 123TES E CK=0.8466$CL=0.12110 6$CM+=0.03233 2 123TE G 182.62 6 0.0156 7 [M1,E2] 0.17 4 C 123TE2 G %IG=0.0130 6 123TES G KC=0.14 3$LC=0.024 10$MC=0.0048 21 123TES G NC=0.0009 4$OC=9.E-5 3 123TE cG E$weighted average of 183.7 {I10} (1968Ra11), 183.0 {I7} (1970Sp03), 123TE2cG and 182.61 {I6} (1976Wa13). Other: 183 {I1} (1967Se05) 123TE cG RI$weighted average of 0.03 {I2} (1968Ra11), 0.03 {I1} (1970Sp03), 123TE2cG 0.0155 {I7} (1976Wa13), and 0.018 {I7} (2012Ko47). Other: 0.026 123TE3cG (1967Se05) 123TE G 198.23 0.004 1 [E2] 0.1545 123TE2 G %IG=0.0033 9 123TES G KC=0.1242 18$LC=0.0243 4$MC=0.00497 7 123TES G NC=0.000952 14$OC=8.92E-5 13 123TE cG RI$other: 0.003 {I5} for 198.2|g+197.2|g (2012Ko47) 123TE G 247.97 5 0.0829 18 (M1+E2) 0.064 8 C 123TE2 G %IG=0.0693 16 123TES G KC=0.054 5$LC=0.0083 21$MC=0.0017 5$NC+=0.00039 10 123TE cG E$weighted average of 248.3 {I5} (1968Ra11), 248.4 {I5} (1970Sp03), and 123TE2cG 247.96 {I5} (1976Wa13). Other: 248 {I1} (1967Se05) 123TE cG RI$weighted average of 0.08 {I1} (1968Ra11), 0.07 {I2} (1970Sp03), 123TE2cG 0.085 {I3} (1976Wa13), and 0.0824 {I18} (2012Ko47). Other: 0.070 123TE3cG (1967Se05) 123TE cG MR$-0.55 to -0.14, or -2.1 to -1.0 from |d{+2}/(1+|d{+2})=0.02 to 0.23 123TE2cG or 0.48 to 0.81 (|d<0), respectively, from |g(|q) anisotropy in 123TE3cG 1979Sc13, with J(688)=5/2 123TE G 528.97 5 1.52 12 (M1+E2) C 123TE2 G %IG=1.27 10 123TE cG E$weighted average of 529.0 {I4} (1968Ra11), 529.3 {I4} (1970Sp03), and 123TE2cG 528.96 {I5} (1976Wa13). Others: 529.0 (1987Ja13), 530 {I10} (1960Gu02) 123TE cG RI$unweighted average of 1.27 {I11} (1968Ra11), 1.26 {I24} (1970Sp03), 123TE2cG 1.67 {I5} (1976Wa13), 1.49 {I3} (2012Ko47), 1.411 {I29} (1987Ja13), and 123TE3cG 2.0 {I3} (1960Gu02). Other: 0.780 (1967Se05) 123TE cG MR$-0.09 {I6} or -2.8 {I+6-7} deduced (by the evaluator) from 123TE2cG A{-2}=-0.19 {I2} of 529|g-159|g(|q) in 1969Se09, using adopted 123TE3cG |d(E2/M1)=+0.079 {I11} for 159|g, with J(688)=3/2. Others: 123TE4cG +0.44 to +0.64, or +4 to +10 from |d{+2}/(1+|d{+2})=0.16 to 0.29 or 123TE5cG 0.94 to 0.99 (|d>0), respectively, from |g(|q) anisotropy in 1979Sc13, 123TE6cG with J(688)=5/2 123TE G 687.94 8 0.0321 9 123TE2 G %IG=0.0268 8 123TE cG E$weighted average of 687.7 {I6} (1968Ra11), 687.7 {I5} (1970Sp03), and 123TE2cG 687.95 {I8} (1976Wa13). Other: 688 {I1} (1967Se05) 123TE cG RI$weighted average of 0.03 {I1} (1968Ra11), 0.04 {I2} (1970Sp03), 123TE2cG 0.0321 {I18} (1976Wa13), and 0.0321 {I9} (2012Ko47). Others: 0.017 123TE3cG (1967Se05), <0.08 (1960Gu02) 123TE L 697.53 5(7/2)+ 123TE cL J$spin=7/2 from |g|g(|q) in 1969Se09 123TE E 0.406 13 7.00 2 0.406 13 123TES E CK=0.8463$CL=0.12130 7$CM+=0.03239 2 123TE G 192.18 7 0.0212 13 [M1,E2] 0.14 3 C 123TE2 G %IG=0.0177 11 123TES G KC=0.117 21$LC=0.020 8$MC=0.0040 16 123TES G NC=0.0008 3$OC=7.6E-5 24 123TE cG E$weighted average of 192.7 {I10} (1968Ra11), 193 {I1} (1970Sp03), and 123TE2cG 192.17 {I7} (1976Wa13). Other: 192 {I1} (1967Se05) 123TE cG RI$weighted average of 0.03 {I2} (1968Ra11), 0.03 {I2} (1970Sp03), 123TE2cG 0.0238 {I11} (1976Wa13), and 0.0194 {I9} (2012Ko47). Other: 0.023 123TE3cG (1967Se05) 123TE G 207.80 0.0013 4 [M1,E2] 0.111 21 A 123TE2 G %IG=0.0011 4 123TES G KC=0.092 15$LC=0.015 6$MC=0.0031 11 123TES G NC=0.00059 20$OC=5.9E-5 17 123TE cG RI$other: 0.0046 {I5} for 207.8|g+206.8|g (2012Ko47) 123TE G 257.51 150.0018 5 [E2] 0.0637 123TE2 G %IG=0.0015 5 123TES G KC=0.0525 8$LC=0.00902 13$MC=0.00183 3 123TES G NC=0.000353 5$OC=3.43E-5 5 123TE cG RI$other: %I|g=0.00016 {I4} in Table 3 of 2012Ko47 could be a misprint 123TE G 538.54 5 0.37 4 C 123TE2 G %IG=0.31 4 123TE cG E$others: 538.5 {I5} (1968Ra11), 538.5 {I5} (1970Sp03), 538 {I1} 123TE2cG (1967Se05), 538.0 (1987Ja13) 123TE cG RI$unweighted average of 0.32 {I2} (1968Ra11), 0.31 {I6} (1970Sp03), 123TE2cG 0.458 {I15} (1976Wa13), 0.411 {I7} (2012Ko47) and 0.379 {I16} 123TE3cG (1987Ja13). Other: 0.195 (1967Se05) 123TE L 769.27 14 123TE E 0.0037 7 8.9 1 0.0037 7 123TES E CK=0.8440 2$CL=0.12306 9$CM+=0.03294 3 123TE G 329.38 170.0031 7 123TE2 G %IG=0.0026 6 123TE G 610.05 230.0013 4 123TE2 G %IG=0.0011 4 123TE cG RI$other: <0.00012 (2012Ko47) 123TE L 783.61 43/2+ 52 FS +33-21 123TE cL J$spin=(3/2,5/2) from |g|g(|q) in 1969Se09; 5/2 ruled out by |g(|q) 123TE2cL anisotropy in 1979Sc13 123TE E 0.150 4 7.27 2 0.150 4 123TES E CK=0.8434 2$CL=0.1235 1$CM+=0.03307 3 123TE G 278.36 120.0027 5 [M1,E2] 0.045 4 123TE2 G %IG=0.0023 5 123TES G KC=0.038 3$LC=0.0057 12$MC=0.00114 24 123TES G NC=0.00022 5$OC=2.3E-5 4 123TE G 343.73 140.0051 5 123TE2 G %IG=0.0043 5 123TE G 624.58 5 0.093 3 M1+E2 0.0050 6 C 123TE2 G %IG=0.078 3 123TES G KC=0.0043 5$LC=0.00055 4$MC=0.000109 8 123TES G NC=2.16E-5 15$OC=2.32E-6 21 123TE cG E$weighted average of 624.9 {I5} (1968Ra11), 624.9 {I5} (1970Sp03), and 123TE2cG 624.57 {I5} (1976Wa13). Other: 624 {I1} (1967Se05) 123TE cG RI$weighted average of 0.08 {I1} (1968Ra11), 0.07 {I2} (1970Sp03), 123TE2cG 0.100 {I3} (1976Wa13), and 0.0910 {I17} (2012Ko47). Other: 0.044 123TE3cG (1967Se05) 123TE cG MR$+0.10 to +0.18, or +2.3 to +4.9 from |d{+2}/(1+|d{+2})=0.01 to 0.03 123TE2cG or 0.84 to 0.96 (|d>0), respectively, from |g(|q) anisotropy in 123TE3cG 1979Sc13 123TE G 783.60 6 0.0634 20 M1+E2 123TE2 G %IG=0.0530 17 123TE cG E$weighted average of 784.4 {I6} (1968Ra11), 784.0 {I6} (1970Sp03), and 123TE2cG 783.59 {I6} (1976Wa13). Other: 784 {I1} (1967Se05) 123TE cG RI$weighted average of 0.05 {I1} (1968Ra11), 0.05 {I2} (1970Sp03), 123TE2cG 0.071 {I3} (1976Wa13), and 0.0624 {I12} (2012Ko47). Other: 0.030 123TE3cG (1967Se05) 123TE cG MR$+0.20 to +0.33, or -4.9 to -3.0 from |d{+2}/(1+|d{+2})=0.04 to 0.10 123TE2cG (|d>0) or 0.90 to 0.96 (|d<0), respectively, from |g(|q) anisotropy in 123TE3cG 1979Sc13 123TE L 894.77 83/2+,5/2+ 45 FS +24-14 123TE E 0.074 3 7.31 2 0.074 3 123TES E CK=0.8373 3$CL=0.12818 18$CM+=0.03453 6 123TE G 197.23 0.0004 2 [M1,E2] 0.13 3 A 123TE2 G %IG=0.00033 17 123TES G KC=0.108 19$LC=0.018 7$MC=0.0037 14 123TES G NC=0.0007 3$OC=7.0E-5 21 123TE G 206.80 0.004 1 [M1,E2] 0.112 22 A 123TE2 G %IG=0.0033 9 123TES G KC=0.093 15$LC=0.015 6$MC=0.0031 11 123TES G NC=0.00060 21$OC=6.0E-5 17 123TE G 295.19 0.0019 A 123TE2 G %IG=0.001588 4 123TE cG E,RI$From author's FIG.4; not given in table 2 (1976Wa13). Other: 123TE2cG I|g<0.00084 (2012Ko47) 123TE G 405.02 130.0032 4 123TE2 G %IG=0.0027 4 123TE cG RI$weighted average of 0.0035 {I7} (1976Wa13) and 0.0031 {I4} 123TE2cG (2012Ko47) 123TE G 454.76 150.0041 3 123TE2 G %IG=0.0034 3 123TE cG RI$weighted average of 0.0047 {I6} (1976Wa13) and 0.00396 {I24} 123TE2cG (2012Ko47) 123TE G 735.87 110.056 7 C 123TE2 G %IG=0.047 6 123TE cG E$unweighted average of 736.10 {I6} (1968Ra11), 735.6 {I6} (1970Sp03), 123TE2cG 735.78 {I7} (1976Wa13), and 736 {I1} (1967Se05) 123TE cG RI$unweighted average of 0.04 {I1} (1968Ra11), 0.05 {I2} (1970Sp03), 123TE2cG 0.074 {I3} (1976Wa13), and 0.0593 {I11} (2012Ko47). Other: 0.029 123TE3cG (1967Se05) 123TE G 894.8 2 0.00084 9 123TE2 G %IG=0.00070 8 123TE cG RI$weighted average of 0.0011 {I3} (1976Wa13) and 0.00082 {I9} 123TE2cG (2012Ko47) 123TE L 996.0712(5/2)- 123TE E 0.0036 5 8.3 1 0.0036 5 123TES E CK=0.8256 6$CL=0.1371 4$CM+=0.03732 13 123TE G 556.05 130.0030 3 123TE2 G %IG=0.0025 3 123TE cG RI$weighted average of 0.0037 {I5} (1976Wa13) and 0.00288 {I24} 123TE2cG (2012Ko47) 123TE G 837.10 200.00056 10 123TE2 G %IG=0.00047 9 123TE cG RI$weighted average of 0.0006 {I1} (1976Wa13) and 0.00049 {I13} 123TE2cG (2012Ko47) 123TE L 1036.65 123/2+ 43 FS +16-12 123TE E 0.0028 11 8.2 2 0.0028 11 123TES E CK=0.8166 9$CL=0.1439 7$CM+=0.03946 21 123TE G 437.5 3 0.0009 9 123TE2 G %IG=0.0008 8 123TE G 877.52 170.00086 11 123TE2 G %IG=0.00072 10 123TE cG E$Value of 887.52 listed in author's table 2 is a misprint. See FIG.4. 123TE cG RI$weighted average of 0.0013 {I8} (1976Wa13) and 0.00085 {I11} 123TE2cG (2012Ko47) 123TE G 1036.63 170.00092 7 123TE2 G %IG=0.00077 6 123TE cG RI$weighted average of 0.0012 {I3} (1976Wa13) and 0.00091 {I7} 123TE2cG (2012Ko47) 123TE L 1068.16 73/2+,5/2+ 123TE E 0.0079 8 7.55 5 0.0079 8 123TES E CK=0.8057 14$CL=0.1522 11$CM+=0.0421 4 123TE G 174.2 3 0.0010 3 [M1,E2] 0.19 5 123TE2 G %IG=0.0008 3 123TES G KC=0.16 4$LC=0.028 13$MC=0.006 3 123TES G NC=0.0011 5$OC=0.00011 4 123TE cG RI$weighted average of 0.0010 {I3} (1976Wa13) and 0.0012 {I6} 123TE2cG (2012Ko47) 123TE G 562.79 120.00108 16 123TE2 G %IG=0.00090 14 123TE cG RI$weighted average of 0.0013 {I5} (1976Wa13) and 0.00106 {I16} 123TE2cG (2012Ko47) 123TE G 578.26 200.0019 5 123TE2 G %IG=0.0016 5 123TE cG RI$weighted average of 0.0018 {I5} (1976Wa13) and 0.0024 {I10} 123TE2cG (2012Ko47) 123TE G 628.26 220.0019 3 123TE2 G %IG=0.0016 3 123TE G 909.12 120.00155 11 123TE2 G %IG=0.00130 10 123TE cG RI$weighted average of 0.0016 {I3} (1976Wa13) and 0.00154 {I11} 123TE2cG (2012Ko47) 123TE G 1068.12 150.00145 25 123TE2 G %IG=0.00121 21 123TE cG RI$unweighted average of 0.0017 {I1} (1976Wa13) and 0.00120 {I10} 123TE2cG (2012Ko47)