194PT 194IR B- DECAY (19.18 H) 2016KR06,1976CL03,1974HEYW21NDS 202109
194PT H TYP=FUL$AUT=Jun Chen and Balraj Singh$CIT=NDS 177, 1 (2021)$
194PT2 H CUT=3-Sep-2021$
194PT c 2016Kr06: {+194}Ir sources produced by neutron irradiation of natural
194PT2c Ir metal, natural IrCl{-3} and 98% enriched {+193}Ir at Oregon State
194PT3c University TRIGA reactor. Measured E|g, I|g, half-life of {+194}Ir
194PT4c activity. A total of 15 gamma spectra were collected using HPGe
194PT5c detectors. The samples were recounted for 5-7 days at distances of
194PT6c 20-28 cm in the beginning and 5-10 cm at the end. Comparison with
194PT7c previous experimental results.
194PT c 1976Cl03 (also 1976ClZT): {+194}Ir sources were produced by thermal
194PT2c neutron irradiation of isotopically enriched (98.7%) {+193}Ir in the
194PT3c Georgia Tech Research Reactor. |g rays were detected with Ge(Li)
194PT4c detectors and conversion electrons were detected with a Si(Li)
194PT5c detector. Measured E|g, I|g, E(ce), I(ce), |g|g-coin, |g|g(|q). Deduced
194PT6c levels, J, |p, decay branching ratios, log| {Ift}, B(E2). Systematics
194PT7c of neighboring Pt isotopes. Comparisons with theoretical calculations.
194PT8c Authors mention that the conversion intensities and coefficients
194PT9c determined from their study are in good agreement with the data of
194PTac {+194}Au |e decay in 1960Ba17, 1964Be23, 1970Be30 and 1971Vi15, but no
194PTbc data are given in 1976Cl03.
194PT c 1974HeYW: measured E|g, I|g with a 55 cm{+3} coaxial Ge(Li) detector.
194PT2c Deduced levels
194PT c Other measurements:
194PT c 1983Ri14: measured |g(|q) and |g(lin pol), 0+ spins for 1267, 1479
194PT2c and 1547 levels, and mixing ratios of 889, 1184 and 1294 transitions
194PT c 1976Ra33: measured |b spectra using a magnetic spectrometer, energies
194PT2c and shape factor of 1- to 0+ and 1- to 2+ |b transition.
194PT c 1975Ka42: measured |g|g(|q,H,t), g factors of the first and second
194PT2c 2+ states, IPAC method.
194PT c 1975Pr11: measured |b|g(|q) for 1- to 2+ to 0+ |b|g-cascade
194PT c 1974BeYP: measured |g|g(|q)
194PT c 1973Si22: measured |g|g(|q) for several cascades using Ge(Li)-NaI(Tl),
194PT2c deduced spins of levels, and multipole mixing ratios of several
194PT3c transitions.
194PT c 1972Be53: measured (ce)|g(t), lifetimes of the first and second
194PT2c 2+ states
194PT c 1972Ro30: measured ce, (ce)x- and (ce)|g-coin.
194PT c 1971Ba79: measured ce, K-conversion coefficient for 293|g, deduced
194PT2c mixing ratio
194PT c 1970Si17: measured |g(|q) of 329 and 646 transitions from polarized
194PT2c nuclei
194PT c 1970Ke14: measured |g|g(|q,H), g factors of 329 and 622 levels
194PT c 1970Br09, 1970BrZW: measured |b(|q,Temp)
194PT c 1969Re06: measured E|g for 37 |g rays, |g(|q,Temp), mixing ratios
194PT c 1968Bu15: measured E|g, I|g of 28 |g rays
194PT c 1967Pa02: measured E|g, I|g for 32 |g rays
194PT c 1967Al09: measured (ce)|g(|q)
194PT c 1966Wi06: measured absolute I|g for three transitions
194PT c 1966Ag02: measured |g|g(|q,H), g factors of 329 and 622 levels
194PT c 1965Ma10: measured |b|g-, (ce)|g-, (ce)|b- and |g|g-coin, E|b, I|b,
194PT2c |g|g(|q) using a magnetic spectrometer and NaI(Tl) detector.
194PT c 1965Ke11: measured |g|g(|q,H), g factors
194PT c 1963Ma08: measured E|g for two |g rays using a curved-crystal
194PT2c spectrometer
194PT c 1962Bu03: measured |g|g(|q) for five |g|g-cascades
194PT c 1960Ma19: measured |g|g(|q) for two cascades, two 0+ excited states
194PT c 1959Jo35: measured |g|g(|q) for 937-329 and 643-620 |g|g cascades.
194PT c 1959Be54: measured E|g of 293|g and 328|g using a curbed-crystal
194PT2c spectrometer
194PT c 1955Ry53: measured E|g of 328|g using a curbed-crystal spectrometer
194PT c 1955Ma34: measured E|g, I|g for 11 |g rays, and |g|g(|q) for one
194PT2c cascade
194PT c 1954Bu02: measured E|g, I|g of five |g rays. Also measured E|g of
194PT2c two |g rays from {+194m}Ir decay
194PT c 1953Kr07: measured |g|g(|q) for one |g|g-cascade
194PT c 1951Co33, 1951Co01: measured ce
194PT c 1950Wi01: measured E|g of two |g rays
194PT c 1948Ma14: measured E|g, |b|g-coin
194PT d 1979Dz07: compilation of reference |g rays
194PT c ce data using external conversion: 1963Vi01, 1962Vi05,
194PT2c 1960Ke09, 1954Jo20.
194PT c |b{+-}, |b|g: 1966Wi06, 1954Jo20, 1941Wi07, 1936Al01
194PT c The total radiation energy released by {+194}Ir is 2228 keV
194PT2c {I37} (calculated by evaluators using the program RADLST).
194PT3c This value agrees with 2228.3 keV {I13} (2021Wa16), which constitutes
194PT4c a test for the self-consistency of the decay scheme.
194PT cB E$From |b|g-coin or |b(ce) data of 1965Ma10, unless stated otherwise
194PT cB IB$Deduced by evaluators from intensity balance considerations
194PT cG $A |g ray of E|g=2207 {I1}, I|g=0.010 {I3} is not reported in 2016Kr06
194PT2cG 1976Cl03. 2016Kr06 set an upper limit with I|g<0.0003.
194PT cG E,RI$Weighted averages of available values from 2016Kr06, 1976Cl03
194PT2cG and 1974HeYW, unless otherwise indicated.
194PT3cG Energies and intensities of the E0 transitions are taken from the
194PT4cG Adopted dataset, based on data from {+194}Au |e decay
194PT cG E(A)$This |g ray from 2016Kr06 only
194PT cG M,MR$From Adopted Gammas. Values from this study are given under
194PT2cG comments
194PT cL E$From a least-squares fit to E|g values. The uncertainties
194PT2cL of the following |g rays were increased to 0.05 keV to obtain the
194PT3cL least-squares fit within a reduced |h{+2}=1.6, a value for critical
194PT4cL |h{+2} at 95% confidence level: 699.331|g, 1186.408|g and 1512.072|g
194PT5cL doublet. Without these adjustments, reduced |h{+2}=2.9. Level energies
194PT6cL given here are very close (within 10 eV or so) to those given in
194PT7cL Table 2 of 2016Kr06
194PT cL J,T$From Adopted Levels. Supporting arguments or values from this study
194PT2cL are given under comments.
194IR P 0.0 1- 19.18 H 3 2228.3 13
194IR cP J,T$From {+194}Ir Adopted Levels
194IR cP QP$From 2021Wa16
194PT N 0.131 17 1.0 1.0 1.0
194PT PN 3
194PT cN NR$From I|g(328|g+294|g+301|g)/I|b(total)=0.160 {I20} (1966Wi06)
194PT L 0.0 0+
194PT B 85.4 19 8.22 1
194PTS B EAV=837.77 56
194PT cB E$2251 {I2} from |b spectrum using a magnetic spectrometer (1976Ra33).
194PT2cB Other: 2236 {I10} (1954Jo20)
194PT cB IB$89 from |b{+-} spectra (1965Ma10). Other: 1954Jo20
194PT cB $|b(|q,T) measurements (1970Br09,1970BrZW)
194PT L 328.475 7 2+ 41.7 PS 17
194PT cL T$other: |g|g(t) gives T{-1/2}=35.0 ps {I35} (1972Be53)
194PT cL $g-factor=+0.35 {I3} (1975Ka42, using T{-1/2}=35 ps {I3}), +0.28 {I3}
194PT3cL (1970Ke14, using T{-1/2}=37 ps {I4}), +0.24 {I3} (1966Ag02, using
194PT4cL T{-1/2}=45 ps {I5}), +0.21 {I3} (1965Ke11, using T{-1/2}=45 ps {I5}),
194PT5cL with all measured using the integral perturbed angular correlation
194PT6cL (IPAC). See Adopted Levels for |m values deduced from these g-factors
194PT7cL with adjustments for adopted T{-1/2}
194PT dL $Measured precession angle |w|t(mrad): 106.7 {I35} (1975Ka42), 87 {I4}
194PT2dL (1970Ke14), 99 {I9} (1966Ag02), 91.6 {I67} (1965Ke11), 97 {I4}
194PT3dL (1964BuAA: A. Buyrn and L. Grodzins MIT Progress Report No. 2098 (1964)
194PT4dL 251)
194PT B 9.3 13 8.9 1
194PTS B EAV=697.65 55
194PT cB E$1921 {I2} from |b spectrum using a magnetic spectrometer (1976Ra33).
194PT2cB Other: 1920 {I10} (1965Ma10)
194PT cB IB$from |b|g and |b(ce)-coin, I|b=5.1 {I6} (1965Ma10). Other: 1954Jo20
194PT cB $|b(|q,T) (1970Si17,1970Br09,1970BrZW) give L=1 as the
194PT2cB main component for 1920|b to the 328 level. The contribution from L=2
194PT3cB is <8% (1970Si17), <4% (1970Br09)
194PT G 328.467 10 100 1 E2 0.0755 C
194PTS G KC=0.0488 7$LC=0.0202 3$MC=0.00504 7
194PTS G NC=0.001236 18$OC=0.000203 3$PC=4.97E-6 7
194PT cG $E|g=328.473 {I10}, I|g=100 {I1} (2016Kr06)
194PT cG $E|g=328.448 {I14}, I|g=100.0 {I31} (1976Cl03)
194PT cG $E|g=328.501 {I30}, I|g=100 {I5} (1974HeYW)
194PT cG $|g(|q) (1970Si17) shows L=1 for 1920|b to 328 level
194PT L 622.023 7 2+ 35 PS 4
194PT cL T$adopted value from (ce)|g(t) (1972Be53)
194PT cL $g-factor from IPAC: 0.32 {I3} (1975Ka42, using T{-1/2}=38 ps {I4}),
194PT3cL 0.22 {I4} (1970Ke14, using T{-1/2}=44 ps {I6}), 0.15 {I5} (1966Ag02,
194PT4cL using T{-1/2}=62 ps {I14}), 0.13 {I3} (1965Ke11, using T{-1/2}=62 ps
194PT5cL {I14}). See Adopted Levels for |m values deduced from these g-factors
194PT6cL with adjustments for adopted T{-1/2}
194PT dL $Measured precession angle |w|t(mrad): 102.7 {I61} (1975Ka42), 91 {I15}
194PT2dL (1970Ke14), 83 {I20} (1966Ag02), 78 {I13} (1965Ke11)
194PT B 1.26 17 9.5 1
194PTS B EAV=574.56 54
194PT cB IB$from |b|g and |b(ce), I|b=1.24 {I15} (1965Ma10)
194PT G 293.544 10 19.1 2 E2+M1+E0 +15 2 0.1060 16 C
194PT2 G EKC=0.069 6 (1971Ba79)
194PTS G KC=0.0654 10$LC=0.0308 5$MC=0.00771 11
194PTS G NC=0.00189 3$OC=0.000307 5$PC=6.58E-6 10
194PT cG E$NRM weighted average
194PT cG $E|g=293.541 {I12}, I|g=19.1 {I2} (2016Kr06)
194PT cG $E|g=293.541 {I14}, I|g=19.5 {I8} (1976Cl03)
194PT cG $E|g=293.435 {I40}, I|g=18.1 {I15} (1974HeYW)
194PT cG MR$|d(E2/M1): from |g|g(|q) in {+194}Au |e decay
194PT cG $(294|g)(328|g)(|q): A{-2}=-0.115 {I8}, A{-4}=+0.06 {I2}
194PT2cG (1974BeYP). Other: A{-2}=-0.071 {I42}, A{-4}=+0.31 {I7} (1962Bu03)
194PT cG $From A{-2}=-0.13 {I2} and A{-4}=0.00 {I2} for (301|g)(ce(K)
194PT2cG 328)(|q) and (301|g)(ce(K) 294)(|q) (1967Al09), |d(294)=+8 {I2} and
194PTxcG E0/E2=0.01-0.13; (645|g)(293|g)(|q) in 1975Ka42 gives |d=+27 {I5}
194PT cG $|a(K)exp gives |d=6.2 {I6}
194PT G 622.003 20 2.56 3E2 0.01484 C
194PTS G KC=0.01141 16$LC=0.00262 4$MC=0.000627 9
194PTS G NC=0.0001543 22$OC=2.65E-5 4$PC=1.208E-6 17
194PT cG E$LWM weighted average
194PT cG $E|g=622.030 {I10}, I|g=2.56 {I3} (2016Kr06)
194PT cG $E|g=621.971 {I19}, I|g=2.56 {I10} (1976Cl03)
194PT cG $E|g=621.990 {I35}, I|g=2.52 {I18} (1974HeYW)
194PT L 811.297 12 4+
194PT G 482.823 13 0.351 3 E2 0.0270 C
194PTS G KC=0.0197 3$LC=0.00550 8$MC=0.001340 19
194PTS G NC=0.000329 5$OC=5.55E-5 8$PC=2.08E-6 3
194PT cG $E|g=482.818 {I10}, I|g=0.351 {I3} (2016Kr06)
194PT cG $E|g=482.857 {I26}, I|g=0.348 {I14} (1976Cl03)
194PT L 922.773 9 3+
194PT cL J$(301|g)(294|g)(|q) and (301|g)(328|g)(|q) in 1973Si22 give J=3
194PT B 0.31 4 10.5 1 1U
194PTS B EAV=445.33 50
194PT G 111.4 4 0.013 4 [M1,E2] 4.0 9 C
194PTS G KC=2.3 17$LC=1.3 7$MC=0.32 17
194PTS G NC=0.08 4$OC=0.013 6$PC=0.00026 20
194PT cG $E|g=111.4 {I4}, I|g=0.013 {I4} from |g|g-coin (1976Cl03). This |g is
194PT2cG not reported in 2016Kr06, but placed accepted in the decay scheme
194PT G 300.751 10 2.66 3 E2(+M1) 5 GT 0.102 5 C
194PTS G KC=0.064 4$LC=0.0283 5$MC=0.00706 11
194PTS G NC=0.00173 3$OC=0.000283 5$PC=6.5E-6 5
194PT cG $E|g=300.756 {I10}, I|g=2.66 {I3} (2016Kr06)
194PT cG $E|g=300.741 {I14}, I|g=2.66 {I11} (1976Cl03)
194PT cG $((301|g)(294|g)+(301|g)(294|g)(328|g))(|q): A{-2}=+0.02 {I5},
194PT2cG A{-4}=-0.02 {I8} (1973Si22). Consistent with M1 or E2 for 301|g
194PT G 594.288 10 0.502 8 E2(+M1) 10 GT 0.0166 3 C
194PTS G KC=0.01270 23$LC=0.00299 5$MC=0.000718 11
194PTS G NC=0.000177 3$OC=3.02E-5 5$PC=1.345E-6 25
194PT cG $E|g=594.287 {I10}, I|g=0.505 {I5} (2016Kr06)
194PT cG $E|g=594.291 {I19}, I|g=0.477 {I15} (1976Cl03)
194PT cG $(594|g)(328|g)(|q): A{-2}=-0.23 {I3}, A{-4}=-0.16 {I6}
194PT2cG (1973Si22). |d(594|g)>+50 or <-10
194PT L 1229.515 17 4+
194PT G 418.27 7 0.0060 8 (E2(+M1)) 3 GT 0.043 5 A
194PTS G KC=0.031 4$LC=0.0091 5$MC=0.00223 9
194PTS G NC=0.000547 23$OC=9.2E-5 5$PC=3.3E-6 5
194PT G 607.502 24 0.037 7 E2 0.01565 C
194PTS G KC=0.01199 17$LC=0.00279 4$MC=0.000670 10
194PTS G NC=0.0001649 23$OC=2.83E-5 4$PC=1.269E-6 18
194PT cG RI$unweighted average
194PT cG $E|g=607.497 {I18}, I|g=0.0435 {I10} (2016Kr06)
194PT cG $E|g=607.61 {I8}, I|g=0.030 {I3} (1976Cl03)
194PT L 1267.203 9 0+
194PT cL J$(939|g)(328|g)(|q) gives J=0 (1973Si22, 1962Bu03, 1960Ma19, 1959Jo35)
194PT B 1.78 24 8.5 1
194PTS B EAV=315.99 50
194PT cB IB$from |b|g and |bce, I|b=1.96 {I20} (1965Ma10)
194PT G 645.169 10 9.01 9 E2 0.01367 C
194PTS G KC=0.01057 15$LC=0.00237 4$MC=0.000566 8
194PTS G NC=0.0001393 20$OC=2.39E-5 4$PC=1.119E-6 16
194PT cG $E|g=645.175 {I10}, I|g=9.02 {I9} (2016Kr06)
194PT cG $E|g=645.146 {I20}, I|g=8.94 {I26} (1976Cl03)
194PT cG $E|g=645.162 {I30}, I|g=9.14 {I60} (1974HeYW)
194PT cG $(645|g)(328|g+293|g)(|q): A{-2}=-0.107 {I56}, A{-4}=+0.32 {I7}
194PT2cG (1962Bu03); A{-2}=+0.10 {I3}, A{-4}=+0.71 {I4} (1959Jo35). |g(|q)
194PT3cG (1970Si17,1983Ri14) shows no anisotropy
194PT cG $(645|g)(293|g)(|q): A{-2}=-0.049 {I5}, A{-4}=+0.340 {I8} (1975Ka42)
194PT G 938.719 10 4.57 13E2 0.00621 C
194PTS G KC=0.00500 7$LC=0.000924 13$MC=0.000216 3
194PTS G NC=5.34E-5 8$OC=9.37E-6 14$PC=5.28E-7 8
194PT cG $E|g=938.725 {I10}, I|g=4.57 {I13} (2016Kr06)
194PT cG $E|g=938.690 {I23}, I|g=4.57 {I14} (1976Cl03)
194PT cG $E|g=938.68 {I6}, I|g=4.56 {I30} (1974HeYW)
194PT cG $(939|g)(328|g)(|q): 1973Si22, 1976Cl03, 1975Ka42, 1965Ma10, 1962Bu03,
194PT2cG 1960Ma19, 1959Jo35. See A{-2}, A{-4} coefficients below
194PT cG $A{-2}=+0.191 {I10}, A{-4}=+0.795 {I17} (1975Ka42)
194PT cG $A{-2}=+0.33 {I2}, A{-4}=+1.08 {I4} (1973Si22)
194PT cG $A{-2}=+0.36 {I4}, A{-4}=+1.05 {I7} (1965Ma10)
194PT cG $A{-2}=+0.35 {I8}, A{-4}=+0.92 {I11} (1962Bu03)
194PT cG $A{-2}=+0.23 {I2}, A{-4}=+0.87 {I4} (1960Ma19)
194PT cG $A{-2}=+0.12 {I3}, A{-4}=+0.78 {I4} (1959Jo35)
194PT G 1267.37 E0 0.010 1 S
194PT L 1432.559 9 3-
194PT B 0.0020 15 11.2 4 ?
194PTS B EAV=253.79 48
194PT G 203.056 21 0.0398 19E1 0.0675 C
194PTS G KC=0.0555 8$LC=0.00929 13$MC=0.00214 3
194PTS G NC=0.000525 8$OC=9.07E-5 13$PC=4.84E-6 7
194PT cG $I|g from 2016Kr06
194PT cG $E|g=203.059 {I21}, I|g=0.0398 {I19} (2016Kr06)
194PT cG $E|g=202.91 {I15}, I|g=0.023 {I5} from |g|g-coin (1976Cl03)
194PT G 621.295 36 0.083 9 E1 0.00527 C
194PTS G KC=0.00441 7$LC=0.000668 10$MC=0.0001527 22
194PTS G NC=3.76E-5 6$OC=6.68E-6 10$PC=4.25E-7 6
194PT cG $E|g=621.295 {I36}, I|g=0.091 {I9} (2016Kr06)
194PT cG $E|g=621.29 {I15}, I|g=0.073 {I10} from |g|g-coin (1976Cl03)
194PT G 810.569 18 0.0206 4 E1 0.00313 C
194PTS G KC=0.00262 4$LC=0.000391 6$MC=8.91E-5 13
194PTS G NC=2.19E-5 3$OC=3.92E-6 6$PC=2.56E-7 4
194PT cG $E|g=810.568 {I18}, I|g=0.0206 {I4} (2016Kr06)
194PT cG $E|g=810.66 {I19}, I|g=0.019 {I4} (1976Cl03)
194PT G 1104.073 10 0.213 3 E1 1.77E-3 C
194PTS G KC=0.001490 21$LC=0.000218 3$MC=4.95E-5 7
194PTS G NC=1.221E-5 17$OC=2.19E-6 3$PC=1.467E-7 21$IPC=1.075E-6 15
194PT cG $E|g=1104.073 {I10}, I|g=0.214 {I2} (2016Kr06)
194PT cG $E|g=1104.05 {I5}, I|g=0.198 {I8} (1976Cl03)
194PT cG $E|g=1104.17 {I13}, I|g=0.23 {I6} (1974HeYW)
194PT cG $(1104|g)(328|g)(|q): 1976Cl03
194PT G 1432.56 8 0.0071 3 [E3] 0.00566
194PTS G KC=0.00450 7$LC=0.000870 13$MC=0.000205 3
194PTS G NC=5.07E-5 7$OC=8.92E-6 13$PC=5.10E-7 8$IPC=1.93E-5 3
194PT cG $E|g=1432.58 {I8}, I|g=0.0071 {I3} (2016Kr06)
194PT cG $E|g=1432.52 {I12}, I|g=0.0087 {I18} (1976Cl03)
194PT L 1479.265 11 0+
194PT cL J$|g(|q) (1983Ri14) and (1151|g)(328|g)(|q) (1962Bu03,1960Ma19) gives
194PT2cL J=0
194PT B 0.63 9 8.6 1
194PTS B EAV=236.63 48
194PT G 857.224 14 0.0445 6 [E2] 0.00746 C
194PTS G KC=0.00597 9$LC=0.001145 16$MC=0.000269 4
194PTS G NC=6.64E-5 10$OC=1.160E-5 17$PC=6.31E-7 9
194PT cG $E|g=857.225 {I14}, I|g=0.0445 {I4} (2016Kr06)
194PT cG $E|g=857.12 {I19}, I|g=0.054 {I6} from |g|g-coin (1976Cl03)
194PT G 1150.799 12 4.56 5 E2 0.00416 C
194PTS G KC=0.00340 5$LC=0.000585 9$MC=0.0001360 19
194PTS G NC=3.36E-5 5$OC=5.94E-6 9$PC=3.58E-7 5$IPC=1.162E-6 17
194PT cG $E|g=1150.800 {I10}, I|g=4.55 {I5} (2016Kr06)
194PT cG $E|g=1150.75 {I5}, I|g=4.56 {I15} (1976Cl03)
194PT cG $E|g=1150.94 {I10}, I|g=4.69 {I25} (1974HeYW)
194PT cG $(1151|g)(328|g)(|q): 1976Cl03, 1975Ka42, 1973Si22, 1965Ma10,
194PT2cG 1962Bu03, 1960Ma19
194PT cG $A{-2}=+0.108 {I9}, A{-4}=+0.745 {I16} (1975Ka42)
194PT cG $A{-2}=+0.10 {I2}, A{-4}=+0.73 {I3} (1965Ma10)
194PT cG $A{-2}=+0.357, A{-4}=+1.14 (1962Bu03)
194PT cG $A{-2}=+0.128 {I10}, A{-4}=+0.85 {I4} (1960Ma19)
194PT G 1479.2 E0 0.024 2
194PT cG TI$deduced from Branching in {+194}Au |e decay. Other: 0.021,
194PT2cG from ce(K)(1479)/ce(K)(328|g)=0.037 (1960Ke09)
194PT L 1512.004 9 2+
194PT cL J$(1184|g)(328|g)(|q) (1973Si22) gives J=2
194PT B 0.55 8 8.6 1
194PTS B EAV=224.72 47
194PT G 244.769 19 0.0660 35 (E2) 0.184 C
194PTS G KC=0.1019 15$LC=0.0623 9$MC=0.01576 22
194PTS G NC=0.00386 6$OC=0.000620 9$PC=9.98E-6 14
194PT cG $E|g=244.763 {I16}, I|g=0.0678 {I20} (2016Kr06)
194PT cG $E|g=244.83 {I5}, I|g=0.059 {I4} (1976Cl03)
194PT G 589.202 19 1.024 12E2+M1 2.2 +6-4 0.0226 23 C
194PTS G KC=0.0178 19$LC=0.00368 25$MC=0.00087 6
194PTS G NC=0.000215 14$OC=3.7E-5 3$PC=1.93E-6 22
194PT cG $E|g=589.217 {I14}, I|g=1.02 {I1} (2016Kr06)
194PT cG $E|g=589.179 {I17}, I|g=1.066 {I34} (1976Cl03)
194PT G 700.687 20 0.199 2 E2 0.01140 C
194PTS G KC=0.00892 13$LC=0.00190 3$MC=0.000452 7
194PTS G NC=0.0001112 16$OC=1.92E-5 3$PC=9.45E-7 14
194PT cG E$NRM-weighted average
194PT cG $E|g=700.693 {I14}, I|g=0.199 {I2} (2016Kr06)
194PT cG $E|g=700.547 {I35}, I|g=0.190 {I31} from |g|g-coin (1976Cl03)
194PT cG $E|g=700.68 {I8}, I|g=0.21 {I5} (1974HeYW)
194PT G 889.986 10 0.401 4 E2+M1 +0.50 16 0.0155 12 C
194PTS G KC=0.0128 10$LC=0.00205 14$MC=0.00047 3
194PTS G NC=0.000117 8$OC=2.10E-5 14$PC=1.41E-6 11
194PT cG $E|g=889.987 {I10}, I|g=0.402 {I4} (2016Kr06)
194PT cG $E|g=889.976 {I35}, I|g=0.386 {I13} (1976Cl03)
194PT cG $E|g=889.93 {I9}, I|g=0.39 {I8} (1974HeYW)
194PT cG MR$other: +1.51 {I40} from |g(|q) (1983Ri14)
194PT G 1183.539 10 2.27 2 M1+E2 +1.09 +18-160.0061 4 C
194PTS G KC=0.0050 4$LC=0.00081 5$MC=0.000186 11
194PTS G NC=4.6E-5 3$OC=8.2E-6 5$PC=5.4E-7 4$IPC=3.68E-6 15
194PT cG $E|g=1183.540 {I10}, I|g=2.26 {I2} (2016Kr06)
194PT cG $E|g=1183.49 {I5}, I|g=2.32 {I8} (1976Cl03)
194PT cG $E|g=1183.68 {I14}, I|g=2.42 {I19} (1974HeYW)
194PT cG MR$others: +1.32 {I9} from |g(|q) (1983Ri14); +0.9 {I1} (1973Si22, from
194PT2cG A{-2}=-0.25 {I2}, A{-4}=+0.18 {I5} for (1183|g)(328|g)(|q)); 1976Cl03
194PT3cG (value not explicitly given)
194PT G 1511.98 10 0.180 22(E2) 0.00255 C
194PTS G KC=0.00206 3$LC=0.000331 5$MC=7.63E-5 11
194PTS G NC=1.88E-5 3$OC=3.36E-6 5$PC=2.15E-7 3$IPC=7.00E-5 10
194PT cG $E|g and I|g from 1976Cl03. In 2016Kr06 and 1974HeYW, values are
194PT2cG given for a doublet of 1511.98 and 1512.15 proposed in 1976Cl03
194PT cG $E|g=1512.072 {I14}, I|g=0.285 {I3} (2016Kr06)
194PT cG $E|g=1511.98 {I10}, I|g=0.180 {I22} from |g|g-coin (1976Cl03)
194PT cG $E|g=1512.6 {I2}, I|g=0.31 {I7} (1974HeYW)
194PT L 1547.293 11 0+
194PT cL J$(1219|g)(328|g)(|q) (1976Cl03) gives J=0
194PT B 0.072 10 9.4 1
194PTS B EAV=212.01 47
194PT G 925.269 14 0.108 1 E2 0.00639 C
194PTS G KC=0.00515 8$LC=0.000955 14$MC=0.000224 4
194PTS G NC=5.52E-5 8$OC=9.69E-6 14$PC=5.43E-7 8
194PT cG $E|g=925.270 {I14}, I|g=0.108 {I1} (2016Kr06)
194PT cG $E|g=925.26 {I6}, I|g=0.097 {I6} (1976Cl03)
194PT cG $E|g=925.22 {I25}, I|g=0.08 {I3} (1974HeYW)
194PT G 1218.813 10 0.433 4 E2 0.00373 C
194PTS G KC=0.00306 5$LC=0.000517 8$MC=0.0001200 17
194PTS G NC=2.96E-5 5$OC=5.25E-6 8$PC=3.21E-7 5$IPC=6.00E-6 9
194PT cG $E|g=1218.813 {I10}, I|g=0.433 {I4} (2016Kr06)
194PT cG $E|g=1218.78 {I5}, I|g=0.429 {I17} (1976Cl03)
194PT cG $E|g=1219.00 {I15}, I|g=0.45 {I8} (1974HeYW)
194PT cG $(1219|g)(328|g)(|q) (1976Cl03) and |g(|q) (1983Ri14)
194PT2cG are consistent with J=0 for 1547 level
194PT G 1547.3 E0 0.00095 12 S
194PT L 1622.197 9 2+
194PT cL J$(1294|g)(328|g)(|q) (1973Si22) gives J=2
194PT B 0.16021 8.9 1
194PTS B EAV=185.45 46
194PT G 699.332 29 0.0361 12[M1,E2] 0.022 11 C
194PTS G KC=0.018 9$LC=0.0031 12$MC=0.0007 3
194PTS G NC=0.00018 7$OC=3.2E-5 13$PC=2.0E-6 11
194PT cG $Uncertainty for E|g was doubled in the least-squares fit procedure
194PT cG $E|g=699.331 {I29}, I|g=0.0362 {I7} (2016Kr06)
194PT cG $E|g=699.49 {I36}, I|g=0.019 {I10} from |g|g-coin (1976Cl03)
194PT G 1000.173 10 0.362 4 E2+M1 1.38 +13-120.0081 4 C
194PTS G KC=0.0066 3$LC=0.00111 5$MC=0.000258 10
194PTS G NC=6.36E-5 24$OC=1.13E-5 5$PC=7.2E-7 4
194PT cG $E|g=1000.177 {I10}, I|g=0.363 {I4} (2016Kr06)
194PT cG $E|g=1000.12 {I4}, I|g=0.355 {I13} (1976Cl03)
194PT cG $E|g=1000.10 {I12}, I|g=0.38 {I8} (1974HeYW)
194PT G 1293.723 14 0.339 3 E2+M1+E0 -0.9 1 0.0192 8 C
194PT cG $E|g=1293.726 {I14}, I|g=0.339 {I3} (2016Kr06)
194PT cG $E|g=1293.67 {I6}, I|g=0.352 {I23} (1976Cl03)
194PT cG $E|g=1294.20 {I20}, I|g=0.34 {I9} (1974HeYW). E|g not used in averaging
194PT cG MR$adopted |d(E2/M1) from (1294|g)(328|g)(|q): A{-2}=+0.37 {I7},
194PT2cG A{-4}=+0.30 {I13} (1973Si22). Others: 1.79 {I3} (from |g(|q),
194PT3cG 1983Ri14), 1976Cl03 (value not explicitly given)
194PT cG CC$from {+194}Au |e decay
194PT G 1622.185 14 0.475 5 E2 0.00229 C
194PTS G KC=0.00181 3$LC=0.000287 4$MC=6.62E-5 10
194PTS G NC=1.633E-5 23$OC=2.92E-6 4$PC=1.89E-7 3$IPC=0.0001085 16
194PT cG $E|g=1622.185 {I14}, I|g=0.474 {I5} (2016Kr06)
194PT cG $E|g=1622.20 {I8}, I|g=0.490 {I22} (1976Cl03)
194PT cG $E|g=1623.08 {I20}, I|g=0.45 {I8} (1974HeYW). E|g not used in averaging
194PT L 1670.685 9 2+
194PT cL J$(1342|g)(328|g)(|q) (1973Si22) gives J=2
194PT B 0.075 10 9.1 1
194PTS B EAV=168.61 45
194PT G 859.396 25 0.0133 6 (E2) 0.00742 C
194PTS G KC=0.00594 9$LC=0.001138 16$MC=0.000268 4
194PTS G NC=6.60E-5 10$OC=1.153E-5 17$PC=6.28E-7 9
194PT cG $E|g=859.395 {I25}, I|g=0.0133 {I6} (2016Kr06)
194PT cG $E|g=859.45 {I18}, I|g=0.013 {I6} (1976Cl03)
194PT G 1048.655 14 0.202 2 M1 0.01161 C
194PTS G KC=0.00964 14$LC=0.001515 22$MC=0.000348 5
194PTS G NC=8.61E-5 12$OC=1.553E-5 22$PC=1.067E-6 15
194PT cG $E|g=1048.656 {I14}, I|g=0.202 {I2} (2016Kr06)
194PT cG $E|g=1048.64 {I5}, I|g=0.199 {I9} (1976Cl03)
194PT cG $E|g=1048.68 {I10}, I|g=0.20 {I5} (1974HeYW)
194PT G 1342.204 10 0.304 3 M1+E2 -0.23 9 0.0061216 C
194PTS G KC=0.00506 14$LC=0.000790 20$MC=0.000181 5
194PTS G NC=4.49E-5 12$OC=8.09E-6 21$PC=5.57E-7 16$IPC=3.70E-5 8
194PT cG $E|g=1342.205 {I10}, I|g=0.305 {I3} (2016Kr06)
194PT cG $E|g=1342.16 {I6}, I|g=0.290 {I11} (1976Cl03)
194PT cG $E|g=1342.70 {I20}, I|g=0.32 {I9} (1974HeYW). E|g not used in averaging
194PT cG MR$others: -0.1 to -1.5 from (1342|g)(328|g)(|q): A{-2}=+0.41 {I6},
194PT2cG A{-4}=+0.14 {I12} (1973Si22). Other: 1976Cl03 (value not explicitly
194PT3cG given)
194PT G 1670.680 16 0.0452 4 (E2) 0.00219
194PTS G KC=0.001714 24$LC=0.000271 4$MC=6.23E-5 9
194PTS G NC=1.539E-5 22$OC=2.75E-6 4$PC=1.79E-7 3$IPC=0.0001272 18
194PT cG $E|g=1670.679 {I16}, I|g=0.0452 {I4} (2016Kr06)
194PT cG $E|g=1670.72 {I10}, I|g=0.0442 {I28} (1976Cl03)
194PT cG $E|g=1671.5 {I3}, I|g=0.05 {I2} (1974HeYW). E|g not used in averaging
194PT L 1778.602 15 2+
194PT B 0.0056 8 9.9 1
194PTS B EAV=132.12 43
194PT G 1156.48 4 0.0250 10M1(+E2) 0.2 LT 0.0089816 C
194PTS G KC=0.00746 14$LC=0.001169 20$MC=0.000269 5
194PTS G NC=6.64E-5 12$OC=1.198E-5 21$PC=8.24E-7 15$IPC=2.20E-6 4
194PT cG $I|g from 2016Kr06
194PT cG $E|g=1156.48 {I4}, I|g=0.0250 {I10} (2016Kr06)
194PT cG $E|g=1156.60 {I30}, I|g=0.014 {I3} (1976Cl03)
194PT G 1450.137 14 0.0154 6 M1+E2 -0.27 10 0.0050615 C
194PTS G KC=0.00414 13$LC=0.000645 19$MC=0.000148 5
194PTS G NC=3.66E-5 11$OC=6.61E-6 19$PC=4.55E-7 14$IPC=7.69E-5 18
194PT cG $E|g=1450.135 {I14}, I|g=0.0155 {I3} (2016Kr06)
194PT cG $E|g=1450.23 {I11}, I|g=0.0125 {I15} (1976Cl03)
194PT G 1778.25 14 0.0023 2 (E2) 0.00201 A
194PTS G KC=0.001531 22$LC=0.000240 4$MC=5.50E-5 8
194PTS G NC=1.359E-5 19$OC=2.43E-6 4$PC=1.596E-7 23$IPC=0.0001710 24
194PT L 1797.402 8 1-
194PT B 0.33 5 8.1 1
194PTS B EAV=125.92 43
194PT G 364.852 10 0.333 4 E2 0.0562 C
194PTS G KC=0.0378 6$LC=0.01389 20$MC=0.00344 5
194PTS G NC=0.000844 12$OC=0.0001394 20$PC=3.90E-6 6
194PT cG $E|g=364.845 {I10}, I|g=0.335 {I3} (2016Kr06)
194PT cG $E|g=364.867 {I15}, I|g=0.314 {I10} (1976Cl03)
194PT cG $E|g=364.90 {I8}, I|g=0.32 {I9} (1974HeYW)
194PT G 530.184 14 0.130 1 E1 0.00730 C
194PTS G KC=0.00609 9$LC=0.000935 13$MC=0.000214 3
194PTS G NC=5.26E-5 8$OC=9.33E-6 13$PC=5.82E-7 9
194PT cG $E|g=530.186 {I14}, I|g=0.130 {I1} (2016Kr06)
194PT cG $E|g=530.173 {I30}, I|g=0.121 {I5} (1976Cl03)
194PT cG $E|g=530.23 {I10}, I|g=0.15 {I5} (1974HeYW)
194PT G 1175.377 10 0.450 4 E1 1.60E-3 C
194PTS G KC=0.001334 19$LC=0.000194 3$MC=4.42E-5 7
194PTS G NC=1.089E-5 16$OC=1.95E-6 3$PC=1.315E-7 19$IPC=1.024E-5 15
194PT cG $E|g=1175.376 {I10}, I|g=0.449 {I4} (2016Kr06)
194PT cG $E|g=1175.38 {I5}, I|g=0.463 {I17} (1976Cl03)
194PT cG $E|g=1175.63 {I18}, I|g=0.43 {I12} (1974HeYW)
194PT cG $(1175|g)(622|g)(|q): A{-2}=-0.054 {I12}, A{-4}=+0.12 {I3} (1974BeYP)
194PT G 1468.910 10 1.42 1 E1 1.23E-3 C
194PTS G KC=0.000908 13$LC=0.0001310 19$MC=2.97E-5 5
194PTS G NC=7.33E-6 11$OC=1.318E-6 19$PC=8.99E-8 13$IPC=0.0001568 22
194PT cG $E|g=1468.910 {I10}, I|g=1.42 {I1} (2016Kr06)
194PT cG $E|g=1468.91 {I7}, I|g=1.46 {I6} (1976Cl03)
194PT cG $E|g=1469.2 {I1}, I|g=1.53 {I12} (1974HeYW)
194PT cG $(1469|g)(328|g)(|q): A{-2}=-0.23 {I2}, A{-4}=+0.05 {I5} (1973Si22).
194PT2cG |d(1469|g)=0.0 {I2}, consistent with E1. Others: 1976Cl03, 1965Ma10,
194PT3cG 1953Kr07. Other: A{-2}=+0.18 {I3}, A{-4}=+0.002 {I36} (1965Ma10)
194PT G 1797.408 14 0.130 1 E1 1.16E-3
194PTS G KC=0.000649 9$LC=9.28E-5 13$MC=2.11E-5 3
194PTS G NC=5.19E-6 8$OC=9.35E-7 13$PC=6.44E-8 9$IPC=0.000393 6
194PT cG $E|g=1797.406 {I14}, I|g=0.130 {I1} (2016Kr06)
194PT cG $E|g=1797.48 {I9}, I|g=0.134 {I7} (1976Cl03)
194PT cG $E|g=1798.3 {I4}, I|g=0.14 {I4} (1974HeYW). E|g not used in averaging
194PT L 1893.597 16 0+
194PT cL J$|g|g(|q) of 1565|g-328|g cascade in 1976Cl03 gives J=0
194PT B 0.021 3 8.9 1
194PTS B EAV=95.02 41
194PT G 1565.116 14 0.161 2 C
194PT cG $E|g=1565.115 {I14}, I|g=0.161 {I2} (2016Kr06)
194PT cG $E|g=1565.15 {I8}, I|g=0.158 {I7} (1976Cl03)
194PT cG $E|g=1565.70 {I25}, I|g=0.20 {I4} (1974HeYW). E|g not used in averaging
194PT cG $(1565|g)(328|g)(|q): 1976Cl03
194PT G 1893.1 4 (E0) S
194PT L 1924.305 19 1+
194PT B 0.0038 5 9.5 1
194PTS B EAV=85.45 41
194PT G 1595.802 23 0.0131 2 M1+E2 -0.071 21 0.00420
194PTS G KC=0.00337 5$LC=0.000523 8$MC=0.0001199 17
194PTS G NC=2.97E-5 5$OC=5.36E-6 8$PC=3.71E-7 6$IPC=0.0001507 22
194PT cG $E|g=1595.805 {I23}, I|g=0.0131 {I2} (2016Kr06)
194PT cG $E|g=1595.77 {I10}, I|g=0.0124 {I12} (1976Cl03)
194PT G 1924.327 28 0.0155 3 M1 0.00290
194PTS G KC=0.00212 3$LC=0.000328 5$MC=7.51E-5 11
194PTS G NC=1.86E-5 3$OC=3.36E-6 5$PC=2.33E-7 4$IPC=0.000352 5
194PT cG $E|g=1924.323 {I28}, I|g=0.0155 {I2} (2016Kr06)
194PT cG $E|g=1924.42 {I14}, I|g=0.0136 {I13} (1976Cl03)
194PT cG $E|g=1926.0 {I5}, I|g=0.020 {I5} (1974HeYW). E|g not used in averaging
194PT L 1930.410 17 2+
194PT B 0.0040 6 9.5 1
194PTS B EAV=83.56 40
194PT G 1007.55 7 0.0044 5 (M1+E2) 1.1 +5-3 0.0088 13 A
194PTS G KC=0.0072 11$LC=0.00119 16$MC=0.00027 4
194PTS G NC=6.8E-5 9$OC=1.21E-5 16$PC=7.9E-7 13
194PT G 1308.304 40 0.0100 3 (M1+E2) 1.7 +11-5 0.0042 6
194PTS G KC=0.0034 5$LC=0.00055 7$MC=0.000128 15
194PTS G NC=3.2E-5 4$OC=5.6E-6 7$PC=3.7E-7 5$IPC=2.05E-5 16
194PT cG $E|g=1308.314 {I31}, I|g=0.0100 {I3} (2016Kr06)
194PT cG $E|g=1308.15 {I12}, I|g=0.0099 {I11} (1976Cl03)
194PT G 1601.947 17 0.0159 3 M1(+E2) -0.2 LT 0.004147
194PTS G KC=0.00332 6$LC=0.000515 9$MC=0.0001181 20
194PTS G NC=2.92E-5 5$OC=5.27E-6 9$PC=3.64E-7 7$IPC=0.0001533 24
194PT cG $E|g=1601.948 {I17}, I|g=0.0159 {I3} (2016Kr06)
194PT cG $E|g=1601.90 {I12}, I|g=0.0149 {I15} (1976Cl03)
194PT L 2003.630 25 (2+)
194PT cL $Population of this level in {+194}Ir decay proposed by 2016Kr06,
194PT2cL based on studies in {+194}Au |e decay to {+194}Pt
194PT B 0.00104 14 9.7 1
194PTS B EAV=61.46 39
194PT G 1675.147 24 0.0079 2 (M1) 0.00379
194PTS G KC=0.00299 5$LC=0.000464 7$MC=0.0001064 15
194PTS G NC=2.63E-5 4$OC=4.75E-6 7$PC=3.29E-7 5$IPC=0.000195 3
194PT cG $Placement from 2016Kr06; unplaced in 1976Cl03 study.
194PT cG $E|g=1675.145 {I24}, I|g=0.0079 {I2} (2016Kr06)
194PT cG $E|g=1675.24 {I17}, I|g=0.0066 {I11} (1976Cl03)
194PT L 2043.736 14 1+
194PT B 0.009112 8.5 1
194PTS B EAV=49.75 38
194PT G 1421.72 4 0.0045 2 M1(+E2) 0.2 LT 0.0054210
194PTS G KC=0.00446 8$LC=0.000694 12$MC=0.000159 3
194PTS G NC=3.94E-5 7$OC=7.11E-6 12$PC=4.91E-7 9$IPC=6.64E-5 11
194PT cG $E|g=1421.72 {I4}, I|g=0.0045 {I2} (2016Kr06)
194PT cG $E|g=1421.48 {I28}, I|g=0.0048 {I15} (1976Cl03)
194PT G 1715.243 25 0.0108 2 E2+M1 -1.10 12 0.0027910 C
194PTS G KC=0.00217 8$LC=0.000339 12$MC=7.8E-5 3
194PTS G NC=1.92E-5 7$OC=3.46E-6 12$PC=2.34E-7 9$IPC=0.000179 5
194PT cG $E|g=1715.241 {I25}, I|g=0.0108 {I2} (2016Kr06)
194PT cG $E|g=1715.28 {I11}, I|g=0.0100 {I9} (1976Cl03)
194PT cG $E|g=1716.0 {I3}, I|g=0.010 {I3} (1974HeYW). E|g not used in averaging
194PT G 2043.727 17 0.0541 5 M1 0.00263
194PTS G KC=0.00183 3$LC=0.000282 4$MC=6.46E-5 9
194PTS G NC=1.599E-5 23$OC=2.89E-6 4$PC=2.01E-7 3$IPC=0.000431 6
194PT cG $E|g=2043.727 {I17}, I|g=0.0541 {I5} (2016Kr06)
194PT cG $E|g=2043.72 {I11}, I|g=0.0539 {I34} (1976Cl03)
194PT cG $E|g=2045.8 {I5}, I|g=0.060 {I15} (1974HeYW). E|g not used in averaging
194PT L 2053.006 24 (2)+
194PT B 0.0021 4 9.0 1
194PTS B EAV=47.09 38
194PT G 1430.95 4 0.0091 10 C
194PT cG $E|g=1430.95 {I3}, I|g=0.0090 {I6} (2016Kr06)
194PT cG $E|g=1431.35 {I34}, I|g=0.017 {I5} (1976Cl03)
194PT G 1724.535 27 0.0072 4
194PT cG $E|g=1724.535 {I27}, I|g=0.0073 {I2} (2016Kr06)
194PT cG $E|g=1724.54 {I15}, I|g=0.0058 {I8} (1976Cl03)
194PT L 2063.759 16 2+
194PT B 0.0046 6 8.6 1
194PTS B EAV=44.02 37
194PT G 1441.733 19 0.0123 3 M1(+E2) 0.6 LT 0.0050 4 C
194PTS G KC=0.0041 3$LC=0.00063 5$MC=0.000146 10
194PTS G NC=3.60E-5 24$OC=6.5E-6 5$PC=4.5E-7 4$IPC=7.2E-5 4
194PT cG $E|g=1441.732 {I19}, I|g=0.0123 {I3} (2016Kr06)
194PT cG $E|g=1441.78 {I14}, I|g=0.0114 {I18} (1976Cl03)
194PT G 1735.272 21 0.0223 4 M1+E2 +0.12 6 0.003516 C
194PTS G KC=0.00273 5$LC=0.000422 7$MC=9.68E-5 16
194PTS G NC=2.39E-5 4$OC=4.32E-6 7$PC=2.99E-7 5$IPC=0.000230 4
194PT cG $E|g=1735.269 {I21}, I|g=0.0224 {I3} (2016Kr06)
194PT cG $E|g=1735.37 {I12}, I|g=0.0190 {I19} (1976Cl03)
194PT cG $E|g=1736.9 {I3}, I|g=0.020 {I5} (1974HeYW). E|g not used in averaging
194PT L 2085.472 16 0+
194PT B 0.0067 9 8.3 1
194PTS B EAV=37.89 37
194PT G 1463.445 14 0.0456 5 (E2) 0.00270 C
194PTS G KC=0.00218 3$LC=0.000353 5$MC=8.16E-5 12
194PTS G NC=2.01E-5 3$OC=3.59E-6 5$PC=2.28E-7 4$IPC=5.51E-5 8
194PT cG $E|g=1463.445 {I14}, I|g=0.0456 {I5} (2016Kr06)
194PT cG $E|g=1463.50 {I15}, I|g=0.045 {I9} (1976Cl03)
194PT G 1756.93 7 0.0037 2 (E2) 0.00204 C
194PTS G KC=0.001564 22$LC=0.000245 4$MC=5.64E-5 8
194PTS G NC=1.391E-5 20$OC=2.49E-6 4$PC=1.632E-7 23$IPC=0.0001621 23
194PT cG $E|g=1756.91 {I4}, I|g=0.0037 {I2} (2016Kr06)
194PT cG $E|g=1757.27 {I19}, I|g=0.0032 {I7} (1976Cl03)
194PT G 2085.8 4 E0 0.00025 6 S
194PT L 2109.079 13 (2)+
194PT B 0.031 4 7.3 1
194PTS B EAV=31.33 36
194PT G 1186.408 26 0.0739 12(M1+E2) 1.1 +6-4 0.0060 10 C
194PT cG $Uncertainty for E|g was doubled in the least-squares fit procedure
194PTS G KC=0.0050 9$LC=0.00080 13$MC=0.00018 3
194PTS G NC=4.6E-5 7$OC=8.2E-6 13$PC=5.4E-7 10$IPC=3.9E-6 4
194PTF G FL=922.773
194PT cG $E|g=1186.408 {I26}, I|g=0.0740 {I12} (2016Kr06)
194PT cG $E|g=1186.4 {I4}, I|g=0.064 {I12} from |g|g-coin (1976Cl03)
194PT G 1487.058 14 0.131 1 (M1(+E2)) 0.3 LT 0.0048312 C
194PTS G KC=0.00394 10$LC=0.000614 15$MC=0.000141 4
194PTS G NC=3.48E-5 9$OC=6.29E-6 15$PC=4.34E-7 11$IPC=9.39E-5 19
194PT cG $E|g=1487.057 {I14}, I|g=0.131 {I1} (2016Kr06)
194PT cG $E|g=1487.05 {I8}, I|g=0.129 {I6} (1976Cl03)
194PT cG $E|g=1487.30 {I20}, I|g=0.16 {I3} (1974HeYW)
194PT G 1780.571 18 0.0342 5 [M1,E2] 0.0027 7 C
194PTS G KC=0.0021 6$LC=0.00032 8$MC=7.3E-5 19
194PTS G NC=1.8E-5 5$OC=3.3E-6 9$PC=2.2E-7 7$IPC=0.00022 5
194PT cG $E|g=1780.568 {I17}, I|g=0.0341 {I3} (2016Kr06)
194PT cG $E|g=1780.69 {I11}, I|g=0.0396 {I28} (1976Cl03)
194PT cG $E|g=1782.0 {I3}, I|g=0.05 {I2} (1974HeYW). E|g not used in averaging
194PT L 2114.096 15 1+
194PT cL J$(1786|g)(328|g)(|q) in 1965Ma10 consistent with J=2
194PT B 0.008712 7.8 1
194PTS B EAV=29.95 36
194PT G 1492.020 27 0.0136 3 M1(+E2) 0.5 LT 0.0046624
194PTS G KC=0.00380 20$LC=0.00059 3$MC=0.000136 7
194PTS G NC=3.36E-5 17$OC=6.1E-6 3$PC=4.17E-7 23$IPC=9.4E-5 4
194PT cG $E|g=1492.015 {I22}, I|g=0.0136 {I2} (2016Kr06)
194PT cG $E|g=1492.18 {I13}, I|g=0.0111 {I16} (1976Cl03)
194PT G 1785.631 21 0.0331 3 M1(+E2) -0.04 3 0.00333 C
194PTS G KC=0.00255 4$LC=0.000395 6$MC=9.06E-5 13
194PTS G NC=2.24E-5 4$OC=4.04E-6 6$PC=2.80E-7 4$IPC=0.000263 4
194PT cG $E|g=1785.628 {I21}, I|g=0.0331 {I3} (2016Kr06)
194PT cG $E|g=1785.69 {I11}, I|g=0.0302 {I23} (1976Cl03)
194PT cG $E|g=1786.2 {I5}, I|g=0.04 {I1} (1974HeYW)
194PT cG $(1786|g)(328|g)(|q): A{-2}=-0.13 {I12}, A{-4}=+0.21 {I14} (1965Ma10)
194PT G 2114.099 26 0.0196 2 M1 0.00250
194PTS G KC=0.001684 24$LC=0.000259 4$MC=5.94E-5 9
194PTS G NC=1.469E-5 21$OC=2.65E-6 4$PC=1.84E-7 3$IPC=0.000478 7
194PT cG $E|g=2114.096 {I26}, I|g=0.0196 {I2} (2016Kr06)
194PT cG $E|g=2114.20 {I14}, I|g=0.0199 {I19} (1976Cl03)
194PT cG $E|g=2116.0 {I5}, I|g=0.020 {I6} (1974HeYW). E|g not used in averaging
194PT L 2134.211 16 1+,2+
194PT B 0.045 7 6.9 1
194PTS B EAV=24.47 36
194PT G 1512.15 21 0.101 14M1,E2 0.0036 11 C
194PTS G KC=0.0030 9$LC=0.00047 14$MC=0.00011 3
194PTS G NC=2.6E-5 8$OC=4.8E-6 14$PC=3.2E-7 11$IPC=8.9E-5 19
194PT cG $E|g and I|g from 1976Cl03. In 2016Kr06 and 1974HeYW, values are
194PT2cG given for a doublet of 1511.98 and 1512.15 proposed in 1976Cl03
194PT cG $E|g=1512.072 {I14}, I|g=0.285 {I3} (2016Kr06)
194PT cG $E|g=1512.15 {I21}, I|g=0.101 {I14} from |g|g-coin (1976Cl03)
194PT cG $E|g=1512.6 {I2}, I|g=0.31 {I7} (1974HeYW)
194PT G 1805.727 14 0.244 2 M1(+E2) 0.5 LT 0.0031314 C
194PTS G KC=0.00239 11$LC=0.000369 16$MC=8.5E-5 4
194PTS G NC=2.09E-5 10$OC=3.78E-6 17$PC=2.61E-7 13$IPC=0.000266 10
194PT cG $E|g=1805.726 {I14}, I|g=0.244 {I2} (2016Kr06)
194PT cG $E|g=1805.75 {I9}, I|g=0.249 {I13} (1976Cl03)
194PT cG $E|g=1807.0 {I5}, I|g=0.24 {I5} (1974HeYW). E|g not used in averaging
194PT cG $(1806|g)(328|g)(|q): 1976Cl03, 1965Ma10
194PT L 2140.679 22 (1+,2+)
194PT B 0.0024 4 8.0 1
194PTS B EAV=22.73 35
194PT G 1518.652 22 0.0140 3 (M1(+E2)) 0.7 LT 0.0043 4
194PTS G KC=0.0035 3$LC=0.00055 5$MC=0.000126 11
194PTS G NC=3.1E-5 3$OC=5.6E-6 5$PC=3.9E-7 4$IPC=0.000104 7
194PT cG $E|g=1518.649 {I22}, I|g=0.0140 {I3} (2016Kr06)
194PT cG $E|g=1518.76 {I14}, I|g=0.0127 {I18} (1976Cl03)
194PT G 1812.18 7 0.0046 12(M1) 0.00324
194PTS G KC=0.00246 4$LC=0.000381 6$MC=8.73E-5 13
194PTS G NC=2.16E-5 3$OC=3.90E-6 6$PC=2.70E-7 4$IPC=0.000280 4
194PT cG $I|g is unweighted average.
194PT cG $E|g=1812.17 {I4}, I|g=0.0058 {I2} (2016Kr06)
194PT cG $E|g=1812.59 {I25}, I|g=0.0034 {I10} (1976Cl03)
194PT L 2158.01 4 (2)+
194PT B 0.0022 3 7.8 1
194PTS B EAV=18.10 35
194PT G 1829.524 33 0.0165 2 M1(+E2) 0.3 LT 0.003137 C
194PTS G KC=0.00237 6$LC=0.000366 8$MC=8.39E-5 18
194PTS G NC=2.08E-5 5$OC=3.75E-6 9$PC=2.59E-7 6$IPC=0.000287 6
194PT cG $E|g=1829.520 {I26}, I|g=0.0165 {I2} (2016Kr06)
194PT cG $E|g=1829.59 {I15}, I|g=0.0142 {I15} (1976Cl03)
194PT cG $E|g=1830.4 {I5}, I|g=0.020 {I5} (1974HeYW).