194PT 194AU EC DECAY (38.02 H) 2015DO06,1996TEZW,1971VI1521NDS 202109
194PT H TYP=FUL$AUT=Jun Chen and Balraj Singh$CIT=NDS 177, 1 (2021)$
194PT2 H CUT=3-Sep-2021$
194PT c 2015Do06: {+194}Au source was from the decay of {+194}Hg which is
194PT2c produced at Los Alamos Meson Physics Facility by 800-MeV proton
194PT3c spallation reactions on a Pb target. |g rays were detected with HPGe
194PT4c detectors (FWHM=1.68 keV at 1332 keV). Measured E|g, I|g. Deduced
194PT5c levels, decay branching ratios, log| {Ift}. Comparisons with available
194PT6c data. Report |g data for 221 transitions.
194PT c 1996TeZW, 1997Te09: two measurements were performed. In the first one,
194PT2c {+194}Au source was produced by irradiating a foil of natural platinum
194PT3c with 10 MeV protons from the cyclotron of the IPEN at the University of
194PT4c Sao Paulo, Brazil; |g rays were detected with a 50-cm{+3} Ge detector
194PT5c for singles measurements; measured E|g, I|g. In the second measurement,
194PT6c {+194}Au was from decay of the {+194}Hg in equilibrium with {+194}Hg
194PT7c produced via {+197}Au(p,4n) reaction with 40-MeV protons from the
194PT8c 88-Inch Cyclotron at LBNL; |g rays were detected with the High Energy
194PT9c Resolution Array (HERA) consisting of 20 Compton-suppressed HPGe
194PTac detectors; measured E|g, I|g, |g|g-coin, |g|g(|q). Deduced levels, J,
194PTbc |p, |g-ray multipolarities, mixing ratios. The main results of this
194PTcc work are given in the thesis by 1996TeZW. About 34 new weak transitions
194PTdc and some revised placements are given in this study and 167 transitions
194PTec in total are reported in 1996TeZW.
194PT c 1971Vi15,1970Ag05: {+194}Au source was produced via {+194}Pt(d,2n)
194PT2c with 13.6 MeV deuteron beams from a cyclotron bombarding platinum
194PT3c targets at the Institute for Nuclear Research of JINR. |g rays were
194PT4c detected with Ge(Li) detectors (FWHM=4.5 keV) and conversion
194PT5c electrons were detected with an iron-core |p|%{2}|b spectrometer
194PT6c (FWHM=0.03-0.04%). Measured E|g, I|g, E(ce), I(ce). Deduced levels,
194PT7c J, |p, conversion coefficients, |g-ray multipolarities, ratios of
194PT8c transition strengths. 1971Vi15 report |g and/or ce data for 144
194PT9c transitions; 1970Ag05 report only ce data for 46 transitions.
194PT c 1974HeYW: {+194}Au source was produced via {+194}Pt(p,n). Measured E|g,
194PT2c I|g with a 55 cm{+3} coaxial Ge(Li) detector. Deduced levels
194PT c 1970Be30: {+194}Au source was produced via {+194}Pt(p,n) with 15 MeV
194PT2c protons from the Oak Ridge Isochronous Cyclotron. |g rays were detected
194PT3c with a 35 cm{+3} and a 15 cm{+3} Ge(Li) detectors. Measured E|g, I|g,
194PT4c |g|g-coin. Deduced levels, conversion coefficients using I(ce) data of
194PT5c 1964Be23, |g-ray multipolarities.
194PT c 1964Be23,1960Ba17 (also 1962Be50): In the measurement of |g-ray
194PT2c intensities by 1964Be23, {+194}Au source was produced by irradiating a
194PT3c platinum target with 20 MeV deuterons from the cyclotron at Birmingham
194PT4c University; |g-ray intensities were measured by the method of external
194PT5c conversion with a double focusing iron yoke spectrometer; measured
194PT6c I|g. In the measurement of conversion electron intensities by 1960Ba17,
194PT7c {+194}Au sources were produced via {+194}Pt(d,2n) with deuterons from
194PT8c cyclotrons of Oak Ridge, Birmingham and Stockholm and synchrocyclotrons
194PT9c of Uppsala and Amsterdam; conversion electrons were detected with a
194PTac double-focusing spectrometer; measured E(ce), I(ce). Deduced levels, J,
194PTbc |p, conversion coefficients, |g-ray multipolarities, mixing ratios.
194PTcc 1964Be23 also re-measure accurately the prominent conversion lines in
194PTdc the entire energy spectrum in 1960B17. For data from the two papers,
194PTec E|g and I(ceK) from 1960Ba17, precise I(ceK), I|g and conversion
194PTfc coefficients from 1964Be23
194PT c Others:
194PT c 1992Si02: measured T{-1/2}, |e/|b{++} ratio from I|g and K| x ray
194PT c 1981Ho18: measured |e/|b{++} ratio from I|g and K| x ray
194PT c 1977Vy01, 1967Cr09: measured E|g, I|g
194PT c |g, ce: 1965Le17 (ce), 1962Ma18 (also 1960Ma19), 1960De17 (ce),
194PT2c 1960De15 (|g), 1957Al45, 1955Br12, 1956Th11, 1949St17
194PT c |b, |b|g: 1970Ag03, 1960Ba17, 1956Th11
194PT c |g|g(|q): 1971Kr01, 1969Ha43
194PT c |g(ce)(|q): 1971Do12, deduced E0/E2 mixing ratio for 293|g
194PT c |g|g(lin pol): 1969Ha43
194PT c $Total energy deposit of 2565 {I60} calculated by RADLIST is
194PT2c in a good agreement with Q=2548.2 {I21} (2021Wa16), indicating
194PT3c completeness of the decay scheme.
194PT cE TI$From I(|g+ce) intensity balance at each level.
194PT cG $A{-2} and A{-4} coefficients are from |g|g(|q) data of 1996TeZW
194PT cG $Conversion coefficients |a(K)exp given under comments have been
194PT2cG re-normalized by evaluators to theoretical |a(K)(328|g, E2)=0.0488
194PT3cG calculated by the BrIcc code. Original values in 1964Be23 and 1970Be30
194PT4cG are normalized to |a(K)(328|g, E2)=0.0494 and those in 1971Vi15 are
194PT5cG normalized to |a(K)(328|g, E2)=0.050. Quoted values of I|g and Ice(K)
194PT6cG are relative to I|g(328)=100 and Ice(K)(328|g)=100, respectively
194PT cG $2015Do06 also report the following unidentified |g rays from the
194PT2cG {+194}Hg source: 119.990 {I7}, 143.367 {I28}, 183.698 {I28}, 592.819
194PT3cG {I11}, 895.27 {I4}, 1289.67 {I7}, 1752.994 {I25}, 1947.637 {I24},
194PT4cG 2081.560 {I20}, 2375.05 {I3}, 2453.77 {I4}
194PT cG E,RI$The most precise values are given by 2015Do06 and 1996TeZW. E|g
194PT2cG values from 1971Vi15 are deduced by authors from ce lines, with
194PT3cG uncertainties assigned by the evaluators as 0.3 keV for E|g<0.8 MeV,
194PT4cG 0.2 keV for E|g=0.8-1.2 MeV, 0.3 for E|g=1.2-1.8 MeV, and 0.4 keV for
194PT5cG E|g>1.8 MeV, according to an authors' general statement that the mean
194PT6cG error in measuring energy is |?0.3 keV in the low-energy region, |?0.2
194PT7cG keV near 1 MeV, and |?0.4 keV near 2 MeV. Quoted values are weighted
194PT8cG average of all available data where applicable. See comments of
194PT9cG individual transitions for details. In cases where I|g values have been
194PTacG deduced from I(ce) data, the data have been normalized to
194PTbcG Ice(K)(328|g)=100 and |a(K)(328|g)=0.0488
194PT cG E(A)$From ce data of 1971Vi15
194PT cG E(K)$|g from 1997Te09 and 1996TeZW only, observed in coincidence with
194PT2cG other |g rays with HERA array of 20 intrinsic germanium detectors.
194PT cG E(X)$Not reported by 1996TeZW and 2015Do06, its existence treated as
194PT2cG uncertain by the evaluators.
194PT cG E(N),RI(N)$Possible new |g ray from 2015Do06
194PT cG E(n),RI(n)$New |g ray from coincidence summing of crossover transitions
194PT2cG in 2015Do06
194PT cG E(Y)$Poor fit; the uncertainty has been increased by the evaluators by
194PT2cG a factor of 5 in the fitting procedure to reduce the reduced |h{+2}
194PT3cG from 6.3 to 1.7, as compared to the critical |h{+2}=1.3
194PT cG M,MR$From Adopted Gammas, which are mostly from ce and |g|g(|q)
194PT2cG data as given under comments in this dataset. Values from this dataset
194PT3cG are also given under comments where applicable, if different from
194PT4cG adopted values.
194PT cL E$From a least-squares fit to |g-ray energies.
194PT cL J$From Adopted Levels
194AU P 0.0 1- 38.02 H 10 2548.2 21
194AU cP J,T$From {+194}Au Adopted Levels
194AU cP QP$From 2021Wa16
194PT N 0.63 2 0.63 2 1.0 1.0
194PT cN NR$From %I(|e+|b{++})(g.s.)+%I(|g+ce)(transitions to g.s.)=100, with
194PT2cN I(|e+|b{++})(g.s.)=36.2 {I41} (relative to I|g(328)=100.0 {I10}),
194PT3cN deduced based on I(|b{++})(total)/I|g(328|g)=0.029 {I2} (1992Si02,
194PT4cN 1956Th11) where I(|b{++})(total)=I(|b{++})(328)+I(|b{++})(g.s.) with
194PT5cN I(|b{++}) to other levels negligible due to very large |e/|b{++} ratios
194PT6cN (>100) and small total I(|e+|b{++}), |e/|b{++}(328)=42.1 {I5} and
194PT7cN |e/|b{++}(g.s.)=18.8 {I2} calculated using the LOGFT code with
194PT8cN Q=2548.2 {I21} (2021Wa16), and I(|e+|b{++})(328)=46.3 {I12} (relative
194PT9cN to I|g(328)=100.0 {I10}) deduced from I(|g+ce) balance at 328 level.
194PTAcN The |e/|b{++} ratios, although calculated for allowed transitions, are
194PTBcN found to be valid first-forbidden transitions in the present case.
194PTCcN Others: |e/|b{++}(328)(exp)=44 {I5}, deduced by the evaluators from
194PTDcN I(|g{+|+})(328 level)/(2|*I|g(328|g))=0.0103 {I10} (estimated by
194PTEcN 1992Si02 from a 328|g-gated |g spectrum in 1970Be30) and
194PTFcN I(|e+|b{++})(328 level)=46.2 {I12}; |e/|b{++}(g.s.)(exp)=30 {I10},
194PTGcN estimated by the evaluators from I(K x ray)/I|g(328|g)=1.45 {I15} and
194PTHcN I(|g{+|+})/(2|*I|g(328|g)) data in 1992Si02).1981Ho18 report a much
194PTIcN lower value of 0.022 {I1} for I(|b{++})(total)/I|g(328|g)
194PT PN 3
194PT G 216.14 9 X
194PT cG E$weighted average of 215.6 {I3} (1971Vi15) and 216.15 {I5}
194PT2cG (1960Ba17). See in ce data only; placed from 2357 level in 1960Ba17.
194PT cG $K/L>5.2 (1960Ba17)
194PT cG $Ice(K)=0.73 {I7} (1960Ba17, 1964Be23), 0.18 {I5} (1971Vi15)
194PT G 236.29 10 X
194PT cG E$seen in ce data only (1960Ba17, 1964Be23); placed from 2398 level
194PT2cG in 1960Ba17
194PT cG $Ice(K)=0.50 {I5} (1960Ba17), 0.46 {I9} (1964Be23)
194PT G 671.8 6 X
194PT cG E$from 1960Ba17. Other: 671.16 (1970Ag05).
194PT cG $Ice(K)=0.0200 {I20} (1960Ba17), |?0.019 (1964Be23)
194PT cG $Reported in ce data only (1960Ba17, 1964Be23 and 1970Ag05). Probably
194PT2cG an impurity line since Ice(K)=0.117 (1970Ag05) and 0.019 (1964Be23)
194PT3cG disagree
194PT G 774.9 13 0.08 4 X
194PT cG E,RI$from 1970Be30
194PT G 886.0 20 0.02 1 X
194PT cG E,RI$from 1970Be30
194PT G 932.4 13 0.06 3 X
194PT cG E,RI$from 1970Be30
194PT G 958.0 20 0.10 5 X
194PT cG E,RI$from 1970Be30
194PT G 2199.6 13 0.02 1 X
194PT cG E,RI$from 1970Be30
194PT G 2204.0 13 0.02 1 X
194PT cG E,RI$from 1970Be30
194PT G 2371 3 0.02 AP X
194PT cG $|g reported only in the photo-electron data of 1964Be23
194PT G 2447.4 13 0.02 1 X
194PT cG E,RI$from 1970Be30
194PT L 0.0 0+
194PT E 1.2 1 22 2 8.01 4 23 2
194PTS E EAV=696.55 93$CK=0.7719 2$CL=0.13460 4$CM+=0.04287 2
194PT cE E$measured E|b{++}=1487 {I15} (1960Ba17), 1550 {I20} (1956Th11).
194PT cE TI$see comments for I|g normalization. I(|e+|b{++})(g.s.)=36.2 {I41}
194PT2cE (relative to I|g(328)=100.0 {I10}) is deduced based on
194PT3cE I(|b{++})(total)/I|g(328|g)=0.029 {I2} (1992Si02, 1956Th11),
194PT4cE calculated |e/|b{++} ratios for g.s. and 328 level by LOGFT,
194PT5cE relative I(|e+|b{++})(328 level) from |g+ce intensity balance.
194PT dE $I|b{++}(total)/I|g(328|g)=0.029 {I2} in 1992Si02 is averaged value
194PT2dE deduced from their measured I(|g{+|+})/I|g(482|g)=2.94 {I10} and
194PT3dE I(|g{+|+})/I|g(528|g+529|g)=1.51 {I5}, and, I(482|g)/I(328|g)=0.0185
194PT4dE {I10} and I(528|g+529|g)/I(328|g)=0.037 {I2} from 1970Be30 and
194PT5dE 1974HeYW, plus an estimated 5% correction for annihilation of positrons
194PT6dE in flight.
194PT L 328.474 4 2+
194PT E 0.68 3 28.4 12 7.770 18 29.1 12
194PTS E EAV=552.40 92$CK=0.7930 1$CL=0.13936 3$CM+=0.044440 9
194PT cE E$E|b{++}=1210 {I20} (1956Th11).
194PT G 328.470 6 100.0 10E2 0.0755 C
194PTS G KC=0.0488 7$LC=0.0202 3$MC=0.00504 7
194PTS G NC=0.001236 18$OC=0.000202 3$PC=4.97E-6 7
194PT2 G %IG=62.8 16
194PT cG E$weighted average of 328.50 {I3} (1974HeYW), 328.464 {I6} (1996TeZW),
194PT2cG 328.481 {I10} (2015Do06), and 328.50 {I3} (1960Ba17). Others: 328.47
194PT3cG {I15} (1970Be30) and 328.5 {I3} (1971Vi15)
194PT cG RI$from 2015Do06. Others: 100.0 {I13} (1996TeZW), 100 {I5} (1974HeYW),
194PT2cG and 100 {I5} (1964Be23)
194PT cG M$L1:L2:L3=1.53 {I18}:1.96 {I20}:1.00 (1970Ag05);
194PT2cG M1:M2:M3=1.25 {I25}:1.87 {I34}:1.00 (1970Ag05); |a(K)exp=0.0505 {I20}
194PT3cG (1965Le17), 0.0409 {I22} (1960De17), 0.056 {I6} (1956Th11);
194PT4cG |a(K)exp=0.10 {I2}, |a(L)exp=0.057 {I10}, |a(M)=0.008 {I4} (1949St17).
194PT cG $Ice(K)=100 used to obtain I|g values of transitions where only
194PT2cG ce data are available.
194PT L 622.023 4 2+
194PT E 0.0034 13 0.39 15 9.51 17 0.39 15 ?
194PTS E EAV=423.78 92$CK=0.8032$CL=0.14248 2$CM+=0.045501 7
194PT G 293.549 7 17.33 17E2+M1+E0 +15 2 0.1060 16 C
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
194PT2 G %IG=10.9 3
194PT cG E$weighted average of 293.548 {I7} (1996TeZW), 293.548 {I10}
194PT2cG (2015Do06), and 293.58 {I3} (1974HeYW). Others: 293.55 {I4} (1960Ba17)
194PT3cG 293.53 {I4} (1960De15), and 293.57 {I15} (1970Be30)
194PT cG RI$weighted average of 18.1 {I6} (1964Be23), 17.5 {I9} (1970Be30), 16.6
194PT2cG {I9} (1974HeYW), 17.5 {I3} (1996TeZW), and 17.24 {I17} (2015Do06).
194PT3cG Other: 18.9 {I13} (1971Vi15)
194PT cG M$L1:L2:L3=1.19 {I8}:1.90 {I12}:1.00 (1970Ag05);
194PT2cG M1:M2:M3=1.2 {I4}:1.8 {I6}:1.0 (1970Ag05); |a(K)exp=0.062 {I7}
194PT3cG (1956Th11), 0.034 {I5} (1949St17), 0.065 {I4} (1964Be23), 0.067 {I4}
194PT4cG (1970Be30), 0.071 {I6} (1971Vi15); |a(L)exp=0.017 {I7} (1949St17),
194PT5cG K/L=1.89 {I20} (1960Ba17).
194PT cG MR$from |g|g(|q): average of +16 {I2} (1996TeZW) and +14.3 {I21}
194PT2cG (1971Kr01). Others: +30 {I+11-39} (|g|g(|q),1969Ha43); >4.5 from L-
194PT3cG and M-subshell ratios (1970Ag05).
194PT cG $q(E0/E2) mixing=-0.17 to +0.24 with penetration
194PT2cG parameter (|l)=-170 to +270 from (294 ce(K))(329|g)(|q) (1971Do12).
194PT cG $(293|g)(328|g)(|q): A{-2}=-0.123 {I5}, A{-4}=+0.293 {I8};
194PT2cG A{-2}=-0.127 {I5}, A{-4}=+0.325 {I10} (1971Kr01)
194PT3cG A{-2}=-0.101 {I14}, A{-4}=+0.323 {I22} (1969Ha43).
194PT cG $Ice(K)=25.2 {I12}, weighted average of 24.0 {I4} (1964Be23), 27.6
194PT2cG {I10} (1971Vi15), and 24.0 {I24} (1960Ba17)
194PT dG $|a(K)exp=0.071 {I4} from adopted Ice(K) and I|g here
194PT G 622.010 10 2.40 2 E2 0.01483 C
194PTS G KC=0.01141 16$LC=0.00262 4$MC=0.000627 9
194PTS G NC=0.0001543 22$OC=2.65E-5 4$PC=1.208E-6 17
194PT2 G %IG=1.51 4
194PT cG E$weighted average of 621.995 {I12} (1996TeZW), 622.019 {I10}
194PT2cG (2015Do06), and 622.05 {I6} (1960Ba17). Others: 622.01 {I11}
194PT3cG (1960De15); 621.74 {I5} (1974HeYW) and 622.1 {I3} (1971Vi15) for a
194PT4cG composite peak
194PT cG RI$weighted average of 2.40 {I5} (1996TeZW) and 2.40 {I2} (2015Do06).
194PT2cG Others: 3.85 {I20} (1974HeYW), 3.85 {I25} (1964Be23), and 4.15 {I25}
194PT3cG for a composite peak
194PT cG M$|a(K)exp=0.0128 {I12} deduced from Ice(K)=0.63 {I6} (1971Vi15) and
194PT2cG I|g=2.40 {I2} here; |a(K)exp=0.0087 {I8} (1964Be23) and 0.0088 {I5}
194PT3cG (1970Be30), K/L=4.2 {I8} (1960Ba17) for a composite peak ;
194PT cG $Other Ice(K): 0.685 {I15} (1964Be23) and 0.77 {I8} (1960Ba17) for
194PT2cG a composite peak
194PT L 811.285 7 4+
194PT cL $In order to balance the transition intensity at this level,
194PT2cL 0.075 {I25} units of relative |g intensity should feed this level.
194PT E 6.6E-5 LT 0.018 LT 10.7 GT 0.018 LT ?
194PTS E EAV=340.89 93$CK=0.8061$CL=0.14410 2$CM+=0.046073 6
194PT cE TI$intensity balance gives 0.046 {I15}, but no direct |e feeding is
194PT2cE expected.
194PT G 482.800 8 1.917 19E2 0.0270 C
194PTS G KC=0.0198 3$LC=0.00550 8$MC=0.001340 19
194PTS G NC=0.000329 5$OC=5.55E-5 8$PC=2.08E-6 3
194PT2 G %IG=1.20 4
194PT cG E$weighted average of 482.80 {I4} (1974HeYW), 482.793 {I8} (1996TeZW),
194PT2cG and 482.811 {I10} (2015Do06). Others: 482.65 {I15} (1970Be30), 482.7
194PT3cG {I3} (1971Vi15), and 482.88 {I10} (1960Ba17)
194PT cG RI$weighted average of 1.86 {I10} (1970Be30), 1.84 {I10} (1974HeYW),
194PT2cG 1.92 {I3} (1996TeZW), and 1.920 {I19} (2015Do06). Others: 1.86 {I25}
194PT3cG (1964Be23); 2.33 {I13} (1971Vi15) is discrepant
194PT cG M$|a(K)exp=0.0174 {I20} (1971Vi15), 0.021 {I3} (1964Be23),
194PT2cG 0.0207 {I13} (1970Be30); L1/L2=1.5 {I3}, L1/L3=3.0 {I10} (1970Ag05);
194PT3cG K/L=4.9 {I8}, L12/L3=6 (1960Ba17)
194PT cG $(483|g)(328|g)(|q): A{-2}=+0.101 {I17}, A{-4}=-0.03 {I3}.
194PT cG $Ice(K)=0.80 {I2}, weighted average of 0.79 {I2} (1964Be23), 0.83 {I8}
194PT2cG (1971Vi15), and 0.95 {I10} (1960Ba17)
194PT dG $|a(K)exp=0.0204 {I6} from adopted Ice(K) and I|g here
194PT cG $Placed from 1962 and 2298 levels by 1960Ba17.
194PT L 922.771 6 3+
194PT E 0.016 LT 11.7 GT 0.016 LT 1U?
194PTS E CK=0.7930$CL=0.15599 3$CM+=0.05067 2
194PT G 300.750 7 1.437 14E2(+M1) 5 GT 0.102 5 C
194PTS G KC=0.064 4$LC=0.0283 5$MC=0.00706 11
194PTS G NC=0.00173 3$OC=0.000283 5$PC=6.5E-6 5
194PT2 G %IG=0.90 3
194PT cG E$weighted average of 300.750 {I7} (1996TeZW) and 300.751 {I10}
194PT2cG (2015Do06). Others: 300.71 {I15} (1970Be30), 300.77 {I6} (1974HeYW),
194PT3cG and 300.71 {I5} (1960Ba17)
194PT cG RI$weighted average of 1.459 {I23} (1996TeZW) and 1.432 {I14}
194PT2cG (2015Do06). Others: 1.35 {I10} (1974HeYW), 1.18 {I19} (1964Be23), and
194PT3cG 1.44 {I12} (1970Be30)
194PT cG M,MR$from |a(K)exp and L-subshell ratios. |g|g(|q) give two solutions
194PT2cG for each correlation, a low value (-0.10 {I8}, +0.2 {I4}, +0.01 {I12})
194PT3cG and a high value (+6 {I4}, >6), only the latter is consistent with |d
194PT4cG value from ce data.
194PT cG $|a(K)exp=0.061 {I6} (1970Be30), 0.074 {I12} (1964Be23);
194PT2cG L1:L2:L3=1.21 {I15}:1.79 {I22}:1.00 (1970Ag05); K/L2=3.5 {I1}, K/L3>8
194PT3cG (1960Ba17)
194PT cG $(301|g)(622|g)(|q): A{-2}=-0.15 {I7}, A{-4}=-0.02 {I11}.
194PT cG $(301|g)(293|g)(|q): A{-2}=-0.006 {I21}, A{-4}=-0.03 {I4}.
194PT cG $(301|g)[293|g](328|g)(|q): A{-2}=+0.009 {I20}, A{-4}=-0.10 {I3}.
194PT cG $Ice(K)=1.78 {I4} from 1964Be23. Other: 1.80 {I18} (1960Ba17)
194PT dG $|a(K)exp=0.0604 {I15} from adopted Ice(K) and I|g here
194PT G 594.299 14 0.267 2 E2(+M1) 10 GT 0.0166 3 C
194PTS G KC=0.01270 23$LC=0.00299 5$MC=0.000718 11
194PTS G NC=0.000177 3$OC=3.02E-5 5$PC=1.345E-6 25
194PT2 G %IG=0.168 5
194PT cG E$weighted average of 594.3 {I3} (1971Vi15), 594.270 {I22} (1996TeZW),
194PT2cG and 594.311 {I14} (2015Do06)
194PT cG RI$weighted average of 0.276 {I12} (1996TeZW) and 0.267 {I2}
194PT2cG (2015Do06). Other: 1.07 {I13} for a composite peak (1971Vi15)
194PT cG M,MR$from the Adopted Gammas. |a(K)exp=0.0227 {I26} from Ice(K)=0.124
194PT2cG {I14} (1971Vi15) and I|g=0.267 {I2} here gives |d=1.3 {I3}. It should
194PT3cG be noted that 593.35|g and 594.28|g are not fully resolved in |g-ray
194PT4cG data of 1971Vi15. The adopted value is taken from |g|g(|q) data in
194PT5cG {+194}Ir |b{+-} where only the 594.28|g is present.
194PT cG $(594|g)(328|g)(|q): A{-2}=-0.43 {I8}, A{-4}=-0.22 {I13}; probably
194PT2cG contains 593|g also. |d=-0.54 {I18} or -3.2 {I15} (1996TeZW).
194PT L 1229.521 10 4+
194PT E 0.005 LT 11.1 GT 0.005 LT ?
194PTS E CK=0.8050$CL=0.14755 2$CM+=0.047362 8
194PT cE TI$intensity balance gives -0.003 {I9}, consistent with expected
194PT2cE no direct |e feeding to this level.
194PT G 418.195 23 0.068 7 (E2(+M1)) 3 GT 0.043 5 C
194PTS G KC=0.031 4$LC=0.0091 5$MC=0.00223 9
194PTS G NC=0.000548 23$OC=9.2E-5 5$PC=3.3E-6 5
194PT2 G %IG=0.043 5
194PT cG E$weighted average of 417.95 {I15} (1996TeZW) and 418.197 {I14}
194PT2cG (2015Do06). Others: 418.06 {I20} (1970Be30) and 418.1 {I3} (1971Vi15)
194PT3cG for a composite peak
194PT cG RI$weighted average of 0.07 {I3} (1996TeZW) and 0.066 {I7} (2015Do06).
194PT2cG Other: 0.140 {I11} (1970Be30) and 0.130 {I15} (1971Vi15) for a
194PT3cG composite peak
194PT cG M,MR$|a(K)exp=0.027 {I11} (1971Vi15) for a composite peak
194PT cG $Ice(K)=0.073 {I29} (1971Vi15) for a composite peak,
194PT G 607.496 10 0.476 5 E2 0.01565 C
194PTS G KC=0.01199 17$LC=0.00279 4$MC=0.000670 10
194PTS G NC=0.0001649 23$OC=2.83E-5 4$PC=1.269E-6 18
194PT2 G %IG=0.299 9
194PT cG E$weighted average of 607.498 {I10} (1996TeZW) and 607.493 {I14}
194PT2cG (2015Do06). Others: 607.5 {I3} (1970Be30), 607.5 {I3} (1971Vi15),
194PT3cG 607.54 {I8} (1974HeYW), and 607.61 {I8} (1960Ba17)
194PT cG RI$weighted average of 0.50 {I3} (1970Be30), 0.46 {I5} (1974HeYW),
194PT2cG 0.493 {I8} (1996TeZW), 0.472 {I4} (2015Do06), and 0.9 {I4} (1964Be23).
194PT3cG Other: 0.685 {I10} (1971Vi15) is discrepant
194PT cG M$|a(K)exp=0.0093 {I8} (1971Vi15), 0.007 {I+7-3} (1964Be23), 0.0122
194PT2cG {I10} (1970Be30).
194PT cG $Ice(K)=0.132 {I10}, weighted average of 0.125 {I10} (1964Be23), 0.130
194PT2cG {I10} (1971Vi15), and 0.150 {I15} (1960Ba17)
194PT dG $|a(K)exp=0.0135 {I11} from adopted Ice(K) and I|g here
194PT G 901.077 25 0.0510 20 C
194PT2 G %IG=0.0320 15
194PT cG E$weighted average of 901.18 {I7} (1996TeZW) and 901.071 {I17}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.060 {I5} (1996TeZW) and 0.0506 {I11}
194PT2cG (2015Do06)
194PT L 1267.198 6 0+
194PT E 0.49 6 9.04 6 0.49 6
194PTS E CK=0.8045$CL=0.14793 3$CM+=0.047504 9
194PT G 645.164 9 3.69 8 E2 0.01367 C
194PTS G KC=0.01057 15$LC=0.00237 4$MC=0.000566 8
194PTS G NC=0.0001393 20$OC=2.39E-5 4$PC=1.119E-6 16
194PT2 G %IG=2.32 8
194PT cG E$weighted average of 645.11 {I15} (1970Be30), 645.2 {I3} (1971Vi15),
194PT2cG 645.18 {I3} (1974HeYW), 645.152 {I9} (1996TeZW), 645.174 {I10}
194PT3cG (2015Do06), and 645.32 {I8} (1960Ba17)
194PT cG RI$unweighted average of 3.8 {I3} (1964Be23), 3.62 {I18} (1970Be30),
194PT2cG 3.90 {I19} (1971Vi15), 3.40 {I20} (1974HeYW), 3.86 {I7} (1996TeZW), and
194PT3cG 3.55 {I3} (2015Do06)
194PT cG M$|a(K)exp=0.0098 {I10} (1971Vi15), 0.0104 {I11} (1964Be23), 0.0109
194PT2cG {I7} (1970Be30); K/L=4.7 {I5}, L12/L3=7 (1960Ba17).
194PT cG $(645|g)(622|g)(|q): A{-2}=+0.38 {I5}, A{-4}=+1.16 {I7}.
194PT cG $Ice(K)=0.81 {I2}, from 1964Be23. Others: 0.78 {I7} (1971Vi15) and 0.90
194PT2cG {I9} (1960Ba17).
194PT dG $|a(K)exp=0.0107 {I4}, from Ice(K)=0.81 {I2} and I|g=3.69 {I8} here
194PT G 938.720 9 1.834 18E2 0.00621 C
194PTS G KC=0.00500 7$LC=0.000924 13$MC=0.000216 3
194PTS G NC=5.34E-5 8$OC=9.37E-6 14$PC=5.28E-7 8
194PT2 G %IG=1.15 3
194PT cG E$weighted average of 938.69 {I15} (1970Be30), 938.71 {I3} (1974HeYW),
194PT2cG 938.706 {I9} (1996TeZW), 938.737 {I10} (2015Do06), and 938.87 {I10}
194PT3cG (1960Ba17)
194PT cG RI$weighted average of 2.2 {I3} (1964Be23), 1.87 {I10} (1970Be30), 1.88
194PT2cG {I13} (1971Vi15), 1.76 {I15} (1974HeYW), 1.90 {I4} (1996TeZW), and
194PT3cG 1.818 {I18} (2015Do06)
194PT cG M$|a(K)exp=0.0044 {I7} (1964Be23), 0.0052 {I4} (1970Be30).
194PT cG $(939|g)(328|g)(|q): A{-2}=+0.332 {I21}, A{-4}=+1.21 {I3}.
194PT cG $Ice(K)=0.202 {I10}, weighted average of 0.198 {I10} (1964Be23) and
194PT2cG 0.220 {I22} (1960Ba17).
194PT dG $|a(K)exp=0.0054 {I3}, from Ice(K)=0.202 {I10} and I|g=1.834 {I18} here
194PT G 1267.36 16 E0 0.0038 2
194PT cG E$transition seen in ce data only (1960Ba17,1964Be23).
194PT cG TI$from Ice(K)=0.067 {I3} (1964Be23) and ce(K)/ce=0.8611 for E0 (BrIcc)
194PT cG M$|a(total)exp=0.004 {I2} for a gamma line at 1270 {I20} (1956Th11);
194PT2cG |a(K)exp>0.024 (1970Be30), >0.012 (1964Be23).
194PT cG $Ice(K)=0.069 {I4}, weighted average of 0.067 {I3} (1964Be23),
194PT2cG and 0.080 {I8} (1960Ba17)
194PT L 1373.764 16 (5-)
194PT cL $In order to balance the transition intensity at this level,
194PT2cL 0.075 {I12} units of relative |g intensity should feed this level
194PT3cL (2015Do06).
194PT E 0.055 8 9.91 7 0.055 8 ?
194PTS E CK=0.8029$CL=0.14910 3$CM+=0.04795 1
194PT cE TI$intensity balance gives 0.046 {I7}, but no direct |e feeding is
194PT2cE expected (2015Do06).
194PT G 562.478 14 0.138 6 (E1) 0.00646 C
194PTS G KC=0.00539 8$LC=0.000823 12$MC=0.000188 3
194PTS G NC=4.63E-5 7$OC=8.22E-6 12$PC=5.17E-7 8
194PT2 G %IG=0.087 5
194PT cG E$weighted average of 562.4 {I3} (1970Be30), 562.5 {I3} (1971Vi15),
194PT2cG 562.6 {I3} (1974HeYW), 562.449 {I20} (1996TeZW), and 562.492 {I14}
194PT3cG (2015Do06)
194PT cG RI$unweighted average of 0.128 {I10} (1970Be30), 0.15 {I4} (1974HeYW),
194PT2cG 0.147 {I5} (1996TeZW), and 0.127 {I1} (2015Do06). Other: |?0.20
194PT3cG (1971Vi15)
194PT cG M$|a(K)exp=0.010 {I4} deduced from Ice(K)=0.027 {I10} (1971Vi15) and
194PT2cG I|g=0.138 {I6} here, gives |d(M2/E1)=0.19 {I+8-13} or Mult=E2.
194PT3cG |g|g(|q) data give a low value (-0.3 {I3} or -0.05 {I17}) and a high
194PT3cG value (-5 {I+3-}|@ or >+4), the former is consistent with |a(K)exp.
194PT cG $Placement from 1997Te09.
194PT cG $(562|g)(483|g)(|q): A{-2}=-0.10 {I6}, A{-4}=-0.05 {I10}.
194PT cG $(562|g)[483|g](328|g)(|q): A{-2}=-0.10 {I11}, A{-4}=-0.02 {I18}.
194PT L 1432.545 6 3-
194PT E 0.08 LT 9.7 GT 0.08 LT ?
194PTS E CK=0.8019$CL=0.14985 3$CM+=0.04824 1
194PT cE TI$intensity balance gives 0.04 {I4}, consistent with expected
194PT2cE no direct |e feeding to this level.
194PT G 59.2 4 0.0008 2 (E2) 50.9 19 A
194PTS G LC=38.2 14$MC=9.9 4
194PTS G NC=2.40 9$OC=0.372 14$PC=0.000406 12
194PT2 G %IG=5.0E-4 13
194PT cG E$weighted average of 58.8 {I3} from |g|g data (1996TeZW) and
194PT2cG 59.5 {I3} from ce data (1971Vi15). Estimated branching is 1% from 1432
194PT3cG level.
194PT cG RI$from Ice(L1)=0.63 {I13} and assigned Mult (1971Vi15).
194PT cG M,MR$M1(+E2), |d<0.1 from L1/L2>7 (1971Vi15), but E2 required
194PT2cG by |DJ|p.
194PT G 202.96 5 0.568 11E1 0.0676 C
194PTS G KC=0.0555 8$LC=0.00930 13$MC=0.00215 3
194PTS G NC=0.000525 8$OC=9.08E-5 13$PC=4.85E-6 7
194PT2 G %IG=0.357 12
194PT cG E$unweighted average of 202.76 {I20} (1970Be30), 203.0 {I3} (1971Vi15),
194PT2cG 203.01 {I10} (1974HeYW), 203.085 {I13} (1996TeZW), 203.004 {I10}
194PT3cG (2015Do06), and 202.91 {I6} (1960Ba17)
194PT cG RI$weighted average of 0.54 {I5} (1970Be30), 0.57 {I6} (1971Vi15),
194PT2cG 0.573 {I15} (1996TeZW), and 0.566 {I11} (2015Do06). Other: 1.2 {I3}
194PT3cG (1974HeYW) is discrepant
194PT cG M$|a(K)exp=0.054 {I7} (1970Be30), 0.062 {I9} (1971Vi15), giving
194PT2cG |d<0.03. Other: |d=-0.09 {I7} from 203|g-328|g(|q), +0.5
194PT2cG {I3} or +1.3 {I7} from 203|g-607|g(|q) of 1996TeZW, only the first
194PT3cG value consistent with |a(K)exp.
194PT cG $(203|g)(607|g)(|q): A{-2}=-0.17 {I4}, A{-4}=+0.03 {I7}.
194PT cG $(203|g)[901](328|g)(|q): A{-2}=-0.06 {I6}, A{-4}=+0.10 {I9}.
194PT cG $Placed from 2366 level by 1960Ba17.
194PT cG $Ice(K)=0.65 {I6}, weighted average of 0.72 {I7} (1971Vi15) and 0.60
194PT2cG {I6} (1960Ba17, 1964Be23).
194PT dG $|a(K)exp=0.056 {I5}, from Ice(K)=0.65 {I6} and I|g=0.568 {I11} here
194PT G 621.250 14 1.33 1 E1 0.00527 C
194PTS G KC=0.00441 7$LC=0.000668 10$MC=0.0001527 22
194PTS G NC=3.76E-5 6$OC=6.68E-6 10$PC=4.25E-7 6
194PT2 G %IG=0.836 24
194PT cG E$weighted average of 621.259 {I15} (1996TeZW) and 621.242 {I14}
194PT2cG (2015Do06). Others: 621.62 {I15} (1970Be30) and 621.74 {I5} (1974HeYW)
194PT3cG for a composite peak; 621.2 {I3} (1971Vi15)
194PT cG RI$weighted average of 1.39 {I5} (1996TeZW) and 1.33 {I1} (2015Do06).
194PT2cG Other: 3.85 {I20} (1974HeYW), 3.81 {I19} (1970Be30) and 4.15 {I25}
194PT3cG (1971Vi15) for a composite peak
194PT cG M$|a(K)exp=0.0055 {I6}, using Ice(K)=0.150 {I15} (1971Vi15) and adopted
194PT2cG I|g=1.33 {I1} here. |g|g(|q) data of 1996TeZW is also consistent with
194PT3cG |d=0 (evaluators' estimate), 1996TeZW quote |d=+0.33 {I10} or +1.8 {I4}
194PT4cG from 621|g-483|g(|q), and -0.010 {I25} from 621|g-328|g(|q).
194PT cG $(621|g)(483|g)(|q): A{-2}=-0.144 {I20}, A{-4}=0.00 {I3}.
194PT cG $(621|g)[483|g](328|g)(|q): A{-2}=-0.134 {I22}, A{-4}=-0.02 {I4}.
194PT G 810.533 14 0.283 3 E1 0.00313 C
194PTS G KC=0.00263 4$LC=0.000391 6$MC=8.91E-5 13
194PTS G NC=2.19E-5 3$OC=3.92E-6 6$PC=2.56E-7 4
194PT2 G %IG=0.178 5
194PT cG E$weighted average of 810.65 {I8} (1974HeYW), 810.53 {I3} (1996TeZW),
194PT2cG and 810.530 {I14} (2015Do06). Others: 810.5 {I3} (1970Be30), 810.47
194PT3cG {I20} (1971Vi15), and 810.9 {I6} (1960Ba17)
194PT cG RI$weighted average of 0.285 {I12} (1996TeZW) and 0.283 {I3}
194PT2cG (2015Do06). Others: 0.31 {I5} (1970Be30), 0.28 {I6} (1971Vi15), and
194PT3cG 0.34 {I3} (1974HeYW)
194PT cG M$|a(K)exp=0.0026 {I10} (1971Vi15) and 0.0021 {I7} (1970Be30) gives
194PT2cG |d<0.1.
194PT cG $Also placed from 2357 level by 1960Ba17.
194PT cG $Ice(K)=0.0148 {I15}, weighted average of 0.013 {I4} (1964Be23), 0.015
194PT2cG {I5} (1971Vi15), and 0.0150 {I15} (1960Ba17).
194PT dG $|a(K)exp=0.0025 {I3}, from Ice(K)=0.0148 {I15} and I|g=0.283 {I3} here
194PT G 1104.056 10 3.42 3 E1 1.77E-3 C
194PTS G KC=0.001490 21$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=1.074E-6 15
194PT2 G %IG=2.15 6
194PT cG E$weighted average of 1104.04 {I15} (1970Be30), 1103.9 {I2} (1971Vi15),
194PT2cG 1104.06 {I5} (1974HeYW), 1104.044 {I10} (1996TeZW), 1104.068 {I10}
194PT3cG (2015Do06), and 1104.12 {I20} (1960Ba17)
194PT cG RI$weighted average of 3.39 {I17} (1970Be30), 3.48 {I13} (1971Vi15),
194PT2cG 3.54 {I7} (1996TeZW), and 3.39 {I3} (2015Do06). Others: 3.91 {I19}
194PT3cG (1964Be23) and 3.27 {I20} (1974HeYW)
194PT cG M$|a(K)exp=0.00185 {I15} (1964Be23), 0.00213 {I14} (1970Be30);
194PT2cG L1/L2=15.4 {I25}, L1/L3=16.3 {I47} (1970Ag05)
194PT cG $(1104|g)(328|g)(|q): A{-2}=-0.122 {I17}, A{-4}=-0.03 {I3} gives
194PT2cG |d=-0.062 {I21} or +9.92 {I21}, only the former consistent with
194PTxcG |a(K)exp.
194PT cG $Ice(K)=0.150 {I5}, weighted average of 0.148 {I5} (1964Be23), 0.15
194PT2cG {I10} (1971Vi15), and 0.170 {I17} (1960Ba17).
194PT dG $|a(K)exp=0.00214 {I8}, from Ice(K)=0.150 {I5} and I|g=3.42 {I4} here
194PT G 1432.542 14 0.112 2 [E3] 0.00566 C
194PTS G KC=0.00450 7$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
194PT2 G %IG=0.0704 23
194PT cG E$weighted average of 1432.50 {I8} (1996TeZW) and 1432.543 {I14}
194PT2cG (2015Do06). Others: 1432.0 {I6} (1970Be30), 1431.6 {I4} (1974HeYW),
194PT3cG 1432.3 {I3} (1960Ba17) could be for a doublet
194PT cG RI$weighted average of 0.116 {I10} (1996TeZW) and 0.112 {I2}
194PT2cG (2015Do06). Others: 0.24 {I5} (1970Be30) and 0.30 {I5} (1974HeYW)
194PT3cG could be for a doublet
194PT cG $|a(K)exp>0.0013 (1964Be23), 0.0029 {I7} (1970Be30) could be for a
194PT2cG doublet.
194PT cG $Ice(K)=0.0153 {I15}, weighted average of 0.0144 {I10} (1964Be23) and
194PT2cG 0.0180 {I18} (1960Ba17).
194PT dG $|a(K)exp=0.0067 {I7}, from Ice(K)=0.0153 {I15} and I|g=0.112 {I2} here
194PT L 1479.270 6 0+
194PT E 1.13 4 8.506 16 1.13 4
194PTS E CK=0.8010$CL=0.15051 4$CM+=0.04849 2
194PT G 857.265 24 0.016 4 C
194PT2 G %IG=0.010 3
194PT cG E$weighted average of 857.59 {I25} (1996TeZW) and 857.263 {I18}
194PT2cG (2015Do06)
194PT cG RI$unweighted average of 0.0124 {I25} (1996TeZW) and 0.020 {I2}
194PT2cG (2015Do06)
194PT G 1150.780 10 2.306 23E2 0.00416 C
194PTS G KC=0.00340 5$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=1.161E-6 17
194PT2 G %IG=1.45 4
194PT cG E$weighted average of 1150.78 {I5} (1974HeYW), 1150.765 {I11}
194PT2cG (1996TeZW), and 1150.792 {I10} (2015Do06). Others: 1150.80 {I15}
194PT3cG (1970Be30), 1150.9 {I2} (1971Vi15), and 1150.91 {I20} (1960Ba17)
194PT cG RI$weighted average of 2.42 {I22} (1964Be23), 2.29 {I13} (1970Be30),
194PT2cG 2.3 {I7} (1971Vi15), 2.26 {I15} (1974HeYW), 2.34 {I4} (1996TeZW), and
194PT3cG 2.295 {I23} (2015Do06)
194PT cG M$|a(K)exp=0.0035 {I4} (1964Be23), 0.00369 {I25} (1970Be30),
194PT2cG 0.0038 {I+23-12} (1971Vi15); L1/L2=6.8 {I16}, L1/L3|?13 (1970Ag05).
194PT3cG Other: |a(total)exp=0.003 {I1} for a gamma line at 1160 {I20}
194PT4cG (1956Th11).
194PT cG $(1151|g)(328|g)(|q): A{-2}=+0.368 {I25}, A{-4}=+1.20 {I4}.
194PT cG $Ice(K)=0.175 {I5}, weighted average of 0.173 {I5} (1964Be23), 0.174
194PT2cG {I16} (1971Vi15), and 0.200 {I20} (1960Ba17).
194PT dG $|a(K)exp=0.00370 {I11}, from Ice(K)=0.175 {I5} and I|g=2.306 {I23}
194PT2dG here
194PT G 1479.33 11 E0 0.113 3
194PT cG E$weighted average of 1479.3 {I3} (1971Vi15), 1479.27 {I10} (2015Do06),
194PT2cG and 1479.75 {I25} (1960Ba17). Transition seen in ce data only
194PT cG M$L1/L2=26 {I7} (1970Ag05) consistent with E0. Others: |a(K)exp>0.087
194PT2cG (1964Be23), >0.45 (1970Be30), >0.89 (1971Vi15).
194PT cG TI$deduced from Ice(K)=2.00 {I5} (1971Vi15) and ce(K)/ce=0.8617
194PT2cG for E0 (BrIcc)
194PT cG $Ice(K)=1.99 {I13}, unweighted average of 1.77 {I3} (1964Be23), 2.00
194PT2cG {I5} (1971Vi15), and 2.20 {I22} (1960Ba17)
194PT L 1512.002 6 2+
194PT E 0.499 21 8.833 19 0.499 21
194PTS E CK=0.8003$CL=0.15101 4$CM+=0.04869 2
194PT G 244.798 22 0.0313 7 (E2) 0.184 C
194PTS G KC=0.1019 15$LC=0.0622 9$MC=0.01576 22
194PTS G NC=0.00386 6$OC=0.000620 9$PC=9.98E-6 14
194PT2 G %IG=0.0197 7
194PT cG E$weighted average of 244.8 {I3} (1971Vi15), 244.92 {I7} (1996TeZW),
194PT2cG and 244.790 {I18} (2015Do06)
194PT cG RI$weighted average of 0.033 {I5} (1996TeZW) and 0.0313 {I7}
194PT2cG (2015Do06). Other: 0.045 {I7} (1977Vy01)
194PT cG M$|a(K)exp=0.22 {I6} deduced from Ice(K)=0.13 {I3} (1971Vi15) and
194PT2cG adopted I|g=0.0313 {I7} here gives |d(E2/M1)=1.4 {I+8-4} or
194PT3cG |d(M2/E1)=0.35 {I+6-7}, but Mult=E2 is required by |DJ|p
194PT G 589.208 10 0.440 4 E2+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
194PT2 G %IG=0.277 8
194PT cG E$weighted average of 589.06 {I15} (1970Be30), 589.24 {I7} (1974HeYW),
194PT2cG 589.199 {I10} (1996TeZW), 589.222 {I14} (2015Do06), and 589.39 {I10}
194PT3cG (1960Ba17)
194PT cG RI$weighted average of 0.7 {I3} (1964Be23), 0.414 {I24} (1970Be30),
194PT2cG 0.41 {I4} (1974HeYW), 0.457 {I10} (1996TeZW), and 0.438 {I4}
194PT3cG (2015Do06). Other: 0.528 {I10} (1971Vi15) is discrepant
194PT cG M,MR$from |a(K)exp=0.010 {I+10-4} (1964Be23), 0.0180 {I16} (1970Be30).
194PT2cG Other: |d=+7.8 {I18} from 589|g-301|g(|q) or -0.16 {I14} from
194PT3cG 589|g-328|g(|q) (1996TeZW), only the former is somewhat consistent
194PT4cG with |a(K)exp.
194PT cG $(589|g)(301|g)(|q): A{-2}=+0.13 {I4}, A{-4}=+0.51 {I6}.
194PT cG $(589|g)[594|g](328|g)(|q): A{-2}=-0.01 {I4}, A{-4}=+0.08 {I7}.
194PT cG $Ice(K)=0.159 {I12}, weighted average of 0.153 {I10} (1964Be23) and
194PT2cG 0.180 {I18} (1960Ba17).
194PT dG $|a(K)exp=0.0158 {I20}, from Ice(K)=0.159 {I12} and I|g=0.49 {I5} here
194PT G 700.675 16 0.0919 9 E2 0.01140 C
194PTS G KC=0.00892 13$LC=0.00190 3$MC=0.000452 7
194PTS G NC=0.0001112 16$OC=1.92E-5 3$PC=9.45E-7 14
194PT2 G %IG=0.0578 17
194PT cG E$weighted average of 700.66 {I4} (1996TeZW) and 700.677 {I16}
194PT2cG (2015Do06). Others: 700.6 {I6} (1970Be30) and 700.8 {I3} (1971Vi15)
194PT cG RI$weighted average of 0.10 {I5} (1970Be30), 0.096 {I5} (1996TeZW), and
194PT2cG 0.0918 {I9} (2015Do06). Other: 0.773 {I10} for a composite peak
194PT3cG (1971Vi15)
194PT cG M$from |a(K)exp=0.0101 {I27} deduced from Ice(K)=0.019 {I5} (1971Vi15)
194PT2cG and I|g=0.0919 {I9} here
194PT G 889.969 14 0.183 3 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
194PT2 G %IG=0.115 4
194PT cG E$weighted average of 889.976 {I24} (1996TeZW) and 889.967 {I14}
194PT2cG (2015Do06). Others: 889.7 {I3} (1970Be30), 889.97 {I10} (1974HeYW),
194PT3cG and 890.09 {I15} (1960Ba17)
194PT cG RI$weighted average of 0.26 {I7} (1970Be30), 0.25 {I6} (1971Vi15), 0.19
194PT2cG {I3} (1974HeYW), 0.200 {I8} (1996TeZW), and 0.182 {I2} (2015Do06)
194PT cG M,MR$from |a(K)exp=0.0128 {I6} deduced from Ice(K)=0.048 {I2} and
194PT2cG I|g=0.183 {I3} here, and |g|g(|q) in 1996TeZW with |d=+0.8 {I19} from
194PT3cG 890|g-293|g(|q) or +0.4 {I7} from 890|g-328|g(|q)
194PT cG $(890|g)(293|g)(|q): A{-2}=+0.13 {I7}, A{-4}=-0.09 {I13}.
194PT cG $(890|g)[293|g](328|g)(|q): A{-2}=+0.02 {I9}, A{-4}=-0.01 {I15}.
194PT cG $Ice(K)=0.048 {I2}, weighted average of 0.047 {I2} (1964Be23) and 0.053
194PT2cG {I5} (1960Ba17).
194PT G 1183.535 10 1.012 10M1+E2 +1.09 +18-160.0061 4 C
194PTS G KC=0.0050 4$LC=0.00081 5$MC=0.000186 11
194PTS G NC=4.6E-5 3$OC=8.3E-6 5$PC=5.4E-7 4$IPC=3.68E-6 15
194PT2 G %IG=0.636 19
194PT cG E$weighted average of 1183.52 {I5} (1974HeYW), 1183.523 {I21}
194PT2cG (1996TeZW), and 1183.539 {I10} (2015Do06). Others: 1183.63 {I20}
194PT3cG (1970Be30), 1183.4 {I2} (1971Vi15), and 1183.63 {I20} (1960Ba17)
194PT cG RI$weighted average of 1.30 {I25} (1964Be23), 1.04 {I10} (1970Be30),
194PT2cG 1.1 {I7} (1971Vi15), 1.04 {I10} (1974HeYW), 1.030 {I18} (1996TeZW), and
194PT3cG 1.006 {I10} (2015Do06)
194PT cG M,MR$|a(K)exp=0.00502 {I20} deduced from Ice(K)=0.104 {I4} and
194PT2cG I|g=1.012 {I10} here, L1/L2=16.9 {I77} (1970Ag05), and |g|g(|q) of
194PT3cG 1996TeZW with |d=+1.5 {I6}. Other |a(K)exp: 0.0039 {I8} (1964Be23),
194PT4cG 0.0049 {I5} (1970Be30), 0.004 {I+8-2} (1971Vi15)
194PT cG $(1183|g)(328|g)(|q): A{-2}=-0.33 {I3}, A{-4}=+0.22 {I6}.
194PT cG $Ice(K)=0.104 {I4}, weighted average of 0.103 {I4} (1964Be23), 0.102
194PT2cG {I5} (1971Vi15), and 0.120 {I12} (1960Ba17).
194PT G 1512.073 14 0.068 15(E2) 0.00255 @C
194PTF G FL=0.0
194PTF G FLAG=Y
194PTS G KC=0.00205 3$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
194PT2 G %IG=0.043 10
194PT cG E$from 2015Do06. Others: 1512.0 {I3} (1971Vi15), 1511.9 {I3}
194PT2cG (1974HeYW), 1512.33 {I11} (1996TeZW) for a composite peak.
194PT cG RI$weighted average of 0.040 {I17} (1996TeZW), and 0.076 {I9}
194PT2cG (2015Do06). Others: 0.19 {I5} (1970Be30), 0.18 {I3} (1971Vi15),
194PT3cG and 0.19 {I3} (1974HeYW) are undivided for a doublet
194PT cG $Total intensity=0.171 {I1} for doublet in 2015Do06 and divided by
194PT2cG evaluators for placement from 1512 based on {+194}Ir |b{+-} decay
194PT3cG (19.3 h) dataset, remaining intensity is assigned from 2134 level.
194PT cG M$|a(K)exp=0.0035 {I+15-11} (1971Vi15) and 0.0029 {I8} (1970Be30)
194PT2cG for the doublet is consistent with M1,E2 for both components; E2
194PT3cG required by |DJ|p.
194PT cG $Ice(K)=0.0121 {I10}, weighted average of 0.0110 {I10} (1964Be23),
194PT2cG 0.0140 {I14} (1960Ba17), and 0.0125 {I20} for a doublet.
194PT L 1547.273 8 0+
194PT E 1.36 5 8.365 17 1.36 5
194PTS E CK=0.7995$CL=0.15159 4$CM+=0.04891 2
194PT G 925.251 14 0.497 5 E2 0.00639 C
194PTS G KC=0.00515 8$LC=0.000955 14$MC=0.000224 4
194PTS G NC=5.52E-5 8$OC=9.69E-6 14$PC=5.43E-7 8
194PT2 G %IG=0.312 9
194PT cG E$weighted average of 925.265 {I14} (2015Do06), 925.15 {I7} (1974HeYW),
194PT2cG and 925.240 {I15} (1996TeZW). Others: 925.28 {I12} (1960Ba17), 925.09
194PT3cG {I20} (1970Be30), and 925.3 {I2} (1971Vi15)
194PT cG RI$weighted average of 0.495 {I5} (2015Do06), 0.75 {I25} (1964Be23),
194PT2cG 0.48 {I4} (1970Be30), 0.60 {I8} (1971Vi15), 0.48 {I5} (1974HeYW), and
194PT3cG 0.508 {I13} (1996TeZW)
194PT cG M$|a(K)exp=0.0040 {I+30-13} (1964Be23), 0.0061 {I6} (1970Be30),
194PT2cG 0.0056 {I+16-12} (1971Vi15) .
194PT cG $Ice(K)=0.062 {I3}, weighted average of 0.060 {I3} (1964Be23), 0.068
194PT2cG {I7} (1971Vi15), and 0.068 {I7} (1960Ba17).
194PT dG $|a(K)exp=0.0061 {I3}, from Ice(K)=0.062 {I3} and I|g=0.497 {I5} here
194PT G 1218.791 10 1.903 19E2 0.00373 C
194PTS G KC=0.00306 5$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=5.99E-6 9
194PT2 G %IG=1.20 4
194PT cG E$weighted average of 1218.802 {I10} (2015Do06), 1218.76 {I5}
194PT2cG (1974HeYW), and 1218.776 {I12} (1996TeZW). Others: 1219.01 {I20}
194PT3cG (1960Ba17), 1218.79 {I22} (1970Be30), and 1218.9 {I2} (1971Vi15)
194PT cG RI$weighted average of 1.894 {I19} (2015Do06), 1.86 {I10} (1970Be30),
194PT2cG and 1.95 {I4} (1996TeZW). Others: 2.17 {I19} (1964Be23), 2.0 {I7}
194PT3cG (1971Vi15), and 1.76 {I15} (1974HeYW)
194PT cG M$|a(K)exp=0.0029 {I3} (1964Be23), 0.00337 {I22} (1970Be30),
194PT2cG 0.0032 {I+21-10} (1971Vi15).
194PT cG $Also placed from 2142 level by 1960Ba17.
194PT cG $Ice(K)=0.130 {I5}, weighted average of 0.128 {I4} (1964Be23), 0.129
194PT2cG {I8} (1971Vi15), and 0.160 {I16} (1960Ba17).
194PT dG $|a(K)exp=0.00333 {I13}, from Ice(K)=0.130 {I5} and I|g=1.903 {I19}
194PT2dG here
194PT G 1547.9 4 E0 0.0041 4
194PT cG E$transition seen in ce data only (1960Ba17, 1964Be23).
194PT cG $I|g<0.62 (1964Be23)
194PT cG TI$deduced from Ice(K)=0.072 {I6} and ce(K)/ce=0.8618 for E0 (BrIcc)
194PT cG $|a(K)exp>0.0053 (1964Be23), >0.027 (1970Be30).
194PT cG $Ice(K)=0.072 {I6}, weighted average of 0.068 {I5} (1964Be23) and
194PT2cG 0.081 {I8} (1960Ba17)
194PT L 1622.197 8 2+
194PT E 0.128 15 9.32 5 0.128 15
194PTS E CK=0.7976$CL=0.15298 5$CM+=0.04944 2
194PT G 699.257 18 0.0253 7 YC
194PTF G FL=922.771
194PT2 G %IG=0.0159 6
194PT cG E$weighted average of 699.20 {I15} (1996TeZW) and 699.258 {I18}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.023 {I4} (1996TeZW) and 0.0254 {I7} (2015Do06)
194PT G 1000.190 15 0.296 22M1+E2 1.38 +13-120.0081 4 C
194PTS G KC=0.0066 3$LC=0.00111 5$MC=0.000258 10
194PTS G NC=6.36E-5 24$OC=1.13E-5 5$PC=7.2E-7 4
194PT2 G %IG=0.186 15
194PT cG E$weighted average of 1000.168 {I14} (2015Do06), 1000.17 {I18}
194PT2cG (1960Ba17), 1000.3 {I3} (1970Be30), 1000.2 {I2} (1971Vi15), 1000.19
194PT3cG {I15} (1974HeYW), and 1000.239 {I21} (1996TeZW)
194PT cG RI$unweighted average of 0.235 {I2} (2015Do06), 0.34 {I7} (1970Be30),
194PT2cG 0.35 {I6} (1971Vi15), 0.27 {I3} (1974HeYW), and 0.286 {I10} (1996TeZW)
194PT cG M,MR$from |a(K)exp=0.0081 {I8} deduced from Ice(K)=0.049 {I3} and
194PT2cG I|g=0.296 {I22} here L1/L2=6.9 {I19}, L1/L3>18.3. Others: |d=-1.3 {I24}
194PT3cG or +1.0 {I19} from 1000|g-293|g(|q), or -0.5 {I13} from
194PT4cG 1000|g-328|g(|q) of 1996TeZW. Other |a(K)exp: 0.0070 {I14} (1970Be30),
194PT5cG 0.0068 {I+20-14} (1971Vi15)
194PT cG $(1000|g)(293|g)(|q): A{-2}=-0.11 {I6}, A{-4}=+0.14 {I10}.
194PT cG $(1000|g)[293|g](328|g)(|q): A{-2}=-0.16 {I7}, A{-4}=-0.09 {I12}.
194PT cG $Ice(K)=0.0495 {I25}, weighted average of 0.0485 {I25} (1964Be23),
194PT2cG 0.049 {I3} (1971Vi15), and 0.057 {I6} (1960Ba17).
194PT G 1293.708 14 0.221 2 E2+M1+E0 -0.9 1 0.0192 8 C
194PT2 G %IG=0.139 4
194PT cG E$weighted average of 1293.709 {I14} (2015Do06) and 1293.69 {I8}
194PT2cG (1996TeZW). Others: 1293.9 {I5} (1960Ba17) and 1293.7 {I3} (1971Vi15)
194PT cG RI$from 2015Do06. Others: 0.2 {I1} (1970Be30), 0.28 {I7} (1971Vi15),
194PT2cG and 0.214 {I23} (1996TeZW)
194PT cG M$|a(K)exp=0.012 {I+5-3} (1971Vi15), 0.015 {I8} (1970Be30), >0.0093
194PT2cG (1964Be23)
194PT cG MR$from Adopted Gammas. Other: <0.8 from |a(K)exp above and +0.07 {I14}
194PT2cG from |g|g(|q) of 1996TeZW
194PT cG $(1294|g)(328|g)(|q): A{-2}=+0.16 {I11}, A{-4}=-0.29 {I18}.
194PT cG $Ice(K)=0.065 {I3}, weighted average of 0.059 {I4} (1964Be23), 0.067
194PT2cG {I3} (1971Vi15), and 0.073 {I7} (1960Ba17).
194PT cG CC$from |a(K)exp=0.0144 {I7}, from Ice(K)=0.065 {I3} and
194PT2cG I|g=0.221 {I2} given here
194PT G 1622.185 14 0.300 3 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$IPC=0.0001085 16
194PT2 G %IG=0.189 6
194PT cG E$from 2015Do06. Others: 1622.2 {I6} (1970Be30), 1622.23 {I15}
194PT2cG (1974HeYW), 1622.21 {I10} (1996TeZW), and 1622.6 {I5} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.32 {I6} (1970Be30), 0.31 {I3} (1971Vi15),
194PT2cG 0.26 {I4} (1974HeYW), and 0.26 {I5} (1996TeZW)
194PT cG M$|a(K)exp=0.00192 {I23}, deduced from Ice(K)=0.0118 {I14} and
194PT2dG I|g=0.300 {I3} here. Other |a(K)exp: 0.0016 {I4} (1970Be30)
194PT cG $Ice(K)=0.0118 {I14}, weighted average of 0.0101 {I15} (1964Be23) and
194PT2cG 0.0130 {I13} (1960Ba17).
194PT L 1670.656 6 2+
194PT E 2.27 8 8.020 16 2.27 8
194PTS E CK=0.7961$CL=0.15401 5$CM+=0.04984 2
194PT G 747.88 4 0.0069 4 N ?
194PT2 G %IG=0.0043 3
194PT G 859.370 24 0.0954 12(E2) 0.00742 C
194PTS G KC=0.00594 9$LC=0.001138 16$MC=0.000268 4
194PTS G NC=6.60E-5 10$OC=1.154E-5 17$PC=6.28E-7 9
194PT2 G %IG=0.0600 18
194PT cG E$weighted average of 859.3 {I13} (1970Be30), 859.46 {I4} (1996TeZW),
194PT2cG 859.353 {I17} (2015Do06), and 860.2 {I8} (1960Ba17)
194PT cG RI$weighted average of 0.0961 {I9} (2015Do06), 0.10 {I4} (1970Be30),
194PT2cG and 0.0911 {I23} (1996TeZW)
194PT cG M$|a(K)exp=0.0041 {I4} deduced from Ice(K)=0.0080 {I8} and
194PT2cG I|g=0.0954 {I12} here. Other |a(K)exp: 0.003 {I2} (1970Be30).
194PT cG $Ice(K)=0.0080 {I8} (1960Ba17). Other: |?0.0064 (1964Be23)
194PT G 1048.633 10 1.428 14M1 0.01161 C
194PTS G KC=0.00964 14$LC=0.001515 22$MC=0.000348 5
194PTS G NC=8.61E-5 12$OC=1.553E-5 22$PC=1.067E-6 15
194PT2 G %IG=0.90 3
194PT cG E$weighted average of 1048.647 {I10} (2015Do06), 1048.72 {I16}
194PT2cG (1960Ba17), 1048.58 {I15} (1970Be30), 1048.6 {I2} (1971Vi15), 1048.58
194PT3cG {I5} (1974HeYW), and 1048.621 {I10} (1996TeZW)
194PT cG RI$weighted average of 1.417 {I14} (2015Do06), 1.55 {I25} (1964Be23),
194PT2cG 1.41 {I8} (1970Be30), 1.5 {I8} (1971Vi15), 1.41 {I10} (1974HeYW), and
194PT3cG 1.48 {I3} (1996TeZW)
194PT cG M,MR$from |a(K)exp=0.0093 {I+30-20} (1964Be23), 0.0103 {I7} (1970Be30),
194PT2cG 0.010 {I+16-5} (1971Vi15), L1/L2=14.3 {I29} and L1/L3>50 (1970Ag05).
194PT3cG Others: |d=-0.7 {I7} or -0.02 {I18} from |g|g(|q) of 1996TeZW
194PT cG $(1049|g)(293|g)(|q): A{-2}=-0.04 {I3}, A{-4}=+0.03 {I4}.
194PT cG $(1049|g)[293|g](328|g)(|q): A{-2}=-0.07 {I3}, A{-4}=-0.11 {I5}.
194PT cG $Ice(K)=0.298 {I6}, weighted average of 0.297 {I6} (1964Be23), 0.30
194PT2cG {I3} (1971Vi15), and 0.35 {I4} (1960Ba17).
194PT dG $|a(K)exp=0.01018 {I23}, from Ice(K)=0.298 {I6} and I|g=1.428 {I14}
194PT2dG here
194PT G 1342.170 10 2.15 4 M1+E2 -0.23 9 0.0061216 C
194PTS G KC=0.00506 14$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
194PT2 G %IG=1.35 5
194PT cG E$weighted average of 1342.173 {I10} (2015Do06) and 1342.164 {I16}
194PT2cG (1996TeZW). Others: 1342.44 {I20} (1960Ba17), 1342.4 {I3} (1970Be30),
194PT3cG 1342.1 {I3} (1971Vi15), and 1342.15 {I10} (1974HeYW)
194PT cG RI$weighted average of 2.128 {I21} (2015Do06), 2.55 {I25} (1964Be23),
194PT2cG 1.96 {I17} (1970Be30), 2.51 {I10} (1971Vi15), 2.03 {I15} (1974HeYW),
194PT3cG and 2.17 {I4} (1996TeZW)
194PT cG M,MR$from |a(K)exp=0.00590 {I16} deduced from Ice(K)=0.260 {I5} and
194PT2cG I|g=2.15 {I4} here, L1/L2=6.6 {I12}, L1/L3=54 {I24} (1970Ag05),
194PT3cG and |g|g(|q) of 1996TeZW with |d=-0.26 {I6}. Other |a(K)exp:
194PT4cG 0.0049 {I6} (1964Be23), 0.0064 {I6} (1970Be30), 0.0051 {I3} (1971Vi15)
194PT cG $(1342|g)(328|g)(|q): A{-2}=+0.41 {I3}, A{-4}=+0.04 {I5}.
194PT cG $Ice(K)=0.260 {I5}, weighted average of 0.258 {I5} (1964Be23), 0.260
194PT2cG {I5} (1971Vi15), and 0.32 {I3} (1960Ba17).
194PT G 1670.665 14 0.301 3 (E2) 0.00219 C
194PTS G KC=0.001714 24$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
194PT2 G %IG=0.189 6
194PT cG E$weighted average of 1670.671 {I14} (2015Do06) and 1670.64 {I3}
194PT2cG (1996TeZW). Others: 1670.9 {I6} (1960Ba17), 1670.8 {I3} (1970Be30),
194PT3cG 1670.5 {I3} (1971Vi15), and 1670.66 {I15} (1974HeYW)
194PT cG RI$weighted average of 0.301 {I3} (2015Do06) and 0.293 {I12}
194PT2cG (1996TeZW). Others: 0.23 {I7} (1970Be30), 0.283 {I25} (1971Vi15), and
194PT3cG 0.36 {I5} (1974HeYW)
194PT cG M$|a(K)exp=0.0031 {I10} (1970Be30) and 0.0030 {I7} (1971Vi15) gives
194PT2cG M1(+E2) with |d<0.9, but |DJ=2 from decay scheme requires E2.
194PT cG $Ice(K)=0.0166 {I18}, weighted average of 0.0143 {I20} (1964Be23),
194PT2cG 0.018 {I3} (1971Vi15), and 0.0180 {I18} (1960Ba17).
194PT dG $|a(K)exp=0.0027 {I3}, from Ice(K)=0.0166 {I18} and I|g=0.301 {I3} here
194PT L 1737.423 14 (3-)
194PT G 304.886 17 0.0290 6 C
194PT2 G %IG=0.0182 6
194PT cG E$weighted average of 304.87 {I8} (1996TeZW) and 304.887 {I17}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.030 {I3} (1996TeZW) and 0.0290 {I6} (2015Do06)
194PT G 363.10 18 0.0098 22 KC
194PTF G FLAG=Y
194PT2 G %IG=0.0062 14
194PT cG E$poor fit, level-energy difference=363.66
194PT G 814.59 6 0.0101 6 C
194PT2 G %IG=0.0063 4
194PT cG E$weighted average of 814.9 {I3} (1996TeZW) and 814.58 {I6} (2015Do06)
194PT cG RI$weighted average of 0.0121 {I22} (1996TeZW) and 0.0100 {I6}
194PT2cG (2015Do06)
194PT L 1778.579 9 2+
194PT cL J$spin=1 or 2 from |g|g(|q) of 1996TeZW; spin=1 is ruled out by
194PT2cL Mult=D+Q from ce data for 855.8|g to 3+; 1156.6|g M1(+E2) to 2+
194PT E 0.89 3 8.302 15 0.89 3
194PTS E CK=0.79221 9$CL=0.15685 7$CM+=0.05093 3
194PT G 345.984 20 0.0077 4 N ?
194PT2 G %IG=0.0048 3
194PT cG E$level-energy difference=346.034
194PT G 855.823 17 0.105 1 (M1+E2) 0.53 +22-240.0168 17 C
194PTS G KC=0.0139 15$LC=0.00224 20$MC=0.00052 5
194PTS G NC=0.000128 12$OC=2.30E-5 21$PC=1.54E-6 17
194PT2 G %IG=0.0660 19
194PT cG E$weighted average of 855.806 {I17} (2015Do06), 856.08 {I20}
194PT2cG (1960Ba17), 855.5 {I13} (1970Be30), 855.8 {I2} (1971Vi15), and 855.87
194PT3cG {I3} (1996TeZW)
194PT cG RI$weighted average of 0.17 {I6} (1970Be30), 0.106 {I7} (1996TeZW), and
194PT2cG 0.105 {I1} (2015Do06)
194PT cG M,MR$|a(K)exp=0.0139 {I14} deduced from Ice(K)=0.030 {I3} and I|g=0.105
194PT2cG {I1} here gives |d(E2/M1)=0.53 {I+22-24} or |d(M2/E1)=0.66 {I6};
194PT3cG |DJ|p requires M1+E2. Other |a(K)exp: 0.009 {I3} (1970Be30), >0.0065
194PT4cG (1971Vi15)
194PT cG $Ice(K)=0.030 {I3}, weighted average of 0.031 {I3} (1964Be23), 0.024
194PT2cG {I4} (1971Vi15), and 0.034 {I4} (1960Ba17).
194PT G 1156.550 14 0.745 7 M1(+E2) 0.2 LT 0.0089816 C
194PTS G KC=0.00746 14$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
194PT2 G %IG=0.468 14
194PT cG E$weighted average of 1156.560 {I14} (2015Do06), 1156.61 {I6}
194PT2cG (1974HeYW), and 1156.525 {I19} (1996TeZW). Others: 1156.59 {I20}
194PT3cG (1960Ba17), 1156.60 {I20} (1970Be30), and 1156.5 {I2} (1971Vi15)
194PT cG RI$weighted average of 0.744 {I7} (2015Do06), 0.87 {I25} (1964Be23),
194PT2cG 0.71 {I7} (1970Be30), 0.79 {I4} (1971Vi15), 0.76 {I6} (1974HeYW), and
194PT3cG 0.738 {I20} (1996TeZW)
194PT cG M,MR$|a(K)exp=0.0085 {I3} deduced from Ice(K)=0.130 {I4} and I|g=0.745
194PT2cG {I7} here, and L1/L2=11.6 {I17}, L1/L3>73 (1970Ag05), gives
194PT3cG |d(E2/M1)<0.2 or |d(M2/E1)=0.87 {I5}, with the former consistent with
194PT4cG |d=+0.5 {I6} or +0.20 {I24} for J(1778)=2 from |g|g(|q) of 1996TeZW.
194PT5cG Others: |d<-0.1 {I4} or >+5 from |g|g(|q) for J(1778)=1, but this spin
194PT6cG ruled out by Mult=D+Q from ce data for 855.8|g to 3+.
194PT7cG Other |a(K)exp: 0.0072 {I+40-22} (1964Be23), 0.0088 {I9} (1970Be30),
194PT8cG 0.0081 {I+13-11} (1971Vi15)
194PT cG $(1156|g)(293|g)(|q): A{-2}=+0.01 {I3}, A{-4}=+0.01 {I6}.
194PT cG $(1156|g)[293|g](328|g)(|q): A{-2}=-0.03 {I4}, A{-4}=-0.16 {I7}.
194PT cG $Ice(K)=0.130 {I4}, weighted average of 0.128 {I4} (1964Be23), 0.13
194PT2cG {I1} (1971Vi15), and 0.150 {I15} (1960Ba17).
194PT G 1450.098 14 0.511 5 M1+E2 -0.27 10 0.0050615 C
194PTS G KC=0.00414 13$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
194PT2 G %IG=0.321 9
194PT cG E$weighted average of 1450.104 {I14} (2015Do06) and 1450.084 {I21}
194PT2cG (1996TeZW). Others: 1450.48 {I20} (1960Ba17), 1450.3 {I3} (1970Be30),
194PT3cG and 1450.06 {I15} (1974HeYW)
194PT cG RI$weighted average of 0.509 {I5} (2015Do06), 0.51 {I4} (1970Be30),
194PT2cG 0.53 {I3} (1971Vi15), 0.55 {I5} (1974HeYW), and 0.520 {I12} (1996TeZW)
194PT cG M,MR$|a(K)exp=0.0042 {I5} deduced from Ice(K)=0.044 {I5} and I|g=0.511
194PT2cG {I5} here gives |d(E2/M1)<0.6 or |d(M2/E1)=0.75 {I9}, with only the
194PT3cG former consistent with |d=-0.27 {I10} from |g|g(|q) of 1996TeZW for
194PT4cG J(1778)=2. Other |d: -0.55 {I5} from |g|g(|q) for J(1778)=1, but this
194PT5cG spin ruled out by ce data for 855.8|g. Other |a(K)exp: 0.0039 {I4}
194PT6cG (1970Be30)
194PT cG $(1450|g)(328|g)(|q): A{-2}=+0.41 {I4}, A{-4}=+0.09 {I7}.
194PT cG $Ice(K)=0.044 {I5}, weighted average of 0.041 {I3} (1964Be23) and 0.051
194PT2cG {I5} (1960Ba17).
194PT G 1778.532 20 0.061 2 (E2) 0.00201
194PTS G KC=0.001530 22$LC=0.000240 4$MC=5.50E-5 8
194PTS G NC=1.358E-5 19$OC=2.43E-6 4$PC=1.596E-7 23$IPC=0.0001712 24
194PT2 G %IG=0.0383 16
194PT cG E$from 2015Do06. Others: 1778.6 {I4} (1971Vi15) and 1778.52 {I16}
194PT2cG (1996TeZW)
194PT cG RI$from 2015Do06. Others: 0.082 {I19} (1971Vi15) and 0.066 {I10}
194PT2cG (1996TeZW)
194PT cG M$|a(K)exp=0.0022 {I10} deduced from Ice(K)=0.0028 {I11} (1971Vi15) and
194PT2cG I|g=0.061 {I2} here, gives M1,E2, and |DJ|p requires E2
194PT L 1797.384 5 1-
194PT E 11.7 4 7.160 16 11.7 4
194PTS E CK=0.7914 1$CL=0.15744 7$CM+=0.05116 3
194PT G 250.102 17 0.0594 7 E1 0.0404 C
194PTS G KC=0.0333 5$LC=0.00546 8$MC=0.001258 18
194PTS G NC=0.000308 5$OC=5.36E-5 8$PC=2.98E-6 5
194PT2 G %IG=0.0373 11
194PT cG E$weighted average of 250.098 {I17} (2015Do06), 250.2 {I3} (1971Vi15),
194PT2cG and 250.12 {I4} (1996TeZW). Other: 250.1 {I13} (1970Be30), unplaced
194PT cG RI$weighted average of 0.053 {I5} (1996TeZW), 0.0596 {I6}
194PT2cG (2015Do06), 0.050 {I6} (1977Vy01), 0.05 {I3} (1970Be30)
194PT cG M$from |a(K)exp=0.025 {I10}, deduced from Ice(K)=0.030 {I12} (1971Vi15)
194PT2cG I|g=0.0594 {I7} here
194PT G 318.122 10 0.345 3 E1 0.0227 C
194PTS G KC=0.0188 3$LC=0.00301 5$MC=0.000693 10
194PTS G NC=0.0001701 24$OC=2.98E-5 5$PC=1.729E-6 25
194PT2 G %IG=0.217 6
194PT cG E$weighted average of 318.122 {I10} (2015Do06) and 318.124 {I18}
194PT2cG (1996TeZW). Others: 318.11 {I20} (1970Be30), 318.2 {I3} (1971Vi15), and
194PT3cG 318.14 {I8} (1974HeYW)
194PT cG RI$weighted average of 0.348 {I10} (1996TeZW) and 0.345 {I3}
194PT2cG (2015Do06). Others: 0.52 {I8} (1970Be30) and 0.30 {I3} (1974HeYW)
194PT cG M$from |a(K)exp=0.035 {I13}, deduced from Ice(K)=0.25 {I9} (1971Vi15)
194PT2cG and I|g=0.345 {I3} here
194PT G 364.836 6 2.548 25E2 0.0562 C
194PTS G KC=0.0378 6$LC=0.01390 20$MC=0.00344 5
194PTS G NC=0.000844 12$OC=0.0001394 20$PC=3.90E-6 6
194PT2 G %IG=1.60 5
194PT cG E$weighted average of 364.846 {I10} (2015Do06) and 364.832 {I6}
194PT2cG (1996TeZW). Others: 364.97 {I6} (1960Ba17), 364.77 {I15} (1970Be30),
194PT3cG 364.8 {I3} (1971Vi15), and 364.87 {I4} (1974HeYW)
194PT cG RI$weighted average of 2.55 {I19} (1964Be23), 2.42 {I14} (1970Be30),
194PT2cG 3.02 {I19} (1971Vi15), 2.52 {I15} (1974HeYW), 2.56 {I4} (1996TeZW), and
194PT3cG 2.540 {I25} (2015Do06)
194PT cG M$|a(K)exp=0.046 {I4} (1964Be23), 0.048 {I3} (1970Be30), 0.038 {I3}
194PT2cG (1971Vi15), L1:L2:L3=1.88 {I27}:1.94 {I27}:1.00 (1970Ag05).
194PT cG $Ice(K)=2.38 {I6}, from 1964Be23. Others: 2.38 {I10} (1971Vi15) and
194PT2cG 2.50 {I25} (1960Ba17).
194PT dG $|a(K)exp=0.0456 {I12}, from Ice(K)=2.38 {I6} and I|g=2.548 {I25} here
194PT G 530.173 10 0.977 9 E1 0.00730 C
194PTS G KC=0.00609 9$LC=0.000935 13$MC=0.000214 3
194PTS G NC=5.26E-5 8$OC=9.33E-6 13$PC=5.83E-7 9
194PT2 G %IG=0.614 18
194PT cG E$weighted average of 530.164 {I10} (1996TeZW) and 530.182 {I10}
194PT2cG (2015Do06). Other: 529.9 {I3} (1971Vi15); 529.06 {I10} (1974HeYW)
194PT3cG is discrepant
194PT cG RI$weighted average of 0.987 {I18} (1996TeZW) and 0.975 {I9}
194PT2cG (2015Do06). Other: 3.6 {I4} 1974HeYW) and 3.9 {I3} (1971Vi15) for a
194PT3cG doublet
194PT cG M$|a(K)exp=0.006 {I1}, deduced from Ice(K)=0.125 {I14} (1971Vi15) and
194PT2cG I|g=0.977 {I9} here.
194PT G 1175.360 10 3.41 3 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$IPC=1.024E-5 15
194PT2 G %IG=2.14 6
194PT cG E$weighted average of 1175.366 {I10} (2015Do06), 1175.34 {I5}
194PT2cG (1974HeYW), and 1175.353 {I11} (1996TeZW). Others: 1175.46 {I20}
194PT3cG (1960Ba17), 1175.37 {I15} (1970Be30), and 1175.3 {I2} (1971Vi15)
194PT cG RI$weighted average of 3.39 {I3} (2015Do06), 3.48 {I22} (1964Be23),
194PT2cG 3.29 {I18} (1970Be30), 3.4 {I9} (1971Vi15), 3.36 {I20} (1974HeYW), and
194PT3cG 3.51 {I7} (1996TeZW)
194PT cG M$|a(K)exp=0.00138 {I12} (1964Be23), 0.00146 {I10} (1970Be30),
194PT2cG 0.0014 {I4} (1971Vi15), L1/L2>14, L1/L3>21 (1970Ag05).
194PT3cG |d=+0.02 {I5}, -0.07 {I19}, or -0.07 {I8} from |g|g(|q) of 1996TeZW
194PT4cG consistent with mult=pure dipole.
194PT cG $(1175|g)(622|g)(|q): A{-2}=-0.27 {I5}, A{-4}=-0.11 {I9}.
194PT cG $(1175|g)(293|g)(|q): A{-2}=+0.014 {I18}, A{-4}=-0.01 {I3}.
194PT cG $(1175|g)[293|g](328|g)(|q): A{-2}=+0.036 {I19}, A{-4}=-0.01 {I3}.
194PT cG $Ice(K)=0.097 {I3}, weighted average of 0.098 {I3} (1964Be23), 0.095
194PT2cG {I3} (1971Vi15), and 0.120 {I12} (1960Ba17).
194PT dG $|a(K)exp=0.00139 {I5}, from Ice(K)=0.097 {I3} and I|g=3.41 {I3} here
194PT G 1468.904 10 10.82 11E1 1.23E-3 C
194PTS G KC=0.000908 13$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
194PT2 G %IG=6.80 20
194PT cG E$weighted average of 1468.914 {I10} (2015Do06), 1469.36 {I25}
194PT2cG (1960Ba17), 1468.92 {I15} (1970Be30), 1468.9 {I3} (1971Vi15), 1468.89
194PT3cG {I5} (1974HeYW), and 1468.882 {I15} (1996TeZW)
194PT cG RI$weighted average of 10.76 {I11} (2015Do06), 11.9 {I6} (1964Be23),
194PT2cG 10.6 {I6} (1970Be30), 11 {I3} (1971Vi15), 10.5 {I6} (1974HeYW), and
194PT3cG 10.94 {I18} (1996TeZW)
194PT cG M$|a(K)exp=0.00101 {I8} (1964Be23), 0.00114 {I8} (1970Be30),
194PT2cG 0.0012 {I4} (1971Vi15), L1/L2=26 {I7}, L1/L3=21 {I6} (1970Ag05).
194PT3cG |d(M2/E2)=-0.006 {I9} from |g|g(|q) of 1996TeZW consistent with
194PT4cG mult=pure dipole.
194PT cG $(1469|g)(328|g)(|q): A{-2}=-0.247 {I10}, A{-4}=-0.054 {I17}.
194PT cG $Ice(K)=0.248 {I5}, weighted average of 0.246 {I5} (1964Be23), 0.265
194PT2cG {I15} (1971Vi15), and 0.26 {I3} (1960Ba17).
194PT dG $|a(K)exp=0.00112 {I3}, from Ice(K)=0.248 {I5} and I|g=10.82 {I11} here
194PT G 1797.404 14 0.940 9 E1 1.16E-3 C
194PTS G KC=0.000649 9$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
194PT2 G %IG=0.591 17
194PT cG E$weighted average of 1797.418 {I14} (2015Do06), 1798.0 {I4}
194PT2cG (1960Ba17), 1797.44 {I20} (1970Be30), 1797.3 {I4} (1971Vi15), 1797.31
194PT3cG {I8} (1974HeYW), and 1797.378 {I21} (1996TeZW)
194PT cG RI$weighted average of 0.935 {I9} (2015Do06), 0.95 {I8} (1970Be30),
194PT2cG 0.94 {I7} (1971Vi15), 1.06 {I10} (1974HeYW), and 0.98 {I3} (1996TeZW)
194PT cG M$|a(K)exp>0.0028 (1964Be23), 0.00107 {I11} (1970Be30),
194PT2cG 0.00078 {I12} (1971Vi15).
194PT cG $Ice(K)=0.021 {I3}, unweighted average of 0.021 {I1} (1964Be23), 0.015
194PT2cG {I2} (1971Vi15), and 0.026 {I3} (1960Ba17).
194PT dG $|a(K)exp=0.00109 {I16}, from Ice(K)=0.021 {I3} and I|g=0.940 {I9} here
194PT L 1802.646 14 1+,2+ ?
194PT cL E$2015Do06 cast doubt about the existence of this level for
194PT2cL two reasons: 1. no other transition from this level reported.
194PT3cL 2. coincidence with 328|g in 1996TeZW work suggests placement of
194PT4cL all or part of the 1802.6|g from a new 2131 level, as proposed by
194PT5cL 2015Do06. Also this level is not reported in any other study of decays
194PT6cL and reactions.
194PT E 0.125 5 9.125 18 0.125 5
194PTS E CK=0.7912 1$CL=0.15761 7$CM+=0.05123 3
194PT G 1802.637 14 0.198 3 M1,E2 0.0026 7 &
194PTS G KC=0.0020 5$LC=0.00031 8$MC=7.1E-5 18
194PTS G NC=1.8E-5 5$OC=3.2E-6 8$PC=2.1E-7 6$IPC=0.00023 5
194PT2 G %IG=0.124 4
194PT cG E$from 2015Do06 for a doublet. Others: 1802.62 {I4} (1996TeZW), 1803.0
194PT2cG {I6} (1970Be30), 1803.1 {I4} (1971Vi15), and 1803.1 {I8} (1960Ba17)
194PT3cG could be also for a doublet
194PT cG RI$from 2015Do06 for a doublet. Others: 0.21 {I1} (1996TeZW), 0.25 {I8}
194PT2cG (1971Vi15), and 0.30 {I9} (1970Be30) could be also for a doublet;
194PT3cG 0.87 {I25} (1964Be23) is discrepant
194PT cG M$|a(K)exp=0.0018 {I9} (1970Be30), 0.0022 {I+15-8} (1971Vi15),
194PT2cG |?0.00062 (1964Be23) for a composite peak
194PT cG $Ice(K)=0.0122 {I12}, weighted average of 0.0115 {I12} (1971Vi15) and
194PT2cG 0.0130 {I13} (1960Ba17) for a composite peak. Other: |?0.011 (1964Be23)
194PT L 1816.585 7 (2)+
194PT E 0.069 9 9.36 6 0.069 9
194PTS E CK=0.7905 1$CL=0.15808 8$CM+=0.05141 3
194PT G 894.07 18 0.050 10(M1+E2) 1.1 +8-4 0.0116 25 C
194PTS G KC=0.0095 21$LC=0.0016 3$MC=0.00037 7
194PTS G NC=9.1E-5 17$OC=1.6E-5 3$PC=1.04E-6 24
194PT2 G %IG=0.031 6
194PT cG E$unweighted average of 894.02 {I6} (1996TeZW), 893.794 {I17}
194PT2cG (2015Do06), and 894.4 {I4} (1960Ba17)
194PT cG RI$unweighted average of 0.060 {I5} (1996TeZW) and 0.0401 {I6}
194PT2cG (2015Do06)
194PT cG M,MR$|a(K)exp=0.0095 {I21} deduced from Ice(K)=0.0097 {I10} and
194PT2cG I|g=0.050 {I10} here gives |d(E2/M1)=1.1 {I+8-4} or |d(M2/E1)=0.53
194PT3cG {I10}, with the former consistent with |D|p=+ based on L(p,d)=1+3 from
194PT4cG 1/2-
194PT cG $Ice(K)=0.0097 {I10}, weighted average of 0.0086 {I20} (1964Be23) and
194PT2cG 0.0100 {I10} (1960Ba17).
194PT G 1005.292 13 0.0272 4 N ?
194PT2 G %IG=0.0171 5
194PT G 1194.529 14 0.059 9 (E2) 0.00388 C
194PTF G FL=622.023
194PTS G KC=0.00317 5$LC=0.000540 8$MC=0.0001254 18
194PTS G NC=3.09E-5 5$OC=5.48E-6 8$PC=3.33E-7 5$IPC=3.73E-6 6
194PT2 G %IG=0.037 6
194PT cG E$weighted average of 1194.526 {I14} (2015Do06) and 1194.60 {I7}
194PT2cG (1996TeZW). Others: 1195.1 {I4} (1960Ba17), 1194.9 {I13} (1970Be30),
194PT cG RI$unweighted average of 0.050 {I3} (1996TeZW) and 0.0672 {I6}
194PT2cG (2015Do06). Others: 0.31 {I19} (1964Be23) and 0.13 {I5} (1970Be30)
194PT3cG could be for a composite peak
194PT cG M$|a(K)exp=0.0008 {I+16-4} (1964Be23) and 0.0020 {I8} (1970Be30) could
194PT2cG be for a composite peak.
194PT cG $Ice(K)=0.0058 {I6}, weighted average of 0.0054 {I5} (1964Be23) and
194PT2cG 0.0066 {I7} (1960Ba17).
194PT G 1489.01 9 0.0188 11 YC
194PTF G FL=328.474
194PT2 G %IG=0.0118 8
194PT cG E$weighted average of 1488.3 {I4} (1996TeZW) and 1489.02 {I5}
194PT2cG (2015Do06). Others: 1487.0 {I3} (1974HeYW) and 1487.9 {I5} (1960Ba17)
194PT3cG for a doublet; 1486.8 {I6} (1970Be30) is discrepant.
194PT cG $Poor fit, level-energy difference=1488.11
194PT cG RI$weighted average of 0.028 {I7} (1996TeZW) and 0.0187 {I8}
194PT2cG (2015Do06). Others: 0.22 {I5} (1970Be30) and 0.20 {I4} (1974HeYW) for a
194PT3cG doublet
194PT cG $|a(K)exp=0.0040 {I11} (1970Be30), >0.0015 (1964Be23) for a doublet.
194PT cG $Ice(K)=0.0206 {I22}, weighted average of 0.018 {I3} (1964Be23) and
194PT2cG 0.0220 {I22} (1960Ba17) for a doublet.
194PT G 1816.33 17 0.002 LT ?
194PT2 G %IG=6E-4 6
194PT cG E$from 1996TeZW. Other: 1817.0 {I5} (1977Vy01)
194PT cG RI$from 2015Do06. Others: 0.014 {I5} (1996TeZW), 0.06 {I2} (1977Vy01)
194PT L 1893.574 19 0+
194PT E 0.039 8 9.51 9 0.039 8
194PTS E CK=0.7864 2$CL=0.1611 1$CM+=0.05256 4
194PT G 1565.20 8 0.075 12 C
194PT2 G %IG=0.047 8
194PT cG E$unweighted average of 1565.28 {I6} (1996TeZW) and 1565.126 {I17}
194PT2cG (2015Do06)
194PT cG RI$unweighted average of 0.086 {I4} (1996TeZW) and 0.0632 {I8}
194PT2cG (2015Do06)
194PT G 1893.1 4 (E0) 0.0010 1 ?
194PT cG E,M$transition seen in ce data only (1960Ba17, 1964Be23).
194PT cG TI$deduced from Ice(K)=0.0175 {I18} and ce(K)/ce=0.8626 for E0 (BrIcc)
194PT cG $Ice(K)=0.0175 {I18}, weighted average of 0.015 {I4} (1964Be23) and
194PT2cG 0.0180 {I18} (1960Ba17)
194PT L 1924.282 8 1+
194PT E 4.16 14 7.431 15 4.16 14
194PTS E CK=0.7844 2$CL=0.1625 1$CM+=0.05311 4
194PT G 126.82 4 0.0092 8 N ?
194PT2 G %IG=0.0058 5
194PT G 253.61 7 0.0052 6 M1(+E2) 1.4 LT 0.38 11 C
194PTS G KC=0.30 11$LC=0.062 4$MC=0.0146 6
194PTS G NC=0.00360 14$OC=0.00063 5$PC=3.3E-5 12
194PT2 G %IG=0.0033 4
194PT cG E$from 2015Do06. Others: 253.6 {I3} (1971Vi15), 253.6 {I4} (1996TeZW)
194PT cG RI$from 2015Do06. Other: 0.005 {I4} (1996TeZW)
194PT cG M$from |a(K)exp=0.40 {I+20-15} deduced from Ice(K)=0.043 {I13}
194PT2cG (1971Vi15) and I|g=0.0052 {I6} here
194PT G 412.288 17 0.0292 4 (M1+E2) 0.9 +8-5 0.09 3 C
194PTS G KC=0.072 25$LC=0.014 3$MC=0.0032 6
194PTS G NC=0.00079 14$OC=0.00014 3$PC=8.E-6 3
194PT2 G %IG=0.0184 6
194PT cG E$weighted average of 412.290 {I17} (2015Do06) and 412.20 {I11}
194PT2cG (1996TeZW). Other: 412.3 {I3} (1971Vi15)
194PT cG RI$from 2015Do06. Other: 0.025 {I7} (1996TeZW)
194PT cG M$|a(K)exp=0.072 {I+24-21} deduced from Ice(K)=0.044 {I13}
194PT2cG (1971Vi15) and I|g=0.0292 {I4} here, gives |d(E2/M1)=0.9 {I+8-5} or
194PT3cG |d(M2/E1)=0.49 {I12}, and |DJ|p requires M1+E2
194PT G 1001.481 28 0.0193 7 N ?
194PT2 G %IG=0.0121 6
194PT G 1302.255 14 0.435 4 (M1+E2) 0.56 +22-230.0059 5 C
194PTS G KC=0.0049 5$LC=0.00077 6$MC=0.000178 14
194PTS G NC=4.4E-5 4$OC=7.9E-6 7$PC=5.4E-7 5$IPC=2.41E-5 14
194PT2 G %IG=0.273 8
194PT cG E$from 2015Do06. Others: 1302.4 {I6} (1970Be30), 1302.29 {I8}
194PT2cG (1974HeYW), 1302.24 {I3} (1996TeZW), and 1302.55 {I15} (1960Ba17)
194PT cG RI$weighted average of 0.422 {I13} (1996TeZW) and 0.436 {I4}
194PT2cG (2015Do06). Others: 0.50 {I25} (1964Be23), 0.45 {I9} (1970Be30), and
194PT3cG 0.43 {I4} (1974HeYW)
194PT cG M,MR$|a(K)exp=0.0049 {I4} deduced from Ice(K)=0.044 {I3} and
194PT2cG I|g=0.435 {I4} here, gives |d(E2/M1)=0.56 {I+22-23} or
194PT3cG |d(M2/E1)=0.68 {I5}, and |DJ|p requires M1+E2. Other |d: -1.7 {I17},
194PT4cG 0 to -4 {I+4-}|@, -0.9 {I+4-}|@ (1996TeZW). Other |a(K)exp: 0.0042
194PT5cG {I+53-17} (1964Be23), 0.0047 {I10} (1970Be30).
194PT cG $(1302|g)(293|g)(|q): A{-2}=-0.18 {I5}, A{-4}=-0.19 {I9}.
194PT cG $(1302|g)[293|g](328|g)(|q): A{-2}=-0.07 {I5}, A{-4}=-0.14 {I9}.
194PT cG $Ice(K)=0.044 {I3}, weighted average of 0.043 {I2} (1964Be23) and 0.051
194PT2cG {I5} (1960Ba17).
194PT G 1595.807 14 3.00 3 M1+E2 -0.071 21 0.00420 C
194PTS G KC=0.00337 5$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
194PT2 G %IG=1.89 6
194PT cG E$weighted average of 1595.797 {I19} (1996TeZW) and 1595.812 {I14}
194PT2cG (2015Do06). Others: 1595.8 {I3} (1970Be30), 1595.8 {I3} (1971Vi15),
194PT3cG 1595.8 {I1} (1974HeYW), and 1596.2 {I4} (1960Ba17)
194PT cG RI$weighted average of 3.00 {I7} (1996TeZW) and 3.00 {I3} (2015Do06).
194PT2cG Others: 2.9 {I8} (1970Be30) and 2.8 {I3} (1974HeYW); 4.7 {I6}
194PT3cG (1964Be23) and 6.0 {I6} (1971Vi15) for a doublet
194PT cG M$|a(K)exp=0.0025 {I+9-6} (1964Be23), 0.0041 {I12} (1970Be30), and
194PT2cG 0.0040 {I3} deduced from Ice(K)=0.243 {I15} (1971Vi15) and I|g=3.00
194PT3cG {I3} here.
194PT cG MR$from |g|g(|q) of 1996TeZW, consistent with |d<0.3 from ce data
194PT2cG above.
194PT cG $(1596|g)(328|g)(|q): A{-2}=-0.167 {I25}, A{-4}=+0.03 {I4}.
194PT cG $Ice(K)=0.250 {I15}, weighted average of 0.245 {I20} (1964Be23), 0.243
194PT2cG {I15} (1971Vi15), and 0.29 {I3} (1960Ba17).
194PT dG $|a(K)exp=0.00407 {I25}, from Ice(K)=0.250 {I15} and I|g=3.00 {I3} here
194PT G 1924.273 20 3.27 5 M1 0.00290 C
194PTS G KC=0.00212 3$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
194PT2 G %IG=2.05 7
194PT cG E$weighted average of 1924.13 {I15} (1970Be30), 1924.2 {I4} (1971Vi15),
194PT2cG 1924.18 {I5} (1974HeYW), 1924.225 {I22} (1996TeZW), 1924.300 {I14}
194PT3cG (2015Do06), and 1924.60 {I20} (1960Ba17)
194PT cG RI$weighted average of 3.26 {I13} (1964Be23), 3.30 {I17} (1970Be30),
194PT2cG 3.5 {I7} (1971Vi15), 3.22 {I20} (1974HeYW), 3.63 {I13} (1996TeZW), and
194PT3cG 3.24 {I4} (2015Do06)
194PT cG M$|a(K)exp=0.00225 {I11} (1964Be23), 0.00219 {I13} (1970Be30), and
194PT2cG 0.0021 {I+6-4} (1971Vi15) gives |d<0.3
194PT cG $Ice(K)=0.150 {I3}, weighted average of 0.148 {I3} (1964Be23), 0.151
194PT2cG {I3} (1971Vi15), and 0.180 {I18} (1960Ba17).
194PT dG $|a(K)exp=0.00224 {I6}, from Ice(K)=0.150 {I3} and I|g=3.27 {I5} here
194PT L 1930.369 8 2+
194PT E 0.470 16 8.369 16 0.470 16
194PTS E CK=0.7840 2$CL=0.1628 1$CM+=0.05323 4
194PT G 308.17 4 0.0061 5 N ?
194PT2 G %IG=0.0038 3
194PT G 1007.582 14 0.0994 13(M1+E2) 1.1 +5-3 0.0088 13 C
194PTS G KC=0.0072 11$LC=0.00119 16$MC=0.00027 4
194PTS G NC=6.8E-5 9$OC=1.21E-5 16$PC=7.9E-7 13
194PT2 G %IG=0.0625 19
194PT cG E$weighted average of 1007.0 {I6} (1970Be30), 1007.5 {I2} (1971Vi15),
194PT2cG 1007.53 {I4} (1996TeZW), 1007.589 {I14} (2015Do06), and 1007.5 {I3}
194PT3cG (1960Ba17)
194PT cG RI$weighted average of 0.14 {I4} (1970Be30), 0.20 {I6} (1971Vi15),
194PT2cG 0.108 {I7} (1996TeZW), and 0.0992 {I10} (2015Do06)
194PT cG M,MR$|a(K)exp=0.0071 {I10}, deduced from Ice(K)=0.0144 {I20}
194PT2cG and I|g=0.0994 {I13} here, gives |d(E2/M1)=1.1 {I+5-3} or
194PT3cG |d(M2/E1)=0.53 {I+6-7}, with the former consistent with |D|p=+
194PT4cG based on L(p,d)=1+3 from 1/2-. Other |a(K)exp: 0.0040 {I14} (1970Be30)
194PT cG $Ice(K)=0.0144 {I20}, weighted average of 0.012 {I2} (1964Be23) and
194PT2cG 0.0160 {I16} (1960Ba17).
194PT G 1119.118 16 0.106 2 [E2] 0.00439 C
194PTS G KC=0.00358 5$LC=0.000622 9$MC=0.0001447 21
194PTS G NC=3.57E-5 5$OC=6.31E-6 9$PC=3.77E-7 6$IPC=3.78E-7 6
194PT2 G %IG=0.0666 22
194PT cG E$weighted average of 1119.8 {I6} (1970Be30), 1119.3 {I3} (1996TeZW),
194PT2cG 1119.117 {I14} (2015Do06), and 1119.7 {I4} (1960Ba17)
194PT cG RI$weighted average of 0.22 {I7} (1970Be30), 0.21 {I5} (1971Vi15), 0.10
194PT2cG {I4} (1996TeZW), and 0.106 {I1} (2015Do06)
194PT cG M$|a(K)exp=0.0046 {I5} deduced from Ice(K)=0.0100 {I10} and
194PT2cG I|g=0.106 {I2} here, gives |d(E2/M1)=1.9 {I+9-5} or |d(M2/E1)=0.46
194PT3cG {I+4-5}, but |DJ|p requires E2
194PT cG $Ice(K)=0.0100 {I10}, weighted average of 0.0092 {I10} (1964Be23) and
194PT2cG 0.0110 {I11} (1960Ba17).
194PT G 1308.331 14 0.239 2 (M1+E2) 1.7 +11-5 0.0042 6 C
194PTS G KC=0.0034 5$LC=0.00055 7$MC=0.000128 15
194PTS G NC=3.1E-5 4$OC=5.6E-6 7$PC=3.7E-7 5$IPC=2.05E-5 16
194PT2 G %IG=0.150 4
194PT cG E$from 2015Do06. Others: 1308.2 {I6} (1970Be30), 1308.55 {I20}
194PT2cG (1974HeYW), 1308.32 {I3} (1996TeZW), and 1308.59 {I20} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.24 {I5} (1970Be30), 0.25 {I5} (1971Vi15),
194PT2cG 0.24 {I3} (1974HeYW), 0.224 {I8} (1996TeZW)
194PT cG M,MR$|a(K)exp=0.0034 {I4}, from Ice(K)=0.0167 {I19} and I|g=0.239 {I2}
194PT2cG here, gives |d(E2/M1)=1.7 {I+11-5}, or |d(M2/E1)=0.49 {I5}, with
194PT3cG the former consistent with |D|p=+ based on L(p,d)=1+3 from 1/2-. Other
194PT4cG |a(K)exp: 0.0036 {I5} (1970Be30)
194PT cG $Ice(K)=0.0167 {I19}, weighted average of 0.0152 {I15} (1964Be23) and
194PT2cG 0.0190 {I19} (1960Ba17).
194PT G 1601.891 14 0.384 4 M1(+E2) -0.2 LT 0.004147 C
194PTS G KC=0.00332 6$LC=0.000515 9$MC=0.0001181 20
194PTS G NC=2.92E-5 5$OC=5.27E-6 9$PC=3.65E-7 7$IPC=0.0001533 24
194PT2 G %IG=0.241 7
194PT cG E$weighted average of 1601.9 {I3} (1970Be30), 1601.7 {I3} (1971Vi15),
194PT2cG 1602.01 {I10} (1974HeYW), 1601.848 {I24} (1996TeZW), 1601.904 {I14}
194PT3cG (2015Do06), and 1602.0 {I5} (1960Ba17)
194PT cG RI$weighted average of 0.377 {I10} (1996TeZW) and 0.385 {I4}
194PT2cG (2015Do06). Others: 0.40 {I5} (1970Be30), 0.39 {I7} (1971Vi15), and
194PT3cG 0.45 {I5} (1974HeYW)
194PT cG M,MR$|a(K)exp=0.0041 {I3} deduced from Ice(K)=0.032 {I2} and I|g=0.384
194PT2cG {I4} here, gives |d(E2/M1)<0.2, |g|g(|q) of 1996TeZW gives |d=-0.5
194PT3cG {I4} or -0.55 {I4}, with the former consistent with |d from ce data.
194PT4cG Other |a(K)exp: 0.0036 {I5} (1970Be30)
194PT cG $(1602|g)(328|g)(|q): A{-2}=+0.52 {I6}, A{-4}=+0.04 {I9}
194PT cG $Ice(K)=0.032 {I2}, weighted average of 0.030 {I2} (1964Be23), 0.032
194PT2cG {I2} (1971Vi15), and 0.036 {I4} (1960Ba17).
194PT G 1930.35 9 0.0027 7 n
194PT2 G %IG=0.0017 5
194PT L 1961.328 6 2-
194PT E 3.40 11 7.459 15 3.40 11
194PTS E CK=0.7817 2$CL=0.1644 2$CM+=0.05386 5
194PT G 144.742 15 0.0171 10 N ?
194PT2 G %IG=0.0107 7
194PT G 163.951 24 0.205 5 M1+E2 0.50 +7-8 1.45 5 C
194PTS G KC=1.13 6$LC=0.244 7$MC=0.0582 20
194PTS G NC=0.0143 5$OC=0.00249 7$PC=0.000128 7
194PT2 G %IG=0.129 5
194PT cG E$weighted average of 163.4 {I3} (1970Be30), 164.0 {I3} (1971Vi15),
194PT2cG 163.6 {I3} (1974HeYW), 164.01 {I3} (1996TeZW), 163.926 {I22}
194PT3cG (2015Do06), and 163.94 {I5} (1960Ba17)
194PT cG RI$weighted average of 0.200 {I17} (1970Be30), 0.22 {I3} (1974HeYW),
194PT2cG 0.190 {I8} (1996TeZW), and 0.209 {I4} (2015Do06)
194PT cG M,MR$from K/L1=7.7 {I7}, L1/L2=7.1 {I25}, L1/L3=16 {I8} (1971Vi15);
194PT2cG K/L=4.6 {I1}, L1/L3>14 (1960Ba17); |a(K)exp=1.2 {I2} deduced from
194PT3cG Ice(K)=5.0 {I5} (1971Vi15) and I|g=0.205 {I5} here. Other |a(K)exp:
194PT4cG 1.0 {I5} (1970Be30)
194PT G 223.911 21 0.0544 10(M1+E2) 1.7 +14-5 0.36 8 C
194PTS G KC=0.24 7$LC=0.0901 14$MC=0.0223 4
194PTS G NC=0.00548 9$OC=0.000904 17$PC=2.6E-5 9
194PT2 G %IG=0.0342 11
194PT cG E$weighted average of 223.99 {I10} (1996TeZW) and 223.907 {I21}
194PT2cG (2015Do06). Other: 224.0 {I3} (1971Vi15)
194PT cG RI$from 2015Do06. Other: 0.0550 {I23} (1996TeZW), 0.052 {I10}
194PT2cG (1977Vy01)
194PT cG M,MR$|a(K)exp=0.24 {I7} deduced from Ice(K)=0.27 {I8} (1971Vi15) and
194PT2cG I|g=0.0544 {I10} here, gives |d(E2/M1)=1.7 {I+14-5} or |d(M2/E1)=0.30
194PT3cG {I6}, with the former consistent with |DJ|p.
194PT G 290.688 14 0.326 5 E1 0.0281 C
194PTS G KC=0.0232 4$LC=0.00375 6$MC=0.000864 12
194PTS G NC=0.000212 3$OC=3.70E-5 6$PC=2.12E-6 3
194PT2 G %IG=0.205 7
194PT cG E$from 2015Do06. Others: 290.8 {I3} (1971Vi15) and 290.690 {I16}
194PT2cG (1996TeZW)
194PT cG RI$weighted average of 0.32 {I1} (1996TeZW) and 0.327 {I5} (2015Do06).
194PT2cG Other: 0.18 {I6} (1977Vy01) is discrepant
194PT cG M$|a(K)exp=0.012 {I5} deduced from Ice(K)=0.08 {I3} (1971Vi15) and
194PT2cG I|g=0.326 {I5} here
194PT G 339.01 13 0.0168 6 C
194PT2 G %IG=0.0106 5
194PT cG E$unweighted average of 338.88 {I10} (1996TeZW) and 339.137 {I26}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.018 {I5} (1996TeZW) and 0.0168 {I6} (2015Do06)
194PT G 449.317 12 0.243 2 (E1) 0.01040 C
194PTS G KC=0.00866 13$LC=0.001346 19$MC=0.000309 5
194PTS G NC=7.59E-5 11$OC=1.340E-5 19$PC=8.19E-7 12
194PT2 G %IG=0.153 4
194PT cG E$weighted average of 449.13 {I20} (1970Be30), 449.1 {I3} (1971Vi15),
194PT2cG 449.36 {I7} (1974HeYW), 449.303 {I12} (1996TeZW), and 449.335 {I14}
194PT3cG (2015Do06)
194PT cG RI$weighted average of 0.240 {I5} (1996TeZW) and 0.243 {I2} (2015Do06).
194PT2cG Others: 0.268 {I21} (1970Be30) and 0.30 {I3} (1974HeYW); 0.44 {I4}
194PT3cG (1971Vi15) could be for a composite peak
194PT cG M$|d<0.1 from |a(K)exp=0.081 {I+19-15} (1971Vi15)
194PT cG $Ice(K)=0.073 {I7} (1971Vi15)
194PT G 528.773 8 2.84 3 M1+E2 -1.68 +8-7 0.0336 10 C
194PTS G KC=0.0265 9$LC=0.00542 12$MC=0.00128 3
194PTS G NC=0.000317 7$OC=5.51E-5 13$PC=2.89E-6 10
194PT2 G %IG=1.78 5
194PT cG E$weighted average of 528.767 {I8} (1996TeZW) and 528.782 {I10}
194PT2cG (2015Do06). Others: 528.8 {I3} (1971Vi15), 529.06 {I10} (1974HeYW), and
194PT3cG 528.95 {I10} (1960Ba17)
194PT cG RI$weighted average of 2.85 {I5} (1996TeZW) and 2.83 {I3} (2015Do06).
194PT2cG Others: 3.2 {I3} (1964Be23), 3.9 {I3} (1971Vi15), and 3.6 {I4}
194PT3cG (1974HeYW) for a composite peak
194PT cG M,MR$from |a(K)exp=0.0265 {I6} deduced from Ice(K)=1.54 {I3}
194PT2cG and I|g=2.84 {I3} here, L2/L3>2.7, K/L2=17 {I3}, K/L3>45 (1970Ag05).
194PT3cG Other |a(K)exp: 0.0233 {I3} (1964Be23), 0.0200 {I12} (1970Be30),
194PT4cG and 0.020 {I2} (1971Vi15), for a composite peak. Other |d: -0.45 {I9},
194PT5cG -5.5 {I23}, -1.3 {I3}, -0.77 {I10}, -2.4 {I4} from |g|g(|q) of
194PT6cG 1996TeZW. Sign of |d from |g|g(|q)
194PT cG $(529|g)(202|g)(|q): A{-2}=-0.21 {I6}, A{-4}=-0.04 {I10}.
194PT cG $(529|g)(1104|g)(|q): A{-2}=-0.309 {I20}, A{-4}=+0.02 {I3}.
194PT cG $(529|g)[1104|g](328|g)(|q): A{-2}=+0.35 {I3}, A{-4}=-0.18 {I5}.
194PT cG $Ice(K)=1.54 {I3}, weighted average of 1.53 {I3} (1964Be23), 1.58 {I10}
194PT2cG (1971Vi15), and 1.80 {I18} (1960Ba17).
194PT G 1038.567 14 0.499 5 E1 0.00198 C
194PTS G KC=0.001662 24$LC=0.000244 4$MC=5.55E-5 8
194PTS G NC=1.367E-5 20$OC=2.45E-6 4$PC=1.634E-7 23
194PT2 G %IG=0.314 9
194PT cG E$from 2015Do06. Others: 1038.45 {I20} (1970Be30), 1038.56 {I8}
194PT2cG (1974HeYW), 1038.57 {I5} (1996TeZW), and 1038.80 {I20} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.56 {I25} (1964Be23), 0.51 {I7} (1970Be30),
194PT2cG 0.53 {I6} (1971Vi15), 0.52 {I5} (1974HeYW), and 0.50 {I7} (1996TeZW)
194PT cG M$|d<0.07 from |a(K)exp=0.0015 {I2} (1970Be30), 0.0014 {I+14-5}
194PT2cG (1964Be23). Other |d: -0.19 {I3} or +0.00 {I15} (1996TeZW,|g|g(|q)).
194PT cG $(1039|g)(301|g)(|q): A{-2}=-0.02 {I4}, A{-4}=-0.07 {I7}.
194PT cG $(1039|g)[594|g](328|g)(|q): A{-2}=-0.06 {I4}, A{-4}=-0.11 {I7}.
194PT cG $Ice(K)=0.0163 {I15}, weighted average of 0.0155 {I10} (1964Be23) and
194PT2cG 0.0190 {I19} (1960Ba17).
194PT dG $|a(K)exp=0.00159 {I15}, from Ice(K)=0.0163 {I15} and I|g=0.499 {I5}
194PT2dG here
194PT G 1339.251 14 0.360 4 E1 1.34E-3 YC
194PTS G KC=0.001063 15$LC=0.0001539 22$MC=3.50E-5 5
194PTS G NC=8.62E-6 12$OC=1.548E-6 22$PC=1.051E-7 15$IPC=7.62E-5 11
194PT2 G %IG=0.226 7
194PT cG E$weighted average of 1339.26 {I4} (1996TeZW) and 1339.250 {I14}
194PT2cG (2015Do06). Others: 1339.7 {I6} (1970Be30), 1339.3 {I3} (1971Vi15), and
194PT3cG 1339.6 {I3} (1974HeYW)
194PT cG $Level-energy difference=1339.300
194PT cG RI$weighted average of 0.354 {I13} (1996TeZW) and 0.361 {I4}
194PT2cG (2015Do06). Others: 0.48 {I24} (1970Be30), 2.51 {I10} (1971Vi15), and
194PT3cG 0.45 {I10} (1974HeYW)
194PT dG $|a(total)exp=0.007 {I3} for a gamma line at 1340 {I20} (1956Th11).
194PT cG M$|a(K)exp=0.0020 {I3} deduced from Ice(K)=0.015 {I2} (1971Vi15) and
194PT2cG I|g=0.360 {I4} here, gives |d=0.30 {I+5-6}; |d=0.0 {I9} from |g|g(|q)
194PT3cG of 1996TeZW.
194PT cG $(1339|g)(293|g)(|q): A{-2}=-0.02 {I6}, A{-4}=-0.09 {I9}.
194PT G 1632.847 16 0.428 5 E1 1.17E-3 C
194PTS G KC=0.000761 11$LC=0.0001092 16$MC=2.48E-5 4
194PTS G NC=6.11E-6 9$OC=1.100E-6 16$PC=7.54E-8 11$IPC=0.000272 4
194PT2 G %IG=0.269 8
194PT cG E$weighted average of 1633.0 {I3} (1970Be30), 1632.86 {I15} (1974HeYW),
194PT2cG 1632.79 {I3} (1996TeZW), 1632.858 {I14} (2015Do06), and 1633.5 {I5}
194PT3cG (1960Ba17)
194PT cG RI$weighted average of 0.385 {I25} (1971Vi15), 0.429 {I13} (1996TeZW),
194PT2cG and 0.429 {I4} (2015Do06). Others: 0.37 {I4} (1970Be30) and 0.47 {I5}
194PT3cG (1974HeYW)
194PT cG M$from |a(K)exp=0.00066 {I15} (1970Be30) gives |d<0.11; |d=-0.23 {I13}
194PT2cG or -1.08 {I29} from |g|g(|q) (1996TeZW).
194PT cG $(1633|g)(328|g)(|q): A{-2}=+0.40 {I6}, A{-4}=+0.07 {I11}.
194PT cG $Ice(K)=0.0063 {I10}, weighted average of 0.005 {I1} (1964Be23) and
194PT2cG 0.0070 {I7} (1960Ba17).
194PT L 2003.665 13 (2+)
194PT E 0.105 4 8.896 17 0.105 4
194PTS E CK=0.7781 2$CL=0.1670 2$CM+=0.05487 6
194PT G 1080.90 11 0.023 2 (M1(+E2)) 0.4 LT 0.0103 5 C
194PTS G KC=0.0086 4$LC=0.00135 6$MC=0.000311 13
194PTS G NC=7.7E-5 3$OC=1.39E-5 6$PC=9.5E-7 5
194PT2 G %IG=0.0145 13
194PT cG E$weighted average of 1081.8 {I19} (1970Be30), 1080.63 {I21}
194PT2cG (1996TeZW), 1080.91 {I10} (2015Do06), and 1081.6 {I4} (1960Ba17).
194PT3cG This transition was placed from 2312 level in 1970Be30 and 1971Vi15
194PT cG RI$from 2015Do06. Others: 0.05 {I3} (1970Be30), 0.020 {I8}
194PT2cG (1996TeZW), <0.15 (1971Vi15)
194PT cG M$|a(K)exp=0.0098 {I14} deduced from Ice(K)=0.0046 {I5} and I|g=0.023
194PT2cG {I2} here, gives |d(E2/M1)<0.4 or |d(M2/E1)=0.84 {I+13-12}, with the
194PT3cG former more likely. Other |a(K)exp: 0.0039 {I20} (1970Be30)
194PT cG $Ice(K)=0.0046 {I5}, weighted average of 0.0039 {I7} (1964Be23) and
194PT2cG 0.0050 {I5} (1960Ba17).
194PT G 1675.188 18 0.139 1 (M1) 0.00379 C
194PTS G KC=0.00299 5$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=0.000196 3
194PT2 G %IG=0.0873 25
194PT cG E,RI$from 2015Do06. Others:1675.1 {I5} (1996TeZW) with I|g=0.10 {I7}
194PT2cG (1996TeZW); 1675.7 {I3} (1974HeYW) with I|g=0.27 {I4}, 1675.9 {I6}
194PT3cG with I|g=0.17 {I5}, and 1675.9 {I3} with I|g=0.226 {I25} for a
194PT4cG composite peak. See also 1676|g placed from 2298 level
194PT cG M$|a(K)exp=0.0048 {I14} (1970Be30) for a composite peak
194PT cG $Ice(K)=0.0195 {I25}, unweighted average of 0.0170 {I10} (1964Be23) and
194PT2cG 0.0220 {I22} (1960Ba17), for a composite peak.
194PT G 2003.651 19 0.0120 5 n
194PT2 G %IG=0.0075 4
194PT L 2043.715 6 1+
194PT E 4.81 16 7.159 15 4.81 16
194PTS E CK=0.7740 3$CL=0.1700 2$CM+=0.05602 7
194PT G 227.05 11 0.0056 6 ?
194PT2 G %IG=0.0035 4
194PT cG E$unweighted average of 227.15 {I4} (2015Do06) and 226.94 {I10}
194PT2cG (1960Ba17). Placement from 1960Ba17 and 2015Do06; not seen in 1996TeZW.
194PT3cG Also placed from 2312 level by 1960Ba17.
194PT cG RI$from 2015Do06
194PT cG $Ice(K)=0.30 {I3}, weighted average of 0.33 {I7} (1964Be23) and 0.30
194PT2cG {I3} (1960Ba17)
194PT G 265.091 27 0.0083 4 N ?
194PT2 G %IG=0.0052 3
194PT G 373.11 4 0.0104 5 C
194PT2 G %IG=0.0065 4
194PT cG E$weighted average of 373.33 {I14} (1996TeZW) and 373.102 {I22}
194PT2cG (2015Do06)
194PT cG RI$from 2015Do06. Other: 0.0111 {I25} (1996TeZW)
194PT G 421.59 6 0.0440 8 C
194PT2 G %IG=0.0277 9
194PT cG E$unweighted average of 421.65 {I5} (1996TeZW) and 421.538 {I17}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.050 {I4} (1996TeZW) and 0.0439 {I5} (2015Do06)
194PT G 531.702 15 0.0384 8 N ?
194PT2 G %IG=0.0241 8
194PT G 564.444 7 0.0293 3 N ?
194PT2 G %IG=0.0184 6
194PT G 776.70 6 0.0041 4 Y
194PT2 G %IG=0.0026 3
194PT cG E,RI$from Table 4 of 2015Do06. According to e-mail reply of
194PT2cG July 8, 2015 from K. Krane, values E|g=776.63 {I8}, I|g=0.0082 {I8}
194PT3cG are for a doublet, the other component belonging to double-escape peak
194PT4cG of 1797.4|g.
194PT cG $Level-energy difference=776.52
194PT G 1120.961 17 0.0565 10 C
194PT2 G %IG=0.0355 12
194PT cG E,RI$from 2015Do06. Other: 1121.3 {I4} with I|g=0.07 {I5} (1996TeZW)
194PT G 1421.679 14 0.580 5 M1(+E2) 0.2 LT 0.0054210 C
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$IPC=6.64E-5 11
194PT2 G %IG=0.364 11
194PT cG E$weighted average of 1421.65 {I7} (1974HeYW), 1421.667 {I20}
194PT2cG (1996TeZW), and 1421.686 {I14} (2015Do06). Others: 1421.6 {I3}
194PT3cG (1970Be30), 1421.5 {I3} (1971Vi15), and 1421.77 {I20} (1960Ba17)
194PT cG RI$weighted average of 0.54 {I5} (1970Be30), 0.54 {I3} (1971Vi15), 0.60
194PT2cG {I5} (1974HeYW), 0.598 {I13} (1996TeZW), and 0.578 {I5} (2015Do06)
194PT dG RI$0.54 {I31} in Table I of 1971Vi15 is most likely 0.540 {I31}
194PT cG M,MR$|a(K)exp=0.00458 {I18}, from Ice(K)=0.0544 {I21} and I|g=0.580
194PT2cG {I5} here gives |d(E2/M1)<0.2 or |d(M2/E1)=0.78 {I4}, with the former
194PT3cG consistent with |d=+0.4 {I5} or -0.01 {I18} from |g|g(|q) of 1996TeZW.
194PT4cG Other |a(K)exp: >0.0047 (1964Be23), 0.0049 {I5} (1970Be30), 0.0049 {I5}
194PT5cG (1971Vi15).
194PT cG $(1422|g)(293|g)(|q): A{-2}=+0.09 {I4}, A{-4}=+0.02 {I7}.
194PT cG $(1422|g)[293|g](328|g)(|q): A{-2}=+0.06 {I4}, A{-4}=+0.06 {I7}.
194PT cG $Ice(K)=0.0544 {I21}, weighted average of 0.0535 {I20} (1964Be23),
194PT2cG 0.054 {I4} (1971Vi15), and 0.066 {I7} (1960Ba17).
194PT G 1715.235 16 1.175 14E2+M1 -1.10 12 0.0027910 C
194PTS G KC=0.00217 8$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
194PT2 G %IG=0.738 22
194PT cG E$weighted average of 1715.16 {I20} (1970Be30), 1715.23 {I6}
194PT2cG (1974HeYW), 1715.195 {I21} (1996TeZW), 1715.252 {I14} (2015Do06), and
194PT3cG 1715.7 {I3} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 1.30 {I25} (1964Be23), 1.12 {I9} (1970Be30),
194PT2cG 1.14 {I10} (1974HeYW), 1.20 {I4} (1996TeZW); 0.12 {I4} in Table I of
194PT3cG 1971Vi15 is most likely a typo and should be 1.2 {I4}, considering
194PT4cG other I|g values are in agreement with those of other studies
194PT cG M,MR$|a(K)exp=0.0026 {I5} deduced from Ice(K)=0.053 {I5} and I|g=1.175
194PT2cG {I14} here, gives |d(E2/M1)<1.3 or |d(M2/E1)=0.69 {I+14-13}, with the
194PT3cG former consistent with |d=-1.10 {I12} from |g|g(|q) of 1996TeZW. Other
194PT4cG |a(K)exp: 0.0019 {I+8-5} (1964Be23), 0.00223 {I23} (1970Be30)
194PT cG $(1715|g)(328|g)(|q): A{-2}=+0.60 {I4}, A{-4}=-0.33 {I6}.
194PT cG $Ice(K)=0.053 {I5}, weighted average of 0.051 {I3} (1964Be23) and 0.064
194PT2cG {I7} (1960Ba17).
194PT G 2043.719 15 5.95 4 M1 0.00263 C
194PTS G KC=0.00183 3$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
194PT2 G %IG=3.74 11
194PT cG E$weighted average of 2043.67 {I6} (1974HeYW), 2043.68 {I3} (1996TeZW),
194PT2cG and 2043.730 {I14} (2015Do06). Others: 2043.67 {I15} (1970Be30) and
194PT3cG 2044.1 {I4} (1960Ba17)
194PT cG RI$weighted average of 6.21 {I25} (1964Be23), 6.0 {I3} (1970Be30), 6.3
194PT2cG {I3} (1971Vi15), 5.92 {I4} (1974HeYW), 6.3 {I3} (1996TeZW), and 6.01
194PT3cG {I8} (2015Do06)
194PT cG M$|a(K)exp=0.00189 {I7}, from Ice(K)=0.231 {I8} and I|g=5.95 {I4} here
194PT2cG gives |d(E2/M1)<0.2 or |d(M2/E1)=0.76 {I3}, with only the former
194PT3cG consistent with this transition feeding 0+ g.s., which requires pure
194PT4cG dipole. Other |a(K)exp: 0.00181 {I+25-22} (1964Be23), 0.00187 {I11}
194PT5cG (1970Be30)
194PT dG $|a(total)exp=0.0018 {I5} for a gamma line at 2050 {I15} (1956Th11).
194PT cG $Ice(K)=0.231 {I8}, weighted average of 0.230 {I5} (1964Be23) and 0.28
194PT2cG {I3} (1960Ba17).
194PT L 2053.016 14(2)+
194PT E 0.072 6 8.97 4 0.072 6
194PTS E CK=0.7729 3$CL=0.17074 18$CM+=0.05632 7
194PT G 1241.93 7 0.0124 10 N ?
194PT2 G %IG=0.0078 7
194PT cG $Level-energy difference=1241.73
194PT G 1430.996 14 0.115 1 C
194PTF G FL=622.023
194PT2 G %IG=0.0723 21
194PT cG E$from 2015Do06. Others: 1430.95 {I8} (1996TeZW); 1431.6 {I4}
194PT2cG (1974HeYW) for a composite peak
194PT cG RI$weighted average of 0.121 {I10} (1996TeZW) and 0.115 {I1}
194PT2cG (2015Do06). Other: 0.30 {I5} (1974HeYW) for a composite peak
194PT G 1724.40 14 0.0894 9 C
194PT2 G %IG=0.0562 17
194PT cG E$unweighted average of 1724.26 {I6} (1996TeZW) and 1724.539 {I17}
194PT2cG (2015Do06). Other: 1724.1 {I13} (1970Be30)
194PT cG RI$weighted average of 0.096 {I7} (1996TeZW) and 0.0893 {I9}
194PT2cG (2015Do06). Other: 0.13 {I7} (1970Be30)
194PT L 2063.739 9 2+
194PT E 0.266 11 8.376 19 0.266 11
194PTS E CK=0.7717 3$CL=0.17167 19$CM+=0.05668 8
194PT G 1140.990 20 0.0309 5 M1 0.00939 C
194PTS G KC=0.00780 11$LC=0.001222 18$MC=0.000281 4
194PTS G NC=6.94E-5 10$OC=1.252E-5 18$PC=8.62E-7 12$IPC=1.351E-6 19
194PT2 G %IG=0.0194 6
194PT cG E$from 2015Do06. Others: 1140.98 {I11} (1996TeZW), 1141.0 {I4}
194PT2cG (1960Ba17), 1141.0 {I2} (1971Vi15)
194PT cG RI$weighted average of 0.031 {I3} (1996TeZW) and 0.0309 {I5}
194PT2cG (2015Do06). Others: 0.6 {I3} (1964Be23), 0.04 {I2} (1977Vy01)
194PT cG M$|a(K)exp=0.0123 {I19}, from Ice(K)=0.0078 {I12} and I|g=0.0309 {I5}
194PT2cG here
194PT cG $Ice(K)=0.0078 {I12}, unweighted average of 0.0075 {I2} (1964Be23),
194PT2cG 0.0058 {I6} (1971Vi15), and 0.0100 {I10} (1960Ba17).
194PT G 1441.703 14 0.255 3 M1(+E2) 0.6 LT 0.0050 4 C
194PTS G KC=0.0041 3$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
194PT2 G %IG=0.160 5
194PT cG E$weighted average of 1441.68 {I3} (1996TeZW) and 1441.705 {I14}
194PT2cG (2015Do06). Others: 1442.0 {I6} (1970Be30), 1441.87 {I15} (1974HeYW),
194PT3cG and 1442.0 {I3} (1960Ba17)
194PT cG RI$weighted average of 0.26 {I6} (1970Be30), 0.30 {I3} (1971Vi15), 0.33
194PT2cG {I4} (1974HeYW), 0.273 {I8} (1996TeZW), and 0.254 {I2} (2015Do06)
194PT cG M,MR$|a(K)exp=0.0042 {I4}, from Ice(K)=0.0218 {I19} and I|g=0.255 {I3}
194PT2cG here, gives |d(E2/M2)<0.6 or |d(M2/E1)=0.74 {I7}, with only the former
194PT3cG consistent with |d=0.0 {I3} or +3 +|@-3 from |g|g(|q) of 1996TeZW.
194PT4cG Other |a(K)exp: >0.0013 (1964Be23), 0.0039 {I9} (1970Be30).
194PT cG $(1442|g)[293|g](328|g)(|q): A{-2}=+0.06 {I7}, A{-4}=+0.13 {I11}.
194PT cG $Ice(K)=0.0218 {I19}, weighted average of 0.0207 {I15} (1964Be23) and
194PT2cG 0.0250 {I25} (1960Ba17).
194PT G 1735.245 14 0.475 5 M1+E2 +0.12 6 0.003516 C
194PTS G KC=0.00273 5$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
194PT2 G %IG=0.299 9
194PT cG E$weighted average of 1735.2 {I3} (1970Be30), 1735.3 {I3} (1971Vi15),
194PT2cG 1735.31 {I10} (1974HeYW), 1735.21 {I3} (1996TeZW), 1735.251 {I14}
194PT3cG (2015Do06). Other: 1735.8 {I3} (1960Ba17) for a doublet
194PT cG RI$weighted average of 0.492 {I17} (1996TeZW) and 0.473 {I5}
194PT2cG (2015Do06). Others: 0.47 {I4} (1970Be30), 0.46 (1974HeYW); 5.2 {I4}
194PT3cG in Table 1 of 1971Vi15 is most likely a typo and should be 0.52 {I4}
194PT cG M,MR$|a(K)exp=0.00292 {I21}, from Ice(K)=0.0284 {I20} and I|g=0.475
194PT2cG {I5} here, gives |d(E2/M1)<0.3 or |d(M2/E1)=0.80 {I+7-6}, with only
194PT3cG the former consistent with |d=+0.12 {I6} for J(2063)=2 from |g|g(|q) of
194PT4cG 1996TeZW. Other |d: -0.36 {I5} for J(2063)=1 from |g|g(|q) of 1996TeZW.
194PT5cG Other |a(K)exp: >0.0041 for a doublet and 0.00278 {I29} (1970Be30)
194PT cG $(1735|g)(328|g)(|q): A{-2}=+0.15 {I5}, A{-4}=-0.13 {I8}.
194PT cG $Ice(K)=0.0284 {I20}, weighted average of 0.0262 {I15} (1964Be23),
194PT2cG 0.031 {I2} (1971Vi15), and 0.034 {I4} (1960Ba17).
194PT G 2063.764 21 0.0091 4
194PT2 G %IG=0.0057 3
194PT cG E$from 2015Do06. Others: 2063.68 {I23} (1996TeZW), 2063.7 {I5}
194PT2cG (1977Vy01)
194PT cG RI$from 2015Do06. Others: 0.013 {I4} (1996TeZW), 0.016 {I4} (1977Vy01)
194PT L 2085.474 11 0+
194PT E 0.77 3 7.868 18 0.77 3
194PTS E CK=0.7688 3$CL=0.17370 21$CM+=0.05747 9
194PT G 288.13 4 0.0253 7 N ?
194PT2 G %IG=0.0159 6
194PT G 1463.434 14 1.095 11(E2) 0.00270 C
194PTS G KC=0.00218 3$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
194PT2 G %IG=0.688 20
194PT cG E$weighted average of 1463.429 {I19} (1996TeZW) and 1463.436 {I14}
194PT2cG (2015Do06). Others: 1463.1 {I6} (1970Be30), 1463.7 {I3} (1971Vi15),
194PT3cG 1463.45 {I10} (1974HeYW), and 1463.69 {I25} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 1.2 {I3} (1970Be30), 1.19 {I10} (1974HeYW),
194PT2cG and 1.094 {I22} (1996TeZW)
194PT cG M$|a(K)exp=0.00214 {I22} deduced from Ice(K)=0.048 {I5} and I|g=1.095
194PT2cG {I11} here gives Mult=E2 or |d(M2/E1)=0.40 {I4}, but |DJ|p=2+ requires
194PT3cG E2. Other |a(K)exp: >0.00091 (1964Be23), 0.0012 {I3} (1970Be30)
194PT cG $Ice(K)=0.048 {I5}, weighted average of 0.047 {I3} (1964Be23), 0.042
194PT2cG {I5} (1971Vi15), and 0.064 {I7} (1960Ba17).
194PT G 1756.998 14 0.0949 9 (E2) 0.00204 C
194PTS G KC=0.001564 22$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
194PT2 G %IG=0.0596 17
194PT cG E$from 2015Do06. Others: 1757.2 {I6} (1970Be30), 1756.98 {I6}
194PT2cG (1996TeZW), and 1757.6 {I15} (1960Ba17)
194PT cG RI$weighted average of 0.10 {I3} (1970Be30), 0.096 {I7} (1996TeZW), and
194PT2cG 0.0949 {I9} (2015Do06). Other: 0.0566 {I19} (1971Vi15) is discrepant
194PT cG M$|a(K)exp=0.00103 {I11} deduced from Ice(K)=0.0020 {I2} and
194PT2cG I|g=0.0949 {I9} here, gives Mult=E2 or |d(M2/E1)=0.26 {I+4-5}, but
194PT3cG |DJ|p=2+ requires E2.
194PT cG $Ice(K)=0.0020 {I2} (1960Ba17). Other: 0.0018 (1964Be23)
194PT G 2085.8 4 E0 0.0063 2
194PT cG E$seen in ce data (1960Ba17, 1964Be23)
194PT cG TI$deduced from Ice(K)=0.111 {I4} and ce(K)/ce=0.8630 for E0 (BrIcc)
194PT cG M$|a(K)exp>0.054 (1964Be23), >0.13 (1970Be30), >0.13 (1971Vi15), which
194PT2cG are larger than any of pure Mult for this transition feeding 0+ g.s.,
194PT3cG and can be explained only by this transition being E0
194PT cG $Ice(K)=0.111 {I4}, weighted average of 0.110 {I5} (1971Vi15), 0.110
194PT2cG {I4} (1964Be23), and 0.130 {I13} (1960Ba17)
194PT L 2109.088 11 (2)+
194PT E 0.154 6 8.514 18 0.154 6
194PTS E CK=0.7654 4$CL=0.17619 24$CM+=0.05845 10
194PT G 1186.325 19 0.108 2 (E2+M1) 1.1 +6-4 0.0060 10 C
194PTS G KC=0.0050 9$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
194PT2 G %IG=0.0679 23
194PT cG E$weighted average of 1186.27 {I4} (1996TeZW) and 1186.332 {I14}
194PT2cG (2015Do06). Others: 1186.3 {I2} (1971Vi15) and 1187.1 {I4} (1960Ba17)
194PT cG RI$weighted average of 0.09 {I4} (1977Vy01), 0.121 {I5} (1996TeZW) and
194PT2cG 0.107 {I1} (2015Do06)
194PT cG M,MR$|a(K)exp=0.0049 {I7}, from Ice(K)=0.0108 {I16} and I|g=0.108 {I2}
194PT2cG here gives |d(E2/M1)=1.1 {I+6-4} or |d(M2/E1)=0.55 {I7}, with only the
194PT3cG former consistent with |D|p=+ based on L(p,d)=1+3 from 1/2-.
194PT cG $Ice(K)=0.0108 {I16}, weighted average of 0.011 {I2} (1964Be23), 0.0079
194PT2cG {I15} (1971Vi15), and 0.0130 {I13} (1960Ba17).
194PT G 1487.102 16 0.197 2 (M1(+E2)) 0.3 LT 0.0048312 C
194PTS G KC=0.00394 10$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
194PT2 G %IG=0.124 4
194PT cG E$weighted average of 1486.8 {I6} (1970Be30), 1486.9 {I3} (1971Vi15),
194PT2cG 1487.0 {I3} (1974HeYW), 1487.16 {I3} (1996TeZW), 1487.089 {I14}
194PT3cG (2015Do06), and 1487.9 {I5} (1960Ba17)
194PT cG RI$weighted average of 0.22 {I5} (1970Be30), 0.26 {I3} (1971Vi15), 0.20
194PT2cG {I4} (1974HeYW), 0.200 {I5} (1996TeZW), and 0.196 {I2} (2015Do06)
194PT cG M,MR$|a(K)exp=0.0049 {I6}, from Ice(K)=0.0199 {I22} and I|g=0.197 {I2}
194PT2cG here, gives |d(E2/M1)<0.3 or |d(M2/E1)=0.95 {I+15-13}, with only the
194PT3cG former consistent with |D|p=+. Other |a(K)exp: 0.0026 {I3} (1949St17),
194PT4cG 0.0040 {I11} (1970Be30), 0.0034 {I7} (1971Vi15), >0.0018 (1964Be23)
194PT cG $Ice(K)=0.0199 {I22}, weighted average of 0.018 {I3} (1964Be23), 0.018
194PT2cG {I3} (1971Vi15), and 0.0220 {I22} (1960Ba17).
194PT G 1780.543 22 0.0474 8 C
194PT2 G %IG=0.0298 10
194PT cG E,RI$from 2015Do06. Other: 1780.57 {I19} with I|g=0.055 {I10}
194PT2cG (1996TeZW)
194PT L 2114.102 8 1+
194PT E 0.62 8 7.90 6 0.62 8
194PTS E CK=0.7646 4$CL=0.17676 25$CM+=0.05867 10
194PT G 190.05 8 0.0055 10M1 1.077
194PTF G FLAG=X
194PTS G KC=0.887 13$LC=0.1461 21$MC=0.0338 5
194PTS G NC=0.00835 12$OC=0.001503 22$PC=0.0001014 15
194PT2 G %IG=0.0035 6
194PT cG E$weighted average of 189.8 {I3} (1971Vi15) and 190.07 {I8} (2015Do06).
194PT2cG This transition was placed from 1622 level by 1971Vi15
194PT cG RI$from 2015Do06.
194PT cG M$|a(K)exp=0.67 {I+39-27} deduced from Ice(K)=0.075 {I22} (1971Vi15)
194PT2cG and I|g=0.0055 {I10} here. 0.42 {I+15-18}
194PT G 491.967 25 0.0084 4 N ?
194PT2 G %IG=0.0053 3
194PT cG $Level-energy difference=491.904
194PT G 566.91 4 0.0055 3 N ?
194PT2 G %IG=0.00346 21
194PT G 602.053 18 0.0141 6 C
194PT2 G %IG=0.0089 5
194PT cG E,RI$from 2015Do06. Other: 602.02 {I9} with I|g=0.030 {I13}
194PT G 846.96 12 0.0657 6 M1 0.0200 C
194PTS G KC=0.01656 24$LC=0.00262 4$MC=0.000602 9
194PTS G NC=0.0001490 21$OC=2.69E-5 4$PC=1.84E-6 3
194PT2 G %IG=0.0413 12
194PT cG E$unweighted average of 846.9 {I6} (1970Be30), 846.8 {I2} (1971Vi15),
194PT2cG 846.786 {I10} (1996TeZW), 846.896 {I14} (2015Do06), and 847.42 {I20}
194PT3cG (1960Ba17)
194PT cG RI$from 2015Do06. Other: 0.09 {I3} (1970Be30), <0.10 (1971Vi15); 0.997
194PT2cG {I20} (1996TeZW) is discrepant
194PT cG M$|a(K)exp=0.015 {I6} (1970Be30), and 0.020 {I3} deduced from
194PT2cG Ice(K)=0.027 {I4} (1971Vi15) and I|g=0.0657 {I6} here give
194PT3cG |d(E2/M1)<0.4, and |DJ|p requires pure M1.
194PT cG $Ice(K)=0.028 {I3}, weighted average of 0.027 {I3} (1964Be23), 0.027
194PT2cG {I4} (1971Vi15), and 0.030 {I3} (1960Ba17).
194PT cG M$|a(K)exp=0.0208 {I23} deduced from Ice(K)=0.028 {I3} and I|g=0.0657
194PT2cG {I6} here, gives Mult=M1 or E1+M2 with |d=0.95 {I12}, but only the
194PT3cG former consistent with this transition feeding 0+
194PT G 1492.065 14 0.285 3 M1(+E2) 0.5 LT 0.0046624 C
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$IPC=9.4E-5 4
194PT2 G %IG=0.179 5
194PT cG E$weighted average of 1492.06 {I6} (1996TeZW) and 1492.067 {I14}
194PT2cG (2015Do06). Others: 1491.8 {I3} (1970Be30), 1491.97 {I15} (1974HeYW),
194PT3cG and 1492.7 {I5} (1960Ba17)
194PT cG RI$weighted average of 0.42 {I19} (1964Be23), 0.29 {I4} (1970Be30),
194PT2cG 0.31 {I3} (1971Vi15), 0.29 {I4} (1974HeYW), 0.293 {I7} (1996TeZW), and
194PT3cG 0.283 {I3} (2015Do06)
194PT cG M,MR$|a(K)exp=0.0045 {I7}, from Ice(K)=0.026 {I4} and I|g=0.285 {I3}
194PT2cG here gives |d(E2/M1)<0.5 or |d(M2/E1)=0.87 {I+16-14}, with only the
194PT3cG former consistent with |d=+0.4 {I8} or -0.2 {I3} from |g|g(|q)
194PT4cG (1996TeZW). Other |a(K)exp: 0.0026 {I+29-11} (1964Be23), 0.0036 {I6}
194PT5cG (1970Be30)
194PT cG $(1492|g)(293|g)(|q): A{-2}=+0.15 {I7}, A{-4}=+0.05 {I11}.
194PT cG $(1492|g)[293|g](328|g)(|q): A{-2}=-0.01 {I8}, A{-4}=+0.18 {I12}.
194PT cG $Ice(K)=0.026 {I4}, unweighted average of 0.022 {I2} (1964Be23) and
194PT2cG 0.029 {I3} (1960Ba17).
194PT G 1785.636 17 0.672 6 M1(+E2) -0.04 3 0.00333 C
194PTS G KC=0.00255 4$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
194PT2 G %IG=0.422 12
194PT cG E$weighted average of 1785.63 {I20} (1970Be30), 1785.7 {I4} (1971Vi15),
194PT2cG 1785.47 {I7} (1974HeYW), 1785.62 {I3} (1996TeZW), 1785.645 {I14}
194PT3cG (2015Do06), and 1786.3 {I4} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.64 {I8} (1970Be30), 0.61 {I5} (1971Vi15),
194PT2cG 0.62 {I6} (1974HeYW), and 0.689 {I25} (1996TeZW)
194PT cG M,MR$|a(K)exp=0.00276 {I15} deduced from Ice(K)=0.038 {I2} and
194PT2cG I|g=0.672 {I6} here, gives |d(E2/M1)<0.2 or |d(M2/E1)=0.81 {I5}, with
194PT3cG only the former consistent with |d=-0.04 {I3} from |g|g(|q) of
194PT4cG 1996TeZW. Other |a(K)exp: 0.0033 {I4} (1971Vi15), 0.0027 {I4}
194PT5cG (1970Be30), >0.0042 (1964Be23)
194PT cG $(1786|g)(328|g)(|q): A{-2}=-0.20 {I3}, A{-4}=-0.04 {I6}.
194PT cG $Ice(K)=0.038 {I2}, weighted average of 0.036 {I2} (1964Be23), 0.041
194PT2cG {I3} (1971Vi15), and 0.044 {I5} (1960Ba17).
194PT G 2114.100 14 0.421 4 M1 0.00250
194PTS G KC=0.001684 24$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
194PT2 G %IG=0.265 8
194PT cG E$weighted average of 2114.06 {I4} (1996TeZW) and 2114.105 {I14}
194PT2cG (2015Do06). Others: 2114.16 {I20} (1970Be30), 2113.93 {I20}
194PT3cG (1974HeYW), and 2114.0 {I4} (1960Ba17)
194PT cG RI$weighted average of 0.40 {I9} (1964Be23), 0.40 {I3} (1970Be30),
194PT2cG 0.440 {I13} (1971Vi15), 0.46 {I5} (1974HeYW), 0.447 {I23} (1996TeZW),
194PT3cG and 0.418 {I4} (2015Do06)
194PT cG M$|a(K)exp=0.00204 {I22}, from Ice(K)=0.0176 {I19} and I|g=0.421 {I4}
194PT2cG here, gives |d(E2/M1)<0.4 or |d(M2/E1)=0.91 {I+13-11}, with only the
194PT3cG former consistent with this transition feeding 0+ g.s., which
194PT4cG requires pure dipole
194PT cG $Ice(K)=0.0176 {I19}, weighted average of 0.0160 {I20} (1964Be23) and
194PT2cG 0.0190 {I19} (1960Ba17).
194PT L 2131.127 11 (2+)
194PT cL $Level and J|p proposed by 2015Do06.
194PT E 0.155 6 8.459 18 0.155 6
194PTS E CK=0.7617 4$CL=0.1788 3$CM+=0.05948 11
194PT G 1208.372 18 0.0246 7
194PT2 G %IG=0.0155 6
194PT cG E,RI$from 2015Do06. Other: 1208.5 {I4} with I|g=0.4 {I2} from
194PT2cG ce data (1960Ba17, 1964Be23), unplaced
194PT G 1319.70 4 0.0097 6 ?
194PT2 G %IG=0.0061 4
194PT cG E,RI$from 2015Do06 only. Level-energy difference=1319.84
194PT G 1509.08 3 0.0121 9 ?
194PT2 G %IG=0.0076 6
194PT cG E,RI$from 2015Do06 only.
194PT G 1802.637 14 0.198 3 M1,E2 0.0026 7 &
194PTS G KC=0.0020 5$LC=0.00031 8$MC=7.1E-5 18
194PTS G NC=1.8E-5 5$OC=3.2E-6 8$PC=2.1E-7 6$IPC=0.00023 5
194PT2 G %IG=0.124 4
194PT cG E,RI$from 2015Do06 only. See also placement from 1802 level
194PT cG M$|a(K)exp=0.0018 {I9} (1970Be30), 0.0022 {I+15-8} (1971Vi15),
194PT2cG |?0.00062 (1964Be23) for a doublet
194PT G 2131.08 7 0.0016 2 ?
194PT2 G %IG=0.00101 13
194PT cG E,RI$from 2015Do06 only
194PT L 2134.107 15 1+,2+
194PT cL J$|g|g(|q) (1996TeZW) forbids J=0
194PT E 0.198 9 8.345 21 0.198 9
194PTS E CK=0.7612 4$CL=0.1792 3$CM+=0.05963 11
194PT G 1512.073 14 0.095 9 M1,E2 0.0037 11 @C
194PTF G FL=622.023
194PTS G KC=0.0030 9$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
194PT2 G %IG=0.060 6
194PT cG E$from 2015Do06. Others: 1512.0 {I3} (1971Vi15), 1511.9 {I3}
194PT2cG (1974HeYW), 1512.33 {I11} (1996TeZW) for a composite peak
194PT cG RI$from 2015Do06. Others: 0.162 {I15} (1996TeZW), 0.19 {I3}
194PT3cG (1974HeYW), 0.19 {I5} (1970Be30), and 0.18 {I3} (1971Vi15) for a
194PT4cG composite peak
194PT cG M$|a(K)exp>0.0017 (1964Be23), 0.0029 {I8} (1970Be30), 0.0035 {I+15-11}
194PT2cG (1971Vi15) for a doublet. See also the placement from 1512 level.
194PT cG $Ice(K)=0.0121 {I10}, weighted average of 0.0110 {I10} (1964Be23),
194PT2cG 0.0140 {I14} (1960Ba17), and 0.0125 {I20} for a doublet.
194PT cG $Total intensity=0.171 {I1} for doublet in 2015Do06 and divided by
194PT2cG evaluators for placement from 1512 based on {+194}Ir |b{+-} decay
194PT3cG (19.3 h) dataset, remaining intensity is assigned from 2134 level.
194PT G 1805.729 14 0.219 3 M1(+E2) 0.5 LT 0.0031314 YC
194PTF G FL=328.474
194PTS G KC=0.00239 11$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
194PT2 G %IG=0.138 4
194PT cG E$from 2015Do06. Others: 1805.7 {I6} (1970Be30), 1806.1 {I4}
194PT2cG (1971Vi15), 1805.72 {I3} (1996TeZW), and 1805.9 {I8} (1960Ba17)
194PT cG $Level-energy difference=1805.624
194PT cG RI$weighted average of 0.29 {I9} (1970Be30), 0.32 {I8} (1971Vi15),
194PT2cG 0.237 {I12} (1996TeZW), and 0.218 {I2} (2015Do06)
194PT cG M,MR$|a(K)exp=0.0026 {I3}, from Ice(K)=0.0117 {I12} and I|g=0.219 {I3}
194PT2cG here gives |d(E2/M1)<0.5 or |d(M2/E1)=0.79 {I10}, with only the former
194PT3cG consistent with |d=-0.25 {I4} for J(2134)=1 or +0.27 {I6} for J(2134)=2
194PT4cG from |g|g(|q) of 1996TeZW. Other |a(K)exp: >0.0015 (1964Be23), 0.0017
194PT5cG {I9} (1970Be30), 0.0017 {I+9-5} (1971Vi15).
194PT cG $(1806|g)(328|g)(|q): A{-2}=+0.03 {I5}, A{-4}=-0.07 {I8}.
194PT cG $Ice(K)=0.0117 {I12}, weighted average of 0.0113 {I12} (1971Vi15) and
194PT2cG 0.0120 {I12} (1960Ba17).
194PT L 2140.698 12(1+,2+)
194PT E 0.103 4 8.612 18 0.103 4
194PTS E CK=0.7599 4$CL=0.1801 3$CM+=0.05997 12
194PT G 1518.659 14 0.112 1 (M1(+E2)) 0.7 LT 0.0043 4 C
194PTS G KC=0.0035 3$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
194PT2 G %IG=0.0704 20
194PT cG E$weighted average of 1518.62 {I5} (1996TeZW) and 1518.662 {I14}
194PT2cG (2015Do06). Others: 1518.8 {I6} (1970Be30), 1518.4 {I3} (1971Vi15),
194PT3cG 1518.5 {I2} (1974HeYW), and 1518.9 {I6} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.13 {I4} (1970Be30), 0.11 {I3} (1971Vi15),
194PT2cG 0.11 {I2} (1974HeYW), and 0.108 {I7} (1996TeZW)
194PT cG M,MR$|a(K)exp=0.0037 {I4}, from Ice(K)=0.0085 {I9} and I|g=0.112 {I1}
194PT2cG here, gives |d(E2/M1)<0.7 or |d(M2/E1)=0.74 {I8}, with the former more
194PT3cG likely. Other: |a(K)exp: >0.0012 (1964Be23), 0.0028 {I9} (1970Be30),
194PT4cG 0.0050 {I+35-19} (1971Vi15).
194PT cG $Ice(K)=0.0085 {I9}, weighted average of 0.0073 {I10} (1964Be23),
194PT2cG 0.0110 {I20} (1971Vi15), and 0.0090 {I9} (1960Ba17).
194PT G 1812.228 17 0.0503 8 (M1) 0.00324 C
194PTS G KC=0.00246 4$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
194PT2 G %IG=0.0316 10
194PT cG E$from 2015Do06. Others: 1812.21 {I25} (1996TeZW), and 1812.8 {I6}
194PT2cG (1960Ba17)
194PT cG RI$from 2015Do06. Other: 0.055 {I12} (1996TeZW)
194PT cG M$|a(K)exp=0.0042 {I4}, from Ice(K)=0.0043 {I4} and I|g=0.0503 {I8}
194PT2cG here gives Mult=M1 or |d(M2/E1)=1.5 {I+4-3}, with the former more
194PT3cG likely
194PT cG $Ice(K)=0.0043 {I4}, weighted average of 0.0041 {I3} (1964Be23) and
194PT2cG 0.0050 {I5} (1960Ba17).
194PT G 2140.71 8 0.0005 2 n
194PT2 G %IG=3.1E-4 13
194PT L 2157.996 14 (2)+
194PT E 0.279 11 8.134 18 0.279 11 ?
194PTS E CK=0.7565 5$CL=0.1826 4$CM+=0.06094 13
194PT G 1346.68 4 0.0251 4 C
194PT2 G %IG=0.0158 5
194PT cG E,RI$from 2015Do06. Other: 1346.7 {I3} with I|g=0.015 {I7} (1996TeZW)
194PT G 1535.781 21 0.024 9 YC
194PTF G FL=622.023
194PT2 G %IG=0.015 6
194PT cG E$from 2015Do06. Other: 1535.5 {I3} (1996TeZW)
194PT cG $Level-energy difference=1535.966
194PT cG RI$unweighted average of 0.016 {I5} (1996TeZW) and 0.0328 {I8}
194PT2cG (2015Do06)
194PT G 1829.519 14 0.392 4 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$IPC=0.000287 6
194PT2 G %IG=0.246 7
194PT cG E$weighted average of 1829.50 {I3} (1996TeZW) and 1829.523 {I14}
194PT2cG (2015Do06). Others: 1829.6 {I3} (1970Be30), 1829.41 {I10} (1974HeYW),
194PT3cG and 1830.1 {I3} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.48 {I19} (1964Be23), 0.39 {I3} (1970Be30),
194PT2cG 0.365 {I19} (1971Vi15), 0.41 {I5} (1974HeYW), 0.421 {I17} (1996TeZW)
194PT cG M,MR$|a(K)exp=0.0029 {I3}, from Ice(K)=0.0232 {I24} and I|g=0.392 {I4}
194PT2cG here, gives |d(E2/M1)<0.3 or |d(M2/E1)=0.92 {I12}, with only the
194PT3cG former consistent with -0.41 {I7} for J(2158)=1, +0.02 {I12} for
194PT4cG J(2158)=2 from |g|g(|q) of 1996TeZW. Other |a(K)exp: 0.0022 {I+20-9}
194PT5cG (1964Be23), 0.0028 {I3} (1970Be30)
194PT cG $(1829|g)(328|g)(|q): A{-2}=+0.23 {I8}, A{-4}=-0.01 {I12}.
194PT cG $Ice(K)=0.0232 {I24}, weighted average of 0.0220 {I15} (1964Be23) and
194PT2cG 0.028 {I3} (1960Ba17).
194PT L 2163.745 10 0+
194PT E 0.81 8 7.66 5 0.81 8
194PTS E CK=0.7553 5$CL=0.1834 4$CM+=0.06128 13
194PT G 49.7 3 0.040 11M1 9.12 21 A
194PTF G FLAG=X
194PTS G LC=7.02 16$MC=1.62 4
194PTS G NC=0.402 10$OC=0.0722 17$PC=0.00486 11
194PT2 G %IG=0.025 7
194PT cG RI$deduced from Ice(L1)=5.4 {I15} and assigned mult and |d.
194PT cG M,MR$from L1/L2=8.5 {I16} (1971Vi15), |d<0.1; |d=0 required
194PT2cG by 0+ to 1+ transition.
194PT dG $|a(total)exp=0.013 {I5} for a gamma line at 2150 {I15} (1956Th11).
194PT G 239.443 17 0.080 3 M1 0.567 C
194PTS G KC=0.467 7$LC=0.0766 11$MC=0.01769 25
194PTS G NC=0.00438 7$OC=0.000788 11$PC=5.32E-5 8
194PT2 G %IG=0.0503 23
194PT cG E$weighted average of 239.43 {I4} (1996TeZW) and 239.445 {I17}
194PT2cG (2015Do06). Other: 239.5 {I3} (1971Vi15)
194PT cG RI$weighted average of 0.099 {I8} (1996TeZW), 0.0792 {I16}
194PT2cG (2015Do06), and 0.090 {I10} (1977Vy01)
194PT cG M$|a(K)exp=0.56 {I11} deduced from Ice(K)=0.92 {I18} (1971Vi15) and
194PT2cG I|g=0.080 {I3} here, gives |d(E2/M1)<0.4; |DJ|p=1+ requires pure
194PT3cG M1
194PT G 366.365 22 0.0477 15 C
194PT2 G %IG=0.0300 13
194PT cG E$weighted average of 366.42 {I4} (1996TeZW) and 366.356 {I16}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.058 {I7} (1996TeZW) and 0.0475 {I10}
194PT2cG (2015Do06)
194PT G 1541.715 18 0.0394 6 C
194PT2 G %IG=0.0248 8
194PT cG E,RI$from 2015Do06. Other: 1541.65 {I13} with I|g=0.034 {I4} (1996TeZW)
194PT G 1835.274 14 0.642 6 E2 0.00193 C
194PTS G KC=0.001445 21$LC=0.000225 4$MC=5.17E-5 8
194PTS G NC=1.276E-5 18$OC=2.29E-6 4$PC=1.507E-7 21$IPC=0.000196 3
194PT2 G %IG=0.403 12
194PT cG E$weighted average of 1835.33 {I7} (1974HeYW), 1835.244 {I24}
194PT2cG (1996TeZW), and 1835.282 {I14} (2015Do06). Others: 1835.19 {I20}
194PT3cG (1970Be30) and 1835.9 {I4} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.45 {I19} (1964Be23), 0.58 {I4} (1970Be30),
194PT2cG 0.66 {I4} (1971Vi15), 0.64 {I6} (1974HeYW), 0.679 {I25} (1996TeZW)
194PT cG M$|a(K)exp=0.00154 {I12} deduced from Ice(K)=0.0203 {I16} and I|g=0.642
194PT2cG {I6} here. Other |a(K)exp: 0.0021 {I+20-8} (1964Be23), 0.00166 {I15}
194PT3cG (1970Be30).
194PT cG $Ice(K)=0.0203 {I16}, weighted average of 0.0196 {I10} (1964Be23) and
194PT2cG 0.0240 {I24} (1960Ba17).
194PT G 2164.1 4 E0 0.018 1
194PT cG E$transition seen in ce data only (1960Ba17, 1964Be23).
194PT cG TI$deduced from Ice(K)=0.314 {I17} and ce(K)/ce=0.8631 for E0 (BrIcc)
194PT cG M$|a(K)exp>0.16 (1964Be23), >0.36 (1970Be30), which are larger than any
194PT2cG of pure Mult for this transition feeding 0+ g.s., and can be explained
194PT3cG only by this transition being E0.
194PT cG $Ice(K)=0.314 {I17}, weighted average of 0.310 {I10} (1964Be23) and
194PT2cG 0.38 {I4} (1960Ba17)
194PT L 2184.910 12 1+,2+
194PT E 0.356 12 7.954 16 0.356 12
194PTS E CK=0.7503 6$CL=0.1870 4$CM+=0.06268 15
194PT G 752.47 7 0.0046 5 N ?
194PT2 G %IG=0.0029 3
194PT G 1262.27 15 0.0402 7 KC
194PT2 G %IG=0.0253 8
194PT cG E$unweighted average of 1262.42 {I9} (1996TeZW) and 1262.124 {I18}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.046 {I5} (1996TeZW) and 0.0401 {I6} (2015Do06)
194PT G 1562.891 14 0.458 5 M1(+E2) 0.3 LT 0.0043211 C
194PTS G KC=0.00349 9$LC=0.000542 13$MC=0.000124 3
194PTS G NC=3.08E-5 8$OC=5.55E-6 13$PC=3.83E-7 10$IPC=0.000131 3
194PT2 G %IG=0.288 9
194PT cG E$weighted average of 1562.91 {I4} (1996TeZW) and 1562.889 {I14}
194PT2cG (2015Do06). Others: 1562.81 {I20} (1970Be30), 1562.8 {I3} (1974HeYW),
194PT3cG and 1563.4 {I4} (1960Ba17)
194PT cG RI$weighted average of 0.469 {I10} (1996TeZW) and 0.456 {I4}
194PT2cG (2015Do06). Others: 0.51 {I4} (1970Be30), 0.55 {I3} (1971Vi15), and
194PT3cG 0.56 {I7} (1974HeYW)
194PT cG M,MR$|a(K)exp=0.0039 {I3}, from Ice(K)=0.037 {I3} and I|g=0.458 {I5}
194PT2cG here, gives |d(E2/M1)<0.3 or |d(M2/E1)=0.84 {I7}, with only the former
194PT3cG consistent with low values of |d=+0.1 {I7}, -0.22 {I25} for J(2185)=1,
194PT4cG -0.5 {I16}, +0.3 {I4}, +2.0 +|@{I-16}, -7 {I+5-}|@ for J(2185)=2 from
194PT5cG |g|g(|q) of 1996TeZW. Other |a(K)exp: 0.0034 {I4} (1970Be30), >0.0028
194PT6cG (1964Be23)
194PT cG $(1563|g)(293|g)(|q): A{-2}=+0.06 {I6}, A{-4}=+0.09 {I10}.
194PT cG $(1563|g)[293|g](328|g)(|q): A{-2}=0.00 {I6}, A{-4}=-0.02 {I10}.
194PT cG $Ice(K)=0.037 {I3}, weighted average of 0.0354 {I20} (1964Be23) and
194PT2cG 0.044 {I5} (1960Ba17).
194PT G 1856.403 17 0.0604 8 C
194PT2 G %IG=0.0380 12
194PT cG E$from 2015Do06. Others: 856.37 {I7} (1996TeZW), 1856.3 {I13}
194PT2cG (1970Be30)
194PT cG RI$weighted average of 0.058 {I3} (1996TeZW), 0.0606 {I6} (2015Do06),
194PT2cG 0.050 {I5} (1971Vi15), and 0.07 {I4} (1970Be30)
194PT L 2214.523 9 (2+)
194PT E 2.89 11 6.954 18 2.89 11
194PTS E CK=0.7420 7$CL=0.1929 5$CM+=0.06502 19
194PT G 397.84 5 0.0055 5 N ?
194PT2 G %IG=0.0035 3
194PT G 702.54 4 0.0388 10(M1) 0.0322 C
194PTS G KC=0.0267 4$LC=0.00425 6$MC=0.000977 14
194PTS G NC=0.000242 4$OC=4.36E-5 7$PC=2.98E-6 5
194PT2 G %IG=0.0244 9
194PT cG E$weighted average of 702.6 {I3} (1971Vi15), 703.09 {I20} (1996TeZW),
194PT2cG and 702.532 {I18} (2015Do06). Other: 703.54 {I5} (1974HeYW), 703.43
194PT3cG {I15} (1970Be30) for a composite peak
194PT cG RI$from 2015Do06. Others: 0.15 {I12} (1996TeZW); 0.66 {I6} (1974HeYW),
194PT2cG 0.773 {I10}, 0.71 {I6} (1970Be30), 1.5 {I8} (1964Be23) for a composite
194PT3cG peak
194PT cG M$|a(K)exp=0.028 {I9} deduced from Ice(K)=0.022 {I7} (1971Vi15) and
194PT2cG I|g=0.0388 {I10} here, consistent with M1, but it also gives
194PT3cG |d(M2/E1)=0.63 {I17}; |a(K)exp=0.011 {I+14-5} (1964Be23) for a
194PT4cG composite peak consistent with M1 but not E1,M2
194PT G 781.974 17 0.0565 7 C
194PT2 G %IG=0.0355 11
194PT cG E$weighted average of 781.97 {I4} (1996TeZW) and 781.975 {I17}
194PT2cG (2015Do06). Other: 781.8 {I20} (1970Be30).
194PT cG RI$weighted average of 0.071 {I8} (1996TeZW), 0.0564 {I5}
194PT2cG (2015Do06), and 0.09 {I5} (1970Be30)
194PT G 1291.765 14 0.127 2 (M1(+E2)) 0.3 LT 0.0067518 C
194PTS G KC=0.00559 15$LC=0.000874 22$MC=0.000201 5
194PTS G NC=4.96E-5 13$OC=8.95E-6 23$PC=6.16E-7 17$IPC=2.35E-5 5
194PT2 G %IG=0.080 3
194PT cG E$from 2015Do06. Others: 1291.7 {I3} (1971Vi15), 1291.89 {I11}
194PT2cG (1996TeZW), and 1291.8 {I10} (1960Ba17)
194PT cG RI$weighted average of 0.2 {I1} (1970Be30), 0.18 {I4} (1971Vi15), 0.106
194PT2cG {I10} (1996TeZW), and 0.127 {I1} (2015Do06)
194PT cG M,MR$|a(K)exp=0.0073 {I8}, from Ice(K)=0.019 {I2} and I|g=0.127 {I2}
194PT2cG here gives |d(E2/M1)<0.3 or |d(M2/E1)=1.00 {I+14-12}, with the former
194PT3cG more likely. Other |a(K)exp: 0.0039 {I20} (1970Be30), 0.0052 {I+23-15}
194PT4cG (1971Vi15), >0.0024 (1964Be23)
194PT cG $Ice(K)=0.019 {I2}, from 1971Vi15. Others: 0.015 {I4} (1964Be23) and
194PT2cG 0.0200 {I20} (1960Ba17).
194PT G 1592.489 14 1.69 3 M1(+E2) 0.3 LT 0.0041510 C
194PTS G KC=0.00333 8$LC=0.000517 12$MC=0.000119 3
194PTS G NC=2.94E-5 7$OC=5.30E-6 13$PC=3.66E-7 9$IPC=0.000147 3
194PT2 G %IG=1.06 4
194PT cG E$weighted average of 1592.46 {I3} (1996TeZW) and 1592.495 {I14}
194PT2cG (2015Do06). Others: 1592.4 {I3} (1971Vi15); 1592.9 {I1} (1974HeYW) for
194PT3cG a composite peak
194PT cG RI$weighted average of 1.85 {I10} (1996TeZW) and 1.68 {I2} (2015Do06).
194PT2cG Others: 6.0 {I6} (1971Vi15) and 2.8 {I3} (1974HeYW) for a composite
194PT3cG peak
194PT dG $|a(total)exp=0.003 {I1} for a gamma line at 1590 {I20} (1956Th11).
194PT cG M,MR$|a(K)exp=0.0039 {I4} deduced from Ice(K)=0.134 {I12} (1971Vi15)
194PT2cG and I|g=1.69 {I3} here, gives |d(E2/M1)<0.3 or |d(M2/E1)=0.88
194PT3cG {I+11-10}, with only the former consistent with |d=-0.2 {I6} or -0.4
194PT4cG {I5} for J(2214)=1 and +0.3 {I9} or 0.0 {I6} for J(2214)=2 from
194PT5cG |g|g(|q) of 1996TeZW. Other |a(K)exp: 0.0031 {I9} (1970Be30) and
194PT6cG >0.0033 (1964Be23) for a composite peak, consistent with M1
194PT cG $(1592|g)(293|g)(|q): A{-2}=+0.01 {I6}, A{-4}=-0.02 {I10}.
194PT cG $(1592|g)[293|g](328|g)(|q): A{-2}=-0.05 {I10}, A{-4}=-0.04 {I17}.
194PT cG $Other Ice(K): 0.170 {I15} (1964Be23) and 0.200 {I20} (1960Ba17)
194PT2cG for a composite peak
194PT G 1885.95 7 2.64 6 M1(+E2) 0.3 LT 0.002967 C
194PTS G KC=0.00220 5$LC=0.000339 8$MC=7.78E-5 17
194PTS G NC=1.92E-5 4$OC=3.47E-6 8$PC=2.41E-7 6$IPC=0.000323 7
194PT2 G %IG=1.66 6
194PT cG E$unweighted average of 1885.9 {I4} (1971Vi15), 1885.86 {I6}
194PT2cG (1996TeZW), and 1886.078 {I14} (2015Do06). Other: 1886.50 {I5}
194PT3cG (1974HeYW), 1886.8 {I3} (1960Ba17), 1886.50 {I15} (1970Be30) for
194PT4cG a composite peak
194PT cG RI$weighted average of 2.1 {I4} (1996TeZW) and 2.65 {I4} (2015Do06).
194PT2cG Others: 5.7 {I9} (1971Vi15), 5.3 {I3} (1974HeYW), 5.84 {I25}
194PT3cG (1964Be23), and 5.4 {I3} (1970Be30) for a composite peak
194PT dG $|a(total)exp=0.0014 {I4} for a gamma line at 1890 {I15} (1956Th11).
194PT cG M,MR$|a(K)exp=0.0029 {I3} deduced from Ice(K)=0.156 {I15} (1971Vi15)
194PT2cG and I|g=2.64 {I6} here, gives |d(E2/M1)<0.3 or |d(M2/E1)=1.00
194PT3cG {I+14-12}, with only the former consistent with |d=-0.26 {I3} for
194PT4cG J(2214)=1, +0.25 {I4} for J(2214)=2 from |g|g(|q) of 1996TeZW.
194PT5cG Other |a(K)exp: 0.00207 {I12} (1970Be30) and 0.00192 {I+27-24}
194PT6cG (1964Be23) for a composite peak, consistent with M1.
194PT cG $(1886|g)(328|g)(|q): A{-2}=+0.04 {I3}, A{-4}=-0.15 {I6}.
194PT cG $Other Ice(K): 0.230 {I4} (1964Be23) and 0.28 {I3} (1960Ba17) for
194PT2cG for a composite peak
194PT G 2214.47 5 0.015 4 n
194PT2 G %IG=0.009 3
194PT L 2215.530 6 1+
194PT E 6.9 4 6.57 3 6.9 4
194PTS E CK=0.7417 7$CL=0.1932 5$CM+=0.06511 19
194PT G 101.46 4 0.0098 6 M1 6.39
194PTS G KC=5.26 8$LC=0.875 13$MC=0.202 3
194PTS G NC=0.0501 7$OC=0.00901 13$PC=0.000606 9
194PT2 G %IG=0.0062 4
194PT cG E$weighted average of 101.38 {I14} (1996TeZW) and 101.47 {I4}
194PT2cG (2015Do06). Other: 101.4 {I3} (1971Vi15)
194PT cG RI$weighted average of 0.0081 {I22} (1996TeZW) and 0.0099 {I6}
194PT2cG (2015Do06)
194PT cG M$from |a(K)exp=4.0 {I15} deduced from Ice(K)=0.8 {I3} (1971Vi15) and
194PT2cG I|g=0.0098 {I6} here
194PT G 106.51 4 0.0146 6 M1 5.56
194PTS G KC=4.58 7$LC=0.761 11$MC=0.1759 25
194PTS G NC=0.0435 7$OC=0.00783 11$PC=0.000527 8
194PT2 G %IG=0.0092 5
194PT cG E$weighted average of 106.5 {I3} (1971Vi15), 106.48 {I8} (1996TeZW),
194PT2cG and 106.52 {I4} (2015Do06). Other: 107.24 {I6} (1960Ba17) is
194PT3cG discrepant and placed from the 1924 level by 1960Ba17
194PT cG RI$from 2015Do06. Other: 0.0137 {I25} (1996TeZW)
194PT cG M$from K/L1=8 {I4}, L1/L2>3.5 (1971Vi15); |a(K)exp=4.0 {I10} deduced
194PT2cG from Ice(K)=1.2 {I3} (1971Vi15) and I|g=0.0146 {I6} here. Other:
194PT3cG |a(L1)exp=8.0 {I8} deduced from Ice(L1)=2.4 {I2} (1960Ba17 and
194PT4cG and 1964Be23) and I|g here gives Mult=M2, inconsistent with ce data
194PT5cG above and |DJ|p, which could indicate a different transition
194PT G 151.83 3 0.116 3 M1 2.03 C
194PTS G KC=1.667 24$LC=0.276 4$MC=0.0637 9
194PTS G NC=0.01577 22$OC=0.00284 4$PC=0.000191 3
194PT2 G %IG=0.073 3
194PT cG E$weighted average of 151.8 {I6} (1970Be30), 151.8 {I3} (1971Vi15),
194PT2cG 151.91 {I3} (1996TeZW), and 151.799 {I17} (2015Do06).
194PT cG RI$weighted average of 0.108 {I8} (1996TeZW) and 0.117 {I2} (2015Do06)
194PT2cG 0.092 {I12} (1977Vy01). Other: 0.10 {I5} (1970Be30)
194PT cG M$from L1/L2>9 and K/L1=5.7 {I12} in 1971Vi15, and |a(K)exp=1.35
194PT2cG {I13} deduced from Ice(K)=3.2 {I3} (1971Vi15) and adopted I|g=0.116
194PT3cG {I3} here.
194PT G 162.58 4 0.0407 13M1(+E2) 0.7 LT 1.52 16 C
194PTS G KC=1.20 18$LC=0.247 20$MC=0.058 6
194PTS G NC=0.0144 15$OC=0.00252 19$PC=0.000136 22
194PT2 G %IG=0.0256 11
194PT cG E$unweighted average of 162.6 {I3} (1971Vi15), 162.64 {I3} (1996TeZW),
194PT2cG and 162.509 {I25} (2015Do06). Other: 163.6 {I3} (1974HeYW) and 163.4
194PT3cG {I3} for a composite peak. See also 163.4|g from 1961 level
194PT cG RI$weighted average of 0.039 {I3} (1996TeZW), 0.0413 {I13}
194PT2cG (2015Do06), and 0.035 {I6} (1977Vy01). Other: 0.22 {I3} (1974HeYW)
194PT3cG for a doublet
194PT cG M,MR$from L1/L2>5 and K/L1=6.2 {I16} (1971Vi15), and |a(K)=1.23 {I13}
194PT2cG deduced from Ice(K)=1.03 {I10} (1971Vi15) and I|g=0.0407 {I13} here.
194PT3cG Other |a(K)exp: 1.0 {I5} (1970Be30) for a composite peak.
194PT G 171.837 23 0.112 2 M1 1.428 C
194PTS G KC=1.176 17$LC=0.194 3$MC=0.0448 7
194PTS G NC=0.01110 16$OC=0.00200 3$PC=0.0001346 19
194PT2 G %IG=0.0704 23
194PT cG E$weighted average of 171.8 {I3} (1971Vi15), 171.91 {I4} (1996TeZW),
194PT2cG and 171.822 {I18} (2015Do06). Other: 171.8 {I6} (1970Be30, unplaced)
194PT cG RI$from 2015Do06. Others: 0.113 {I10} (1996TeZW), 0.100 {I10}
194PT2cG (1977Vy01), 0.08 {I4} (1970Be30)
194PT cG M,MR$from L1/L2>8.4 and K/L1=7.3 {I14} (1971Vi15) and |a(K)exp=1.12
194PT2cG {I7} deduced from Ice(K)=2.56 {I14} (1971Vi15) and I|g=0.112 {I2} here.
194PT G 211.87 3 0.0082 6 C
194PT2 G %IG=0.0052 4
194PT cG E,RI$from 2015Do06. Other: 212.11 {I25} with I|g=0.009 {I4} (1996TeZW)
194PT G 285.315 14 0.0802 9 (M1+E2) 1.5 +3-2 0.187 18 YC
194PTF G FL=1930.369
194PTS G KC=0.137 16$LC=0.0382 11$MC=0.00930 21
194PTS G NC=0.00229 6$OC=0.000386 12$PC=1.49E-5 19
194PT2 G %IG=0.0504 15
194PT cG E$weighted average of 285.32 {I3} (1996TeZW), 285.312 {I14} (2015Do06),
194PT2cG and 285.34 {I5} (1960Ba17). Others: 285.3 {I7} (1970Be30) and 285.3
194PT3cG {I3} (1971Vi15). Also placed from 1798 and 2398 levels by 1960Ba17.
194PT cG $Level-energy difference=285.160
194PT cG RI$weighted average of 0.09 {I3} (1970Be30), 0.081 {I4} (1996TeZW), and
194PT2cG 0.0801 {I9} (2015Do06)
194PT cG M,MR$from |a(K)exp=0.14 {I5} (1970Be30), 0.09 {I3} (1971Vi15) deduced
194PT2cG from Ice(K)=0.15 {I5} and I|g=0.0802 {I9}. Other |d: +0.4 {I5}
194PT3cG from |g|g(|q) of 1996TeZW. Sign of |d from |g|g(|q)
194PT cG $(285|g)[1601|g](328|g)(|q): A{-2}=-0.04 {I11}, A{-4}=+0.41
194PT2cG {I18}.
194PT cG $Ice(K)=0.225 {I24}, weighted average of 0.24 {I6} (1964Be23), 0.15
194PT2cG {I5} (1971Vi15), and 0.240 {I24} (1960Ba17).
194PT cG M,MR$|a(K)exp=0.137 {I15} deduced from Ice(K)=0.225 {I24} and
194PT2cG I|g=0.0802 {I9} here gives |d(E2/M1)=1.5 {I+3-2} or |d(M2/E1)=0.35
194PT3cG {I3}, with the former consistent with |D|p=+
194PT G 291.52 7 0.038 5 E2(+M1) 2.0 GT 0.130 23 YC
194PTF G FL=1924.282
194PTS G KC=0.086 21$LC=0.0328 14$MC=0.0081 3
194PTS G NC=0.00200 7$OC=0.000329 15$PC=9.0E-6 25
194PT2 G %IG=0.024 3
194PT cG E$weighted average of 291.2 {I3} (1971Vi15), 291.4 {I6} (1996TeZW), and
194PT2cG 291.54 {I7} (2015Do06)
194PT cG $Level-energy difference=291.25
194PT cG RI$weighted average of 0.035 {I7} (1996TeZW) and 0.040 {I5} (2015Do06)
194PT cG M,MR$|a(K)exp=0.078 {I29} deduced from Ice(K)=0.061 {I21} (1971Vi15)
194PT2cG and I|g=0.038 {I5} here. Other |d=+0.8 {I6} from |g|g(|q) for
194PT3cG J(2215)=2, inconsistent with |d from ce data
194PT cG $(291|g)[1342|g](328|g)(|q): A{-2}=-0.13 {I9}, A{-4}=+0.04 {I15}.
194PT G 321.960 18 0.0139 5 N ?
194PTF G FL=1893.574
194PT2 G %IG=0.0087 4
194PT G 398.937 8 0.0192 7 C
194PTF G FL=1816.585
194PT2 G %IG=0.0121 6
194PT cG E,RI$from 2015Do06. Other: 398.95 {I11} with I|g=0.023 {I7} (1996TeZW)
194PT G 418.200 25 0.078 6 [E1] 0.01218 C
194PTS G KC=0.01012 15$LC=0.001584 23$MC=0.000363 5
194PTS G NC=8.93E-5 13$OC=1.575E-5 22$PC=9.53E-7 14
194PT2 G %IG=0.049 4
194PT cG E$weighted average of 418.41 {I12} (1996TeZW) and 418.197 {I14}
194PT2cG (2015Do06). Others: 418.06 {I20} (1970Be30) and 418.1 {I3} (1971Vi15)
194PT3cG for a composite peak
194PT cG RI$from 2015Do06. Others: 0.07 {I3} (1996TeZW); 0.130 {I15} (1971Vi15)
194PT2cG for a composite peak
194PT cG M,MR$|a(K)exp=0.027 {I11} (1971Vi15) for a composite peak gives
194PT2cG |d(E2/M1)>3, but inconsistent with |DJ|p which requires E1
194PT cG $Ice(K)=0.073 {I29} (1971Vi15) for a composite peak,
194PT G 436.90 9 0.0196 6 C
194PT2 G %IG=0.0123 5
194PT cG E$unweighted average of 436.81 {I8} (1996TeZW) and 436.987 {I20}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.022 {I4} (1996TeZW) and 0.0195 {I6} (2015Do06)
194PT G 544.826 17 0.0400 9 (M1(+E2)) 0.7 LT 0.055 7 C
194PTS G KC=0.046 6$LC=0.0075 8$MC=0.00174 17
194PTS G NC=0.00043 4$OC=7.7E-5 8$PC=5.1E-6 7
194PT2 G %IG=0.0251 9
194PT cG E$weighted average of 544.78 {I5} (1996TeZW) and 544.831 {I17}
194PT2cG (2015Do06). Others: 544.4 {I6} (1970Be30), 544.9 {I3} (1971Vi15), and
194PT3cG 544.66 {I20} (1960Ba17)
194PT cG RI$weighted average of 0.041 {I15} (1970Be30), 0.051 {I7} (1996TeZW),
194PT2cG and 0.0399 {I8} (2015Do06). Other: <0.30 (1971Vi15)
194PT cG M,MR$|a(K)exp=0.048 {I8} deduced from Ice(K)=0.039 {I6} and I|g=0.0400
194PT2cG {I9} here gives |d(E2/M1)<0.7 or |d(M2/E1)=0.66 {I9}, with the former
194PT3cG consistent with |DJ|p=+. Other |a(K)exp: 0.044 {I18} (1970Be30)
194PT cG $Ice(K)=0.039 {I6}, unweighted average of 0.037 {I6} (1964Be23),
194PT2cG 0.029 {I5} (1971Vi15), and 0.050 {I5} (1960Ba17)
194PT G 593.37 3 0.465 4 M1+E2 -0.25 18 0.048 4 C
194PTS G KC=0.040 3$LC=0.0064 4$MC=0.00147 8
194PTS G NC=0.000364 20$OC=6.6E-5 4$PC=4.4E-6 4
194PT2 G %IG=0.292 9
194PT cG E$unweighted average of 593.4 {I3} (1971Vi15), 593.319 {I16}
194PT2cG (1996TeZW), and 593.386 {I14} (2015Do06). Others: 593.70 {I5}
194PT3cG (1974HeYW), 593.58 {I15} (1970Be30), and 593.72 {I11} (1960Ba17) for a
194PT4cG composite peak
194PT cG RI$weighted average of 0.470 {I13} (1996TeZW) and 0.465 {I4}
194PT2cG (2015Do06). Others: 0.6 {I3} (1964Be23), 1.07 {I13} (1971Vi15),
194PT3cG 0.746 {I41} (1970Be30), and 0.77 {I5} (1974HeYW) for a composite peak
194PT cG M,MR$|a(K)exp=0.047 {I5} deduced from Ice(K)=0.45 {I5} (1971Vi15) and
194PT2cG I|g=0.465 {I4} here, gives |d(E2/M1)<0.2 or |d(M2/E1)=0.80 {I8}, with
194PT3cG only the former consistent with |d=-0.25 {I18} from |g|g(|q) of
194PT4cG 1996TeZW. Other |a(K)exp: 0.031 {I4} (1970Be30) and 0.037 {I+51-17}
194PT5cG (1964Be23) for a composite peak.
194PT cG $(593|g)[1293|g](328|g)(|q): A{-2}=+0.01 {I10}, A{-4}=+0.14 {I16}.
194PT cG $Other Ice(K): 0.57 {I6} (1960Ba17) and 0.47 {I5} (1964Be23) for a
194PT2cG composite peak
194PT G 668.247 17 0.175 2 M1 0.0366 C
194PTS G KC=0.0304 5$LC=0.00484 7$MC=0.001114 16
194PTS G NC=0.000276 4$OC=4.96E-5 7$PC=3.39E-6 5
194PT2 G %IG=0.110 3
194PT cG E$weighted average of 668.16 {I20} (1970Be30), 668.27 {I10} (1974HeYW),
194PT2cG 668.247 {I17} (1996TeZW), 668.240 {I14} (2015Do06), and 668.56 {I10}
194PT3cG (1960Ba17)
194PT cG RI$weighted average of 0.182 {I11} (1970Be30), 0.180 {I5} (1996TeZW),
194PT2cG and 0.174 {I2} (2015Do06). Other: 0.17 {I2} (1974HeYW)
194PT cG M$|a(K)exp=0.029 {I3} (1970Be30), and 0.032 {I3} deduced from
194PT2cG Ice(K)=0.0114 {I10} and I|g=0.175 {I2} here, give |d<0.3, and |DJ|p
194PT3cG requires pure dipole
194PT cG $Ice(K)=0.114 {I10}, weighted average of 0.11 {I1} (1964Be23) and 0.120
194PT2cG {I12} (1960Ba17)
194PT G 703.525 14 0.654 6 M1+E2 +0.24 6 0.0310 8 C
194PTS G KC=0.0256 7$LC=0.00410 9$MC=0.000945 20
194PTS G NC=0.000234 5$OC=4.21E-5 9$PC=2.86E-6 7
194PT2 G %IG=0.411 12
194PT cG E$weighted average of 703.42 {I15} (1970Be30), 703.6 {I3} (1971Vi15),
194PT2cG 703.56 {I4} (1996TeZW), and 703.521 {I14} (2015Do06). Others: 703.54
194PT3cG {I5} (1974HeYW) and 703.61 {I10} (1960Ba17) for a composite peak
194PT cG RI$from 2015Do06. Others: 0.61 {I12} (1996TeZW), 0.71 {I6} (1970Be30),
194PT2cG 0.773 {I10} (1971Vi15) and 0.66 {I6} (1974HeYW); 1.5 {I8} (1964Be23)
194PT3cG for a composite peak
194PT cG M,MR$|a(K)exp=0.0254 {I8} deduced from Ice(K)=0.34 {I1} and I|g=0.654
194PT2cG {I6} here, gives |d(E2/M1)=0.27 {I+9-13} or |d(M2/E1)=0.71 {I2}, with
194PT3cG the former consistent with |d=+0.24 {I6} (or +1.46 {I19}) from
194PT4cG |g|g(|q) of 1996TeZW. Other |a(K)exp=0.0236 {I22} (1970Be30)
194PT cG $(703|g)(1183|g)(|q): A{-2}=-0.48 {I5}, A{-4}=-0.03 {I9}.
194PT cG $Ice(K)=0.34 {I1}, from 1964Be23. Others: 0.34 {I3} (1971Vi15) and 0.40
194PT2cG {I4} (1960Ba17).
194PT G 736.249 14 0.201 12M1 0.0285 C
194PTS G KC=0.0237 4$LC=0.00376 6$MC=0.000865 13
194PTS G NC=0.000214 3$OC=3.86E-5 6$PC=2.64E-6 4
194PT2 G %IG=0.126 8
194PT cG E$weighted average of 736.240 {I22} (1996TeZW) and 736.253 {I14}
194PT2cG (2015Do06). Others: 735.92 {I20} (1970Be30), 736.2 {I3} (1971Vi15),
194PT3cG 736.23 {I15} (1974HeYW), and 736.45 {I15} (1960Ba17)
194PT cG RI$unweighted average of 0.208 {I16} (1970Be30), 0.233 {I11}
194PT2cG (1971Vi15), 0.22 {I3} (1974HeYW), 0.171 {I5} (1996TeZW), and 0.174 {I2}
194PT3cG (2015Do06)
194PT cG M$|a(K)exp=0.026 {I3} (1971Vi15) and 0.0235 {I24} (1970Be30) gives
194PT2cG |d(E2/M1)<0.3, but this transition feeding 0+ requires pure dipole.
194PT dG E$also placed from 2357 level by 1960Ba17.
194PT cG $Ice(K)=0.108 {I8}, weighted average of 0.100 {I6} (1964Be23), 0.125
194PT2cG {I11} (1971Vi15), and 0.120 {I12} (1960Ba17).
194PT G 948.323 9 3.65 3 M1 0.01497 C
194PTS G KC=0.01243 18$LC=0.00196 3$MC=0.000450 7
194PTS G NC=0.0001114 16$OC=2.01E-5 3$PC=1.378E-6 20
194PT2 G %IG=2.29 7
194PT cG E$weighted average of 948.31 {I15} (1970Be30), 948.2 {I2} (1971Vi15),
194PT2cG 948.29 {I4} (1974HeYW), 948.310 {I9} (1996TeZW), 948.341 {I10}
194PT3cG (2015Do06), and 948.40 {I12} (1960Ba17)
194PT cG RI$weighted average of 3.7 {I3} (1964Be23), 3.71 {I19} (1970Be30), 3.96
194PT2cG {I19} (1971Vi15), 3.53 {I20} (1974HeYW), 3.76 {I7} (1996TeZW), and 3.62
194PT3cG {I3} (2015Do06)
194PT cG M$|a(K)exp=0.0118 {I+20-18} (1971Vi15), 0.0127 {I7} (1970Be30),
194PT2cG 0.0126 {I+23-19} (1964Be23), and L1/L2=11.2 {I18}, L1/L3>72 (1970Ag05)
194PT3cG give |d(E2/M1)<0.5, but this transition feeding 0+ requires pure dipole
194PT cG $Ice(K)=0.964 {I10}, weighted average of 0.963 {I10} (1964Be23), 0.96
194PT2cG {I9} (1971Vi15), and 1.10 {I11} (1960Ba17).
194PT G 1593.530 20 1.22 2 (M1+E2) 0.74 8 0.0035611 C
194PTS G KC=0.00285 9$LC=0.000445 13$MC=0.000102 3
194PTS G NC=2.53E-5 8$OC=4.55E-6 14$PC=3.10E-7 10$IPC=0.000131 4
194PT2 G %IG=0.767 25
194PT cG E$weighted average of 1593.63 {I7} (1996TeZW) and 1593.526 {I14}
194PT2cG (2015Do06). Others: 1592.9 {I3} (1970Be30), 1593.5 {I3} (1971Vi15),
194PT3cG 1592.9 {I1} (1974HeYW), and 1592.9 {I4} (1960Ba17)
194PT cG RI$weighted average of 1.19 {I8} (1996TeZW) and 1.22 {I2} (2015Do06).
194PT2cG Others: 2.7 {I8} (1970Be30), 6.0 {I6} (1971Vi15), and 2.8 {I3}
194PT3cG (1974HeYW) for a composite peak
194PT cG M$|a(K)exp=0.00285 {I6} deduced from Ice(K)=0.0712 {I7} (1971Vi15) and
194PT2cG I|g=1.22 {I2} here gives |d(E2/M1)=0.74 {I8} and also
194PT3cG |d(M2/E1)=0.64 {I2}; |a(K)exp=0.0031 {I9} (1970Be30) and >0.0033
194PT4cG (1964Be23) for a composite peak {I+27-24} consistent with M1.
194PT5cG See also comments for 1592|g from 2214 level.
194PT cG $Other Ice(K): 0.170 {I15} (1964Be23) and 0.200 {I20} (1960Ba17)
194PT2cG for a composite peak
194PT G 1887.030 23 3.3 4 (M1+E2) +0.75 24 0.0026018 C
194PTS G KC=0.00192 14$LC=0.000297 21$MC=6.8E-5 5
194PTS G NC=1.68E-5 12$OC=3.04E-6 22$PC=2.08E-7 16$IPC=0.000289 18
194PT2 G %IG=2.1 3
194PT cG E$weighted average of 1887.0 {I4} (1971Vi15), 1886.89 {I6}
194PT2cG (1996TeZW), and 1887.037 {I14} (2015Do06). Others: 1886.50 {I5}
194PT3cG (1974HeYW), 1886.8 {I3} (1960Ba17), 1886.50 {I15} (1970Be30) for
194PT4cG a composite peak
194PT cG RI$unweighted average of 3.7 {I3} (1996TeZW), and 2.84 {I4}
194PT2cG (2015Do06). Others: 5.7 {I9} (1971Vi15), 5.3 {I3} (1974HeYW), 5.84
194PT3cG {I25} (1964Be23), and 5.4 {I3} (1970Be30) for a composite peak
194PT cG M$|a(K)exp=0.00167 {I25} deduced from Ice(K)=0.113 {I12} (1971Vi15)
194PT2cG and I|g=3.3 {I4} here; |a(K)exp: 0.00207 {I12} (1970Be30) and 0.00192
194PT3cG {I+27-24} for a composite peak. See also comments for 1886|g from
194PT4cG 2214 level
194PT cG MR$from |g|g(|q) of 1996TeZW. Other: 1.4 {I+29-6} from ce data above
194PT cG $(1887|g)(328|g)(|q): A{-2}=-0.66 {I7}, A{-4}=-0.29 {I12}.
194PT cG $Other Ice(K): 0.230 {I4} (1964Be23) and 0.28 {I3} (1960Ba17) for
194PT2cG for a composite peak
194PT G 2215.509 16 0.267 5 M1 0.00235
194PTS G KC=0.001500 21$LC=0.000231 4$MC=5.28E-5 8
194PTS G NC=1.307E-5 19$OC=2.36E-6 4$PC=1.642E-7 23$IPC=0.000546 8
194PT2 G %IG=0.168 6
194PT cG E$weighted average of 2215.39 {I21} (1970Be30), 2215.5 {I4} (1971Vi15),
194PT2cG 2215.15 {I15} (1974HeYW), 2215.47 {I6} (1996TeZW), 2215.515 {I14}
194PT3cG (2015Do06), and 2215.6 {I7} (1960Ba17)
194PT cG RI$weighted average of 0.292 {I19} (1964Be23), 0.282 {I22} (1970Be30),
194PT2cG 0.289 {I19} (1971Vi15), 0.32 {I4} (1974HeYW), 0.285 {I18} (1996TeZW),
194PT3cG and 0.263 {I4} (2015Do06)
194PT cG M$|a(K)exp=0.00179 {I23} (1964Be23), 0.00185 {I23} (1970Be30),
194PT2cG 0.0018 {I3} (1971Vi15).
194PT L 2239.635 8 (2)-
194PT E 0.454 16 7.673 17 0.454 16
194PTS E CK=0.7333 9$CL=0.1992 6$CM+=0.06749 24
194PT G 442.225 19 0.0125 4 N ?
194PT2 G %IG=0.0079 3
194PT G 807.119 21 0.025 8 C
194PT2 G %IG=0.016 5
194PT cG E$from 2015Do06. Other: 807.1 {I3} (1996TeZW)
194PT cG RI$unweighted average of 0.033 {I8} (1996TeZW) and 0.0175 {I5}
194PT2cG (2015Do06)
194PT G 1316.857 14 0.117 1 C
194PT2 G %IG=0.0735 21
194PT cG E$weighted average of 1316.82 {I7} (1996TeZW) and 1316.858 {I14}
194PT2cG (2015Do06). Other: 1317.3 {I13} (1970Be30)
194PT cG RI$from 2015Do06. Others: 0.13 {I5} (1971Vi15), 0.118 {I8}
194PT2cG (1996TeZW), 0.08 {I4} (1970Be30)
194PT G 1617.604 14 0.365 4 E1 1.18E-3 C
194PTS G KC=0.000773 11$LC=0.0001110 16$MC=2.52E-5 4
194PTS G NC=6.21E-6 9$OC=1.118E-6 16$PC=7.66E-8 11$IPC=0.000261 4
194PT2 G %IG=0.229 7
194PT cG E$weighted average of 1617.62 {I3} (1996TeZW) and 1617.601 {I14}
194PT2cG (2015Do06). Others: 1617.6 {I6} (1970Be30), 1617.73 {I15} (1974HeYW),
194PT3cG and 1617.8 {I6} (1960Ba17)
194PT cG RI$weighted average of 0.34 {I5} (1970Be30), 0.42 {I3} (1971Vi15), 0.34
194PT2cG {I4} (1974HeYW), 0.368 {I12} (1996TeZW), and 0.364 {I4} (2015Do06)
194PT cG M$|a(K)exp=0.00081 {I12} (1970Be30). |d=-0.5 {I18} or -2.1 {I24} from
194PT2cG |g|g(|q) (1996TeZW) consistent with ce data.
194PT cG $(1618|g)(293|g)(|q): A{-2}=-0.10 {I7}, A{-4}=-0.03 {I11}.
194PT cG $(1618|g)[293|g](328|g)(|q): A{-2}=-0.10 {I6}, A{-4}=+0.42 {I11}.
194PT cG $Ice(K)=0.0065 {I9}, unweighted average of 0.0056 {I1} (1964Be23) and
194PT2cG 0.0073 {I7} (1960Ba17).
194PT dG $|a(K)exp=0.00087 {I12}, from Ice(K)=0.0065 {I9} and I|g=0.365 {I4}
194PT2dG here
194PT G 1911.154 14 0.201 2 E1 1.17E-3 C
194PTS G KC=0.000587 9$LC=8.38E-5 12$MC=1.90E-5 3
194PTS G NC=4.69E-6 7$OC=8.44E-7 12$PC=5.83E-8 9$IPC=0.000476 7
194PT2 G %IG=0.126 4
194PT cG E$weighted average of 1911.1 {I6} (1970Be30), 1911.30 {I15} (1974HeYW),
194PT2cG 1911.08 {I4} (1996TeZW), 1911.162 {I14} (2015Do06), and 1911.1 {I5}
194PT3cG (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.209 {I24} (1970Be30), 0.174 {I16}
194PT2cG (1971Vi15), 0.21 {I3} (1974HeYW), and 0.209 {I10} (1996TeZW)
194PT cG M$|a(K)exp=0.00065 {I23} (1970Be30).
194PT cG $Ice(K)=0.0028 {I9} (1964Be23)
194PT L 2250.665 21 (1,2+) ?
194PT cL E$level suggested by 2015Do06.
194PT cL J$2015Do06 analyze coincident summing and suggest that 0+ for this
194PT2cL state is unlikely. The ground-state transition suggests J=1,2+.
194PT E 0.099 4 8.294 20 0.099 4 ?
194PTS E CK=0.7289 9$CL=0.2023 7$CM+=0.0688 3
194PT G 1922.171 22 0.156 3 ?
194PT2 G %IG=0.098 3
194PT cG E,RI$from 2015Do06 only
194PT G 2250.73 6 0.0012 1 ?
194PT2 G %IG=7.5E-4 7
194PT cG E,RI$from 2015Do06 only
194PT L 2287.375 10 (1+,2+)
194PT E 0.218 10 7.803 22 0.218 10
194PTS E CK=0.7103 13$CL=0.2157 10$CM+=0.0741 4
194PT G 173.3 3 0.008 3 [M1] 1.395
194PTS G KC=1.149 17$LC=0.189 3$MC=0.0438 7
194PTS G NC=0.01084 16$OC=0.00195 3$PC=0.0001314 20
194PT2 G %IG=0.0050 19
194PT cG E$from ce data (1971Vi15)
194PT cG RI$deduced from Ice(K)=0.20 {I7} (1971Vi15) and assigned Mult=M1
194PT G 243.65 3 0.0123 7 C
194PT2 G %IG=0.0077 5
194PT cG E$weighted average of 243.66 {I17} (1996TeZW) and 243.65 {I3}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.015 {I5} (1996TeZW) and 0.0122 {I7} (2015Do06)
194PT G 490.030 22 0.0113 4 N ?
194PT2 G %IG=0.0071 3
194PT G 1665.321 18 0.0464 6 C
194PT2 G %IG=0.0292 9
194PT cG E$weighted average of 1665.42 {I13} (1996TeZW) and 1665.319 {I18}
194PT2cG (2015Do06)
194PT cG RI$from 2015Do06. Other: 0.045 {I7} (1996TeZW)
194PT G 1958.898 14 0.272 3 (M1(+E2)) 0.6 LT 0.0026814 C
194PTS G KC=0.00193 11$LC=0.000298 16$MC=6.8E-5 4
194PTS G NC=1.69E-5 9$OC=3.05E-6 17$PC=2.11E-7 13$IPC=0.000359 18
194PT2 G %IG=0.171 5
194PT cG E$weighted average of 1958.87 {I3} (1996TeZW) and 1958.904 {I14}
194PT2cG (2015Do06). Others: 1958.9 {I3} (1970Be30), 1958.74 {I20} (1974HeYW),
194PT3cG and 1959.7 {I6} (1960Ba17)
194PT cG RI$weighted average of 0.277 {I13} (1971Vi15), 0.288 {I13} (1996TeZW),
194PT2cG and 0.271 {I3} (2015Do06). Others: 0.30 {I13} (1964Be23), 0.27 {I3}
194PT3cG (1970Be30), and 0.26 {I4} (1974HeYW)
194PT cG M$|a(K)exp=0.0018 {I4} (1970Be30), 0.0016 {I+20-8} (1964Be23).
194PT cG $Ice(K)=0.0115 {I12}, weighted average of 0.010 {I2} (1964Be23) and
194PT2cG 0.0120 {I12} (1960Ba17).
194PT cG M,MR$|a(K)exp=0.00206 {I22} deduced from Ice(K)=0.0115 {I12} and
194PT2cG I|g=0.272 {I3} here, gives |d(E2/M1)<0.6 or |d(M2/E1)=0.75 {I9},
194PT3cG with the former more likely
194PT G 2287.28 5 0.0010 2 n
194PT2 G %IG=6.3E-4 13
194PT L 2298.160 8 1+
194PT E 0.693 23 7.252 18 0.693 23
194PTS E CK=0.7033 15$CL=0.2206 11$CM+=0.0761 5
194PT G 189.17 6 0.0066 10M1 1.091
194PTS G KC=0.899 13$LC=0.1480 21$MC=0.0342 5
194PTS G NC=0.00846 12$OC=0.001523 22$PC=0.0001027 15
194PT2 G %IG=0.0041 6
194PT cG E,RI$from 2015Do06. Other: 189.1 {I3} from ce data with I|g=0.0063
194PT2cG {I12} deduced from Ice(K)=0.120 {I24} (1971Vi15).
194PT dG $Suggested (1971Vi15) placement with 811 level is incorrect
194PT2dG since this |g not seen in {+194}Ir |b{+-} (171 d) and in in-beam |g-ray
194PT3dG reactions where this level is strongly populated.
194PT cG M$|a(K)exp=0.89 {I+37-27} deduced from Ice(K)=0.120 {I24} (1971Vi15)
194PT2cG and I|g=0.0066 {I10} (2015Do06)
194PT G 500.737 24 0.0103 5 C
194PT2 G %IG=0.0065 4
194PT cG E,RI$from 2015Do06. Other: 500.72 {I19} with I|g=0.012 {I3} (1996TeZW)
194PT G 627.59 3 0.0075 5 C
194PT2 G %IG=0.0047 4
194PT cG E$from 2015Do06. Other: 627.7 {I6} (1996TeZW)
194PT cG RI$weighted average of 0.0061 {I17} (1996TeZW) and 0.0076 {I5}
194PT2cG (2015Do06)
194PT G 675.943 16 0.0707 7 M1(+E2) 0.4 LT 0.0340 17 C
194PTS G KC=0.0281 15$LC=0.00452 19$MC=0.00104 5
194PTS G NC=0.000257 11$OC=4.63E-5 20$PC=3.13E-6 17
194PT2 G %IG=0.0444 13
194PT cG E$weighted average of 676.2 {I6} (1970Be30), 675.9 {I3} (1971Vi15),
194PT2cG 675.75 {I11} (1996TeZW), 675.947 {I16} (2015Do06), and 676.1 {I3}
194PT3cG (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.4 {I4} (1964Be23), 0.10 {I3} (1970Be30),
194PT2cG and 0.079 {I20} (1996TeZW)
194PT cG M,MR$|a(K)exp=0.019 {I7} (1970Be30), and 0.034 {I6} deduced from
194PT2cG Ice(K)=0.049 {I8} and I|g=0.0707 {I7} here.
194PT cG $Ice(K)=0.049 {I8}, unweighted average of 0.037 {I7} (1964Be23),
194PT2cG 0.064 {I7} (1971Vi15), and 0.046 {I5} (1960Ba17)
194PT cG M,MR$|a(K)exp=0.034 {I6} deduced from Ice(K)=0.049 {I8} and I|g=0.0707
194PT2cG {I7} here, gives |d(E2/M1)<0.4 or |d(M2/E1)=0.83 {I+15-13}, with
194PT3cG the former consistent with |D|p=+. Other |a(K)exp: 0.019 {I7}
194PT4cG (1970Be30)
194PT G 786.07 5 0.0062 4 N ?
194PT2 G %IG=0.0039 3
194PT G 818.856 18 0.0543 7 M1 0.0217 C
194PTS G KC=0.0180 3$LC=0.00286 4$MC=0.000657 10
194PTS G NC=0.0001625 23$OC=2.93E-5 5$PC=2.01E-6 3
194PT2 G %IG=0.0341 10
194PT cG E$weighted average of 818.87 {I5} (1996TeZW) and 818.854 {I18}
194PT2cG (2015Do06). Others: 818.9 {I2} (1971Vi15) and 818.7 {I3} (1960Ba17)
194PT cG RI$weighted average of 0.056 {I3} (1996TeZW) and 0.0542 {I7}
194PT2cG (2015Do06). Other: 0.050 {I10} (1977Vy01)
194PT cG M$|a(K)exp=0.0200 {I22} deduced from Ice(K)=0.0223 {I24} and
194PT2cG I|g=0.0543 {I7} here gives |d(E2/M1)<0.3 or |d(M2/E1)=0.83 {I9},
194PT3cG with only the former consistent with this transition feeding 0+, which
194PT4cG requires pure dipole
194PT cG $Ice(K)=0.0223 {I24}, weighted average of 0.021 {I3} (1964Be23),
194PT2cG 0.020 {I4} (1971Vi15), and 0.0240 {I24} (1960Ba17)
194PT G 1030.997 23 0.0173 5 M1 0.01212 C
194PTS G KC=0.01006 14$LC=0.001582 23$MC=0.000363 5
194PTS G NC=8.99E-5 13$OC=1.622E-5 23$PC=1.114E-6 16
194PT2 G %IG=0.0109 4
194PT cG E$from 2015Do06. Others: 1031.0 {I3} (1996TeZW) and 1030.9 {I4}
194PT2cG (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.017 {I5} (1996TeZW), 0.030 {I10} (1977Vy01)
194PT cG M$|a(K)exp=0.0135 {I12} deduced from Ice(K)=0.0048 {I4} and
194PT2cG I|g=0.0173 {I5} here gives |d(E2/M1)<0.2 or |d(M2/E1)=1.05 {I12},
194PT3cG with only the former consistent with this transition feeding 0+, which
194PT4cG requires pure dipole
194PT cG $Ice(K)=0.0048 {I4}, weighted average of 0.0042 {I7} (1964Be23)
194PT2cG and 0.0051 {I5} (1960Ba17)
194PT G 1676.111 21 0.121 1 (M1) 0.00379 C
194PTS G KC=0.00299 5$LC=0.000463 7$MC=0.0001062 15
194PTS G NC=2.63E-5 4$OC=4.74E-6 7$PC=3.29E-7 5$IPC=0.000196 3
194PT2 G %IG=0.0760 22
194PT cG E$from 2015Do06. Others: 1675.9 {I3} (1996TeZW); 1675.9 {I6}
194PT2cG (1970Be30), 1675.7 {I3} (1974HeYW), and 1675.9 {I5} (1960Ba17) for a
194PT3cG composite peak
194PT cG RI$from 2015Do06. Others: 0.13 {I7} (1996TeZW); 0.17 {I5} (1970Be30),
194PT2cG 0.226 {I25} (1971Vi15), and 0.27 {I4} (1974HeYW) for a composite peak
194PT cG M$|a(K)exp=0.0048 {I14} (1970Be30) for a composite peak
194PT cG $Ice(K)=0.0195 {I25}, unweighted average of 0.0170 {I10} (1964Be23) and
194PT2cG 0.0220 {I22} (1960Ba17), for a composite peak.
194PT G 1969.680 14 0.750 7 M1+E2 -0.35 4 0.002685 C
194PTS G KC=0.00192 4$LC=0.000297 5$MC=6.81E-5 12
194PTS G NC=1.68E-5 3$OC=3.04E-6 5$PC=2.10E-7 4$IPC=0.000368 6
194PT2 G %IG=0.471 14
194PT cG E$weighted average of 1969.65 {I7} (1974HeYW), 1969.64 {I3} (1996TeZW),
194PT2cG and 1969.690 {I14} (2015Do06). Others: 1969.63 {I20} (1970Be30) and
194PT3cG 1970.1 {I3} (1960Ba17)
194PT cG RI$from 2015Do06. Others: 0.68 {I9} (1964Be23), 0.72 {I4} (1970Be30),
194PT2cG 0.742 {I25} (1971Vi15), 0.71 {I7} (1974HeYW), and 0.80 {I3} (1996TeZW)
194PT cG M,MR$|a(K)exp=0.00184 {I13} deduced from Ice(K)=0.0283 {I20} and
194PT2cG I|g=0.750 {I7} here, gives |d(E2/M1)=0.54 {I+29-33} or
194PT3cG |d(M2/E1)=0.67 {I5}, with only the former consistent with |d=-0.35
194PT4cG {I4} from |g|g(|q) of 1996TeZW. Other |a(K)exp: 0.0019 {I+6-5}
194PT5cG (1964Be23), 0.00184 {I18} (1970Be30), and 0.0017 {I5} (1971Vi15).
194PT cG $(1970|g)(328|g)(|q): A{-2}=+0.14 {I5}, A{-4}=-0.09 {I8}.
194PT cG $Ice(K)=0.0283 {I20}, weighted average of 0.0271 {I20} (1964Be23),
194PT2cG 0.026 {I7} (1971Vi15), and 0.034 {I4} (1960Ba17).
194PT G 2298.171 17 0.0426 6 M1 0.00224
194PTS G KC=0.001371 20$LC=0.000211 3$MC=4.82E-5 7
194PTS G NC=1.193E-5 17$OC=2.16E-6 3$PC=1.500E-7 21$IPC=0.000601 9
194PT2 G %IG=0.0268 8
194PT cG E$weighted average of 2297.9 {I6} (1970Be30), 2298.2 {I3} (1974HeYW),
194PT2cG 2298.41 {I14} (1996TeZW), 2298.167 {I17} (2015Do06), and 2298.7 {I10}
194PT3cG (1960Ba17)
194PT cG RI$weighted average of 0.0453 {I25} (1971Vi15), 0.0424 {I5}
194PT2cG (2015Do06), 0.046 {I8} (1970Be30), and 0.056 {I8} (1996TeZW). Other:
194PT3cG 0.720 {I15} (1974HeYW) is discrepant.
194PT cG M$|a(K)exp=0.00215 {I23} deduced from Ice(K)=0.00188 {I20} and
194PT2cG I|g=0.0426 {I6} here. Other |a(K)exp: 0.0017 {I4} (1970Be30)
194PT cG $Ice(K)=0.00188 {I20}, weighted average of 0.0016 {I3} (1964Be23)
194PT2cG and 0.00200 {I20} (1960Ba17)
194PT L 2311.879 9 2+
194PT E 0.427 15 7.397 19 0.427 15
194PTS E CK=0.6931 18$CL=0.2279 13$CM+=0.0790 5
194PT G 197.82 7 0.0071 16M1 0.963
194PTS G KC=0.793 12$LC=0.1305 19$MC=0.0302 5
194PTS G NC=0.00746 11$OC=0.001343 19$PC=9.06E-5 13
194PT2 G %IG=0.0045 10
194PT cG E$weighted average of 197.8 {I3} (1971Vi15), 198.16 {I20} (1996TeZW),
194PT2cG and 197.79 {I6} (2015Do06)
194PT cG RI$weighted average of 0.009 {I5} (1996TeZW) and 0.0069 {I16}
194PT2cG (2015Do06)
194PT cG M$|a(K)exp=1.3 {I+7-4} deduced from Ice(K)=0.19 {I3} (1971Vi15) and
194PT2cG I|g=0.0071 {I16} here
194PT G 387.65 5 0.0051 5 N ?
194PT2 G %IG=0.0032 3
194PT G 689.61 3 0.0082 3 N ?
194PT2 G %IG=0.00515 24
194PT cG $Level-energy difference=689.68
194PT G 799.857 26 0.0090 4 N ?
194PT2 G %IG=0.0057 3
194PT G 1081.8 19 0.015 LT ?
194PT2 G %IG LT 0.0094
194PT cG E$placement from 1970Be30 and 1971Vi15 only; this transition could be
194PT2cG the same transition in 1996TeZW and 2015Do06 which depopulates the 2003
194PT3cG level. See 1081|g from 2003 level.
194PT cG RI$limit from 2015Do06. Others: 0.05 {I3} (1970Be30), <0.15 (1971Vi15)
194PT cG $|a(K)exp=0.004 {I3} (1970Be30)
194PT G 1388.93 19 0.0267 6 C
194PT2 G %IG=0.0168 6
194PT cG E$unweighted average of 1388.74 {I19} (1996TeZW) and 1389.119 {I18}
194PT2cG (2015Do06)
194PT cG RI$from 2015Do06. Other: 0.026 {I7} (1996TeZW)
194PT G 1500.66 13 0.048 6 (E2) 0.00259 C
194PTS G KC=0.00208 3$LC=0.000336 5$MC=7.75E-5 11
194PTS G NC=1.91E-5 3$OC=3.41E-6 5$PC=2.18E-7 3$IPC=6.64E-5 10
194PT2 G %IG=0.030 4
194PT cG E$unweighted average of 1500.5 {I3} (1971Vi15), 1500.92 {I8}
194PT2cG (1996TeZW), and 1500.573 {I21} (2015Do06)
194PT cG RI$unweighted average of 0.054 {I3} (1996TeZW) and 0.0421 {I5}
194PT2cG (2015Do06). Other: 0.63 {I3} (1971Vi15) is discrepant, and it is
194PT3cG most likely that it should read as 0.06 3 instead of 0.63 3.
194PT cG M$|a(K)exp=0.0041 {I12} deduced from Ice(K)=0.0040 {I10} (1971Vi15)
194PT2cG and I|g=0.048 {I6} here, gives M1,E2, but |DJ|p=2+ requires E2.
194PT G 1689.845 14 0.212 3 (M1(+E2)) 0.4 LT 0.0036212 C
194PTS G KC=0.00284 10$LC=0.000441 15$MC=0.000101 4
194PTS G NC=2.50E-5 9$OC=4.51E-6 15$PC=3.12E-7 11$IPC=0.000199 6
194PT2 G %IG=0.133 4
194PT cG E$weighted average of 1689.87 {I3} (1996TeZW) and 1689.839 {I14}
194PT2cG (2015Do06). Others: 1690.1 {I6} (1970Be30), 1689.7 {I2} (1974HeYW), and
194PT3cG 1690.2 {I4} (1960Ba17)
194PT cG RI$weighted average of 0.20 {I6} (1970Be30), 0.28 {I4} (1971Vi15), 0.28
194PT2cG {I5} (1974HeYW), 0.202 {I7} (1996TeZW), and 0.212 {I2} (2015Do06)
194PT cG M,MR$|a(K)exp=0.0036 {I5} deduced from Ice(K)=0.0158 {I22} and
194PT2cG I|g=0.213 {I3} here, give |d(E2/M1)<0.4 or |d(M2/E1)=0.95 {I+17-15},
194PT3cG with the former consistent with |D|p=+. Other |a(K)exp: 0.0034 {I11}
194PT4cG (1970Be30)
194PT cG $Ice(K)=0.0158 {I22}, unweighted average of 0.0136 {I10} (1964Be23)
194PT2cG and 0.0180 {I18} (1960Ba17)
194PT G 1983.411 17 0.0593 6 M1+E2+E0 0.026 4 C
194PT2 G %IG=0.0373 11
194PT cG E$from 2015Do06. Others: 1984.1 {I6} (1970Be30), 1983.3 {I4}
194PT2cG (1971Vi15), 1983.39 {I7} (1996TeZW), and 1983.9 {I4} (1960Ba17)
194PT cG RI$weighted average of 0.06 {I2} (1970Be30), 0.060 {I5} (1971Vi15),
194PT2cG 0.070 {I7} (1996TeZW), and 0.0592 {I6} (2015Do06). Other: 0.21 {I11}
194PT3cG (1964Be23)
194PT cG M$|a(K)exp=0.0198 {I33} deduced from Ice(K)=0.024 {I4} and I|g=0.0593
194PT2cG {I6} here. This large value can be explained only by the presence of
194PT3cG a strong E0 component. Other |a(K)exp: 0.0034 {I11} (1970Be30)
194PT cG CC$from 1.33(|a(K)exp), where |a(K)exp=0.0198 {I33}
194PT cG $Ice(K)=0.024 {I4}, unweighted average of 0.0225 {I20} (1964Be23),
194PT2cG 0.018 {I3} (1971Vi15), and 0.030 {I3} (1960Ba17)
194PT G 2311.856 14 0.287 4 (E2) 1.56E-3
194PTS G KC=0.000954 14$LC=0.0001444 21$MC=3.30E-5 5
194PTS G NC=8.16E-6 12$OC=1.466E-6 21$PC=9.91E-8 14$IPC=0.000415 6
194PT2 G %IG=0.180 6
194PT cG E$from 2015Do06. Others: 2311.72 {I21} (1970Be30), 2312.01 {I15}
194PT2cG (1974HeYW), 2311.86 {I8} (1996TeZW), and 2312.7 {I8} (1960Ba17)
194PT cG RI$weighted average of 0.311 {I25} (1964Be23), 0.278 {I16} (1970Be30),
194PT2cG 0.289 {I19} (1971Vi15), 0.308 {I20} (1996TeZW), and 0.286 {I4}
194PT3cG (2015Do06). Other: 0.28 {I3} (1974HeYW)
194PT cG M$|a(K)exp=0.00122 {I16} deduced from Ice(K)=0.0072 {I9} and
194PT2cG I|g=0.287 {I4} here, gives |d(E2/M1)<1.7 or |d(M2/E1)=0.64
194PT3cG {I9}; but |DJ|p requires E2. Other |a(K)exp: 0.00110 {I9} (1970Be30)
194PT cG $Ice(K)=0.0072 {I9}, unweighted average of 0.0063 {I3} (1964Be23) and
194PT2cG 0.0080 {I8} (1960Ba17)
194PT L 2356.065 14 0+
194PT E 0.31 5 7.28 8 0.31 5
194PTS E CK=0.645 4$CL=0.2625 23$CM+=0.0930 10
194PT G 69.6 3 0.0039 13 3.52 A
194PTF G FL=2287.375
194PTF G FLAG=XY
194PTS G LC=2.61 4$MC=0.604 9
194PTS G NC=0.1494 22$OC=0.0269 4$PC=0.00181 3
194PT2 G %IG=0.0025 8
194PT cG $Level-energy difference=68.7
194PT cG RI$deduced from Ice(L1)=0.19 {I6} (1971Vi15) and calculated |a(L1)=2.35
194PT2cG from BrIcc assuming Mult=M1. I|g=0.041 {I13} if Mult=E2.
194PT G 140.514 18 0.0860 19M1 2.52 C
194PTS G KC=2.08 3$LC=0.344 5$MC=0.0794 12
194PTS G NC=0.0197 3$OC=0.00354 5$PC=0.000238 4
194PT2 G %IG=0.0540 19
194PT cG E$weighted average of 140.5 {I3} (1971Vi15), 140.547 {I23} (1996TeZW),
194PT2cG and 140.494 {I18} (2015Do06)
194PT cG RI$weighted average of 0.079 {I5} (1996TeZW), 0.0865 {I17}
194PT2cG (2015Do06), and 0.095 {I10} (1977Vy01)
194PT cG M$L1/L2=11.3 {I33}, K/L1=6 {I2}, and |a(K)exp=3.4 {I6} deduced from
194PT2cG Ice(K)=6.0 {I10} (1971Vi15) and I|g=0.0860 {I19} here
194PT G 431.61 6 0.0040 4 N ?
194PT2 G %IG=0.0025 3
194PT cG $Level-energy difference=431.78
194PT G 843.89 20 0.002 LT 0.00779 A ?
194PTF G FLAG=X
194PTF G FL=1512.002
194PTS G KC= 0.00619 $LC= 0.00120
194PT2 G %IG LT 0.0013
194PT cG E$seen in ce data only (1960Ba17, 1964Be23, 1971Vi15); placement by
194PT2cG 1971Vi15
194PT cG RI$not seen and only a limit given in 2015Do06. Other: 0.21 {I4}
194PT2cG deduced from Ice(K)=0.027 {I4} (1971Vi15) and assumed Mult=E2; 0.078
194PT3cG {I12} if Mult=M1. The possibility of its being a higher multipolarity
194PT5cG or an E0 transition still exists, however.
194PT cG $Ice(K)=0.013 {I4} (1964Be23), 0.0160 {I16} (1960Ba17), 0.027 {I4}
194PT2cG (1971Vi15)
194PT G 1091.6 5 ?
194PTF G FL=1267.198
194PT cG E$from 1960Ba17 only, with Ice(K)=0.0040 {I4}. Very poor-fit, with
194PT2cG level-energy difference=1088.9
194PT G 1735.5 3 0.31 LT ?
194PTF G FL=622.023
194PT2 G %IG LT 0.20
194PT cG E,RI$placement from 1960Ba17 and 1964Be23 only. See also the 1735
194PT2cG transition from 2064 level
194PT cG $Level-energy difference=1734.0
194PT G 2027.608 20 0.0077 2 N ?
194PT2 G %IG=0.00484 18
194PT G 2357.0 8 E0
194PT cG E,M$transition seen in ce data only (1960Ba17, 1964Be23, 1970Be30).
194PT2cG |a(K)exp>0.014 (1964Be23) and >0.023 (1970Be30), are larger than any
194PT3cG of pure Mult for this transition feeding 0+ g.s., and can be
194PT4cG explained only by this transition being E0
194PT cG $Ice(K)=0.0066 {I5} (1964Be23), 0.0080 {I8} (1960Ba17)
194PT L 2365.932 21 1+
194PT E 0.0731 25 7.841 22 0.0731 25
194PTS E CK=0.628 4$CL=0.274 3$CM+=0.0977 11
194PT G 1743.77 15 0.0373 5 C
194PT2 G %IG=0.0234 7
194PT cG E$unweighted average of 1743.63 {I13} (1996TeZW) and 1743.918 {I18}
194PT2cG (2015Do06)
194PT cG RI$from 2015Do06. Other: 0.041 {I5} (1996TeZW), 0.052 {I15} (1977Vy01)
194PT G 2365.919 21 0.0785 11M1 0.00218
194PTS G KC=0.001276 18$LC=0.000196 3$MC=4.49E-5 7
194PTS G NC=1.110E-5 16$OC=2.00E-6 3$PC=1.396E-7 20$IPC=0.000645 9
194PT2 G %IG=0.0493 15
194PT cG E$weighted average of 2365.56 {I20} (1974HeYW), 2366.07 {I12}
194PT2cG (1996TeZW), 2365.919 {I17} (2015Do06), and 2366.1 {I8} (1960Ba17)
194PT cG RI$weighted average of 0.070 {I6} (1964Be23), 0.076 {I11} (1970Be30),
194PT2cG 0.083 {I8} (1971Vi15), 0.057 {I10} (1974HeYW), 0.086 {I10} (1996TeZW),
194PT3cG and 0.0788 {I9} (2015Do06)
194PT cG M$|a(K)exp=0.0018 {I2} deduced from Ice(K)=0.0029 {I3} and I|g=0.0785
194PT2cG {I11} here, gives |d(E2/M1)<0.3 or |d(M2/E1)=1.05 {I+15-13}, but the
194PT3cG latter is ruled out by this transition feeding 0+. Other |a(K)exp:
194PT4cG 0.0017 {I3} (1970Be30)
194PT cG $Ice(K)=0.0029 {I3}, weighted average of 0.0027 {I3} (1964Be23) and
194PT2cG 0.0030 {I3} (1960Ba17)
194PT L 2397.320 14 2+
194PT E 0.068 3 7.62 3 0.068 3
194PTS E CK=0.553 7$CL=0.327 5$CM+=0.1200 21
194PT G 435.935 28 0.0119 6 N ?
194PT2 G %IG=0.0075 4
194PT G 1474.37 7 0.0273 12 C
194PT2 G %IG=0.0172 9
194PT cG E$weighted average of 1474.20 {I13} (1996TeZW) and 1474.40 {I5}
194PT2cG (2015Do06)
194PT cG RI$weighted average of 0.035 {I5} (1996TeZW) and 0.0271 {I8} (2015Do06)
194PT G 1775.795 27 0.0339 6 YC
194PTF G FL=622.023
194PT2 G %IG=0.0213 7
194PT cG E,RI$from 2015Do06. Other: 1775.82 {I21} with I|g=0.033 {I8} (1996TeZW)
194PT cG $Level-energy difference=1775.288
194PT G 2068.869 17 0.0297 21
194PT2 G %IG=0.0187 14
194PT cG E$from 2015Do06. Other: 2068.96 {I15} (1996TeZW), 2068.2 {I13}
194PT2cG (1970Be30)
194PT cG RI$unweighted average of 0.03 {I2} (1970Be30), 0.0352 {I11} (1971Vi15),
194PT2cG 0.028 {I5} (1996TeZW), and 0.0254 {I3} (2015Do06)
194PT G 2397.25 4 0.0054 3 [E2] 1.52E-3
194PTS G KC=0.000893 13$LC=0.0001348 19$MC=3.08E-5 5
194PTS G NC=7.61E-6 11$OC=1.369E-6 20$PC=9.28E-8 13$IPC=0.000455 7
194PT2 G %IG=0.00339 21
194PT cG E$weighted average of 2397.7 {I4} (1971Vi15), 2396.3 {I4} (1996TeZW),
194PT2cG 2397.246 {I23} (2015Do06), and 2398.9 {I10} (1960Ba17)
194PT cG RI$weighted average of 0.0063 {I13} (1971Vi15), 0.007 {I3} (1996TeZW),
194PT2cG and 0.0053 {I3} (2015Do06)
194PT cG M$|a(K)exp=0.0059 {I7} deduced from Ice(K)=0.00065 {I7} and
194PT2cG I|g=0.0054 {I3} here, indicates Mult=M3, which is inconsistent with
194PT3cG adopted J|p=2+ based on L(p,d)=1+3 from 1/2-
194PT cG $Ice(K)=0.00065 {I7}, weighted average of 0.00055 {I10} (1964Be23) and
194PT2cG 0.00070 {I7} (1960Ba17)
194PT L 2412.744 13 1+
194PT E 0.056 4 7.54 4 0.056 4
194PTS E CK=0.491 11$CL=0.370 8$CM+=0.138 3
194PT G 1790.6 1 0.006 1
194PT2 G %IG=0.0038 6
194PT cG E,RI$from 2015Do06. Other: 1790.2 {I20} unplaced (1970Be30)
194PT G 2084.290 17 0.059 4 C
194PT2 G %IG=0.037 3
194PT cG E$weighted average of 2084.15 {I12} (1996TeZW), 2084.288 {I17}
194PT2cG (2015Do06), and 2083.2 {I1.3} (1970Be30). See also 2085|g from 2085
194PT3cG level
194PT cG RI$unweighted average of 0.0578 {I10} (1971Vi15), 0.056 {I7}
194PT2cG (1996TeZW), 0.0505 {I5} (2015Do06), and 0.07 {I4} (1970Be30)
194PT G 2412.693 19 0.0236 4 M1 0.00213
194PTS G KC=0.001216 17$LC=0.000187 3$MC=4.27E-5 6
194PTS G NC=1.057E-5 15$OC=1.91E-6 3$PC=1.330E-7 19$IPC=0.000676 10
194PT2 G %IG=0.0148 5
194PT cG E$from 2015Do06. Others: 2412.3 {I6} (1970Be30), 2412.98 {I21}
194PT2cG (1996TeZW), and 2413.5 {I10} (1960Ba17)
194PT cG RI$weighted average of 0.0258 {I25} (1971Vi15) and 0.0235 {I4}
194PT2cG (2015Do06). Others: 0.028 {I5} (1970Be30) and 0.028 {I7} (1996TeZW)
194PT cG M$|a(K)exp=0.0023 {I3} deduced from Ice(K)=0.00111 {I2} and I|g=0.0236
194PT2cG {I4} here, gives |d(E2/M1)<0.3 or |d(M2/E1)=1.5 {I+4-3}, but this
194PT3cG transition feeding 0+ g.s. requires pure dipole. Other |a(K)exp:
194PT4cG 0.0017 {I4} (1970Be30)
194PT cG $Ice(K)=0.00111 {I12}, weighted average of 0.00097 {I15} (1964Be23)
194PT2cG and 0.00120 {I12} (1960Ba17)