233PA 237NP A DECAY (2.144E+6 Y) 2002WO03,2000SC04,1979GO1220NDS 202012
233PA H TYP=FUL$AUT=B. Singh, J. K. Tuli, E. Browne$CIT=NDS 170, 499 (2020)$
233PA2 H CUT=8-Oct-2020$
233PA c Following points should be noted:
233PA c 1. The directly measured %|a feedings (adopted here from 2002Wo03) and
233PA2c those deduced from the gamma-ray intensity balances in the decay scheme
233PA3c (given under comments) are not always in good agreement.
233PA c 2. Below 115 keV the photon spectrum is mainly dominated by
233PA2c many (complex) peaks from Pa x-rays (from {+237}Np |a decay) and
233PA3c U x-rays (from {+233}Pa |b decay), which makes it difficult to extract
233PA4c accurate intensities of |g rays in this energy region.
233PA c 2000Sc04, 2002Wo03 (also 2000Wo01,2000Si02): measured |a, |g,
233PA2c |a|g, |b|g, x-rays using Ge(Li), two HPGe and Si(Li) detectors at PTB.
233PA3c Survey of previous measurements. The photon intensities in 2002Wo03
233PA4c were originally listed in 2000Sc04 together with detailed information
233PA5c about the origin of a radiation. The |a results given in 2002Wo03 were
233PA6c originally listed in 2000Si02. 2000Wo01 give absolute intensities of
233PA7c only 10 prominent |g rays.
233PA c 2004Sh07: measured x-ray and |g-ray emission probabilities for
233PA2c {+237}Np decay in equilibrium with {+233}Pa decay. Euromet project.
233PA c 2002Lu01, 2000Lu01: measured emission probabilities of x-rays
233PA2c and |g rays for {+237}Np-{+233}Pa source in equilibrium. The results
233PA3c are also listed in 2002Wo03. Euromet project.
233PA c 1992Lo03: measured half-life of decay of {+237}Np
233PA c 1990Pe16: ce
233PA c 1990Lo04: |a, |g
233PA c 1990Bo44: E|a, I|a
233PA c 1988Wo01: ce, |a, |g|g-coin
233PA c 1984Va27: photon emission probabilities of five x-ray lines and ten
233PA2c |g rays
233PA c 1981Ba68: relative and absolute |g-ray intensities of 40 |g rays
233PA c 1979Go12: measured |a, |g, |g|g- and |a|g-coin, x rays, |g(x ray)-coin;
233PA2c 51 |g rays assigned to the decay of {+237}Np; absolute intensities of
233PA3c 31 |g rays measured
233PA c 1976Sk01: energies and relative intensities of 42 |g rays
233PA c 1975PeZI: E|g, I|g, |g|g- and |a|g-coin
233PA c 1974HeYW (also 1971Cl01): measured E|g, I|g of 31 |g rays.
233PA c 1969Br12 (also 1968Br25,1969BrZV): E|g, I|g, ce, |a, |g|g-, |a|g- and
233PA2c |a(ce)-coin. Data from 1969Br12 are cited in 1971El11 evaluation of
233PA3c A=137 nuclides.
233PA c 1960Br12: measured half-life of decay of {+237}Np
233PA c 1949Ma01: measured half-life of decay of {+237}Np
233PA c Others:
233PA c First identification of {+237}Np isotope: 1948Wa04, 1948Ma16
233PA d 1949Ma01 is the same as 1948Ma16
233PA c |g measurements: 1975IoZZ, 1974ChXY, 1969Va06,
233PA2c 1969HoZY, 1961Ba44, 1955St04, 1955Ma67
233PA c |a: 1976BaZZ, 1969Va06, 1968Ba25, 1961Ba44, 1956Ko56, 1955Ma67
233PA c |g|g-coin: 1969HoZY
233PA c |a|g(|q): 1967Hu03
233PA c |a(|q,temp) from oriented {+237}Np: 1961Ha34, 1974Go08.
233PA c |a|g(t), |a(ce)(t) measurements: 1972Mc12, 1972Mc29, 1972Wi11,
233PA2c 1971Ga16, 1968Ob02, 1961Ma10, 1955St88, 1954En11
233PA cA E$From 2002Wo03 (also 2000Si02). In an earlier evaluation (1990Ak02),
233PA2cA the adopted values were from 1961Ba44, 1968Ba25, 1976BaZZ.
233PA3cA Others: 1979Go12 (semi), 1969Br12 (semi), 1969Va06 (semi),
233PA4cA 1956Ko56 (s), 1955Ma67.
233PA cA IA$From 2002Wo03 (also 2000Si02). Values from 1990Bo44 are given under
233PA2cA comments. Earlier measurements: 1969Br12 (also 1968Br25), 1956Ko56.
233PA3cA Measurements of 1961Ba44 and 1979Go12 do not agree well with the
233PA4cA intensities given by 2002Wo03
233PA cA HF$The nuclear radius parameter r{-0}({+233}Pa)=1.51670 {I40}
233PA2cA is deduced from interpolation (or unweighted average) of radius
233PA3cA parameters of the adjacent even-even nuclides (2020Si16)
233PA cA E(a)$Transition seen by 2002Wo03 (also 2000Si02)
233PA cA IA(B)$Reported by 1961Ba44 only, treated as uncertain
233PA cA E(G)$From level scheme. This possible |a was observed only by
233PA2cA 1979Go12 in |a|g-coin spectrum (indicated by 1979Go12 in their
233PA3cA table for |a|g-coin results).
233PA cA E(H)$From 1961Ba44, 1968Ba25 and 1976BaZZ.
233PA cA E(K),IA(K)$Combined to 163.25+169.1 levels: E|a=4710.8 {I7},
233PA2cA I|a=1.174% {I13} (2002Wo03); E|a=4710.6, I|a=1.20% {I5} (1990Bo44)
233PA tG $ ------------------------------------------------------------------
233PA tG $ Pa x-ray intensities
233PA tG $ E(x ray) Radiation I(x ray) (%)
233PA tG $ -------- --------- ---------------------------------------
233PA tG $ 2000Sc04 2004Sh07 2000Sc04
233PA tG $ 2002Wo03 2002Wo03
233PA tG $ --------- ------------- --------------------
233PA tG $ 3.15 M (?) 4.8 {I25}
233PA tG $ 11.37 L{-1} 1.31 {I20} 1.55 {I8}
233PA tG $ 13.27 L{-|a} 23.3 {I24} 26 {I3}
233PA tG $ 14.95 L{-|c} 0.50 {I4} 0.64 {I6}
233PA tG $ 15.4(b) L{-|b6} <0.66 {I5}
233PA tG $ 16.0 L{-|b2,15;|b4} 6.3 {I6} 7.9 {I3}
233PA tG $ 16.6(b) L{-|b1,|b5,|b3} <27.4 {I11}
233PA tG $ 17.2(b) L{-L1-M4,5} <11.5 {I5}
233PA tG $ 18.9(a) L{-L1-N1} 0.126 {I12}
233PA tG $ 19.50 L{-|g1} 4.65 {I17}
233PA tG $ 20.16(b) L{-|g2,|g3,|g6} <3.49 {I13}
233PA tG $ 20.7 (b) L{-L1-O2,4} 1.22 {I11}
233PA tG $ 92.29(c) K{-|a2,|a3} 1.80 {I3} 1.82 {I5}
233PA tG $ 95.87(c) K{-|a1} 2.89 {I4} 2.98 {I7}
233PA tG $ 107.60(c) K{-|b3} 0.330 {I24} 0.249 {I8}
233PA tG $ 108.43(c) K{-b1} 0.69 {I3} 0.864 {I19}(d)
233PA tG $ 109.1(a) K{-b5} 0.0252 {I12}
233PA tG $ 111.50(c) K{-|b2} 0.269 {I13} (b)
233PA tG $ 111.9(a) K{-|b4} 0.0078 {I4}
233PA tG $ 112.5(a) K{-OP} 0.099 {I15}
233PA tG $
233PA tG $ K x-ray intensities are in agreement with those from
233PA tG $ 2002Lu01 and 1984Va27
233PA tG $ (a) From 2004Sh07
233PA tG $ (b) Combined with U x-rays from {+233}Pa |b{+-} decay
233PA tG $ (c) From 1979Go12 and 1984Va27
233PA tG $ (d) For 108.43+109.1
233PA tG $ -------------------------------------------------------------------
233PA cG $|g|g-coin from 1988Wo01 and 1976Sk01; |g|g- and |a|g-coin from
233PA2cG 1979Go12; |a|g-coin and |a(ce)-coin from 1969Br12
233PA cG E$From weighted averages of 1979Go12, 1976Sk01 and 1974HeYW for
233PA2cG several transitions, unless otherwise stated. Energies measured by
233PA3cG 1988Wo01, 1975IoZZ, 1969Br12 and 1969HoZY are in good agreement.
233PA4cG Others: 1975PeZI, 1974ChXY, 1969Va06, 1961Ba44, 1955Ma67, 1955St04.
233PA cG RI$Weighted or unweighted averages from 2004Sc04, 2002Lu01 (also
233PA2cG 2000Lu01), 2000Sc04 (also 2002Wo03,2000Wo01), 1990Lo04, 1988Wo01,
233PA3cG and others, as stated with each |g ray.
233PA3cG Minimum uncertainty of 1% was used in the
233PA4cG averaging procedure, as well as in the final result. Other
233PA5cG measurements: 1984Va27, 1981Ba68, 1979Go12, 1976Sk01, 1975IoZZ,
233PA6cG 1975PeZI, 1971Cl03, 1969Br12, 1969Va06, 1969HoZY
233PA cG M$From ce data of 1988Wo01 and 1969Br12. See also 1969HoZY and
233PA2cG {+233}Th |b{+-} decay. Assumed mixing ratios are from analogous
233PA3cG transitions. Experimental conversion data quoted here are from
233PA4cG 1988Wo01, unless otherwise stated. Assignment are the same in
233PA5cG the Adopted Gammas
233PA cG M(u)$E1 from upper limit of |a(L1+L2)exp deduced from |a(ce)-coin
233PA2cG (1969Br12)
233PA cG MR$From BrIccMixing code when ce data are available.
233PA cG MR(x)$|d(E2/M1) assumed as |?0.4 from analogous transitions
233PA2cG as in 1990Ak02 evaluation of A=233 nuclei.
233PA cG E(A)$Seen only by 1979Go12.
233PA cG E(B),RI(B)$From 1990Pe16.
233PA cG E(C)$Not observed; existence has been inferred by coincidence
233PA2cG data. Energy from level scheme.
233PA cG E(E)$From 2000Sc04, isotopic assignment is uncertain.
233PA cG E(F)$From 1981Ba68, 1976Sk01 or 1969Br12. Transition is not
233PA2cG reported by 2000Sc04, or in any other recent experiments.
233PA cG E(I)$Expected interband transition has not been observed. This
233PA2cG transition is not listed in the Adopted dataset
233PA cG E(S)$From {+233}Th |b{+-} decay; not seen in {+237}Np |a decay.
233PA cG RI(G)$Photon intensities of transitions deexciting the 257.3
233PA2cG level are assumed very small in comparison to their doublets, since
233PA3cG the |a transition feeding the level is uncertain or very weak.
233PA cL $(|a)(140|g,200|g)(t): T{-1/2}<2 ns (1955St88)
233PA cL $(|a)(E|g>100)(t): T{-1/2}|<1.02 ns (1968Ob02)
233PA cL E$From least-squares fit to E|g values, assuming 0.2 keV
233PA2cL uncertainty when not given
233PA cL J$From the Adopted Levels.
233PA CL BAND(A)$|p1/2[530]
233PA CL BAND(B)$|p3/2[651]
233PA CL BAND(C)$|p1/2[660]
233PA CL BAND(D)$|p5/2[642]
233PA CL BAND(E)$|p5/2[523]
237NP P 0.0 5/2+ 2.144E+6 Y 7 4957.3 7
237NP cP J,T$Values are from {+237}Np Adopted Levels in the ENSDF database
237NP2cP (March 2006), and are still valid.
237NP cP QP$From 2017Wa10
233PA N 1.0 1.0 1.0
233PA cN BR$%|a=100. The SF and cluster decay modes are insignificant
233PA PN 3
233PA A 4386 AP 0.02 46265 B
233PA A 4550.5 220.011 3 8.4E4 24 a
233PA A 4680.5 180.020 4 4.6E4 10 a
233PA A 4825 4 0.014 11 6.6E4 52 a
233PA A 4849 5 0.006 4 1.5E5 11 a
233PA G 21.5 0.356 13 E
233PA cG RI$0.65 {I5} (2004Sh07)
233PA G 27.7 0.84 7 E
233PA G 288.3 0.0164 5 E
233PA L 0.0 3/2- 26.975 D 13 A
233PA cL T$From the Adopted Levels
233PA A 4872.7 14 2.39 4 353 7
233PA cA E$others: 4873.0 (1990Bo44), 4871 {I3} (1961Ba44)
233PA cA IA$others: 2.43 {I3} (1990Bo44), 2.6 {I2} (1969Br12), 0.925 (1961Ba44);
233PA2cA 3.5 {I17} (to g.s. +6.66 level) (from decay scheme)
233PA L 6.658 17 1/2- A
233PA A 4866.4 14 0.53 4 1.43E3 11
233PA cA E$other: 4866.4 (1990Bo44)
233PA cA IA$others: 0.49 {I3} (1990Bo44), 0.24 (1961Ba44), |>0.3 {I1}
233PA2cA (1969Br12); 3.5 {I17} (to g.s. +6.66 level) (from decay scheme)
233PA G 6.68 5 (M1) 3.04E3 8 S S
233PAS G MC=2.25E3 6
233PAS G NC=610 17$OC=146 4$PC=28.0 8$QC=2.33 7
233PA cG E,M$from the Adopted Gammas
233PA L 57.112 10 7/2- A
233PA A 4816.8 10 2.430 17 142 2
233PA cA E$4817.0 (1990Bo44)
233PA cA IA$others: 2.47 {I2} (1990Bo44), 4.1 {I21} (from decay scheme)
233PA G 57.113 20 0.362 4 E2 175.6 C
233PA cG E$weighted average of 57.104 {I20} (1979Go12), 57.15 {I4} (1976Sk01),
233PA2cG 57.112 {I20} (1974HeYW)
233PA cG RI$weighted average of 0.356 {i16} (2004Sh07), 0.366 {i3} (2002Lu01),
233PA2cG 0.360 {I5} (2002Wo03), 0.354 {I8} (2000Sc04), 0.34 {I1} (1988Wo01),
233PA3cG 0.38 {I4} (1979Go12). Others: 0.39 {I1} (1984Va27), 0.42 {I2}
233PA4cG (1981Ba68), 0.43 {I3} (1976Sk01)
233PA cG M$L1, L2, L3 ce lines used for normalization (1988Wo01)
233PA2 G EM2C=23 1$ EM3C=19 1$ ENC+=11 1$ EM1C<1.2 3 (1988Wo01)
233PA2 G EM4C=1.2 3$ EM5C<1.2 3 (1988Wo01)
233PA2 G ELC=122 18
233PA cG $L12:L3:M:N=26:18:16:5.6 (1969Br12)
233PAS G LC=128.2 18$MC=35.3 5
233PAS G NC=9.51 14$OC=2.15 3$PC=0.345 5$QC=0.000911 13
233PA cG E$admixture of {+233}Pa decay
233PA L 70.526 20 5/2- A
233PA A 4803.5 10 2.014 17 139 2
233PA cA E$other: 4803.6 (1990Bo44)
233PA cA IA$from 1961Ba44. Others: 2.06 {I5} (1990Bo44), |?3% (1969Br12),
233PA2cA 1.4 {i3} (from decay scheme)
233PA G 63.90 10 0.0108 4 (E2) 102.3 F
233PAS G LC=74.7 12$MC=20.6 4
233PAS G NC=5.55 9$OC=1.252 20$PC=0.202 4$QC=0.000565 9
233PA cG RI$from 1981Ba68
233PA cG M$from Adopted Gammas
233PA G 70.49 10 0.0108 4 [M1+E2] 38 27 F
233PAS G LC=28 19$MC=7.5 54
233PAS G NC=2.0 15$OC=0.46 33$PC=0.076 51$QC=0.00126 89
233PA cG RI$from I|g(63.9)/I|g(70.75)=1.0 (1975IoZZ)
233PA L 86.482 8 5/2+ 36.5 NS 4 B
233PA cL T$from |a(86.5|g)(t), unless otherwise stated. Weighted average of
233PA2cL 35.7 ns {I4} (1972Mc12), 36.4 ns {I5} (1972Mc29), 35.7 ns {I5}
233PA3cL (1972Wi11), 35.4 ns {I8} (|a(29.6|g)(t),1972Wi11), 37.4 ns {I4}
233PA4cL (|a(65-105 |a)(t),1971Ga16), 36.8 ns {I16} (|a(70-90 |g)(t),1968Ob02),
233PA5cL 36.9 ns {I5} (1961Ma10), 36.9 ns {I4} (|a(ce, <100 keV)(t),1954En11).
233PA A 4788.0 9 47.64 6 4.55 3 C
233PA cA E$4788.1 (1990Bo44)
233PA cA IA$others: 47.75 {I20} (1990Bo44); 82 {I2} (to 86+95+104+109 levels)
233PA2cA (from decay scheme)
233PA G 29.374 10 14.5 4 E1 3.07 C
233PA2 G EM1C<0.0078 5$ EM2C=0.059 8$ EM3C=0.054 7$ EM4C=0.012 3 (1988Wo01)
233PA2 G EM5C=0.009 2$ ENC+=0.048 2 (1988Wo01)
233PAS G LC=2.29 4$MC=0.585 9
233PAS G NC=0.1527 22$OC=0.0331 5$PC=0.00487 7$QC=0.0001509 22
233PA cG E$weighted average of 29.374 {I20} (1979Go12), 29.373 {I10} (1976Sk01),
233PA2cG 29.375 {I20} (1974HeYW)
233PA cG $1990Pe16: Ice(L1)=1.4% {I2}, Ice(L2)=1.6% {I2}, Ice(L3)=2.6% {I2}
233PA cG RI$unweighted average of 13.2 {I4} (2004Sh07), 13.51 {I16} (2002Lu01),
233PA2cG 14.12 {I15} (2000Sc04), 13.9 {I1} (1990Lo04), 15.0 {I4} (1984Va27),
233PA3cG 15.6 {I2} (1981Ba68), 16.3 {I9} (1976Sk01). Weighted average is
233PA4cG 14.2 {I3}, but reduced |h{+2}=14. Others: 19.3 {I9} (1988Wo01),
233PA5cG 9.8 {I10} (1979Go12), both seem discrepant.
233PA cG M$ce data of 1988Wo01 indicate that this transition may be an
233PA2cG anomalous E1, as is the 86.477|g. Measured I(ce) are:
233PA3cG M1:M2:M3:M4:M5=<8:61 {I8}:55 {I7}:12 {I3}:9.0 {I18}; the theoretical
233PA4cG ratios for E1 are: 36:41.1:(55):14.1:16.9 (normalized at M3 line). The
233PA5cG deduced M conversion coefficients are smaller than the theoretical
233PA6cG ones, in contrast to the 86.477|g. However, as 1988Wo01 pointed out,
233PA7cG the detector efficiency was not completely reliable for E(ce)<50 keV.
233PA8cG The theoretical conversion coefficients are given here for that reason,
233PA9cG rather than the deduced ones from measured I(ce)/I|g ratios.
233PA cG $|a(29|g)(|q): A{-2}=+0.28 {I17} (1967Hu03)
233PA G 86.484 10 12.2 3 E1 1.43 8 C
233PA cG E$weighted average of 86.477 {I10} (1979Go12), 86.503 {I20} (1976Sk01),
233PA2cG 86.486 {I10} (1974HeYW)
233PA cG RI$unweighted average of 12.86 {I21} (2000Wo01), 11.40 {I24}
233PA2cG (2002Lu01), 12.44 {I33} (1984Va27), 11.5 {I3} (1981Ba68), 12.6 {I13}
233PA3cG (1969Br12). Weighted average is 12.1 {I3}, but reduced |h{+2}=6.7.
233PA4cG Others: I|g(86.48+86.8 from {+233}Pa decay)=13.6 {I5}
233PA5cG (2004Sh07), 14.1 {I3} (2000Sc04,2002Wo03), 14.0 {I4} (2002Lu01)
233PA2 G ELC=1.13 5 $ EMC=0.22 6 $ ENC=0.08 1 $ EL1C=0.54 3 (1988Wo01)
233PA2 G EL2C=0.55 3$ EL3C=0.035 7$ EM1C=(0.03 3)$ EM2C=0.09 1 (1988Wo01)
233PA2 G EM3C<0.056 3$ EM4C<0.017 1$ EM5C=0.024 3$ ENC+=0.08 1 (1988Wo01)
233PA2 G ELC=1.0 1
233PA cG $L12:L3:M:N=133:8:40:13 (1969Br12)
233PA cG $The M and N+ regions of the ce spectra are highly complex.
233PA cG CC$from I(ce)/I|g measured by 1988Wo01. Other: 1.49 {I18}, analyzed
233PA2cG by 2008Go10 from data for measured conversion L-shell conversion
233PA3cG coefficients for anomalous E1 transition. The total conversion
233PA4cG coefficient is much enhanced as compared to the theoretical value of
233PA5cG 0.177.
233PA cG M$anomalous E1. See 1960As02 for discussions. Others: 1969Br12,
233PA2cG 2008Go10
233PA cG $|a(87|g)(|q): A{-2}=+0.12 {I4} (1967Hu03)
233PA L 94.651 12 3/2+ B
233PA G 8.22 5 0.0055 AP (M1) 1.64E3 4 9 AP
233PAS G MC=1.22E+3 3$ NC=329 8$ OC=78.9 19$ PC=15.1 4$ QC=1.25 3
233PA cG E$from {+233}Th |b{+-} decay. Other: 8.03 (1990Lo04) with
233PA2cG I|g=0.034 {I11}
233PA cG $Total I(ce)(8.22|g)/I|g(88.0|g)|?62, as deduced in {+233}Th |b{+-}
233PA2cG decay, yields total Ice(8.22|g)|?9.
233PA cG M$from Adopted Gammas
233PA G 87.99 3 0.148 10[E1] 0.1694 FC
233PAS G LC=0.1277 18$MC=0.0312 5
233PAS G NC=0.00824 12$OC=0.00189 3$PC=0.000321 5$QC=1.539E-5 22
233PA cG RI$unweighted average of 0.134 {I13} (2004Sh07), 0.167 {I4} (2002Lu01),
233PA2cG 0.143 {I1} (1990Lo04). Weighted average is 0.146 {I6} with reduced
233PA3cG |h{+2}=16
233PA G 94.65 5 0.591 20 E1 0.1398 C
233PAS G LC=0.1054 15$MC=0.0257 4
233PAS G NC=0.00680 10$OC=0.001561 22$PC=0.000267 4$QC=1.312E-5 19
233PA cG E$weighted average of 94.64 {I5} (1979Go12), 94.66 {I5} (1976Sk01)
233PA cG M$from Adopted Gammas
233PA cG RI$weighted average of 0.575 {I19} (2004Sh07) and 0.615 {I23}
233PA2cG (2002Lu01)
233PA L 103.651 18 7/2+ B
233PA A 4771.4 8 23.2 3 7.1 1 C
233PA cA E,IA$other: 4771.4, 22.7 {I4} (1990Bo44)
233PA G 9.0 [E2] 4.2E5 C S
233PA cG $E|g=9.78, I|g=0.36 (1990Lo04) may partly belong to {+237}Np decay
233PA G 17.40 5 [M1+E2] 8.0E3 78 S S
233PAF G FL=86.482
233PA cG E$17.78 in 1990Lo04
233PA G 46.53 4 0.109 3 [E1] 0.914 C
233PAS G LC=0.687 10$MC=0.1707 25
233PAS G NC=0.0448 7$OC=0.01000 15$PC=0.001587 23$QC=5.98E-5 9
233PA cG E$weighted average of 46.53 {I6} (1979Go12), 46.534 {I40} (1976Sk01)
233PA cG RI$unweighted average of 0.100 {I13} (2004Sh07), 0.103 {I2} (2002Wo03),
233PA2cG 0.104 {I4} (2000Sc04), 0.113 {I1} (1990Lo04),
233PA3cG 0.121 {I10} (1988Wo01), 0.110 {I10} (1984Va27), 0.119 {I4} (1981Ba68),
233PA4cG 0.100 {I10} (1979Go12). Weighted average is 0.111 {I2} with reduced
233PA5cG |h{+2}=4.5. Other: 0.163 {I5} (2002Lu01) seems discrepant
233PA L 109.05 3 9/2+ B
233PA A 4766.5 8 9.3 3 16.3 6 C
233PA cA E,IA$other: 4766.4, 9.7 {I3} (1990Bo44)
233PA G 5.18 C S
233PA cG E$from 1990Lo04, I|g=0.222 {I5} listed which may be transition
233PA2cG intensity
233PAF G FLAG=F
233PA G 22.6 C S
233PA L 133.25 20(11/2+) B
233PA A 4741.3 20 0.019 5395 C
233PAF A FLAG=BH
233PA cA E$not in 2002Wo03; E|a=4748? (1990Bo44)
233PA G 24.14 10 A ?
233PA G 29.6 I S
233PA L 163.32 5 (11/2-) A
233PA A 4712.3 201.174 LE 53 GE H
233PAF A FLAG=K
233PA cA IA$other: 0.484 {I13} (from decay scheme)
233PA G 54.40 10 A
233PA G 106.12 5 0.048 1 [E2] 9.30 FC
233PAS G LC=6.78 10$MC=1.87 3
233PAS G NC=0.505 8$OC=0.1143 17$PC=0.0186 3$QC=7.89E-5 12
233PA cG E$from 1976Sk01. Other: 106.15 {I25} (1979Go12)
233PA cG RI$weighted average of 0.051 {I3} (2004Sh07), 0.049 {I1} (2002Lu01),
233PA2cG 0.048 {I1} (1990Lo04), 0.042 {I3} (1988Wo01)
233PA L 169.160 17 1/2+ C
233PA A 4708.3 201.174 LE 48 GE H
233PAF A FLAG=K
233PA cA IA$other: 0.24 {I4} (from decay scheme)
233PA G 74.54 10 0.012 3 [M1+E2] 29 20 FC
233PAS G LC=7.43 11$MC=1.79 3
233PAS G NC=0.481 7$OC=0.1153 17$PC=0.0220 4$QC=0.00183 3
233PA cG RI$from 1981Ba68
233PA G 162.51 3 0.0326 12(E1) 0.1574 *C
233PA cG M$from Adopted Gammas
233PAS G KC=0.1230 18$LC=0.0260 4$MC=0.00629 9
233PAS G NC=0.001670 24$OC=0.000389 6$PC=6.91E-5 10$QC=3.99E-6 6
233PA cG E$weighted average of 162.41 {I8} (1979Go12), 162.50 {I6} (1976Sk01),
233PA2cG 162.52 {I3} (1974HeYW)
233PA cG RI$weighted average of 0.0327 {I12} (2000Sc04) and 0.032 {I4}
233PA2cG (1988Wo01)
233PA G 169.156 20 0.0621 24[E1] 0.1431 C
233PAS G KC=0.1120 16$LC=0.0235 4$MC=0.00568 8
233PAS G NC=0.001508 22$OC=0.000352 5$PC=6.26E-5 9$QC=3.65E-6 6
233PA cG RI$weighted average of 0.0633 {I19} (2000Sc04) and 0.057 {I4}
233PA2cG (1988Wo01)
233PA L 179.59 10(9/2-) A
233PA A 4698.2 8 0.535 10 90 2
233PA cA E,IA$other: 4698.0, 0.54 {I4} (1990Bo44)
233PA G 109.10 10 B ?
233PA cG E$overlap with Pa K{-|b5}-x rays
233PA L 201.619 14 3/2+ C
233PA G 32.46 C S
233PA G 115.44 20 0.0026 8 [M1+E2] 10.0 35 ?
233PAS G KC=5.4 52$LC=3.3 13$MC=0.89 39
233PAS G NC=0.24 11$OC=0.055 23$PC=0.0094 32$QC=2.9E-4 23
233PA cG E$weighted average of 115.40 {I35} (1979Go12), 115.45 {I20} (1976Sk01)
233PA cG RI$from 1976Sk01. Others: 0.32 (1979Go12) is in disagreement,
233PA2cG probably includes sum peak; 0.332 {I10} for sum peak (2000Sc04)
233PA cG E$admixture with U K x-rays
233PA G 131.093 20 0.0849 31 E1 0.262 uC
233PAS G KC=0.202 3$LC=0.0451 7$MC=0.01095 16
233PAS G NC=0.00290 4$OC=0.000672 10$PC=0.0001179 17$QC=6.40E-6 9
233PA cG E$weighted average of 131.101 {I25} (1979Go12), 131.043 {I30}
233PA2cG (1976Sk01), 131.11 {I2} (1974HeYW)
233PA cG RI$weighted average of 0.075 {I5} (2004Sh07), 0.0857 {I22} (2000Sc04),
233PA2cG and 0.091 {I5} (1988Wo01)
233PA2 G EL1C LT 0.06 (1969Br12)
233PA G 194.96 2 0.182 5 E1 0.1024 uC
233PAS G KC=0.0806 12$LC=0.01644 23$MC=0.00397 6
233PAS G NC=0.001055 15$OC=0.000247 4$PC=4.43E-5 7$QC=2.68E-6 4
233PA cG E$weighted average of 194.95 {I3} (1979Go12),
233PA2cG 194.97 {I2} (1974HeYW). Other: 195.096 {I20} (1976Sk01)
233PA cG RI$weighted average of 0.16 {I3} (2004Sh07), 0.177 {I5} (2000Sc04),
233PA2cG 0.191 {I6} (1988Wo01)
233PA2 G EL1C+EL2C<0.05 (1969Br12)
233PA G 201.670 25 0.0394 9 E1 0.0946 uC
233PAS G KC=0.0746 11$LC=0.01512 22$MC=0.00365 6
233PAS G NC=0.000970 14$OC=0.000227 4$PC=4.08E-5 6$QC=2.49E-6 4
233PA cG E$weighted average of 201.62 {I5} (1979Go12), 201.72 {I5} (1976Sk01),
233PA2cG 201.670 {I25} (1974HeYW).
233PA cG RI$weighted average of 0.0393 {I9} (2000Sc04) and 0.041 {I4} (1988Wo01)
233PA2 G EL1C+EL2C<0.05 (1969Br12)
233PA L 212.346 13 5/2+ C
233PA A 4665.0 9 3.478 24 8.1 8 C
233PA cA E$other: 4664.6 (1990Bo44)
233PA cA IA$others: 3.43 {I4} (1990Bo44), 2.76 {I20} (from decay scheme)
233PA G 10.7 I S
233PA G 43.2 I S
233PA G 108.7 0.071 3 M1(+E2) 0.9 LT 4.4 12 C
233PAS G LC=3.3 8$MC=0.84 25
233PAS G NC=0.226 66$OC=0.053 15$PC=0.0094 21$QC=0.00049 12
233PA cG E$from level-energy difference. E|g=108.0 was given by 1969Br12 from
233PA2cG E(ceL12) and E(ceM) measured in coincidence with |a.
233PA cG RI$weighted average of 0.072 {I4} (2004Sh07) and 0.070 {I3} (2002Lu01).
233PA2cG Other: 0.068 {I15} from I|g(108|g):I|g(117|g):I|g(155|g):I|g(212|g)=
233PA3cG 23 {I4}:56 {I6}:31 {I2}:55 {I4}, measured by 1969Br12 in |a|g-coin
233PA4cG spectrum. I|g(108.2+108.7+109.1)+x-ray=0.864 {I19} (2000Sc04).
233PA2 G EL1C+EL2C=2.7 6 (1969Br12)
233PA cG $L12:L3:M=62:<3:17 (1969Br12)
233PA G 117.705 20 0.170 4 M1+E2 0.46 +22-13 11.5 10 C
233PAS G KC=8.4 14$LC=2.4 4$MC=0.60 10
233PAS G NC=0.16 3$OC=0.038 6$PC=0.0068 8$QC=0.00041 7
233PA cG E$weighted average of 117.702 {I20} (1979Go12), 117.681 {I30}
233PA2cG (1976Sk01), 117.718 {I20} (1974HeYW).
233PA cG RI$weighted average of 0.169 {I17} (2004Sh07), 0.184 {I12} (2002Lu01),
233PA2cG 0.169 {I4} (2000Sc04) and 0.15 {I2} (1988Wo01)
233PA2 G ELC=1.8 3 (1969Br12)$
233PA cG $L12:L3:M:N=90:8:51:|?8 (1969Br12)
233PA G 141.74 10 AC
233PA G 155.242 20 0.0887 18 E1 0.1755 uC
233PAS G KC=0.1368 20$LC=0.0292 4$MC=0.00708 10
233PAS G NC=0.00188 3$OC=0.000437 7$PC=7.74E-5 11$QC=4.41E-6 7
233PA cG E$weighted average of 155.239 {I20} (1979Go12), 155.22 {I4} (1976Sk01),
233PA2cG 155.25 {I2} (1974HeYW).
233PA cG RI$weighted average of 0.087 {I6} (2004Sh07), 0.091 {I6} (2002Lu01),
233PA2cG 0.0889 {I18} (2000Sc04) and 0.086 {I6} (1988Wo01)
233PA2 G EL1C+EL2C<0.09 (1969Br12)
233PA G 212.32 2 0.152 3 E1 0.0839 uC
233PAS G KC=0.0663 10$LC=0.01331 19$MC=0.00321 5
233PAS G NC=0.000854 12$OC=0.000200 3$PC=3.60E-5 5$QC=2.22E-6 4
233PA cG E$weighted average of 212.29 {I5} (1979Go12),
233PA2cG 212.33 {I2} (1974HeYW). Other: 212.415 {I25} (1976Sk01),
233PA cG RI$weighted average of 0.150 {I4} (2002Lu01), 0.151 {I3} (2000Sc04)
233PA2cG and 0.156 {I4} (1988Wo01). Other: 0.209 {I7} for 212.4+214.1 (2004Sh07)
233PA2 G EL1C+EL2C<0.013 (1969Br12)
233PA L 218 3 ?
233PA cL E$level not included in the Adopted dataset
233PA A 4659.1 20 0.57 LE 45 GE B ?
233PA cA E$|a not in 2002Wo03 and 1990Bo44
233PA L 237.904 11 5/2+ D
233PA A 4640.0 10 6.43 3 2.86 3 C
233PA cA E$other: 4839.5 (1990Bo44)
233PA cA IA$others: 6.45 {I4} (1990Bo44); 6.0 {I7} (from decay scheme)
233PA G 36.32 2 0.005 1 M1+E2 0.31 9 2.1E+2 8 BC
233PAF G FLAG=F
233PAS G LC=1.57E+2 56$MC=41 16
233PAS G NC=11.1 41$OC=2.56 93$PC=0.44 15$QC=0.0144 5
233PA cG $L1:L2:L3=1.1 {I4}:1.3 {I5}:1.0 {I3} (1990Pe16)
233PA cG RI$from 1990Lo04
233PA G 134.276 20 0.072 3 [M1+E2] 0.4 AP 8.04 AP xC
233PAS G KC=6.05 9$LC=1.484 21$MC=0.369 6
233PAS G NC=0.0991 14$OC=0.0235 4$PC=0.00433 6$QC=0.000291 4
233PA cG E$weighted average of 134.285 {I20} (1979Go12), 134.23 {I4} (1976Sk01),
233PA2cG 134.28 {I3} (1974HeYW).
233PA cG RI$unweighted average of 0.073 {I6} (2004Sh07), 0.075 {I3} (2002Lu01),
233PA2cG 0.067 {I3} (2000Sc04), 0.0640 {I9} (1990Lo04) and 0.080 {I5}
233PA3cG (1988Wo01). Weighted average is 0.066 {I3} with reduced |h{+2}=5.8
233PA G 143.248 10 0.416 11M1+E2 0.69 19 5.8 6 C
233PA cG E$weighted average of 143.249 {I20} (1979Go12), 143.208 {I25}
233PA2cG (1976Sk01), 143.254 {I10} (1974HeYW).
233PA cG RI$unweighted average of 0.394 {I24} (2004Sh07), 0.428 {I3} (2002Lu01),
233PA2cG 0.443 {I8}, 0.387 {I2} (1990Lo04) and 0.43 {I1} (1988Wo01). Weighted
233PA3cG average is 0.410 {I11} with reduced |h{+2}=17
233PA2 G EKC=3.1 4$ EL1C=1.5 2$ EL2C=0.3 1$ EM1C=0.3 1 (1988Wo01)
233PA cG $|a(N+)exp<0.76 {i3} (1988Wo01)
233PA cG $|a(L3)exp=|a(M2)exp=|a(M3)exp=|a(M4)exp=|a(M5)exp<0.44 {I2} (1988Wo01)
233PA cG $From their ce data, 1988Wo01 give %E2=9 {I7} or
233PA2cG |d(E2/M1)=0.31 {I+13-17}
233PA2 G EL1C+EL2C=0.9 1 (1969Br12)
233PA cG $K:L12:L3:M:N=250:69:<5:15:6 (1969Br12)
233PAS G KC=4.0 7$LC=1.32 8$MC=0.34 3
233PAS G NC=0.091 7$OC=0.0212 15$PC=0.00379 18$QC=0.00020 3
233PA G 151.408 15 0.244 3 M1+E2 0.28 12 5.9 3 C
233PA cG E$weighted average of 151.414 {I20} (1979Go12), 151.375 {I35}
233PA2cG (1976Sk01), 151.410 {I15} (1974HeYW).
233PA cG RI$weighted average of 0.223 {I14} (2004Sh07), 0.244 {I3} (2002Lu01),
233PA2cG 0.232 {I24} (2000Sc04) and 0.248 {I7} (1988Wo01)
233PA cG $Measured conversion electron intensities for this transition
233PA2cG do not agree well: Ice(K)/Ice(L1+L2)=2.0 {I6} (1988Wo01), |?6.5
233PA3cG (1968Br12). Ice(L1)/Ice(L2)=15.8 {I26}:8.3 {I21} measured by
233PA4cG 1988Wo01 is used to determine the M1+E2 admixture. Other: 1969Br12
233PA2 G EKC=5.3 7$ EL1C=1.2 2$ EL2C=0.6 2$ ENC+<1.12 6$ EL3C<0.78 4 (1988Wo01)
233PA2 G EL1C+EL2C=1.0 2 (1969Br12)
233PA cG $|a(M1)exp=|a(M2)exp=|a(M3)exp=|a(M4)exp=|a(M5)exp<0.71 {I4} (1988Wo01)
233PA cG $K:L12:L3:M=|?220:34:2:8 (1969Br12)
233PA cG MR$deduced by evaluators considering experimental ce data for K, L1 and
233PA2cG L2 shells from 1988Wo01, and K:L12:L3:M ratio data (with 25%
233PA3cG uncertainty) from 1969Br12. Using data from 1988Wo01 only,
233PA4cG evaluators obtain |d<0.5, whereas 1988Wo01 give %E2=33 {I9} or
233PA5cG |d(E2/M1)=0.70 {I16}, which the evaluators cannot reproduce.
233PAS G KC=4.6 4 $LC=0.99 3$MC=0.242 10
233PAS G NC=0.065 3 $OC=0.0155 6$PC=0.00291 7$QC=0.000220 14
233PA G 180.79 5 0.0156 10[E1] 0.1223 C
233PAS G KC=0.0960 14$LC=0.0199 3$MC=0.00480 7
233PAS G NC=0.001275 18$OC=0.000298 5$PC=5.32E-5 8$QC=3.15E-6 5
233PA cG E$weighted average of 180.81 {I10} (1979Go12), 180.80 {I8} (1976Sk01),
233PA2cG 180.78 {I5} (1974HeYW).
233PA cG RI$weighted average of 0.0158 {I10} and 0.015 {I2} (1988Wo01)
233PA G 237.884 24 0.0572 9 [E1] 0.0645 C
233PAS G KC=0.0511 8$LC=0.01008 15$MC=0.00243 4
233PAS G NC=0.000646 9$OC=0.0001516 22$PC=2.75E-5 4$QC=1.740E-6 25
233PA cG E$weighted average of 237.86 {I2} (1979Go12),
233PA2cG 237.908 {I20} (1974HeYW). Other: 238.04 {I4} (1976Sk01)
233PA cG RI$weighted average of 0.067 {I4} (2004Sh07), 0.056 {I3} (2002Lu01),
233PA2cG 0.0569 {I6} (2000Sc04) and 0.059 {I3} (1988Wo01)
233PA L 257.129 24 5/2- E
233PA A 4619.7 21 0.032 8 4.2E2 11 C
233PA cA E$other: 4619, uncertain |a (1990Bo44)
233PA G 153.37 10 *
233PAF G FLAG=FG
233PA G 162.51 3 *
233PAF G FLAG=G
233PA G 170.62 5 *
233PAF G FLAG=G
233PA G 186.86 35 M1+E2 0.8 3 2.5 5 *
233PAF G FLAG=FG
233PA cG M,MR$from the Adopted Gammas
233PA G 250.58 A
233PAF G FLAG=G
233PA G 257.09 20 M1+E2 1.1 2 0.80 12 *
233PAF G FLAG=FG
233PA cG M,MR$from the Adopted Gammas
233PA L 279.719 22(7/2+) C
233PA A 4599.1 18 0.371 9 24.5 7
233PA cA E$other: 4598.5 (1990Bo44)
233PA cA IA$others: 0.39 {I2} (1990Bo44); 0.36 {I3} (from decay scheme)
233PA G 170.62 5 0.020 4 [M1+E2] 0.4 AP 4.0 AP *C
233PAF G FLAG=x
233PAS G KC AP 3.09$LC AP 0.698$MC AP 0.1720
233PAS G NC AP 0.0462$OC AP 0.01097$PC AP 0.00205$QC AP 0.0001466
233PA cG E$weighted average of 170.59 {I6} (1979Go12), 170.63 {I8}
233PA2cG (1976Sk01), 170.64 {I5} (1974HeYW)
233PA cG RI$weighted average of 1976Sk01 and 1979Go12
233PA G 176.09 5 0.016 4 [M1+E2] 0.4 AP 3.67 AP xC
233PAS G KC AP 2.82$LC AP 0.633$MC AP 0.1559
233PAS G NC AP 0.0418$OC AP 0.00995$PC AP 0.00186$QC AP 0.0001340
233PA cG E$weighted average of 176.12 {I6} (1979Go12), 176.09 {I7}
233PA2cG (1976Sk01), 176.06 {I5} (1974HeYW)
233PA cG RI$weighted average of 0.012 {I4} (2000Sc04) and 0.020 {I4} (1988Wo01)
233PA G 193.24 3 0.0437 18[M1+E2] 0.4 AP 2.8 AP xC
233PAS G KC AP 2.18$LC AP 0.477$MC AP 0.1172
233PAS G NC AP 0.0314$OC AP 0.00748$PC AP 0.001403$QC AP 0.0001030
233PA cG E$weighted average of 193.26 {I5} (1979Go12), 193.26 {I4}
233PA2cG (1976Sk01), 193.22 {I3} (1974HeYW)
233PA cG RI$weighted average of 0.041 {I8} (2004Sh07), 0.030 {I5} (2002Lu01),
233PA2cG 0.0437 {I10} (2000Sc04), 0.049 {I3} (1988Wo01). Reduced |h{+2}=3.6
233PA G 209.20 3 0.0142 9 [E1] 0.0868 C
233PAS G KC=0.0685 10$LC=0.01381 20$MC=0.00333 5
233PAS G NC=0.000886 13$OC=0.000207 3$PC=3.73E-5 6$QC=2.30E-6 4
233PA cG E$weighted average of 209.19 {I5} (1979Go12), 209.25 {I5}
233PA2cG (1976Sk01), 209.18 {I3} (1974HeYW)
233PA cG RI$from 2000Sc04. Others: <0.02 (2004Sh07), 0.019 {I2} (2002Lu01),
233PA2cG 0.010 {I2} (1988Wo01)
233PA G 222.6 2 0.0020 10 [E1] 0.075 F
233PA cG RI$average of 1976Sk01 and 1981Ba68
233PA L 283 3 ?
233PA cL E$level not included in the Adopted Levels
233PA A 4594.9 20 0.085 101 B ?
233PA cA E$not reported in 2002Wo03 and 1990Bo44
233PA L 300.483 25 7/2+ D
233PA A 4578.6 14 0.369 23 17.3 11
233PA cA E$other: 4577.5 (1990Bo44)
233PA cA IA$others: 0.41 {I2} (1990Bo44); 0.7 {I4} (from decay scheme)
233PA G 62.59 10 0.006 2 [M1+E2] 65 49 F
233PAS G LC=47 35$MC=12.9 99
233PAS G NC=3.5 27$OC=0.79 60$PC=0.130 93$QC=0.0018 13
233PA cG RI$from 1981Ba68. Other: |?0.012 (1976Sk01)
233PA cG $|a(M1)=17.5, |a(E2)=115.3.
233PA G 191.43 3 0.0187 13[M1+E2] 2.0 12 C
233PAS G KC=1.4 12$LC=0.487 10$MC=0.125 7
233PAS G NC=0.0337 19$OC=0.00786 25$PC=0.00140 7$QC=6.7E-5 54
233PA cG E$weighted average of 191.46 {I5} (1979Go12), 191.45 {I6}
233PA2cG (1976Sk01), 191.42 {I3} (1974HeYW)
233PA cG RI$weighted average of 0.023 {I5} (2004Sh07), 0.015 {I4} (2002Lu01),
233PA2cG 0.0192 {I15} (2000Sc04) and 0.014 {I5} (1988Wo01)
233PA G 196.85 5 0.0209 12[M1+E2] 0.4 AP 2.67 AP xC
233PAS G KC AP 2.07$LC AP 0.451$MC AP 0.1108
233PAS G NC AP 0.0297$OC AP 0.00708$PC AP 0.001327$QC AP 9.77E-5
233PA cG E$weighted average of 196.86 {I5} (1979Go12), 196.84 {I6}
233PA2cG (1976Sk01), 196.8 {I1} (1974HeYW)
233PA cG RI$weighted average of 0.020 {I4} (2004Sh07), 0.024 {I5} (2002Lu01),
233PA2cG 0.0208 {I12} (2000Sc04) and 0.021 {I2} (1988Wo01). Other: 0.156 {I2}
233PA3cG (1990Lo04) seems discrepant
233PA G 214.01 4 0.0357 10[M1+E2] 0.4 AP 2.1 AP C
233PAS G KC AP 1.637$LC AP 0.351$MC AP 0.0860
233PAS G NC AP 0.0231$OC AP 0.00550$PC AP 0.001034$QC AP 7.72E-5
233PA cG E$weighted average of 214.01 {I5} (1979Go12), 214.09 {I5}
233PA2cG (1976Sk01), 213.96 {I4} (1974HeYW)
233PA cG RI$weighted average of 0.039 {I2} (2002Lu01), 0.0362 {I8} (2000Sc04),
233PA2cG and 0.034 {I1} (1988Wo01).
233PA3cG Others: 0.209 {I7} for 212.4+214.0 (2004Sh07), 0.132 {I2} (1990Lo04)
233PA cG CC$ for assumed |d|?0.4
233PA G 229.94 5 0.011 3 [E1] 0.0697 FC
233PAS G KC=0.0552 8$LC=0.01095 16$MC=0.00264 4
233PAS G NC=0.000702 10$OC=0.0001646 23$PC=2.98E-5 5$QC=1.87E-6 3
233PA cG RI$average of 1981Ba68, 1976Sk01 and 1969Br12
233PA L 303.51 6(9/2+) C
233PA A 4573 3 0.048 23 127 61 B
233PA cA IA$possibly includes I|a to 306.05 level
233PA cA IA$other: 0.059 {I9} (from decay scheme)
233PA G 139.9 1 0.0046 4 [E1] 0.225 F ?
233PAS G KC=0.1742 25$LC=0.0381 6$MC=0.00925 13
233PAS G NC=0.00245 4$OC=0.000569 8$PC=0.0001002 15$QC=5.55E-6 8
233PA cG RI$from 1981Ba68. I|g=0.019 {I5} (1976Sk01) is in disagreement.
233PA2cG Not reported in any other study
233PA G 194.67 20 0.033 8 [M1+E2] 1.9 12
233PA cG E$from 1976Sk01
233PA cG RI$from 2002Lu01. Others: 0.03 {I1} (2004Sh07), 0.051 {I15} (1976Sk01).
233PA2cG Alaga rule suggests I|g|<0.013 if I|g(199.95|g) deexciting the
233PA3cG 303.6 level is <0.004.
233PA G 199.95 6 0.0053 8 [M1+E2] 1.8 11 F
233PA cG RI$from 1981Ba68
233PA L 306.09 7(7/2-) E
233PA A 4567 0.010 4 G ?
233PA cA IA$from decay scheme
233PA G 48.96 10 [M1+E2] 2.0E2 17 B ?
233PAF G FLAG=F
233PA G 219.8 [E1] 0.0774 A ?
233PA G 248.93 10 0.0050 14[M1+E2] 0.93 61 C
233PAS G KC=0.67 57$LC=0.20 4$MC=0.050 7
233PAS G NC=0.0135 18$OC=0.0032 5$PC=0.00057 13$QC=3.2E-5 26
233PA cG E$weighted average of 248.95 {I10} (1979Go12), 248.90 {I10} (1976Sk01)
233PA cG RI$others: 0.006 {I3} (2002Lu01); for 248.5
233PA2cG (from {+233}Pa decay)+248.9: 0.0618 {I11} (2000Sc04),
233PA3cG 0.10 {I5} (2004Sh07)
233PA L 365.96 7 9/2+ D
233PA A 4515.1 19 0.035 4 59 7
233PA cA E$other: 4513.7 (1990Bo44)
233PA cA IA$others: 0.041 {I4} (1990Bo44); 0.066 {I7} (from decay scheme)
233PA G 153.37 10 0.0061 11[E2] 1.96 *C
233PAF G FLAG=F
233PAS G KC=0.226 4$LC=1.268 19$MC=0.349 5
233PAS G NC=0.0942 14$OC=0.0214 3$PC=0.00350 5$QC=2.42E-5 4
233PA cG RI$average of 1976Sk01 and 1981Ba68
233PA G 186.86 35 0.003 3 [E1] 0.1131 *
233PAF G FLAG=F
233PAS G KC=0.0889 13$LC=0.0183 3$MC=0.00442 7
233PAS G NC=0.001173 18$OC=0.000274 4$PC=4.91E-5 8$QC=2.93E-6 5
233PA cG RI$from 1976Sk01. Others: I|g=0.0069 {I14} (1969Br12),
233PA2cG 0.0013 {I8} (1981Ba68)
233PA G 202.9 2 0.0048 19[E1] 0.0932 C
233PAS G KC=0.0735 11$LC=0.01489 22$MC=0.00360 6
233PAS G NC=0.000955 14$OC=0.000223 4$PC=4.02E-5 6$QC=2.45E-6 4
233PA cG E$from 1976Sk01
233PA cG RI$other: I|g(201.6+202.9)=0.0393 {I9} (2000Sc04)
233PA G 257.09 20 0.0064 14[M1+E2] 0.9 6 *C
233PAF G FLAG=F
233PA cG RI$average of 1981Ba68, 1971Cl03 and 1969Br12. Others: 0.019 {I6}
233PA2cG (1979Go12) for 257.1+258.2 (from {+233}Pa decay): <0.05 (2004Sh07),
233PA3cG 0.036 {I5} (2002Lu01)
233PA G 262.44 15 0.0047118[M1+E2] 0.8 6 C
233PA cG E$from 1976Sk01. Value is the same in 1979Go12, with uncertainty
233PA2cG of 0.20
233PA cG RI$from 2000Sc04
233PA G 279.65 20 0.0109 4 [E2] 0.222 C
233PAS G KC=0.0847 12$LC=0.1005 15$MC=0.0272 4
233PAS G NC=0.00733 11$OC=0.001676 24$PC=0.000282 4$QC=5.02E-6 7
233PA cG RI$from 2000Sc04. Others: 0.0017 {I17} (1976Sk01), 0.011 {I4}
233PA2cG (1979Go12), 0.0023 (1971Cl03)