233U 233PA B- DECAY (26.975 D) 2011KO32,1990KO41,2002WO0320NDS 202012
233U H TYP=FUL$AUT=B. Singh, J. K. Tuli, E. Browne$CIT=NDS 170, 499 (2020)$
233U 2 H CUT=8-Oct-2020$
233U c {+233}Pa isotope with T{-1/2}|?27 d is relevant in U-Th fuel cycle,
233U 2c and important for reactor reactivity control. The isotope is formed in
233U 3c {+232}Th+n |) {+233}Th, which decays through |b{+-} to {+233}Pa.
233U c 2012Le03: measurement of absolute intensities of 300.1, 312.0 and
233U 2c 1028.5-keV gamma rays using a new method: combination of pile
233U 3c oscillation and |g activation experiments at the MINERVE
233U 4c reactor, Cadarache, France.
233U c 2011Ko32, 2010Ko27: {+233}Pa source was chemically separated from a
233U 2c {+237}Np source in secular equilibrium with {+233}Pa. Measured absolute
233U 3c intensities for x-rays and |g-rays using planar LEPS and coaxial Ge
233U 4c detectors. See 2010Ko27 for comparison with earlier measurements from
233U 5c 2008De10, 2004Sh07, 2002Lu01 (also 2000Lu01), 2000Sc04, 2000Wo01
233U 6c (also 1988Wo01), 1990Ko41, 1984Va27, 1979Ge08 and 1973Va33. Measured
233U 7c value of absolute I|g(28.6|g)=0.076% {I3} in 2010Ko27 and 0.075% {I4}
233U 8c in 2011Ko32 is in agreement with that from 1973Va33, 1988Wo01 and
233U 9c 1990Ko41, but differs significantly with that from 2004Sh07, 2002Lu01
233U Ac and 1984Va27. The I|g values in 2010Ko27 and 2011Ko32 for E|g>40 are
233U Bc in good agreement with earlier measurements.
233U c 2008De10: chemically purified source obtained as {+237}Np in
233U 2c equilibrium with {+233}Pa. Measured absolute intensities of
233U 3c x-rays and |g-rays using HPGe detectors. The disintegration rates were
233U 4c measured using liquid scintillation counting.
233U c 2006Ha53: measured |g-emission probability of the 312-keV |g-ray.
233U c 2004Sh07: measured absolute intensities of x-rays and |g-rays using
233U 2c planar Ge detector using the full response function method.
233U c 2002Lu01: measured photon-emission probabilities of x-rays
233U 2c and low-energy |g rays up to |?120 keV using planar Ge detector.
233U c 2002Wo03: summary of the measurements reported in 2000Wo01, 2004Sh07,
233U 2c 2002Lu01 (also 2000Lu01), 2000Sc04 from {+237}Np-{+233}Pa source in
233U 3c equilibrium, as part of the EUROMET collaborative project (No. 416)
233U c 2000Lu01 (same group as 2002Lu01): measured photon-emission
233U 2c probabilities of x-rays and |g rays up to 416 keV using HPGe detector.
233U c 2000Wo01: measured |g-ray emission probabilities using HPGe detector,
233U 2c and 4|p(PC)-|g counting for standardization.
233U c 2000Sc04: measured photon emission probabilities of x-rays and |g-rays
233U 2c using Ge(Li), two HPGe and Si(Li) detectors.
233U c 2000Us01: measured half-life of {+233}Pa activity
233U c 1993Pa12: measured angular correlations between K|a x-rays and
233U 2c subsequent L{-3} x-ray transitions using HPGe and Si(Li) detectors
233U c 1990Ko41: Source produced via {+232}Th(n,|g) at Saclay and source
233U 2c separated at Nice; measured E|g, I|g, |g|g- and (x ray)|g-coin,
233U 3c HPGe detector.
233U c 1990Pe16: ce data, {+237}Np-{+233}Pa source in equilibrium
233U c 1989Br24: source was chemically separated from {+237}Np parent
233U 2c activity by means of ion-exchange column techniques. Measured
233U 3c conversion coefficients for the 300-, 312-, and 340-keV |g-rays
233U 4c from simultaneous measurements of their |g-ray and conversion-electron
233U 5c intensities, the |g rays detected by an HPGe detector and conversion
233U 6c electrons, by a windowless Si(Li) detector. Deduced nuclear penetration
233U 7c effects for the three |g rays. The ce data were normalized to
233U 8c |a(K)exp(392|g in {+113}Sn)=0.437 {I7}. Also measured |b spectrum and
233U 9c deduced feeding to the ground state.
233U c 1988Wo01: measured ce, and absolute internal conversion coefficients
233U 2c for seven |g-ray transitions from the decay of {+233}Pa; deduced E|g
233U 3c values from the conversion electron lines for these transitions.
233U c 1985DeZR (thesis): measured E|g, I|g, ce, |g|g-coin. A large number of
233U 2c very weak transitions were reported only by 1985DeZR and many of these
233U 3c have been assigned to new levels and band structures. These have not
233U 4c been used in the present dataset due to reasons mentioned below. See
233U 5c 2005Si15 evaluation for some of the placement suggested
233U 6c by 1985DeZR, and a complete table of |g rays from 1985DeZR.
233U c 1987He11: measured |g(|q,temp), low-temperature nuclear orientation
233U 2c for 340-keV gamma transition.
233U c 1986Kr10: measured |g|g(|q) for five |g|g-cascades using two Ge(Li)
233U 2c detectors, deduced mixing ratios by combining |g|g(|q) data with
233U 3c previous ce data, and with theoretical estimates from Nilsson model
233U 4c assignments
233U c 1984Va27: measured E|g, absolute I|g, selected x rays using HPGe
233U 2c detector
233U c 1979Ge08: measured E|g,, I|g, x rays, absolute intensity of 312-keV
233U 2c gamma ray using Ge(Li) detector.
233U c 1978-Poenitz: W.P. Poenitz and D.L. Smith, Rept. ANL/NDM-42
233U 2c (March 1978), cited in 2010BeZQ and 2006Ch39 DDEP evaluation: measured
233U 3c photon emission probability of 312-keV |g ray.
233U c 1973Va33: measured E|g, I|g, |g|g-coin.
233U c 1972De67: measured E|g, I|g for four |g rays.
233U c 1971Vo02: measured precise E|g for seven |g rays using Riso
233U 2c bent crystal spectrometer.
233U c 1971Cl03: measured E|g, I|g using Ge(Li) detector
233U c 1968Ma13: measured level half-lives by |b(ce)(t)
233U c 1968Da24: measured E|g for three |g rays
233U c 1967Br20: measured E|g
233U c 1965Be38: measured x rays, E|g and conversion lines using Si(Li)
233U 2c detector, 11 |g rays reported.
233U c 1963De22: measured I|g of six gamma rays using NaI(Tl) detector
233U c 1963Bi03 (also 1959Bi14): measured |b spectra, ce, (ce)|g-coin using a
233U 2c six-gap and a single-gap beta ray spectrometer. Deduced end-point
233U 3c energies, K-conversion coefficient and multipolarity for 312|g. A total
233U 4c of 13 transitions assigned to the decay of {+233}Pa, with E|g,
233U 5c transition intensities, multipolarities and mixing ratios.
233U c 1962Sc03: measured conversion electrons using a wedge-shaped
233U 2c magnetic spectrometer. Deduced E|g values, multipolarities and
233U 3c mixing ratios for 14 |g transitions assigned to the decay of {+233}Pa.
233U c 1961Al19: measured |b spectrum, conversion lines, E|g, I|g, and x rays
233U 2c using a high resolution permanent-magnet 180|' electron spectrographs,
233U 3c an iron free double-focusing beta spectrometer, DuMond curved-crystal
233U 4c spectrometer, and a NaI(Tl) detector. Measured values of relative
233U 5c conversion electron and photon intensities. Deduced conversion
233U 6c coefficients, multipolarities and mixing ratios. A total of 13 |g rays
233U 7c were assigned to the decay of {+233}Pa
233U c 1960Al08, 1959Al02: measured conversion electrons and Auger lines.
233U c 1960Un01 (thesis): measured |b|g-coin
233U c 1958Hi78 (thesis): measured |g
233U c 1955On05: measured conversion electron lines using a magnetic
233U 2c spectrograph, deduced E|g for 15 transitions, intensities and
233U 3c multipolarities for some of these.
233U c 1954Br37: measured |b spectrum and electron conversion lines
233U 2c using a magnetic spectrometer. Deduced E|g values for 13 transitions.
233U c 1952Br84 (thesis): measured x rays and |g rays.
233U c 1952El26: measured gamma rays
233U c 1950Ke54: measured conversion electrons using a permanent magnet-type
233U 2c photographic beta-spectrometer, deduced E|g values for 13 transitions.
233U c 1947Le01, 1941Gr03, 1941Se09, 1941-Haggstrom (Phys. Rev. 59, 322),
233U 2c 1938Me04: discovery of {+233}Pa activity and decay studies.
233U c
233U c Results from 1985DeZR have not been used here for the following
233U 2c reasons: 1. many gamma rays are multiply placed without separation
233U 3c of intensities into the components; 2. a significant number of
233U 4c low-energy transitions are given without any knowledge of
233U 5c multipolarities and associated conversion coefficients; 3.
233U 6c with Q(|b{+-})=570.1 {I20}, the levels proposed by the author at
233U 7c 570.2 and 571.3 keV would be unlikely to be populated; 4.
233U 8c several high-spin (J>7/2) levels are shown as populated, which
233U 9c would be unlikely from 3/2- parent state.
233U c Evaluations: 2010BeZQ (DDEP), 2006Ch39 (related to DDEP), 2005Hu06.
233U c The decay scheme has been known since detailed studies by 1961Al19,
233U 2c 1960Al08 and 1959Al02. However, it has gone through some
233U 3c modifications and improvements in energies of radiations since then,
233U 4c as a result of a large number of publications using Ge and Si(Li)
233U 5c detectors. The last detailed study was by 2011Ko32
233U cB IB$Deduced from in-out transition intensity balances. The feeding to
233U 2cB ground state is from measurement of |b spectrum by 1989Br24
233U cG $A 145.42 {I5} |g with an intensity of |?1.3 (relative to 100 for
233U 2cG 312|g) was reported only by 1961Al19 in the curved crystal
233U 3cG spectrometer. Another transition at 57.9 keV was seen by 1961Al19
233U 4cG in their ce spectra. Authors discussed in detail the existence and
233U 5cG possible placement of the 145-keV transition. Weak 57.9-keV
233U 6cG was placed by the authors from 399-keV to 340-keV level. Both these
233U 7cG |g rays are omitted here for lack of confirmation in other studies.
233U cG E$Weighted averages of values from several studies as indicated in
233U 2cG a comment for each |g ray. In 1990Ko41, some of the uncertainties
233U 3cG were 0.005 keV, evaluators considered a minimum uncertainty
233U 4cG of 0.010 keV in the averaging procedure, with the same restriction
233U 5cG on the final value.
233U cG RI$Weighted or unweighted averages of values from several studies as
233U 2cG indicated in a comment for each |g ray. Some of the uncertainties were
233U 3cG lower than 1%, evaluators considered a minimum uncertainty of 1% in
233U 4cG the averaging procedure, with the same restriction on the final value.
233U 5cG All the intensities are expressed as relative to 100.0 for the 311.9|g.
233U cG E(a),RI(b)$Weak |g from 1990Ko41 only.
233U cG M$From ce data of 1961Al19, 1962Sc03, 1963Bi03, 1966Ze02, and 1988Wo01.
233U 2cG Multipolarities in square brackets are assumed, as expected from |DJ|p.
233U 3cG The |d(E2/M1) values given in comments have been taken from %E2 values
233U 4cG listed in Table 1 in 1986Kr10, which were deduced from ce data in
233U 5cG 1966Ze02, 1963Bi03, 1962Sc03 and 1961Al19.
233U cG MR(k)$From |g|g(|q) data of 1986Kr10. As the measured angular
233U 2cG correlation coefficients in most cases were close to zero, the authors,
233U 3cG in their analysis, considered available conversion electron data (e.g.
233U 4cG from 1966Ze02), as well as theoretical estimates based on B(E2)/B(M1)
233U 5cG calculations from Nilsson band assignments and K|p assignments.
233U cG CC(p)$From measured conversion coefficient (1989Br24) for the
233U 2cG transition with a significant penetration effect, resulting in the
233U 3cG reduction of the theoretical conversion coefficients.
233U tG $ -------------------------------------------------------------------
233U tG $ U x-rays (2010Ko27)
233U tG $
233U tG $ E(x-ray) U(x-rays) I(x-ray)@
233U tG $ ----------- -------- ----------
233U tG $ 13.64 {I15} L{-|a} 39.7 {I41}
233U tG $ 15.46 {I15} L{-|c} 1.00 {I11}
233U tG $ 15.79 {I13} L{|b6} 1.35 {I14}
233U tG $ 16.53 {I6} L{-|b2,15,4} 18.9 {I20}
233U tG $ 17.27 {I6} L{-|b1,5,3} 35.3 {I37}
233U tG $ 18.04 {I10} L{-L1,M4,5} 0.712 {I42}
233U tG $ 19.48 {I10} L{-L1,N1} 0.462 {I27}
233U tG $ 20.22 {I6} L{-|g1} 7.05 {I29}
233U tG $ 20.75 {I7} L{-|g2,3,6} 3.84 {I16}
233U tG $ 21.56 {I9} L{-L1,O2,4} 0.958 {I40}
233U tG $ 94.64 {I7} K{-|a2,3} 22.97 {I66}
233U tG $ 98.42 {I6} K{-|a1} 37.0 {I11}
233U tG $ 110.41 {I8} K{-|b3} 4.46 {I13}
233U tG $ 111.30 {I8} K{-|b1,5} 9.30 {I27}
233U tG $ 114.48 {I7} K{-|b2,4} 3.66 {I11}
233U tG $ 115.38 {I9} K{-O2,3,P2,3} 1.256 {I37}
233U tG $ @: I(x-ray) is relative to 100 for I|g(312|g)
233U tG $
233U tG $---------------------------------------------
233U tG $ U x-rays (2008De10)
233U tG $
233U tG $ E(x-ray) U(x-rays) I(x-ray)@
233U tG $ ----------- -------- ---------------
233U tG $ 11.62 L{-1} 1.19 {I4}
233U tG $ 13.93 L{-|a} 21.46 {I23}
233U tG $ 15.73 L{|b6} 0.89 {I2}
233U tG $ 16.41 L{-|b2,15,4} 8.93 {I11}
233U tG $ 17.22 L{-|b1,5} 16.23 {I19}
233U tG $ 17.45 L{-|b3} 0.22 {I2}
233U tG $ 20.17 L{-|g1} 3.38 {I5}
233U tG $ 20.49 L{-|g2} 1.83 {I3}
233U tG $ 20.84 L{-|g3,6} 0.520 {I11}
233U tG $ 94.65 K{-|a2,3} 8.50 {I11}
233U tG $ 98.43 K{-|a1} 14.2 {I19}
233U tG $ 110.43 K{-|b3} 1.694 {I26}
233U tG $ 111.30 K{-|b1} 3.24 {I5}
233U tG $ 111.98 K{-|b5} 0.139 {I18}
233U tG $ 114.46 K{-|b2,4} 1.317 {I21}
233U tG $ 115.42 K{-OP} 0.406 {I11}
233U tG $ @: I(x-ray) is relative to 38.08 {I29} for I|g(312|g)
233U tG $
233U tG $----------------------------------------------------------
233U tG $ U x-rays (1990Ko41)
233U tG
233U tG $ E(x-ray) U(x-rays) I(x-ray) @
233U tG $ --------- -------- ------------
233U tG $ 93.967 {I10} K|a{-3} 0.17 {I2}
233U tG $ 94.656 {I4} K|a{-2}| 8.4 {I4}
233U tG $ 98.434 {I4} K|a{-1}| 13.5 {I7}
233U tG $ 110.431 {I5} K|b{-3} 1.62 {I8}
233U tG $ 111.303 {I5} K|b{-1} 3.14 {I15}
233U tG $ 111.984 {I10} K|b{-5} 0.15 {I1}
233U tG $ 114.339 {I8} K|b{-2} 0.52 {I7}
233U tG $ 114.602 {I8} K|b{-4} 0.79 {I7}
233U tG $ 115.419 {I10} KO{-23},KP{-23} 0.39 {I2}
233U tG $ @: I(x-ray) is relative to 38.6 for I(312|g)
233U tG $Other x-ray measurements: 1984Va27, 1979Ge08, 1967Br20, 1961Al19.
233U 2tG The x-ray intensities from 2004Sh07, 2002Wo03, 2002Lu01 and 2000Sc04
233U 3tG are also available from {+237}Np-{+233}Pa equilibrium source, but
233U 4tG generally the peaks are complex structures with x-rays contributed
233U 5tG by {+237}Np decay.
233U tG $---------------------------------------------------------------------
233U cL E$From least-squares fit to E|g data
233U cL J$From the Adopted Levels
233U cL BAND(A)$|n5/2[633]
233U cL BAND(B)$|n5/2[752]
233U cL BAND(D)$|n3/2[631]
233U cL BAND(E)$|n1/2[631]
233PA P 0.0 3/2- 26.975 D 13 570.3 20
233PA cP J,T$From {+233}Pa Adopted Levels
233PA cP QP$From 2017Wa10
233U N 0.3818 23 1.0 1.0
233U cN NR$From %I|g(311.9|g)=38.18 {I23}, weighted average of the following
233U 2cN measurements: 37.79 {I64} (2012Le03), 37.8 {I8} (2011Ko32), 38.08 {I29}
233U 3cN (2008De10), 37.5 {I24} (2004Sh07), 37.80 {I23} (2002Lu01), 38.5 {I4}
233U 4cN (2000Sc04), 38.7 {I4} (2000Wo01), 38.65 {I39} (1984Va27), 38.6 {I5}
233U 4cN (1979Ge08), and 38.6 {I15} (1978-Poenitz).
233U 5cN Other: %I|g(311.9|g)=41.6 {I9} (2006Ha53) seems discrepant.
233U PN 3
233U L 0.0 5/2+ A
233U B 8.8 14 8.9 1
233U S B EAV=169.55 67
233U cB E$measurements: 568 {I5} (1954Br37,1955On05), 578 {I10} (1963Bj03)
233U cB IB$from 1989Br24, for the g.s. and 40.4-keV level from |b{+-} spectrum
233U 2cB above 420 keV, taken in anticoincidence mode. Other measurements: 5
233U 3cB (1954Br37,1955On05), 12 (1963Bj03). As no significant feeding is
233U 4cB expected to the 40.4, 7/2+ level, consistent with I|b=-1.9 {I16}
233U 5cB from the present level scheme, evaluators assign the feeding measured
233U 6cB by 1989Br24 to the g.s. only. The analysis of the present decay scheme
233U 7cB with |g-normalization factor of 0.3818 {I23} and transition intensity
233U 8cB balance at each level gives I|b(g.s.)=8.8% {I20}, consistent with
233U 9cB the measurement of 1989Br24.
233U L 40.350 7 7/2+ A
233U B ?
233U cB IB$-1.9 {I16} from intensity balance, consistent with no |b feeding
233U 2cB to this level.
233U G 40.351 10 0.0597 32 M1+E2 0.93 11 5.1E2 6 C
233U S G LC=3.7E2 5$MC=102 13
233U S G NC=28 4$OC=6.4 8$PC=1.04 12$QC=0.0087 5
233U cG E$weighted average of 40.33 {I10} (2011Ko32), 40.349 {I5} (1990Ko41),
233U 2cG 40.5 {I1} (1972De67), 40.35 {I1} (1961Al19, crystal), 40.47 {I10}
233U 3cG (1952Br84)
233U cG RI$weighted average of 0.0582 {I26} (2011Ko32), 0.085 {I11} (2004Sh07),
233U 2cG 0.074 {I11} (2002Lu01), 0.056 {I4} (2000Wo01), 0.062 {I10}
233U 3cG (1990Ko41), 0.10 {I2} (1973Va33)
233U cG $Triple placement in 1985DeZR, but from other studies
233U 2cG the main placement is from 40.3 level
233U cG $L1:L2:L3:M1:M2:M3:N:O+P=13:100:91:5:20:16:12:3.4 (1966Ze02),
233U 2cG %E2=54 {I5} or |d=1.08 {I10}; L1:L2:M1:M2:M3:M4=14:100:4:39:29:2
233U 3cG (1962Sc03), %E2=54 {I4} or |d=1.08 {I+10-8};
233U 4cG L1:L2:L3:M2:M3=30:100:80:25:23 (1961Al19), %E2=30 {I10} or
233U 5cG |d=0.65 {I16}; %E2=31 {I2} or |d=0.67 {I3} from ce data (1963Bi03);
233U 6cG |d=1.23 from ce data (1959Al02). Other: 1985DeZR
233U cG MR$deduced by evaluators using BrIccMixing code on all the L- and
233U 2cG M-subshell ratios quoted above, assuming 20% uncertainty in each ratio
233U L 92.13 4 9/2+ A
233U G 51.5 5 0.0026 LT [M1+E2] 1.7E+2 15 b ?
233U S G LC=1.3E+2 11$MC=35 29
233U S G NC=9.4 79$OC=2.2 18$PC=0.36 29$QC=0.0038 22
233U cG E$from Adopted Gammas.
233U G 92.1 5 0.0052 LT [E2] 19.6 6 b ?
233U S G LC=14.3 5$MC=3.96 12
233U S G NC=1.07 4$OC=0.247 8$PC=0.0403 12$QC=0.000148 4
233U cG E$average of 92.1 {I5} (1990Ko41) and 92.0 {I5} (1973Va33)
233U cG RI$<0.01 (1973Va33)
233U L 298.815 10 (5/2-) B
233U B 0.127 20 9.7 1
233U S B EAV=74.64 60
233U G 258.45 3 0.073 5 [E1] 0.0547 C
233U S G KC=0.0433 6$LC=0.00857 12$MC=0.00207 3
233U S G NC=0.000553 8$OC=0.0001318 19$PC=2.41E-5 4$QC=1.496E-6 21
233U cG E$weighted average of 258.63 {I12} (2011Ko32), 258.45 {I2} (1990Ko41),
233U 2cG 258.2 {I2} (1973Va33)
233U cG RI$weighted average of 0.077 {I5} (2011Ko32), 0.071 {I8} (2000Sc04),
233U 2cG 0.070 {I5} (1990Ko41). Other: 0.010 {I4} (1973Va33)
233U G 298.81 2 0.32 5 [E1] 0.0396 C
233U S G KC=0.0315 5$LC=0.00609 9$MC=0.001469 21
233U S G NC=0.000393 6$OC=9.38E-5 14$PC=1.729E-5 25$QC=1.106E-6 16
233U cG E$weighted average of 298.81 {I9} (2011Ko32), 298.81 {I2} (1990Ko41),
233U 2cG 298.89 {I20} (1973Va33)
233U cG RI$unweighted average of 0.357 {I13} (2011Ko32), 0.39 {I8} (2002Lu01),
233U 2cG 0.223 {I18} (1990Ko41). Weighted average is 0.31 {I5} but reduced
233U 3cG |h{+2}=19. Other: 0.09 (1973Va33)
233U cG $Observed by 1973Va33 in |g|g-coin
233U L 301.93 10 (5/2-)
233U B 0.014 4 10.7 1
233U S B EAV=73.71 60
233U G 301.93 10 0.036 9 [E1] 0.0387 C
233U S G KC=0.0308 5$LC=0.00595 9$MC=0.001434 21
233U S G NC=0.000384 6$OC=9.16E-5 13$PC=1.689E-5 24$QC=1.083E-6 16
233U cG E$weighted average of 301.85 {I12} (2011Ko32), 301.99 {I10} (1990Ko41)
233U cG RI$unweighted average of 0.045 {I5} (2011Ko32), 0.026 {I5} (1990Ko41).
233U L 311.905 6 3/2+ 0.120 NS 15 D
233U cL T$|bce(K 312|g)(t) (1968Ma13). Other: 0.20 ns {I3} (1960Jo15)
233U B 25 4 7.4 1
233U S B EAV=70.75 60
233U cB E$ measurements: 256 {I4} (1954Br37), 257 {I5} (1955On05), 250 {I5}
233U 2cB (1960Un01), 254 {I5} (1963Bj03)
233U cB IB$ measurements: 45 (1954Br37), 58 (1955On05), 56 (1963Bj03)
233U G 271.556 10 0.840 8 E2 0.258 C
233U S G KC=0.0904 13$LC=0.1226 18$MC=0.0334 5
233U S G NC=0.00905 13$OC=0.00210 3$PC=0.000357 5$QC=5.77E-6 8
233U cG E$weighted average of 271.57 {I8} (2011Ko32), 271.555 {I10} (1990Ko41),
233U 2cG 271.48 {I8} (1971Vo02, crystal), 271.58 {I4} (1971Cl03),
233U 3cG 271.62 {I23} (1961Al19, crystal)
233U cG RI$weighted average of 0.847 {I26} (2011Ko32), 0.77 {I15} (2004Sh07),
233U 2cG 0.855 {I13} (2002Lu01), 0.839 {I10} (2000Sc04), 0.834 {I8} (2000Wo01),
233U 3cG 0.88 {I4} (1990Ko41), 0.828 {I26} (1984Va27), 0.85 {I3} (1979Ge08),
233U 4cG 0.79 {I8} (1973Va33)
233U cG $K:L1:L2:L3:M1+M2=100:21:84:35:33 (1966Ze02); K:L2:L3:M2=100:75:19:38
233U 2cG (1962Sc03); K:L1:L3=100:98:|?7 (1961Al19); E2 in all including ce
233U 3cG in 1963Bi03. Others: 1985DeZR, 1959Al02
233U G 311.901 11 100.0 10 M1+E2 -0.10 1 0.80 3 kC
233U F G FLAG=p
233U cG E$weighted average of 311.94 {I5} (2011Ko32), 311.904 {I5} (1990Ko41),
233U 2cG 311.887 {I10} (1971Cl03), 311.98 {I3} (1971Vo02, crystal), 311.91 {I13}
233U 3cG (1961Al19, crystal). Other: 312.17 {I12} (1988Wo01), seems somewhat
233U 4cG discrepant
233U cG RI$100.0 {I21} (2011Ko32), 100.0 {I8} (2008De10),
233U 2cG 100 {I6} (2004Sh07), 100.0 {I6} (2002Lu01), 100.0 {I10} (2000Sc04),
233U 3cG 100.0 {I10} (2000Wo01), 100.0 {I10} (1990Ko41), 100 {I5} (1988Wo01),
233U 4cG 100.0 {I10} (1984Va27), 100 (1979Ge08), 100 (1973Va33)
233U 2 G EKC=0.64 2$ EL1C+EL2C=0.123 4$ EM1C=0.029 1 (1989Br24)$
233U 2 G EKC=0.69 7 (1963Bi03)$ EKC=0.70 7 (1966Ze02)
233U cG M,CC$from measured |a(K)exp, |a(L1+L2)exp and |a(M1)exp (1989Br24).
233U 2cG Deduced penetration parameter |l=2.3 {I4} (1989Br24), assuming pure M1.
233U cG $K:L1:L2:M:N:O=100:17:2.0:4.3:1.1:0.3 (1966Ze02);
233U 2cG K:L1:L2:M:N=100:15:1.5:4.3:1.1 (1962Sc03);
233U 3cG K:L1:L2:M:N:O=100:17:1.6:3.7:1.7:0.4; K/L=1653 {I82}/311 {I28}
233U 4cG (1988Wo01). M1 in 1963Bi03 and 1959Al02 from ce; %E2<1.6 (1966Ze02),
233U 5cG <3 (1962Sc03), <2 (1961Al19). Other: |d=0.26 {I2} (1985DeZR).
233U L 320.76 5 7/2- B
233U B 0.024 2 10.3 ?
233U S B EAV=68.14 59
233U cB IB$no |b feeding is expected for |DJ=2, |D|p=no
233U G 228.57 5 0.0109 18 [E1] 0.0723 aC
233U F G FLAG=b
233U S G KC=0.0571 8$LC=0.01151 17$MC=0.00279 4
233U S G NC=0.000744 11$OC=0.0001769 25$PC=3.22E-5 5$QC=1.94E-6 3
233U G 280.58 8 0.035 4 [E1] 0.0455
233U S G KC=0.0362 5$LC=0.00706 10$MC=0.001703 24
233U S G NC=0.000455 7$OC=0.0001086 16$PC=2.00E-5 3$QC=1.260E-6 18
233U cG E$weighted average of 280.37 {I14} (2011Ko32), 280.61 {I5} (1990Ko41)
233U cG RI$weighted average of 0.0370 {I26} (2011Ko32), 0.028 {I5} (1990Ko41).
233U G 320.73 10 0.0132 8 [E1] 0.0339 a
233U F G FLAG=b
233U S G KC=0.0270 4$LC=0.00518 8$MC=0.001247 18
233U S G NC=0.000334 5$OC=7.97E-5 12$PC=1.474E-5 21$QC=9.57E-7 14
233U L 340.478 6 5/2+ 52 PS 10 D
233U cL T$|bce(K 340|g)(t) (1968Ma13)
233U B 27 6 7.2 1
233U S B EAV=62.36 59
233U G 28.562 11 0.192 11 M1+E2 0.16 2 3.2E2 4 C
233U cG E$weighted average (NRM) of 28.57 {I8} (2011Ko32), 28.559 {I10}
233U 2cG (1990Ko41), 28.6 {I1} (1972De67), 28.54 {I3} (1961Al19, crystal),
233U 3cG 28.67 {I2} (1952Br84). Other: 28.375 {I5} (1988Wo01), seems discrepant.
233U cG RI$weighted average of 0.198 {I11} (2011Ko32), 0.194 {I21} (1990Ko41),
233U 2cG 0.180 {I24} (1988Wo01), 0.18 {I2} (1973Va33). Others: 0.051 {I5}
233U 3cG (2004Sh07), 0.090 {I26} (2002Lu01), 0.388 {I26} (1984Va27); all
233U 4cG seem discrepant.
233U 2 G EM1C=23 6$ EM2C=17 8$ ENC+=11 2 (1988Wo01)
233U S G LC=2.4E2 3$MC=60 7
233U S G NC=16.3 19$OC=3.9 5$PC=0.69 7$QC=0.0336 5
233U cG $L1/(M1+M2)=2.7 {I3} (1990Pe16);
233U 2cG L1:L2:L3:M1:M2:M3:N:O+P=51.6:26.2:20.0:8.3:4.3:3.1:4.8:1.4
233U 3cG (1966Ze02), %E2=2.4 {I2} or |d=0.16 {I1}; L3:M2:M3=9.3:4.7:3.1
233U 4cG (1962Sc03), %E2=1.02 {I8} or |d=0.10 {I1}; M1:M2:M3=8.0:2.9:3.1
233U 5cG (1961Al19), %E2=3.0 {I5} or |d=0.18 {I1}; M1:M2:N+=88 {I21}:64
233U 6cG {I30}:40.6 {I51} (1988Wo01); %E2=2% {I1} or |d=0.14 {I3} in 1963Bi03
233U 7cG from ce; %E2=4 or |d=0.20 (1959Al02) from ce. Others: |d=0.14 {I1}
233U 8cG (1985DeZR)
233U cG MR$deduced by evaluators using BrIccMixing code on all the
233U 2cG L- and M-subshell ratios given above, assuming 20% uncertainty on
233U 3cG the ratio when not given.
233U G 41.660 10 0.0346 27 [E1] 1.254 C
233U S G LC=0.940 14$MC=0.236 4
233U S G NC=0.0621 9$OC=0.01399 20$PC=0.00219 3$QC=7.52E-5 11
233U cG E$weighted average of 41.65 {I10} (2011Ko32), 41.663 {I10}
233U 2cG (1990Ko41), 41.65 {I2} (1961Al19, crystal).
233U cG RI$weighted average of 0.0344 {I27} (2011Ko32), 0.036 {I8} (1990Ko41),
233U 2cG 0.035 {I10} (1973Va33)
233U G 248.37 4 0.158 3 [E2] 0.346 C
233U cG E$weighted average of 248.35 {I12} (2011Ko32), 248.38 {I4}
233U 2cG (1990Ko41), 248.0 {I2} (1973Va33), 248.69 {I24} (1968Ma13), 248.3 {I3}
233U 3cG (1967Br20).
233U cG RI$weighted average of 0.164 {I11} (2011Ko32), 0.151 {I16} (2002Lu01),
233U 2cG 0.161 {I3} (2000Sc04), 0.157 {I3} (2000Wo01), 0.150 {I10} (1990Ko41),
233U 3cG 0.155 {I26} (1984Va27), 0.154 {I6} (1979Ge08). Other: 0.010 {I3}
233U 4cG (1973Va33)
233U S G KC=0.1065$ LC=0.1755 25 $ MC=0.0480 7
233U S G NC=0.01301 19$OC=0.00301 5$PC=0.000509 8$QC=7.17E-6 10
233U cG $K, L2, L3, M2, N2 lines seen in ce (1985DeZR)
233U G 300.128 10 17.14 17 M1+E2 -0.08 2 0.87 3 kC
233U F G FLAG=p
233U cG E$weighted average of 300.16 {I6} (2011Ko32), 300.129 {I5}
233U 2cG (1990Ko41), 300.12 {I3} (1971Vo02, crystal), 300.124 {I20} (1971Cl03),
233U 3cG 300.20 {I24} (1961Al19, crystal). Other: 300.34 {I2} (1988Wo01), seems
233U 4cG discrepant
233U cG RI$weighted average of 16.88 {I50} (2011Ko32), 16.99 {I13} (2008De10),
233U 2cG 16.8 {I5} (2004Sh07), 16.90 {I16} (2002Lu01), 17.01 {I18} (2000Sc04),
233U 3cG 17.21 {I16} (2000Wo01), 17.67 {I18} (1990Ko41), 17.2 {I12} (1988Wo01),
233U 4cG 17.18 {I16} (1984Va27), 17.14 {I15} (1979Ge08), 17.2 {I8} (1973Va33)
233U 2 G EKC=0.70 2$ EL1C+EL2C=0.128 4 (1989Br24)
233U cG M,CC$from |a(K)exp and |a(L1+L2)exp (1989Br24).
233U 2cG Deduced penetration parameter |l=2.6 {I9} (1989Br24), assuming pure M1.
233U 2 G EKC=0.83 7$ ELC=0.15 2 (1988Wo01)
233U cG $K:L1:L2:M1+M2:N=100:16:1.9:4.6:1.1 (1966Ze02), |d=0;
233U 2cG K:L1:L2:M1:N1=100:15:1.3:3.8:1.5 (1962Sc03), |d<0.18;
233U 3cG K:L1:L2:M1:N1=100:16:2.3:4.4:1.4 (1961Al19), |d=0.37 {I+16-23}
233U 4cG K/L=301 {I13}/53.4 {I73} (1988Wo01). M1 in 1963Bi03 and 1959Al02
233U 5cG from ce. Other: |d=0.16 {I2} (1985DeZR)
233U G 340.477 10 11.63 12 M1+E2 -0.23 5 0.62 3 kC
233U F G FLAG=p
233U cG E$weighted average of 340.55 {I12} (2011Ko32), 340.476 {I5}
233U 2cG (1990Ko41), 340.50 {I4} (1971Vo02, crystal), 340.47 {I2} (1971Cl03),
233U 3cG 340.51 {I18} (1961Al19, crystal). Other: 340.81 {I3} (1988Wo01),
233U 4cG seems discrepant
233U cG RI$weighted average of 11.46 {I37} (2011Ko32), 11.65 {I9} (2008De10),
233U 2cG 11.6 {I12} (2004Sh07), 11.67 {I8} (2002Lu01), 11.69 {I13} (2000Sc04),
233U 3cG 11.68 {I10} (2000Wo01), 10.92 {I13} (1990Ko41), 11.7 {I13} (1988Wo01),
233U 4cG 11.69 {I13} (1984Va27), 11.57 {I10} (1979Ge08), 11.7 {I12} (1973Va33).
233U 5cG Uncertainty was doubled in 1990Ko41 in the averaging procedure.
233U 2 G EKC=0.50 2$ EL1C+EL2C=0.090 3$ EM1C=0.022 1 (1989Br24)$
233U 2 G EKC=0.62 9 (1988Wo01)
233U cG M,CC$from |a(K)exp, |a(L12)exp and |a(M1)exp (1989Br24).
233U 2cG Deduced penetration parameter |l=2.4 {I8} (1989Br24), assuming pure M1.
233U cG $K:L1:L2:M:N:O=100:16:2.1:4.6:1.4:0.4 (1966Ze02), |d<0.25;
233U 2cG K:L1:L2:L3:M:N:O=100:17:1.0:0.2:3.5:1.4:0.2 (1962Sc03), |d=0.29 {I9};
233U 3cG K:L1:L2:M:N=100:22:2.8:7.0:2.8 (1961Al19), |d=0.3 {I+2-3}; M1 in
233U 4cG 1963Bi03 and 1959Al02 from ce data. Other: |d=0.4 {I1} (1985DeZR)
233U L 380.37 8 (7/2+) D
233U B 0.037 10 9.3 1 1U?
233U S B EAV=55.84 62
233U G 288.33 10 0.050 5 [M1+E2] 0.67 46
233U S G KC=0.49 41$LC=0.134 38$MC=0.034 8
233U S G NC=0.0092 21$OC=0.0022 6$PC=4.0E-4 13$QC=2.3E-5 19
233U cG E$weighted average of 288.17 {I13} (2011Ko32), 288.42 {I10} (1990Ko41).
233U cG RI$weighted average of 0.053 {I5} (2011Ko32), 0.041 {I8} (1990Ko41).
233U G 380.28 10 0.0096 23 [M1+E2] 0.31 22 aC
233U F G FLAG=b
233U S G KC=0.23 19$LC=0.057 23$MC=0.0143 51
233U S G NC=0.0038 14$OC=9.2E-4 35$PC=1.73E-4 72$QC=1.11E-5 84
233U L 398.496 8 1/2+ 55 PS 20 E
233U cL T$|bce(L 86.6|g)(t) (1968Ma13)
233U B 12.9 23 7.1 1
233U S B EAV=45.71 57
233U cB E$measurement: 175 {I8} (1960Un01)
233U G 57.9 0.0024 AP [E2] 178 4 ?
233U cG $L2 and L3 conversion lines reported by 1961Al19, but no intensities
233U 2cG were given. 1962Sc03 reported Ice(L3)=0.2 relative to Ice(K)=100 for
233U 3cG 311.9|g. Using theoretical K-conversion coefficient of 0.71 {I1} for
233U 4cG 311.9|g and L3 conversion coefficient of 57.4 {I13} for 57.9-keV
233U 5cG transition (with assumed uncertainty of 0.2 keV), I|g(57.9)=0.0024.
233U 6cG 1973Va33 reported I|g<0.01.
233U cG CC$assuming |DE|g=0.2 keV
233U S G LC=130 3$ MC=36.0 8 $NC=9.76 22 $OC=2.24 5$PC=0.363 8$QC=0.000975 20
233U G 86.591 10 5.26 18 M1(+E2) 0.09 LT 7.09 13 kC
233U cG E$weighted average of 86.57 {I5} (2011Ko32), 86.595 {I5}
233U 2cG (1990Ko41), 86.58 {I3} (1972De67), 86.59 {I1} (1961Al19, crystal).
233U 3cG Others: 86.814 {I3} (1988Wo01, seems discrepant), 87.0 {I3} (1952Br84)
233U cG RI$weighted average of 5.34 {I19} (2011Ko32), 6.9 {I6} (2002Lu01),
233U 2cG 4.99 {I28} (1990Ko41), 4.9 {I7} (1988Wo01), 5.1 {I3} (1979Ge08),
233U 3cG 4.9 {I6} (1973Va33)
233U cG $(86.6|g)(311.9|g)(|q): A{-2}=-0.008 {I4}, A{-4}=+0.008 {I5}
233U 2cG (liquid,1986Kr10)
233U cG $(86.6|g)(311.9|g)(|q): A{-2}=-0.006 {I3}, A{-4}=+0.003 {I5}
233U 2cG (solid,1986Kr10); A{-2}=-0.008 {I4} (liquid), -0.005 {I3} (solid),
233U 3cG for assumed A{-4}=0 (1986Kr10)
233U 2 G EL1C=5.6 7$ EL2C=1.0 2$ EL3C=0.3 2 (1988Wo01)$ EL1C=5.2 5 (1966Ze02)
233U S G LC=5.34 10$MC=1.296 25
233U S G NC=0.350 7$OC=0.0849 16$PC=0.0163 3$QC=0.001292 19
233U cG $L1:L2:M1:M2:N1:O=100:12:25:3.3:6.9:1.7 (1966Ze02), |d<0.08;
233U 2cG L1:L2:M1:M2:N1:O=100:7:22:2.3:4.4:1.5 (1962Sc03), |d<0.05;
233U 3cG L1:L2:L3:M1:M2:N1:O=100:14:3:28:6.2:6.9:1.7 (1961Al19), |d=0.14 {I2};
233U 4cG L1:L2:L3=573 {I14}:105.0 {I98}:34 {I16} (1988Wo01); |d=0.10 {I+4-10}
233U 5cG in 1963Bi03 and |d<0.1 in 1959Al02 from ce data. Other: 1985DeZR
233U cG MR$deduced by evaluators using BrIccMixing code on all the L- and
233U 2cG M-subshell ratios, assuming 20% uncertainty on ratio when not given.
233U 3cG This values agrees with <0.1 based on |g|g(|q) data in 1986Kr10.
233U 4cG Other: 0.07 {I1} (1985DeZR)
233U G 398.494 10 3.55 6 E2 0.0835
233U cG E$weighted average of 398.58 {I12} (2011Ko32), 398.492 {I5}
233U 2cG (1990Ko41), 398.62 {I8} (1971Vo02), 398.49 {I2} (1971Cl03),
233U 3cG 398.57 {I40} (1961Al19, crystal).
233U cG RI$unweighted average of 3.52 {I13} (2011Ko32), 3.55 {I27} (2004Sh07),
233U 2cG 3.685 {I34} (2002Lu01), 3.652 {I39} (2000Sc04), 3.636 {I28} (2000Wo01),
233U 3cG 3.29 {I5} (1990Ko41), 3.70 {I5} (1984Va27), 3.60 {I3} (1979Ge08),
233U 4cG 3.35 {I40} (1973Va33). Weighted average is 3.61 {I4}, but
233U 5cG reduced |h{+2} is 6.4.
233U S G KC=0.0439 7$LC=0.0291 4$MC=0.00777 11
233U S G NC=0.00210 3$OC=0.000492 7$PC=8.58E-5 12$QC=2.39E-6 4
233U cG $K:L1:L2:L3:M:N=100:17:38:11:11:5 (1966Ze02);
233U 2cG K:L1:L2:L3=100:22:37:13(1962Sc03); L2/L3=100/31 (1961Al19);
233U 3cG E2 in 1966Ze02, 1963Bi03, 1962Sc03 and 1961Al19 from ce data.
233U 4cG Other: 1985DeZR
233U L 415.761 7 3/2+ 30 PS LE E
233U cL T$|bce(L 75.3|g)(t), |bce(L 104|g)(t) (1968Ma13)
233U B 28 3 6.62 5
233U S B EAV=40.86 56
233U cB E$measurements: 140 {I14} (1954Br37), 145 {I10} (1955On05), 155 {I7}
233U 2cB (1960Un01), 154 {I5} (1963Bj03)
233U cB IB$measurements: 50 (1954Br37), 37 (1955On05), 32 (1963Bj03)
233U G 17.26 4 0.025 10 M1+E2 0.13 2 5.0E2 10
233U S G M1C=130.9 21$ M2C=120 40 $ M3C=110 40$
233U S G MC=370 80$NC=100 20$OC=23 5$ PC=4.1 8 $ QC=0.1521 24
233U cG $Transition seen in conversion electron spectra by 1961Al19,
233U 2cG 1962Sc03 and 1966Ze02.
233U cG RI$deduced from Ice(M1+M2)=5.4 relative to Ice(K)=100, and
233U 2cG |a(K)=0.710 {I10} for 311.9|g (1962Sc03), and |a(M1+M2)(theory)=151
233U 3cG {I40} for transition energy of 17.26 keV {I4} and |d(E2/M1)=0.13 {I2}.
233U 4cG Uncertainty of 25% is assumed in measured Ice(M1+M2).
233U cG E$from observation of M1, M2, M3, N1 and N2 conversion lines by
233U 2cG 1961Al19. Uncertainty is not given in 1961Al19. However, from
233U 3cG the spread of energies of several conversion lines, it is estimated
233U 4cG as 0.04 keV. Other: 17.2 (1962Sc03, from M1 and M2 lines)
233U cG MR$from M1:M2:M3=20:18:16 (1966Ze02), assuming 25% uncertainty in
233U 2cG the subshell ratios. Others: M1/M2=2.0/3.4, 8% {I5} E2 or
233U 3cG |d=0.30 {I+8-12} (1962Sc03).
233U G 75.274 10 3.37 6 M1+E2 +0.15 8 11.4 12 kC
233U S G LC=8.6 9$MC=2.11 24
233U S G NC=0.57 7$OC=0.138 15$PC=0.0261 23$QC=0.00192 6
233U cG E$weighted average of 75.26 {I5} (2010Ko27), 75.269 (1991Ko41),
233U 2cG 75.27 {I3} (1972De67), 75.28 {I1} (1961Al19, crystal), 75.4 {I2}
233U 3cG (1952Br84). Uncertainty is not given in 1990Ko41, assumed by
233U 4cG evaluators as 0.010 in averaging, based on uncertainties in this
233U 5cG for other |g rays.
233U cG RI$unweighted average of 3.36 {I13} (2011Ko32), 3.01 {I10} (2004Sh07),
233U 2cG 3.360 {I21} (2002Lu01), 3.59 {I10} (2000Sc04), 3.62 {I7} (2000Wo01),
233U 3cG 3.26 {I23} (1990Ko41), 3.27 {I24} (1988Wo01), 3.36 {I10} (1984Va27),
233U 4cG 3.6 {I2} (1979Ge08), 3.26 {I20} (1973Va33). Weighted average is
233U 5cG 3.39 {I5}, but reduced |h{+2} is 3.6.
233U cG MR$other: 0.090 {I5} (1985DeZR) from ce data
233U cG $(75.27|g)(300.1|g)(|q): A{-2}=-0.008 {I10}, A{-4}=+0.015 {I15}
233U 2cG (liquid,1986Kr10)
233U cG $(75.27|g)(300.1|g)(|q): A{-2}=-0.001 {I10}, A{-4}=+0.019 {I14}
233U 2cG (solid,1986Kr10); A{-2}=+0.010 {I10} (liquid), +0.003 {I9} (solid),
233U 3cG for assumed A{-4}=0 (1986Kr10)
233U cG $(75.27|g)(340.5|g)(|q): A{-2}=-0.140 {I10}, A{-4}=+0.020 {I13}
233U 2cG (liquid,1986Kr10)
233U cG $(75.27|g)(340.5|g)(|q): A{-2}=-0.128 {I13}, A{-4}=+0.022 {I19}
233U 2cG (solid,1986Kr10); A{-2}=-0.133 {I9} (liquid), -0.123 {I11} (solid)
233U 3cG for assumed A{-4}=0 (1986KR10)
233U cG $(75.27|g)[28.6|g](311.9|g)(|q): A{-2}=-0.014 {I13}, A{-4}=0.000 {I18}
233U 2cG (liquid,1986Kr10); A{-2}=-0.015 {I13} (liquid) for assumed A{-4}=0
233U 3cG (1986Kr10)
233U 2 G EL1C=8.0 6$ EL2C=0.85 9$ EL3C LT 0.14$ ENC+EOC=0.7 1 (1988Wo01)
233U cG $L1:L2:L3:N:O+=550 {I18}:58.4 {I45}:36.9 {I52}:<0.14:9.8 {I19}
233U 2cG (1988Wo01); L1:L2:M1:M2:N1:O=100:12:22:3:7:1.5 (1966Ze02), |d<0.07;
233U 3cG L1:L2:M1:M2:N1=100:6:19:2:5 (1962Sc03), |d<0.02;
233U 4cG L1:L2:M1:N1:O=100:14:24:8:3 (1961Al19), |d=0.10 {I1};
233U 5cG M1 in 1963Bi03 from ce data. Other: 1985DeZR
233U G 103.860 10 2.226 22 M1(+E2) +0.1 1 4.21 21 kC
233U S G LC=3.17 15$MC=0.77 5
233U S G NC=0.208 12$OC=0.050 3$PC=0.0097 4$QC=0.000758 22
233U cG E$weighted average of 103.84 {I8} (2010Ko27), 103.860 {I10} (1991Ko41),
233U 2cG 103.862 {I10} (1971Cl03), 103.86 {I2} (1961Al19, crystal)
233U cG RI$weighted average of 2.25 {I8} (2011Ko32), 2.20 {I7} (2004Sh07),
233U 2cG 2.262 {I16} (2002Lu01), 2.192 {I44} (2000Sc04), 2.204 {I21} (2000Wo01),
233U 3cG 2.22 {I16} (1990Ko41), 1.90 {I24} (1988Wo01), 2.25 {I8} (1984Va27),
233U 4cG 2.25 {I8} (1979Ge08), 1.92 {I20} (1973Va33).
233U cG MR$other: 0.15 {I1} from ce data (1985DeZR)
233U cG $(103.86|g)(311.9|g)(|q): A{-2}=+0.005 {I5}, A{-4}=-0.008 {I8}
233U 2cG (liquid,1986Kr10)
233U cG $(103.86|g)(311.9|g)(|q): A{-2}=-0.001 {I6}, A{-4}=+0.012 {I8}
233U 2cG (solid,1986Kr10);
233U 3cG A{-2}=+0.002 {I5} (liquid), +0.001 {I4} (solid) FOR A{-4}=0 (1986Kr10)
233U 2 G EL1C=2.9 6 (1966Ze02)
233U cG $L1:L2:M1:M2:M3:N:O=100:15:24:4.2:1.2:7.0:1.6 (1966Ze02), |d=0.14 {I7};
233U 2cG L1:L2:M1:M2:N:O=100:7:24:7.1:4.7:1.2 (1962Sc03), |d<0.17;
233U 3cG L1:L2:L3:M1:N=100:18:4:30:13 (1961Al19), |d=0.20 {I3};
233U 4cG 1% {I1} E2 or |d=0.10 {I+4-10} in 1963Bi03, and |d<0.1 (1959Al02)
233U 5cG from ce. Other: 1985DeZR
233U G 375.407 10 1.781 18 E2 0.0981 C
233U S G KC=0.0491 7$LC=0.0360 5$MC=0.00963 14
233U S G NC=0.00261 4$OC=0.000610 9$PC=0.0001058 15$QC=2.72E-6 4
233U cG E$weighted average of 375.48 {I16} (2010Ko27), 375.404 {I5} (1990Ko41),
233U 2cG 375.45 {I4} (1971Vo02, crystal), 375.40 {I5} (1971Cl03),
233U 3cG 375.35 {I32} (1961Al19, crystal)
233U cG RI$weighted average of 1.75 {I8} (2011Ko32), 1.55 {I21} (2004Sh07),
233U 2cG 1.817 {I16} (2002Lu01), 1.782 {I18} (2000Sc04), 1.783 {I16} (2000Wo01),
233U 3cG 1.604 {I26} (1990Ko41), 1.785 {I26} (1984Va27), 1.76 {I2} (1979Ge08),
233U 4cG 1.6 {I3} (1973Va33). Uncertainty was doubled in 1990Ko41 in the
233U 5cG averaging procedure.
233U 2 G EL3C=0.40 8$ EM1C=1.0 1 (1988Wo01)
233U cG $L3:M1:M2=15.8 {I23}:40.9 {I22}:<0.32 (1988Wo01);
233U 2cG K:L1:L2:L3:M1+M2:N=100:20:46:16:16:11 (1966Ze02);
233U 3cG K:L2:L3:M2:N2=100:70:22:4:2 (1962Sc03); E2 in all including
233U 4cG 1963Bi03 from ce data. Other: 1985DeZR
233U G 415.767 10 4.55 5 M1+E2 2.5 1 0.121 4 *
233U S G KC=0.080 3$LC=0.0303 6$MC=0.00785 14
233U S G NC=0.00212 4$OC=0.000502 9$PC=9.03E-5 18$QC=3.98E-6 15
233U cG E$weighted average of 415.87 {I12} (2011Ko32), 415.764 {I5}
233U 2cG (1990Ko41), 415.76 {I4} (1971Vo02, crystal), 415.78 {I2} (1971Cl03),
233U 3cG 415.87 {I42} (1961Al19, crystal).
233U cG RI$weighted average of 4.44 {I16} (2011Ko32), 4.53 {I5} (2008De10),
233U 2cG 4.24 {I27} (2004Sh07), 4.603 {I19} (2002Lu01), 4.58 {I5} (2000Sc04),
233U 3cG 4.576 {I36} (2000Wo01), 4.50 {I5} (1984Va27), 4.52 {I4} (1979Ge08),
233U 4cG 4.2 {I4} (1973Va33). Other: 4.11 {I5} (1990Ko41), seems discrepant.
233U cG RI$most of the intensity belongs with placement from 415.77 level
233U cG $K:L1:L2:L3:M:N=100:22:14:4:9.1:3.2 (1966Ze02), |d=1.78 {I15};
233U 2cG K:L2:L3:M2=100:43:6.5:13 (1962Sc03), |d=4.9 {I+|@-15};
233U 3cG K:L1:L2:L3=100:22:16:3.8 (1961Al19), |d=2.1 {I+7-4}; 78% {I8} E2 or
233U 2cG |d=1.9 {I5} in 1963Bi03 from ce. Other: 1985DeZR
233U cG MR$deduced by evaluators using BrIccMixing code on ce data listed
233U 2cG above from 1966Ze02, 1962Sc03 and 1961Al19, except the L2/K ratio
233U 3cG from 1962Sc03 which seems discrepant. Uncertainty of 20% was assumed
233U 4cG in each ratio.
233U L 455.96 10 (5/2+) E
233U B 0.0013 3 10.6 1
233U S B EAV=29.78 55
233U G 415.767 * ?
233U F G FL=40.350
233U G 455.96 10 0.0028 5 [M1+E2] 0.19 13 a
233U F G FLAG=b
233U S G KC=0.14 11$LC=0.034 16$MC=0.0083 35
233U S G NC=0.00224 93$OC=5.4E-4 23$PC=1.01E-4 47$QC=6.8E-6 51