234U 234PA B- DECAY (1.159 M) 1963Bj02,1967Wa09,1975Ar2326NDS 202601
234U H TYP=FUL$AUT=S. Ota$CIT=NDS 207, 351 (2026)$CUT=1-Dec-2023$
234U dL E$Least-squares fitting is done by GLSC (version 17-Jul-2025)
234U c The |b-decay scheme of 1.17-min {+234}Pa isomer is based mainly on
234U 2c studies by 1963Bj02, 1967Wa09, and 1975Ar23. Others: 1990SC09,
234U 3c 1999Nz01 (data compilation) and 2004Br43.
234U cB IB$Deduced from intensity balance at each level.
234U cG $|b|g: 1963Bj02, 1955De40
234U cG $|g|g, |gce: see 1975Ar23, 1963Bj02
234U cG $|g|g(|q): 1960Wo05.
234U cG E$Weighted average of values in 1975Ar23 and 1990Sc09, except as
234U 2cG noted. Energies in 1967Wa09 and 1963Bj02 generally agree with those
234U 3cG given here. Earlier measurements: 1953St36, 1954Cr32, 1954Jo19,
234U 4cG 1955De40, 1956On07, 1959Sc31.
234U cG RI$Unless otherwise noted, from 1999Nz01, which were deduced by using
234U 2cG a statistical analysis of experimental results reported in 1992Si17,
234U 3cG 1990Sc09, 1986Mo09, 1975Ar23, 1971GuZQ, 1967Wa09, and 1963Bj02. The
234U 4cG Normalized Residuals (1994Ka08) method was applied to discrepant data
234U 5cG in 1999Nz01.
234U cG M$From conversion electron data in 1963Bj02. The intensities of
234U 2cG strong conversion electron lines have a 10% precision. Conversion
234U 3cG electron data from {+234}Pa (6.75 h) and {+234}Np decay also have
234U 4cG been used here.
234U cG RI(D)$Transitions identified in equilibrium spectrum ({+234}Th +
234U 2cG {+234}Pa g.s. + 1.17-min {+234}Pa). Intensities have been corrected
234U 3cG for contributions from {+234}Pa g.s. decay (1975Ar23).
234U cG M(N,M,O)$From {+234}Np |e decay.
234U cG M(P,R)$From {+234}Pa g.s. decay.
234U cG RI(C,O)$Measured by 1990Sc09 following the decay of {+238}U, in
234U 2cG equilibrium with its daughter nuclei. Only |g rays that do not have
234U 3cG any or have negligible contributions from {+234}Pa g.s. decay have
234U 4cG been included here. See 1990Sc09 for their complete list of
234U 5cG experimental |g-ray intensities.
234U cG E(S,R,M)$Transition was not observed in 1.17-min {+234}Pa |b{+-}
234U 2cG decay. Energy is from "adopted levels, gammas".
234U cG E(Y)$Reported only by 2004Br43 (in Russian). Intensity relative to
234U 2cG I|g(1001|g)=1000.
234U cL E$Deduced by evaluator from a least-squares fit to |g-ray energies.
234U cL J$From Adopted Levels.
234U cL J(K)$K=1-: |n7/2[743],|n5/2[633] state.
234U cL J(N)$K=1: |p3/2[651],|p5/2[642] state.
234U cL E(X)$If the 338.1|g to (2-) state is E1, then J|p(1796 level)=(1+).
234U cL $Additional levels at 750 keV, 1353 keV, and 1759 keV have been
234U 2cL proposed in 1999Nz01 with insufficient supporting experimental
234U 3cL evidence.
234U CL BAND(A)$KPI=0+ GS BAND.
234U CL BAND(B)$KPI=0- OCTUPOLE-VIBRATIONAL BAND.
234U CL BAND(D)$KPI=0+ COLLECTIVE BAND.
234U CL BAND(E)$KPI=2+ GAMMA-VIBRATIONAL BAND.
234U CL BAND(F)$KPI=2- OCTUPOLE-VIBRATIONAL BAND.
234U CL BAND(G)$KPI=0+ BAND.
234U CL BAND(H)$KPI=2+ BAND.
234U CL BAND(I)$KPI=(0-) BAND.
234U c 1963Bj02: |b-decay from the {+234}Pu isomer from {+234}Th was studied
234U 2c two |b spectrometers ("orange" spectrometer") and NaI scintillators
234U 3c using a |b-|g coincidence technique.
234U c 1967Wa09: |b-decay from the {+234}Pu isomer from {+234}Th was studied
234U 2c a |b spectrometer ("orange" spectrometer"), NaI scintillators, and
234U 3c Ge(Li) detectors using a |b-|g coincidence technique.
234U c 1975Ar23: |b-decay from the {+234}Pu isomer from {+234}Th was studied
234U 2c using NaI scintillators and Ge(Li) detectors by |b-|g coincidence
234U 3c technique.
234U c 1999Nz01: Compiled data and provided evaluation of I|g.
234U c 2004Br43 (in Russian): |b-decay from the {+234}Pu isomer from
234U 2c {+234}Th (produced by {+238}U |a decay) was studied. Measured E|g and
234U 3c I|g above 2000 keV .
234U c 2006Al28: Natural U decay (decays to {+234}Pa via |a-decay to
234U 2c {+234}Th) was studied using a single HPGe detector surrounded by 10
234U 3c cm thick lead cylinder. One U sample was in the form of fine powder
234U 4c and the other was powdered U mixed with distilled water.
234U D Transition strength is calculated by Java-RULER (version 28-Apr-2022)
234U D Modified by E. Browne (June 2006).
234U D BG(T): BCE(K 811G)(T) T(810 level) LT 0.1 NS (1962Lo11).
234U D X rays: I(XK)=0.50% (scin 1963Bj02).
234U D CC$FROM BrIcc v2.3e (17-Jun-2020) 2008Ki07, "Frozen Orbitals" appr.
234U DB EAV,LOGFT$FROM BetaShape v2.4 (Jun-2024) 2023MO21.
234PA P 76.5 4 (0-) 1.159 M 11 2194 4
234PA cP QP$From 2021WA16
234U N 0.000843 8 0.9984 4 1.0016
234U cN NR$The absolute intensities of photons from {+234}Pa |b{+-} decay
234U 2cN were measured in equilibrium with its parents, {+234}Th and {+238}U,
234U 3cN by various groups. The absolute intensity of I|g(1001|g)=0.843% {I8}
234U 4cN per 100 1.159 min {+234}Pa |b{+-} decays has been adopted and used to
234U 5cN normalize the decay scheme in this evaluation. This value is a
234U 6cN weighted average (|h{+2}/|n=4.6) of the following absolute |g-ray
234U 7cN intensities: I|g(1001|g)=0.828% {I18} (1971GuZY)(evaluator increased
234U 8cN its uncertainty by 2% because the original value included only the
234U 9cN statistical component). 0.834% {I7} (1986Mo09); 0.839% {I5}
234U acN (1990Sc09); 0.788% {I43} (1992Li02); 0.845% {I21} (1992Si17); 0.818%
234U bcN {I30} (1992Ja17); 0.910% {I25} (1993Su37); 0.924% {I17} (1999An40);
234U ccN 0.861% {I15} (2003Yu06). Other recommended evaluated absolute
234U dcN intensities are: 0.839% {I12} (1994Ak05, 1994Du15); 0.835% {I11}
234U ecN (1998Ad08); 0.835% {I4} (1999Nz01). Other: 1963Bj02. The
234U fcN experimentally deduced average radiation energy of 2258.8 keV {I24}
234U gcN is consistent with 2267.9 keV {I40} from the most recent mass
234U hcN adjustment (2021Wa16) suggesting that the decay scheme is consistent
234U icN and complete.
234U PN 1.0 3
234U G 243.5 8 0.59 10
234U 2 G %IG=5.0E-4 9
234U G 557.3 10 0.85 17
234U 2 G %IG=7.2E-4 15
234U G 647.7 8 1.87 17
234U 2 G %IG=0.00157 15
234U G 760.3 10 1.87 17
234U 2 G %IG=0.00157 15
234U G 887.29 10 8.42 11
234U F G FLAG=C
234U 2 G %IG=0.00709 12
234U G 1220.37 10 1.08 10
234U F G FLAG=C
234U 2 G %IG=9.1E-4 9
234U G 1353.0 15 1.29 9
234U F G FLAG=D
234U 2 G %IG=0.00109 8
234U G 1720.5 15 0.40 17
234U F G FLAG=D
234U 2 G %IG=3.4E-4 15
234U G 1732.2 15 2.2 3
234U 2 G %IG=0.00185 27
234U G 1759.81 10 1.74 6
234U F G FLAG=C
234U 2 G %IG=0.00146 5
234U G 2022.24 12 0.22 2
234U F G FLAG=Y
234U 2 G %IG=1.85E-4 17
234U G 2041.23 13 0.13 1
234U F G FLAG=Y
234U 2 G %IG=1.09E-4 9
234U G 2065.80 13 0.084 12
234U F G FLAG=Y
234U 2 G %IG=7.1E-5 11
234U G 2093.19 38 0.024 7
234U F G FLAG=Y
234U 2 G %IG=2.0E-5 6
234U G 2102.14 15 0.072 10
234U F G FLAG=Y
234U 2 G %IG=6.1E-5 9
234U G 2136.69 14 0.084 5
234U F G FLAG=Y
234U 2 G %IG=7.1E-5 4
234U L 0.0 0+ A
234U B 97.57 4 5.605 5
234U S B EAV=822.9 16
234U cB E$E|b=2305 (I|b=90) (1953St36), 2300 (I|b=98) (1955De40), and 2290
234U 2cB {I20} (1963Bj02), respectively.
234U L 43.4980 10 2+ A
234U G 43.498 1 E2 713 10
234U S G LC=520 7$MC=143.5 20$NC=38.9 5$OC=8.91 12$PC=1.441 20$QC=0.00339 5
234U cG E$From {+238}Pu |a decay.
234U cG $Ice(L2)=250; L2:L3:M=25:27:34 (1963Bj02).
234U L 143.09 9 4+ A
234U G 99.9 E2 13.39 19 S
234U S G LC=9.75 14$MC=2.71 4$NC=0.735 10$OC=0.1688 24$PC=0.0276 4$
234U S G QC=0.0001097 15
234U L 786.312 5 1- B
234U G 742.813 5 126.6 24 E1 0.006369
234U S G KC=0.00518 7$LC=0.000895 13$MC=0.0002131 30$NC=5.71E-5 8$
234U S G OC=1.378E-5 19$PC=2.61E-6 4$QC=1.951E-7 27
234U 2 G %IG=0.1066 23
234U cG E,RI$From 2000Ni13. Other intensity results: I|g=95.8 {I4}
234U 2cG (1975Ar23), I|g=106.6 {I24} (1971GuZQ), I|g=117 {I2} (1986Mo09).
234U cG E$From 1972Sa06.
234U cG $Ice(K)<1 (not observed).
234U G 786.28 10 64.6 8 (E1) 0.005738
234U S G KC=0.00467 7$LC=0.000804 11$MC=0.0001912 27$NC=5.12E-5 7$
234U S G OC=1.237E-5 17$PC=2.349E-6 33$QC=1.766E-7 25
234U 2 G %IG=0.0544 9
234U cG E$From 1972Sa06.
234U cG $Ice(K)<1 (not observed).
234U B 0.059 4 8.138 30
234U S B EAV=506.0 16
234U L 810.36 8 0+ 0.1 NS LT D
234U cL T$From 1962Lo11
234U G 766.42 10 377 4 (E2) 0.0186726
234U S G KC=0.01336 19$LC=0.00396 6$MC=0.001003 14$NC=0.000271 4$OC=6.45E-5 9$
234U S G PC=1.182E-5 17$QC=6.25E-7 9
234U 2 G %IG=0.317 5
234U cG E$From 1972Sa06.
234U cG RI$Other measurement: 429 {I22} (2006Al28)
234U G 811 E0 850
234U cG TI$from Ice(811)/I|g(1001)=0.51/0.60=0.85 (1963Bj02)
234U cG E$From 1963Bj02. 809.8 from {+234}Np |e decay, and 810.0 {I7} from
234U 2cG 6.75-h {+234}Pa |b{+-} decay.
234U B 0.948 13 6.907 9
234U S B EAV=496.6 16
234U cB $E|b=1500 (I|b=9) (1953St36), 1500 (1955De40), and 1530 {I50}
234U 2cB (1963Bj02), respectively.
234U L 849.17 7 3- B
234U G 705.94 12 6.7 4 [E1] 0.0069810
234U S G KC=0.00568 8$LC=0.000987 14$MC=0.0002350 33$NC=6.30E-5 9$
234U S G OC=1.519E-5 21$PC=2.88E-6 4$QC=2.134E-7 30
234U 2 G %IG=0.00564 34
234U G 805.75 10 7.0 4 [E1] 0.005498
234U S G KC=0.00447 6$LC=0.000768 11$MC=0.0001826 26$NC=4.89E-5 7$
234U S G OC=1.182E-5 17$PC=2.245E-6 31$QC=1.693E-7 24
234U 2 G %IG=0.00589 34
234U L 851.92 5 2+ D
234U G 41.82 S
234U G 708.2 10 0.8 [E2] 0.0219431
234U S G KC=0.01537 22$LC=0.00489 7$MC=0.001247 18$NC=0.000337 5$OC=8.00E-5 12$
234U S G PC=1.458E-5 21$QC=7.28E-7 10
234U 2 G %IG=6.7E-4
234U G 808.20 10 3.3 2 E0+E2
234U F G FLAG=N
234U 2 G %IG=0.00278 17
234U cG $Ice(K)<20 (line questionable, 1963Bj02).
234U G 851.58 10 8.2 1 [E2] 0.0151421
234U S G KC=0.01109 16$LC=0.00302 4$MC=0.000760 11$NC=0.0002049 29$
234U S G OC=4.89E-5 7$PC=9.03E-6 13$QC=5.10E-7 7
234U 2 G %IG=0.00690 11
234U L 926.66 7 2+ E
234U G 783.4 1 0.046 3 [E2] 0.0178725 S
234U F G FLAG=S
234U S G KC=0.01285 18$LC=0.00374 5$MC=0.000946 13$NC=0.000255 4$OC=6.08E-5 9$
234U S G PC=1.116E-5 16$QC=5.99E-7 8
234U 2 G %IG=3.87E-5 26
234U cG RI$Deduced by evaluator from I|g(783.4|g)/I|g(926.7|g)=0.29 {I3}/9.3
234U 2cG {I6}=0.031 {I4} in {+234}Pa g.s. decay.
234U G 883.22 10 4.2 4 E2 0.0140920
234U S G KC=0.01040 15$LC=0.00276 4$MC=0.000692 10$NC=0.0001866 26$
234U S G OC=4.46E-5 6$PC=8.25E-6 12$QC=4.76E-7 7
234U 2 G %IG=0.00354 34
234U cG RI$From 1975Ar23. I|g=20.5 {I7} (1971GuZQ) and I|g=22.2 {I2}
234U 2cG (1990Sc09) significantly disagree with value from 1975Ar23, probably
234U 3cG due to source contamination.
234U cG E$measured by 1972Sa06 from decays of 6.75-h and 1.17-min {+234}Pa in
234U 2cG equilibrium with {+238}U source.
234U cG $I|g(883)/I|g(926)=1.3 {I1} from {+238}Pu |a decay compares with
234U 2cG I|g(883)/I|g(926)=1.10 {I3} from {+234}Pa(1.159 min) |b{+-} decay
234U 3cG suggesting most of its intensity de-excites the 927-keV level.
234U G 926.61 10 1.47 16 (E2) 0.0128418
234U F G FLAG=P
234U S G KC=0.00956 13$LC=0.002453 34$MC=0.000613 9$NC=0.0001653 23$
234U S G OC=3.96E-5 6$PC=7.34E-6 10$QC=4.35E-7 6
234U 2 G %IG=0.00124 15
234U cG RI$From 1975Ar23. I|g=20.5 {I12} (1971GuZQ) and I|g=20.6 {I2}
234U 2cG (1990Sc09) significantly disagree with value from 1975Ar23, probably
234U 3cG due to source contamination.
234U L 989.435 20 2- F
234U G 62.70 1 1.4 5 E1 0.426 6 S
234U F G FLAG=R
234U S G LC=0.320 4$MC=0.0791 11$NC=0.02094 29$OC=0.00481 7$PC=0.000795 11$
234U S G QC=3.22E-5 5
234U 2 G %IG=0.0012 +5-4
234U cG RI$Deduced by evaluator from the ratios of
234U 2cG I|g(62.70|g)/I|g(203|g)=1.5 {I4}/1.19 {I10} and
234U 3cG I|g(62.70|g)/I|g(946|g)=1.5 {I4}/13.0 {I8}, in {+234}Pa g.s. |b{+-}
234U 4cG decay.
234U G 140.1 10 1.52 17 M1+E2 1.2 6 5.3 18
234U L G FL=849.17
234U F G FLAG=P
234U S G KC=2.9 21$LC=1.76 25$MC=0.47 8$NC=0.127 23$OC=0.030 5$PC=0.0051 6$
234U S G QC=1.5E-4 9
234U 2 G %IG=0.00128 16
234U cG $I|g=0.42 {I10} is expected from I|g(140|g)/I|g(203|g) =49 {I5}/119
234U 2cG {I10}, I|g=0.37 {I6} from I|g(140|g)/I|g(945|g) =0.49 {I5}/13.0 {I8},
234U 3cG measured in {+234}Pa g.s. decay.
234U G 203.3 8 2.0 5 M1+E2 1.5 4 1.40 33
234U F G FLAG=P
234U S G KC=0.83 32$LC=0.420 12$MC=0.1109 23$NC=0.0300 6$OC=0.00705 15$
234U S G PC=0.00124 4$QC=4.3E-5 14
234U 2 G %IG=0.0017 +5-4
234U G 945.94 2 12 1 (E1) 0.004126
234U F G FLAG=P
234U S G KC=0.00337 5$LC=0.000571 8$MC=0.0001355 19$NC=3.63E-5 5$OC=8.79E-6 12$
234U S G PC=1.675E-6 23$QC=1.286E-7 18
234U 2 G %IG=0.0101 9
234U cG RI$From 1975Ar23. I|g=30.2 {I7} (1971GuZQ) and I|g=28.2 {I3}
234U 2cG (1990Sc09) significantly disagree with value from 1975Ar23, probably
234U 3cG due to source contamination.
234U B 0.009 3 9.39 15 ?
234U S B EAV=400.8 14
234U cB $E|b= 1250 (1963Bj02). E|b=580 (I|b=1) (1953St36) and 600 (1955De40).
234U 2cB Others: 1954Jo19, 1959Sc31.
234U L 1044.54 1 0+ G
234U G 193.4 8 0.85 17 [E2] 0.847 18 &
234U L G FL=851.92
234U S G KC=0.1629 25$LC=0.500 11$MC=0.1376 31$NC=0.0374 9$OC=0.00862 20$
234U S G PC=0.001440 33$QC=1.371E-5 25
234U 2 G %IG=7.2E-4 15
234U G 236 1 E0
234U X G K/T=0.80$L/T=0.15
234U cG E$measured by 1963Bj02 (s ce). E|g=234.6 {I2} was measured in
234U 2cG {+234}Np decay.
234U cG $Total Ice=87 {I9} from measured Ice(K)=70 and K/L=70/13.
234U G 258.227 3 90.3 24 (E1) 0.05488
234U S G KC=0.0434 6$LC=0.00859 12$MC=0.002074 29$NC=0.000554 8$
234U S G OC=0.0001321 18$PC=2.419E-5 34$QC=1.499E-6 21
234U 2 G %IG=0.0760 22
234U cG E,RI$From 2000Ni13. Other intensity results: I|g=97 {I4} (1975Ar23),
234U 2cG I|g=87 {I2} (1971GuZQ), I|g=87 {I4} (1986Mo09), I|g=87{I5},
234U 3cG (1990Sc09), I|g=91.4 {I48} (2006Al28).
234U cG $Ice(K)<5 (not observed). 80.9 {I33} (1975Ar23).
234U G 1001.03 10 1000.0 24 E2 0.0110716
234U S G KC=0.00835 12$LC=0.002039 29$MC=0.000507 7$NC=0.0001367 19$
234U S G OC=3.28E-5 5$PC=6.10E-6 9$QC=3.76E-7 5
234U 2 G %IG=0.842 8
234U cG E$measurement of 1972Sa06.
234U cG $Ice(K)=5.7.
234U cG RI$Other measurement: 1116 {I57} (2006Al28).
234U B 1.002 13 6.610 9
234U S B EAV=406.0 15
234U L 1084.95 6 2+ G
234U G 233.6 2 S
234U L G FL=851.92
234U F G FLAG=S
234U cG TI$I(|g+ce)|?0.8%, from I(|g+ce)(233.6|g)/I|g(1042|g)|?0.7, deduced
234U 2cG in {+234}Np |e decay.
234U G 235.9 3 0.10 5 [E1] 0.067310 S
234U L G FL=849.17
234U F G FLAG=S
234U S G KC=0.0532 8$LC=0.01067 15$MC=0.00258 4$NC=0.000689 10$OC=0.0001639 23$
234U S G PC=2.99E-5 4$QC=1.815E-6 26
234U 2 G %IG=8E-5 4
234U cG RI$deduced by evaluators from branching of
234U 2cG I|g(235.9|g)/I|g(942|g)=0.034 {I13}, adopted from measurements in
234U 3cG {+238}Pu |a decay and {+234}Np |e decay.
234U G 299.0 10 0.77 16 [E1] 0.03956
234U S G KC=0.0315 5$LC=0.00608 10$MC=0.001467 24$NC=0.000392 6$OC=9.37E-5 15$
234U S G PC=1.726E-5 28$QC=1.105E-6 17
234U 2 G %IG=6.5E-4 14
234U cG RI$I|g(299|g)/I|g(942|g)=0.10 {I3} from {+238}Pu |a decay, 0.085
234U 2cG {I10} from {+234}Np |e decay, 0.30 {I13} from 6.75-h {+234}Pa |b{+-}
234U 3cG decay, and 0.26 {I6} here. The adopted ratio of 0.10 {I3} yields
234U 4cG I|g(299.0|g)=0.25 {I8}.
234U G 941.96 10 3.0 1 [E2] 0.0124417
234U F G FLAG=C
234U S G KC=0.00929 13$LC=0.002357 33$MC=0.000589 8$NC=0.0001587 22$
234U S G OC=3.80E-5 5$PC=7.05E-6 10$QC=4.21E-7 6
234U 2 G %IG=0.00253 9
234U G 1041.70 10 1.47 8 [E2,M1] 0.023 12
234U F G FLAG=C
234U S G KC=0.018 10$LC=0.0036 17$MC=9.E-4 4$NC=2.3E-4 11$OC=5.7E-5 27$
234U S G PC=1.1E-5 5$QC=8.E-7 5
234U 2 G %IG=0.00124 7
234U cG $Ice(K)<0.8 (not observed).
234U G 1084.25 10 1.0 3 [E2] 0.0095213
234U L G FL=0.0
234U S G KC=0.00726 10$LC=0.001694 24$MC=0.000419 6$NC=0.0001130 16$
234U S G OC=2.71E-5 4$PC=5.07E-6 7$QC=3.24E-7 5
234U 2 G %IG=8.4E-4 26
234U L 1125.01 10 2+ H
234U G 137.23 5 0.056 22 [E1] 0.238934 S
234U L G FL=989.435
234U F G FLAG=S
234U S G KC=0.1841 26$LC=0.0413 6$MC=0.01006 14$NC=0.00268 4$OC=0.000630 9$
234U S G PC=0.0001117 16$QC=5.88E-6 8
234U 2 G %IG=4.7E-5 19
234U cG RI$Deduced from I|g(137.23|g)/I|g(1082|g)=2.6 {I8}/49 {I3}, measured
234U 2cG in {+234}Pa g.s. decay.
234U G 199.9 10 0.68 13(E0+E2+M1) 1.9 12
234U F G FLAG=P
234U S G KC=1.3 12$LC=0.457 25$MC=0.1177 32$NC=0.0318 9$OC=0.00755 18$
234U S G PC=0.00136 11$QC=6.E-5 5
234U 2 G %IG=5.7E-4 12
234U cG $I|g(199.9|g)/I|g(1082|g)=0.14 {I5} from 6.75-h {+234}Pa |b{+-}
234U 2cG decay, 0.64 {I20} here. Use of the ratio from 6.75-h {+234}Pa decay
234U 3cG yields I|g(199.9|g)=0.12 {I5}. Since accuracy and correctness of a
234U 4cG conversion coefficient rely on the measured I|g and Ice values,
234U 5cG because of the uncertainty on I|g's, no conversion coefficient has
234U 6cG been adopted, and I(|g+ce)|?5% [deduced from
234U 7cG I(|g+ce)(199.9|g)/I|g(1082|g)|?5.9 in {+234}Pa g.s. decay data] has
234U 8cG been used for obtaining the I|b value.
234U G 275.5 8 0.37 7 [M1,E2] 0.8 5
234U L G FL=851.92
234U S G KC=0.5 5$LC=0.16 4$MC=0.039 8$NC=0.0106 21$OC=0.0025 6$PC=4.7E-4 13$
234U S G QC=2.7E-5 21
234U 2 G %IG=3.1E-4 6
234U G 316.7 1 0.22 6 [E2] 0.159722 S
234U F G FLAG=S
234U S G KC=0.0677 9$LC=0.0674 9$MC=0.01822 26$NC=0.00494 7$OC=0.001150 16$
234U S G PC=0.0001972 28$QC=4.01E-6 6
234U 2 G %IG=1.9E-4 5
234U cG RI$Deduced by evaluator from I|g(3167|g)/I|g(1082|g)=10 {I1}/49 {I3}
234U 2cG in {+234}Pa g.s. decay.
234U G 340.2 1 0.08 4 [E1] 0.02984 S
234U F G FLAG=S
234U S G KC=0.02385 33$LC=0.00453 6$MC=0.001090 15$NC=0.000292 4$OC=6.97E-5 10$
234U S G PC=1.292E-5 18$QC=8.49E-7 12
234U 2 G %IG=6.8E-5 34
234U cG RI$Deduced from I|g(340.1|g)/I|g(1082|g)=3.9 {I8}/49 {I3} in {+234}Pa
234U 2cG g.s. |b{+-} decay.
234U G 1081.9 10 1.07 22 (M1) 0.03185
234U F G FLAG=P
234U S G KC=0.0255 4$LC=0.00478 7$MC=0.001151 16$NC=0.000310 4$OC=7.53E-5 11$
234U S G PC=1.454E-5 21$QC=1.167E-6 17
234U 2 G %IG=9.0E-4 20
234U G 1124.93 10 0.4 1 [E2] 0.0088812 @
234U L G FL=0.0
234U S G KC=0.00681 10$LC=0.001558 22$MC=0.000385 5$NC=0.0001036 15$
234U S G OC=2.489E-5 35$PC=4.67E-6 7$QC=3.02E-7 4
234U 2 G %IG=3.4E-4 9
234U cG RI$4.0 {I5} was measured for this doubly-placed |g. I|g(leaving 1126
234U 2cG level)=0.53 {I3}, deduced by the evaluator from
234U 3cG I|g(1126|g)/I|g(1082|g)=29 {I3}/49 {I3} in {+234}Pa g.s. |b{+-} decay.
234U B 0.0043 4 9.451 41 1U
234U S B EAV=354.0 14
234U L 1174.1 4 (1,2+)
234U G 184.7 5 2.0 2
234U 2 G %IG=0.00169 19
234U G 387.6 8 1.1 1 @
234U 2 G %IG=9.3E-4 9
234U cG RI$1.70 {I17} was measured for this doubly placed |g. I|g=0.556 {I20}
234U 2cG has been deduced by the evaluators for the 387.6|g deexciting the
234U 3cG 1237-keV level.
234U cG CC$if the 184.7|g (decays to 2- state) is M1, then, J|p(1174
234U 2cG level)=1-, and the 387.6|g (which decays to 1- state) should be
234U 3cG M1,E2. |a(M1)=0.529, |a(E2)=0.0917, |a(E1)=0.0228.
234U G 1174.2 10 2.3 2
234U 2 G %IG=0.00194 17
234U B 0.0045 3 8.786 30
234U S B EAV=356.9 15
234U L 1237.37 5 1- I
234U G 193.4 8 0.85 17 [E1] 0.106518 &
234U S G KC=0.0835 14$LC=0.01735 30$MC=0.00421 7$NC=0.001123 20$OC=0.000266 5$
234U S G PC=4.81E-5 8$QC=2.78E-6 5
234U 2 G %IG=7.2E-4 15
234U G 247.7 8 0.29 2 [M1,E2] 1.0 7
234U S G KC=0.7 6$LC=0.22 4$MC=0.056 8$NC=0.0151 20$OC=0.0036 6$PC=0.00066 14$
234U S G QC=3.6E-5 28
234U 2 G %IG=2.44E-4 17
234U cG RI$Deduced by the evaluator from I|g(247.79|g)/I|g(1193.77|g)=0.109
234U 2cG {I7}/6.02 {I24} in {+234}Np |e decay. I|g=1.14 {I25} was measured by
234U 3cG 1975Ar23. The I(247.7|g) measured in 1.159 min {+234}Pa |b-decay may
234U 4cG possibly include contribution from another source.
234U G 311.0 10 0.10 1 [E1] 0.03636
234U S G KC=0.0289 5$LC=0.00556 9$MC=0.001339 21$NC=0.000358 6$OC=8.55E-5 14$
234U S G PC=1.579E-5 25$QC=1.019E-6 16
234U 2 G %IG=8.4E-5 9
234U cG RI$Deduced from I|g(310.52|g)/I|g(1193.77|g)= 0.039 {I4}/6.02 {I24}
234U 2cG in {+234}Np |e decay. I|g(311|g)=0.61 {I12} was measured by 1975Ar23.
234U 3cG The I(311.0|g) measured in 1.159 min {+234}Pa |b-decay may possibly
234U 4cG include contribution from another source.
234U cG E$E|g=310.52 {I10} from {+234}Np |e decay.
234U G 387.6 8 0.556 20 [E2] 0.089914 @
234U L G FL=849.17
234U S G KC=0.0463 7$LC=0.0321 5$MC=0.00858 14$NC=0.00232 4$OC=0.000543 9$
234U S G PC=9.45E-5 15$QC=2.54E-6 4
234U 2 G %IG=4.68E-4 18
234U cG E$387.94 {I6} was measured in {+234}Np |e decay.
234U cG RI$Deduced from I|g(387.6|g)/I|g(1193.77|g)= 0.208 {I12}/6.02 {I24}
234U 2cG in {+234}Np |e decay.
234U G 427.4 2 0.024 6 [E1] 0.0185026 S
234U F G FLAG=S
234U S G KC=0.01488 21$LC=0.00274 4$MC=0.000657 9$NC=0.0001758 25$OC=4.22E-5 6$
234U S G PC=7.88E-6 11$QC=5.40E-7 8
234U 2 G %IG=2.0E-5 5
234U cG RI$Deduced from I|g(427.4|g)/I|g(1193.77|g)= 0.009 {I2}/6.02 {I24} in
234U 2cG {+234}Np |e decay.
234U G 450.97 10 3.70 17 M1+E2 0.70 0.240634
234U F G FLAG=O
234U S G KC=0.1874 26$LC=0.0400 6$MC=0.00979 14$NC=0.00264 4$OC=0.000638 9$
234U S G PC=0.0001213 17$QC=8.79E-6 12
234U 2 G %IG=0.00311 15
234U G 1193.73 12 16.14 12 E1 0.002774
234U F G FLAG=O
234U S G KC=0.002260 32$LC=0.000377 5$MC=8.93E-5 12$NC=2.392E-5 33$
234U S G OC=5.80E-6 8$PC=1.109E-6 16$QC=8.70E-8 12
234U 2 G %IG=0.01358 17
234U cG E$measurement of 1972Sa06.
234U cG RI$Other measurement: 17.8 {I83} (2006Al28).
234U G 1237.26 10 6.24 11 E1 0.002624
234U F G FLAG=O
234U S G KC=0.002127 30$LC=0.000354 5$MC=8.38E-5 12$NC=2.246E-5 31$
234U S G OC=5.44E-6 8$PC=1.042E-6 15$QC=8.20E-8 11
234U 2 G %IG=0.00525 11
234U B 0.0109 7 8.311 29
234U S B EAV=333.3 15
234U L 1434.73 7 1- K
234U G 197.91 15 0.032 8 [M1,E2] 2.0 12 S
234U F G FLAG=S
234U S G KC=1.3 12$LC=0.473 22$MC=0.1220 31$NC=0.0330 9$OC=0.00782 11$
234U S G PC=0.00141 10$QC=7.E-5 5
234U 2 G %IG=2.7E-5 7
234U cG RI$Deduced from I|g(197.9|g)/I|g(1434.13|g)=0.018 {I4}/6.38 {I25} in
234U 2cG {+234}Np |e decay.
234U G 445.91 10 0.036 8 [M1,E2] 0.20 14 S
234U F G FLAG=S
234U S G KC=0.15 12$LC=0.036 16$MC=0.009 4$NC=0.0024 10$OC=5.8E-4 24$
234U S G PC=1.1E-4 5$QC=7.E-6 5
234U 2 G %IG=3.0E-5 7
234U cG RI$Deduced from I|g(445.9|g)/I|g(1434.13|g)=0.020 {I4}/6.38 {I25} in
234U 2cG {+234}Np |e decay.
234U G 624.6 10 0.137 15 [E1] 0.0087713
234U S G KC=0.00712 10$LC=0.001252 18$MC=0.000299 4$NC=8.00E-5 11$
234U S G OC=1.929E-5 28$PC=3.64E-6 5$QC=2.66E-7 4
234U 2 G %IG=1.15E-4 14
234U cG RI$1.42 {I15} listed by 1975Ar23 is assumed by the evaluators to be
234U 2cG in error: the ratio of I|g(625|g)/I|g(1434|g)=0.0119 {I12} from I|g's
234U 3cG measured in {+234}Np |e decay does not agree with the ratio that one
234U 4cG obtains in 1.17-min {+234}Pa |b{+-} decay, if I|g(625|g)=1.42 {I5}.
234U 5cG The ratio observed in {+234}Np |e decay is adopted, since data of
234U 6cG 1967Wa09 confirm it.
234U G 649.0 10 0.049 10 [M1,E2] 0.08 5 @
234U S G KC=0.06 4$LC=0.012 6$MC=0.0031 15$NC=8.E-4 4$OC=2.0E-4 10$
234U S G PC=3.8E-5 19$QC=2.7E-6 18
234U 2 G %IG=4.1E-5 9
234U cG RI$1.06 {I22} was measured for this doubly-placed |g. The total I|g
234U 2cG is divided by the evaluator such that the I|g(649|g)/I|g(1434|g)
234U 3cG ratio from the 1435-keV level and the I|g(649|g)/I|g(691|g) ratio
234U 4cG from the 1500-keV level agree with those in {+234}Np |e decay.
234U G 1392.7 10 4.11 24 E1 2.21E-33
234U F G FLAG=N
234U S G KC=0.001743 24$LC=0.000288 4$MC=6.82E-5 10$NC=1.827E-5 26$
234U S G OC=4.43E-6 6$PC=8.50E-7 12$QC=6.75E-8 9
234U 2 G %IG=0.00346 21
234U cG E$From 1975Ar23
234U cG $I|g=3.89 {I10} measured by 1990Sc09 and 1.56 {I15} measured by
234U 2cG 1975Ar23 do not agree with each other. I|g of 1990Sc09 may include
234U 3cG some counts from the 1393.9|g of {+234}Pa g.s. decay. However, the
234U 4cG 1434|g deexciting the same level should not have such contamination
234U 5cG from neighboring |g in the |b{+-} decay from {+234}Pa g.s. The ratio,
234U 6cG I|g(1392|g)/I|g(1434|g)=0.356 {I20} in {+234}Np |e decay, while it is
234U 7cG 0.402 {I12} (1990Sc09) and 0.190 {I28} (1975Ar23), respectively. The
234U 8cG evaluator therefore used the ratio of 0.356 {I20} to obtain
234U 9cG I|g(1392|g) given here.
234U G 1434.14 10 11.56 23 E1 2.13E-33
234U L G FL=0.0
234U F G FLAG=O
234U S G KC=0.001660 23$LC=0.000274 4$MC=6.48E-5 9$NC=1.737E-5 24$OC=4.21E-6 6$
234U S G PC=8.08E-7 11$QC=6.44E-8 9
234U 2 G %IG=0.00973 22
234U cG $Other measurements: I|g=8.2 {I9} (1975Ar23), 9.4 {I15} (1992Si17).
234U B 0.0097 4 8.042 20
234U S B EAV=261.2 14
234U L 1457.42 8 (2-)
234U G 670.8 10 0.44 10 [M1,E2] 0.07 4
234U S G KC=0.05 4$LC=0.011 6$MC=0.0028 13$NC=8.E-4 4$OC=1.8E-4 9$PC=3.5E-5 18$
234U S G QC=2.5E-6 17
234U 2 G %IG=3.7E-4 9
234U G 1413.88 10 2.69 8 [E1] 2.17E-33
234U F G FLAG=C
234U S G KC=0.001700 24$LC=0.000281 4$MC=6.64E-5 9$NC=1.780E-5 25$OC=4.32E-6 6$
234U S G PC=8.28E-7 12$QC=6.59E-8 9
234U 2 G %IG=0.00226 7
234U L 1501.34 29 (1)
234U G 649.0 10 1.2 3 @
234U L G FL=851.92
234U 2 G %IG=0.00101 26
234U G 691.0 3 10.6 2
234U 2 G %IG=0.00892 19
234U G 1458.5 15 2.2 5
234U 2 G %IG=0.0019 5
234U G 1501 2 1.1 AP
234U F G FLAG=D
234U 2 G %IG AP 9.3E-4
234U B 0.0127 6 7.802 22
234U S B EAV=237.5 14
234U L 1553.69 6 (1)
234U G 468.43 10 2.72 17
234U F G FLAG=C
234U 2 G %IG=0.00229 15
234U cG RI$Other measurement: 2.37 {I119} (2006Al28).
234U G 509.2 8 2.5 3
234U 2 G %IG=0.00211 27
234U G 702.00 10 8.6 2
234U L G FL=851.92
234U F G FLAG=C
234U 2 G %IG=0.00724 18
234U cG RI$Other measurement: 7.1 {I36} (2006Al28).
234U G 1510.21 10 15.5 2
234U F G FLAG=C
234U 2 G %IG=0.01305 21
234U G 1553.75 10 9.75 11
234U F G FLAG=C
234U 2 G %IG=0.00821 12
234U B 0.0321 6 7.295 12
234U S B EAV=219.1 14
234U L 1570.74 7 1+ N
234U G 135.32 8 0.0051 6 [E1] 0.246935 S
234U F G FLAG=S
234U S G KC=0.1901 27$LC=0.0428 6$MC=0.01043 15$NC=0.00278 4$OC=0.000653 9$
234U S G PC=0.0001156 16$QC=6.07E-6 9
234U 2 G %IG=4.3E-6 6
234U cG RI$Deduced from I|g(135|g)/I|g(1527|g)= 0.20 {I2}/112 {I5} in
234U 2cG {+234}Np |e decay.
234U G 485.44 7 0.0226 23 [M1,E2] 0.16 11 S
234U F G FLAG=S
234U S G KC=0.12 9$LC=0.028 13$MC=0.0069 30$NC=0.0019 8$OC=4.5E-4 20$
234U S G PC=8.E-5 4$QC=6.E-6 4
234U 2 G %IG=1.91E-5 21
234U cG RI$Deduced from I|g(485|g)/I|g(1527|g)= 0.89 {I7}/112 {I5} in
234U 2cG {+234}Np |e decay.
234U G 526.02 10 0.011 2 [M1] 0.217130 S
234U F G FLAG=S
234U S G KC=0.1732 24$LC=0.0331 5$MC=0.00797 11$NC=0.002148 30$OC=0.000522 7$
234U S G PC=0.0001007 14$QC=8.04E-6 11
234U 2 G %IG=9.3E-6 18
234U cG RI$Deduced from I|g(526|g)/I|g(1527|g)= 0.43 {I5}/112 {I5} in
234U 2cG {+234}Np |e decay.
234U G 581.19 10 0.097 12 [E1] 0.0100614 S
234U F G FLAG=S
234U S G KC=0.00815 11$LC=0.001445 20$MC=0.000345 5$NC=9.24E-5 13$
234U S G OC=2.227E-5 31$PC=4.20E-6 6$QC=3.03E-7 4
234U 2 G %IG=8.2E-5 11
234U cG RI$Deduced from I|g(581|g)/I|g(1527|g)= 3.8 {I4}/112 {I5} in {+234}Np
234U 2cG |e decay.
234U G 719.01 7 0.031 4 [M1+E2] 0.06 4 S
234U L G FL=851.92
234U F G FLAG=S
234U S G KC=0.045 30$LC=0.009 5$MC=0.0023 11$NC=6.2E-4 30$OC=1.5E-4 7$
234U S G PC=2.9E-5 15$QC=2.1E-6 14
234U 2 G %IG=2.6E-5 4
234U cG RI$Deduced from I|g(720|g)/I|g(1527|g)= 1.22 {I7}/112 {I5} in
234U 2cG {+234}Np |e decay.
234U G 760.53 15 0.0051 11 [M1] 0.081111 S
234U F G FLAG=S
234U S G KC=0.0648 9$LC=0.01226 17$MC=0.00295 4$NC=0.000795 11$OC=0.0001933 27$
234U S G PC=3.73E-5 5$QC=2.98E-6 4
234U 2 G %IG=4.3E-6 10
234U cG $Deduced from I|g(760|g)/I|g(1527|g)= 0.20 {I4}/112 {I5} in {+234}Np
234U 2cG |e decay.
234U G 1527.27 10 2.39 9 E2+M1 0.009 4
234U F G FLAG=C
234U S G KC=0.0071 31$LC=0.0014 6$MC=3.3E-4 13$NC=8.8E-5 35$OC=2.1E-5 9$
234U S G PC=4.1E-6 17$QC=3.2E-7 15
234U 2 G %IG=0.00201 8
234U cG $Other measurement: I|g=2.1 {I3} (1975Ar23).
234U G 1570.67 10 1.29 10 M1 0.0120417
234U F G FLAG=O
234U S G KC=0.00951 13$LC=0.001769 25$MC=0.000425 6$NC=0.0001145 16$
234U S G OC=2.79E-5 4$PC=5.38E-6 8$QC=4.34E-7 6
234U 2 G %IG=0.00109 9
234U cG $Other measurement: I|g=1.2 {I3} (1975Ar23).
234U B 0.00194 21 8.479 48 ?
234U S B EAV=213.2 14
234U L 1592.57 6 (1)
234U G 507.5 10 1.87 17
234U 2 G %IG=0.00157 15
234U G 740.10 8 13 2
234U L G FL=851.92
234U F G FLAG=C
234U 2 G %IG=0.0109 18
234U G 781.75 10 9.23 22
234U L G FL=810.36
234U F G FLAG=C
234U 2 G %IG=0.00777 20
234U cG $Other measurements: I|g=7.5 {I7} (1975Ar23), 7.2 {I10} (1992Si17).
234U G 1550.0 10 1.35 8
234U 2 G %IG=0.00114 7
234U G 1593.87 10 2.25 7
234U L G FL=0.0
234U F G FLAG=C
234U 2 G %IG=0.00189 6
234U B 0.0233 18 7.353 35
234U S B EAV=205.6 14
234U L 1601.9 8 1+
234U G 166.5 1 0.000298 [E1] 0.151421 S
234U F G FLAG=S
234U S G KC=0.1179 17$LC=0.0253 4$MC=0.00613 9$NC=0.001636 23$OC=0.000386 5$
234U S G PC=6.93E-5 10$QC=3.85E-6 5
234U 2 G %IG=2.4E-7 7
234U cG RI$Deduced from I|g(166.5|g)/I|g(1558|g)=0.6 {I1}/1872 {I20} in
234U 2cG {+234}Np |e decay.
234U G 516.60 6 0.016 4 (M1) 0.227932 S
234U F G FLAG=M
234U S G KC=0.1819 25$LC=0.0347 5$MC=0.00837 12$NC=0.002255 32$OC=0.000548 8$
234U S G PC=0.0001058 15$QC=8.44E-6 12
234U 2 G %IG=1.4E-5 4
234U cG RI$Deduced from I|g(516|g)/I|g(1558|g)= 31.3 {I19}/1872 {I20} in
234U 2cG {+234}Np |e decay.
234U G 557.24 6 0.010 2 (M1) 0.185926 S
234U F G FLAG=M
234U S G KC=0.1485 21$LC=0.0283 4$MC=0.00682 10$NC=0.001837 26$OC=0.000447 6$
234U S G PC=8.62E-5 12$QC=6.88E-6 10
234U 2 G %IG=8.4E-6 18
234U cG RI$Deduced from I|g(557|g)/I|g(1558|g)=21.4 {I13}/1872 {I20} in
234U 2cG {+234}Np |e decay.
234U G 750.12 6 0.021 5 (M1) 0.084112 S
234U L G FL=851.92
234U F G FLAG=M
234U S G KC=0.0672 9$LC=0.01272 18$MC=0.00306 4$NC=0.000825 12$OC=0.0002006 28$
234U S G PC=3.87E-5 5$QC=3.09E-6 4
234U 2 G %IG=1.8E-5 +5-4
234U cG RI$Deduced by the evaluator from I|g(750.7|g)/I|g(1558|g)=44.0
234U 2cG {I26}/1872 {I20} in {+234}Np |e decay.
234U G 791.94 5 0.012 4 [M1] 0.072810 S
234U F G FLAG=S
234U S G KC=0.0582 8$LC=0.01100 15$MC=0.00265 4$NC=0.000713 10$OC=0.0001735 24$
234U S G PC=3.35E-5 5$QC=2.68E-6 4
234U 2 G %IG=1.01E-5 35
234U cG RI$Deduced by the evaluator from the ratios of
234U 2cG I|g(791.9|g)/I|g(1558|g)=25.4 {I15}/1872 {I20} in {+234}Np |e decay.
234U G 1558.4 10 0.85 10 M1 0.0122817
234U F G FLAG=N
234U S G KC=0.00971 14$LC=0.001807 25$MC=0.000434 6$NC=0.0001169 16$
234U S G OC=2.84E-5 4$PC=5.49E-6 8$QC=4.43E-7 6
234U 2 G %IG=7.2E-4 9
234U G 1601.8 15 0.56 25 (M1) 0.0114616
234U F G FLAG=N
234U S G KC=0.00902 13$LC=0.001679 24$MC=0.000403 6$NC=0.0001086 15$
234U S G OC=2.64E-5 4$PC=5.10E-6 7$QC=4.11E-7 6
234U 2 G %IG=4.7E-4 22
234U B 0.00126 23 8.60 8
234U S B EAV=202.4 14
234U L 1667.3 4 (1-)
234U G 818.2 5 1.2 3 [E2] 0.0163823
234U S G KC=0.01190 17$LC=0.00334 5$MC=0.000843 12$NC=0.0002275 32$
234U S G OC=5.43E-5 8$PC=9.99E-6 14$QC=5.51E-7 8
234U 2 G %IG=0.00101 26
234U G 880.9 5 4.7 5
234U 2 G %IG=0.0040 5
234U G 1667.6 10 1.37 8
234U F G FLAG=D
234U 2 G %IG=0.00115 7
234U B 0.0061 5 7.765 37
234U S B EAV=180.1 14
234U L 1693.7 5 (1-) ?
234U G 456.7 10 0.85 17 [M1] 0.318 5
234U S G KC=0.253 4$LC=0.0485 7$MC=0.01171 18$NC=0.00315 5$OC=0.000767 12$
234U S G PC=0.0001479 23$QC=1.179E-5 18
234U 2 G %IG=7.2E-4 15
234U G 844.1 8 1.3 3 [E2] 0.0154022
234U S G KC=0.01127 16$LC=0.00309 4$MC=0.000777 11$NC=0.0002097 30$
234U S G OC=5.01E-5 7$PC=9.23E-6 13$QC=5.19E-7 7
234U 2 G %IG=0.00110 26
234U G 1694.1 10 0.54 11
234U F G FLAG=D
234U 2 G %IG=4.5E-4 10
234U B 0.0025 4 8.09 7
234U S B EAV=171.2 14
234U L 1781.28 7 (0+,1)
234U G 209.9 4 1.6 2
234U 2 G %IG=0.00135 18
234U G 543.98 10 4.36 19 0.11 10
234U 2 G %IG=0.00367 17
234U cG RI$Other measurement: 3.56 {I237} (2006Al28).
234U G 655.3 10 1.64 17 0.068 60
234U 2 G %IG=0.00138 16
234U G 695.5 10 1.93 16 0.059 52
234U 2 G %IG=0.00162 14
234U G 996.1 20 6.7 5
234U 2 G %IG=0.0056 4
234U G 1737.75 10 25.3 2
234U F G FLAG=C
234U 2 G %IG=0.02129 26
234U B 0.0355 8 6.699 16
234U S B EAV=142.3 13
234U L 1796.3 5 (1) X
234U G 338.1 8 1.3 3
234U 2 G %IG=0.00110 26
234U cG $The intensity imbalance at the 1457-keV level (I|b=-0.0014 {I6})
234U 2cG improves if the 338.1|g decaying to that level is E1 with |a=0.0304.
234U G 362.8 10 0.81 17
234U 2 G %IG=6.8E-4 15
234U cG $If the 338.1|g, decaying to (2-) state is E1, then the 362.8|g
234U 2cG decaying to the 1- state is also E1, with |a=0.0262.
234U G 1796.2 10 0.50 8
234U 2 G %IG=4.2E-4 7
234U B 0.0022 3 7.86 6
234U S B EAV=137.4 13
234U L 1809.00 7 (1-)
234U G 572.0 10 1.03 2 [M1] 0.173426
234U S G KC=0.1384 20$LC=0.0264 4$MC=0.00636 9$NC=0.001712 25$OC=0.000416 6$
234U S G PC=8.03E-5 12$QC=6.41E-6 9
234U 2 G %IG=8.67E-4 19
234U G 683.4 10 0.68 13 [E1] 0.0074111
234U S G KC=0.00603 9$LC=0.001050 15$MC=0.000250 4$NC=6.70E-5 10$
234U S G OC=1.618E-5 23$PC=3.06E-6 4$QC=2.261E-7 32
234U 2 G %IG=5.7E-4 12
234U G 960.0 10 1.0 4
234U 2 G %IG=8.5E-4 35
234U G 1765.44 10 10.4 1
234U F G FLAG=C
234U 2 G %IG=0.00875 12
234U G 1809.04 10 4.44 8
234U F G FLAG=C
234U 2 G %IG=0.00374 8
234U cG $Other measurements: I|g=4.3 {I5} (1975Ar23), 3.9 {I8} (1992Si17).
234U B 0.0149 4 6.993 18
234U S B EAV=133.3 13
234U L 1863.15 7 (1)
234U G 936.3 10 1.3 4
234U 2 G %IG=0.0011 4
234U G 1819.69 10 1.05 6
234U F G FLAG=C
234U 2 G %IG=8.8E-4 5
234U G 1863.09 10 1.44 11 C
234U 2 G %IG=0.00121 9
234U cG $Other measurement: I|g=1.21 {I25} (1975Ar23).
234U B 0.0032 4 7.49 6
234U S B EAV=116.0 13
234U L 1874.88 7 (1)
234U G 1831.36 10 20.7 2
234U F G FLAG=C
234U 2 G %IG=0.01742 24
234U G 1874.88 10 9.72 11
234U F G FLAG=C
234U 2 G %IG=0.00818 12
234U B 0.0256 3 6.541 16
234U S B EAV=112.3 13
234U L 1911.04 4 (1-)
234U G 357.5 10 0.95 20
234U 2 G %IG=8.0E-4 18
234U G 453.58 10 2.53 14 [M1] 0.324 5
234U F G FLAG=C
234U S G KC=0.258 4$LC=0.0495 7$MC=0.01193 17$NC=0.00321 5$OC=0.000781 11$
234U S G PC=0.0001507 21$QC=1.201E-5 17
234U 2 G %IG=0.00213 12
234U G 475.74 10 2.84 17 [M1] 0.285 4
234U F G FLAG=C
234U S G KC=0.2270 32$LC=0.0434 6$MC=0.01048 15$NC=0.00282 4$OC=0.000686 10$
234U S G PC=0.0001323 19$QC=1.055E-5 15
234U 2 G %IG=0.00239 15
234U G 673.9 10 0.77 16 [M1] 0.111816
234U S G KC=0.0894 13$LC=0.01695 25$MC=0.00408 6$NC=0.001100 16$OC=0.000268 4$
234U S G PC=5.16E-5 8$QC=4.12E-6 6
234U 2 G %IG=6.5E-4 14
234U G 825.6 5 7.8 4 [E1] 0.005257
234U S G KC=0.00428 6$LC=0.000733 10$MC=0.0001744 24$NC=4.67E-5 7$
234U S G OC=1.129E-5 16$PC=2.146E-6 30$QC=1.623E-7 23
234U 2 G %IG=0.00657 34
234U G 866.8 10 1.35 17
234U 2 G %IG=0.00114 16
234U G 921.72 10 15.19 12
234U F G FLAG=C
234U 2 G %IG=0.01279 16
234U cG RI$Other measurement: 14.25 {I475} (2006Al28).
234U G 1059.4 8 2.71 12
234U 2 G %IG=0.00228 10
234U G 1061.86 10 2.54 14
234U F G FLAG=C
234U 2 G %IG=0.00214 12
234U G 1124.93 10 3.6 1 @
234U 2 G %IG=0.00303 9
234U G 1867.69 10 11.0 1
234U F G FLAG=C
234U 2 G %IG=0.00926 12
234U G 1911.19 11 7.41 8
234U F G FLAG=C
234U 2 G %IG=0.00624 9
234U B 0.0508 8 6.109 18
234U S B EAV=101.0 12
234U L 1936.77 7 (1)
234U G 699.02 10 6.8 3
234U L G FL=1237.37
234U 2 G %IG=0.00572 26
234U G 1893.51 11 2.25 6
234U F G FLAG=C
234U 2 G %IG=0.00189 6
234U G 1937.04 13 2.49 8
234U F G FLAG=C
234U 2 G %IG=0.00210 7
234U B 0.0097 3 6.725 22
234U S B EAV=93.1 12
234U L 1969.9 5 (1-)
234U G 732.5 10 1.54 17
234U 2 G %IG=0.00130 16
234U G 1120.6 8 2.04 17
234U 2 G %IG=0.00172 15
234U G 1926.5 10 0.54 5
234U 2 G %IG=4.5E-4 4
234U G 1970.0 15 0.49 4
234U 2 G %IG=4.12E-4 34
234U B 0.0039 2 6.976 30
234U S B EAV=83.1 12