234U 234NP EC DECAY 1983Ar13 26NDS 202601
234U H TYP=FUL$AUT=S. Ota$CIT=NDS 207, 351 (2026)$CUT=1-Dec-2023$
234U cE IB,TI$deduced by the evaluator from intensity balance at each level.
234U c $|g|g, |gce: 1967Wa09
234U cG E$Unless otherwise noted, measurements of 1983Ar13 are given. Other
234U 2cG measurements: 1967Wa09, 1967Ha04, 1959Ga13. Earlier measurements:
234U 3cG 1951Ok06, 1953Ho49, 1956Hu28, 1958Le73.
234U cG RI$Measurements of 1983Ar13, unless otherwise noted.
234U cG M$Adopted values from ce measurements of 1967Wa09 and 1959Ga13. For a
234U 2cG tabulation of measured ce intensities, see 1970El22. The Ice's have
234U 3cG been renormalized by the evaluator such that the K-conversion
234U 4cG coefficient for the 1558.31|g is 0.00971. Multipolarities in square
234U 5cG brackets are from level scheme.
234U cG E(A,S)$Transition was not observed in {+234}Np |e decay. E|g is from
234U 2cG the Adopted Gammas.
234U cG RI(A,S)$Calculated by the evaluator from Adopted Gammas branchings.
234U cL E$Deduced by the evaluator from a least-squares fit to |g-ray
234U 2cL energies.
234U cL J$From Adopted Levels.
234U CG MR$From Adopted Levels.
234U c 1983Ar13: {+234}Np decay was measured with a coaxial Ge(Li) detector.
234U 2c The {+234}Np source was prepared by the {+235}U(d,3n) reaction (23
234U 3c MeV deuteron beam on an enriched {+235}U target) and purified from
234U 4c fission products by radiochemical separation.
234U c 1967Ha05: {+234}Np sample was produced in the reaction
234U 2c {+235}U(p,2n){+234}Np by irradiating an enriched {+235}U target with
234U 3c a 30 MeV proton beam (17.5-22 MeV on target due to absorbers). The
234U 4c sample was radiochemically purified and deposited on a nickel foil.
234U 5c Small contaminations of {+238}Np and {+239}Pu were found. |b and |g
234U 6c (by Ge(Li)) were measured in coincidence.
234U c 1955Pr29: {+234}Np sample was produced by irradiating {+235}U with a
234U 2c 21 MeV deuteron beam. After chemical purification, decay |b was
234U 3c measured with proportional counters and |g were measured with NaI.
234U 4c Determined the ratio of positron emission to electron capture.
234U D E$Least-squares fitting is done by GLSC (version 17-Jul-2025)
234U D CC$FROM BrIcc v2.3e (17-Jun-2020) 2008Ki07, "Frozen Orbitals" appr.
234U D LOGFT,CK,CL,CM,CN$FROM BetaShape v2.4 (Jun-2024) 2019MO35.
234U D EAV,LOGFT$FROM BetaShape v2.4 (Jun-2024) 2023MO21.
234U D LOGFT,CK,CL,CM,CN$FROM BetaShape v2.4 (Jun-2024) 2019MO35.
234U D EAV,LOGFT$FROM BetaShape v2.4 (Jun-2024) 2023MO21.
234U tG
234U 2tG x-rays:
234U 3tG E(x-ray) I(x-ray) I(x-ray)
234U 4tG 1983Ar13 1983Ar13 calculated
234U 5tG -------- --------- ----------
234U 6tG 94.64 {I5} 18.5 {I9} 19.1 {I15} K|a{-2}| x ra
234U +tG y
234U 7tG 98.43 {I5} 31.0 {I15} 31.0 {I25} K|a{-1}| x ra
234U +tG y
234U 8tG 111.24 {I6} 10.7 {I6} K|b{-1}'| x r
234U 9tG 114.48 {I6} 3.77 {I23} K|b{-2}'| x r
234U tG 14.4 {I12} K|b{-1}'| x r
234U +tG {-2}'| x ray
234U tG L| x ray/K| x
234NP P 0.0 (0+) 4.4 D 1 1810 8
234NP cP QP$From 2021WA16
234U N 1.0 1.0 1.0
234U PN 3
234U G 171.41 10 0.011 2
234U 2 G %IG=0.011 2
234U G 238.6 4
234U cG E$from 1959Ga13. An extremely weak line in electron spectrum was
234U 2cG interpreted as K 238.6|g. This transition was placed by 1959Ga13 in
234U 3cG the decay scheme to deexcite a level proposed at 1092 keV. This
234U 4cG transition was not observed by 1983Ar13 and others.
234U G 265.8 5 0.04 LT
234U 2 G %IG LT 0.04
234U cG E$from 1959Ga13. An extremely weak line in electron spectrum was
234U 2cG assigned as K 265.8|g. This transition was placed by 1959Ga13 in the
234U 3cG decay scheme to deexcite the 1602-keV level to a level proposed at
234U 4cG 1340 keV. This transition was not observed by 1983Ar13 and others.
234U G 383.75 10 0.042 5
234U 2 G %IG=0.042 5
234U G 702.11 20 0.020 4
234U 2 G %IG=0.020 4
234U G 1105 2
234U cG E$from 1959Ga13. An extremely weak ce line observed in the spectrum
234U 2cG was assigned as K 1105|g. This transition was not observed by
234U 3cG 1983Ar13 and others.
234U G 1220.38 15 0.040 5
234U 2 G %IG=0.040 5
234U G 1738.0 5 0.003 1
234U 2 G %IG=0.003 1
234U L 0.0 0+
234U E 0.046734 24.553 8.6 24.6
234U S E EAV=376.8 35$CK=0.7680 8$CL=0.16900 37$CM+=0.06107 26
234U cE $E|b+: others: |?800, I(|b{++})=0.046 {I10} (absolute counting)
234U 2cE (1955Pr29), 790 {I10}, I|b{++}/ce(K)=0.060 {I6}, I(|b{++})=0.084 {I1}
234U 3cE (1967Ha04), I(|b{++})=0.048 (1983Ar13).
234U L 43.50 2 2+
234U G 43.49 5 0.067 1 E2 713 11
234U S G LC=520 8$MC=143.7 22$NC=38.9 6$OC=8.92 13$PC=1.442 22$QC=0.00339 5
234U 2 G %IG=0.067 1
234U cG E$measurement of 1959Ga13. E|g=43.498 {I1} was measured in {+238}Pu
234U 2cG |a decay.
234U cG RI$deduced by the evaluator from intensity balance at the 43-keV
234U 2cG level.
234U L 143.31 7 4+
234U G 99.7 1 0.0318 13 E2 13.52 20
234U S G LC=9.84 15$MC=2.73 4$NC=0.741 11$OC=0.1703 25$PC=0.0279 4$
234U S G QC=0.0001105 16
234U 2 G %IG=0.0318 13
234U cG E$measurement of 1959Ga13. E|g=99.853 {I3} is adopted from
234U 2cG measurements in {+238}Pu |a decay.
234U cG RI$deduced by the evaluator from intensity balance at the 143-keV
234U 2cG level.
234U E 2.418E-7 0.031 LT14.4 GT 0.031 LT
234U S E EAV=347.5 37$CK=0.6850 16$CL=0.2270 9$CM+=0.08793 49
234U L 786.27 3 1-
234U G 742.78 4 5.27 21 E1 0.006369
234U S G KC=0.00518 7$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=5.27 21
234U G 786.28 4 3.19 13 (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=3.19 13
234U E 1.E-26 1 6.81 268.637 23 6.81 26
234U S E EAV=1.8 47$CK=0.7528 10$CL=0.1809 5$CM+=0.06633 32
234U L 809.85 4 0+
234U G 766.37 5 0.584 29 (E2) 0.0186726
234U S G KC=0.01336 19$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$QC=6.25E-7 9
234U 2 G %IG=0.584 29
234U G 809.8 E0 1.7 AP
234U X G K/T=0.78$L/T=0.15
234U cG E$measurement of 1967Ha04.
234U cG TI$Ice(K)=1.34 for the 809.8-keV E0 transition from the measured
234U 2cG intensity of Ice(K 809 doublet)=1.67 (1967Wa09) and Ice(K
234U 3cG 809.8|g)/Ice(K 808.13|g)=4 {I1} (1959Ga13). The ratio of K/LMN=3.5,
234U 4cG as measured for 809.8 E0 transition in {+238}Pu decay, is used to
234U 5cG deduce the total ce intensity.
234U E 0.86 9.5 0.86
234U S E CK=0.7518 11$CL=0.1815 5$CM+=0.06664 32
234U L 849.39 4 3-
234U G 706.04 10 0.153 9 [E1] 0.0069810
234U S G KC=0.00568 8$LC=0.000986 14$MC=0.0002349 33$NC=6.29E-5 9$
234U S G OC=1.519E-5 21$PC=2.88E-6 4$QC=2.134E-7 30
234U 2 G %IG=0.153 9
234U G 805.86 7 0.182 19 [E1] 0.005488
234U S G KC=0.00447 6$LC=0.000767 11$MC=0.0001825 26$NC=4.89E-5 7$
234U S G OC=1.181E-5 17$PC=2.244E-6 31$QC=1.692E-7 24
234U 2 G %IG=0.182 19
234U L 851.69 3 2+
234U G 708.11 20 0.052 6 [E2] 0.0219431
234U S G KC=0.01537 22$LC=0.00489 7$MC=0.001247 17$NC=0.000337 5$OC=8.00E-5 11$
234U S G PC=1.459E-5 20$QC=7.29E-7 10
234U 2 G %IG=0.052 6
234U G 808.13 10 0.101 10 E0+E2 4.2
234U S G KC=3.3
234U 2 G %IG=0.101 10
234U cG CC$Ice(K 808.13|g)=0.33 from Ice(K 809 doublet)=1.67 (1967Wa09) and
234U 2cG Ice(K 809.8)/Ice(K 808.13)=4 {I1} (1959Ga13). The ratio of K/LMN=3.5,
234U 3cG as measured for 809.8 E0 transition in {+238}Pu decay, is used to
234U 4cG deduce the total ce intensity. [|a(K)(E2; 808.13|g)=0.0123;
234U 5cG therefore, the measured ce intensity is essentially due to the E0
234U 6cG part of the transition].
234U G 851.77 6 0.167 10 [E2] 0.0151321
234U S G KC=0.01109 16$LC=0.00302 4$MC=0.000759 11$NC=0.0002048 29$
234U S G OC=4.89E-5 7$PC=9.02E-6 13$QC=5.10E-7 7
234U 2 G %IG=0.167 10
234U E 0.2 LT10.6 GT 0.2 LT
234U S E CK=0.7018 18$CL=0.2157 10$CM+=0.0824 5
234U L 926.66 7 2+
234U G 783.42 1 0.027 13 [E2] 0.0178625 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=0.027 13
234U cG $A peak reported in 1983Ar13 at 782.32 {I15} keV with I|g=0.027
234U 2cG {I13}. Possibly E|g=783.4 given the energy difference of the two
234U 3cG levels especially because it lies right below the large 786|g peak,
234U 4cG or may be due mostly to an impurity (as its relative intensity to
234U 5cG 883|g is larger than that reported in {+234}Pu |b{+-} decay). Not
234U 6cG observed in 1967Ha04.
234U G 883.04 15 0.105 10 E2 0.0141020
234U S G KC=0.01041 15$LC=0.00276 4$MC=0.000692 10$NC=0.0001867 26$
234U S G OC=4.46E-5 6$PC=8.25E-6 12$QC=4.76E-7 7
234U 2 G %IG=0.105 10
234U G 926.63 10 0.068 7 (E2) 0.0128418
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=4.34E-7 6
234U 2 G %IG=0.068 7
234U E 0.135 1710.58 6 0.135 17
234U S E CK=0.6924 20$CL=0.2221 11$CM+=0.0854 6
234U L 989.44 4 2-
234U G 62.70 1 0.115 11 E1 0.426 6 S
234U F G FLAG=S
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=0.115 11
234U G 140.1 2 0.029 3 M1+E2 1.3 5 5.1 13
234U L G FL=849.39
234U S G KC=2.6 15$LC=1.79 18$MC=0.48 6$NC=0.130 17$OC=0.030 4$PC=0.0052 5$
234U S G QC=1.4E-4 7
234U 2 G %IG=0.029 3
234U G 203.16 7 0.041 4 M1+E2 1.4 4 1.5 4
234U S G KC=0.9 4$LC=0.423 11$MC=0.1112 16$NC=0.0301 4$OC=0.00708 11$
234U S G PC=0.00125 4$QC=4.6E-5 16
234U 2 G %IG=0.041 4
234U G 945.91 5 0.432 26 (E1) 0.004126
234U S G KC=0.00337 5$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$QC=1.286E-7 18
234U 2 G %IG=0.432 26
234U E 0.23 LT10.2 GT 0.23 LT 1U
234U S E CK=0.6829 23$CL=0.2286 13$CM+=0.0885 7
234U L 1044.53 3 0+
234U G 192.91 7 0.066 7 [E2] 0.856 12 &
234U L G FL=851.69
234U S G KC=0.1635 23$LC=0.505 7$MC=0.1391 20$NC=0.0378 5$OC=0.00872 12$
234U S G PC=0.001455 20$QC=1.381E-5 19
234U 2 G %IG=0.066 7
234U G 234.6 2 E0 0.165 19
234U X G K/T=0.78$L/T=0.15
234U cG E$from 1959Ga13.
234U cG TI$Calculated by the evaluator from [total Ice(234.6|g)]/Ice(K
234U 2cG 1001.05|g)=[87 {I9}]/837 {I10}, as measured in 1.17-min {+234}Pa
234U 3cG |b{+-} decay. Extremely weak K- and L1 lines were observed by
234U 4cG 1959Ga13. The 234.6-keV transition was also seen by 1967Ha04 and
234U 5cG placed twice on the level scheme. The intensity of 0.2% shown on
234U 6cG their decay scheme is consistent with the intensity deduced here.
234U G 258.19 7 0.119 8 (E1) 0.05488
234U S G KC=0.0434 6$LC=0.00859 12$MC=0.002075 29$NC=0.000555 8$
234U S G OC=0.0001321 19$PC=2.420E-5 34$QC=1.499E-6 21
234U 2 G %IG=0.119 8
234U G 1001.05 5 1.59 7 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=1.59 7
234U E 1.62 158.979 45 1.62 15
234U S E CK=0.7384 14$CL=0.1908 8$CM+=0.0708 4
234U L 1085.29 4 2+
234U G 233.6 2
234U L G FL=851.69
234U cG E$from 1959Ga13.
234U cG TI$|?0.1%. Very weak K and L1 lines were observed by 1959Ga13.
234U 2cG 1967Ha04 observed in their electron spectrum the 234-keV transition,
234U 3cG corresponding to 233.6- and 234.6-keV transitions of 1959Ga13. Total
234U 4cG ce intensities of 0.1% and 0.2% for these two transitions,
234U 5cG respectively, were shown on the decay scheme of 1967Ha04; the method
234U 6cG of dividing the observed intensity for 234-keV transition was not
234U 7cG explained. Intensity balance at the 1085.4-keV level yields
234U 8cG I(|g+ce)=0.04 {I+7-4}, if there is no direct |e decay to the level.
234U G 235.62 10 0.012 2 [E1] 0.06759
234U L G FL=849.39
234U S G KC=0.0533 7$LC=0.01070 15$MC=0.00259 4$NC=0.000691 10$OC=0.0001644 23$
234U S G PC=3.00E-5 4$QC=1.820E-6 26
234U 2 G %IG=0.012 2
234U G 299.70 10 0.021 2 [E1] 0.03936
234U L G FL=786.27
234U S G KC=0.0313 4$LC=0.00605 8$MC=0.001459 20$NC=0.000390 5$OC=9.32E-5 13$
234U S G PC=1.717E-5 24$QC=1.099E-6 15
234U 2 G %IG=0.021 2
234U G 941.93 17 0.248 15 [E2] 0.0124417
234U S G KC=0.00929 13$LC=0.002358 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=0.248 15
234U G 1041.62 10 0.15 2
234U 2 G %IG=0.15 2
234U G 1085.45 15 0.019 4
234U 2 G %IG=0.019 4
234U L 1237.26 3 1-
234U G 192.91 7 0.066 7 [E1] 0.107215 &
234U S G KC=0.0840 12$LC=0.01746 24$MC=0.00423 6$NC=0.001130 16$OC=0.000268 4$
234U S G PC=4.84E-5 7$QC=2.80E-6 4
234U 2 G %IG=0.066 7
234U G 247.79 7 0.109 7 [M1,E2] 1.0 7
234U S G KC=0.7 6$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=0.109 7
234U G 310.52 10 0.039 4 [E1] 0.03645
234U S G KC=0.0290 4$LC=0.00558 8$MC=0.001344 19$NC=0.000359 5$OC=8.58E-5 12$
234U S G PC=1.585E-5 22$QC=1.022E-6 14
234U 2 G %IG=0.039 4
234U G 387.94 6 0.208 12 [E2] 0.089713
234U L G FL=849.39
234U S G KC=0.0462 6$LC=0.0320 4$MC=0.00855 12$NC=0.002317 32$OC=0.000542 8$
234U S G PC=9.42E-5 13$QC=2.534E-6 35
234U 2 G %IG=0.208 12
234U G 427.4 2 0.009 2 [E1] 0.0185026
234U S G KC=0.01488 21$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$QC=5.40E-7 8
234U 2 G %IG=0.009 2
234U G 450.93 4 1.15 5 M1+E2 0.70 0.240734
234U S G KC=0.1875 26$LC=0.0400 6$MC=0.00980 14$NC=0.00264 4$OC=0.000638 9$
234U S G PC=0.0001213 17$QC=8.79E-6 12
234U 2 G %IG=1.15 5
234U G 1193.78 4 6.02 24 E1 0.002774
234U S G KC=0.002260 32$LC=0.000377 5$MC=8.92E-5 12$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=6.02 24
234U G 1237.22 4 2.30 9 E1 0.002624
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=2.30 9
234U E 10.25 317.885 26 10.25 31
234U S E CK=0.7172 21$CL=0.2054 12$CM+=0.0774 6
234U L 1435.38 3 1-
234U G 197.91 15 0.018 4 [M1,E2] 2.0 12
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$QC=7.E-5 5
234U 2 G %IG=0.018 4
234U G 445.91 10 0.020 4 [M1,E2] 0.20 14
234U S G KC=0.15 12$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$QC=7.E-6 5
234U 2 G %IG=0.020 4
234U G 625.66 7 0.076 7 [E1] 0.0087512
234U S G KC=0.00710 10$LC=0.001248 17$MC=0.000298 4$NC=7.98E-5 11$
234U S G OC=1.923E-5 27$PC=3.63E-6 5$QC=2.65E-7 4
234U 2 G %IG=0.076 7
234U G 649.12 10 0.027 6 [M1,E2] 0.07 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$QC=2.7E-6 18
234U 2 G %IG=0.027 6
234U G 1391.87 4 2.27 9 E1 2.21E-33
234U S G KC=0.001745 24$LC=0.000288 4$MC=6.82E-5 10$NC=1.829E-5 26$
234U S G OC=4.44E-6 6$PC=8.51E-7 12$QC=6.76E-8 9
234U 2 G %IG=2.27 9
234U G 1435.36 4 6.38 25 E1 2.13E-33
234U S G KC=0.001658 23$LC=0.000274 4$MC=6.47E-5 9$NC=1.734E-5 24$OC=4.21E-6 6$
234U S G PC=8.07E-7 11$QC=6.43E-8 9
234U 2 G %IG=6.38 25
234U E 8.82 277.491 35 8.82 27
234U S E CK=0.6633 48$CL=0.2422 30$CM+=0.0944 12
234U L 1457.11 30 (2-)
234U G 670.8 10 0.0035 11 [M1,E2] 0.07 4 S
234U F G FLAG=S
234U S G KC=0.05 4$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=0.0035 11
234U G 1413.6 3 0.021 4
234U 2 G %IG=0.021 4
234U E 0.021 4 9.55 10 0.021 4 1U
234U S E CK=0.443 13$CL=0.388 8$CM+=0.1688 36
234U L 1500.87 8 (1)
234U G 649.12 10 0.005 AP @
234U L G FL=851.69
234U 2 G %IG AP 0.005
234U G 691.08 10 0.038 4
234U 2 G %IG=0.038 4
234U G 1458.5 15 0.009 3 S
234U F G FLAG=S
234U 2 G %IG=0.009 3
234U E 0.04 9.6 0.04
234U S E CK=0.623 8$CL=0.2698 49$CM+=0.1075 19
234U L 1510.23 12 1
234U G 1466.5 2 0.032 3
234U 2 G %IG=0.032 3
234U G 1510.35 15 0.024 3
234U 2 G %IG=0.024 3
234U E 0.056 4 9.43 5 0.056 4
234U S E CK=0.615 8$CL=0.275 5$CM+=0.1099 21
234U L 1570.69 3 1+
234U G 135.32 8 0.020 2 [E1] 0.246935
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$QC=6.07E-6 9
234U 2 G %IG=0.020 2
234U G 485.44 7 0.089 7 [M1,E2] 0.16 11
234U S G KC=0.12 9$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$QC=6.E-6 4
234U 2 G %IG=0.089 7
234U G 526.02 10 0.043 5 [M1] 0.217130
234U S G KC=0.1732 24$LC=0.0331 5$MC=0.00797 11$NC=0.002148 30$OC=0.000522 7$
234U S G PC=0.0001007 14$QC=8.04E-6 11
234U 2 G %IG=0.043 5
234U G 581.19 10 0.38 4 [E1] 0.0100614
234U S G KC=0.00815 11$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=0.38 4
234U G 719.01 7 0.122 7 [M1+E2] 0.06 4
234U L G FL=851.69
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$QC=2.1E-6 14
234U 2 G %IG=0.122 7
234U G 760.53 15 0.020 4 [M1] 0.081111
234U S G KC=0.0648 9$LC=0.01226 17$MC=0.00295 4$NC=0.000795 11$OC=0.0001933 27$
234U S G PC=3.73E-5 5$QC=2.98E-6 4
234U 2 G %IG=0.020 4
234U G 1527.21 4 11.2 5 E2+M1 0.009 4
234U S G KC=0.0071 31$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$QC=3.2E-7 15
234U 2 G %IG=11.2 5
234U G 1570.68 4 5.09 21 M1 0.0120417
234U S G KC=0.00951 13$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=4.33E-7 6
234U 2 G %IG=5.09 21
234U E 17.2 6 6.65 5 17.2 6
234U S E CK=0.539 16$CL=0.326 10$CM+=0.1348 40
234U L 1601.81 3 1+
234U G 166.5 1 0.006 1 [E1] 0.151421
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$QC=3.85E-6 5
234U 2 G %IG=0.006 1
234U G 516.60 6 0.313 19 (M1) 0.227932
234U S G KC=0.1819 25$LC=0.0347 5$MC=0.00837 12$NC=0.002255 32$OC=0.000548 8$
234U S G PC=0.0001058 15$QC=8.44E-6 12
234U 2 G %IG=0.313 19
234U G 557.24 6 0.214 13 (M1) 0.185926
234U S G KC=0.1485 21$LC=0.0283 4$MC=0.00682 10$NC=0.001837 26$OC=0.000447 6$
234U S G PC=8.62E-5 12$QC=6.88E-6 10
234U 2 G %IG=0.214 13
234U G 750.12 6 0.440 26 (M1) 0.084112
234U L G FL=851.69
234U S G KC=0.0672 9$LC=0.01272 18$MC=0.00306 4$NC=0.000825 12$OC=0.0002006 28$
234U S G PC=3.87E-5 5$QC=3.09E-6 4
234U 2 G %IG=0.440 26
234U G 791.94 5 0.254 15 [M1] 0.072810
234U S G KC=0.0582 8$LC=0.01100 15$MC=0.00265 4$NC=0.000713 10$OC=0.0001735 24$
234U S G PC=3.35E-5 5$QC=2.68E-6 4
234U 2 G %IG=0.254 15
234U G 1558.31 4 18.72 20 M1 0.0122817
234U S G KC=0.00971 14$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=18.72 20
234U G 1601.80 4 9.1 4 (M1) 0.0114616
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=9.1 4
234U E 29.6 5 6.23 6 29.6 5
234U S E CK=0.470 24$CL=0.372 16$CM+=0.157 6