146LA 146BA B- DECAY 1985CH16 16NDS 201609
146LA H TYP=ERR$AUT=Balraj Singh$DAT=25-Feb-2021$COM=ECC for 6 G rays removed$
146LA H TYP=FUL$AUT=Yu. KHAZOV, A. RODIONOV AND G. SHULYAK$
146LA2 H CIT=NDS 136, 163 (2016)$CUT=14-Jul-2016$
146LA c Note: edited by Balraj Singh, Feb 25, 2021, in consultation with
146LA2c A. Rodionov, one of the evaluators of 2016 update: removed quoted
146LA3c experimental total conversion coefficients for 114.90, 121.20, 140.70,
146LA4c 144.70, 175.30 and 197.0 |g rays. The 2016 evaluation did not cite a
146LA5c source reference for these values, but the values are in 1978BlZY,
146LA6c where these are theoretical total conversion coefficients.
146LA7c In general comment for multipolarity assignment, removed assignment
146LA8c from 1978BlZY from ce data. 114.90 gamma: mult=M1 edited to [M1], and
146LA9c reference to 1978BlZY removed.
146LA c 1985Ch16: {+146}Ba |b{+-} decay [from {+235}U(n,F), E=th]; measured
146LA2c E|g, I|g, |g|g(t), |g|g(|q). {+146}La; deduced levels, J|p, I{-|b},
146LA3c |d, log| {Ift}. Mass-separator TRISTAN, tape transport system, Ge(Li),
146LA4c Ge planar detectors.
146LA c 1984So18: {+146}Ba |b{+-} decay (from {+235}U(n,F), E=th); measured
146LA2c absolute E|g, I|g. Mass-separator OSTIS, Ge(Li) detectors
146LA c 1978BlZY: {+146}Ba |b{+-} decay; measured E|g, I|g. {+146}La; deduced
146LA2c levels, log| {Ift}.
146LA c 1986Gr11: {+146}Ba |b{+-} decay; measured E|b, I|b, |b|g coin,
146LA2c |b-endpoint energies; deduced Q(|b). Mass-separator OSTIS,
146LA3c plastic and Ge(Li) detectors
146LA c Decay scheme from 1985Ch16
146LA cB IB$Deduced from transition intensity balance at the levels, assuming
146LA2cB [M1] mult for transitions between states with the same parity and
146LA3cB |DJ=1, and assuming [E1] mult for transitions between states with
146LA4cB different parity and |DJ=1, unless there was evidence to support a
146LA5cB specific |d value or |DJ=2 (1985Ch16). Since mults are not known for
146LA6cB any low energy |g's therefore I|b and the corresponding log| {Ift} for
146LA7cB levels below 1 MeV should be considered approximate; {Icf} complete
146LA8cB list of |b feedings in table III of 1985Ch16.
146LA9cB Measurements of Q(|b): 1981De25, 1979Ke02.
146LA cG E,RI$From 1985Ch16. Fitting of the level scheme of 1985Ch16 by
146LA2cG a least-squares method gave a result of normalized |h{+2}=2.9.
146LA3cG For this reason the evaluators added quadratically 0.1 keV to all
146LA4cG the |DE|g taken from
146LA5cG 1985Ch16 to fit the level scheme. E|g's deduced from coincidences are
146LA6cG given without uncertainties, the evaluators assumed |DE|g=0.5 keV for
146LA7cG such cases.
146LA cG E(B)$Energy of |g ray is not used in a least-squares fitting
146LA cG M$From |g|g(|q) (1985Ch16)
146LA cG M(A)$D+Q from |g|g(|q), large |d rules out E1+M2
146LA cG MR$From |g|g(|q) (1985Ch16)
146LA cL E$If |DE|g not given, |+0.50 keV assumed for least-squares fitting
146LA cL E$From a least-squares fit to E|g's; normalized |h{+2}=1.4
146LA cL J$From 'Adopted Levels'
146LA cL T$From 1978Mo33, 1978MoYW. Some of the measured half-life values are
146LA2cL grouped close to T{-1/2}=8.0-8.5 s
146LA3cL (1974SeZZ,1976AmZW,1969WiZX,1979En02). The
146LA3cL evaluators tend to believe that these results were
146LA4cL obtained for a mixture of |b decays of the ground and isomeric states.
146LA DG CC$FROM BrIcc v2.3a (10-Sep-2014) 2008Ki07, "Frozen Orbitals" appr.
146BA P 0.0 0+ 2.21 S 6 4110 30
146LA N 0.0142 7 0.0119 7 1.0 1.0
146LA cN NR,NT$from Rajeval technique of I(140.7|g)=22.6% {I30},
146LA2cN I(121.2|g)=14.2% {I14}, I(197.0|g)=12.7% {I13}, I(231.6|g)=10.6% {I11},
146LA3cN I(251.2|g)=18.0% {I20} (1984So18)
146LA PN 4
146LA G 310.70 22
146LA G 509.5 3
146LA G 588.5 216 3
146LA G 1021.4 72 2
146LA G 1155.70 2213 2
146LA G 1492.8 3
146LA G 1581.80 229 1
146LA G 1650.2 64 2
146LA G 1667.4 37 2
146LA G 1708.8 314 2
146LA G 1767.3 8
146LA G 1899.8 48 2
146LA G 1903.6 38 2
146LA G 1964.5 5
146LA G 1992.8 5
146LA G 2030.60 22
146LA L 0.0 (2-) 6.1 S 3
146LA cL T$weighted average of 6.2 s {I6} (1978Mo33,1978MoYW) and 6.0 s {I4}
146LA2cL (1981GoZN)
146LA B 6.2 LT 7.2 GT 1U?
146LAS B EAV=1726 14
146LA L 0.0+X (6-) 9.8 S 4 M1
146LA DL E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT
146LA cL E$introduced in level scheme by 1998Hw08 ({+252}Cf SF); X=130 {I130}
146LA2cL keV is evaluated by 2012Au07. No electron peaks corresponding to the
146LA3cL E4 or M5 (M3 in 1993Sh10; this is a misprint)
146LA4cL transitions of unplaced |g rays had been observed, therefore
146LA5cL IT transition must be very weak if present (1993Sh10).
146LA cL T,J$from 1978Mo33, 1978MoYW
146LA L 121.18 71-,2-
146LA B 1.2 LT 7.9 GT 1U?
146LAS B EAV=1670 14
146LA G 121.20 121000 20M1+E2 +0.04 10 0.627 12
146LAF G FL=0.0
146LAS G KC=0.535 8$LC=0.073 4$MC=0.0151 8
146LAS G NC=0.00332 17$OC=0.000539 23$PC=4.17E-5 6
146LA cG RI 14.2% {I14} (1984So18)
146LA cG MR$the 2{+nd} value |d=-3.9 {I+12-26}; both |d values were derived
146LA2cG from A{-2}=-0.060 {I39}, A{-4}=-0.069 {I74} for the cascade
146LA3cG 251|g-121|g assuming |d(251|g)=0
146LA L 140.85 6(2-)
146LA B 1.6 LT 6.1 GT C
146LAS B EAV=1680 14
146LA cB E$3920 {I150} (1986Gr11)
146LA G 140.70 141421 31M1+E2 -0.66 +11-150.468 19
146LAF G FL=0.0
146LAS G KC=0.373 9$LC=0.075 9$MC=0.0160 19
146LAS G NC=0.0035 4$OC=0.00053 6$PC=2.65E-5 5
146LA cG MR$the 2{+nd} value |d=-6.0 {I+23-58}; both |d values were derived
146LA2cG from A{-2}=0.119 {I38}, A{-4}=0.046 {I72} for the cascade 232|g-140|g
146LA3cG assuming |d(232|g)=0
146LA cG RI 22.6% {I30} (1984So18)
146LA L 144.62 9(3-)
146LA G 4.0 0.18 3[M1] 450
146LAS G MC=358 5
146LAS G NC=78.5 11$OC=12.69 18$PC=0.968 14
146LA cG E$from level energy difference. Existence is required by |g|g
146LA cG RI$from intensities balance at the level, assuming M1 mult;
146LA2cG I(|g+ce)=87 {I2} (the evaluators). I(|g+ce)=170 {I11} from |g|g
146LA3cG (1985Ch16).
146LA G 144.70 14189 5M1+E2 +0.61 10 0.424 12 A
146LAF G FL=0.0
146LAS G KC=0.342 7$LC=0.065 6$MC=0.0139 12
146LAS G NC=0.00300 25$OC=0.00046 4$PC=2.46E-5 4
146LA cG MR$The 2{+nd} value |d=-5.4 {I+19-60}; both |d values were derived
146LA2cG from A{-2}=0.119 {I38}, A{-4}=0.046 {I72} for the cascade 232|g-140|g
146LA3cG assuming |d(232|g)=0
146LA L 197.03 6 (1-)
146LA B 4.3 10 5.65 11
146LAS B EAV=1654 14
146LA cB E$3830 {I150} (1986Gr11)
146LA G 56.4 1 53 5 (M1+E2) 11 6
146LAS G KC=5.1 3$LC=5 4$MC=1.0 9
146LAS G NC=0.22 19$OC=0.03 3$PC=0.00033 5
146LA cG M$|a estimated from intensity balance at the level (1985Ch16)
146LA G 75.90 149 1[M1] 2.39 C
146LAS G KC=2.04 3$LC=0.277 5$MC=0.0576 9
146LAS G NC=0.01266 19$OC=0.00206 3$PC=0.0001589 24
146LA G 197.00 14890 26M1+E2 0.10 +13-150.163 3 A
146LAF G FL=0.0
146LAS G KC=0.1393 20$LC=0.0188 7$MC=0.00390 16
146LAS G NC=0.00086 4$OC=0.000139 5$PC=1.079E-5 18
146LA cG RI 12.7% {I13} (1984So18)
146LA cG MR$the 2{+nd} value |d=27 {I+|@-18}; both |d values were derived
146LA2cG from A{-2}=0.013 {I41}, A{-4}=0.06 {I78} for the 269|g-197|g cascade
146LA3cG assuming |d(269|g)=0
146LA L 294.97 6(2)
146LA B 0.6 LT 6.5 GT C ?
146LAS B EAV=1608 14
146LA cB E$3720 {I200} (1986Gr11)
146LA G 97.70 1426 2[M1] 1.155 C
146LAS G KC=0.987 15$LC=0.1338 20$MC=0.0278 4
146LAS G NC=0.00611 9$OC=0.000993 15$PC=7.69E-5 12
146LA G 294.9 3 384 13[M1] 0.0553
146LAF G FL=0.0
146LAS G KC=0.0474 7$LC=0.00626 9$MC=0.001299 19
146LAS G NC=0.000286 4$OC=4.65E-5 7$PC=3.66E-6 6
146LA cG $A{-2}=0.046 {I55}, A{-4}=0.03 {I12} for the cascade 172|g-294|g;
146LA2cG A{-2}=-0.019 {I82}, A{-4}=-0.12 {I18} for the cascade 114|g-294|g.
146LA L 326.70 9(3)
146LA G 182.20 2219 5[M1] 0.201 C
146LAS G KC=0.1723 25$LC=0.0231 4$MC=0.00480 7
146LAS G NC=0.001054 16$OC=0.0001716 25$PC=1.339E-5 20
146LA G 185.90 14106 3[M1+E2] -0.01 +10-9 0.191 C
146LAS G KC=0.1631 24$LC=0.0218 4$MC=0.00454 8
146LAS G NC=0.000998 18$OC=0.000162 3$PC=1.267E-5 18
146LA cG MR$the 2{+nd} value |d=2.7 {I+10-6}; both |d values were derived
146LA2cG from A{-2}=0.122 {I45}, A{-4}=0.033 {I94} for the cascade 185|g-140|g
146LA G 326.30 2224 7[M1] 0.0424
146LAF G FL=0.0
146LAS G KC=0.0364 6$LC=0.00479 7$MC=0.000994 14
146LAS G NC=0.000219 3$OC=3.56E-5 5$PC=2.81E-6 4
146LA L 372.53 51+
146LA B 28.2 16 4.75 4 C
146LAS B EAV=1572 14
146LA cB E$3810 keV {I150} in table 1 of 1986Gr11 is a misprint; 3673 keV is
146LA2cB obtained by the evaluators using Q(|b)=4045 keV of 1986Gr11
146LA G 77.70 1464 7[E1] 0.471 C
146LAS G KC=0.400 6$LC=0.0567 9$MC=0.01171 18
146LAS G NC=0.00253 4$OC=0.000391 6$PC=2.36E-5 4
146LA G 175.30 14338 8[E1] 0.0500 C
146LAS G KC=0.0428 6$LC=0.00567 8$MC=0.001170 17
146LAS G NC=0.000255 4$OC=4.05E-5 6$PC=2.80E-6 4
146LA cG M$balance of I(|g+ce) at the 326.5 keV level depends little on |a for
146LA2cG this |g; present level scheme conforms to E1 mult for this transition
146LA3cG but not M1 as follows from assumption of 1978BlZY
146LA G 231.60 14756 16(E1) 0.0235 C
146LAS G KC=0.0202 3$LC=0.00264 4$MC=0.000545 8
146LAS G NC=0.0001188 17$OC=1.90E-5 3$PC=1.357E-6 20
146LA cG RI 10.6% {I11} (1984So18)
146LA G 251.20 141379 37[E1] 0.0189 C
146LAS G KC=0.01628 23$LC=0.00212 3$MC=0.000438 7
146LAS G NC=9.55E-5 14$OC=1.530E-5 22$PC=1.102E-6 16
146LA cG RI 18.0% {I20} (1984So18)
146LA G 372.50 1470 10[E1] 0.00690
146LAF G FL=0.0
146LAS G KC=0.00594 9$LC=0.000762 11$MC=0.0001573 22
146LAS G NC=3.44E-5 5$OC=5.55E-6 8$PC=4.14E-7 6
146LA L 392.61 7(2+)
146LA cL J$no direct population in the |b-decay but populated by 18
146LA2cL transitions from levels above 600 keV (1985Ch16).
146LA G 392.50 14435 14[E1+M2] -0.28 +9-10 0.013 5
146LAF G FL=0.0
146LAS G KC=0.011 4$LC=0.0015 7$MC=0.00032 14
146LAS G NC=7.E-5 3$OC=1.1E-5 5$PC=8.E-7 4
146LA cG MR$the 2{+nd} value |d=6.6 {I+91-25}; both |d values were derived
146LA2cG from A{-2}=-0.019 {I49}, A{-4}=0.081 {I90} for the 316|g-392|g cascade.
146LA3cG Values |d=-0.42 {I+16-19} and |d=38 {I+|@-32} from A{-2}=0.041 {I79},
146LA4cG A{-4}=0.00 {I16} for the 488|g-392|g cascade.
146LA B 0.8 LE 6.3 GE ?
146LAS B EAV=1563 14
146LA L 409.91 11(3)
146LA G 114.90 1468 2 [M1] 0.728 C
146LAS G KC=0.622 9$LC=0.0842 13$MC=0.0175 3
146LAS G NC=0.00385 6$OC=0.000625 9$PC=4.85E-5 7
146LA L 417.55 8 (2)
146LA B 0.21 LT 6.9 GT C ?
146LAS B EAV=1551 14
146LA G 220.70 1416 1[M1] 0.1196 C
146LAS G KC=0.1024 15$LC=0.01365 20$MC=0.00283 4
146LAS G NC=0.000623 9$OC=0.0001015 15$PC=7.94E-6 12
146LA G 272.9 319 4
146LA G 417.50 1495 6
146LAF G FL=0.0
146LA L 429.21 62-
146LA B 0.5 LE 6.5 GE ?
146LAS B EAV=1546 14
146LA G 284.5 3 192 6(M1+E2) +0.39 +15-350.0601 11 AC
146LAS G KC=0.0511 12$LC=0.00712 25$MC=0.00148 6
146LAS G NC=0.000325 12$OC=5.24E-5 15$PC=3.88E-6 15
146LA cG MR$the 2{+nd} value |d=-1.7 {I7}; both |d values were derived
146LA2cG from A{-2}=0.139 {I77}, A{-4}=-0.05 {I19} for the cascade 279|g-284|g
146LA3cG assuming |d(279|g)=0.
146LA G 429.30 14427 11M1+E2 +0.66 +10-120.0194 5 A
146LAF G FL=0.0
146LAS G KC=0.0165 5$LC=0.00228 4$MC=0.000475 8
146LAS G NC=0.0001041 17$OC=1.68E-5 3$PC=1.24E-6 4
146LA cG MR$the 2{+nd} value |d=-6.1 {I+21-49}; both |d values were derived
146LA2cG from A{-2}=0.129 {I31}, A{-4}=-0.002 {I88} for the cascade 279|g-429|g
146LA3cG assuming |d(279|g)=0
146LA L 439.04 61-
146LA cL J$log| {Ift} value and ground-state |g branch suggest J|p=1{+-}
146LA2cL assignment.
146LA B 1.4 4 6.02 13 C
146LAS B EAV=1541 14
146LA cB E$3550 {I210} (1986Gr11)
146LA G 144.10 1422 3[M1] 0.385 C
146LAS G KC=0.329 5$LC=0.0444 7$MC=0.00922 14
146LAS G NC=0.00203 3$OC=0.000330 5$PC=2.56E-5 4
146LA G 241.8 3 199 6(M1+E2) -0.22 8 0.0936 A
146LAS G KC=0.0799 12$LC=0.01089 25$MC=0.00227 6
146LAS G NC=0.000497 12$OC=8.06E-5 16$PC=6.14E-6 11
146LA cG MR$the 2{+nd} value |d=-61 {I+51-|@}; both |d values were derived
146LA2cG from A{-2}=0.060 {I44}, A{-4}=-0.076 {I85} for the cascade 242|g-197|g
146LA G 298.00 14300 7M1(+E2) -0.009 +10-9 0.0538
146LAS G KC=0.0461 7$LC=0.00609 9$MC=0.001263 18
146LAS G NC=0.000278 4$OC=4.53E-5 7$PC=3.56E-6 5
146LA cG E$other: E{-|g}=298.794 {I16} (1979Bo26).
146LA cG MR$the 2{+nd} value |d=2.7 {I+9-6}; both |d values were derived
146LA2cG from A{-2}=0.126 {I41}, A{-4}=0.000 {I80} for the cascade 298|g-140|g
146LA3cG assuming |d(232|g)=0
146LA G 317.9 328 6 C
146LA G 439.00 1496 4
146LAF G FL=0.0
146LA L 443.59 12(1-)
146LA B 1.20 14 6.09 6
146LAS B EAV=1539 14
146LA G 148.7 6 1[M1] 0.353 C
146LAS G KC=0.302 5$LC=0.0406 6$MC=0.00844 12
146LAS G NC=0.00186 3$OC=0.000302 5$PC=2.35E-5 4
146LA G 246.6 3 48 3[M1] 0.0888 C
146LAS G KC=0.0761 11$LC=0.01011 15$MC=0.00210 3
146LAS G NC=0.000461 7$OC=7.51E-5 11$PC=5.89E-6 9
146LA G 322.20 2225 4 C
146LA G 443.50 2222 4
146LAF G FL=0.0
146LA L 466.54 62+
146LA B 0.6 LT 6.4 GT
146LAS B EAV=1528 14
146LA G 94.00 149 1[M1+E2] 0.4 6 1.5 5 C
146LAS G KC=1.15 13$LC=0.24 24$MC=0.05 6
146LAS G NC=0.011 12$OC=0.0017 16$PC=8.5E-5 4
146LA G 139.80 1463 2[E1] 0.0931 C
146LAS G KC=0.0797 12$LC=0.01068 16$MC=0.00220 4
146LAS G NC=0.000479 7$OC=7.57E-5 11$PC=5.08E-6 8
146LA G 171.60 1427 4[E1] 0.0530 C
146LAS G KC=0.0454 7$LC=0.00601 9$MC=0.001241 18
146LAS G NC=0.000270 4$OC=4.30E-5 6$PC=2.96E-6 5
146LA G 269.6 3 303 10[E1] 0.01573 C
146LAS G KC=0.01352 20$LC=0.00176 3$MC=0.000362 6
146LAS G NC=7.91E-5 12$OC=1.270E-5 19$PC=9.21E-7 14
146LA G 466.80 1461 21 &
146LAF G FL=0.0
146LA L 488.14 8 (1-,2-)
146LA B 0.50 19 6.44 17 C
146LAS B EAV=1518 14
146LA G 193.3 5 1[M1] 0.1714 C
146LAS G KC=0.1466 21$LC=0.0196 3$MC=0.00407 6
146LAS G NC=0.000896 13$OC=0.0001458 21$PC=1.139E-5 16
146LA G 290.6 3 41 5[M1] 0.0575 C
146LAS G KC=0.0493 7$LC=0.00651 10$MC=0.001351 20
146LAS G NC=0.000297 5$OC=4.84E-5 7$PC=3.80E-6 6
146LA G 343.7 311 1 C
146LA G 488.00 1497 9
146LAF G FL=0.0
146LA L 500.11 7 (1-,2-)
146LA B 0.28 LE 6.7 GE C ?
146LAS B EAV=1513 14
146LA G 173.3 9 1 C
146LA G 355.6 371 4 &C
146LA G 359.10 2225 5
146LA G 500.10 1426 4
146LAF G FL=0.0
146LA L 574.50 6 (1-,2)
146LA B 0.4 LT 6.5 GT C ?
146LAS B EAV=1478 14
146LA G 107.90 148 1[E1] 0.191 C
146LAS G KC=0.1626 24$LC=0.0222 4$MC=0.00459 7
146LAS G NC=0.000995 15$OC=0.0001560 23$PC=1.004E-5 15
146LA G 145.30 1417 3[M1] 0.377 C
146LAS G KC=0.322 5$LC=0.0434 7$MC=0.00901 13
146LAS G NC=0.00198 3$OC=0.000322 5$PC=2.51E-5 4
146LA G 164.60 1429 4[M1] 0.266 C
146LAS G KC=0.228 4$LC=0.0306 5$MC=0.00636 9
146LAS G NC=0.001398 20$OC=0.000227 4$PC=1.77E-5 3
146LA G 247.8 350 4 C
146LA G 279.50 1422 3 &
146LA G 377.50 1483 4 C
146LA G 433.6 413 7 C
146LA G 574.50 1449 4
146LAF G FL=0.0
146LA cG $marked as coinciding with 488|g (1985Ch16); this is a misprint,
146LA2cG should be 489.8|g (evaluators).
146LA L 647.13 61
146LA cL J$population (log| {Ift}=5.7) in |b{+-} decay from 0+, decay pattern.
146LA B 2.37 22 5.69 5
146LAS B EAV=1444 14
146LA G 146.90 1415 3[E1] 0.0812 C
146LAS G KC=0.0695 10$LC=0.00929 14$MC=0.00192 3
146LAS G NC=0.000417 6$OC=6.60E-5 10$PC=4.46E-6 7
146LA G 158.90 1426 2[M1] 0.294 C
146LAS G KC=0.251 4$LC=0.0338 5$MC=0.00701 10
146LAS G NC=0.001542 22$OC=0.000251 4$PC=1.95E-5 3
146LA G 180.3 12 2[E1+M2] 0.18 +3-4 0.085 15 C
146LAS G KC=0.071 13$LC=0.0109 23$MC=0.0023 5
146LAS G NC=0.00051 11$OC=8.1E-5 17$PC=5.7E-6 12
146LA G 208.50 2211 3[M1] 0.1395 C
146LAS G KC=0.1194 17$LC=0.01594 23$MC=0.00331 5
146LAS G NC=0.000728 11$OC=0.0001185 17$PC=9.26E-6 14
146LA G 218.00 2221 2[M1] 0.1237 C
146LAS G KC=0.1059 15$LC=0.01412 21$MC=0.00293 5
146LAS G NC=0.000644 10$OC=0.0001049 15$PC=8.21E-6 12
146LA G 254.4 15 3 C
146LA G 274.30 1464 8 C
146LA G 352.00 1427 3 C
146LA G 450.00 1470 4 C
146LA G 506.2 12 2 C
146LA L 675.22 9 (1-,2-)
146LA B 0.50 12 7.84 11 C1U
146LAS B EAV=1414 14
146LA G 478.80 2218 3 C
146LA G 530.60 1425 2 C
146LA G 534.10 1424 4 C
146LA L 686.90 10 (1-,2-)
146LA B 0.16 13 8.3 4 C1U
146LAS B EAV=1409 14
146LA G 198.4 8 1[M1] 0.1597 C
146LAS G KC=0.1366 20$LC=0.0183 3$MC=0.00379 6
146LAS G NC=0.000834 12$OC=0.0001357 19$PC=1.060E-5 15
146LA G 247.5 12 2[M1] 0.0880 C
146LAS G KC=0.0753 11$LC=0.01001 14$MC=0.00208 3
146LAS G NC=0.000457 7$OC=7.44E-5 11$PC=5.83E-6 9
146LA G 314.00 1431 3 C
146LA G 360.2 314 5 C
146LA L 708.84 81+
146LA B 9.1 6 5.07 4 C
146LAS B EAV=1416 14
146LA cB E$3350 {I150} (1986Gr11)
146LA G 209.1 10 2 C
146LA G 270.9 394 5 BC
146LA3 G FL=439.04
146LA cG E$poor fit: the energy level difference equals 269.79 {I9}
146LA G 279.50 14277 12D &C
146LA G 291.5 369 12 C
146LA G 316.30 14188 11D C
146LA G 335.80 2218 4 C
146LA G 511.9 32 3 C
146LA G 568.20 2220 5 C
146LA L 722.39 9 (1,2-)
146LA B 0.82 16 6.11 9
146LAS B EAV=1409 14
146LA G 283.2 311 3 C
146LA G 349.5 350 6 C
146LA G 525.70 2210 4
146LA G 722.50 1452 5
146LAF G FL=0.0
146LA L 757.88 12 (1,2-)
146LA B 0.23 13 8.11 25 C1U
146LAS B EAV=1376 14
146LA G 347.6 426 5 C
146LA G 385.40 1426 4 C
146LA G 617.0 10 2 C
146LA L 880.24 71+
146LA B 8.6 6 5.00 4 C
146LAS B EAV=1336 14
146LA cB E$3140 {I180} (1986Gr11)
146LA G 380.1 324 5 C
146LA G 413.60 14160 6M1+E2 -0.33 +8-9 0.0225 5 AC
146LAS G KC=0.0193 4$LC=0.00257 4$MC=0.000533 8
146LAS G NC=0.0001171 17$OC=1.90E-5 3$PC=1.47E-6 4
146LA cG MR$the 2{+nd} value |d=21 {I+|@-13}; both |d values were derived
146LA2cG from A{-2}=0.096 {I67}, A{-4}=0.04 {I15} for the cascade 414|g-269|g
146LA3cG assuming |d(269|g)=0
146LA G 436.40 2223 6 C
146LA G 441.20 14138 6 C
146LA G 462.60 2216 3 C
146LA G 487.7 57 7D C
146LA G 507.8 3 74 13M1+E2 +0.37 +18-130.0133 5 AC
146LAS G KC=0.0114 5$LC=0.00150 4$MC=0.000311 8
146LAS G NC=6.84E-5 17$OC=1.11E-5 3$PC=8.7E-7 4
146LA cG MR$the 2{+nd} value |d=2.7 {I+14-9}; both |d values were derived
146LA2cG from A{-2}=-0.134 {I74}, A{-4}=-0.10 {I16} for the cascade 508|g-251|g
146LA G 585.60 2222 3 C
146LA G 683.40 2218 4 C
146LA G 759.10 1462 6 C
146LA G 880.20 1467 4
146LAF G FL=0.0
146LA L 1005.5 3 (1)
146LA B 0.30 10 6.38 15 C
146LAS B EAV=1278 14
146LA G 296.5 8 5 C
146LA G 612.9 313 4 C
146LA L 1041.38 13 (1)
146LA B 0.62 14 6.05 10
146LAS B EAV=1262 14
146LA G 466.80 1431 5 &C
146LA G 669.10 2219 8 C
146LA L 1064.51 61+
146LA B 6.3 4 5.03 4
146LAS B EAV=1251 14
146LA G 342.30 1457 4 C
146LA G 355.6 314 2 &C
146LA G 389.70 2227 6 C
146LA G 489.80 1457 4 C
146LA G 564.40 1439 5 C
146LA G 576.30 2214 4
146LA G 598.40 2219 5 C
146LA G 635.20 1440 4 C
146LA G 672.0 11 3 C
146LA G 692.00 1499 4 C
146LA G 768.90 2215 4 C
146LA G 1064.70 1457 12
146LAF G FL=0.0
146LA L 1181.91 81+
146LA B 3.15 24 5.26 4
146LAS B EAV=1197 14
146LA G 301.4 315 3 C
146LA G 607.80 1427 5 C
146LA G 681.8 413 4 C
146LA G 715.30 2218 4 C
146LA G 742.80 2221 3 C
146LA G 752.60 1462 6 C
146LA G 764.3 10 2 C
146LA G 788.80 2210 2 C
146LA G 809.00 2229 6 C
146LA G 1061.4 311 1 C
146LA G 1182.3 46 2
146LAF G FL=0.0
146LA L 1190.18 91+
146LA B 3.21 23 5.24 4
146LAS B EAV=1193 14
146LA G 431.4 322 2 C
146LA G 502.80 2217 6 C
146LA G 702.0 28 3 C
146LA G 724.00 1483 5 C
146LA G 750.8 321 6 C
146LA G 760.8 36 1 C
146LA G 818.00 2218 2 C
146LA G 993.20 2225 2 C
146LA G 1049.2 46 3 C
146LA L 1224.10 11 1+
146LA B 1.70 23 5.50 7
146LAS B EAV=1177 14
146LA G 735.80 2224 4 C
146LA G 785.2 44 13 C
146LA G 795.20 2232 6 C
146LA G 851.50 1420 2 &C
146LA L 1268.96 81+
146LA B 2.39 18 5.32 4
146LAS B EAV=1157 14
146LA G 388.50 2225 6 C
146LA G 546.4 38 3
146LA G 621.60 2221 3 C
146LA G 802.50 2244 5 C
146LA G 829.9 4 1 C
146LA G 851.50 145 1 &C
146LA G 876.50 1416 1 C
146LA G 896.70 2222 2 C
146LA G 973.80 1410 1 C
146LA G 1128.1 13 2 C
146LA L 1308.44 16 (1)
146LA B 0.87 15 5.74 8
146LAS B EAV=1138 14
146LA G 550.9 7 1 C
146LA G 733.9 311 4 C
146LA G 842.00 2226 3 C
146LA G 869.1 317 8 C
146LA L 1415.71 12 (1)
146LA B 0.64 7 5.80 6
146LAS B EAV=1089 14
146LA G 841.00 2219 3 C
146LA G 1023.00 229 2 C
146LA G 1043.30 1417 1 C
146LA L 1443.45 71+
146LA B 3.31 22 5.07 4
146LAS B EAV=1076 14
146LA G 868.80 2242 8 C
146LA G 943.40 1421 1 C
146LA G 955.3 310 2 C
146LA G 976.80 1422 2 C
146LA G 1003.80 2210 1 C
146LAF G FL=439.04
146LA G 1050.9 423 3 C
146LA G 1070.80 1485 4 C
146LA G 1148.70 1410 1 C
146LA G 1247.00 2210 1 C
146LA L 1469.15 81+
146LA B 3.5 3 5.03 5
146LAS B EAV=1065 14
146LA G 821.80 1445 2 C
146LA G 894.60 1490 15 C
146LA G 981.2 3 1 C
146LA G 1002.0 36 2 C
146LA G 1040.10 1424 1 C
146LA G 1076.50 1432 2 C
146LA G 1097.10 2221 9 C
146LA G 1174.5 318 3 C
146LA G 1328.5 5 1 C
146LA L 1481.50 101+
146LA B 1.83 13 5.30 4
146LAS B EAV=1059 14
146LA G 773.0 410 4 C
146LA G 834.20 2219 4 C
146LA G 1052.40 2228 1 C
146LA G 1088.90 1422 1 C
146LA G 1108.90 1429 1 C
146LA G 1341.2 21 3 C
146LA3 G FL=140.85
146LA L 1507.73 15
146LA B 0.70 8 5.70 6
146LAS B EAV=1047 14
146LA G 1068.9 12 2 C
146LA G 1078.50 1437 4 C
146LA L 1534.43 7 1+
146LA B 4.30 23 4.89 4
146LAS B EAV=1035 14
146LA G 847.30 1438 2 C
146LA G 887.10 1435 2 C
146LA G 1068.00 1456 2 C
146LA G 1095.50 1490 3 C
146LA G 1105.30 1451 1 C
146LA G 1142.2 55 2 C
146LA G 1162.00 1422 1 C
146LA G 1337.1 66 2 C
146LA L 1606.47 24
146LA B 0.36 6 5.92 8
146LAS B EAV=1002 14
146LA G 565.4 56 2 C
146LA G 1213.8 11 2 C
146LA G 1311.4 38 2 C
146LA L 1624.43 91+
146LA B 2.33 16 5.09 4
146LAS B EAV=994 14
146LA G 745.20 2212 3 BC
146LAF G FL=880.24
146LA cG E$poor fit: the energy level difference equals 744.19 {I10}
146LA G 867.00 2217 5
146LA G 915.50 2216 2 C
146LA G 949.00 155 1 C
146LAF G FL=675.22
146LA G 1186.70 1427 1 BC
146LAF G FL=439.04
146LA cG E$poor fit: the energy level difference equals 1185.38 {I10}
146LA G 1195.4 20 2 C
146LA G 1207.2 11 2 C
146LA G 1231.60 227 1 C
146LA G 1484.0 22 3 C
146LA G 1503.30 1427 2 C
146LA L 1650.80 11
146LA B 0.67 9 5.62 7
146LAS B EAV=982 14
146LA G 1184.20 1416 1 C
146LA G 1211.80 1418 5 C
146LA G 1258.2 6 1 C
146LA G 1453.7 7 1 C
146LA L 1693.36 13
146LA B 0.80 8 5.51 5
146LAS B EAV=962 14
146LA G 814.2 410 4 C
146LAF G FL=880.24
146LA G 1226.80 225 1 C
146LA G 1253.70 2214 1 C
146LA G 1321.10 2215 1 C
146LA G 1495.00 2212 2 BC
146LAF G FL=197.03
146LA cG E$poor fit: the energy level difference equals 1496.32 {I13}
146LA L 1722.35 14
146LA B 0.80 10 5.49 6
146LAS B EAV=949 14
146LA G 1013.40 2213 5 C
146LA G 1283.4 39 1 C
146LA G 1350.1 320 3 C
146LA G 1427.2 39 1 C
146LA G 1525.2 5 1 C
146LA L 1777.68 141+
146LA B 0.88 8 5.40 5
146LAS B EAV=924 14
146LA G 1203.40 2211 2 C
146LA G 1339.0 314 2 C
146LA G 1384.9 14 2 C
146LA G 1405.0 37 2 C
146LA G 1481.8 410 2 C
146LA G 1656.2 6 1 C
146LA L 1882.15 21
146LA B 0.41 8 5.66 9
146LAS B EAV=877 14
146LA G 1443.10 2222 5 C
146LA G 1489.5 7 1 C
146LA L 2060.51 24
146LA B 0.51 8 5.41 8
146LAS B EAV=796 14
146LA G 1642.9 326 5 C
146LA G 1919.8 4 1 C
146LA G 1939.3 6 1 C
146LA L 2165.91 171+
146LA B 0.53 9 5.31 8
146LAS B EAV=749 14
146LA G 1102.0 38 1 C
146LA G 1456.8 9 2 C
146LA G 1773.2 4 1 C
146LA G 1870.5 38 2 C
146LA G 2044.6 48 2 C