147PR 147CE B- DECAY 1993MA39,1997GR09 22NDS 202203
147PR H TYP=FUL$AUT=N. Nica and B. Singh$CIT=NDS 181, 1 (2022)$CUT=9-Mar-2022$
147CE P 0.0 (5/2-) 56.4 S 10 3430 16
147CE cP E,J,T$From {+147}Ce Adopted Levels
147CE cP QP$From 2021Wa16
147PR c 1997Gr09, 1996Gr20: {+252}Cf SF, measured |b{+-}-decay intensity
147PR2c distribution by total absorption |g-ray spectrometer (TAGS)
147PR c 1993Ma39: n{-th}-induced {+235}U fission products analyzed with
147PR2c Tristan ISOL isotope separator at BNL with thermoionization source
147PR2c and moving tape collector. Used two Ge(Li), two Ge and Si(Li).
147PR2c Measured |g, |g|g, |a(K)exp. Supersede 1988MaZI, 1987MaZO
147PR c 1987ScZG, 1981ScZM: fission products analyzed with ISOL systems
147PR2c Lohengrin and Ostis (ILL Grenoble), and Josef (K.F.A Julich).
147PR2c Measured |g, |g|g, |g|g(t), |b|g(t). Measured conversion electrons and
147PR2c mixing ratios (K/L ratio).
147PR c 1984So18: measured ratio of count rates of a |g ray relative to
147PR2c a reference |g ray (with known %I|g relative to the |b{+-} decay of
147PR2c the parent) using mass separators (HELIOS, OSTIS) and Ge(Li)
147PR2c detectors at radioactive equilibrium
147PR c 1979Bo26: precision E|g with curved-crystal spectrometer; used the
147PR2c 411.8044 keV |g transition in {+198}Au |b{+-} decay as
147PR2c energy-calibration standard (so called gold standard) to obtain
147PR2c 98.4345 keV for the uranium KL3 x-ray. 2000He14 recommend 411.80205
147PR2c keV {I17} for the gold standard (data reported here are not adjusted)
147PR c Others: 1995Ik03, 1986Gr11 (|b, |b|g, |b end point, Q(|b{+-})),
147PR2c 1993Sh33, 1975Pi03, 1964Ho03 (see {+147}Pr |b{+-}, used for I|g
147PR2c normalization), 1982To16 (|g, |g|g), 1981Ya06 (|g, |g|g, |b|g,
147PR2c T{-1/2}, Q(|b{+-})), 1977Bj02 (|g, |g|g), 1977Re11 (|g, T{-1/2}),
147PRxc 1975Do15 (|g, |g|g, T{-1/2})
147PR c Level scheme is from 1993Ma39 and might be incomplete
147PR cL E$From least-squares fit to E|g's; as E|g's were reported with no
147PR2cL uncertainties, |DE|g=0.30 keV assumed for least-squares fitting
147PR cL J,T(a)$From Adopted Levels
147PR cL T(b)$From 1981ScZM
147PR cG E$From 1993Ma39, except when noted. E|g's listed in table are given
147PR2cG with one, two, or three decimal digits as listed in 1993Ma39,
147PR2cG although usually one does not expect more than one significant
147PR2cG decimal digit for their method
147PR cG RI$From 1993Ma39 (no uncertainties are reported)
147PR cG E(A)$E|g is from measurements with curved crystal spectrometers
147PR2cG (1979Bo26)
147PR cG M$From 1981ScZM based on |g-ray, conversion electron studies
147PR2cG and K/L ratios (values not given), except as noted (same values are
147PR2cG adopted in the Adopted Levels, Gammas dataset)
147PR cG E(N),RI(N)$From 1981ScZM
147PR cG CC(B)$|a not known. The value shown is the average of the smallest and
147PR2cG largest values for the E1, E2, and M1 multipolarities for this
147PR2cG transition with an uncertainty taken large enough to overlap these
147PR2cG values
147PR cB $Q(|b{+-})|?3.4 MeV and the highest level at |?2.2 MeV indicate that
147PR2cB the level scheme might be incomplete. However based on the existing
147PR2cB data, |SI|b=102 {I17}, which indicates that the level scheme is rather
147PR2cB complete. This contradiction suggests that these data should be used
147PR2cB rather cautiously; new studies are needed for {+147}Ce |b{+-} decay
147PR cB $Although 1993Ma39 and 1997Gr09 are in general agreement, there is
147PR2cB an excess of I|b for states <1300 keV and a deficient of I|b for
147PR2cB states >1300 keV of 1993Ma39 compared to 1997Gr09 (1997Gr09 used
147PR2cB 1993Ma39 level scheme for TAGS simulated spectrum). Based on
147PR2cB substantial agreement between measured and simulated shapes of TAGS
147PR2cB spectra, 1997Gr09 suggest that 1993Ma39 failed to identify all the
147PR2cB level deexcitation modes (rather than undetected levels)
147PR cB IB,LOGFT$The uncertainties are underestimated because measured I|g
147PR2cB values have no reported uncertainties, which makes these values
147PR2cB tentative.
147PR N 0.092 1.00
147PR PN 4
147PR cN NR$0.092 {I12} based on the average ratio, 0.0635 {I52}, of |g-ray
147PR2cN counting rates
147PR2cN (at radioactive equilibrium) of five |g rays in this decay (269|g,
147PR2cN 374|g, 467|g, 452|g, and 219|g) to that of 315|g ({+147}Pr |b{+-}
147PR2cN decay), all measured by 1984So18, with %I|g(315|g)=12.6 (1975Pi03) used
147PR2cN by 1984So18 replaced by evaluator with %I|g(315|g)=18.2 {I18} (see
147PR2cN discussion on I|g normalization in {+147}Pr |b{+-} decay in {+147}Nd
147PR2cN datasets). Alternatively if one uses %I|b=14.0 {I20} from 1997Gr09
147PR2cN (for the |b feeding of g.s., 2.7, 28, and 93 levels) one gets
147PR2cN 0.121 {I5} for I|g normalization.
147PR G 48.4 3 N
147PR2 G %IG=0.28
147PR G 77.2 3.5 N
147PR2 G %IG=0.32
147PR L 0.0 (3/2+) 13.44 M 10 a
147PR B 32 6.0
147PRS B EAV=1423.9 74
147PR cB IB$sum of I|b for g.s. plus first two excited states (obtained
147PR2cB from I|g imbalance at each level); compare to 12.8
147PR2cB (1993Ma39) and 79 {I3} (1992De38);
147PR2cB also compare the sum of I|b for ground state plus first three excited
147PR2cB states obtained here, 38 {I8}, with 14.0 {I20} (1996Gr20, 1997Gr09,
147PR2cB TAGS, same group). The differences are due to different I|g
147PR2cB normalizations (see {+147}Pr |b{+-} decay dataset).
147PR L 2.67 11(5/2+)
147PR B
147PR cB IB$included in g.s. I|b
147PR G 2.7 10 S
147PR L 27.77 11(7/2+)
147PR B
147PR cB IB$included in g.s. I|b
147PR G 25.3 [M1,E2] 3.4E2 33
147PR L 93.29 9 (5/2+) 12 NS b
147PR B 6 6.7
147PRS B EAV=1380.8 74
147PR G 65.21 10.3 [M1,E2] 7.3 29
147PR2 G %IG=0.95
147PR G 90.44 15 [M1,E2] 2.39 66
147PR2 G %IG=1.4
147PR G 93.17 73 M1 1.586
147PR2 G %IG=6.7
147PRS G KC=1.350 19$LC=0.186 3$MC=0.0393 6
147PRS G NC=0.00879 13$OC=0.001414 20$PC=0.0001037 15
147PR L 246.52 11(9/2+)
147PR B 0.34 7.8
147PRS B EAV=1310.0 74
147PR G 218.751 10 25.5 M1+E2 0.57 0.1446
147PR2 G %IG=2.4
147PRF G FLAG=A
147PRF G FL=27.77
147PRS G KC=0.1203 17$LC=0.0192 3$MC=0.00410 6
147PRS G NC=0.000910 13$OC=0.0001423 20$PC=8.80E-6 13
147PR cG E$218.384 (1993Ma39)
147PR cG M$from |a(K)exp=0.175 {I4} (1993Ma39); M1 in 1993Ma39
147PR G 243.693 8.6 E2 0.0985
147PR2 G %IG=0.79
147PRS G KC=0.0908 13$LC=0.01326 19$MC=0.00281 4
147PRS G NC=0.000626 9$OC=9.95E-5 14$PC=6.78E-6 10
147PR cG M$from |a(K)exp=0.077 {I4} (1993Ma39); E2 in 1993Ma39
147PR L 291.82 9(5/2+)
147PR B 1.2 7.2
147PRS B EAV=1289.1 74
147PR G 198.534 12 33.6 M1 0.190 A
147PR2 G %IG=3.1
147PRF G FL=93.29
147PRS G KC=0.1621 23$LC=0.0221 3$MC=0.00465 7
147PRS G NC=0.001040 15$OC=0.0001675 24$PC=1.239E-5 18
147PR cG E$198.214 (1993Ma39)
147PR cG M$from |a(K)exp=0.175 {I5} (1993Ma39)
147PR G 263.70 1.2 0.05 4 B
147PR2 G %IG=0.11
147PR G 289.345 21.4 M1 0.0690
147PR2 G %IG=2.0
147PRS G KC=0.0590 9$LC=0.00795 12$MC=0.001672 24
147PRS G NC=0.000374 6$OC=6.03E-5 9$PC=4.49E-6 7
147PR cG M$from |a(K)exp=0.074 {I2} (1993Ma39)
147PR G 292.036 6.9 M1+E2 0.061 7
147PR2 G %IG=0.64
147PRS G KC=0.051 7$LC=0.0083 6$MC=0.00178 15
147PRS G NC=0.00039 3$OC=6.1E-5 3$PC=3.6E-6 8
147PR cG M$from |a(K)exp=0.0522 {I4} (1993Ma39)
147PR L 362.03 10(7/2-)
147PR B 5.2 6.6
147PRS B EAV=1256.7 74
147PR cB IB$1.31 (1997Gr09)
147PR G 69.89 2 [E1] 0.667
147PR2 G %IG=0.18
147PR G 115.5 0.36 [E1] 0.1691
147PR2 G %IG=0.033
147PR G 268.80 6 100 E1 0.01725 A
147PR2 G %IG=9.2
147PRS G KC=0.01478 21$LC=0.00196 3$MC=0.000410 6
147PRS G NC=9.10E-5 13$OC=1.441E-5 21$PC=9.82E-7 14
147PR cG E$268.913 (1993Ma39)
147PR cG M$from |a(K)exp=0.0140 {I4} (1993Ma39); M1+E2 (1981ScZM)
147PR G 358.95 15.4 (E1) 0.00828 @
147PR2 G %IG=1.4
147PRS G KC=0.00710 10$LC=0.000929 13$MC=0.000194 3
147PRS G NC=4.33E-5 6$OC=6.89E-6 10$PC=4.82E-7 7
147PR cG M$from |a(K)exp=0.0077 {I11} for unresolved 359|g+359|g+361|g
147PRxcG multiplet (1993Ma39)
147PR G 361.7 1 @
147PR2 G %IG=0.092
147PR L 384.76 15(11/2-)
147PR G 23 2 AP [E2] 1067 ?
147PR G 138.37 7.4 [E1] 0.1029
147PR2 G %IG=0.68
147PR L 452.32 12(3/2-,5/2-)
147PR B 2.6 6.8
147PRS B EAV=1215.1 74
147PR cB IB$0.93 (1997Gr09)
147PR G 358.96 8.4 (E1) 0.00828 @
147PR2 G %IG=0.77
147PRS G KC=0.00710 10$LC=0.000929 13$MC=0.000194 3
147PRS G NC=4.33E-5 6$OC=6.89E-6 10$PC=4.82E-7 7
147PR cG M$from |a(K)exp=0.0077 {I11} for unresolved 359|g+359|g+361|g multiplet
147PR2cG (1993Ma39); assignment made tentative by evaluator
147PR G 449.55 10.7 (E1) 0.00481
147PR2 G %IG=0.98
147PRS G KC=0.00413 6$LC=0.000536 8$MC=0.0001120 16
147PRS G NC=2.50E-5 4$OC=3.99E-6 6$PC=2.84E-7 4
147PR cG M$from |a(K)exp=0.0034 {I5} for unresolved 450|g+452|g multiplet
147PR2cG (1993Ma39); assignment made tentative by evaluator
147PR G 452.222 47.2 (E1) 0.00474
147PR2 G %IG=4.3
147PRS G KC=0.00408 6$LC=0.000528 8$MC=0.0001105 16
147PRS G NC=2.46E-5 4$OC=3.93E-6 6$PC=2.80E-7 4
147PR cG M$from |a(K)exp=0.0034 {I5} for unresolved 450|g+452|g multiplet @
147PR2cG (1993Ma39); assignment made tentative by evaluator
147PR L 467.49 10(3/2-,5/2-)
147PR B 5.9 6.4
147PRS B EAV=1208.2 74
147PR cB IB$2.09 (1997Gr09)
147PR G 105.59 0.7 [M1,E2] 1.4 4
147PR2 G %IG=0.064
147PR G 175.37 6.7 (E1) 0.0539
147PR2 G %IG=0.62
147PRS G KC=0.0460 7$LC=0.00622 9$MC=0.001303 19
147PRS G NC=0.000288 4$OC=4.53E-5 7$PC=2.93E-6 5
147PR cG M$from |a(K)exp=0.087 {I8} (1993Ma39); comparing |a(K)exp with
147PR2cG calculated values, E1 is least discrepant
147PR G 374.23 6 55.0 E1 0.00747 A
147PR2 G %IG=5.1
147PRS G KC=0.00641 9$LC=0.000838 12$MC=0.0001752 25
147PRS G NC=3.90E-5 6$OC=6.21E-6 9$PC=4.36E-7 7
147PR cG E$374.313 (1993Ma39)
147PR cG M$from |a(K)exp=0.061 {I6} (1993Ma39)
147PR G 464.713 18.1 (E1) 0.00445 @
147PR2 G %IG=1.7
147PRS G KC=0.00383 6$LC=0.000495 7$MC=0.0001035 15
147PRS G NC=2.31E-5 4$OC=3.69E-6 6$PC=2.63E-7 4
147PR cG M$from |a(K)exp=0.0062 {I15} (1993Ma39); comparing |a(K)exp with
147PR2cG calculated values, E1 is least discrepant
147PR G 467.33 43 E1 0.00439
147PR2 G %IG=4.0
147PRS G KC=0.00378 6$LC=0.000489 7$MC=0.0001022 15
147PRS G NC=2.28E-5 4$OC=3.64E-6 5$PC=2.60E-7 4
147PR cG M$from |a(K)exp=0.0047 {I7} (1993Ma39)
147PR L 470.69 15(9/2+)
147PR G 108.9 0.5 [E1] 0.199
147PR2 G %IG=0.046
147PR G 178.72 4.5 (E2) 0.278
147PR2 G %IG=0.41
147PRS G KC=0.203 3$LC=0.0586 9$MC=0.01296 19
147PRS G NC=0.00282 4$OC=0.000409 6$PC=1.201E-5 17
147PR cG M$from |a(K)exp=0.317 {I13} (1993Ma39)
147PR G 377.59 4.1
147PR2 G %IG=0.38
147PR G 442.55 4.8
147PR2 G %IG=0.44
147PR L 545.91 14(9/2+)
147PR B 0.58 7.4
147PRS B EAV=1172.1 74
147PR cB IB$0.83 (1997Gr09)
147PR G 161.56 4.1 [E1] 0.0674
147PR2 G %IG=0.38
147PR G 183.8 0.2 [E1] 0.0474
147PR2 G %IG=0.018
147PR G 254.09 11.6 E2 0.0859 12
147PR2 G %IG=1.1
147PRS G KC=0.075 9$LC=0.0130 18$MC=0.0028 5
147PRS G NC=0.00062 9$OC=9.5E-5 10$PC=5.3E-6 11
147PR cG M$from |a(K)exp=0.078 {I3} (1993Ma39)
147PR G 299.63 1.1 0.04 3 B
147PR2 G %IG=0.10
147PR L 608.01 14(7/2-)
147PR B 8.3 6.2
147PRS B EAV=1143.6 74
147PR cB IB$2.00 (1997Gr09)
147PR G 316.4 5 0.03 2 B
147PR2 G %IG=0.46
147PR G 361.42 9 @
147PR2 G %IG=0.83
147PR G 514.81 6.3
147PR2 G %IG=0.58
147PR G 580.28 63 (E1) 0.00269
147PR2 G %IG=5.8
147PRS G KC=0.00232 4$LC=0.000297 5$MC=6.21E-5 9
147PRS G NC=1.384E-5 20$OC=2.22E-6 4$PC=1.609E-7 23
147PR cG M$from |a(K)exp=0.0027 {I4} for unresolved 579|g+580|g multiplet
147PR2cG (1993Ma39); assignment made tentative by evaluator
147PR G 605.4 22.7 (E1) 0.00245
147PR2 G %IG=2.1
147PRS G KC=0.00211 3$LC=0.000270 4$MC=5.65E-5 8
147PRS G NC=1.260E-5 18$OC=2.02E-6 3$PC=1.469E-7 21
147PR cG M$K-conversion peak not observed excludes M1+E2 (1993Ma39)
147PR L 638.00 20(3/2,5/2,7/2-)
147PR B 0.24 7.7
147PRS B EAV=1129.9 74
147PR cB IB$0.0 (1997Gr09)
147PR G 185.7 3.2 0.15 10 B
147PR2 G %IG=0.29
147PR G 544.89 3.8
147PR2 G %IG=0.35
147PR L 701.32 14(5/2-)
147PR B 3.8 6.5
147PRS B EAV=1100.9 74
147PR cB IB$1.24 (1997Gr09)
147PR G 233.95 1.5 0.07 5 B
147PR2 G %IG=0.14
147PR G 248.5 3.4 0.06 4 B
147PR2 G %IG=0.31
147PR G 455.3 1.29
147PR2 G %IG=0.12
147PR G 607.60 9.3
147PR2 G %IG=0.86
147PR G 698.59 6.3
147PR2 G %IG=0.58
147PR G 701.13 27.9 (E1) 0.00180
147PR2 G %IG=2.6
147PRS G KC=0.001547 22$LC=0.000197 3$MC=4.11E-5 6
147PRS G NC=9.17E-6 13$OC=1.473E-6 21$PC=1.081E-7 16
147PR cG M$K-conversion peak not observed excludes M1+E2 (1993Ma39)
147PR L 748.88 15(5/2+,7/2)
147PR B 1.6 6.8
147PRS B EAV=1079.1 74
147PR cB IB$0.35 (1997Gr09)
147PR G 202.87 1.5 0.11 7 B
147PR2 G %IG=0.14
147PR G 386.8 2.1
147PR2 G %IG=0.19
147PR G 456.9 1.4
147PR2 G %IG=0.13
147PR G 502.31 3.3
147PR2 G %IG=0.30
147PR G 656.07 3.8
147PR2 G %IG=0.35
147PR G 746.36 7.3
147PR2 G %IG=0.67
147PR L 783.6 4
147PR B 0.29 7.6
147PRS B EAV=1063.3 74
147PR cB IB$0.0 (1997Gr09)
147PR G 537.10 3.1
147PR2 G %IG=0.29
147PR L 802.84 13(5/2+)
147PR B 2.3 6.6
147PRS B EAV=1054.5 73
147PR cB IB$0.69 (1997Gr09)
147PR G 335.2 4 0.03 2 B
147PR2 G %IG=0.37
147PR G 350.4 1.5 0.03 2 B
147PR2 G %IG=0.14
147PR G 440.62 8.2
147PR2 G %IG=0.75
147PR G 510.9 1.4 @
147PR2 G %IG=0.13
147PR G 709.4 2
147PR2 G %IG=0.18
147PR G 802.86 11.5 (M1+E2) 0.0044 10
147PR2 G %IG=1.1
147PRS G KC=0.0037 8$LC=0.00050 9$MC=0.000106 19
147PRS G NC=2.4E-5 5$OC=3.8E-6 7$PC=2.7E-7 7
147PR cG M$from |a(K)exp=0.009 {I2} for unresolved 800|g+802|g multiplet
147PR2cG (1993Ma39)
147PR L 931.57 17(3/2,5/2,7/2+)
147PR B 0.99 6.9
147PRS B EAV=995.8 73
147PR cB IB$0.27 (1997Gr09)
147PR G 464.2 3 @
147PR2 G %IG=0.28
147PR G 639.3 1.8
147PR2 G %IG=0.17
147PR G 838.62 0.8
147PR2 G %IG=0.074
147PR G 931.57 5.2
147PR2 G %IG=0.48
147PR L 951.63 14(5/2+,7/2+)
147PR B 2.0 6.6
147PRS B EAV=986.7 73
147PR cB IB$0.48 (1997Gr09)
147PR G 484.56 4.0
147PR2 G %IG=0.37
147PR G 659.15 4.6 @
147PR2 G %IG=0.42
147PR G 705.6 1 @
147PR2 G %IG=0.092
147PR G 857.87 8.5
147PR2 G %IG=0.78
147PR G 949.13 4
147PR2 G %IG=0.37
147PR G 951.93 6 @
147PR2 G %IG=0.55
147PR L 961.06 17(5/2+,7/2)
147PR B 0.95 6.9
147PRS B EAV=982.4 73
147PR cB IB$0.21 (1997Gr09)
147PR G 414.8 1.5
147PR2 G %IG=0.14
147PR G 489.99 1.9
147PR2 G %IG=0.18
147PR G 493.44 3.1
147PR2 G %IG=0.29
147PR G 599.52 2.8
147PR2 G %IG=0.26
147PR G 714.9 1
147PR2 G %IG=0.092
147PR L 978.07 17 (7/2-)
147PR B 0.14 7.7
147PRS B EAV=974.7 73
147PR cB IB$0.0 (1997Gr09)
147PR G 510.4 1.1 @
147PR2 G %IG=0.10
147PR G 593.29 5.1 @
147PR2 G %IG=0.47
147PR G 616.0 2.9
147PR2 G %IG=0.27
147PR L 1045.94 13(3/2-,5/2)
147PR B 1.9 6.6
147PRS B EAV=943.9 73
147PR cB IB$0.65 (1997Gr09)
147PR G 297.37 2.4 0.04 3 B
147PR2 G %IG=0.22
147PR G 344.25 2.2 0.03 2 B
147PR2 G %IG=0.20
147PR G 578.5 3.4
147PR2 G %IG=0.31
147PR G 593.0 3.2 @
147PR2 G %IG=0.29
147PR G 684.2 1.7
147PR2 G %IG=0.16
147PR G 754.66 1.4
147PR2 G %IG=0.13
147PR G 952.3 0.7 @
147PR2 G %IG=0.064
147PR G 1045.82 6.9
147PR2 G %IG=0.64
147PR L 1058.90 24 (7/2-,9/2+)
147PR B 0.23 7.5
147PRS B EAV=938.0 73
147PR cB IB$0.085 (1997Gr09)
147PR G 674.08 1.5
147PR2 G %IG=0.14
147PR G 1056.27 1.02
147PR2 G %IG=0.094
147PR L 1068.05 16(7/2+)
147PR B 1.6 6.6
147PRS B EAV=933.9 73
147PR cB IB$0.59 (1997Gr09)
147PR G 682.9 1.1
147PR2 G %IG=0.10
147PR G 705.7 2 @
147PR2 G %IG=0.18
147PR G 776.53 7.4
147PR2 G %IG=0.68
147PR G 1065.41 4.8
147PR2 G %IG=0.44
147PR G 1068.40 1.7
147PR2 G %IG=0.16
147PR L 1159.58 24(3/2,5/2,7/2-)
147PR B 0.61 7.0
147PRS B EAV=892.5 73
147PR cB IB$0.40 (1997Gr09)
147PR G 707.4 3
147PR2 G %IG=0.28
147PR G 1156.77 3.6
147PR2 G %IG=0.33
147PR L 1170.20 16(7/2+)
147PR B 0.52 7.0
147PRS B EAV=887.7 73
147PR cB IB$0.35 (1997Gr09)
147PR G 785.67 2.3
147PR2 G %IG=0.21
147PR G 808.2 1.6
147PR2 G %IG=0.15
147PR G 878.5 1.1
147PR2 G %IG=0.10
147PR G 1170.5 2.6
147PR2 G %IG=0.24
147PR L 1172.88 20(3/2-,5/2,7/2-)
147PR B 1.7 6.5
147PRS B EAV=886.5 73
147PR cB IB$1.29 (1997Gr09)
147PR G 705.5 9 @
147PR2 G %IG=0.83
147PR G 721.0 5.9
147PR2 G %IG=0.54
147PR G 810.3 3.2
147PR2 G %IG=0.29
147PR L 1194.43 14(5/2+,7/2+)
147PR B 3.0 6.2
147PRS B EAV=876.8 73
147PR cB IB$2.03 (1997Gr09)
147PR G 649.13 2.5
147PR2 G %IG=0.23
147PRF G FL=545.91
147PR G 727.01 6.1
147PR2 G %IG=0.56
147PR G 832.346 18
147PR2 G %IG=1.7
147PR G 1100.94 8.2
147PR2 G %IG=0.75
147PR G 1166.2 3.3
147PR2 G %IG=0.30
147PR G 1193.97 1.7
147PR2 G %IG=0.56
147PR L 1267.30 18(5/2+,7/2)
147PR B 1.3 6.5
147PRS B EAV=843.9 72
147PR cB IB$0.84 (1997Gr09)
147PR G 659.6 0.3 @
147PR2 G %IG=0.028
147PR G 796.8 4.6
147PR2 G %IG=0.42
147PR G 799.81 3 AP @
147PR G 1264.13 6.1
147PR2 G %IG=0.56
147PR L 1285.79 20(3/2-,5/2,7/2-)
147PR B 1.1 6.6
147PRS B EAV=835.6 72
147PR cB IB$0.69 (1997Gr09)
147PR G 818.22 2.7
147PR2 G %IG=0.25
147PR G 833.5 3.8
147PR2 G %IG=0.35
147PR G 923.79 5.2
147PR2 G %IG=0.48
147PR L 1724.93 14(5/2+,7/2+)
147PR B 1.5 6.1
147PRS B EAV=640.6 71
147PR cB IB$4.82 (1997Gr09)
147PR G 530.7 2.5
147PR2 G %IG=0.23
147PR G 773.53 6.9
147PR2 G %IG=0.64
147PR G 921.5
147PR G 1116.42 3.1
147PR2 G %IG=0.29
147PR G 1179.1 1.9
147PR2 G %IG=0.18
147PR G 1478.7 0.8
147PR2 G %IG=0.074
147PR G 1725.2 0.6
147PR2 G %IG=0.055
147PR L 1845.92 15(5/2,7/2-)
147PR B 1.8 5.9
147PRS B EAV=587.8 70
147PR cB IB$5.70 (1997Gr09)
147PR G 676.4 2
147PR2 G %IG=0.18
147PR G 799.7 1.0 @
147PR2 G %IG=0.092
147PR G 867.98 6.6
147PR2 G %IG=0.61
147PR G 1042.9
147PR G 1378.29 2.6
147PR2 G %IG=0.24
147PR G 1393.72 3.8
147PR2 G %IG=0.35
147PR G 1483.51 3.1
147PR2 G %IG=0.29
147PR L 1856.34 20(3/2-,5/2,7/2)
147PR B 0.7 6.3
147PRS B EAV=583.3 70
147PR cB IB$2.48 (1997Gr09)
147PR G 1388.81 4.0
147PR2 G %IG=0.37
147PR G 1494.3 3.0
147PR2 G %IG=0.28
147PR G 1564.53 0.9
147PR2 G %IG=0.083
147PR L 1864.94 15(3/2-,5/2-,7/2-)
147PR B 1.9 5.8
147PRS B EAV=579.5 70
147PR cB IB$6.20 (1997Gr09)
147PR G 1062.14 4.1
147PR2 G %IG=0.38
147PR G 1227.13 4.9
147PR2 G %IG=0.45
147PR G 1257.0 3.4
147PR2 G %IG=0.31
147PR G 1397.49 3.5
147PR2 G %IG=0.32
147PR G 1412.52 3.2
147PR2 G %IG=0.29
147PR G 1572.8
147PR G 1862.3 1.3
147PR2 G %IG=0.12
147PR L 1943.85 13(7/2-)
147PR B 4.4 5.4
147PRS B EAV=545.4 69
147PR cB IB$9.65 (1997Gr09)
147PR G 965.4 1.0
147PR2 G %IG=0.092
147PR G 1335.93 7.1
147PR2 G %IG=0.65
147PR G 1473.16 4.9
147PR2 G %IG=0.45
147PR G 1476.60 10.7
147PR2 G %IG=0.98
147PR G 1491.84 6.9
147PR2 G %IG=0.64
147PR G 1582.06 2.4
147PR2 G %IG=0.22
147PR G 1697.29 2.4
147PR2 G %IG=0.22
147PR G 1850.0 7.5
147PR2 G %IG=0.69
147PR G 1915.8 1.0
147PR2 G %IG=0.092
147PR G 1941.5 4.4
147PR2 G %IG=0.41
147PR L 2060.58 18(5/2,7/2)
147PR B 0.96 5.9
147PRS B EAV=495.5 69
147PR cB IB$4.41 (1997Gr09)
147PR G 1452.88 2.8
147PR2 G %IG=0.26
147PR G 1768.4 3.1
147PR2 G %IG=0.29
147PR G 2032.5 0.20
147PR2 G %IG=0.018
147PR G 2058.2 4.3
147PR2 G %IG=0.40
147PR L 2135.32 18(7/2-)
147PR B 1.1 5.7
147PRS B EAV=463.9 68
147PR cB IB$1.83 (1997Gr09)
147PR G 1589.51 2.2
147PR2 G %IG=0.20
147PR G 1773.4 4.3
147PR2 G %IG=0.40
147PR G 1843.5 1.5
147PR2 G %IG=0.14
147PR G 2107.3 3.4
147PR2 G %IG=0.31
147PR L 2182.85 16(7/2-)
147PR B 1.3 5.6
147PRS B EAV=443.9 68
147PR cB IB$2.22 (1997Gr09)
147PR G 987.76 4.4
147PR2 G %IG=0.41
147PRF G FL=1194.43
147PR G 1637.2 2.3
147PR2 G %IG=0.21
147PR G 1798.0 1.3
147PR2 G %IG=0.12
147PR G 1936.8 3.3
147PR2 G %IG=0.30
147PR G 2089.4 1.8
147PR2 G %IG=0.17
147PR G 2180.3 0.56
147PR2 G %IG=0.052
147PR L 2249.64 18(7/2-)
147PR B 1.5 5.5
147PRS B EAV=416.0 67
147PR cB IB$4.97 (1997Gr09)
147PR G 1548.08 6.2
147PR2 G %IG=0.57
147PR G 1779.0 5.8
147PR2 G %IG=0.53
147PR G 1887.8 2.1
147PR2 G %IG=0.19
147PR G 2246.9 1.7
147PR2 G %IG=0.16