161TB 161GD B- DECAY 1975GA16,1976HN01 11NDS 201111
161TB H TYP=FUL$AUT=C. W. Reich$CIT=NDS 112,2497 (2011)$CUT=1-Jun-2011$
161TB D DATA SET UPDATED (OCTOBER, 2009) TO INCLUDE NEW QP VALUE, ICC
161TB2D VALUES FROM BRICC AND REVISED COMMENTS
161TB D The experimental methods were:
161TB D 161GD produced from 160GD(N,G), unless otherwise noted.
161TB D 1959Sc29: CE's measured in magnetic spectrograph. Enriched (95.4%)
161TB2D samples. ECK's from CE's and RI's from NaI spectra. Deduced
161TB3D several multipolarities. 1976Hn01 have better ECK's from better
161TB4D RI's.
161TB D 1960Wi10: Measured activation cross section and 161GD half-life.
161TB D 1964Lo09: 417-level half-life measured by GB- coincidences with plastic
161TB2D scintillators.
161TB D 1965Ma24: 417-, 480-, and 586-level half-lives from GB- coincidences wi
161TB2D plastic scintillators.
161TB D 1966FuZZ: Thesis including EG's and RI's.
161TB D 1966Zy02: Enriched sample (98.7%) was used in the production. G single
161TB2D were measured with Ge detector. Some GG coincidences were
161TB3D measured with NaI detectors. B- spectrum measured with
161TB4D anthracene detector. Measured 161GD half-life.
161TB D 1967Ma33: 480-level half-life from CEB- coincidences with plastic
161TB2D scintillator and magnetic lens spectrometer.
161TB D 1969Be54: 417-level half-life from GB- coincidences with plastic and
161TB2D stilbene crystals and GG coincidences with NaI detectors.
161TB D 1973Ga27: Conference report; see 1975Ga16 for complete work.
161TB D 1973MaZI: Progress report; give preliminary list of |g's assigned to
161TB2D this decay, but not useful.
161TB D 1973ViZN: 1973MaZI is better keyno.
161TB D 1974OkZW: Enriched (95.95%) sample used in production. G singles
161TB2D measured with Ge detector. GG(THETA) with Ge and NaI detectors
161TB3D and deduced four MR values, but 2nd solution not quoted.
161TB D 1975Ga16: Enriched (99.999%) sample used in production. G singles
161TB2D and GG coincidences measured with Ge detectors. Report 29 G's
161TB3D below 530 keV and 101 G's above 750 keV.
161TB D 1975GnZZ: Conference report; these data are repeated in 1976Hn01.
161TB D 1975HiZE: Abstract; saw 45 G's above 600 keV, but no data given. Not
161TB2D published.
161TB D 1976Hn01: G singles and GG coincidences measured with Ge detectors.
161TB2D Report 29 G's below 600 keV and none above that. Deduce G
161TB3D multipolarities from ECK's using CE data of 1959Sc29.
161TB cB E Measured E(|b{+-}) value is from 1966Zy02.
161TB cB IB,LOGFT I|b{+-} values are computed from |g-intensity balances and
161TB2cB the I|g values are normalized to give a total I|b{+-} of 100%. They
161TB3cB are not normalized to give 100% feeding of the ground state because
161TB4cB this value depends significantly on the very uncertain |a of the 56|g.
161TB5cB I|b{+-} and log| {Ift} values are not given for levels above 600 keV,
161TB6cB as the I|b{+-} values are too small (|<0.04%) to be meaningful, since
161TB7cB the unplaced |g's can change the values significantly.
161TB8cB The total I|b{+-} given is 99.4%.
161TB cB IB The calculated I|b{+-}(g.s.)=8% {I12} is not included since
161TB2cB it is assumed that this value results from an error in the
161TB3cB transition intensity of the 56-keV |g. This assumption is
161TB4cB supported by the calculated I|b{+-}(56)=-7% {I12}. See comments on
161TB5cB |a for the 56|g.
161TB cG E,RI From 1975Ga16; the nine doubtful unplaced |g's and one
161TB2cG possible sum peak (1975Ga16) have been omitted.
161TB3cG Others: 1976Hn01, 1974OkZW, 1966Zy02, and 1966FuZZ.
161TB cG M From K| x ray/|g and L{-1}/M ratios for 56-keV |g (1959Sc29
161TB2cG and 1976Hn01) and from |a(K)exp's (1976Hn01), using ce data of
161TB3cG 1959Sc29 for all other |g's with the |g and ce data scaled to the
161TB4cG theoretical M1 value for the 56-keV |g. The precision of the
161TB5cG ce data (1959Sc29)
161TB6cG is judged by the evaluator to be sufficient to distinguish between E1
161TB7cG and M1+E2 transitions, but not between M1 and E2 transitions.
161TB cG MR From |g|g(|q) results of 1974OkZW.
161TB cG E(M) Authors (1975Ga16) indicate |g is doubtful even though it is
161TB2cG placed in scheme and intensity is >0.
161TB cG RI(H) This I|g and the |a result in an intensity for the |b{+-}
161TB2cG feeding of the 56-keV level of -7% {I12}. If the theoretical |a for an
161TB3cG M1 |g is used, this computed I|b{+-} becomes -23%. To obtain an
161TB4cG intensity balance, I|g would need to increase by about 10%.
161TB cL Decay scheme is primarily that of 1975Ga16, which is the only
161TB2cL report of levels above 750 keV. Below 750 keV, similar schemes are
161TB3cL given by 1976Hn01, 1974OkZW, 1966Zy02, and 1966FuZZ.
161TB cL The following data have been measured: |g-ray energies and
161TB2cL intensities (1975Ga16, also 1976Hn01,1966Zy02,1966FuZZ), level
161TB3cL half-lives (1964Lo09,1965Ma24,1967Ma33,1969Be54), |g|g coincidences
161TB4cL (1966Zy02,1969Be54,1974OkZW,1975Ga16,1976Hn01), and multipolarities
161TB5cL from ce data (1959Sc29,1976Hn01) and from |g|g(|q) data (1974OkZW).
161TB cL The |g|g-coincidence data on the drawing are from 1976Hn01.
161TB cL E From least-squares fit to |g energies.
161TB cL J The J{+|p} and band assignments are from {+161}Tb
161TB2cL Adopted Levels. They agree with those from the {+161}Gd |b{+-}
161TB3cL decay results of 1975Ga16 and are based on |g multipolarities
161TB4cL and expected band structure. Other J{+|p} and band assignments from
161TB5cL 1975Ga16 which are not adopted are given in comments.
161TB cL T From {+161}Tb Adopted Levels. All data are from this decay.
161TB DL Levels are 3/2(0), 5/2(56), 7/2(133), and 9/2(230).
161TB DL Levels are 5/2(314) and 7/2(394).
161TB DL Levels are 7/2(417) and 9/2(488).
161TB DL Levels are 5/2(480), 7/2(585), and 9/2(707).
161TB DL Level is 5/2(1252).
161TB cL BAND(A) 3/2[411] band
161TB cL BAND(B) 5/2[413] band
161TB cL BAND(C) 7/2[523] band
161TB cL BAND(D) 5/2[532] band
161TB cL BAND(F) 5/2[402] bandhead
161GD P 0 5/2- 3.66 M 5 1955.5 14
161GD DP J From 161GD Adopted Levels.
161GD DP T From 161GD Adopted Levels.
161GD DP QP From 2009AuZZ. Value also listed by 2003Au03. From
161GD2DP E(B-)=1560 30 to 417 level, 1966Zy02 give QP=1977 30.
161TB N 0.00991 4 1.00 1.00
161TB cN NR the normalization is that of the evaluator. It assumes
161TB2cN that the total I|b{+-} is 100% and the I|b{+-} feeding of the
161TB3cN ground-state band is |<0.5%. The total ground-state feeding is not
161TB4cN used for normalization because the transition intensity of the 56 |g is
161TB5cN not well known.
161TB PN 3
161TB G 89.43 15 5. 1
161TB G 832.0 3 0.10 2
161TB G 869.3 2 0.097 15
161TB G 911.53 12 0.19 2
161TB G 928.42 14 0.13 2
161TB G 932.85 10 0.29 2
161TB G 979.37 14 0.11 1
161TB G 1012.90 10 0.30 2
161TB G 1044.30 22 0.055 10
161TB G 1057.06 10 0.36 2
161TB G 1113.49 10 0.53 8
161TB G 1117.15 14 0.12 2
161TB G 1126.3 3 0.064 15
161TB G 1160.09 12 0.158 15
161TB G 1171.4 5 0.030 12
161TB G 1186.06 18 0.073 10
161TB G 1197.07 13 0.140 15
161TB G 1238.01 18 0.073 6
161TB G 1242.0 4 0.038 7
161TB G 1258.88 13 0.126 8
161TB G 1354.9 3 0.043 7
161TB G 1357.8 3 0.045 7
161TB G 1379.74 13 0.165 12
161TB G 1433.82 16 0.085 6
161TB G 1472.4 2 0.059 6
161TB G 1590.5 5 0.024 5
161TB G 1600.55 15 0.42 3
161TB G 1738.8 3 0.033 5
161TB L 0 3/2+ 6.906 D 19 A
161TB cL J from {+161}Tb Adopted Levels; J measured.
161TB cL T from {+161}Tb Adopted Levels.
161TB L 56.289 9 5/2+ A
161TB G 56.290 12 380 16 M1 16 3 C
161TB2 G KC=13.5 30 $ LC=2.0 4 $ MC+=0.5 1
161TB3 G FLAG=H
161TB CG M from L1/M=3.0 5 (1959Sc29) and EKC=15 3 (1959Sc29) and
161TB2CG 13.5 30 (1976Hn01 who used CE data of 1959Sc29). From theory,
161TB3CG |a=11.51 and |a(K)=9.67 for M1.
161TB cG CC values deduced by evaluator who assumes |a and |a(K) are
161TB2cG both anomolous by the ratio |a(K)exp/|a(K)theory=1.40.
161TB L 133.681 11 7/2+ A
161TB G 77.393 10 107 10M1+E2 0.12 1 4.63 C
161TBS G KC=3.84 6$LC=0.611 12$MC=0.135 3$NC+=0.0360 7
161TBS G NC=0.0310 6$OC=0.00470 9$PC=0.000286 4
161TB CG M from K/L|?2.0 and EKC=5.3 (1959Sc29)
161TB CG MR The expected E2 component in this intraband cascade
161TB2CG transition was computed by the evaluator using the Alaga rules
161TB3CG (1955Al58) and the intensity of the crossover (133.68) E2 transition.
161TB G 133.68 2 16 2[E2] 0.915 C
161TBS G KC=0.516 8$LC=0.307 5$MC=0.0725 11$NC+=0.0185 3
161TBS G NC=0.01630 23$OC=0.00214 3$PC=2.68E-5 4
161TB L 230.72 7 9/2+ A
161TB G 97.04 7 12.5 20 [M1,E2] 2.7 3 & ?
161TBS G KC=1.6 4$LC=0.8 5$MC=0.19 13$NC+=0.05 3
161TBS G NC=0.04 3$OC=0.006 4$PC=0.00011 5
161TB L 314.914 11 5/2+ B
161TB B 5.0 6.19
161TBS B EAV=605.1 7
161TB G 181.232 12 75 3M1+E2 -0.87 AP 0.371 25 C
161TBS G KC AP 0.288$LC AP 0.0645$MC AP 0.01463$NC+ AP 0.00383
161TBS G NC AP 0.00334$OC AP 0.000477$PC AP 1.97E-5
161TB G 258.62 3 99 4M1+E2 -0.6 +3-2 0.140 11 C
161TBS G KC=0.115 11$LC=0.0192 4$MC=0.00425 13$NC+=0.00113 3
161TBS G NC=0.00098 3$OC=0.0001462 21$PC=8.3E-6 10
161TB cG MR from 1974OkZW; authors report only smaller of the two
161TB2CG values from the analysis based on |a(K)exp AP 0.22 (1959Sc29) which
161TB3cG implies predominately M1. M1 also deduced by 1976Hn01 from |a(K)exp
161TB4cG based on ce data of 1959Sc29, but |a(K)exp value is not reported.
161TB G 314.92 2 2290 90M1+E2 +0.29 6 0.0884 18 C
161TBS G KC=0.0745 16$LC=0.01092 16$MC=0.00239 4$NC+=0.000641 10
161TBS G NC=0.000551 8$OC=8.46E-5 13$PC=5.45E-6 13
161TB cG MR from 1974OkZW; authors report only smaller of the two
161TB2cG values from the analysis based on |a(K)exp=0.10 and K/L|>6.3
161TB3cG (1959Sc29) which imply predominately M1. E2+M1 is reported by 1976Hn01
161TB4cG from |a(K)exp based ce data of 1959Sc29 which might support larger
161TB5cG |d value, but |a(K)exp value is not reported.
161TB L 394.364 17 7/2+ B
161TB B 1.5 6.63
161TBS B EAV=571.0 7
161TB G 79.41 4 6 1[M1,E2] 5.2 10 C
161TBS G KC=2.8 9$LC=1.9 14$MC=0.5 4$NC+=0.11 9
161TBS G NC=0.10 8$OC=0.013 10$PC=0.00018 9
161TB cG E placement by 1976Hn01, unplaced by 1975Ga16.
161TB G 338.07 2 170 10M1+E2 +0.08 3 0.0755 C
161TBS G KC=0.0639 10$LC=0.00910 13$MC=0.00198 3$NC+=0.000534 8
161TBS G NC=0.000458 7$OC=7.07E-5 10$PC=4.70E-6 7
161TB G 394.34 6 22 2[E2] 0.0278 C
161TBS G KC=0.0219 3$LC=0.00456 7$MC=0.001030 15$NC+=0.000270 4
161TBS G NC=0.000235 4$OC=3.37E-5 5$PC=1.428E-6 20
161TB L 417.228 12 7/2- 0.88 NS 2 C
161TB cL T weighted average of 0.87 ns {I5} (1964Lo09), 0.84 ns {I4}
161TB2cL (1965Ma24), and 0.90 ns {I3} (1969Be54) from |b|g(t).
161TB B 1560 30 83.5 4.86
161TBS B EAV=561.2 7
161TB G 102.315 101400 80E1 0.283 C
161TBS G KC=0.237 4$LC=0.0361 5$MC=0.00786 11$NC+=0.00206 3
161TBS G NC=0.00179 3$OC=0.000259 4$PC=1.316E-5 19
161TB cG M from K/L=5.5 and |a(K)exp=0.22 (1959Sc29). E1 also deduced
161TB2cG by 1976Hn01 from |a(K)exp based on ce data of 1959Sc29, but |a(K)exp
161TB3cG value is not reported.
161TB G 283.55 3 600 25E1 0.0191 C
161TBS G KC=0.01618 23$LC=0.00227 4$MC=0.000493 7$NC+=0.0001311 19
161TBS G NC=0.0001131 16$OC=1.701E-5 24$PC=1.019E-6 15
161TB cG M from |a(K)exp=0.041 (1959Sc29). E1 also deduced
161TB2cG by 1976Hn01 from |a(K)exp based on ce data of 1959Sc29, but |a(K)exp
161TB3cG value is not reported.
161TB G 360.94 2 606E1 15E1 0.01051 C
161TBS G KC=0.00893 13$LC=0.001237 18$MC=0.000268 4$NC+=7.15E-5 10
161TBS G NC=6.16E-5 9$OC=9.33E-6 13$PC=5.73E-7 8
161TB cG M from |a(K)exp=0.018 (1959Sc29). E1 also deduced
161TB2cG by 1976Hn01 from |a(K)exp based on ce data of 1959Sc29, but |a(K)exp
161TB3cG value is not reported.
161TB G 417.0 4 31 4[M2] 0.1524
161TBS G KC=0.1254 18$LC=0.0211 3$MC=0.00470 7$NC+=0.001265 19
161TBS G NC=0.001088 16$OC=0.0001664 24$PC=1.053E-5 16
161TB L 480.130 12 5/2- 0.1 NS LT D
161TB cL T from 1967Ma33 from |be{+-}(t). Other: <0.2 ns (1965Ma24)
161TB2cL from |b|g(t).
161TB B 4.4 6.07
161TBS B EAV=534.4 7
161TB G 62.910 25 6 2 [M1,E2] 12 4
161TBS G KC=4.9 22$LC=5 5$MC=1.3 11$NC+=0.3 3
161TBS G NC=0.29 24$OC=0.04 3$PC=0.00034 19
161TB G 85.79 7 15 3[E1] 0.453 C
161TBS G KC=0.377 6$LC=0.0591 9$MC=0.01289 19$NC+=0.00336 5
161TBS G NC=0.00292 5$OC=0.000418 6$PC=2.05E-5 3
161TB G 165.213 15 260 20E1 0.0780 C
161TBS G KC=0.0658 10$LC=0.00957 14$MC=0.00208 3$NC+=0.000549 8
161TBS G NC=0.000475 7$OC=7.03E-5 10$PC=3.91E-6 6
161TB cG M from |a(K)exp=0.10 (1959Sc29). E1 also deduced
161TB2cG by 1976Hn01 from |a(K)exp based on ce data of 1959Sc29, but |a(K)exp
161TB3cG value is not reported.
161TB G 423.86 7 18 3[E1] 0.00718 C
161TBS G KC=0.00611 9$LC=0.000839 12$MC=0.000182 3$NC+=4.85E-5 7
161TBS G NC=4.18E-5 6$OC=6.35E-6 9$PC=3.96E-7 6
161TB G 480.12 2 270 15[E1] 0.00539 C
161TBS G KC=0.00459 7$LC=0.000627 9$MC=0.0001357 19$NC+=3.63E-5 5
161TBS G NC=3.12E-5 5$OC=4.75E-6 7$PC=3.00E-7 5
161TB L 488.78 3 9/2- C
161TB G 71.57 3 6 2[M1,E2] 7.6 18
161TBS G KC=3.6 13$LC=3.0 24$MC=0.7 6$NC+=0.18 15
161TBS G NC=0.16 13$OC=0.021 16$PC=0.00024 12
161TB L 585.776 15 7/2- 0.2 NS LT D
161TB cL T from 1965Ma24 from |b|g(t).
161TB B 5.7 5.83
161TBS B EAV=489.9 7
161TB cB IB value assumes that one-half of the intensity of the 97-keV |g
161TB2cB depopulates this level.
161TB G 97.04 7 12.5 20 [M1,E2] 2.7 3 &
161TBS G KC=1.6 4$LC=0.8 5$MC=0.19 13$NC+=0.05 3
161TBS G NC=0.04 3$OC=0.006 4$PC=0.00011 5
161TB G 105.64 2 74 10[M1,E2] 2.00 13 C
161TBS G KC=1.3 3$LC=0.6 4$MC=0.13 8$NC+=0.033 20
161TBS G NC=0.029 18$OC=0.0039 22$PC=8.E-5 4
161TB G 168.47 7 8.2 12 [M1,E2] 0.46 5
161TBS G KC=0.34 8$LC=0.09 3$MC=0.020 7$NC+=0.0052 16
161TBS G NC=0.0045 15$OC=0.00064 17$PC=2.3E-5 9
161TB G 191.38 3 64 3[E1] 0.0528 C
161TBS G KC=0.0446 7$LC=0.00641 9$MC=0.001394 20$NC+=0.000369 6
161TBS G NC=0.000319 5$OC=4.74E-5 7$PC=2.70E-6 4
161TB G 270.87 5 88 4[E1] 0.0214 C
161TBS G KC=0.0182 3$LC=0.00256 4$MC=0.000555 8$NC+=0.0001475 21
161TBS G NC=0.0001272 18$OC=1.91E-5 3$PC=1.139E-6 16
161TB G 452.2 2 6 1
161TB G 529.50 2 127 7
161TB L 707.19 25 9/2- D
161TB G 121.7 3 1.0 3[M1,E2] 1.265 24
161TBS G KC=0.87 20$LC=0.31 16$MC=0.07 4$NC+=0.019 10
161TBS G NC=0.016 9$OC=0.0022 11$PC=5.7E-5 23
161TB L 1149.88 7 (3/2+)
161TB cL J authors (1975Ga16) comment that a possible assignment is
161TB2cL K{+|p}=3/2{++} |b-vibrational band based on 3/2[411] ground
161TB3cL state.
161TB DL Level is 3/2(1149).
161TB G 835.0 3 0.09 2 &
161TB G 1093.52 9 0.64 4
161TB G 1149.94 9 1.20 6
161TB L 1209.72 9
161TB CL J assigned (3/2+) by 1975Ga16, but assignment not adopted.
161TB G 1153.43 12 0.155 20
161TB G 1209.72 11 0.187 15
161TB L 1252.37 6 5/2+ F
161TB G 772.18 10 0.36 3
161TB G 835.0 3 0.09 2 ?
161TB G 857.93 11 0.21 2
161TB G 937.53 9 0.92 5
161TB G 1252.42 12 0.181 12
161TB L 1349.66 5
161TB CL J assigned J{+|p}=(5/2+) and as bandhead of 5/2{++}
161TB2cL |b-vibrational band based on 5/2[413] state at 314 keV by 1975Ga16,
161TB3cL but assignment not adopted.
161TB G 955.35 8 0.79 4
161TB G 1034.72 8 2.74 7
161TB G 1349.60 9 0.51 3
161TB L 1404.68 12
161TB CL J assigned (5/2+) by 1975GA16, but assignment not adopted.
161TB G 818.9 3 0.07 2 M
161TB G 924.55 12 0.19 2
161TB L 1420.62 7
161TB CL J assigned J{+|p}=(7/2+) and as member of 5/2{++}
161TB2cL |b-vibrational band based on 5/2[413] state at 314 keV by 1975Ga16,
161TB3cL but assignment not adopted.
161TB G 835.0 3 0.09 2 & ?
161TB G 1026.25 10 0.28 2
161TB G 1105.84 13 0.133 12
161TB G 1364.19 13 0.119 13
161TB L 1460.54 10
161TB CL J assigned (7/2) by 1975Ga16, but assignment not adopted.
161TB G 972.3 8 0.024 8 M
161TB G 1066.22 12 0.145 15
161TB G 1145.50 18 0.09 2
161TB L 1477.63 11
161TB CL J assigned J{+|p}=(3/2-) and as bandhead of 3/2{+-}[541], but
161TB2cL assignment not adopted.
161TB G 1344.2 4 0.033 7 M
161TB G 1421.37 15 0.089 7
161TB G 1477.55 15 0.136 10 &
161TB L 1533.80 9
161TB CL J assigned J{+|p}=(5/2) and as member of 3/2{+-}[541] band,
161TB2cL but assignment not adopted.
161TB G 947.75 24 0.053 6
161TB G 1053.7 3 0.045 10 M
161TB G 1400.13 12 0.175 12
161TB G 1477.55 15 0.136 10 & ?
161TB G 1533.87 15 0.138 10
161TB L 1537.43 8
161TB G 951.10 22 0.055 6
161TB G 1048.75 12 0.19 2
161TB G 1143.15 12 0.20 2
161TB G 1480.9 3 0.040 5
161TB L 1552.17 12
161TB CL J assigned (7/2) by 1975Ga16, but assignment not adopted.
161TB G 1063.4 2 0.073 12
161TB G 1135.2 4 0.038 8
161TB G 1495.82 16 0.082 7 &
161TB L 1558.18 11
161TB CL J assigned (5/2) by 1975Ga16, but assignment not adopted.
161TB G 1424.3 2 0.066 5
161TB G 1501.8 2 0.058 5
161TB G 1558.33 15 0.099 8
161TB L 1601.02 7
161TB CL J assigned J{+|p}=(7/2-) and as member of 3/2{+-}[541] band,
161TB2cL but assignment not adopted.
161TB G 1015.10 14 0.12 2
161TB G 1112.20 15 0.18 5
161TB G 1120.92 10 0.42 3
161TB G 1286.4 4 0.039 7
161TB G 1544.80 14 0.116 8
161TB L 1623.11 7
161TB CL J assigned (5/2) by 1975Ga16, but assignment not adopted.
161TB G 1228.72 14 0.109 10
161TB G 1308.27 10 0.296 20
161TB G 1489.42 15 0.140 10
161TB G 1567.0 6 0.012 3 M
161TB G 1622.95 15 0.212 15 &
161TB L 1655.81 7
161TB CL J assigned (7/2) by 1975Ga16, but assignment not adopted.
161TB G 1175.82 11 0.20 2
161TB G 1261.11 11 0.195 10
161TB G 1341.10 12 0.166 15
161TB L 1778.19 12
161TB CL J assigned (7/2-) by 1975Ga16, but assignment not adopted.
161TB G 1071.5 4 0.035 6 M
161TB G 1192.42 15 0.103 15
161TB G 1297.9 2 0.073 12
161TB G 1547.5 5 0.024 6 M
161TB L 1810.75 12
161TB G 1224.93 20 0.056 10
161TB G 1495.82 16 0.082 7 &
161TB G 1677.3 4 0.028 5
161TB L 1825.2 3
161TB G 1430.7 6 0.012 4 M
161TB G 1691.7 4 0.029 5
161TB G 1768.6 5 0.022 4 M
161TB L 1853.6 3
161TB CL J assigned (7/2-) by 1975Ga16, but assignment not adopted.
161TB G 1373.2 5 0.027 6 M
161TB G 1459.5 5 0.027 5 M
161TB G 1538.7 5 0.024 6
161TB G 1622.95 15 0.212 15 &
161TB L 1856.95 22
161TB G 1271.8 5 0.019 5 M
161TB G 1376.7 3 0.041 6
161TB G 1439.5 4 0.035 5