ADOPTED LEVELS, GAMMAS for 156Tb
Author: C. W. Reich | Citation: Nucl. Data Sheets 113, 2537 (2012) | Cutoff date: 1-Mar-2012
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=438 keV 4 | S(n)= 6912 keV 10 | S(p)= 5310 keV 4 | Q(α)= 373 keV 4 | ||
S(2n)= 1.608×104 keV 10 | S(2p)= 12931 keV 4 | Q(EC)= 2444 keV 4 | |||
Reference: 2017WA10 |
References: | |||
A | 150Nd(11B,5nγ),124Sn(36S,p3nγ) | B | 155Gd(3He,d),(α,t) |
C | 156Tb IT decay (5.3 H) | D | 156Tb IT decay (24.4 H) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCD | 3- | 5.35 d 10 % ε = 100 | |||||
49.630 10 | A D | 4+ | 49 ns 7 | 49.630 10 | 100 | E1 | 0.0 | 3- |
49.630+X | D | (7-) | 24.4 h 10 % IT = 100 | |||||
87 | B | 4- | ||||||
88.4 | C | (0+) | 5.3 h 2 % ε > 0 % IT < 100 | 88.4 | 100 | E3 | 0.0 | 3- |
100 | B | 1- | ||||||
109.7 | A | 5+ | 59.97 | 100 | D | 49.630 | 4+ | |
156 | B | 2- | ||||||
183.5 | A | 6+ | 73.95 133.94 | 100 31 | D | 109.7 49.630 | 5+ 4+ | |
188 | B | 3- | ||||||
222 | B | |||||||
245 | B | |||||||
281.9 | A | 7+ | 98.50 172.10 | 100 ≤96 | D | 183.5 109.7 | 6+ 5+ | |
290 | B | 4- | ||||||
313 | B | |||||||
378.9 | AB | 6(-) | 269.26 | 100 | D | 109.7 | 5+ | |
393.6 | A | 8+ | 111.62 210.14 | 100 90 | D Q | 281.9 183.5 | 7+ 6+ | |
405 | B | |||||||
442.0 | A | 7(-) | 63.0 258.48 | 79 100 | D D | 378.9 183.5 | 6(-) 6+ | |
483 | B | |||||||
530.6 | A | 9+ | 137.02 248.6 | 94 100 | D Q | 393.6 281.9 | 8+ 7+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
546.6 | A | 8(-) | 104.61 | 100 | D | 442.0 | 7(-) | |
550 | B | |||||||
590 | B | |||||||
615 | B | |||||||
638 | B | |||||||
646.8 | A | 9(-) | 100.21 204.80 | 100 40 | D Q | 546.6 442.0 | 8(-) 7(-) | |
686.2 | A | 10+ | 155.64 292.74 | 81 100 | D Q | 530.6 393.6 | 9+ 8+ | |
695 | B | |||||||
754 | B | |||||||
790 | B | |||||||
800.0 | A | 10(-) | 153.22 253.51 | 100 60 | D Q | 646.8 546.6 | 9(-) 8(-) | |
858.2 | A | 11+ | 172.10 327.39 | ≤91 100 | Q | 686.2 530.6 | 10+ 9+ | |
954.5 | A | 11(-) | 154.40 307.65 | 100 100 | D Q | 800.0 646.8 | 10(-) 9(-) | |
1060.4 | A | 12+ | 202.27 374.2 | 55 100 | Q | 858.2 686.2 | 11+ 10+ | |
1146.9 | A | 12(-) | 192.50 347.06 | 71 100 | D | 954.5 800.0 | 11(-) 10(-) | |
1263.3 | A | 13+ | 203.00 405.1 | 35 100 | Q | 1060.4 858.2 | 12+ 11+ | |
1366.8 | A | 13(-) | 219.88 412.1 | 37 100 | D Q | 1146.9 954.5 | 12(-) 11(-) | |
1510.6 | A | 14+ | 247.3 450.3 | 22 100 | Q | 1263.3 1060.4 | 13+ 12+ | |
1584.3 | A | 14(-) | 217.46 437.5 | 26 100 | D | 1366.8 1146.9 | 13(-) 12(-) | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1741.4 | A | 15+ | 230.8 478.0 | 25 100 | Q | 1510.6 1263.3 | 14+ 13+ | |
1873.9 | A | 15(-) | 289.74 507.0 | 23 100 | D Q | 1584.3 1366.8 | 14(-) 13(-) | |
2029.6 | A | 16+ | ≈288 519.0 | 8 <100 | 1741.4 1510.6 | 15+ 14+ | ||
2103.2 | A | 16(-) | 229.15 519.0 | ≤83 <100 | D | 1873.9 1584.3 | 15(-) 14(-) | |
2285.9 | A | 17+ | 256 544.7 | 32 100 | Q | 2029.6 1741.4 | 16+ 15+ | |
2461.5 | A | 17(-) | 358.4 587.6 | 54 100 | Q | 2103.2 1873.9 | 16(-) 15(-) | |
2609.9 | A | 18+ | 580.3 | 100 | Q | 2029.6 | 16+ | |
2694.2 | A | 18(-) | 232.6 591.0 | ≥15 100 | D Q | 2461.5 2103.2 | 17(-) 16(-) | |
2890.5 | A | 19+ | 604.6 | 100 | 2285.9 | 17+ | ||
3114.5 | A | 19(-) | 420.2 653.1 | 30 100 | 2694.2 2461.5 | 18(-) 17(-) | ||
3243.7 | A | 20+ | 633.8 | 100 | Q | 2609.9 | 18+ | |
3345.7 | A | 20(-) | 651.5 | 100 | 2694.2 | 18(-) | ||
3548.4 | A | 21+ | 657.9 | 100 | 2890.5 | 19+ | ||
3815 | A | 21(-) | 700 | 100 | 3114.5 | 19(-) | ||
4049 | A | 22(-) | 703 | 100 | 3345.7 | 20(-) | ||
4255? | A | (23+) | 707? | 100 | 3548.4 | 21+ | ||
4556 | A | 23(-) | 741 | 100 | 3815 | 21(-) | ||
4794 | A | 24(-) | 745 | 100 | 4049 | 22(-) | ||
5579 | A | (26-) | 785 | 100 | 4794 | 24(-) | ||
6407 | A | (28-) | 828 | 100 | 5579 | (26-) | ||
7280 | A | (30-) | 873 | 100 | 6407 | (28-) | ||
8198 | A | (32-) | 918 | 100 | 7280 | (30-) | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
9159 | A | (34-) | 961 | 100 | 8198 | (32-) | ||
10160 | A | (36-) | 1001 | 100 | 9159 | (34-) | ||
11204 | A | (38-) | 1044 | 100 | 10160 | (36-) | ||
12293 | A | (40-) | 1089 | 100 | 11204 | (38-) | ||
13435 | A | (42-) | 1142 | 100 | 12293 | (40-) | ||
14638 | A | (44-) | 1203 | 100 | 13435 | (42-) | ||
15907 | A | (46-) | 1269 | 100 | 14638 | (44-) |
E(level): From unweighted least-squares fit to γ energies.
Jπ(level): Specific arguments are given for the levels below 300 keV. Above this energy, the assignments are entirely from the heavy-ion data set. These depend on the γ multipolarities and the band-structure considerations customarily employed in such studies.
M(γ): Specific multipolarities are from ce studies of the isomeric decays (1970To11,1957Mi67,1957Mi01) and d or Q assignments are from γ(θ) in the heavy-ion study, as interpreted by the evaluator.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - Kπ=3- Band, conf=π3/2[411]+ν3/2[521]. | |||||||
0.0 | 3- | 5.35 d 10 % ε = 100 | |||||
87 | 4- | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower | |||||||
49.630 10 | 4+ | 49 ns 7 | |||||
183.5 | 6+ | 73.95 133.94 | 100 31 | D | 109.7 49.630 | 5+ 4+ | |
393.6 | 8+ | ||||||
686.2 | 10+ | ||||||
1060.4 | 12+ | 202.27 374.2 | 55 100 | Q | 858.2 686.2 | 11+ 10+ | |
1510.6 | 14+ | ||||||
2029.6 | 16+ | ≈288 519.0 | 8 <100 | 1741.4 1510.6 | 15+ 14+ | ||
2609.9 | 18+ | ||||||
3243.7 | 20+ | 633.8 | 100 | Q | 2609.9 | 18+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower | |||||||
109.7 | 5+ | ||||||
281.9 | 7+ | 98.50 172.10 | 100 ≤96 | D | 183.5 109.7 | 6+ 5+ | |
530.6 | 9+ | ||||||
858.2 | 11+ | ||||||
1263.3 | 13+ | 203.00 405.1 | 35 100 | Q | 1060.4 858.2 | 12+ 11+ | |
1741.4 | 15+ | ||||||
2285.9 | 17+ | 256 544.7 | 32 100 | Q | 2029.6 1741.4 | 16+ 15+ | |
2890.5 | 19+ | ||||||
3548.4 | 21+ | 657.9 | 100 | 2890.5 | 19+ | ||
4255 | (23+) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - Probable (νi13/2)(πh11/2) band, α=0. At the lower | |||||||
378.9 | 6(-) | ||||||
546.6 | 8(-) | 104.61 | 100 | D | 442.0 | 7(-) | |
800.0 | 10(-) | ||||||
1146.9 | 12(-) | ||||||
1584.3 | 14(-) | 217.46 437.5 | 26 100 | D | 1366.8 1146.9 | 13(-) 12(-) | |
2103.2 | 16(-) | ||||||
2694.2 | 18(-) | 232.6 591.0 | ≥15 100 | D Q | 2461.5 2103.2 | 17(-) 16(-) | |
3345.7 | 20(-) | ||||||
4049 | 22(-) | 703 | 100 | 3345.7 | 20(-) | ||
4794 | 24(-) | ||||||
5579 | (26-) | ||||||
6407 | (28-) | ||||||
7280 | (30-) | 873 | 100 | 6407 | (28-) | ||
8198 | (32-) | ||||||
9159 | (34-) | ||||||
10160 | (36-) | 1001 | 100 | 9159 | (34-) | ||
11204 | (38-) | 1044 | 100 | 10160 | (36-) | ||
12293 | (40-) | ||||||
13435 | (42-) | 1142 | 100 | 12293 | (40-) | ||
14638 | (44-) | ||||||
15907 | (46-) | 1269 | 100 | 14638 | (44-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 5 - Probable (νi13/2)(πh11/2) band, α=1. At the lower | |||||||
442.0 | 7(-) | ||||||
646.8 | 9(-) | 100.21 204.80 | 100 40 | D Q | 546.6 442.0 | 8(-) 7(-) | |
954.5 | 11(-) | ||||||
1366.8 | 13(-) | ||||||
1873.9 | 15(-) | 289.74 507.0 | 23 100 | D Q | 1584.3 1366.8 | 14(-) 13(-) | |
2461.5 | 17(-) | ||||||
3114.5 | 19(-) | 420.2 653.1 | 30 100 | 2694.2 2461.5 | 18(-) 17(-) | ||
3815 | 21(-) | ||||||
4556 | 23(-) | 741 | 100 | 3815 | 21(-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 6 - Kπ=7- Bandhead, conf=π3/2[411]+ν11/2[505]. | |||||||
49.630+X | (7-) | 24.4 h 10 % IT = 100 | |||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 7 - Kπ=0+ Bandhead, conf=π3/2[411]-ν3/2[402]. | |||||||
88.4 | (0+) | 5.3 h 2 % ε > 0 % IT < 100 | |||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 8 - Kπ=0- Band, conf=π3/2[411]-ν3/2[521]. | |||||||
100 | 1- | ||||||
156 | 2- | ||||||
188 | 3- | ||||||
290 | 4- |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Conversion Coefficient | Additional Data |
49.630 | 4+ | 49 ns 7 | 49.630 10 | E1 | 0.357 | B(E1)(W.u.)=2.9E-5 4, α=0.357 |
88.4 | (0+) | 5.3 h 2 % ε > 0 % IT < 100 | 88.4 | E3 | 86.2 | α=86.2 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 3- | 5.35 d 10 % ε = 100 | Q=+2.3 8, μ=1.41 18 E(level): Kπ=3- Band, conf=π3/2[411]+ν3/2[521]. |
49.630 | 4+ | 49 ns 7 | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower. |
49.630+X | (7-) | 24.4 h 10 % IT = 100 | E(level): Kπ=7- Bandhead, conf=π3/2[411]+ν11/2[505]. |
87 | 4- | E(level): Kπ=3- Band, conf=π3/2[411]+ν3/2[521]. Jπ(level): From comparison of the measured (3He,d) and (α,t) cross sections with those predicted for the members of the band having the proposed configuration, together with the expected energy spacings (1974ElZW). | |
88.4 | (0+) | 5.3 h 2 % ε > 0 % IT < 100 | E(level): Kπ=0+ Bandhead, conf=π3/2[411]-ν3/2[402]. |
100 | 1- | E(level): Kπ=0- Band, conf=π3/2[411]-ν3/2[521]. Jπ(level): From comparison of the measured (3He,d) and (α,t) cross sections with those predicted for the members of the band having the proposed configuration, together with the expected energy spacings (1974ElZW). | |
109.7 | 5+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
156 | 2- | E(level): Kπ=0- Band, conf=π3/2[411]-ν3/2[521]. Jπ(level): From comparison of the measured (3He,d) and (α,t) cross sections with those predicted for the members of the band having the proposed configuration, together with the expected energy spacings (1974ElZW). | |
183.5 | 6+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower. | |
188 | 3- | E(level): Kπ=0- Band, conf=π3/2[411]-ν3/2[521]. Jπ(level): From comparison of the measured (3He,d) and (α,t) cross sections with those predicted for the members of the band having the proposed configuration, together with the expected energy spacings (1974ElZW). | |
281.9 | 7+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
290 | 4- | E(level): Kπ=0- Band, conf=π3/2[411]-ν3/2[521]. Jπ(level): From comparison of the measured (3He,d) and (α,t) cross sections with those predicted for the members of the band having the proposed configuration, together with the expected energy spacings (1974ElZW). | |
378.9 | 6(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
393.6 | 8+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower. | |
442.0 | 7(-) | E(level): Probable (νi13/2)(πh11/2) band, α=1. At the lower. | |
530.6 | 9+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
546.6 | 8(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
646.8 | 9(-) | E(level): Probable (νi13/2)(πh11/2) band, α=1. At the lower. | |
686.2 | 10+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower. | |
800.0 | 10(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
858.2 | 11+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
954.5 | 11(-) | E(level): Probable (νi13/2)(πh11/2) band, α=1. At the lower. | |
1060.4 | 12+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower. | |
1146.9 | 12(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
1263.3 | 13+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
1366.8 | 13(-) | E(level): Probable (νi13/2)(πh11/2) band, α=1. At the lower. | |
1510.6 | 14+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower. | |
1584.3 | 14(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
1741.4 | 15+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
1873.9 | 15(-) | E(level): Probable (νi13/2)(πh11/2) band, α=1. At the lower. | |
2029.6 | 16+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower. | |
2103.2 | 16(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
2285.9 | 17+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
2461.5 | 17(-) | E(level): Probable (νi13/2)(πh11/2) band, α=1. At the lower. | |
2609.9 | 18+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower. | |
2694.2 | 18(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
2890.5 | 19+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
3114.5 | 19(-) | E(level): Probable (νi13/2)(πh11/2) band, α=1. At the lower. | |
3243.7 | 20+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=0. At the lower. | |
3345.7 | 20(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
3548.4 | 21+ | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
3815 | 21(-) | E(level): Probable (νi13/2)(πh11/2) band, α=1. At the lower. | |
4049 | 22(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
4255 | (23+) | E(level): Kπ=4+ Band, (π3/2[411])(νi13/2), α=1. At the lower. | |
4556 | 23(-) | E(level): Probable (νi13/2)(πh11/2) band, α=1. At the lower. | |
4794 | 24(-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
5579 | (26-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
6407 | (28-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
7280 | (30-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
8198 | (32-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
9159 | (34-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
10160 | (36-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
11204 | (38-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
12293 | (40-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
13435 | (42-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
14638 | (44-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. | |
15907 | (46-) | E(level): Probable (νi13/2)(πh11/2) band, α=0. At the lower. |
E(level) | E(gamma) | Comments |
49.630 | 49.630 | M(γ): From L-subshell ratios in 156Tb IT decay (24.4 h). |
88.4 | 88.4 | M(γ): Assignment based on K/L2/L3/M/n data from 156Tb IT decay (5.3 h). |
281.9 | 172.10 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
858.2 | 172.10 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
2029.6 | 519.0 | E(γ): Multiply placed |
2103.2 | 519.0 | E(γ): Multiply placed |
Data are from 24H and 5H IT decays (1970To11, 1957Mi01, and 1955Ha52) for three levels below 100 keV; from single-particle transfer (1974ElZW) for five levels below 300 keV; and from the 150Nd(11B,5nγ) reaction (1982Be46).
Other studies of possible interest:
Coulomb displacement energies for 156Gd - 156Tb: 1983Ja03
Model calculations of μ and Q: 1978Ko15
α survey of the features of the nuclear structure of the low-lying states of the odd-odd deformed nuclides is given by 1998Ja07.
α survey of the properties of K=0 bands in strongly deformed nuclides is given by 1988Fr16.
Numerous discussions of signature inversion in the (νi13/2)(πh11/2) band in 156Tb as well as in a number of other odd-odd nuclides have been published. See, e.g., 1992Ja03, 1994Yo02, 1994Yo03, 1995Li40, 1996Go19, 1997Zh13, 2001Zh16, 2001Ri19, 2003Ya19.
Gammas: Unplaced γ’s are not included here; see the heavy-ion-induced reaction data set.