ADOPTED LEVELS, GAMMAS for 161Tb
Author: C. W. Reich | Citation: Nucl. Data Sheets 112,2497 (2011) | Cutoff date: 1-Jun-2011
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=593.7 keV 14 | S(n)= 7696.6 keV 6 | S(p)= 6808.9 keV 11 | Q(α)= -427 keV 5 | ||
Reference: 2012WA38 |
References: | |||
A | 160Gd(p,p) IAR | B | 161Gd β- decay |
C | 160Gd(3He,d),160Gd(α,t) | D | 162Dy(t,α) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | BCD | 3/2+ | 6.89 d 2 % β- = 100 | |||||
56.289 9 | BCD | 5/2+ | 56.290 12 | 100 | M1 | 0.0 | 3/2+ | |
133.681 11 | BCD | 7/2+ | 77.393 10 133.68 2 | 100 9 15 2 | M1+E2 | 56.289 0.0 | 5/2+ 3/2+ | |
230.72 7 | BCD | 9/2+ | 97.04 7 | 100 | 133.681 | 7/2+ | ||
314.914 11 | BCD | 5/2+ | 181.232 12 258.62 3 314.92 2 | 3.3 1 4.3 2 100 4 | M1+E2 M1+E2 M1+E2 | 133.681 56.289 0.0 | 7/2+ 5/2+ 3/2+ | |
394.364 17 | BCD | 7/2+ | 79.41 4 338.07 2 394.34 6 | 3.5 6 100 6 13 1 | M1+E2 | 314.914 56.289 0.0 | 5/2+ 5/2+ 3/2+ | |
417.228 13 | BCD | 7/2- | 0.88 ns 2 | 102.315 10 283.55 3 360.94 2 417.0 4 | 23.1 13 9.9 4 100 2 0.51 7 | E1 E1 E1 [M2] | 314.914 133.681 56.289 0.0 | 5/2+ 7/2+ 5/2+ 3/2+ |
480.130 12 | B D | 5/2- | < 0.1 ns | 62.910 25 85.79 7 165.213 15 423.86 7 480.12 2 | 2.2 7 5.6 11 96 7 6.7 11 100 6 | [M1+E2] [E1] E1 [E1] [E1] | 417.228 394.364 314.914 56.289 0.0 | 7/2- 7/2+ 5/2+ 5/2+ 3/2+ |
488.78 3 | BCD | 9/2- | 71.57 3 | 100 | 417.228 | 7/2- | ||
499 | CD | 9/2+ | ||||||
520 3 | CD | 1/2+ | ||||||
558 3 | CD | 3/2+ | ||||||
584 3 | CD | 11/2- | ||||||
585.776 15 | B D | 7/2- | < 0.2 ns | 97.04 7 105.64 2 168.47 7 191.38 3 270.87 5 452.2 2 529.50 2 | ≤11.4 58 8 6.5 9 50.4 24 69 3 4.7 8 100 6 | 488.78 480.130 417.228 394.364 314.914 133.681 56.289 | 9/2- 5/2- 7/2- 7/2+ 5/2+ 7/2+ 5/2+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
602 3 | CD | 5/2+ | ||||||
638 4 | C | |||||||
698 3 | CD | 7/2+ | ||||||
707.19 25 | B D | 9/2- | 121.7 3 | 100 | 585.776 | 7/2- | ||
743 3 | C | |||||||
772 5 | C | |||||||
847 3 | CD | 11/2- | ||||||
920 3 | CD | 1/2- | ||||||
950 3 | CD | 5/2- | ||||||
980 | D | 1/2+ | ||||||
997 3 | CD | |||||||
1020 3 | C | 3/2- | ||||||
1064 3 | C | 9/2- | ||||||
1080 3 | CD | (5/2+) | ||||||
1111 3 | CD | |||||||
1130 3 | CD | |||||||
1141 4 | C | |||||||
1149.88 7 | B | (3/2+) | 835.0 3 1093.52 9 1149.94 9 | ≤9.2 53 3 100 5 | 314.914 56.289 0.0 | 5/2+ 5/2+ 3/2+ | ||
1178 3 | CD | 7/2- | ||||||
1209.72 9 | BCD | 1153.43 12 1209.72 11 | 83 11 100 8 | 56.289 0.0 | 5/2+ 3/2+ | |||
1232 3 | CD | |||||||
1252.37 6 | BCD | 5/2+ | 772.18 10 835.0 3 ? 857.93 11 937.53 9 1252.42 12 | 39 3 ≤12 22.8 22 100 5 19.7 13 | 480.130 417.228 394.364 314.914 0.0 | 5/2- 7/2- 7/2+ 5/2+ 3/2+ | ||
1281 2 | D | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1302 3 | C | |||||||
1333 | D | |||||||
1349.66 5 | BCD | 955.35 8 1034.72 8 1349.60 9 | 28.8 15 100 3 18.6 11 | 394.364 314.914 0.0 | 7/2+ 5/2+ 3/2+ | |||
1386 3 | CD | |||||||
1404.68 12 | BC | 818.9 3 924.55 12 | <47 100 11 | 585.776 480.130 | 7/2- 5/2- | |||
1420.62 7 | BC | 835.0 3 ? 1026.25 10 1105.84 13 1364.19 13 | 32 7 100 7 48 4 42 5 | 585.776 394.364 314.914 56.289 | 7/2- 7/2+ 5/2+ 5/2+ | |||
1433 3 | C | |||||||
1436 2 | D | |||||||
1460.54 10 | B | 972.3 8 1066.22 12 1145.50 18 | <22 100 10 62 14 | 488.78 394.364 314.914 | 9/2- 7/2+ 5/2+ | |||
1477.63 11 | B | 1344.2 4 1421.37 15 1477.55 15 | <45 100 8 <164 | 133.681 56.289 0.0 | 7/2+ 5/2+ 3/2+ | |||
1498 3 | C | |||||||
1524 | D | |||||||
1533.80 9 | BC | 947.75 24 1053.7 3 1400.13 12 1477.55 15 1533.87 15 | 30 3 <31 100 7 <83 79 6 | 585.776 480.130 133.681 56.289 0.0 | 7/2- 5/2- 7/2+ 5/2+ 3/2+ | |||
1537.43 8 | B | 951.10 22 1048.75 12 1143.15 12 1480.9 3 | 28 3 95 10 100 10 20.0 25 | 585.776 488.78 394.364 56.289 | 7/2- 9/2- 7/2+ 5/2+ | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1552.17 12 | B D | 1063.4 2 1135.2 4 1495.82 16 | 100 16 52 11 <122 | 488.78 417.228 56.289 | 9/2- 7/2- 5/2+ | |||
1558.18 11 | BC | 1424.3 2 1501.8 2 1558.33 15 | 67 5 59 5 100 8 | 133.681 56.289 0.0 | 7/2+ 5/2+ 3/2+ | |||
1601.02 7 | BC | 1015.10 14 1112.20 15 1120.92 10 1286.4 4 1544.80 14 | 29 5 43 12 100 7 9.3 17 27.6 19 | 585.776 488.78 480.130 314.914 56.289 | 7/2- 9/2- 5/2- 5/2+ 5/2+ | |||
1623.11 7 | B | 1228.72 14 1308.27 10 1489.42 15 1567.0 6 1622.95 15 | 37 3 100 7 47 3 <5.1 <77 | 394.364 314.914 133.681 56.289 0.0 | 7/2+ 5/2+ 7/2+ 5/2+ 3/2+ | |||
1655.81 7 | B D | 1175.82 11 1261.11 11 1341.10 12 | 100 10 98 5 83 8 | 480.130 394.364 314.914 | 5/2- 7/2+ 5/2+ | |||
1680 3 | C | |||||||
1718 8 | C | |||||||
1756 3 | C | |||||||
1778.19 12 | BC | 1071.5 4 1192.42 15 1297.9 2 1547.5 5 | <40 100 15 71 12 <29 | 707.19 585.776 480.130 230.72 | 9/2- 7/2- 5/2- 9/2+ | |||
1810.75 12 | BC | 1224.93 20 1495.82 16 1677.3 4 | 100 18 <159 50 9 | 585.776 314.914 133.681 | 7/2- 5/2+ 7/2+ | |||
1825.2 3 | B D | 1430.7 6 1691.7 4 1768.6 5 | <55 100 17 <90 | 394.364 133.681 56.289 | 7/2+ 7/2+ 5/2+ | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1845 | D | |||||||
1853.6 3 | BC | 1373.2 5 1459.5 5 1538.7 5 1622.95 15 | <137 <133 100 25 <946 | 480.130 394.364 314.914 230.72 | 5/2- 7/2+ 5/2+ 9/2+ | |||
1856.95 22 | B | 1271.8 5 1376.7 3 1439.5 4 | <58 100 15 85 12 | 585.776 480.130 417.228 | 7/2- 5/2- 7/2- | |||
1900 | D | 11/2- | ||||||
1946 | D | |||||||
1979 | D | |||||||
17040 | A | (5/2-) | ||||||
17113 | A | (7/2-) | ||||||
17353 | A | (3/2-) | ||||||
17369 | A | (1/2-) | ||||||
17478 | A | (5/2-) | ||||||
17569 | A | (7/2-) | ||||||
17874 | A | (1/2-,3/2-) | ||||||
17929 | A | (7/2-) |
E(level): From least-squares fit to γ energies for 161Gd decay and otherwise from reactions.
Jπ(level): Jπ and band assignments are from agreement of calculated cross sections for (3He,d), (α,t), and (t,α) reactions with measured cross sections and intensity patterns and level spacings within bands. Other Jπ arguments are noted explicitly.
Jπ(level): See levels from 161Gd β- decay for possible band assignment for β-vibrational bandheads at 1149 and 1349 keV and 3/2[541] band at 1477 keV.
E(γ): See 161Gd β- decay for unplaced γ’s.
M(γ): From 161Gd β- decay (1976Hn01,1959Sc29). From K| x ray/γ and L1/M ratios for 56γ (1959Sc29,1976Hn01) and α(K)exp for all other γ’s with the γ and ce data scaled to the theoretical M1 value for the 56-keV γ.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - 3/2[411] band. | |||||||
0.0 | 3/2+ | 6.89 d 2 % β- = 100 | |||||
56.289 9 | 5/2+ | 56.290 12 | 100 | M1 | 0.0 | 3/2+ | |
133.681 11 | 7/2+ | 77.393 10 133.68 2 | 100 9 15 2 | M1+E2 | 56.289 0.0 | 5/2+ 3/2+ | |
230.72 7 | 9/2+ | 97.04 7 | 100 | 133.681 | 7/2+ | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - 5/2[413] band. | |||||||
314.914 11 | 5/2+ | ||||||
394.364 17 | 7/2+ | 79.41 4 338.07 2 394.34 6 | 3.5 6 100 6 13 1 | M1+E2 | 314.914 56.289 0.0 | 5/2+ 5/2+ 3/2+ | |
499 | 9/2+ | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - 7/2[523] band. | |||||||
417.228 13 | 7/2- | 0.88 ns 2 | |||||
488.78 3 | 9/2- | 71.57 3 | 100 | 417.228 | 7/2- | ||
584 3 | 11/2- | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - 5/2[532] band. | |||||||
480.130 12 | 5/2- | < 0.1 ns | |||||
585.776 15 | 7/2- | < 0.2 ns | 97.04 7 105.64 2 168.47 7 191.38 3 270.87 5 452.2 2 529.50 2 | ≤11.4 58 8 6.5 9 50.4 24 69 3 4.7 8 100 6 | 488.78 480.130 417.228 394.364 314.914 133.681 56.289 | 9/2- 5/2- 7/2- 7/2+ 5/2+ 7/2+ 5/2+ | |
707.19 25 | 9/2- | 121.7 3 | 100 | 585.776 | 7/2- | ||
847 3 | 11/2- | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 5 - Kπ=1/2+ band. | |||||||
520 3 | 1/2+ | ||||||
558 3 | 3/2+ | ||||||
602 3 | 5/2+ | ||||||
698 3 | 7/2+ | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 6 - 1/2[541] band. | |||||||
920 3 | 1/2- | ||||||
950 3 | 5/2- | ||||||
1020 3 | 3/2- | ||||||
1064 3 | 9/2- | ||||||
1178 3 | 7/2- | ||||||
1900 | 11/2- | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 7 - 5/2[402] bandhead | |||||||
1252.37 6 | 5/2+ | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 8 - fragment of 1/2[411] | |||||||
980 | 1/2+ | ||||||
997 3 | |||||||
1080 3 | (5/2+) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 9 - 7/2[404] bandhead | |||||||
997 3 |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
56.289 | 5/2+ | 56.290 12 | M1 | 16 | α=16 3 | ||
133.681 | 7/2+ | 77.393 10 | M1+E2 | 0.12 1 | 4.63 | α=4.63 | |
7/2+ | 133.68 2 | 0.915 | α=0.915 | ||||
230.72 | 9/2+ | 97.04 7 | 2.7 | α=2.7 3 | |||
314.914 | 5/2+ | 181.232 12 | M1+E2 | -0.87 AP | 0.371 | α=0.371 25 | |
5/2+ | 258.62 3 | M1+E2 | -0.6 +3-2 | ||||
5/2+ | 314.92 2 | M1+E2 | +0.29 6 | ||||
394.364 | 7/2+ | 79.41 4 | 5.2 | α=5.2 10 | |||
7/2+ | 338.07 2 | M1+E2 | +0.08 3 | ||||
417.228 | 7/2- | 0.88 ns 2 | 102.315 10 | E1 | 0.283 | B(E1)(W.u.)=4.0E-5 3, α=0.283 | |
7/2- | 0.88 ns 2 | 283.55 3 | E1 | 0.0191 | B(E1)(W.u.)=8.0E-7 4, α=0.0191 | ||
7/2- | 0.88 ns 2 | 360.94 2 | E1 | 0.01051 | B(E1)(W.u.)=3.91E-6 14, α=0.01051 | ||
7/2- | 0.88 ns 2 | 417.0 4 | [M2] | 0.1524 | B(M2)(W.u.)=0.34 5, α=0.1524 | ||
480.130 | 5/2- | < 0.1 ns | 62.910 25 | [M1+E2] | 12 | α=12 4 | |
5/2- | < 0.1 ns | 85.79 7 | [E1] | 0.453 | B(E1)(W.u.)>8.2E-5, α=0.453 | ||
5/2- | < 0.1 ns | 165.213 15 | E1 | 0.0780 | B(E1)(W.u.)>0.00020, α=0.0780 | ||
5/2- | < 0.1 ns | 423.86 7 | [E1] | 0.00718 | B(E1)(W.u.)>8.1E-7, α=0.00718 | ||
5/2- | < 0.1 ns | 480.12 2 | [E1] | 0.00539 | B(E1)(W.u.)>8.4E-6, α=0.00539 | ||
488.78 | 9/2- | 71.57 3 | 7.6 | α=7.6 18 | |||
585.776 | 7/2- | < 0.2 ns | 97.04 7 | 2.7 | α=2.7 3 | ||
7/2- | < 0.2 ns | 105.64 2 | 2.00 | α=2.00 13 | |||
7/2- | < 0.2 ns | 168.47 7 | 0.46 | α=0.46 5 | |||
7/2- | < 0.2 ns | 191.38 3 | 0.0528 | α=0.0528 | |||
7/2- | < 0.2 ns | 270.87 5 | 0.0214 | α=0.0214 | |||
707.19 | 9/2- | 121.7 3 | 1.265 | α=1.265 24 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 3/2+ | 6.89 d 2 % β- = 100 | Q=+1.2 6, μ=2.2 1 E(level): 3/2[411] band. |
56.289 | 5/2+ | E(level): 3/2[411] band. | |
133.681 | 7/2+ | E(level): 3/2[411] band. | |
230.72 | 9/2+ | XREF: C(236)d(233). E(level): 3/2[411] band. | |
314.914 | 5/2+ | E(level): 5/2[413] band. | |
394.364 | 7/2+ | E(level): 5/2[413] band. | |
417.228 | 7/2- | 0.88 ns 2 | E(level): 7/2[523] band. |
480.130 | 5/2- | < 0.1 ns | E(level): 5/2[532] band. |
488.78 | 9/2- | E(level): 7/2[523] band. | |
499 | 9/2+ | E(level): 5/2[413] band. | |
520 | 1/2+ | E(level): Kπ=1/2+ band. | |
558 | 3/2+ | E(level): Kπ=1/2+ band. | |
584 | 11/2- | E(level): 7/2[523] band. | |
585.776 | 7/2- | < 0.2 ns | E(level): 5/2[532] band. |
602 | 5/2+ | E(level): Kπ=1/2+ band. | |
698 | 7/2+ | E(level): Kπ=1/2+ band. | |
707.19 | 9/2- | E(level): 5/2[532] band. | |
847 | 11/2- | E(level): 5/2[532] band. | |
920 | 1/2- | E(level): 1/2[541] band. | |
950 | 5/2- | E(level): 1/2[541] band. | |
980 | 1/2+ | E(level): fragment of 1/2[411]. | |
997 | E(level): fragment of 1/2[411]. 7/2[404] bandhead. | ||
1020 | 3/2- | E(level): 1/2[541] band. | |
1064 | 9/2- | E(level): 1/2[541] band. | |
1080 | (5/2+) | E(level): fragment of 1/2[411]. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
1178 | 7/2- | E(level): 1/2[541] band. | |
1252.37 | 5/2+ | E(level): 5/2[402] bandhead. | |
1778.19 | XREF: C(1782). | ||
1900 | 11/2- | E(level): 1/2[541] band. |
The data adopted here are from the 161Gd β- decay and the 160Gd(3He,d), 160Gd(α,t), and 162Dy(t,α) reactions.
For calculations of the wave functions for some of these levels, see 1972So12 or 1973Ga29 and 1970WeZS. For a discussion of the band assignments, see 1975Ni03.
The contributions of Nilsson states and vibrations to the various bandheads have been calculated by 1970WeZS, 1971SoZW, 1972So12, 1973Ga29, and 1983So01. The last four articles have some authors in common and similar results. These contributions are greater than 90% for the 3/2+[411], 5/2+[413], and 5/2-[532] bandheads. For spins of 7/2 and greater, the 7/2-[523] and 5/2-[532] bands are mixed, with the main contributions being 63% to 73% in the 7/2- levels and less at 9/2-. For the 1/2+[411] bandhead, the various calculations give a 54% to 73% contribution from the Nilsson state and 24% to 35% contribution from a vibrational state based on the 3/2+[411] ground state. For the 5/2+[402] band, the calculations give a 65% contribution from the Nilsson state and 11% and 12% from two vibrational states. 1970WeZS also give the calculated contributions for the first one or two rotational states in these bands.
Q-value: Note: Current evaluation has used the following Q record $ 593.0 13 7696.6 6 6808.6 10 -426 5 2009AuZZ
Q-value: Values are essentially the same as those of 2003Au03.