ADOPTED LEVELS, GAMMAS for 135Ba
Authors: Balraj Singh, Alexander A. Rodionov and Yuri L. Khazov | Citation: Nucl. Data Sheets 109, 517 (2008) | Cutoff date: 22-Jan-2008
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-1207 keV 10 | S(n)= 6971.97 keV 10 | S(p)= 8248.5 keV 3 | Q(α)= -1862.0 keV 4 | ||
Reference: 2012WA38 |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCDEFGHIJKL | 3/2+ | STABLE | |||||
220.968 13 | C EFGHIJKL | 1/2+ | 0.64 ns 27 | 220.94 2 | 100 | M1+E2 | 0.0 | 3/2+ |
268.218 20 | BCDEFGHI K | 11/2- | 28.7 h 2 % IT = 100 | 268.218 20 | 100 | M4 | 0.0 | 3/2+ |
480.532 14 | C EFGHIJKL | 5/2+ | 13 ps 2 | 259.58 4 480.52 2 | 0.29 2 100 | (E2) M1+E2 | 220.968 0.0 | 1/2+ 3/2+ |
587.827 15 | C EFGHIJKL | 3/2+ | 107.32 9 366.83 2 587.84 2 | 0.93 4 28.8 6 100 1 | E2(+M1) M1(+E2) M1+E2 | 480.532 220.968 0.0 | 5/2+ 1/2+ 3/2+ | |
714.20 4 | EFGHIJK | (7/2-) | 445.97 3 | 100 | 268.218 | 11/2- | ||
855.012 14 | C EFGHI KL | 3/2+ | 267.17 9 374.46 2 634.04 2 855.02 2 | 1.5 2 78 4 100 2 75 4 | M1+E2 M1(+E2) M1(+E2) | 587.827 480.532 220.968 0.0 | 3/2+ 5/2+ 1/2+ 3/2+ | |
874.518 18 | CDEFGH JKL | 7/2+ | 1.32 ps 5 | 287? 394.04 4 874.51 2 | 2.4 2 100.0 10 | [E2] [M1,E2] E2 | 587.827 480.532 0.0 | 3/2+ 5/2+ 3/2+ |
910.29 3 | C EFGHIJKL | 1/2+ | 322.3 2 689.38 19 910.28 3 | 6.0 8 38 3 100 2 | 587.827 220.968 0.0 | 3/2+ 1/2+ 3/2+ | ||
950.5 3 | D | (15/2-) | 682.3 | 100 | Q | 268.218 | 11/2- | |
979.965 18 | C EFGHIJKL | 3/2+,5/2+ | 124.89 7 392.08 9 499.36 6 758.94 9 979.98 2 | 2.9 9 3.5 9 3.5 12 14 3 100 6 | M1,E2 | 855.012 587.827 480.532 220.968 0.0 | 3/2+ 3/2+ 5/2+ 1/2+ 3/2+ | |
1008.00 10 ? | C | 420.12 10 787.9 5 1008.4 5 | 100 30 41 12 7 4 | 587.827 220.968 0.0 | 3/2+ 1/2+ 3/2+ | |||
1130? | L | 1130 | 100 | 0.0 | 3/2+ | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1165.2 22 ? | F H | |||||||
1200.48 6 ? | K | 932.25 5 | 100 | 268.218 | 11/2- | |||
1213.73 7 | EFGHIJK | (3/2) | 234.03 22 359.1 7 626.2 3 993.5 5 1213.69 7 | 5.6 14 2.1 11 10.4 21 4.9 14 100 3 | 979.965 855.012 587.827 220.968 0.0 | 3/2+,5/2+ 3/2+ 3/2+ 1/2+ 3/2+ | ||
1225.86 7 | EFGHI K | (3/2) | 245.44 6 ? 371.1 5 638.00 11 745.4 1 1005.3 4 1225.80 8 | 27.5 13 5.0 25 34 2 27 2 6.3 13 100 4 | 979.965 855.012 587.827 480.532 220.968 0.0 | 3/2+,5/2+ 3/2+ 3/2+ 5/2+ 1/2+ 3/2+ | ||
1238.41 7 | E K | (5/2) | 382.8 7 649.4 3 ? 757.98 9 1238.3 1 | 6 3 12 3 100 18 <254 | 855.012 587.827 480.532 0.0 | 3/2+ 3/2+ 5/2+ 3/2+ | ||
1298.54 10 | E K | (1/2+,3/2+) | 710.52 16 1077.30 21 1298.97 18 | 100 7 42 6 41 11 | 587.827 220.968 0.0 | 3/2+ 1/2+ 3/2+ | ||
1446.41 7 | E I K | 7/2- | 732? 965.88 7 1178.1 2 | 100 5 42 4 | 714.20 480.532 268.218 | (7/2-) 5/2+ 11/2- | ||
1557.35 5 | K | (5/2,7/2+) | 682.89 5 701.96 14 969.44 11 1077.1 4 1557.3 13 | 100 4 28 4 55 3 ≈1.3 4.7 25 | 874.518 855.012 587.827 480.532 0.0 | 7/2+ 3/2+ 3/2+ 5/2+ 3/2+ | ||
1584.52 6 | EFGHI K | (3/2)- | 1363.53 6 1583 1 | 100.0 12 <38 | 220.968 0.0 | 1/2+ 3/2+ | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1609.31 14 | E K | (1/2+,3/2+) | 1021.5 3 1128.2 5 1388.2 3 1609.7 4 | 100 7 49 10 63 13 56 11 | 587.827 480.532 220.968 0.0 | 3/2+ 5/2+ 1/2+ 3/2+ | ||
1670.67 12 | EFGH K | (3/2-) | 956.43 12 | 100 | 714.20 | (7/2-) | ||
1719.57 13 | E K | (1/2+,3/2+) | 739.3 3 864.5 4 1238.55 25 1720.0 2 | <73 100 27 <435 <270 | 979.965 855.012 480.532 0.0 | 3/2+,5/2+ 3/2+ 5/2+ 3/2+ | ||
1787.42 18 | E K | (5/2-) | 1073.22 17 | 100 | 714.20 | (7/2-) | ||
1794.4 6 | FG | (1/2,3/2) | ||||||
1830.5 4 | FGH | (1/2,3/2) | 1830.7 5 | 100 | 0.0 | 3/2+ | ||
1871.46 22 | IJK | (3/2+,5/2) | 996.6 5 1390.7 4 1871.7 3 | 37 8 45 9 100 9 | 874.518 480.532 0.0 | 7/2+ 5/2+ 3/2+ | ||
1878.9 3 | FGHI | (1/2,3/2) | 1291.3 3 | 100 | 587.827 | 3/2+ | ||
1941.17 20 | JK | (3/2+,5/2+) | 1066.7 3 1720.2 5 1941.1 3 | 100 30 <44 43 5 | 874.518 220.968 0.0 | 7/2+ 1/2+ 3/2+ | ||
1955.4 5 | D | (11/2+) | 1080.9 | 100 | 874.518 | 7/2+ | ||
1964.83 17 | E IJ | (1/2+,3/2+) | 739.4 4 1054.39 20 1090.2 5 ? 1964.9 5 | <35 100 21 60 10 73 25 | 1225.86 910.29 874.518 0.0 | (3/2) 1/2+ 7/2+ 3/2+ | ||
1971.6 3 | GHI K | (3/2,5/2) | 1491.1 4 1971.3 7 | 100 18 80 12 | 480.532 0.0 | 5/2+ 3/2+ | ||
1991.02 16 | E JK | (3/2,5/2) | 1402.8 4 1510.6 2 1990.8 6 | 99 20 100 20 76 7 | 587.827 480.532 0.0 | 3/2+ 5/2+ 3/2+ | ||
1997.57 9 | EFGHI | (1/2)- | 413.03 7 1142.6 3 1776.6 5 | 72 4 34 5 100 13 | 1584.52 855.012 220.968 | (3/2)- 3/2+ 1/2+ | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2002.6 5 | D | (19/2-) | 1052.1 | 100 | Q | 950.5 | (15/2-) | |
2075.43 16 | K | (3/2,5/2+) | 1165.0 2 1488.1 4 1595.3 7 2075.3 4 | 89 8 72 12 70 12 100 13 | 910.29 587.827 480.532 0.0 | 1/2+ 3/2+ 5/2+ 3/2+ | ||
2077.43 13 | EFGHIJ | (1/2-,3/2-) | 1489.2 3 1856.4 2 2077.22 25 | 37 7 100 8 87 9 | 587.827 220.968 0.0 | 3/2+ 1/2+ 3/2+ | ||
2117.8 9 | FGHI | (1/2,3/2) | ||||||
2133.9 5 | D | (19/2-) | 1183.4 | 100 | Q | 950.5 | (15/2-) | |
2150.7 5 | FGHI | (1/2,3/2) | 2150.5 8 ? | 100 | 0.0 | 3/2+ | ||
2283 | J | 2283 | 100 | 0.0 | 3/2+ | |||
2334 | J | 2334 | 100 | 0.0 | 3/2+ | |||
2388.0 6 | D | 254.1 | 100 | 2133.9 | (19/2-) | |||
2393.5 5 | D | (21/2-) | 390.6 | 100 | D | 2002.6 | (19/2-) | |
2396.6 3 | E | (1/2+,3/2) | 1916.4 4 2396.2 8 | 100 28 45 18 | 480.532 0.0 | 5/2+ 3/2+ | ||
2420 | J | 2420 | 100 | 0.0 | 3/2+ | |||
2440 | J | 2440 | 100 | 0.0 | 3/2+ | |||
2447.76 20 | E IJ | 1/2-,3/2- | 1466.6 5 ? 1592.8 8 1860.4 7 2227 2447.68 24 | 8.2 20 2.8 14 13.1 17 15 100 4 | 979.965 855.012 587.827 220.968 0.0 | 3/2+,5/2+ 3/2+ 3/2+ 1/2+ 3/2+ | ||
2478 15 | IJ | (5/2-) | 2478 | 100 | 0.0 | 3/2+ | ||
2485 | J | 2485 | 100 | 0.0 | 3/2+ | |||
2496 | J | 2496 | 100 | 0.0 | 3/2+ | |||
2579.2 3 | E I | (1/2+,3/2) | 2098.3 7 2579.4 5 | 100 11 27 7 | 480.532 0.0 | 5/2+ 3/2+ | ||
2602? | IJ | 2602 | 100 | 0.0 | 3/2+ | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2621 | IJ | 2621 | 100 | 0.0 | 3/2+ | |||
2638 | J | 2638 | 100 | 0.0 | 3/2+ | |||
2651 | J | 2651 | 100 | 0.0 | 3/2+ | |||
2658.5 3 | E IJ | (1/2,3/2) | 2177.1 5 2659.2 4 | <25 100 13 | 480.532 0.0 | 5/2+ 3/2+ | ||
2667? | J | 2447 2667 | 100 37 41 7 | 220.968 0.0 | 1/2+ 3/2+ | |||
2688.0 3 | E I | (1/2,3/2) | 2467.2 3 2687.7 5 | 100 18 64 20 | 220.968 0.0 | 1/2+ 3/2+ | ||
2708? | J | 2708 | 100 | 0.0 | 3/2+ | |||
2710.78 25 | E IJ | 1/2,3/2 | 1101.6 3 2489.3 5 2710.9 6 | <96 98 18 100 21 | 1609.31 220.968 0.0 | (1/2+,3/2+) 1/2+ 3/2+ | ||
2730.05 14 | EF IJ | 1/2,3/2 | 1120.48 23 2142.19 21 2510.8 7 2730.2 3 | 13 3 36 3 10.1 27 100 6 | 1609.31 587.827 220.968 0.0 | (1/2+,3/2+) 3/2+ 1/2+ 3/2+ | ||
2739.6 6 | D | (23/2-) | 737.0 | 100 | Q | 2002.6 | (19/2-) | |
2781 | IJ | (1/2-,3/2-) | 2781 | 100 | 0.0 | 3/2+ | ||
2824.7 6 | D | (23/2+) | 431.1 | 100 | 2393.5 | (21/2-) | ||
2850 15 ? | I | (5/2-,7/2-) | ||||||
2873.0 3 | E IJ | (1/2,3/2) | 2652.3 4 2872.2 5 | 100 12 <100 | 220.968 0.0 | 1/2+ 3/2+ | ||
2888.1 6 | E I | (1/2,3/2) | 2888.1 6 | 100 | 0.0 | 3/2+ | ||
2897.1 4 | E I | (1/2+,3/2) | 2309.5 5 2416.5 11 | 100 35 90 40 | 587.827 480.532 | 3/2+ 5/2+ | ||
2947 | IJ | (5/2-) | 2947 | 100 | 0.0 | 3/2+ | ||
3084.1 5 | D | (21/2+) | 1081.7 | 100 | D | 2002.6 | (19/2-) | |
3085.84 22 | E I | 1/2,3/2 | 1415.41 27 2864.7 4 3085.1 10 | 54 9 100 20 43 5 | 1670.67 220.968 0.0 | (3/2-) 1/2+ 3/2+ | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3092.6 3 | E J | (1/2,3/2) | 1101.6 3 2872.2 5 3094.0 10 | <92 <250 100 10 | 1991.02 220.968 0.0 | (3/2,5/2) 1/2+ 3/2+ | ||
3111 | J | 3111 | 100 | 0.0 | 3/2+ | |||
3122 | J | 3122 | 100 | 0.0 | 3/2+ | |||
3126 | J | 2645 3126 | 100 38 45 6 | 480.532 0.0 | 5/2+ 3/2+ | |||
3148 | J | 2667 3148 | 92 33 100 13 | 480.532 0.0 | 5/2+ 3/2+ | |||
3154.1 3 | E | (1/2-,3/2-) | 2566.0 4 3153.7 13 | 100 12 15 8 | 587.827 0.0 | 3/2+ 3/2+ | ||
3163 | J | 2683 3163 | 30E1 14 100 16 | 480.532 0.0 | 5/2+ 3/2+ | |||
3169.2 3 | E | (1/2,3/2) | 1498.1 3 3173.4? | 100 18 68 10 | 1670.67 0.0 | (3/2-) 3/2+ | ||
3182 | J | 3182 | 100 | 0.0 | 3/2+ | |||
3190 | J | 2602 2708 3190 | 135 50 265 75 100 10 | 587.827 480.532 0.0 | 3/2+ 5/2+ 3/2+ | |||
3196 | J | 3196 | 100 | 0.0 | 3/2+ | |||
3210.3 6 | D | (27/2-) | 470.7 | 100 | Q | 2739.6 | (23/2-) | |
3211.8 6 | D | (23/2+) | 128.0 818.1 | 73.4 20 100 3 | D D | 3084.1 2393.5 | (21/2+) (21/2-) | |
3272? | J | 2683 3272 | 100 30 100 10 | 587.827 0.0 | 3/2+ 3/2+ | |||
3294.0 4 | E | (1/2,3/2) | 2438.8 4 3298.0? | 36 11 100 20 | 855.012 0.0 | 3/2+ 3/2+ | ||
3324? | IJ | 3324 | 100 | 0.0 | 3/2+ | |||
3410 | J | 3190 3410 | 18 5 100 7 | 220.968 0.0 | 1/2+ 3/2+ | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3415 | J | 3415 | 100 | 0.0 | 3/2+ | |||
3415.7 6 | D | (25/2+) | 204.0 591.0 | 100 4 <1.5 | D | 3211.8 2824.7 | (23/2+) (23/2+) | |
3422 | J | 3422 | 100 | 0.0 | 3/2+ | |||
3454 | J | 2973.5 3454 | 100 26 45 4 | 480.532 0.0 | 5/2+ 3/2+ | |||
3510.3 3 | E | (1/2,3/2) | 931.1 3 3511.8 12 | 100 55 23 | 2579.2 0.0 | (1/2+,3/2) 3/2+ | ||
3587 | J | 3587 | 100 | 0.0 | 3/2+ | |||
3632.6 5 | E IJ | (1/2,3/2) | 3632.2 6 | 100 | 0.0 | 3/2+ | ||
3647.5 7 | D | (29/2-) | 437.2 | 100 | 3210.3 | (27/2-) | ||
3656 | J | 3068 3656 | 100 45 79 13 | 587.827 0.0 | 3/2+ 3/2+ | |||
3670 20 ? | I | |||||||
3696 | J | 3696 | 100 | 0.0 | 3/2+ | |||
3708 | J | 2799 3708 | 85 28 100 11 | 910.29 0.0 | 1/2+ 3/2+ | |||
3720 | J | 3720 | 100 | 0.0 | 3/2+ | |||
3753 | J | 3272 3753 | 203 64 100 9 | 480.532 0.0 | 5/2+ 3/2+ | |||
3758.3 7 | D | (27/2+) | 342.6 | 100 | D | 3415.7 | (25/2+) | |
3779 | J | 2799 3190 3779 | 173 65 112 42 100 12 | 979.965 587.827 0.0 | 3/2+,5/2+ 3/2+ 3/2+ | |||
3786.0 3 | E I | (1/2,3/2) | 2177.1 5 3197.7 4 | <65 100 19 | 1609.31 587.827 | (1/2+,3/2+) 3/2+ | ||
3805.2 7 | D | (29/2-) | 594.9 | 100 | 3210.3 | (27/2-) | ||
3813 | J | 3813 | 100 | 0.0 | 3/2+ | |||
3881 | J | 3881 | 100 | 0.0 | 3/2+ | |||
3929.7 20 ? | E I | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4072.3 20 ? | E I | |||||||
4180.9 7 | D | (29/2+) | 422.6 | 100 | D | 3758.3 | (27/2+) | |
4254.1 7 | D | (31/2+) | 495.8 | 100 | Q | 3758.3 | (27/2+) | |
4269 20 ? | I | |||||||
4695.8 8 | D | (31/2+) | 514.9 | 100 | D | 4180.9 | (29/2+) | |
4713.2 8 | D | (35/2+) | 459.1 | 100 | 4254.1 | (31/2+) | ||
4729 20 ? | I | |||||||
4816.6 7 | D | (33/2-) | 1011.4 1169.1 | <100 <100 | 3805.2 3647.5 | (29/2-) (29/2-) | ||
4890 20 ? | I | |||||||
4940 20 ? | I | |||||||
5023.4 8 | D | (33/2+) | 327.6 | 100 | D | 4695.8 | (31/2+) | |
5235.8 8 | D | (33/2+) | 540.0 | 100 | D | 4695.8 | (31/2+) | |
5850.2 9 | D | (35/2+) | 614.4 826.8 | <63 100 13 | 5235.8 5023.4 | (33/2+) (33/2+) |
E(level): From least-squares fit to Eγ’s including primary γ rays from (n,γ) reactions, 0.3 keV uncertainty when not stated. For 86 neutron resonances in the range 102 eV to 10.6 keV see 134Ba(n,γ):resonances dataset.
Jπ(level): For high-spin (J>11/2), the assignments are as proposed by 2006Ch51 based on their γγ(θ)(DCO) data and systematics in this mass region. The evaluators place all the assignments in parentheses
M(γ): For γ rays from low-spin levels, the assignments are from ce data in 135La ε decay. The mult=Q and d are from DCO ratios in 130Te(9Be,4nγ), mult=Q corresponds to ΔJ=2, quadrupole and mult=d to ΔJ=1, dipole (with possible quadrupole admixture for Δπ=no). The mult=Q most likely corresponds to E2 transition
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - νd3/2, DECOUPLED band (?). | |||||||
0.0 | 3/2+ | STABLE | |||||
874.518 18 | 7/2+ | 1.32 ps 5 | 287? 394.04 4 874.51 2 | 2.4 2 100.0 10 | [E2] [M1,E2] E2 | 587.827 480.532 0.0 | 3/2+ 5/2+ 3/2+ |
1955.4 5 | (11/2+) | 1080.9 | 100 | 874.518 | 7/2+ | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - νh11/2-1 multiplet. | |||||||
268.218 20 | 11/2- | 28.7 h 2 % IT = 100 | |||||
950.5 3 | (15/2-) | 682.3 | 100 | Q | 268.218 | 11/2- | |
2002.6 5 | (19/2-) | 1052.1 | 100 | Q | 950.5 | (15/2-) | |
2393.5 5 | (21/2-) | 390.6 | 100 | D | 2002.6 | (19/2-) | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - γ cascade based on (21/2+) | |||||||
3084.1 5 | (21/2+) | ||||||
3211.8 6 | (23/2+) | 128.0 818.1 | 73.4 20 100 3 | D D | 3084.1 2393.5 | (21/2+) (21/2-) | |
3415.7 6 | (25/2+) | 204.0 591.0 | 100 4 <1.5 | D | 3211.8 2824.7 | (23/2+) (23/2+) | |
3758.3 7 | (27/2+) | 342.6 | 100 | D | 3415.7 | (25/2+) | |
4180.9 7 | (29/2+) | 422.6 | 100 | D | 3758.3 | (27/2+) | |
4695.8 8 | (31/2+) | 514.9 | 100 | D | 4180.9 | (29/2+) | |
5235.8 8 | (33/2+) | 540.0 | 100 | D | 4695.8 | (31/2+) | |
5850.2 9 | (35/2+) | 614.4 826.8 | <63 100 13 | 5235.8 5023.4 | (33/2+) (33/2+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - γ cascade based on (23/2-) | |||||||
2739.6 6 | (23/2-) | ||||||
3210.3 6 | (27/2-) | 470.7 | 100 | Q | 2739.6 | (23/2-) | |
3805.2 7 | (29/2-) | 594.9 | 100 | 3210.3 | (27/2-) | ||
4816.6 7 | (33/2-) | 1011.4 1169.1 | <100 <100 | 3805.2 3647.5 | (29/2-) (29/2-) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
220.968 | 1/2+ | 0.64 ns 27 | 220.94 2 | M1+E2 | 0.38 8 | 0.1110 | B(E2)(W.u.)=4.6 2, B(M1)(W.u.)=0.0025 11, α=0.1110 17, α(K)=0.0941 14, α(L)=0.0134 5, α(M)=0.00279 10, α(N)=0.000598 21, α(O)=9.0E-5 3, α(P)=6.03E-6 10, α(N+)=0.000694 23 |
268.218 | 11/2- | 28.7 h 2 % IT = 100 | 268.218 20 | M4 | 5.31 | B(M4)(W.u.)=2.50 7, α=5.31, α(K)=3.79 6, α(L)=1.182 17, α(M)=0.267 4, α(N)=0.0572 8, α(O)=0.00820 12, α(P)=0.000405 6, α(N+)=0.0658 10 | |
480.532 | 5/2+ | 13 ps 2 | 259.58 4 | (E2) | 0.0721 | B(E2)(W.u.)=2.6 5, α=0.0721, α(K)=0.0579 9, α(L)=0.01129 16, α(M)=0.00239 4, α(N)=0.000505 7, α(O)=7.19E-5 10, α(P)=3.21E-6 5, α(N+)=0.000580 9 | |
5/2+ | 13 ps 2 | 480.52 2 | M1+E2 | +1.6 +5-4 | 0.0120 | B(E2)(W.u.)=28.3 10, B(M1)(W.u.)=0.0042 20, α=0.0120 5, α(K)=0.0102 5, α(L)=0.00146 4, α(M)=0.000304 7, α(N)=6.51E-5 15, α(O)=9.7E-6 3, α(P)=6.3E-7 4, α(N+)=7.54E-5 18 | |
587.827 | 3/2+ | 107.32 9 | E2(+M1) | 1.5 GT | 1.39 | α=1.39 11, α(K)=0.93 5, α(L)=0.36 5, α(M)=0.079 11, α(N)=0.0164 23, α(O)=0.0022 3, α(P)=4.56×10-5 7, α(N+)=0.019 3 | |
3/2+ | 366.83 2 | M1(+E2) | 0.5 LT | 0.0283 | α=0.0283 6, α(K)=0.0243 6, α(L)=0.00323 5, α(M)=0.000665 10, α(N)=0.0001434 21, α(O)=2.19×10-5 3, α(P)=1.57E-6 5, α(N+)=0.0001669 24 | ||
3/2+ | 587.84 2 | M1+E2 | 1.0 4 | 0.0076 | B(E2)(W.u.)=18.0 10, α=0.0076 6, α(K)=0.0065 6, α(L)=0.00088 5, α(M)=0.000181 10, α(N)=3.89E-5 21, α(O)=5.9E-6 4, α(P)=4.1E-7 4, α(N+)=4.52E-5 25 | ||
855.012 | 3/2+ | 374.46 2 | M1+E2 | -0.43 3 | 0.0266 | α=0.0266, α(K)=0.0227 4, α(L)=0.00306 5, α(M)=0.000631 9, α(N)=0.0001359 19, α(O)=2.07×10-5 3, α(P)=1.461E-6 22, α(N+)=0.0001581 23 | |
3/2+ | 634.04 2 | M1(+E2) | 1.3 LT | 0.0067 | α=0.0067 7, α(K)=0.0057 6, α(L)=0.00075 6, α(M)=0.000155 11, α(N)=3.34×10-5 25, α(O)=5.1E-6 5, α(P)=3.7E-7 5, α(N+)=3.9E-5 3 | ||
3/2+ | 855.02 2 | M1(+E2) | 0.5 LT | 0.00349 | B(E2)(W.u.)=7.0 10, α=0.00349 12, α(K)=0.00301 10, α(L)=0.000382 12, α(M)=7.85E-5 23, α(N)=1.69E-5 5, α(O)=2.60E-6 8, α(P)=1.93E-7 7, α(N+)=1.97E-5 6 | ||
874.518 | 7/2+ | 1.32 ps 5 | 287 | [E2] | B(E2)(W.u.)<1.0 (<a href= "http://www.nndc.bnl.gov/nsr/nsrlink.jsp?2006Fe06 ">2006Fe06</a>) | ||
7/2+ | 1.32 ps 5 | 394.04 4 | [M1,E2] | 0.0217 | B(E2)(W.u.)=12.8 12, B(M1)(W.u.)=0.0032 3, α=0.0217 23, α(K)=0.0184 23, α(L)=0.00265 5, α(M)=0.000550 8, α(N)=0.0001179 19, α(O)=1.77E-5 6, α(P)=1.15E-6 20, α(N+)=0.0001368 25 | ||
7/2+ | 1.32 ps 5 | 874.51 2 | E2 | 0.00244 | B(E2)(W.u.)=19.9 8, α=0.00244, α(K)=0.00209 3, α(L)=0.000279 4, α(M)=5.74E-5 8, α(N)=1.234E-5 18, α(O)=1.87E-6 3, α(P)=1.289E-7 18, α(N+)=1.434E-5 20 | ||
910.29 | 1/2+ | 910.28 3 | 0.0027 | B(E2)(W.u.)=11.7 10, α=0.0027 5, α(K)=0.0023 4, α(L)=0.00030 5 | |||
979.965 | 3/2+,5/2+ | 124.89 7 | M1,E2 | 0.70 | α=0.70 18, α(K)=0.53 8, α(L)=0.14 8, α(M)=0.029 17, α(N)=0.006 4, α(O)=0.0009 5, α(P)=2.95×10-5 5, α(N+)=0.007 4 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 3/2+ | STABLE | μ=+0.837943 17 (1972Ol01,1989Ra17), Q=+0.160 3 (1988We07,1989Ra17) Δ<r2>(138Ba-135Ba)=-0.079 fm2 12 (1979Be25). E(level): γ from 135La ε decay only. νd3/2, DECOUPLED band (?). |
268.218 | 11/2- | 28.7 h 2 % IT = 100 | μ=-1.001 15 (1979Be25,1989Ra17), Q=+0.96 8 (1983Mu12,1989Ra17) Δ<r2>(138Ba-135Ba isomer)=-0.053 fm2 12 (1979Be25). E(level): From (n,γ) E=th only. νh11/2-1 multiplet. |
874.518 | 7/2+ | 1.32 ps 5 | (2J+1)Γ0/4=0.00092 eV 12, B(E2)=0.22 3 in (γ,γ’). E(level): γ from 135La ε decay only. νd3/2, DECOUPLED band (?). |
950.5 | (15/2-) | Configuration=νh11/2-1~#2+. E(level): From (n,γ) E=th only. νh11/2-1 multiplet. Jπ(level): From proposed band structure. E(level): From (n,γ) E=th only. νh11/2-1 multiplet. | |
979.965 | 3/2+,5/2+ | B(E2)≤0.003 (2J+1)Γ0/4=0.0028 eV 5 in (γ,γ’). | |
1213.73 | (3/2) | (2J+1)Γ0/4=0.00092 eV 21 in (γ,γ’). | |
1238.41 | (5/2) | Jπ(level): From the deexcitation pattern in (n,n’γ), statistical-model comparisons. | |
1298.54 | (1/2+,3/2+) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
1557.35 | (5/2,7/2+) | Jπ(level): From the deexcitation pattern in (n,n’γ), statistical-model comparisons. | |
1609.31 | (1/2+,3/2+) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
1719.57 | (1/2+,3/2+) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
1794.4 | (1/2,3/2) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
1830.5 | (1/2,3/2) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
1871.46 | (3/2+,5/2) | (2J+1)Γ0/4=0.0059 eV 16 in (γ,γ’). Jπ(level): From the deexcitation pattern in (n,n’γ), statistical-model comparisons. | |
1878.9 | (1/2,3/2) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
1941.17 | (3/2+,5/2+) | (2J+1)Γ0/4=0.0024 eV 6 in (γ,γ’). | |
1955.4 | (11/2+) | E(level): γ from 135La ε decay only. νd3/2, DECOUPLED band (?). Jπ(level): From proposed band structure. | |
1964.83 | (1/2+,3/2+) | (2J+1)Γ0/4=0.0025 eV 17 in (γ,γ’). Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
1971.6 | (3/2,5/2) | Jπ(level): From the deexcitation pattern in (n,n’γ), statistical-model comparisons. | |
1991.02 | (3/2,5/2) | (2J+1)Γ0/4=0.0041 eV 7 in (γ,γ’). Jπ(level): From the deexcitation pattern in (n,n’γ), statistical-model comparisons. | |
2002.6 | (19/2-) | Configuration=νh11/2-1~#4+. E(level): From (n,γ) E=th only. νh11/2-1 multiplet. Jπ(level): From proposed band structure. | |
2077.43 | (1/2-,3/2-) | (2J+1)Γ0/4=0.0045 eV 13 in (γ,γ’). | |
2117.8 | (1/2,3/2) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
2283 | (2J+1)Γ0/4=0.0013 eV 3. | ||
2334 | (2J+1)Γ0/4=0.0018 eV 3. | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
2393.5 | (21/2-) | E(level): From (n,γ) E=th only. νh11/2-1 multiplet. | |
2420 | (2J+1)Γ0/4=0.0018 eV 3. | ||
2440 | (2J+1)Γ0/4=0.0022 eV 3. | ||
2447.76 | 1/2-,3/2- | (2J+1)Γ0/4=0.0039 eV 8 in (γ,γ’). | |
2478 | (5/2-) | (2J+1)Γ0/4=0.0021 eV 3 in (γ,γ’). | |
2485 | (2J+1)Γ0/4=0.0027 eV 4. | ||
2496 | (2J+1)Γ0/4=0.0019 eV 3. | ||
2579.2 | (1/2+,3/2) | XREF: I(?). | |
2602 | (2J+1)Γ0/4=0.0017 eV 3 in (γ,γ’). | ||
2621 | (2J+1)Γ0/4=0.0036 eV 4 in (γ,γ’). | ||
2638 | (2J+1)Γ0/4=0.0023 eV 4. | ||
2651 | (2J+1)Γ0/4=0.0018 eV 4. | ||
2658.5 | (1/2,3/2) | XREF: I(?). Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
2667 | (2J+1)Γ0/4=0.0056 eV 7. | ||
2688.0 | (1/2,3/2) | XREF: I(?). Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
2708 | (2J+1)Γ0/4=2.3×10-3 eV 5 or 4.0×10-3 eV 5. | ||
2710.78 | 1/2,3/2 | XREF: I(?). | |
2730.05 | 1/2,3/2 | XREF: I(?). | |
2739.6 | (23/2-) | E(level): γ cascade based on (23/2-). | |
2781 | (1/2-,3/2-) | XREF: I(?). | |
2873.0 | (1/2,3/2) | XREF: I(?). Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
2888.1 | (1/2,3/2) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
2947 | (5/2-) | XREF: I(?). | |
3084.1 | (21/2+) | Configuration=νh11/2-2~#νs1/2. E(level): From (n,n’γ) only. γ cascade based on (21/2+). | |
3085.84 | 1/2,3/2 | XREF: I(?). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
3092.6 | (1/2,3/2) | (2J+1)Γ0/4=0.0225 eV 17 in (γ,γ’) for 51% branch to the g.s., 0.0183 eV 16 for 63% branch to g.s. E(level): (2J+1)Γ0/4=0.0225 eV 17 in (γ,γ’) for 51% branch to the g.s., 0.0183 eV 16 for 63% branch to g.s. Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
3111 | (2J+1)Γ0/4=0.0026 eV 6. | ||
3122 | (2J+1)Γ0/4=0.0027 eV 6. | ||
3126 | (2J+1)Γ0/4=0.0082 eV 10. | ||
3148 | (2J+1)Γ0/4=0.0074 eV 10 for 52% branch to the g.s., 0.0039 eV 6 for 100% branch to the g.s. E(level): (2J+1)Γ0/4=0.0074 eV 10 for 52% branch to the g.s., 0.0039 eV 6 for 100% branch to the g.s. | ||
3154.1 | (1/2-,3/2-) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
3163 | (2J+1)Γ0/4=0.0064 eV 10 for 25% branch to the g.s., 0.0016 eV 5 for 100% branch to the g.s. E(level): (2J+1)Γ0/4=0.0064 eV 10 for 25% branch to the g.s., 0.0016 eV 5 for 100% branch to the g.s. | ||
3169.2 | (1/2,3/2) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
3182 | (2J+1)Γ0/4=0.0036 eV 5. | ||
3190 | (2J+1)Γ0/4=0.0165 eV 14. | ||
3196 | (2J+1)Γ0/4=0.0028 eV 6. | ||
3210.3 | (27/2-) | E(level): γ cascade based on (23/2-). | |
3211.8 | (23/2+) | Configuration=νh11/2-1~#π(h11/2d5/2-1). E(level): From (n,n’γ) only. γ cascade based on (21/2+). Configuration=νh11/2-1~#π(h11/2d5/2-1). | |
3272 | (2J+1)Γ0/4=0.0116 eV 12. | ||
3294.0 | (1/2,3/2) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
3324 | XREF: I(?). | ||
3410 | (2J+1)Γ0/4=0.0285 eV 23 for 85% branch to the g.s., 0.0334 eV 24 for 100% branch to the g.s. E(level): (2J+1)Γ0/4=0.0285 eV 23 for 85% branch to the g.s., 0.0334 eV 24 for 100% branch to the g.s. | ||
3415 | (2J+1)Γ0/4=0.0028 eV 7. | ||
3415.7 | (25/2+) | Configuration=νh11/2-1~#π(h11/2d5/2-1). E(level): From (n,n’γ) only. γ cascade based on (21/2+). | |
3422 | (2J+1)Γ0/4=0.0028 eV 6. | ||
3454 | (2J+1)Γ0/4=0.0183 eV 17. | ||
3510.3 | (1/2,3/2) | Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
3587 | (2J+1)Γ0/4=0.0032 eV 10. | ||
3632.6 | (1/2,3/2) | XREF: I(?). Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
3656 | (2J+1)Γ0/4=0.0108 eV 17. | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
3696 | (2J+1)Γ0/4=0.0045 eV 10. | ||
3708 | (2J+1)Γ0/4=0.0161 eV 18. | ||
3720 | (2J+1)Γ0/4=0.0128 eV 15. | ||
3753 | (2J+1)Γ0/4=0.026 eV 3 for 33% branch to the g.s., 0.0087 eV 16 for 100% branch to the g.s. E(level): (2J+1)Γ0/4=0.026 eV 3 for 33% branch to the g.s., 0.0087 eV 16 for 100% branch to the g.s. | ||
3758.3 | (27/2+) | Configuration=νh11/2-1~#π(h11/2g7/2-1). E(level): From (n,n’γ) only. γ cascade based on (21/2+). | |
3779 | (2J+1)Γ0/4=0.043 eV 5 for 26% branch to the g.s., 0.0112 eV 19 for 100% branch to the g.s. E(level): (2J+1)Γ0/4=0.043 eV 5 for 26% branch to the g.s., 0.0112 eV 19 for 100% branch to the g.s. | ||
3786.0 | (1/2,3/2) | XREF: I(?). Jπ(level): Primary (assumed dipole) γ from 1/2+ capture states. π: from comparison of reduced intensities of primary transitions to final states with known Jπ. | |
3805.2 | (29/2-) | E(level): γ cascade based on (23/2-). | |
3813 | (2J+1)Γ0/4=0.0071 eV 20. | ||
3881 | (2J+1)Γ0/4=0.0090 eV 18. | ||
4180.9 | (29/2+) | Configuration=νh11/2-1~#π(h11/2g7/2-1)#2+. E(level): From (n,n’γ) only. γ cascade based on (21/2+). | |
4695.8 | (31/2+) | Configuration=νh11/2-1~#π(h11/2g7/2-1)#2+. E(level): From (n,n’γ) only. γ cascade based on (21/2+). Configuration=νh11/2-1~#π(h11/2g7/2-1)#2+. | |
4816.6 | (33/2-) | E(level): γ cascade based on (23/2-). | |
5235.8 | (33/2+) | E(level): From (n,n’γ) only. γ cascade based on (21/2+). | |
5850.2 | (35/2+) | E(level): From (n,n’γ) only. γ cascade based on (21/2+). |
E(level) | E(gamma) | Comments |
268.218 | 268.218 | M(γ): from ce data in 135Ba IT decay |
587.827 | 107.32 | I(γ): from 135La ε. Iγ=5.0 10 in (n,n’γ) |
979.965 | 124.89 | E(γ): γ from 135La ε decay only | 392.08 | E(γ): γ from 135La ε decay only | 499.36 | E(γ): γ from 135La ε decay only |
1130 | 1130 | E(γ): unplaced γ rays of Eγ=1130.89 11 and Eγ=1130.6 6 were reported in 135La ε decay and (n,n’γ), respectively |
1213.73 | 234.03 | E(γ): From (n,n’γ) only | 359.1 | E(γ): From (n,n’γ) only |
1225.86 | 245.44 | E(γ): From (n,n’γ) only | 371.1 | E(γ): From (n,n’γ) only | 1005.3 | E(γ): From (n,n’γ) only |
1238.41 | 382.8 | E(γ): From (n,n’γ) only | 649.4 | E(γ): From (n,n’γ) only | 1238.3 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1298.54 | 1298.97 | E(γ): From (n,γ) E=th only |
1446.41 | 1178.1 | E(γ): From (n,n’γ) only |
1584.52 | 1583 | I(γ): from (n,γ) E=24.3 keV |
1609.31 | 1128.2 | E(γ): From (n,γ) E=th only | 1388.2 | E(γ): From (n,γ) E=th only |
1719.57 | 739.3 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity | 1238.55 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity | 1720.0 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1830.5 | 1830.7 | E(γ): from (n,γ) E=24.3 keV res only |
1878.9 | 1291.3 | E(γ): from (n,γ) E=102 eV res only |
1941.17 | 1720.2 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
E(level) | E(gamma) | Comments |
1964.83 | 739.4 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1971.6 | 1491.1 | E(γ): From (n,n’γ) only | 1971.3 | E(γ): From (n,n’γ) only |
1991.02 | 1990.8 | E(γ): From (n,n’γ) only |
1997.57 | 413.03 | E(γ): From (n,γ) E=th only | 1142.6 | E(γ): From (n,γ) E=th only | 1776.6 | E(γ): From (n,γ) E=th only |
2077.43 | 1489.2 | E(γ): From (n,γ) E=th only |
2150.7 | 2150.5 | E(γ): from (n,γ) E=102 eV res only |
2602 | 2602 | E(γ): Multiply placed |
2658.5 | 2177.1 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
2667 | 2447 | E(γ): second placement of a γ ray of near this energy is from 2447.6 level | 2667 | E(γ): Multiply placed |
2708 | 2708 | E(γ): Multiply placed |
2710.78 | 1101.6 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
2730.05 | 1120.48 | E(γ): From (n,γ) E=th only | 2142.19 | E(γ): from (n,γ) E=th. Eγ=2142.8 2 in (n,γ) E=102 eV res | 2510.8 | E(γ): From (n,γ) E=th only | 2730.2 | E(γ): From (n,γ) E=th only |
2873.0 | 2872.2 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
3092.6 | 1101.6 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity | 2872.2 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
3148 | 2667 | E(γ): Multiply placed |
3163 | 2683 | E(γ): Multiply placed |
3169.2 | 3173.4 | E(γ): Poor energy fit. Level energy differs by 4 keV |
E(level) | E(gamma) | Comments |
3190 | 2602 | E(γ): Multiply placed | 2708 | E(γ): Multiply placed |
3272 | 2683 | E(γ): Multiply placed | 3272 | E(γ): Multiply placed |
3294.0 | 3298.0 | E(γ): Poor energy fit. Level energy differs by 4 keV |
3410 | 3190 | E(γ): Multiply placed |
3708 | 2799 | E(γ): Multiply placed |
3753 | 3272 | E(γ): Multiply placed |
3779 | 2799 | E(γ): Multiply placed | 3190 | E(γ): Multiply placed |
3786.0 | 2177.1 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
Isotope shifts, hyperfine structure, moments, etc. measurements: 2000Tr07, 1995Va36, 1993Vi10, 1988Ya13, 1988We07, 1987Va16, 1986Si03, 1986Ca25, 1985Si24, 1985Va04, 1985Si24, 1985Ca40, 1985We15, 1984Va08, 1984Pe06, 1983Ri02, 1983Ho06, 1983Gr15, 1983El06, 1983El04, 1983Be12, 1982Sh05, 1982Ri07, 1982Ri03, 1982Ne13, 1982Ne12, 1982Ne11, 1982Gr14, 1982Gr15, 1981Wa19, 1980Si14, 1980Ji01, 1979Gu09, 1979Ba74, 1979Be25, 1978Lu07, 1977Kr12, 1976Ma28, 1970Vo08, 1970Ho31, 1969Su04, 1968Op01, 1968Be60, 1966Ol02, 1966Co32, 1966Co28, 1966Co26, 1966Co18, 1964Ja11, 1963Zu05, 1963Na11, 1963Ja15, 1962Wi10, 1962Ko22
Nuclear structure calculations: 2004Yo04 (levels, transition rates), 2000Dm04 (anapole moments), 1999Dr18 (IBA model), 1990Lo16 (levels, IBFM model), 1987Mi15 (levels, transition rates, magnetic moment, Q), 1985Ha34 (levels), 1984Ab01 (yrast levels)
For 86 neutron resonances from 102 eV to 10.6 keV, see 134Ba(n,γ):resonances dataset compiled from 1996Ko27. See also 2006MuZX evaluation.
Q-value: Note: Current evaluation has used the following Q record -1200 10 6971.9610 8248.3 4 -1860.210 2003Au03