ADOPTED LEVELS, GAMMAS for 179Hf
Author: Coral M. Baglin | Citation: Nucl. Data Sheets 110, 265 (2009) | Cutoff date: 15-Nov-2008
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-105.6 keV 4 | S(n)= 6098.99 keV 8 | S(p)= 7414.5 keV 21 | Q(α)= 1806.3 keV 15 | ||
Reference: 2012WA38 |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCDEFGHIJK | 9/2+ | STABLE | |||||
122.7904 24 | AB D FGH K | 11/2+ | 37 ps 3 | 122.793 3 | 100 | M1+E2 | 0.0 | 9/2+ |
214.3395 22 | ABC E G KL | 7/2- | 1.85 ns 4 | 214.335 3 | 100 | E1 | 0.0 | 9/2+ |
268.92 6 | D FGH K | 13/2+ | 21 ps 3 | 146.15 7 268.85 14 | 100 4 39.4 4 | M1+E2 E2 | 122.7904 0.0 | 11/2+ 9/2+ |
337.7178 23 | AB E GH L | 9/2- | 123.3790 20 214.930 3 337.713 5 | 100 4 78 4 21.2 9 | E2 [E1] E1 | 214.3395 122.7904 0.0 | 7/2- 11/2+ 9/2+ | |
375.0352 25 | A C E G KL | 1/2- | 18.67 s 4 % IT = 100 | 160.696 2 ≈375 | 100 ≈0.2 | M3 [M4] | 214.3395 0.0 | 7/2- 9/2+ |
420.8943 25 | A E G KL | 3/2- | 45.8610 10 | 100 | M1+E2 | 375.0352 | 1/2- | |
438.68 8 | D FGH | 15/2+ | 169.77 9 315.88 11 | 96 4 100 | M1+E2 E2 | 268.92 122.7904 | 13/2+ 11/2+ | |
476.3341 25 | A E GH K | 5/2- | 55.4420 10 101.2980 10 262.02 3 | 100 1 90 5 0.22 6 | M1 E2 | 420.8943 375.0352 214.3395 | 3/2- 1/2- 7/2- | |
487.709 5 | A G KL | (11/2-) | 150.019 15 273.368 4 487.704 11 | 21.5 15 100 5 52 17 | 337.7178 214.3395 0.0 | 9/2- 7/2- 9/2+ | ||
518.3279 24 | AB E G K | 5/2- | < 0.2 ns | 41.9960 10 97.4350 20 143.301 9 180.613 2 303.977 4 | 0.26 6 0.89 4 0.11 3 0.79 4 100.0 22 | M1(+E2) M1+E2 (E2) E2 M1+E2 | 476.3341 420.8943 375.0352 337.7178 214.3395 | 5/2- 3/2- 1/2- 9/2- 7/2- |
582.230 3 | A E G K | 7/2- | 105.899 3 161.3390 20 367.891 17 | 100 2 19.0 8 0.55 9 | M1 (E2) | 476.3341 420.8943 214.3395 | 5/2- 3/2- 7/2- | |
614.204 3 | A E G | 1/2- | 0.50 ns 15 | 137.873 2 193.310 2 239.165 3 | 0.72 4 100.0 21 16.4 12 | E2 M1+E2 M1 | 476.3341 420.8943 375.0352 | 5/2- 3/2- 1/2- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
616.7562 25 | AB E GH K | 7/2- | 98.433 2 140.4260 20 195.861 6 279.029 4 402.409 6 616.768 9 | 100 1 10.8 7 2.05 24 75.9 8 37.2 7 22.9 19 | M1+E2 M1+E2 M1+E2 M1+E2 | 518.3279 476.3341 420.8943 337.7178 214.3395 0.0 | 5/2- 5/2- 3/2- 9/2- 7/2- 9/2+ | |
631.30 10 | D FGH K | 17/2+ | 192.62 11 362.39 13 | 54 5 100.0 22 | M1+E2 E2 | 438.68 268.92 | 15/2+ 13/2+ | |
664.3 7 | G KL | (13/2-) | 176.3 326.8 | 0.7 7 100 5 | 487.709 337.7178 | (11/2-) 9/2- | ||
679.516 3 | A E G K | 3/2- | 161.191 2 203.182 3 258.615 3 304.465 7 | 100 3 16.7 3 75 5 7.3 7 | M1 M1+E2 M1+E2 M1 | 518.3279 476.3341 420.8943 375.0352 | 5/2- 5/2- 3/2- 1/2- | |
681.036 3 | A KL | 9/2- | 98.808 12 204.696 3 | 15 4 100.0 22 | E2 | 582.230 476.3341 | 7/2- 5/2- | |
701.0552 25 | A E GH K | 5/2- | 84.2970 10 86.857 5 118.8260 10 182.7350 20 224.715 3 280.154 4 326.010 14 486.735 14 | 13.2 8 5.5 7 100 3 25.2 5 6.5 7 4.82 15 35.6 15 12.6 11 | M1+E2 E2 M1+E2 M1+E2 M1(+E0) M1+E2 E2 M1 | 616.7562 614.204 582.230 518.3279 476.3341 420.8943 375.0352 214.3395 | 7/2- 1/2- 7/2- 5/2- 5/2- 3/2- 1/2- 7/2- | |
720.613 3 | A E G K | 3/2- | ≤ 0.3 ns | 106.409 1 202.283 3 244.278 8 299.716 4 345.575 5 506.299 20 | 2.64 15 100 2 10.6 10 38.7 8 9.60 10 4.6 15 | M1(+E2) M1+E2 M1(+E2) M1+E2 M1+E2 (E2) | 614.204 518.3279 476.3341 420.8943 375.0352 214.3395 | 1/2- 5/2- 5/2- 3/2- 1/2- 7/2- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
732.2 6 | G | |||||||
742.710 3 | A G K | 9/2- | 125.957 1 224.367 4 619.90 5 | 100 9 23.4 19 12 6 | M1+E2 | 616.7562 518.3279 122.7904 | 7/2- 5/2- 11/2+ | |
788.185 3 | A E GH KL | 5/2- | 87.127 13 108.678 4 171.432 2 173.977 3 205.950 3 269.857 4 311.844 4 413.132 7 450.47 3 573.825 22 | 2.6 13 3.6 6 100 1 5.0 3 53.3 10 94 7 21.4 9 43.6 9 2.9 3 41.1 24 | M1+E2 E2 M1+E2 M1+E0 M1(+E2) E2 M1 | 701.0552 679.516 616.7562 614.204 582.230 518.3279 476.3341 375.0352 337.7178 214.3395 | 5/2- 3/2- 7/2- 1/2- 7/2- 5/2- 5/2- 1/2- 9/2- 7/2- | |
842.9 10 | K | 11/2- | 260.7 | 100 | 582.230 | 7/2- | ||
848.37 12 | D F K | 19/2+ | 217.07 13 409.68 15 | 42 3 100.0 25 | M1+E2 E2 | 631.30 438.68 | 17/2+ 15/2+ | |
849.200 3 | A GH | 7/2- | 106.492 1 148.148 4 168.162 2 169.675 4 232.439 3 266.974 4 330.856 9 372.853 5 428.292 6 634.94 4 | 12.4 15 6.8 15 13.8 7 15.0 9 47.6 18 35.9 18 10.6 5 71.4 7 12.9 15 100 12 | M1+E2 M1 E2 M1+E2 M1(+E2) M1 (E2) M1+E2 | 742.710 701.0552 681.036 679.516 616.7562 582.230 518.3279 476.3341 420.8943 214.3395 | 9/2- 5/2- 9/2- 3/2- 7/2- 7/2- 5/2- 5/2- 3/2- 7/2- | |
865.9 10 | G KL | (15/2-) | 378.2 | 100 | (E2) | 487.709 | (11/2-) | |
870.222 8 | AB E G K | 7/2- | 532.49 4 655.888 20 870.243 13 | 7.5 5 45.6 19 100.0 20 | M1 M1(+E2) E1 | 337.7178 214.3395 0.0 | 9/2- 7/2- 9/2+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
889.1 10 | G | |||||||
896.7 7 | G K | 11/2- | 153.5 280.1 | 88 13 100 13 | 742.710 616.7562 | 9/2- 7/2- | ||
912.0 10 | G K | 9/2- | 210.9 | 100 | 701.0552 | 5/2- | ||
935.643 3 | A GH KL | 7/2- | 147.458 3 192.933 3 215? 318.887 4 353.425 6 459.287 9 | 33 5 43 4 <10 100.0 24 76 4 30.1 24 | M1 M1+E2 M1 M1(+E2) | 788.185 742.710 720.613 616.7562 582.230 476.3341 | 5/2- 9/2- 3/2- 7/2- 7/2- 5/2- | |
958.6 14 | G | |||||||
985.7 10 | K | 13/2- | 304.7 | 100 | 681.036 | 9/2- | ||
992.0 15 | G | (9/2-) | ||||||
1003.650 4 | AB E G | 5/2+ | 386.898 9 485.323 7 789.188 20 ? 1003.690 23 | 0.54 4 2.7 6 2.05 13 100 6 | (E1) E2 | 616.7562 518.3279 214.3395 0.0 | 7/2- 5/2- 7/2- 9/2+ | |
1024.0 17 | G | |||||||
1030.8 6 | G L | 9/2- | ||||||
1073.565 13 | AB G L | 7/2- | 735.83 5 859.254 16 | 26.8 14 100 2 | M1+E2 M1+E2 | 337.7178 214.3395 | 9/2- 7/2- | |
1074.7 10 | G K | (5/2-) | 860.4 | 100 | 214.3395 | 7/2- | ||
1076.6 8 | K | 13/2- | 179.5 334.2 | 83 17 100 17 | 896.7 742.710 | 11/2- 9/2- | ||
1078.349 10 | A G | (7/2)+ | 357.731 11 863.98 15 1078.37 8 | 2.71 22 7.1 21 100 4 | E2(+M1) | 720.613 214.3395 0.0 | 3/2- 7/2- 9/2+ | |
1080.4 13 | G | |||||||
1084.73 15 | D F K | 21/2+ | 236.36 14 453.43 17 | 27.7 8 100 4 | M1+E2 E2 | 848.37 631.30 | 19/2+ 17/2+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1087.8 8 | G | |||||||
1092.7 13 | G K | (17/2-) | 428.4 | 100 | 664.3 | (13/2-) | ||
1105.74 16 | D K | 25/2- | 25.05 d 25 % IT = 100 | 21.01 12 257.37 15 | 0.254 13 100 17 | M2 E3 | 1084.73 848.37 | 21/2+ 19/2+ |
1105.92 9 | B | (7/2+) | 891.5 3 983.17 20 1105.92 10 | 8.1 20 33 6 100 10 | 214.3395 122.7904 0.0 | 7/2- 11/2+ 9/2+ | ||
1120.816 19 | AB G | 9/2+ | 906.44 6 998.06 10 1120.833 24 | 11.2 9 25 4 100 | M1+E2 M1+E0 | 214.3395 122.7904 0.0 | 7/2- 11/2+ 9/2+ | |
1138.8 6 | G | |||||||
1150.411 5 | A G | 1/2+ | 429.800 6 470.891 7 536.195 10 729.517 10 775.35 8 | 14.4 12 43 4 2.1 3 100 3 1.85 25 | (E1) E1 E1 | 720.613 679.516 614.204 420.8943 375.0352 | 3/2- 3/2- 1/2- 3/2- 1/2- | |
1162.4 7 | G L | |||||||
1168.95 3 | AB GH | (9/2+) | 831.24 3 953.9 3 1046.16 6 1168.4 3 | 67.0 26 35 11 100 21 36 11 | 337.7178 214.3395 122.7904 0.0 | 9/2- 7/2- 11/2+ 9/2+ | ||
1176.2 9 | G | (9/2+) | ||||||
1185.848 5 | A G L | 3/2+ | 182.178 11 397.67 3 465.222 6 484.799 15 506.299 20 571.653 14 709.527 18 764.968 11 810.831 12 | 1.19 16 0.70 13 18.8 10 17.8 18 ≤4.4 53 3 9.3 4 91 3 100.0 22 | (E1) (E1) E1+M2 E1 E1 | 1003.650 788.185 720.613 701.0552 679.516 614.204 476.3341 420.8943 375.0352 | 5/2+ 5/2- 3/2- 5/2- 3/2- 1/2- 5/2- 3/2- 1/2- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1196.2 15 | K | 15/2- | 353.3 | 100 | 842.9 | 11/2- | ||
1198.4 13 | G K | (7/2-) | 123.3 | 100 | 1074.7 | (5/2-) | ||
1199.52 14 | AB GH | (7/2+) | 680.2 5 1076.9 2 1199.5 2 | 7 3 100 20 60 13 | 518.3279 122.7904 0.0 | 5/2- 11/2+ 9/2+ | ||
1235.440 4 | A G | 5/2+ | 231.809 6 386.244 6 514.827 10 534.394 12 555.888 11 653.190 13 759.060 14 | 3.66 25 17.3 3 9.1 26 6.2 3 6.5 6 100 4 22.9 7 | (E1) E1 (E1) | 1003.650 849.200 720.613 701.0552 679.516 582.230 476.3341 | 5/2+ 7/2- 3/2- 5/2- 3/2- 7/2- 5/2- | |
1249.552 6 | A G | 3/2- | 548.508 15 570.036 8 635.26 4 731.22 3 773.15 5 1035.197 15 | 4.7 4 9.5 6 29.4 14 15.6 8 5.6 6 100 6 | M1 M1 M1(+E2) E2+M1 E2 | 701.0552 679.516 614.204 518.3279 476.3341 214.3395 | 5/2- 3/2- 1/2- 5/2- 5/2- 7/2- | |
1255.8 10 | K | 11/2- | 320.2 | 100 | 935.643 | 7/2- | ||
1269.445 6 | A G | 3/2- | 399.17 4 548.858 21 568.382 8 589.923 8 655.256 19 751.14 3 1055.06 5 | 1.79 14 26.1 18 10.6 9 29.2 20 92 4 10.8 5 100 6 | M1+E2 M1 M1+E2 M1+E2 M1 (E2) | 870.222 720.613 701.0552 679.516 614.204 518.3279 214.3395 | 7/2- 3/2- 5/2- 3/2- 1/2- 5/2- 7/2- | |
1282.5 9 | GH | (11/2+) | ||||||
1283.7 10 | K | 15/2- | 207.2 387 | 100 60 60 20 | 1076.6 896.7 | 13/2- 11/2- | ||
1296.64 12 | E | (3/2-,5/2,7/2-) | 596.0 2 616.6 2 1082.4 2 | 34 7 23 5 100 20 | 701.0552 679.516 214.3395 | 5/2- 3/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1309.8 6 | K | (17/2+) | 3 ns 1 | 678.4 871.1 1041.0 | 2.3 12 53 5 100 7 | [M1] [M1] [E2] | 631.30 438.68 268.92 | 17/2+ 15/2+ 13/2+ |
1313.500 13 | A G L | 5/2- | 633.967 22 696.74 5 699.15 8 731.22 3 795.27 6 975.72 6 1099.26 7 | 15.0 14 12.3 10 5.6 10 57 3 13.8 24 100 6 92 12 | M1+E2 E2 E2(+M1) | 679.516 616.7562 614.204 582.230 518.3279 337.7178 214.3395 | 3/2- 7/2- 1/2- 7/2- 5/2- 9/2- 7/2- | |
1343.8 15 | K | (19/2-) | 477.9 | 100 | 865.9 | (15/2-) | ||
1344.6 6 | G | + | ||||||
1348.6 13 | K | (9/2-) | 149.9 274.2 | 42 25 100 50 | 1198.4 1074.7 | (7/2-) (5/2-) | ||
1350.7 7 | F K | 23/2+ | 266.0 502.3 | 33 3 100 7 | 1084.73 848.37 | 21/2+ 19/2+ | ||
1359.0 5 | GH | (13/2)+ | ||||||
1372.3 7 | K | (17/2+) | 933.4 1103.5 | 18 9 100 18 | 438.68 268.92 | 15/2+ 13/2+ | ||
1375 2 | L | 7/2- | ||||||
1381.9 15 | K | 17/2- | 396.2 | 100 | 985.7 | 13/2- | ||
1386.5 6 | G | |||||||
1393.0 8 | K | (27/2-) | 287.0 | 100 | (M1+E2) | 1105.74 | 25/2- | |
1404.5 11 | K | (23/2+) | 4 ns 1 | 298.8 | 100 | (E1(+M2)) | 1105.74 | 25/2- |
1404.5+X 11 | K | (21/2+) | 14 ns 2 | XS | | 1404.5 | (23/2+) | |
1405.2 6 | G L | (7/2-) | ||||||
1428.6 5 | G | (7/2-) | ||||||
1433.189 11 | A E | 3/2- | 753.48 16 816.42 5 914.867 18 956.79 3 1012.296 18 | 4.5 8 12.9 17 38.0 15 39 13 100 7 | E2(+M1) M1 M1+E2 | 679.516 616.7562 518.3279 476.3341 420.8943 | 3/2- 7/2- 5/2- 5/2- 3/2- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1436.353 6 | A G L | 7/2- | 315.49 8 357.999 16 432.701 6 566.159 15 819.66 9 918.029 14 | 1.1 4 4.5 4 7.0 7 4.9 5 23.3 14 100 2 | (E1) M1+E0 M1 M1(+E2) | 1120.816 1078.349 1003.650 870.222 616.7562 518.3279 | 9/2+ (7/2)+ 5/2+ 7/2- 7/2- 5/2- | |
1437 5 | H | 11/2+,13/2+ | ||||||
1453.1 7 | G | |||||||
1458.994 9 | A G | 3/2- | 588.774 8 670.89 6 738.388 22 779.41 3 1038.11 4 1083.93 6 1244.73 6 | 100 4 23.3 18 22.3 16 37 3 75 4 76 4 67 | E2 M1+E2 M1(+E0) M1+E2 E2(+M1) M1 | 870.222 788.185 720.613 679.516 420.8943 375.0352 214.3395 | 7/2- 5/2- 3/2- 3/2- 3/2- 1/2- 7/2- | |
1482.031 5 | A G | 3/2+ | 478.369 7 693.89 4 761.413 11 867.816 13 | 36 3 20.4 11 100 3 78.9 15 | M1(+E2) E1 E1 | 1003.650 788.185 720.613 614.204 | 5/2+ 5/2- 3/2- 1/2- | |
1491.0 7 | K | (17/2+) | 1052.4 1222.0 | 53 6 100 18 | 438.68 268.92 | 15/2+ 13/2+ | ||
1498 2 | L | 7/2- | ||||||
1509.2 8 | G | |||||||
1520.6 10 | K | (19/2+) | 210.9 | 100 | 1309.8 | (17/2+) | ||
1529 3 | L | 7/2- | ||||||
1530.2 5 | G | 1/2+ | ||||||
1532.277 5 | A G | 5/2+ | 528.626 7 744.079 15 811.65 5 852.798 16 1014.06 13 | 100 4 23.1 12 12.4 21 47.8 23 34 3 | M1 | 1003.650 788.185 720.613 679.516 518.3279 | 5/2+ 5/2- 3/2- 3/2- 5/2- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1534.6 5 | G | (5/2-) | ||||||
1557.4 5 | G L | 1/2,3/2- | ||||||
1570.1 7 | GH | (9/2+) | ||||||
1572.56 3 | A E | 3/2- | 955.82 3 1053.2 1151.63 15 1197.46 8 ? | 100 10 <105 36 4 <123 | E2 M1(+E0) | 616.7562 518.3279 420.8943 375.0352 | 7/2- 5/2- 3/2- 1/2- | |
1580.5 5 | G | |||||||
1582.4 5 | G | |||||||
1586.0 6 | G L | |||||||
1598.4 6 | G | |||||||
1602.3 9 | G L | |||||||
1614.125 13 | A G | 3/2-,1/2- | 463.710 12 825.98 5 1095.77 8 1138.03 16 1239.18 23 | 13.5 10 25 3 100 17 48 8 92 33 | E2(+M1) M1,E2 | 1150.411 788.185 518.3279 476.3341 375.0352 | 1/2+ 5/2- 5/2- 5/2- 1/2- | |
1617.7 16 | K | (21/2-) | 525.0 | 100 | 1092.7 | (17/2-) | ||
1624.3 8 | F K | 25/2+ | 273.4 539.6 | 25 6 100 13 | 1350.7 1084.73 | 23/2+ 21/2+ | ||
1638.7 6 | G L | LE 7/2 | ||||||
1658.4 5 | G L | (1/2-) | ||||||
1665.7 5 | E G | 1/2+ | ||||||
1668.957 6 | A E | 3/2+ | 433.520 9 483.106 7 518.544 9 1293.49 18 | 15.1 7 59 8 100 8 15 | M1 M1 M1 | 1235.440 1185.848 1150.411 375.0352 | 5/2+ 3/2+ 1/2+ 1/2- | |
1672 5 | H | (11/2+,13/2+) | ||||||
1675.3 12 | K | (19/2+) | 365.5 | 100 | 1309.8 | (17/2+) | ||
1679.5+X 8 | K | (23/2+) | 275.0 | 100 | 1404.5+X | (21/2+) | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1687.13 4 | A G | (3/2)- | 816.42 5 966.53 4 1007.57 7 1072.93 9 | 35 5 70 3 100 14 32 7 | M1(+E0) M1(+E0) | 870.222 720.613 679.516 614.204 | 7/2- 3/2- 3/2- 1/2- | |
1687.8+X 10 | K | (19/2-) | 283.3 | 100 | 1404.5+X | (21/2+) | ||
1689 3 | L | 11/2- | ||||||
1698.6 6 | G | |||||||
1702.5 8 | K | (29/2-) | 309.6 597.0 | 100 7 83 10 | 1393.0 1105.74 | (27/2-) 25/2- | ||
1706.062 10 | A E G | (3/2)- | 247.069 4 436.59 4 985.458 25 1024.71 8 1089.40 17 1092.00 13 1187.83 13 1330.95 20 1492.6 7 | 5.3 3 2.2 7 45 3 17 12.4 26 16.9 25 70 2 100 5 5.5 24 | M1+E2 M1+E2 M1 E2 E2(+M1) | 1458.994 1269.445 720.613 681.036 616.7562 614.204 518.3279 375.0352 214.3395 | 3/2- 3/2- 3/2- 9/2- 7/2- 1/2- 5/2- 1/2- 7/2- | |
1713.0 13 | K | (25/2+) | 308.6 | 100 | 1404.5 | (23/2+) | ||
1715.935 5 | A G | 1/2+,3/2+,5/2+ | 183.661 3 233.900 4 466.380 6 565.51 4 | 22.1 11 38.1 12 100 6 13.9 18 | M1+E2 E1 | 1532.277 1482.031 1249.552 1150.411 | 5/2+ 3/2+ 3/2- 1/2+ | |
1725.786 12 | A E G | 3/2- | 456.346 16 876.56 7 937.55 3 1005.24 3 1024.71 8 1046.16 6 1111.55 7 1350.75 9 | 16.3 6 14.0 15 27.9 23 98 15 31 25 100 15 48 | M1 M1 M1 | 1269.445 849.200 788.185 720.613 701.0552 679.516 614.204 375.0352 | 3/2- 7/2- 5/2- 3/2- 5/2- 3/2- 1/2- 1/2- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1731.438 11 | A | 3/2- | 158.94 6 295.104 14 461.935 23 1030.39 4 1051.87 4 1117.23 3 1310.70 8 1356.34 10 | 2.5 11 11.7 17 12.8 8 56 11 65 5 100 11 94 8 67 6 | (E2) M1(+E2) M1(+E2) M1(+E2) (M1) (E2) M1 | 1572.56 1436.353 1269.445 701.0552 679.516 614.204 420.8943 375.0352 | 3/2- 7/2- 3/2- 5/2- 3/2- 1/2- 3/2- 1/2- | |
1748 5 | GH | 11/2+,13/2+ | ||||||
1753.1 10 | K | (21/2+) | 232.9 443.2 | 100 11 21 11 | 1520.6 1309.8 | (19/2+) (17/2+) | ||
1755.337 17 | A E G | 3/2- | 1054.25 3 1141.16 3 1334.23 8 | 100 5 76.4 20 72 7 | M1+E2 M1 E2 | 701.0552 614.204 420.8943 | 5/2- 1/2- 3/2- | |
1756.02 8 | A | 3/2- | 1036.1 1076.70 20 1237.84 12 1279.45 11 1381.2 3 | 28 39 63 100 8 97 22 | E2(+M1) M1 | 720.613 679.516 518.3279 476.3341 375.0352 | 3/2- 3/2- 5/2- 5/2- 1/2- | |
1757.72 11 | A G | (3/2-,5/2+) | 969.49 11 1543.7 3 | 82 8 100 21 | 788.185 214.3395 | 5/2- 7/2- | ||
1762.80 4 | A E G L | (3/2)- | 1042.28 7 1061.63 5 1148.50 16 1244.73 6 1342.6 3 1387.84 6 1548.78 12 | 15.6 17 39 23.2 19 37 49 17 100 10 34 | M1,E2 M1 M1 M1+E2 | 720.613 701.0552 614.204 518.3279 420.8943 375.0352 214.3395 | 3/2- 5/2- 1/2- 5/2- 3/2- 1/2- 7/2- | |
1771 3 | G | |||||||
1783.11 12 | A E G | 1/2,3/2,5/2+ | 779.1 2 1082.4 2 1103.6 2 | 65 13 100 20 38 15 | 1003.650 701.0552 679.516 | 5/2+ 5/2- 3/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1796.5 4 | A G | 1/2,3/2,5/2+ | ||||||
1800.52 7 | A G | 3/2- | 1324.36 13 1379.43 13 1425.49 9 | 52 6 100 11 52 6 | M1(+E2) | 476.3341 420.8943 375.0352 | 5/2- 3/2- 1/2- | |
1811.50 7 | A G | 3/2- | 941.17 13 1110.38 10 1131.86 18 1197.46 8 1293.49 18 1336.6? 1391.09 17 | 6.2 11 78 7 21 3 100 13 24 70 36 4 | M1(+E2) E2(+M1) | 870.222 701.0552 679.516 614.204 518.3279 476.3341 420.8943 | 7/2- 5/2- 3/2- 1/2- 5/2- 5/2- 3/2- | |
1816 4 | L | |||||||
1821.29 7 | A E | (1/2-,3/2) | 1121.0 2 1141.3 2 ? 1207.0 2 1446.16 7 | 100 20 125 25 80 16 | 701.0552 679.516 614.204 375.0352 | 5/2- 3/2- 1/2- 1/2- | ||
1826.9+X 10 | K | (21/2+) | 422.4 | 100 | 1404.5+X | (21/2+) | ||
1829 5 | H | |||||||
1839 3 | G | |||||||
1846.32 15 | A E G | (3/2-) | 975.7 2 1167.2 2 ≈1231.6 | 52 11 100 21 16 6 | 870.222 679.516 614.204 | 7/2- 3/2- 1/2- | ||
1851.504 12 | A G | 3/2+,5/2+ | 319.216 13 847.877 20 | 21.8 9 100 4 | M1(+E2) M1+E2 | 1532.277 1003.650 | 5/2+ 5/2+ | |
1856.0 18 | K | 21/2- | 474.1 | 100 | 1381.9 | 17/2- | ||
1859.2 12 | K | (21/2+) | 549.4 | 100 | 1309.8 | (17/2+) | ||
1861.238 7 | A G | 5/2+ | 328.955 5 547.86 5 740.48 4 782.78 7 787.732 23 857.601 21 926.4 3 1072.93 9 | 14.3 11 13.9 15 24.8 26 17 3 30.8 23 100 4 12 4 33 7 | M1+E0 (E2) M1(+E2) | 1532.277 1313.500 1120.816 1078.349 1073.565 1003.650 935.643 788.185 | 5/2+ 5/2- 9/2+ (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 | |
1877 3 | G | |||||||
1884 3 | G | |||||||
1893.9 5 | A G | 1/2,3/2,5/2+ | ||||||
1899.66 24 | A G | 1/2,3/2,5/2+ | ||||||
1904 3 | GH | (5/2-,7/2-) | ||||||
1913.471 13 | A E G | 3/2- | 480.268 20 599.965 8 644.09 5 678.18 8 1192.95 4 1492.6 7 | 9.2 16 49.2 10 9.8 14 5.7 6 100 14 10 4 | M1 M1 | 1433.189 1313.500 1269.445 1235.440 720.613 420.8943 | 3/2- 5/2- 3/2- 5/2+ 3/2- 3/2- | |
1915.0 18 | K | (23/2-) | 571.2 | 100 | 1343.8 | (19/2-) | ||
1928.846 9 | A E G | 1/2+,3/2+ | 259.889 7 396.602 25 742.91 6 778.39 5 1507.66 18 ? | 30.4 16 7.7 9 75 5 100 6 85 11 | M1+E2 M1(+E0) | 1668.957 1532.277 1185.848 1150.411 420.8943 | 3/2+ 5/2+ 3/2+ 1/2+ 3/2- | |
1941.6 10 | F K | 27/2+ | 317? 591.1 | 100 | 1624.3 1350.7 | 25/2+ 23/2+ | ||
1945.864 14 | A | (1/2,3/2) | 190.513 21 220.080 9 676.13 18 1267.0? 1332.3? 1525.5 3 1571.7 7 | 7 5 8.0 18 18 4 100 17 67 20 | 1755.337 1725.786 1269.445 679.516 614.204 420.8943 375.0352 | 3/2- 3/2- 3/2- 3/2- 1/2- 3/2- 1/2- | ||
1956.1+X 13 | K | (21/2-) | 268 | 100 | 1687.8+X | (19/2-) | ||
1957.58 9 | A | 1/2,3/2,5/2+ | ||||||
1965 3 | G | |||||||
1974.1+X 8 | K | (25/2+) | 294.9 569.6 | 100 14 36 14 | 1679.5+X 1404.5+X | (23/2+) (21/2+) | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1977 3 | G | |||||||
1987 3 | G | |||||||
2007.2 12 | K | (23/2+) | 254.3 486.4 | 100 25 75 25 | 1753.1 1520.6 | (21/2+) (19/2+) | ||
2009 3 | G | |||||||
2011 5 | H | (13/2)+ | ||||||
2021 3 | G | |||||||
2032 3 | G | |||||||
2033.6 10 | K | (31/2-) | 331.3 640.4 | 100 13 22 9 | 1702.5 1393.0 | (29/2-) (27/2-) | ||
2044.1 13 | K | (27/2+) | 331.2 639.4 | 100 13 25 13 | 1713.0 1404.5 | (25/2+) (23/2+) | ||
2047.0 3 | A E G | (1/2,3/2) | 1625.9 1672.0 3 | 77 100 | 420.8943 375.0352 | 3/2- 1/2- | ||
2052.6 15 | A E G | 1/2,3/2,5/2+ | 1332.0 1351.5 | 100 68 | 720.613 701.0552 | 3/2- 5/2- | ||
2070.7 15 | A G | (1/2,3/2) | 1350.4 3 1456.5 1649.78 10 1695.7 | 88 86 100 79 | 720.613 614.204 420.8943 375.0352 | 3/2- 1/2- 3/2- 1/2- | ||
2082.8 15 | A E | (1/2,3/2) | 1078.1 2 ? 1381.7 1403.3? 1606.5 1661.9 1707.8 | <333 23 32 100 99 47 | 1003.650 701.0552 679.516 476.3341 420.8943 375.0352 | 5/2+ 5/2- 3/2- 5/2- 3/2- 1/2- | ||
2088.4 15 | A G | (1/2,3/2) | 1408.9 1713.4 | 43 100 | 679.516 375.0352 | 3/2- 1/2- | ||
2093.40 20 | E G | 1305.3 2 ? 1672.5 2 | 27 6 100 21 | 788.185 420.8943 | 5/2- 3/2- | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2133.2 16 ? | K | (23/2+) | 274? | 100 | 1859.2 | (21/2+) | ||
2146.1 15 | A E G | (1/2,3/2) | 1445.0 1531.9 | 57 100 | 701.0552 614.204 | 5/2- 1/2- | ||
2150.3 6 | A G | 1/2(-),3/2,5/2+ | 1429.7 1674.0 1729.4 | 39 100 92 | 720.613 476.3341 420.8943 | 3/2- 5/2- 3/2- | ||
2168.2 8 | A E G | 1/2,3/2,5/2+ | ||||||
2183.1 7 | A E G | 1/2,3/2,5/2+ | 1462.5 1503.6 ≈1707.0? | 100 71 | 720.613 679.516 476.3341 | 3/2- 3/2- 5/2- | ||
2214.4 3 | A G | (1/2,3/2) | 1600.1 3 1840.6 | 83 100 | 614.204 375.0352 | 1/2- 1/2- | ||
2228.1 4 | A G | 1/2,3/2,5/2+ | 1507.66 18 1548.78 12 1807.3 | 78 34 100 | 720.613 679.516 420.8943 | 3/2- 3/2- 3/2- | ||
2242.5 11 ? | F | (29/2+) | 301? 618? | | 1941.6 1624.3 | 27/2+ 25/2+ | ||
2243.5+X 13 ? | K | (23/2-) | 287? 556? | ≤100 ≤100 | 1956.1+X 1687.8+X | (21/2-) (19/2-) | ||
2249.97 20 | A G | (3/2-) | 1461.4 1529.0 1875.3 4 2035.53 23 | 41 36 95 100 | 788.185 720.613 375.0352 214.3395 | 5/2- 3/2- 1/2- 7/2- | ||
2254.2 15 | A G | 1/2(-),3/2,5/2+ | 1735.9 1833.3 | 100 99 | 518.3279 420.8943 | 5/2- 3/2- | ||
2281.1 16 | K | (25/2+) | 273.9 | 100 | 2007.2 | (23/2+) | ||
2282 3 | G | |||||||
2287.2+X 10 | K | (27/2+) | 313.2 607.5 | 100 17 100 33 | 1974.1+X 1679.5+X | (25/2+) (23/2+) | ||
2297 3 | G J | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2309.2 15 | A J | 1/2,3/2,5/2+ | 1588.6 1888.3 | 91 100 | 720.613 420.8943 | 3/2- 3/2- | ||
2354 3 | G | |||||||
2366.9 15 | A | (1/2-,3/2) | 1646.3 1687.4 1752.7 1848.6 1890.6 1946.0 1991.9 | 20 12 13 13 100 22 28 | 720.613 679.516 614.204 518.3279 476.3341 420.8943 375.0352 | 3/2- 3/2- 1/2- 5/2- 5/2- 3/2- 1/2- | ||
2386.3 11 | K | (33/2-) | 352.8 683.9 | 100 25 100 25 | 2033.6 1702.5 | (31/2-) (29/2-) | ||
2394.2 15 | A G J | 1/2(-),3/2,5/2+ | 1606.0 1714.7 3 1973.3 | 21 19 100 | 788.185 679.516 420.8943 | 5/2- 3/2- 3/2- | ||
2395.1 20 | K | 25/2- | 539.1 | 100 | 1856.0 | 21/2- | ||
2396.5 14 | K | (29/2+) | 352.5 683.5 | 100 14 29 14 | 2044.1 1713.0 | (27/2+) (25/2+) | ||
2415.5 3 | A G | (1/2-,3/2) | 1627.7 5 1800.7 1938.6 1994.0 | 28 77 60 100 | 788.185 614.204 476.3341 420.8943 | 5/2- 1/2- 5/2- 3/2- | ||
2425.3 7 | A G | (1/2-,3/2) | 1724.2 1811.1 | 92 100 | 701.0552 614.204 | 5/2- 1/2- | ||
2451.31 23 | A G | (3/2-) | 1771.5 1836.8 2030.1 2236.97 23 | 23 64 100 24 | 679.516 614.204 420.8943 214.3395 | 3/2- 1/2- 3/2- 7/2- | ||
2456.7 11 | K | (29/2-) | 1351 | 100 | 1105.74 | 25/2- | ||
2460.3 15 | A G | (1/2,3/2) | 2039.4 2085.3 | 100 73 | 420.8943 375.0352 | 3/2- 1/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2475.5 15 | A | (3/2-) | 1774.4 1861.3 2054.6 2100.5 2261.2 | 18 35 100 87 12 | 701.0552 614.204 420.8943 375.0352 214.3395 | 5/2- 1/2- 3/2- 1/2- 7/2- | ||
2497 3 | G J | 7/2+,9/2+,11/2+ | ||||||
2509.5 15 | A | (1/2,3/2) | 1830.0 2088.6 2134.5 | 30 86 100 | 679.516 420.8943 375.0352 | 3/2- 3/2- 1/2- | ||
2522.7 15 | A G | (1/2-,3/2) | 2046.4 2101.8 2147.7 | 76 56 100 | 476.3341 420.8943 375.0352 | 5/2- 3/2- 1/2- | ||
2549.6 13 | K | (33/2-) | 30 ns 10 | 91? 516? 847.1 | <6 100 13 | [E2] [M1] [E2] | 2456.7 2033.6 1702.5 | (29/2-) (31/2-) (29/2-) |
2556 3 | G J | 7/2+,9/2+,11/2+ | ||||||
2590 | G | |||||||
2601.2 3 | A G | (1/2-,3/2) | 2124.9 2180.3 2226.2 | 29 93 100 | 476.3341 420.8943 375.0352 | 5/2- 3/2- 1/2- | ||
2610.7 5 | A G | (1/2-,3/2) | 1996.6 3 2092.4 2189.66 19 2235.7 | 21 20 29 100 | 614.204 518.3279 420.8943 375.0352 | 1/2- 5/2- 3/2- 1/2- | ||
2617.6 15 ? | F | (31/2+) | 676? | 100 | 1941.6 | 27/2+ | ||
2638.8 3 | A | (1/2,3/2) | 1918.2 3 2263.3 | 66 100 | 720.613 375.0352 | 3/2- 1/2- | ||
2640 15 | J | |||||||
2654.13 24 | A G | (1/2-,3/2) | 1865.94 24 1932.5 2134.8 2278.1 | 97 72 92 100 | 788.185 720.613 518.3279 375.0352 | 5/2- 3/2- 5/2- 1/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2655 5 | GH | (13/2)+ | ||||||
2702.9 15 | A G | (1/2-,3/2) | 2184.6 2327.9 | 61 100 | 518.3279 375.0352 | 5/2- 1/2- | ||
2705 15 | G J | 7/2+,9/2+,11/2+ | ||||||
2727 | G | |||||||
2743.69 21 | A G | (1/2-,3/2) | 2042.7 2126.96 21 2321.9 | 61 62 100 | 701.0552 616.7562 420.8943 | 5/2- 7/2- 3/2- | ||
2759.6 12 | K | (35/2-) | 373.5 725.8 | 100 50 50 50 | 2386.3 2033.6 | (33/2-) (31/2-) | ||
2769.6 15 | K | (31/2+) | 373.2 725.5 | 25 25 100 25 | 2396.5 2044.1 | (29/2+) (27/2+) | ||
2788 3 | G | |||||||
2857 | G J | 9/2+ | ||||||
2898.0 15 | K | (35/2-) | 348.4 | 100 | 2549.6 | (33/2-) | ||
2905.2 15 | A | (1/2,3/2) | 2184.5 2225.7 2484.3 2530.2 | 50 42 92 100 | 720.613 679.516 420.8943 375.0352 | 3/2- 3/2- 3/2- 1/2- | ||
2921 3 | G J | |||||||
2950 3 | G J | |||||||
2969 | G | |||||||
2983.3 15 | A G | 1/2(-),3/2,5/2+ | 2303.8 2507.0 | 38 100 | 679.516 476.3341 | 3/2- 5/2- | ||
3030 15 | J | |||||||
3076.2 3 | A | (1/2-,3/2) | 2397.7 2463.0 2559.7 5 | 38 42 100 | 679.516 614.204 518.3279 | 3/2- 1/2- 5/2- | ||
3095 15 | J | 9/2+ | ||||||
3148.8 5 | A | (1/2-,3/2) | 2447.7 5 2534.9 | 55 100 | 701.0552 614.204 | 5/2- 1/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3151.5 13 ? | K | (37/2-) | 392? 765? | | 2759.6 2386.3 | (35/2-) (33/2-) | ||
3155 15 | J | 7/2+,9/2+,11/2+ | ||||||
3161.6 16 ? | K | (33/2+) | 392? 765? | | 2769.6 2396.5 | (31/2+) (29/2+) | ||
3177.9 3 | A | 1/2(-),3/2,5/2+ | 2459.0 2703.3 | 87 100 | 720.613 476.3341 | 3/2- 5/2- | ||
3240 15 | J | 7/2+,9/2+,11/2+ | ||||||
3268.2 15 | K | (37/2-) | 370.4 718.5 | 100 25 50 25 | 2898.0 2549.6 | (35/2-) (33/2-) | ||
3345.4 3 | A | 1/2(-),3/2,5/2+ | 2644.3 3 2924.3 | 62 100 | 701.0552 420.8943 | 5/2- 3/2- | ||
3347.2 4 | A | (1/2,3/2) | 2668.2 2972.7 | 58 100 | 679.516 375.0352 | 3/2- 1/2- | ||
3360 15 | J | 7/2+,9/2+,11/2+ | ||||||
3373.6 18 ? | F | (35/2+) | 756? | 100 | 2617.6 | (31/2+) | ||
3409.5 15 | A | (1/2,3/2) | 2729.9 3034.4 | 100 79 | 679.516 375.0352 | 3/2- 1/2- | ||
3439.2 18 | K | (39/2-) | 12 ns 6 | 171.0 | 100 | (M1,E2) | 3268.2 | (37/2-) |
3490 15 | J | |||||||
3659.1 17 ? | K | (39/2-) | 391? 761? | | 3268.2 2898.0 | (37/2-) (35/2-) | ||
3775.2 21 | K | (43/2+) | 15 µs 5 | 336.0 | 100 | (M2) | 3439.2 | (39/2-) |
4204.7 20 ? | F | (39/2+) | 831? | 100 | 3373.6 | (35/2+) |
E(level): From least-squares fit to Eγ, assigning ΔE=1 keV to data for which authors did not state uncertainty and excluding uncertain or multiply-placed transitions, except as noted.
Jπ(level): Assignments given without comment are based on γ multipolarities, γ decay patterns, g-factor analysis, calculated bandhead energies and observed band structure in 176Yb(9Be,α2nγ)
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - Kπ=17/2+ band (2000Mu06). | |||||||
1309.8 6 | (17/2+) | 3 ns 1 | |||||
1520.6 10 | (19/2+) | 210.9 | 100 | 1309.8 | (17/2+) | ||
1753.1 10 | (21/2+) | 232.9 443.2 | 100 11 21 11 | 1520.6 1309.8 | (19/2+) (17/2+) | ||
2007.2 12 | (23/2+) | 254.3 486.4 | 100 25 75 25 | 1753.1 1520.6 | (21/2+) (19/2+) | ||
2281.1 16 | (25/2+) | 273.9 | 100 | 2007.2 | (23/2+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - 9/2[624] band. | |||||||
0.0 | 9/2+ | STABLE | |||||
122.7904 24 | 11/2+ | 37 ps 3 | 122.793 3 | 100 | M1+E2 | 0.0 | 9/2+ |
268.92 6 | 13/2+ | 21 ps 3 | 146.15 7 268.85 14 | 100 4 39.4 4 | M1+E2 E2 | 122.7904 0.0 | 11/2+ 9/2+ |
438.68 8 | 15/2+ | 169.77 9 315.88 11 | 96 4 100 | M1+E2 E2 | 268.92 122.7904 | 13/2+ 11/2+ | |
631.30 10 | 17/2+ | 192.62 11 362.39 13 | 54 5 100.0 22 | M1+E2 E2 | 438.68 268.92 | 15/2+ 13/2+ | |
848.37 12 | 19/2+ | 217.07 13 409.68 15 | 42 3 100.0 25 | M1+E2 E2 | 631.30 438.68 | 17/2+ 15/2+ | |
1084.73 15 | 21/2+ | 236.36 14 453.43 17 | 27.7 8 100 4 | M1+E2 E2 | 848.37 631.30 | 19/2+ 17/2+ | |
1350.7 7 | 23/2+ | 266.0 502.3 | 33 3 100 7 | 1084.73 848.37 | 21/2+ 19/2+ | ||
1624.3 8 | 25/2+ | 273.4 539.6 | 25 6 100 13 | 1350.7 1084.73 | 23/2+ 21/2+ | ||
1941.6 10 | 27/2+ | 317? 591.1 | 100 | 1624.3 1350.7 | 25/2+ 23/2+ | ||
2242.5 11 | (29/2+) | 301? 618? | | 1941.6 1624.3 | 27/2+ 25/2+ | ||
2617.6 15 | (31/2+) | 676? | 100 | 1941.6 | 27/2+ | ||
3373.6 18 | (35/2+) | 756? | 100 | 2617.6 | (31/2+) | ||
4204.7 20 | (39/2+) | 831? | 100 | 3373.6 | (35/2+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - 7/2[514] band. | |||||||
214.3395 22 | 7/2- | 1.85 ns 4 | |||||
337.7178 23 | 9/2- | 123.3790 20 214.930 3 337.713 5 | 100 4 78 4 21.2 9 | E2 [E1] E1 | 214.3395 122.7904 0.0 | 7/2- 11/2+ 9/2+ | |
487.709 5 | (11/2-) | 150.019 15 273.368 4 487.704 11 | 21.5 15 100 5 52 17 | 337.7178 214.3395 0.0 | 9/2- 7/2- 9/2+ | ||
664.3 7 | (13/2-) | 176.3 326.8 | 0.7 7 100 5 | 487.709 337.7178 | (11/2-) 9/2- | ||
865.9 10 | (15/2-) | 378.2 | 100 | (E2) | 487.709 | (11/2-) | |
1092.7 13 | (17/2-) | 428.4 | 100 | 664.3 | (13/2-) | ||
1343.8 15 | (19/2-) | 477.9 | 100 | 865.9 | (15/2-) | ||
1617.7 16 | (21/2-) | 525.0 | 100 | 1092.7 | (17/2-) | ||
1915.0 18 | (23/2-) | 571.2 | 100 | 1343.8 | (19/2-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - 1/2[510] band. | |||||||
375.0352 25 | 1/2- | 18.67 s 4 % IT = 100 | |||||
420.8943 25 | 3/2- | 45.8610 10 | 100 | M1+E2 | 375.0352 | 1/2- | |
476.3341 25 | 5/2- | 55.4420 10 101.2980 10 262.02 3 | 100 1 90 5 0.22 6 | M1 E2 | 420.8943 375.0352 214.3395 | 3/2- 1/2- 7/2- | |
582.230 3 | 7/2- | 105.899 3 161.3390 20 367.891 17 | 100 2 19.0 8 0.55 9 | M1 (E2) | 476.3341 420.8943 214.3395 | 5/2- 3/2- 7/2- | |
681.036 3 | 9/2- | 98.808 12 204.696 3 | 15 4 100.0 22 | E2 | 582.230 476.3341 | 7/2- 5/2- | |
842.9 10 | 11/2- | 260.7 | 100 | 582.230 | 7/2- | ||
985.7 10 | 13/2- | 304.7 | 100 | 681.036 | 9/2- | ||
1196.2 15 | 15/2- | 353.3 | 100 | 842.9 | 11/2- | ||
1381.9 15 | 17/2- | 396.2 | 100 | 985.7 | 13/2- | ||
1856.0 18 | 21/2- | 474.1 | 100 | 1381.9 | 17/2- | ||
2395.1 20 | 25/2- | 539.1 | 100 | 1856.0 | 21/2- | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 5 - 5/2[512] band. | |||||||
518.3279 24 | 5/2- | < 0.2 ns | |||||
616.7562 25 | 7/2- | 98.433 2 140.4260 20 195.861 6 279.029 4 402.409 6 616.768 9 | 100 1 10.8 7 2.05 24 75.9 8 37.2 7 22.9 19 | M1+E2 M1+E2 M1+E2 M1+E2 | 518.3279 476.3341 420.8943 337.7178 214.3395 0.0 | 5/2- 5/2- 3/2- 9/2- 7/2- 9/2+ | |
742.710 3 | 9/2- | 125.957 1 224.367 4 619.90 5 | 100 9 23.4 19 12 6 | M1+E2 | 616.7562 518.3279 122.7904 | 7/2- 5/2- 11/2+ | |
896.7 7 | 11/2- | 153.5 280.1 | 88 13 100 13 | 742.710 616.7562 | 9/2- 7/2- | ||
1076.6 8 | 13/2- | 179.5 334.2 | 83 17 100 17 | 896.7 742.710 | 11/2- 9/2- | ||
1283.7 10 | 15/2- | 207.2 387 | 100 60 60 20 | 1076.6 896.7 | 13/2- 11/2- | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 6 - 1/2[521] band. | |||||||
614.204 3 | 1/2- | 0.50 ns 15 | |||||
679.516 3 | 3/2- | 161.191 2 203.182 3 258.615 3 304.465 7 | 100 3 16.7 3 75 5 7.3 7 | M1 M1+E2 M1+E2 M1 | 518.3279 476.3341 420.8943 375.0352 | 5/2- 5/2- 3/2- 1/2- | |
701.0552 25 | 5/2- | 84.2970 10 86.857 5 118.8260 10 182.7350 20 224.715 3 280.154 4 326.010 14 486.735 14 | 13.2 8 5.5 7 100 3 25.2 5 6.5 7 4.82 15 35.6 15 12.6 11 | M1+E2 E2 M1+E2 M1+E2 M1(+E0) M1+E2 E2 M1 | 616.7562 614.204 582.230 518.3279 476.3341 420.8943 375.0352 214.3395 | 7/2- 1/2- 7/2- 5/2- 5/2- 3/2- 1/2- 7/2- | |
849.200 3 | 7/2- | 106.492 1 148.148 4 168.162 2 169.675 4 232.439 3 266.974 4 330.856 9 372.853 5 428.292 6 634.94 4 | 12.4 15 6.8 15 13.8 7 15.0 9 47.6 18 35.9 18 10.6 5 71.4 7 12.9 15 100 12 | M1+E2 M1 E2 M1+E2 M1(+E2) M1 (E2) M1+E2 | 742.710 701.0552 681.036 679.516 616.7562 582.230 518.3279 476.3341 420.8943 214.3395 | 9/2- 5/2- 9/2- 3/2- 7/2- 7/2- 5/2- 5/2- 3/2- 7/2- | |
912.0 10 | 9/2- | 210.9 | 100 | 701.0552 | 5/2- | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 7 - 3/2[512] band. | |||||||
720.613 3 | 3/2- | ≤ 0.3 ns | |||||
788.185 3 | 5/2- | 87.127 13 108.678 4 171.432 2 173.977 3 205.950 3 269.857 4 311.844 4 413.132 7 450.47 3 573.825 22 | 2.6 13 3.6 6 100 1 5.0 3 53.3 10 94 7 21.4 9 43.6 9 2.9 3 41.1 24 | M1+E2 E2 M1+E2 M1+E0 M1(+E2) E2 M1 | 701.0552 679.516 616.7562 614.204 582.230 518.3279 476.3341 375.0352 337.7178 214.3395 | 5/2- 3/2- 7/2- 1/2- 7/2- 5/2- 5/2- 1/2- 9/2- 7/2- | |
935.643 3 | 7/2- | 147.458 3 192.933 3 215? 318.887 4 353.425 6 459.287 9 | 33 5 43 4 <10 100.0 24 76 4 30.1 24 | M1 M1+E2 M1 M1(+E2) | 788.185 742.710 720.613 616.7562 582.230 476.3341 | 5/2- 9/2- 3/2- 7/2- 7/2- 5/2- | |
1030.8 6 | 9/2- | ||||||
1255.8 10 | 11/2- | 320.2 | 100 | 935.643 | 7/2- | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 8 - Kπ=5/2+ K-2 G-VIBRATION band. | |||||||
1003.650 4 | 5/2+ | ||||||
1078.349 10 | (7/2)+ | 357.731 11 863.98 15 1078.37 8 | 2.71 22 7.1 21 100 4 | E2(+M1) | 720.613 214.3395 0.0 | 3/2- 7/2- 9/2+ | |
1176.2 9 | (9/2+) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 9 - 7/2[503] band. | |||||||
870.222 8 | 7/2- | ||||||
992.0 15 | (9/2-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 10 - Kπ=3/2+ (1/2[521]+1-) band. | |||||||
1482.031 5 | 3/2+ | ||||||
1532.277 5 | 5/2+ | 528.626 7 744.079 15 811.65 5 852.798 16 1014.06 13 | 100 4 23.1 12 12.4 21 47.8 23 34 3 | M1 | 1003.650 788.185 720.613 679.516 518.3279 | 5/2+ 5/2- 3/2- 3/2- 5/2- | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 11 - 7/2[633] band. | |||||||
1105.92 9 | (7/2+) | ||||||
1168.95 3 | (9/2+) | 831.24 3 953.9 3 1046.16 6 1168.4 3 | 67.0 26 35 11 100 21 36 11 | 337.7178 214.3395 122.7904 0.0 | 9/2- 7/2- 11/2+ 9/2+ | ||
1282.5 9 | (11/2+) | ||||||
1359.0 5 | (13/2)+ | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 12 - Kπ=9/2+ [9/2[624]+0+] GS B-VIBRATIONAL band. | |||||||
1120.816 19 | 9/2+ | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 13 - Kπ=1/2+ (1/2[510]-1-) band. | |||||||
1150.411 5 | 1/2+ | ||||||
1185.848 5 | 3/2+ | 182.178 11 397.67 3 465.222 6 484.799 15 506.299 20 571.653 14 709.527 18 764.968 11 810.831 12 | 1.19 16 0.70 13 18.8 10 17.8 18 ≤4.4 53 3 9.3 4 91 3 100.0 22 | (E1) (E1) E1+M2 E1 E1 | 1003.650 788.185 720.613 701.0552 679.516 614.204 476.3341 420.8943 375.0352 | 5/2+ 5/2- 3/2- 5/2- 3/2- 1/2- 5/2- 3/2- 1/2- | |
1235.440 4 | 5/2+ | 231.809 6 386.244 6 514.827 10 534.394 12 555.888 11 653.190 13 759.060 14 | 3.66 25 17.3 3 9.1 26 6.2 3 6.5 6 100 4 22.9 7 | (E1) E1 (E1) | 1003.650 849.200 720.613 701.0552 679.516 582.230 476.3341 | 5/2+ 7/2- 3/2- 5/2- 3/2- 7/2- 5/2- | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 14 - Kπ=3/2- [7/2[514]-2+] γ-vibrational band. | |||||||
1249.552 6 | 3/2- | ||||||
1313.500 13 | 5/2- | 633.967 22 696.74 5 699.15 8 731.22 3 795.27 6 975.72 6 1099.26 7 | 15.0 14 12.3 10 5.6 10 57 3 13.8 24 100 6 92 12 | M1+E2 E2 E2(+M1) | 679.516 616.7562 614.204 582.230 518.3279 337.7178 214.3395 | 3/2- 7/2- 1/2- 7/2- 5/2- 9/2- 7/2- | |
1405.2 6 | (7/2-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 15 - 3/2[521] band. | |||||||
1269.445 6 | 3/2- | ||||||
1428.6 5 | (7/2-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 16 - 3/2[501] band. | |||||||
1458.994 9 | 3/2- | ||||||
1534.6 5 | (5/2-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 17 - 1/2[501] band. | |||||||
1658.4 5 | (1/2-) | ||||||
1706.062 10 | (3/2)- | 247.069 4 436.59 4 985.458 25 1024.71 8 1089.40 17 1092.00 13 1187.83 13 1330.95 20 1492.6 7 | 5.3 3 2.2 7 45 3 17 12.4 26 16.9 25 70 2 100 5 5.5 24 | M1+E2 M1+E2 M1 E2 E2(+M1) | 1458.994 1269.445 720.613 681.036 616.7562 614.204 518.3279 375.0352 214.3395 | 3/2- 3/2- 3/2- 9/2- 7/2- 1/2- 5/2- 1/2- 7/2- |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
122.7904 | 11/2+ | 37 ps 3 | 122.793 3 | M1+E2 | -0.27 3 | 2.18 | B(E2)(W.u.)=245 14, B(M1)(W.u.)=0.094 8, α=2.18 4 |
214.3395 | 7/2- | 1.85 ns 4 | 214.335 3 | E1 | 0.063 | B(E1)(W.u.)=1.110E-5 25, α=0.063 4 | |
268.92 | 13/2+ | 21 ps 3 | 146.15 7 | M1+E2 | -0.39 4 | 1.291 | B(E2)(W.u.)=320 80, B(M1)(W.u.)=0.106 17, α=1.291 22 |
13/2+ | 21 ps 3 | 268.85 14 | E2 | 0.1107 | B(E2)(W.u.)=49 6, α=0.1107 | ||
337.7178 | 9/2- | 123.3790 20 | E2 | 1.582 | α=1.582 | ||
9/2- | 214.930 3 | [E1] | 0.0491 | α=0.0491 | |||
9/2- | 337.713 5 | E1 | 0.01607 | α=0.01607 | |||
375.0352 | 1/2- | 18.67 s 4 % IT = 100 | 160.696 2 | M3 | 34.1 | B(M3)(W.u.)=0.0364 9, α=34.1 | |
1/2- | 18.67 s 4 % IT = 100 | ≈375 | [M4] | 3.57 | B(M4)(W.u.)≈0.14, α=3.57 | ||
420.8943 | 3/2- | 45.8610 10 | M1+E2 | 0.117 +22-26 | 7.9 | α=7.9 6 | |
438.68 | 15/2+ | 169.77 9 | M1+E2 | -0.33 5 | 0.852 | α=0.852 17 | |
15/2+ | 315.88 11 | E2 | 0.0679 | α=0.0679 | |||
476.3341 | 5/2- | 55.4420 10 | M1 | 3.74 | α=3.74 | ||
5/2- | 101.2980 10 | E2 | 3.35 | α=3.35 | |||
518.3279 | 5/2- | < 0.2 ns | 41.9960 10 | M1(+E2) | 0.13 +6-11 | 11 | B(M1)(W.u.)>0.0023, α=11 3 |
5/2- | < 0.2 ns | 97.4350 20 | M1+E2 | 0.28 +10-14 | 4.29 | B(E2)(W.u.)>0.93, B(M1)(W.u.)>0.00074, α=4.29 7 | |
5/2- | < 0.2 ns | 143.301 9 | (E2) | 0.914 | B(E2)(W.u.)>0.68, α=0.914 | ||
5/2- | < 0.2 ns | 180.613 2 | E2 | 0.406 | B(E2)(W.u.)>1.6, α=0.406 | ||
5/2- | < 0.2 ns | 303.977 4 | M1+E2 | 0.62 +7-6 | 0.151 | B(E2)(W.u.)>3.4, B(M1)(W.u.)>0.0021, α=0.151 5 | |
582.230 | 7/2- | 105.899 3 | M1 | 3.40 | α=3.40 | ||
7/2- | 161.3390 20 | (E2) | 0.600 | α=0.600 | |||
614.204 | 1/2- | 0.50 ns 15 | 137.873 2 | E2 | 1.051 | B(E2)(W.u.)=1.5 5, α=1.051 | |
1/2- | 0.50 ns 15 | 193.310 2 | M1+E2 | 0.59 4 | 0.543 | B(E2)(W.u.)=10 4, B(M1)(W.u.)=0.0025 8, α=0.543 11 | |
1/2- | 0.50 ns 15 | 239.165 3 | M1 | 0.344 | B(M1)(W.u.)=0.00030 10, α=0.344 | ||
616.7562 | 7/2- | 98.433 2 | M1+E2 | 0.35 4 | 4.14 | α=4.14 | |
7/2- | 140.4260 20 | M1+E2 | 0.40 +15-19 | 1.45 | α=1.45 6 | ||
7/2- | 279.029 4 | M1+E2 | 0.69 +12-11 | 0.185 | α=0.185 10 | ||
7/2- | 402.409 6 | M1+E2 | 1.28 8 | 0.0534 | α=0.0534 18 | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
631.30 | 17/2+ | 192.62 11 | M1+E2 | -0.26 6 | 0.607 | α=0.607 13 | |
17/2+ | 362.39 13 | E2 | 0.0457 | α=0.0457 | |||
679.516 | 3/2- | 161.191 2 | M1 | 1.030 | α=1.030 | ||
3/2- | 203.182 3 | M1+E2 | 0.70 6 | 0.452 | α=0.452 12 | ||
3/2- | 258.615 3 | M1+E2 | 0.53 13 | 0.244 | α=0.244 14 | ||
3/2- | 304.465 7 | M1 | 0.1785 | α=0.1785 | |||
681.036 | 9/2- | 204.696 3 | E2 | 0.266 | α=0.266 | ||
701.0552 | 5/2- | 84.2970 10 | M1+E2 | 2.6 3 | 6.93 | α=6.93 | |
5/2- | 86.857 5 | E2 | 6.18 | α=6.18 | |||
5/2- | 118.8260 10 | M1+E2 | 0.36 8 | 2.37 | α=2.37 5 | ||
5/2- | 182.7350 20 | M1+E2 | 0.67 6 | 0.621 | α=0.621 16 | ||
5/2- | 280.154 4 | M1+E2 | 0.5 +3-4 | 0.198 | α=0.198 25 | ||
5/2- | 326.010 14 | E2 | 0.0619 | α=0.0619 | |||
5/2- | 486.735 14 | M1 | 0.0516 | α=0.0516 | |||
720.613 | 3/2- | ≤ 0.3 ns | 106.409 1 | M1(+E2) | 0.37 LE | 3.32 | B(M1)(W.u.)>0.00060, α=3.32 6 |
3/2- | ≤ 0.3 ns | 202.283 3 | M1+E2 | 0.57 4 | 0.480 | B(E2)(W.u.)>8.7, B(M1)(W.u.)>0.0028, α=0.480 10 | |
3/2- | ≤ 0.3 ns | 244.278 8 | M1(+E2) | 0.7 LE | 0.30 | B(M1)(W.u.)>0.00014, α=0.30 3 | |
3/2- | ≤ 0.3 ns | 299.716 4 | M1+E2 | 1.53 6 | 0.1114 | B(E2)(W.u.)>1.5, B(M1)(W.u.)>0.00013, α=0.1114 24 | |
3/2- | ≤ 0.3 ns | 345.575 5 | M1+E2 | 0.64 4 | 0.1054 | B(E2)(W.u.)>0.070, B(M1)(W.u.)>5.0E-5, α=0.1054 25 | |
3/2- | ≤ 0.3 ns | 506.299 20 | (E2) | 0.0187 | B(E2)(W.u.)>0.019, α=0.0187 | ||
742.710 | 9/2- | 125.957 1 | M1+E2 | 0.67 +20-19 | 1.88 | α=1.88 8 | |
788.185 | 5/2- | 171.432 2 | M1+E2 | 0.67 4 | 0.748 | α=0.748 15 | |
5/2- | 173.977 3 | E2 | 0.461 | α=0.461 | |||
5/2- | 205.950 3 | M1+E2 | 0.84 6 | 0.412 | α=0.412 11 | ||
5/2- | 311.844 4 | M1(+E2) | 0.43 LE | 0.160 | α=0.160 8 | ||
5/2- | 413.132 7 | E2 | 0.0318 | α=0.0318 | |||
5/2- | 573.825 22 | M1 | 0.0337 | α=0.0337 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
848.37 | 19/2+ | 217.07 13 | M1+E2 | -0.37 3 | 0.421 | α=0.421 8 | |
19/2+ | 409.68 15 | E2 | 0.0325 | α=0.0325 | |||
849.200 | 7/2- | 106.492 1 | M1+E2 | 1.0 +4-3 | 3.05 | α=3.05 11 | |
7/2- | 148.148 4 | M1 | 1.306 | α=1.306 | |||
7/2- | 169.675 4 | E2 | 0.503 | α=0.503 | |||
7/2- | 232.439 3 | M1+E2 | 1.04 +14-12 | 0.270 | α=0.270 13 | ||
7/2- | 266.974 4 | M1(+E2) | 0.18 | α=0.18 7 | |||
7/2- | 372.853 5 | M1 | 0.1038 | α=0.1038 | |||
7/2- | 428.292 6 | (E2) | 0.0289 | α=0.0289 | |||
7/2- | 634.94 4 | M1+E2 | 0.018 | α=0.018 8 | |||
865.9 | (15/2-) | 378.2 | (E2) | 0.0405 | α=0.0405 | ||
870.222 | 7/2- | 532.49 4 | M1 | 0.0409 | α=0.0409 | ||
7/2- | 655.888 20 | M1(+E2) | 0.017 | α=0.017 7 | |||
7/2- | 870.243 13 | E1 | 0.00212 | α=0.00212 3 | |||
935.643 | 7/2- | 147.458 3 | M1 | 1.324 | α=1.324 | ||
7/2- | 318.887 4 | M1+E2 | 0.71 +20-18 | 0.127 | α=0.127 11 | ||
7/2- | 353.425 6 | M1 | 0.1197 | α=0.1197 | |||
7/2- | 459.287 9 | M1(+E2) | 0.042 | α=0.042 18 | |||
1003.650 | 5/2+ | 789.188 20 | (E1) | 0.00256 | α=0.00256 4 | ||
5/2+ | 1003.690 23 | E2 | 0.00406 | α=0.00406 6 | |||
1073.565 | 7/2- | 735.83 5 | M1+E2 | 1.1 +9-4 | 0.012 | α=0.012 3 | |
7/2- | 859.254 16 | M1+E2 | 0.43 +11-13 | 0.0111 | α=0.0111 5 | ||
1078.349 | (7/2)+ | 1078.37 8 | E2(+M1) | 0.0052 | α=0.0052 17 | ||
1084.73 | 21/2+ | 236.36 14 | M1+E2 | -0.30 3 | 0.340 | α=0.340 6 | |
21/2+ | 453.43 17 | E2 | 0.0249 | α=0.0249 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
1105.74 | 25/2- | 25.05 d 25 % IT = 100 | 21.01 12 | M2 | 1.15×104 | B(M2)(W.u.)=9.1×10-12 10, α=1.15E4 4 | |
25/2- | 25.05 d 25 % IT = 100 | 257.37 15 | E3 | 0.669 | B(E3)(W.u.)=1.28E-10 23, α=0.669 | ||
1120.816 | 9/2+ | 998.06 10 | M1+E2 | 0.9 +13-6 | 0.0065 | α=0.0065 17 | |
1150.411 | 1/2+ | 429.800 6 | (E1) | 0.00919 | α=0.00919 13 | ||
1/2+ | 470.891 7 | E1 | 0.00749 | α=0.00749 11 | |||
1/2+ | 729.517 10 | E1 | 0.00299 | α=0.00299 5 | |||
1185.848 | 3/2+ | 465.222 6 | (E1) | 0.00769 | α=0.00769 11 | ||
3/2+ | 484.799 15 | (E1) | 0.00702 | α=0.00702 10 | |||
3/2+ | 571.653 14 | E1+M2 | 0.10 3 | 0.0059 | α=0.0059 7 | ||
3/2+ | 764.968 11 | E1 | 0.00272 | α=0.00272 4 | |||
3/2+ | 810.831 12 | E1 | 0.00243 | α=0.00243 4 | |||
1235.440 | 5/2+ | 386.244 6 | (E1) | 0.01173 | α=0.01173 | ||
5/2+ | 653.190 13 | E1 | 0.00374 | α=0.00374 6 | |||
5/2+ | 759.060 14 | (E1) | 0.00277 | α=0.00277 4 | |||
1249.552 | 3/2- | 548.508 15 | M1 | 0.0379 | α=0.0379 | ||
3/2- | 570.036 8 | M1 | 0.0343 | α=0.0343 | |||
3/2- | 635.26 4 | M1(+E2) | 0.018 | α=0.018 8 | |||
3/2- | 773.15 5 | E2+M1 | 0.9 +13-7 | 0.012 | α=0.012 4 | ||
3/2- | 1035.197 15 | E2 | 0.00381 | α=0.00381 6 | |||
1269.445 | 3/2- | 548.858 21 | M1+E2 | 0.027 | α=0.027 12 | ||
3/2- | 568.382 8 | M1 | 0.0345 | α=0.0345 | |||
3/2- | 589.923 8 | M1+E2 | 0.55 23 | 0.027 | α=0.027 3 | ||
3/2- | 655.256 19 | M1+E2 | 0.70 +10-9 | 0.0194 | α=0.0194 9 | ||
3/2- | 751.14 3 | M1 | 0.01699 | α=0.01699 | |||
3/2- | 1055.06 5 | (E2) | 0.00367 | α=0.00367 6 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
1309.8 | (17/2+) | 3 ns 1 | 678.4 | [M1] | 0.0220 | B(M1)(W.u.)=9.E-7 6, α=0.0220 | |
(17/2+) | 3 ns 1 | 871.1 | [M1] | 0.01172 | B(M1)(W.u.)=1.0×10-5 4, α=0.01172 | ||
(17/2+) | 3 ns 1 | 1041.0 | [E2] | 0.00377 | B(E2)(W.u.)=0.00019 7, α=0.00377 6 | ||
1313.500 | 5/2- | 633.967 22 | M1+E2 | 0.019 | α=0.019 8 | ||
5/2- | 975.72 6 | E2 | 0.00430 | α=0.00430 6 | |||
5/2- | 1099.26 7 | E2(+M1) | 0.0050 | α=0.0050 16 | |||
1393.0 | (27/2-) | 287.0 | (M1+E2) | 0.15 | α=0.15 6 | ||
1404.5 | (23/2+) | 4 ns 1 | 298.8 | (E1(+M2)) | 0.09 LT | 0.025 | B(E1)(W.u.)>1.4E-6, α=0.025 3 |
1433.189 | 3/2- | 914.867 18 | E2(+M1) | 0.008 | α=0.008 3 | ||
3/2- | 956.79 3 | M1 | 0.00928 | α=0.00928 13 | |||
3/2- | 1012.296 18 | M1+E2 | 0.81 +27-23 | 0.0065 | α=0.0065 6 | ||
1436.353 | 7/2- | 432.701 6 | (E1) | 0.00905 | α=0.00905 13 | ||
7/2- | 819.66 9 | M1 | 0.01365 | α=0.01365 | |||
7/2- | 918.029 14 | M1(+E2) | 0.32 LE | 0.0100 | α=0.0100 3 | ||
1458.994 | 3/2- | 588.774 8 | E2 | 0.01298 | α=0.01298 | ||
3/2- | 670.89 6 | M1+E2 | 0.7 +5-4 | 0.018 | α=0.018 4 | ||
3/2- | 779.41 3 | M1+E2 | 0.011 | α=0.011 5 | |||
3/2- | 1038.11 4 | E2(+M1) | 0.0057 | α=0.0057 19 | |||
3/2- | 1083.93 6 | M1 | 0.00682 | α=0.00682 10 | |||
1482.031 | 3/2+ | 478.369 7 | M1(+E2) | 0.038 | α=0.038 17 | ||
3/2+ | 761.413 11 | E1 | 0.00275 | α=0.00275 4 | |||
3/2+ | 867.816 13 | E1 | 0.00213 | α=0.00213 3 | |||
1532.277 | 5/2+ | 528.626 7 | M1 | 0.0416 | α=0.0416 | ||
1572.56 | 3/2- | 955.82 3 | E2 | 0.00448 | α=0.00448 7 | ||
1614.125 | 3/2-,1/2- | 1095.77 8 | E2(+M1) | 0.0050 | α=0.0050 17 | ||
3/2-,1/2- | 1239.18 23 | M1,E2 | 0.0038 | α=0.0038 12 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
1668.957 | 3/2+ | 433.520 9 | M1 | 0.0698 | α=0.0698 | ||
3/2+ | 483.106 7 | M1 | 0.0526 | α=0.0526 | |||
3/2+ | 518.544 9 | M1 | 0.0438 | α=0.0438 | |||
1706.062 | (3/2)- | 247.069 4 | M1+E2 | 1.2 +18-6 | 0.21 | α=0.21 6 | |
(3/2)- | 985.458 25 | M1+E2 | 1.2 +7-4 | 0.0060 | α=0.0060 9 | ||
(3/2)- | 1092.00 13 | M1 | 0.00670 | α=0.00670 10 | |||
(3/2)- | 1187.83 13 | E2 | 0.00291 | α=0.00291 4 | |||
(3/2)- | 1330.95 20 | E2(+M1) | 0.0033 | α=0.0033 9 | |||
1715.935 | 1/2+,3/2+,5/2+ | 233.900 4 | M1+E2 | 1.1 +4-3 | 0.26 | α=0.26 3 | |
1/2+,3/2+,5/2+ | 466.380 6 | E1 | 0.00765 | α=0.00765 11 | |||
1725.786 | 3/2- | 937.55 3 | M1 | 0.00976 | α=0.00976 14 | ||
3/2- | 1005.24 3 | M1 | 0.00821 | α=0.00821 12 | |||
3/2- | 1111.55 7 | M1 | 0.00641 | α=0.00641 9 | |||
1731.438 | 3/2- | 295.104 14 | (E2) | 0.0832 | α=0.0832 | ||
3/2- | 461.935 23 | M1(+E2) | 0.041 | α=0.041 18 | |||
3/2- | 1030.39 4 | M1(+E2) | 0.0058 | α=0.0058 20 | |||
3/2- | 1051.87 4 | M1(+E2) | 0.0055 | α=0.0055 19 | |||
3/2- | 1117.23 3 | (M1) | 0.00633 | α=0.00633 9 | |||
3/2- | 1310.70 8 | (E2) | 0.00242 | α=0.00242 4 | |||
3/2- | 1356.34 10 | M1 | 0.00398 | α=0.00398 6 | |||
1755.337 | 3/2- | 1054.25 3 | M1+E2 | 0.0055 | α=0.0055 19 | ||
3/2- | 1141.16 3 | M1 | 0.00601 | α=0.00601 9 | |||
3/2- | 1334.23 8 | E2 | 0.00234 | α=0.00234 4 | |||
1756.02 | 3/2- | 1279.45 11 | E2(+M1) | 0.0035 | α=0.0035 11 | ||
3/2- | 1381.2 3 | M1 | 0.00382 | α=0.00382 6 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
1762.80 | (3/2)- | 1042.28 7 | M1,E2 | 0.0056 | α=0.0056 19 | ||
(3/2)- | 1148.50 16 | M1 | 0.00592 | α=0.00592 9 | |||
(3/2)- | 1342.6 3 | M1 | 0.00407 | α=0.00407 6 | |||
(3/2)- | 1387.84 6 | M1+E2 | 1.0 +6-4 | 0.0030 | α=0.0030 4 | ||
1800.52 | 3/2- | 1324.36 13 | M1(+E2) | 0.0033 | α=0.0033 10 | ||
1811.50 | 3/2- | 1110.38 10 | M1(+E2) | 0.0049 | α=0.0049 16 | ||
3/2- | 1391.09 17 | E2(+M1) | 0.0030 | α=0.0030 8 | |||
1851.504 | 3/2+,5/2+ | 319.216 13 | M1(+E2) | 0.11 | α=0.11 5 | ||
3/2+,5/2+ | 847.877 20 | M1+E2 | 0.8 +5-4 | 0.0099 | α=0.0099 18 | ||
1861.238 | 5/2+ | 740.48 4 | (E2) | 0.00769 | α=0.00769 11 | ||
5/2+ | 857.601 21 | M1(+E2) | 0.009 | α=0.009 4 | |||
1913.471 | 3/2- | 599.965 8 | M1 | 0.0301 | α=0.0301 | ||
3/2- | 644.09 5 | M1 | 0.0251 | α=0.0251 | |||
1928.846 | 1/2+,3/2+ | 742.91 6 | M1+E2 | 0.013 | α=0.013 5 | ||
2549.6 | (33/2-) | 30 ns 10 | 91 | [E2] | 5.12 | α=5.12 | |
(33/2-) | 30 ns 10 | 516 | [M1] | 0.0443 | B(M1)(W.u.)=1.5×10-7 +17-15, α=0.0443 | ||
(33/2-) | 30 ns 10 | 847.1 | [E2] | 0.00576 | B(E2)(W.u.)=0.0007 3, α=0.00576 8 | ||
3439.2 | (39/2-) | 12 ns 6 | 171.0 | (M1,E2) | 0.68 | α=0.68 20 | |
3775.2 | (43/2+) | 15 µs 5 | 336.0 | (M2) | 0.518 | B(M2)(W.u.)=0.010 4, α=0.518 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 9/2+ | STABLE | μ=-0.6409 13, Q=+3.79 3 Δ<r2>(179Hf-178Hf)=+0.027 2 (1994An14), +0.028 3 (1997Zh36), +0.036 1 (1999Le11, 10% systematic normalization uncertainty not included; value is relative to Δ<r2>(178Hf,180Hf)=0.098 as measured by 1994Zi04, much higher than Δ<r2>(178Hf,180Hf)=0.075 4 and 0.076 5 from 1994An14 and 1997Zh36, respectively). Other Δ<r2>: 1994Zi04. E(level): Δ<r2>(179Hf-178Hf)=+0.027 2 (1994An14), +0.028 3 (1997Zh36), +0.036 1 (1999Le11, 10% systematic normalization uncertainty not included; value is relative to Δ<r2>(178Hf,180Hf)=0.098 as measured by 1994Zi04, much higher than Δ<r2>(178Hf,180Hf)=0.075 4 and 0.076 5 from 1994An14 and 1997Zh36, respectively). Other Δ<r2>: 1994Zi04. 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. |
122.7904 | 11/2+ | 37 ps 3 | Q=1.88 3 E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. |
214.3395 | 7/2- | 1.85 ns 4 | E(level): 7/2[514] band. |
268.92 | 13/2+ | 21 ps 3 | XREF: γ(269.1). E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. |
337.7178 | 9/2- | E(level): 7/2[514] band. | |
375.0352 | 1/2- | 18.67 s 4 % IT = 100 | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. |
420.8943 | 3/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
438.68 | 15/2+ | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
476.3341 | 5/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
487.709 | (11/2-) | E(level): 7/2[514] band. | |
518.3279 | 5/2- | < 0.2 ns | E(level): 5/2[512] band. Jπ(level): Definite Jπ assigned to J|<15/2 members of 5/2[512] band based on observed band structure combined with independently established Jπ=5/2- for 518 level and mult=M1+E2 for intraband 98γ. |
582.230 | 7/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
614.204 | 1/2- | 0.50 ns 15 | E(level): 1/2[521] band. Jπ(level): Definite Jπ assigned to J|<9/2 members of 1/2[521] band based on observed band structure combined with independently established Jπ=3/2- for 680 level and mult=M1 for intraband 148γ. |
616.7562 | 7/2- | E(level): 5/2[512] band. Jπ(level): Definite Jπ assigned to J|<15/2 members of 5/2[512] band based on observed band structure combined with independently established Jπ=5/2- for 518 level and mult=M1+E2 for intraband 98γ. | |
631.30 | 17/2+ | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
664.3 | (13/2-) | E(level): 7/2[514] band. | |
679.516 | 3/2- | E(level): 1/2[521] band. Jπ(level): Definite Jπ assigned to J|<9/2 members of 1/2[521] band based on observed band structure combined with independently established Jπ=3/2- for 680 level and mult=M1 for intraband 148γ. | |
681.036 | 9/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
701.0552 | 5/2- | E(level): 1/2[521] band. Jπ(level): Definite Jπ assigned to J|<9/2 members of 1/2[521] band based on observed band structure combined with independently established Jπ=3/2- for 680 level and mult=M1 for intraband 148γ. | |
720.613 | 3/2- | ≤ 0.3 ns | E(level): 3/2[512] band. Jπ(level): Definite Jπ assigned to J|<11/2 members of 3/2[512] band based on observed band structure combined with independently established Jπ=3/2- for 721 level and mult=M1 for intraband 147γ. |
732.2 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
742.710 | 9/2- | E(level): 5/2[512] band. Jπ(level): Definite Jπ assigned to J|<15/2 members of 5/2[512] band based on observed band structure combined with independently established Jπ=5/2- for 518 level and mult=M1+E2 for intraband 98γ. | |
788.185 | 5/2- | E(level): 3/2[512] band. Jπ(level): Definite Jπ assigned to J|<11/2 members of 3/2[512] band based on observed band structure combined with independently established Jπ=3/2- for 721 level and mult=M1 for intraband 147γ. | |
842.9 | 11/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
848.37 | 19/2+ | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
849.200 | 7/2- | E(level): 1/2[521] band. Jπ(level): Definite Jπ assigned to J|<9/2 members of 1/2[521] band based on observed band structure combined with independently established Jπ=3/2- for 680 level and mult=M1 for intraband 148γ. | |
865.9 | (15/2-) | XREF: γ(860.3). E(level): 7/2[514] band. | |
870.222 | 7/2- | E(level): 7/2[503] band. | |
889.1 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
896.7 | 11/2- | E(level): 5/2[512] band. Jπ(level): Definite Jπ assigned to J|<15/2 members of 5/2[512] band based on observed band structure combined with independently established Jπ=5/2- for 518 level and mult=M1+E2 for intraband 98γ. | |
912.0 | 9/2- | E(level): 1/2[521] band. Jπ(level): Definite Jπ assigned to J|<9/2 members of 1/2[521] band based on observed band structure combined with independently established Jπ=3/2- for 680 level and mult=M1 for intraband 148γ. | |
935.643 | 7/2- | XREF: H(908). E(level): 3/2[512] band. Jπ(level): Definite Jπ assigned to J|<11/2 members of 3/2[512] band based on observed band structure combined with independently established Jπ=3/2- for 721 level and mult=M1 for intraband 147γ. | |
958.6 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
985.7 | 13/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
992.0 | (9/2-) | E(level): 7/2[503] band. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1003.650 | 5/2+ | E(level): Kπ=5/2+ K-2 G-VIBRATION band. | |
1024.0 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1030.8 | 9/2- | E(level): 3/2[512] band. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. Jπ(level): Definite Jπ assigned to J|<11/2 members of 3/2[512] band based on observed band structure combined with independently established Jπ=3/2- for 721 level and mult=M1 for intraband 147γ. | |
1076.6 | 13/2- | E(level): 5/2[512] band. Jπ(level): Definite Jπ assigned to J|<15/2 members of 5/2[512] band based on observed band structure combined with independently established Jπ=5/2- for 518 level and mult=M1+E2 for intraband 98γ. | |
1078.349 | (7/2)+ | E(level): Kπ=5/2+ K-2 G-VIBRATION band. | |
1080.4 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1084.73 | 21/2+ | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
1087.8 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1092.7 | (17/2-) | XREF: γ(1096.8). E(level): 7/2[514] band. | |
1105.92 | (7/2+) | E(level): 7/2[633] band. | |
1120.816 | 9/2+ | E(level): Kπ=9/2+ [9/2[624]+0+] GS B-VIBRATIONAL band. | |
1138.8 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1150.411 | 1/2+ | E(level): Kπ=1/2+ (1/2[510]-1-) band. | |
1162.4 | Doublet. E(level): Doublet. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1168.95 | (9/2+) | XREF: H(1161). E(level): 7/2[633] band. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
1176.2 | (9/2+) | E(level): Kπ=5/2+ K-2 G-VIBRATION band. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1185.848 | 3/2+ | E(level): Kπ=1/2+ (1/2[510]-1-) band. | |
1196.2 | 15/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
1199.52 | (7/2+) | XREF: H(1191). | |
1235.440 | 5/2+ | E(level): Kπ=1/2+ (1/2[510]-1-) band. | |
1249.552 | 3/2- | E(level): Kπ=3/2- [7/2[514]-2+] γ-vibrational band. | |
1255.8 | 11/2- | E(level): 3/2[512] band. Jπ(level): Definite Jπ assigned to J|<11/2 members of 3/2[512] band based on observed band structure combined with independently established Jπ=3/2- for 721 level and mult=M1 for intraband 147γ. | |
1269.445 | 3/2- | E(level): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. 3/2[521] band. | |
1282.5 | (11/2+) | XREF: H(1275). E(level): 7/2[633] band. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1283.7 | 15/2- | E(level): 5/2[512] band. Jπ(level): Definite Jπ assigned to J|<15/2 members of 5/2[512] band based on observed band structure combined with independently established Jπ=5/2- for 518 level and mult=M1+E2 for intraband 98γ. | |
1309.8 | (17/2+) | 3 ns 1 | E(level): From Coulomb excitation; uncertainty unstated by authors. Kπ=17/2+ band (2000Mu06). |
1313.500 | 5/2- | E(level): Kπ=3/2- [7/2[514]-2+] γ-vibrational band. | |
1343.8 | (19/2-) | E(level): 7/2[514] band. | |
1344.6 | + | L=4,6 in (d,p); so J=7/2 to 13/2. E(level): L=4,6 in (d,p); so J=7/2 to 13/2. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1350.7 | 23/2+ | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
1359.0 | (13/2)+ | E(level): 7/2[633] band. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1372.3 | (17/2+) | Configuration=((ν 1/2[510])+(π 7/2[404])+(π 9/2][514])) (2000Mu06). E(level): Configuration=((ν 1/2[510])+(π 7/2[404])+(π 9/2][514])) (2000Mu06). | |
1381.9 | 17/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
1386.5 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1405.2 | (7/2-) | E(level): Kπ=3/2- [7/2[514]-2+] γ-vibrational band. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1428.6 | (7/2-) | E(level): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. 3/2[521] band. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1453.1 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1458.994 | 3/2- | E(level): 3/2[501] band. | |
1482.031 | 3/2+ | E(level): Kπ=3/2+ (1/2[521]+1-) band. | |
1491.0 | (17/2+) | Configuration=((ν 1/2[521])+(π 7/2[404])+(π 9/2][514])) (2000Mu06). E(level): Configuration=((ν 1/2[521])+(π 7/2[404])+(π 9/2][514])) (2000Mu06). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
1509.2 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1520.6 | (19/2+) | E(level): From Coulomb excitation; uncertainty unstated by authors. Kπ=17/2+ band (2000Mu06). | |
1530.2 | 1/2+ | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1532.277 | 5/2+ | E(level): Kπ=3/2+ (1/2[521]+1-) band. | |
1534.6 | (5/2-) | E(level): 3/2[501] band. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1557.4 | 1/2,3/2- | L=0,1 in (d,p). E(level): L=0,1 in (d,p). From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1570.1 | (9/2+) | L(3He,α)=(4) and rotational structure. E(level): L(3He,α)=(4) and rotational structure. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1580.5 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1582.4 | Doublet. E(level): Doublet. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1586.0 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1598.4 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1602.3 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1617.7 | (21/2-) | E(level): 7/2[514] band. | |
1624.3 | 25/2+ | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
1638.7 | LE 7/2 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1658.4 | (1/2-) | E(level): 1/2[501] band. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1665.7 | 1/2+ | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1689 | 11/2- | Configuration: probable Kπ=11/2- (7/2[514]+ 2+) γ vibration bandhead (2005Bu07). E(level): Configuration: probable Kπ=11/2- (7/2[514]+ 2+) γ vibration bandhead (2005Bu07). | |
1698.6 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1706.062 | (3/2)- | E(level): 1/2[501] band. | |
1753.1 | (21/2+) | E(level): From Coulomb excitation; uncertainty unstated by authors. Kπ=17/2+ band (2000Mu06). | |
1771 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1796.5 | 1/2,3/2,5/2+ | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
1826.9+X | (21/2+) | Configuration=((ν 5/2[512])+(π 7/2[404])+(π 9/2][514])) (2000Mu06). E(level): Configuration=((ν 5/2[512])+(π 7/2[404])+(π 9/2][514])) (2000Mu06). | |
1839 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
1856.0 | 21/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
1877 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1884 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1893.9 | 1/2,3/2,5/2+ | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
1899.66 | 1/2,3/2,5/2+ | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
1904 | (5/2-,7/2-) | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
1915.0 | (23/2-) | E(level): 7/2[514] band. | |
1941.6 | 27/2+ | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
1945.864 | (1/2,3/2) | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
1957.58 | 1/2,3/2,5/2+ | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
1965 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1977 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
1987 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2007.2 | (23/2+) | E(level): From Coulomb excitation; uncertainty unstated by authors. Kπ=17/2+ band (2000Mu06). | |
2009 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2021 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2032 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2047.0 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2052.6 | 1/2,3/2,5/2+ | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
2070.7 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2082.8 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2088.4 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2146.1 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2168.2 | 1/2,3/2,5/2+ | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
2183.1 | 1/2,3/2,5/2+ | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
2214.4 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2228.1 | 1/2,3/2,5/2+ | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
2242.5 | (29/2+) | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
2249.97 | (3/2-) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2- and to 7/2-. | |
2281.1 | (25/2+) | E(level): From Coulomb excitation; uncertainty unstated by authors. Kπ=17/2+ band (2000Mu06). | |
2282 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2297 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2309.2 | 1/2,3/2,5/2+ | E(level): From (9Be,α2nγ). Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal. | |
2354 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2395.1 | 25/2- | E(level): 1/2[510] band. Jπ(level): Definite Jπ assigned to J|<25/2 members of 1/2[510] band based on observed band structure combined with independently established Jπ=1/2- for 375 level and mult=M1+E2 for intraband 46γ. | |
2451.31 | (3/2-) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2- and to 7/2-. | |
2456.7 | (29/2-) | Suggested configuration=((ν 3/2[512])+(ν 9/2[624])+(ν 1/2[521])+(π 7/2[404])+ (π 9/2][514])) (2000Mu06). E(level): Suggested configuration=((ν 3/2[512])+(ν 9/2[624])+(ν 1/2[521])+(π 7/2[404])+ (π 9/2][514])) (2000Mu06). | |
2460.3 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2475.5 | (3/2-) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2- and to 7/2-. | |
2497 | 7/2+,9/2+,11/2+ | XREF: J(2480). E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
2509.5 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2556 | 7/2+,9/2+,11/2+ | XREF: J(2565). E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
2590 | E(level): ΔE>3 keV. | ||
2617.6 | (31/2+) | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
2638.8 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2655 | (13/2)+ | XREF: γ(2665). E(level): ΔE>3 keV. | |
2705 | 7/2+,9/2+,11/2+ | E(level): ΔE>10 keV. | |
2727 | E(level): ΔE>3 keV. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2788 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2857 | 9/2+ | XREF: J(2850). E(level): ΔE>3 keV. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
2905.2 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
2921 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2950 | E(level): From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
2969 | E(level): ΔE>3 keV. From (9Be,α2nγ). From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. | ||
3148.8 | (1/2-,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
3347.2 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
3373.6 | (35/2+) | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. | |
3409.5 | (1/2,3/2) | Jπ(level): Fed by primary γ from 1/2+ in (n,γ) E=thermal; γ to 1/2-. | |
3439.2 | (39/2-) | 12 ns 6 | Suggested configuration=((ν 7/2[514])+(ν 9/2[624])+(ν 7/2[503])+(π 7/2[404])+ (π 9/2][514])) (2000Mu06). E(level): Suggested configuration=((ν 7/2[514])+(ν 9/2[624])+(ν 7/2[503])+(π 7/2[404])+ (π 9/2][514])) (2000Mu06). |
3775.2 | (43/2+) | 15 µs 5 | Suggested configuration=((ν 7/2[514])+(ν 9/2[624])+(ν 11/2[615])+(π 7/2[404]) +(π 9/2][514])) (2000Mu06). E(level): Suggested configuration=((ν 7/2[514])+(ν 9/2[624])+(ν 11/2[615])+(π 7/2[404]) +(π 9/2][514])) (2000Mu06). |
4204.7 | (39/2+) | E(level): 9/2[624] band. Jπ(level): Definite Jπ assigned to J|<27/2 members of 9/2[624] band based on observed band structure combined with independently established Jπ=9/2+ and 11/2+ for the g.s. and 123 levels and mult=M1+E2 for the intraband 123γ connecting them. The existence of J|>29/2 levels is based on transitions whose placement is uncertain. |
E(level) | E(gamma) | Comments |
268.92 | 146.15 | I(γ): from (9Be,α2nγ). | 268.85 | I(γ): from (9Be,α2nγ). |
375.0352 | 160.696 | I(γ): From 179Hf IT decay (18.67 s). |
438.68 | 169.77 | E(γ): From 179Hf IT decay (25.05 d). | 315.88 | E(γ): From 179Hf IT decay (25.05 d). |
487.709 | 150.019 | I(γ): from (9Be,α2nγ); 30 6 from (n,γ) E=thermal. |
518.3279 | 143.301 | M(γ): α(K)exp in (n,γ) E=thermal consistent with E1 or E2; Δπ=no from level scheme. |
631.30 | 192.62 | E(γ): From 179Hf IT decay (25.05 d). | 362.39 | E(γ): From 179Hf IT decay (25.05 d). |
664.3 | 176.3 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 326.8 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
720.613 | 506.299 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
842.9 | 260.7 | E(γ): From (9Be,α2nγ). |
848.37 | 217.07 | E(γ): From 179Hf IT decay (25.05 d). | 409.68 | E(γ): From 179Hf IT decay (25.05 d). |
865.9 | 378.2 | E(γ): From (9Be,α2nγ). M(γ): Q intraband γ from γ(θ) in (9Be,α2nγ). |
896.7 | 153.5 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 280.1 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
912.0 | 210.9 | E(γ): From (9Be,α2nγ). |
985.7 | 304.7 | E(γ): From (9Be,α2nγ). |
1074.7 | 860.4 | E(γ): From (9Be,α2nγ). |
1076.6 | 179.5 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 334.2 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
1084.73 | 236.36 | E(γ): From 179Hf IT decay (25.05 d). | 453.43 | E(γ): From 179Hf IT decay (25.05 d). |
E(level) | E(gamma) | Comments |
1092.7 | 428.4 | E(γ): From (9Be,α2nγ). |
1105.74 | 21.01 | E(γ): From 179Hf IT decay (25.05 d). I(γ): from I(γ+ce)=2917 104 from 179Hf IT decay (25.05 d) and α=11500. M(γ): from 179Hf IT decay (25.05 d). | 257.37 | E(γ): From 179Hf IT decay (25.05 d). |
1105.92 | 891.5 | E(γ): From 179Lu β- decay. I(γ): from β- decay. | 983.17 | E(γ): From 179Lu β- decay. I(γ): from β- decay. | 1105.92 | E(γ): From 179Lu β- decay. I(γ): from β- decay. |
1168.95 | 953.9 | E(γ): From 179Lu β- decay. I(γ): from β- decay. | 1046.16 | E(γ): Multiply placed with intensity suitably divided I(γ): from β- decay.. Multiply placed with intensity suitably divided | 1168.4 | E(γ): From 179Lu β- decay. I(γ): from β- decay. |
1185.848 | 484.799 | M(γ): α(K)exp<α(K)(E2) for transition with possible ce contamination in (n,γ) E=thermal; Δπ=yes from level scheme. | 506.299 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1196.2 | 353.3 | E(γ): From (9Be,α2nγ). |
1198.4 | 123.3 | E(γ): From (9Be,α2nγ). |
1249.552 | 731.22 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1255.8 | 320.2 | E(γ): From (9Be,α2nγ). |
1283.7 | 207.2 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 387 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
1296.64 | 596.0 | E(γ): From 178Hf(n,γ) E=7.78 eV res. | 616.6 | E(γ): From 178Hf(n,γ) E=7.78 eV res. | 1082.4 | E(γ): From 178Hf(n,γ) E=7.78 eV res. |
1309.8 | 678.4 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 871.1 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 1041.0 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
1313.500 | 731.22 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1343.8 | 477.9 | E(γ): From (9Be,α2nγ). |
E(level) | E(gamma) | Comments |
1348.6 | 149.9 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 274.2 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
1350.7 | 266.0 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 502.3 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
1372.3 | 933.4 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 1103.5 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
1381.9 | 396.2 | E(γ): From (9Be,α2nγ). |
1393.0 | 287.0 | E(γ): From (9Be,α2nγ). M(γ): D+Q intraband γ from (9Be,α2nγ). |
1404.5 | 298.8 | E(γ): From (9Be,α2nγ). M(γ): D+Q from γ(θ) in (9Be,α2nγ); Δπ=(yes) from level scheme; δ(E1,M2)<0.09 from RUL. |
1433.189 | 816.42 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1458.994 | 1244.73 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1491.0 | 1052.4 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 1222.0 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
1520.6 | 210.9 | E(γ): From (9Be,α2nγ). |
1572.56 | 1053.2 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): from I(1053γ):I(1197γ) for two-photon cascade data in (n,γ) E=thermal assuming 1197γ is not a doublet there.. Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1197.46 | E(γ): Multiply placed |
1617.7 | 525.0 | E(γ): From (9Be,α2nγ). |
1624.3 | 273.4 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 539.6 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
1668.957 | 1293.49 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1675.3 | 365.5 | E(γ): From (9Be,α2nγ). |
1679.5+X | 275.0 | E(γ): From (9Be,α2nγ). |
1687.13 | 816.42 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity | 1072.93 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1702.5 | 309.6 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 597.0 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
E(level) | E(gamma) | Comments |
1706.062 | 1492.6 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1713.0 | 308.6 | E(γ): From (9Be,α2nγ). |
1725.786 | 1046.16 | E(γ): for doublet in (n,γ) E=thermal.. Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1731.438 | 1117.23 | M(γ): M1+E0 from α(K)exp, but E0 component inconsistent with adopted Jπ; it could conceivably arise from an undetected impurity in ce spectrum in (n,γ) E=thermal. | 1356.34 | M(γ): M1(+E0) from α(K)exp, but E0 component inconsistent with placement. |
1753.1 | 232.9 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 443.2 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
1756.02 | 1036.1 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1076.70 | I(γ): from (n,γ) E=thermal; doublet Iγ suitably divided. |
1762.80 | 1244.73 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 1548.78 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1783.11 | 779.1 | E(γ): From 178Hf(n,γ) E=7.78 eV res. | 1082.4 | E(γ): From 178Hf(n,γ) E=7.78 eV res. | 1103.6 | E(γ): From 178Hf(n,γ) E=7.78 eV res. |
1811.50 | 1197.46 | E(γ): Multiply placed M(γ): M1+E0 for doubly-placed 1197γ. | 1293.49 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 1336.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
1821.29 | 1121.0 | E(γ): From 178Hf(n,γ) E=7.78 eV res. | 1141.3 | E(γ): From 178Hf(n,γ) E=7.78 eV res. | 1207.0 | E(γ): From 178Hf(n,γ) E=7.78 eV res. |
1826.9+X | 422.4 | E(γ): From (9Be,α2nγ). |
1846.32 | 975.7 | E(γ): From 178Hf(n,γ) E=7.78 eV res. | 1167.2 | E(γ): From 178Hf(n,γ) E=7.78 eV res. | 1231.6 | E(γ): From 178Hf(n,γ) E=7.78 eV res. |
1856.0 | 474.1 | E(γ): From (9Be,α2nγ). |
E(level) | E(gamma) | Comments |
1859.2 | 549.4 | E(γ): From (9Be,α2nγ). |
1861.238 | 740.48 | M(γ): E2,M1 from α(K)exp in (n,γ) E=thermal; ΔJ|>2 from placement. | 1072.93 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1913.471 | 1492.6 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1915.0 | 571.2 | E(γ): From (9Be,α2nγ). |
1928.846 | 778.39 | M(γ): M1+E0 from α(K)exp in (n,γ) E=thermal is deduced from ce doublet; evaluator does not consider E0 component sufficiently certain to constitute the basis for a J assignment. |
1941.6 | 317 | E(γ): From Coulomb excitation; uncertainty unstated by authors. | 591.1 | E(γ): From (9Be,α2nγ). |
1945.864 | 1267.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): I(1267γ)/I(1332γ)=0.77.. Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1332.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
1956.1+X | 268 | E(γ): From (9Be,α2nγ). |
1974.1+X | 294.9 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 569.6 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2007.2 | 254.3 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 486.4 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2033.6 | 331.3 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 640.4 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2044.1 | 331.2 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 639.4 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2047.0 | 1625.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2052.6 | 1332.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1351.5 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2070.7 | 1350.4 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 1456.5 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1649.78 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 1695.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
E(level) | E(gamma) | Comments |
2082.8 | 1078.1 | E(γ): From 178Hf(n,γ) E=7.78 eV res. I(γ): from I(1078γ doublet):I(1606γ) in (n,γ) E=7.78 eV res. | 1381.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1403.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1606.5 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1661.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): 76 15 from (n,γ) E=7.78 eV res.. Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1707.8 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2088.4 | 1408.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1713.4 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2093.40 | 1305.3 | E(γ): From 178Hf(n,γ) E=7.78 eV res. I(γ): from 178Hf(n,γ) E=7.78 eV res. | 1672.5 | E(γ): From 178Hf(n,γ) E=7.78 eV res. I(γ): from 178Hf(n,γ) E=7.78 eV res. |
2133.2 | 274 | E(γ): From (9Be,α2nγ). |
2146.1 | 1445.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1531.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2150.3 | 1429.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1674.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1729.4 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2183.1 | 1462.5 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1503.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1707.0 | E(γ): from (n,γ) E=7.78 eV res. Similar Eγ placed from 2083 level in (n,γ) E=thermal. |
2214.4 | 1600.1 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 1840.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2228.1 | 1507.66 | E(γ): for doubly-placed γ. | 1548.78 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 1807.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2242.5 | 301 | E(γ): From Coulomb excitation; uncertainty unstated by authors. | 618 | E(γ): From Coulomb excitation; uncertainty unstated by authors. |
E(level) | E(gamma) | Comments |
2243.5+X | 287 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 556 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2249.97 | 1461.4 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1529.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1875.3 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 2035.53 | I(γ): From two-photon cascade data in (n,γ) E=thermal. |
2254.2 | 1735.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1833.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2281.1 | 273.9 | E(γ): From (9Be,α2nγ). |
2287.2+X | 313.2 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 607.5 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2309.2 | 1588.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1888.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2366.9 | 1646.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1687.4 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1752.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1848.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1890.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1946.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1991.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2386.3 | 352.8 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 683.9 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2394.2 | 1606.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1714.7 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 1973.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
E(level) | E(gamma) | Comments |
2395.1 | 539.1 | E(γ): From (9Be,α2nγ). |
2396.5 | 352.5 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 683.5 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2415.5 | 1627.7 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 1800.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1938.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1994.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2425.3 | 1724.2 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1811.1 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2451.31 | 1771.5 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1836.8 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2030.1 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2236.97 | I(γ): From two-photon cascade data in (n,γ) E=thermal. |
2456.7 | 1351 | E(γ): From (9Be,α2nγ). |
2460.3 | 2039.4 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2085.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2475.5 | 1774.4 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 1861.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2054.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2100.5 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2261.2 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2509.5 | 1830.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2088.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2134.5 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2522.7 | 2046.4 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2101.8 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2147.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
E(level) | E(gamma) | Comments |
2549.6 | 91 | E(γ): From (9Be,α2nγ). | 516 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 847.1 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2601.2 | 2124.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2180.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2226.2 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2610.7 | 1996.6 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 2092.4 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2189.66 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 2235.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2617.6 | 676 | E(γ): From Coulomb excitation; uncertainty unstated by authors. |
2638.8 | 1918.2 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 2263.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2654.13 | 1865.94 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 1932.5 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2134.8 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2278.1 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2702.9 | 2184.6 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2327.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2743.69 | 2042.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2126.96 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 2321.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2759.6 | 373.5 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 725.8 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
2769.6 | 373.2 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 725.5 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
E(level) | E(gamma) | Comments |
2898.0 | 348.4 | E(γ): From (9Be,α2nγ). |
2905.2 | 2184.5 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2225.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2484.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2530.2 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
2983.3 | 2303.8 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2507.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
3076.2 | 2397.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2463.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2559.7 | I(γ): From two-photon cascade data in (n,γ) E=thermal. |
3148.8 | 2447.7 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 2534.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
3151.5 | 392 | E(γ): Multiply placed with undivided intensity. From (9Be,α2nγ). I(γ): Multiply placed with undivided intensity | 765 | E(γ): Multiply placed with undivided intensity. From (9Be,α2nγ). I(γ): Multiply placed with undivided intensity |
3161.6 | 392 | E(γ): Multiply placed with undivided intensity. From (9Be,α2nγ). I(γ): Multiply placed with undivided intensity | 765 | E(γ): Multiply placed with undivided intensity. From (9Be,α2nγ). I(γ): Multiply placed with undivided intensity |
3177.9 | 2459.0 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2703.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
3268.2 | 370.4 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). | 718.5 | E(γ): From (9Be,α2nγ).. From 178Hf(d,p), 180Hf(d,t). ΔE includes a systematic uncertainty of 0.5 keV (for E<1700) or 3 keV (for 1700<E<2050) combined in quadrature with the relevant statistical ΔE. If no uncertainty is stated, ΔE>3 keV. I(γ): From (9Be,α2nγ). |
3345.4 | 2644.3 | I(γ): From two-photon cascade data in (n,γ) E=thermal. | 2924.3 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
3347.2 | 2668.2 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 2972.7 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
3373.6 | 756 | E(γ): From Coulomb excitation; uncertainty unstated by authors. |
E(level) | E(gamma) | Comments |
3409.5 | 2729.9 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. | 3034.4 | E(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. I(γ): Eγ from level energy difference in (n,γ) E=thermal. Iγ is relative to 100 for strongest transition observed; stronger transition(s) from level may exist. Transition is deduced from two-photon cascade data of 1988Bo44, assuming that authors’ cascade γ order is correct, that cascade γ rays are consecutive and that only two-photon cascades were identified. |
3439.2 | 171.0 | E(γ): From (9Be,α2nγ). M(γ): from α(exp) in (9Be,α2nγ). |
3659.1 | 391 | E(γ): From (9Be,α2nγ). | 761 | E(γ): From (9Be,α2nγ). |
3775.2 | 336.0 | E(γ): From (9Be,α2nγ). M(γ): from α(exp) in (9Be,α2nγ). |
4204.7 | 831 | E(γ): From Coulomb excitation; uncertainty unstated by authors. |
For hfs and/or isotope shift measurements, see 1994An14, 1994Ji07, 1994Zi04, 1995Ji15, 1996Zh35, 1997Zh36, 1999Le11.
Levels: Levels from (γ,γ’), (e,e’) with E|<2310 have been omitted from XREF because their ΔE is large compared with the energy spacing of many low-lying levels.
Levels: band(v) Kπ=(33/2-) band (2000Mu06). Configuration=((ν 7/2[514])+(ν 9/2[624])+(ν 1/2[510])+(π 7/2[404])+ (π 9/2][514])) (2000Mu06); supported by gK(exp)=0.46 4 cf. 0.45 from Nilsson model.
Levels: band(r) Kπ=(21/2+) band (2000Mu06). Configuration=((ν 9/2[624])+(π 7/2[404])+(π 5/2][402])) (2000Mu06); supported by gK(exp)=0.54 5 cf. 0.48 from Nilsson model.
Levels: band(s) Kπ=23/2+ band (2000Mu06). Configuration=((ν 7/2[514])+(π 7/2[404])+(π 9/2][514])) (2000Mu06); supported by gK(exp)=0.86 20 cf. 0.78 from Nilsson model.
Levels: band(t) Kπ=(19/2-) band (2000Mu06). Configuration=((ν 7/2[514])+(π 7/2[404])+(π 5/2][402])) (2000Mu06).
Levels: band(u) Kπ=25/2- band (2000Mu06). Configuration=((ν 9/2[624])+(π 7/2[404])+(π 9/2][514])) (2000Mu06); supported by gK(exp)=0.60 7 cf. 0.55 from Nilsson model.
Levels: band(w) (ν 5/2[523])? band (2000Mu06). Deexcites to 7/2[514] band.
Q-value: Note: Current evaluation has used the following Q record -105.6 4 6098.99 87417.9 201803.8 15 2003Au03