ADOPTED LEVELS, GAMMAS for 208Pb
Author: M. J. Martin | Citation: Nucl. Data Sheets 108,1583 (2007) | Cutoff date: 1-Jun-2007
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-2878.4 keV 21 | S(n)= 7367.87 keV 5 | S(p)= 8004 keV 6 | Q(α)= 517.2 keV 13 | ||
Reference: 2012WA38 |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0 | ABCDEFGHIJKLM QRS VWXYZabcdef | 0+ | STABLE | |||||
2614.522 10 | ABCD FGHIJKLM QRS VW Y abcdef | 3- | 16.7 ps 3 | 2614.511 10 | | E3 | 0 | 0+ |
3197.711 10 | ABCD FGHIJKL Q V Y cd | 5- | 294 ps 15 | 583.187 2 | | E2 | 2614.522 | 3- |
3475.078 11 | A CD F HIJKL Q f | 4- | 4 ps 3 | 277.371 5 860.557 4 | 50.8 8 100 | M1+E2 M1+E2 | 3197.711 2614.522 | 5- 3- |
3708.451 12 | ABCD FGHIJKL V d f | 5- | 233.33 6 510.74 5 1093.95 24 | 1.36 9 100.0 13 1.75 13 | M1+E2 M1+E2 [E2] | 3475.078 3197.711 2614.522 | 4- 5- 3- | |
3919.966 13 | A D H JKL f | 6- | > 690 fs | 211.51 2 722.252 8 | 82 5 100 | M1(+E2) M1+E2 | 3708.451 3197.711 | 5- 5- |
3946.578 14 | A D HIJKL f | 4- | > 430 fs | 238.22 3 471.498 14 748.845 12 | 25.3 18 26.3 19 100 7 | [M1+E2] [M1+E2] [M1+E2] | 3708.451 3475.078 3197.711 | 5- 4- 5- |
3961.162 13 | ABCD GHIJKL V cd f | 5- | 252.755 12 485.95 15 763.429 9 | 38.3 22 2.5 3 100 3 | M1+E2 M1+E2 | 3708.451 3475.078 3197.711 | 5- 4- 5- | |
3995.438 13 | A D F HI KLM Q f | 4- | > 690 fs | 797.741 10 1380.889 12 | 29.7 12 100 | [M1+E2] [M1(+E2)] | 3197.711 2614.522 | 5- 3- |
4037.443 14 | ABCD GH J L V c | 7- | > 690 fs | 117.53 13 839.734 9 | 11 3 100 | [M1,E2] [E2] | 3919.966 3197.711 | 6- 5- |
4051.134 13 | AB D F HI LM f | 3- | 326 fs +28-21 | 576.057 13 1436.602 12 | 17.2 17 100 | [M1+E2] | 3475.078 2614.522 | 4- 3- |
4085.52 4 | ABCDE GHI LM QR V c ef | 2+ | 0.80 fs 4 | 1471.5 4 4085.47 4 | 0.46 15 100 | [E1] [E2] | 2614.522 0 | 3- 0+ |
4125.347 12 | AB D FGHIJKL d f | 5- | > 490 fs | 164.34 20 179.5 6 416.79 6 650.207 14 927.650 8 | 4.9 7 0.92 26 5.0 9 25.3 13 100.0 25 | [M1,E2] [M1,E2] [M1+E2] [M1+E2] [M1+E2] | 3961.162 3946.578 3708.451 3475.078 3197.711 | 5- 4- 5- 4- 5- |
4144 5 ? | I | + | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4180.414 14 | AB D FGHI KL V c f | 5- | 319 fs 35 | 705.33 2 982.709 10 | 10.7 20 100 | [M1+E2] [M1+E2] | 3475.078 3197.711 | 4- 5- |
4206.277 14 | A D F HIJ L f | 6- | > 690 fs | 497.90 4 1008.558 10 | 20.6 24 100 | [M1+E2] [M1+E2] | 3708.451 3197.711 | 5- 5- |
4229.590 17 | A D F H LM | 2- | 333 fs 28 | 1615.068 15 4229.49 9 | 100 21.4 21 | [M1+E2] M2 | 2614.522 0 | 3- 0+ |
4254.795 17 | AB D FGHI LM V c | 3- | 97 fs 7 | 779.2 4 ? 1640.267 15 | 5.50 6 100 | [M1+E2] | 3475.078 2614.522 | 4- 3- |
4261.871 13 | A D F HI KL f | 4- | > 520 fs | 553.414 8 786.79? 1064.15 2 1647.38 2 | 49 4 58 2 4.4 6 100 4 | [M1+E2] [M1+E2] [M1+E2] [M1+E2] | 3708.451 3475.078 3197.711 2614.522 | 5- 4- 5- 3- |
4296.560 13 | AB D F HI KL V c f | 5- | 201 fs +49-35 | 171.00 20 588.096 6 821.540 13 1098.85 4 | 5.3 14 100 3 63 3 10.8 21 | [M1,E2] [M1+E2] [M1+E2] [M1,E2] | 4125.347 3708.451 3475.078 3197.711 | 5- 5- 4- 5- |
4323.946 14 | ABCD GHIJ L Q V c f | 4+ | 11.7 ps +15-18 | 362.81 7 848.88 4 1126.236 13 1709.6 2 4324.3 4 | 14.8 12 2.42 4 100 3 0.51 8 0.31 4 | [E1] [E1] [E1+M2] [E2] [E4] | 3961.162 3475.078 3197.711 2614.522 0 | 5- 4- 5- 3- 0+ |
4358.670 13 | A CD F HI KL f | 4- | 194 fs 21 | 178.5 5 362.8 5 883.605 9 1160.90 2 1744.12 2 | 2.1 11 2.8 7 100 5 38 3 15.5 13 | [M1+E2] [M1+E2] [M1+E2] | 4180.414 3995.438 3475.078 3197.711 2614.522 | 5- 4- 4- 5- 3- |
4383.285 17 | A D FGHI KL f | 6- | > 690 fs | 176.8 5 257.7 5 463.30 10 1185.571 13 | 0.85 25 0.67 25 4.1 7 100 11 | [M1+E2] [M1+E2] | 4206.277 4125.347 3919.966 3197.711 | 6- 5- 6- 5- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4423.647 15 | ABCD FGHIJ L Q V c f | 6+ | > 110 fs | 715.23 2 1225.916 13 | 8.6 11 100 | [E1+M2] [E1+M2] | 3708.451 3197.711 | 5- 5- |
4447 5 ? | I | - | ||||||
4480.746 16 | ABCD FGHIJKL f | 6- | 97 fs 7 | 771.6 4 1283.031 12 | 8.7 18 100 | [M1+E2] [M1+E2] | 3708.451 3197.711 | 5- 5- |
4610.748 16 | AB D FGHIJ L V | 8+ | 3.2 ns 5 | 573.41 8 1413.026 13 | 3.1 6 100 | [E1+M2] [E3] | 4037.443 3197.711 | 7- 5- |
4680.266 22 | AB D H J | 7- | > 690 fs | 473.98 5 760.30 2 | 40 11 100 | [M1+E2] [M1+E2] | 4206.277 3919.966 | 6- 6- |
4698.323 17 | AB D FGHI L V c | 3- | 139 fs +42-28 | 436.41 10 443.57 8 468.76 7 612.88 15 647.25 9 702.86 14 1223.27 2 1500.49 3 2083.90 4 4697.88 14 | 7.9 13 41.2 20 10.0 9 1.7 5 4.3 9 4.1 6 100 5 38 4 27 3 4.4 6 | [M1,E2] [M1+E2] [M1,E2] [E1] [M1,E2] [M1,E2] [M1+E2] [E2] [M1,E2] [E3] | 4261.871 4254.795 4229.590 4085.52 4051.134 3995.438 3475.078 3197.711 2614.522 0 | 4- 3- 2- 2+ 3- 4- 4- 5- 3- 0+ |
4708.727 21 | AB D HI | 5- | 0.24 ps +20-9 | 412.17 4 714.0 10 748.3 5 1000.51 12 1511.00 2 | 21 5 12 6 67 8 100 7 60 4 | [M1,E2] [M1,E2] [M1,E2] [M1+E2] [M1+E2] | 4296.560 3995.438 3961.162 3708.451 3197.711 | 5- 4- 5- 5- 5- |
4711.817 21 | A D F H M | 4- | > 340 fs | 1236.79 4 2097.27 2 | 29 4 100 | [M1+E2] [M1+E2] | 3475.078 2614.522 | 4- 3- |
4761.956 23 | A D FGH | 6- | 0.26 ps +18-9 | 555.63 6 636.57 3 1564.29 3 | 15 4 25 5 100 9 | 4206.277 4125.347 3197.711 | 6- 5- 5- | |
4830 | G | (8,9,10) | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4841.60 5 | AB DEFGH L c | 1- | 0.068 fs +21-15 | 4841.46 12 | | [E1] | 0 | 0+ |
4860.78 6 | AB D F HIJ | 8+ | > 22 fs | 250.00 9 823.28 11 | 100 34 6 | 4610.748 4037.443 | 8+ 7- | |
4867.91 4 | A D F H | 7+ | > 97 fs | 257.06 5 386.7 3 444.15 10 484.6 3 830.55 4 | 100 15 26 13 73 15 14 5 38 6 | [M1+E2] [M1+E2] | 4610.748 4480.746 4423.647 4383.285 4037.443 | 8+ 6- 6+ 6- 7- |
4868.35 5 | AB H L V c | 0+ | > 312 fs | 782.83 2 4870 3 | | E0 | 4085.52 0 | 2+ 0+ |
4878 2 | D F | |||||||
4895.23 5 | AB D G IJ | 10+ | 0.50 µs 5 | 34.4 284.49 5 857.71 10 | 0.041 14 100 8 20 4 | [E2] [E2] [E3] | 4860.78 4610.748 4037.443 | 8+ 8+ 7- |
4909.5 3 | D F | |||||||
4911.343 20 | H | 4 | 215 fs +63-42 | 964.56 6 1713.62 4 2296.83 2 | 11.7 17 32.8 24 100 5 | [M1+E2] [M1+E2] | 3946.578 3197.711 2614.522 | 4- 5- 3- |
4918.8 4 | D | 8- | ||||||
4928.1 15 | D V c | 2+ | ||||||
4937.19 4 | AB D F HI LM | 3- | 17.3 fs +35-28 | 2322.65 3 4937.19 4 ? | 100 7 1 | [M1+E2] [E3] | 2614.522 0 | 3- 0+ |
4953.302 17 | AB D F H | 3- | 33.3 fs 14 | 2338.765 14 | | [M1+E2] | 2614.522 | 3- |
4962.428 21 | D H | 4(-),5(+) | > 440 fs | 638.48 2 1764.71 3 | 43 8 100 | [M1+E2] | 4323.946 3197.711 | 4+ 5- |
4973.918 19 | AB D FGH L V | 3- | 166 fs 21 | 275.72 24 615.7 5 712.13 25 719.19 4 1265.0 6 1499.10 10 1776.10 5 2359.39 2 4974.1 6 | 1.4 6 1.6 5 2.9 6 17.0 10 3.2 11 18.0 10 98 3 100 4 1.1 4 | [M1,E2] [M1,E2] [M1,E2] [M1,E2] [E2] [M1,E2] [E2] [M1+E2] [E3] | 4698.323 4358.670 4261.871 4254.795 3708.451 3475.078 3197.711 2614.522 0 | 3- 4- 4- 3- 5- 4- 5- 3- 0+ |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4992.5 6 | F | (2)- | ||||||
4994.7 6 | D | GE 7 | ||||||
5010.43 14 | A D G J | 9+ | 399.60 17 | | 4610.748 | 8+ | ||
5037.536 18 | AB D F H L V | 3- | 90 fs 7 | 808.04 6 986.39 7 1562.32 10 2422.997 15 5037.4 7 | 4.8 9 4.0 5 7.5 5 100 4 1.20 15 | [M1+E2] [E3] | 4229.590 4051.134 3475.078 2614.522 0 | 2- 3- 4- 3- 0+ |
5056.1 3 | D F | |||||||
5069.31 10 | AB D G IJ | 10+ | 174.13 9 | | M1(+E2) | 4895.23 | 10+ | |
5074.81 6 | D H | 69 fs +13-10 | 868.53 6 894.45 3 1113.57 3 | 57 7 79 11 100 14 | 4206.277 4180.414 3961.162 | 6- 5- 5- | ||
5075.78 18 | A D F H | 1367.0 10 | | 3708.451 | 5- | |||
5079.912 20 | D F H | 6- | 111 fs +28-21 | 873.635 15 1882.09 10 | 100 14.7 22 | 4206.277 3197.711 | 6- 5- | |
5085.470 24 | AB D HI L | 7- | > 229 fs | 702.1 10 879.19 2 | 13 5 100 | [M1+E2] | 4383.285 4206.277 | 6- 6- |
5087.9 15 | D I | 3- | ||||||
5092.99 3 | AB D F HI | 8+ | > 690 fs | 232.2 3 482.24 2 | 7.6 18 100 | 4860.78 4610.748 | 8+ 8+ | |
5103.3 15 | D | |||||||
5127.356 16 | A D F HI L | 2-,3- | 64 fs 3 | 1652.18 17 2512.818 12 5127.5 2 | 6.6 8 100 4 7.5 8 | [M1+E2] [M2,E3] | 3475.078 2614.522 0 | 4- 3- 0+ |
5162.05 5 | A D F IJ | 9+ | 151.50 20 266.70 20 301.25 10 551.32 5 | 47 5 17 3 22 3 100 8 | 5010.43 4895.23 4860.78 4610.748 | 9+ 10+ 8+ 8+ | ||
5193.428 25 | A HI | 5+ | > 319 fs | 769.78 2 869.43 20 1995.5 5 ? | 100 13 96 10 29.2 23 | 4423.647 4323.946 3197.711 | 6+ 4+ 5- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5195.054 23 | D F H | 3-,4- | 187 fs +42-35 | 1199.62 2 2580.41 7 | 100 42 5 | 3995.438 2614.522 | 4- 3- | |
5195.37 10 | A HIJ | 7+ | > 690 fs | 327.44 20 334.5 4 584.62 15 715.0 6 771.73 20 1275.5 5 | 18.7 22 2.6 9 36 6 2.20 22 100 14 7.5 31 | 4867.91 4860.78 4610.748 4480.746 4423.647 3919.966 | 7+ 8+ 8+ 6- 6+ 6- | |
5213.007 21 | A D HIJ | 6+ | 76 fs +21-14 | 789.358 15 2015.5 5 | 100 65 8 | [E1] | 4423.647 3197.711 | 6+ 5- |
5213.98 3 | FGH | (5-) | 14 fs 3 | 1252.98 4 1505.43 3 2016.14 3 ? | 28.2 26 26.9 26 100 7 | 3961.162 3708.451 3197.711 | 5- 5- 5- | |
5216.214 18 | AB D HIJ | 4+ | 32 fs 3 | 892.25 2 2601.69 2 | 31 4 100 | [E1+M2] | 4323.946 2614.522 | 4+ 3- |
5234 5 | I | + | ||||||
5235.37 11 | D J | (11+) | 340.16 10 | | 4895.23 | 10+ | ||
5239.3 4 | A D F H | 4- | 2625.2 5 | | 2614.522 | 3- | ||
5241.1 3 | A H L V c | 0+ | > 690 fs | 2626.6 3 5241 3 | | [E3] E0 | 2614.522 0 | 3- 0+ |
5245.246 21 | AB D FGH L | 3- | 17 fs +7-6 | 307.80 20 921.5 2 1193.9 4 1770.20 8 2630.71 2 5245.0 7 | 1.4 5 1.9 4 1.9 6 6.7 5 100.0 25 1.0 2 | [E1] [M1+E2] [M1+E2] [E3] | 4937.19 4323.946 4051.134 3475.078 2614.522 0 | 3- 4+ 3- 4- 3- 0+ |
5254.12 15 | A F H J | 178.34 10 1779.04 15 | 19 6 100 | 5075.78 3475.078 | 4- | |||
5260 | G | 9+ | ||||||
5261.2 8 | F | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5266.6 9 | F | |||||||
5270 | G | (11+) | ||||||
5276.418 24 | D F HI | 4- | 44 fs +6-5 | 1070.13 3 1567.97 4 2078.64 3 2662.02 5 | 18.4 23 43 5 100 7 15.0 9 | [E2] | 4206.277 3708.451 3197.711 2614.522 | 6- 5- 5- 3- |
5280.47 4 | A D F H L | 0- | > 319 fs | 438.83 5 1050.90 4 | 27.6 15 100 | 4841.60 4229.590 | 1- 2- | |
5286.484 17 | D F H | 2,3- | 76 fs 7 | 2671.942 13 5287.1 3 | 100 21 3 | [D+Q] | 2614.522 0 | 3- 0+ |
5291 6 | G | 11+ | ||||||
5291.90 12 | AB DEF H L | 1- | 0.049 fs +28-18 | 5291.74 13 | | [E1] | 0 | 0+ |
5307.6 15 | F | |||||||
5317.041 18 | A D F HI | (3)+ | > 690 fs | 993.105 12 2702.42 3 | 100 23 3 | 4323.946 2614.522 | 4+ 3- | |
5317.2 6 | A D F | 2119.5 6 | | 3197.711 | 5- | |||
5326.6 2 | D F | + | ||||||
5339.46 6 | A D F HI | 8+ | 32 fs +37-18 | 478.59 11 728.78 6 1301.74 14 | | [E1] | 4860.78 4610.748 4037.443 | 8+ 8+ 7- |
5347.270 18 | ABCD FGH | 3- | 28.4 fs 14 | 1295.8 5 2732.729 15 | 18 7 100 | [M1+E2] | 4051.134 2614.522 | 3- 3- |
5352 6 | I | + | ||||||
5364 3 | D | |||||||
5373.8 8 | B D FG | (6)+ | ||||||
5380.6 8 | A G I | - | 2766.1 8 | | 2614.522 | 3- | ||
5382.82 3 | A GHI | 3+,4+,5+ | 37 fs +7-6 | 1387.37 3 | | [E1] | 3995.438 | 4- |
5384.59 3 | AB D FGH LM | 3- | 76 fs 14 | 1155.00 2 1333.48 22 2770.45 20 5384.37 12 | 60 6 31 6 100 4 16.9 11 | [D+Q] [E3] | 4229.590 4051.134 2614.522 0 | 2- 3- 3- 0+ |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5401 2 | D | |||||||
5418.6 5 | D | (6)+ | ||||||
5473 6 | I | + | ||||||
5481.87 3 | AB D FGH L Q | 5- | 90 fs 14 | 1356.49 4 2867.35 3 | 83 9 100 | [E2+M3] | 4125.347 2614.522 | 5- 3- |
5490 2 ? | B | |||||||
5490.34 5 | A F HI | (4-,6-) | 1107.0 5 1193.52 20 1283.5 10 1365.0 5 1529.0 5 1781.5 5 | 83 13 59 9 35 7 100 13 75 13 69 15 | 4383.285 4296.560 4206.277 4125.347 3961.162 3708.451 | 6- 5- 6- 5- 5- 5- | ||
5491.53 3 | A D F HI L | (4-,6-) | 125 fs +35-21 | 1571.49 4 2293.85 3 | 38 4 100 | [M1+E2] | 3919.966 3197.711 | 6- 5- |
5502 3 | D G | |||||||
5511.78 14 | AB DEFGH L | 1- | 0.0194 fs +12-18 | 5511.70 14 | | [E1] | 0 | 0+ |
5516.714 23 | AB D FGH | 3- | 40.9 fs 21 | 2902.17 2 | | [M1+E2] | 2614.522 | 3- |
5524 3 | D I | + | ||||||
5531 3 | D F | |||||||
5536.58 19 | A D G | 10+ | 467.30 20 641.3 3 | 23 7 100 | 5069.31 4895.23 | 10+ 10+ | ||
5543.01 14 | AB D G I | 7- | 457.45 20 1062.9 5 1119.1 10 1159.6 3 1336.5 5 1505.9 5 1623.2 5 | 29 3 16.2 25 7 3 100 8 43 5 25 4 14 4 | 5085.470 4480.746 4423.647 4383.285 4206.277 4037.443 3919.966 | 7- 6- 6+ 6- 6- 7- 6- | ||
5545.46 4 | AB D H | (5-) | 37 fs +8-6 | 1248.5 5 1283.48 10 1420.3 5 1584.35 10 1599.1 5 1837.06 4 2347.51 9 | 16 3 44 9 38 8 25 9 38 6 100 12 74 15 | 4296.560 4261.871 4125.347 3961.162 3946.578 3708.451 3197.711 | 5- 4- 5- 5- 4- 5- 5- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5548.113 23 | A D F H L | 2- | 83 fs 7 | 2933.57 2 5547.6 3 | 100 2.6 4 | [M2] | 2614.522 0 | 3- 0+ |
5554 2 | D | |||||||
5557.2 10 | F | |||||||
5561.31 5 | B D H | 2+ | 38 fs 4 | 2946.79 5 5560.8 2 | 100 36 3 | [M1+E2] [E2] | 2614.522 0 | 3- 0+ |
5563.73 4 | A F H L | 3- | 44 fs +9-7 | 2366.3 3 2949.18 4 | 57 7 100 | [E2] | 3197.711 2614.522 | 5- 3- |
5565.2 5 | A G J | (4+) | 2089.7 5 | | 3475.078 | 4- | ||
5572.0 8 | F | |||||||
5576.6 15 | D I | |||||||
5579.0 9 | F I | |||||||
5587.7 5 | D F I | |||||||
5599.48 6 | A D F H L | 0- | > 159 fs | 757.93 7 1369.83 7 | 41 3 100 | 4841.60 4229.590 | 1- 2- | |
5615.4 4 | D FG | 7+ | ||||||
5627 5 | I | + | ||||||
5639.55 9 | AB D F H L | 1- | 0.13 ps +12-5 | 3024.96 9 5639.7 2 | 10.3 9 100 | [E1] | 2614.522 0 | 3- 0+ |
5641.98 20 | B D H | 1,2+ | < 5.5 fs | 5641.9 2 | | 0 | 0+ | |
5643 4 | B I | 2 TO 7- | ||||||
5649.01 6 | A D FGH | 3-,4- | 37 fs +13-10 | 1387.4 10 1523.8 10 1654.2 5 2451.20 8 3034.52 9 | 35 9 82 14 59 12 100 15 37 2 | [D+Q] | 4261.871 4125.347 3995.438 3197.711 2614.522 | 4- 5- 4- 5- 3- |
5649.5 4 | D | 6 TO 9+ | ||||||
5658.51 4 | B D FGHI | 5- | 31 fs +7-6 | 1663.05 5 2460.80 5 3044.0 2 | 60 6 100 6 11.4 16 | [E2] | 3995.438 3197.711 2614.522 | 4- 5- 3- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5665.7 11 | B D I | |||||||
5675.366 23 | A D F HI | 2-,3,4 | 13 fs +6-5 | 1317.0 10 1413.0 10 1420.0 10 3060.82 2 | 4.9 20 10.0 20 21 5 100 9 | [D+Q] | 4358.670 4261.871 4254.795 2614.522 | 4- 4- 3- 3- |
5686.5 7 | A D F HI | 6- | 1561.0 10 1726.0 10 1767.0 10 | 99 8 100 9 100 10 | 4125.347 3961.162 3919.966 | 5- 5- 6- | ||
5690.117 23 | ABCD GHI | 4+ | 46 fs 4 | 3075.57 2 | | [E1+M2] | 2614.522 | 3- |
5694.22 12 | A D HI | 7- | 58 fs +84-30 | 1774.25 12 | 100 | 3919.966 | 6- | |
5715.53 9 | A DE GHI | 2+ | 3.7 fs 11 | 3101.07 10 5715.1 2 | 12.6 11 100 | [E1] [E2] | 2614.522 0 | 3- 0+ |
5721.51 4 | B D F H | 7- | 28 fs +9-7 | 1297.86 3 | | [E1] | 4423.647 | 6+ |
5727 6 | I | + | ||||||
5737.9 3 | D L | 1314.6 12 | | 4423.647 | 6+ | |||
5741.1 4 | D F | 6 TO 9+ | ||||||
5749.67 14 | J | (11+) | 680.6 2 854.6 2 | 100 14 10 | 5069.31 4895.23 | 10+ 10+ | ||
5763.7 8 | D I | 6+ | ||||||
5777.96 3 | A D FGHI L | 2-,3- | 15.9 fs 14 | 1523.03 15 1726.66 17 3163.43 3 5777.4 3 | 17.8 22 16.6 25 100 9 5.1 10 | [D+Q] [D+Q] [M2,E3] | 4254.795 4051.134 2614.522 0 | 3- 3- 3- 0+ |
5783.22 7 | A H | 41 fs +22-14 | 1399.93 6 | | 4383.285 | 6- | ||
5789.34 4 | HI | 2+,3+,4+ | 40 fs +4-3 | 3174.79 3 | | 2614.522 | 3- | |
5799.41 9 | A D H | > 690 fs | 2324.32 9 | | 3475.078 | 4- | ||
5805.0 3 | A D H L | 1 | 5.1 fs +11-10 | 5804.9 3 | | [E1,M1] | 0 | 0+ |
5813.27 4 | ABCD FGH L | 3- | 22 fs +4-3 | 2338.18 26 3198.72 4 | 85 14 100 | [M1+E2] | 3475.078 2614.522 | 4- 3- |
5819.49 20 | F HI | 1+,2+ | 222 fs +42-35 | 5819.4 2 | | [M1,E2] | 0 | 0+ |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5825.3 5 | A D F | 1214.5 5 | | 4610.748 | 8+ | |||
5835 2 | B | |||||||
5835.8 6 | D F | 8- | ||||||
5844.49 20 | A CDE GHI M | 1+ | ≤ 0.31 fs | 5844.4 2 | | 0 | 0+ | |
5860 6 | G | 11+ | ||||||
5867 4 | I | + | ||||||
5873.573 23 | AB D F H J L | 3- | 13.2 fs +21-14 | 2398.48 2 | | 3475.078 | 4- | |
5885.55 4 | AB D F HI L | 3- | 13.9 fs 14 | 1588.5 5 3271.00 3 | 14 6 100 | [E2] | 4296.560 2614.522 | 5- 3- |
5901 3 | D I | (8)+ | ||||||
5918.28 4 | D H | 3-,4,5- | 173 fs +56-42 | 2720.57 4 3303.65 7 | 100 42 3 | 3197.711 2614.522 | 5- 3- | |
5923.67 3 | A D F H L | 2- | 104 fs +90-42 | 631.3 3 678.50 8 796.7 4 886.35 25 949.82 4 1225.41 7 1668.60 8 1694.08 17 1872.43 8 3308.99 15 5922.6 8 | 3.7 7 30.7 12 3.9 7 8.0 9 100 3 98 5 26.7 16 10.7 11 52 3 13.5 18 11.1 21 | [E1,M2] | 5291.90 5245.246 5127.356 5037.536 4973.918 4698.323 4254.795 4229.590 4051.134 2614.522 0 | 1- 3- 2-,3- 3- 3- 3- 3- 2- 3- 3- 0+ |
5928.0 3 | A G I | 10+ | 858.4 4 1033.0 4 | 54 21 100 | 5069.31 4895.23 | 10+ 10+ | ||
5944 5 | I | + | ||||||
5946.77 20 | A DEF H L | 1- | ≤ 0.48 fs | 5946.6 2 | | 0 | 0+ | |
5954 6 | G | 9+ | ||||||
5957.3 6 | D | |||||||
5965.8 4 | A | 749.6 4 | | 5216.214 | 4+ | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5967.8 8 | D | AP 9 | ||||||
5968.55 6 | A D F H L | 4- | 7.6 fs +42-35 | 1644.1 8 1762.6 3 2260.02 8 2770.88 8 | 1.0 5 3.4 3 34.2 21 100 5 | [E1] [E2] | 4323.946 4206.277 3708.451 3197.711 | 4+ 6- 5- 5- |
5973.0 4 | AB | 2+ | 1648.5 5 5973.5 8 | 40 17 100 | 4323.946 0 | 4+ 0+ | ||
5981 2 | D | |||||||
5989.1 12 | D F | |||||||
5992.67 25 | ABCD FG | 6+ | 779.8 5 797.4 5 1511.6 6 1609.3 6 2795.0 6 | 43 18 54 21 66 21 73 23 100 28 | 5213.007 5195.37 4480.746 4383.285 3197.711 | 6+ 7+ 6- 6- 5- | ||
5996 5 | I | - | ||||||
6009.75 4 | ABCD FGH L | 3- | 11 fs +5-4 | 1685.7 4 1924.19 9 2534.66 4 | 13.7 17 26 3 100 5 | [E1] [E1] | 4323.946 4085.52 3475.078 | 4+ 2+ 4- |
6011.64 6 | H | 57 fs +13-11 | 3397.09 6 | | 2614.522 | 3- | ||
6020.4 20 | D | |||||||
6025.8 6 | A D F | 2030.4 6 | | 3995.438 | 4- | |||
6033 2 | D | |||||||
6037.5 12 | D F | (5+,6+) | ||||||
6053.7 6 | B D G | 4+ | ||||||
6068.2 12 | D F | (5+,6+) | ||||||
6071 5 | I | - | ||||||
6076.4 13 | D F | 0-,1- | ||||||
6086.56 4 | AB D F H L | 1- | 37 fs +25-15 | 841.40 20 959.5 3 1112.70 6 1388.19 13 1831.77 7 1856.73 12 2035.30 17 3471.9 2 6085.4 10 | 9.5 10 4.6 10 52 4 100 5 73 5 53 4 100 5 27 6 3.2 18 | [E2] [E2] [E2] [E2] [E2] [E2] [E1] | 5245.246 5127.356 4973.918 4698.323 4254.795 4229.590 4051.134 2614.522 0 | 3- 2-,3- 3- 3- 3- 2- 3- 3- 0+ |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
6099.8 4 | A D | 860.50 6 1802.7 5 | 100 45 22 | 5239.3 4296.560 | 4- 5- | |||
6100.69 14 | D G J | 12+ | 351.4 2 865.34 20 | 20 4 100 | 5749.67 5235.37 | (11+) (11+) | ||
6101.1 10 | D F H | (5+) | > 690 fs | 2626 | | 3475.078 | 4- | |
6103.5 5 | A | 538.0 4 1807.6 6 | 100 63 33 | 5565.2 4296.560 | (4+) 5- | |||
6147.8 8 | A H | 2672.7 8 | | 3475.078 | 4- | |||
6179 5 | D I | 2+ | ||||||
6191.0 15 | D F | 3- | ||||||
6193.1 4 | B DE G | 2+ | 0.62 fs 5 | 6193.1 4 | | [E2] | 0 | 0+ |
6216.8 15 | D | |||||||
6223.9 15 | D | |||||||
6234.9 6 | D G | |||||||
6242.4 9 | AB D FGHI | 3627.8 9 | | 2614.522 | 3- | |||
6250.6 15 | D G I | |||||||
6255.68 6 | A DEF H | 2+ | ≤ 0.91 fs | 3641.13 6 6255.5 4 | | 2614.522 0 | 3- 0+ | |
6263.7 1 | AB DEFG L | 1- | ≤ 0.21 fs | 6263.6 1 | | 0 | 0+ | |
6274.55 22 | AB D F H | 3- | 12 fs +16-10 | 757.8 4 2278.3 5 3660.3 3 | 19 6 41 11 100 7 | 5516.714 3995.438 2614.522 | 3- 4- 3- | |
6283 6 | G | 10- | ||||||
6313.9 1 | AB DEF L | 1- | ≤ 0.17 fs | 6313.8 1 | | 0 | 0+ | |
6317.6 15 | D | |||||||
6327.2 15 | D | |||||||
6332.9 15 | D G | |||||||
6340 5 | A D FG M | 1-,2,3- | 3725 5 | | 2614.522 | 3- | ||
6348.3 15 | D G | |||||||
6354.4 4 | A D F | 2303.3 4 | | 4051.134 | 3- | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
6361.6 1 | AB DEF L | 1- | ≤ 0.30 fs | 6361.5 1 | | [E1] | 0 | 0+ |
6371.8 15 | D G | 2+,3- | ||||||
6378.8 6 | D | |||||||
6389.6 5 | D FG L | - | ||||||
6397.1 15 | D G L | |||||||
6420.2 14 | D F | (5+,6+) | ||||||
6427.6 15 | D G | |||||||
6428 10 | G | 2- | ||||||
6435.57 23 | D G J | 12- | 1200.2 2 | | 5235.37 | (11+) | ||
6444.4 2 | D F L | 3- | 6444.3 2 | | 0 | 0+ | ||
6448.40 14 | D J | (13-) | 348.00 15 1552.7 2 | 100 15 4 | 6100.69 4895.23 | 12+ 10+ | ||
6452.0 5 | B D | |||||||
6462.7 4 | D F I | - | ||||||
6472.6 15 | D | |||||||
6482.0 15 | D G | 2- | ||||||
6486.5 2 | AB DEF L | 1- | 0.78 fs +37-23 | 512.98 25 3871.7 7 6485.9 12 | 20 5 21 13 100 8 | [E1] [E2] [E1] | 5973.0 2614.522 0 | 2+ 3- 0+ |
6505.6 22 | DE | 1 | ≤ 1.0 fs | 6505.6 22 | | 0 | 0+ | |
6512.8 6 | DE G | 1 | ≤ 4.2 fs | 6512.7 6 | | 0 | 0+ | |
6529.0 15 | A D G I | - | ||||||
6531.7 15 | A D | |||||||
6541.6 6 | B D | |||||||
6545.2 11 | A | 3930.6 11 | | 2614.522 | 3- | |||
6551.93 16 | A L | 1-,2,3- | 3937.37 16 6551.8 21 | 100 14 1 | 2614.522 0 | 3- 0+ | ||
6561.0 15 | D | |||||||
6573.2 15 | D F | |||||||
6579.0 | D | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
6588 10 | G | 2- | ||||||
6589.0 15 | D F | |||||||
6609.2 15 | D | |||||||
6617.0 3 | AB D FG I L | 3- | 2436.8 5 4002.8 5 | 51 15 100 | 4180.414 2614.522 | 5- 3- | ||
6631.5 6 | B D | |||||||
6655.3 15 | D F | |||||||
6657.8 5 | AB D G L | 4+ | 2478.7 5 4042.7 2 | 34 9 100 | 4180.414 2614.522 | 5- 3- | ||
6682.46 14 | A D F L | (5-) | 2324.2 5 2974.10 20 4067.5 8 | 63 15 34 7 100 15 | 4358.670 3708.451 2614.522 | 4- 5- 3- | ||
6687.8 7 | B D L | 5- | 2207.1 7 | | 4480.746 | 6- | ||
6699.60 23 | AB D FG | (3-) | 1049.9 4 2470.1 6 4085.4 3 | 22 6 21 7 100 7 | 5649.01 4229.590 2614.522 | 3-,4- 2- 3- | ||
6708.9 15 | D G | |||||||
6719.8 5 | AB DEF L | 1- | 0.052 fs +6-12 | 6719.7 5 | | 0 | 0+ | |
6728 2 | D | |||||||
6734.4 11 | D FG | |||||||
6739.6 7 | D L | 2381.4 1 | | 4358.670 | 4- | |||
6743.42 16 | D G J | 14- | 295.31 25 1508.1 2 | 47 8 100 | 6448.40 5235.37 | (13-) (11+) | ||
6756.4 7 | D G | |||||||
6766.6 10 | A D FG | 4152.0 10 | | 2614.522 | 3- | |||
6773.4 15 | A D FG | 1,2,3- | 6773.3 15 | | 0 | 0+ | ||
6789.1 6 | A D FG | (2-,3+) | 4174.5 6 | | 2614.522 | 3- | ||
6794.1 15 | D | |||||||
6800.8 20 | D F L | 2504.2 20 | | 4296.560 | 5- | |||
6820.0 4 | A D F | (2-,3-) | 872.2 7 2873.7 4 | 100 85 59 | 5946.77 3946.578 | 1- 4- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
6825.6 7 | D F | |||||||
6831.5 15 | D G | (8-) | ||||||
6845.7 6 | D | (8+) | ||||||
6861.4 6 | D G | 9- | ||||||
6868.0 6 | D G | 10- | ||||||
6877.7 5 | D F | |||||||
6879 6 | G | 7- | ||||||
6884 6 | G | 10- | ||||||
6897.3 4 | A D | 2188.1 5 2668.1 5 | 52 16 100 | 4708.727 4229.590 | 5- 2- | |||
6913 4 | E | 2+ | ≤ 0.85 fs | 6913 4 | | 0 | 0+ | |
6917.5 6 | D | |||||||
6920.7 8 | A | 4306.1 8 | | 2614.522 | 3- | |||
6929.6 5 | A D FG | 2- | 4315.0 5 | | 2614.522 | 3- | ||
6939.9 15 | D | 3- | ||||||
6947 2 | D | |||||||
6969.3 5 | A D FG | 2- | 3771.6 5 | | 3197.711 | 5- | ||
6980 40 | E | 1,2+ | ≈ 1.8 fs | 6980 40 | | 0 | 0+ | |
6988.7 15 | D G | |||||||
6995.1 15 | D G | |||||||
7000 | G | (9+) | ||||||
7001.0 4 | A D F | 3803.3 4 | | 3197.711 | 5- | |||
7020.2 6 | FG | 1- | ||||||
7020.2 4 | A D | (3-) | 1052.3 6 2660.3 6 2696.7 7 2758.6 7 | 38 11 100 19 44 11 55 14 | 5968.55 4358.670 4323.946 4261.871 | 4- 4- 4+ 4- | ||
7034 2 | D | |||||||
7057.9 15 | D | |||||||
7061 5 | D G | 12- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7063.53 20 | AB DEFG L | 1- | 0.025 fs +1-3 | 7063.4 2 | | [E1] | 0 | 0+ |
7083.2 3 | A DEF L | 1- | 0.050 fs 4 | 7083.1 3 | | [E1] | 0 | 0+ |
7086 6 | G | 12- | ||||||
7095.6 3 | D | |||||||
7108 10 | G | (1-,3-) | ||||||
7117.0 3 | D F | (3-) | ||||||
7137.3 4 | A D F | 3-,4- | 4522.7 4 | | 2614.522 | 3- | ||
7143 10 | G | (3+,2-) | ||||||
7146.1 15 | D F | (5-,6-) | ||||||
7157 2 | D | |||||||
7167 2 | D F | |||||||
7177.0 3 | DE | 1 | ≤ 0.57 fs | 7176.9 3 | | 0 | 0+ | |
7191.6 15 | D | |||||||
7196.6 10 | AB D FG | 4582.0 10 | | 2614.522 | 3- | |||
7206.9 5 | AB E G | 1 | ≤ 0.51 fs | 7206.8 5 | | 0 | 0+ | |
7218.6 14 | A D F | 4020.8 14 | | 3197.711 | 5- | |||
7232.2 15 | D F | |||||||
7240 2 | A D F | 1- | ≤ 0.24 fs | 7240 2 | | 0 | 0+ | |
7255.3 15 | D FG | |||||||
7264.4 10 | A G | 4066.6 10 | | 3197.711 | 5- | |||
7265.9 15 | D G | 2+ | ||||||
7278.68 20 | DEFG | 1+ | 0.585 fs 15 | 7278.54 20 | | [M1] | 0 | 0+ |
7280 | B | |||||||
7291.4 23 | D F | |||||||
7301.2 17 | D F | |||||||
7311 2 | F | |||||||
7313 4 | G | (2-,3+) | ||||||
7315.4 20 | A D L | 2+ | 7315.3 20 | | 0 | 0+ | ||
7332.4 8 | A DEF | 1- | 0.016 fs +2-4 | 7332.3 8 | | [E1] | 0 | 0+ |
7334.8 15 | D | 3- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7335.4 15 | F | (5-,6-) | ||||||
7346 3 | D G | |||||||
7360 50 | D e | 2+ | ||||||
7360.1 15 | D F | (5-,6-) | ||||||
7370.92 5 | NOP | 2+ | ||||||
7371.6 17 | D F | |||||||
7378.01 5 | NOP | 2+ | ||||||
7380.17 5 | N | |||||||
7382 9 | D | (4+) | ||||||
7383.96 6 | OP | 2+ | ||||||
7384.55 5 | N P | 1+ | ||||||
7389.0 10 | A D G | 3- | 3913.9 10 | | 3475.078 | 4- | ||
7397.12 6 | NO | (2)+ | ||||||
7398.21 3 | OP | 1 | ||||||
7399.4 11 | BCD F | 4+ | ||||||
7400.68 6 | O | 2+ | ||||||
7405.41 6 | NOP | 1+ | ||||||
7408.5 11 | D F | |||||||
7408.94 5 | NOP | 1- | ||||||
7415 3 | E G | 1- | ≤ 0.17 fs | 7415 3 | | 0 | 0+ | |
7416.04 7 | OP | 2+ | ||||||
7420.9 11 | D F | |||||||
7428.9 11 | D F | |||||||
7430.38 7 | O | 2+ | ||||||
7435.34 9 | O | |||||||
7435.90 5 | NO | 2+ | ||||||
7440.53 5 | NO | 1+ | ||||||
7449.4 12 | D F | (5-,6-) | ||||||
7449.55 5 | N | 0+ | ||||||
7450.45 5 | NO | 2+ | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7455.19 5 | NO | 2+ | ||||||
7459 2 | D FG | 2- | ||||||
7465.79 5 | NOP | 1+ | ||||||
7465.79 6 | NO | 2+ | ||||||
7468.6 6 | D F | 1- | ||||||
7469.18 6 | NOP | 1- | ||||||
7470.94 6 | N | 0+ | ||||||
7479.38 6 | NO | (2+) | ||||||
7482 10 | G | (1-,3-) | ||||||
7482.49 6 | NOP | 1+ | ||||||
7491 | D | 2+ | ||||||
7494.92 8 | NOP | 2+ | ||||||
7495.17 8 | NO | 1+ | ||||||
7497.47 6 | NOP | 1+ | ||||||
7499.41 7 | NO | 1(+) | ||||||
7502.47 7 | N | 0+ | ||||||
7503.70 7 | NO | (2+) | ||||||
7505.0 3 | D F | 1- | ||||||
7506.89 7 | NO | 2+ | ||||||
7508.12 15 | O | (2+) | ||||||
7509 4 | G | 2- | ||||||
7512.58 7 | NO | 1+ | ||||||
7515.38 7 | NO | (1+) | ||||||
7516.29 7 | N | (1+) | ||||||
7517 | D | 3- | ||||||
7517 2 | F | 0-,1- | ||||||
7520.90 7 | NO | 2+ | ||||||
7522.89 7 | NO | 1+ | ||||||
7523.84 7 | N P | (0+,1+) | ||||||
7526.01 10 | NO | 2+ | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7528.79 17 | J | 1080.2 2 1428.0 2 | | 6448.40 6100.69 | (13-) 12+ | |||
7535.57 7 | NO | 1+ | ||||||
7537.60 18 | O | (2+) | ||||||
7538.18 7 | NO | 2+ | ||||||
7546.02 10 | NO | 1+ | ||||||
7546.24 11 | N | 0+ | ||||||
7547.98 10 | NO | 1+ | ||||||
7548.18 7 | NO | 2+ | ||||||
7548.49 11 | NOP | 1- | ||||||
7548.6 6 | DEFG | 1- | ≤ 0.35 fs | 7548.5 6 | | 0 | 0+ | |
7549.09 11 | N | (0+) | ||||||
7553.29 10 | N | (0+) | ||||||
7563.94 11 | NO | (2+) | ||||||
7566.43 10 | N | (0+) | ||||||
7567.89 11 | N | (+) | ||||||
7568.00 8 | N | |||||||
7573 7 | D | |||||||
7574.49 10 | N | 0+ | ||||||
7576.31 10 | N | 2- | ||||||
7577.41 11 | NO | 1+ | ||||||
7578.62 11 | N | (2)- | ||||||
7580.71 11 | N | |||||||
7585.27 10 | NO | 1+ | ||||||
7586.85 23 | O | (1) | ||||||
7587.04 10 | NO | 2+ | ||||||
7590.79 10 | NO | (2)+ | ||||||
7594 7 | D | |||||||
7595.26 11 | N | 0- | ||||||
7596.53 10 | NO | 1+ | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7598.07 11 | N | |||||||
7600.01 11 | NO | (1+) | ||||||
7607.38 11 | NO | 2+ | ||||||
7610.21 11 | N | (1)+ | ||||||
7610.64 11 | NO | (2+) | ||||||
7616.16 10 | NOP | 2+ | ||||||
7616.55 11 | NO | 1+ | ||||||
7621.09 10 | N | 3- | ||||||
7623.07 26 | NOP | 1- | ||||||
7627.20 11 | N | |||||||
7628.77 16 | NO | (1)+ | ||||||
7631 4 | E G | 1- | ≤ 0.57 fs | 7631 4 | | 0 | 0+ | |
7632.03 10 | NO | 1+ | ||||||
7636.02 21 | NO | (2+) | ||||||
7636.4 3 | O | 2+ | ||||||
7640.01 11 | NO | (2+) | ||||||
7642.98 21 | N | (0+) | ||||||
7644.5 2 | N | |||||||
7650.2 | P | |||||||
7651.18 11 | NO | 1+ | ||||||
7651.52 10 | N | (2)+ | ||||||
7653.93 11 | NO | (1+) | ||||||
7655.3 3 | O | (2+) | ||||||
7656 8 | D G | (10+) | ||||||
7656.66 11 | N | 0+ | ||||||
7662.91 11 | NO | 1(+) | ||||||
7664.41 10 | NOP | 1+ | ||||||
7666.32 11 | NO | (1+) | ||||||
7667.81 11 | N | (0+) | ||||||
7670.83 11 | N | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7672.51 11 | NO | (1+) | ||||||
7676.35 11 | N | (2)- | ||||||
7676.59 10 | N | (1-) | ||||||
7680.18 11 | N | |||||||
7680.44 11 | NO | 1+ | ||||||
7683.31 11 | NOP | 1- | ||||||
7683.7 2 | N | (0+) | ||||||
7685.4 5 | DE | 1,2+ | 7685.2 5 | | 0 | 0+ | ||
7685.89 11 | N | 2- | ||||||
7689.63 11 | NO | 2+ | ||||||
7696.02 11 | N | 3- | ||||||
7696.5 3 | N | 1- | ||||||
7698.68 10 | NO | (2)+ | ||||||
7700 10 | G | |||||||
7701.87 10 | NO | 1+ | ||||||
7702.80 10 | N | (2)+ | ||||||
7706.62 11 | N | |||||||
7712.68 10 | N | (2+) | ||||||
7715.95 11 | N | |||||||
7721.52 11 | N | 2- | ||||||
7722.6 24 | DE | 1 | ≤ 0.62 fs | 7722.5 24 | | 0 | 0+ | |
7725.92 11 | N | 2+ | ||||||
7734.87 11 | N | 2+ | ||||||
7736.17 11 | NO | 1+ | ||||||
7738.94 11 | N | (0+) | ||||||
7740 10 | N | |||||||
7743.03 11 | N | (0+) | ||||||
7743.09 12 | N | |||||||
7744.65 11 | NO | 2+ | ||||||
7745.33 11 | NO | (1+) | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7748.55 11 | NO | 2+ | ||||||
7749.60 11 | N | (0+) | ||||||
7751.92 21 | NO | (1+) | ||||||
7757.55 13 | N | |||||||
7761.1 2 | G NO | 2+ | ||||||
7762.1 2 | N | (0)+ | ||||||
7767.5 2 | G NO | 2+ | ||||||
7768.3 2 | G NO | 2+ | ||||||
7771.6 2 | N | 0+ | ||||||
7777.09 14 | N | |||||||
7777.9 2 | NO | (2)+ | ||||||
7780.8 1 | N | 3- | ||||||
7785.78 14 | NO | (2+) | ||||||
7786.4 2 | NO | 2+ | ||||||
7790.0 2 | NO | 1+ | ||||||
7790.8 2 | N | |||||||
7791.56 14 | N | |||||||
7792.9 2 | NO | 1+ | ||||||
7794.2 2 | N | 2- | ||||||
7795.9 2 | N | (2)+ | ||||||
7798.23 14 | N | |||||||
7802.1 2 | N | 0+ | ||||||
7803.40 14 | N | |||||||
7807 6 | G | (1-,2+,3-) | ||||||
7808.13 14 | N | |||||||
7808.76 14 | N | |||||||
7811.13 14 | N | |||||||
7812.0 2 | NO | 2+ | ||||||
7812.9 2 | N | 1- | ||||||
7817.75 15 | NO | 2+ | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7818.21 15 | N | |||||||
7823.15 15 | N | |||||||
7825 8 | D | (10-) | ||||||
7828.3 2 | N | 3- | ||||||
7829.5 2 | N | 1- | ||||||
7830.04 15 | N | |||||||
7830.61 15 | N | |||||||
7831.9 2 | N | (1)+ | ||||||
7832.5 2 | N | |||||||
7837.1 2 | N | (2)- | ||||||
7838.1 2 | N | 3- | ||||||
7839.9 2 | N | |||||||
7840.9 2 | N | |||||||
7844.5 2 | N | |||||||
7845 10 | D G e | 2+ | ||||||
7846.8 2 | N | |||||||
7852 | P | |||||||
7858 | P | |||||||
7869 | P | |||||||
7872 6 | G | (1-,2) | ||||||
7901.9 6 | O | 2+ | ||||||
7904.3 6 | O | 2+ | ||||||
7907.2 6 | OP | 1- | ||||||
7913 3 | DE | 1(-) | ≤ 0.48 fs | 7913 3 | | 0 | 0+ | |
7913.8 6 | OP | 2+ | ||||||
7918 | P | |||||||
7924 3 | G | 2- | ||||||
7961 3 | G | (1-,3-) | ||||||
7965 | P | |||||||
7967.5 2 | N | 3- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7968.5 2 | N | 0+ | ||||||
7970.0 2 | N | (2)+ | ||||||
7971.2 2 | N P | 1- | ||||||
7974.04 19 | J | (15-) | 445.1 2 1230.8 2 | | 7528.79 6743.42 | 14- | ||
7974.2 2 | N | 1+ | ||||||
7977.7 2 | N | 2- | ||||||
7978.8 2 | N | (0+,1+,2+) | ||||||
7980.9 2 | NOP | 1- | ||||||
7981.7 2 | N | (1,2)+ | ||||||
7982.6 2 | N | (1,2)+ | ||||||
7987.3 2 | N | 2- | ||||||
8001 | P | |||||||
8008 3 | D G | 2- | ||||||
8008.2 7 | OP | 2+ | ||||||
8018 | P | 1- | ||||||
8026.95 17 | J | (14-) | 498.0 2 1283.4 2 1578.6 2 | | 7528.79 6743.42 6448.40 | 14- (13-) | ||
8051.1 7 | O | 2+ | ||||||
8065 | P | |||||||
8071.9 7 | N | 2+ | ||||||
8092 | P | |||||||
8102 | P | 1- | ||||||
8109.1 8 | O | 2+ | ||||||
8110 50 | BCD | 4+ | ||||||
8144.5 8 | OP | 2+ | ||||||
8166 8 | D | 3- | ||||||
8167.0 8 | O | 2+ | ||||||
8185 | P | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8202 | P | |||||||
8206 | P | |||||||
8212 | P | 1- | ||||||
8219.9 9 | OP | 1 | ||||||
8220 | D | (1-) | ||||||
8252 | P | |||||||
8264 | P | |||||||
8264.38 23 | J | 237.5 2 | | 8026.95 | (14-) | |||
8274 | P | 1- | ||||||
8293 | P | |||||||
8310 | P | |||||||
8319 | P | 1- | ||||||
8338 | P | |||||||
8343 | P | |||||||
8350 50 | D | 3- | ||||||
8350.79 19 | J | (15-) | 323.7 2 376.8 2 1607.6 2 | | 8026.95 7974.04 6743.42 | (14-) (15-) 14- | ||
8358 | P | |||||||
8365 | P | 1- | ||||||
8369 8 | D | 12+ | ||||||
8400 | G | |||||||
8470 | D | 3- | ||||||
8493 20 | V | |||||||
8520 20 | V | |||||||
8562.94 24 | J | (16-) | 212.3 2 | | 8350.79 | (15-) | ||
8620 | D | 2+ | ||||||
8723.50 23 | J | 459.2 2 1980.0 2 | | 8264.38 6743.42 | 14- | |||
8750 | D | 2+ | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8812.70 23 | J | (14-,15,16-) | 249.9 2 785.6 2 | | 8562.94 8026.95 | (16-) (14-) | ||
8860 50 | D G | 2+ | ||||||
8950 | D G | 2+ | ||||||
9061.2 3 | J | (17+) | 2317.8 2 | | 6743.42 | 14- | ||
9103.1 3 | J | 42 290.4 2 | | 9061.2 8812.70 | (17+) (14-,15,16-) | |||
9180 | D | 3- | ||||||
9340 50 | D | 2+ | ||||||
9380 | DE | 3- | ||||||
9394.4 4 | J | 291.3 2 | | 9103.1 | ||||
9520 | D G | 2+ | ||||||
10070 30 | E G | (1,2) | ||||||
10136.8 5 | J | 742.4 2 | | 9394.4 | ||||
10196.1 11 | J | 801.7 | | 9394.4 | ||||
10342.0 11 | J | 947.6 | | 9394.4 | ||||
10357.4 11 | J | 963.0 | | 9394.4 | ||||
10372.2 11 | J | 235.4 | | 10136.8 | ||||
10552.4 15 | J | 356.3 | | 10196.1 | ||||
10600 40 | CDE G | (1,2) | ||||||
10.9E+3 3 | BCD e | 2+ | ||||||
11270 | E | (1,2) | ||||||
11361.0 15 | J | 1019.0 | | 10342.0 | ||||
11450 | E | (1,2) | ||||||
11.60E+3 10 | E | |||||||
11958.1 17 | J | 597.0 | | 11361.0 | ||||
12250 | B D | 4+ | ||||||
12949.6 17 | J | 991.4 1588.7 | | 11958.1 11361.0 | ||||
13.5E+3 1 | B DE G P | 1- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
13675.0 20 | J | 725.4 | | 12949.6 | ||||
13.96E+3 20 | BCD G | 0+ | ||||||
16000 | B | 6+ | ||||||
19.6E+3 5 | B D Q | 3- | ||||||
22.1E+3 3 | B Q | 1- | ||||||
23.94E+3 20 | N T | |||||||
24.48E+3 20 | N T | |||||||
26.9E+3 2 | B | 2+ | ||||||
27200 | T |
E(level): From a least-squares fit to the adopted Eγ values. For levels with no observed deexciting gammas, the energies are weighted averages of values from all reactions. For levels above the neutron separation energy, the energies from the resonance data in (n,γ) E=resonance, (n,X), and (γ,n), have been calculated using S(n)=7367.87 5. In addition to the levels shown, a level at 9300 has been reported in 204Hg(16O,12C). Levels in (t,p) are reported up to 8520; however, the resolution and the quoted uncertainties are such that it is not possible to make a unique correspondence with the adopted levels above 5000, except for the 0+ level at 5241, and for the two highest levels at 8493 20 and 8520 20 which are not reported in other reactions. The same holds for the (p,t) reaction, which reports levels up to 6726, and the (t,α) reaction for levels above 4200
Jπ(level): Assignments for levels above S(n), except where the argument is explicitly given, are from 207Pb(n,X) based on transmission measurements, from 207Pb(n,γ) E=resonance based on Γγ0/Γ, or from 208Pb(γ,n) based on neutron polarization measurements. See the source datasets for details. For some levels, where a single deexciting transition is known, this fact is stated in a Jπ comment even though the resulting Jπ range is too large to Be useful in the Jπ field
T1/2(level): From (n,n’γ), except where noted otherwise
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
2614.522 | 3- | 16.7 ps 3 | 2614.511 10 | E3 | 0.00247 | B(E3)(W.u.)=33.8 6, α=0.00247 | |
3197.711 | 5- | 294 ps 15 | 583.187 2 | E2 | 0.0205 | B(E2)(W.u.)=0.382 20, α=0.0205 | |
3475.078 | 4- | 4 ps 3 | 277.371 5 | M1+E2 | +0.017 11 | 0.533 | B(E2)(W.u.)=0.10 +35-10, B(M1)(W.u.)=0.07 +22-3, α=0.533 |
4- | 4 ps 3 | 860.557 4 | M1+E2 | +0.014 8 | 0.0264 | B(E2)(W.u.)=0.0005 +15-4, B(M1)(W.u.)=0.005 +33-2, α=0.0264 | |
3708.451 | 5- | 233.33 6 | M1+E2 | 0.6 AP | 0.70 | α0.70 AP | |
5- | 510.74 5 | M1+E2 | -0.052 45 | 0.1027 | α=0.1027 16 | ||
3919.966 | 6- | > 690 fs | 211.51 2 | M1(+E2) | +0.04 +7-6 | 1.126 | B(E2)(W.u.)<94, B(M1)(W.u.)<1.0, α=1.126 16 |
6- | > 690 fs | 722.252 8 | M1+E2 | +0.31 7 | 0.0390 | B(E2)(W.u.)<2.5, B(M1)(W.u.)<0.029, α=0.0390 12 | |
3946.578 | 4- | > 430 fs | 238.22 3 | [M1+E2] | -0.06 6 | B(E2)(W.u.)<40, B(M1)(W.u.)<0.61 | |
4- | > 430 fs | 471.498 14 | [M1+E2] | 0.125 | α=0.125 2 | ||
4- | > 430 fs | 748.845 12 | [M1+E2] | +0.072 25 | 0.0377 | B(E2)(W.u.)<0.42, B(M1)(W.u.)<0.077, α=0.0377 1 | |
3961.162 | 5- | 252.755 12 | M1+E2 | -0.35 10 | 0.633 | α=0.633 27 | |
5- | 763.429 9 | M1+E2 | -0.12 5 | 0.0356 | α=0.0356 6 | ||
3995.438 | 4- | > 690 fs | 797.741 10 | [M1+E2] | +0.34 5 | 0.0299 | B(E2)(W.u.)<1.0, B(M1)(W.u.)<0.013, α=0.0299 5 |
4- | > 690 fs | 1380.889 12 | [M1(+E2)] | +0.000 +31-21 | 0.0079 | B(M1)(W.u.)<0.0092, α=0.0079 | |
4037.443 | 7- | > 690 fs | 117.53 13 | [M1,E2] | 4.6 | α=4.6 13 | |
7- | > 690 fs | 839.734 9 | [E2] | 0.0094 | B(E2)(W.u.)<17, α=0.0094 | ||
4085.52 | 2+ | 0.80 fs 4 | 1471.5 4 | [E1] | 0.00143 | B(E1)(W.u.)=0.00035 12, α=0.00143 | |
2+ | 0.80 fs 4 | 4085.47 4 | [E2] | 0.00165 | B(E2)(W.u.)=8.4 5, α=0.00165 | ||
4125.347 | 5- | > 490 fs | 164.34 20 | [M1,E2] | 1.6 | α=1.6 7 | |
5- | > 490 fs | 179.5 6 | [M1,E2] | 1.2 | α=1.2 6 | ||
5- | > 490 fs | 416.79 6 | [M1+E2] | +0.1 +8-4 | 0.15 | B(E2)(W.u.)<7.2, B(M1)(W.u.)<0.025, α=0.15 3 | |
5- | > 490 fs | 650.207 14 | [M1+E2] | 0.035 | α=0.035 20 | ||
5- | > 490 fs | 927.650 8 | [M1+E2] | 0.018 | α=0.018 3 | ||
4229.590 | 2- | 333 fs 28 | 1615.068 15 | [M1+E2] | +0.18 +9-10 | 0.00536 | B(E2)(W.u.)=0.05 6, B(M1)(W.u.)=0.0125 12, α=0.00536 8 |
2- | 333 fs 28 | 4229.49 9 | M2 | 0.00235 | B(M2)(W.u.)=0.34 5, α=0.00235 | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
4296.560 | 5- | 201 fs +49-35 | 171.00 20 | [M1,E2] | 1.4 | α=1.4 6 | |
5- | 201 fs +49-35 | 588.096 6 | [M1+E2] | -0.18 +9-8 | 0.0694 | B(E2)(W.u.)=9 9, B(M1)(W.u.)=0.268 9, α=0.0694 19 | |
5- | 201 fs +49-35 | 821.540 13 | [M1+E2] | 0.020 | α=0.020 10 | ||
5- | 201 fs +49-35 | 1098.85 4 | [M1,E2] | 0.010 | α=0.010 4 | ||
4323.946 | 4+ | 11.7 ps +15-18 | 362.81 7 | [E1] | 0.0191 | B(E1)(W.u.)=4.2E-5 +8-7, α=0.0191 | |
4+ | 11.7 ps +15-18 | 848.88 4 | [E1] | 0.00338 | B(E1)(W.u.)=5.4E-7 +9-8, α=0.00338 | ||
4+ | 11.7 ps +15-18 | 1126.236 13 | [E1+M2] | +0.042 21 | 0.02077 | B(E1)(W.u.)=9.558E-6 17, B(M2)(W.u.)=0.06 6, α=0.02077 6 | |
4+ | 11.7 ps +15-18 | 1709.6 2 | [E2] | 0.00258 | B(E2)(W.u.)=0.00019 +5-4, α=0.00258 | ||
4+ | 11.7 ps +15-18 | 4324.3 4 | [E4] | 0.00121 | B(E4)(W.u.)=18 1, α=0.00121 | ||
4383.285 | 6- | > 690 fs | 463.30 10 | [M1+E2] | -0.69 +15-19 | B(E2)(W.u.)<8.5, B(M1)(W.u.)<0.0096 | |
4610.748 | 8+ | 3.2 ns 5 | 573.41 8 | [E1+M2] | +0.15 +30-26 | 0.024 | B(E1)(W.u.)=9.3E-9 25, B(M2)(W.u.)=0.003 +12-3, α=0.024 17 |
8+ | 3.2 ns 5 | 1413.026 13 | [E3] | 0.00728 | B(E3)(W.u.)=12.6 20, α=0.00728 | ||
4698.323 | 3- | 139 fs +42-28 | 436.41 10 | [M1,E2] | 0.10 | α=0.10 6 | |
3- | 139 fs +42-28 | 443.57 8 | [M1+E2] | -0.13 +16-14 | 0.146 | B(E2)(W.u.)=9 +22-9, B(M1)(W.u.)=0.297 13, α=0.146 4 | |
3- | 139 fs +42-28 | 468.76 7 | [M1,E2] | 0.08 | α=0.08 4 | ||
3- | 139 fs +42-28 | 612.88 15 | [E1] | 0.00632 | B(E1)(W.u.)=4.1E-5 +15-18, α=0.00632 | ||
3- | 139 fs +42-28 | 647.25 9 | [M1,E2] | 0.036 | α=0.036 20 | ||
3- | 139 fs +42-28 | 702.86 14 | [M1,E2] | 0.029 | α=0.029 15 | ||
3- | 139 fs +42-28 | 1223.27 2 | [M1+E2] | 0.008 | α=0.008 3 | ||
3- | 139 fs +42-28 | 1500.49 3 | [E2] | 0.00316 | B(E2)(W.u.)=1.1 +3-4, α=0.00316 | ||
3- | 139 fs +42-28 | 2083.90 4 | [M1,E2] | 0.0026 | α=0.0026 6 | ||
3- | 139 fs +42-28 | 4697.88 14 | [E3] | 0.00174 | B(E3)(W.u.)=1.2 +3-5, α=0.00174 | ||
4708.727 | 5- | 0.24 ps +20-9 | 412.17 4 | [M1,E2] | 0.12 | α=0.12 7 | |
5- | 0.24 ps +20-9 | 714.0 10 | [M1,E2] | 0.028 | α=0.028 15 | ||
5- | 0.24 ps +20-9 | 748.3 5 | [M1,E2] | 0.025 | α=0.025 13 | ||
5- | 0.24 ps +20-9 | 1000.51 12 | [M1+E2] | -0.19 +7-8 | 0.0175 | B(E2)(W.u.)=0.4 3, B(M1)(W.u.)=0.0332 9, α=0.0175 3 | |
5- | 0.24 ps +20-9 | 1511.00 2 | [M1+E2] | 0.0048 | α=0.0048 16 | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
4841.60 | 1- | 0.068 fs +21-15 | 4841.46 12 | [E1] | B(E1)(W.u.)=0.021 3 | ||
4895.23 | 10+ | 0.50 µs 5 | 34.4 | [E2] | 1003 | B(E2)(W.u.)=0.08 3, α=1003 | |
10+ | 0.50 µs 5 | 284.49 5 | [E2] | 0.136 | B(E2)(W.u.)=0.0047 8, α=0.136 | ||
10+ | 0.50 µs 5 | 857.71 10 | [E3] | 0.0223 | B(E3)(W.u.)=0.32 8, α=0.0223 | ||
4937.19 | 3- | 17.3 fs +35-28 | 4937.19 4 | [E3] | B(E3)(W.u.)=25 +6-25 | ||
4962.428 | 4(-),5(+) | > 440 fs | 1764.71 3 | [M1+E2] | +0.78 +22-32 | B(E2)(W.u.)<0.37, B(M1)(W.u.)<0.0048 | |
4973.918 | 3- | 166 fs 21 | 275.72 24 | [M1,E2] | 0.34 | α=0.34 20 | |
3- | 166 fs 21 | 615.7 5 | [M1,E2] | 0.041 | α=0.041 22 | ||
3- | 166 fs 21 | 712.13 25 | [M1,E2] | 0.028 | α=0.028 15 | ||
3- | 166 fs 21 | 719.19 4 | [M1,E2] | 0.028 | α=0.028 14 | ||
3- | 166 fs 21 | 1265.0 6 | [E2] | 0.00427 | B(E2)(W.u.)=0.19 7, α=0.00427 | ||
3- | 166 fs 21 | 1499.10 10 | [M1,E2] | 0.0048 | α=0.0048 17 | ||
3- | 166 fs 21 | 1776.10 5 | [E2] | 0.00244 | B(E2)(W.u.)=1.05 14, α=0.00244 | ||
3- | 166 fs 21 | 2359.39 2 | [M1+E2] | 0.0022 | α=0.0022 5 | ||
3- | 166 fs 21 | 4974.1 6 | [E3] | 0.00060 | B(E3)(W.u.)=0.17 7, α=0.00060 | ||
5037.536 | 3- | 90 fs 7 | 5037.4 7 | [E3] | B(E3)(W.u.)=0.65 10 | ||
5069.31 | 10+ | 174.13 9 | M1(+E2) | 0.6 LT | 1.78 | α=1.78 17 | |
5127.356 | 2-,3- | 64 fs 3 | 2512.818 12 | [M1+E2] | +1.3 +9-6 | B(E2)(W.u.)=0.7 4, B(M1)(W.u.)=0.007 7 | |
5213.007 | 6+ | 76 fs +21-14 | 2015.5 5 | [E1] | B(E1)(W.u.)=0.00012 +3-4 | ||
5216.214 | 4+ | 32 fs 3 | 2601.69 2 | [E1+M2] | +0.095 +45-43 | B(E1)(W.u.)=0.00026 3, B(M2)(W.u.)=1.6 15 | |
5241.1 | 0+ | > 690 fs | 2626.6 3 | [E3] | B(E3)(W.u.)<635 | ||
5245.246 | 3- | 17 fs +7-6 | 921.5 2 | [E1] | B(E1)(W.u.)=0.00025 9 | ||
3- | 17 fs +7-6 | 5245.0 7 | [E3] | B(E3)(W.u.)=2.3 8 | |||
5286.484 | 2,3- | 76 fs 7 | 2671.942 13 | [D+Q] | +0.05 +8-3 | ||
5291.90 | 1- | 0.049 fs +28-18 | 5291.74 13 | [E1] | B(E1)(W.u.)=0.021 5 | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
5382.82 | 3+,4+,5+ | 37 fs +7-6 | 1387.37 3 | [E1] | B(E1)(W.u.)=0.0020 3 | ||
5384.59 | 3- | 76 fs 14 | 5384.37 12 | [E3] | B(E3)(W.u.)=3.8 | ||
5481.87 | 5- | 90 fs 14 | 2867.35 3 | [E2+M3] | +0.042 +53-32 | B(E2)(W.u.)=0.24 4, B(M3)(W.u.)=4.×102 +10-4 | |
5511.78 | 1- | 0.0194 fs +12-18 | 5511.70 14 | [E1] | B(E1)(W.u.)=0.058 +4-3 | ||
5516.714 | 3- | 40.9 fs 21 | 2902.17 2 | [M1+E2] | -0.94 +15-16 | B(E2)(W.u.)=0.43 8, B(M1)(W.u.)=0.0117 19 | |
5548.113 | 2- | 83 fs 7 | 5547.6 3 | [M2] | B(M2)(W.u.)=0.051 9 | ||
5561.31 | 2+ | 38 fs 4 | 2946.79 5 | [M1+E2] | +0.23 +23-17 | B(E2)(W.u.)=0.03 +7-3, B(M1)(W.u.)=0.0158 24 | |
2+ | 38 fs 4 | 5560.8 2 | [E2] | B(E2)(W.u.)=0.0101 14 | |||
5563.73 | 3- | 44 fs +9-7 | 2366.3 3 | [E2] | B(E2)(W.u.)=0.86 +18-21 | ||
5639.55 | 1- | 0.13 ps +12-5 | 5639.7 2 | [E1] | B(E1)(W.u.)=0.008 4 | ||
5658.51 | 5- | 31 fs +7-6 | 3044.0 2 | [E2] | B(E2)(W.u.)=0.063 +16-18 | ||
5690.117 | 4+ | 46 fs 4 | 3075.57 2 | [E1+M2] | -0.031 +31-21 | B(E1)(W.u.)=0.000144 13, B(M2)(W.u.)=0.07 +14-7 | |
5715.53 | 2+ | 3.7 fs 11 | 3101.07 10 | [E1] | B(E1)(W.u.)=0.00022 +9-6 | ||
2+ | 3.7 fs 11 | 5715.1 2 | [E2] | B(E2)(W.u.)=0.30 +12-8 | |||
5721.51 | 7- | 28 fs +9-7 | 1297.86 3 | [E1] | B(E1)(W.u.)=0.0031 +8-11 | ||
5777.96 | 2-,3- | 15.9 fs 14 | 1523.03 15 | [D+Q] | -1.3 +6-42 | ||
2-,3- | 15.9 fs 14 | 5777.4 3 | [M2,E3] | B(E3)(W.u.)=5.1 11, B(M2)(W.u.)=0.32 7 | |||
5885.55 | 3- | 13.9 fs 14 | 1588.5 5 | [E2] | B(E2)(W.u.)=7 3 | ||
5923.67 | 2- | 104 fs +90-42 | 5922.6 8 | [E1,M2] | B(E1)(W.u.)=2.8E-7 +19-14, B(M2)(W.u.)=0.037 +26-20 | ||
5968.55 | 4- | 7.6 fs +42-35 | 1644.1 8 | [E1] | B(E1)(W.u.)=4E-5 +4-2 | ||
4- | 7.6 fs +42-35 | 1762.6 3 | [E2] | B(E2)(W.u.)=1.5 +7-9 | |||
6009.75 | 3- | 11 fs +5-4 | 1685.7 4 | [E1] | B(E1)(W.u.)=0.00036 +14-17 | ||
3- | 11 fs +5-4 | 1924.19 9 | [E1] | B(E1)(W.u.)=0.00046 +18-22 | |||
6086.56 | 1- | 37 fs +25-15 | 841.40 20 | [E2] | B(E2)(W.u.)=11 +5-11 | ||
1- | 37 fs +25-15 | 1112.70 6 | [E2] | B(E2)(W.u.)=15 +7-11 | |||
1- | 37 fs +25-15 | 1388.19 13 | [E2] | B(E2)(W.u.)=10 +4-10 | |||
1- | 37 fs +25-15 | 1831.77 7 | [E2] | B(E2)(W.u.)=1.8 +8-12 | |||
1- | 37 fs +25-15 | 2035.30 17 | [E2] | B(E2)(W.u.)=1.4 +6-10 | |||
1- | 37 fs +25-15 | 3471.9 2 | [E2] | B(E2)(W.u.)=0.026 +13-19 | |||
1- | 37 fs +25-15 | 6085.4 10 | [E1] | B(E1)(W.u.)=1.8E-7 +13-16 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
6193.1 | 2+ | 0.62 fs 5 | 6193.1 4 | [E2] | B(E2)(W.u.)=1.36 11 | ||
6361.6 | 1- | ≤ 0.30 fs | 6361.5 1 | [E1] | B(E1)(W.u.)=0.0028 3 | ||
6486.5 | 1- | 0.78 fs +37-23 | 512.98 25 | [E1] | B(E1)(W.u.)=0.26 4 | ||
1- | 0.78 fs +37-23 | 3871.7 7 | [E2] | B(E2)(W.u.)=1.6 10 | |||
1- | 0.78 fs +37-23 | 6485.9 12 | [E1] | B(E1)(W.u.)=0.00063 19 | |||
6719.8 | 1- | 0.052 fs +6-12 | 6719.7 5 | B(E1)(W.u.)=0.0121 +18-11 | |||
7063.53 | 1- | 0.025 fs +1-3 | 7063.4 2 | [E1] | B(E1)(W.u.)=0.0218 +14-20 | ||
7083.2 | 1- | 0.050 fs 4 | 7083.1 3 | [E1] | B(E1)(W.u.)=0.0108 9 | ||
7278.68 | 1+ | 0.585 fs 15 | 7278.54 20 | [M1] | B(M1)(W.u.)=0.098 3 | ||
7332.4 | 1- | 0.016 fs +2-4 | 7332.3 8 | [E1] | B(E1)(W.u.)=0.031 +5-3 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
2614.522 | 3- | 16.7 ps 3 | μ=+1.9 2 (1973ScYX,1969Bo12,2005St24), Q=-0.34 15 (1984Ve07,1983Sp02,2005St24) Isomer shift=6.25 28 from muonic atom (1977Sh07). |
3197.711 | 5- | 294 ps 15 | μ=+0.11 4 (1969Bo01,2005St24) configuration=ν2g9/2ν3p1/2-1 + ν2g9/2ν2f5/2-1 + ν2g9/2ν3p3/2-1 + π1h9/2π3s1/2-1. |
3475.078 | 4- | 4 ps 3 | configuration=ν2g9/2ν3p1/2-1. |
3708.451 | 5- | configuration=ν2g9/2ν2f5/2-1 + ν2g9/2ν3p1/2-1 + ν1i11/2ν3p1/2-1 + π1h9/2π3s1/2-1 + π1h9/2π2d3/2-1. | |
3919.966 | 6- | > 690 fs | configuration=ν2g9/2ν2f5/2-1. |
3946.578 | 4- | > 430 fs | configuration=π1h9/2π3s1/2-1 + π1h9/2π2d3/2-1 + ν2g9/2ν2f5/2-1. |
3961.162 | 5- | configuration=π1h9/2π3s1/2-1 + ν2g9/2ν2f5/2-1. | |
3995.438 | 4- | > 690 fs | configuration=π1h9/2π3s1/2-1 + ν2g9/2ν2f5/2-1. |
4037.443 | 7- | > 690 fs | configuration=ν2g9/2ν2f5/2-1. |
4085.52 | 2+ | 0.80 fs 4 | Q=-0.7 3 (1984Ve07,2005St24) configuration=π1h9/2π1h11/2-1. |
4125.347 | 5- | > 490 fs | configuration=ν2g9/2ν2f5/2-1 + ν1i11/2ν3p1/2-1 + π1h9/2π3s1/2-1 + π1h9/2π2d3/2-1. |
4144 | + | configuration=π1h9/2π1h11/2-1. | |
4180.414 | 5- | 319 fs 35 | configuration=ν2g9/2ν3p3/2-1 + ν1i11/2ν3p1/2-1 + π1h9/2π3s1/2-1 + π1h9/2π2d3/2-1. |
4206.277 | 6- | > 690 fs | configuration=ν1i11/2ν3p1/2-1 + ν2g9/2ν2f5/2-1 π1h9/2π2d3/2-1. |
4229.590 | 2- | 333 fs 28 | configuration=ν3d5/2ν3p1/2-1. |
4254.795 | 3- | 97 fs 7 | configuration=ν3d5/2ν3p1/2-1. |
4261.871 | 4- | > 520 fs | For the neutron configuration see reference 24 of 2006He21. |
4296.560 | 5- | 201 fs +49-35 | configuration=ν1i11/2ν3p1/2-1 + ν2g9/2ν3p3/2-1 + π1h9/2π2d3/2-1. |
4323.946 | 4+ | 11.7 ps +15-18 | configuration=π1h9/2π1h11/2-1. |
4358.670 | 4- | 194 fs 21 | For the neutron configuration see reference 24 of 2006He21. |
4383.285 | 6- | > 690 fs | configuration=π1h9/2π2d3/2-1 + ν1i11/2ν3p1/2-1 + ν2g9/2ν3p3/2-1 + ν2g9/2ν2f5/2-1. |
4423.647 | 6+ | > 110 fs | configuration=π1h9/2π1h11/2-1. |
4447 | - | configuration=π1h9/2π2d3/2-1. | |
4480.746 | 6- | 97 fs 7 | configuration=π1h9/2π2d3/2-1 + ν2g9/2ν3p3/2-1 + ν1i11/2ν3p1/2-1. |
4610.748 | 8+ | 3.2 ns 5 | configuration=ν1j15/2ν3p1/2-1 + π1h9/2π1h11/2-1. |
E(level) | Jπ(level) | T1/2(level) | Comments |
4680.266 | 7- | > 690 fs | configuration=ν1i11/2ν2f5/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. |
4698.323 | 3- | 139 fs +42-28 | configuration=ν3d5/2ν3p1/2-1 + π1h9/2π2d3/2-1 + ν1i11/2ν2f5/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. |
4708.727 | 5- | 0.24 ps +20-9 | configuration=π1h9/2π2d3/2-1 + ν1i11/2ν2f5/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. |
4711.817 | 4- | > 340 fs | configuration=ν1i11/2ν2f5/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. |
4761.956 | 6- | 0.26 ps +18-9 | configuration=ν1i11/2ν2f5/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. |
4841.60 | 1- | 0.068 fs +21-15 | configuration=ν4s1/2ν3p1/2-1 + ν3d3/2ν3p1/2-1. |
4860.78 | 8+ | > 22 fs | configuration=ν1j15/2ν3p1/2-1 + π1h9/2π1h11/2-1. |
4867.91 | 7+ | > 97 fs | configuration=ν1j15/2ν3p1/2-1. |
4895.23 | 10+ | 0.50 µs 5 | configuration=π1h9/2π1h11/2-1. |
4918.8 | 8- | configuration=ν1i11/2ν2f5/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. | |
4937.19 | 3- | 17.3 fs +35-28 | configuration=ν3d5/2ν3p1/2-1 + ν2g7/2ν3p1/2-1 and π1h9/2π2d5/2-1. |
4973.918 | 3- | 166 fs 21 | configuration=ν3d5/2ν3p1/2-1. |
4992.5 | (2)- | configuration=ν3d5/2ν3p1/2-1. | |
5010.43 | 9+ | configuration=ν2g9/2ν1i13/2-1. | |
5037.536 | 3- | 90 fs 7 | configuration=ν3d5/2ν3p1/2-1. |
5069.31 | 10+ | configuration=π1h9/2π1h11/2-1. | |
5074.81 | 69 fs +13-10 | Jπ(level): From a comparison of the branchings in (n,n’γ) and (d,pγ), the evaluator proposes two levels at 5074. The 5074.803 is seen in (n,n’γ) and the 5075.78 in (n,n’γ) and (d,pγ). The (d,p) level at 5074.8 4 presumably corresponds to the (d,pγ) level. The (p,p’) level at 5074.7 5 could correspond to either or both members of the doublet. 2006He21 determine Jπ=5- with configuration=ν1i11/2ν3p3/2-1 for the (p,p’) level. See the comment on, for example, the 5080 level, for the Jπ assignment. | |
5075.78 | Jπ(level): From a comparison of the branchings in (n,n’γ) and (d,pγ), the evaluator proposes two levels at 5074. The 5074.803 is seen in (n,n’γ) and the 5075.78 in (n,n’γ) and (d,pγ). The (d,p) level at 5074.8 4 presumably corresponds to the (d,pγ) level. The (p,p’) level at 5074.7 5 could correspond to either or both members of the doublet. 2006He21 determine Jπ=5- with configuration=ν1i11/2ν3p3/2-1 for the (p,p’) level. See the comment on, for example, the 5080 level, for the Jπ assignment. | ||
5079.912 | 6- | 111 fs +28-21 | configuration=ν1i11/2ν3p3/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. |
5085.470 | 7- | > 229 fs | configuration=ν1i11/2ν3p3/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. L(d,3He)=5 for E=5084 2 gives configuration=π1h9/2π1h11/2-1 for the 5085.47 and/or 5087.9 levels. |
5087.9 | 3- | Jπ(level): L(d,3He)=5 for E=5084 2 gives configuration=π1h9/2π1h11/2-1 for the 5085.47 and/or 5087.9 levels. | |
5092.99 | 8+ | > 690 fs | configuration=π1h9/2π1h11/2-1 + ν1j15/2νlj-1 with a 3p1/2, 2f5/2, or 3p3/2 neutron hole state. |
5127.356 | 2-,3- | 64 fs 3 | configuration=ν3d5/2ν3p1/2-1 + π1h9/2π2d5/2-1. |
5162.05 | 9+ | configuration=π1h9/2π1h11/2-1. | |
5193.428 | 5+ | > 319 fs | configuration=π1h9/2π1h11/2-1. Jπ(level): L(d,3He)=5 for E=5191 5 gives configuration=π1h9/2π1h11/2-1 for the 5193.4 and 5195.37 levels. L(d,3He)=5 for E=5210 5 gives configuration=π1h9/2π1h11/2-1 for the 5213.007 and 5216.214 levels. α comparison of the spectroscopic factor for these (d,3He) peaks with those for the resolved (t,αγ) peaks shows that in each case both levels are being populated in (d,3He). From the observed γ decay modes and the spectroscopic factors in (t,αγ), 1997Sc21 assign the Jπ values as shown. The evaluator adopts these assignments. |
E(level) | Jπ(level) | T1/2(level) | Comments |
5195.054 | 3-,4- | 187 fs +42-35 | configuration=ν2g7/2ν3p1/2-1. |
5195.37 | 7+ | > 690 fs | configuration=π1h9/2π1h11/2-1 + ν1j15/2νlj-1 with a 3p1/2, 2f5/2, or 3p3/2 neutron hole state. Jπ(level): L(d,3He)=5 for E=5191 5 gives configuration=π1h9/2π1h11/2-1 for the 5193.4 and 5195.37 levels. L(d,3He)=5 for E=5210 5 gives configuration=π1h9/2π1h11/2-1 for the 5213.007 and 5216.214 levels. α comparison of the spectroscopic factor for these (d,3He) peaks with those for the resolved (t,αγ) peaks shows that in each case both levels are being populated in (d,3He). From the observed γ decay modes and the spectroscopic factors in (t,αγ), 1997Sc21 assign the Jπ values as shown. The evaluator adopts these assignments. |
5213.007 | 6+ | 76 fs +21-14 | configuration=π1h9/2π1h11/2-1. Jπ(level): L(d,3He)=5 for E=5191 5 gives configuration=π1h9/2π1h11/2-1 for the 5193.4 and 5195.37 levels. L(d,3He)=5 for E=5210 5 gives configuration=π1h9/2π1h11/2-1 for the 5213.007 and 5216.214 levels. α comparison of the spectroscopic factor for these (d,3He) peaks with those for the resolved (t,αγ) peaks shows that in each case both levels are being populated in (d,3He). From the observed γ decay modes and the spectroscopic factors in (t,αγ), 1997Sc21 assign the Jπ values as shown. The evaluator adopts these assignments. |
5213.98 | (5-) | 14 fs 3 | configuration=ν2d5/2νlj-1. |
5216.214 | 4+ | 32 fs 3 | configuration=π1h9/2π1h11/2-1. Jπ(level): L(d,3He)=5 for E=5191 5 gives configuration=π1h9/2π1h11/2-1 for the 5193.4 and 5195.37 levels. L(d,3He)=5 for E=5210 5 gives configuration=π1h9/2π1h11/2-1 for the 5213.007 and 5216.214 levels. α comparison of the spectroscopic factor for these (d,3He) peaks with those for the resolved (t,αγ) peaks shows that in each case both levels are being populated in (d,3He). From the observed γ decay modes and the spectroscopic factors in (t,αγ), 1997Sc21 assign the Jπ values as shown. The evaluator adopts these assignments. |
5234 | + | configuration=π1h9/2π1h11/2-1. | |
5235.37 | (11+) | 1993Sc08 propose configuration=ν2g9/2ν1i13/2-1. Jπ(level): Based on γ decay pattern, available shell-model states, and shell-model calculations involving two-particle two-hole excitations using semi-empirical effective interactions (2004Br19, 2001Wr02, 1993Sc08). | |
5239.3 | 4- | configuration=π2f7/2π2d3/2-1 + ν1i11/2ν3p3/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. | |
5245.246 | 3- | 17 fs +7-6 | configuration=ν3d5/2ν3p1/2-1. |
5260 | 9+ | configuration=π1h9/2π1h11/2-1. | |
5276.418 | 4- | 44 fs +6-5 | configuration=π1h9/2π2d5/2-1 + ν1i11/2ν3p3/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. |
5280.47 | 0- | > 319 fs | configuration=ν4s1/2ν3p1/2-1 with a small admixture of configuration=ν3d5/2ν2f5/2-1. |
5291 | 11+ | configuration=ν2g9/2ν1i13/2-1. | |
5291.90 | 1- | 0.049 fs +28-18 | configuration=ν4s1/2ν3p1/2-1. |
5317.041 | (3)+ | > 690 fs | XREF: F(1513). Jπ(level): L(p,p’)=3, with E=5321 4, suggesting Jπ=3- for the 5317.041, 5317.2, or 5326.7 levels. L(d,3He)=5 for 5314 3 gives π=+ for one or both members of the 5317 doublet. In the (d,pγ),(t,αγ) work, the 5317.041 level is seen only in (t,αγ) and the 5317.2 level only in (d,pγ). The evaluator assumes that the (t,αγ) and (d,3He) works are populating the same level, thus π=+ for the 5317.041 level. The 5326.7 level resonates strongly at the ν1j15/2 resonance in (p,p’) and thus has π=+, given the available negative parity neutron hole states. This leaves the 5317.7 level as the possible candidate for Jπ=3-. |
5317.2 | Jπ(level): L(p,p’)=3, with E=5321 4, suggesting Jπ=3- for the 5317.041, 5317.2, or 5326.7 levels. L(d,3He)=5 for 5314 3 gives π=+ for one or both members of the 5317 doublet. In the (d,pγ),(t,αγ) work, the 5317.041 level is seen only in (t,αγ) and the 5317.2 level only in (d,pγ). The evaluator assumes that the (t,αγ) and (d,3He) works are populating the same level, thus π=+ for the 5317.041 level. The 5326.7 level resonates strongly at the ν1j15/2 resonance in (p,p’) and thus has π=+, given the available negative parity neutron hole states. This leaves the 5317.7 level as the possible candidate for Jπ=3-. | ||
5326.6 | + | configuration=π1h9/2π1h11/2-1 + ν1j15/2νlj-1 with a 3p1/2, 2f5/2, or 3p3/2 neutron hole state. Jπ(level): L(p,p’)=3, with E=5321 4, suggesting Jπ=3- for the 5317.041, 5317.2, or 5326.7 levels. L(d,3He)=5 for 5314 3 gives π=+ for one or both members of the 5317 doublet. In the (d,pγ),(t,αγ) work, the 5317.041 level is seen only in (t,αγ) and the 5317.2 level only in (d,pγ). The evaluator assumes that the (t,αγ) and (d,3He) works are populating the same level, thus π=+ for the 5317.041 level. The 5326.7 level resonates strongly at the ν1j15/2 resonance in (p,p’) and thus has π=+, given the available negative parity neutron hole states. This leaves the 5317.7 level as the possible candidate for Jπ=3-. | |
5339.46 | 8+ | 32 fs +37-18 | configuration=π1h9/2π1h11/2-1 + ν1j15/2νlj-1, with a 3p1/2, 2f5/2, or 3p3/2 neutron hole state. |
5347.270 | 3- | 28.4 fs 14 | configuration=ν3d5/2ν3p1/2-1 + ν2g7/2ν3p1/2-1. |
5352 | + | configuration=π1h9/2π1h11/2-1. | |
5380.6 | - | configuration=π1h9/2π2d5/2-1. E(level): In the 207Pb(d,pγ),209Bi(t,αγ) dataset, based on data from (t,αγ), two levels are proposed at around 5380, one at 5380.6 8 deexciting via a 2766.1 8 transition, and one at 5383.7 11 deexciting via a 1387.8 10 transition. In (n,n’γ) a single level is proposed deexciting via 1387.37 3 and 2768.31 5 transitions, giving E(level)=5382.81 3 and 5382.83 5, respectively. There are two levels at about this energy in (d,3He), so the evaluator adopts the two-level proposal from the (t,αγ) work. The discrepancy in the energy of the 2766γ should Be noted, and it is of course possible that the (n,n’γ) 2768γ is a different transition and that the 5380.6 level is not populated in (n,n’γ). | |
5382.82 | 3+,4+,5+ | 37 fs +7-6 | configuration=π1h9/2π1h11/2-1. E(level): In the 207Pb(d,pγ),209Bi(t,αγ) dataset, based on data from (t,αγ), two levels are proposed at around 5380, one at 5380.6 8 deexciting via a 2766.1 8 transition, and one at 5383.7 11 deexciting via a 1387.8 10 transition. In (n,n’γ) a single level is proposed deexciting via 1387.37 3 and 2768.31 5 transitions, giving E(level)=5382.81 3 and 5382.83 5, respectively. There are two levels at about this energy in (d,3He), so the evaluator adopts the two-level proposal from the (t,αγ) work. The discrepancy in the energy of the 2766γ should Be noted, and it is of course possible that the (n,n’γ) 2768γ is a different transition and that the 5380.6 level is not populated in (n,n’γ). |
5384.59 | 3- | 76 fs 14 | configuration=ν3d5/2ν3p1/2-1. |
5473 | + | configuration=π1h9/2π1h11/2-1. | |
5481.87 | 5- | 90 fs 14 | E(level): α level at 5481 is proposed in (n,n’γ) deexciting via a 1356γ and a 2867γ. The 2867γ is seen in (d,pγ) but the 1356γ is not reported. The 1356γ is seen in (p,p’γ) but the 2867γ is not reported. It is possible that there are two levels, one seen in (n,n’γ) and (p,p’γ), and the other in (n,n’γ) and (d,pγ). |
E(level) | Jπ(level) | T1/2(level) | Comments |
5490 | E(level): There is a single level at 5491 proposed in (d,pγ), (n,n’γ), and (p,p’γ); however, the branchings are not consistent. Iγ(1571γ)/Iγ(2293γ) in (d,pγ) and (n,n’γ) agree, but Iγ(1107γ)/Iγ(2293γ) and Iγ(1781γ)/Iγ(2293γ) are both a factor of 4-5 higher in (d,pγ) than in (n,n’γ), and only the 2293γ is reported in (p,p’γ). The branchings from all three reactions can Be reconciled if two levels are proposed. The evaluator has thus proposed a doublet with transitions divided as shown in adopted gammas. For the 5491.53 level one has Iγ(1571γ)/Iγ(2293γ)=0.38 4 in (n,n’γ) and 0.48 +19-14 in (d,pγ). For the 5490.34 level one has Iγ(1107γ):Iγ(1529γ):Iγ(1781γ)=100 12:85 9:94 9 in (n,n’γ), and 100 16:91 16:84 18 in (d,pγ). The 1193, 1283, and 1365γ’s are multiplets in (n,n’γ) and the intensity of each of these transitions can Be divided such that the branchings for each placement are consistent with the (d,pγ) results. Both levels deexcite to levels with Jπ=5- and 6-, suggesting Jπ=4-, 5, 6, or 7-. In addition to the γ reactions, the (d,p) reaction reports E=5491.9 6 with a γ7/2 transfer, giving Jπ=4- for one or both levels, the 3- alternative being ruled out by the γ decay modes. In (d,3He) a level at 5487 2 is reported, with L=2. The authors state that the strength requires Jπ=6- given Jπ=7- for their 5541 2 level. α 5490 2 level is reported in (α,α’) so there must also Be a natural parity level in the region of E=5490. Jπ(level): There is a single level at 5491 proposed in (d,pγ), (n,n’γ), and (p,p’γ); however, the branchings are not consistent. Iγ(1571γ)/Iγ(2293γ) in (d,pγ) and (n,n’γ) agree, but Iγ(1107γ)/Iγ(2293γ) and Iγ(1781γ)/Iγ(2293γ) are both a factor of 4-5 higher in (d,pγ) than in (n,n’γ), and only the 2293γ is reported in (p,p’γ). The branchings from all three reactions can Be reconciled if two levels are proposed. The evaluator has thus proposed a doublet with transitions divided as shown in adopted gammas. For the 5491.53 level one has Iγ(1571γ)/Iγ(2293γ)=0.38 4 in (n,n’γ) and 0.48 +19-14 in (d,pγ). For the 5490.34 level one has Iγ(1107γ):Iγ(1529γ):Iγ(1781γ)=100 12:85 9:94 9 in (n,n’γ), and 100 16:91 16:84 18 in (d,pγ). The 1193, 1283, and 1365γ’s are multiplets in (n,n’γ) and the intensity of each of these transitions can Be divided such that the branchings for each placement are consistent with the (d,pγ) results. Both levels deexcite to levels with Jπ=5- and 6-, suggesting Jπ=4-, 5, 6, or 7-. In addition to the γ reactions, the (d,p) reaction reports E=5491.9 6 with a γ7/2 transfer, giving Jπ=4- for one or both levels, the 3- alternative being ruled out by the γ decay modes. In (d,3He) a level at 5487 2 is reported, with L=2. The authors state that the strength requires Jπ=6- given Jπ=7- for their 5541 2 level. α 5490 2 level is reported in (α,α’) so there must also Be a natural parity level in the region of E=5490. | ||
5490.34 | (4-,6-) | E(level): There is a single level at 5491 proposed in (d,pγ), (n,n’γ), and (p,p’γ); however, the branchings are not consistent. Iγ(1571γ)/Iγ(2293γ) in (d,pγ) and (n,n’γ) agree, but Iγ(1107γ)/Iγ(2293γ) and Iγ(1781γ)/Iγ(2293γ) are both a factor of 4-5 higher in (d,pγ) than in (n,n’γ), and only the 2293γ is reported in (p,p’γ). The branchings from all three reactions can Be reconciled if two levels are proposed. The evaluator has thus proposed a doublet with transitions divided as shown in adopted gammas. For the 5491.53 level one has Iγ(1571γ)/Iγ(2293γ)=0.38 4 in (n,n’γ) and 0.48 +19-14 in (d,pγ). For the 5490.34 level one has Iγ(1107γ):Iγ(1529γ):Iγ(1781γ)=100 12:85 9:94 9 in (n,n’γ), and 100 16:91 16:84 18 in (d,pγ). The 1193, 1283, and 1365γ’s are multiplets in (n,n’γ) and the intensity of each of these transitions can Be divided such that the branchings for each placement are consistent with the (d,pγ) results. Both levels deexcite to levels with Jπ=5- and 6-, suggesting Jπ=4-, 5, 6, or 7-. In addition to the γ reactions, the (d,p) reaction reports E=5491.9 6 with a γ7/2 transfer, giving Jπ=4- for one or both levels, the 3- alternative being ruled out by the γ decay modes. In (d,3He) a level at 5487 2 is reported, with L=2. The authors state that the strength requires Jπ=6- given Jπ=7- for their 5541 2 level. α 5490 2 level is reported in (α,α’) so there must also Be a natural parity level in the region of E=5490. Jπ(level): There is a single level at 5491 proposed in (d,pγ), (n,n’γ), and (p,p’γ); however, the branchings are not consistent. Iγ(1571γ)/Iγ(2293γ) in (d,pγ) and (n,n’γ) agree, but Iγ(1107γ)/Iγ(2293γ) and Iγ(1781γ)/Iγ(2293γ) are both a factor of 4-5 higher in (d,pγ) than in (n,n’γ), and only the 2293γ is reported in (p,p’γ). The branchings from all three reactions can Be reconciled if two levels are proposed. The evaluator has thus proposed a doublet with transitions divided as shown in adopted gammas. For the 5491.53 level one has Iγ(1571γ)/Iγ(2293γ)=0.38 4 in (n,n’γ) and 0.48 +19-14 in (d,pγ). For the 5490.34 level one has Iγ(1107γ):Iγ(1529γ):Iγ(1781γ)=100 12:85 9:94 9 in (n,n’γ), and 100 16:91 16:84 18 in (d,pγ). The 1193, 1283, and 1365γ’s are multiplets in (n,n’γ) and the intensity of each of these transitions can Be divided such that the branchings for each placement are consistent with the (d,pγ) results. Both levels deexcite to levels with Jπ=5- and 6-, suggesting Jπ=4-, 5, 6, or 7-. In addition to the γ reactions, the (d,p) reaction reports E=5491.9 6 with a γ7/2 transfer, giving Jπ=4- for one or both levels, the 3- alternative being ruled out by the γ decay modes. In (d,3He) a level at 5487 2 is reported, with L=2. The authors state that the strength requires Jπ=6- given Jπ=7- for their 5541 2 level. α 5490 2 level is reported in (α,α’) so there must also Be a natural parity level in the region of E=5490. | |
5491.53 | (4-,6-) | 125 fs +35-21 | E(level): There is a single level at 5491 proposed in (d,pγ), (n,n’γ), and (p,p’γ); however, the branchings are not consistent. Iγ(1571γ)/Iγ(2293γ) in (d,pγ) and (n,n’γ) agree, but Iγ(1107γ)/Iγ(2293γ) and Iγ(1781γ)/Iγ(2293γ) are both a factor of 4-5 higher in (d,pγ) than in (n,n’γ), and only the 2293γ is reported in (p,p’γ). The branchings from all three reactions can Be reconciled if two levels are proposed. The evaluator has thus proposed a doublet with transitions divided as shown in adopted gammas. For the 5491.53 level one has Iγ(1571γ)/Iγ(2293γ)=0.38 4 in (n,n’γ) and 0.48 +19-14 in (d,pγ). For the 5490.34 level one has Iγ(1107γ):Iγ(1529γ):Iγ(1781γ)=100 12:85 9:94 9 in (n,n’γ), and 100 16:91 16:84 18 in (d,pγ). The 1193, 1283, and 1365γ’s are multiplets in (n,n’γ) and the intensity of each of these transitions can Be divided such that the branchings for each placement are consistent with the (d,pγ) results. Both levels deexcite to levels with Jπ=5- and 6-, suggesting Jπ=4-, 5, 6, or 7-. In addition to the γ reactions, the (d,p) reaction reports E=5491.9 6 with a γ7/2 transfer, giving Jπ=4- for one or both levels, the 3- alternative being ruled out by the γ decay modes. In (d,3He) a level at 5487 2 is reported, with L=2. The authors state that the strength requires Jπ=6- given Jπ=7- for their 5541 2 level. α 5490 2 level is reported in (α,α’) so there must also Be a natural parity level in the region of E=5490. Jπ(level): There is a single level at 5491 proposed in (d,pγ), (n,n’γ), and (p,p’γ); however, the branchings are not consistent. Iγ(1571γ)/Iγ(2293γ) in (d,pγ) and (n,n’γ) agree, but Iγ(1107γ)/Iγ(2293γ) and Iγ(1781γ)/Iγ(2293γ) are both a factor of 4-5 higher in (d,pγ) than in (n,n’γ), and only the 2293γ is reported in (p,p’γ). The branchings from all three reactions can Be reconciled if two levels are proposed. The evaluator has thus proposed a doublet with transitions divided as shown in adopted gammas. For the 5491.53 level one has Iγ(1571γ)/Iγ(2293γ)=0.38 4 in (n,n’γ) and 0.48 +19-14 in (d,pγ). For the 5490.34 level one has Iγ(1107γ):Iγ(1529γ):Iγ(1781γ)=100 12:85 9:94 9 in (n,n’γ), and 100 16:91 16:84 18 in (d,pγ). The 1193, 1283, and 1365γ’s are multiplets in (n,n’γ) and the intensity of each of these transitions can Be divided such that the branchings for each placement are consistent with the (d,pγ) results. Both levels deexcite to levels with Jπ=5- and 6-, suggesting Jπ=4-, 5, 6, or 7-. In addition to the γ reactions, the (d,p) reaction reports E=5491.9 6 with a γ7/2 transfer, giving Jπ=4- for one or both levels, the 3- alternative being ruled out by the γ decay modes. In (d,3He) a level at 5487 2 is reported, with L=2. The authors state that the strength requires Jπ=6- given Jπ=7- for their 5541 2 level. α 5490 2 level is reported in (α,α’) so there must also Be a natural parity level in the region of E=5490. |
5511.78 | 1- | 0.0194 fs +12-18 | configuration=ν3d3/2ν3p1/2-1. |
5516.714 | 3- | 40.9 fs 21 | configuration=ν2g7/2ν3p1/2-1. |
5524 | + | configuration=π1h9/2π1h11/2-1. | |
5536.58 | 10+ | configuration=π1h9/2π1h11/2-1 + ν1j15/2ν2f5/2-1. | |
5543.01 | 7- | configuration=π1h9/2π2d5/2-1. | |
5548.113 | 2- | 83 fs 7 | configuration=ν3d3/2ν3p1/2-1 + ν3d5/2ν3p1/2-1. |
5563.73 | 3- | 44 fs +9-7 | configuration=ν3d5/2ν3p1/2-1 + ν2g7/2ν3p1/2-1. |
5576.6 | Jπ(level): L(d,3He)=2 and thus configuration=π1h9/2π2d5/2-1 for E=5581 6. | ||
5579.0 | Jπ(level): L(d,3He)=2 and thus configuration=π1h9/2π2d5/2-1 for E=5581 6. | ||
5587.7 | Jπ(level): L(d,3He)=2 and thus configuration=π1h9/2π2d5/2-1 for E=5581 6. | ||
5599.48 | 0- | > 159 fs | configuration=ν3d5/2ν2f5/2-1 with a small admixture of configuration=ν4s1/2ν3p1/2-1. |
5627 | + | configuration=π1h9/2π1h11/2-1. | |
5639.55 | 1- | 0.13 ps +12-5 | configuration=ν3d3/2ν3p1/2-1. |
5643 | 2 TO 7- | configuration=π1h9/2π2d5/2-1. | |
5658.51 | 5- | 31 fs +7-6 | Jπ(level): L(d,3He)=2 and thus configuration=π1h9/2π2d5/2-1 for E=5665 5. |
5665.7 | Jπ(level): L(d,3He)=2 and thus configuration=π1h9/2π2d5/2-1 for E=5665 5. | ||
5675.366 | 2-,3,4 | 13 fs +6-5 | Jπ(level): L(d,3He)=2 and thus configuration=π1h9/2π2d5/2-1 for E=5680 6. |
5686.5 | 6- | configuration=ν2g9/2ν2f7/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. L(d,3He)=2 and thus configuration=π1h9/2π2d5/2-1 for E=5680 6. | |
5690.117 | 4+ | 46 fs 4 | configuration=π1h9/2π1h11/2-1. |
5694.22 | 7- | 58 fs +84-30 | configuration=π1h9/2π2d5/2-1 + ν2g9/2ν2f7/2-1. Jπ(level): From 2006He21 in (p,p’) from a study of excitations via IAR in 209Bi. The assignments are based on a comparison of the experimental σ(θ) values and cross-sections with calculations based on the schematic shell model. The cross-sections are averaged values for the members of the ν1i11/2ν2f5/2-1 multiplet and for members of the ν1i11/2ν3p3/2-1 multiplet. The same arguments hold for the 5686, 5695 and 5835 levels which have configuration=ν2g9/2ν2f7/2-1. Additional arguments are given. |
5715.53 | 2+ | 3.7 fs 11 | configuration=π1h9/2π1h11/2-1. |
5727 | + | configuration=π1h9/2π1h11/2-1. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
5749.67 | (11+) | Jπ(level): Based on γ decay pattern, available shell-model states, and shell-model calculations involving two-particle two-hole excitations using semi-empirical effective interactions (2004Br19, 2001Wr02, 1993Sc08). | |
5763.7 | 6+ | configuration=π1h9/2π1h11/2-1 + ν1j15/2ν3p3/2-1. | |
5777.96 | 2-,3- | 15.9 fs 14 | configuration=ν2g7/2ν3p1/2-1 + ν3d5/2ν3p1/2-1 or ν3d3/2ν3p1/2-1 + ν3d5/2ν3p1/2-1 + π1h9/2π2d5/2-1. |
5789.34 | 2+,3+,4+ | 40 fs +4-3 | configuration=π1h9/2π1h11/2-1. |
5813.27 | 3- | 22 fs +4-3 | configuration=ν2g7/2ν3p1/2-1. |
5819.49 | 1+,2+ | 222 fs +42-35 | configuration=π1h9/2π1h11/2-1. |
5835.8 | 8- | configuration=ν2g9/2ν2f7/2-1. | |
5844.49 | 1+ | ≤ 0.31 fs | configuration=π1h9/2π1h11/2-1. |
5860 | 11+ | configuration=ν1i11/2ν1i13/2-1. | |
5867 | + | configuration=π1h9/2π1h11/2-1. | |
5873.573 | 3- | 13.2 fs +21-14 | configuration=ν2g7/2ν3p1/2-1. |
5885.55 | 3- | 13.9 fs 14 | configuration=ν3d5/2ν3p1/2-1 + ν2g7/2ν3p1/2-1 + π1h9/2π2d5/2-1. |
5901 | (8)+ | configuration=π1h9/2π1h11/2-1. | |
5923.67 | 2- | 104 fs +90-42 | configuration=ν3d3/2ν3p1/2-1. |
5928.0 | 10+ | configuration=π1h9/2π1h11/2-1. | |
5944 | + | configuration=π1h9/2π1h11/2-1. | |
5946.77 | 1- | ≤ 0.48 fs | configuration=ν3d3/2ν3p1/2-1. |
5954 | 9+ | configuration=ν1i11/2ν1i13/2-1 + π2f7/2π1h11/2-1. | |
5968.55 | 4- | 7.6 fs +42-35 | configuration=ν2g7/2ν3p1/2-1. |
5996 | - | configuration=π1h9/2π2d5/2-1. | |
6009.75 | 3- | 11 fs +5-4 | configuration=ν2g7/2ν3p1/2-1. |
6037.5 | (5+,6+) | configuration=ν2h11/2ν3p1/2-1?. | |
6068.2 | (5+,6+) | configuration=ν2h11/2ν3p1/2-1?. | |
6071 | - | configuration=π1h9/2π2d5/2-1. | |
6076.4 | 0-,1- | configuration=ν4s1/2ν3p1/2-1. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
6086.56 | 1- | 37 fs +25-15 | configuration=ν3d3/2ν3p1/2-1. |
6100.69 | 12+ | configuration=ν1i11/2ν1i13/2-1. | |
6101.1 | (5+) | > 690 fs | configuration=ν2h11/2ν3p1/2-1?. |
6179 | 2+ | configuration=π1h9/2π1h11/2-1. | |
6193.1 | 2+ | 0.62 fs 5 | XREF: B(6195.6). |
6242.4 | Jπ(level): L(d,3He)=2 and thus configuration=π1h9/2π2d5/2-1 for E=6249 7. | ||
6250.6 | Jπ(level): L(d,3He)=2 and thus configuration=π1h9/2π2d5/2-1 for E=6249 7. | ||
6263.7 | 1- | ≤ 0.21 fs | configuration=ν4s1/2ν3p1/2-1 + ν3d3/2ν3p1/2-1. |
6274.55 | 3- | 12 fs +16-10 | configuration=ν3d5/2ν3p1/2-1 + ν2g7/2ν3p1/2-1. |
6313.9 | 1- | ≤ 0.17 fs | configuration=ν4s1/2ν3p1/2-1. |
6332.9 | Jπ(level): Jπ=3- from σ and form factor in (e,e’) for E=6343 10. | ||
6340 | 1-,2,3- | Jπ(level): Jπ=3- from σ and form factor in (e,e’) for E=6343 10. | |
6348.3 | Jπ(level): Jπ=3- from σ and form factor in (e,e’) for E=6343 10. | ||
6361.6 | 1- | ≤ 0.30 fs | configuration=ν3d3/2ν3p1/2-1. |
6389.6 | - | configuration=ν3d3/2ν3p1/2-1 or ν2g7/2ν3p1/2-1. Jπ(level): E(p,p’γ)=6394.5 30 deexciting via Eγ=2432.8 30, and E(e,e’)=6403 10 with Jπ=3-, established by σ and form factor, could correspond to either the 6389.6 5 or 6397.1 15 levels. | |
6397.1 | Jπ(level): E(p,p’γ)=6394.5 30 deexciting via Eγ=2432.8 30, and E(e,e’)=6403 10 with Jπ=3-, established by σ and form factor, could correspond to either the 6389.6 5 or 6397.1 15 levels. | ||
6420.2 | (5+,6+) | XREF: d(6418.8)F(6421.6). | |
6435.57 | 12- | configuration=ν1j15/2ν1i13/2-1. | |
6444.4 | 3- | configuration=ν3d5/2ν3p1/2-1 + ν2g7/2ν3p1/2-1. | |
6448.40 | (13-) | Jπ(level): Based on γ decay pattern, available shell-model states, and shell-model calculations involving two-particle two-hole excitations using semi-empirical effective interactions (2004Br19, 2001Wr02, 1993Sc08). | |
6462.7 | - | configuration=π1h9/2π2d5/2-1. | |
6482.0 | 2- | B(M2)≈8 from (e,e’). | |
6486.5 | 1- | 0.78 fs +37-23 | configuration=ν4s1/2ν3p1/2-1 + ν3d3/2ν3p1/2-1. |
6529.0 | - | configuration=π1h9/2π2d5/2-1. E(level): In (d,pγ) there is a level with E=6534 5 deexciting via a single transition with Eγ=3920 5 to a 3- level. | |
6531.7 | E(level): In (d,pγ) there is a level with E=6534 5 deexciting via a single transition with Eγ=3920 5 to a 3- level. | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
6588 | 2- | B(M2)≈3 from (e,e’). | |
6617.0 | 3- | configuration=ν2g7/2ν3p1/2-1 + π1h9/2π2d5/2-1. | |
6682.46 | (5-) | configuration=ν2h11/2ν3p1/2-1?. | |
6687.8 | 5- | XREF: L(6692.0). | |
6699.60 | (3-) | Jπ(level): Jπ=1- or, less likely, 2- or 3- for a peak at 6701 9 in (e,e’). | |
6708.9 | Jπ(level): Jπ=1- or, less likely, 2- or 3- for a peak at 6701 9 in (e,e’). | ||
6719.8 | 1- | 0.052 fs +6-12 | XREF: L(6718.4). |
6739.6 | XREF: L(6740.1). | ||
6743.42 | 14- | configuration=ν1j15/2ν1i13/2-1. | |
6773.4 | 1,2,3- | XREF: d(6777.0)F(6774.7). | |
6831.5 | (8-) | configuration=ν1j15/2ν1i13/2-1. | |
6861.4 | 9- | configuration=π1i13/2π1h11/2-1. E(level): Levels with E=6861.4 6 and 6868.0 6 are reported in (p,p’) with no spectroscopic information, and levels with E=6859, Jπ=9- and 6865, Jπ=10- are reported in (e,e’). The evaluator assigns two levels; however, it is possible that the two reactions are exciting different levels. Jπ(level): Levels with E=6861.4 6 and 6868.0 6 are reported in (p,p’) with no spectroscopic information, and levels with E=6859, Jπ=9- and 6865, Jπ=10- are reported in (e,e’). The evaluator assigns two levels; however, it is possible that the two reactions are exciting different levels. | |
6868.0 | 10- | E(level): Levels with E=6861.4 6 and 6868.0 6 are reported in (p,p’) with no spectroscopic information, and levels with E=6859, Jπ=9- and 6865, Jπ=10- are reported in (e,e’). The evaluator assigns two levels; however, it is possible that the two reactions are exciting different levels. Jπ(level): Levels with E=6861.4 6 and 6868.0 6 are reported in (p,p’) with no spectroscopic information, and levels with E=6859, Jπ=9- and 6865, Jπ=10- are reported in (e,e’). The evaluator assigns two levels; however, it is possible that the two reactions are exciting different levels. | |
6879 | 7- | configuration=π1i13/2π1h11/2-1. | |
6884 | 10- | configuration=π1i13/2π1h11/2-1. | |
6929.6 | 2- | BM2≈20 configuration=ν3d3/2ν3p1/2-1 + ν3d5/2ν3p1/2-1. | |
6969.3 | 2- | configuration=ν3d3/2ν3p1/2-1 + ν3d5/2ν3p1/2-1. | |
7020.2 | 1- | configuration=ν4s1/2ν3p1/2-1 + ν3d3/2ν3p1/2-1. | |
7061 | 12- | configuration=π1i13/2π1h11/2-1. | |
7063.53 | 1- | 0.025 fs +1-3 | XREF: L(7062.1). |
7083.2 | 1- | 0.050 fs 4 | configuration=ν3d3/2ν3p1/2-1. |
7086 | 12- | configuration=π1i13/2π1h11/2-1. | |
7137.3 | 3-,4- | configuration=ν2g7/2ν3p1/2-1. | |
7146.1 | (5-,6-) | configuration=ν2h11/2ν3p1/2-1?. | |
7240 | 1- | ≤ 0.24 fs | configuration=ν4s1/2ν3p1/2-1 + ν3d3/2ν3p1/2-1. |
E(level) | Jπ(level) | T1/2(level) | Comments |
7332.4 | 1- | 0.016 fs +2-4 | XREF: d(7326.5)F(7329.2). |
7335.4 | (5-,6-) | configuration=ν2h11/2ν3p1/2-1?. | |
7360 | 2+ | Γ=400 keV 50. %EWSR=6.5 10. E(level): This level may correspond to one or more of the close-lying levels determined in the higher-resolution resonance work. | |
7360.1 | (5-,6-) | configuration=ν2h11/2ν3p1/2-1?. | |
7408.5 | E(level): This level may correspond to one or more of the close-lying levels determined in the higher-resolution resonance work. | ||
7449.4 | (5-,6-) | configuration=ν2h11/2ν3p1/2-1?. | |
7459 | 2- | B(M2)≈11 from (e,e’). | |
7468.6 | 1- | configuration=ν4s1/2ν3p1/2-1 + ν3d3/2ν3p1/2-1. | |
7505.0 | 1- | configuration=ν4s1/2ν3p1/2-1 + ν3d3/2ν3p1/2-1. | |
7509 | 2- | B(M2)≈10 from (e,e’). | |
7548.6 | 1- | ≤ 0.35 fs | configuration=ν4s1/2ν3p1/2-1 + ν3d3/2ν3p1/2-1. |
7573 | E(level): This level may correspond to one or more of the close-lying levels determined in the higher-resolution resonance work. | ||
7594 | E(level): This level may correspond to one or more of the close-lying levels determined in the higher-resolution resonance work. | ||
7700 | E(level): This level may correspond to one or more of the close-lying levels determined in the higher-resolution resonance work. | ||
7740 | E(level): This level may correspond to one or more of the close-lying levels determined in the higher-resolution resonance work. | ||
7825 | (10-) | configuration=ν1i11/2ν2h9/2-1. | |
7845 | 2+ | XREF: d(7840). E(level): This level may correspond to one or more of the close-lying levels determined in the higher-resolution resonance work. | |
7913 | 1(-) | ≤ 0.48 fs | XREF: d(7920). |
7924 | 2- | B(M2)≈20 in (e,e’). | |
7974.04 | (15-) | Jπ(level): Based on γ decay pattern, available shell-model states, and shell-model calculations involving two-particle two-hole excitations using semi-empirical effective interactions (2004Br19, 2001Wr02, 1993Sc08). | |
8008 | 2- | B(M2)≈11 in (e,e’). | |
8026.95 | (14-) | Jπ(level): Based on γ decay pattern, available shell-model states, and shell-model calculations involving two-particle two-hole excitations using semi-empirical effective interactions (2004Br19, 2001Wr02, 1993Sc08). | |
8110 | 4+ | XREF: B(8100)C(8100). | |
8220 | (1-) | E(level): This level may correspond to one or more of the close-lying levels determined in the higher-resolution resonance work. | |
8350 | 3- | Γ=400 keV 50. %EWSR=4.0 12. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
8350.79 | (15-) | Jπ(level): Based on γ decay pattern, available shell-model states, and shell-model calculations involving two-particle two-hole excitations using semi-empirical effective interactions (2004Br19, 2001Wr02, 1993Sc08). | |
8369 | 12+ | configuration=ν1j15/2ν2h9/2-1. | |
8400 | E(level): This level may correspond to one or more of the close-lying levels determined in the higher-resolution resonance work. | ||
8562.94 | (16-) | Jπ(level): Based on γ decay pattern, available shell-model states, and shell-model calculations involving two-particle two-hole excitations using semi-empirical effective interactions (2004Br19, 2001Wr02, 1993Sc08). | |
8860 | 2+ | Γ=400 keV 50 in (p,p’). %EWSR=5.0 8 in (p,p’). | |
9061.2 | (17+) | Jπ(level): Based on γ decay pattern, available shell-model states, and shell-model calculations involving two-particle two-hole excitations using semi-empirical effective interactions (2004Br19, 2001Wr02, 1993Sc08). | |
9340 | 2+ | Γ=400 keV 50. %EWSR=5.0 8. | |
9380 | 3- | XREF: E(9400). | |
9520 | 2+ | XREF: γ(9600). | |
10070 | (1,2) | XREF: E(10040). | |
10.9E+3 | 2+ | Γ=3.0 3 MeV, %EWSR=100 13 (2004Yo02). See (α,α’) for other values and a discussion of possible higher L components. Γ=2.0 MeV 2 in (p,p’). | |
11450 | (1,2) | Γ<70 keV. | |
11.60E+3 | Γ=2.1 MeV if E1. %EWSR=11. | ||
12250 | 4+ | XREF: B(12500)d(12000). | |
13.5E+3 | 1- | Γ=7.7 5 MeV (2004Yo02 in (α,α’)), 4.05 MeV (1970Ve03 in (γ,n)) and 3.7 MeV in (γ,γ’). | |
13.96E+3 | 0+ | %EWSR=99 15 (2004Yo02 in (α,α’)). See (α,α’) for other values. | |
16000 | 6+ | Γ=2.9 MeV, %EWSR=15. | |
19.6E+3 | 3- | %EWSR=70 14 (2004Yo02 in (α,α’)). See (α,α’) for other values. | |
22.1E+3 | 1- | From α-proton and α-neutron coincidence work, 2004Hu04 determine branching for direct proton decay to the 2s1/2 + 2d3/2 states and 1h11/2 + 2d5/2 final states in 207Tl of 2.3% 11 and 1.2% 7, respectively. The value for direct neutron decay to final states in 207Pb with excitation energies from O to 6 MeV is 23% 5. | |
23.94E+3 | Data are from 1980Be52 in (n,X) who suggest that the resonance is the IAR of a possible 1- level in 208Tl predicted at ≈1500 by 1970Do03. See also (γ,p),(e,e’p) where E=24400 and the same interpretation is given. | ||
24.48E+3 | Data are from 1980Be52 in (n,X) who suggest that the resonance is the IAR of a possible 1- level in 208Tl predicted at ≈2000 by 1970Do03. See also (γ,p),(e,e’p) where E=25000 and the same interpretation is given. | ||
26.9E+3 | 2+ | configuration: suggested as an overtone of the isoscalar giant quadrupole resonance (2004Hu04, 2003Hu13). | |
27200 | Interpreted by 1975Sh12, 1975Sh13 as the IAR of a possible 2+ level in 208Tl predicted at ≈2800 by 1970Do03. |
E(level) | E(gamma) | Comments |
3197.711 | 583.187 | M(γ): from γγ(θ) in β- decay and T1/2 |
3475.078 | 277.371 | E(γ): from Eγ(860γ)=Eγ(277γ)+Eγ(583γ), with recoil corrections taken into account M(γ): from β- decay | 860.557 | M(γ): from β- decay |
3919.966 | 211.51 | M(γ): from β- decay | 722.252 | M(γ): from β- decay |
3961.162 | 252.755 | M(γ): from β- decay | 763.429 | M(γ): from β- decay |
4037.443 | 839.734 | M(γ): δ(M3/E2)=+0.010 +21-31 |
4229.590 | 1615.068 | M(γ): the large solution is <-11, >+10, an unlikely alternative. Other: +0.04 3 or -7.8 +29-16 (1990Go33) | 4229.49 | M(γ): from (d,pγ) |
4261.871 | 786.79 | E(γ): rounded-off value from the level energies. The level energy difference gives Eγ=786.791 17 (recoil corrected). The value of 786.891 10 given in the source dataset, and placed from this level, may Be a misprint |
4841.60 | 4841.46 | I(γ): Γγ0/Γ=0.85 +139 from (γ,γ’) |
4868.35 | 4870 | M(γ): from (p,p’γ) |
4895.23 | 34.4 | E(γ): not observed. Eγ is rounded-off from the level energies. See (x,x’γ) for a discussion of this transition |
4937.19 | 4937.19 | E(γ): from the level energies. Reported only in (p,p’γ) where the energies for the two transitions from this level are given as 2320.6 2 and 4934.7 1 |
5074.81 | 868.53 | E(γ): from the level energies |
5127.356 | 5127.5 | I(γ): from (d,pγ). Note, however, that Iγ/Iγ(2513γ)=0.177 13 in (n,n’γ) and 0.14 1 in (d,pγ) |
5213.98 | 2016.14 | E(γ): from the level energies. The transition is a multiplet in the cource dataset |
5241.1 | 5241 | M(γ): from (p,p’γ) |
5276.418 | 1070.13 | E(γ): from the level energies. The measured value from (n,n’γ) is 1069.72 4. Not included in the least-squares fit |
5291.90 | 5291.74 | I(γ): Γγ0/Γ=0.78 +22-11 from (γ,γ’) |
5339.46 | 478.59 | E(γ): In the 207Pb(d,pγ),209Bi(t,αγ) dataset, based on data from (t,αγ), two levels are proposed at around 5380, one at 5380.6 8 deexciting via a 2766.1 8 transition, and one at 5383.7 11 deexciting via a 1387.8 10 transition. In (n,n’γ) a single level is proposed deexciting via 1387.37 3 and 2768.31 5 transitions, giving E(level)=5382.81 3 and 5382.83 5, respectively. There are two levels at about this energy in (d,3He), so the evaluator adopts the two-level proposal from the (t,αγ) work. The discrepancy in the energy of the 2766γ should Be noted, and it is of course possible that the (n,n’γ) 2768γ is a different transition and that the 5380.6 level is not populated in (n,n’γ) I(γ): For the 5339 level, Iγ(478γ):728γ:1301γ is reported as 63 8err; aut=J. Tuli; dat=18-Dec-2007; com=Fixed typos from pnpi rpt; 63 8:100 11:25 11 in (d,pγ) and as 130 29:100 19:48 9 in (n,n’γ). These data suggest that Iγ(728γ) in (d,pγ) may Be a factor of two too large. The alternative possibility is that Iγ(478γ) and Iγ(1301γ) are both a factor of two too large in (n,n’γ) | 728.78 | E(γ): In the 207Pb(d,pγ),209Bi(t,αγ) dataset, based on data from (t,αγ), two levels are proposed at around 5380, one at 5380.6 8 deexciting via a 2766.1 8 transition, and one at 5383.7 11 deexciting via a 1387.8 10 transition. In (n,n’γ) a single level is proposed deexciting via 1387.37 3 and 2768.31 5 transitions, giving E(level)=5382.81 3 and 5382.83 5, respectively. There are two levels at about this energy in (d,3He), so the evaluator adopts the two-level proposal from the (t,αγ) work. The discrepancy in the energy of the 2766γ should Be noted, and it is of course possible that the (n,n’γ) 2768γ is a different transition and that the 5380.6 level is not populated in (n,n’γ) I(γ): For the 5339 level, Iγ(478γ):728γ:1301γ is reported as 63 8err; aut=J. Tuli; dat=18-Dec-2007; com=Fixed typos from pnpi rpt; 63 8:100 11:25 11 in (d,pγ) and as 130 29:100 19:48 9 in (n,n’γ). These data suggest that Iγ(728γ) in (d,pγ) may Be a factor of two too large. The alternative possibility is that Iγ(478γ) and Iγ(1301γ) are both a factor of two too large in (n,n’γ) | 1301.74 | E(γ): In the 207Pb(d,pγ),209Bi(t,αγ) dataset, based on data from (t,αγ), two levels are proposed at around 5380, one at 5380.6 8 deexciting via a 2766.1 8 transition, and one at 5383.7 11 deexciting via a 1387.8 10 transition. In (n,n’γ) a single level is proposed deexciting via 1387.37 3 and 2768.31 5 transitions, giving E(level)=5382.81 3 and 5382.83 5, respectively. There are two levels at about this energy in (d,3He), so the evaluator adopts the two-level proposal from the (t,αγ) work. The discrepancy in the energy of the 2766γ should Be noted, and it is of course possible that the (n,n’γ) 2768γ is a different transition and that the 5380.6 level is not populated in (n,n’γ) I(γ): For the 5339 level, Iγ(478γ):728γ:1301γ is reported as 63 8err; aut=J. Tuli; dat=18-Dec-2007; com=Fixed typos from pnpi rpt; 63 8:100 11:25 11 in (d,pγ) and as 130 29:100 19:48 9 in (n,n’γ). These data suggest that Iγ(728γ) in (d,pγ) may Be a factor of two too large. The alternative possibility is that Iγ(478γ) and Iγ(1301γ) are both a factor of two too large in (n,n’γ) |
5481.87 | 1356.49 | E(γ): not reported in (d,pγ) |
E(level) | E(gamma) | Comments |
5490.34 | 1107.0 | I(γ): From (d,pγ). See comment on the 5490 multiplet | 1193.52 | I(γ): From (d,pγ). See comment on the 5490 multiplet | 1283.5 | I(γ): From (d,pγ). See comment on the 5490 multiplet | 1365.0 | I(γ): From (d,pγ). See comment on the 5490 multiplet | 1529.0 | I(γ): From (d,pγ). See comment on the 5490 multiplet | 1781.5 | I(γ): From (d,pγ). See comment on the 5490 multiplet |
5491.53 | 1571.49 | I(γ): from (n,n’γ). Iγ/Iγ(2294γ)=0.48 +19-14 in (d,pγ). The 1572γ is not reported in (p,p’γ) |
5511.78 | 5511.70 | I(γ): Γγ0/Γ=0.98 +2-4 from (γ,γ’) |
6255.68 | 3641.13 | E(γ): from (n,n’γ). Eγ=3636 5 reported in (d,pγ) | 6255.5 | E(γ): from (γ,γ’). Not seen in (d,pγ). Energy is above the cutoff for transitions reported in (n,n’γ) |
6512.8 | 6512.7 | E(γ): from E(level)in (p,p’). Eγ=6515.2 18 reported in (γ,γ’) |
6687.8 | 2207.1 | E(γ): from the level energies. Eγ=2211.0 5 is reported in (p,p’γ) for what is probably the same level as that seen in (p,p’) at 6689.1 15 and in (α,α’) at 6687.4 8 |
6719.8 | 6719.7 | E(γ): from (γ,γ’). Others: 6718.4 3 (p,p’γ), 6716.2 4 (d,pγ) I(γ): Γγ0/Γ=1.00 +0-11 from (γ,γ’) |
6980 | 6980 | I(γ): Γγ0=0.95 eV 10. Γγ0/Γ≈0.27 |
7063.53 | 7063.4 | E(γ): from (γ,γ’). Others: 7062.1 1 (p,p’γ), 7063.4 5 (d,pγ). Note that E(level)=7063.4 15 in (p,p’) and 7064.1 6 in (d,p) I(γ): Γγ0/Γ=0.98 +2-7 from (γ,γ’) |
7083.2 | 7083.1 | I(γ): Γγ0/Γ=1 from (γ,γ’) |
7177.0 | 7176.9 | E(γ): from the level energy. Eγ=7176 4 in (γ,γ’) |
7218.6 | 4020.8 | E(γ): from the level energies. Eγ=4018 5 in (d,pγ) |
7240 | 7240 | E(γ): from the level energies. See the comment on E(level) |
7278.68 | 7278.54 | I(γ): Γγ0/Γ=1 from (γ,γ’) |
7332.4 | 7332.3 | I(γ): Γγ0/Γ=1.00 +0-12 in (γ,γ’) |
7548.6 | 7548.5 | E(γ): from the level energy. Eγ=7547.4 26 in (γ,γ’) |
Neutron and ground-state γ widths are given in the resonance reactions, (n,γ), (n,X), and (γ,n)
For measurements of the neutron-skin thickness see 2004Kr02 and references contained therein. The rms(n)-rms(p) values, in fm, range from 0.12 7 to 0.20 4
Levels: The neutron-particle, neutron-hole configurations are from (d,p) and from (p,p’) (via IAR). The proton-particle, proton-hole configurations are from (d,3He). Other configurations, especially for the high-spin states are from (e,e’). In addition to the configurations given in those source datasets, 2006He21 (in their reference 24) analyze (p,p’) via IAR, (d,p), and (d,3He) data to deduce configuration amplitudes for several levels below 4500. Amplitudes for non-dominant configurations are included in their calculations but are not given here. Only the dominant neutron particle-hole and/or proton particle-hole configurations are given
Levels: The B(EL) values for levels above the 2614.5 level are from (e,e’)
Q-value: Note: Current evaluation has used the following Q record -2878.4 20 7367.87 5 8004 5 516.9 13 2003Au03