ADOPTED LEVELS, GAMMAS for 186Re
Authors: J. C. Batchelder and A. M. Hurst, M. S. Basunia | Citation: Nucl. Data Sheets 183, 1 (2022) | Cutoff date: 1-Mar-2022
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=1072.71 keV 83 | S(n)= 6179.591 keV 5 | S(p)= 5828.42 keV 66 | Q(α)= 2078.4 keV 16 | ||
Reference: 2021WA16 |
References: | |||
A | 186Re IT decay (2.0×105 Y) | B | 185Re(n,γ) E=THERMAL |
C | 185Re(n,γ) E=2-110 EV | D | 185Re(d,p) |
E | 186W(d,2nγ) | F | 187Re(p,d) |
G | 187Re(n,2nγ) | H | 187Re(d,t) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCDEFGH | 1- | 3.7185 d 5 % ε = 7.50 10 % β- = 92.50 10 | |||||
59.010 3 | ABCD FGH | 2- | 59.009 4 | 100 | M1+E2 | 0.0 | 1- | |
99.361 3 | ABCDEFGH | 3- | 25.5 ns 25 | 40.350 3 99.362 4 | 100.0 7 21.3 9 | M1+E2 E2 | 59.010 0.0 | 2- 1- |
146.275 4 | BCD FGH | 3- | 87.266 4 146.273 12 | 100.0 59 8.4 17 | M1(+E2) | 59.010 0.0 | 2- 1- | |
148.2 5 | AB E G | (8+) | 2.0×10+5 y % IT = 100 | 48.84 50 | 100 | (E5) | 99.361 | 3- |
173.929 4 | BC EF H | 4- | 74.568 3 | 100.0 | M1+E2 | 99.361 | 3- | |
180.2 7 | B DEFG | (6-) | ||||||
210.699 5 | BCD FGH | 2- | < 0.2 ns | 64.42 4 111.337 8 151.686 5 210.685 17 | 1.67 30 42.0 59 80.3 46 100.0 59 | M1(+E2) M1+E2 M1 | 146.275 99.361 59.010 0.0 | 3- 3- 2- 1- |
268.800 6 | BC FG | 4- | 122.525 5 169.431 8 209.82 2 | 100.0 71 19.8 50 22.5 22 | M1+E2 | 146.275 99.361 59.010 | 3- 3- 2- | |
273.627 5 | BCD FGH | 4- | 99.696 4 127.352 4 174.271 9 | 27.0 63 68 15 100.0 63 | M1+E2 M1+E2 | 173.929 146.275 99.361 | 4- 3- 3- | |
314.009 5 | BC G | (3+) | 24.1 ns 11 | 103.310 6 167.737 8 214.648 8 254.995 15 | 20.3 12 8.64 45 100 6 48.2 29 | [E1] E1+M2 E1 E1 | 210.699 146.275 99.361 59.010 | 2- 3- 3- 2- |
316.459 10 | BC FG | (1-) | 0.20 ns 10 | 257.446 15 316.473 20 | 55.2 32 100.0 28 | M1+E2 M1 | 59.010 0.0 | 2- 1- |
317.846 7 | BC EF | 5- | 143.919 5 218.6187 5 ? | 100 13 5.6 28 | M1+E2 | 173.929 99.361 | 4- 3- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
322.378 6 | BCD FGH | 3- | 111.674 6 148.37 6 176.112 8 223.035 15 263.33 20 | 100 21 5.9 14 27.1 57 35.7 21 16.4 36 | M1+E2 M1+E2 M1+E2 | 210.699 173.929 146.275 99.361 59.010 | 2- 4- 3- 3- 2- | |
324.2 5 | B E G | 5+ | 17.3 ns 6 | 144.0 5 150.3 5 | 100.0 49 13.2 10 | E1 E1+M2 | 180.2 173.929 | (6-) 4- |
342 2 ? | D | |||||||
351.202 16 | BC G | (4)+ | < 0.2 ns | 204.96 15 251.841 15 | 1.29 36 100 7 | E1 | 146.275 99.361 | 3- 3- |
378.387 10 | BCD F H | (2-) | 61.928 4 232.100 16 319.44 10 378.42 5 | 73 11 36.2 39 24.2 15 100.0 59 | M1+E2 M1+E2 M1+E2 | 316.459 146.275 59.010 0.0 | (1-) 3- 2- 1- | |
414.7 7 | B DEFG | (9+) | 266.69 4 ? | 100 | 148.2 | (8+) | ||
417.794 8 | B F H | 5- | 144.152 5 ? 148.994 5 271.47 10 | 13.16 70 100 18 40 12 | M1+E2 | 273.627 268.800 146.275 | 4- 4- 3- | |
420.560 7 | B GH | (4+) | 106.550 4 321.1896 7 | 100 12 5.9 32 | M1+E2 | 314.009 99.361 | (3+) 3- | |
425.823 7 | BC F | (4+) | 111.814 4 326.4786 7 | 100 36 5.9 29 | M1+E2 | 314.009 99.361 | (3+) 3- | |
462.969 9 | BC FG | 5- | 145.131 8 189.313 17 193.95 10 289.06 15 363.45 15 | 14.2 44 100 26 29.6 17 9.2 27 49.8 35 | M1+E2 | 317.846 273.627 268.800 173.929 99.361 | 5- 4- 4- 4- 3- | |
465.4 7 | B E G | 6+ | 141.1 5 | 100.0 | M1+E2 | 324.2 | 5+ | |
469.794 8 | BCD FGH | 4- | 147.417 6 200.981 16 295.88 15 370.3793 7 | 100.0 29 18.4 39 13.7 11 8.6 43 | M1+E2 M1 | 322.378 268.800 173.929 99.361 | 3- 4- 4- 3- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
470.509 11 | BCD H | (3-) | 92.122 4 148.09 6 201.78 10 411.18 20 | 100 23 6.8 21 6.8 21 54.5 42 | M1+E2 | 378.387 322.378 268.800 59.010 | (2-) 3- 4- 2- | |
497.294 10 | B DEF | (6-) | 179.448 7 323.5 5 | 100 13 1 | 317.846 173.929 | 5- 4- | ||
500.722 16 | BC FG | (5)+ | 149.520 5 176.2941 3 401.3 3 | 100 50 11.1 56 12.6 13 | M1+E2 [M2] | 351.202 324.2 99.361 | (4)+ 5+ 3- | |
534.37 4 | BCD F H | (4-) | 260.87 15 265.6131 5 354.1162 2 360.43 4 434.9956 9 | 76 16 14.6 79 100 15 100.0 63 6.7 33 | (M1) M1 | 273.627 268.800 180.2 173.929 99.361 | 4- 4- (6-) 4- 3- | |
549.330 9 | B D F | (5+) | 123.507 6 128.7442 5 375.4003 12 | 100 11.7 88 <17.5 | M1+E2 | 425.823 420.560 173.929 | (4+) (4+) 4- | |
556.0 7 | B DEF H | (6+) | 231.8 5 | 100 | M1+E2 | 324.2 | 5+ | |
559.976 9 | B D FGH | (5+) | 134.158 16 139.416 7 | 18.1 22 100 16 | M1+E2 | 425.823 420.560 | (4+) (4+) | |
577.720 15 | BCD F | (2-) | 199.5? 261.266 12 | 53 18 100 16 | (M1+E2) | 378.387 316.459 | (2-) (1-) | |
588.705 12 | BC FG | (4-) | 118.196 4 266.3501 4 442.2817 11 | 100.0 61 7.9 30 6.1 52 | 470.509 322.378 146.275 | (3-) 3- 3- | ||
595.059 3 | B | (6-) | 177.2728 2 | 100 | 417.794 | 5- | ||
601.57 3 | B G | (1+) | 223.1878 4 285.10 3 390.91 5 | 6.5 27 18.0 12 100.0 18 | E1+M2 E1+M2 | 378.387 316.459 210.699 | (2-) (1-) 2- | |
606.8 10 | F | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
610.1 10 | F | |||||||
623.89 6 | BC G | (1-) | 301.36 15 350.226 1 413.21 6 524.4963 7 564.8843 11 623.8411 10 | 33 12 13.2 79 100.0 71 34 11 16.4 71 20.9 69 | 322.378 273.627 210.699 99.361 59.010 0.0 | 3- 4- 2- 3- 2- 1- | ||
646.346 11 | B D F H | 5- | 176.552 8 228.5199 7 ? 328.42 20 ? | 100 24 12.6 72 21.0 63 | M1+E2 | 469.794 417.794 317.846 | 4- 5- 5- | |
651.6 7 | B DE H | (7+) | 186.1 5 327.5 5 | 100 9 1 | 465.4 324.2 | 6+ 5+ | ||
657.98 3 | B | (2+) | 56.408 3 335.66 20 341.38 15 447.1410 7 | 90 27 41 14 100 11 70 30 | M1+E2 | 601.57 322.378 316.459 210.699 | (1+) 3- (1-) 2- | |
660.722 5 | B | (1-) | 344.2823 9 | 100 | 316.459 | (1-) | ||
665.188 18 | B G | (6)+ | 164.466 8 313.9705 7 | 100 23 40 17 | M1+E2 | 500.722 351.202 | (5)+ (4)+ | |
680.05 12 | BCD F H | (2-) | 357.65 15 469.39 20 505.9847 10 580.5283 8 620.8425 5 680.0 10 | 52.9 35 30.2 27 19.2 77 11.5 39 32.7 77 100 23 | 322.378 210.699 173.929 99.361 59.010 0.0 | 3- 2- 4- 3- 2- 1- | ||
686.055 16 | BCD F H | (3-) | 108.336 5 215.28 15 307.56 6 | 25.7 57 14.0 34 100.0 71 | M1+E2 | 577.720 470.509 378.387 | (2-) (3-) (2-) | |
689.3 | CD F H | (1-) | ||||||
691.37 9 | B F H | (6-) | 193.95 10 ? 228.42 10 273.5703 7 373.49 15 | 90 18 68.5 71 35 17 100.0 87 | 497.294 462.969 417.794 317.846 | (6-) 5- 5- 5- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
705.048 5 | B | (6+) | 155.6944 4 | 100 | 549.330 | (5+) | ||
705.2 7 | EF | (10+) | 290.4 5 557.1 5 | 59 7 100 | 414.7 148.2 | (9+) (8+) | ||
709.6 4 | EF | (7-) | 212.7 5 391.4 5 | | 497.294 317.846 | (6-) 5- | ||
722.962 3 | B F H | (5-) | 188.5670 3 542.5661 10 | 100 38 9.4 50 | 534.37 180.2 | (4-) (6-) | ||
728.2 15 | F H | |||||||
736.127 15 | B F | (5-) | 147.417 6 ? 266.3501 4 318.2979 7 | 100 11 11.7 44 26 14 | (M1+E2) | 588.705 469.794 417.794 | (4-) 4- 5- | |
744.80 5 | B D | (3+) | 86.84 4 | 100.0 | M1 | 657.98 | (2+) | |
753.267 4 | BCD F H | (2-,3-) | 282.9159 7 606.9903 5 753.2663 8 | 15.6 74 100 19 93 30 | 470.509 146.275 0.0 | (3-) 3- 1- | ||
761.42 19 | BC F H | (1-,2-,3-) | 439.01 20 444.9631 7 550.9 5 615.3883 16 702.6092 19 ? 761.6 10 | 100 10 49 21 95 32 25 13 30 16 131 14 | 322.378 316.459 210.699 146.275 59.010 0.0 | 3- (1-) 2- 3- 2- 1- | ||
773.6 9 | EF | (7+) | 217.6 5 | 100 | 556.0 | (6+) | ||
774.879 18 | B | (7-) | 360.6248 17 594.5845 18 626.8018 20 | 100 60 39 23 14 | 414.7 180.2 148.2 | (9+) (6-) (8+) | ||
785.58 15 | B | (1-,2-,3-) | 406.92 20 468.8837 15 726.3659 12 | 100.0 96 14 11 68 23 | 378.387 316.459 59.010 | (2-) (1-) 2- | ||
791.225 5 | BCD F H | (1-,2-,3-) | 468.8837 15 580.5283 8 644.9220 8 691.6333 13 732.2170 8 | 14 11 50 17 11 4 25 10 100 22 | 322.378 210.699 146.275 99.361 59.010 | 3- 2- 3- 3- 2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
795.9 7 | E G | (10+) | 381.2 5 647.6 5 | 50 5 100 | 414.7 148.2 | (9+) (8+) | ||
796.45 9 | BCD F H | (LE 3-) | 218.69 10 418.37 20 473.9867 11 ? 479.3 584.3 7 737.1875 10 796.5 15 | 18.1 19 36 17 12 5 100.0 63 25 13 16 5 28 25 | 577.720 378.387 322.378 316.459 210.699 59.010 0.0 | (2-) (2-) 3- (1-) 2- 2- 1- | ||
803 10 | D H | |||||||
814.187 9 | BC F H | (1-,2-) | 603.4963 10 813.9455 15 | 71 24 100 42 | 210.699 0.0 | 2- 1- | ||
819.00 19 | BC F H | (2-,3-) | 496.59 20 545.1537 13 607.5 8 645.3 8 672.5994 14 761.6 10 | 100.0 54 6.6 36 65 24 30 11 8.4 45 56 6 | 322.378 273.627 210.699 173.929 146.275 59.010 | 3- 4- 2- 4- 3- 2- | ||
821.30 6 | B H | (0+) | 163.31 6 219.78 10 821.3334 19 | 55 21 100.0 75 51 28 | 657.98 601.57 0.0 | (2+) (1+) 1- | ||
826.150 17 | BC H | (4-) | 140.095 5 237.60 15 355.63 5 | 100 12 14 4 42.3 96 | M1+E2 | 686.055 588.705 470.509 | (3-) (4-) (3-) | |
855.04 5 ? | B D | (4+) | 110.240 4 196.98 10 ? | 100 11 14.0 26 | 744.80 657.98 | (3+) (2+) | ||
856.225 7 | BCD F | (2-,3-) | 539.7864 9 645.6312 14 856.2132 16 | 50 17 22 12 100 44 | 316.459 210.699 0.0 | (1-) 2- 1- | ||
860.386 7 | B | (6-) | 213.8470 5 362.9614 12 ? 397.5339 8 542.5661 10 | 100 50 63 38 75 38 45 23 | 646.346 497.294 462.969 317.846 | 5- (6-) 5- 5- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
864.17 15 | BCD F | (2-,3-) | 286.45 15 | 100 | 577.720 | (2-) | ||
869.2 7 | E | (8+) | 217.5 5 403.8 5 | 100 22 2 | 651.6 465.4 | (7+) 6+ | ||
871.0 10 | BCD F | (2-,3-,4-) | 548.6176 10 597.9591 8 ? 660.1877 12 696.9010 11 ? 771.7231 8 | 54 24 98 27 14 7 61 21 100 25 | 322.378 273.627 210.699 173.929 99.361 | 3- 4- 2- 4- 3- | ||
879.183 8 | BCD | (2-,3-) | 556.8625 12 610.3402 14 779.7021 10 ? | 50 22 28 14 100 38 | 322.378 268.800 99.361 | 3- 4- 3- | ||
888.777 3 | BCD F | (4-) | 202.6952 3 418.5012 9 | 100 29 87 33 | 686.055 470.509 | (3-) (3-) | ||
889.676 4 | CD F | (1-,2-,3-) | 311.9945 6 419.8915 5 567.2060 11 ? 573.2576 18 | 23 10 100 25 25 12 19 12 | 577.720 469.794 322.378 316.459 | (2-) 4- 3- (1-) | ||
895.283 9 | BCD F | (2-,3-,4-) | 208.9310 5 577.4762 12 684.5342 13 721.6994 20 | 55.6 31 100 44 72 37 54 30 | 686.055 317.846 210.699 173.929 | (3-) 5- 2- 4- | ||
902.336 8 | BCD F | (2-,3-) | 324.4419 7 579.8404 14 ? 691.6333 13 803.0772 12 ? | 29 17 28 16 16 6 100 35 | 577.720 322.378 210.699 99.361 | (2-) 3- 2- 3- | ||
910.478 11 | B | (2+) | 253.6189 6 308.8557 5 | 87 45 100 53 | 657.98 601.57 | (2+) (1+) | ||
912.378 5 | B | (6-) | 176.2941 3 317.4579 8 | 100 43 34 18 | 736.127 595.059 | (5-) (6-) | ||
913.58 3 | BC F | (2-,3-) | 644.9220 8 767.1551 12 813.9455 15 | 12.7 47 100 33 80 33 | 268.800 146.275 99.361 | 4- 3- 3- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
923.629 3 | BC F | (2-,3-) | 237.5479 3 453.1551 14 545.1537 13 601.3946 7 613.3660 13 ? 755.8149 10 ? 824.2034 18 | 21.4 64 18 13 10.0 55 68 18 15.9 82 100 27 73 32 | 686.055 470.509 378.387 322.378 316.459 173.929 99.361 | (3-) (3-) (2-) 3- (1-) 4- 3- | ||
929.6 15 | C F | (-) | ||||||
935.31 20 | BC F | (2-,3-) | ||||||
937.4 15 | C F | (1-) | ||||||
944.238 10 | BC F | (2-,3-) | 733.5210 11 798.042 2 | 100 36 64 36 | 210.699 146.275 | 2- 3- | ||
953.2 5 | EF | (8-) | 243 1 ? 455.9 5 | | 709.6 497.294 | (7-) (6-) | ||
954.72 23 | B F | (2-,3-,4-) | 365.8498 7 ? 484.0470 11 ? 576.1214 16 743.8408 18 808.4161 16 895.9148 17 954.737 1 | 7.4 37 7.4 37 2.3 17 7.4 37 9.3 37 19 10 100 26 | 588.705 470.509 378.387 210.699 146.275 59.010 0.0 | (4-) (3-) (2-) 2- 3- 2- 1- | ||
965.427 4 | B | (1+) | 144.0450 3 304.7179 6 307.4080 8 | 100 42 84 34 48 28 | 821.30 660.722 657.98 | (0+) (1-) (2+) | ||
973.861 8 | BC F | (2-,3-,4-) | 396.1636 7 503.8689 11 ? 651.5000 8 704.7114 16 ? | 100 44 78 33 87 27 48 23 | 577.720 469.794 322.378 268.800 | (2-) 4- 3- 4- | ||
982.27 18 | B F | (2-,3-,4-) | 404.7001 8 660.1877 12 771.7231 8 808.4161 16 | 16.7 71 3.8 19 40.5 95 100 43 | 577.720 322.378 210.699 173.929 | (2-) 3- 2- 4- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
988.973 5 | BC F | (2-,3-) | 454.5360 9 518.5086 12 815.0087 23 842.7101 6 889.866 3 | 6.8 29 6.8 39 12.6 68 100 17 25 17 | 534.37 470.509 173.929 146.275 99.361 | (4-) (3-) 4- 3- 3- | ||
996.685 4 | B | (5-) | 170.5111 4 260.5964 5 | 100 57 86 36 | 826.150 736.127 | (4-) (5-) | ||
997.84 6 ? | B | (5+) | 142.80 4 | 100 | 855.04 | (4+) | ||
999.320 6 | BC | (2-,3-,4-) | 410.6935 6 528.6262 11 725.5955 21 | 100 33 48 23 50 25 | 588.705 470.509 273.627 | (4-) (3-) 4- | ||
1002.678 9 | B F | (3-,4-,5-) | 266.3501 4 ? 414.0423 9 | 23.3 83 100 50 | 736.127 588.705 | (5-) (4-) | ||
1003.526 4 | B F | (2-,3-) | 317.4579 8 425.8998 6 ? 533.0151 5 | 13.3 71 38 14 100 24 | 686.055 577.720 470.509 | (3-) (2-) (3-) | ||
1004.156 6 | BC F | (2-,3-,4-) | 415.5635 12 426.3975 7 | 61 37 100 43 | 588.705 577.720 | (4-) (2-) | ||
1007.5 3 | FG | 1007.5 3 | 100 | 0.0 | 1- | |||
1013.72 25 | BC | (2-,3-,4-) | ||||||
1017.60 17 | BC F | (1-,2-,3-) | ||||||
1018.0 8 | E | (11+) | 312.7 5 603.3 5 | 26 13 100 | 705.2 414.7 | (10+) (9+) | ||
1019.7 20 | C F | (1-,2-,3-) | ||||||
1027.2 20 | F | |||||||
1040.25 19 | BC F | (2-,3-,4-) | ||||||
1042.9 | C | (1-) | ||||||
1046.9 | C | (2-,3-,4-) | ||||||
1050.7 15 | F | |||||||
1053.8 6 | BC F | (1-,2-,3-) | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1057.5 5 | BC | (2-,3-) | ||||||
1068.56 22 | BC F | (2-,3-) | ||||||
1071.5 6 | BC F | (2-,3-) | ||||||
1097.01 18 | BC | (4-) | ||||||
1101.3 3 | BC FG | (2-,3-) | 1101.3 3 | 100 | 0.0 | 1- | ||
1115.2 8 | E | (9+) | 246.0 5 463.7 5 | 100 51 4 | 869.2 651.6 | (8+) (7+) | ||
1119.6 7 | E | (11+) | 323.4 5 414.3 5 705.2 5 | | 795.9 705.2 414.7 | (10+) (10+) (9+) | ||
1122.50 23 | BC | (2-,3-) | ||||||
1132.07 20 | B | (2-,3-,4-) | ||||||
1138.1 8 | E | (11+) | 433.0 5 723.3 5 | | 705.2 414.7 | (10+) (9+) | ||
1140.9 3 | BC | (2-,3-) | ||||||
1151.14 18 | BC | (4-) | ||||||
1157.8 2 | BC F | (2-,3-,4-) | ||||||
1163.1 5 | C F | (1-) | ||||||
1172.19 18 | BC F | (2-,3-,4-) | ||||||
1184.99 19 | BC | (2-,3-) | ||||||
1194.3 | C | (2-,3-,4-) | ||||||
1197.89 18 | BC F | (2-,3-) | ||||||
1212.0 4 | B F | (2+,3+,4+) | ||||||
1219.5 10 | C F | (1-) | ||||||
1225.8 | C | (1-,2-,3-) | ||||||
1227.88 21 | B | (2-,3-,4-) | ||||||
1229.7 15 | F | |||||||
1231.3 3 | BC | (2-,3-) | ||||||
1240.3 3 | B F | (2-,3-,4-) | ||||||
1242.64 21 | BC | (2-,3-) | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1248.5 | C | (-) | ||||||
1261.3 | BC | (1-) | ||||||
1266.4 10 | B F | |||||||
1271.8 | C | (2-,3-,4-) | ||||||
1275.3 | C | (1-,2-,3-) | ||||||
1285.8 9 | BC | (2-,3-) | ||||||
1290.6 9 | E | 494.7 5 | 100 | 795.9 | (10+) | |||
1298.1 15 | C F | (1-,2-,3-) | ||||||
1306.4 10 | BC F | (2-,3-,4-) | ||||||
1317.32 17 | BC | (2-,3-,4-) | ||||||
1321.64 20 | BC | (2-,3-) | ||||||
1326.5 10 | F | |||||||
1342.3 4 | B F | (2+,3+,4+) | ||||||
1349.1 15 | F | |||||||
1351.16 19 | BC | (4-) | ||||||
1352.6 8 | E | (12+) | 334.5 5 647.5 5 | | 1018.0 705.2 | (11+) (10+) | ||
1355.4 3 | BC F | (2-,3-) | ||||||
1360.3 4 | BC | (2-,3-,4-) | ||||||
1369.2 15 | F | |||||||
1375.7 7 | BC F | (1-,2-,3-) | ||||||
1385.3 | C | (2-,3-) | ||||||
1386.4 8 | E | (10+) | 271.2 5 517.1 5 | 100 69 6 | 1115.2 869.2 | (9+) (8+) | ||
1390.5 15 | F | |||||||
1393.0 3 | BC | (2-,3-) | ||||||
1398.8 | C | (1-,2-,3-) | ||||||
1403.2 | C F | (1-) | ||||||
1405.43 16 | BC F | (2-,3-,4-) | ||||||
1419.0 3 | BC | (2-,3-) | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1421.7 10 | F | |||||||
1424.5 | C | (2-,3-) | ||||||
1431.0 | C | (4-) | ||||||
1434.2 20 | F | |||||||
1437.71 24 | B | (2-,3-,4-) | ||||||
1449.8 4 | BC F | (1-,2-,3-) | ||||||
1457.45 21 | BC F | (2-,3-) | ||||||
1462.4 5 | BC | (2-,3-) | ||||||
1472.7 20 | F | |||||||
1475.9 3 | BC | (2-,3-,4-) | ||||||
1486.66 17 | B F | (2-,3-,4-) | ||||||
1512.7 20 | F | |||||||
1520.5 20 | F | |||||||
1525.24 20 | BC | (4-) | ||||||
1529.4 20 | C F | (2-,3-) | ||||||
1538.8 | C | (1-,2-,3-) | ||||||
1544.95 17 | BC F | (2-,3-,4-) | ||||||
1550.65 20 | BC | (1-,2-,3-) | ||||||
1566.35 18 | BC | (2-,3-,4-) | ||||||
1571.98 20 | BC | (1-,2-,3-) | ||||||
1575.8 | C | (2-,3-,4-) | ||||||
1587.05 16 | BC F | (2-,3-) | ||||||
1601.7 3 | B F | (2-,3-,4-) | ||||||
1607.10 22 | B | (2-,3-,4-) | ||||||
1613.8 20 | F | |||||||
1628.18 22 | BC | (2-,3-,4-) | ||||||
1633.8 20 | F | |||||||
1637 5 | B | (2-,3-,4-) | ||||||
1643.9 | C | (1-,2-,3-) | ||||||
1646.87 23 | BC F | (2-,3-,4-) | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1659.12 15 | BC F | (2-,3-,4-) | ||||||
1667.8 | BC | (2-,3-,4-) | ||||||
1672.3 3 | BC | (1-,2-,3-) | ||||||
1684.2 | C | (2-,3-,4-) | ||||||
1694.7 4 | BC F | (2-,3-) | ||||||
1707.6 20 | F | |||||||
1711.1 | C | (2-,3-) | ||||||
1718.91 24 | BC F | (2-,3-,4-) | ||||||
1742.4 20 | F | |||||||
1743.16 22 | B | (2-,3-,4-) | ||||||
1758.0 4 | BC | (2-,3-) | ||||||
1768.4 20 | B F | |||||||
1776.4 20 | F | |||||||
1794.0 | BC | (2-,3-,4-) | ||||||
1818.1 | C | (2-,3-,4-) | ||||||
1827.54 17 | BC | (2-,3-,4-) | ||||||
1838.7 3 | BC | (1-,2-,3-) | ||||||
1846.41 22 | BC | (2-,3-) | ||||||
1881.34 22 | B | (2-,3-,4-) | ||||||
1905.8 4 | B F | (2-,3-,4-) | ||||||
1964.77 14 | B | (2-,3-,4-) | ||||||
1985 4 | B | (2-,3-,4-) | ||||||
2004 3 | B F | (2-,3-,4-) | ||||||
2055 4 | B | (2-,3-,4-) | ||||||
2063 4 | B | (2-,3-,4-) | ||||||
2083 3 | B | (2-,3-,4-) | ||||||
2106 3 | B | (2-,3-,4-) | ||||||
2141.2 10 | B | (2-,3-,4-) | ||||||
2203.4 3 | B | (2-,3-,4-) | ||||||
2219.19 22 | B | (2-,3-,4-) | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2244.81 15 | B | (2-,3-,4-) | ||||||
2261 3 | B | (2-,3-,4-) | ||||||
2319.76 23 | B F | (2-,3-,4-) | ||||||
2359.0 5 | B F | (2+,3+,4+) |
E(level): From least-squares fit to Eγ data, except where otherwise noted, yielding a normalized χ2=0.86. Tentative γ rays not used in fit to level energies. 2020Kr05 report high precision Eγ, almost all fit poorly and were not used during the fit; in this data set 140 out of 288 deviate by more than 3σ from their calculated values, yielding χ2=5905 cf. χ2crit= 1.3. Quoted level energies from 2020Kr05 are marked with a footnote.
Jπ(level): All firm assignments are also in agreement with statistical-model calculations using the DICEBOX computer code in the analysis of the partial (n,γ) cross-section data in 2016Ma35. Many of the tentative assignments are also supported by the statistical-model calculations; see comments.
T1/2(level): From (n,γ) E=thermal, except as noted.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - Kπ=2-, (π5/2[402])-(ν1/2[510]) band. | |||||||
210.699 5 | 2- | < 0.2 ns | |||||
322.378 6 | 3- | 111.674 6 148.37 6 176.112 8 223.035 15 263.33 20 | 100 21 5.9 14 27.1 57 35.7 21 16.4 36 | M1+E2 M1+E2 M1+E2 | 210.699 173.929 146.275 99.361 59.010 | 2- 4- 3- 3- 2- | |
469.794 8 | 4- | 147.417 6 200.981 16 295.88 15 370.3793 7 | 100.0 29 18.4 39 13.7 11 8.6 43 | M1+E2 M1 | 322.378 268.800 173.929 99.361 | 3- 4- 4- 3- | |
646.346 11 | 5- | 176.552 8 228.5199 7 ? 328.42 20 ? | 100 24 12.6 72 21.0 63 | M1+E2 | 469.794 417.794 317.846 | 4- 5- 5- | |
860.386 7 | (6-) | 213.8470 5 362.9614 12 ? 397.5339 8 542.5661 10 | 100 50 63 38 75 38 45 23 | 646.346 497.294 462.969 317.846 | 5- (6-) 5- 5- | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - Kπ=4-, (π5/2[402])+(ν3/2[512]) band. | |||||||
173.929 4 | 4- | ||||||
317.846 7 | 5- | 143.919 5 218.6187 5 ? | 100 13 5.6 28 | M1+E2 | 173.929 99.361 | 4- 3- | |
497.294 10 | (6-) | 179.448 7 323.5 5 | 100 13 1 | 317.846 173.929 | 5- 4- | ||
709.6 4 | (7-) | 212.7 5 391.4 5 | | 497.294 317.846 | (6-) 5- | ||
953.2 5 | (8-) | 243 1 ? 455.9 5 | | 709.6 497.294 | (7-) (6-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - Kπ=3-, (π5/2[402])+(ν1/2[510]) band. | |||||||
99.361 3 | 3- | 25.5 ns 25 | |||||
273.627 5 | 4- | 99.696 4 127.352 4 174.271 9 | 27.0 63 68 15 100.0 63 | M1+E2 M1+E2 | 173.929 146.275 99.361 | 4- 3- 3- | |
462.969 9 | 5- | 145.131 8 189.313 17 193.95 10 289.06 15 363.45 15 | 14.2 44 100 26 29.6 17 9.2 27 49.8 35 | M1+E2 | 317.846 273.627 268.800 173.929 99.361 | 5- 4- 4- 4- 3- | |
691.37 9 | (6-) | 193.95 10 ? 228.42 10 273.5703 7 373.49 15 | 90 18 68.5 71 35 17 100.0 87 | 497.294 462.969 417.794 317.846 | (6-) 5- 5- 5- | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - Kπ=1-, (π5/2[402])-(ν3/2[512]) band. | |||||||
0.0 | 1- | 3.7185 d 5 % ε = 7.50 10 % β- = 92.50 10 | |||||
59.010 3 | 2- | 59.009 4 | 100 | M1+E2 | 0.0 | 1- | |
146.275 4 | 3- | 87.266 4 146.273 12 | 100.0 59 8.4 17 | M1(+E2) | 59.010 0.0 | 2- 1- | |
268.800 6 | 4- | 122.525 5 169.431 8 209.82 2 | 100.0 71 19.8 50 22.5 22 | M1+E2 | 146.275 99.361 59.010 | 3- 3- 2- | |
417.794 8 | 5- | 144.152 5 ? 148.994 5 271.47 10 | 13.16 70 100 18 40 12 | M1+E2 | 273.627 268.800 146.275 | 4- 4- 3- | |
595.059 3 | (6-) | 177.2728 2 | 100 | 417.794 | 5- | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 5 - Kπ=2-, (π5/2[402])-(ν9/2[505]) band. | |||||||
577.720 15 | (2-) | ||||||
686.055 16 | (3-) | 108.336 5 215.28 15 307.56 6 | 25.7 57 14.0 34 100.0 71 | M1+E2 | 577.720 470.509 378.387 | (2-) (3-) (2-) | |
826.150 17 | (4-) | 140.095 5 237.60 15 355.63 5 | 100 12 14 4 42.3 96 | M1+E2 | 686.055 588.705 470.509 | (3-) (4-) (3-) | |
996.685 4 | (5-) | 170.5111 4 260.5964 5 | 100 57 86 36 | 826.150 736.127 | (4-) (5-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 6 - Kπ=3+, (π5/2[402])-(ν11/2[615]) band. | |||||||
314.009 5 | (3+) | 24.1 ns 11 | |||||
420.560 7 | (4+) | 106.550 4 321.1896 7 | 100 12 5.9 32 | M1+E2 | 314.009 99.361 | (3+) 3- | |
559.976 9 | (5+) | 134.158 16 139.416 7 | 18.1 22 100 16 | M1+E2 | 425.823 420.560 | (4+) (4+) | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 7 - Kπ=(4)+, (π9/2[514])-(ν1/2[510]) band. See comments for | |||||||
351.202 16 | (4)+ | < 0.2 ns | |||||
500.722 16 | (5)+ | 149.520 5 176.2941 3 401.3 3 | 100 50 11.1 56 12.6 13 | M1+E2 [M2] | 351.202 324.2 99.361 | (4)+ 5+ 3- | |
665.188 18 | (6)+ | 164.466 8 313.9705 7 | 100 23 40 17 | M1+E2 | 500.722 351.202 | (5)+ (4)+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 8 - Kπ=(1+), (π9/2[514])-(ν7/2[503]) band. | |||||||
601.57 3 | (1+) | ||||||
657.98 3 | (2+) | 56.408 3 335.66 20 341.38 15 447.1410 7 | 90 27 41 14 100 11 70 30 | M1+E2 | 601.57 322.378 316.459 210.699 | (1+) 3- (1-) 2- | |
744.80 5 | (3+) | 86.84 4 | 100.0 | M1 | 657.98 | (2+) | |
855.04 5 | (4+) | 110.240 4 196.98 10 ? | 100 11 14.0 26 | 744.80 657.98 | (3+) (2+) | ||
997.84 6 | (5+) | 142.80 4 | 100 | 855.04 | (4+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 9 - Kπ=1-, (π5/2[402])-(ν7/2[503]) band. | |||||||
316.459 10 | (1-) | 0.20 ns 10 | |||||
378.387 10 | (2-) | 61.928 4 232.100 16 319.44 10 378.42 5 | 73 11 36.2 39 24.2 15 100.0 59 | M1+E2 M1+E2 M1+E2 | 316.459 146.275 59.010 0.0 | (1-) 3- 2- 1- | |
470.509 11 | (3-) | 92.122 4 148.09 6 201.78 10 411.18 20 | 100 23 6.8 21 6.8 21 54.5 42 | M1+E2 | 378.387 322.378 268.800 59.010 | (2-) 3- 4- 2- | |
588.705 12 | (4-) | 118.196 4 266.3501 4 442.2817 11 | 100.0 61 7.9 30 6.1 52 | 470.509 322.378 146.275 | (3-) 3- 3- | ||
736.127 15 | (5-) | 147.417 6 ? 266.3501 4 318.2979 7 | 100 11 11.7 44 26 14 | (M1+E2) | 588.705 469.794 417.794 | (4-) 4- 5- | |
912.378 5 | (6-) | 176.2941 3 317.4579 8 | 100 43 34 18 | 736.127 595.059 | (5-) (6-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 10 - Kπ=5+, (π9/2[514])+(ν1/2[510]) band. | |||||||
324.2 5 | 5+ | 17.3 ns 6 | |||||
465.4 7 | 6+ | 141.1 5 | 100.0 | M1+E2 | 324.2 | 5+ | |
651.6 7 | (7+) | 186.1 5 327.5 5 | 100 9 1 | 465.4 324.2 | 6+ 5+ | ||
869.2 7 | (8+) | 217.5 5 403.8 5 | 100 22 2 | 651.6 465.4 | (7+) 6+ | ||
1115.2 8 | (9+) | 246.0 5 463.7 5 | 100 51 4 | 869.2 651.6 | (8+) (7+) | ||
1386.4 8 | (10+) | 271.2 5 517.1 5 | 100 69 6 | 1115.2 869.2 | (9+) (8+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 11 - Kπ=(8+), (π5/2[402])+(ν11/2[615]) band. | |||||||
148.2 5 | (8+) | 2.0×10+5 y % IT = 100 | |||||
414.7 7 | (9+) | 266.69 4 ? | 100 | 148.2 | (8+) | ||
705.2 7 | (10+) | 290.4 5 557.1 5 | 59 7 100 | 414.7 148.2 | (9+) (8+) | ||
1018.0 8 | (11+) | 312.7 5 603.3 5 | 26 13 100 | 705.2 414.7 | (10+) (9+) | ||
1352.6 8 | (12+) | 334.5 5 647.5 5 | | 1018.0 705.2 | (11+) (10+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 12 - Kπ=(6+), (π9/2[514])+(ν3/2[512]) band. | |||||||
556.0 7 | (6+) | ||||||
773.6 9 | (7+) | 217.6 5 | 100 | 556.0 | (6+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 13 - Kπ=(10+). Band built on the Jπ=(10+) state at 796 keV; see | |||||||
795.9 7 | (10+) | ||||||
1119.6 7 | (11+) | 323.4 5 414.3 5 705.2 5 | | 795.9 705.2 414.7 | (10+) (10+) (9+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 14 - Kπ=(6-), (π5/2[402])+(ν7/2[503]) band. | |||||||
180.2 7 | (6-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 15 - Kπ=(1-), (π9/2[514])-(ν11/2[615]) band. | |||||||
660.722 5 | (1-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 16 - Kπ=(4-), (π1/2[411])+(ν7/2[503]) band. | |||||||
534.37 4 | (4-) | ||||||
722.962 3 | (5-) | 188.5670 3 542.5661 10 | 100 38 9.4 50 | 534.37 180.2 | (4-) (6-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 17 - Kπ=(7-), (π5/2[402])+(ν9/2[505]) band. | |||||||
774.879 18 | (7-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 18 - Kπ=(0+), (π9/2[514])-(ν9/2[505]) band. | |||||||
821.30 6 | (0+) | ||||||
910.478 11 | (2+) | 253.6189 6 308.8557 5 | 87 45 100 53 | 657.98 601.57 | (2+) (1+) | ||
965.427 4 | (1+) | 144.0450 3 304.7179 6 307.4080 8 | 100 42 84 34 48 28 | 821.30 660.722 657.98 | (0+) (1-) (2+) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
59.010 | 2- | 59.009 4 | M1+E2 | 0.042 10 | 4.21 | α=4.21 7, α(L)=3.25 5, α(M)=0.744 12, α(N)=0.1804 30, α(O)=0.0302 5, α(P)=0.002171 30 | |
99.361 | 3- | 25.5 ns 25 | 40.350 3 | M1+E2 | 0.145 6 | 17.7 | B(E2)(W.u.)=3.42 +50-42, B(M1)(W.u.)=6.5E-4 +8-6, α=17.7 5, α(L)=13.6 4, α(M)=3.21 9, α(N)=0.773 22, α(O)=0.1233 32, α(P)=0.00653 9 |
3- | 25.5 ns 25 | 99.362 4 | E2 | 4.23 | B(E2)(W.u.)=0.391 +48-39, α=4.23 6, α(K)=0.848 12, α(L)=2.55 4, α(M)=0.650 9, α(N)=0.1543 22, α(O)=0.02198 31, α(P)=7.86E-5 11 | ||
146.275 | 3- | 87.266 4 | M1(+E2) | 0.14 LE | 7.64 | α=7.64 11, α(K)=6.27 10, α(L)=1.06 4, α(M)=0.243 10, α(N)=0.0589 23, α(O)=0.00982 33, α(P)=0.000689 11 | |
148.2 | (8+) | 2.0×10+5 y % IT = 100 | 48.84 50 | (E5) | 4.8×106 | α=4.8×106 4, α(L)=2.48E6 19, α(M)=1.82E6 16, α(N)=4.7E5 4, α(O)=4.9E4 4, α(P)=36.8 26 | |
173.929 | 4- | 74.568 3 | M1+E2 | 0.12 +5-8 | 11.97 | α=11.97 17, α(K)=9.72 18, α(L)=1.73 12, α(M)=0.400 30, α(N)=0.097 7, α(O)=0.0160 10, α(P)=0.001084 20 | |
210.699 | 2- | < 0.2 ns | 111.337 8 | M1(+E2) | 0.27 LE | 3.76 | α=3.76 6, α(K)=3.06 9, α(L)=0.540 35, α(M)=0.125 9, α(N)=0.0302 22, α(O)=0.00499 29, α(P)=0.000334 11 |
2- | < 0.2 ns | 151.686 5 | M1+E2 | 1.7 +11-5 | 1.03 | α=1.03 11, α(K)=0.59 15, α(L)=0.332 26, α(M)=0.082 7, α(N)=0.0197 17, α(O)=0.00291 20, α(P)=5.8×10-5 17 | |
2- | < 0.2 ns | 210.685 17 | M1 | 0.628 | α=0.628 9, α(K)=0.520 7, α(L)=0.0829 12, α(M)=0.01893 27, α(N)=0.00459 6, α(O)=0.000772 11, α(P)=5.65×10-5 8 | ||
268.800 | 4- | 169.431 8 | M1+E2 | 1.75 55 | 0.71 | α=0.71 10, α(K)=0.43 11, α(L)=0.212 13, α(M)=0.052 4, α(N)=0.0125 9, α(O)=0.00186 10, α(P)=4.2×10-5 13 | |
273.627 | 4- | 127.352 4 | M1+E2 | 1.7 +70-7 | 1.86 | α=1.86 24, α(K)=0.9 4, α(L)=0.70 12, α(M)=0.174 31, α(N)=0.041 7, α(O)=0.0061 9, α(P)=9.E-5 5 | |
4- | 174.271 9 | M1+E2 | 0.71 +26-23 | 0.88 | α=0.88 8, α(K)=0.67 10, α(L)=0.162 10, α(M)=0.0387 29, α(N)=0.0093 7, α(O)=0.00147 7, α(P)=7.1×10-5 11 | ||
314.009 | (3+) | 24.1 ns 11 | 103.310 6 | [E1] | 0.352 | B(E1)(W.u.)=8.1E-7 +7-6, α=0.352 5, α(K)=0.287 4, α(L)=0.0507 7, α(M)=0.01162 16, α(N)=0.00276 4, α(O)=0.000433 6, α(P)=2.206E-5 31 | |
(3+) | 24.1 ns 11 | 167.737 8 | E1+M2 | 0.26 6 | 0.53 | B(E1)(W.u.)=7.5E-8 6, B(M2)(W.u.)=0.83 +39-33, α=0.53 20, α(K)=0.40 15, α(L)=0.10 4, α(M)=0.024 10, α(N)=0.0058 24, α(O)=1.0E-3 4, α(P)=6.1E-5 25 | |
(3+) | 24.1 ns 11 | 214.648 8 | E1 | 0.0539 | B(E1)(W.u.)=4.45E-7 25, α=0.0539 8, α(K)=0.0447 6, α(L)=0.00716 10, α(M)=0.001632 23, α(N)=0.000391 5, α(O)=6.33E-5 9, α(P)=3.80E-6 5 | ||
(3+) | 24.1 ns 11 | 254.995 15 | E1 | 0.0351 | B(E1)(W.u.)=1.28E-7 10, α=0.0351 5, α(K)=0.0292 4, α(L)=0.00460 6, α(M)=0.001048 15, α(N)=0.0002516 35, α(O)=4.09E-5 6, α(P)=2.533E-6 35 | ||
316.459 | (1-) | 0.20 ns 10 | 257.446 15 | M1+E2 | 0.55 +22-23 | 0.310 | B(E2)(W.u.)=2.6 +30-17, B(M1)(W.u.)=0.0014 +13-5, α=0.310 31, α(K)=0.250 30, α(L)=0.0460 11, α(M)=0.01069 18, α(N)=0.00258 5, α(O)=0.000424 13, α(P)=2.67E-5 35 |
(1-) | 0.20 ns 10 | 316.473 20 | M1 | 0.2061 | B(M1)(W.u.)=0.0018 +15-6, α=0.2061 29, α(K)=0.1712 24, α(L)=0.0270 4, α(M)=0.00616 9, α(N)=0.001494 21, α(O)=0.0002513 35, α(P)=1.847×10-5 26 | ||
317.846 | 5- | 143.919 5 | M1+E2 | 1.5 +9-5 | 1.27 | α=1.27 16, α(K)=0.74 22, α(L)=0.40 4, α(M)=0.100 12, α(N)=0.0238 29, α(O)=0.0035 4, α(P)=7.3×10-5 25 | |
322.378 | 3- | 111.674 6 | M1+E2 | 1.29 +51-32 | 3.08 | α=3.08 16, α(K)=1.60 34, α(L)=1.12 14, α(M)=0.28 4, α(N)=0.067 9, α(O)=0.0098 11, α(P)=0.00017 4 | |
3- | 176.112 8 | M1+E2 | 0.93 +43-31 | 0.78 | α=0.78 10, α(K)=0.57 12, α(L)=0.164 11, α(M)=0.0396 34, α(N)=0.0095 8, α(O)=0.00147 8, α(P)=5.9×10-5 14 | ||
3- | 223.035 15 | M1+E2 | 0.97 +28-22 | 0.38 | α=0.38 4, α(K)=0.29 4, α(L)=0.0717 10, α(M)=0.01712 35, α(N)=0.00412 8, α(O)=0.000649 9, α(P)=3.0×10-5 5 | ||
324.2 | 5+ | 17.3 ns 6 | 144.0 5 | E1 | 0.1495 | B(E1)(W.u.)=3.01E-6 13, α=0.1495 25, α(K)=0.1229 20, α(L)=0.02059 35, α(M)=0.00471 8, α(N)=0.001124 19, α(O)=0.0001790 30, α(P)=9.91E-6 16 | |
5+ | 17.3 ns 6 | 150.3 5 | E1+M2 | 0.17 5 | 0.42 | B(E1)(W.u.)=3.38E-7 30, α=0.42 18, α(K)=0.32 13, α(L)=0.08 4, α(M)=0.018 9, α(N)=0.0045 22, α(O)=7.E-4 4, α(P)=4.6E-5 24 | |
351.202 | (4)+ | < 0.2 ns | 251.841 15 | E1 | 0.0362 | α=0.0362 5, α(K)=0.0301 4, α(L)=0.00475 7, α(M)=0.001082 15, α(N)=0.000260 4, α(O)=4.22×10-5 6, α(P)=2.61E-6 4 | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
378.387 | (2-) | 61.928 4 | M1+E2 | 0.54 8 | 10.0 | α=10.0 15, α(L)=7.6 11, α(M)=1.88 29, α(N)=0.45 7, α(O)=0.067 9, α(P)=0.00152 9 | |
(2-) | 232.100 16 | M1+E2 | 0.57 17 | 0.410 | α=0.410 31, α(K)=0.329 31, α(L)=0.0630 9, α(M)=0.01469 23, α(N)=0.00355 5, α(O)=0.000578 9, α(P)=3.5×10-5 4 | ||
(2-) | 378.42 5 | M1+E2 | 0.4 2 | 0.116 | α=0.116 11, α(K)=0.096 9, α(L)=0.0157 9, α(M)=0.00361 18, α(N)=0.00087 4, α(O)=0.000146 9, α(P)=1.03×10-5 11 | ||
417.794 | 5- | 148.994 5 | M1+E2 | 1.1 +8-4 | 1.24 | α=1.24 18, α(K)=0.82 24, α(L)=0.32 4, α(M)=0.079 12, α(N)=0.0188 29, α(O)=0.00285 35, α(P)=8.4×10-5 28 | |
420.560 | (4+) | 106.550 4 | M1+E2 | 1.5 +16-5 | 3.54 | α=3.54 24, α(K)=1.6 6, α(L)=1.46 27, α(M)=0.37 7, α(N)=0.087 17, α(O)=0.0127 23, α(P)=1.7×10-4 7 | |
425.823 | (4+) | 111.814 4 | M1+E2 | 1.29 +50-32 | 3.06 | α=3.06 16, α(K)=1.60 34, α(L)=1.11 14, α(M)=0.28 4, α(N)=0.066 9, α(O)=0.0097 11, α(P)=0.00016 4 | |
462.969 | 5- | 189.313 17 | M1+E2 | 0.91 +35-26 | 0.64 | α=0.64 7, α(K)=0.47 8, α(L)=0.126 5, α(M)=0.0303 17, α(N)=0.0073 4, α(O)=0.00114 4, α(P)=4.9×10-5 10 | |
5- | 193.95 10 | α(K)=0.42 24, α(L)=0.117 13, α(M)=0.028 4, α(N)=0.0068 10, α(O)=0.00105 8, α(P)=4.3×10-5 28 | |||||
465.4 | 6+ | 141.1 5 | M1+E2 | 0.7 +7-6 | 1.66 | α=1.66 28, α(K)=1.2 4, α(L)=0.34 9, α(M)=0.082 24, α(N)=0.020 6, α(O)=0.0031 7, α(P)=1.3×10-4 5 | |
469.794 | 4- | 147.417 6 | M1+E2 | 0.95 +27-22 | 1.34 | α=1.34 10, α(K)=0.92 13, α(L)=0.320 25, α(M)=0.078 7, α(N)=0.0187 17, α(O)=0.00285 20, α(P)=9.6×10-5 16 | |
4- | 295.88 15 | M1 | 0.2472 | α=0.2472 35, α(K)=0.2053 29, α(L)=0.0324 5, α(M)=0.00740 10, α(N)=0.001796 25, α(O)=0.000302 4, α(P)=2.217×10-5 31 | |||
470.509 | (3-) | 92.122 4 | M1+E2 | 0.80 +44-34 | 6.24 | α=6.24 19, α(K)=3.7 10, α(L)=2.0 6, α(M)=0.48 16, α(N)=0.12 4, α(O)=0.017 5, α(P)=4.0×10-4 11 | |
500.722 | (5)+ | 149.520 5 | M1+E2 | 1.8 +14-5 | 1.06 | α=1.06 11, α(K)=0.59 15, α(L)=0.356 27, α(M)=0.089 8, α(N)=0.0212 18, α(O)=0.00312 21, α(P)=5.8×10-5 17 | |
(5)+ | 401.3 3 | [M2] | 0.369 | α=0.369 5, α(K)=0.293 4, α(L)=0.0583 8, α(M)=0.01373 20, α(N)=0.00334 5, α(O)=0.000557 8, α(P)=3.85×10-5 5 | |||
534.37 | (4-) | 260.87 15 | (M1) | 0.348 | α=0.348 5, α(K)=0.289 4, α(L)=0.0458 6, α(M)=0.01046 15, α(N)=0.00254 4, α(O)=0.000427 6, α(P)=3.13×10-5 4 | ||
(4-) | 360.43 4 | M1 | 0.1453 | α=0.1453 20, α(K)=0.1208 17, α(L)=0.01898 27, α(M)=0.00433 6, α(N)=0.001050 15, α(O)=0.0001766 25, α(P)=1.300×10-5 18 | |||
549.330 | (5+) | 123.507 6 | M1+E2 | 0.75 35 | 2.46 | α=2.46 23, α(K)=1.7 4, α(L)=0.58 13, α(M)=0.141 34, α(N)=0.034 8, α(O)=0.0052 10, α(P)=1.8×10-4 5 | |
556.0 | (6+) | 231.8 5 | M1+E2 | 0.47 17 | 0.430 | α=0.430 32, α(K)=0.348 32, α(L)=0.0633 10, α(M)=0.01469 25, α(N)=0.00355 6, α(O)=0.000583 10, α(P)=3.7×10-5 4 | |
559.976 | (5+) | 139.416 7 | M1+E2 | 1.8 +41-7 | 1.35 | α=1.35 19, α(K)=0.72 27, α(L)=0.48 6, α(M)=0.119 17, α(N)=0.028 4, α(O)=0.0042 5, α(P)=7.0×10-5 32 | |
577.720 | (2-) | 261.266 12 | (M1+E2) | 0.4 2 | 0.318 | α=0.318 27, α(K)=0.260 26, α(L)=0.0447 11, α(M)=0.01031 18, α(N)=0.00249 5, α(O)=0.000413 12, α(P)=2.79×10-5 30 | |
601.57 | (1+) | 285.10 3 | E1+M2 | 0.32 8 | 0.13 | α=0.13 5, α(K)=0.10 4, α(L)=0.021 8, α(M)=0.0049 20, α(N)=0.0012 5, α(O)=2.0×10-4 8, α(P)=1.3E-5 5 | |
(1+) | 390.91 5 | E1+M2 | 0.26 8 | 0.037 | α=0.037 16, α(K)=0.030 12, α(L)=0.0055 25, α(M)=0.0013 6, α(N)=3.1×10-4 14, α(O)=5.2E-5 24, α(P)=3.6E-6 17 | ||
646.346 | 5- | 176.552 8 | M1+E2 | 0.89 +41-30 | 0.79 | α=0.79 10, α(K)=0.58 12, α(L)=0.161 11, α(M)=0.0388 33, α(N)=0.0093 8, α(O)=0.00145 8, α(P)=6.1×10-5 14 | |
5- | 328.42 20 | α(K)=0.10 5, α(L)=0.020 4, α(M)=0.0048 8, α(N)=0.00116 20, α(O)=0.00019 4, α(P)=1.1×10-5 6 | |||||
657.98 | (2+) | 56.408 3 | M1+E2 | 0.85 25 | 24 | α=24 7, α(L)=18 5, α(M)=4.5 14, α(N)=1.08 32, α(O)=0.16 4, α(P)=0.00159 33 | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
665.188 | (6)+ | 164.466 8 | M1+E2 | 1.1 +9-4 | 0.91 | α=0.91 16, α(K)=0.62 19, α(L)=0.219 25, α(M)=0.053 7, α(N)=0.0128 17, α(O)=0.00195 19, α(P)=6.4×10-5 23 | |
686.055 | (3-) | 307.56 6 | M1+E2 | 0.3 2 | 0.211 | α=0.211 17, α(K)=0.174 16, α(L)=0.0285 11, α(M)=0.00653 20, α(N)=0.00158 5, α(O)=0.000264 11, α(P)=1.87×10-5 18 | |
736.127 | (5-) | 147.417 6 | (M1+E2) | 0.95 +27-22 | 1.34 | α=1.34 10, α(K)=0.92 13, α(L)=0.320 25, α(M)=0.078 7, α(N)=0.0187 17, α(O)=0.00285 20, α(P)=9.6×10-5 16 | |
744.80 | (3+) | 86.84 4 | M1 | 7.75 | α=7.75 11, α(K)=6.41 9, α(L)=1.037 15, α(M)=0.2371 33, α(N)=0.0575 8, α(O)=0.00966 14, α(P)=0.000705 10 | ||
826.150 | (4-) | 140.095 5 | M1+E2 | 2.5 5 | 1.24 | α=1.24 6, α(K)=0.59 8, α(L)=0.495 18, α(M)=0.124 5, α(N)=0.0296 12, α(O)=0.00431 15, α(P)=5.5×10-5 9 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 1- | 3.7185 d 5 % ε = 7.50 10 % β- = 92.50 10 | μ=+1.734 3, Q=+0.618 6 %ε, %β-: from 186Re ε decay (3.7186 d). E(level): %ε, %β-: from 186Re ε decay (3.7186 d). Kπ=1-, (π5/2[402])-(ν3/2[512]) band. T1/2(level): Weighted average of 3.7160 d 24 (89.256 h 58) (2016Lu16), 3.7186 d 5 (2004Sc04), 3.719 d 8 (89.25 h 18) (2014Un01 supersedes 2002Un02,1991Co17,1994Co02), and 3.7183 d 11 (89.239 h 26) (1994Sc39). Other values not used in average because outliers or lower accuracy: 3.6813 d 67 (88.35 h 16) (2018Ka49), 3.765 d 32 (90.36 h 77) (2011Bo11), 3.775 d 1 (90.600 h 24) (1989Ab18), 3.777 d 4 (90.64 h 9) (1971Mi16), 3.78 d 13 (90.6 h 31) (1958Gu09), 3.704 d 8 (88.9 h 2) (1956Po28), 3.867 d 8 (92.8 h 2) (1947Go01). |
59.010 | 2- | E(level): Kπ=1-, (π5/2[402])-(ν3/2[512]) band. | |
99.361 | 3- | 25.5 ns 25 | E(level): Energy and corresponding branching ratio (if given) from 187Re(n,2nγ) (2015Ma60). Kπ=3-, (π5/2[402])+(ν1/2[510]) band. |
146.275 | 3- | E(level): Kπ=1-, (π5/2[402])-(ν3/2[512]) band. | |
148.2 | (8+) | 2.0×10+5 y % IT = 100 | E(level): Kπ=(8+), (π5/2[402])+(ν11/2[615]) band. |
173.929 | 4- | XREF: H(177). E(level): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). Kπ=4-, (π5/2[402])+(ν3/2[512]) band. | |
180.2 | (6-) | E(level): Kπ=(6-), (π5/2[402])+(ν7/2[503]) band. From 186W(d,2nγ) (2017Ma39). | |
210.699 | 2- | < 0.2 ns | E(level): Kπ=2-, (π5/2[402])-(ν1/2[510]) band. |
268.800 | 4- | E(level): Kπ=1-, (π5/2[402])-(ν3/2[512]) band. | |
273.627 | 4- | E(level): Energy and corresponding branching ratio (if given) from 187Re(n,2nγ) (2015Ma60). Kπ=3-, (π5/2[402])+(ν1/2[510]) band. | |
314.009 | (3+) | 24.1 ns 11 | μ=+2.18 6 E(level): Kπ=3+, (π5/2[402])-(ν11/2[615]) band. |
316.459 | (1-) | 0.20 ns 10 | XREF: F(317.4). E(level): Kπ=1-, (π5/2[402])-(ν7/2[503]) band. |
317.846 | 5- | XREF: F(317.4). E(level): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). Kπ=4-, (π5/2[402])+(ν3/2[512]) band. | |
322.378 | 3- | E(level): Kπ=2-, (π5/2[402])-(ν1/2[510]) band. | |
324.2 | 5+ | 17.3 ns 6 | μ=+4.62 11 E(level): Kπ=5+, (π9/2[514])+(ν1/2[510]) band. |
351.202 | (4)+ | < 0.2 ns | E(level): Kπ=(4)+, (π9/2[514])-(ν1/2[510]) band. See comments for. |
378.387 | (2-) | E(level): Kπ=1-, (π5/2[402])-(ν7/2[503]) band. | |
414.7 | (9+) | E(level): Kπ=(8+), (π5/2[402])+(ν11/2[615]) band. From 187Re(p,d) (2009Wh01). | |
417.794 | 5- | E(level): Kπ=1-, (π5/2[402])-(ν3/2[512]) band. | |
420.560 | (4+) | E(level): Kπ=3+, (π5/2[402])-(ν11/2[615]) band. | |
462.969 | 5- | E(level): Energy and corresponding branching ratio (if given) from 187Re(n,2nγ) (2015Ma60). Kπ=3-, (π5/2[402])+(ν1/2[510]) band. | |
465.4 | 6+ | E(level): Kπ=5+, (π9/2[514])+(ν1/2[510]) band. | |
469.794 | 4- | E(level): Kπ=2-, (π5/2[402])-(ν1/2[510]) band. | |
470.509 | (3-) | E(level): Kπ=1-, (π5/2[402])-(ν7/2[503]) band. | |
497.294 | (6-) | E(level): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). Kπ=4-, (π5/2[402])+(ν3/2[512]) band. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
500.722 | (5)+ | E(level): Kπ=(4)+, (π9/2[514])-(ν1/2[510]) band. See comments for. | |
534.37 | (4-) | E(level): Kπ=(4-), (π1/2[411])+(ν7/2[503]) band. | |
556.0 | (6+) | XREF: F(563.1). E(level): Kπ=(6+), (π9/2[514])+(ν3/2[512]) band. From 186W(d,2nγ) (2017Ma39). | |
559.976 | (5+) | E(level): Kπ=3+, (π5/2[402])-(ν11/2[615]) band. | |
577.720 | (2-) | E(level): Kπ=2-, (π5/2[402])-(ν9/2[505]) band. | |
588.705 | (4-) | E(level): Kπ=1-, (π5/2[402])-(ν7/2[503]) band. | |
595.059 | (6-) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=1-, (π5/2[402])-(ν3/2[512]) band. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
601.57 | (1+) | E(level): Kπ=(1+), (π9/2[514])-(ν7/2[503]) band. | |
646.346 | 5- | E(level): Kπ=2-, (π5/2[402])-(ν1/2[510]) band. | |
651.6 | (7+) | E(level): Kπ=5+, (π9/2[514])+(ν1/2[510]) band. | |
657.98 | (2+) | E(level): Kπ=(1+), (π9/2[514])-(ν7/2[503]) band. | |
660.722 | (1-) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=(1-), (π9/2[514])-(ν11/2[615]) band. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
665.188 | (6)+ | E(level): Kπ=(4)+, (π9/2[514])-(ν1/2[510]) band. See comments for. | |
686.055 | (3-) | E(level): Kπ=2-, (π5/2[402])-(ν9/2[505]) band. | |
689.3 | (1-) | XREF: F(690.3). | |
691.37 | (6-) | XREF: F(690.3). E(level): Energy and corresponding branching ratio (if given) from 187Re(n,2nγ) (2015Ma60). Kπ=3-, (π5/2[402])+(ν1/2[510]) band. | |
705.048 | (6+) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
705.2 | (10+) | E(level): Kπ=(8+), (π5/2[402])+(ν11/2[615]) band. | |
709.6 | (7-) | E(level): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). Kπ=4-, (π5/2[402])+(ν3/2[512]) band. | |
722.962 | (5-) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=(4-), (π1/2[411])+(ν7/2[503]) band. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
736.127 | (5-) | E(level): Kπ=1-, (π5/2[402])-(ν7/2[503]) band. | |
744.80 | (3+) | E(level): Kπ=(1+), (π9/2[514])-(ν7/2[503]) band. | |
753.267 | (2-,3-) | (d,p) presumed to excite this, but not the 745-keV, level because the latter’s configuration should not be excited in (d,p); (2)- in (n,γ) E=thermal (2020Kr05). E(level): (d,p) presumed to excite this, but not the 745-keV, level because the latter’s configuration should not be excited in (d,p); (2)- in (n,γ) E=thermal (2020Kr05). From 2020Kr05 - (n,γ) E=Thermal. | |
773.6 | (7+) | E(level): Kπ=(6+), (π9/2[514])+(ν3/2[512]) band. | |
774.879 | (7-) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=(7-), (π5/2[402])+(ν9/2[505]) band. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
791.225 | (1-,2-,3-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. | |
795.9 | (10+) | E(level): Kπ=(10+). Band built on the Jπ=(10+) state at 796 keV; see. | |
814.187 | (1-,2-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. | |
821.30 | (0+) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=(0+), (π9/2[514])-(ν9/2[505]) band. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
826.150 | (4-) | E(level): Kπ=2-, (π5/2[402])-(ν9/2[505]) band. | |
855.04 | (4+) | E(level): Kπ=(1+), (π9/2[514])-(ν7/2[503]) band. | |
856.225 | (2-,3-) | Complex level in (d,p) which presumably includes this level but not the 855 level because the latter’s configuration should not be excited in (d,p). E(level): Complex level in (d,p) which presumably includes this level but not the 855 level because the latter’s configuration should not be excited in (d,p). From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
860.386 | (6-) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=2-, (π5/2[402])-(ν1/2[510]) band. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
864.17 | (2-,3-) | XREF: F(861.2). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
869.2 | (8+) | E(level): Kπ=5+, (π9/2[514])+(ν1/2[510]) band. | |
871.0 | (2-,3-,4-) | E(level): From 187Re(p,d) (2009Wh01). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
879.183 | (2-,3-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
888.777 | (4-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
889.676 | (1-,2-,3-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
895.283 | (2-,3-,4-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
902.336 | (2-,3-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
910.478 | (2+) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=(0+), (π9/2[514])-(ν9/2[505]) band. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
912.378 | (6-) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=1-, (π5/2[402])-(ν7/2[503]) band. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
913.58 | (2-,3-) | E(level): From 187Re(p,d) (2009Wh01). From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
923.629 | (2-,3-) | XREF: F(926.8). E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
929.6 | (-) | E(level): From 187Re(p,d) (2009Wh01). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
935.31 | (2-,3-) | XREF: F(937.4). E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
937.4 | (1-) | E(level): From 187Re(p,d) (2009Wh01). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
944.238 | (2-,3-) | XREF: C(946.4). E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
953.2 | (8-) | E(level): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). Kπ=4-, (π5/2[402])+(ν3/2[512]) band. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
954.72 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
965.427 | (1+) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=(0+), (π9/2[514])-(ν9/2[505]) band. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
973.861 | (2-,3-,4-) | XREF: C(975). E(level): 1-keV uncertainty assumed (by evaluators) during fit. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
982.27 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
988.973 | (2-,3-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
996.685 | (5-) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. Kπ=2-, (π5/2[402])-(ν9/2[505]) band. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
997.84 | (5+) | E(level): Kπ=(1+), (π9/2[514])-(ν7/2[503]) band. | |
999.320 | (2-,3-,4-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1002.678 | (3-,4-,5-) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
1003.526 | (2-,3-) | E(level): 1-keV uncertainty assumed (by evaluators) during fit. From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From analysis of depopulation data in (n,γ) E=thermal (2020Kr05). | |
1004.156 | (2-,3-,4-) | E(level): From 2020Kr05 - (n,γ) E=Thermal. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1013.72 | (2-,3-,4-) | XREF: C(1015). E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1017.60 | (1-,2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1018.0 | (11+) | E(level): Kπ=(8+), (π5/2[402])+(ν11/2[615]) band. | |
1019.7 | (1-,2-,3-) | E(level): From 187Re(p,d) (2009Wh01). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1027.2 | E(level): From 187Re(p,d) (2009Wh01). | ||
1040.25 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1042.9 | (1-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1046.9 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1053.8 | (1-,2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1057.5 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1068.56 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1071.5 | (2-,3-) | XREF: C(1073.3). E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1097.01 | (4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1101.3 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
1115.2 | (9+) | E(level): Kπ=5+, (π9/2[514])+(ν1/2[510]) band. | |
1119.6 | (11+) | E(level): Kπ=(10+). Band built on the Jπ=(10+) state at 796 keV; see. | |
1122.50 | (2-,3-) | XREF: C(1123.9). E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1132.07 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1140.9 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1151.14 | (4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1157.8 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1163.1 | (1-) | E(level): From 187Re(p,d) (2009Wh01). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1172.19 | (2-,3-,4-) | XREF: C(1173.6). E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1184.99 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1194.3 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1197.89 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1212.0 | (2+,3+,4+) | XREF: F(1213.9). E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1219.5 | (1-) | E(level): From 187Re(p,d) (2009Wh01). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1225.8 | (1-,2-,3-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1227.88 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1229.7 | E(level): From 187Re(p,d) (2009Wh01). | ||
1231.3 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1240.3 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1242.64 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1248.5 | (-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1261.3 | (1-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1266.4 | E(level): From 187Re(p,d) (2009Wh01). | ||
1271.8 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1275.3 | (1-,2-,3-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
1285.8 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1298.1 | (1-,2-,3-) | E(level): From 187Re(p,d) (2009Wh01). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1306.4 | (2-,3-,4-) | XREF: C(1307.5). E(level): From 187Re(p,d) (2009Wh01). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1317.32 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1321.64 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1326.5 | E(level): From 187Re(p,d) (2009Wh01). | ||
1342.3 | (2+,3+,4+) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1349.1 | E(level): From 187Re(p,d) (2009Wh01). | ||
1351.16 | (4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1352.6 | (12+) | E(level): Kπ=(8+), (π5/2[402])+(ν11/2[615]) band. | |
1355.4 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1360.3 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1375.7 | (1-,2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1385.3 | (2-,3-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1386.4 | (10+) | E(level): Kπ=5+, (π9/2[514])+(ν1/2[510]) band. | |
1390.5 | E(level): From 187Re(p,d) (2009Wh01). | ||
1393.0 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1398.8 | (1-,2-,3-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1403.2 | (1-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1405.43 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1419.0 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1421.7 | E(level): From 187Re(p,d) (2009Wh01). | ||
1424.5 | (2-,3-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1431.0 | (4-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1434.2 | E(level): From 187Re(p,d) (2009Wh01). | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
1437.71 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1449.8 | (1-,2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1457.45 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1462.4 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1472.7 | E(level): From 187Re(p,d) (2009Wh01). | ||
1475.9 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1486.66 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1512.7 | E(level): From 187Re(p,d) (2009Wh01). | ||
1520.5 | E(level): From 187Re(p,d) (2009Wh01). | ||
1525.24 | (4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1529.4 | (2-,3-) | E(level): From 187Re(p,d) (2009Wh01). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1538.8 | (1-,2-,3-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1544.95 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1550.65 | (1-,2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1566.35 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1571.98 | (1-,2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1575.8 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1587.05 | (2-,3-) | XREF: C(1591.6). E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1601.7 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1607.10 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1613.8 | E(level): From 187Re(p,d) (2009Wh01). | ||
1628.18 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1633.8 | E(level): From 187Re(p,d) (2009Wh01). | ||
1637 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=thermal (1969La11). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1643.9 | (1-,2-,3-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
1646.87 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1659.12 | (2-,3-,4-) | XREF: C(1662.1). E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1667.8 | (2-,3-,4-) | XREF: B(1665). E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1672.3 | (1-,2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1684.2 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1694.7 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1707.6 | E(level): From 187Re(p,d) (2009Wh01). | ||
1711.1 | (2-,3-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1718.91 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1742.4 | E(level): From 187Re(p,d) (2009Wh01). | ||
1743.16 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1758.0 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1768.4 | E(level): From 187Re(p,d) (2009Wh01). | ||
1776.4 | E(level): From 187Re(p,d) (2009Wh01). | ||
1794.0 | (2-,3-,4-) | XREF: B(1791). E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1818.1 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=2-110 eV (1983Be27,1980BeYB). Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1827.54 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1838.7 | (1-,2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1846.41 | (2-,3-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=2-110 eV (1983Be27,1980BeYB). Based on analysis of primary Iγ to final level from each of 26 Jπ=2+ or 3+ neutron resonances populated in s-wave capture, and on average primary Iγ intensity from all resonances with a given Jπ. | |
1881.34 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1905.8 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1964.77 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
1985 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=thermal (1969La11). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2004 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=thermal (1969La11). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2055 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=thermal (1969La11). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
2063 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=thermal (1969La11). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2083 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=thermal (1969La11). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2106 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=thermal (1969La11). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2141.2 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=thermal (1969La11). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2203.4 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2219.19 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2244.81 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2261 | (2-,3-,4-) | E(level): From 185Re(n,γ) E=thermal (1969La11). Jπ(level): From (n,γ) E=thermal (1969La11). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2319.76 | (2-,3-,4-) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. | |
2359.0 | (2+,3+,4+) | E(level): From least-squares fit to (n,γ) E=thermal primary γ-ray data measured in 2016Ma35 together with secondary γ rays from 2016Ma35 and 1969La11, yielding normalized χ2=0.86. Jπ(level): From (n,γ) E=thermal (2016Ma35). Spin window deduced from primary γ rays deexciting the capture state (+185Re target g.s. Jπ=5/2+). This assumes the most likely E1 γ via the dominant 3+ component (98.8% 2016Ma35). The spin window extends to J=1,2,3,4 if taking into account the 2+ component. Lower-probability M1 primary γ rays also allow for π=+ states. |
E(level) | E(gamma) | Comments |
59.010 | 59.009 | E(γ): From 2020Kr05 - (n,γ) E=Thermal I(γ): From 186Re IT decay (2.0×105 y). |
99.361 | 40.350 | E(γ): From 2020Kr05 - (n,γ) E=Thermal I(γ): From 186Re IT decay (2.0×105 y). | 99.362 | E(γ): From 2020Kr05 - (n,γ) E=Thermal I(γ): From 186Re IT decay (2.0×105 y). |
148.2 | 48.84 | E(γ): Deduced according to energy-level difference from precision measurement of (8+) isomer in 2015Ma60.. From 2020Kr05 - (n,γ) E=Thermal I(γ): From 186Re IT decay (2.0×105 y). M(γ): From 186Re IT decay (1972Se06). |
322.378 | 263.33 | I(γ): Other value also in (n,γ): 3.7 15 in 2020Kr05. |
324.2 | 144.0 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 150.3 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
378.387 | 232.100 | I(γ): Resolved from doublet with 231.8γ. |
414.7 | 266.69 | E(γ): Other: 266.1373 6 (n’γ) E=Thermal. Energy and corresponding branching ratio (if given) from 187Re(n,2nγ) (2015Ma60). |
462.969 | 193.95 | I(γ): Other value also in (n,γ): 11.5 23 in 1969La11 (undivided Iγ); <5.7 in 2020Kr05. |
465.4 | 141.1 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
469.794 | 147.417 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
497.294 | 323.5 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
500.722 | 176.2941 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 401.3 | M(γ): [E1] if Jπ=4+ |
534.37 | 260.87 | I(γ): Other value also in (n,γ): 31 in 1969La11. |
556.0 | 231.8 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). I(γ): Resolved from doublet with 232.1γ. |
559.976 | 134.158 | I(γ): Other value also in (n,γ): 41 6 in 1969La11. |
588.705 | 266.3501 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
651.6 | 186.1 | E(γ): Other: 186.0535 5 (2020Kr05 - (n,γ) E=Thermal). Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 327.5 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
680.05 | 357.65 | I(γ): Other value also in (n,γ): 81 15 in 1969La11. | 469.39 | I(γ): Other value also in (n,γ) (undivided Iγ): 81 22 in 1969La11. | 580.5283 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
691.37 | 228.42 | I(γ): Other value also in (n,γ): 15.6 89 in 2020Kr05. |
E(level) | E(gamma) | Comments |
705.2 | 290.4 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 557.1 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
709.6 | 212.7 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 391.4 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
722.962 | 542.5661 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
736.127 | 147.417 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 266.3501 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
761.42 | 761.6 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
773.6 | 217.6 | E(γ): Other: 217.8928 5 (2020Kr05 - (n,γ) E=Thermal). Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
785.58 | 468.8837 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
791.225 | 468.8837 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 580.5283 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 644.9220 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 691.6333 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
795.9 | 381.2 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 647.6 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
796.45 | 218.69 | I(γ): Other value also in (n,γ): 8.6 17 in 1969La11. | 479.3 | E(γ): 479.3 3 for complex γ (1969La11); 479.68 6 (2016Ma35).. 1-keV uncertainty assumed (by evaluators) during fit. |
814.187 | 813.9455 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
819.00 | 545.1537 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 607.5 | I(γ): Other value also in (n,γ): 27 11 in 2020Kr05. | 645.3 | I(γ): Other value also in (n,γ): 16 6 in 2020Kr05. | 761.6 | E(γ): Multiply placed with undivided intensity I(γ): Other value also in (n,γ) (undivided Iγ) 83 26 in 1969La11.. Multiply placed with undivided intensity |
860.386 | 542.5661 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
869.2 | 217.5 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 403.8 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
E(level) | E(gamma) | Comments |
871.0 | 660.1877 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 771.7231 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
902.336 | 691.6333 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
912.378 | 176.2941 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 317.4579 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
913.58 | 644.9220 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 813.9455 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
923.629 | 545.1537 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
953.2 | 243 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 455.9 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
954.72 | 808.4161 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
982.27 | 660.1877 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 771.7231 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 808.4161 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1002.678 | 266.3501 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1003.526 | 317.4579 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1007.5 | 1007.5 | E(γ): Energy and corresponding branching ratio (if given) from 187Re(n,2nγ) (2015Ma60). |
1018.0 | 312.7 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 603.3 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
1101.3 | 1101.3 | E(γ): γ decay only observed in 187Re(n,2nγ) (2015Ma60). Energy and corresponding branching ratio (if given) from 187Re(n,2nγ) (2015Ma60). |
1115.2 | 246.0 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 463.7 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
1119.6 | 323.4 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 414.3 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 705.2 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
E(level) | E(gamma) | Comments |
1138.1 | 433.0 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 723.3 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
1290.6 | 494.7 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
1352.6 | 334.5 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 647.5 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
1386.4 | 271.2 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). | 517.1 | E(γ): Energy and corresponding branching ratio (if given) from 186W(d,2nγ) (2017Ma39). |
Levels: Band assignments are those suggested in 1973Gl06, 2009Wh01, and 2017Ma39. Configurations are also discussed in 1969La11 and 1972Se06.
Levels: μ for excited levels: from 2020StZV, based on 1980Za10, corrected for diamagnetic shielding and Knight shift.