ADOPTED LEVELS, GAMMAS for 236U
Author: Shaofei Zhu | Citation: Nucl. Data Sheets 182, 2 (2022). | Cutoff date: 1-Apr-2022
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-9.3×102 keV 5 | S(n)= 6545.5 keV 3 | S(p)= 7133 keV 14 | Q(α)= 4573.0 keV 9 | ||
Reference: 2021WA16 |
E(level): Deduced by evaluator from a least-squares fit to adopted γ-ray energies.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - Kπ=0+ GS Rotational band | |||||||
0.0 | 0+ | 2.342×107 y 4 % α = 100 % SF = 9.4×10-8 4 | |||||
45.2431 20 | 2+ | 235 ps 6 | 45.243 2 | 100 | E2 | 0.0 | 0+ |
149.480 5 | 4+ | 130 ps 9 | 104.237 4 | 100 | E2 | 45.2431 | 2+ |
309.788 6 | 6+ | 58 ps 3 | 160.308 3 | 100 | E2 | 149.480 | 4+ |
522.26 4 | 8+ | 23.9 ps 19 | 212.47 4 | 100 | E2 | 309.788 | 6+ |
782.4 5 | 10+ | 11.6 ps 11 | 260.1 5 | 100 | E2 | 522.26 | 8+ |
1085.4 7 | 12+ | 5.5 ps +18-33 | 303.0 5 | 100 | E2 | 782.4 | 10+ |
1426.4 9 | 14+ | 2.8 ps 3 | 341.0 5 | 100 | E2 | 1085.4 | 12+ |
1801.0 10 | 16+ | 2.1 ps 2 | 374.6 5 | 100 | E2 | 1426.4 | 14+ |
2204.0 12 | 18+ | 1.17 ps 12 | 403.0 5 | 100 | E2 | 1801.0 | 16+ |
2631.8 13 | 20+ | 0.84 ps 12 | 427.8 5 | 100 | E2 | 2204.0 | 18+ |
3081.0 14 | 22+ | 0.65 ps 15 | 449.2 5 | 100 | E2 | 2631.8 | 20+ |
3550.0 17 | 24+ | 0.41 ps 8 | 469 1 | 100 | E2 | 3081.0 | 22+ |
4039.0 20 | 26+ | 0.33 ps 9 | 489 1 | 100 | E2 | 3550.0 | 24+ |
4549.0 22 | 28+ | 0.17 ps 7 | 510 1 | 100 | E2 | 4039.0 | 26+ |
5077 4 | (30+) | ≈528 | 100 | (E2) | 4549.0 | 28+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - Kπ=0- Octupole vibrational band | |||||||
687.56 4 | 1- | 3.78 ns 9 | |||||
744.18 7 | 3- | 56.6 8 594.5 3 | ≈5 100 | [E2] [E1] | 687.56 149.480 | 1- 4+ | |
848.3 10 | 5- | ≈103.4 | 100 | (E2) | 744.18 | 3- | |
999.8 12 | 7- | 151.5 5 | 100 | E2 | 848.3 | 5- | |
1198.6 12 | 9- | 198.8 3 | 100 | E2 | 999.8 | 7- | |
1443.6 13 | 11- | 245.0 5 | 100 | E2 | 1198.6 | 9- | |
1732.6 17 | 13- | 289 1 | 100 | E2 | 1443.6 | 11- | |
2060.6 19 | 15- | 328 1 | 100 | E2 | 1732.6 | 13- | |
2426.6 22 | 17- | 366 1 | 100 | E2 | 2060.6 | 15- | |
2823 4 | (19-) | ≈396 | 100 | (E2) | 2426.6 | 17- | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - Kπ=3- Configuration=((n,7/2(743))-(n,1/2(631))) | |||||||
1191.6 10 | (3-) | ||||||
1232.2 10 | (4-) | ||||||
1282.2 10 | (5-) | ||||||
1342.8 10 | (6-) | ||||||
1413.3 19 | (7-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - Kπ=6- Configuration=((n,7/2(743))+(n,5/2(622))) | |||||||
1471.7 10 | (6-) | ||||||
1541.8 13 | (7-) | ||||||
1621.8 12 | (8-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 5 - Kπ=0+ | |||||||
919.18 12 | 0+ | ||||||
960.05 20 | (2+) | ≈810.9 914.8 2 ≈959.9 | ≈68 100 ≈80 | (E0+M1) | 149.480 45.2431 0.0 | 4+ 2+ 0+ | |
1050.86 15 | (4+) | 901.25 17 1006.0 3 | 100 | (E0+E2) | 149.480 45.2431 | 4+ 2+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 6 - Kπ=(2+) | |||||||
957.90 15 | 2+ | ||||||
1001.6 3 | (3+) | ≈258.4 ≈852.2 956.3 3 | ≈13 100 12 | 744.18 149.480 45.2431 | 3- 4+ 2+ | ||
1058.8 3 | (4+) | 909.3 3 1014.1 | 100 9 ≈69 | M1 | 149.480 45.2431 | 4+ 2+ | |
1127.38 20 | (5+) | 977.9 2 | 100 | 149.480 | 4+ | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 7 - Kπ=1- Configuration=((n,7/2(743))-(n,5/2(622))) | |||||||
966.58 9 | (1-) | ||||||
987.66 8 | 2- | 243.6 2 300.0 1 942.4 2 | 26 3 17 3 100 7 | M1+E2 [M1+E2] (E1) | 744.18 687.56 45.2431 | 3- 1- 2+ | |
1035.6 22 | 3- | ≈886.2 ≈990.2 | 100 ≈88 | [E1] [E1] | 149.480 45.2431 | 4+ 2+ | |
1070.0 10 | (4-) | 920.5 | 100 | 149.480 | 4+ | ||
≈1164 | (5-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 8 - Kπ=4- Configuration=((n,7/2(743))+(n,1/2(631))) | |||||||
1052.9 4 | 4- | 101 ns 6 | |||||
1104.4 14 | (5-) | ||||||
1164 3 | (6-) | ||||||
≈1232 | (7-) | ||||||
1320 4 | (8-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 9 - Kπ=2- | |||||||
1110.66 8 | (2-) | ||||||
1149.4 10 | (3-) | 405.2 | 100 | 744.18 | 3- |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
45.2431 | 2+ | 235 ps 6 | 45.243 2 | E2 | 589 | B(E2)(W.u.)=248 8, α=589 8, α(L)=429 6, α(M)=118.6 17, α(N)=32.1 5, α(O)=7.36 10, α(P)=1.191 17, α(Q)=0.00285 4 | |
149.480 | 4+ | 130 ps 9 | 104.237 4 | E2 | 10.99 | B(E2)(W.u.)=340 24, α=10.99 15, α(L)=8.00 11, α(M)=2.220 31, α(N)=0.603 8, α(O)=0.1385 19, α(P)=0.02268 32, α(Q)=9.41E-5 13 | |
309.788 | 6+ | 58 ps 3 | 160.308 3 | E2 | 1.761 | B(E2)(W.u.)=385 21, α=1.761 25, α(K)=0.2079 29, α(L)=1.132 16, α(M)=0.313 4, α(N)=0.0850 12, α(O)=0.01958 27, α(P)=0.00325 5, α(Q)=2.327E-5 33 | |
522.26 | 8+ | 23.9 ps 19 | 212.47 4 | E2 | 0.599 | B(E2)(W.u.)=3.9×102 4, α=0.599 8, α(K)=0.1400 20, α(L)=0.335 5, α(M)=0.0920 13, α(N)=0.02498 35, α(O)=0.00577 8, α(P)=0.000968 14, α(Q)=1.068E-5 15 | |
687.56 | 1- | 3.78 ns 9 | 538.09 7 | E3 | 0.20 | B(E3)(W.u.)=56 5, α=0.20 8, α(K)=0.0623 9, α(L)=0.0587 8, α(M)=0.01603 22, α(N)=0.00437 6, α(O)=0.001025 14, α(P)=0.0001801 25, α(Q)=4.97E-6 7 | |
1- | 3.78 ns 9 | 642.23 7 | E1(+M2+E3) | 0.15 | B(E1)(W.u.)=5.81E-8 22, α=0.15 2, α(K)=0.0091 23, α(L)=0.0017 6, α(M)=4.2E-4 14, α(N)=1.1E-4 4, α(O)=2.7E-5 9, α(P)=5.2E-6 17, α(Q)=3.9E-7 13 | ||
1- | 3.78 ns 9 | 687.59 6 | E1 | 0.31 | B(E1)(W.u.)=2.59E-8 8, α=0.31 2, α(K)=0.00596 8, α(L)=0.001038 15, α(M)=0.0002473 35, α(N)=6.63E-5 9, α(O)=1.599E-5 22, α(P)=3.03E-6 4, α(Q)=2.237E-7 31 | ||
744.18 | 3- | 56.6 8 | [E2] | 199 | α=199 14, α(L)=145 11, α(M)=40.1 29, α(N)=10.9 8, α(O)=2.50 18, α(P)=0.405 29, α(Q)=0.00107 7 | ||
3- | 594.5 3 | [E1] | 0.00964 | α=0.00964 14, α(K)=0.00781 11, α(L)=0.001381 19, α(M)=0.000330 5, α(N)=8.83×10-5 12, α(O)=2.128E-5 30, α(P)=4.01E-6 6, α(Q)=2.91E-7 4 | |||
782.4 | 10+ | 11.6 ps 11 | 260.1 5 | E2 | 0.297 | B(E2)(W.u.)=3.6×102 4, α=0.297 5, α(K)=0.0979 14, α(L)=0.1456 23, α(M)=0.0397 6, α(N)=0.01078 17, α(O)=0.00250 4, α(P)=0.000423 7, α(Q)=6.40E-6 9 | |
848.3 | 5- | ≈103.4 | (E2) | 11.41 | α=11.41 16, α(L)≈8.31, α(M)≈2.305, α(N)≈0.626, α(O)≈0.1438, α(P)≈0.02355, α(Q)≈9.69×10-5 | ||
919.18 | 0+ | 873.98 12 | [E2] | 0.01439 | α=0.01439 20, α(K)=0.01060 15, α(L)=0.00283 4, α(M)=0.000711 10, α(N)=0.0001917 27, α(O)=4.58×10-5 6, α(P)=8.47E-6 12, α(Q)=4.85E-7 7 | ||
957.90 | 2+ | 912.4 3 | [M1+E2] | 0.032 | α=0.032 18, α(K)=0.025 15, α(L)=0.0050 25, α(M)=0.0012 6, α(N)=3.3×10-4 16, α(O)=8.E-5 4, α(P)=1.5E-5 8, α(Q)=1.1E-6 7 | ||
2+ | 958.0 2 | [E2] | 0.01204 | α=0.01204 17, α(K)=0.00902 13, α(L)=0.002264 32, α(M)=0.000565 8, α(N)=0.0001522 21, α(O)=3.64×10-5 5, α(P)=6.77E-6 9, α(Q)=4.08E-7 6 | |||
966.58 | (1-) | 921.2 2 | (E1) | 0.00432 | α=0.00432 6, α(K)=0.00353 5, α(L)=0.000599 8, α(M)=0.0001423 20, α(N)=3.81×10-5 5, α(O)=9.22E-6 13, α(P)=1.757E-6 25, α(Q)=1.345E-7 19 | ||
(1-) | 966.8 2 | (E1) | 0.00397 | α=0.00397 6, α(K)=0.00325 5, α(L)=0.000549 8, α(M)=0.0001302 18, α(N)=3.49×10-5 5, α(O)=8.44E-6 12, α(P)=1.610E-6 23, α(Q)=1.239E-7 17 | |||
987.66 | 2- | 243.6 2 | M1+E2 | 1.5 4 | 0.81 | α=0.81 21, α(K)=0.51 19, α(L)=0.216 13, α(M)=0.0564 23, α(N)=0.0153 6, α(O)=0.00360 17, α(P)=0.00064 4, α(Q)=2.6×10-5 9 | |
2- | 300.0 1 | [M1+E2] | 0.6 | α=0.6 4, α(K)=0.4 4, α(L)=0.12 4, α(M)=0.030 7, α(N)=0.0081 20, α(O)=0.0019 5, α(P)=3.6×10-4 11, α(Q)=2.1E-5 16 | |||
2- | 942.4 2 | (E1) | 0.00415 | α=0.00415 6, α(K)=0.00339 5, α(L)=0.000575 8, α(M)=0.0001365 19, α(N)=3.66×10-5 5, α(O)=8.85E-6 12, α(P)=1.686E-6 24, α(Q)=1.294E-7 18 | |||
999.8 | 7- | 151.5 5 | E2 | 2.21 | α=2.21 4, α(K)=0.2183 31, α(L)=1.455 30, α(M)=0.403 8, α(N)=0.1093 22, α(O)=0.0252 5, α(P)=0.00417 8, α(Q)=2.75×10-5 5 | ||
1035.6 | 3- | ≈886.2 | [E1] | 0.00463 | α=0.00463 6, α(K)≈0.00378, α(L)≈0.000643, α(M)≈0.0001528, α(N)≈4.09×10-5, α(O)≈9.90E-6, α(P)≈1.885E-6, α(Q)≈1.437E-7 | ||
3- | ≈990.2 | [E1] | 0.00381 | α=0.00381 5, α(K)≈0.00311, α(L)≈0.000526, α(M)≈0.0001247, α(N)≈3.34×10-5, α(O)≈8.09E-6, α(P)≈1.543E-6, α(Q)≈1.190E-7 | |||
1050.86 | (4+) | 1006.0 3 | 0.01097 | α=0.01097 15 | |||
1052.9 | 4- | 101 ns 6 | ≈65 | (E2) | 102.4 | α=102.4 14, α(L)≈74.6, α(M)≈20.66, α(N)≈5.61, α(O)≈1.286, α(P)≈0.2088, α(Q)≈0.000597 | |
4- | 101 ns 6 | 204.6 10 | (E2) | 0.687 | α=0.687 16, α(K)=0.1490 24, α(L)=0.393 10, α(M)=0.1080 27, α(N)=0.0293 7, α(O)=0.00678 17, α(P)=0.001134 29, α(Q)=1.179×10-5 23 | ||
4- | 101 ns 6 | 307.9 10 | M1+E2 | 1.3 5 | 0.46 | α=0.46 18, α(K)=0.32 16, α(L)=0.100 16, α(M)=0.0256 34, α(N)=0.0069 9, α(O)=0.00165 24, α(P)=0.00030 5, α(Q)=1.6×10-5 7 | |
4- | 101 ns 6 | 903.6 4 | (E1) | 0.00447 | α=0.00447 6, α(K)=0.00365 5, α(L)=0.000621 9, α(M)=0.0001474 21, α(N)=3.95×10-5 6, α(O)=9.55E-6 13, α(P)=1.819E-6 26, α(Q)=1.390E-7 19 | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
1058.8 | (4+) | 909.3 3 | M1 | 0.0505 | α=0.0505 7, α(K)=0.0404 6, α(L)=0.00760 11, α(M)=0.001830 26, α(N)=0.000493 7, α(O)=0.0001198 17, α(P)=2.313×10-5 32, α(Q)=1.852E-6 26 | ||
1085.4 | 12+ | 5.5 ps +18-33 | 303.0 5 | E2 | 0.1826 | B(E2)(W.u.)=4.1×102 7, α=0.1826 27, α(K)=0.0736 11, α(L)=0.0798 12, α(M)=0.02163 33, α(N)=0.00587 9, α(O)=0.001364 21, α(P)=0.000233 4, α(Q)=4.44E-6 6 | |
1198.6 | 9- | 198.8 3 | E2 | 0.764 | α=0.764 12, α(K)=0.1561 22, α(L)=0.444 7, α(M)=0.1222 19, α(N)=0.0332 5, α(O)=0.00766 12, α(P)=0.001281 20, α(Q)=1.273×10-5 19 | ||
1426.4 | 14+ | 2.8 ps 3 | 341.0 5 | E2 | 0.1285 | B(E2)(W.u.)=4.5×102 5, α=0.1285 19, α(K)=0.0589 8, α(L)=0.0511 8, α(M)=0.01375 21, α(N)=0.00373 6, α(O)=0.000869 13, α(P)=0.0001497 22, α(Q)=3.38E-6 5 | |
1443.6 | 11- | 245.0 5 | E2 | 0.363 | α=0.363 6, α(K)=0.1091 16, α(L)=0.1855 30, α(M)=0.0507 8, α(N)=0.01377 23, α(O)=0.00319 5, α(P)=0.000538 9, α(Q)=7.42×10-6 11 | ||
1732.6 | 13- | 289 1 | E2 | 0.211 | α=0.211 4, α(K)=0.0805 12, α(L)=0.0959 19, α(M)=0.0260 5, α(N)=0.00706 14, α(O)=0.001641 32, α(P)=0.000280 5, α(Q)=4.97×10-6 8 | ||
1791.3 | 1(+) | 1746.1 10 | (M1) | 0.00926 | α=0.00926 13, α(K)=0.00717 10, α(L)=0.001332 19, α(M)=0.000320 5, α(N)=8.61×10-5 12, α(O)=2.096E-5 30, α(P)=4.05E-6 6, α(Q)=3.27E-7 5 | ||
1(+) | 1791.3 10 | (M1) | 0.00870 | α=0.00870 12, α(K)=0.00669 9, α(L)=0.001243 18, α(M)=0.000299 4, α(N)=8.04×10-5 11, α(O)=1.957E-5 28, α(P)=3.78E-6 5, α(Q)=3.05E-7 4 | |||
1801.0 | 16+ | 2.1 ps 2 | 374.6 5 | E2 | 0.0987 | B(E2)(W.u.)=3.8×102 4, α=0.0987 14, α(K)=0.0493 7, α(L)=0.0363 5, α(M)=0.00971 14, α(N)=0.00263 4, α(O)=0.000614 9, α(P)=0.0001066 16, α(Q)=2.74E-6 4 | |
2054.2 | 1(+) | 2009.0 10 | (M1) | 0.00668 | α=0.00668 9, α(K)=0.00492 7, α(L)=0.000913 13, α(M)=0.0002193 31, α(N)=5.90×10-5 8, α(O)=1.436E-5 20, α(P)=2.77E-6 4, α(Q)=2.243E-7 32 | ||
1(+) | 2054.2 10 | (M1) | 0.00637 | α=0.00637 9, α(K)=0.00463 7, α(L)=0.000859 12, α(M)=0.0002065 29, α(N)=5.56×10-5 8, α(O)=1.352E-5 19, α(P)=2.61E-6 4, α(Q)=2.113E-7 30 | |||
2060.6 | 15- | 328 1 | E2 | 0.1439 | α=0.1439 24, α(K)=0.0634 10, α(L)=0.0591 11, α(M)=0.01593 29, α(N)=0.00432 8, α(O)=0.001006 18, α(P)=0.0001729 31, α(Q)=3.70×10-6 6 | ||
2086.54 | 1(-) | 2041.3 1 | (E1) | 1.66×10-3 | α=1.66×10-3 2, α(K)=0.000929 13, α(L)=0.0001512 21, α(M)=3.57E-5 5, α(N)=9.57E-6 13, α(O)=2.325E-6 33, α(P)=4.48E-7 6, α(Q)=3.64E-8 5 | ||
1(-) | 2086.5 2 | (E1) | 1.65×10-3 | α=1.65×10-3 2, α(K)=0.000896 13, α(L)=0.0001458 20, α(M)=3.44E-5 5, α(N)=9.22E-6 13, α(O)=2.242E-6 31, α(P)=4.32E-7 6, α(Q)=3.52E-8 5 | |||
2095.7 | 1(+) | 2050.5 10 | (M1) | 0.00639 | α=0.00639 9, α(K)=0.00466 7, α(L)=0.000864 12, α(M)=0.0002075 29, α(N)=5.58×10-5 8, α(O)=1.359E-5 19, α(P)=2.63E-6 4, α(Q)=2.123E-7 30 | ||
1(+) | 2095.7 10 | (M1) | 0.00610 | α=0.00610 9, α(K)=0.00439 6, α(L)=0.000814 11, α(M)=0.0001956 27, α(N)=5.26×10-5 7, α(O)=1.281E-5 18, α(P)=2.475E-6 35, α(Q)=2.002E-7 28 | |||
2188.8 | 1(+) | 2143.6 10 | (M1) | 0.00582 | α=0.00582 8, α(K)=0.00413 6, α(L)=0.000766 11, α(M)=0.0001840 26, α(N)=4.95×10-5 7, α(O)=1.205E-5 17, α(P)=2.328E-6 33, α(Q)=1.884E-7 26 | ||
1(+) | 2188.8 10 | (M1) | 0.00558 | α=0.00558 8, α(K)=0.00391 5, α(L)=0.000724 10, α(M)=0.0001738 24, α(N)=4.68×10-5 7, α(O)=1.139E-5 16, α(P)=2.200E-6 31, α(Q)=1.781E-7 25 | |||
2204.0 | 18+ | 1.17 ps 12 | 403.0 5 | E2 | 0.0811 | B(E2)(W.u.)=4.9×102 5, α=0.0811 12, α(K)=0.0430 6, α(L)=0.0280 4, α(M)=0.00746 11, α(N)=0.002021 30, α(O)=0.000473 7, α(P)=8.25E-5 12, α(Q)=2.330E-6 33 | |
2284.7 | 1(+) | 2239.5 10 | (M1) | 0.00533 | α=0.00533 7, α(K)=0.00367 5, α(L)=0.000680 10, α(M)=0.0001634 23, α(N)=4.40×10-5 6, α(O)=1.070E-5 15, α(P)=2.068E-6 29, α(Q)=1.674E-7 24 | ||
1(+) | 2284.7 10 | (M1) | 0.00512 | α=0.00512 7, α(K)=0.00348 5, α(L)=0.000644 9, α(M)=0.0001547 22, α(N)=4.17×10-5 6, α(O)=1.014E-5 14, α(P)=1.959E-6 28, α(Q)=1.586E-7 22 | |||
2426.6 | 17- | 366 1 | E2 | 0.1052 | α=0.1052 17, α(K)=0.0515 8, α(L)=0.0394 7, α(M)=0.01057 18, α(N)=0.00286 5, α(O)=0.000669 12, α(P)=0.0001158 20, α(Q)=2.88×10-6 4 | ||
2435.6 | 1(+) | 2390.4 10 | (M1) | 0.00471 | α=0.00471 7, α(K)=0.00308 4, α(L)=0.000570 8, α(M)=0.0001368 19, α(N)=3.68×10-5 5, α(O)=8.96E-6 13, α(P)=1.732E-6 24, α(Q)=1.404E-7 20 | ||
1(+) | 2435.6 10 | (M1) | 0.00456 | α=0.00456 6, α(K)=0.00292 4, α(L)=0.000541 8, α(M)=0.0001300 18, α(N)=3.50×10-5 5, α(O)=8.52E-6 12, α(P)=1.646E-6 23, α(Q)=1.334E-7 19 | |||
2440.2 | 1(+) | 2395.0 10 | (M1) | 0.00470 | α=0.00470 7, α(K)=0.00306 4, α(L)=0.000567 8, α(M)=0.0001361 19, α(N)=3.66×10-5 5, α(O)=8.92E-6 13, α(P)=1.723E-6 24, α(Q)=1.396E-7 20 | ||
1(+) | 2440.2 10 | (M1) | 0.00455 | α=0.00455 6, α(K)=0.00291 4, α(L)=0.000539 8, α(M)=0.0001293 18, α(N)=3.48×10-5 5, α(O)=8.47E-6 12, α(P)=1.637E-6 23, α(Q)=1.328E-7 19 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
2457.3 | 1(+) | 2412.1 10 | (M1) | 0.00464 | α=0.00464 7, α(K)=0.00300 4, α(L)=0.000556 8, α(M)=0.0001335 19, α(N)=3.59×10-5 5, α(O)=8.75E-6 12, α(P)=1.690E-6 24, α(Q)=1.370E-7 19 | ||
1(+) | 2457.3 10 | (M1) | 0.00449 | α=0.00449 6, α(K)=0.00285 4, α(L)=0.000528 7, α(M)=0.0001269 18, α(N)=3.42×10-5 5, α(O)=8.31E-6 12, α(P)=1.607E-6 23, α(Q)=1.303E-7 18 | |||
2494.5 | 1(+) | 2449.3 10 | (M1) | 0.00452 | α=0.00452 6, α(K)=0.00288 4, α(L)=0.000533 7, α(M)=0.0001280 18, α(N)=3.45×10-5 5, α(O)=8.39E-6 12, α(P)=1.621E-6 23, α(Q)=1.314E-7 18 | ||
1(+) | 2494.5 10 | (M1) | 0.00438 | α=0.00438 6, α(K)=0.00274 4, α(L)=0.000507 7, α(M)=0.0001218 17, α(N)=3.28×10-5 5, α(O)=7.98E-6 11, α(P)=1.542E-6 22, α(Q)=1.251E-7 18 | |||
2498.5 | 1(+) | 2453.3 10 | (M1) | 0.00451 | α=0.00451 6, α(K)=0.00287 4, α(L)=0.000531 7, α(M)=0.0001275 18, α(N)=3.43×10-5 5, α(O)=8.35E-6 12, α(P)=1.614E-6 23, α(Q)=1.308E-7 18 | ||
1(+) | 2498.5 10 | (M1) | 0.00437 | α=0.00437 6, α(K)=0.00273 4, α(L)=0.000505 7, α(M)=0.0001213 17, α(N)=3.26×10-5 5, α(O)=7.95E-6 11, α(P)=1.535E-6 22, α(Q)=1.245E-7 17 | |||
2631.8 | 20+ | 0.84 ps 12 | 427.8 5 | E2 | 0.0694 | B(E2)(W.u.)=5.1×102 8, α=0.0694 10, α(K)=0.0385 5, α(L)=0.02281 33, α(M)=0.00605 9, α(N)=0.001638 24, α(O)=0.000384 6, α(P)=6.73E-5 10, α(Q)=2.047E-6 29 | |
2699.0 | 1(+) | 2653.8 10 | (M1) | 0.00398 | α=0.00398 6, α(K)=0.002315 32, α(L)=0.000428 6, α(M)=0.0001028 14, α(N)=2.77×10-5 4, α(O)=6.74E-6 9, α(P)=1.302E-6 18, α(Q)=1.057E-7 15 | ||
1(+) | 2699.0 10 | (M1) | 0.00388 | α=0.00388 5, α(K)=0.002210 31, α(L)=0.000409 6, α(M)=9.82×10-5 14, α(N)=2.64E-5 4, α(O)=6.43E-6 9, α(P)=1.243E-6 17, α(Q)=1.009E-7 14 | |||
2712.1 | 1(-) | 2666.9 10 | (E1) | 1.67×10-3 | α=1.67×10-3 2, α(K)=0.000603 8, α(L)=9.74E-5 14, α(M)=2.296E-5 32, α(N)=6.15E-6 9, α(O)=1.497E-6 21, α(P)=2.89E-7 4, α(Q)=2.378E-8 33 | ||
1(-) | 2712.1 10 | (E1) | 1.68×10-3 | α=1.68×10-3 2, α(K)=0.000587 8, α(L)=9.47E-5 13, α(M)=2.234E-5 31, α(N)=5.99E-6 8, α(O)=1.456E-6 20, α(P)=2.81E-7 4, α(Q)=2.315E-8 32 | |||
2750 | (0+) | 67 ns 3 % IT = 88 3 % SF = 12 3 | 560 10 | (E1) | 0.0108 | B(E1)(W.u.)=5.6E-10 4, α=0.0108 4, α(K)=0.00875 33, α(L)=0.00156 6, α(M)=0.000372 15, α(N)=0.000100 4, α(O)=2.40E-5 10, α(P)=4.52E-6 18, α(Q)=3.24E-7 12 | |
(0+) | 67 ns 3 % IT = 88 3 % SF = 12 3 | 1170 10 | (E1) | 0.00286 | B(E1)(W.u.)=1.02E-10 5, α=0.00286 6, α(K)=0.00234 5, α(L)=0.000390 8, α(M)=9.25E-5 19, α(N)=2.48E-5 5, α(O)=6.00E-6 12, α(P)=1.149E-6 24, α(Q)=9.00E-8 18 | ||
(0+) | 67 ns 3 % IT = 88 3 % SF = 12 3 | 1783 10 | (E1) | 1.76×10-3 | B(E1)(W.u.)=1.45E-10 6, α=1.76E-3 3, α(K)=0.001159 19, α(L)=0.0001895 32, α(M)=4.48E-5 8, α(N)=1.200E-5 20, α(O)=2.91E-6 5, α(P)=5.60E-7 9, α(Q)=4.53E-8 8 | ||
(0+) | 67 ns 3 % IT = 88 3 % SF = 12 3 | 2062 10 | (E1) | 1.66×10-3 | B(E1)(W.u.)=2.43E-11 10, α=1.66E-3 2, α(K)=0.000914 15, α(L)=0.0001487 24, α(M)=3.51E-5 6, α(N)=9.41E-6 15, α(O)=2.29E-6 4, α(P)=4.40E-7 7, α(Q)=3.58E-8 6 | ||
2756.2 | 1(+) | 2711.0 10 | (M1) | 0.00386 | α=0.00386 5, α(K)=0.002184 31, α(L)=0.000404 6, α(M)=9.70×10-5 14, α(N)=2.61E-5 4, α(O)=6.36E-6 9, α(P)=1.228E-6 17, α(Q)=9.97E-8 14 | ||
1(+) | 2756.2 10 | (M1) | 0.00377 | α=0.00377 5, α(K)=0.002087 29, α(L)=0.000386 5, α(M)=9.27×10-5 13, α(N)=2.496E-5 35, α(O)=6.08E-6 9, α(P)=1.174E-6 16, α(Q)=9.53E-8 13 | |||
2770 | (2+) | 20 Calc. | (E2) | 1.96×104 | α=1.96×104, α(L)=1.125E4 16, α(M)=6.23E3 9, α(N)=1686 24, α(O)=385 6, α(P)=61.9 9, α(Q)=0.1021 15, α(N+)=2.13E3 3 | ||
2817 | (4+) | 47.0 | (E2) | 489 | α=489 7, α(L)=357 5, α(M)=98.6 14, α(N)=26.7 4, α(O)=6.12 9, α(P)=0.990 14, α(Q)=0.002409 34 | ||
2823 | (19-) | ≈396 | (E2) | 0.0849 | α=0.0849 12, α(K)≈0.0444, α(L)≈0.0298, α(M)≈0.00794, α(N)≈0.002152, α(O)≈0.000503, α(P)≈8.77×10-5, α(Q)≈2.422E-6 | ||
2823.3 | 1(+) | 2778.1 10 | (M1) | 0.00373 | α=0.00373 5, α(K)=0.002042 29, α(L)=0.000378 5, α(M)=9.07×10-5 13, α(N)=2.442E-5 34, α(O)=5.94E-6 8, α(P)=1.149E-6 16, α(Q)=9.33E-8 13 | ||
1(+) | 2823.3 10 | (M1) | 0.00365 | α=0.00365 5, α(K)=0.001954 27, α(L)=0.000361 5, α(M)=8.68×10-5 12, α(N)=2.336E-5 33, α(O)=5.69E-6 8, α(P)=1.099E-6 15, α(Q)=8.93E-8 13 | |||
2838.3 | 1(+) | 2793.1 10 | (M1) | 0.00370 | α=0.00370 5, α(K)=0.002013 28, α(L)=0.000372 5, α(M)=8.94×10-5 13, α(N)=2.406E-5 34, α(O)=5.86E-6 8, α(P)=1.132E-6 16, α(Q)=9.19E-8 13 | ||
1(+) | 2838.3 10 | (M1) | 0.00363 | α=0.00363 5, α(K)=0.001926 27, α(L)=0.000356 5, α(M)=8.55×10-5 12, α(N)=2.303E-5 32, α(O)=5.61E-6 8, α(P)=1.083E-6 15, α(Q)=8.80E-8 12 | |||
2877.8 | 1(-) | 2832.6 10 | (E1) | 1.70×10-3 | α=1.70×10-3 2, α(K)=0.000547 8, α(L)=8.83E-5 12, α(M)=2.081E-5 29, α(N)=5.58E-6 8, α(O)=1.357E-6 19, α(P)=2.62E-7 4, α(Q)=2.161E-8 30 | ||
1(-) | 2877.8 10 | (E1) | 1.71×10-3 | α=1.71×10-3 2, α(K)=0.000534 7, α(L)=8.60E-5 12, α(M)=2.028E-5 28, α(N)=5.44E-6 8, α(O)=1.322E-6 19, α(P)=2.55E-7 4, α(Q)=2.108E-8 30 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
2891 | (6+) | 73.9 | (E2) | 55.5 | α=55.5 8, α(L)=40.4 6, α(M)=11.20 16, α(N)=3.04 4, α(O)=0.697 10, α(P)=0.1135 16, α(Q)=0.000352 5 | ||
2969.0 | 1(+) | 2923.8 10 | (M1) | 0.00350 | α=0.00350 5, α(K)=0.001775 25, α(L)=0.000328 5, α(M)=7.88×10-5 11, α(N)=2.122E-5 30, α(O)=5.17E-6 7, α(P)=9.98E-7 14, α(Q)=8.11E-8 11 | ||
1(+) | 2969.0 10 | (M1) | 0.00344 | α=0.00344 5, α(K)=0.001702 24, α(L)=0.000315 4, α(M)=7.56×10-5 11, α(N)=2.035E-5 29, α(O)=4.95E-6 7, α(P)=9.57E-7 13, α(Q)=7.78E-8 11 | |||
2991 | (8+) | 100.8 | (E2) | 12.84 | α=12.84 18, α(L)=9.35 13, α(M)=2.59 4, α(N)=0.705 10, α(O)=0.1619 23, α(P)=0.0265 4, α(Q)=0.0001062 15 | ||
3081.0 | 22+ | 0.65 ps 15 | 449.2 5 | E2 | 0.0614 | B(E2)(W.u.)=5.2×102 12, α=0.0614 9, α(K)=0.0351 5, α(L)=0.01935 28, α(M)=0.00511 7, α(N)=0.001384 20, α(O)=0.000325 5, α(P)=5.72E-5 8, α(Q)=1.844E-6 26 | |
3143.8 | 1(+) | 3098.6 10 | (M1) | 0.00330 | α=0.00330 5, α(K)=0.001514 21, α(L)=0.000280 4, α(M)=6.72×10-5 9, α(N)=1.809E-5 25, α(O)=4.40E-6 6, α(P)=8.51E-7 12, α(Q)=6.92E-8 10 | ||
1(+) | 3143.8 10 | (M1) | 0.00326 | α=0.00326 5, α(K)=0.001454 20, α(L)=0.000269 4, α(M)=6.45×10-5 9, α(N)=1.738E-5 24, α(O)=4.23E-6 6, α(P)=8.18E-7 11, α(Q)=6.65E-8 9 | |||
3550.0 | 24+ | 0.41 ps 8 | 469 1 | E2 | 0.0552 | B(E2)(W.u.)=6.7×102 13, α=0.0552 8, α(K)=0.0324 5, α(L)=0.01678 26, α(M)=0.00442 7, α(N)=0.001196 19, α(O)=0.000281 4, α(P)=4.96E-5 8, α(Q)=1.682E-6 25 | |
4039.0 | 26+ | 0.33 ps 9 | 489 1 | E2 | 0.0498 | B(E2)(W.u.)=6.7×102 19, α=0.0498 7, α(K)=0.0300 4, α(L)=0.01465 23, α(M)=0.00385 6, α(N)=0.001041 16, α(O)=0.000245 4, α(P)=4.34E-5 7, α(Q)=1.541E-6 23 | |
4549.0 | 28+ | 0.17 ps 7 | 510 1 | E2 | 0.0451 | B(E2)(W.u.)=1.1×103 5, α=0.0451 7, α(K)=0.0278 4, α(L)=0.01281 20, α(M)=0.00335 5, α(N)=0.000907 14, α(O)=0.0002137 33, α(P)=3.80E-5 6, α(Q)=1.411E-6 21 | |
5077 | (30+) | ≈528 | (E2) | 0.0416 | α=0.0416 6, α(K)≈0.0261, α(L)≈0.01149, α(M)≈0.00300, α(N)≈0.000812, α(O)≈0.0001913, α(P)≈3.41×10-5, α(Q)≈1.313E-6 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 0+ | 2.342×107 y 4 % α = 100 % SF = 9.4×10-8 4 | Q0=13.8 b2 2 from Isotope shifts (1978Ge10). E(level): Q0=13.8 b2 2 from Isotope shifts (1978Ge10). Kπ=0+ GS Rotational band. From 236Pa β- decay. |
45.2431 | 2+ | 235 ps 6 | B(E2)=11.60 15 Measured isotopic shift, gyromagnetic factors. Δ<r2>/<r2>=-21×10-6 21 (1974Mo12), <6×10-6 (1974Me18). E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. |
149.480 | 4+ | 130 ps 9 | B(E4)|^=1.7 e2b4 6 (1973Be44) from Coul. ex. E(level): B(E4)|^=1.7 e2b4 6 (1973Be44) from Coul. ex. Kπ=0+ GS Rotational band. From 236Pa β- decay. |
309.788 | 6+ | 58 ps 3 | E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From Recoil Distance Doppler Method (RDDM) in Coul. ex. |
522.26 | 8+ | 23.9 ps 19 | B(E2)=6.1 8 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From Recoil Distance Doppler Method (RDDM) in Coul. ex. |
687.56 | 1- | 3.78 ns 9 | E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. Jπ(level): From cross section signature in 235U(d,p). |
744.18 | 3- | B(E3)=0.70 5 E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. Jπ(level): From cross section signature in 235U(d,p). | |
782.4 | 10+ | 11.6 ps 11 | B(E2)=5.0 4 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From Recoil Distance Doppler Method (RDDM) in Coul. ex. |
848.3 | 5- | E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. | |
919.18 | 0+ | E(level): Kπ=0+. | |
957.90 | 2+ | B(E2)=0.195 14 E(level): Kπ=(2+). | |
960.05 | (2+) | E(level): Kπ=0+. | |
966.58 | (1-) | E(level): Kπ=1- Configuration=((n,7/2(743))-(n,5/2(622))). Jπ(level): From cross section signature in 235U(d,p). | |
987.66 | 2- | E(level): Kπ=1- Configuration=((n,7/2(743))-(n,5/2(622))). Jπ(level): From cross section signature in 235U(d,p). | |
999.8 | 7- | E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. | |
1001.6 | (3+) | E(level): Kπ=(2+). | |
1035.6 | 3- | B(E3)=0.35 2 XREF: O(1040). E(level): Kπ=1- Configuration=((n,7/2(743))-(n,5/2(622))). Jπ(level): From cross section signature in 235U(d,p). | |
1050.86 | (4+) | E(level): Kπ=0+. | |
1052.9 | 4- | 101 ns 6 | Configuration=((ν 1/2[631])+(ν 7/2[743])) from (d,p) strength. E(level): Kπ=4- Configuration=((n,7/2(743))+(n,1/2(631))). Jπ(level): From cross section signature in 235U(d,p). |
1058.8 | (4+) | E(level): Kπ=(2+). | |
1070.0 | (4-) | E(level): Kπ=1- Configuration=((n,7/2(743))-(n,5/2(622))). Jπ(level): From cross section signature in 235U(d,p). | |
1085.4 | 12+ | 5.5 ps +18-33 | B(E2)=4.1 6 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From B(E2) in Coul. ex. |
1104.4 | (5-) | E(level): Kπ=4- Configuration=((n,7/2(743))+(n,1/2(631))). Jπ(level): From cross section signature in 235U(d,p). | |
1110.66 | (2-) | E(level): Kπ=2-. | |
1127.38 | (5+) | E(level): Kπ=(2+). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
1149.4 | (3-) | B(E3)=0.26 3 E(level): Kπ=2-. | |
1164 | (5-) | E(level): Kπ=1- Configuration=((n,7/2(743))-(n,5/2(622))). Jπ(level): From cross section signature in 235U(d,p). | |
1164 | (6-) | E(level): Kπ=4- Configuration=((n,7/2(743))+(n,1/2(631))). Jπ(level): From cross section signature in 235U(d,p). | |
1191.6 | (3-) | E(level): Kπ=3- Configuration=((n,7/2(743))-(n,1/2(631))). | |
1198.6 | 9- | E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. | |
1232 | (7-) | E(level): Kπ=4- Configuration=((n,7/2(743))+(n,1/2(631))). Jπ(level): From cross section signature in 235U(d,p). | |
1232.2 | (4-) | E(level): Kπ=3- Configuration=((n,7/2(743))-(n,1/2(631))). Jπ(level): From cross section signature in 235U(d,p). | |
1282.2 | (5-) | E(level): Kπ=3- Configuration=((n,7/2(743))-(n,1/2(631))). Jπ(level): From cross section signature in 235U(d,p). | |
1320 | (8-) | E(level): Kπ=4- Configuration=((n,7/2(743))+(n,1/2(631))). Jπ(level): From cross section signature in 235U(d,p). | |
1342.8 | (6-) | E(level): Kπ=3- Configuration=((n,7/2(743))-(n,1/2(631))). Jπ(level): From cross section signature in 235U(d,p). | |
1413.3 | (7-) | E(level): Kπ=3- Configuration=((n,7/2(743))-(n,1/2(631))). Jπ(level): From cross section signature in 235U(d,p). | |
1426.4 | 14+ | 2.8 ps 3 | B(E2)=4.5 5 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From B(E2) in Coul. ex. |
1443.6 | 11- | E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. | |
1471.7 | (6-) | E(level): Kπ=6- Configuration=((n,7/2(743))+(n,5/2(622))). Jπ(level): From cross section signature in 235U(d,p). | |
1541.8 | (7-) | E(level): Kπ=6- Configuration=((n,7/2(743))+(n,5/2(622))). Jπ(level): From cross section signature in 235U(d,p). | |
1604.80 | (1-,2+) | XREF: F(1600.8). | |
1621.8 | (8-) | E(level): Kπ=6- Configuration=((n,7/2(743))+(n,5/2(622))). Jπ(level): From cross section signature in 235U(d,p). | |
1732.6 | 13- | E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. | |
1791.3 | 1(+) | BM1=0.38 5 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). | |
1801.0 | 16+ | 2.1 ps 2 | B(E2)=3.8 3 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From B(E2) in Coul. ex. |
2054.2 | 1(+) | BM1=0.25 4 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). | |
2060.6 | 15- | E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. | |
2095.7 | 1(+) | BM1=0.15 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2188.8 | 1(+) | BM1=0.92 9 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2204.0 | 18+ | 1.17 ps 12 | B(E2)=4.7 5 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From B(E2) in Coul. ex. |
E(level) | Jπ(level) | T1/2(level) | Comments |
2243.9 | 1 | Jπ(level): Jπ from γ’(θ) in 236U(γ,γ’). | |
2251.1 | 1(+) | BM1=0.25 4 Jπ(level): Jπ from γ’(θ) in 236U(γ,γ’). | |
2284.7 | 1(+) | BM1=0.31 4 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2426.6 | 17- | E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. | |
2435.6 | 1(+) | BM1=0.25 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2440.2 | 1(+) | BM1=0.19 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2457.3 | 1(+) | BM1=0.21 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2494.5 | 1(+) | BM1=0.21 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2498.5 | 1(+) | BM1=0.20 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2631.8 | 20+ | 0.84 ps 12 | B(E2)=4.9 7 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From B(E2) in Coul. ex. |
2699.0 | 1(+) | BM1=0.19 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2712.1 | 1(-) | BE1=1.4 3 Jπ(level): Jπ from γ’(θ) in 236U(γ,γ’). | |
2750 | (0+) | 67 ns 3 % IT = 88 3 % SF = 12 3 | ce’s preceding fission observed, interpreted as g.s. cascade in second minimum with inertia constant α=3.54 (1974HeZE), and α=3.36 keV 1 (1977Bo09) following E=AJ(J+1). E(level): ce’s preceding fission observed, interpreted as g.s. cascade in second minimum with inertia constant α=3.54 (1974HeZE), and α=3.36 keV 1 (1977Bo09) following E=AJ(J+1). |
2756.2 | 1(+) | BM1=0.08 2 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2770 | (2+) | E(level): g.s. band in second potential well with inertia constant α=3.36 keV 1 following E=AJ(J+1). Jπ(level): From (d,pγ). Based on ce cascade interpreted as rotational band (in second minimum) built on fission isomer. | |
2817 | (4+) | E(level): g.s. band in second potential well with inertia constant α=3.36 keV 1 following E=AJ(J+1). Jπ(level): From (d,pγ). Based on ce cascade interpreted as rotational band (in second minimum) built on fission isomer. | |
2823 | (19-) | E(level): Kπ=0- Octupole vibrational band. From 235U(n,γ) E=thermal. | |
2823.3 | 1(+) | BM1=0.11 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2838.3 | 1(+) | BM1=0.09 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2877.8 | 1(-) | BE1=1.6 4 Jπ(level): Jπ from γ’(θ) in 236U(γ,γ’). | |
2891 | (6+) | E(level): g.s. band in second potential well with inertia constant α=3.36 keV 1 following E=AJ(J+1). Jπ(level): From (d,pγ). Based on ce cascade interpreted as rotational band (in second minimum) built on fission isomer. | |
2969.0 | 1(+) | BM1=0.12 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
2991 | (8+) | E(level): g.s. band in second potential well with inertia constant α=3.36 keV 1 following E=AJ(J+1). Jπ(level): From (d,pγ). Based on ce cascade interpreted as rotational band (in second minimum) built on fission isomer. | |
3081.0 | 22+ | 0.65 ps 15 | B(E2)=4.9 11 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From B(E2) in Coul. ex. |
3143.8 | 1(+) | BM1=0.15 3 Jπ(level): (M1) γ rays to g.s. (Jπ=0+) and 45.2-keV level (Jπ=2+). Jπ from γ’(θ) in 236U(γ,γ’). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
3550.0 | 24+ | 0.41 ps 8 | B(E2)=6.3 12 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From B(E2) in Coul. ex. |
4039.0 | 26+ | 0.33 ps 9 | B(E2)=6.3 16 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From B(E2) in Coul. ex. |
4549.0 | 28+ | 0.17 ps 7 | B(E2)=10 4 E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. T1/2(level): From B(E2) in Coul. ex. |
5077 | (30+) | E(level): Kπ=0+ GS Rotational band. From 236Pa β- decay. |
E(level) | E(gamma) | Comments |
45.2431 | 45.243 | E(γ): weighted average of 45.29 6 (1956Ho54); 45.3 2 (1959Tr37); 45.273 20 (1971Cl03,1972ClZS); 45.242 6 (1972Sc01); 45.232 5 (1971GuZY,1976GuZN); 45.244 2 (1981He16) and 45.23 3 (1983Ah02); others: 44.2 1 (1956Gr11); 45.62 1 (1958Sa21); 45.32 (1959Ga13) and 45.28 (1968Du06). M(γ): from 236Np ε decay (22.5 h) and 240Pu α decay.. From conversion electron subshell ratios in 236U(d,pnγ). |
149.480 | 104.237 | E(γ): weighted average of 104.244 5 (1971GuZY,1976GuZN), 104.233 5 (1972Sc01), 104.234 6 (1981He16,1986He12); others: 103.95 50 (1958Sa21), 103.6 3 (1959Tr37), 104.15 2 (1971Cl03,1972ClZS) and 104.23 2 (1983Ah02). M(γ): from 236Np ε decay (155×103 y). From conversion electron subshell ratios in 236U(d,pnγ). |
309.788 | 160.308 | E(γ): weighted average of 160.280 15 (1971GuZY,1976GuZN), 160.310 8 (1972Sc01), 160.312 10 (1975OtZX), 160.308 3 (1981He16,1986He12), others: 160.0 15 (1959Tr37), 160.27 2 (1971Cl03,1972ClZS) and 160.33 2 (1983Ah02). M(γ): from 236Np ε decay (155×103 y). From conversion electron subshell ratios in 236U(d,pnγ). |
522.26 | 212.47 | E(γ): weighted average of 212.48 5 (1975OtZX) and 212.46 5 (1982Ow01). M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
687.56 | 538.09 | E(γ): weighted average of 538.25 20 (1969Le05), 538.09 15 (1975OtZX), 537.92 20 (1977Po05) and 538.1 1 (1984Mi02). I(γ): weighted average of 1.11 12 (1969Le05) 1.1 1 (1975OtZX), 1.6 6 (1977Po05) and 1.6 3 (1984Mi02). M(γ): from α(L1+L2)exp=0.086 27 (1969Le05) and α(K)exp=0.11 5 (1983Fa15). | 642.23 | E(γ): weighted average of 642.42 10 (1969Le05), 642.06 17 (1969BaZW), 642.48 15 (1971Cl03,1972ClZS), 641.8 1 (1972MaYR), 642.2 1 (1973Gr20), 642.3 3 (1973Or06), 642.33 10 (1975OtZX), 642.24 10 (1977Po05) and 642.3 1 (1984Mi02). M(γ): from α(K)exp=0.112 10, α(K)/α(L)=3.59 11, α(L1)/α(L2)=11 4, α(L1+L2)/α(L3)=36 +10-7 (1969Le05); α(K)exp=0.11 3, α(L)exp=0.031 9, α(K)/α(L)=3.56 50 (1977Po05); α(K)exp=0.11 1, α(L1)exp=0.032 3, α(L2)exp=0.0034 4, α(L3)exp=0.0016 11, α(M1)exp=0.0058 7, Anomalous conversion due to penetration effect. The M2 and E3 admixtures are smalls (1983Fa15). | 687.59 | E(γ): Weighted average of 687.71 10 (1969Le05), 687.39 17 (1969BaZW), 688.01 15 (1971Cl03,1972ClZS), 687.5 10 (1972MaYR), 687.5 1 (1973Gr20), 687.6 3 (1973Or06), 687.57 16 (1975OtZX), 687.52 10 (1977Po05) and 687.5 1 (1984Mi02). I(γ): weighted average of 26.5 5 (1969Le05), 28.5 5 (1971GuZY,1976GuZN), 24.8 36 (1973Or06), 21 3 (1973Gr20), 26.2 7 (1975OtZX), 29.4 9 (1977Po05), 26.8 20 (1984Mi02) and 29 4 (1979McZP). M(γ): from α(K)exp=0.22 2, α(K)/α(L)=3.26 16, α(L1)/α(L2)=7 3, α(L1+L2)/α(L3)=46 +40-20 (1969Le05); α(K)exp=0.219 14, α(L)exp=0.069 9, α(K)/α(L)=3.19 38 (1977Po05); α(L1)exp=0.059 3, α(L2)exp=0.0129 15, α(L3)exp=0.0016 11, α(M1)exp=0.0195 23, Anomalous conversion due to penetration effects. The M2 and E3 admixtures are small (1983Fa15). |
744.18 | 56.6 | E(γ): from 236U(d,pnγ), uncertainty deduced from level energy difference, I(γ): deduced from γ-ray intensity balance in 236Pa β- decay; other: Iγ|>5 from 236U(d,pnγ). | 594.5 | E(γ): from 236Pa β- decay. |
782.4 | 260.1 | E(γ): from Coul. ex. M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
848.3 | 103.4 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
919.18 | 873.98 | E(γ): weighted average of 874.1 2 (1984Mi02) and 873.92 15 (1975OtZX). | 918.9 | E(γ): From 235U(n,γ) E=thermal M(γ): From conversion electron data in 235U(n,γ) E=thermal. |
957.90 | 912.4 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal | 958.0 | E(γ): from 236Pa β- decay.. From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal. From 235U(n,γ) E=thermal |
960.05 | 810.9 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal | 914.8 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal M(γ): From conversion electron data in 235U(n,γ) E=thermal. | 959.9 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal |
966.58 | 279.0 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 921.2 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay M(γ): From conversion electron data in 235U(n,γ) E=thermal. | 966.8 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay M(γ): From conversion electron data in 235U(n,γ) E=thermal. |
987.66 | 243.6 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay M(γ): From conversion electron data in 235U(n,γ) E=thermal. | 300.0 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 942.4 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay M(γ): From conversion electron data in 235U(n,γ) E=thermal. |
999.8 | 151.5 | E(γ): From 236U(d,pnγ) I(γ): From 236U(d,pnγ) M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
E(level) | E(gamma) | Comments |
1001.6 | 258.4 | E(γ): From 235U(n,γ) E=thermal | 852.2 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal | 956.3 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal |
1035.6 | 886.2 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal | 990.2 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal |
1050.86 | 901.25 | E(γ): From 235U(n,γ) E=thermal | 1006.0 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal |
1052.9 | 65 | M(γ): From conversion electron data in 235U(n,γ) E=thermal. | 204.6 | M(γ): From conversion electron data in 235U(n,γ) E=thermal. | 307.9 | M(γ): From conversion electron data in 235U(n,γ) E=thermal. | 903.6 | I(γ): from delayed Iγ in 235U(n,γ) E=thermal M(γ): From conversion electron data in 235U(n,γ) E=thermal. |
1058.8 | 909.3 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal M(γ): From conversion electron data in 235U(n,γ) E=thermal. | 1014.1 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal |
1070.0 | 920.5 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal |
1085.4 | 303.0 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
1110.66 | 366.6 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 423.1 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1065.0 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
1127.38 | 977.9 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal |
1149.4 | 405.2 | E(γ): From 235U(n,γ) E=thermal I(γ): From 235U(n,γ) E=thermal |
1198.6 | 198.8 | E(γ): From 236U(d,pnγ) I(γ): From 236U(d,pnγ) M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
1271.10 | 526.7 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1225.9 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
1426.4 | 341.0 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
1443.6 | 245.0 | E(γ): From 236U(d,pnγ) I(γ): From 236U(d,pnγ) M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
E(level) | E(gamma) | Comments |
1580 | 1580 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) |
1604.80 | 333.7 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 617.1 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 860.6 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 917.0 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1559.6 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1604.9 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
1662.36 | 674.5 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 975.0 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1617.1 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1662.4 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
1732.6 | 289 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
1791.3 | 1746.1 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 1791.3 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
1801.0 | 374.6 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From conversion electron subshell ratios in 236U(d,pnγ). |
1807.88 | 1762.7 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1807.8 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
1865.39 | 1177.7 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1865.5 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
1972.62 | 1927.0 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1972.7 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
1979.15 | 1234.9 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1291.6 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1934.1 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
1981.04 | 870.4 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1023.1 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay | 1981.0 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
E(level) | E(gamma) | Comments |
2054.2 | 2009.0 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2054.2 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2060.6 | 328 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From E2 matrix elements deduced in Coulomb excitation measurements. |
2086.54 | 2041.3 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2086.5 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2095.7 | 2050.5 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2095.7 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2155.40 | 550.6 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
2188.8 | 2143.6 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2188.8 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2190 | 2190 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) |
2204.0 | 403.0 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From E2 matrix elements deduced in Coulomb excitation measurements. |
2226.9 | 2181.6 | E(γ): From 236Pa β- decay I(γ): From 236Pa β- decay |
2243.9 | 2243.9 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) |
2251.1 | 2205.9 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) | 2251.1 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) |
2284.7 | 2239.5 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2284.7 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2426.6 | 366 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From E2 matrix elements deduced in Coulomb excitation measurements. |
2435.6 | 2390.4 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2435.6 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2440.2 | 2395.0 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2440.2 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2457.3 | 2412.1 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2457.3 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
E(level) | E(gamma) | Comments |
2494.5 | 2449.3 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2494.5 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2498.5 | 2453.3 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2498.5 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2631.8 | 427.8 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From E2 matrix elements deduced in Coulomb excitation measurements. |
2699.0 | 2653.8 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2699.0 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2712.1 | 2666.9 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) | 2712.1 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) |
2750 | 560 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) M(γ): From γγ angular correlations in 235U(d,pγ). | 1170 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) M(γ): From γγ angular correlations in 235U(d,pγ). | 1783 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) | 2062 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) |
2756.2 | 2711.0 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2756.2 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2770 | 20 | E(γ): from level energy difference. From 235U(d,pγ) I(γ): From 235U(d,pγ) M(γ): From in-band transition of rotational band in the second well of the nuclear potential in 235U(d,pγ). |
2817 | 47.0 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) M(γ): From in-band transition of rotational band in the second well of the nuclear potential in 235U(d,pγ). |
2823 | 396 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From E2 matrix elements deduced in Coulomb excitation measurements. |
2823.3 | 2778.1 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2823.3 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2838.3 | 2793.1 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2838.3 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2877.8 | 2832.6 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2877.8 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2891 | 73.9 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) M(γ): From in-band transition of rotational band in the second well of the nuclear potential in 235U(d,pγ). |
E(level) | E(gamma) | Comments |
2969.0 | 2923.8 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 2969.0 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
2991 | 100.8 | E(γ): From 235U(d,pγ) I(γ): From 235U(d,pγ) M(γ): From in-band transition of rotational band in the second well of the nuclear potential in 235U(d,pγ). |
3081.0 | 449.2 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From E2 matrix elements deduced in Coulomb excitation measurements. |
3143.8 | 3098.6 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). | 3143.8 | E(γ): From 236U(γ,γ’) I(γ): From 236U(γ,γ’) M(γ): From γ’(θ) and systematics of branching ratios to the first Jπ=2+ excited states in 236U(γ,γ’). |
3550.0 | 469 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From E2 matrix elements deduced in Coulomb excitation measurements. |
4039.0 | 489 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From E2 matrix elements deduced in Coulomb excitation measurements. |
4549.0 | 510 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): From E2 matrix elements deduced in Coulomb excitation measurements. |
5077 | 528 | E(γ): From Coulomb excitation I(γ): From Coulomb excitation M(γ): from in-band transition of ground-state band in Coul. ex. |
Spontaneous fission: 2005Xu01, 2004Ro01, 2001Vl04, 1997Ro12, 1993Mo16, 2001Po31 and 1994Pi12 (ternary fission accompanied by emission of light charged particles); 2000Gu28 (fission fragments distribution, theory)
Q-value: S(2n)=11843.0 3, S(2p)=12746.3 24 (2021Wa16)