ADOPTED LEVELS, GAMMAS for 209Bi
Authors: J. Chen and F.G. Kondev | Citation: Nucl. Data Sheets 126, 373 (2015) | Cutoff date: 30-Sep-2013
Full ENSDF file | Adopted Levels (PDF version)
| Q(β-)=-1892.6 keV 16 | S(n)= 7459.8 keV 19 | S(p)= 3799.0 keV 8 | Q(α)= 3137.3 keV 8 | ||
| Reference: 2012WA38 |
E(level): From a least-squares fit to γ-ray energies, unless otherwise noted.
M(γ): From γ(θ) in (t,2nγ) (1983Ma15), unless otherwise noted.
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
| 896.28 | 7/2- | 8.2 ps 12 | 896.28 7 | M1+E2 | -0.62 6 | 0.0208 | B(E2)(W.u.)=0.44 9, B(M1)(W.u.)=0.0026 5, α=0.0208 8, α(K)=0.0170 6, α(L)=0.00293 9, α(M)=0.000687 21, α(N)=0.000176 6, α(O)=3.58E-5 11, α(P)=4.23E-6 14 |
| 1608.57 | 13/2+ | 0.23 ns 13 | 1608.53 8 | M2+E3 | +0.33 10 | 0.0127 | B(E3)(W.u.)=7 6, B(M2)(W.u.)=0.32 18, α=0.0127 5, α(K)=0.0103 4, α(L)=0.00182 7, α(M)=0.000431 15, α(N)=0.000110 4, α(O)=2.25E-5 8, α(P)=2.67E-6 10 |
| 2442.92 | 1/2+ | 11.3 ns 4 | 1546.52 9 | E3 | 0.00639 | B(E3)(W.u.)=1.95 7, α=0.00639, α(K)=0.00499 7, α(L)=0.001032 15, α(M)=0.000248 4, α(N)=6.34E-5 9, α(O)=1.276E-5 18, α(P)=1.437E-6 21 | |
| 2492.86 | 3/2+ | ≈ 31 ps | 49.94 7 | [M1] | 14.51 | B(M1)(W.u.)≈0.073, α=14.51, α(L)=11.08 17, α(M)=2.61 4, α(N)=0.668 10, α(O)=0.1364 20, α(P)=0.01623 24 | |
| 3/2+ | ≈ 31 ps | 2492.86 11 | [E3] | 0.00275 | B(E3)(W.u.)≈20, α=0.00275, α(K)=0.00197 3, α(L)=0.000347 5, α(M)=8.17E-5 12, α(N)=2.09E-5 3, α(O)=4.24E-6 6, α(P)=4.96E-7 7 | ||
| 2564.14 | (9/2)+ | 0.015 ps 3 | 2564.12 10 | E1+E3 | 0.026 3 | 1.43×10-3 | B(E1)(W.u.)=0.00076 16, B(E3)(W.u.)=29 9, α=1.43E-3, α(K)=0.000449 7, α(L)=6.65E-5 10, α(M)=1.531E-5 22, α(N)=3.90E-6 6, α(O)=7.98E-7 12, α(P)=9.57E-8 14 |
| 2583.02 | (7/2)+ | 0.31 ps 10 | 1686.66 10 | E1 | 1.36×10-3 | B(E1)(W.u.)=9.E-5 3, α=1.36E-3, α(K)=0.000885 13, α(L)=0.0001327 19, α(M)=3.06E-5 5, α(N)=7.80E-6 11, α(O)=1.591E-6 23, α(P)=1.90E-7 3 | |
| (7/2)+ | 0.31 ps 10 | 2583.07 10 | E1+E3 | 0.19 3 | 1.48×10-3 | B(E1)(W.u.)=1.1E-5 4, B(E3)(W.u.)=22 10, α=1.48E-3 3, α(K)=0.000492 18, α(L)=7.4E-5 3, α(M)=1.72E-5 8, α(N)=4.38E-6 19, α(O)=9.0E-7 4, α(P)=1.07E-7 5 | |
| 2599.91 | 11/2+ | 36 fs 10 | 992.0 5 | [M1] | 0.0196 | B(M1)(W.u.)=0.09 3, α=0.0196, α(K)=0.01611 23, α(L)=0.00269 4, α(M)=0.000629 9, α(N)=0.0001609 23, α(O)=3.29×10-5 5, α(P)=3.94E-6 6 | |
| 11/2+ | 36 fs 10 | 2599.9 1 | E1+E3 | 0.051 8 | 1.45×10-3 | B(E1)(W.u.)=0.00026 8, B(E3)(W.u.)=36 15, α=1.45E-3, α(K)=0.000442 7, α(L)=6.55E-5 10, α(M)=1.508E-5 22, α(N)=3.84E-6 6, α(O)=7.86E-7 12, α(P)=9.43E-8 14 | |
| 2600.92 | 13/2+ | 0.44 ps 14 | 992.35 2 | M1(+E2) | -0.04 4 | 0.0196 | B(E2)(W.u.)=(0.03 +6-3), B(M1)(W.u.)=(0.050 16), α=0.0196, α(K)=0.01608 23, α(L)=0.00269 4, α(M)=0.000628 9, α(N)=0.0001606 23, α(O)=3.28E-5 5, α(P)=3.93E-6 6 |
| 13/2+ | 0.44 ps 14 | 2600.6 5 | (M2+E3) | 0.9 GT | 0.0031 | B(E3)(W.u.)>3.7, B(M2)(W.u.)<0.18, α=0.0031 6, α(K)=0.0022 5, α(L)=0.00038 7, α(M)=9.0E-5 16, α(N)=2.3E-5 4, α(O)=4.7E-6 9, α(P)=5.6E-7 11 | |
| 2617.34 | 5/2+ | 7.2 ps 11 | 124.48 5 | M1(+E2) | 5.45 | α=5.45, α(K)=4.43 7, α(L)=0.778 11, α(M)=0.183 3, α(N)=0.0468 7, α(O)=0.00957 14, α(P)=0.001139 16 | |
| 5/2+ | 7.2 ps 11 | 1721.08 13 | E1(+M2) | 0.00145 | α=0.00145 11, α(K)=0.00094 9, α(L)=0.000143 15, α(M)=3.3×10-5 4, α(N)=8.4E-6 9, α(O)=1.72E-6 19, α(P)=2.05E-7 22 | ||
| 5/2+ | 7.2 ps 11 | 2617.35 10 | E3(+M2) | 0.00354 | α=0.00354 97, α(K)=0.00254 75, α(L)=4.3×10-4 12, α(M)=1.02E-4 29, α(N)=2.60E-5 72, α(O)=5.3E-6 15, α(P)=6.3E-7 19 | ||
| 2741.05 | 15/2+ | 9.1 ps 12 | 140.13 1 | M1(+E2) | 0.3 LT | 3.80 | B(E2)(W.u.)<89, B(M1)(W.u.)>0.042, α=3.80 11, α(K)=3.05 13, α(L)=0.572 20, α(M)=0.136 6, α(N)=0.0347 15, α(O)=0.0070 3, α(P)=0.000818 14 |
| 15/2+ | 9.1 ps 12 | 1132.46 4 | M1+E2 | +0.14 4 | 0.01380 | B(E2)(W.u.)=0.0025 15, B(M1)(W.u.)=0.00046 7, α=0.01380 22, α(K)=0.01133 18, α(L)=0.00189 3, α(M)=0.000441 7, α(N)=0.0001128 18, α(O)=2.31E-5 4, α(P)=2.76E-6 5 | |
| 15/2+ | 9.1 ps 12 | 2741.03 6 | E3 | 0.00243 | B(E3)(W.u.)=18.6 25, α=0.00243, α(K)=0.001645 23, α(L)=0.000283 4, α(M)=6.65E-5 10, α(N)=1.699E-5 24, α(O)=3.46E-6 5, α(P)=4.06E-7 6 | ||
| 2766.66 | 3/2+ | 149.3 1 | [M1] | 3.25 | α=3.25, α(K)=2.65 4, α(L)=0.462 7, α(M)=0.1088 16, α(N)=0.0278 4, α(O)=0.00569 8, α(P)=0.000677 10 | ||
| 3/2+ | 273.80 3 | [M1] | 0.596 | α=0.596, α(K)=0.486 7, α(L)=0.0841 12, α(M)=0.0198 3, α(N)=0.00506 7, α(O)=0.001033 15, α(P)=0.0001230 18 | |||
| 3/2+ | 323.74 2 | M1 | 0.377 | α=0.377, α(K)=0.308 5, α(L)=0.0530 8, α(M)=0.01246 18, α(N)=0.00319 5, α(O)=0.000651 10, α(P)=7.75×10-5 11 | |||
| 2826.1 | 5/2- | 6.9 fs 9 | 1929.9 5 | [M1] | 0.00397 | B(M1)(W.u.)=0.124 19, α=0.00397, α(K)=0.00294 5, α(L)=0.000483 7, α(M)=0.0001128 16, α(N)=2.88×10-5 4, α(O)=5.90E-6 9, α(P)=7.08E-7 10 | |
| 5/2- | 6.9 fs 9 | 2826.0 4 | E2 | 1.67×10-3 | B(E2)(W.u.)=4.4 6, α=1.67E-3, α(K)=0.000850 12, α(L)=0.0001339 19, α(M)=3.11E-5 5, α(N)=7.93E-6 12, α(O)=1.620E-6 23, α(P)=1.93E-7 3 | ||
| 2916.62 | (1/2)+ | 149.98 5 | M1+E2 | 3.21 | α=3.21, α(K)=2.61 4, α(L)=0.457 7, α(M)=0.1074 15, α(N)=0.0275 4, α(O)=0.00561 8, α(P)=0.000668 10 | ||
| 2955.93 | (3/2)+ | 110.67 15 | [M1] | 7.63 | α=7.63, α(K)=6.20 9, α(L)=1.091 16, α(M)=0.257 4, α(N)=0.0657 10, α(O)=0.01342 20, α(P)=0.001597 24 | ||
| (3/2)+ | 338.65 10 | [M1] | 0.334 | α=0.334, α(K)=0.272 4, α(L)=0.0469 7, α(M)=0.01101 16, α(N)=0.00282 4, α(O)=0.000575 8, α(P)=6.85×10-5 10 | |||
| (3/2)+ | 463.04 8 | [M1] | 0.1438 | α=0.1438, α(K)=0.1175 17, α(L)=0.0201 3, α(M)=0.00471 7, α(N)=0.001204 17, α(O)=0.000246 4, α(P)=2.94×10-5 5 | |||
| (3/2)+ | 513.0 | [M1] | 0.1095 | α=0.1095, α(K)=0.0896 13, α(L)=0.01526 22, α(M)=0.00358 5, α(N)=0.000915 13, α(O)=0.000187 3, α(P)=2.23×10-5 4 | |||
| (3/2)+ | 2954.7 4 | [E3] | 0.00223 | α=0.00223, α(K)=0.001424 20, α(L)=0.000242 4, α(M)=5.66×10-5 8, α(N)=1.447E-5 21, α(O)=2.95E-6 5, α(P)=3.48E-7 5 | |||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
| 2986.80 | 19/2+ | 17.9 ns 5 | 245.73 2 | E2 | 0.224 | B(E2)(W.u.)=0.387 12, α=0.224, α(K)=0.1046 15, α(L)=0.0893 13, α(M)=0.0233 4, α(N)=0.00593 9, α(O)=0.001114 16, α(P)=9.44E-5 14 | |
| 19/2+ | 17.9 ns 5 | 385.9 | [M3] | 2.14 | B(M3)(W.u.)=8.×103 8, α=2.14, α(K)=1.444 21, α(L)=0.520 8, α(M)=0.1349 19, α(N)=0.0350 5, α(O)=0.00699 10, α(P)=0.000759 11 | ||
| 3038.88 | 5/2+ | 272.2 1 | (M1+E2) | 0.606 | α=0.606, α(K)=0.494 7, α(L)=0.0855 12, α(M)=0.0201 3, α(N)=0.00514 8, α(O)=0.001050 15, α(P)=0.0001250 18 | ||
| 5/2+ | 2142.78 18 | E1 | 1.34×10-3 | α=1.34×10-3, α(K)=0.000598 9, α(L)=8.89E-5 13, α(M)=2.05E-5 3, α(N)=5.22E-6 8, α(O)=1.066E-6 15, α(P)=1.276E-7 18 | |||
| 3090.16 | (7/2)+ | 2194.1 2 | [E1] | 1.35×10-3 | α=1.35×10-3, α(K)=0.000576 8, α(L)=8.55E-5 12, α(M)=1.97E-5 3, α(N)=5.02E-6 7, α(O)=1.026E-6 15, α(P)=1.227E-7 18 | ||
| (7/2)+ | 3089.96 12 | (E1+M2) | 0.00161 | α=0.00161 3, α(K)=0.000353 20, α(L)=5.2×10-5 4, α(M)=1.21E-5 8, α(N)=3.07E-6 20, α(O)=6.3E-7 4, α(P)=7.6E-8 5 | |||
| 3119.48 | 3/2- | 0.021 ps 14 | 2223.23 10 | E2 | 0.00195 | B(E2)(W.u.)=7 5, α=0.00195, α(K)=0.001308 19, α(L)=0.000212 3, α(M)=4.93E-5 7, α(N)=1.258E-5 18, α(O)=2.56E-6 4, α(P)=3.03E-7 5 | |
| 3132.97 | 11/2+ | 1524.2 3 | [M1] | 0.00666 | α=0.00666, α(K)=0.00537 8, α(L)=0.000887 13, α(M)=0.000207 3, α(N)=5.29×10-5 8, α(O)=1.084E-5 16, α(P)=1.299E-6 19 | ||
| 11/2+ | 3132.96 9 | E1 | 1.61×10-3 | α=1.61×10-3, α(K)=0.000327 5, α(L)=4.82E-5 7, α(M)=1.108E-5 16, α(N)=2.82E-6 4, α(O)=5.78E-7 8, α(P)=6.94E-8 10 | |||
| 3135.77 | (15/2)+ | 394.72 7 | M1 | 0.220 | α=0.220, α(K)=0.180 3, α(L)=0.0309 5, α(M)=0.00725 11, α(N)=0.00185 3, α(O)=0.000379 6, α(P)=4.52×10-5 7 | ||
| (15/2)+ | 1527.13 14 | M1 | 0.00663 | α=0.00663, α(K)=0.00535 8, α(L)=0.000882 13, α(M)=0.000206 3, α(N)=5.27×10-5 8, α(O)=1.079E-5 16, α(P)=1.292E-6 18 | |||
| 3152.83 | (9/2)+ | 3152.80 20 | E1 | 1.61×10-3 | α=1.61×10-3, α(K)=0.000324 5, α(L)=4.77E-5 7, α(M)=1.097E-5 16, α(N)=2.79E-6 4, α(O)=5.72E-7 8, α(P)=6.87E-8 10 | ||
| 3154.06 | 17/2+ | 167.16 6 | M1 | 2.36 | α=2.36, α(K)=1.92 3, α(L)=0.335 5, α(M)=0.0789 11, α(N)=0.0202 3, α(O)=0.00412 6, α(P)=0.000491 7 | ||
| 17/2+ | 413.04 3 | M1(+E2) | 0.195 | α=0.195, α(K)=0.1594 23, α(L)=0.0273 4, α(M)=0.00641 9, α(N)=0.001640 23, α(O)=0.000335 5, α(P)=3.99×10-5 6 | |||
| 3159.33 | 3/2(+) | 314.2 2 | (M1) | 0.409 | α=0.409, α(K)=0.334 5, α(L)=0.0576 9, α(M)=0.01352 19, α(N)=0.00346 5, α(O)=0.000707 10, α(P)=8.42×10-5 12 | ||
| 3169.07 | (13/2)+ | 1560.49 4 | M1 | 0.00630 | α=0.00630, α(K)=0.00506 7, α(L)=0.000835 12, α(M)=0.000195 3, α(N)=4.98×10-5 7, α(O)=1.020E-5 15, α(P)=1.223E-6 18 | ||
| 3197.60 | (1/2+,3/2+) | 352.30 8 | (M1) | 0.300 | α=0.300, α(K)=0.245 4, α(L)=0.0421 6, α(M)=0.00988 14, α(N)=0.00253 4, α(O)=0.000517 8, α(P)=6.15×10-5 9 | ||
| 3211.85 | (17/2)+ | 225.05 2 | (M1) | 1.026 | α=1.026, α(K)=0.836 12, α(L)=0.1451 21, α(M)=0.0341 5, α(N)=0.00873 13, α(O)=0.001783 25, α(P)=0.000212 3 | ||
| 3221.65 | 5/2+ | 455.02 10 | (M1) | 0.1506 | α=0.1506, α(K)=0.1231 18, α(L)=0.0210 3, α(M)=0.00494 7, α(N)=0.001262 18, α(O)=0.000258 4, α(P)=3.08×10-5 5 | ||
| 3269.64 | 1/2+,3/2+ | 424.5 1 | (M1) | 0.181 | α=0.181, α(K)=0.1482 21, α(L)=0.0254 4, α(M)=0.00595 9, α(N)=0.001523 22, α(O)=0.000311 5, α(P)=3.71×10-5 6 | ||
| 3378.16 | (9/2+) | 3378.11 10 | (E1) | 1.68×10-3 | α=1.68×10-3, α(K)=0.000291 4, α(L)=4.28E-5 6, α(M)=9.84E-6 14, α(N)=2.51E-6 4, α(O)=5.13E-7 8, α(P)=6.17E-8 9 | ||
| 3393.38 | (15/2+) | 1784.8 2 | D | α(K)=0.00359 5, α(L)=0.000591 9, α(M)=0.0001379 20, α(N)=3.53×10-5 5, α(O)=7.22E-6 11, α(P)=8.66E-7 13, α(N+)=0.000332 5 | |||
| 3406.21 | 13/2+ | 1797.64 12 | M1 | 0.00458 | α=0.00458, α(K)=0.00353 5, α(L)=0.000580 9, α(M)=0.0001354 19, α(N)=3.46×10-5 5, α(O)=7.09E-6 10, α(P)=8.50E-7 12 | ||
| 3449.7 | (7/2+) | 2553.4 4 | D | α(K)=0.000451 7, α(L)=6.68×10-5 10, α(M)=1.537E-5 22, α(N)=3.92E-6 6, α(O)=8.01E-7 12, α(P)=9.61E-8 14, α(N+)=0.000896 13 | |||
| 3464.12 | 11/2+ | 3464.09 10 | E1 | 1.71×10-3 | α=1.71×10-3, α(K)=0.000280 4, α(L)=4.11E-5 6, α(M)=9.46E-6 14, α(N)=2.41E-6 4, α(O)=4.93E-7 7, α(P)=5.93E-8 9 | ||
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
| 3467.67 | 19/2+ | 313.70 16 | M1 | 0.411 | α=0.411, α(K)=0.335 5, α(L)=0.0578 9, α(M)=0.01358 20, α(N)=0.00347 5, α(O)=0.000710 10, α(P)=8.45×10-5 12 | ||
| 19/2+ | 480.87 5 | M1 | 0.1300 | α=0.1300, α(K)=0.1063 15, α(L)=0.0181 3, α(M)=0.00426 6, α(N)=0.001088 16, α(O)=0.000222 4, α(P)=2.65×10-5 4 | |||
| 3486.93 | (19/2+) | 500.12 5 | (M1) | 0.1172 | α=0.1172, α(K)=0.0958 14, α(L)=0.01633 23, α(M)=0.00383 6, α(N)=0.000979 14, α(O)=0.000200 3, α(P)=2.39×10-5 4 | ||
| 3579.00 | (17/2+:21/2+) | 592.2 1 | D | α(K)=0.0614 9, α(L)=0.01041 15, α(M)=0.00244 4, α(N)=0.000624 9, α(O)=0.0001276 18, α(P)=1.522×10-5 22, α(N+)=0.000767 11 | |||
| 3597.14 | 19/2+ | 610.33 15 | M1 | 0.0693 | α=0.0693, α(K)=0.0567 8, α(L)=0.00961 14, α(M)=0.00225 4, α(N)=0.000576 8, α(O)=0.0001177 17, α(P)=1.405×10-5 20 | ||
| 3601.72 | (5/2+,7/2+,9/2+) | 2705.42 10 | (E1) | 1.47×10-3 | α=1.47×10-3, α(K)=0.000412 6, α(L)=6.08E-5 9, α(M)=1.400E-5 20, α(N)=3.57E-6 5, α(O)=7.30E-7 11, α(P)=8.76E-8 13 | ||
| 3633.85 | 1/2- | 514.37 2 | [M1] | 0.1087 | α=0.1087, α(K)=0.0889 13, α(L)=0.01515 22, α(M)=0.00355 5, α(N)=0.000908 13, α(O)=0.000186 3, α(P)=2.21×10-5 4 | ||
| 1/2- | 677.8 2 | [E1] | 0.00538 | α=0.00538, α(K)=0.00446 7, α(L)=0.000706 10, α(M)=0.0001640 23, α(N)=4.17×10-5 6, α(O)=8.44E-6 12, α(P)=9.77E-7 14 | |||
| 1/2- | 788.8 2 | [E1] | 0.00403 | α=0.00403, α(K)=0.00335 5, α(L)=0.000523 8, α(M)=0.0001214 17, α(N)=3.09×10-5 5, α(O)=6.26E-6 9, α(P)=7.30E-7 11 | |||
| 1/2- | 867.2 2 | [E1] | 0.00338 | α=0.00338, α(K)=0.00281 4, α(L)=0.000436 7, α(M)=0.0001011 15, α(N)=2.57×10-5 4, α(O)=5.22E-6 8, α(P)=6.11E-7 9 | |||
| 1/2- | 1140.8 2 | [E1] | 0.00207 | α=0.00207, α(K)=0.001721 24, α(L)=0.000263 4, α(M)=6.07×10-5 9, α(N)=1.546E-5 22, α(O)=3.15E-6 5, α(P)=3.71E-7 6 | |||
| 1/2- | 1191.0 2 | [E1] | 0.00193 | α=0.00193, α(K)=0.001596 23, α(L)=0.000243 4, α(M)=5.62×10-5 8, α(N)=1.431E-5 20, α(O)=2.91E-6 4, α(P)=3.44E-7 5 | |||
| 3703.55 | 7/2(+) | 664.8 2 | D | α(K)=0.0454 7, α(L)=0.00767 11, α(M)=0.00180 3, α(N)=0.000459 7, α(O)=9.39×10-5 14, α(P)=1.121E-5 16, α(N+)=0.000564 8 | |||
| 3812.25 | 23/2+ | 825.45 15 | E2 | 0.01024 | α=0.01024, α(K)=0.00795 12, α(L)=0.001739 25, α(M)=0.000420 6, α(N)=0.0001072 15, α(O)=2.13×10-5 3, α(P)=2.32E-6 4 | ||
| 4141.95 | 21/2(+) | 544.85 10 | D | α(K)=0.0764 11, α(L)=0.01299 19, α(M)=0.00305 5, α(N)=0.000779 11, α(O)=0.0001592 23, α(P)=1.90×10-5 3, α(N+)=0.000957 14 | |||
| 21/2(+) | 654.98 10 | D | α(K)=0.0471 7, α(L)=0.00797 12, α(M)=0.00187 3, α(N)=0.000478 7, α(O)=9.77×10-5 14, α(P)=1.166E-5 17, α(N+)=0.000587 9 | ||||
| 5609 | 11/2- | 0.48 fs 10 | 5609 5 | M1 | 0.00252 | B(M1)(W.u.)=0.26 6, α=0.00252, α(K)=0.000201 3, α(L)=3.20×10-5 5, α(M)=7.44E-6 11, α(N)=1.90E-6 3, α(O)=3.90E-7 6, α(P)=4.69E-8 7 | |
| 7168.1 | 9/2+ | 0.56 fs 3 | 7168 | E1 | B(E1)(W.u.)=0.00093 5 |
Additional Level Data and Comments:
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 0.0 | 9/2- | 2.01×1019 y 8 % α = 100 | μ=+4.1103 5 (1953Ti01), Q=-0.55 1 (1983De07) π0 emission not found (1989St01). Isotope shift(207Bi-209Bi)=0.0999 cm-1 20 (1985Ba21). Charge density distribution measured (1973Si20,1978Eu01). |
| 896.28 | 7/2- | 8.2 ps 12 | configuration=π(2f7/2)+1. |
| 1608.57 | 13/2+ | 0.23 ns 13 | Q=-0.37 3 (1972Le07) Isomer shift measured in muonic atom: 3.7 +6-8 (1974Ba77), 3.5 6 (1972Le07), 3.8 3 (1984Ru08). |
| 2442.92 | 1/2+ | 11.3 ns 4 | XREF: f(2430). |
| 2492.86 | 3/2+ | ≈ 31 ps | XREF: f(2480)h(2480). Jπ(level): L(p,p’)=3, σ(p,p’). See comment "particle-vibration coupled states (208Pb 3-) ". |
| 2564.14 | (9/2)+ | 0.015 ps 3 | Q=+0.11 5 (1972Le07), μ=3.5 7 Isomer shift=6.2 5 (1974Ba77), 5.8 5 (1972Le07), 6.6 3 (1984Ru08) in Muonic atom dataset. E(level): Isomer shift=6.2 5 (1974Ba77), 5.8 5 (1972Le07), 6.6 3 (1984Ru08) in Muonic atom dataset. Jπ(level): L(p,p’)=3, σ(p,p’). See comment "particle-vibration coupled states (208Pb 3-) ". |
| 2583.02 | (7/2)+ | 0.31 ps 10 | B(E3)=0.052 8 (1969He07) β3=0.122 6 from inelastic scattering (1967Al14). Jπ(level): L(p,p’)=3, σ(p,p’). See comment "particle-vibration coupled states (208Pb 3-) ". |
| 2599.91 | 11/2+ | 36 fs 10 | B(E3)|^=0.094 14 in Coulomb excitation (1969He07). Jπ(level): L(p,p’)=3, σ(p,p’). See comment "particle-vibration coupled states (208Pb 3-) ". |
| 2600.92 | 13/2+ | 0.44 ps 14 | B(E3)|^=0.108 15 from B(E3)=0.072 11 in Coulomb excitation (1969He07). Jπ(level): L(p,p’)=3, σ(p,p’). See comment "particle-vibration coupled states (208Pb 3-) ". |
| 2617.34 | 5/2+ | 7.2 ps 11 | configuration=π(1h9/2)+1~#3- (1974Cl07,1983Ma15). Jπ(level): L(p,p’)=3, σ(p,p’). See comment "particle-vibration coupled states (208Pb 3-) ". |
| 2741.05 | 15/2+ | 9.1 ps 12 | Q=0.0 4 (1972Le07), μ=6.2 12 B(E3)|^=0.077 10 from B(E3)=0.048 6, weighted average of 0.048 7 in Coulomb excitation (1969He07) and 0.047 10 in Muonic atom (1972Le07). E(level): B(E3)|^=0.077 10 from B(E3)=0.048 6, weighted average of 0.048 7 in Coulomb excitation (1969He07) and 0.047 10 in Muonic atom (1972Le07). |
| 2766.66 | 3/2+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)5- \ (1974Cl07,1983Ma15). Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". | |
| 2826.1 | 5/2- | 6.9 fs 9 | B(E2)|^=0.029 10 in Coulomb excitation (1970Br12). |
| 2845.20 | 1/2+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)5- \ (1974Cl07,1983Ma15). | |
| 2916.62 | (1/2)+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)4- \ (1974Cl07,1983Ma15). | |
| 2955.93 | (3/2)+ | configuration=π(2d3/2)-1+π(1h9/2)+1~#3- (1972Ba81). | |
| 2986.80 | 19/2+ | 17.9 ns 5 | μ=3.50 8 (1978Be17) XREF: d(2979). Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". |
| 3038.88 | 5/2+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)5- \ (1974Cl07,1983Ma15). Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". | |
| 3090.16 | (7/2)+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)5- \ (1983Ma15). Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". | |
| 3119.48 | 3/2- | 0.021 ps 14 | XREF: n(3139). |
| 3132.97 | 11/2+ | β5=0.067 4 from inelastic scattering (1967Al14). Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". | |
| 3135.77 | (15/2)+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)5- \ (1983Ma15). Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". | |
| 3152.83 | (9/2)+ | Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". | |
| 3154.06 | 17/2+ | Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". | |
| 3159.33 | 3/2(+) | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)4- \ (1983Ma15). | |
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 3169.07 | (13/2)+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)5- \ (1974Cl07,1983Ma15). Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". | |
| 3211.85 | (17/2)+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)4- \ (1983Ma15). Note, that π(1h9/2)+1~#51- is proposed in 1974Cl07. Jπ(level): L(p,p’)=5. See comment "particle-vibration coupled states (208Pb 4-, 5-) ". | |
| 3221.65 | 5/2+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)4- \ (1974Cl07,1983Ma15). E(level): From (t,2nγ). Jπ(level): See comment "particle-vibration coupled states (208Pb 4-,5-). | |
| 3311.14 | (7/2+,9/2+) | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)4- \ (1974Cl07). | |
| 3354.8 | (5/2+) | E(level): From (t,2nγ). Jπ(level): See comment "particle-vibration coupled states (208Pb 4-,5-). | |
| 3378.16 | (9/2+) | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)4- \ (1983Ma15). E(level): From (t,2nγ). Jπ(level): See comment "particle-vibration coupled states (208Pb 4-,5-). | |
| 3393.38 | (15/2+) | E(level): From (t,2nγ). Jπ(level): See comment "particle-vibration coupled states (208Pb 4-,5-). | |
| 3406.21 | 13/2+ | XREF: d(3400). E(level): From (t,2nγ). Jπ(level): See comment "particle-vibration coupled states (208Pb 4-,5-). | |
| 3449.7 | (7/2+) | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)4- \ (1974Cl07,1983Ma15). E(level): From (t,2nγ). Jπ(level): See comment "particle-vibration coupled states (208Pb 4-,5-). | |
| 3464.12 | 11/2+ | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)4- \ (1974Cl07,1983Ma15). E(level): From (t,2nγ). Jπ(level): See comment "particle-vibration coupled states (208Pb 4-,5-). | |
| 3467.67 | 19/2+ | E(level): From (t,2nγ). Jπ(level): See comment "particle-vibration coupled states (208Pb 4-,5-). | |
| 3486.93 | (19/2+) | probable configuration=π(1h9/2)+1~#ν(1i11/2+13p1/2- \1) (1983Ma15). | |
| 3502.23 | (15/2+) | configuration=π(1h9/2)+1~#ν(2g9/2+13p1/2-1)4- \ (1974Cl07,1983Ma15). E(level): From (t,2nγ). Jπ(level): See comment "particle-vibration coupled states (208Pb 4-,5-). | |
| 3579.00 | (17/2+:21/2+) | probable configuration=π(1h9/2)+1~#ν(1i11/2+13p1/2- \1) (1983Ma15). | |
| 3597.14 | 19/2+ | configuration=π(1h9/2)+1~#52- or π(1h9/2)+1~#51- (1974Cl07). | |
| 3601.72 | (5/2+,7/2+,9/2+) | probable configuration=π(2f7/2)+1~#3- or π(1h9/2)+1~#5- (1983Ma15). | |
| 3633.85 | 1/2- | XREF: n(3650)R(?). | |
| 3692.14 | (11/2-) | XREF: d(?). | |
| 3703.55 | 7/2(+) | XREF: d(?). | |
| 3752.2 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 3766.9 | (11/2)+ | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 3783.08 | (5/2,7/2,9/2) | Jπ(level): From 1996De48 in (n,n’γ), based on comparisons of the measured γ-yields with the theoretical predictions based on the statistical model of the compound nucleus. | |
| 3812.25 | 23/2+ | probable configuration=π(1h9/2)+1~#ν(2g9/2+12f5/2-1 \) (1983Ma15). | |
| 3839 | 11/2+,13/2+ | XREF: R(3870). | |
| 3884.3 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 3889.5 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 3936.74 | (13/2-) | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 3980.04 | (11/2,13/2)- | configuration=π(1h9/2)+1~#2+ (1974Cl07). | |
| 4000.71 | 9/2+,11/2,13/2- | Jπ(level): From 1996De48 in (n,n’γ), based on comparisons of the measured γ-yields with the theoretical predictions based on the statistical model of the compound nucleus. | |
| 4009.3 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4036.5 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4046.54 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4065 | E(level): L(d,t)=1 from 9- for 4065+4084+4122 peak. | ||
| 4079 | E(level): L(d,t)=1 from 9- for 4065+4084+4122 peak. | ||
| 4088.34 | (5/2:13/2)- | XREF: a(4092). | |
| 4091.4 | (1/2-,3/2-) | configuration=π(1h9/2)+1~#2+ or π(2f5/2)+1 (1974Cl07). | |
| 4096.34 | (9/2+,11/2,13/2-) | XREF: a(4101). | |
| 4134.0 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4148.11 | (9/2+,11/2-) | gΓ2γ0/Γ=0.07 2. | |
| 4158.79 | - | XREF: a(4157). | |
| 4160.9 | (13/2-) | XREF: a(4162). E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 4176.14 | (7/2,9/2,11/2)+ | gΓ2γ0/Γ=0.21 4. | |
| 4207.5 | XREF: a(4210). | ||
| 4222.9 | XREF: h(4220). E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4233.75 | (13/2)- | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 4286 | 15/2-,17/2-,19/2- | XREF: d(4276)R(4270). | |
| 4297.73 | XREF: a(4294). | ||
| 4300.75 | (+) | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 4340.7 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4376.5 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 4397.85 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4409.05 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4415.33 | 1/2- | XREF: L(4421)n(4459). | |
| 4441.7 | (7/2)- | configuration=π(2f7/2)+1 (1970El13). E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 4471.0 | (9/2+,11/2,13/2-) | XREF: a(4469). | |
| 4532 | (13/2-,15/2-) | XREF: n(4543). | |
| 4588.3 | XREF: a(4592). | ||
| 4602.6 | (5/2-,7/2,9/2+) | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 4646.1 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4755.76 | (7/2,9/2,11/2) | gΓ2γ0/Γ=2.8 4. E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| 4796.1 | (7/2,9/2,11/2) | gΓ2γ0/Γ=2.9 5. E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| 4830.3 | (7/2,9/2,11/2) | gΓ2γ0/Γ=1.4 2. E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| 4853.46 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 4967.6 | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | ||
| 5056.7 | (11/2)+ | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 5182.7 | 5/2-,7/2- | XREF: n(5173)U(?). | |
| 5235.1 | (7/2,9/2,11/2) | XREF: a(5241). E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| 5281.9 | (7/2,9/2,11/2) | gΓ2γ0/Γ=5.5 11. E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| 5293.4 | (7/2,9/2,11/2) | gΓ2γ0/Γ=2.2 6. E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| 5312.6 | (7/2,9/2,11/2) | gΓ2γ0/Γ=3.0 9. E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| 5354.0 | (7/2,9/2,11/2) | gΓ2γ0/Γ=3.0 9. E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| 5404.5 | (11/2)+ | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 5424.62 | (9/2+,11/2) | gΓ2γ0/Γ=1.7 5. | |
| 5440.2 | (7/2,9/2,11/2) | gΓ2γ0/Γ=1.6 5. | |
| 5484.4 | (7/2,9/2,11/2) | gΓ2γ0/Γ=4.0 8. E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 5498.0 | (7/2,9/2,11/2) | gΓ2γ0/Γ=4.8 9. E(level): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. Jπ(level): Excitation in (γ,γ’) is probably d (or D+Q). The measured values of gΓ(γ0)2/Γ lead to B(E2)(W.u.)>10. Values this large are not expected for the probable configurations involved. | |
| 5559.6 | (7/2,9/2,11/2) | gΓ2γ0/Γ=2.6 8. | |
| 5652.6 | (11/2)+ | E(level): From Eγ to ground state in (n,n’γ). The placement of the authors is based on the agreement in energy with a previously-known level. Since only a single transition is observed, the existence of the (n,n’γ) level is not definitely established. | |
| 5662.1 | (7/2,9/2,11/2) | gΓ2γ0/Γ=1.6 4. | |
| 6911 | (7/2,9/2,11/2) | gΓ2γ0/Γ=2.4 5. | |
| 6944.8 | (7/2,9/2,11/2) | XREF: U(?). | |
| 6983 | (7/2,9/2,11/2) | gΓ2γ0/Γ=2.6 5. | |
| 7106 | (7/2,9/2,11/2) | gΓ2γ0/Γ=1.0 3. | |
| 7168.1 | 9/2+ | 0.56 fs 3 | XREF: L(7153). |
| 7171 | (7/2,9/2,11/2) | gΓ2γ0/Γ=4.7 10. | |
| 7176.6 | (7/2,9/2,11/2) | XREF: U(?). | |
| 7202 | 11/2+,13/2+ | XREF: n(7200). | |
| 7243.9 | (7/2,9/2,11/2) | gΓ2γ0/Γ=3.7 8. | |
| 7264 | (7/2,9/2,11/2) | gΓ2γ0/Γ=2.4 9. | |
| 7287 | (7/2,9/2,11/2) | gΓ2γ0/Γ=2.6 7. | |
| 7360 | (7/2,9/2,11/2) | gΓ2γ0/Γ=4.3 11. | |
| 10.9E+3 | Γ=2.7 3 %EWSR(E2)=50 30 from (e,n); 90-150 for L=2, or 50-150 for L=2 with 20-40% for L=4 from (α,α’). | ||
| 13450 | Γ=3.89 3 %EWSR=80-120 for L=0 and 30-50 for L=2 with the maximum contribution from L=4 giving %EWSR=15-30 ((α,α’): giant resonance). | ||
| 18627 | 9/2+ | E(level): IAR from 208Pb(p,p’),(pol p,p’). See the IAR source data sets for information on widths. Jπ(level): from 208Pb(p,pol p), analog resonance to the levels in 209Pb. | |
| 19382 | (11/2+) | E(level): IAR from 208Pb(p,p’),(pol p,p’). See the IAR source data sets for information on widths. Jπ(level): from 208Pb(p,pol p), analog resonance to the levels in 209Pb. | |
| 20.10E+3 | (15/2+) | E(level): IAR from 208Pb(p,p’),(pol p,p’). See the IAR source data sets for information on widths. Jπ(level): from 208Pb(p,pol p), analog resonance to the levels in 209Pb. | |
| 20186 | 5/2+ | E(level): IAR from 208Pb(p,p’),(pol p,p’). See the IAR source data sets for information on widths. Jπ(level): from 208Pb(p,pol p), analog resonance to the levels in 209Pb. | |
| 20671 | (1/2+) | E(level): IAR from 208Pb(p,p’),(pol p,p’). See the IAR source data sets for information on widths. Jπ(level): from 208Pb(p,pol p), analog resonance to the levels in 209Pb. | |
| 21114 | 7/2+ | E(level): IAR from 208Pb(p,p’),(pol p,p’). See the IAR source data sets for information on widths. Jπ(level): from 208Pb(p,pol p), analog resonance to the levels in 209Pb. | |
| 21172 | 3/2+ | E(level): IAR from 208Pb(p,p’),(pol p,p’). See the IAR source data sets for information on widths. Jπ(level): from 208Pb(p,pol p), analog resonance to the levels in 209Pb. | |
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 22000 | %EWSR(E2)=200 90 determined in (e,n). E2 or E0 excitation suggested in (e,e’), but observation in (p,γ) rules out E0. Possible isovector E2 giant resonance. |
| E(level) | E(gamma) | Comments |
| 896.28 | 896.28 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. |
| 1608.57 | 1608.53 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. M(γ): A2=+0.47 2 (1978Be17) in (7Li,α2nγ) and A2=+0.42 1 (1983Ma15) in (t,2nγ) |
| 2442.92 | 1546.52 | E(γ): weighted average of 1546.47 5 in (t,2nγ), 1546.7 1 in (n,n’γ) and 1546.2 5 in (d,nγ) M(γ): α(K)exp=0.0054 14 in (d,nγ) (1978El07), γ(θ) is isotropic from (t,2nγ) (1983Ma15) |
| 2492.86 | 49.94 | M(γ): from Jπ difference and RUL. B(E2)(W.u.)(49.94γ) would be 710 if mult were pure E2. This is an unreasonably large value for this mass region | 2492.86 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. |
| 2564.14 | 2564.12 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. M(γ): A2=+0.25 3 (1983Ma15) in (t,2nγ). |
| 2583.02 | 1686.66 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. M(γ): from γ(θ) from (t,2nγ), A2=+0.08 2 (1983Ma15) | 2583.07 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): In (n,n’γ), the 30 1 from 1984Pr08 appears to be an outlier and in weighted average, 46.8 18 from 2008Mi01 in (n,n’γ) is used.. Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. |
| 2599.91 | 2599.9 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. M(γ): (d) from γ(θ) in (t,2nγ). |
| 2600.92 | 992.35 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. M(γ): A2=+0.27 4 in (7Li,α2nγ) (1978Be17), A2=+0.27 2 in (t,2nγ) (1983Ma15). |
| 2617.34 | 124.48 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.05 5 from (t,2nγ) (1983Ma15) | 1721.08 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. M(γ): A2=-0.04 4 from (t,2nγ) (1983Ma15) | 2617.35 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. M(γ): from Coulomb excitation |
| 2741.05 | 140.13 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 1132.46 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). M(γ): A2=-0.12 1, A4=-0.02 3 (1978Be17) in (7Li,α2nγ) | 2741.03 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). M(γ): A2=+0.48 1 (1983Ma15) in (t,2nγ) and A2=+0.42 3 (1978Be17) in (7Li,α2nγ) |
| 2766.66 | 149.3 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 273.80 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 323.74 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.08 4 (1983Ma15) |
| 2826.1 | 1929.9 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. I(γ): weighted average of 33 9 from (t,2nγ), and 48 4 (1984Pr08) and 37.1 19 (2008Mi01) from (n,n’γ). | 2826.0 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation. M(γ): A2=+0.17 5 (1983Ma15) in (t,2nγ). |
| 2845.20 | 78.60 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 402.27 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). |
| 2916.62 | 149.98 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=+0.04 8 (t,2nγ) (1983Ma15) |
| 2955.93 | 110.67 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 338.65 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 463.04 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 513.0 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). |
| E(level) | E(gamma) | Comments |
| 2986.80 | 245.73 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=+0.26 3 in (7Li,α2nγ) (1978Be17), A2=+0.31 5 in (t,2nγ) (1983Ma15), T1/2 rules out M2 |
| 3038.88 | 272.2 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.02 4 (1983Ma15) | 2142.78 | I(γ): from (t,2nγ) M(γ): A2=-0.07 3 (1983Ma15) in (t,2nγ) |
| 3090.16 | 3089.96 | M(γ): A2=+0.10 5 (1983Ma15) |
| 3119.48 | 2223.23 | M(γ): A2=+0.09 5 (1983Ma15) in (t,2nγ) |
| 3132.97 | 1524.2 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 3132.96 | M(γ): A2=-0.24 4 (1983Ma15) in (t,2nγ) |
| 3135.77 | 394.72 | E(γ): From (t,2nγ). I(γ): Other: 17.5 23 (2008Mi01) in (n,n’γ). From (t,2nγ). M(γ): A2=+0.12 8 (1983Ma15) in (t,2nγ) | 1527.13 | M(γ): A2=-0.06 2 (1983Ma15) in (t,2nγ) |
| 3152.83 | 3152.80 | M(γ): A2=+0.26 6 (1983Ma15) in (t,2nγ) |
| 3154.06 | 167.16 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.25 10 (1983Ma15) in (t,2nγ) | 413.04 | M(γ): A2=-0.32 3 (1983Ma15) in (t,2nγ) |
| 3159.33 | 242.73 | E(γ): weighted average of 242.73 5 in (t,2nγ) and 242.7 1 in (3He,dγ) I(γ): weighted average of 92 12 in (t,2nγ) and 55 20 in (3He,dγ) | 314.2 | E(γ): weighted average of 314.2 2 in (t,2nγ) and 314.2 2 in (3He,dγ) I(γ): weighted average of 100 13 in (t,2nγ) and 100 10 in (3He,dγ) M(γ): A2=-0.15 10 (1983Ma15) in (t,2nγ) | 392.56 | E(γ): weighted average of 392.56 10 in (t,2nγ) and 39.5 2 in (3He,dγ) I(γ): weighted average of 72 5 in (t,2nγ) and 40 10 in (3He,dγ) |
| 3169.07 | 1560.49 | M(γ): A2=+0.18 5 (1983Ma15) in (t,2nγ) |
| 3197.60 | 352.30 | E(γ): from (t,2nγ) I(γ): from (3He,dγ) M(γ): A2=+0.03 5 (1983Ma15) in (t,2nγ) |
| 3211.85 | 225.05 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.15 4 (1983Ma15) in (t,2nγ) |
| 3221.65 | 131.45 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 265.74 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 455.02 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.12 10 (1983Ma15) in (t,2nγ) |
| 3269.64 | 424.5 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=+0.14 3 (1983Ma15) in (t,2nγ) |
| 3311.14 | 3310.6 | E(γ): From (n,n’γ). I(γ): from (n,n’γ). The 3310γ is not reported in (t,2nγ); however, there is a peak at this energy in the (t,2nγ) spectrum in 1983Ma15, with Iγ/Iγ(2414γ) estimated by evaluators as ≈0.5. The energy expected from the level scheme is 3311.15 6. From (n,n’γ). |
| 3354.8 | 588.1 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=+0.05 8 (1983Ma15) in (t,2nγ) |
| 3362.00 | 2465.70 | M(γ): A2=-0.01 10 (1983Ma15) in (t,2nγ) |
| E(level) | E(gamma) | Comments |
| 3378.16 | 2481.94 | I(γ): from (n,n’γ). Iγ(2481γ)/Iγ(3378γ)<0.11 is reported in (t,2nγ) | 3378.11 | M(γ): A2=+0.10 5 (1983Ma15) in (t,2nγ) |
| 3393.38 | 1784.8 | E(γ): Other: 1785.9 1 from (n,n’γ) (1984Pr08). From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.21 4 (1983Ma15) in (t,2nγ) |
| 3395.00 | 2498.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 3395.6 | E(γ): observed only in 1996De48. From (n,n’γ). I(γ): From (n,n’γ). |
| 3406.21 | 270.4 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 1797.64 | M(γ): A2=+0.23 4 (1983Ma15) in (t,2nγ) |
| 3449.7 | 2553.4 | E(γ): weighted average of 2553.9 6 in (t,2nγ), 2552.8 2 in (3He,dγ) and 2554.0 2 in (n,n’γ) M(γ): A2=+0.10 17 (1983Ma15) in (t,2nγ) |
| 3464.12 | 3464.09 | M(γ): A2=-0.28 8 (1983Ma15) in (t,2nγ) |
| 3467.67 | 313.70 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): from γ(θ) in (t,2nγ) (1983Ma15) | 480.87 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=+0.43 4 (1983Ma15) in (t,2nγ) |
| 3486.93 | 500.12 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=+0.42 4 (1983Ma15) in (t,2nγ) |
| 3502.23 | 290.38 | E(γ): From (t,2nγ). M(γ): A2=-0.13 8 (1983Ma15) in (t,2nγ) |
| 3505.28 | 921.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 2609.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3541.60 | 2645.3 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 3542.7 | E(γ): From (n,n’γ). I(γ): reported only in (n,n’γ). Branching is too weak to be seen in the (t,2nγ) spectrum. The energy expected from the level scheme is 3541.61 18. From (n,n’γ). |
| 3575.08 | 808.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3579.00 | 592.2 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.36 12 (1983Ma15) in (t,2nγ) |
| 3590.50 | 745.3 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 3597.14 | 443.15 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). | 610.33 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=+0.49 7 (1983Ma15) in (t,2nγ) |
| 3601.72 | 2705.42 | M(γ): A2=-0.29 8 (1983Ma15) in (t,2nγ) | 3601.7 | E(γ): From (n,n’γ). I(γ): reported only in (n,n’γ). Branching is too weak to be seen in the (t,2nγ) spectrum. From (n,n’γ). |
| 3633.85 | 514.37 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) | 677.8 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) | 788.8 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) | 867.2 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) | 1140.8 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) | 1191.0 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| E(level) | E(gamma) | Comments |
| 3703.55 | 664.8 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.25 10 (1983Ma15) in (t,2nγ) | 2806.2 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 3703.4 | E(γ): from (t,2nγ). Eγ=3702.3 1 is reported in (n,n’γ), but this value is inconsistent with E(level) deduced from the 664.8γ |
| 3717.64 | 3717.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3752.2 | 2855.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3759.0 | 2862.7 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 3766.9 | 3766.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3772.60 | 2876.3 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 3783.08 | 2886.78 | E(γ): weighted average of 2887.3 4 in (t,2nγ), 2886.3 3 in (3He,dγ) and 2886.8 1 in (n,n’γ) |
| 3800.85 | 2904.8 | E(γ): weighted average of 2904.5 2 in (n,n’γ) and 2905.1 2 in (3He,dγ) | 3800.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3808.29 | 2199.7 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 3812.25 | 825.45 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=+0.36 7 (1983Ma15) in (t,2nγ) |
| 3816.70 | 2920.4 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 3817.86 | 1253 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 2209.3 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3849.94 | 3849.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3884.3 | 3884.3 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3889.5 | 3889.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3905.9 | 3009.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 3905.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3913.26 | 1420.4 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 3921.22 | 3024.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 3921.2 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3936.74 | 3936.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| E(level) | E(gamma) | Comments |
| 3962.27 | 3066.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 3962.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 3980.04 | 3980.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4000.71 | 2391.8 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4001.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4009.3 | 4009.3 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4036.5 | 4036.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4046.54 | 4046.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4088.34 | 4088.3 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4091.4 | 1648.5 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4096.34 | 2488.2 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4096.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4096.59 | 977.1 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4134.0 | 4134 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4141.95 | 544.85 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.23 7 (1983Ma15) in (t,2nγ) | 654.98 | E(γ): From (t,2nγ). I(γ): From (t,2nγ). M(γ): A2=-0.28 8 (1983Ma15) in (t,2nγ) |
| 4148.11 | 2539.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 3251.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4148.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4158.79 | 3262.8 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4158.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4160.9 | 4160.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4176.14 | 4176.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4207.5 | 4207.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4222.9 | 4222.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| E(level) | E(gamma) | Comments |
| 4233.75 | 4233.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4236.9 | 3340.6 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4262.95 | 4262.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4297.73 | 3401.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4297.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4300.75 | 4300.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4335.3 | 2726.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4340.7 | 4340.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4361.89 | 2753.3 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4376.5 | 4376.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4381.31 | 3485.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4388.15 | 3491.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4387.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4397.85 | 4397.8 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4409.05 | 4409.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4415.33 | 1295.9 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) | 1922.4 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4426.7 | 3530.4 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4441.7 | 3542.6 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) | 4439.1 | E(γ): Other: 4441.6 keV from 208Pb(3He,dγ). From (3He,dγ) I(γ): From (3He,dγ) |
| 4471.0 | 2862.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4470.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4478.2 | 3581.9 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4484.79 | 2876.2 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4506.85 | 4506.8 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| E(level) | E(gamma) | Comments |
| 4515.23 | 2906.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4515.3 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4516.5 | 3620.2 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4588.3 | 3692.1 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) | 4587.8 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4602.6 | 4602.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4646.1 | 4646.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4682.0 | 3785.4 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4682.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4739.62 | 3843.3 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4750.79 | 3854.4 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4750.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4755.76 | 4755.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). M(γ): Excitation in (γ,γ’) is probably d (or D+Q) based on the measured values of gΓ(γ0)2/Γ, which leads to unexpected large B(E2)(W.u.)>10 and rules out the possibilities of pure quadrupole transitions. |
| 4762.3 | 3866.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4762.2 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4786.32 | 3890.0 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4789.8 | 3181.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4790.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4796.1 | 4796.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4830.3 | 4830.2 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). M(γ): Excitation in (γ,γ’) is probably d (or D+Q) based on the measured values of gΓ(γ0)2/Γ, which leads to unexpected large B(E2)(W.u.)>10 and rules out the possibilities of pure quadrupole transitions. |
| 4837.6 | 3941.4 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4837.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4853.46 | 4853.4 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4879.47 | 3983.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4879.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| E(level) | E(gamma) | Comments |
| 4904.2 | 4007.9 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 4948.3 | 4051.8 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 4948.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4967.6 | 4967.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 4996.2 | 4996.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5054.0 | 4157.7 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 5056.7 | 5056.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5152.2 | 4255.9 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 5167.3 | 3558.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 5167.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5182.7 | 5182.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5190.7 | 4294.4 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 5235.1 | 5235.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). M(γ): Excitation in (γ,γ’) is probably d (or D+Q) based on the measured values of gΓ(γ0)2/Γ, which leads to unexpected large B(E2)(W.u.)>10 and rules out the possibilities of pure quadrupole transitions. |
| 5281.9 | 5281.8 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). M(γ): Excitation in (γ,γ’) is probably d (or D+Q) based on the measured values of gΓ(γ0)2/Γ, which leads to unexpected large B(E2)(W.u.)>10 and rules out the possibilities of pure quadrupole transitions. |
| 5292.7 | 2095.1 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) | 2525.6 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 5293.4 | 5293.3 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). M(γ): Excitation in (γ,γ’) is probably d (or D+Q) based on the measured values of gΓ(γ0)2/Γ, which leads to unexpected large B(E2)(W.u.)>10 and rules out the possibilities of pure quadrupole transitions. |
| 5312.6 | 5312.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). M(γ): Excitation in (γ,γ’) is probably d (or D+Q) based on the measured values of gΓ(γ0)2/Γ, which leads to unexpected large B(E2)(W.u.)>10 and rules out the possibilities of pure quadrupole transitions. |
| 5354.0 | 5353.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). M(γ): Excitation in (γ,γ’) is probably d (or D+Q) based on the measured values of gΓ(γ0)2/Γ, which leads to unexpected large B(E2)(W.u.)>10 and rules out the possibilities of pure quadrupole transitions. |
| 5369.8 | 2926.9 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 5404.5 | 5404.4 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5411.2 | 5411.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5424.62 | 3815.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 5424.6 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5440.2 | 5440.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| E(level) | E(gamma) | Comments |
| 5464.6 | 5464.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5484.4 | 5484.3 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). M(γ): Excitation in (γ,γ’) is probably d (or D+Q) based on the measured values of gΓ(γ0)2/Γ, which leads to unexpected large B(E2)(W.u.)>10 and rules out the possibilities of pure quadrupole transitions. |
| 5498.0 | 5497.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). M(γ): Excitation in (γ,γ’) is probably d (or D+Q) based on the measured values of gΓ(γ0)2/Γ, which leads to unexpected large B(E2)(W.u.)>10 and rules out the possibilities of pure quadrupole transitions. |
| 5510.53 | 3902.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 5510.4 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5523.5 | 4627.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 5523.9 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5538.4 | 4641.8 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 5538.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5559.6 | 4663.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). | 5559.8 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5563.4 | 3070.5 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 5570.6 | 5570.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5589.2 | 5589.1 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5609 | 5609 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). M(γ): from γ(θ) and γ(pol) in (γ,γ’) |
| 5609.8 | 4713.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5652.6 | 5652.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 5662.1 | 5662 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 5668.3 | 4772.0 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 5788.7 | 4892.4 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 5925.1 | 5925.0 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 6301.1 | 5404.7 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 6382.0 | 5485.6 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 6392 | 6392 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 6556.1 | 6556 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| E(level) | E(gamma) | Comments |
| 6712.2 | 5815.8 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 6900.5 | 6004.1 | E(γ): From (3He,dγ) I(γ): From (3He,dγ) |
| 6911 | 6911 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 6944.8 | 6944.7 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 6983 | 6983 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 7106 | 7106 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 7168.1 | 7168 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). M(γ): from γ(θ) and γ(pol) in (γ,γ’), δ<0.05 if J(7168)=9/2 and -0.1 if J(7168)=11/2 |
| 7171 | 7171 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 7176.6 | 7176.5 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 7202 | 7202 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 7243.9 | 7243.8 | E(γ): From (n,n’γ). I(γ): From (n,n’γ). |
| 7264 | 7264 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 7279.1 | 7279.0 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 7279+X | 6382 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). | 7279 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 7287 | 7287 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 7360 | 7360 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). |
| 7416.1 | 7416 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). M(γ): A2=+0.20 3 (1969Ra09) in (γ,γ’) |
| 7632.1 | 7632 | E(γ): Weighted average of values from (t,2nγ), (n,n’γ) and Coulomb excitation.. From (γ,γ’) I(γ): From (t,2nγ). M(γ): A2=+0.24 4 (1974Wo05) in (γ,γ’) |
Levels: Each of the six single-particle proton states predicted, on the basis of the shell-model, for 82<N|<126, has been observed in single-particle proton stripping reactions on 208Pb. Except for the 1i13/2 and 3p1/2 members, these states appear to contain most of the single- particle strength. The missing 3p1/2 strength may be concentrated in one of the components of a doublet at 4421+4447 (1970El13; see also 1968Ba34 and 1968El01). The 1i13/2 state at 1608, the only single- particle in the 82<N|<126 shell with positive parity, is expected to have its strength fragmented because of coupling with the positive- parity, particle-vibration states. This state is excited in inelastic scattering with σ≈20% that of the 13/2+ member of the assumed configuration=π(1h9/2)+1~#3- multiplet (1971Un01). Also, the 13/2+ member of the multiplet is excited in single-particle transfer (on 208Pb) with strength ≈10% that of the 13/2+ single-particle level (1967Li09,1968El01).
Levels: See 1974Sc20 for a discussion of core-polarization effects in the structure of the single-proton states as deduced from (p,p’) inelastic scattering. These authors deduce 8% for the admixture of the configuration=π(1h9/2)+1~#3- in the 1i13/2 state
Levels: The group of seven states with E(level)=2492-2741 appear to be well described as a multiplet formed by coupling a 1h9/2 single-particle proton state (209Bi g.s.) with the 3- collective excitation at 2614 in 208Pb. The strongest evidence for this configuration assignment is the excellent agreement between the B(E3) and (β3)2 values for the combined seven states (0.54 7 from Coulomb excitation and 0.11 from (p,p’)) and those for the 3- state in 208Pb (0.58 4 and 0.110) as well as the agreement between the energy of the septuplet centroid (2620 with spins as adopted) and that for the 3- state (2614). The spins of the individual levels in the septuplet have been assigned partly from (p,p’) σ data on the basis of the (2J+1)-rule (1966Ha35), and partly from γ(θ) data in (t,2nγ). The doublet at 2600 was unresolved in (p,p’) and assigned as 11/2+13/2. The doublet was subsequently resolved and the J-assignments of 1966Ha35 confirmed by the Coulomb-excitation data of 1969He07 and 1970Br12 and the (t,2nγ) data of 1983Ma15. See these authors, especially 1970Br12 and 1983Ma15, for a detailed discussion of the spin assignments for the septuplet. From (p,p’) data, 1974Cl07 show that the 3/2+ state at 2492 contains only 64% 7 of the expected strength for the 3/2-member of the multiplet. They suggest that the 2957 level contains an additional 17% 6 of the configuration=π(1h9/2)+1~#3- strength. See also "particle-vibration coupled states (210Po 0+,4+) " below
Levels: The coupling of the 1h9/2 209Bi g.s. to the core states in 208Pb at 3198 (Jπ=5-) and 3475 (Jπ=4-) would result in a decuplet and a nonet of states, respectively. As pointed out by 1974Cl06, these core states are dominated by configuration=ν(2g9/213p1/2-1)2 so that the nineteen states of the decuplet and nonet should be dominated by the configuration=π(1h9/2)+1~#ν(2g9/213p1/2-1)2. 1974Cl06 suggest that an alternate representation of these 19 states is in terms of the coupling of a 3p1/2 neutron hole to the 10 states with J=0- to 9- in 210Bi identified as members of the configuration=π(1h9/2)#ν(2g9/2)) multiplet. (see also 1980Cl05 who, on the basis of the (d,t) reaction on a 9- 210Bi target, suggest that the levels seen in that reaction have a dominant configuration=9-~#ν(nlj)-1 structure). Insofar as this alternate representation is correct, the 19 states should be populated in 209Bi(p,p’) at proton energies corresponding to excitation of isobaric analogs in 210Po. Of the 10 210Bi core states mentioned above, a group of 8 states with energies in the range 2766-3170 in (p,p’) (two states assumed doublets) has been interpreted as the decuplet with configuration=π(1h9/2)+1~#5- (1974Cl06,1974Cl07). These states account for 88% 6 of the 208Pb L=5 strength (1974Cl07). The centroid of the decuplet is at 3090 (with spins as adopted). 1974Cl07 observe that the 2987 19/2+ level contains only 59% 7 of the strength expected for the configuration=π(1h9/2)+1~#5- 19/2+ member of the decuplet, which implies strong fragmentation of this configuration. They suggest that the 3957 level contains most of the missing strength. The spin assignments for the assumed members of the decuplet (except for the 19/2+ level) from 1974Cl06 and 1974Cl07 are based on the strength in 209Bi(p,p’) via direct scattering and in 209Bi(p,p’) via analog resonances. The spin of 19/2+ for the 2987 level suggested by these authors is confirmed by the γ-branching observed by 1978Be17 in 208Pb(7Li,α2nγ) but is in disagreement with that based solely on the (2J+1)-rule in (p,p’) (see 1975Wa03). For other differences between assignments based on the (2J+1)-rule and those of 1974Cl06 and 1974Cl07, see 1975Wa03. Confirming arguments for J are based on γ(θ) in (t,2nγ). α group of 9 states with energies in the range 2919 to 3503 have been interpreted by 1974Cl06 as the above mentioned multiplet with configuration=π(1h9/2)+1~#4-. The spin assignments for the assumed members of this multiplet from 1974Cl06 are based on the strength of resonances in 209Bi(p,p’) excitation functions at energies corresponding to isobaric analogs of states with known spin in 210Bi along with the assumption that the 19 states of the decuplet and nonet exhaust all the spins possible from the two-particle, one-hole configurations involving the 1h9/2 proton and 1g9/2 neutron single-particle and 3p1/2 neutron single-hole states. See 1974Cl06 for detailed assignments. Confirming arguments for J are based on γ(θ) in (t,2nγ). See 1983Ma15 for a calculation of the energies and wave functions for all nineteen states. The calculation is based on the configuration=π(1h9/2)+1~#ν(1g9/213p1/2-1)2. representation
Levels: On the basis of a comparison of experimental energies and spectroscopic factors with values predicted by a core-coupling calculation, 1972Ba81 in (t,α) propose configurations of the type configuration=(0+~#π(nlj)-1)+(3-~#π(nlj)) for several of the states seen in (t,α), as indicated below. The authors also propose configuration=(0+~#π(nlj)-1)+(4+~#π(nlj)-1) for states at 4000 15 and 4120 15. It is not clear whether these correspond to states seen at these energies in other reactions, or whether they are separate states
Levels: For a discussion of particle-vibration coupling involving 208Pb core states other than those discussed above, see 1974Cl06, 1974Cl07, 1975Wa03, and 1983Ma15