ADOPTED LEVELS, GAMMAS for 232U
Author: E. Browne | Citation: Nucl. Data Sheets 107, 2579 (2006) | Cutoff date: 1-Nov-2004
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-2.75×103 keV SY | S(n)= 7268 keV 3 | S(p)= 6104.1 keV 20 | Q(α)= 5413.63 keV 9 | ||
Reference: 2012WA38 |
References: | |||
A | 232Pa β- decay | B | 232Np ε decay |
C | 236Pu α decay | D | 232Th(α,4nγ), 230Th(α,2nγ) |
E | 234U(p,t) |
E(level): Deduced by evaluator from a least squares fit of adopted γ-ray energies, unless otherwise specified.
Jπ(level): Most Jπ assignments are based on rotational band structure. For some individual levels additional arguments based on γ-ray multipolarities are given.
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+ | 68.9 y 4 % α = 100 % SF = 2.7×10-12 6 % 24NE = 8.9×10-10 7 | |||||
47.573 8 | 2+ | 245 ps 20 | 47.57 2 | 100 | E2 | 0 | 0+ |
156.566 10 | 4+ | 108.95 2 | 100 | E2 | 47.573 | 2+ | |
322.69 7 | 6+ | 166.09 7 | 100 | E2 | 156.566 | 4+ | |
541.1 1 | 8+ | 218.4 1 | 100 | E2 | 322.69 | 6+ | |
805.88 16 | 10+ | 264.8 1 | 100 | E2 | 541.1 | 8+ | |
1111.6 2 | 12+ | 305.7 1 | 100 | E2 | 805.88 | 10+ | |
1453.8 3 | 14+ | 342.2 2 | 100 | E2 | 1111.6 | 12+ | |
1828.2 4 | 16+ | 374.4 2 | 100 | E2 | 1453.8 | 14+ | |
2231.6 6 | 18+ | 403.4 5 | 100 | E2 | 1828.2 | 16+ | |
2659.8 9 | (20+) | 428.2 6 | 100 | (E2) | 2231.6 | 18+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - Kπ=0- Octupole vibrational band | |||||||
563.194 7 | 1- | ||||||
628.965 8 | 3- | 472.390 6 581.398 8 | 64 2 100 3 | E1 E1 | 156.566 47.573 | 4+ 2+ | |
746.8 1 | (5-) | 423.85 20 590.28 10 | 35 2 100 6 | 322.69 156.566 | 6+ 4+ | ||
915.2 4 | (7-) | 374.2 5 592.4 5 | | 541.1 322.69 | 8+ 6+ | ||
1131.1 6 | (9-) | 590.0 5 | 100 | 541.1 | 8+ | ||
1390.9 6 | 11- | 585.0 5 | 100 | 805.88 | 10+ | ||
2023.2 1 | (15-) | 569.4 | 100 | [E1] | 1453.8 | 14+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - Kπ=0+ Beta vibrational band | |||||||
691.42 9 | 0+ | ||||||
734.57 5 | 2+ | 577.95 10 687.04 10 734.55 10 S | 39 7 75 3 100 4 | E0+[E2] [E2] | 156.566 47.573 0 | 4+ 2+ 0+ | |
833.07 20 | 4+ | 676.5 2 | | E0+[E2] | 156.566 | 4+ | |
984.9 2 | 6+ | 662.2 2 | | E0 | 322.69 | 6+ | |
1186.6 4 | 8+ | 645.5 3 | | E0 | 541.1 | 8+ | |
1434.3 5 | 10+ | 628.4 4 | | E0 | 805.88 | 10+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - Kπ=2+ Gamma vibrational band | |||||||
866.790 8 | 2+ | ||||||
911.49 4 | (3)+ | 176.3 754.8 2 863.89 4 911.4? | 0.2 1 28 2 100 4 0.60 5 | M1,E2 E2 E2 [M3] | 734.57 156.566 47.573 0 | 2+ 4+ 2+ 0+ | |
970.71 7 | (4+) | 814.2 1 923.1 | 100 30 45 14 | 156.566 47.573 | 4+ 2+ | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 5 - Kπ=2- | |||||||
1016.850 8 | 2- | < 50 ps | |||||
1050.90 1 | 3- | < 50 ps | 80.23 10 139.2 1 184.101 9 421.932 7 894.351 12 1003.28 4 1051.4 1 | 2.7 4 4.7 3 11.8 3 12.7 10 100.0 15 0.80 4 0.087 10 | [E1] [E1] [E1] E2+M1 E1 E1 [E3] | 970.71 911.49 866.790 628.965 156.566 47.573 0 | (4+) (3)+ 2+ 3- 4+ 2+ 0+ |
1098.2 4 | (4-) | 941.6 4 | 100 | 156.566 | 4+ | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 6 - Kπ=(1)- | |||||||
1173.06 17 | (2)- | ||||||
1211.3 3 | 3- | 1054.5 3 1164.5 5 | 100 6 23 4 | E1 E1 | 156.566 47.573 | 4+ 2+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 7 - Kπ=(0+) Two-phonon octupole vibrational band | |||||||
927.3 1 | (0+) | ||||||
967.6 1 | (2)+ | 338.5 1 404.46 10 811.26 20 920.23 20 967.9 3 | 100 2 76 2 13.0 2 13.0 2 5 1 | [E1] [E1] [E2] M1+E2 [E2] | 628.965 563.194 156.566 47.573 0 | 3- 1- 4+ 2+ 0+ |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
47.573 | 2+ | 245 ps 20 | 47.57 2 | E2 | 464 | B(E2)(W.u.)=241 21, α=464 | |
156.566 | 4+ | 108.95 2 | E2 | 9.15 | α=9.15 | ||
322.69 | 6+ | 166.09 7 | E2 | 1.58 | α=1.58 | ||
541.1 | 8+ | 218.4 1 | E2 | 0.554 | α=0.554 | ||
563.194 | 1- | 515.607 9 | E1 | 0.01274 | α=0.01274 | ||
1- | 563.197 7 | E1 | 0.01074 | α=0.01074 | |||
628.965 | 3- | 472.390 6 | E1 | 0.01516 | α=0.01516 | ||
3- | 581.398 8 | E1 | 0.01010 | α=0.01010 | |||
691.42 | 0+ | 643.87 3 | [E2] | 0.027 | α=0.027 | ||
805.88 | 10+ | 264.8 1 | E2 | 0.286 | α=0.286 | ||
866.790 | 2+ | 132.5 2 | M1,E2 | 7 | α=7 3 | ||
2+ | 174.9 2 | [E2] | 1.268 | α=1.268 | |||
2+ | 710.1 3 | E2 | 0.02206 | α=0.02206 | |||
2+ | 819.187 13 | E2 | 0.017 | α=0.017 | |||
2+ | 866.760 19 | E2 | 0.01484 | α=0.01484 | |||
911.49 | (3)+ | 176.3 | M1,E2 | 3.0 | α=3.0 17 | ||
(3)+ | 754.8 2 | E2 | 0.01950 | α=0.01950 | |||
(3)+ | 863.89 4 | E2 | 0.01494 | α=0.01494 | |||
(3)+ | 911.4 | [M3] | 0.2282 | α=0.2282 | |||
927.3 | (0+) | 364.0 1 | [E1] | 0.0260 | α=0.0260, α(K)=0.0208, α(L)=0.00392, α(M)=0.00094, α(N+)=0.00033 | ||
(0+) | 879.9 1 | [E2] | 0.0144 | α=0.0144, α(K)=0.0106, α(L)=0.00284 | |||
967.6 | (2)+ | 338.5 1 | [E1] | 0.0304 | α=0.0304, α(K)=0.0243, α(L)=0.00462, α(M)=0.00110, α(N+)=0.00039 | ||
(2)+ | 404.46 10 | [E1] | 0.0209 | α=0.0209, α(K)=0.0168, α(L)=0.00310, α(M)=0.00074, α(N+)=0.00026 | |||
(2)+ | 811.26 20 | [E2] | 0.0169 | α=0.0169, α(K)=0.0123, α(L)=0.00348 | |||
(2)+ | 920.23 20 | M1+E2 | 1.14 20 | 0.030 | α=0.030 4, α(K)=0.024 3, α(L)=0.0049 6 | ||
(2)+ | 967.9 3 | [E2] | 0.0120 | α=0.0120, α(K)=0.0090, α(L)=0.00226 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
1016.850 | 2- | < 50 ps | 105.4 1 | [E1] | 0.1102 | α=0.1102 | |
2- | < 50 ps | 150.059 3 | E1 | 0.1962 | α=0.1962 | ||
2- | < 50 ps | 282.2 1 | [E1] | 0.0452 | α=0.0452 | ||
2- | < 50 ps | 387.884 4 | E2+M1 | 4.6 5 | 0.111 | α=0.111 5 | |
2- | < 50 ps | 453.655 5 | E2+M1 | 2.8 3 | 0.093 | α=0.093 7 | |
2- | < 50 ps | 969.315 11 | E1 | 0.00397 | α=0.00397 | ||
2- | < 50 ps | 1016.4 4 | M2 | 0.0915 | α=0.0915 | ||
1050.90 | 3- | < 50 ps | 80.23 10 | [E1] | 0.2255 | α=0.2255 | |
3- | < 50 ps | 139.2 1 | [E1] | 0.2327 | α=0.2327 | ||
3- | < 50 ps | 184.101 9 | [E1] | 0.1208 | α=0.1208 | ||
3- | < 50 ps | 421.932 7 | E2+M1 | 1.96 15 | 0.145 | α=0.145 1 | |
3- | < 50 ps | 894.351 12 | E1 | 0.00457 | α=0.00457 | ||
3- | < 50 ps | 1003.28 4 | E1 | 0.00373 | α=0.00373 | ||
3- | < 50 ps | 1051.4 1 | [E3] | 0.026 | α=0.026 | ||
1111.6 | 12+ | 305.7 1 | E2 | 0.182 | α=0.182 | ||
1173.06 | (2)- | 1125.48 17 | E1 | 0.003 | α=0.003 | ||
1194.0 | (3+,4+) | 143.4 5 | [E1] | .22 | α=.22 | ||
(3+,4+) | 223.6 4 | [E2] | .51 | α=.51 | |||
(3+,4+) | 282.0 4 | [E2] | 0.23 | α=0.23 | |||
(3+,4+) | 327.3 3 | [E2] | 0.148 | α=0.148 | |||
1211.3 | 3- | 1054.5 3 | E1 | 0.00342 | α=0.00342 | ||
3- | 1164.5 5 | E1 | 0.00289 | α=0.00289 | |||
1453.8 | 14+ | 342.2 2 | E2 | 0.1297 | α=0.1297 | ||
1828.2 | 16+ | 374.4 2 | E2 | 0.1007 | α=0.1007 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0 | 0+ | 68.9 y 4 % α = 100 % SF = 2.7×10-12 6 % 24NE = 8.9×10-10 7 | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. |
47.573 | 2+ | 245 ps 20 | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. |
156.566 | 4+ | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. | |
322.69 | 6+ | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. | |
541.1 | 8+ | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. | |
563.194 | 1- | E(level): Kπ=0- Octupole vibrational band. Jπ(level): Rotational band structure, γ-ray deexcitation. | |
628.965 | 3- | E(level): Kπ=0- Octupole vibrational band. Jπ(level): Rotational band structure, γ-ray deexcitation. | |
691.42 | 0+ | E(level): Kπ=0+ Beta vibrational band. | |
734.57 | 2+ | E(level): Kπ=0+ Beta vibrational band. | |
746.8 | (5-) | E(level): Kπ=0- Octupole vibrational band. Jπ(level): Rotational band structure, γ-ray deexcitation. | |
805.88 | 10+ | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. | |
833.07 | 4+ | E(level): Kπ=0+ Beta vibrational band. | |
866.790 | 2+ | E(level): Kπ=2+ Gamma vibrational band. | |
911.49 | (3)+ | E(level): Kπ=2+ Gamma vibrational band. | |
915.2 | (7-) | E(level): Kπ=0- Octupole vibrational band. Jπ(level): Rotational band structure, γ-ray deexcitation. | |
927.3 | (0+) | E(level): Kπ=(0+) Two-phonon octupole vibrational band. | |
967.6 | (2)+ | E(level): Kπ=(0+) Two-phonon octupole vibrational band. | |
970.71 | (4+) | E(level): Kπ=2+ Gamma vibrational band. | |
984.9 | 6+ | E(level): Kπ=0+ Beta vibrational band. | |
1016.850 | 2- | < 50 ps | E(level): Kπ=2-. |
1050.90 | 3- | < 50 ps | E(level): Kπ=2-. |
1098.2 | (4-) | E(level): Kπ=2-. | |
1111.6 | 12+ | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. | |
1131.1 | (9-) | E(level): Kπ=0- Octupole vibrational band. Jπ(level): Rotational band structure, γ-ray deexcitation. | |
1173.06 | (2)- | E(level): Kπ=(1)-. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
1186.6 | 8+ | E(level): Kπ=0+ Beta vibrational band. | |
1194.0 | (3+,4+) | 2-neutron level from low log ft in 232Np ε decay; possible configuration=((ν 5/2[633])(ν 3/2[631])) resulting in Jπ=4+ (suggesting that the 1193.9γ is misplaced). It compares with log|ft’s≈5.3 for analogous transitions in the decays of 233Np and 235Pu (π 5/2[642]) to (ν 5/2[633]). No other log ft’s in the actinide region are that low. E(level): 2-neutron level from low log ft in 232Np ε decay; possible configuration=((ν 5/2[633])(ν 3/2[631])) resulting in Jπ=4+ (suggesting that the 1193.9γ is misplaced). It compares with log|ft’s≈5.3 for analogous transitions in the decays of 233Np and 235Pu (π 5/2[642]) to (ν 5/2[633]). No other log ft’s in the actinide region are that low. | |
1211.3 | 3- | E(level): Kπ=(1)-. | |
1227 | E(level): From 234U(p,t). | ||
1277.2 | 0+ | E(level): From 234U(p,t). | |
1301 | E(level): From 234U(p,t). | ||
1349 | E(level): From 234U(p,t). | ||
1390.9 | 11- | E(level): Kπ=0- Octupole vibrational band. Jπ(level): Rotational band structure, γ-ray deexcitation. | |
1434.3 | 10+ | E(level): Kπ=0+ Beta vibrational band. | |
1438 | E(level): From 234U(p,t). | ||
1453.8 | 14+ | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. | |
1482.0 | 0+ | E(level): From 234U(p,t). | |
1489 | E(level): From 234U(p,t). | ||
1520 | E(level): From 234U(p,t). | ||
1569.0 | 0+ | E(level): From 234U(p,t). | |
1600 | E(level): From 234U(p,t). | ||
1746 | E(level): From 234U(p,t). | ||
1772 | E(level): From 234U(p,t). | ||
1797.0 | 0+ | E(level): From 234U(p,t). | |
1822.1 | 0+ | E(level): From 234U(p,t). | |
1828.2 | 16+ | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. | |
1861.5 | 0+ | E(level): From 234U(p,t). | |
1872 | E(level): From 234U(p,t). | ||
1931.8 | 0+ | E(level): From 234U(p,t). | |
1972 | E(level): From 234U(p,t). | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
1979 | E(level): From 234U(p,t). | ||
1998 | E(level): From 234U(p,t). | ||
2023.2 | (15-) | E(level): Kπ=0- Octupole vibrational band. Jπ(level): Rotational band structure, γ-ray deexcitation. | |
2043 | E(level): From 234U(p,t). | ||
2061 | E(level): From 234U(p,t). | ||
2072 | E(level): From 234U(p,t). | ||
2147 | E(level): From 234U(p,t). | ||
2172 | E(level): From 234U(p,t). | ||
2204 | E(level): From 234U(p,t). | ||
2231.6 | 18+ | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. | |
2284 | E(level): From 234U(p,t). | ||
2333 | E(level): From 234U(p,t). | ||
2659.8 | (20+) | E(level): Kπ=0+ GS rotational band. Jπ(level): Rotational band structure, γ-ray cascade of stretched E2 transitions in 232Th(α,4nγ) and Coulomb excitation. |
E(level) | E(gamma) | Comments |
47.573 | 47.57 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay |
156.566 | 108.95 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay |
322.69 | 166.09 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay |
541.1 | 218.4 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
563.194 | 515.607 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 563.197 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
628.965 | 472.390 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 581.398 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
691.42 | 643.87 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay | 691.3 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay |
734.57 | 577.95 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay | 687.04 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay | 734.55 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay |
746.8 | 423.85 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay | 590.28 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay |
805.88 | 264.8 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
833.07 | 676.5 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
866.790 | 132.5 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 174.9 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 710.1 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 819.187 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 866.760 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
911.49 | 176.3 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 754.8 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 863.89 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 911.4 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
E(level) | E(gamma) | Comments |
915.2 | 374.2 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) | 592.4 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
927.3 | 364.0 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay | 879.9 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay |
967.6 | 338.5 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay | 404.46 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay | 811.26 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay | 920.23 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay | 967.9 | E(γ): From 236Pu α decay I(γ): From 236Pu α decay |
970.71 | 814.2 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 923.1 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
984.9 | 662.2 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
1016.850 | 105.4 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 150.059 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 387.884 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 453.655 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 969.315 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 1016.4 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
1050.90 | 80.23 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 139.2 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 184.101 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 421.932 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 894.351 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 1003.28 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 1051.4 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
E(level) | E(gamma) | Comments |
1098.2 | 941.6 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
1111.6 | 305.7 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
1131.1 | 590.0 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
1132.97 | 1085.4 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay M(γ): E1 or E2. Decay scheme requires E2. | 1132.7 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay M(γ): E1 or E2. Decay scheme requires E2. |
1173.06 | 1125.48 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
1186.6 | 645.5 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
1194.0 | 143.4 | E(γ): From 232Np ε decay I(γ): From 232Np ε decay | 223.6 | E(γ): From 232Np ε decay I(γ): From 232Np ε decay | 282.0 | E(γ): From 232Np ε decay I(γ): From 232Np ε decay | 327.3 | E(γ): From 232Np ε decay I(γ): From 232Np ε decay | 1037.4 | E(γ): From 232Np ε decay I(γ): From 232Np ε decay | 1146.3 | E(γ): From 232Np ε decay I(γ): From 232Np ε decay | 1193.9 | E(γ): From 232Np ε decay I(γ): From 232Np ε decay |
1211.3 | 1054.5 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay | 1164.5 | E(γ): From 232Pa β- decay I(γ): From 232Pa β- decay |
1390.9 | 585.0 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
1434.3 | 628.4 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
1453.8 | 342.2 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
1828.2 | 374.4 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
2023.2 | 569.4 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
2231.6 | 403.4 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
2659.8 | 428.2 | E(γ): From 232Th(α,4nγ), 230Th(α,2nγ) I(γ): From 232Th(α,4nγ), 230Th(α,2nγ) |
233U(γ,n): measured cross-section (1993De36).
T1/2(24Ne):Others (mostly theoretical papers and systematic studies of cluster decay): 2004Re22, 2004He16, 2004Ba64, 2002Sa25, 2002Du16, 2002Ba80), 2001St29, 1998Ro11, 1997Tr17, 1997Ro24, 1997MiZP, 1997Bu20, 1995Ar33, 1993Si26, 1993Ka21, 1993Go18, 1993Bu05, 1992Sa30, 1992Lu07, 1992Gu10, 1992Ar02, 1991Ro03, 1991Bu01, 1991Bl07, 1990Sh01, 1990Ka15, 1990Bu13, 1990Ba20.
Q-value: Note: Current evaluation has used the following Q record -2750 syst 7268.0 28 6104 2 5413.63 9 2003Au03