ADOPTED LEVELS, GAMMAS for 133Cs
Authors: Yu. Khazov and A. Rodionov, F.G. Kondev | Citation: Nucl. Data Sheets 112, 855 (2011) | Cutoff date: 31-Oct-2010
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-517.3 keV 10 | S(n)= 8986.0 keV 20 | S(p)= 6080.940 keV 10 | Q(α)= -1989 keV 4 | ||
Reference: 2012WA38 |
References: | |||
A | 133Xe β- decay (5.2475 d) | B | 133Ba ε decay (10.551 Y) |
C | 133Ba ε decay (38.93 H) | D | 130Te(6Li,3nγ) |
E | 133Cs(n,n’γ) | F | Coulomb Excitation |
G | 133Cs(γ,γ’) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCDEFG | 7/2+ | STABLE | |||||
80.9979 8 | AB DEF | 5/2+ | 6.283 ns 14 | 80.9979 11 | 100 | M1+E2 | 0.0 | 7/2+ |
160.6121 9 | AB EF | 5/2+ | 172 ps 4 | 79.6142 12 160.6120 16 | 100.0 19 24.07 19 | M1+E2 M1+E2 | 80.9979 0.0 | 5/2+ 7/2+ |
383.8491 8 | AB DEF | 3/2+ | 44 ps 11 | 223.2368 13 302.8508 5 383.8485 12 | 2.47 2 100.0 3 48.8 3 | M1+E2 M1+E2 E2 | 160.6121 80.9979 0.0 | 5/2+ 5/2+ 7/2+ |
437.0113 9 | B EF | 1/2+ | ≤ 150 ps | 53.1622 6 276.3989 12 356.0129 7 | 3.53 3 11.54 7 100.0 | M1+E2 E2 E2 | 383.8491 160.6121 80.9979 | 3/2+ 5/2+ 5/2+ |
632.56 10 | CDEF | 11/2+ | 5.3 ps 4 | 632.56 10 | 100 | E2 | 0.0 | 7/2+ |
640.40 7 | EF | (3/2)+ | 0.76 ps 14 | 480.03 10 559.14 10 641 1 S | 100 15 96 12 4 | M1+E2 M1+E2 [E2] | 160.6121 80.9979 0.0 | 5/2+ 5/2+ 7/2+ |
705.57 9 | DEF | 9/2+ | 624.58 10 705.56 15 | 100 28 3 | E2 | 80.9979 0.0 | 5/2+ 7/2+ | |
729.16 25 | E | 647.8 4 728.2 5 | 29 4 100 | 80.9979 0.0 | 5/2+ 7/2+ | |||
767.68 10 | DEF | (9/2)+ | 2.0 ps 4 | 606.9 5 767.68 10 | 9 1 100 | (E2) (M1+E2) | 160.6121 0.0 | 5/2+ 7/2+ |
788.6 3 ? | EF | 788.6 3 | 100 | 0.0 | 7/2+ | |||
819.06 7 | EF | (5/2,7/2,9/2+) | 1.0 ps 3 | 658.61 10 737.4 6 818.92 10 | 61 9 43 9 100 17 | 160.6121 80.9979 0.0 | 5/2+ 5/2+ 7/2+ | |
871.86 10 | EF | (7/2)+ | 1.2 ps 3 | 712.6 5 871.80 10 | 18 100 | M1+E2 | 160.6121 0.0 | 5/2+ 7/2+ |
916.09 7 | EF | (5/2,7/2,9/2+) | 2.3 ps +10-5 | 755.58 10 834.9 3 916.00 10 | 100 15 33 4 85 15 | 160.6121 80.9979 0.0 | 5/2+ 5/2+ 7/2+ | |
941.6 6 | EF | 861.1 7 940.8 9 | 100 12 38 10 | 80.9979 0.0 | 5/2+ 7/2+ | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1071.1 4 | DE | (11/2-) | 303.4 3 365.95 10 | <19 100 | D D+Q | 767.68 705.57 | (9/2)+ 9/2+ | |
1089.25 9 | E | (3/2+,5/2,7/2+) | 705.56 15 928.54 10 1009.6 14 1090.8 13 | 100 12 10.9 16 4.1 9 3.1 7 | 383.8491 160.6121 80.9979 0.0 | 3/2+ 5/2+ 5/2+ 7/2+ | ||
1172.69 20 | E | (3/2+,5/2,7/2+) | 788.8 2 1174.1 12 | 100 7 21 10 | 383.8491 0.0 | 3/2+ 7/2+ | ||
1219.33 22 ? | E | 347.5 2 1218.7 11 | 100 15 87 25 | 871.86 0.0 | (7/2)+ 7/2+ | |||
1429.9 4 | D | 15/2+ | 797.3 3 | 100 | E2 | 632.56 | 11/2+ | |
1442.22 14 ? | E | 674.54 10 | 100 | 767.68 | (9/2)+ | |||
1509.6 3 | E | 780.4 1 1510.6 4 | 100 7 55 19 | 729.16 0.0 | 7/2+ | |||
1603.9 4 | D | (15/2-) | 532.78 9 | 100 | E2 | 1071.1 | (11/2-) | |
1674.65 22 | E | (5/2+,7/2+) | 969.1 2 1033.5 15 1674.2 13 | 100 8 15 8 50 23 | 705.57 640.40 0.0 | 9/2+ (3/2)+ 7/2+ | ||
1692.4 11 ? | E | 1610.3 16 1693.4 15 | 59 30 100 40 | 80.9979 0.0 | 5/2+ 7/2+ | |||
1744.8 5 | D | (15/2-) | 673.7 3 | 100 | E2 | 1071.1 | (11/2-) | |
1880.6 3 | E | (3/2+,5/2,7/2+) | 1496.9 3 1879.7 8 | 100 33 57 27 | 383.8491 0.0 | 3/2+ 7/2+ | ||
1919.4 11 ? | E | 1046.4 15 1132.2 16 1919.5 5 ? | 100 20 29 13 28 16 | 871.86 788.6 0.0 | (7/2)+ 7/2+ | |||
1923.0 5 | D | (19/2) | 319.1 3 | 100 | Q | 1603.9 | (15/2-) | |
1951.5 5 | D | (17/2) | 347.6 3 | 100 | D+Q | 1603.9 | (15/2-) | |
2001.4 17 ? | E | 1272.2 16 2002.3 11 ? | 100 50 67 30 | 729.16 0.0 | 7/2+ | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2035.6 8 ? | E | (3/2+,5/2,7/2+) | 1306.6 13 1652.2 17 2035.3 12 | 61 30 100 50 25 11 | 729.16 383.8491 0.0 | 3/2+ 7/2+ | ||
2156.2 9 | G | (5/2,7/2,9/2) | 1.34×10-3 eV 22 | 937.0 15 1066.4 14 2156.9 17 | 21 7 100 30 26 13 | (D) (D) (D) | 1219.33 1089.25 0.0 | (3/2+,5/2,7/2+) 7/2+ |
2295.1 5 | D | 19/2+ | 865.2 3 | 100 | E2 | 1429.9 | 15/2+ | |
2321.0 8 | G | (5/2) | 8.4×10-4 eV 19 | 1404.6 14 1937.3 9 | 100 50 65 40 | (D) (D) | 916.09 383.8491 | (5/2,7/2,9/2+) 3/2+ |
2415 | G | (5/2,7/2,9/2) | 2.7×10-3 eV 4 | |||||
2438 | G | (5/2,7/2,9/2) | 1.5×10-3 eV 3 | |||||
2462 | G | (5/2,7/2,9/2) | 1.10×10-3 eV 22 | |||||
2528.3 6 | D | (21/2) | 233.2 3 | 100 | D | 2295.1 | 19/2+ | |
2643.4 6 | D | (23/2) | 115.1 3 | 100 | D | 2528.3 | (21/2) | |
2645 | G | (5/2,7/2,9/2) | 5.1×10-3 eV 4 | |||||
2672 | G | (5/2,7/2,9/2) | 2.4×10-3 eV 3 | |||||
2722 | G | (5/2,7/2,9/2) | 2.4×10-3 eV 5 | |||||
2744 | G | (5/2,7/2,9/2) | 3.5×10-3 eV 5 | |||||
2759 | G | (5/2,7/2,9/2) | 3.1×10-3 eV 4 | |||||
2815 | G | (5/2,7/2,9/2) | 1.0×10-3 eV 3 | |||||
2834.2 7 | D | (25/2) | 190.8 3 | 100 | D+Q | 2643.4 | (23/2) | |
2858 | G | (5/2,7/2,9/2) | 2.8×10-3 eV 5 | |||||
2873 | G | (5/2,7/2,9/2) | 2.6×10-3 eV 3 | |||||
2909 | G | (5/2,7/2,9/2) | 4.9×10-3 eV 6 | |||||
2944 | G | (5/2,7/2,9/2) | 2.3×10-3 eV 3 | |||||
3039 | G | (5/2,7/2,9/2) | 9.7×10-4 eV 24 | |||||
3296 | G | (5/2,7/2,9/2) | 1.8×10-3 eV 6 | |||||
3322 | G | (5/2,7/2,9/2) | 1.4×10-3 eV 4 | |||||
3422 | G | (5/2,7/2,9/2) | 1.7×10-3 eV 6 | |||||
3517 | G | (5/2,7/2,9/2) | 1.4×10-3 eV 5 | |||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3526 | G | (5/2,7/2,9/2) | 3.3×10-3 eV 5 | |||||
3672 | G | (5/2,7/2,9/2) | 3.2×10-3 eV 7 |
E(level): From a least-squares fit to Eγ’s
T1/2(level): For levels with E|>2156.2 keV from 133Cs(γ,γ’), quoted gΓ0 in eV
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - ΔJ=2 band based on 7/2+ (π(g7/2+1)) g.s. | |||||||
0.0 | 7/2+ | STABLE | |||||
632.56 10 | 11/2+ | 5.3 ps 4 | 632.56 10 | 100 | E2 | 0.0 | 7/2+ |
1429.9 4 | 15/2+ | 797.3 3 | 100 | E2 | 632.56 | 11/2+ | |
2295.1 5 | 19/2+ | 865.2 3 | 100 | E2 | 1429.9 | 15/2+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - ΔJ=2 band based on the 11/2- (π(h11/2+1)) state | |||||||
1071.1 4 | (11/2-) | ||||||
1744.8 5 | (15/2-) | 673.7 3 | 100 | E2 | 1071.1 | (11/2-) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
80.9979 | 5/2+ | 6.283 ns 14 | 80.9979 11 | M1+E2 | 0.158 5 | 1.703 | B(E2)(W.u.)=5.8 4, B(M1)(W.u.)=0.002381 22, α=1.703, α(K)=1.431 20, α(L)=0.216 4, α(M)=0.0447 8, α(N)=0.00939 16, α(O)=0.001271 20, α(P)=5.56E-5 8, α(N+)=0.01071 18 |
160.6121 | 5/2+ | 172 ps 4 | 79.6142 12 | M1+E2 | 0.124 15 | 1.77 | B(E2)(W.u.)=1.3×102 3, B(M1)(W.u.)=0.081 4, α=1.77 3, α(K)=1.495 22, α(L)=0.217 6, α(M)=0.0447 13, α(N)=0.00940 25, α(O)=0.00128 3, α(P)=5.84E-5 9, α(N+)=0.0107 3 |
5/2+ | 172 ps 4 | 160.6120 16 | M1+E2 | 0.96 5 | 0.294 | B(E2)(W.u.)=28.6 18, B(M1)(W.u.)=0.00126 8, α=0.294 6, α(K)=0.234 4, α(L)=0.0471 13, α(M)=0.0099 3, α(N)=0.00205 6, α(O)=0.000261 7, α(P)=8.08E-6 12, α(N+)=0.00232 7 | |
383.8491 | 3/2+ | 44 ps 11 | 223.2368 13 | M1+E2 | -0.114 14 | 0.0975 | B(E2)(W.u.)=0.12 4, B(M1)(W.u.)=0.00070 18, α=0.0975, α(K)=0.0836 12, α(L)=0.01103 16, α(M)=0.00226 4, α(N)=0.000477 7, α(O)=6.64E-5 10, α(P)=3.26E-6 5, α(N+)=0.000547 8 |
3/2+ | 44 ps 11 | 302.8508 5 | M1+E2 | 0.022 20 | 0.0434 | B(E2)(W.u.)=0.04 +7-4, B(M1)(W.u.)=0.011 3, α=0.0434, α(K)=0.0373 6, α(L)=0.00484 7, α(M)=0.000988 14, α(N)=0.000209 3, α(O)=2.92E-5 4, α(P)=1.453E-6 21, α(N+)=0.000240 4 | |
3/2+ | 44 ps 11 | 383.8485 12 | E2 | 0.0202 | B(E2)(W.u.)=12 3, α=0.0202, α(K)=0.01684 24, α(L)=0.00270 4, α(M)=0.000560 8, α(N)=0.0001166 17, α(O)=1.541E-5 22, α(P)=5.90E-7 9, α(N+)=0.0001326 19 | ||
437.0113 | 1/2+ | ≤ 150 ps | 53.1622 6 | M1+E2 | 0.08 +2-3 | 5.66 | B(E2)(W.u.)>18, B(M1)(W.u.)>0.024, α=5.66 10, α(K)=4.78 7, α(L)=0.70 4, α(M)=0.144 8, α(N)=0.0303 16, α(O)=0.00413 18, α(P)=0.000188 3, α(N+)=0.0346 18 |
1/2+ | ≤ 150 ps | 276.3989 12 | E2 | 0.0566 | B(E2)(W.u.)>4.8, α=0.0566, α(K)=0.0460 7, α(L)=0.00842 12, α(M)=0.001763 25, α(N)=0.000365 6, α(O)=4.70E-5 7, α(P)=1.545E-6 22, α(N+)=0.000414 6 | ||
1/2+ | ≤ 150 ps | 356.0129 7 | E2 | 0.0254 | B(E2)(W.u.)>12, α=0.0254, α(K)=0.0211 3, α(L)=0.00346 5, α(M)=0.000721 10, α(N)=0.0001499 21, α(O)=1.97E-5 3, α(P)=7.32E-7 11, α(N+)=0.0001704 24 | ||
632.56 | 11/2+ | 5.3 ps 4 | 632.56 10 | E2 | 0.00503 | B(E2)(W.u.)=26.1 20, α=0.00503 7, α(K)=0.00428 6, α(L)=0.000599 9, α(M)=0.0001230 18, α(N)=2.58E-5 4, α(O)=3.51E-6 5, α(P)=1.563E-7 22, α(N+)=2.95E-5 5 | |
640.40 | (3/2)+ | 0.76 ps 14 | 480.03 10 | M1+E2 | -0.10 3 | 0.01337 | B(E2)(W.u.)=3.6 23, B(M1)(W.u.)=0.13 4, α=0.01337, α(K)=0.01153 17, α(L)=0.001473 21, α(M)=0.000301 5, α(N)=6.36E-5 9, α(O)=8.89E-6 13, α(P)=4.45E-7 7, α(N+)=7.29E-5 11 |
(3/2)+ | 0.76 ps 14 | 559.14 10 | M1+E2 | 1.3 +10-6 | 0.0078 | B(E2)(W.u.)=1.0×102 7, B(M1)(W.u.)=0.03 3, α=0.0078 7, α(K)=0.0066 7, α(L)=0.00091 5, α(M)=0.000186 10, α(N)=3.91E-5 22, α(O)=5.4E-6 4, α(P)=2.5E-7 3, α(N+)=4.5E-5 3 | |
(3/2)+ | 0.76 ps 14 | 641 1 | [E2] | 0.00487 | B(E2)(W.u.)=3.4 7, α=0.00487 7, α(K)=0.00414 6, α(L)=0.000577 9, α(M)=0.0001186 18, α(N)=2.49E-5 4, α(O)=3.39E-6 5, α(P)=1.513E-7 22, α(N+)=2.84E-5 5 | ||
705.57 | 9/2+ | 624.58 10 | E2 | 0.00520 | α=0.00520 8, α(K)=0.00442 7, α(L)=0.000620 9, α(M)=0.0001273 18, α(N)=2.67×10-5 4, α(O)=3.63E-6 5, α(P)=1.613E-7 23, α(N+)=3.05E-5 5 | ||
767.68 | (9/2)+ | 2.0 ps 4 | 606.9 5 | (E2) | 0.00560 | B(E2)(W.u.)=7.0 17, α=0.00560 8, α(K)=0.00476 7, α(L)=0.000671 10, α(M)=0.0001379 20, α(N)=2.89E-5 5, α(O)=3.93E-6 6, α(P)=1.732E-7 25, α(N+)=3.30E-5 5 | |
(9/2)+ | 2.0 ps 4 | 767.68 10 | (M1+E2) | 0.0037 | α=0.0037 6, α(K)=0.0032 6, α(L)=0.00041 6, α(M)=8.4×10-5 11, α(N)=1.78E-5 23, α(O)=2.5E-6 4, α(P)=1.20E-7 22, α(N+)=2.0E-5 3 | ||
871.86 | (7/2)+ | 1.2 ps 3 | 871.80 10 | M1+E2 | +0.70 +5-8 | 0.00290 | B(E2)(W.u.)=6.5 18, B(M1)(W.u.)=0.016 4, α=0.00290 6, α(K)=0.00250 6, α(L)=0.000317 6, α(M)=6.47E-5 13, α(N)=1.37E-5 3, α(O)=1.91E-6 4, α(P)=9.48E-8 21, α(N+)=1.57E-5 3 |
1429.9 | 15/2+ | 797.3 3 | E2 | 0.00286 | α=0.00286 4, α(K)=0.00245 4, α(L)=0.000328 5, α(M)=6.71×10-5 10, α(N)=1.411E-5 20, α(O)=1.94E-6 3, α(P)=9.02E-8 13, α(N+)=1.614E-5 23 | ||
1603.9 | (15/2-) | 532.78 9 | E2 | 0.00791 | α=0.00791 11, α(K)=0.00669 10, α(L)=0.000972 14, α(M)=0.000200 3, α(N)=4.20×10-5 6, α(O)=5.66E-6 8, α(P)=2.41E-7 4, α(N+)=4.79E-5 7 | ||
1744.8 | (15/2-) | 673.7 3 | E2 | 0.00429 | α=0.00429 6, α(K)=0.00366 6, α(L)=0.000505 7, α(M)=0.0001037 15, α(N)=2.18×10-5 3, α(O)=2.97E-6 5, α(P)=1.340E-7 19, α(N+)=2.49E-5 4 | ||
2295.1 | 19/2+ | 865.2 3 | E2 | 0.00237 | α=0.00237 4, α(K)=0.00203 3, α(L)=0.000268 4, α(M)=5.48×10-5 8, α(N)=1.155E-5 17, α(O)=1.591E-6 23, α(P)=7.49E-8 11, α(N+)=1.322E-5 19 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 7/2+ | STABLE | μ=+2.582025 3 (1973Wh01,2005St24), Q=-0.00371 14 (1988Ta17,2005St24) Other: Q=-0.009 4 from LASER spectroscopy (1981Th06). E(level): ΔJ=2 band based on 7/2+ (π(g7/2+1)) g.s. |
632.56 | 11/2+ | 5.3 ps 4 | E(level): ΔJ=2 band based on 7/2+ (π(g7/2+1)) g.s. |
1071.1 | (11/2-) | E(level): ΔJ=2 band based on the 11/2- (π(h11/2+1)) state. | |
1429.9 | 15/2+ | E(level): ΔJ=2 band based on 7/2+ (π(g7/2+1)) g.s. | |
1744.8 | (15/2-) | E(level): ΔJ=2 band based on the 11/2- (π(h11/2+1)) state. | |
2156.2 | (5/2,7/2,9/2) | 1.34×10-3 eV 22 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2295.1 | 19/2+ | E(level): ΔJ=2 band based on 7/2+ (π(g7/2+1)) g.s. | |
2321.0 | (5/2) | 8.4×10-4 eV 19 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2415 | (5/2,7/2,9/2) | 2.7×10-3 eV 4 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2438 | (5/2,7/2,9/2) | 1.5×10-3 eV 3 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2462 | (5/2,7/2,9/2) | 1.10×10-3 eV 22 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2645 | (5/2,7/2,9/2) | 5.1×10-3 eV 4 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2672 | (5/2,7/2,9/2) | 2.4×10-3 eV 3 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2722 | (5/2,7/2,9/2) | 2.4×10-3 eV 5 | 0.60 21 branching ratio to 160.6, 5/2+. Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2744 | (5/2,7/2,9/2) | 3.5×10-3 eV 5 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2759 | (5/2,7/2,9/2) | 3.1×10-3 eV 4 | 1.63 24 branching ratio to 160.6, 5/2+. Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2815 | (5/2,7/2,9/2) | 1.0×10-3 eV 3 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2858 | (5/2,7/2,9/2) | 2.8×10-3 eV 5 | 1.6 4 branching ratio to 160.6, 5/2+. Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2873 | (5/2,7/2,9/2) | 2.6×10-3 eV 3 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2909 | (5/2,7/2,9/2) | 4.9×10-3 eV 6 | 0.66 18 branching ratio to 81.0, 5/2+. Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
2944 | (5/2,7/2,9/2) | 2.3×10-3 eV 3 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
3039 | (5/2,7/2,9/2) | 9.7×10-4 eV 24 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
3296 | (5/2,7/2,9/2) | 1.8×10-3 eV 6 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
3322 | (5/2,7/2,9/2) | 1.4×10-3 eV 4 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
3422 | (5/2,7/2,9/2) | 1.7×10-3 eV 6 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
E(level) | Jπ(level) | T1/2(level) | Comments |
3517 | (5/2,7/2,9/2) | 1.4×10-3 eV 5 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
3526 | (5/2,7/2,9/2) | 3.3×10-3 eV 5 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
3672 | (5/2,7/2,9/2) | 3.2×10-3 eV 7 | Jπ(level): From dipole excitation in 133Cs(γ,γ’). |
E(level) | E(gamma) | Comments |
80.9979 | 80.9979 | E(γ): From 2000He14 I(γ): From 133Ba ε decay (10.539 y) |
160.6121 | 79.6142 | E(γ): From 2000He14 I(γ): From 133Ba ε decay (10.539 y) |
160.6120 | E(γ): From 2000He14 I(γ): From 133Ba ε decay (10.539 y) | |
383.8491 | 223.2368 | E(γ): From 2000He14 I(γ): From 133Ba ε decay (10.539 y) |
302.8508 | E(γ): From 2000He14 I(γ): From 133Ba ε decay (10.539 y) | |
383.8485 | E(γ): From 2000He14 I(γ): From 133Ba ε decay (10.539 y) | |
437.0113 | 53.1622 | E(γ): From 2000He14 I(γ): From 133Ba ε decay (10.539 y) |
276.3989 | E(γ): From 2000He14 I(γ): From 133Ba ε decay (10.539 y) | |
356.0129 | E(γ): From 2000He14 I(γ): From 133Ba ε decay (10.539 y) | |
632.56 | 632.56 | M(γ): from γ(θ) in 130Te(6Li,3nγ) and Coulomb excitation |
640.40 | 641 | E(γ): from Coulomb excitation I(γ): From Coulomb excitation. |
705.57 | 624.58 | I(γ): From Coulomb excitation. M(γ): from γ(θ) in 130Te(6Li,3nγ) and Coulomb excitation |
705.56 | I(γ): From Coulomb excitation. | |
767.68 | 606.9 | E(γ): from Coulomb excitation I(γ): From Coulomb excitation. |
767.68 | I(γ): From Coulomb excitation. M(γ): d (ΔJ=1) in 130Te(6Li,3nγ) | |
819.06 | 658.61 | I(γ): From Coulomb excitation. |
737.4 | I(γ): From Coulomb excitation. | |
818.92 | I(γ): From Coulomb excitation. | |
871.86 | 712.6 | I(γ): From Coulomb excitation. |
871.80 | I(γ): From Coulomb excitation. | |
1071.1 | 303.4 | E(γ): γ-rays are observed, but unplaced in 133Cs(n,n’γ); these transitions are inserted in the level scheme by evaluators on the basis of energy relations I(γ): branching for a doublet from 130Te(6Li,3nγ) |
365.95 | E(γ): γ-rays are observed, but unplaced in 133Cs(n,n’γ); these transitions are inserted in the level scheme by evaluators on the basis of energy relations M(γ): from γ(θ) in 130Te(6Li,3nγ) | |
1429.9 | 797.3 | E(γ): From 130Te(6Li,3nγ) I(γ): From 130Te(6Li,3nγ) M(γ): from γ(θ) in 130Te(6Li,3nγ) |
1603.9 | 532.78 | E(γ): From 130Te(6Li,3nγ) I(γ): From 130Te(6Li,3nγ) M(γ): from γ(θ) in 130Te(6Li,3nγ) |
1744.8 | 673.7 | E(γ): From 130Te(6Li,3nγ) I(γ): From 130Te(6Li,3nγ) M(γ): from γ(θ) in 130Te(6Li,3nγ) |
E(level) | E(gamma) | Comments |
1923.0 | 319.1 | E(γ): From 130Te(6Li,3nγ) I(γ): From 130Te(6Li,3nγ) M(γ): from γ(θ) in 130Te(6Li,3nγ) |
1951.5 | 347.6 | E(γ): From 130Te(6Li,3nγ) I(γ): From 130Te(6Li,3nγ) M(γ): from γ(θ) in 130Te(6Li,3nγ) |
2156.2 | 937.0 | E(γ): γ-rays are observed, but unplaced in 133Cs(n,n’γ); these transitions are inserted in the level scheme by evaluators on the basis of energy relations |
1066.4 | E(γ): γ-rays are observed, but unplaced in 133Cs(n,n’γ); these transitions are inserted in the level scheme by evaluators on the basis of energy relations | |
2156.9 | E(γ): γ-rays are observed, but unplaced in 133Cs(n,n’γ); these transitions are inserted in the level scheme by evaluators on the basis of energy relations | |
2295.1 | 865.2 | E(γ): From 130Te(6Li,3nγ) I(γ): From 130Te(6Li,3nγ) M(γ): from γ(θ) in 130Te(6Li,3nγ) |
2321.0 | 1404.6 | E(γ): γ-rays are observed, but unplaced in 133Cs(n,n’γ); these transitions are inserted in the level scheme by evaluators on the basis of energy relations |
1937.3 | E(γ): γ-rays are observed, but unplaced in 133Cs(n,n’γ); these transitions are inserted in the level scheme by evaluators on the basis of energy relations | |
2528.3 | 233.2 | E(γ): From 130Te(6Li,3nγ) I(γ): From 130Te(6Li,3nγ) M(γ): from γ(θ) in 130Te(6Li,3nγ) |
2643.4 | 115.1 | E(γ): From 130Te(6Li,3nγ) I(γ): From 130Te(6Li,3nγ) M(γ): from γ(θ) in 130Te(6Li,3nγ) |
2834.2 | 190.8 | E(γ): From 130Te(6Li,3nγ) I(γ): From 130Te(6Li,3nγ) M(γ): from γ(θ) in 130Te(6Li,3nγ) |