ADOPTED LEVELS, GAMMAS for 125Sb
Author: J. Katakura | Citation: Nucl. Data Sheets 112, 495 (2011) | Cutoff date: 1-Jan-2010
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=766.7 keV 22 | S(n)= 8707 keV 3 | S(p)= 7311 keV 3 | Q(α)= -4.84×103 keV 3 | ||
Reference: 2012WA38 |
References: | |||
A | 124Sn(pol p,p) IAR | B | 124Sn(3He,d) |
C | 125Sn β- decay (9.52 M) | D | 125Sn β- decay (9.64 d) |
E | 126Te(d,3He) | F | 126Te(t,α) |
G | 238U(12C,xγ) | H | 124Sn(7Li,α2nγ) |
I | 125Sb IT decay (25 μs) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | BCDEFGHI | 7/2+ | 2.75856 y 25 % β- = 100 | |||||
332.06 3 | BCDEF | 5/2+ | 156 ps 8 | 331.96 6 | 100 1 | M1+E2 | 0.0 | 7/2+ |
642.97 2 | BC EF | 3/2+,5/2+ | 310.96 4 642.96 2 | 29 3 100.0 19 | 332.06 0.0 | 5/2+ 7/2+ | ||
921.67 3 | BC EF | 1/2+ | 278.56 15 589.61 2 | 12 3 100.0 21 | 642.97 332.06 | 3/2+,5/2+ 5/2+ | ||
1067.30 3 | D HI | 9/2+ | 1067.10 5 | 100 | M1+E2 | 0.0 | 7/2+ | |
1089.50 3 | D GHI | 11/2+ | 1089.15 10 | 100 | E2 | 0.0 | 7/2+ | |
1349.60 3 | CD | 7/2+ | 258.25 10 ? 282.45 5 1017.50 8 1349.39 6 | <6.4 5.8 6 100 4 18.7 8 | M1+E2 | 1089.50 1067.30 332.06 0.0 | 11/2+ 9/2+ 5/2+ 7/2+ | |
1419.85 4 | D | 9/2+ | 1087.70 10 1419.70 5 | 100 16 40.8 8 | D(+Q) | 332.06 0.0 | 5/2+ 7/2+ | |
1483.78 2 | BC | 3/2+,5/2+ | 840.83 5 1151.70 8 1483.77 2 | 40.4 17 18.0 17 100.0 17 | 642.97 332.06 0.0 | 3/2+,5/2+ 5/2+ 7/2+ | ||
1560 5 | B | |||||||
1591.57 5 | D | 7/2+,9/2+ | 524.30 5 1259.35 10 1591.4 2 | 31 3 100 6 81 6 | 1067.30 332.06 0.0 | 9/2+ 5/2+ 7/2+ | ||
1660 20 | B | |||||||
1700.69 5 | C | 1/2+,3/2,5/2+ | 779.5 3 1057.77 21 1368.61 4 | 13 4 18 4 100 3 | 921.67 642.97 332.06 | 1/2+ 3/2+,5/2+ 5/2+ | ||
1736.13 3 | BC | (3/2)+ | 386.52 3 1093.27 14 1404.06 2 1736.07 7 | 14.3 4 5.2 4 100.0 10 4.4 3 | 1349.60 642.97 332.06 0.0 | 7/2+ 3/2+,5/2+ 5/2+ 7/2+ | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1800 20 | B | 1/2+ | ||||||
1806.700 16 | DEF | (9/2)+ | 386.6 2 1806.690 16 | 3.3 7 100.0 20 | 1419.85 0.0 | 9/2+ 7/2+ | ||
1889.848 15 | B D | 9/2-,11/2- | 469.85 5 800.28 5 822.48 5 1557.3 1 1889.884 16 | 34.7 7 24.9 5 100.0 20 0.095 23 1.7 1 | E1(+M2) E1(+M2) E1 | 1419.85 1089.50 1067.30 332.06 0.0 | 9/2+ 11/2+ 9/2+ 5/2+ 7/2+ | |
1894 10 | F | |||||||
1913.77 8 | C | 3/2+,5/2 | 430.03 14 1581.96 20 1913.66 10 | 63 16 53 11 100 11 | 1483.78 332.06 0.0 | 3/2+,5/2+ 5/2+ 7/2+ | ||
1947.45 4 | BC | (3/2)+ | 1025.46 22 1304.42 10 1615.38 3 1947.50 13 | 12 5 11 3 100 3 13 3 | 921.67 642.97 332.06 0.0 | 1/2+ 3/2+,5/2+ 5/2+ 7/2+ | ||
1971.25 20 | HI | 15/2- | 4.1 µs 2 | 881.8 3 904.0 3 | 63.8 8 100.0 25 | E3(+M2) E3 | 1089.50 1067.30 | 11/2+ 9/2+ |
1971.25+X 20 | I | (19/2-) | 25 µs 4 | |||||
1982.84 4 | D | 11/2- | 563.0 2 893.40 5 915.55 5 1982.5 2 | 0.38 5 7.04 23 100.0 21 0.077 23 | D+Q E1+M2 | 1419.85 1089.50 1067.30 0.0 | 9/2+ 11/2+ 9/2+ 7/2+ | |
1993.64 25 | GH | (15/2)+ | 904.1 3 | 100 | E2 | 1089.50 | 11/2+ | |
2002.140 12 | D | 9/2,11/2+ | 652.6 1 912.0 5 ? 934.63 5 2002.134 12 | 2.12 5 0.35 10 10.86 20 100.0 20 | 1349.60 1089.50 1067.30 0.0 | 7/2+ 11/2+ 9/2+ 7/2+ | ||
2112.1 3 | H | (19/2-) | 28.0 µs 7 | 140.9 3 | 100 | E2 | 1971.25 | 15/2- |
2113.0 10 | C EF | 1/2-,3/2- | 2113 1 | 100 | 0.0 | 7/2+ | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2193.4 3 | GH | 15/2+ | 1103.7 5 | 100 | 1089.50 | 11/2+ | ||
2201.023 12 | D | 9/2,11/2+ | 311.3 1 1111.4 1 2201.002 12 | 22.5 25 35 5 100 5 | 1889.848 1089.50 0.0 | 9/2-,11/2- 11/2+ 7/2+ | ||
2217.2 3 | H | (17/2)- | 105.1 3 246.1 3 | 28.9 24 100 4 | M1 | 2112.1 1971.25 | (19/2-) 15/2- | |
2227.0 4 | D | 1137.5 5 2227.0 5 | ≈100 ≈70 | 1089.50 0.0 | 11/2+ 7/2+ | |||
2240.72 4 | D | 9/2+ | 258.25 10 ? 350.95 5 434.13 10 890.5 5 ? 1151.23 5 1173.30 5 | <7.7 100.0 18 9.2 7 3.3 7 43.4 7 68.8 15 | D+Q M1+E2 M1+E2 | 1982.84 1889.848 1806.700 1349.60 1089.50 1067.30 | 11/2- 9/2-,11/2- (9/2)+ 7/2+ 11/2+ 9/2+ | |
2253.39 5 | D | 9/2,11/2,13/2 | 270.60 5 363.5 2 903.5 5 ? 1163.84 5 | 100.0 18 2.7 5 12 3 29.1 18 | 1982.84 1889.848 1349.60 1089.50 | 11/2- 9/2-,11/2- 7/2+ 11/2+ | ||
2275.769 10 | D | 9/2,11/2+ | 684.0 2 1186.15 15 1208.4 2 2275.748 10 | 5.9 11 4.8 5 4.3 11 100.0 21 | 1591.57 1089.50 1067.30 0.0 | 7/2+,9/2+ 11/2+ 9/2+ 7/2+ | ||
2288.21 8 | D | (11/2+) | 286.2 2 1198.70 15 1220.88 10 | 2.2 4 5.8 4 100.0 22 | M1+E2 | 2002.140 1089.50 1067.30 | 9/2,11/2+ 11/2+ 9/2+ | |
2299 10 | EF | 1/2-,3/2- | ||||||
2325.0 3 | GH | (19/2)+ | 31 ns 2 | 107.9 3 131.59 17 331.36 24 | 55 3 55 3 100 5 | [E1] E2 (E2) | 2217.2 2193.4 1993.64 | (17/2)- 15/2+ (15/2)+ |
2471.0 4 | GH | (23/2)+ | 272 ns 16 | 146.02 19 | 100 | E2 | 2325.0 | (19/2)+ |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2480 20 | B | |||||||
2483.8 4 | G | 490.2 3 | 100 | 1993.64 | (15/2)+ | |||
2488.5 5 | G | 295.1 4 | 100 | 2193.4 | 15/2+ | |||
2515 10 | F | 1/2-,3/2- | ||||||
2570 20 | B | 1/2+ | ||||||
2636.5 5 | G | 152.7 3 | 100 | 2483.8 | ||||
2670 20 | B | 1/2+ | ||||||
2678 10 | F | 5/2-,7/2,9/2+ | ||||||
2710 20 | B | 1/2+ | ||||||
2780 20 | B | |||||||
2815.4 6 | G | 331.6 | 100 | 2483.8 | ||||
2820 20 | B | |||||||
2890 20 | B | 3/2+,5/2+ | ||||||
2917.3 5 | G | 446.3 3 | 100 | 2471.0 | (23/2)+ | |||
3122 10 | F | 7/2+,9/2+ | ||||||
3190 10 | F | 5/2-,7/2- | ||||||
3399.2 6 | G | 481.8 3 | 100 | 2917.3 | ||||
3462 10 | F | 1/2-,3/2- | ||||||
3941.8 6 | G | 542.5 3 1024.7 5 | 100 33 22 8 | 3399.2 2917.3 | ||||
4479.9 6 | G | 538.1 4 1080.5 5 | 1.0E2 3 60 20 | 3941.8 3399.2 | ||||
4933.1 7 | G | 452.9 5 991.5 5 | 100 25 38 15 | 4479.9 3941.8 | ||||
5365.1 9 | G | 432.0 5 | 100 | 4933.1 | ||||
15172 20 | A | 3/2+ | ||||||
15379 20 | A | 1/2+ | ||||||
16417 20 | A | (5/2)+ | ||||||
16701 20 | A | (5/2)+ | ||||||
17869 20 | A | 7/2- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
18468 20 | A | (3/2-) | ||||||
18537 20 | A | (3/2-) | ||||||
18959 20 | A | (1/2)- | ||||||
19118 20 | A | (1/2)- |
E(level): From a least-squares fit to adopted Eγ’s for levels connecting with γ’s. Others from (d,3He), unless otherwise noted
E(γ): From 125Sn β- decay (9.64 d), unless otherwise noted
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
332.06 | 5/2+ | 156 ps 8 | 331.96 6 | M1+E2 | -0.24 4 | 0.0242 | B(E2)(W.u.)=1.3 5, B(M1)(W.u.)=0.00356 20, α=0.0242, α(K)=0.0210 3, α(L)=0.00264 4, α(M)=0.000523 8, α(N)=0.0001008 16, α(O)=9.94E-6 15, α(N+)=0.0001108 17 |
1067.30 | 9/2+ | 1067.10 5 | M1+E2 | -0.86 18 | 0.00134 | α=0.00134 4, α(K)=0.00117 4, α(L)=0.000142 4, α(M)=2.79×10-5 7, α(N)=5.39E-6 14, α(O)=5.35E-7 14, α(N+)=5.93E-6 15 | |
1089.50 | 11/2+ | 1089.15 10 | E2 | 0.001133 | α=0.001133 16, α(K)=0.000983 14, α(L)=0.0001211 17, α(M)=2.39×10-5 4, α(N)=4.60E-6 7, α(O)=4.52E-7 7, α(N+)=5.05E-6 | ||
1349.60 | 7/2+ | 1017.50 8 | M1+E2 | 2.1 +5-3 | 0.00137 | α=0.00137 3, α(K)=0.001190 23, α(L)=0.000147 3, α(M)=2.89×10-5 6, α(N)=5.57E-6 10, α(O)=5.48E-7 11, α(N+)=6.11E-6 11 | |
1419.85 | 9/2+ | 1419.70 5 | D(+Q) | +0.01 3 | 0.000830 | α=0.000830 12, α(K)=0.000680 10, α(L)=8.11×10-5 12, α(M)=1.595E-5 23, α(N)=3.09E-6 5, α(O)=3.09E-7 5, α(N+)=5.30E-5 | |
1889.848 | 9/2-,11/2- | 469.85 5 | E1(+M2) | +0.010 24 | 0.00292 | α=0.00292 6, α(K)=0.00254 5, α(L)=0.000307 6, α(M)=6.03×10-5 12, α(N)=1.160E-5 22, α(O)=1.138E-6 22, α(N+)=1.274E-5 25 | |
9/2-,11/2- | 800.28 5 | E1(+M2) | 0.18 +11-8 | 0.0011 | α=0.0011 3, α(K)=0.0010 3, α(L)=0.00012 4, α(M)=2.3×10-5 7, α(N)=4.4E-6 13, α(O)=4.4E-7 13, α(N+)=4.8E-6 15 | ||
9/2-,11/2- | 822.48 5 | E1 | 0.000849 | α=0.000849 12, α(K)=0.000740 11, α(L)=8.79×10-5 13, α(M)=1.727E-5 25, α(N)=3.33E-6 5, α(O)=3.30E-7 5, α(N+)=3.66E-6 | |||
1971.25 | 15/2- | 4.1 µs 2 | 881.8 3 | E3(+M2) | 0.75 GE | 0.0045 | B(E3)(W.u.)≥0.10, B(M2)(W.u.)≤0.00015, α=0.0045 6, α(K)=0.0039 6, α(L)=0.00053 5, α(M)=0.000104 10, α(N)=2.01E-5 20, α(O)=1.94E-6 22, α(N+)=2.20E-5 22 |
15/2- | 4.1 µs 2 | 904.0 3 | E3 | 0.00372 | B(E3)(W.u.)=0.395 23, α=0.00372 6, α(K)=0.00317 5, α(L)=0.000442 7, α(M)=8.80E-5 13, α(N)=1.684E-5 24, α(O)=1.601E-6 23, α(N+)=1.84E-5 3 | ||
1982.84 | 11/2- | 893.40 5 | D+Q | 0.29 17 | 0.0011 | α=0.0011 5, α(K)=0.0010 4, α(L)=0.00012 6, α(M)=2.3×10-5 11, α(N)=4.4E-6 20, α(O)=4.4E-7 20, α(N+)=4.8E-6 22 | |
11/2- | 915.55 5 | E1+M2 | -0.02 1 | 0.000688 | α=0.000688 10, α(K)=0.000600 9, α(L)=7.11×10-5 11, α(M)=1.395E-5 21, α(N)=2.69E-6 4, α(O)=2.67E-7 4, α(N+)=2.96E-6 5 | ||
1993.64 | (15/2)+ | 904.1 3 | E2 | 0.001712 | α=0.001712 24, α(K)=0.001482 21, α(L)=0.000186 3, α(M)=3.67×10-5 6, α(N)=7.06E-6 10, α(O)=6.89E-7 10, α(N+)=7.75E-6 11 | ||
2112.1 | (19/2-) | 28.0 µs 7 | 140.9 3 | E2 | 0.490 | B(E2)(W.u.)=0.00658 19, α=0.490 8, α(K)=0.379 6, α(L)=0.0892 15, α(M)=0.0182 3, α(N)=0.00336 6, α(O)=0.000267 5, α(N+)=0.00363 6 | |
2217.2 | (17/2)- | 246.1 3 | M1 | 0.0524 | α=0.0524, α(K)=0.0453 7, α(L)=0.00570 9, α(M)=0.001128 17, α(N)=0.000218 4, α(O)=2.16×10-5 3, α(N+)=0.000239 4 | ||
2240.72 | 9/2+ | 350.95 5 | D+Q | 0.42 3 | |||
9/2+ | 1151.23 5 | M1+E2 | 2.1 +12-10 | 0.00105 | α=0.00105 6, α(K)=0.00091 6, α(L)=0.000111 6, α(M)=2.20×10-5 12, α(N)=4.23E-6 22, α(O)=4.19E-7 24, α(N+)=6.92E-6 19 | ||
9/2+ | 1173.30 5 | M1+E2 | 1.1 GE | 0.00102 | α=0.00102 5, α(K)=0.00088 5, α(L)=0.000107 5, α(M)=2.12×10-5 10, α(N)=4.08E-6 19, α(O)=4.04E-7 20, α(N+)=8.37E-6 15 | ||
2288.21 | (11/2+) | 1220.88 10 | M1+E2 | 9.9 GE | 0.000901 | α=0.000901 13, α(K)=0.000774 11, α(L)=9.44×10-5 14, α(M)=1.86E-5 3, α(N)=3.59E-6 5, α(O)=3.54E-7 5, α(N+)=1.349E-5 1 | |
2325.0 | (19/2)+ | 31 ns 2 | 107.9 3 | [E1] | 0.152 | B(E1)(W.u.)=1.50E-6 14, α=0.152 | |
(19/2)+ | 31 ns 2 | 131.59 17 | E2 | 0.624 | B(E2)(W.u.)=2.68 25, α=0.624, α(K)=0.476 7, α(L)=0.1185 18, α(M)=0.0243 4, α(N)=0.00446 7, α(O)=0.000350 6, α(N+)=0.00481 8 | ||
(19/2)+ | 31 ns 2 | 331.36 24 | (E2) | 0.0269 | B(E2)(W.u.)=0.048 5, α=0.0269, α(K)=0.0226 4, α(L)=0.00345 5, α(M)=0.000690 10, α(N)=0.0001304 19, α(O)=1.178E-5 17, α(N+)=0.0001422 21 | ||
2471.0 | (23/2)+ | 272 ns 16 | 146.02 19 | E2 | 0.432 | B(E2)(W.u.)=0.59 4, α=0.432, α(K)=0.336 5, α(L)=0.0770 12, α(M)=0.01573 24, α(N)=0.00290 5, α(O)=0.000232 4, α(N+)=0.00313 5 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 7/2+ | 2.75856 y 25 % β- = 100 | μ=+2.63 4 (1989Ra17) Configuration=(π 1g7/2). |
332.06 | 5/2+ | 156 ps 8 | Configuration=(π 2d5/2). |
642.97 | 3/2+,5/2+ | Jπ(level): From L=2 in (3He,d), reaction strength favors 3/2+. Those states are considered to excite by 2d3/2 stripping, because the 332-keV level exhausts essentially all of the 2d5/2 strength in the (3He,d) reaction. | |
921.67 | 1/2+ | Configuration=(π 3s1/2). | |
1067.30 | 9/2+ | Jπ(level): γγ(θ) and (pol γ)γ(θ) in 125Sn β- decay (9.52 min, 9.64 d). | |
1089.50 | 11/2+ | Jπ(level): γγ(θ) and (pol γ)γ(θ) in 125Sn β- decay (9.52 min, 9.64 d). | |
1560 | E(level): From (3He,d). | ||
1660 | E(level): From (3He,d). | ||
1736.13 | (3/2)+ | Jπ(level): From L=2 in (3He,d), reaction strength favors 3/2+. Those states are considered to excite by 2d3/2 stripping, because the 332-keV level exhausts essentially all of the 2d5/2 strength in the (3He,d) reaction. | |
1800 | 1/2+ | E(level): From (3He,d). | |
1894 | E(level): From (t,α). | ||
1947.45 | (3/2)+ | Jπ(level): From L=2 in (3He,d), reaction strength favors 3/2+. Those states are considered to excite by 2d3/2 stripping, because the 332-keV level exhausts essentially all of the 2d5/2 strength in the (3He,d) reaction. | |
2299 | 1/2-,3/2- | E(level): From (t,α). | |
2480 | E(level): From (3He,d). | ||
2515 | 1/2-,3/2- | E(level): From (t,α). | |
2570 | 1/2+ | E(level): From (3He,d). | |
2670 | 1/2+ | E(level): From (3He,d). | |
2678 | 5/2-,7/2,9/2+ | E(level): From (t,α). | |
2710 | 1/2+ | E(level): From (3He,d). | |
2780 | E(level): From (3He,d). | ||
2820 | E(level): From (3He,d). | ||
2890 | 3/2+,5/2+ | E(level): From (3He,d). | |
3122 | 7/2+,9/2+ | E(level): From (t,α). | |
3190 | 5/2-,7/2- | E(level): From (t,α). | |
3462 | 1/2-,3/2- | E(level): From (t,α). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
15172 | 3/2+ | IAR of 27.5-keV level in 125Sn. E(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. Jπ(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. | |
15379 | 1/2+ | IAR of 215.1-keV level in 125Sn. E(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. Jπ(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. | |
16417 | (5/2)+ | IAR of 1258-keV level in 125Sn. E(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. Jπ(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. | |
16701 | (5/2)+ | IAR of 1540-keV level in 125Sn. E(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. Jπ(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. | |
17869 | 7/2- | IAR of 2676-keV level in 125Sn. E(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. Jπ(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. | |
18468 | (3/2-) | IAR of 3349-keV level in 125Sn. E(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. Jπ(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. | |
18537 | (3/2-) | IAR of 3421-keV level in 125Sn. E(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. Jπ(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. | |
18959 | (1/2)- | IAR of 3830-keV level in 125Sn. E(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. Jπ(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. | |
19118 | (1/2)- | The closest level of L=(1) is observed at 4060 keV in 124Sn(d,p). Energy difference is too large. E(level): The closest level of L=(1) is observed at 4060 keV in 124Sn(d,p). Energy difference is too large. Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. Jπ(level): Analog resonance, Jπ from analyzing power in 124Sn(pol p,p). The uncertainties in the resonance energies are 5-20 keV. |
E(level) | E(gamma) | Comments |
642.97 | 310.96 | E(γ): From 125Sn β- decay (9.52 min) | 642.96 | E(γ): From 125Sn β- decay (9.52 min) |
921.67 | 278.56 | E(γ): From 125Sn β- decay (9.52 min) | 589.61 | E(γ): From 125Sn β- decay (9.52 min) |
1349.60 | 258.25 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1483.78 | 840.83 | E(γ): From 125Sn β- decay (9.52 min) | 1151.70 | E(γ): From 125Sn β- decay (9.52 min) | 1483.77 | E(γ): From 125Sn β- decay (9.52 min) |
1700.69 | 779.5 | E(γ): From 125Sn β- decay (9.52 min) | 1057.77 | E(γ): From 125Sn β- decay (9.52 min) | 1368.61 | E(γ): From 125Sn β- decay (9.52 min) |
1736.13 | 386.52 | E(γ): From 125Sn β- decay (9.52 min) | 1093.27 | E(γ): From 125Sn β- decay (9.52 min) | 1404.06 | E(γ): From 125Sn β- decay (9.52 min) | 1736.07 | E(γ): From 125Sn β- decay (9.52 min) |
1913.77 | 430.03 | E(γ): From 125Sn β- decay (9.52 min) | 1581.96 | E(γ): From 125Sn β- decay (9.52 min) | 1913.66 | E(γ): From 125Sn β- decay (9.52 min) |
1947.45 | 1304.42 | E(γ): From 125Sn β- decay (9.52 min) | 1615.38 | E(γ): From 125Sn β- decay (9.52 min) | 1947.50 | E(γ): From 125Sn β- decay (9.52 min) |
1971.25 | 904.0 | M(γ): From 124Sn(7Li,α2nγ) |
1993.64 | 904.1 | E(γ): Weighted average of 238U(12C,Xγ) and 124Sn(7Li,α2nγ) M(γ): From 124Sn(7Li,α2nγ) |
2112.1 | 140.9 | M(γ): From 124Sn(7Li,α2nγ) |
2113.0 | 2113 | E(γ): From 125Sn β- decay (9.52 min) |
E(level) | E(gamma) | Comments |
2193.4 | 1103.7 | E(γ): Weighted average of 238U(12C,Xγ) and 124Sn(7Li,α2nγ) |
2217.2 | 246.1 | M(γ): From 124Sn(7Li,α2nγ) |
2240.72 | 258.25 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
2325.0 | 107.9 | E(γ): From 124Sn(7Li,α2nγ) | 131.59 | E(γ): Weighted average of 238U(12C,Xγ) and 124Sn(7Li,α2nγ) I(γ): From 124Sn(7Li,α2nγ) M(γ): From 124Sn(7Li,α2nγ) | 331.36 | E(γ): Weighted average of 238U(12C,Xγ) and 124Sn(7Li,α2nγ) I(γ): From 124Sn(7Li,α2nγ) M(γ): M1 or E2 from 124Sn(7Li,α2nγ). Placement in the level scheme requires ΔJ=2. |
2471.0 | 146.02 | E(γ): Weighted average of 238U(12C,Xγ) and 124Sn(7Li,α2nγ) M(γ): From 124Sn(7Li,α2nγ) |
Other reaction: 1992NiZZ; heavy ion reaction, but no data are available
Q-value: Note: Current evaluation has used the following Q record 766.7 218706.7 267307.7 26 -4839 28 2009AuZZ