Nucleus[1]
|
Binding energy (MeV)
|
g.s. Radius[3] & Deformation[4]
|
11250Sn62 Tin J(π)=0+ T1/2=stable Abundance: 0.97% 1 |
|
Experiment [2] |
Theory [4] |
Sh.corr. [4] |
Mass Excess |
-88.65599 (0.000573) |
-88.620 |
0.510 |
BE |
953.527 |
953.491 |
BE/A |
8.514 |
8.513 |
|
<R2ch>1/2 = 4.5948 ± 0.0022 fm [3]
Charge-density Distribution [6]
β2= 0.000 β3= 0.000 β4= 0.000 β6= 0.000 |
Excited States[1] click on a plot to process it
|
Known and possible Decays[1]
|
Q-values (keV) roman [2], italic [4]
|
| | α - decay | -1828.34 | β- - decay | -7056.99 | β+ - decay | -1686.95 | e-capture | -664.95 | 1p - decay | -7554.09 | 2p - decay | -12885.22 | 1n - decay | -10787.77 | 2n - decay | -18956.61 | 2β- - decay | -11088.41 | β-,n | -15890.52 | β-,2n | -27348.82 | β-,d | -15949.67 | β-,t | -20974.84 | β-,α | -6960.91 | β-,n,α | -15587.91 | EC,p | -6691.95 | EC,2p | -15776.26 | EC,α | -3474.24 |
|
Metastable states and Resonances[1]
|
Radiation energies (keV)[1]
|
Thermal neutrons[1]
|
El.-Magn. properties[5,7,8]
|
|
|
σ
(b)
|
μ (nm) |
Q (b) |
E* (keV) | +0.2(2) | | 2550 | +0.61(5) | | 2550 | +0.53(3) | | 2550 | +1.5(7) | | 2248 | +0.7(3) | | 1257 | +0.21(7) | | 1257 | | (-)0.25(5) | 2550 | | -0.09(10) | 1257 |
B(E2)↑ = 0.232 ( | 11 | ) e2b2, |
β |
0 |
| = 0.1207 ( | 29 | ) |
2 | |
B(E3)↑ = 0.087 ( | 12 | ) e2b3, |
β |
0 |
| = 0.128 ( | 0 | ) |
3 | | |