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Tin-126

 
Wikipedia: Tin-126
 
Long-lived
fission products
Prop:
Unit:
t½
Ma
Yield
%
Q *
KeV
βγ
*
99Tc .211 6.1385 294 β
126Sn .230 .1084 4050 βγ
79Se .295 .0447 151 β
93Zr 1.53 5.4575 91 βγ
135Cs 2.3  6.9110 269 β
107Pd 6.5  1.2499 33 β
129I 15.7  .8410 194 βγ

Tin-126 is a radioisotope of tin and one of only 7 long-lived fission products. While tin-126's halflife of 230,000 years translates to a low specific activity that limits its radioactive hazard, its shortlived decay product, antimony-126, emits high-energy gamma radiation, making external exposure to tin-126 a potential concern.

126Sn is in the middle of the mass range for fission products. Thermal reactors, which make up almost all current nuclear power plants, produce it at a very low yield (such as 0.0236% or 0.06%), since slow neutrons almost always fission 235U or 239Pu into unequal halves. Fast fission in a fast reactor or nuclear weapon, or fission of some heavy minor actinides like californium, will produce it at higher yields.

Chain yield, % per fission[1]
Thermal Fast 14 MeV
232Th not fissile .0593±.0087 1.08 ± .17
233U .233 ± .032 .325 ± .075 1.79 ± .24
235U .0594±.0052 .098 ± .020 1.62 ± .49
238U not fissile .093 ± .020 1.38 ± .25
239Pu .314 ± .049 .209 ± .044 secret
241Pu .362 ± .089 .157 ± .031 secret

References

See also


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Wikipedia. This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Tin-126" Read more