Plutonium Biokinetics in Human Body A. Luciani - Kit-Bibliothek - FZK
Plutonium Biokinetics in Human Body A. Luciani - Kit-Bibliothek - FZK
Plutonium Biokinetics in Human Body A. Luciani - Kit-Bibliothek - FZK
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adionuclide. Therefore only isotopes with long halftimes are likely to be found, such as 244 Pu,<br />
that was found <strong>in</strong> the rare-earth m<strong>in</strong>eral bastnasite [6].<br />
At present 20 isotopes are known, from N = 228 to N = 247, but only for 17 isotopes,<br />
from N = 231 to N = 247, the halftimes are known [7]. In Table 1.2.1 the physical<br />
characteristics of the most important <strong>Plutonium</strong> isotopes with their respective halftime, type<br />
of decay and specific activity are given. Most of the <strong>Plutonium</strong> isotopes are unstable to alpha<br />
emission [8]. Alpha decays energies are frequently used to identify heavy nuclei. However<br />
some <strong>Plutonium</strong> isotopes can be hardly dist<strong>in</strong>guished with current energy analysis. For<br />
example the ma<strong>in</strong> alpha transitions of 239 Pu, one of the most important isotopes for <strong>in</strong>dustrial<br />
application, have alpha-energies close to those of 240 Pu. So it is extremely difficult to separate<br />
these two isotopes by alpha- spectrometry. Other isotopes with N = 241, 243 and from 245 to<br />
247 are unstable to beta decay. 241 Pu also decays by alpha emission, but the alpha halftime is<br />
around 40,000 times that of the betas. Spontaneous fission can also occur with different<br />
probabilities for <strong>Plutonium</strong> isotopes, with even N values from 236 to 244 and for the odd<br />
atomic mass number 239. For other radioisotopes such decay is less significant.<br />
Among all these radioisotopes the most common and extensively used is 239 Pu. Its<br />
complete decay scheme is given <strong>in</strong> Figure 1.2.1 [9].<br />
Table 1.2.1 Physical characteristics of major <strong>Plutonium</strong> isotopes (only the ma<strong>in</strong> emissions<br />
are given).<br />
Isotopes Half time<br />
[years]<br />
Type of decay,<br />
(yield [%] - energy [Mev])<br />
238 Pu 87.74 α<br />
(71.6 - 5.499)<br />
(28.3 - 5.456)<br />
sf (a)<br />
239 Pu 2.410 • 10 4 α<br />
(73.8 - 5.157)<br />
(15.2 - 5.144)<br />
(10.7 - 5.105)<br />
sf (a)<br />
240 Pu 6563 α<br />
(73.4 - 5.168)<br />
(26.5 - 5.124)<br />
sf (a)<br />
241 Pu 14.35 β<br />
(100 - 0.02 (b) )<br />
α<br />
(2.04 10 -3 - 4.897)<br />
(a) spontaneous fission.<br />
(b) maximum energy.<br />
10<br />
Specific activity<br />
[Bqg -1 ]<br />
6.34•10 11<br />
2.30•10 9<br />
8.40•10 9<br />
3.83•10 12