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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

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