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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2.3.2.2 Performances<br />
Energy resolution of the HPGe and phoswich detect<strong>in</strong>g systems are evaluated for γ<br />
59.5 keV energy peak of 241 Am, the radionuclide of <strong>in</strong>terest for the direct measurements<br />
performed on the contam<strong>in</strong>ated subject. The results for the energy resolution R of the two<br />
detect<strong>in</strong>g systems expressed as percentage are given <strong>in</strong> Table 2.3.2.<br />
Table 2.3.2 Energy resolution (R) of each detector of the HPGe and Phoswich detect<strong>in</strong>g<br />
systems for 59.5 keV energy peak of 241 Am.<br />
Detect<strong>in</strong>g system Detector R [%]<br />
HPGe<br />
Phoswich<br />
63<br />
D 1 1.1<br />
D 2 1.2<br />
D 3 0.9<br />
D 4 1.0<br />
D 1 29<br />
D 2 24<br />
D 3 23<br />
It can be po<strong>in</strong>ted out the two detect<strong>in</strong>g systems are characterized by significantly<br />
different energy resolution performances. Therefore different energy calibration methods<br />
were applied.<br />
The energy calibration of HPGe detect<strong>in</strong>g system <strong>in</strong> the low energy range of the<br />
spectrum was carried out us<strong>in</strong>g two po<strong>in</strong>t sources of 241 Am and 57 Co of 40 and 1 kBq activity,<br />
respectively. They were located at about 25 cm distance from the detectors on the symmetry<br />
central axis of the whole detect<strong>in</strong>g system. Three full energy peaks of 241 Am were considered:<br />
13.9, 26.4 and 59.5 keV. For 57 Co the 121 keV peak was considered. The choice of such peaks<br />
allowed to uniformly cover the energy range of <strong>in</strong>terest. The spectrum from the energy<br />
calibration sources was acquired us<strong>in</strong>g Silena IMCA Plus programme for spectroscopy [138]<br />
and the peaks were visually located. The centroid of eack peak is calculated by the acquisition<br />
programme on the basis of a Gaussian filter for the fitt<strong>in</strong>g of spectrum peaks. Each<br />
Germanium detector was s<strong>in</strong>gularly calibrated us<strong>in</strong>g a 3 rd degree polynomial curve to fit the<br />
considered energy peaks. A m<strong>in</strong>imum least square fitt<strong>in</strong>g procedures was applied for this<br />
purpose.<br />
The poor energy resolution of phoswich detect<strong>in</strong>g system doesn’t allow to <strong>in</strong>dividuate<br />
each s<strong>in</strong>gle peak as for the HPGe detectors. Therefore a proper energy calibration curve was<br />
not calculated, but a spectrum for just 241 Am was acquired and the channels for delimit<strong>in</strong>g the<br />
region of <strong>in</strong>terest for the 59.5 peak energy were fixed.<br />
The efficiency calibration of both the detect<strong>in</strong>g systems were carried out by acquir<strong>in</strong>g<br />
the spectra of Americium loaded calibration phantoms. In the actual conditions of<br />
measurements, HPGe detect<strong>in</strong>g system was used for thorax measurements, and phoswich<br />
detectors for measurements of activity <strong>in</strong> lungs, liver, head and knee. In Figure 2.3.10 the<br />
measurement positions of the detect<strong>in</strong>g systems <strong>in</strong> respect of subject are presented. In case of<br />
measurements on the skull with the phoswich detect<strong>in</strong>g system (measurement position: Head),