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Regional Basic Professional Training Course in Korea

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<strong>Regional</strong> <strong>Basic</strong> <strong>Professional</strong> <strong>Tra<strong>in</strong><strong>in</strong>g</strong> <strong>Course</strong> (BPTC) on Nuclear Safety<br />

delay of 10 ‐8 s or less. The emission of energy through phosphorescence and delayed<br />

fluorescence should be m<strong>in</strong>imal. In addition, it is necessary that sc<strong>in</strong>tillators be<br />

transparent to their own fluorescent radiation and that the photons emitted have energies,<br />

known as a spectral distribution, consistent with the response of available collect<strong>in</strong>g<br />

apparatus usually photocathodes. (Photocathodes play a role for sc<strong>in</strong>tillators similar to<br />

that of anodes which are the collectors for gas‐filled detectors. However, there is no<br />

analogous attraction of the photons to the photocathode, but rather an optical coupl<strong>in</strong>g is<br />

required to channel the light.)<br />

Pr<strong>in</strong>ciple of Operation<br />

The process whereby a substance absorbs energy and then re‐emits it as photons <strong>in</strong> the<br />

visible or near‐visible energy range, is termed lum<strong>in</strong>escence. The <strong>in</strong>itial excitation energy<br />

for this process has many orig<strong>in</strong>s such as light chemical reactions, mechanical stra<strong>in</strong>s,<br />

heat, and ioniz<strong>in</strong>g radiation. The last named causes a sc<strong>in</strong>tillation because of the<br />

excitation or ionization produced <strong>in</strong> the substance. Only sc<strong>in</strong>tillants that de‐excite<br />

promptly, i.e., through prompt fluorescence <strong>in</strong> 10 ‐8 s or less, are useful as radiation<br />

detectors. However, most energy deposited <strong>in</strong> the substance by ioniz<strong>in</strong>g radiation is<br />

quickly degraded <strong>in</strong>to heat. In choos<strong>in</strong>g a sc<strong>in</strong>tillation material, therefore, it is important<br />

to determ<strong>in</strong>e the efficiency with which the k<strong>in</strong>etic energy of charged particles is<br />

converted <strong>in</strong>to visible light and also to determ<strong>in</strong>e that this conversion is l<strong>in</strong>ear, i.e., that<br />

the light yield is proportional to deposited energy over as wide a range as possible.<br />

2.4.2.2. Semiconductor Detectors<br />

Another type of solid state detector, known as a “semiconductor” detector, also takes<br />

advantage of the properties of particular crystals. In this case, the crystal is a very good<br />

<strong>in</strong>sulator which under certa<strong>in</strong> conditions, can be made to conduct electricity. The typical<br />

semiconductor detector can be thought of as a sandwich with the crystal <strong>in</strong> the center and<br />

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