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40 4 Scintillation detec<strong>to</strong>rs<br />

Figure 4.9: Emission spectrum of CsI:Tl, NaI:Tl, BGO and CWO [36]<br />

and large a<strong>to</strong>mic number. It has very little self-absorption and its mechanical<br />

and chemical properties make it easy <strong>to</strong> handle. However its<br />

low light yield of just 10-20 % compared <strong>to</strong> NaI:Tl leads <strong>to</strong> a resolution<br />

of about a fac<strong>to</strong>r two worse than NaI:Tl. It also has a high refraction<br />

index of 2.15, making the light collection more difficult. BGO is suitable<br />

if high gamma ray detection efficiency is more important than a<br />

good energy resolution. The primary decay component is 300 ns and<br />

an additional fast component (60 ns) has a fraction of 10 %. The emission<br />

peak wavelength lies at 505 nm. The light yield increases at low<br />

temperatures, so it has a limited use at temperatures higher than room<br />

temperature. BGO is two <strong>to</strong> three times more expensive than NaI:Tl<br />

[26, 27, 28, 29].<br />

CADMIUM TUNGSTATE (CdWO4 or CWO) has been known as a scintilla<strong>to</strong>r<br />

since about 1950, but has been produced only since 1990 with<br />

interesting crystal size and good optical properties. The light yield is<br />

40 % of NaI:Tl and the emission peak wavelength is at 495 nm. The<br />

density and the effective a<strong>to</strong>mic number are even higher than these of<br />

BGO. A pulse shape discrimination is also possible. The use of CWO is,<br />

due <strong>to</strong> its long decay time of 1.1 µs (40 %) and 14.5 µs (60 %) limited <strong>for</strong><br />

low count rates. With an refraction index of 2.3 the light collection and<br />

coupling <strong>to</strong> readout devices are also difficult. CWO is more expensive<br />

than BGO [26, 27, 28, 29].

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