CdZnTe and CdTe detector performance can be significantly improved wit
h low-noise electronics. The main sources of noise that broaden the sp
ectrum peaks in a room-temperature system are incomplete charge collec
tion and leakage current of the detector, and the feedback resistor of
the preamplifier. The detector leakage current can be reduced by cool
ing the detector to about -30 degrees C. Normally, at these temperatur
es the leakage current of a small detector crystal drops to the picoam
pere level which enables the use of low-noise, pulsed-optical feedback
preamplifiers instead of noisier resistive feedback preamplifiers. Al
so, because of lower leakage currents, it is possible to use higher bi
as voltages at low temperatures which is important for more efficient
charge collection. This reduces spectrum background and peak tailing.
Applying rise time discrimination circuitry to the linear amplifier re
duces the tailing effect even further, especially at higher energies.
By employing all these methods a number of Cd0.9Zn0.1Te, Cd0.8Zn0.2Te
and PIN-structure CdTe detector crystals were tested at temperatures b
etween -20 degrees C and -40 degrees C, and at best FWHM energy resolu
tions of 240 eV at the 5.9-keV line of Fe-55, 600 eV at the 59.5-keV l
ine of Am-241, and 4.4 keV (0.7 %) at the 662-keV line of Cs-137 were
obtained. These energy resolutions measured at room temperature with c
onventional methods are typically about 4 to 10 times poorer.