According to a barrier photoconductance theory recently developed, two
current noise sources can be envisaged, related respectively to the f
luctuation of the barrier height (photoinduced noise component) and to
the trapping-detrapping processes in shallow states within the photoc
onducting material (g-r and 1/f noise component). It is shown that the
first noise component, which can be separated by the second one, give
s information on the energy gap and on the photoionization cross secti
on of the deep energy levels of the photoconducting material. In parti
cular for thin films it will be shown that the photoionization cross s
ection of the deep energy levels varies inversely to the total number
of photons impinging on the photoconductor and proportionally to the n
oise power spectral density as the photon energy changes. Such relatio
nship suggests that the wavelength dependence of the noise power spect
rum provides the correction to be taken into account if the constant p
hotocurrent method is used and the variations of the minority carrier
lifetime with the photon energy cannot be disregarded. Results concern
ing the energy gap and its temperature dependence, in the interval ran
ging from the room temperature to 200 K, are reported and compared wit
h the results found in the literature for CdS based samples. The photo
ionization cross section of the deep centers as a function of the phot
on energy, at room temperature, is reported for the same sample. Such
quantities have been obtained by measuring the spectral density of the
photoinduced noise vs wavelength at constant photoconductance value.
As for the other kinds of noise spectroscopy, the main advantage of th
e present method is to work out in the operative condition of the semi
conductor device. (C) 1996 American Institute of Physics.