Abstract:
The growth and study of dielectric layers are
receiving greater attention because of their wide and
diversified applications in the fabrication of Thin-film
distributed RC networks, interfacial devices, integrated
circuits and in surface passivation of semiconductors etc.
The performance of these devices and in particular, of those
made with amorphous semiconductors is highly dependent on
the quality of the insulating films used in them. Most of
the amorphous semiconductors have very high resistivities.
This imposes a condition on the resistivity of the dielectric
layer to be still higher. Several oxide and nitride films
such as silicon dioxide (SiO ), silicon nitride (Si_N, )
have been studied to meet these requirements but none of them
resulted in stable high-quality dielectric layers. The use of
alumina (AlpCL) layers as a dielectric has proved to be more
promising as it is free from the instabilities like migration
of foreign ions at elevated temperatures and high electric
fields.
Accepting this fact, a process of growing highquality
alumina dielectric layers by wet anodization technique
was developed. The electrolytic bath used consists of boric
acid buffered with ammonium hydroxide and diluted with
ethylene glycol. The properties of the alumina layers grown
with this bath were found superior as compared to those
grown in tartaric acid bath under the similar environmental
conditions in the laboratory. The anodization process was
optimised by studying the effect of pH and the concentration
of the boric acid in the electrolytic bath.
Several Al-AlgCL-Al MINI structures were fabricated
to study the quality and reproducibility of the as-.grown
alumina dielectric layers. An arrangement for vacuum holding
of the substrate on brass stage and a micromanupulator with
two platinum ball tipped probes was constructed to make
electrical contacts with the base aluminum film and top
aluminum counter electrode of MIM structure. The whole
arrangement was enclosed in light-tight grounded metallic box.
The quality of the dielectric layer was determined by
measuring its electrical parameters like resistivity, di
electric constant and breakdown field. The dependence of the
capacitance density and dissipation factor on frequency and
the anodization voltage were also studied and reported in the
thesis. The dissipation factor was strongly dependent on the
post-baking of the alumina layers.
The as-grown high-quality low-loss alumina dielectric
layers were used to fabricate the distributed RC (RC)
structures. The RC structures provide the characteristics
such as sharper cut-off in filters and large phase-shift with
less attenuation which can not be achieved with the circuits
employing finite numbers of lumped elements. Fabrication of
RC structures particularly for applications in audio frequency
range where large values of Rpand Cj are required, is difficult
as they need dielectric layers of large area free from
defects. Several uniformly distributed RC (URC) structures
were fabricated using the as-grown high-quality alumina as
a dielectric layer in between a top resistive film and a
bottom aluminum conducting film. The top resistive film was
deposited on the alumina layer by flash evaporation of
nichrome through the mechanical mask. The characteristics
of notch network made with this URC structure in coniunction
with lumped resistor have been studied. Unfortunately the
RC structures fabricated with alumina dielectric layers
showed high leakage and, some times, even short circuit from
the top resistive film to the bottom conducting film when the
measurements were conducted on the structures after a month
or so for determining the stability of the films with time.
The use of silicon-monooxide as a protettive film over the
alumina dielectric layer was thought to be the solution of
the problem. Thus the URC structures were fabricated with
composite dielectric layer consisting of alumina covered with
thin layer of silicon-monooxide as a protective layer. These
URC structures were used to form different circuits such as
one port two-terminal networks', low-pass, high-pass, band
pass and notch filters; attenuators and phase-compensating
networks. The effect of variation of lumped load across out
put terminals on the characteristics of the above filter
networks was also thoroughly investigated. Adetailed study
of the effect of variation of lumped resistor on notchfrequency
as well as notch-depth is also presented. The
geometrical tapering of RC structure results in very useful
improvement in cut-off rate of attenuation versus frequency
characteristics of the filters and produce more phase shift
with less attenuation than obtained with a URC structure.
The exponentially tapered RC (ERG) structures with different
degree of tapering were fabricated with the composite di
electric layers to study the effect of tapering on the
characteristics of the above networks fabricated with URC
structures.
The experimental results were compared with the
theoretically computed ones to check their authentisity and
accuracy. The analysis of RC networks made with RC structure
in conjunction with lumped and active elements using con
ventional methods is very complicated and lengthy. Avery
simple and straight forward technique for analysing above
mentioned experimentally-studied and other networks was
developed and is presented in the thesis. The three..terminal
two port RC structure is replaced by pi and tee lumpedequivalents.
The three impedances of each lumped-equivalent
model are expressed in terms of the characteristic function
of RC structure. To make the analysis more easier the new
and modified characteristic functions are used. It has been
shown that the clearer insight into the mechanism of null
and the optimum notch-parameters of the notch network can be
obtained by analysing only one of each of the impedances of
the pi and tee lumped-equivalents. The scope for further work
in this field is also discussed in the thesis.