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Chapter I
The New Alchemy And The World of Neglected Dimensions
1. THE NEW ALCHEMY AND THE WORLD OF NEGLECTED DIMENSIONS
1 .1 The Emerging World of Materials Science and Technology
Materials have always influenced the basic fabric of human life. Using
new and ultraprecise technologies, researchers are probing worlds far tinier than
the submicroscopic realm of viruses.' They are peering into the world of atoms
and unlocking the secrets of how they interact. Using technology developed
primarily to deal with the rapidly decreasing dimensions of microelectronics,
modem-day alchemists are rearranging molecules - and even atoms - to assemble
novel substances.
Using modeling software that incorporates a wealth of knowledge from the
exploding field of materials research, one can design entirely new substances,
atom by atom. These include custom-made ceramic superconductors, and
ultrahigh strength plastics and alloys. There are reports1 of a super alloy of five
metals and the resulting extra-tough steel has been tested for bearings in space
shuttle engines and turbo pumps, which now must be rebuilt after every flight.
Researchers are making 'aerogels', often called 'frozen smoke', airy silicon
concoctions that far outperform the best insulators, ceramics pliable enough for
use in car or jet engines and composites embedded with artificial 'nerves' and
'muscles' that let them respond to stress almost as a living thing would, which are
called 'smart materials'.' The most dramatic advances have come in electronics.
To meet the increasing demand for improved performance in storing and
processing data, researchers are working harder than ever on techniques and
equipments to shrink silicon circ~itry.~"' One of the newest tools is the scanning
tunneling microscope (sTM)',~ that uncovers incredibly accurate information
about the positions of individual atoms on surfaces. The new materials are
pushing the speed of chips and computers to the edge of physical limits." These
advances, leading eventually to products such as hand held super computers, will
change the way of life.
The most important outcome of present research in materials science is the
creation of an entirely new class of materials - the nanophase materials often
called in the synonyms nanocrystalline materials or nanostructured materials?22
In nanophase materials, each crystal is less than 100 nm that is smaller than most
viruses. The individual crystals of most metals or ceramics consist of millions or
billions of atoms. But the grains that make up nanophase materials contain just a
few thousand. After these grains are squeezed under pressure, into a solid
material, they exhibit remarkable properties. Such superdense ceramics'37 can be
bend and molded like plastics and extruded or formed into a final shape without
the shrinkage normally typical of ceramics. Nanophase versions of metals such as
copper, palladium, nickel, etc. and inter-metallics are five times stronger as their 23-30 large-grained counterparts. Other extraordinary properties - optical, 31-35
36-40 magnetic and electrical proper tie^^'"^ - have been reported for nanophase
materials.
1.2 History of Nanostructured Materials
Nanostructured materials apparently had its genesis with the Big-Bang.
The structures of the earliest meteorites suggest that matter is formed by the
condensation of atoms into larger masses under the action of gravity.7 Many
examples of the natural nanostructures can be found as well in biological systems
from seashells to the human body.
Fine dispersion of gold14 was synthesized by Michael Faraday as early as
1857. In 1861, British chemist Thomas Graham coined the term colloid as colloid
chemistry was beginning to develop.13 Woltgang Ostwald classified the dispersed
systems of particles with sizes of about 1-100 nm as colloid. John Tyndall,
Hermann Helmholtz, Lord Rayleigh, James Clerk Maxwell and Albert Einstein
were among the physicists who studied the characteristics of colloids around 1900.
In 1915, Wo Ostwald entitled his famous book on colloid chemistry "The World
of Neglected Dimensions", implying that this was a science in its own right."
During 1930s, the new commonly used gas-condensation technique for synthesis
of small particles of materials was pioneered by A. H. Pfund in the United States
and H. G. Burger and P. H. Van Clittert in ~ e r m a n ~ . ' ~ Certain types of fine
particles22 have been produced commercially for more than half a century. During
the same period, Arne Tiselius studied the properties of protein and other
biological colloids and developed a precise electrical migration device.I3 In 1934,
the so-called Langmuir-Blodgett method became a new tool in surface chemistry.
By early 1940s, precipitated and fumed silica fine particles were being
manufactured and sold in the United States and ~ e r m a n ~ . ' ~
As long ago as 1959, Nobel laureate physicist Richard Feynrnann, in a
lecture before the annual meeting of the American Physical Society, predicted
about the creation of materials with new properties by the manipulation of matter
on a small scale:
"I can hardly doubt that when we have some control of the arrangement of things on a small scale we will get an enormously greater range of possible properties that substances can have" and "there is aplenty of room at the bottom".
-Feynman
By these keywords7, he strongly pointed out that there is a lot of scope for
research on materials on a very small scale. By 'small scale', again he meant the
dimensions of particles at the nanometer scale.
The theoretical formulation of quantum confinement of electrons by Royo
Kubo, at Tokyo University in the 1960s did much to launch the interest in the
nanostructuring of condensed matter, although ultrafine particles had long been
synthesized and used for their unique He pointed out that electrons in
metallic ultrafine particles are in a unique situation and do not obey Fermi
statistics because the number of such electrons is small. Kubo also noted that for
particles smaller than 10 nrn, it is difficult either to add or to remove a single
electron and such particles have a stronger tendency to remain electrically neutral.
The way this affects specific heat, magnetization and superconductivity is now r 7,13 called 'Kubo effect . Following Kubo's work, researchers began to understand
that ensembles of matter containing only tens to thousands of atoms could have
structures and properties quite different from those of conventional materials on a
coarser size scale, and work began in earnest around the world to investigate
ultrafine particles and ultrathin films of matter.
Also, in the 1960s, Ryozi Uyeda and his coworkers at Nagoya University
used electron microscope A d electron diffraction to determine the morphologies
and crystal structures of single particles of metals and metallic compounds. They
also made advances in producing relatively clean ultrafine particles through
evaporation and condensation in an inert gas. The 1960s saw the use of arc
furnaces to produce submicron particles of alumina, carbonated tungsten, Si3N4,
and other heat and acid resistant carbonates and nitrides of active metals and rare
earth metals.13
The interest on nanometer-sized particles in the 1970s included both
experimental studies and theoretical calculations of atomic and electronic
structures. Researchers during these years found that ultrafine iron particles that
are carefully covered with an oxide film less than 1 nrn thick are very stable and
resistant to weather corrosion at normal temperatures.43'4 During 1970s magnetic
fluids containing suspended iron oxide nanoparticles, which evolved from
technology developed at NASA in the late 1960s, entered the US market.14 By the
same period researchers in Japan developed 30 nm particles of magnetic alloys for
use in magnetic tapes. They found that an ultrafine particles made form an
iron-nickel-cobalt alloy exhibited excellent recording characteristics. The
Research and Development Corporation of Japan in 1971 instituted a five-year
development programme focused on metallic nanopowder production for magnetic
recording tapes.I4
The synthesis of materials by consolidation of small particles was first
suggested in the early 1980s by Herbert ~ l e i t e r ~ at the University of Saarlandes in
Germany and was applied initially to metals and then to nanophase ceramics. In
1981, a five-year ultrafine particle project known as Exploratory Research for
Advanced Technology (ERATO) was launched in Japan.
The 1990s have seen ever-increasing interest in nanostructured materials.
More than 5000 papers detailing research developments in the field were
published in the scientific literature during this period.
1.3 The Nanophase Regime
The properties of nanoparticles are so strikingly different from those of the
bulk material that some authors are even inclined to classify them as a new (fifth)
aggregate state of matter: liquid phase, solid phase, nanophase, gas phase and
plasma.58 The evolution of the structural, electronic and other properties, as atoms
form progressively larger clusters (nanocrystals) and particles leading to a
macroscopic solid has long been a challenging problem for solid state and
theoretical physicists. Many quantities such as the temperature, surface tension,
surface area and even volume that are used in the description of macroscopic
systems become ill-defmed as the size of the particle decrease^.'^"^ To understand
how molecules evolve into solids, the study of small particles that contain a few to
several thousand atoms are critical. They provide a new arena for probing the
interactions between atoms and offer new hope for the synthesis of new materials
possessing unusual proper tie^.^'
1.4 Unique Properties of Nanoparticles
Some of the unique characteristics of nanoparticles, which identify them from the
bulk material, are:
*:* Large surface-to-volume ratio: The uniqueness of very small particles lies in
their large surface-to-volume ratio.62b3 In the nanophase regime the fraction of
atoms associated with the surface is large and as the size of the particle
decreases the characteristics of the surface atoms become increasingly sharper.
Assuming that grains have the shape of spheres or cubes the volume fraction of
nanocrystalline materials associated with the boundaries can be calculated as
V& = 3d/D where d is the average grain boundary thickness and D is the
average grain diameter.I9 The volume fraction of atoms in the grain
boundaries can be as much as 50 % for 5 nm grains, about 30 % for 10 nm and
3 % for 100 nm grains.
*:* Quantum size effect: The dependence of the specific properties of nanoparticles
on their geometrical dimension is termed quantum size effect. 32-34.64-68
$3 The defect structure : Nanocrystalline materials contain such a high density of
defects (point defects, dislocations, dangling bonds, grain boundaries,
interphase boundaries etc.) that the spacing between neighboring defects
approach interatomic distances?6p12 This increased defect density can play an
important role in the electrical, optical and mechanical properties of
nanocrystalline materials.
*:* Thermodynamic size e f f e ~ t s : ~ ~ . ~ ~ ~ n important class of size effects involves the
dependence of some intensive thermodynamic properties, eg. surface tension,
vapor pressure and characteristics of phase transition, on the sample size and
shape.
Any attempt to generate materials with properties beyond the present
limitations has to focus attention on generating microstructures with new types of
atomic arrangement andlor new chemical compositions.
As far as the atomic arrangement is concerned, all existing materials may
be divided into crystal and glasses, which differ by the presence or absence of
long-range order, whereas the short-range order is s imi~ar?~. '~, '~ As properties
depend primarily on short-range order, the availability of materials without
short-range order appears attractive. By the generation nanocrystalline materials,
a new solid state structure without short-range order (i.e. solids with a completely
disordered 'gas-like' struct~re) '~ and the alloying of components, which are
immiscible in the solid andlor molten state may, however, be achieved.
The basic feature of nanocrystalline materials is the utilization of the atomic
arrangements in the cores of lattice defects (grain or interphase boundaries) to
generate solids with a new type of atomic structure. Because of the constraints
exerted by the two adjacent lattices on the atoms in the core of an incoherent
interphase, the atomic arrangements in the cores of grain or interphase grain
boundaries differ from the unconstrained atomic arrangements of glasses and
ctysta~s.'~
A schematic cross section through a hard sphere model6 of a nanocrystalline
material is shown in figure 1.2. All atoms are assumed chemically identical. As
far as the atomic structure is concerned, two kinds of atoms may be distinguished:
'crystal atoms', the nearest-neighbor configurations of which corresponds to the
lattice configurations; and 'boundary atoms' characterized by the nearest-neighbor
configurations which are different from the lattice configurations. Hence, in terms
Fig.l.2 Schematic representation of a nanocrystalline material distinguishing between the atoms associated with the individual crystallites (full circles) and those constituting the boundary network (open circles)
of nearest neighbor configurations, a nanocrystalline material consists of a
crystalline component (formed by all the crystal atoms) and a boundary
component with a froth-like morphology (formed by all the boundary atoms). The
atomic structure of all the crystallites is identical. However, the atomic structures
of the boundaries are different because their atomic arrangement depends, among
other parameters, on the orientation relationships between the crystallites. If the
crystallites forming the nanocrystalline materials are oriented at random, the same
applies to all other boundaries. As nanocrystalline materials contain typically
about boundaries per cubic centimeters, the interfacial component represents
the sum over 1019 atomic arrangements, all of which are different. If the
interatomic spacing do not occur preferentially, the interfacial component is
expected to exhibit no preferred interatomic spacing apart from excluding
interatomic penetration. In other words, the interfacial component represents a
structure, which exhibits no short-range order. This does not imply that the grain
boundaries are disordered. In fact, every boundary is assumed to have a two-
dimensionally ordered structure, the periodicity and interatomic spacing of which
are different from boundary to boundary. The physical reason for this new type of
structure of a solid material are the crystallographic constraints imposed on the
atoms in the cores of the boundaries by the adjacent crystal lattices of different
orientations. In grain boundaries, the atoms can only relax into structures
compatible with adjacent crystal lattice. The interfacial component has an average
atomic density, which is 10 to 30 % less than the crystal density, depending on the
type of chemical bonding between the atoms. 19,71,72 In glasses and crystals, no
constrains of this type exist. This has led Gleiter to coin the nanocrystals as a
'new form of matter'.19
1.5 Synthesis of Nanocrystalline Materials
Several novel methods have been developed during the past two decades to
prepare nanocrystalline materials. Increased activity on the synthesis of
nanocrystalline materials dates back to the pioneering investigations of Herbert
~ l e i t e r . ~ , ~ He synthesized the ultrafine metal particles in gas condensation
technique. Since then a number of techniques have been developed in which the
starting material can be either in a solid, liquid or gaseous state. These include 71-75 76,77 inert gas condensation, mechanical alloying, rapid ~olidification,7~ spray 79,80 conversion processing, sputtering,8' electrochemica1,8~ arrested (controlled)
precipitation, 30-34.50-51.83-87 88-91 sol-gel process, microemulsion t e ~ h n i ~ u e : ~ - ~ ~ Ball
Milling, 96,97 98.99 hydrothermal method , solvothermal method,Io0 plasma
processing, 101,102 laser ablation, 103-105 . ion exchange rpocess,106 sliding wear,Io7
spark erosion,'08 torsional deformation technique,109 etc. The grain size,
morphology and texture can be varied by suitably modifying the process variables
in these methods.
A central underlying theme in all these methods is to energize the material
to bring it into a highly non-equilibrium (metastable) state (also including a
possible change of state from the solid to liquid or gas) through melting,
evaporation, irradiation, application of pressure, storing of mechanical, energy,
etc. The material is then brought to another lower-energy state by quenching or
related process when it can exist as a supersaturated solid solution, metastable
crystalline or quasicrystalline phase, or even in a glassy state, affording ample
opportunities to modify the crystal structure andlor microstructures. In principle,
any method capable of producing ultrafine polycrystalline materials (by increasing
nucleation rate and reducing the growth rate during formation) can be utilized to
produce nanocrystalline materials.
Even though all of the above methods have been used to produce
nanocrystalline phases, gas condensation, sol-gel process and controlled (arrested)
chemical precipitation techniques have been most commonly employed to produce
nanocrystalline materials in large quantities.
In chemical precipitation technique, the rate of nucleation consists of two
exponential factors.22 Of these, one is an expression of the probability of forming
a nucleus of size greater than the critical size, and the other is concerned with the
rate at which material can be supplied to the nucleus for growth. Once a nucleus
has exceeded the critical size it will continue to grow at a rate controlled by the
provision of fresh material in the correct orientation at the surface of the growing
nucleus and by the ease of formation of new bonds in the required positions. The
requirement for the production of a fine powder having dimensions of few
nanometers is initially for the formation of a large number of nuclei, the
subsequent growth of which is restricted. To produce many nuclei a high degree
of supersaturation is necessary and, as a result, nucleation will tend to be
homogeneous. Under these conditions, the size of the critical 'nucleus is
approximately inversely proportional to the degree of supersaturation. Rates of
nucleation and growth vary widely in reactions in which a precipitate is formed
and, consequently, there are wide differences in the effect of conditions on the
particle size of the final precipitate. After precipitation is complete, there is still
change in the particle size distribution in the precipitate. The agglomeration of the
particles can be eliminated by using a suitable stabilizer or capping agent2* The
capping agents are known to inhibit the growth of particles, since the polymeric
chain is strongly bound to the metal ions near the surface of the nanoparticles. ,3436
When a precursor is used for the production of a nanocrystalline material,
the particle size of the product depends mainly on two factors viz. temperature at
which the decomposition is performed and the rate of decomposition.22 The size
of the particles of the resulting powder can be controlled by suitably selecting the
above two parameters. A t h e r m ~ ~ r a m " ~ can be used to choose these factors.
1.6 Techniques for Characterization of Nanocrystalline Materials
The complete characterization of a nanocrystalline material requires a
variety of techniques and instruments. The nanocrystalline materials should be
characterized on both atomic and nanometerscale. The microstructural factors to
be taken into account during characterization include:
chemical and phase composition
size distribution, morphology and roughness of the primary particles
nature and morphology of the grain boundaries and interphases
surface area of the primary particles
number and size distribution of pores
whether single crystalline, polycrystalline or amorphous
state of surface and interfacial stress
nature and concentration of defects
presence of adsorbed film or adsorbed impurities
state of agglomeration
identification of residual trapped species from processing
Presently, a number of simple as well as sophisticated experimental
techniques are available that can yield structural information on nanocrystalline
materials. These include direct microscopic techniques such as Scanning Electron
Microscopy (SEM), Transmission Electron Microscopy (TEM), High Resolution
Transmission Electron Microscopy (HRTEM), Scanning Tunneling Microscopy
(STM), Field Ion Microscopy (FIM), Atomic Force Microscopy (AFM) and the
less direct x-ray and neutron diffraction techniques. Indirect spectroscopic
techniques such as EXAFS, NMR, Raman and Mossbauer spectroscopies and
Positron Annihilation Spectroscopy (PAS) have also been used. Other useful tools
include DSC, Mass Spectroscopy, X-ray Fluorescence and ESCA (XPS and UPS)
The broadening of x-ray diffraction line is primarily a measure of the
departure from single crystal perfection and regularity in the specimen. IIL,112
Thus, in addition to small size, lattice strain, dislocations, impurities and other
defects lead to line broadening. Nevertheless, as the only method which gives the
size of the primary crystallites irrespective of how they are aggregated or sintered,
x-ray diffraction broadening is of great value for research in nanocrystalline
materials. X-ray line broadening can also be used for analysis of particle shape.
Some of the diffraction lines will be markedly more broader than others. This
broadening is due to the shape and orientation of the particles.
1.7. Improved Properties and Applications
Nanocrystalline materials exhibit a variety of properties that are different
and often considerably improved in comparison with those of the conventional
coarser-grained polycrystalline materials. Several potential technological
applications are suggested based on the special attributes of nanocrystalline
material. 2.4.14
The improved properties, which may be put to use in industrial and technological
applications, include:
Thin films and coatings - the smaller the particle size, the thinner the coating
can be.
Electronic ceramics - reduction in grain size results in reduced dielectric
thickness and improved dielectric properties.
Strength-bearing ceramics - strength increases with decreasing grain size.
Cutting tools - smaller grain size results in a finer cutting edge, which can
enhance the surface finish.
Impact resistance - finer microstructure increases the toughness of high-
temperature steels
Cements - finer grain size yields better homogeneity and density.
Gas sensors - finer grain size gives increased sensitivity.
Adhesives - finer grain size gives thinner adhesive layer and higher bond
strength.
Chromatography - the increase in specific surface area associated with small
particles, allows column lengths to be reduced.
The vast range of technological and industrial applications of fine particles
is largely a direct result of their diversity of structure on microscopic and
mesoscopic scales. Industry has long used fine particles in dyes, pigments,
adhesives and catalysts. Since reducing the grain size to nanometer-dimensions
can provide increased strength and hardness, supertough and superstrong ceramics
can be synthesized.19 Such superceramics may find use in several engineering
applications such as high efficiency gas turbines, and in aerospace and automotive
components.' Nanocrystalline materials can be made into wear-resistant coatings
or pressed and sintered to make rigid objects. Applications of such powders
include fine drill bits and cutting tools.
Since the optical transparency of nanocrystalline ceramics can be controlled
by controlling the grain size and porosity, they may find application in optical
filtration technology. The main demand for optics having surface roughness in the
0.1 nm range arises from the requirements for high energy laser mirrors, to reduce
laser-induced damage,''' and to minimize scatter in laser gyroscopic optics and x-
ray optics.
The increased diffusion rates in nanocrystalline metals and ceramics
considerably reduce the temperature at which sintering can occur.19 The enhanced
diffusivity can be used to make gas sensors and fuel cells capable of operation at
much lower temperature.4
The electrical and magnetic properties of nanocrystalline materials will
probably form the basis of their widespread and industrial applications. The
phenomenon of giant magneto resistance (GMR)'~ is now shown to be present
even in equiaxed nanocrystalline materials. Thus, nanocrystalline materials
exhibiting large GhtR can be promising candidates for the reading heads of the
next generation of information systems. The excellent combination of soft
magnetic properties can be useful in producing tape-wound cores for common
mode chokes, saturable reactors, high frequency transformers and magnetic heads.
Another useful property of nanocomposites is the magnetocaloric effect, which
can be used for magnetic refrigeration replacing compressed gas containing
harmful CFC'~.
Fine particles of latex, which is an organic polymer, are commonly used as
a vehicle for biological and chemical manipulation in the pharmaceutical industry
and other fields." Aerosols, which are fine dispersions of a solid material in a gas,
are used in agriculture, forestry, military technologies, and medicine.
Nanoparticulate thin films possessing desirable electronic qualities would
be of great interest in microelectronics. To meet the increasing demand for
improved performance in storing and processing data, researchers are working
harder than ever on techniques and equipments to shrink silicon circuitry.
Chipmakers are entering a realm where transistors will be too tiny to print on
silicon. Instead, they will be grown in the material as clusters of atoms. 114,115
Nanometer-sized structures perpendicular to the substrate have been produced by
x-ray, electron- and ion-beam t e ~ h n i ~ u e s ~ . " ~ Nano-devices based on GaAs have
captured a significant amount of attention because they offer the highest digital
processing speed coupled with the additional advantages over the silicon of having
a higher temperature tolerance and having greater radiation re~istance.~
A bridge-like Josephson junction having a bridge length of the order of the
coherence length of superconducting electrons, which is about a few nanometers
offers an entirely different approach to the development of high-speed digital
circuits.
1.8 A Look into the Future
Research publications in various journals over the past two decades
indicate that there are tremendous opportunities for synthesizing nanostructured
materials with new architecture. This synthesis can be done from atomic or
molecular precursors via the assembly of atom layers and clusters and by a myriad
of other techniques now becoming available, such as nanoscale lithography and
biological templating.
By extrapolating thin film technology and nanoscale lithography for
miniaturization, it may take approximately one decade for electronic switches to
be reduced to molecular dimensions. The impact of molecular biology and genetic
engineering has thus provided a stimulus to attempt engineer upwards, starting
with the concept that single molecules, each acting as an electronic device in their
own right, might be assembled using nanotechnology, to form molecular
electronic devices (MEDs) or open biochip computers (BCCs). Conducting or
insulating molecular wires would be built up in some areas. This field of
molecular electronic devices is a promising filed.
Nanoelectronics will be the watchword of the coming revolution in
semiconductor devices. Chipmakers are entering a realm where transistors will be
too tiny to print on silicon. Instead, they will be 'grown' as clusters of atoms.
Tinier transistors can be packed more closely, which means more powerful
circuits, which run faster. When these technologies are perfected, they will bring
'quantum leaps' in performance of all things that use chips. A shirt-pocket
supercomputer as well as memory chips that hold a library can be real. A
technique called band-gap-engineering looks like the best way to harness quantum
electronics. Researchers are looking to band-gap engineering to fashion quantum
wires having a cross-section of about 30 x 30 atoms.
It is now becoming apparent that scanning tunneling microscopy (STM)
may provide the basis of a new technology, which can be called scanning
tunneling engineering. An important broadening of STM technology is emerging
through the realization that the tip can be employed for purposes other than
microscopy, and that the tip may be used to modify the surface of the sample in a
number of ways. The STM tip has demonstrated its ability to draw fine lines,
which exhibit nanometer-sized structure, and hence may provide a new tool for
nanometer lithography. "7x"8 The first step in atomic-scale writing and reading
have already been taken, and if the technology could be fully implemented, would
lead to the development of computers unprecedented power and speed.
In scanning probe microscopy, a tiny sharpened tip, such as that in STM,
can move atoms and create atomic-scale images.2.4 If many developmental
hurdles can be overcome, the technology holds the promise of being suitable for
storing bits of information by moving atoms 'on' or 'off a surface.
According to Bernard S. Meyerson, an IBM physicist, "By getting the
dimensional control down to atomic level you can do pretty amazing
things ........." and ".....never bet on what somebody can't do"'. K. Eric Drexler,
the avatar of nanotechnology predicts that, in the course of a few years, by using
nanotechnology one could produce anything form a rocket ship to minute disease-
fighting submarines that roam the blood stream and like biological cells, the robots
that populate in a nanofactory could even make copies of themselves. The
Drexlerian future posits fundamental social changes: nanotechnology could
alleviate world hunger, clean the environment, cure cancer, guarantee biblical life
spans or concoct superweapons of untold horror. For the time being, nanoists can
only wait for these breakthroughs to arrive, while continuing to formulate their
computerized models of molecular machine parts.
The keys to the future of nanostructured materials, however, are our ability
to continue to improve the properties of materials by artificially structuring them
on nanometer length scale and our ability to develop the methods for producing
these materials in commercially viable quantities. Based on what we have learned
to date about mesoscopic physics and on the successes secured by the entry of
nanostructured devices into industry, it appears that the future holds great promise
for nanostructured materials.
1.9 Scope of the present study
Present work consists of the synthesis, characterization and a systematic
investigation of electrical properties of nanophase ZnO and its nanocomposites
with other nanoparticles of A1203, CdO and silver. These materials were selected
for the present study in view of their technological importance. The size and
crystallinity of the nanoparticles were determined using x-ray diffraction and
Transmission Electron Microscopy (TEM). The effect of particle size on the
vibrational properties was investigated by FT-IR spectroscopy. The ac electrical
properties of nano-ZnO and of the nanocomposites Zn0-A1203, ZnO-Ag and
ZnO-CdO were analyzed in detail by using impedance spectroscopy. The
investigation of ac and dc conductivity and dielectric properties of consolidated
nanoparticles of these materials were performed. The change in properties of
these materials compared to their bulk counterparts is attributed to the size effect,
defect structure of the grain boundaries, grain boundary structure modification and
grain boundary interactions.
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