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Background
The attempt to develop and understand materials with new and useful properties
is perhaps the most fundamental of all scientific endeavors; the use of
the terms "stone age," "bronze age," and "iron
age" is indicative of the value of materials to society, and the extent
to which a society is defined by the materials it uses. Recent years have
demonstrated this point more firmly than ever before as materials such as
aluminum, teflon, and silicon have found their way into every aspect of
our lives. Most recently, condensed matter science has engendered a new
and compelling member in this progression: artificially structured materials.
Comprised of amorphous metals, granular materials, metastable crystalline
alloys, superlattices, etc., artificially structured materials have grown
rapidly in importance during the last decade. There is an underlying reason
for the widespread interest in these materials. They each offer one or more
degrees of freedom not found in ordinary materials--degrees of freedom
over which the investigator has a great deal of control. Using this capability,
a researcher may tailor a new material to meet his or her needs--either
for the investigation of fundamental phenomena or to effect some practical
application. For fundamental studies, we may tailor the material to suppress
some well known phenomenon; this allows us to study subtle effects which
are usually overshadowed in natural materials. For applications, the properties
of the material may be tailored to suit some technological need.
Artificially Structured Materials
In my research, I study the magnetic properties
of artificially structured materials (ASM's). For now, I will focus on amorphous
metals, also known as metallic glasses. Metallic glasses are metals (they
conduct electricity, and may be magnetic) yet they are also glasses. That
is, they have no crystal structures, and thus share some of the properties
normally associated with glass. Some display a great resistance to corrosion,
and many are brittle compared to other metals. These materials are interesting
both as the subjects of fundamental research (for example, on the origins
of magnetism and electrical conductivity) and because they have many technological
applications. For instance, metallic glasses are now being used to improve
the efficiency of power distribution transformers.*
As an example, let me turn to metallic glasses again. Because the atoms
do not have to lie on an orderly crystal lattice, it is possible to make
mixtures of different metals (alloys) which cannot be made in crystalline
form thus the composition is a degree of freedom that the researcher can
control. Also, by heating the metallic glass, it is often possible to partially
crystallize the material. By changing the amount of heat, the degree of
crystallinity is also controllable. This process is used to fine tune the
metallic glass used in high frequency transformers. These are similar to
the power transformers mentioned earlier, but are smaller and are used in
high speed electronics.
Other examples of ASM's include multilayered structures, quaicrystals, and
granular metals. I cannot discuss all of these here, so I will focus on
multilayers, which are atomic level "club sandwiches." These structures
contain alternating layers of two or more elements. These layers are extremely
thin--sometimes only a few atoms across. In this case, the degrees of freedom
include the compositions and thicknesses of the layers. Structures such
as these are now used as read head elements in high-capacity hard disk drives. They have also been used in fundamental studies, as
a means of understanding the transition from two dimensional to three dimensional
behavior. Other applications include the velocity sensors that are used
in antilock brakes.
* These are the transformers that convert high voltage electricity in power
lines to 120 and 240 V power used in people's homes. They usually look like
a big cylindrical can located at the top of a telephone pole, or like a
large green box on a concrete pad near the edge of a property.
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