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Materials physics
" I3 ^2 _- T, Q8 {1 o1 ~: r0 nP. Chaudhari
/ p9 P/ l" v2 N8 p" g" A. X2 Y; |IBM Watson Research Center, P.O. Box 218, Yorktown Heights, New York 105981 W) @$ D8 ^' Q: `% W
M. S. Dresselhaus* n. ~ C/ z/ T
Massachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307
( n2 y. b" ^! t2 ], n' R( C8 [4 K1 ?Extraordinary advances in materials physics have occurred over the last century. These advances have( n3 c- ]; k7 b+ X" Q" \+ ]* y
influenced almost every aspect of human endeavor. In this note, the authors sketch some of these7 |1 L7 f* v3 r( X: \
exciting developments in structural, polymeric, and electronic materials. [S0034-6861(99)01502-0]( k- B5 }+ ?7 |6 N) X6 I
I. INTRODUCTION
4 b' u1 R) w6 u- w% c6 }- kOver the last one hundred years there have been stunning
' j& e6 b) u ?7 [- Nadvances in materials research. At the turn of the
8 U) [7 o7 j2 n- v- A, jlast century we did not know what the atomic structure
1 R S; \4 o: g mof a material was. Today, not only do we know the structure,& N9 x+ I7 L/ a/ M$ f) e
but we routinely make artificial structures that require" I2 R9 h r( _3 J; O: d
placement of atoms at specified locations, that mix2 o9 O5 ]7 W% G' B! Q+ L5 \
atoms to create properties not found in naturally occurring' \4 W' U5 u: B4 R
materials, that have the functionality needed by today’s" v1 F* z# {5 _7 \' M
technology, and that adjust their properties to a
: V0 N- T+ f T/ W7 a- c/ Achanging environment (smart materials). Over the last
i" q1 E ^9 I! @$ bfew years we have begun to manipulate individual atoms
$ _ x* @/ x, C8 m* s9 }2 Lto form structures that enable us to explore scientific3 o( z" s5 P% ~' C% D! G6 P9 s
issues, but that will surely lead to profound technological
u3 h" Z0 A) Q2 N6 Oand social consequences; for example, the manipulation
0 [, x' J* b: V" J! F0 K8 dof nucleotides in a DNA molecule, which is then
; }% b( m4 r/ f; T! _correlated with the functioning of, say, a gene and with
/ J. L; g/ M M) ^0 S. c# D" Iits expression in the control of disease.3 Y! [7 T$ _% t. B9 P
A hundred years ago there were no electronic devices,6 a/ b# A4 c6 ~3 I/ P
and today there is hardly any electrical appliance without
4 Y' o4 K! P( N9 v; h/ @+ }0 O! ~' Ythem. It is anticipated that in the near future there
: ?9 t7 k [8 x, F, Dwill be a microprocessor embedded in almost all electrical
7 L4 H8 J) ^/ ` P. G% fappliances and not just in those used for computation
2 p% h+ O" e+ ? @7 Por information storage. These devices, inconceivable a
& U: H `% @2 x* c& x t( Y7 X4 hcentury ago, could without exception not be made without' Z; Z- f& c& {$ i; T }& y
the knowledge gained from materials research on' x; A1 N9 h6 Y. x3 w+ O
insulators, semiconductors, metals, ceramics, and polymers.2 N6 z' l% N% E9 p
At the end of this century, we have begun a debate6 F/ Q+ U* a+ w2 X
on how far the present devices can continue to develop,
1 v, \" d! q$ Y* Bgiven the limits imposed by the speed of light and
$ m$ P' v% t5 d9 o. f0 ithe discrete nature of atoms, a debate that would have8 F4 f/ n8 w/ } P8 X, e3 x9 D
been incomprehensible to scientists and technologists of+ ~% w5 ~1 v0 k) B( w+ n
a century ago and a debate in which we now discuss the
/ }6 N) F' y6 R, L' }( t* z3 U7 Hpossibilities of using single electrons to switch a device
* Y' c$ q8 U- V. xon or off.0 H; ]6 q: C) ?2 l
Our ability to measure temporal phenomena was limited i4 T1 t% X2 J4 S5 B
to fractions-of-a-second resolution a hundred years
7 i+ I9 a5 F2 c x2 [: Y7 oago. Today we can measure changes in properties with a
- o7 S2 u; I! b: U( I# kfew femtoseconds’ resolution. Strobelike probes enable3 E( l9 L& A- l+ O4 K9 n
us to measure phenomena ranging over time scales covering! n7 s# t) S' M; V4 W$ M: Y) ^
more than ten orders of magnitude. We can, for
6 i4 @' K: C' U7 A" |example, study the relaxation of electrons in a semiconductor
h* m" }- \4 ?2 ~8 xon a femtosecond time scale, the visible motion2 c8 q0 D- J7 O( j4 X. {: ]* E
of bacteria in a petri dish, or the slow motion of a sand
, J7 Y( z; X$ |2 W# E# ndollar on a beach.
4 f9 p) `) J7 K( @" H3 iMaterials research spans the range from basic science,
7 E% }! `& m* R7 {through engineering, to the factory floor. This has not1 x1 \ ^. X. H" W# a. r
changed over the last hundred years or, for that matter,
. M: Q6 t9 ^' k' K, @4 r2 z( ^throughout the history of human civilization. Materials1 J# U3 _, S/ v, W
research came out of the practical needs of mankind.: y/ W9 l- @4 s& I3 |
Eras of civilization were named after materials, so central4 e7 K2 M8 H" _9 J j
has been their role in achieving mankind’s mastery
$ n' L* u2 [% x/ pover nature. The field of materials research can trace its8 N3 u$ N: C9 B8 P/ K' }
roots to alchemy, metallurgy, natural philosophy, and
6 N+ r1 J5 W( ~, o6 g& ?+ ]even art, as practiced over many centuries. However, the
" J* L _. Q8 kfield of modern materials research, as represented by
0 Q# y& q+ d7 T9 ?# s) Q/ v, G, Lmaterials physics, is only about sixty years old.2 j# ^1 r/ J9 ]0 b, E3 J' g6 I
Shifts in materials usage from one type to another are
/ C! v% J( P( D( ?. Ausually gradual. This is due to the very large investments
& G2 Z6 a4 G$ {3 dassociated with products in the materials-related industries,4 \9 g9 y' ?9 U" S; j6 d
complex relationships between reliability and functionality," s& u; T' G. V1 O2 i, r6 O1 l: j
environmental issues, and energy demands.! V2 J2 c* E- G2 ~/ I
However, measured over time, these shifts become quite
. ~8 Z" P' g- l, W2 | M% M/ W+ Dperceptible. For example, in automobiles the ratio of* n* y& i& n8 b+ n1 Y3 o9 l
plastic components to iron-based alloys has changed& f' Y$ K7 W' b5 k" F6 R" G8 z
from less than 3% to more than 15% over the last two
) Y; c! v6 Z( u* @) \decades. Although the percentage change appears to be
`/ E5 r$ g; k; }modest, the actual volume of material is large; over 40
$ v7 }6 }+ i4 kmillion tons of structural materials are used annually in
) t- c. }: K# q( Lcars.. ^6 _) H$ K2 } b7 t' y0 I
The advances of materials research in this century,1 X8 O% D& `4 c1 @- K z9 {8 v
which far exceed those of all prior centuries put together,
8 D+ ~! X8 a. w8 n6 [can be illustrated by three examples: structural,1 _0 {* I' T r, C4 A0 z
polymeric, and electronic materials. Our choice of these
+ d9 f: s: u. h' t* hthree is somewhat, but not completely, arbitrary. It is. H8 Y, L5 Q) C! S3 i1 Z8 I8 X3 V
out of structural materials, particularly from the fields of
% n4 j) `2 e* @metallurgy and metal physics, that modern materials
0 b% C( D6 \! z# [! f) g- O/ A& Kphysics has evolved. From the crude weaponry of our
" ^! L1 B: k* lforefathers to our mastery of air travel, space flight, surface
) Z8 Z1 t" v+ y9 R; i& ?# Y$ x+ mtransportation, and housing, structural materials
9 h+ z' b0 a0 W$ a9 xplay a role that is unequivocally important. Nature uses
* |; H( a; t( D4 J- i9 _the second category of materials, polymers, in amazing! ?3 i. x/ ~' \: z) ?* v
ways, to perform very complex functions. We humans
/ k- X2 b" ~: e% p1 V% oare an example of that. Over the last hundred years, we9 S. C7 D( O; ?: x" {! O6 y
have begun to understand and develop polymers for$ ~3 O6 h6 D, d. o N' y( {
uses in food packaging, fabrics, and structural applications./ P. c$ ^7 K% k
We anticipate that polymer research will play an) }% [* Y/ N6 B/ u7 V2 I
increasingly important role in biomaterials of the future.5 T- o6 v3 y5 `5 n- o4 X" h2 V
The third category, electronic materials, were not conceived
$ A5 Z j9 `- }3 S4 yuntil quantum mechanics was discovered in this
! U8 c7 L* e6 }' V X/ W7 ?. _century. Today we cannot imagine a world without telecommunication, I& {7 E9 [6 _/ J
computers, radio, and television. These
$ P* Y3 G: `9 c8 U9 t: Q/ p0 jand future devices that will make information available
5 p$ z0 b' ], q2 w+ {( y6 C0 {, |Reviews of Modern Physics, Vol. 71, No. 2, Centenary 1999 0034-6861/99/71(2)/331(5)/$16.00 ©1999 The American Physical Society S331
& i) J# U7 H' d+ w; ^* `instantly are only possible because of advances in the5 l% M1 ]$ J d s, p1 b3 e
control of materials structure and processing to achieve) b0 z6 w: k; {# X, G
a desired functionality.
6 h. w1 K2 e. w7 G; x& a! ?1 qII. STRUCTURAL MATERIALS3 ^3 ^4 O3 C6 S/ x
At the turn of the last century, mankind’s use of structural8 Z, i8 z- d* D, }7 |
materials was limited primarily to metals, particularly
3 N/ d u( i8 a+ z+ c4 Giron and its alloys, ceramics (most notably Portland
' m/ _0 S K; |cement), and polymers, which were limited to naturally) h# q, @. L0 E3 A0 l; D+ h
occurring rubbers, glues, and fibers. Composites, as a
4 w% ~) H3 x! {% A0 L l: E. Bconcept were nonexistent even though wood and animals,
# v, D6 l6 L) ?8 s- }% Weach composed of different materials, were used in+ {7 S3 R* ^9 K& _* B) E9 Z0 E
a variety of ways. However, the uses of alloying to enhance
4 y9 x8 ]6 ]- p dthe strength of lightweight materials, such as pewter,( A. v% @0 n1 x" Z
or copper additions to aluminum, were established
1 B# y! `6 N+ e0 V/ Stechniques, known well before this century. This knowledge
7 S) K% G# g( f) a9 G- ^- `2 x3 h2 r* Twas used to build the first dirigibles. The useful
4 y4 l8 X5 ^* r& `8 Znature of a material was often understood through serendipity. q' I1 ]; v* F' B. u
and not through an understanding of its structure
& U( ~# }" L2 M7 N3 U( Eor the relation between structure and properties.7 y: I! m+ F( J/ ]% C( Z0 T L
We still cannot predict in any quantitative way the evolution
) i1 W; w) y1 H. tof structure with deformation or processing of a0 e% G2 k4 k, m% x
material. However, we have come a very long way from+ Y, L7 q1 n( A& J
the situation that existed a hundred years ago, thanks to
' Q$ K* E6 Q1 Y. |; M( othe contributions of twentieth century science to our understanding. Y4 i% y% q. K+ N
of atomic arrangement and its determination* r) k3 Z8 T. `; d
in a material. Our classification of materials by symmetry+ Y1 }7 Z" o$ ]
considerations came into existence once atomic4 V C, i! O: U5 a& s' X
arrangement became known. To the seven crystal systems+ ?8 W! E" b* G% Q& V
and amorphous structures, typified by the glasses
k0 E" N/ ^1 S& x4 f& B Zand liquids, we can now add quasicrystals and molecular: Z- G+ x$ F- {" ~4 N9 h
phases, such as fullerenes and nanotubes, in a crystalline) m# |0 T. W% Q1 ^
solid.
! Q( f2 y W2 G- \8 a2 cThe crystal systems define perfect crystals. At finite
( ^4 t; M! P7 D: ]) G+ ztemperatures, the crystals are no longer perfect but contain( j4 a( u4 [& x: z. f, G
defects. It is now understood that these defects are) w' Q) q' P0 ?5 ?& H) v6 c7 a3 w) g
responsible for atomic transport in solids. In fact, the8 A* H9 u$ @- d; [4 _4 c2 k# c
structural properties of materials are not only a function
4 A2 c1 x0 G" M D8 M: Q5 Iof the inherent strength of a material but also of the
u1 S: ?9 k8 [' Q+ s, _3 Ydefects that may be present. We know that aluminum is, ~# }2 J; N& O# c
soft because crystallographic defects, called dislocations,
% y" J* Y8 T. Jcan be readily generated and moved in this metal. In# |! U* x$ }+ f& o& D" f
contrast, in alumina (Al2O3), dislocation generation and. c- `2 N. d& i$ f
motion are difficult; hence alumina can be strong but& R2 \( E0 g" f( u1 @ d. B9 D/ _
brittle at room temperature. The addition of copper or7 E' a/ a: m' d' @3 v
manganese to aluminum creates second-phase precipitates,
3 U* R3 [3 H& xwhich inhibit the motion of dislocations, thus enhancing
; F( R+ l5 ]' P( _4 kits strength-to-weight ratio. Our ability to improve; v: G6 c& o% ^/ \
the strength-to-weight ratio in materials has3 {: m) m' Y! K) U/ _; @
increased more than tenfold during the twentieth century.
, y0 {- s8 P) T/ @$ MThis is to be compared with a change of less than/ b0 D# X: a: b3 D* U
ten over the last twenty centuries. Much of the increase1 ~9 L7 p) K! F8 \# T9 l% C) b8 E: o
in this century has come from an understanding of the
8 n. E1 n5 T+ K2 a4 z0 Trelationship between the processing of materials and6 R: F7 j7 t2 k5 g2 _
their structure. The highest strength-to-weight ratios
! Q+ d3 v% e2 N' j! i% ]have been achieved in materials in the form of fibers and
# Z% L4 m5 r8 m& _0 v# Knanotubes. In these structures, dislocations either do not2 X' I: l- X7 m1 ~0 l ^
exist or do not move.1 ~$ l x# @! w- O$ E O4 M
Most structural materials are not single crystals. In
. I" z) ?9 W& K* i8 Rfact, they consist of a large number of crystals joined at* Q6 l* k' f6 @
interfaces, which in single-phase materials are called
. }4 @0 @+ p1 T+ D ?grain boundaries. These interfaces can, for example, influence
' v! p5 |/ ~+ ?3 Y# E) f E# I4 tthe mechanical and electrical properties of materials.
" f& v/ j* Z d( ~At temperatures where the grain boundary diffusion
8 R$ t* Z* @' ?! d; trate is low, a small grain size enhances the strength
8 _1 P9 |) D+ p8 ~" pof a material. However, when the grain boundary diffusion
# s: C& C: y! R+ qrate is high, the material can exhibit very large elongation
' `3 [! S0 e I7 C9 f4 L8 uunder a tensile load (superplastic behavior), or
+ O/ ]8 x O: k2 q+ x9 F) |can exhibit high creep rates under moderate or small* E) L& \2 N9 y* p. F/ E/ m( h2 y
conditions of loading. In demanding high-temperature9 c; Q' `/ a: e& l8 e9 b
environments, such as the engine of a modern aircraft,
2 }6 g& J( [/ m+ {: Z1 u3 K5 j7 Dgrain boundaries are eliminated so that a complex part,
1 W* l6 O* L9 @7 V L. [9 Hsuch as a turbine blade, made of a nickel alloy, is a single
; ?7 O F9 o/ A/ X5 N# S/ Q6 \crystal. Thus the use of materials for structural purposes
2 m! t, x- p+ E: Wrequires an understanding of the behavior of defects in8 ~7 W/ E3 F5 V( L
solids. This is true for metallic, ceramic, and glassy materials.0 i' M4 R" R* D& m( K! X" f
Both ceramics and glasses were known to ancient civilizations.' `' Y3 k+ `/ I1 l5 n( {
Ceramics were used extensively in pottery and: W" z1 L) C! g! F6 f& ]
art. The widespread use of ceramics for structural purposes
6 z# u8 M7 D. n! g% {) f5 Z1 K0 Fis largely limited by their brittle behavior. This is
& p3 W' l( |8 p& L/ Bnow well understood, and schemes have been proposed# {- j5 Y8 J. L% I. D: m
to overcome brittleness by controlling the propagation
5 B; T4 F, H8 }) j* N4 g8 Gof cracks. In metals, dislocations provide the microscopic
( x% Z' A7 o0 O* y `6 M' ^1 t" nmechanism that carries energy away from the tip5 A/ i# ~0 N. U& z2 d% n5 K
of a crack, thereby blunting it. In ceramics, the use of
, k( h) W- k* M$ e/ c* a/ Fphase transformations induced at the tip of a propagating. }$ L' P0 v. t0 S i6 o3 Y
crack is one analog of dislocations in metals. Other
, w( [) J: _6 n2 C- Y, v7 ^. m5 jschemes involve the use of bridging elements across
! B% {, Y9 R. n3 d" n0 ~cracks so as to inhibit their opening and hence their
; {# s o' e6 r2 |/ Ipropagation. Still another scheme is to use the frictional/ {$ U0 I0 `5 `$ n0 W* m) r- |
dissipation of a sliding fiber embedded in a matrix not6 @, p8 |. C2 j4 t: Z* V; y
only to dissipate the energy of crack propagation, but
7 Y$ a; u4 C5 h4 |8 Yalso, if the crack propagates through the material, to( o6 k4 l! ^/ m* m1 P
provide structural integrity. Use of these so-called faulttolerant
`7 V4 z, V) \) H2 G+ hmaterials requires both an understanding of mechanical/ {+ v6 `8 f5 T2 _! L) Y$ @
properties and control over the properties of3 @) d: ?1 f! [5 k1 ^8 h I; ]
interfaces to enable some sliding between the fiber and
2 u3 e! }+ m, g3 Lthe matrix without loss of adhesion between them. Such
% [9 Y, V; C4 C* ischemes rely either on composite materials or on microstructures
V4 X8 e) E& Z) @# t: l: x" Othat are very well controlled.$ [1 T& ^( z: \3 g) m$ y
The widespread use of silicate glasses, ranging from+ E# u% @$ h! z
windows to laptop displays, is only possible through the" I0 O; t3 b/ E) [3 Q0 }
elimination of flaws, which are introduced, for example,! A4 ?! x# t8 R; W0 X
by inhomogeneous cooling. These flaws, which are( P7 t5 c: U& @& H
minute cracks, are eliminated during processing by controlling
& ^- [1 A5 V7 T! j( Pthe cooling conditions, as in a tempered glass,, W! D! H9 m9 h: |; [
and also by introducing compressive strains through7 k0 C9 {9 b. y
composition modulations.1 m. Y/ e' `# y+ Y k+ _
There are a number of fibers that are available for use9 r# K6 Z, d# h8 q
with ceramics, polymers, and metals to form composite, ~2 g: s: u1 P) b3 q
materials with specific applications; these include carbon
$ M' D) d- X/ Hfibers, well known for their use in golf clubs and fishing% i( r! H6 c( r, l: w3 @' K
rods, and silicon carbide or nitride fibers. Optical fibers,1 c* q+ M; O/ N! e" `* `4 w
which are replacing copper wires in communication6 X7 M- @& S1 Y9 x3 F1 o# Z* H
technologies, owe their widespread use not only to their
2 c# e( Q6 F, B. toptical transparency, but also to improvements in their5 G; R2 _, C. i' R, X! x
S332 P. Chaudhari and M. S. Dresselhaus: Materials physics: u- J, G1 p& c2 @# [/ \8 [& P- T$ W" h% R
Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
# R2 n2 a- v- r; l6 U# G8 tstructural properties. Fibers must withstand mechanical2 {4 ^5 [: ] f8 q/ `
strains introduced during their installation and operation.
% U' S+ ^: f4 d0 g+ GThe use of composite materials in today’s civilization/ Z, L' N$ a: c/ G( M/ y: F
is quite widespread, and we expect it to continue as new
9 i! ]+ D! s+ japplications and ‘‘smart’’ materials are developed. An4 L$ t2 Z! y' _6 e
outstanding example of a functional composite product' {; z6 e3 s# o. [4 h2 }# t9 W& [0 R8 p
comes from the electronics industry. This is a substrate,) {+ I6 w: S. _" O2 B' P0 e$ |
called a package, which carries electronic devices. Substrates
; N1 y$ S6 p" B1 z) q9 Pare complicated three-dimensionally designed
; S5 H& C' R% b4 E0 Y& }structures, consisting of ceramics, polymers, metals,
; j" D( K! j* R2 Dsemiconductors, and insulators. These packages must
2 Z$ x3 d; u, j- tsatisfy not only structural needs but also electrical requirements.
: T9 B# \9 r5 P9 s) `Although we have made great progress over the last% n3 O: a: ~# M/ p
hundred years in materials physics, our microscopic understanding: b) U2 ?" l$ ]! {
of the physics of deformation (particularly9 V- P1 j# Q" {$ k* g& x
in noncrystalline solids), fracture, wear, and the role of' E% l* l$ y- p' m
internal interfaces is still far from complete. There has9 b r! h2 U" s9 k* Z: t/ K
been considerable progress in computer simulation of
+ J p. s3 i; ?/ ssome of these issues. For example, there is now a concerted
0 p4 z7 L; k% s: o0 Z( eeffort to model the motion of dislocations, during
& L7 n+ ^3 A }- [" @) adeformation, in simulations of simple metallic systems.
: j* r T0 z. K# h- [8 ~3 [We anticipate that within the next decade, as computational
( A0 x% L3 z. _- N r: ?& O5 d* jpower continues to increase, many of these problems8 x1 @' s, u+ w$ S P
will become tractable. The ultimate goal is to design$ g- a2 `/ f8 a: M! J" f x
a structural component for a set of specified; T# @1 m- Q7 j
environmental conditions and for a predictable lifetime.1 K+ p: i. c' Z0 j2 c+ _: ]
III. POLYMERS
' ]! S2 U3 s" S q6 Z+ APolymers, also known as macromolecules, are longchain# v6 \- K/ N/ v! s) R @ V
molecules in which a molecular unit repeats itself7 k+ j, _* j# X/ P
along the length of the chain. The word polymer was
* ^! J. T: Q/ o9 b6 lcoined approximately 165 years ago (from the Greek
' s, m9 d/ r- n- V$ kpolys, meaning many, and meros, parts). However, the2 s+ T, m5 {: U; Z3 `4 ^( {
verification of the structure of polymers, by diffraction: e2 r) E2 u4 ` V+ w
and other methods, had to wait, approximately, another
5 J8 e. Z$ r- U: _' D6 I100 years. We now know that the DNA molecule, proteins,
3 |/ E4 d. T1 {4 `/ h- Icellulose, silk, wool, and rubber are some of the
; K6 u6 M6 k( |+ d. Jnaturally occurring polymers. Synthetic polymers, derived' q Z% {* K7 }) z W4 J. ?
mainly from petroleum and natural gas, became a
) H- v0 I" q5 c' C, R% k- ncommodity starting approximately 50 years ago. Polymers5 H9 e2 E; P! {" I
became widely known to the public when nylon
3 y F# f2 f# zwas introduced as a substitute for silk and, later, when; W1 b Y0 @& n% u
Teflon-coated pans became commercially available.( ~* G! `3 ]+ B0 U8 P
Polymers are now widely used in numerous household
! `4 d! [! E; _applications. Their industrial use is even more widespread." M. z/ `6 R: y, c' @; k
Most of the applications associated with polymers
5 c+ i+ Q" U p; k) Y$ Hhave been as structural materials. Since the 1970s it was
" e* d# |. r: n( U1 x5 e8 Lrealized that with suitable doping of the polymers, a; y: C) p( B, w) n4 S$ ~
wide variety of physical properties could be achieved,
8 e7 a% S# o- eresulting in products ranging from photosensitive materials. ~" X1 L5 F% H ?. j, T
to superconductors. The field of materials physics9 t' s2 H1 m. T
of polymers has grown rapidly from this period onwards.
1 x( ]" U& t0 A3 U( }% a- w7 N6 nPolymers are a remarkably flexible class of materials,
- `% l6 l2 }( O6 \; }whose chemical and physical properties can be modified" V. c' c( E9 R. [3 U1 _# }6 }
by molecular design. By substitution of atoms, by adding
: m; ^- G) Q+ k" mside groups, or by combining (blending) different polymers,
! G% o% @# V# ?/ G) A, ]3 Y [chemists have created a myriad of materials with
9 R; d, \6 u% J3 f+ W& Z$ zremarkable, wide ranging, and useful properties. This" c) D7 w( a9 X) o r: P
research is largely driven by the potential applications of: ]: P+ K2 G" @/ o/ F
these materials in many diverse areas, ranging from cosmetics$ z% ^8 c+ f3 b+ e, i4 c
to electronics. Compared to most other materials,
% }" F% y/ p& Dpolymers offer vast degrees of freedom through blending
1 C* ?' o8 ?+ `and are generally inexpensive to fabricate in large
0 a' \+ C# S# C6 evolumes. They are light weight and can have very good
1 e$ }2 \* S$ h3 }) H& T. ]strength-to-weight ratios.) J& T# v3 ?* Q5 D
Polymers have traditionally been divided into five' m5 g( s2 e. d& ? M0 R" {$ o
classes:1 u' V5 g. ?4 _2 W6 l- M5 y- u
(1) Plastics are materials that are molded and shaped
- p4 R: }' c/ U! O& T7 p% m. Aby heat and pressure to produce low-density, transparent,/ k. o' u& `* o& Y2 r" G' K+ Z
and often tough products, for uses ranging from4 l* z! \" i: E7 h/ N- @- c
beverage bottles to shatterproof windows.2 x+ E/ Q$ C3 K! g
(2) Elastomers are chemically cross-linked or entangled# D+ g# Q& G" L
polymers in which the chains form irregular coils
, H6 H- e1 F5 N# _8 @/ Ithat straighten out during strain (above their glass transition
L$ Q1 @+ U8 k0 ]6 j S" jtemperatures), thus providing large elongations,, V# |0 P, @6 k' S/ P% M1 ~! B4 B
as in natural and synthetic rubbers.7 J+ F" s- y. l6 ~
(3) Fibers, which are spun and woven, are used primarily
* D, I0 L+ c2 ~/ }8 q7 e+ D* cin fabrics. About fifty million tons of fibers are produced+ z/ u1 I7 {6 e& \
annually for uses ranging from clothing to drapes.
/ M1 g+ f0 D6 OApart from naturally occurring fibers such as silk and8 i. T2 R6 [, `3 K
wool, there are regenerated fibers made from cellulose5 B5 ~) ?5 ] J$ C P5 Z
polymers that make up wood (rayon) and synthetic fibers,! w" R5 Z( N! q, H
comprising molecules not found in nature (nylon).7 c. q) j* Z+ T
(4) Organic adhesives have been known since antiquity.
# N% f6 C: ^+ e7 O7 R7 W) EHowever, with demanding environments and performance
7 |3 ]) a7 _+ ]2 p* b3 Zrequirements, synthetic adhesives and glues3 s3 b4 n( L+ o/ u! i
have largely replaced natural ones. The microscopic
- Q! A, f) `3 t! O1 k8 \. Cmechanisms of adhesion and the toughness of joints are6 z" ?4 Z5 K; O3 e0 j
still debated. There is an increasing trend to use UV
/ f- [- ~' D: l1 o9 n, F. `: Yradiation to promote polymerization in adhesives and,
% M6 E; Q8 q) ~0 l2 Pmore generally, as a method of polymerization and cross
6 D; P- p: l* P3 I S9 Nlinking in polymers.6 T4 ?0 K2 n* \* B+ q
(5) Finally, polymers, frequently with additives, are. Y1 y6 o" W1 q7 G, A) n; N
used as protective films, such as those found in paints or' v8 H- ~/ p3 S+ X0 B, W$ P5 o5 m+ K
varnishes.
% ^& A! A3 _% m, sPhysicists have played a significant role in explaining; X4 J d& Q/ O+ L
the physical properties of polymeric materials. However,
' C" m7 h. J2 {( F3 Gthe interest of physicists in polymers accelerated when it
+ g8 B1 y& p9 j4 d1 M" ]was discovered that polyacetylene could be made conductive
# T1 m1 K& V$ f0 w) C0 L8 A1 tby doping. This development was noteworthy
$ x6 z" W: O1 {3 Q, q+ Z2 zfor it opened the possibility of deliberately controlling+ N- Y2 ?) u( r) T- {
conductivity in materials that are generally regarded as/ p4 h% c1 ?' z7 v& x
good insulators. The structure of all conjugated polymers,
$ d# Z% R* d3 u" g5 ?* las these materials are known, is characterized by a
, U- E. j% G8 d" g6 e$ n. ^( i I$ Qrelatively easily delocalized p bond, which, with suitable
- [* y. G, |( o idoping, results in effective charge motion by solitons,
t! q R; _% o" q! m; l0 _polarons, or bipolarons. Since the discovery that polymers' J' X2 B3 t& t. ?' _2 U
could be electrical conductors, active research areas8 k- ?5 N1 h: W* v \' f; ]
have developed on the physics of polymer superconductors,9 ~9 c- n# N' C1 o* s
ferro- and ferri-magnets, piezoelectrics,
: |4 I6 P# w# b" aferroelectrics, and pyroelectrics. Within the field of. o0 M7 j. e3 _2 m, y6 ]7 X
doped polymers, devices have been built to demonstrate
$ u$ n s4 w' O' y7 j8 olight-emitting diodes, photovoltaic cells, and transistors.4 |3 u: }& c9 z! ~/ x
Conjugated polymers have also been investigated extensively
% @& Q% l+ T3 m1 d# P4 P; h+ [for their large nonlinear, third-order polarizability,' U$ P9 E4 T, e0 T4 U! z5 i& R+ _
which is of interest to the field of nonlinear op-
8 S( q5 U. K# S3 SP. Chaudhari and M. S. Dresselhaus: Materials physics S333
6 S: _9 m( W+ O- o3 f ]Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999! [. F4 p$ l/ V! d& L
tics. Large nonlinearities are associated with the strong
1 P% m! X; S; _1 Q4 o! j1 F2 _polarizability of the individual molecules that make up7 U% Y: n" i" c: |
the building blocks of the polymer. Furthermore, the
" f8 y1 M- r" T' x5 Mflexibility of polymer chemistry has allowed the optical
5 Y/ B- ^1 h- Wresponse of polymers to be tailored by controlling their6 O, A- z) C5 a; N# ]5 P
molecular structure, through the selective addition of
$ ^: ~9 f! O& {5 a# O: Tphotoactive molecules. Hence these materials have been
3 }, j# I# w, X3 E+ b! U/ C1 K) Pwidely investigated by physicists and engineers for optical
2 F$ K" u2 n0 i& ~9 J6 H- Gapplications, such as in holographic displays (dichromated0 a6 V0 T6 L. v# F
gelatin), diffraction gratings, optocouplers, and1 \$ O4 A" N7 I6 G) f
wave guides.
! f- }- Z6 y% H/ }4 k# ^( WPolymers have long interested physicists for their conformational$ {( {3 @" i! Y# \/ c
and topological properties. This interest has, u# |1 O( L2 b R+ M g
shifted from the conformational behavior of individual- S6 P8 r M7 P8 Z$ E/ Z" \2 x
molecules to that of a macromolecular assembly, phase( l& v5 d Y' b; Q
behavior, and a search for universal classes. Block copolymers,
3 p" E, Q! G# [3 v, y8 O2 J vconsisting of two or more polymers, can give
/ k6 g. `* L j5 \' m5 s' Zrise to nanoscale phases, which may, for example, be
0 t- ~8 }* \9 {/ o1 `+ Fpresent as spheres, rods, or parallel lamallae. The distribution+ v8 ^& M6 J% Q: x6 g: M2 _6 d
of these phases and their topologies are of current
/ f7 ~% C- s2 Z. R5 otheoretical and practical interest. Block copolymer
+ ]+ T4 z( ?( _' ?0 i" G! emorphologies are also being used as nanoscale templates: F4 Z3 ^" u$ H, n, x' H
for production of ceramics of unique properties having& F7 @: S6 Z- x+ ?, Q' e
the same morphology." G1 A; r( |0 L
Block copolymers are also of interest as biomaterials.
7 U$ m1 p( ?& D% M5 @Proteins are an example of block copolymers, in which# W* O, F* g' B
the two phases form helical coils and sheets. Attempts to
0 n% m' [/ B+ P5 x) _mimic the hierarchical structure present in natural polymers
9 X0 @ X3 g8 q4 X. ghave only been partly successful. The principal difficulty
9 O; I0 e* q- _, I0 C; S. a F0 Dhas been to control the length of the polymer
( i8 O8 ~8 Q5 F3 Z8 [chains to the precision that Nature demands. Significant
' _* k3 \0 V7 r5 J/ W; |: d( jprogress has been made in controlling polymer morphologies( h- `0 ~6 m4 N
with the use of new catalysts. For example,
6 J& a( E) A8 j' X0 {, P# mmetallocenes have been used as catalysts to control
# N3 L x. D: Y n% |0 W8 L8 lbranched polymers and organonickel initiators to suppress! X- l9 m2 H8 c( K6 W1 H
chain transfer and termination, so that polypeptides
/ f8 \9 x2 E* kwith well-defined sequences and with potential for
) G3 n7 w/ I$ i6 s" ?7 Japplications in tissue engineering could be made. The3 ?. O" }. O' V8 J3 r
growth of well-controlled polymer chains is an example
' j* {" X6 {! F4 jof ‘‘living’’ polymerization.
+ y4 I5 ~) H# Y/ U& PThe static and dynamic arrangement of atoms on the
' n8 U* i. w( l4 O" c" p8 R. l/ dsurfaces and interfaces of polymers is another area of; z" W' Z6 _7 p: U# y
active investigation. For example, thin films of polymers," B4 T- k) _) E- A7 L
in which the chain lengths are long compared to the
8 ?4 P% o; \1 _3 {6 l" @7 }- {" ythickness of a film, show unusual physical properties: the
1 m0 _9 J# C1 [3 L2 i+ nglass transition temperature for a thin-film polymer decreases
& b4 ^& D6 t% ?5 s; V1 @; h+ Gsignificantly, but between solid surfaces polymer
' z+ \& S# }' ~/ p9 _liquids solidify.6 ^* r- ]; ?5 V/ v& G; Y
Even though we have some way to go in making tailored
% P8 O" z2 U8 Bproteinlike structures, polymer research has: P* j1 x2 L4 m" i8 T: i& n% Y
played a significant role in the class of materials called
0 L8 Y# h( i5 ^0 Y" kbiomaterials. Polymers have been used, for example, to
; t8 z. `, |% z% b+ H: C) mproduce artificial skin, for dental fillings that are polymerized
2 ?. P; D T5 R* v' `0 r ]! _in situ by a portable UV lamp, and for highdensity0 `: F: E5 Q" r' L# Q8 \
polyethylene used in knee prostheses. Physicists3 j! Q9 |1 U6 N8 i, m7 a* K( q/ l, t
play a significant role in these developments, not only
& j, X# Z. f2 s/ D7 n' T C' O) x" W6 ]for their interest in the materials, but also because of; C) \' K2 |1 M6 [( D
their familiarity with physical processes that can be used
" J! ^: B- y6 ]' W6 \to tailor the properties of polymers. A particularly good7 P% p/ p9 f8 P& Y$ V* i: o
example of this interplay is the recent and rapidly growing
. m# Z0 J2 w% X1 I) N0 Xuse of excimer laser radiation to correct corneal abnormalities;
: a' r8 ^ B+ a: a2 {using a technology developed from studies6 \7 l. K. L& Y$ Q0 _1 s
of the ablation of polymeric materials for applications in
; I( T6 i' p# r1 a/ xthe electronics industry, physicists realized that the* x) U& h; S X; C+ p
small, yet precisely controlled, ablation of a polymeric
a0 h* a% y' O! ~' k6 psurface might be useful in shaping the surface of an eye.
$ k: S, D+ G: A' J }9 P5 W3 IIV. ELECTRONIC MATERIALS
6 X' {: r5 | I! M3 u" B/ mThe roots of the electronic materials field can be( q$ H& I2 y4 |9 w( c0 ~( H2 |
traced back to Europe in the 1920s, with the advent of) i! V& D+ k, N+ ^
quantum mechanics and its application to periodic structures4 x$ @) c( D7 E8 a
like those occurring in crystals. The early experimental4 P, t# c H8 w t( A
focus was on alkali halides, because these materials& B% d3 G& W9 S2 R3 ?6 ?
could be prepared in a controlled way from both a
9 c: P# \+ f! h( I; H& W5 u( O; }structural and a compositional standpoint. The creation
5 e, l0 K* d, b: K1 Gof a strong academic program in solid-state physics at a/ s" m, U; l6 ~
the University of Illinois in the 1930s had an important+ `7 ~* f" s2 X; K+ b& T& L
impact on the early history of the electronic materials; k: [# d. T. [8 J* A- }
field in the United States. This knowledgeable human
% Z# `" x2 o; i, i' sresource played a significant role in mobilizing the national8 j3 J- B* G; ? z) Y* T) q3 k, n
materials program during World War II, especially8 M9 j, p' i% R3 z6 U8 J
in the development of semiconducting materials
0 D0 Q% d7 C4 b i0 n# }& lwith enhanced purity, suitable for use in diode detectors! ~1 N" _) o, d$ X% C0 D
at microwave frequencies for communications applications.
* r% F# f: ?. @. U ^- a5 \' g1 HThe availability of these new semiconducting materials
$ k) x) d* G o9 t/ U' u: Pin purified, crystalline form soon led to the discovery; l. N8 v% J1 n$ T( s
of the transistor, which ushered in the modern( r+ @) {1 Y/ q* |
era of electronics, computers, and communications," P$ `6 R1 ]+ V/ ^- x j7 m0 _4 f
which is now simply called the ‘‘information age.’’: T2 v- Q. i& a. i# ^8 S
Semiconductors have been a central focus for electronic
/ n# Z' j5 g! T/ mmaterials. Quantum-mechanical treatments of a
3 ]3 A: q5 @$ q! }. N7 r; d Iperiodic lattice were successful in laying the groundwork
5 z5 }& ` A0 A, {for describing the electronic band structure, which could
2 g! m( r' j) C( U" X: N eaccount for electrical conduction by electrons and holes,, @$ |; E! s" |4 N/ P( [; `% Y
carrier transport under the action of forces and fields,+ S- s7 b* h; ], w
and the behavior of early electronic devices. Because of0 M1 v J/ `! {6 z3 V$ P) O8 O
the interest of industrial laboratories and the Defense
7 _4 O% G6 j7 KDepartment in the newly emerging field of semiconductor
4 X- M' Q, z# y l& P& Yelectronics, semiconductor physics developed rapidly,8 W' g M D- i0 x5 ~ e$ t7 [
and this focus soon led to the development of the
* Z" ~. w4 u: m5 m3 t+ ~1 n, n9 lintegrated circuit and the semiconductor laser.* k/ Y) |! E+ F: K* }. Q) E
The strong interplay between technological advances0 p* T+ g" X/ q; i: } |9 @) i
and basic scientific discovery has greatly energized semiconductor2 ^# U3 n. z7 q1 O9 T: I
physics, by raising challenging fundamental. \5 w% C6 k! o2 n0 S/ Y# J
questions and by providing new, better materials and9 _; I0 s E. j% n" D* p
devices, which in turn opened up new research areas.1 O' V: z& a" F- [' q5 l
For example, the development of molecular-beam epitaxy
4 M+ N8 Z8 h" S4 [8 j/ }5 Z9 a) din the 1960s and 1970s led to the ability to control2 M8 { X0 }& ~2 a/ J' }
layer-by-layer growth of semiconductor quantum wells
- E* p1 a5 @3 n5 O) _$ Nand superlattices. The use of modulation doping of the
. r4 G, X9 a0 F' b/ w& [0 fquantum wells, whereby the dopants are introduced
3 P- H T4 d% T1 x* j, V$ Aonly in the barrier regions, led to the possibility of preparing
, m W O6 w, A+ [$ C+ W2 Osemiconductors with low-temperature carrier mobilities,
. D& E) q/ [6 ~" Torders of magnitude greater than in the best5 M) t" u3 i. h' L M8 Y0 ^( _
bulk semiconductors. These technological advances& j @/ L1 T1 i; n3 E3 k
soon led to the discovery of the quantum Hall effect, the
% f+ Y1 ?, d# T5 efractional quantum Hall effect, and a host of new phenomena,
0 k1 q- w" K" H- E( [1 F. Rsuch as Wigner crystallization, which continue8 q5 X$ x8 M( T1 j
to challenge experimentalists and theorists. Lithographic
2 N; \1 R K4 XS334 P. Chaudhari and M. S. Dresselhaus: Materials physics! ^ `( G. t5 }& R: i
Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
6 b+ p3 [2 d7 p; b: ^; _and patterning technologies developed for the semiconductor b% b" L3 m, A: ?2 o
industry have led to the discovery of the quantized4 h% `- K/ N6 p6 I; e( q( g
conductance for one-dimensional semiconductors8 s7 t( I- g/ r% a1 F5 |5 r- g
and to the fabrication of specially designed semiconductor
& ^& M, d }9 ]devices, in which the transport of a single electron
0 m( T; c2 E; K$ A' v. Ycan be controlled and studied. The ever decreasing size
* d; X* n3 k1 R( G7 G$ Oof electronic devices (now less than 0.2 microns in the
8 X% u- @& e3 }6 b# H$ E3 h1 _semiconductor industry) is greatly stimulating the study( N3 _+ j/ h6 j# ?3 {* A
of mesoscopic physics, in which carriers can be transported
! U ?1 R4 |4 ~# U1 J4 ?ballistically without scattering and the effect of6 f$ c6 U1 W) s3 K: r1 A
the electrical leads must be considered as part of the# @6 o; F3 u, E Q" I
electronic system. New materials, such as carbon nanotubes3 }3 j) u0 C+ ?
with diameters of 1 nm, have recently been discovered,
0 X4 J* K8 @. p: ]! Yand junctions between such nanotubes are being
. v# {6 j V/ W- Lconsidered for possible future electronics applications
2 s) h* \/ j7 q! ]: H) Lon the nm scale, utilizing their unique one-dimensional9 s0 X3 y, h' |/ I3 ], C
characteristics.
5 M! g) X& q- K" N$ UThe electronic materials field today is highly focused L$ l" Z0 j% \5 l& Z
on the development of new materials with special properties
5 ^3 C5 d( L. u" J% d7 X3 e8 Qto meet specific needs. Advances in condensedmatter
8 L% a" T$ G2 K' W+ |physics offer the possibility of new materials
; ?9 o O2 R. oproperties. In photonics, new materials are providing increased" e/ L8 S' E( U2 @
spectral range for light-emitting diodes, smaller
' e2 E: j" v b4 c8 m+ D [9 H/ G wand more functional semiconducting lasers, new and improved" ~: h! Y, u. t% g/ d
display materials. The new field of photonic
% g. L |' y; z& Z' Q1 U7 u3 |band-gap crystals, based on structures with periodic) a, @. {; W; y; t
variations in the dielectric constant, is just now emerging.
% h5 I7 a: P3 xResearch on optoelectronic materials has been
D) f) O( g7 m8 G. b3 _1 \& m( x2 Zgreatly stimulated by the optical communications industry,
6 f: i% j5 D2 ]1 {: @which was launched by the development of low-loss
- Y# p/ y; b! P' l! j; `; moptical fibers, amplifiers, and lasers., i- f Z+ ^5 t+ t
Ferroelectrics have become important for use as capacitors7 O) z9 d- R+ g2 ?; d1 k& z3 r5 F
and actuators, which are needed in modern robotics+ O- O- j. |+ F" U
applications, as are also piezoelectric materials,
* v8 m. }) D# a) Q* M5 ]0 owhich are critical to the operation of scanning tunneling7 g( {6 U# X6 Q% D
probes that provide information at the atomic level on
( C1 K$ t# X. N3 @8 i) V ystructure, stoichiometry, and electronic structure. The9 X4 W* j+ h, w- D
technological development of microelectromechanical! F' {8 M! c( A# l- d7 Q" J3 j
systems (MEMS), based on silicon and other materials,4 x/ X F! n( |
is making possible the use of miniature motors and actuators
# \3 ?, F7 ^- a0 pat the micrometer level of integrated circuits.6 ^+ X" L- `: q7 w: M1 B% F
Some of these have already found applications, such as
. | B7 O7 r" q9 ?/ jthe triggering mechanism for the release of airbags in# E: y+ v8 B/ T0 c/ K/ m9 S% Z6 c
automobiles. Such developments are not only important
. U2 {6 d* j& w. e" ?to the electronics industry, but are also having great impact: z Q3 _% E9 P6 f
on fields such as astronomy and space science,8 P4 d$ [9 l' n5 f1 G& _
which are dependent on small, light-weight instruments+ {7 Q# ^. O$ Q1 p# a
with enhanced capabilities to gather signals at ever increasing) Y+ V) X! H8 I# O/ V3 E
data rates and from ever increasing distances
' S$ @1 c) f, f* j) efrom Earth. The developments in new materials and4 Q1 y8 P3 F5 z6 a, L5 H% h
low-dimensional fabrication techniques have recently rejuvenated2 @! `8 @: {+ p
the field of thermoelectricity, where there is
2 X) e' u( X' c5 a5 H% Dnow renewed hope for enhanced thermoelectric performance9 R4 L* s) h8 i3 w
over a wider temperature range.- s$ I* Y7 n1 Y- Z$ K* `
Research on magnetic materials has been strongly influenced' k1 U+ z2 @4 K# g% G2 y
by applications ranging from the development
5 R$ o+ N% O! cof soft magnetic materials (by the utilization of rapid
. e6 K+ @ Y" D/ F9 qsolidification techniques) to hard magnetic materials$ b5 X1 t' ?' s( d
such as neodymium-iron-boron for use in permanent8 \% o s% b1 }; I
magnets. In the 1980s efforts focused on the development, e3 F# u" a' h- o2 ?( P4 y
of small magnetic particles for magnetic memory8 R; N$ d ~4 m% o
storage applications. New magnetic materials, especially# H7 m5 ?; P7 a$ k$ |) c- Q2 a! X& F
magnetic nanostructures, are now an extremely active
' m$ j9 a. L* _1 x" u/ x8 x2 Qresearch field, where the discovery of new phenomena3 D' r$ a" U% n3 q; \
such as giant magnetoresistance and colossal magnetoresistance5 X3 m* a! b/ k$ W# X; J& L/ J
are now being developed for computer memory
6 a5 _9 k2 v& Zapplications.
/ f g: i) J9 EThe strong interplay between fundamental materials
[; t7 u2 R8 {physics and applications is also evident in the area of, T2 G/ T5 U3 x( X( f
superconducting materials. Early use of superconducting+ @' n- g% s0 k. x
materials was in the fabrication of superconducting magnets," E: x* q0 s8 _0 p# P
which in turn promoted understanding of type-II7 S+ c G, p' Z% c, \) D
superconductors, flux dynamics, and flux pinning phenomena.
! ^4 r8 T: o$ Q" g1 W& J ]2 oThe discovery of the Josephson tunneling effect; u6 _6 |. y+ E) V, A3 O
led to the development of the SQUID (superconducting( o1 L: O( |+ }: S- N" g; L' @
quantum interference device), which has
/ O3 ^0 @& N9 Z( p+ N& Obecome a standard laboratory tool for materials characterization
$ s* |. ?" o9 O9 Oand for the sensitive measurement of extremely
; H+ w+ }6 ?& `5 zsmall magnetic fields, such as the fields associated5 n! z$ ]& \' \* Y- m$ H' K, ~
with brain stimuli. The discovery of high-Tc
* h" m. g, y9 O( V$ l8 xsuperconductivity in 1986 has revolutionized this field," h i3 S7 j t8 s
with much effort being devoted to studies of the mechanism
6 M; `% m( S7 \for high-Tc superconductivity, along with efforts to" ~3 q( A) s$ {- ]; Z
discover materials with yet higher Tc and critical current- v% @# l" R& |: g0 U
values, to improve synthesis methods for the cuprate superconductors,
, Q0 I, q4 g' S* T" O. m6 K; C3 {/ G. uand to develop applications for these
" I* i( R0 \3 z, Y5 u# _materials to electronics, energy storage, and highmagnetic-& E+ x9 n% X2 A, {& u
field generation.
( R7 F$ ~ E' Y/ o( z4 r" iWhen viewed from the perspective of time, the developments' L" U) L& F7 i/ a* z, j4 V: `, O
in electronic materials have been truly remarkable.
( x& v0 D; y$ {; \" V- f, rThey have generated businesses that approach a' D% F [, s; e4 _# C
trillion dollars, have provided employment to millions of1 q6 P! X# [: E7 F: v6 A, F
workers, either directly and indirectly associated with8 Q2 f3 `! T& B. j1 J5 k: x; N
these industries, and have enabled us, as humans, to extend+ {6 P4 i5 p5 \$ D9 P/ Y2 Z2 U& j0 L1 S
our abilities, for example, in information gathering,
1 V2 P3 @$ L7 w& E) j/ J9 qcommunication, and computational capabilities. Science
! P9 R; E- v5 G& t5 R; Fhas been the key to these marvellous developments, and6 l# X3 S5 s4 W {: o& p9 n% ^' R" e
in turn these developments have enabled us, as scientists,$ \5 [9 I+ Q9 S7 y
to explore and understand the subtleties of nature.
* j+ h3 ?2 \0 K/ p0 S1 |5 k/ WV. SUMMARY! b* x: w9 ~8 ?% @- M
In this very brief note, we have only touched on some
7 t: R) r o1 V6 q5 ]4 sof the advances made in structural, polymeric, and electronic
' x0 h: n) w3 O- Qmaterials over the last century, showing how materials
1 [# y% @. f4 o" G- D6 U4 Vphysics has played a central role in connecting0 G& N; }$ G0 ]4 Y+ N: [2 ~: o
science to technology and, in the process, revolutionized) V9 M+ z3 b) B" ~7 d s
our lives.
& g3 S# l/ @+ d& ^" h, b- H' j1 cP. Chaudhari and M. S. Dresselhaus: Materials physics S335
( e B9 E L/ I( E0 A8 |/ `Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999 |
|