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Materials physics
6 J( `0 k1 c$ T4 A9 ^P. Chaudhari
) U' M4 X/ x4 }, }! l/ vIBM Watson Research Center, P.O. Box 218, Yorktown Heights, New York 10598
5 o1 o$ ]' e2 ?% GM. S. Dresselhaus- j5 J' v6 r; `
Massachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307) ^' r7 K" w6 \ W) B0 x) {
Extraordinary advances in materials physics have occurred over the last century. These advances have" j7 I8 w0 h9 j9 ]
influenced almost every aspect of human endeavor. In this note, the authors sketch some of these
. f2 a) M* L; L4 U" W! _exciting developments in structural, polymeric, and electronic materials. [S0034-6861(99)01502-0]7 _. j: o' r6 V( X1 N
I. INTRODUCTION
" d& q& N7 k4 H; Y3 L& {8 mOver the last one hundred years there have been stunning5 M* A3 J, a4 c6 V' l
advances in materials research. At the turn of the
) `/ |+ K1 w9 L0 C9 C" }last century we did not know what the atomic structure* t, N4 _' z! H, p% p
of a material was. Today, not only do we know the structure,/ V% o1 l C8 ?2 g& E, d
but we routinely make artificial structures that require
0 F4 P: S4 X( R' rplacement of atoms at specified locations, that mix$ W7 D2 u& I ^2 B9 S5 n
atoms to create properties not found in naturally occurring2 s' N& c$ F6 I4 X4 t. E3 }
materials, that have the functionality needed by today’s
, z5 t8 p" F+ L# n6 l% d+ [technology, and that adjust their properties to a
! [4 O; Y, S+ K" r2 Q' ]changing environment (smart materials). Over the last: T0 L$ M& q0 x5 e
few years we have begun to manipulate individual atoms
3 Y! @- ?& b! [" mto form structures that enable us to explore scientific
, i! {6 h' m- O# ~- C U0 ^issues, but that will surely lead to profound technological% Z- K& ]; V6 Y/ }
and social consequences; for example, the manipulation
8 N/ l" X4 K, p* f& T6 d. V6 [of nucleotides in a DNA molecule, which is then
7 U0 d; V+ `9 j. M1 z! N+ R, zcorrelated with the functioning of, say, a gene and with9 L; W& G' F0 w, p
its expression in the control of disease.
6 r1 [) e6 q7 ~% j: i SA hundred years ago there were no electronic devices,
& `& o. b' X) L' cand today there is hardly any electrical appliance without
( |+ I# j' a4 Z' y0 y m+ Othem. It is anticipated that in the near future there
/ J: i4 \( d$ w5 b/ s) |4 m% Jwill be a microprocessor embedded in almost all electrical* L" b! p4 f' J' Q, |7 u
appliances and not just in those used for computation
9 g! P C& p E5 p. |or information storage. These devices, inconceivable a4 _- N: ?, b% N# X+ }- V
century ago, could without exception not be made without7 D8 b( s4 i1 ?: O1 m8 j
the knowledge gained from materials research on
1 w2 b) r) Y/ e5 @: v+ C2 xinsulators, semiconductors, metals, ceramics, and polymers.
9 Z4 W2 U4 z/ O% q5 Y8 \3 DAt the end of this century, we have begun a debate
4 k l+ I1 P$ C( B# r# Eon how far the present devices can continue to develop,
, ^6 j- F+ e2 _' I( Agiven the limits imposed by the speed of light and! |! a$ f% [- r; J
the discrete nature of atoms, a debate that would have# r& c# ]) p8 f1 x
been incomprehensible to scientists and technologists of8 p- |4 ~# \4 x* Y% H# d
a century ago and a debate in which we now discuss the
z; p0 Z- n7 _; H% d3 Z0 upossibilities of using single electrons to switch a device3 x4 H2 k! P8 s; a# y
on or off.
5 H; w8 J" k& `! e' QOur ability to measure temporal phenomena was limited
# N! l5 F! ` u9 {7 Rto fractions-of-a-second resolution a hundred years' z4 O, O$ R/ h2 c- l* t% m/ w
ago. Today we can measure changes in properties with a
& p3 s8 x+ B r7 W4 l; r! N5 i0 Lfew femtoseconds’ resolution. Strobelike probes enable5 S# l) a# V0 l9 P* h2 |% ]% l
us to measure phenomena ranging over time scales covering
/ n8 c( J {: wmore than ten orders of magnitude. We can, for
1 p4 @- s& b- ]( S8 V8 ]example, study the relaxation of electrons in a semiconductor! @2 }* c: l$ i$ u( a
on a femtosecond time scale, the visible motion
! O: P- |, V, F: bof bacteria in a petri dish, or the slow motion of a sand" Y) k% P! s7 w9 V t) w/ b
dollar on a beach.
9 w3 C8 ~* k4 [3 u3 c; N# Z# H( JMaterials research spans the range from basic science,
# s2 l" L& w% L$ Vthrough engineering, to the factory floor. This has not6 w! v2 y1 s8 m+ a
changed over the last hundred years or, for that matter,3 }4 m5 T( }" u
throughout the history of human civilization. Materials" O5 Z1 T$ R3 z! C7 m
research came out of the practical needs of mankind.% [$ ^8 t1 ?- `& a( ?
Eras of civilization were named after materials, so central
, j, ?0 J7 o1 S4 }# G9 \) [has been their role in achieving mankind’s mastery: p* q+ F$ u4 B+ j& j7 w
over nature. The field of materials research can trace its
$ w8 t+ h$ _" aroots to alchemy, metallurgy, natural philosophy, and$ K% h6 p$ V. S, D5 |2 K% m
even art, as practiced over many centuries. However, the
- j- m7 b! F# [& k2 zfield of modern materials research, as represented by" d; r2 C# e& V' ^9 N3 B7 ?
materials physics, is only about sixty years old.
) b8 F9 z3 m* f/ P9 _, x7 a$ hShifts in materials usage from one type to another are8 c/ {# g- r) H
usually gradual. This is due to the very large investments
- j* Q Z7 D9 u0 v, rassociated with products in the materials-related industries,
$ a- J& Z0 }% e% R! ycomplex relationships between reliability and functionality,9 M2 J$ a/ I4 ]% t) j
environmental issues, and energy demands.9 q% R% u' ]! S/ d
However, measured over time, these shifts become quite
: | U7 Q' o9 Fperceptible. For example, in automobiles the ratio of9 f3 V e9 K; u- U! z: m1 ]: q
plastic components to iron-based alloys has changed" v7 }/ ^: c5 R/ z. T& I( B
from less than 3% to more than 15% over the last two. H' s( ?0 U! X" _- `2 k
decades. Although the percentage change appears to be6 a, _, X2 C" ~5 S' R b2 w* s
modest, the actual volume of material is large; over 40
9 ~" K; U# T- U' t+ }/ xmillion tons of structural materials are used annually in$ C* {9 H6 d4 q- q* ~- p* y+ K5 w4 e
cars.# m# K0 L8 s0 @( l. X- D$ S
The advances of materials research in this century,2 U2 V# [. K6 ~+ T6 h4 C5 C
which far exceed those of all prior centuries put together,
/ X( } p' P; g- t* ^! @can be illustrated by three examples: structural,
# t; Y w, X( T- E7 npolymeric, and electronic materials. Our choice of these v; a5 R6 C9 Z$ l- [- A6 `
three is somewhat, but not completely, arbitrary. It is
/ \$ Q1 U, Y: P) j l9 zout of structural materials, particularly from the fields of" X( j: t, G1 Y1 O0 O6 Q
metallurgy and metal physics, that modern materials
f2 x" E- |. [5 ophysics has evolved. From the crude weaponry of our
9 _; Z2 I2 T4 I9 G) `: N! o8 G+ uforefathers to our mastery of air travel, space flight, surface6 a& _8 m% X- o5 P$ ~* K
transportation, and housing, structural materials6 e! k! t' p1 p& F
play a role that is unequivocally important. Nature uses
6 E0 T" D' [- p9 O! w# _the second category of materials, polymers, in amazing
) C% ?. n; |2 `1 d5 [% dways, to perform very complex functions. We humans0 a5 Y3 |3 F! ~# i- H
are an example of that. Over the last hundred years, we
C. `3 f2 J! j' s6 V/ yhave begun to understand and develop polymers for7 D" D) U2 ~' h* |
uses in food packaging, fabrics, and structural applications.
0 x8 {7 Q2 `* {+ }2 c3 XWe anticipate that polymer research will play an
( A$ P w3 ^' h9 A8 F; ~& t2 J/ Y: rincreasingly important role in biomaterials of the future.
, X+ u2 G; L: \7 C. t8 C3 dThe third category, electronic materials, were not conceived
" G1 [) e( [( C. d kuntil quantum mechanics was discovered in this
2 r" h2 W) ?0 S# w Q8 {century. Today we cannot imagine a world without telecommunication,+ @& C! z! @% Q' l
computers, radio, and television. These
4 L: q7 N; | N0 h7 r( z5 u2 jand future devices that will make information available/ ?( |8 p o0 O1 S: o9 G! h, Q
Reviews of Modern Physics, Vol. 71, No. 2, Centenary 1999 0034-6861/99/71(2)/331(5)/$16.00 ©1999 The American Physical Society S331
( S0 _5 K0 v/ o# X$ t7 ~% Ainstantly are only possible because of advances in the6 s. e7 J& M& Q% J+ t
control of materials structure and processing to achieve
+ [2 z$ R6 P% J0 v7 aa desired functionality.+ `+ ~# U$ a4 q. l# S+ j: Q
II. STRUCTURAL MATERIALS9 V8 E7 n3 A7 S H9 z
At the turn of the last century, mankind’s use of structural' D8 S: ]) Z6 f2 f1 y0 Z/ m
materials was limited primarily to metals, particularly0 _0 V. w, I2 o: m: D* M
iron and its alloys, ceramics (most notably Portland' y( M$ X( _0 G2 i `9 c( L* f3 M
cement), and polymers, which were limited to naturally
) {$ Z0 J& k/ u5 F% voccurring rubbers, glues, and fibers. Composites, as a& H, V1 c1 K8 _
concept were nonexistent even though wood and animals,9 ?# y+ \% r: j: K6 f3 A# Q
each composed of different materials, were used in
% `8 ^& C3 X5 E# l! |, ^4 }, Ta variety of ways. However, the uses of alloying to enhance
: O* p. B7 [* f# [# @6 mthe strength of lightweight materials, such as pewter,
* Y0 \6 r2 x* J; z" u$ Q+ eor copper additions to aluminum, were established
- }# n2 Q$ d( n$ J- w8 {techniques, known well before this century. This knowledge. T' b4 h) i$ f
was used to build the first dirigibles. The useful4 B W9 b- S1 ?* V
nature of a material was often understood through serendipity: d* q; Z& j& J" ~1 J4 [; o
and not through an understanding of its structure
! t8 k. ]& V/ F% V3 M8 Z5 Cor the relation between structure and properties.1 g3 r5 E4 i9 E7 y( M
We still cannot predict in any quantitative way the evolution4 g C l, F8 G0 _0 J
of structure with deformation or processing of a/ ?+ V9 R) A% o, t- g! \
material. However, we have come a very long way from( ?* L8 A+ e7 n- N3 V( X) O
the situation that existed a hundred years ago, thanks to& \% S7 x8 _/ ^# Q( w
the contributions of twentieth century science to our understanding4 L" M# v7 s( g" j! j0 a3 R) U
of atomic arrangement and its determination
- p0 S9 ?& L1 e0 t, {/ O$ y: c" jin a material. Our classification of materials by symmetry: ?8 J& t7 `$ F6 i, p# I. T& o4 k
considerations came into existence once atomic
# t! G$ z' Q6 m9 sarrangement became known. To the seven crystal systems
; f* _& r" e8 X/ [/ i7 o$ J- Oand amorphous structures, typified by the glasses
3 ?6 u) h# ?% R1 Q% @and liquids, we can now add quasicrystals and molecular! u: b; y* H9 e5 |# [$ V
phases, such as fullerenes and nanotubes, in a crystalline6 ^+ c! ^+ J8 L9 h. c
solid." I- s1 Q# ]( m6 S
The crystal systems define perfect crystals. At finite2 Q- a- E! ^2 k' B
temperatures, the crystals are no longer perfect but contain2 w% a0 k2 w: r3 p
defects. It is now understood that these defects are8 p. O! p; V3 H& E! s- k ?# n+ t$ }
responsible for atomic transport in solids. In fact, the
& o) C ` {' ?' }structural properties of materials are not only a function
% R3 v8 ]4 a6 R/ M7 t. E' S3 hof the inherent strength of a material but also of the, @" b# ]/ j: |$ h- m
defects that may be present. We know that aluminum is. J; L& S0 T+ x) W7 R( ?
soft because crystallographic defects, called dislocations,, }- |7 i8 z/ o$ u( g+ ` B4 }. @
can be readily generated and moved in this metal. In0 A. @; D0 d0 ^# k& Y
contrast, in alumina (Al2O3), dislocation generation and
2 L; c: q: f$ @7 l; f) jmotion are difficult; hence alumina can be strong but; z2 R: M0 R- I e: I: P
brittle at room temperature. The addition of copper or1 z r7 Y- o$ D% ~1 l& t
manganese to aluminum creates second-phase precipitates,+ D e4 u) ^* | z7 Z. \7 C
which inhibit the motion of dislocations, thus enhancing3 G; E0 A6 M+ m# o6 w9 ^( z# V
its strength-to-weight ratio. Our ability to improve( h8 M/ \6 P/ W
the strength-to-weight ratio in materials has
% O% F: P' y7 l8 e" Kincreased more than tenfold during the twentieth century.
6 V1 p% I. K: Z! d6 `7 r' lThis is to be compared with a change of less than. V# O3 _: M" b
ten over the last twenty centuries. Much of the increase
$ [- L0 K3 }. d, T" a, {in this century has come from an understanding of the
! E$ \. l/ N! y! F* X0 Urelationship between the processing of materials and
P0 ]& b. Z2 C6 w# _+ ztheir structure. The highest strength-to-weight ratios! K- D: J# ^/ V" S3 k" E4 C3 u8 r1 ~
have been achieved in materials in the form of fibers and
2 N4 v1 V# q7 \0 P7 onanotubes. In these structures, dislocations either do not
- P7 F& U. |9 Zexist or do not move.
0 x/ |5 i9 A# mMost structural materials are not single crystals. In6 A, `- }1 x/ W- i
fact, they consist of a large number of crystals joined at5 @: e( M6 W F# f6 a
interfaces, which in single-phase materials are called7 c2 @* o: k% j+ O/ ^+ l' K
grain boundaries. These interfaces can, for example, influence i7 j4 q- M& T: l% T3 \
the mechanical and electrical properties of materials." Q; i- D# b" y2 f& o% Q% U( l
At temperatures where the grain boundary diffusion
p) \9 [% C+ M6 L) V' e Frate is low, a small grain size enhances the strength. L! ^. s0 g, m3 J6 l- f
of a material. However, when the grain boundary diffusion( {+ a1 E7 j% j1 u! `7 h: {2 J( y
rate is high, the material can exhibit very large elongation7 w' V' F1 ^! Q" T8 y0 n
under a tensile load (superplastic behavior), or1 \. G+ N. F/ P% x: I) ^
can exhibit high creep rates under moderate or small8 T3 C' p9 D( l9 j
conditions of loading. In demanding high-temperature
, V) p$ j( ?8 X& lenvironments, such as the engine of a modern aircraft,
( l! Y0 X' e- Z, C9 d* {" j! C* ?grain boundaries are eliminated so that a complex part,
' m, J0 k* F$ f) Xsuch as a turbine blade, made of a nickel alloy, is a single
* f3 R" `7 c& h1 r5 Q* p3 U, vcrystal. Thus the use of materials for structural purposes' {4 A5 W- j9 s8 y% p* V
requires an understanding of the behavior of defects in/ m( }4 i- c* K7 g$ T% _
solids. This is true for metallic, ceramic, and glassy materials.
# |' A- {* |0 Y0 T: l* r5 d. IBoth ceramics and glasses were known to ancient civilizations.
3 I, X9 C* A& _5 e! f- XCeramics were used extensively in pottery and
; Q: A, |1 u. E2 I7 @* T: N; xart. The widespread use of ceramics for structural purposes
3 Z0 E7 ^3 r3 \6 X' |# v& m3 zis largely limited by their brittle behavior. This is+ B* l3 }% w' r* Z9 u) q, X. V
now well understood, and schemes have been proposed
# G6 w& q2 e- W" K5 R7 o) X2 P- x* Sto overcome brittleness by controlling the propagation
+ G! w' h' k( h" h" Y& yof cracks. In metals, dislocations provide the microscopic
; B4 p ?% g$ `( A2 l8 F) [mechanism that carries energy away from the tip2 Q' v0 s; g( H# C4 {
of a crack, thereby blunting it. In ceramics, the use of
$ K2 a! u3 S0 ]3 S6 Nphase transformations induced at the tip of a propagating
! ?! w6 L, |) q. Bcrack is one analog of dislocations in metals. Other0 y, Z. {$ |6 ?; K% ?
schemes involve the use of bridging elements across2 y; ^& P/ h( `5 B
cracks so as to inhibit their opening and hence their3 G3 w6 y% |& o7 F, V7 |
propagation. Still another scheme is to use the frictional8 l1 c, S. C9 `! N+ D9 Z$ H, F, t
dissipation of a sliding fiber embedded in a matrix not! e$ R% i+ z: h K
only to dissipate the energy of crack propagation, but; N$ F% i" z c& i! y
also, if the crack propagates through the material, to
( m N* _ f9 `provide structural integrity. Use of these so-called faulttolerant2 N& q' k" P4 W1 e
materials requires both an understanding of mechanical& p2 ^3 I q3 ~ t6 O/ s
properties and control over the properties of. l3 K6 l7 V4 c. J* K: d! P
interfaces to enable some sliding between the fiber and
0 u2 G1 o0 A3 H5 _8 d9 Wthe matrix without loss of adhesion between them. Such
' J, @8 b+ w1 g1 |; ischemes rely either on composite materials or on microstructures
" Y& B7 X1 s/ J- R/ ]- \5 Hthat are very well controlled.. V+ W4 Y0 b: Y: a
The widespread use of silicate glasses, ranging from0 P8 V, E8 ]( d; B
windows to laptop displays, is only possible through the
' t6 f5 D3 g- `" relimination of flaws, which are introduced, for example,
?1 c- t) O4 |; x9 bby inhomogeneous cooling. These flaws, which are
* X$ ]+ X0 S0 ~1 U6 H/ sminute cracks, are eliminated during processing by controlling+ ?% _: I9 z4 i% e' E% N
the cooling conditions, as in a tempered glass,
" q: k: L# [! z) h2 ` v2 yand also by introducing compressive strains through
2 F- p/ R8 J9 Acomposition modulations.
: V4 G& P5 U2 A9 g( u dThere are a number of fibers that are available for use
% ? w M) M$ A) o; ^ V- zwith ceramics, polymers, and metals to form composite* R9 r2 f9 }9 d8 g, M$ G+ M
materials with specific applications; these include carbon$ h$ F8 p! `" m2 }- x" z" W
fibers, well known for their use in golf clubs and fishing5 U# Z/ N% z P6 ^
rods, and silicon carbide or nitride fibers. Optical fibers,
" ~" m1 E4 M/ U! m0 L+ A$ i/ Fwhich are replacing copper wires in communication# F: b2 Y3 q$ c7 w$ ]( v* \% O
technologies, owe their widespread use not only to their+ |0 n2 y" s- S& ^. z2 \& E
optical transparency, but also to improvements in their
8 |0 q! H) }" U1 _4 D7 jS332 P. Chaudhari and M. S. Dresselhaus: Materials physics
! z) X1 n6 j: `. x) V9 VRev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
: l$ i, }9 M, c: U! W t: s3 {structural properties. Fibers must withstand mechanical) r8 c5 f" {! j
strains introduced during their installation and operation.
3 p0 F! U( Z q9 _+ eThe use of composite materials in today’s civilization2 d/ \/ o. [4 Q3 h# o, G
is quite widespread, and we expect it to continue as new
9 l+ K* {& m+ m, oapplications and ‘‘smart’’ materials are developed. An ~& x. y: ]3 U8 A
outstanding example of a functional composite product% n$ q4 E2 k) t6 B1 x/ e
comes from the electronics industry. This is a substrate,
9 \. n2 _# W- f6 F$ Tcalled a package, which carries electronic devices. Substrates
& {' m0 e& f3 Nare complicated three-dimensionally designed
" U, [5 o- }# D estructures, consisting of ceramics, polymers, metals,
1 v. p0 E# W0 Wsemiconductors, and insulators. These packages must- J% d. D) ~1 ?% {- x# z, @3 R0 ^! E
satisfy not only structural needs but also electrical requirements.
) v9 f" R V) f9 p; n& y; tAlthough we have made great progress over the last" D. \! E" \: C4 n' o8 u$ x
hundred years in materials physics, our microscopic understanding8 ~2 i0 b' d' u4 U( z' u
of the physics of deformation (particularly
9 g- Z' r9 A9 B3 S9 B4 win noncrystalline solids), fracture, wear, and the role of- @) t& u- y5 j. K! t& Y
internal interfaces is still far from complete. There has, {: n A T: T
been considerable progress in computer simulation of K( d3 A$ Y; Q- U% G5 X
some of these issues. For example, there is now a concerted
& T% @/ E k* f) {effort to model the motion of dislocations, during
" O i$ r5 R" `. O- v3 Y3 edeformation, in simulations of simple metallic systems.
0 ~3 a0 f, ] m) mWe anticipate that within the next decade, as computational
' ^/ A; Q8 K- n* ^) Fpower continues to increase, many of these problems
& t- ]5 {* o5 {" R s K: Vwill become tractable. The ultimate goal is to design
, A7 l. t1 O( H. Ea structural component for a set of specified- n, ?( m* ?+ \2 k0 b# w' z# z( ~
environmental conditions and for a predictable lifetime.
3 a4 l% @7 }+ Q2 Q) M) y* ?7 C; `III. POLYMERS
5 t+ _# t+ Q4 jPolymers, also known as macromolecules, are longchain; R; @: A. a' A5 F1 A' ]
molecules in which a molecular unit repeats itself
) {7 A% S6 o5 q) E9 A1 s9 j, _% ?along the length of the chain. The word polymer was
# c1 u# a5 {# @ dcoined approximately 165 years ago (from the Greek
6 y( U. ?/ a6 l. L; x* W4 S. l8 Y2 Gpolys, meaning many, and meros, parts). However, the$ O/ P/ ?0 J4 G: q" \; i
verification of the structure of polymers, by diffraction
' O. y3 r; ^: k# B7 }/ yand other methods, had to wait, approximately, another
5 I& Y7 a9 T' A; m f4 O/ q100 years. We now know that the DNA molecule, proteins,
2 M, D' p+ d, k9 f' wcellulose, silk, wool, and rubber are some of the* v: `( U( j( }5 B+ X& z) F
naturally occurring polymers. Synthetic polymers, derived
3 Q* a1 W+ O! T$ {mainly from petroleum and natural gas, became a
1 i0 V" M6 U ]3 k) `# q% }4 ]" Wcommodity starting approximately 50 years ago. Polymers7 m# U9 x1 Q) m3 o( ~: D; H/ \- t
became widely known to the public when nylon+ K& K' o0 \- f) [* i
was introduced as a substitute for silk and, later, when
0 T' H3 T1 ~5 H( \Teflon-coated pans became commercially available.
1 n: i! b+ b {" l0 u _* @Polymers are now widely used in numerous household0 P! p1 O4 K/ a8 H* W# H
applications. Their industrial use is even more widespread.
. k- g+ O+ ?$ V4 T* n* o: v' t5 lMost of the applications associated with polymers
, |! H3 v. B0 {3 t; Q- L. A# I+ bhave been as structural materials. Since the 1970s it was8 t4 ~/ T" q9 `! O& r( V; m$ q/ {8 @
realized that with suitable doping of the polymers, a* m% t0 d( a9 a9 s/ O: ?
wide variety of physical properties could be achieved,) i7 V7 \6 t5 f& a g
resulting in products ranging from photosensitive materials# `/ N; n' d7 J+ U6 f9 A
to superconductors. The field of materials physics" W. G: Z. T) Q; m
of polymers has grown rapidly from this period onwards.. y' q3 f; G1 V, C0 W
Polymers are a remarkably flexible class of materials,$ O; N4 K7 n, P
whose chemical and physical properties can be modified
0 y1 [6 S) b: k$ P3 K3 _1 dby molecular design. By substitution of atoms, by adding
4 B/ T3 L" r( b) F; w! Aside groups, or by combining (blending) different polymers,* W) c) j/ O0 W( {% w8 T% s" E
chemists have created a myriad of materials with' M& r$ Y% E& `
remarkable, wide ranging, and useful properties. This3 @: s! P7 x- G; j
research is largely driven by the potential applications of
2 {1 s7 S+ r7 P& M6 r& W% ethese materials in many diverse areas, ranging from cosmetics
# {) Y) J( b6 A3 ~2 G1 ~to electronics. Compared to most other materials,/ r3 ]0 G$ b3 X0 p. q8 U- i
polymers offer vast degrees of freedom through blending' t+ n4 A7 M8 t+ m3 o
and are generally inexpensive to fabricate in large
7 F r6 f, c8 ]7 Y% H/ Mvolumes. They are light weight and can have very good3 s4 r5 Z$ k9 `$ P" g: B& H
strength-to-weight ratios.: z2 f5 R8 ~! a. X, x
Polymers have traditionally been divided into five! t4 C$ H' X( `. ?; W! e/ T- }
classes:
1 n* G8 w- j- f) k(1) Plastics are materials that are molded and shaped
0 N2 K+ ?+ c/ m# hby heat and pressure to produce low-density, transparent,1 N4 d- l1 n# y5 O
and often tough products, for uses ranging from, d* O+ b, y& H8 U7 C* h
beverage bottles to shatterproof windows.+ K! J6 R, ?2 j% R5 g1 K2 @" H: a
(2) Elastomers are chemically cross-linked or entangled2 B. A# Z' s& m* }
polymers in which the chains form irregular coils
3 E$ R5 M# h. G: lthat straighten out during strain (above their glass transition l3 T& d1 M, R+ e. {4 j2 A- z' [& w( u
temperatures), thus providing large elongations,2 m1 N3 O$ ~& h, h
as in natural and synthetic rubbers.! x: `0 l9 G" ^
(3) Fibers, which are spun and woven, are used primarily
" v+ y0 v" H1 @: T, {! y' K9 Zin fabrics. About fifty million tons of fibers are produced
; | ^8 J& S) ?8 s1 ^annually for uses ranging from clothing to drapes.4 k4 w9 j$ ^& R
Apart from naturally occurring fibers such as silk and
5 W: A5 P% a0 ?6 K0 X* Lwool, there are regenerated fibers made from cellulose
d, w, v1 K1 ?3 ?" y6 ~0 ]* R9 }polymers that make up wood (rayon) and synthetic fibers,0 w/ G# A u2 _1 b/ f
comprising molecules not found in nature (nylon).
1 z P* Z! w: U) q5 r. Y(4) Organic adhesives have been known since antiquity.
5 X; \% N' C) B wHowever, with demanding environments and performance! _- a' z7 _( q- {2 e
requirements, synthetic adhesives and glues
, r3 i. u4 j4 L) g- Hhave largely replaced natural ones. The microscopic8 L% q( ?+ n9 c; i3 ~7 k- h4 ]! ^
mechanisms of adhesion and the toughness of joints are) F' [ Y `, {7 U3 O/ d( m7 K: }
still debated. There is an increasing trend to use UV
8 O- t5 x+ F% M# o$ Q! bradiation to promote polymerization in adhesives and,$ e' _% D0 F6 n4 J8 Z; [7 x+ _
more generally, as a method of polymerization and cross3 B6 {5 N' b" |8 _
linking in polymers.
$ B0 m5 f/ @8 a9 i. A, }(5) Finally, polymers, frequently with additives, are
5 l m3 ^" ~- q- H: n% U+ K9 A+ bused as protective films, such as those found in paints or
! N! Q5 I& x4 Avarnishes.7 B0 |. \% {5 Q. |2 w, s
Physicists have played a significant role in explaining
! W1 ~( `# Q$ t R5 A- R0 g( hthe physical properties of polymeric materials. However,. F3 F- W3 S8 D( x# c4 y
the interest of physicists in polymers accelerated when it
0 H" o6 x, }+ X* v5 p' ]6 kwas discovered that polyacetylene could be made conductive% }9 O! K5 A$ g, I
by doping. This development was noteworthy1 _/ ]: g! O" `; H4 ~1 c P
for it opened the possibility of deliberately controlling
3 k l4 s$ M) }% Y0 r. Sconductivity in materials that are generally regarded as: D7 r' g6 X2 ?% O* J5 j. \
good insulators. The structure of all conjugated polymers,
5 N: m1 I; o7 S& k8 o( mas these materials are known, is characterized by a
q5 ^, x6 Q1 o( {+ n5 A- k Nrelatively easily delocalized p bond, which, with suitable
% ?+ g% X2 A O; r2 [& Ndoping, results in effective charge motion by solitons,
; F8 o, J% @% n b1 [polarons, or bipolarons. Since the discovery that polymers% A& l+ K( ^5 ~" E: m3 u$ t
could be electrical conductors, active research areas% ?, h1 D- ?4 G' f% s/ W, Y" k# b3 U
have developed on the physics of polymer superconductors, K$ C/ d5 v% P! [
ferro- and ferri-magnets, piezoelectrics,- x6 V0 R0 I% Q3 ]7 r7 O
ferroelectrics, and pyroelectrics. Within the field of) S, w. J; h( ]6 w3 o H6 G% C0 ?
doped polymers, devices have been built to demonstrate
* t/ x! G( s4 nlight-emitting diodes, photovoltaic cells, and transistors.
# x) g/ M3 I$ K: HConjugated polymers have also been investigated extensively
4 N3 [) I& w7 a8 ^; F' lfor their large nonlinear, third-order polarizability,
. M: A- q1 ?1 a, m4 w% i @which is of interest to the field of nonlinear op-
7 R' V4 V& P6 W5 t" C1 c! ~P. Chaudhari and M. S. Dresselhaus: Materials physics S333
$ R+ o( b. w5 w) ?3 K: \* |* yRev. Mod. Phys., Vol. 71, No. 2, Centenary 19993 n8 ^( h$ G+ r5 h
tics. Large nonlinearities are associated with the strong
" J7 a, B& v: N0 E- [polarizability of the individual molecules that make up
1 W' }7 `3 H2 J6 `the building blocks of the polymer. Furthermore, the
& n |3 x) _: `1 F! d3 k( |. Dflexibility of polymer chemistry has allowed the optical& o1 P1 v% y# S' }0 ^$ M2 {
response of polymers to be tailored by controlling their! Y) G9 f, |& F+ t/ U
molecular structure, through the selective addition of
# G8 u9 a( N5 w4 Rphotoactive molecules. Hence these materials have been" P8 k3 _: Y; G3 z# |6 I
widely investigated by physicists and engineers for optical: B# t* A+ G" K. @
applications, such as in holographic displays (dichromated8 t8 M) i9 w4 ^% [; c
gelatin), diffraction gratings, optocouplers, and' K$ P5 Q2 k/ G! C, V+ J; C9 h
wave guides.
/ T. o: E" |) k8 K* a1 _Polymers have long interested physicists for their conformational
3 N) z) h% q$ {8 X( ?6 p5 [and topological properties. This interest has
- L [& ]+ r7 V# h& ?% Y9 |( X( xshifted from the conformational behavior of individual9 s( ?9 B2 x9 ?" H1 x3 k3 C8 _4 J9 K
molecules to that of a macromolecular assembly, phase
! C4 I+ {! g1 K* Bbehavior, and a search for universal classes. Block copolymers,
% A! f9 N. X7 O" qconsisting of two or more polymers, can give
& n0 o) T2 `% |) A) frise to nanoscale phases, which may, for example, be4 T/ v2 p7 `- f4 |
present as spheres, rods, or parallel lamallae. The distribution8 y$ T3 v9 {1 r$ O6 `3 z
of these phases and their topologies are of current
5 J i n$ O* \# h- ~ ^theoretical and practical interest. Block copolymer/ F8 U; Z9 I8 q; p
morphologies are also being used as nanoscale templates' F" }' O- P. L/ [" t) V: T9 c0 U* ^
for production of ceramics of unique properties having
% Q( M% M9 T' lthe same morphology.
( Q; ?) G7 ~* mBlock copolymers are also of interest as biomaterials.
$ {/ i. r5 O0 P% F. j- ]Proteins are an example of block copolymers, in which% B8 x( J1 d* I* p
the two phases form helical coils and sheets. Attempts to
$ P) ]1 a+ k* i, H* Q7 f: ]mimic the hierarchical structure present in natural polymers6 Y1 [( A! k# s+ ^+ f
have only been partly successful. The principal difficulty, m: o) a! G, e# F
has been to control the length of the polymer5 c/ K& ` o* R( ^
chains to the precision that Nature demands. Significant6 Q4 B( l$ F' G z5 [2 A! C
progress has been made in controlling polymer morphologies
) X/ ]& y/ W* M, twith the use of new catalysts. For example,1 K' k4 Z. L# `* E# n: y
metallocenes have been used as catalysts to control$ P: n. Q, M$ R+ z1 W& q) k
branched polymers and organonickel initiators to suppress4 @! V& @9 `/ P7 c! v) }
chain transfer and termination, so that polypeptides, [0 [8 x- }7 z+ f/ l$ T: X7 p
with well-defined sequences and with potential for' n9 a- O" C6 q) z8 J9 D- V
applications in tissue engineering could be made. The( r, O% D+ u) u. Z" W
growth of well-controlled polymer chains is an example. D2 {1 p% n# T7 _6 {0 y3 B( x& }
of ‘‘living’’ polymerization.
* E6 N! m9 [! tThe static and dynamic arrangement of atoms on the
* a% {! }1 W1 {: e5 xsurfaces and interfaces of polymers is another area of
, f) ` ?9 R0 f8 D: C( c( ~4 Oactive investigation. For example, thin films of polymers,( w/ S( R& E% s) J) n
in which the chain lengths are long compared to the3 f6 ~8 A8 F+ A$ a
thickness of a film, show unusual physical properties: the. [6 N6 B, N& k& [ u ]/ R
glass transition temperature for a thin-film polymer decreases
4 l' H/ S, h" f& v0 q& Jsignificantly, but between solid surfaces polymer
7 ?: E% ^3 [" ^- }- W8 G) f- k8 Yliquids solidify.
3 \: |- u( n K) c; x7 I, VEven though we have some way to go in making tailored1 m0 f6 j7 h1 j* L% C3 V
proteinlike structures, polymer research has0 n+ I. O% j( ]
played a significant role in the class of materials called4 O+ S# c. `* L' }& I3 |
biomaterials. Polymers have been used, for example, to
+ z1 d. L- Z( Jproduce artificial skin, for dental fillings that are polymerized" _% J9 a$ h R' F8 H' u* I
in situ by a portable UV lamp, and for highdensity
5 }: \% \4 V" Dpolyethylene used in knee prostheses. Physicists
1 z+ ^* h0 W; P% Eplay a significant role in these developments, not only
+ ~' w" G% i2 o4 i1 R. wfor their interest in the materials, but also because of
8 a7 m3 y: n4 R* F5 V' O, A. O, Ptheir familiarity with physical processes that can be used1 {0 z7 D) F: h% F y) y
to tailor the properties of polymers. A particularly good
! \6 u' J, w! a$ ]* q) Nexample of this interplay is the recent and rapidly growing/ ~( |, a' P, m+ g8 Q
use of excimer laser radiation to correct corneal abnormalities;
U+ n+ @* d3 C, H: D" h" Vusing a technology developed from studies
- q9 p6 b& b: m' m. pof the ablation of polymeric materials for applications in
8 n, m% v# k* v0 q5 i6 Athe electronics industry, physicists realized that the
1 J7 `/ _2 j v6 g& gsmall, yet precisely controlled, ablation of a polymeric6 Q9 s9 ]) k& t0 `5 N+ M6 }
surface might be useful in shaping the surface of an eye.
A$ n4 ~( @7 d+ [) }( ]4 }IV. ELECTRONIC MATERIALS* R7 q; I9 B* P5 a* h2 S
The roots of the electronic materials field can be, k+ L/ k+ ^9 y0 S' c; I* C
traced back to Europe in the 1920s, with the advent of, I7 Z- U2 r( Q8 J
quantum mechanics and its application to periodic structures
" a- M3 Q+ L4 e6 u9 x% X# rlike those occurring in crystals. The early experimental! {6 L0 D) { a/ }# F
focus was on alkali halides, because these materials
- ?' _/ g0 Y/ }4 ncould be prepared in a controlled way from both a
) g! T8 N+ P8 |3 ^% |structural and a compositional standpoint. The creation& i l! {" J f" S; l7 e* e( o
of a strong academic program in solid-state physics at! a$ k8 h2 P4 e1 O
the University of Illinois in the 1930s had an important
# u+ e; F; x& D+ k& @# ~impact on the early history of the electronic materials8 X$ c! n. A! D) w r: C: M$ U7 W
field in the United States. This knowledgeable human( k# N& J1 Z2 \( ?5 r) g
resource played a significant role in mobilizing the national
3 m: g7 u- g; _1 p7 O5 k' d- `materials program during World War II, especially7 H/ e* c( c; t% \) f2 a: D
in the development of semiconducting materials' c% `; M5 D6 A6 h
with enhanced purity, suitable for use in diode detectors+ `0 Y* R/ r; N# s% \
at microwave frequencies for communications applications.+ R; `# w4 v$ R' {5 K
The availability of these new semiconducting materials
9 x9 j- T* _6 q! w! \0 O2 I" Vin purified, crystalline form soon led to the discovery
$ ]+ W; a7 B& W& X1 I3 x dof the transistor, which ushered in the modern
# |9 J. ?/ D# a9 |& s+ h% R) Wera of electronics, computers, and communications,
4 l. |+ r9 j# W7 G1 Zwhich is now simply called the ‘‘information age.’’
% v! d8 A5 U. `1 ]/ Y' ^' G8 _Semiconductors have been a central focus for electronic
% n: j9 m" }, Umaterials. Quantum-mechanical treatments of a) [& f( E+ }0 H# A
periodic lattice were successful in laying the groundwork
$ `) |- D/ I* J3 Q- r" Nfor describing the electronic band structure, which could9 R1 R0 @- N$ T: ~8 G4 R- m
account for electrical conduction by electrons and holes,# d: V& g) R" ?% f
carrier transport under the action of forces and fields,; t) \; S2 J0 z8 \
and the behavior of early electronic devices. Because of
9 O( s; e1 c0 I- ythe interest of industrial laboratories and the Defense
, Q& I% M! M% a2 Y7 Q3 iDepartment in the newly emerging field of semiconductor
7 J6 y1 G! o; I+ ~# c! C3 Kelectronics, semiconductor physics developed rapidly,
3 t! k& q; U8 @4 F8 |, aand this focus soon led to the development of the' ^( _4 r6 X* D
integrated circuit and the semiconductor laser.+ O) q) }$ b6 M5 f8 a* Z' r
The strong interplay between technological advances) C& @1 _, F% O2 ?+ u
and basic scientific discovery has greatly energized semiconductor
# E' I4 ?/ L# G% W! ?/ j) hphysics, by raising challenging fundamental
, Y2 d+ [! b0 S& B6 bquestions and by providing new, better materials and
$ t" v5 S* v% H7 K9 Y! zdevices, which in turn opened up new research areas.
1 D2 R# E* t+ |. f- ^# ]" R" fFor example, the development of molecular-beam epitaxy2 }0 Z! X" ]6 }/ Q \) A. |4 W0 P
in the 1960s and 1970s led to the ability to control
, j4 T% G& g5 h$ T$ Klayer-by-layer growth of semiconductor quantum wells ^. c( I8 G7 S; y! P9 Z! g: l
and superlattices. The use of modulation doping of the
+ W, E- l* g9 R& i! V' C1 D, Cquantum wells, whereby the dopants are introduced, a2 X; t1 L$ i4 Y) k. A0 G
only in the barrier regions, led to the possibility of preparing1 X/ s/ i8 ?. k/ f/ A
semiconductors with low-temperature carrier mobilities,; f& @3 Y3 N q1 c6 x7 E: _; U" L( h
orders of magnitude greater than in the best
, D; P; o) w8 _8 @bulk semiconductors. These technological advances; i1 P# h* ]- a+ t4 p! x7 c" x+ ~
soon led to the discovery of the quantum Hall effect, the
5 ~! }) J) S* F) c. L, {! W/ lfractional quantum Hall effect, and a host of new phenomena,3 Y- p' J3 w# l5 ~ X9 h
such as Wigner crystallization, which continue8 f% i, S% C5 c4 O/ l2 E) n
to challenge experimentalists and theorists. Lithographic4 t- B+ ?8 w: \8 d2 S
S334 P. Chaudhari and M. S. Dresselhaus: Materials physics+ s* k! o; N) O- E, p
Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
6 U+ J; C% h. X9 cand patterning technologies developed for the semiconductor3 g9 L' m6 H$ r! q
industry have led to the discovery of the quantized
1 {- h* I1 p0 F0 H# _: s( uconductance for one-dimensional semiconductors6 X, d3 [& N' F9 Y+ Z8 I8 i4 r* A
and to the fabrication of specially designed semiconductor3 c4 j/ A8 r8 R" _! O
devices, in which the transport of a single electron# I- y$ ?: m; y1 L1 ^
can be controlled and studied. The ever decreasing size \$ G4 w6 l0 L( l2 i: f
of electronic devices (now less than 0.2 microns in the
, T# P- ]- e, j p" jsemiconductor industry) is greatly stimulating the study
( q$ A9 A: Q5 f! nof mesoscopic physics, in which carriers can be transported; E5 n# m- ^8 w$ M0 ^5 ]
ballistically without scattering and the effect of
* t- u4 b- C0 w6 l% K5 b5 ?the electrical leads must be considered as part of the* v* I! h: O% {" d: f( ?
electronic system. New materials, such as carbon nanotubes
% C' W+ J! h0 \with diameters of 1 nm, have recently been discovered,
, T- I9 k* n4 M% {$ rand junctions between such nanotubes are being# Z, S- p$ e' E" D
considered for possible future electronics applications+ {0 c8 y2 O% Y, B# U
on the nm scale, utilizing their unique one-dimensional+ o* D6 g i# i+ t# |$ A; l( S% [
characteristics.3 W) _9 o8 r8 L& g5 g2 R5 h
The electronic materials field today is highly focused
2 u% k/ O5 p7 k: B2 z0 L- aon the development of new materials with special properties
- y& L2 t [9 Q% N1 m+ O% s' eto meet specific needs. Advances in condensedmatter
& e" b9 b. {1 h& Rphysics offer the possibility of new materials
$ \0 Q3 G( j1 V% r6 ~properties. In photonics, new materials are providing increased
2 O$ b, |, E; j2 fspectral range for light-emitting diodes, smaller0 Z3 f( t9 x' t4 E
and more functional semiconducting lasers, new and improved
- w5 h: t& T6 Y0 @) ~. a9 Gdisplay materials. The new field of photonic
+ n7 L3 J! i6 r% }$ ] Gband-gap crystals, based on structures with periodic/ @- Q. Z& o) s$ b( ~
variations in the dielectric constant, is just now emerging.
. s0 h; d7 F i, \2 ]Research on optoelectronic materials has been
/ F; m. m9 r" i4 ogreatly stimulated by the optical communications industry,. y' d0 j O9 R! Z
which was launched by the development of low-loss
# s; j8 c- l, S+ x ~, coptical fibers, amplifiers, and lasers.
M4 w- L# p' ]( a F- q) I5 aFerroelectrics have become important for use as capacitors
q' h' e# R5 C) s4 q3 Fand actuators, which are needed in modern robotics
) B+ D9 R+ u9 V" J8 n; c2 `applications, as are also piezoelectric materials,
* Q+ ^# n, C9 P2 ~which are critical to the operation of scanning tunneling
; i) y$ I2 I% eprobes that provide information at the atomic level on6 g; \, }* p7 ?5 }8 e. h
structure, stoichiometry, and electronic structure. The
7 E) f' I' M. T t* c- Rtechnological development of microelectromechanical0 n% D* d# M/ B
systems (MEMS), based on silicon and other materials,; b }, x6 ]9 H" L, c
is making possible the use of miniature motors and actuators
: a0 |9 |4 E& N' e! w! bat the micrometer level of integrated circuits.% P U5 c) p% M1 O1 [+ w
Some of these have already found applications, such as
, O3 r7 t$ |; }. }3 Rthe triggering mechanism for the release of airbags in; {8 x" m4 |3 q' ~9 P. H
automobiles. Such developments are not only important3 p8 @9 S7 Q, L: R9 b
to the electronics industry, but are also having great impact9 A6 g) ?& U0 }
on fields such as astronomy and space science,' ?9 A, ^4 Z7 |1 z: {0 q+ g" f
which are dependent on small, light-weight instruments* |3 q5 q1 I. _# [# {# T: b2 T
with enhanced capabilities to gather signals at ever increasing
1 o$ k1 v# H+ a5 x& Vdata rates and from ever increasing distances* ~" R" L1 A- P* ]
from Earth. The developments in new materials and, x/ ~- [ D, a0 Z7 @, I
low-dimensional fabrication techniques have recently rejuvenated3 [! E* D. x1 ], }0 d2 R; q2 z- f
the field of thermoelectricity, where there is9 x( y6 N6 R& N& a1 n
now renewed hope for enhanced thermoelectric performance! V' n1 f0 Q( p# h
over a wider temperature range., K# n, g0 [# f: g
Research on magnetic materials has been strongly influenced) Z# K/ U# T* q
by applications ranging from the development
& D: v5 u" [" Z" }: w" K$ |of soft magnetic materials (by the utilization of rapid/ O5 ]% q; S8 W! D5 B- w
solidification techniques) to hard magnetic materials
3 P8 g7 ]( i) k+ u5 Z, V2 K" s: ?such as neodymium-iron-boron for use in permanent
8 n) Z7 w W* M& j* P5 A( jmagnets. In the 1980s efforts focused on the development
2 {; h- V4 c& B* o8 Kof small magnetic particles for magnetic memory, p# E- m- K- x/ |- G t0 K
storage applications. New magnetic materials, especially
; Q2 e' x- k; a) `magnetic nanostructures, are now an extremely active$ |4 A/ ?4 C! G0 p L v
research field, where the discovery of new phenomena
) O% z" k- ]+ e- B' d0 H) qsuch as giant magnetoresistance and colossal magnetoresistance
( K+ Z S5 \0 Bare now being developed for computer memory
6 {' P2 \6 g' j$ y! |applications.
4 R" B) b# |9 n3 [4 wThe strong interplay between fundamental materials
: O$ a. R0 q# q9 h1 I" q, B3 Zphysics and applications is also evident in the area of
1 f! L; d* T+ D5 d5 hsuperconducting materials. Early use of superconducting
$ a, v/ B0 ~" P5 W; { n! ~materials was in the fabrication of superconducting magnets,7 F6 I& f, J* q3 _/ \- l
which in turn promoted understanding of type-II% Y2 x; k4 I; a/ i
superconductors, flux dynamics, and flux pinning phenomena.
' U( W' q- w% {- ^$ J# ~" pThe discovery of the Josephson tunneling effect
# l' {, o& L0 ]7 ~$ i3 Iled to the development of the SQUID (superconducting
) y8 q Q2 D# I; M4 A6 Yquantum interference device), which has' A0 s- D5 K# @$ ]$ h" V/ E
become a standard laboratory tool for materials characterization
. f- |) R* Y8 f* Z& S! s; h fand for the sensitive measurement of extremely! S6 t+ X2 T& {' X/ ^
small magnetic fields, such as the fields associated2 R. @/ C2 u* v% ^* l6 R4 u
with brain stimuli. The discovery of high-Tc
$ v$ C4 {- O- s5 e: {2 L9 r2 G3 {: osuperconductivity in 1986 has revolutionized this field,
7 l8 ]# {7 ~4 U& ?, y& Awith much effort being devoted to studies of the mechanism
( I2 q9 [0 v' ?for high-Tc superconductivity, along with efforts to
. M! `" j/ X' @: _. s: i2 Qdiscover materials with yet higher Tc and critical current
- ?& G. E1 H! F6 A0 yvalues, to improve synthesis methods for the cuprate superconductors,/ \% i; C6 a1 X
and to develop applications for these* |" E; C( H/ W+ _- l! T! M
materials to electronics, energy storage, and highmagnetic-
4 Z5 B( m0 l3 i; H. q1 s9 Ufield generation. C# j, ?1 t( S) F! m: }7 X' ^
When viewed from the perspective of time, the developments
: M! x8 z0 q- Q0 G8 k+ x: ain electronic materials have been truly remarkable.
6 p7 K. ] `0 I, M3 R; l: kThey have generated businesses that approach a
1 @2 ^( z; m/ a0 F# ~) _7 U4 s! {trillion dollars, have provided employment to millions of
' `* ^2 o" q2 Z" ~" {2 u! iworkers, either directly and indirectly associated with" G5 J9 a. b0 _
these industries, and have enabled us, as humans, to extend
" `) v( @# i: G- Q0 j d3 q9 N8 rour abilities, for example, in information gathering,
6 B( ]3 `! {- w% T3 Z2 \communication, and computational capabilities. Science
% H2 p- p0 f7 Z1 ?% ghas been the key to these marvellous developments, and* E! l0 z4 u( l; w! `; e
in turn these developments have enabled us, as scientists,+ t: J* a6 N6 |& v, P1 I
to explore and understand the subtleties of nature.
+ Q D, X7 \' K, o7 e1 e/ c0 sV. SUMMARY
& q- G" k) ^$ ~* B! m; B, Z& u* U1 nIn this very brief note, we have only touched on some
7 I4 s9 R8 ^8 s# qof the advances made in structural, polymeric, and electronic( J( S& n& T& d( s- H. B, J
materials over the last century, showing how materials
+ q; D% r) z/ K* D& G' Xphysics has played a central role in connecting
: l& a7 f: K7 K3 O8 B8 h+ uscience to technology and, in the process, revolutionized4 L. n! h6 O& C# F" c5 ?5 w
our lives.
- e a# H2 O0 ~6 R1 n# X6 g5 eP. Chaudhari and M. S. Dresselhaus: Materials physics S335
( `* }4 K* I z4 S! w k3 }" IRev. Mod. Phys., Vol. 71, No. 2, Centenary 1999 |
|