|
Materials physics$ A2 ? F" {# M3 |
P. Chaudhari, O6 F5 {- E" Z( F+ ]0 P
IBM Watson Research Center, P.O. Box 218, Yorktown Heights, New York 10598% K' s2 E+ e! o# u4 H
M. S. Dresselhaus! z1 E+ P/ I6 {- w
Massachusetts Institute of Technology, Cambridge, Massachusetts 02139-43077 X- I b# q q! |* w* W" J
Extraordinary advances in materials physics have occurred over the last century. These advances have
3 P4 L- P) R8 s6 |influenced almost every aspect of human endeavor. In this note, the authors sketch some of these% _- Y- |/ A4 V: [
exciting developments in structural, polymeric, and electronic materials. [S0034-6861(99)01502-0]
! s3 ^0 I: j1 }. K5 BI. INTRODUCTION( u1 ]. I2 Z A p: ^- d; ]
Over the last one hundred years there have been stunning
6 j+ [* b& O3 ladvances in materials research. At the turn of the
; K* z0 F) m5 Llast century we did not know what the atomic structure+ {2 m+ n9 d) a: e
of a material was. Today, not only do we know the structure," o+ {1 V% c% k, t
but we routinely make artificial structures that require
3 r8 c8 y: U6 `0 t* }- }placement of atoms at specified locations, that mix1 l s: e7 Y1 ^$ B. M& w
atoms to create properties not found in naturally occurring b4 H+ A8 U2 @( o
materials, that have the functionality needed by today’s" B R( g0 l7 b# d: r4 Y. V+ ~
technology, and that adjust their properties to a
1 r* i. X* [* V$ V: F! r: ychanging environment (smart materials). Over the last1 e2 b$ o4 u" Z, O
few years we have begun to manipulate individual atoms2 w V" f2 \: ^8 K* U
to form structures that enable us to explore scientific
( T7 K* z( }, o! }issues, but that will surely lead to profound technological6 [7 c: r* t/ d, k" y
and social consequences; for example, the manipulation
" }3 B9 i/ z# p9 Uof nucleotides in a DNA molecule, which is then1 {- l! Y1 t3 e0 E# p2 J
correlated with the functioning of, say, a gene and with* b/ h# Z6 g# `
its expression in the control of disease.
6 j9 k2 g/ x4 u }# [A hundred years ago there were no electronic devices,
& x. g8 Z X: P0 ?+ Pand today there is hardly any electrical appliance without
* M$ r/ |' T1 G' qthem. It is anticipated that in the near future there. [ d) r2 J/ e( Z$ G+ k
will be a microprocessor embedded in almost all electrical. [+ {! N8 @: {
appliances and not just in those used for computation
h! V% ?0 O, ~ \7 d- q2 l, e7 |or information storage. These devices, inconceivable a
2 o0 }' ]1 v) k0 ]' `; hcentury ago, could without exception not be made without6 W2 |5 C0 }4 Z$ T8 \8 @% H
the knowledge gained from materials research on) H5 m- G3 [& t0 ?9 [
insulators, semiconductors, metals, ceramics, and polymers.9 b) q- F& T) c7 H# y& q2 u* I- R& ^
At the end of this century, we have begun a debate
7 h, I" @9 M1 C Jon how far the present devices can continue to develop,. r: S& Z2 N+ ?% n
given the limits imposed by the speed of light and
* d% z- O d8 a/ h) wthe discrete nature of atoms, a debate that would have
& G+ m% v$ ~; a( p* abeen incomprehensible to scientists and technologists of" \5 R# y, h& K* r+ j% b4 }
a century ago and a debate in which we now discuss the
! I7 v! p* _3 e: v) z3 z6 s2 qpossibilities of using single electrons to switch a device
2 E: s+ ^, B5 q" t- x& H' Hon or off.
6 I2 V4 l+ O8 t2 BOur ability to measure temporal phenomena was limited& i8 h; U$ k8 ]0 M ?- @- q7 _4 r6 l3 f
to fractions-of-a-second resolution a hundred years; I. z2 H: ~* C, S1 D
ago. Today we can measure changes in properties with a$ y0 x- j+ Y' W- d7 @2 H
few femtoseconds’ resolution. Strobelike probes enable4 z1 M* x! D+ R# j" n o
us to measure phenomena ranging over time scales covering. c- \; t# L7 f4 U
more than ten orders of magnitude. We can, for
7 W, x8 Z* z, ]$ N9 m c: @example, study the relaxation of electrons in a semiconductor
9 |5 z7 W1 W* z3 L4 V3 y6 Lon a femtosecond time scale, the visible motion6 L) j+ _( C. M& `% d
of bacteria in a petri dish, or the slow motion of a sand
! V- s0 m4 B3 }% O. q7 Odollar on a beach./ j+ o+ A7 ~( k% _6 v" @6 W
Materials research spans the range from basic science,/ ^0 ^, `$ N& i6 G9 X8 W& `: C
through engineering, to the factory floor. This has not* t5 I2 x4 \/ j
changed over the last hundred years or, for that matter, G4 X) N, d6 ~* d, k2 j( q
throughout the history of human civilization. Materials3 b& ^9 b. H/ s L( g; v* ]
research came out of the practical needs of mankind.1 ^: |6 o3 S1 F/ H' L c
Eras of civilization were named after materials, so central
) t7 T }5 n, u. l5 W/ s2 a Whas been their role in achieving mankind’s mastery# ?: y8 }& }1 x4 }% F8 u# w9 y
over nature. The field of materials research can trace its/ ~0 Z7 s) r' d; e5 e: @3 Q9 a# @
roots to alchemy, metallurgy, natural philosophy, and5 e9 |8 e* t5 b3 o* \
even art, as practiced over many centuries. However, the
: N' k2 w& ^; nfield of modern materials research, as represented by' t( p2 z/ [8 n7 i5 C0 ~% f
materials physics, is only about sixty years old.
0 d7 l1 o b& l6 h* X$ ^Shifts in materials usage from one type to another are
# |1 c/ A+ d" ?& Zusually gradual. This is due to the very large investments
& p% Z5 w% c: r; g! cassociated with products in the materials-related industries,
0 R9 n6 O3 j2 U- w% z2 |complex relationships between reliability and functionality,2 p7 A/ Q g6 c' c" E, e; ^
environmental issues, and energy demands.8 o: {& L) Y( R6 F
However, measured over time, these shifts become quite
: R! G2 \, @ b7 u! ~perceptible. For example, in automobiles the ratio of
4 d0 V, p9 L* ~8 A; bplastic components to iron-based alloys has changed
7 m0 }0 ?2 ?( Jfrom less than 3% to more than 15% over the last two) x. A& z/ R" O* Q& I# Q: U% U
decades. Although the percentage change appears to be5 u9 B4 N3 o* q5 P
modest, the actual volume of material is large; over 40
' y" {* K0 j* [2 O+ T3 `million tons of structural materials are used annually in
. Z: g9 c1 q$ O' g8 V ?cars.
$ Q# R& k' q% G. IThe advances of materials research in this century,+ z1 P5 f( l/ s6 W8 B7 A2 G
which far exceed those of all prior centuries put together,# w3 }# c* O0 u- |7 \" m. X
can be illustrated by three examples: structural,$ ^4 k- Z2 G. e- m- Z) A5 v4 d
polymeric, and electronic materials. Our choice of these
, B7 L" T: L4 Q5 K; l: e- \three is somewhat, but not completely, arbitrary. It is
. e: `: t; C7 H5 cout of structural materials, particularly from the fields of
" l: R& p3 Q& d, w* r) b8 B0 }metallurgy and metal physics, that modern materials0 f l+ V' q* t! b
physics has evolved. From the crude weaponry of our, Q" ]2 y; ^$ W0 p* w
forefathers to our mastery of air travel, space flight, surface! X& I! \: E F" Y. m8 B
transportation, and housing, structural materials+ ^7 |8 [" T# Z# v$ r9 [$ ^' ~1 @
play a role that is unequivocally important. Nature uses
# I& B+ y& l* J8 ?% ethe second category of materials, polymers, in amazing
$ Z- R9 q6 s2 ^- q( E ~ways, to perform very complex functions. We humans9 w" D* c" k& c* R H2 r
are an example of that. Over the last hundred years, we
! Z% U8 o6 @* k1 dhave begun to understand and develop polymers for
( {& W9 _( H! ~$ u& Luses in food packaging, fabrics, and structural applications.' c& a0 ~. R; S% o
We anticipate that polymer research will play an
2 R8 ?# M$ d7 Yincreasingly important role in biomaterials of the future.
1 T5 r' {, h& a; P% d+ BThe third category, electronic materials, were not conceived
! ?0 v* A( k0 F% k2 s3 t' s# \until quantum mechanics was discovered in this: S. h' G" t5 w( O* O! @
century. Today we cannot imagine a world without telecommunication,& O( t# u2 S* k
computers, radio, and television. These7 O0 x4 ^* A1 R4 z1 |) E* o
and future devices that will make information available
& l. C' M9 p+ {$ J) g9 `8 c# ?Reviews of Modern Physics, Vol. 71, No. 2, Centenary 1999 0034-6861/99/71(2)/331(5)/$16.00 ©1999 The American Physical Society S3317 p' g9 M% A- ~* U
instantly are only possible because of advances in the
* \9 g, l) A: v: B1 }( v' ~# L0 Zcontrol of materials structure and processing to achieve6 r- e* J. o! g1 Z
a desired functionality.2 M4 L7 e, Y. @8 K$ O& j% y" e
II. STRUCTURAL MATERIALS
7 L8 l$ a* w- l7 S& JAt the turn of the last century, mankind’s use of structural
. B$ }: m/ z( J' i Z% ^( |, wmaterials was limited primarily to metals, particularly$ {! j1 T9 y6 C8 x& E% m% w
iron and its alloys, ceramics (most notably Portland. T( N$ U- y1 |9 `4 j
cement), and polymers, which were limited to naturally8 C, k M M, h' i
occurring rubbers, glues, and fibers. Composites, as a
+ \; i+ a' F) H, d# Qconcept were nonexistent even though wood and animals,
, A; M4 m9 S# U$ ueach composed of different materials, were used in
~8 G4 w9 v/ H3 Va variety of ways. However, the uses of alloying to enhance
8 j3 o; l1 w1 X# ^ ?# h! K9 wthe strength of lightweight materials, such as pewter,
6 ~8 I2 T6 [* M& D2 S5 L5 Yor copper additions to aluminum, were established* g+ k# D" T/ \
techniques, known well before this century. This knowledge
* i, q8 y. `6 ? N% Uwas used to build the first dirigibles. The useful/ ~. s2 }/ H( u( K, L# `
nature of a material was often understood through serendipity9 ~& ?! Y2 a3 \ `8 g$ O- l8 K
and not through an understanding of its structure, c; |4 C; m" r7 `8 w
or the relation between structure and properties.9 X! p9 g0 D! R1 l0 x
We still cannot predict in any quantitative way the evolution# [& [" {& M1 W2 ^
of structure with deformation or processing of a
) w" Q. n7 B" c5 qmaterial. However, we have come a very long way from
( @5 R$ \$ X: c$ o1 s' B7 kthe situation that existed a hundred years ago, thanks to
+ G& Z2 G, E9 m' w4 }the contributions of twentieth century science to our understanding, ~" G: G/ F, U- l& t5 j: u
of atomic arrangement and its determination: w1 J( `- S* h9 U( W) N$ n
in a material. Our classification of materials by symmetry5 o, N. U {2 _/ f; m% t
considerations came into existence once atomic
' ^! x4 V* g9 w w& }arrangement became known. To the seven crystal systems
: {, i3 T) u% z1 i: h+ y/ Dand amorphous structures, typified by the glasses* k! h2 H) |! C4 }$ e. n
and liquids, we can now add quasicrystals and molecular+ S0 T% S5 z$ w/ s1 L: k/ U# y
phases, such as fullerenes and nanotubes, in a crystalline
C8 G R7 B9 w' \+ A- J) Qsolid.
) k* {4 {) W( P* GThe crystal systems define perfect crystals. At finite$ F. f3 O; ]2 Y% P7 F& r& l
temperatures, the crystals are no longer perfect but contain5 |, `: [! Q4 Z4 k
defects. It is now understood that these defects are
2 k& d0 T3 w4 D; k, E8 @responsible for atomic transport in solids. In fact, the+ X4 S) C+ D- U( H/ @
structural properties of materials are not only a function3 V) E, `: p0 m( q
of the inherent strength of a material but also of the& [ w$ _% Y- i" a: ^2 l
defects that may be present. We know that aluminum is" E7 F- a+ \7 [( ?7 C. V* t
soft because crystallographic defects, called dislocations,
% [& P! ?# }* q7 [6 ?+ `) Mcan be readily generated and moved in this metal. In$ c: f9 P# T- e7 s# P
contrast, in alumina (Al2O3), dislocation generation and
. X% C) w2 v6 f4 M* g& b% lmotion are difficult; hence alumina can be strong but( l! Z2 P1 q3 l$ s% r" u' `
brittle at room temperature. The addition of copper or) t! a C0 y* z$ f3 T
manganese to aluminum creates second-phase precipitates,1 W6 N2 k% A. y/ f
which inhibit the motion of dislocations, thus enhancing& V+ e) O: c4 P' ]( }
its strength-to-weight ratio. Our ability to improve
9 p8 }( J/ T8 |8 u: C1 e& e- b0 ]the strength-to-weight ratio in materials has8 s6 x8 G) C0 l
increased more than tenfold during the twentieth century.
- h$ j$ i! n2 k: ?* \' ?/ lThis is to be compared with a change of less than: ~6 d9 N5 Y( ] {
ten over the last twenty centuries. Much of the increase
) @% U9 _0 E( \9 lin this century has come from an understanding of the# Z' U X2 p, i
relationship between the processing of materials and+ N$ x/ u8 h! ^5 }
their structure. The highest strength-to-weight ratios
) m1 u+ j' v) X1 G0 t, c' X1 hhave been achieved in materials in the form of fibers and4 @6 x4 F6 \8 l& }; t r: _ j* X
nanotubes. In these structures, dislocations either do not
( }5 H. ]1 N3 n/ {3 z) Y. Kexist or do not move.
; m( j; u: L; ^/ V6 GMost structural materials are not single crystals. In$ S1 T. I$ w! ^* `
fact, they consist of a large number of crystals joined at
2 q) W( }3 D8 P& w# a9 binterfaces, which in single-phase materials are called% G9 f" h" n1 z$ w" z H
grain boundaries. These interfaces can, for example, influence C! k0 B. B* O: [) X2 S
the mechanical and electrical properties of materials.
* R, l* d; M) P1 a& m$ tAt temperatures where the grain boundary diffusion
. n, [" _$ G; X- j2 xrate is low, a small grain size enhances the strength2 g+ X2 l( p: W: z( J! q
of a material. However, when the grain boundary diffusion# k5 G8 e4 i E% _' h# M
rate is high, the material can exhibit very large elongation/ O% B, `6 Q, X- g8 ^9 U- ~
under a tensile load (superplastic behavior), or
1 g" e9 U- i+ i- F7 Lcan exhibit high creep rates under moderate or small
4 n8 Y7 d* p* O5 B3 Pconditions of loading. In demanding high-temperature
# f- D9 z; M" a3 y* E2 Cenvironments, such as the engine of a modern aircraft,% F6 _! H4 o8 ?9 {3 x3 T) c) E
grain boundaries are eliminated so that a complex part,
* T& x/ ^% T/ Z9 b8 `such as a turbine blade, made of a nickel alloy, is a single
- }1 u( U, L: a! v& ^" h" R- dcrystal. Thus the use of materials for structural purposes1 c' e n( ?. S3 E2 E+ ]$ Q$ [
requires an understanding of the behavior of defects in
' ~* g w5 y j5 Isolids. This is true for metallic, ceramic, and glassy materials.$ p" K5 [! l6 y' j
Both ceramics and glasses were known to ancient civilizations.( V# G4 H" K: l4 X6 l4 P. D
Ceramics were used extensively in pottery and
3 Y3 s+ G% b" u0 ]. {* T* e- V' `& Vart. The widespread use of ceramics for structural purposes
$ {4 ]3 O- x3 [is largely limited by their brittle behavior. This is2 j$ a+ q, [4 e
now well understood, and schemes have been proposed
1 \/ f) G- {/ \$ T" R' Z& j: ^to overcome brittleness by controlling the propagation
0 _4 E' H" W4 H; n, X C9 ?of cracks. In metals, dislocations provide the microscopic
% g7 Y( A* M0 Q: n& Dmechanism that carries energy away from the tip
& ?6 j e6 o y" f+ L& i& u8 Mof a crack, thereby blunting it. In ceramics, the use of
: t+ h5 j8 K8 C( o8 T" M8 S. Z7 ?phase transformations induced at the tip of a propagating
3 V, ~6 U2 A9 Y% J5 v# k$ n: w5 ?crack is one analog of dislocations in metals. Other$ M7 d U9 S. r6 H" r
schemes involve the use of bridging elements across
8 n% h7 b3 p9 _! o( B6 B& ?9 Vcracks so as to inhibit their opening and hence their
/ l" x2 z4 A1 {+ j( f" W& @" ]propagation. Still another scheme is to use the frictional6 [# K+ P' l" G9 S
dissipation of a sliding fiber embedded in a matrix not) t# _5 f9 i5 u3 A$ \- z* O
only to dissipate the energy of crack propagation, but* e) E: }3 Y; X5 e9 E* Q. o1 E
also, if the crack propagates through the material, to
1 q6 P: K# T9 Q8 h5 L' @* lprovide structural integrity. Use of these so-called faulttolerant
1 e/ W( @& W9 m! G$ \materials requires both an understanding of mechanical4 o9 f4 f" ]1 P7 N
properties and control over the properties of
; F# n! J% I$ u4 Z# a3 Iinterfaces to enable some sliding between the fiber and
6 q1 h2 N3 ?& ~; D+ r5 v/ O+ B, `the matrix without loss of adhesion between them. Such
3 B' N0 i8 ? k* ?# dschemes rely either on composite materials or on microstructures
- X9 p E* X6 s& T. z5 V6 u8 _that are very well controlled.
! i% L6 r: P: g1 X8 V3 aThe widespread use of silicate glasses, ranging from9 f. g$ Z" ?, V) Z4 P1 ~
windows to laptop displays, is only possible through the. L. E& |! j9 c
elimination of flaws, which are introduced, for example,
5 e) \9 Y5 k' K% f: c! Tby inhomogeneous cooling. These flaws, which are0 x: h5 ~2 [$ L" ~4 b" x1 \
minute cracks, are eliminated during processing by controlling
7 U% W8 c; T- y' H+ \" Othe cooling conditions, as in a tempered glass,- M" L |5 M6 e% R* E/ a
and also by introducing compressive strains through
, x c" n2 g, N6 N' N* Jcomposition modulations.' }+ e) h/ z+ C9 F& a! l. R
There are a number of fibers that are available for use
8 ^4 }! v1 N% [$ |1 u2 A3 |with ceramics, polymers, and metals to form composite }3 e6 y! A, B; B1 @! z
materials with specific applications; these include carbon
% z1 d5 S5 v8 `( G- ^. Zfibers, well known for their use in golf clubs and fishing" \4 C' W1 E4 g X) E8 s8 v5 F
rods, and silicon carbide or nitride fibers. Optical fibers,7 Z8 f2 [' F W* Z5 t
which are replacing copper wires in communication4 o; @+ l6 n e( q( s( Z' _! z
technologies, owe their widespread use not only to their& {( Y& W0 W {
optical transparency, but also to improvements in their0 K" V6 d6 a- c0 k1 L; m
S332 P. Chaudhari and M. S. Dresselhaus: Materials physics
6 h: I5 }6 P0 H$ W' I" XRev. Mod. Phys., Vol. 71, No. 2, Centenary 1999* l6 h7 ^) x7 z% \% E
structural properties. Fibers must withstand mechanical. R. e+ z0 M/ n
strains introduced during their installation and operation.
% J( A& e$ U. [8 wThe use of composite materials in today’s civilization
0 {. G3 M$ _! |8 _' xis quite widespread, and we expect it to continue as new
0 Z! Q( g4 x* O5 S7 Wapplications and ‘‘smart’’ materials are developed. An* b6 e3 q2 B0 e, T' \- N7 Q
outstanding example of a functional composite product
( B9 _) }) l7 O8 mcomes from the electronics industry. This is a substrate,
( Z) o' h8 I. D/ {called a package, which carries electronic devices. Substrates
0 V& z$ @. W8 A9 w+ v% _are complicated three-dimensionally designed) I( m9 T2 y" f9 I, _
structures, consisting of ceramics, polymers, metals,' ]# N; m. M) t
semiconductors, and insulators. These packages must
- I% x+ E" V1 @8 \% M* Q0 psatisfy not only structural needs but also electrical requirements.
$ F$ E* V4 C$ c$ v3 u% ~/ EAlthough we have made great progress over the last
( g- Z4 j6 t. K3 `7 A: D6 A3 o$ A Ihundred years in materials physics, our microscopic understanding
# L6 R: s. H) P1 Oof the physics of deformation (particularly6 D( ^+ b$ I) C: @+ x
in noncrystalline solids), fracture, wear, and the role of; q) a7 E- P5 U* f# B0 \
internal interfaces is still far from complete. There has, t- a5 t A& U7 E1 q8 |# G; Z
been considerable progress in computer simulation of
8 ]" u l; o2 C0 Asome of these issues. For example, there is now a concerted; @3 T+ v/ ~2 @/ N# K3 O
effort to model the motion of dislocations, during
6 P% X8 V' o$ [# B) W& ]3 g* adeformation, in simulations of simple metallic systems.
2 o: e- z! v1 kWe anticipate that within the next decade, as computational
% J/ l" e) Y% a1 P2 P0 L0 Z- e1 qpower continues to increase, many of these problems6 b6 e/ ?5 V& `7 F: s' y8 {
will become tractable. The ultimate goal is to design+ q& z; w: a0 N. x
a structural component for a set of specified
6 h# s- j& F4 y4 jenvironmental conditions and for a predictable lifetime.
6 t' x. A$ y2 o: `8 M: c6 @III. POLYMERS3 v9 U/ ?) h+ N5 e" w
Polymers, also known as macromolecules, are longchain3 s& r& w7 X$ D, L
molecules in which a molecular unit repeats itself U' V9 p& i! H. Z! E7 Q$ J" w
along the length of the chain. The word polymer was$ [9 I+ O U( m
coined approximately 165 years ago (from the Greek: O5 y: V: l U1 N
polys, meaning many, and meros, parts). However, the
' e. s4 g! {, }- pverification of the structure of polymers, by diffraction# ?8 g+ W2 q4 o
and other methods, had to wait, approximately, another. {, E5 K2 x7 {- l0 } q& j B
100 years. We now know that the DNA molecule, proteins,5 o. o; l1 [; F
cellulose, silk, wool, and rubber are some of the; W3 i) h' t0 x9 F( j3 r
naturally occurring polymers. Synthetic polymers, derived
. {: s5 G+ D* B& ]; q R' bmainly from petroleum and natural gas, became a k& Z9 g7 s; _
commodity starting approximately 50 years ago. Polymers
4 m! M" a" o( {5 G; j# rbecame widely known to the public when nylon
6 S; b4 }7 K6 }1 n" k" w5 Owas introduced as a substitute for silk and, later, when: y$ {# W$ C' R0 N
Teflon-coated pans became commercially available.0 }' S6 _0 L! _. {$ ^$ \
Polymers are now widely used in numerous household! Q$ u: f2 Q* L+ e6 `" d3 a
applications. Their industrial use is even more widespread.
% I# @ b' R3 p0 T* S2 rMost of the applications associated with polymers+ M9 C; X5 M1 z) |* D
have been as structural materials. Since the 1970s it was2 s8 b( ~ J& o6 \
realized that with suitable doping of the polymers, a, Q2 I9 y4 | H$ |( h2 g
wide variety of physical properties could be achieved,' ~5 F) y5 U4 h
resulting in products ranging from photosensitive materials
# S2 i% f! ^1 |9 f4 \, n+ |to superconductors. The field of materials physics$ l* i# P. O! f6 f
of polymers has grown rapidly from this period onwards./ U& b: z( U8 ~: L& f& o3 }
Polymers are a remarkably flexible class of materials,9 f8 q, B/ h( B7 @. I
whose chemical and physical properties can be modified6 U; k9 F0 O2 B( S! u M& m8 \% c& v
by molecular design. By substitution of atoms, by adding
0 ^/ w2 R3 D. ^; x `side groups, or by combining (blending) different polymers,. D9 J- a& [$ L" X( o# m9 j: w' W
chemists have created a myriad of materials with
+ [2 n6 \8 h0 A' E' C/ J' fremarkable, wide ranging, and useful properties. This7 X6 b. w0 p' S( Q( h9 G! F
research is largely driven by the potential applications of
" _1 k. H4 D( L& g0 d( O4 X* gthese materials in many diverse areas, ranging from cosmetics
T: u% c( C" D1 m7 [+ }; ^) w) n5 C( Mto electronics. Compared to most other materials,/ x0 V& z. T, L9 u' T/ ?
polymers offer vast degrees of freedom through blending
* R: C2 |8 |) x+ ^% U' L5 gand are generally inexpensive to fabricate in large; T$ {2 M/ }& v' w4 \
volumes. They are light weight and can have very good
6 W' j, {( j0 }- n* j% b1 Z. ]: dstrength-to-weight ratios.7 `( D2 n, @* J9 j
Polymers have traditionally been divided into five; E3 T! Z9 J8 c' j4 a
classes:7 B+ V" e: s- R2 A9 Y7 l/ p9 w
(1) Plastics are materials that are molded and shaped
: a8 T3 g6 x2 q( nby heat and pressure to produce low-density, transparent,. v+ E% w! T9 u6 C* a8 F
and often tough products, for uses ranging from8 _; l& a: r: I1 v% M
beverage bottles to shatterproof windows.$ e5 H4 ~. ?* A, H/ E }! c
(2) Elastomers are chemically cross-linked or entangled
5 k8 Q/ z3 z. c4 j) \polymers in which the chains form irregular coils/ f- V& I* W% h
that straighten out during strain (above their glass transition
: ~. U7 J; h. c# p1 C9 {temperatures), thus providing large elongations,
1 d' @8 s" h% J( P& `/ l! @# Gas in natural and synthetic rubbers.
* q# f I/ x1 [( a" N/ `(3) Fibers, which are spun and woven, are used primarily
% ]3 k- \3 X% f" o) @! W3 X0 H% X2 ~in fabrics. About fifty million tons of fibers are produced
4 H6 N- n( x7 ^, x9 ]4 ^annually for uses ranging from clothing to drapes.0 T) R: J* \" Z$ d7 N6 r
Apart from naturally occurring fibers such as silk and
* a, d d8 X' c j5 K" v2 Q5 L- Rwool, there are regenerated fibers made from cellulose* \' J# K4 h4 i: d! B
polymers that make up wood (rayon) and synthetic fibers,$ Q+ P% ^: g% C4 \' S( ]9 s' u
comprising molecules not found in nature (nylon).
6 x6 n' x! @4 c ~1 ](4) Organic adhesives have been known since antiquity.$ h( N k- g5 x1 L" U: m, \7 X
However, with demanding environments and performance
: {: }! ^ X" G5 b. Z# b% ?4 }: ]& hrequirements, synthetic adhesives and glues$ Y: @* R. ?. c3 U6 `
have largely replaced natural ones. The microscopic
0 |) t- D1 U& ymechanisms of adhesion and the toughness of joints are( b: {& f8 [( X) o9 v8 J: ?
still debated. There is an increasing trend to use UV$ _0 ^: S g! p$ B8 E' R. p1 f
radiation to promote polymerization in adhesives and,: B4 _: M; s7 K
more generally, as a method of polymerization and cross
* u0 I7 }+ b* Y" |- v0 \) s) n Llinking in polymers.& t2 z$ @* }3 N- U- Q7 c# j" l" O" M% c
(5) Finally, polymers, frequently with additives, are
0 p: l0 c7 _, E5 Y0 b c pused as protective films, such as those found in paints or0 O4 U9 p7 H" e
varnishes.# X/ _- z; s' V; l$ M. U
Physicists have played a significant role in explaining
5 b. s( @% h* D& [, t5 Q1 Uthe physical properties of polymeric materials. However,
, Y! D% _0 r" `, I( E Ethe interest of physicists in polymers accelerated when it
0 ?% i' M# n+ p; p. {was discovered that polyacetylene could be made conductive$ g6 @$ q0 a7 h, ]$ [& Z" e, y) Y& U8 O
by doping. This development was noteworthy) V2 \7 o% E2 g$ t
for it opened the possibility of deliberately controlling: X- n3 p t; n; ~- F% x
conductivity in materials that are generally regarded as- t6 n' Q2 s* S+ e- j* n( j5 f
good insulators. The structure of all conjugated polymers,) g5 d3 @4 s4 M
as these materials are known, is characterized by a8 _0 h+ F2 ~& K. r9 q
relatively easily delocalized p bond, which, with suitable
% E7 B2 u2 v8 k. w7 P% f. O( I1 b$ Wdoping, results in effective charge motion by solitons,
1 p j3 ?9 c5 a. l- y9 Qpolarons, or bipolarons. Since the discovery that polymers
& U1 S9 A/ `! J- x7 ncould be electrical conductors, active research areas
?6 n. M7 L% ]2 Whave developed on the physics of polymer superconductors,
. y6 W% B2 v% v# ^ferro- and ferri-magnets, piezoelectrics,
( l. B% p, s8 Fferroelectrics, and pyroelectrics. Within the field of
2 K( e0 l/ B/ Q% g/ B, @ n. Pdoped polymers, devices have been built to demonstrate2 Y( \& P I# P# G" P
light-emitting diodes, photovoltaic cells, and transistors.
6 M/ w$ k$ A) o1 Q) iConjugated polymers have also been investigated extensively m# ^5 d. k3 R
for their large nonlinear, third-order polarizability,
8 X0 I9 N: i2 |8 J; Ywhich is of interest to the field of nonlinear op-+ z1 F3 Z: W @1 V4 R
P. Chaudhari and M. S. Dresselhaus: Materials physics S333
& u, D+ P- W. {3 }Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
6 c0 }3 P8 k9 F$ x; i9 Ntics. Large nonlinearities are associated with the strong
, `& y9 H! i) Z; Y, H" |, C* Spolarizability of the individual molecules that make up
; g" C5 K, F* J( E: fthe building blocks of the polymer. Furthermore, the9 _& ^3 G( t' b% A) H
flexibility of polymer chemistry has allowed the optical
& a# h- j. k" d: `response of polymers to be tailored by controlling their
$ b/ Z0 q8 ?- a9 l2 umolecular structure, through the selective addition of6 E7 V" @0 r( e. M, s; n
photoactive molecules. Hence these materials have been5 F6 G( K& r. c( ]) \$ y: }' f
widely investigated by physicists and engineers for optical4 B) r# \9 R# T2 |. c, v5 w
applications, such as in holographic displays (dichromated# a' Y3 l5 ~4 A+ {
gelatin), diffraction gratings, optocouplers, and; P5 [0 {+ Q" W: y. d
wave guides.
# v% `; ^: Z9 S* X( w& \Polymers have long interested physicists for their conformational
T, P- ?8 c: m1 \5 T5 F9 uand topological properties. This interest has+ n9 X( a* R; l/ E! U% ^. O
shifted from the conformational behavior of individual( x4 v; \, R+ {9 r* y0 M
molecules to that of a macromolecular assembly, phase
, [+ ?2 N9 G( |3 ~1 o0 Rbehavior, and a search for universal classes. Block copolymers,
% i4 o& ^, C5 |" p- C! y: Q% J& w% xconsisting of two or more polymers, can give0 j* a. R/ j5 Y4 i y" J7 `3 Z
rise to nanoscale phases, which may, for example, be
# J( l9 b' p: P6 r. bpresent as spheres, rods, or parallel lamallae. The distribution7 B& ]* X+ V9 Z2 C$ u
of these phases and their topologies are of current
- `& Q0 y, s* a, S+ Ptheoretical and practical interest. Block copolymer
1 H, Z8 ~- G" w% Hmorphologies are also being used as nanoscale templates
9 C5 B4 k! L7 O3 W" Ffor production of ceramics of unique properties having: h K& R) g' |. g6 }; c
the same morphology." v+ ]; ?2 W% u- u- C! t4 P' }6 p
Block copolymers are also of interest as biomaterials.
1 z4 n0 c; {; j+ s& W( pProteins are an example of block copolymers, in which2 Y0 R* ]2 m% a Z
the two phases form helical coils and sheets. Attempts to. D. X7 `0 w. U: G# ^. |
mimic the hierarchical structure present in natural polymers
9 ?* d/ l+ d; s, A) Ihave only been partly successful. The principal difficulty
+ D" D/ E9 Q* V8 s) z* X) Dhas been to control the length of the polymer
3 K% j( l* S' Q* ~4 f6 D- I; a+ Q/ X" ?chains to the precision that Nature demands. Significant
4 C% F& m% g& i* Z4 S! j+ zprogress has been made in controlling polymer morphologies- M! X0 y% h7 m# L, b
with the use of new catalysts. For example,0 g. w% W3 A: {) ]1 _
metallocenes have been used as catalysts to control
* K/ T' C" \$ c/ p- B" zbranched polymers and organonickel initiators to suppress
* z7 _5 d }2 E) }8 i$ _+ @chain transfer and termination, so that polypeptides5 I' ^3 i# t8 q/ |: |4 V2 Z
with well-defined sequences and with potential for8 p, K8 C, {# u5 [4 `8 q$ X7 {* d
applications in tissue engineering could be made. The. X2 p V9 x/ K
growth of well-controlled polymer chains is an example$ k; s7 ~( L2 }1 A7 o9 u
of ‘‘living’’ polymerization.) t U# N0 F. S. _
The static and dynamic arrangement of atoms on the
) s, r! @0 \1 m* Usurfaces and interfaces of polymers is another area of
8 [: H3 w3 @$ s+ yactive investigation. For example, thin films of polymers,- h. L U2 N q; m2 u( B6 j
in which the chain lengths are long compared to the- S9 p& S" z+ G0 R5 h
thickness of a film, show unusual physical properties: the
1 \; a5 s/ L. |' r/ pglass transition temperature for a thin-film polymer decreases b7 {; [ s/ U
significantly, but between solid surfaces polymer5 r4 K1 W3 |; `& I: v
liquids solidify.8 }4 r9 B1 m3 Z6 f' k P& M0 L
Even though we have some way to go in making tailored# {9 Y* F: K. W; B
proteinlike structures, polymer research has. p! E& }0 s2 Z( v
played a significant role in the class of materials called
8 P) l6 a9 O# Y' ]biomaterials. Polymers have been used, for example, to
, P' [- t4 P- b0 G9 Jproduce artificial skin, for dental fillings that are polymerized( L, V+ S* {: q
in situ by a portable UV lamp, and for highdensity
8 t+ Y5 v2 P2 n4 N0 [polyethylene used in knee prostheses. Physicists8 b% g8 l$ F9 b
play a significant role in these developments, not only
i( x, Q$ w) Y; wfor their interest in the materials, but also because of7 ]" j s0 H: x% p# w8 D- v0 o
their familiarity with physical processes that can be used# S3 S! {- G9 [% E# V2 X" }
to tailor the properties of polymers. A particularly good1 G" M- l) ^9 {8 v# l% L* w
example of this interplay is the recent and rapidly growing
" L1 y, W, `5 \+ L& l9 Nuse of excimer laser radiation to correct corneal abnormalities;" s U+ x1 Z: b# ~# x2 y6 f
using a technology developed from studies$ C2 k& {$ B" ~6 T
of the ablation of polymeric materials for applications in
% h- f1 b4 I& f7 j1 ?the electronics industry, physicists realized that the
7 T K& h: r7 u) t0 usmall, yet precisely controlled, ablation of a polymeric
! }% Z) H3 `% k5 G" u0 i! dsurface might be useful in shaping the surface of an eye.1 G( g- f2 G. ]+ v& y/ {
IV. ELECTRONIC MATERIALS
: X; u, n# E- ]( O& ~0 {9 uThe roots of the electronic materials field can be
- ]3 k+ t5 n2 G: @traced back to Europe in the 1920s, with the advent of- J' N. P0 J# t; J( t- }' Z+ a' P
quantum mechanics and its application to periodic structures
9 S' ?, p- P# |+ v; H. Ilike those occurring in crystals. The early experimental4 P/ t! X4 [/ i/ A9 w
focus was on alkali halides, because these materials
8 e) x& R5 o7 r4 S2 Y3 L }& Fcould be prepared in a controlled way from both a
3 M& y* N- y7 F' h0 P) Jstructural and a compositional standpoint. The creation/ W3 z& Y: q% z. S0 G
of a strong academic program in solid-state physics at% j% f* {, ^6 ]- g8 M" d
the University of Illinois in the 1930s had an important6 G" D W4 w5 [4 `) R3 Y$ o
impact on the early history of the electronic materials
" n U# u2 t4 O* `+ Dfield in the United States. This knowledgeable human7 ]% n4 l" }) ?7 Y
resource played a significant role in mobilizing the national" K: B7 \9 H; X
materials program during World War II, especially
1 |0 y1 s4 W. |$ Q0 s2 \in the development of semiconducting materials3 f4 A5 l) m/ q0 {7 q7 E
with enhanced purity, suitable for use in diode detectors
7 k1 ?: Y- ~4 \# Xat microwave frequencies for communications applications.
+ a ~0 z) X4 nThe availability of these new semiconducting materials7 @2 J1 j; L8 L! m ~- K
in purified, crystalline form soon led to the discovery
% F6 Z& |6 }2 cof the transistor, which ushered in the modern
) O7 }0 U: L1 m$ x! Y% _ eera of electronics, computers, and communications,( j/ m( K: S7 A% o6 t) D
which is now simply called the ‘‘information age.’’" ]" s. Y/ u/ m+ C! ?, s8 v! h
Semiconductors have been a central focus for electronic9 D7 W- G6 K! r# b: ?
materials. Quantum-mechanical treatments of a
! W& l! r+ f/ z0 x) zperiodic lattice were successful in laying the groundwork6 O9 U/ _; R$ l% |- L, D
for describing the electronic band structure, which could
' o) v- J% e* R4 z' k! Uaccount for electrical conduction by electrons and holes,
8 V- Y8 F& ?) ]/ ^8 I9 d" r5 zcarrier transport under the action of forces and fields,
' c2 u- J7 y; V' e6 }2 d0 uand the behavior of early electronic devices. Because of
; K1 P$ w" B# @8 ?- gthe interest of industrial laboratories and the Defense& _5 }' d* T) @0 k7 |" h
Department in the newly emerging field of semiconductor
4 K* G5 ]' X& C: a/ Lelectronics, semiconductor physics developed rapidly,
4 A8 A3 V: s2 t- K4 Jand this focus soon led to the development of the
9 S% _; s! h5 W% e [4 @integrated circuit and the semiconductor laser.
6 u4 A! j- g) o& {) b( tThe strong interplay between technological advances
; ?9 K/ N9 N' v4 ?( }, p b& vand basic scientific discovery has greatly energized semiconductor. q% t' S% D, |) g: F" [
physics, by raising challenging fundamental
2 s5 V; o. Q8 D. |( tquestions and by providing new, better materials and `8 [; X" r; B6 a
devices, which in turn opened up new research areas.
" A" d: H! H9 K/ x& Q4 mFor example, the development of molecular-beam epitaxy
2 k Q$ |3 ~! uin the 1960s and 1970s led to the ability to control
$ s- q+ N( ^+ X6 S5 \; m" ilayer-by-layer growth of semiconductor quantum wells2 `- b( ~% Y. m
and superlattices. The use of modulation doping of the5 _1 o- T% t4 K+ Q2 c
quantum wells, whereby the dopants are introduced1 V1 F' M+ I$ ]
only in the barrier regions, led to the possibility of preparing& d0 S4 n$ \9 B$ [
semiconductors with low-temperature carrier mobilities,4 O, m# z2 T% h) ]4 I5 ~
orders of magnitude greater than in the best& ]' a& l5 p: p6 z
bulk semiconductors. These technological advances
2 O, p& G4 D* p1 Q/ ]/ ?/ g2 V2 rsoon led to the discovery of the quantum Hall effect, the% p$ X0 @# u3 a8 N' f' u
fractional quantum Hall effect, and a host of new phenomena,! y& h) N1 `1 X% J$ c6 \
such as Wigner crystallization, which continue4 I6 _: E8 g% ?
to challenge experimentalists and theorists. Lithographic4 ` t6 T! ^/ t) m* H s
S334 P. Chaudhari and M. S. Dresselhaus: Materials physics9 }7 {. u; F3 l: f2 u+ L- ]
Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
" c/ Y9 {1 ?. {: q. d ?) {and patterning technologies developed for the semiconductor
& y% Y5 q3 ^% nindustry have led to the discovery of the quantized
4 `4 {, p+ w* X* Gconductance for one-dimensional semiconductors! M% D m$ X/ f) F6 f* I
and to the fabrication of specially designed semiconductor5 \# z, L1 l6 _. s4 d0 l
devices, in which the transport of a single electron2 F( C0 I5 r1 E9 ]7 u+ N5 H
can be controlled and studied. The ever decreasing size5 g; J- r3 t( s; ^5 c: n" ^( d
of electronic devices (now less than 0.2 microns in the
2 A# T5 @% j' q% j! C" X9 wsemiconductor industry) is greatly stimulating the study8 G! z$ Y3 q @0 W( B# q
of mesoscopic physics, in which carriers can be transported: h8 ]2 R- ^; j7 |& S. `: {2 A
ballistically without scattering and the effect of
+ I1 F5 q) ?6 |$ kthe electrical leads must be considered as part of the
2 D9 b9 i6 q& W+ velectronic system. New materials, such as carbon nanotubes
6 N5 X- _' Q& K$ Cwith diameters of 1 nm, have recently been discovered,
, q* G6 A1 U5 ]; R: |* |. Pand junctions between such nanotubes are being
7 n5 j9 L. u+ C8 k/ h0 ]. aconsidered for possible future electronics applications+ c6 B1 O+ V0 K! {8 v
on the nm scale, utilizing their unique one-dimensional0 \5 f4 a8 A7 O) y
characteristics.
0 r- M8 S, ^$ x$ F8 RThe electronic materials field today is highly focused
7 q, f; l1 U8 G' Y3 mon the development of new materials with special properties
8 V5 h! M6 H. w$ I* l; Sto meet specific needs. Advances in condensedmatter
* ^" u$ L( K% ?2 ~+ D# dphysics offer the possibility of new materials; o6 z4 V) W+ ^4 F
properties. In photonics, new materials are providing increased, S% m( o" Q# S; _3 H
spectral range for light-emitting diodes, smaller; O7 `+ z. O4 y& Z, U1 I
and more functional semiconducting lasers, new and improved
3 y" F" G6 C# C6 b) g: g) j. ?' Idisplay materials. The new field of photonic$ @0 P0 \& P- W
band-gap crystals, based on structures with periodic
" O1 o: ^# _5 p: p) M1 u" @) dvariations in the dielectric constant, is just now emerging.
% m- O5 d) ~- HResearch on optoelectronic materials has been
& S. O! T) N! K$ r7 k1 Y8 dgreatly stimulated by the optical communications industry,
3 W; M, e; B- J: [6 S& Q$ Awhich was launched by the development of low-loss
+ R! g6 J/ Q f3 q I# Joptical fibers, amplifiers, and lasers.
1 P! e% z. W; T1 O* r+ |; FFerroelectrics have become important for use as capacitors Y! s$ I0 ^4 ^8 K) D' e2 W
and actuators, which are needed in modern robotics4 ^0 P0 x- H' @: }; c! l" X
applications, as are also piezoelectric materials,1 T; \* q- ]( \3 x' F
which are critical to the operation of scanning tunneling
' N, S& W) v$ K; Iprobes that provide information at the atomic level on
7 P* m; X b; g; i: `structure, stoichiometry, and electronic structure. The5 E2 H* a8 f- F8 g$ R5 ^2 ~
technological development of microelectromechanical
5 F8 o w9 P' I5 Y$ ~systems (MEMS), based on silicon and other materials,, d. q i1 l. I; w: f9 `* ]
is making possible the use of miniature motors and actuators( ], V/ W( R/ W% g* O( Y" f: J
at the micrometer level of integrated circuits.
* S# @$ i& T$ Q. u& q& fSome of these have already found applications, such as4 V- @9 R4 p8 E' u, v, C; z( ]
the triggering mechanism for the release of airbags in
; n1 M6 S: v; B( ^1 D# {* ]automobiles. Such developments are not only important
: [7 E1 N1 u) X1 {to the electronics industry, but are also having great impact
+ G8 u2 ?+ A6 uon fields such as astronomy and space science,. |1 o/ ^3 o' u: ]
which are dependent on small, light-weight instruments1 T( I% A6 B7 C' k8 P5 N
with enhanced capabilities to gather signals at ever increasing
0 Q: D6 q- Z6 f# Q" s" }, a& Ndata rates and from ever increasing distances
3 ~+ x9 d4 N& K7 w" @. K9 nfrom Earth. The developments in new materials and Z# {9 b1 X/ B8 M( g# u
low-dimensional fabrication techniques have recently rejuvenated
" p ]1 d% P7 f3 h# k$ M9 qthe field of thermoelectricity, where there is( H& B) p, p' f2 j; }
now renewed hope for enhanced thermoelectric performance5 F. R9 T1 d, @' K5 B
over a wider temperature range.
9 W0 e' v: d- R" r' m5 M' w% o0 d7 r/ rResearch on magnetic materials has been strongly influenced
4 n* c" ?6 A/ }3 J* _7 Lby applications ranging from the development4 z* X/ y) }6 |
of soft magnetic materials (by the utilization of rapid
# v4 s" i4 f5 C4 b2 d+ F8 d* n, _solidification techniques) to hard magnetic materials
+ B1 g/ e5 `6 j3 r; tsuch as neodymium-iron-boron for use in permanent
' D9 A8 ]8 V3 k! wmagnets. In the 1980s efforts focused on the development# D6 s, v ]8 f, Q+ a: i
of small magnetic particles for magnetic memory/ d$ Z& @/ ~8 v7 x' D0 m G- |
storage applications. New magnetic materials, especially
$ C% W$ N6 I# V* g }3 t; smagnetic nanostructures, are now an extremely active
. k0 p- h% y1 H1 G5 |research field, where the discovery of new phenomena
. f5 _5 J$ M2 b2 X2 Ksuch as giant magnetoresistance and colossal magnetoresistance
! @0 o4 g0 E( ~! Y& Y( Care now being developed for computer memory: U- [5 z3 O9 q9 s9 j. b4 {
applications.
7 d! A% Z0 d) A* ~The strong interplay between fundamental materials. L" r; \+ i$ `; A
physics and applications is also evident in the area of
+ u8 w" E. B4 Y$ G$ s; P+ \superconducting materials. Early use of superconducting& D% t# S. ?$ t6 p+ N
materials was in the fabrication of superconducting magnets,
; {: d% ~/ I; s1 X; M/ o6 ]which in turn promoted understanding of type-II
8 J$ G2 T6 }# ]0 F0 Ysuperconductors, flux dynamics, and flux pinning phenomena.
3 c$ E9 P4 m1 pThe discovery of the Josephson tunneling effect
% ]; ], }0 M5 i* k* H# Fled to the development of the SQUID (superconducting# ~9 L# ^9 |3 Q
quantum interference device), which has F5 l2 K# c, j2 t) s* N( s
become a standard laboratory tool for materials characterization
* p5 ]; {- d( ]9 v* c0 s9 eand for the sensitive measurement of extremely
- D% V3 }* W3 Osmall magnetic fields, such as the fields associated0 w" T. j) d. o K0 l, }" `( A. x, b
with brain stimuli. The discovery of high-Tc4 p n. v' i! O
superconductivity in 1986 has revolutionized this field,+ j0 w5 R& z4 M3 k% Q9 R
with much effort being devoted to studies of the mechanism
6 C& o' i! Y3 X* E1 |$ ]6 ?for high-Tc superconductivity, along with efforts to
* s. ]2 h( r G( w. I, Ndiscover materials with yet higher Tc and critical current
/ D. ]- C0 ~, P i8 R K5 T" cvalues, to improve synthesis methods for the cuprate superconductors,
( h1 n# L8 T/ H2 E8 b. xand to develop applications for these
* K7 Z* D3 ?5 M% `, w! m7 D2 m! J omaterials to electronics, energy storage, and highmagnetic-
6 x" C& q6 |0 n" s- ~! O8 W6 v1 R& ufield generation.
3 X6 J X% C$ o& E$ U& aWhen viewed from the perspective of time, the developments
0 E: W+ E. a( Win electronic materials have been truly remarkable./ q- y; d; Y g) C* m7 B
They have generated businesses that approach a: l8 R( x& p$ Y z, J8 n7 L5 T; L& r
trillion dollars, have provided employment to millions of
m) e$ a& g; \: @, J" j5 Iworkers, either directly and indirectly associated with
# Q! J9 E. o3 K( xthese industries, and have enabled us, as humans, to extend
5 x+ _4 d1 ]4 e5 v$ N$ eour abilities, for example, in information gathering,
$ F5 S/ B" D7 k8 Z" b6 v Bcommunication, and computational capabilities. Science
6 `" k6 }3 X+ Y! Q1 n4 o# x. p; Fhas been the key to these marvellous developments, and
' `& q2 c8 S1 C1 k% y9 i2 @4 Kin turn these developments have enabled us, as scientists,9 i2 T/ E* d$ ]- b2 |
to explore and understand the subtleties of nature. }7 ~! x. a+ Q
V. SUMMARY
% h. R" I3 E7 p( RIn this very brief note, we have only touched on some
0 |* e9 e' R8 v! Y; vof the advances made in structural, polymeric, and electronic
V# [1 m& _7 f' ~- Xmaterials over the last century, showing how materials3 O$ B2 [$ Y; B) Z) K
physics has played a central role in connecting
( j* b# J- R% |% m. Rscience to technology and, in the process, revolutionized
) x% ]+ d3 W! d" ~. Kour lives.
9 ?$ _9 `' X& L# Y0 _$ L$ oP. Chaudhari and M. S. Dresselhaus: Materials physics S335
J9 u- Q! x8 m2 Y) oRev. Mod. Phys., Vol. 71, No. 2, Centenary 1999 |
|