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Materials physics
# i' H% Z( U' b" N& A! |, DP. Chaudhari
) d$ M: L. i. } R$ lIBM Watson Research Center, P.O. Box 218, Yorktown Heights, New York 10598
0 m" \ E' \( c3 k% _M. S. Dresselhaus u$ V; ~! X6 C" P- t% ^+ e3 F
Massachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307- I9 z B Q; T' z7 w! F" N
Extraordinary advances in materials physics have occurred over the last century. These advances have
4 \3 n$ l# u7 u/ f) jinfluenced almost every aspect of human endeavor. In this note, the authors sketch some of these* T4 ~9 }- u- n H* q- J
exciting developments in structural, polymeric, and electronic materials. [S0034-6861(99)01502-0]
' `# g' X! Y+ s D7 ]! R2 MI. INTRODUCTION
1 G' ~4 @" F' z# |" mOver the last one hundred years there have been stunning
9 d b6 m3 u9 q2 K0 u6 B0 dadvances in materials research. At the turn of the O, U5 m! B4 W6 S% ]
last century we did not know what the atomic structure
V1 n1 z2 l0 p* x& v* z0 \- Eof a material was. Today, not only do we know the structure,
5 j4 G1 [% x i- a5 ?% [but we routinely make artificial structures that require% a. p; ?* a, @/ ]% r N& D% p: H8 r
placement of atoms at specified locations, that mix
+ r x6 }7 v4 A! w0 `# x2 P' Z8 Eatoms to create properties not found in naturally occurring
6 T* T2 S4 ?6 ^* }4 vmaterials, that have the functionality needed by today’s
6 _0 o: w- ]( ~0 X, J" g. }technology, and that adjust their properties to a1 l8 p# B+ G# w2 p+ E, G
changing environment (smart materials). Over the last
' r3 v# n& Z$ M5 xfew years we have begun to manipulate individual atoms2 t) g) W% J( B8 i4 f
to form structures that enable us to explore scientific; N+ y* u- }' U9 x" ~7 h6 |
issues, but that will surely lead to profound technological
# c9 f8 |: G3 Q* r3 a7 Nand social consequences; for example, the manipulation) I5 K6 }! U% y. [# ~! [
of nucleotides in a DNA molecule, which is then) `2 V$ g0 O M: A# z
correlated with the functioning of, say, a gene and with
. {$ W6 k+ B4 [# iits expression in the control of disease.. j' i4 D* w# D+ |9 \
A hundred years ago there were no electronic devices,' e; V. C) R4 d9 k
and today there is hardly any electrical appliance without
& l/ ~; P+ J! b5 q- zthem. It is anticipated that in the near future there- n4 ?+ Z1 c3 V: X, m5 Z
will be a microprocessor embedded in almost all electrical* n: S9 {; k D5 n
appliances and not just in those used for computation
/ K w9 R4 Z) ~' {& uor information storage. These devices, inconceivable a
8 M2 n& H$ _/ H+ o8 bcentury ago, could without exception not be made without% c3 ]; ^' M) K) ?' \: n
the knowledge gained from materials research on( J3 H9 v4 L1 d. g+ C3 W S6 y2 X
insulators, semiconductors, metals, ceramics, and polymers.
, @: u5 q* I. s' oAt the end of this century, we have begun a debate
: ~; U, Y. V! L( e% pon how far the present devices can continue to develop,
4 U8 A( \8 S8 I& rgiven the limits imposed by the speed of light and
; n; e3 s; h/ Y7 ~' @4 S$ n }the discrete nature of atoms, a debate that would have1 P( V9 I: N' f- s
been incomprehensible to scientists and technologists of
4 w7 ^$ y! C7 T; Qa century ago and a debate in which we now discuss the, r+ {% M" |4 X4 p% u! q! V
possibilities of using single electrons to switch a device1 p0 B/ M( k, v( A! g6 Z r+ R' ?
on or off.
+ H, o" @4 d* R- Q; m* S8 EOur ability to measure temporal phenomena was limited* v8 d# O3 L7 C4 ~% r' a
to fractions-of-a-second resolution a hundred years E: D+ i5 X; {8 g- ]
ago. Today we can measure changes in properties with a
6 n( _; Q0 k9 T( Zfew femtoseconds’ resolution. Strobelike probes enable
: J& l2 x' A9 k$ \( Jus to measure phenomena ranging over time scales covering
/ j4 M4 Z; s5 T& Kmore than ten orders of magnitude. We can, for
# U& Z L7 |& c9 `example, study the relaxation of electrons in a semiconductor
. B1 z0 H/ @+ D3 M) h2 \' Won a femtosecond time scale, the visible motion
8 v7 M$ O9 y! y# T0 a$ P# lof bacteria in a petri dish, or the slow motion of a sand- X i9 t% E1 G) Z7 w! e
dollar on a beach.3 f* y2 f* R: ~) g* X+ E
Materials research spans the range from basic science,3 R5 Z" l X' \5 h, D1 C
through engineering, to the factory floor. This has not, `1 ^; ^* c1 n5 j5 ~" E
changed over the last hundred years or, for that matter,
" f- I( S# @; ?. \4 }# Tthroughout the history of human civilization. Materials4 C1 E9 I6 g. f
research came out of the practical needs of mankind.
U, J! Q% y) Y5 B m o8 mEras of civilization were named after materials, so central5 D, A; b# Q7 w3 k/ L
has been their role in achieving mankind’s mastery
- I8 c z7 ?7 W( s6 w0 Oover nature. The field of materials research can trace its/ h% [ U- ~; \, i* L& X3 s
roots to alchemy, metallurgy, natural philosophy, and
% W( ?# K2 q& Z" Q9 z' p, D! Veven art, as practiced over many centuries. However, the
2 i5 I' W+ ~% z! s% X2 N8 vfield of modern materials research, as represented by: E- i( L. O$ `1 ^" y
materials physics, is only about sixty years old.
- D: ^7 c* ^7 W# Y; M# fShifts in materials usage from one type to another are
- b. T+ Q: r4 t! s- q7 E) K, ousually gradual. This is due to the very large investments1 l+ o. A1 l! H) M+ ~' B
associated with products in the materials-related industries,7 |# t) m7 T6 ?+ L/ u# t
complex relationships between reliability and functionality,5 o; O. o t: `6 j W7 c4 J
environmental issues, and energy demands.8 j, D$ q- _1 X) Q2 L3 \2 @' W6 w
However, measured over time, these shifts become quite
3 }- {0 _1 z9 rperceptible. For example, in automobiles the ratio of9 W9 ^+ P5 G; F+ f
plastic components to iron-based alloys has changed
6 J$ A9 s U$ _2 U( pfrom less than 3% to more than 15% over the last two
: ? r7 s6 W) g8 R$ ^- Cdecades. Although the percentage change appears to be
' d1 W+ ^! ]% s( H" N; fmodest, the actual volume of material is large; over 40
2 V( j" O0 j) n* v1 F9 cmillion tons of structural materials are used annually in) F- G# v+ P9 Z- T; f- Z
cars.
1 [3 L! \( w/ g# o/ yThe advances of materials research in this century,4 a+ p) {) a( |; h! ~3 w5 O- r
which far exceed those of all prior centuries put together,9 S- ?' {8 _, R" Q8 D
can be illustrated by three examples: structural,4 m4 @% G8 G/ _7 P% `- P
polymeric, and electronic materials. Our choice of these
# b: p- ^3 c8 Q2 y0 b3 v. _* Xthree is somewhat, but not completely, arbitrary. It is
& a( G& X p! R0 D7 S( }( `9 j Mout of structural materials, particularly from the fields of9 O2 j: I* i+ v# @2 y8 h
metallurgy and metal physics, that modern materials- Q3 x: E" ^2 m
physics has evolved. From the crude weaponry of our$ c0 @2 f2 z, M" ?; A7 h* u
forefathers to our mastery of air travel, space flight, surface* Q; v. G8 n1 C0 K& _4 m
transportation, and housing, structural materials
. z* x, O e* d" Z- Iplay a role that is unequivocally important. Nature uses' z! G- T+ w) T2 v* X3 o
the second category of materials, polymers, in amazing3 ?! }) e. U: Z4 E0 m+ l5 E
ways, to perform very complex functions. We humans
; ]8 q( U( d- D6 O& |are an example of that. Over the last hundred years, we# I( j2 T3 t2 T0 P
have begun to understand and develop polymers for
3 U# r7 h( B6 Buses in food packaging, fabrics, and structural applications.) T: ]0 A& E# ^
We anticipate that polymer research will play an
- B u" f/ g& z zincreasingly important role in biomaterials of the future.$ A, S: ^1 M% A+ e6 k$ @
The third category, electronic materials, were not conceived
( f1 ^, d+ X2 w; b& K( s, y. Runtil quantum mechanics was discovered in this0 _# T$ [4 F9 w$ c9 R
century. Today we cannot imagine a world without telecommunication,: N0 g6 m+ U4 h/ W* L8 N3 r
computers, radio, and television. These
5 j4 n" _- l; r& _; {# \6 u- Pand future devices that will make information available
$ l0 v8 H \! X( R' K4 e, |9 }6 yReviews of Modern Physics, Vol. 71, No. 2, Centenary 1999 0034-6861/99/71(2)/331(5)/$16.00 ©1999 The American Physical Society S331
2 L' n! p1 r. Q7 ~, e$ Winstantly are only possible because of advances in the
" A+ Y2 P/ X2 L1 ~5 l9 Y) d. |: r8 ncontrol of materials structure and processing to achieve
% g4 E6 Q' e4 G9 m3 K3 ka desired functionality.# G3 U( V# s3 i+ F, o4 u
II. STRUCTURAL MATERIALS" }' I7 `# }& }5 K( @5 K
At the turn of the last century, mankind’s use of structural
- i; H1 |9 W. X0 `! L$ {2 F! umaterials was limited primarily to metals, particularly
P$ H* I) ^5 R. hiron and its alloys, ceramics (most notably Portland
: F4 z7 b, \& ^# Ecement), and polymers, which were limited to naturally" T2 E @2 t; O2 ]9 @8 |
occurring rubbers, glues, and fibers. Composites, as a
, x1 N! ?6 }9 M6 k; fconcept were nonexistent even though wood and animals,
/ D w5 U' v: l; oeach composed of different materials, were used in& o. H6 w+ p) D' ?- Y; f
a variety of ways. However, the uses of alloying to enhance7 V" V3 ]. t/ r9 `8 J, {
the strength of lightweight materials, such as pewter,9 h2 M' c& ]9 M
or copper additions to aluminum, were established. W- }0 U- w$ D9 Y
techniques, known well before this century. This knowledge
' m5 R# i7 H8 l* dwas used to build the first dirigibles. The useful7 Y$ k; t5 W+ V0 a5 b* q
nature of a material was often understood through serendipity/ m+ @1 s* S; k1 J( ]. t0 U
and not through an understanding of its structure6 b; f. v" Q5 i0 T& y2 S2 ]
or the relation between structure and properties.
3 ?+ {5 a6 @$ j% Q7 d. d! iWe still cannot predict in any quantitative way the evolution, L+ d" W( Q4 K* S3 o1 W1 h r
of structure with deformation or processing of a
: O" t3 \. _$ p) l& {& Zmaterial. However, we have come a very long way from
1 d6 _4 ^& s3 u/ Bthe situation that existed a hundred years ago, thanks to
7 ^# {: I8 h, b! }' Jthe contributions of twentieth century science to our understanding
* A) U* b9 s. kof atomic arrangement and its determination
( h4 [1 x% L% V9 V, Q& I$ Ein a material. Our classification of materials by symmetry8 _6 R, ~9 i0 {. d M' o
considerations came into existence once atomic: }) ~: M& ]) g
arrangement became known. To the seven crystal systems' w$ _: k Z6 ]# C7 P: C1 N1 @- ~ M
and amorphous structures, typified by the glasses
2 v2 Q" c4 x( ~6 V# p8 @/ g6 @and liquids, we can now add quasicrystals and molecular" r2 n1 r. K& x& c3 x. k) }
phases, such as fullerenes and nanotubes, in a crystalline
! t6 w5 g& i% I- l$ O; H3 wsolid.
* Y7 ~) f L. E8 s4 Q" rThe crystal systems define perfect crystals. At finite* V6 `% b. @1 S* a! i4 {8 N: ?
temperatures, the crystals are no longer perfect but contain8 p9 E: R0 L" R5 }/ W8 i
defects. It is now understood that these defects are# S& d: \ V$ \( I4 j+ L, q
responsible for atomic transport in solids. In fact, the
3 g! o& W6 Q2 j2 H; p pstructural properties of materials are not only a function, W0 q* Q1 G9 O4 g* Y
of the inherent strength of a material but also of the1 A, N) {' a" ?+ ^( i6 X
defects that may be present. We know that aluminum is$ {6 M" L5 D( P0 | {1 S! e
soft because crystallographic defects, called dislocations,$ \# M$ [8 o" z/ Q' O3 `/ {
can be readily generated and moved in this metal. In3 S, E; K2 q" B2 l
contrast, in alumina (Al2O3), dislocation generation and
/ i" y4 V G. S9 @) ~4 C ymotion are difficult; hence alumina can be strong but
0 y5 u$ z0 r, s+ ?6 vbrittle at room temperature. The addition of copper or
# }/ }. @+ P2 b# Y5 ~0 Qmanganese to aluminum creates second-phase precipitates,
6 f: m# n E- V9 @which inhibit the motion of dislocations, thus enhancing) j0 J. u8 i+ \# S$ [- j
its strength-to-weight ratio. Our ability to improve/ A- K. i/ z2 e$ c
the strength-to-weight ratio in materials has- E- @9 T( w3 | F. K4 m8 I! K- d
increased more than tenfold during the twentieth century.
; `* c' ]2 e1 O( O2 jThis is to be compared with a change of less than
; o1 I6 U% Q- Q( H" Zten over the last twenty centuries. Much of the increase6 k/ a, i! D) m+ ?2 ?5 t2 K
in this century has come from an understanding of the) e& a0 ] V |. C% g* s3 \
relationship between the processing of materials and3 f) L A8 R6 ^# H7 d
their structure. The highest strength-to-weight ratios
( q9 V/ l R8 s! K$ khave been achieved in materials in the form of fibers and
! ~& a, W+ w9 h" q0 p( U7 Nnanotubes. In these structures, dislocations either do not
2 a7 t9 k0 }* K: T9 `exist or do not move.; d U- M! }- M! W& B, S
Most structural materials are not single crystals. In- _$ W! r f1 J4 f3 d% A8 E
fact, they consist of a large number of crystals joined at
j5 U9 F, u& F- `; J6 L6 H8 Qinterfaces, which in single-phase materials are called
) \" @3 @' w* V: o0 @. a7 |$ ]3 sgrain boundaries. These interfaces can, for example, influence
( O. Q& ?- o& g3 ~: U7 dthe mechanical and electrical properties of materials.6 ^: }6 x' z5 `, C+ K$ X: L/ m
At temperatures where the grain boundary diffusion [) Q1 G; a' \! m( F Q
rate is low, a small grain size enhances the strength
5 O' i- o% q) ^1 @7 e! c+ B$ Pof a material. However, when the grain boundary diffusion
/ V' v' R* w! N4 c4 O, b4 x trate is high, the material can exhibit very large elongation7 i/ B$ b a1 ?
under a tensile load (superplastic behavior), or
b' G; Y6 R% Wcan exhibit high creep rates under moderate or small$ [* A5 L3 d! ?% ]
conditions of loading. In demanding high-temperature
' T0 p* b+ F: t: R4 `. e) a9 J% Aenvironments, such as the engine of a modern aircraft,
: R0 z" i* @4 @/ X( Agrain boundaries are eliminated so that a complex part,
5 e) f! c) m; n; d. S/ dsuch as a turbine blade, made of a nickel alloy, is a single0 }/ Q# l, I' f" j0 t# p
crystal. Thus the use of materials for structural purposes
: L3 A" c O! P5 j. P( Q9 _requires an understanding of the behavior of defects in5 p) t7 a; B3 F
solids. This is true for metallic, ceramic, and glassy materials.2 G; G. B& q( g$ }8 S$ N2 R
Both ceramics and glasses were known to ancient civilizations.7 S- S$ y% d5 n$ Z/ |1 T A6 K# r
Ceramics were used extensively in pottery and
9 [! W# Z5 Q# c9 oart. The widespread use of ceramics for structural purposes5 c) c0 [- f; \$ K5 |/ S
is largely limited by their brittle behavior. This is
: n) [. v# [ {2 T" F/ cnow well understood, and schemes have been proposed# b2 |! }4 h: t- y6 Y1 N, X; X: A5 L% a' A
to overcome brittleness by controlling the propagation
( {- x6 Q1 d' L" M P* i* {2 Lof cracks. In metals, dislocations provide the microscopic
" m3 Y4 g4 Y& q! H; pmechanism that carries energy away from the tip* m. q7 O4 [$ T; | L4 ~* T/ n
of a crack, thereby blunting it. In ceramics, the use of
; i& G0 O1 l& Qphase transformations induced at the tip of a propagating
6 i l& i; z* ]7 acrack is one analog of dislocations in metals. Other
* A$ }& q9 \# ~, F Q2 hschemes involve the use of bridging elements across
; z9 d, v: d4 S4 |cracks so as to inhibit their opening and hence their
, Z: r2 L3 x: U" ^4 Q# @7 Xpropagation. Still another scheme is to use the frictional$ l- @/ v9 u7 d7 `
dissipation of a sliding fiber embedded in a matrix not4 x8 ]0 n6 K- J
only to dissipate the energy of crack propagation, but
7 Z5 U6 x+ H2 nalso, if the crack propagates through the material, to
1 e8 a. C, H/ q$ N' Oprovide structural integrity. Use of these so-called faulttolerant# a* ?* D6 F F) e& \0 p0 f
materials requires both an understanding of mechanical
" l8 R4 t7 N6 K2 W# ~; x+ Xproperties and control over the properties of: @: U: Z) ]4 F% q1 P/ a |3 b
interfaces to enable some sliding between the fiber and" q% b, e5 C0 G# u# E0 b
the matrix without loss of adhesion between them. Such
( N$ U. v5 ^6 lschemes rely either on composite materials or on microstructures/ g( d6 U: R( {( w$ B1 u% @3 p
that are very well controlled.* n u8 f, H Z( e
The widespread use of silicate glasses, ranging from
/ h$ L/ C4 K1 ~' r7 @7 r% X; Vwindows to laptop displays, is only possible through the+ G) L9 I4 t j3 f! v* h5 p2 o+ Y0 l
elimination of flaws, which are introduced, for example,
6 `6 c! w" x5 I% t1 U- V7 Eby inhomogeneous cooling. These flaws, which are
8 y2 \4 L8 S' t$ S; U0 e2 p- qminute cracks, are eliminated during processing by controlling
% ]" @/ H4 k% Kthe cooling conditions, as in a tempered glass,3 C* ~3 i/ X. M1 u# {
and also by introducing compressive strains through
2 U3 M6 \6 e' m5 qcomposition modulations.
; Y/ C5 K# r! \There are a number of fibers that are available for use
/ f2 C. E9 m. W! R2 Z7 zwith ceramics, polymers, and metals to form composite0 T5 Q, B4 |9 a6 m$ v9 I$ `7 n
materials with specific applications; these include carbon; t6 b: X6 y( [4 u, F" a0 }4 r
fibers, well known for their use in golf clubs and fishing
9 [0 p# n1 k) Qrods, and silicon carbide or nitride fibers. Optical fibers,- L" \4 S9 k6 J7 I8 V+ {
which are replacing copper wires in communication
9 K0 S1 m5 A. _( Y6 V" @technologies, owe their widespread use not only to their4 K5 o; P) I% Q+ ] c) o
optical transparency, but also to improvements in their( s3 [" ^7 C2 P! ]) C/ i |3 W7 }
S332 P. Chaudhari and M. S. Dresselhaus: Materials physics% v4 z6 O6 |( ^8 @
Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999- Z0 h2 D% \) Z
structural properties. Fibers must withstand mechanical
8 q. D0 ?; v/ A" K' _0 K- xstrains introduced during their installation and operation.
5 e- Z. {3 _( b* a: g1 BThe use of composite materials in today’s civilization
' H/ ]- f( D% n% g. cis quite widespread, and we expect it to continue as new
) Y: m3 G) ^1 W2 B% q( S& P; F# papplications and ‘‘smart’’ materials are developed. An
# v+ \2 U& m6 c1 R2 |outstanding example of a functional composite product& B" k' E& G! B r/ |! p
comes from the electronics industry. This is a substrate,; [+ `% d+ d$ {) i
called a package, which carries electronic devices. Substrates
) V/ H: ~: V) {; k( [- bare complicated three-dimensionally designed% n+ r) Y- L6 A9 L
structures, consisting of ceramics, polymers, metals,
6 @6 H u. {8 |7 [0 N. Q: v! esemiconductors, and insulators. These packages must0 h# e: A8 ?2 R* O* A7 d& y
satisfy not only structural needs but also electrical requirements.% f1 ~+ ^+ A9 H& j, C K
Although we have made great progress over the last8 x4 U4 K; x% n/ _. b. D
hundred years in materials physics, our microscopic understanding
/ L3 `: e! h& l, m, g# N) Z. Zof the physics of deformation (particularly
4 }) s. G0 W) Q1 p9 c2 f5 xin noncrystalline solids), fracture, wear, and the role of1 r5 r5 P! j, D7 h- X
internal interfaces is still far from complete. There has
' [8 _; U- M& C* g2 _3 [been considerable progress in computer simulation of
' x" m5 a+ d. n9 a8 y8 H# Msome of these issues. For example, there is now a concerted j& E T, c# z/ |5 U+ f0 |
effort to model the motion of dislocations, during/ p- a" g" g3 z( C
deformation, in simulations of simple metallic systems.
- l* R/ u: o t/ _; P0 J8 aWe anticipate that within the next decade, as computational
! U1 I$ ?" G5 ^ |1 \% A c6 Npower continues to increase, many of these problems. d9 P- [0 [1 Q2 ]. \
will become tractable. The ultimate goal is to design
) x; P/ |: m) q2 T( za structural component for a set of specified
) Q! B& v) S. M( |0 B0 Q9 ienvironmental conditions and for a predictable lifetime.
0 R, q( g+ F* O# V p0 NIII. POLYMERS5 [1 p& Y U: C, V
Polymers, also known as macromolecules, are longchain0 G1 @& _8 t! f2 U
molecules in which a molecular unit repeats itself
( n; p$ |7 w7 P$ B) O D. ralong the length of the chain. The word polymer was$ c/ _& X1 b0 ], y9 X
coined approximately 165 years ago (from the Greek) \) e J* c: c2 I% d6 x- I
polys, meaning many, and meros, parts). However, the
9 R/ i g4 b3 rverification of the structure of polymers, by diffraction
" E3 k& U( \9 R* w; \( Kand other methods, had to wait, approximately, another
4 C; v# s; p, [$ o+ J100 years. We now know that the DNA molecule, proteins,
8 A; _9 f c1 ]) q5 ucellulose, silk, wool, and rubber are some of the4 G4 K; s* @) {* s) u2 s8 K
naturally occurring polymers. Synthetic polymers, derived
" J% F" A* s1 s& D' W. `mainly from petroleum and natural gas, became a: d! s y: `4 T# ]0 A: N A
commodity starting approximately 50 years ago. Polymers# X- J, @4 Z8 [, B$ _8 N' E
became widely known to the public when nylon) Q0 k3 W2 B# n6 \6 e
was introduced as a substitute for silk and, later, when
/ S7 M; d I O$ n6 l& f- xTeflon-coated pans became commercially available.
5 P: p' v. X4 Z) `+ aPolymers are now widely used in numerous household. J H) d4 S, [' `% q
applications. Their industrial use is even more widespread.( B! B; m: y! T5 j8 z- Z
Most of the applications associated with polymers
+ K# t3 ?+ Q r6 e! }have been as structural materials. Since the 1970s it was
! E( a, i- ^; L9 E3 Y v) q7 @& R1 jrealized that with suitable doping of the polymers, a; T3 [3 A: i- Y6 L+ ]
wide variety of physical properties could be achieved,8 P& ?& y4 Y: W
resulting in products ranging from photosensitive materials5 p3 O5 Q0 U, k
to superconductors. The field of materials physics: C N2 X" r% K# d' O& ]
of polymers has grown rapidly from this period onwards.0 U7 S( i3 K$ ^" F9 _$ O* B( M
Polymers are a remarkably flexible class of materials,( B [- ~# T7 ~
whose chemical and physical properties can be modified
. T& Q5 O0 a' s) K2 d( ~" @/ M: Mby molecular design. By substitution of atoms, by adding4 Q8 M" N1 Z1 M1 [" i
side groups, or by combining (blending) different polymers,
4 |. e! r3 P5 O+ L; k! ^* jchemists have created a myriad of materials with: j, l3 B) W. z. z& n
remarkable, wide ranging, and useful properties. This0 j4 L+ t2 }5 K* n- A
research is largely driven by the potential applications of
/ ?* `+ r2 c+ H7 Bthese materials in many diverse areas, ranging from cosmetics
% k: _3 E' E* x+ R* Bto electronics. Compared to most other materials,: H' n: V8 P5 l! h
polymers offer vast degrees of freedom through blending
5 Z7 t+ v! A$ |1 e; yand are generally inexpensive to fabricate in large% B3 a9 ?: R7 f( Z. p- q. [9 Y
volumes. They are light weight and can have very good
% G0 i) I6 I& q/ C5 v& xstrength-to-weight ratios.
+ T% ]6 P8 h8 `8 nPolymers have traditionally been divided into five+ z+ n! C; {" l7 o* s9 ^* k
classes:
, F; n Q. b8 v& S. u6 [(1) Plastics are materials that are molded and shaped
4 [: [7 H- k8 f7 [# pby heat and pressure to produce low-density, transparent,
. _; M: n9 X1 r3 [, cand often tough products, for uses ranging from; c; \2 B" q- V2 w) h: F$ r
beverage bottles to shatterproof windows.
+ f( G' y3 f8 E(2) Elastomers are chemically cross-linked or entangled- t. Z1 k# e/ |: L: @- q
polymers in which the chains form irregular coils
: [" l0 A! e6 Q j. X6 u- Rthat straighten out during strain (above their glass transition+ ?6 Z3 H4 }4 p! w- e
temperatures), thus providing large elongations,
8 z8 I4 |& e0 _1 s! i; Jas in natural and synthetic rubbers.4 R0 K3 F/ Y1 K" f) n
(3) Fibers, which are spun and woven, are used primarily2 }" _/ q( `8 e% e1 E) @5 Y1 F
in fabrics. About fifty million tons of fibers are produced* q% h! M+ U/ j4 U$ y [
annually for uses ranging from clothing to drapes.
4 e4 B8 {/ M/ V& ]! C/ @Apart from naturally occurring fibers such as silk and# c: p, x3 [- j: j0 |
wool, there are regenerated fibers made from cellulose
' z+ v! d8 j/ C; Qpolymers that make up wood (rayon) and synthetic fibers,
) ]' \/ }! q1 R* a' n; v, M/ jcomprising molecules not found in nature (nylon).
6 o/ X2 {2 K) Q: k9 f9 N* e(4) Organic adhesives have been known since antiquity.
3 `$ g% {& q% dHowever, with demanding environments and performance
- u: v- j# ^% ]& w2 L; ?1 X% w3 @requirements, synthetic adhesives and glues
) {4 T- k- G( n( T0 h- _) `2 ?have largely replaced natural ones. The microscopic( s5 l C3 L x9 U; k4 Q- W+ k% u% S
mechanisms of adhesion and the toughness of joints are+ U* e. `/ w/ j- ?, o( @
still debated. There is an increasing trend to use UV% t( z8 S" \% d
radiation to promote polymerization in adhesives and,
$ ^7 z$ y6 s/ {3 M3 k) zmore generally, as a method of polymerization and cross* \& ~7 z0 w7 C$ m/ l$ X
linking in polymers.
' ?6 s* G O+ O9 l3 l(5) Finally, polymers, frequently with additives, are
8 x' o& ], X Y9 W- Dused as protective films, such as those found in paints or/ \. H" d1 L2 ~9 B* H( v. C
varnishes.
/ P# F) }: c% \; ] z7 C' SPhysicists have played a significant role in explaining
+ g. M- `8 H; b Z" a7 bthe physical properties of polymeric materials. However,
& ]& I( j; I, J U" Ethe interest of physicists in polymers accelerated when it
+ T- N3 B& @: f/ [8 f* v0 owas discovered that polyacetylene could be made conductive! Q, q8 Y+ v0 P, q
by doping. This development was noteworthy
, `' g6 B/ e: _for it opened the possibility of deliberately controlling
' z- d/ b, b& x: G; p% P: iconductivity in materials that are generally regarded as, D7 q G: Q, f" l2 s
good insulators. The structure of all conjugated polymers,) V& g" U7 u' S# v$ m) y, b5 P* o
as these materials are known, is characterized by a
4 g( [. J" B$ Z5 r* q4 O. Erelatively easily delocalized p bond, which, with suitable
1 v( Q# d' z z+ Qdoping, results in effective charge motion by solitons,
/ d6 U0 j3 e6 w; upolarons, or bipolarons. Since the discovery that polymers
S2 K+ y2 K/ y K( Pcould be electrical conductors, active research areas: m2 D9 w: @8 c4 N+ t" _5 Q
have developed on the physics of polymer superconductors,
& i2 Q) a6 g' _$ J# _ferro- and ferri-magnets, piezoelectrics,/ l" L, Y- K! T$ V) w9 B8 v. m( s
ferroelectrics, and pyroelectrics. Within the field of: z. |) i- a% [
doped polymers, devices have been built to demonstrate* M( k, z0 F, o7 r% o+ A
light-emitting diodes, photovoltaic cells, and transistors.% R% z( ?2 ^5 c( a( d1 _/ C
Conjugated polymers have also been investigated extensively
( m% f8 E- u9 h' i, Gfor their large nonlinear, third-order polarizability,
3 `; p0 {- @) f$ d% ?+ ~which is of interest to the field of nonlinear op-
, M; a4 F6 Y6 b+ m' w& j1 KP. Chaudhari and M. S. Dresselhaus: Materials physics S3334 K0 Y j' F; F, w
Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999* D7 E0 l& Z) U
tics. Large nonlinearities are associated with the strong- }# L) X; G( M+ c X
polarizability of the individual molecules that make up- Z# f. D* @% H; C# P
the building blocks of the polymer. Furthermore, the- M7 U2 |8 P3 p. {1 w0 A
flexibility of polymer chemistry has allowed the optical8 L N1 j# h) Q [- E2 Z% e
response of polymers to be tailored by controlling their
; J" `0 m* J, L jmolecular structure, through the selective addition of
/ x3 s( j5 Q1 M8 N; Ephotoactive molecules. Hence these materials have been+ ~1 I0 R. `5 |& Y% V2 [( E" M
widely investigated by physicists and engineers for optical+ l* Q# f8 [5 {- L _
applications, such as in holographic displays (dichromated
; f5 {+ a9 X7 I' r4 b/ Jgelatin), diffraction gratings, optocouplers, and% h; M9 M% e2 l; r) H
wave guides.
( n2 u l. [! F( s; ?) K3 SPolymers have long interested physicists for their conformational
% p1 R% m4 |; Eand topological properties. This interest has
: e# \! s) R% wshifted from the conformational behavior of individual* z) v) o, D' c8 o8 n, c
molecules to that of a macromolecular assembly, phase
" |5 v- J1 E3 k" Xbehavior, and a search for universal classes. Block copolymers,6 H( h/ k2 {! B
consisting of two or more polymers, can give) V* w( x8 O* A' p
rise to nanoscale phases, which may, for example, be/ R( }/ W: t( Z- Q
present as spheres, rods, or parallel lamallae. The distribution
9 J- N# m- E* o. a1 a1 D3 v0 i# Rof these phases and their topologies are of current2 l% E" z" v ]9 N' i" l+ }$ E
theoretical and practical interest. Block copolymer; r) k5 ^/ g V% m
morphologies are also being used as nanoscale templates
; [1 a+ @1 L- F7 q' F/ p9 d& Pfor production of ceramics of unique properties having
, V9 I4 ^* N, ythe same morphology.
% ~+ W7 _# Z# t9 D( q& x5 wBlock copolymers are also of interest as biomaterials.4 a$ X$ z" G' m, x0 F1 K
Proteins are an example of block copolymers, in which
& f* g$ ~. W. |the two phases form helical coils and sheets. Attempts to) T% p9 _$ i* @% e! B; w* E
mimic the hierarchical structure present in natural polymers$ O, C5 d' ^9 s4 l/ ]7 F+ J
have only been partly successful. The principal difficulty3 Z* h* v3 a5 g; _
has been to control the length of the polymer3 Q& o; q+ O- o" I: L p5 j$ w
chains to the precision that Nature demands. Significant
' }% x! m" @8 J. t* W$ Zprogress has been made in controlling polymer morphologies
1 }3 R) y I0 ? Y7 C* Hwith the use of new catalysts. For example,3 F! N9 ]8 t6 g& [) v
metallocenes have been used as catalysts to control
, d) H `0 q2 k4 rbranched polymers and organonickel initiators to suppress# e& B+ }( l0 @$ s; O' S
chain transfer and termination, so that polypeptides6 N3 w3 a( [, R6 N- U
with well-defined sequences and with potential for x7 S& K, Z: x2 y! ?. {
applications in tissue engineering could be made. The
% S5 W* w* h: X9 t' H. Cgrowth of well-controlled polymer chains is an example
/ S7 d2 @' M ~. M9 y6 a9 cof ‘‘living’’ polymerization.
+ O2 K+ r$ k5 ?6 e$ e/ i# R: d6 KThe static and dynamic arrangement of atoms on the
# {$ |2 t: I e9 j' lsurfaces and interfaces of polymers is another area of
: I" ?& ^! J) Q; ~active investigation. For example, thin films of polymers,. m: ^3 V. v/ d k
in which the chain lengths are long compared to the
4 Y9 {9 r' S# y; \) N2 Cthickness of a film, show unusual physical properties: the
5 J% @2 W0 g& i' b% ^ |glass transition temperature for a thin-film polymer decreases& R0 Q" D! r+ X# J) _( C
significantly, but between solid surfaces polymer* y) U6 }9 b# T% t. m
liquids solidify.
$ g3 j0 E6 z5 v: I. V8 H4 OEven though we have some way to go in making tailored
" s3 K, _. G7 ^proteinlike structures, polymer research has
2 y+ m J& f: v# splayed a significant role in the class of materials called5 ?5 L' r. c) W# A" m
biomaterials. Polymers have been used, for example, to1 J8 v& W/ G/ N" o3 i9 g
produce artificial skin, for dental fillings that are polymerized3 s0 O9 [, v0 r/ c
in situ by a portable UV lamp, and for highdensity# J0 J ]" D( @ Q/ R
polyethylene used in knee prostheses. Physicists
0 V; r; x8 u7 c* T0 ^5 B& gplay a significant role in these developments, not only" P' ~$ Z0 R8 m" E
for their interest in the materials, but also because of0 \/ n0 Y; [7 c+ j
their familiarity with physical processes that can be used
. R, q1 {2 y; r8 n( ^3 j) R: t$ dto tailor the properties of polymers. A particularly good
s$ z4 n* M1 L. n. K9 ]example of this interplay is the recent and rapidly growing% W T/ x( c! s1 y! W
use of excimer laser radiation to correct corneal abnormalities;
9 Q2 a1 u( q% c3 _: U% B* f% ~using a technology developed from studies
7 _0 d( W. O; Oof the ablation of polymeric materials for applications in
6 d( p, u2 ?9 T- O' o% ?+ Lthe electronics industry, physicists realized that the' t* V( z: K9 h$ b; M
small, yet precisely controlled, ablation of a polymeric
' g }' S4 E& _. Lsurface might be useful in shaping the surface of an eye.) h" f$ \! T3 t; Q: i, v0 y8 X2 Y
IV. ELECTRONIC MATERIALS1 V! M" v" w; R
The roots of the electronic materials field can be; }8 I" B4 Y1 v1 X: T G
traced back to Europe in the 1920s, with the advent of$ a4 t8 \- ?/ h2 K5 G: Y7 x
quantum mechanics and its application to periodic structures
) A) e, Y! m2 z- p) }/ Flike those occurring in crystals. The early experimental( Z$ t, o- a0 ^5 v d6 D
focus was on alkali halides, because these materials
( @0 u: o5 [/ |8 ecould be prepared in a controlled way from both a2 @# x' O2 |, Q! {3 L
structural and a compositional standpoint. The creation$ d+ Q/ d- z8 z7 p7 d
of a strong academic program in solid-state physics at
- Q0 f6 j: D4 Nthe University of Illinois in the 1930s had an important: `! R7 M8 _* y; ?; N. Q
impact on the early history of the electronic materials
" f9 r" H6 _ n y& Y5 Hfield in the United States. This knowledgeable human0 i( R1 h6 b2 |$ `% k* k
resource played a significant role in mobilizing the national- v6 |7 \* V7 r2 ]/ K& ?
materials program during World War II, especially
& R' ^: m1 G J% W; Lin the development of semiconducting materials
' p Q# ]: F+ ~+ B. gwith enhanced purity, suitable for use in diode detectors' M5 d- c, k' e Z! w
at microwave frequencies for communications applications.( E. c" p7 J/ V0 l
The availability of these new semiconducting materials
, a: N: k5 O# V) K7 rin purified, crystalline form soon led to the discovery! n6 i1 B% b4 q( g u6 s
of the transistor, which ushered in the modern
7 J: I8 T' [3 o5 Qera of electronics, computers, and communications,
. i* n- t2 x; x( W: pwhich is now simply called the ‘‘information age.’’
, z, U4 D) F8 v }, A+ r, ~# eSemiconductors have been a central focus for electronic' s: I8 M5 Z# S( u
materials. Quantum-mechanical treatments of a3 r" \6 p1 d# S5 U
periodic lattice were successful in laying the groundwork
8 S7 r4 w; n9 c! T1 jfor describing the electronic band structure, which could
) q# j! g3 ?* ]" [ ^& Xaccount for electrical conduction by electrons and holes,
( W7 k$ @; z! h+ Y7 M1 ycarrier transport under the action of forces and fields,
! n+ e3 B* g0 i- Rand the behavior of early electronic devices. Because of% h) k7 k' ~0 W+ I# l! x
the interest of industrial laboratories and the Defense
& ]; H0 ~5 h; |. x4 D) cDepartment in the newly emerging field of semiconductor
# a# ^+ U' c* |9 f! Helectronics, semiconductor physics developed rapidly,
8 Y8 A! g2 @# ]* W7 ^3 Rand this focus soon led to the development of the
# B5 T* W g8 U/ \& v |2 w8 ^integrated circuit and the semiconductor laser.
% p. j* i* i9 X/ v" E, e1 m) r- qThe strong interplay between technological advances, Z/ |9 L; M# o
and basic scientific discovery has greatly energized semiconductor) o5 q* G5 J0 W' J% u
physics, by raising challenging fundamental
/ J/ l/ n( @) q" a' `& Kquestions and by providing new, better materials and5 i3 Z* z' `0 B1 ]* |; P) i
devices, which in turn opened up new research areas.
: E3 ]3 t7 r4 I* y1 _- \) G( CFor example, the development of molecular-beam epitaxy; n* g- z2 |' _/ A4 T1 R4 ^
in the 1960s and 1970s led to the ability to control# u$ Q- t" O+ C- l6 a# s: ?# L
layer-by-layer growth of semiconductor quantum wells: r$ x3 ] Z- Y
and superlattices. The use of modulation doping of the
6 k! Q$ c6 C ]$ f5 D' zquantum wells, whereby the dopants are introduced
2 e" j, H. J5 Yonly in the barrier regions, led to the possibility of preparing$ q2 K8 H+ e. }* z. p }
semiconductors with low-temperature carrier mobilities,
3 y8 `8 P, f( p& K* Forders of magnitude greater than in the best, L0 K0 X# g& q$ o$ m! \
bulk semiconductors. These technological advances
) p& x9 D' N) Y/ c2 D8 isoon led to the discovery of the quantum Hall effect, the9 {3 y0 C, S4 |' {- f) E
fractional quantum Hall effect, and a host of new phenomena,
5 W' X ]/ G0 T4 Gsuch as Wigner crystallization, which continue) k$ y7 ]0 Q/ K( t1 b
to challenge experimentalists and theorists. Lithographic& M7 B! G: ~! Z8 O& b \+ c
S334 P. Chaudhari and M. S. Dresselhaus: Materials physics' E2 ~- K& b+ O7 [2 E
Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
: b: u: w; H4 @9 l: j& F" Aand patterning technologies developed for the semiconductor3 _* @3 a8 M) S
industry have led to the discovery of the quantized! P% }4 [+ t1 G$ l$ E) t0 b
conductance for one-dimensional semiconductors
" ~% w" P) n3 H1 w, {# F z- dand to the fabrication of specially designed semiconductor/ Z4 f, }+ _% X* C3 }# R
devices, in which the transport of a single electron8 W9 O; H4 C, l3 [* b& S
can be controlled and studied. The ever decreasing size
/ r `- H* W% s" P6 X4 d: e1 Dof electronic devices (now less than 0.2 microns in the
' [ x8 m5 [$ [) Q0 _" ?2 x& [semiconductor industry) is greatly stimulating the study# D' E6 M& C, z# q, [9 z
of mesoscopic physics, in which carriers can be transported
6 G2 I4 V$ Q# M0 x& e" fballistically without scattering and the effect of
0 f; \, x9 n1 t4 mthe electrical leads must be considered as part of the
( R4 D. W6 z$ }4 \. h" s4 M9 G, \electronic system. New materials, such as carbon nanotubes/ v& O+ L) P5 h3 E3 w
with diameters of 1 nm, have recently been discovered,+ Q! l% j2 W- b3 j1 x5 F2 m
and junctions between such nanotubes are being
" Y- |2 X3 I( s# `" D, wconsidered for possible future electronics applications# B. @* p$ u2 ?- |! d
on the nm scale, utilizing their unique one-dimensional- {% o* F$ B5 l% r
characteristics.
: T/ t4 j$ A6 k y+ Z! x8 F, G6 q( hThe electronic materials field today is highly focused A; ]" D# }+ D1 E, s. Q1 ?
on the development of new materials with special properties
' F6 }+ |9 X8 Ato meet specific needs. Advances in condensedmatter
3 e' J/ T& e. P9 Y9 pphysics offer the possibility of new materials
3 b ^) A, ` x+ p/ lproperties. In photonics, new materials are providing increased8 l, h* P' l' O% q9 M" q6 l9 t
spectral range for light-emitting diodes, smaller1 s: b2 E# ]6 y! Q
and more functional semiconducting lasers, new and improved
! u( w. A7 m, ndisplay materials. The new field of photonic/ ^' _( m8 y# D6 Y+ \
band-gap crystals, based on structures with periodic
. }. j. ~- Z+ E3 _0 x8 F2 _variations in the dielectric constant, is just now emerging.) n3 i6 a2 x6 H3 {
Research on optoelectronic materials has been0 z/ d1 Q) b9 F! c7 k: k3 ?# F
greatly stimulated by the optical communications industry,
! L) C$ f6 z# X$ x, _) \: zwhich was launched by the development of low-loss8 S$ g8 s- t/ e j3 z, B; f. _
optical fibers, amplifiers, and lasers.5 }& O8 ~; e# ~4 O
Ferroelectrics have become important for use as capacitors8 b9 a7 ~0 s: q. E0 K% a
and actuators, which are needed in modern robotics
" ~( M$ H" y! C/ `1 h: v8 n1 N- Yapplications, as are also piezoelectric materials,
' ~& A$ c( O' z! U. bwhich are critical to the operation of scanning tunneling7 D' {( I* q- o$ X9 Y. r
probes that provide information at the atomic level on
7 |1 N7 K, b3 m5 q$ A5 ^structure, stoichiometry, and electronic structure. The1 u3 p0 `- m; ?0 t' e
technological development of microelectromechanical7 l! k+ s }; U& `. [
systems (MEMS), based on silicon and other materials,
5 [! Z" {9 {* }' f V1 ]8 kis making possible the use of miniature motors and actuators
5 \2 e: i0 O. vat the micrometer level of integrated circuits.6 b( j, N- s7 [; ~
Some of these have already found applications, such as
) e1 G1 x( T7 w( p1 wthe triggering mechanism for the release of airbags in
6 n! i2 g, I& H$ yautomobiles. Such developments are not only important
- l+ R: z! a8 p8 b$ N# w6 yto the electronics industry, but are also having great impact# j: c5 O9 h9 D$ K2 u* P
on fields such as astronomy and space science,4 u" j, P) E; s9 {
which are dependent on small, light-weight instruments. D, [3 L2 H0 q* n
with enhanced capabilities to gather signals at ever increasing Q% P* N" {; }& _8 L6 v/ h
data rates and from ever increasing distances9 l" W- \$ `' }4 m, O! L
from Earth. The developments in new materials and9 I) k) W3 z& l) b _/ z
low-dimensional fabrication techniques have recently rejuvenated: w3 y( k3 j, N' a. A! Y( n& G
the field of thermoelectricity, where there is
" l/ T1 v. N7 }4 o' ?% v3 a7 y8 Enow renewed hope for enhanced thermoelectric performance
( K, |1 k( o! I" B! Y, D! Vover a wider temperature range.' f( ~- d8 q+ a5 C4 J
Research on magnetic materials has been strongly influenced
9 o- \1 K! K, \+ Vby applications ranging from the development
~$ e1 ~$ ~0 P1 W3 A Iof soft magnetic materials (by the utilization of rapid0 x3 ~& I2 v3 y7 G- K: m; H
solidification techniques) to hard magnetic materials" \/ F& ?0 O& E, L% l3 @1 A, x
such as neodymium-iron-boron for use in permanent7 Y; E5 Q1 {9 t7 Q& o m
magnets. In the 1980s efforts focused on the development
* A+ O5 J5 L* }- c5 S8 B+ }) uof small magnetic particles for magnetic memory
' G- [' g/ n; i4 Sstorage applications. New magnetic materials, especially2 ^, q& H; @$ W( e# K
magnetic nanostructures, are now an extremely active
$ f: K& X0 Q9 C3 b, V6 ` Qresearch field, where the discovery of new phenomena
8 x4 M* z' B/ u2 N& u/ q F3 S1 dsuch as giant magnetoresistance and colossal magnetoresistance0 E# k0 Z# d3 [+ I
are now being developed for computer memory
) Z# e* b$ D: [- R; ?+ ?applications.
- O8 f* o0 {- O% L$ eThe strong interplay between fundamental materials2 c( h3 R8 K0 {
physics and applications is also evident in the area of5 b' T: N# R: g" X) H
superconducting materials. Early use of superconducting
8 ]( R1 g# ]+ mmaterials was in the fabrication of superconducting magnets,
6 f# B; @0 S$ l3 z2 zwhich in turn promoted understanding of type-II7 |; ?0 z( D: t- ~2 e6 j
superconductors, flux dynamics, and flux pinning phenomena.2 q3 ?/ e/ ^: n8 p
The discovery of the Josephson tunneling effect
& r: O- Z |( o" M. G6 Zled to the development of the SQUID (superconducting
! G. N# E! y, q( \. Y! Cquantum interference device), which has
) [/ C$ N7 S* L& q u5 R" z/ z5 n3 ?become a standard laboratory tool for materials characterization# K: Z/ d, L" C
and for the sensitive measurement of extremely
0 O' Y3 v+ l% M2 }& A) {small magnetic fields, such as the fields associated
- a% S( o8 a% ]! `, G' Cwith brain stimuli. The discovery of high-Tc/ y- z4 F4 C3 o% R0 [
superconductivity in 1986 has revolutionized this field,6 n) t, b! J9 y9 s$ v+ B' ^8 w. V
with much effort being devoted to studies of the mechanism& o/ `* R* b. V; q8 q
for high-Tc superconductivity, along with efforts to5 U: x& E3 e' ~- r, z6 v' F3 G
discover materials with yet higher Tc and critical current: V6 W8 R) u6 e& Q$ z4 ?& I, H5 f
values, to improve synthesis methods for the cuprate superconductors,
! S3 O# w2 \" l& T# c0 b- V' \# H0 zand to develop applications for these
- f7 w1 }. k3 N0 d+ b! K* H& rmaterials to electronics, energy storage, and highmagnetic-! ]9 h h0 E9 S
field generation.
: L# w5 I: S2 O$ s9 z1 ?; l1 w; y) D5 tWhen viewed from the perspective of time, the developments
# \( F a. A7 _3 J* b9 G/ o Din electronic materials have been truly remarkable.8 U Z" M) J" ^7 M' J
They have generated businesses that approach a/ r- j+ ]$ ?2 \# g0 `) X
trillion dollars, have provided employment to millions of5 k# ?" r. {( c- ]
workers, either directly and indirectly associated with0 p0 |* g4 q2 r, A+ X& g
these industries, and have enabled us, as humans, to extend( O3 A O, D+ k# c
our abilities, for example, in information gathering,7 O- `: F' T) @
communication, and computational capabilities. Science9 J. @$ b9 v5 F9 t
has been the key to these marvellous developments, and
9 ^+ b$ @( i5 B0 E; Zin turn these developments have enabled us, as scientists,
, \* ?- @3 o7 ]$ \3 U5 {7 H0 Rto explore and understand the subtleties of nature.
9 N5 m9 K* d! l+ e5 DV. SUMMARY
2 {5 J: ^* B( kIn this very brief note, we have only touched on some
; D6 _0 V5 ^% w1 m v6 Pof the advances made in structural, polymeric, and electronic r1 h; U, ?: N R* _: t
materials over the last century, showing how materials
. s( S ^* ?- @3 |physics has played a central role in connecting
! U0 m' k0 x$ k0 Yscience to technology and, in the process, revolutionized G) g7 v1 {; @" }5 m6 k/ J
our lives.
' B7 A8 C9 t1 Y/ R4 y" [P. Chaudhari and M. S. Dresselhaus: Materials physics S335* a' A1 Q3 n7 ~* ^2 R6 ~
Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999 |
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