|
|
Materials physics1 i- x- `! v1 J6 ]. U# Z
P. Chaudhari7 T. j( m% r( r+ E& G7 @
IBM Watson Research Center, P.O. Box 218, Yorktown Heights, New York 10598
+ ^% n8 T8 I/ V0 Z$ q3 g WM. S. Dresselhaus' j( l3 A9 i) i, X/ }
Massachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307
: G" s l; w. A8 y, O9 lExtraordinary advances in materials physics have occurred over the last century. These advances have
9 q4 F* ]* m# `5 r! Sinfluenced almost every aspect of human endeavor. In this note, the authors sketch some of these
" i0 f: [0 n" C% Sexciting developments in structural, polymeric, and electronic materials. [S0034-6861(99)01502-0]
! O: d! _; o% q0 r/ {I. INTRODUCTION
2 S) l _6 Z0 T/ [: [) u: ]" POver the last one hundred years there have been stunning
' P4 G0 W( i3 ~5 |1 j9 V/ H3 Padvances in materials research. At the turn of the
4 k: U0 A3 d& q/ G2 _0 _( r8 ylast century we did not know what the atomic structure
; s6 d4 e9 r& @9 L" j8 U: Qof a material was. Today, not only do we know the structure,. |( R* x! _; p+ c# {
but we routinely make artificial structures that require
& r) z3 E& b7 {; X! Xplacement of atoms at specified locations, that mix% j' J) D4 r9 H# m& v6 s# h2 Y
atoms to create properties not found in naturally occurring' [+ m) f1 {% a% r+ Z7 T
materials, that have the functionality needed by today’s
& [5 |% r% T0 w0 x5 ktechnology, and that adjust their properties to a
0 `1 @1 V8 [! F& N' c- Vchanging environment (smart materials). Over the last
. U+ ~5 ]$ F9 _: _/ n0 tfew years we have begun to manipulate individual atoms
9 v% e7 v; R& {- i/ T) \* zto form structures that enable us to explore scientific
, I! m# }2 ^- P4 H4 G2 f+ {issues, but that will surely lead to profound technological
* l4 G. t( a% y$ G0 Hand social consequences; for example, the manipulation
7 H" _9 p8 f3 o- @2 `. V K5 }5 Xof nucleotides in a DNA molecule, which is then
$ n7 M: }) F% a4 F$ f/ u) @correlated with the functioning of, say, a gene and with; v- G/ V3 E6 `* q6 M& O
its expression in the control of disease., a, b; g8 P; B
A hundred years ago there were no electronic devices,7 {3 T9 I% ]- X; O( f0 {
and today there is hardly any electrical appliance without; M, Z6 n8 n) q, H A* d# ~
them. It is anticipated that in the near future there
0 ~( ^+ p: z% S3 Ywill be a microprocessor embedded in almost all electrical7 r- o7 ~6 }, _, X
appliances and not just in those used for computation, Y- R: X7 m8 Y9 z
or information storage. These devices, inconceivable a% e7 k& J; d8 ~: a6 t
century ago, could without exception not be made without! h$ x, k( j& E
the knowledge gained from materials research on
$ \1 {8 s. ~5 a0 ^3 ]5 u- o9 d5 l kinsulators, semiconductors, metals, ceramics, and polymers.2 ?: K% {' x; [0 v# b0 V! u
At the end of this century, we have begun a debate
X K9 k) h6 v8 P3 Z' eon how far the present devices can continue to develop,
. K4 U& {: T2 Z# O/ u6 t! Bgiven the limits imposed by the speed of light and
6 a N% h& j$ z6 g/ hthe discrete nature of atoms, a debate that would have
8 f5 ~: Q( Q3 ^7 ^4 obeen incomprehensible to scientists and technologists of: A4 H- }* Q% Z& C. u9 M. p
a century ago and a debate in which we now discuss the
* V; t& ^% Z9 ]7 @6 ypossibilities of using single electrons to switch a device. T! Z& f: ?8 w' R" v) r
on or off.# o, ~, B& X: {
Our ability to measure temporal phenomena was limited
8 J* S9 p& H$ R" V$ cto fractions-of-a-second resolution a hundred years
+ Y( d) {. y8 K2 q4 i1 e& w' Vago. Today we can measure changes in properties with a
, Y/ c" ?( B/ ?few femtoseconds’ resolution. Strobelike probes enable
$ U. N4 E! c! l+ p: S* f+ J! Jus to measure phenomena ranging over time scales covering
1 a9 h; w: X9 ~! e! Amore than ten orders of magnitude. We can, for8 K! P q( x- d0 ]) Y
example, study the relaxation of electrons in a semiconductor( v# j: H( g9 o, }% H
on a femtosecond time scale, the visible motion' \; }: J& ~# P! I/ F' _* ?5 }
of bacteria in a petri dish, or the slow motion of a sand& {0 e4 x8 I. y5 E0 ]/ G9 T
dollar on a beach.
, n2 s5 r1 f, r3 U' e# X! v2 jMaterials research spans the range from basic science,
3 U% P7 k% g- W6 i4 Kthrough engineering, to the factory floor. This has not* `1 |9 I4 C* Y5 t
changed over the last hundred years or, for that matter,' e3 G8 ^" M! @4 x
throughout the history of human civilization. Materials
4 O+ Y6 |1 S3 Z( O9 a& k, ~! |research came out of the practical needs of mankind.' e. Q" Z- u# d* Y: Q2 s9 e u
Eras of civilization were named after materials, so central$ ?0 T( [2 u! K& r6 [2 E2 D
has been their role in achieving mankind’s mastery
! G1 P* T [. |+ [! j+ L% ]over nature. The field of materials research can trace its
9 B- c* R/ f3 t9 `9 Sroots to alchemy, metallurgy, natural philosophy, and6 T# B9 q& ^0 \0 f
even art, as practiced over many centuries. However, the, ?* R ~$ |& K: }0 A! n. o6 s
field of modern materials research, as represented by F; H9 r7 H( C9 y" m
materials physics, is only about sixty years old.
+ z. B5 b6 p0 N c w0 D, fShifts in materials usage from one type to another are
) z8 X* z: g6 p' p' k* ousually gradual. This is due to the very large investments
( K( ^; C) K+ y9 X! v, A& \3 Fassociated with products in the materials-related industries,8 ], l* k _8 M$ Y. { V
complex relationships between reliability and functionality,7 {7 {5 X, m: B) U- p# R% `
environmental issues, and energy demands.
0 ^* E+ f ]! b h; O: cHowever, measured over time, these shifts become quite8 |# w# Y7 h: a0 u; `0 f
perceptible. For example, in automobiles the ratio of" K ^+ o* f# W8 f
plastic components to iron-based alloys has changed
+ ^! u' _1 w& X( k8 ^+ ]8 \, ^$ Z* ~from less than 3% to more than 15% over the last two4 \$ j$ p* [4 y
decades. Although the percentage change appears to be0 ?2 ~ H) w5 T6 P% t( @0 u
modest, the actual volume of material is large; over 40
% |7 y- F& `/ F9 m2 |million tons of structural materials are used annually in0 N, |. _. E8 ?7 N3 x9 ?. }, R0 ~
cars.
# q; Q8 O" j& j, ?& }The advances of materials research in this century,. N( O; O: r) F0 l7 J
which far exceed those of all prior centuries put together,
& p4 }; h: U( n7 t; m" B# l+ Tcan be illustrated by three examples: structural,& L( L1 [) r6 H. Y# E4 z- I- e
polymeric, and electronic materials. Our choice of these
/ t, z# D- f6 cthree is somewhat, but not completely, arbitrary. It is" j% N+ W! Q2 c0 s% g7 P" H0 s
out of structural materials, particularly from the fields of
N& ] }* Y) H0 o4 @0 cmetallurgy and metal physics, that modern materials
( J. }4 o7 T- i: R p% lphysics has evolved. From the crude weaponry of our1 T1 e; J. ^/ ~/ \6 T- Q. U% s
forefathers to our mastery of air travel, space flight, surface
2 t2 T" r Z1 w- ttransportation, and housing, structural materials
* e2 z* f/ j' [3 [ r) Dplay a role that is unequivocally important. Nature uses
, t# j! U9 Z& f9 Ithe second category of materials, polymers, in amazing( f. B4 i- O' q) P4 n9 _7 q
ways, to perform very complex functions. We humans
" L1 e4 c( K" a4 Ware an example of that. Over the last hundred years, we
2 P6 X9 n* f' t! x1 @have begun to understand and develop polymers for
* W4 Y( e+ a3 G( n1 ^uses in food packaging, fabrics, and structural applications.
/ I) v8 O& J3 {' N$ F; S. U0 QWe anticipate that polymer research will play an: R) e' x2 h& t i$ u
increasingly important role in biomaterials of the future.
+ {, d! P x, p" D* ?The third category, electronic materials, were not conceived& t( L8 Y/ d- V
until quantum mechanics was discovered in this9 j8 Q2 ?* O* V+ a& ~7 H1 U# y4 J
century. Today we cannot imagine a world without telecommunication,
^9 K# o# I3 s+ d7 {8 lcomputers, radio, and television. These+ t# j) N, y2 x2 Y3 ^7 a
and future devices that will make information available5 s. a L/ w7 Z7 h
Reviews of Modern Physics, Vol. 71, No. 2, Centenary 1999 0034-6861/99/71(2)/331(5)/$16.00 ©1999 The American Physical Society S331
; j9 y0 g4 W/ B7 p* kinstantly are only possible because of advances in the( u2 C+ Y( p7 T0 y" ^( u4 Y
control of materials structure and processing to achieve# W" x3 D9 L1 H) P m
a desired functionality.
" _: @3 U5 {: A2 q- r4 d" d- LII. STRUCTURAL MATERIALS
# G- q8 E, i+ QAt the turn of the last century, mankind’s use of structural! W, d4 D0 A# D/ x7 I# C- I/ o
materials was limited primarily to metals, particularly* i: |) y: ?* t$ d4 A' q9 Q( O
iron and its alloys, ceramics (most notably Portland; {; D- o u$ e. _
cement), and polymers, which were limited to naturally3 C2 h3 ~9 m6 Y
occurring rubbers, glues, and fibers. Composites, as a
$ h5 G0 |9 T: F4 y" R/ g8 Xconcept were nonexistent even though wood and animals,( @7 m) N: T. ~/ ]
each composed of different materials, were used in
/ V% B$ n1 q8 I5 G/ u+ E+ C( Ka variety of ways. However, the uses of alloying to enhance
. v" \ T, b* U) ?$ K+ Bthe strength of lightweight materials, such as pewter,$ j; c! n. V( J( u) z9 ]
or copper additions to aluminum, were established8 R1 m& k( w7 |1 b/ o
techniques, known well before this century. This knowledge
6 g$ e c7 \, k! Z) b4 Qwas used to build the first dirigibles. The useful
i% U% V! A. j' tnature of a material was often understood through serendipity: H' h1 H; q* c, B* o& H I
and not through an understanding of its structure
7 h1 u' L2 A, t' zor the relation between structure and properties.
6 ]1 U! p# r9 x! k4 Z3 D! bWe still cannot predict in any quantitative way the evolution1 C% }3 _1 h( r% W& \
of structure with deformation or processing of a
9 D) a, e* q' T: omaterial. However, we have come a very long way from( O- Y/ ^ o8 R: Q$ i! p: _$ k4 [
the situation that existed a hundred years ago, thanks to$ A, u% t; g. t* j" }
the contributions of twentieth century science to our understanding) `" A# \$ s0 O$ c
of atomic arrangement and its determination X# W& |5 a# z+ E T3 `1 j& \. h
in a material. Our classification of materials by symmetry
4 ]3 d2 u" s- Uconsiderations came into existence once atomic2 _, |8 h3 k! U7 @& o
arrangement became known. To the seven crystal systems
- Y! V6 @* Y/ P5 I0 R) O6 B Band amorphous structures, typified by the glasses
# L; i4 A4 H" F" @* t( yand liquids, we can now add quasicrystals and molecular
5 W4 D6 g( X+ S/ W7 U, hphases, such as fullerenes and nanotubes, in a crystalline! L5 {4 E8 j# F! Z2 u
solid.) K6 k* _% q7 P' U4 p
The crystal systems define perfect crystals. At finite
* a! c6 _$ \8 wtemperatures, the crystals are no longer perfect but contain& [1 Q1 E( m9 V
defects. It is now understood that these defects are
0 {- B8 g- d2 s0 ]responsible for atomic transport in solids. In fact, the1 P0 Y8 @6 R1 o: D
structural properties of materials are not only a function
0 Q' ]& N. r! S/ b7 v: Xof the inherent strength of a material but also of the! u% V _1 F$ v0 |2 S
defects that may be present. We know that aluminum is
3 g0 w3 }5 Y$ D- l1 u2 Gsoft because crystallographic defects, called dislocations,! M: T7 G' X/ b/ ]
can be readily generated and moved in this metal. In
# M/ G7 C, B, ccontrast, in alumina (Al2O3), dislocation generation and( y" P" p. f* {& a; s4 x6 Q6 V
motion are difficult; hence alumina can be strong but# \* n5 A( i: U I5 y( b1 a7 i6 i
brittle at room temperature. The addition of copper or
* S) T5 n7 M) {" g/ {) dmanganese to aluminum creates second-phase precipitates,
% x7 q% I2 l- Y8 |0 V5 fwhich inhibit the motion of dislocations, thus enhancing
# k4 T$ p' q/ O( A# v: Z* qits strength-to-weight ratio. Our ability to improve
+ {" `3 ^' P0 ^4 _* g4 ~the strength-to-weight ratio in materials has
6 d% R# S1 V; e, d. A2 }increased more than tenfold during the twentieth century.
2 R' l& Z; K+ u6 M' x1 u. tThis is to be compared with a change of less than
% D- |; T9 X+ E. sten over the last twenty centuries. Much of the increase
. u- O9 x' d' [in this century has come from an understanding of the0 {# I4 R+ e) M
relationship between the processing of materials and
: U3 I) O8 ]7 |: @; p3 [+ }5 {their structure. The highest strength-to-weight ratios9 A, _ |' n" c1 w9 l8 z, d: z9 G
have been achieved in materials in the form of fibers and. y, B8 B/ Z1 i; T
nanotubes. In these structures, dislocations either do not, z; {4 t$ r1 @& S
exist or do not move.
# I$ L+ z+ T1 b3 RMost structural materials are not single crystals. In
6 w+ B1 ^; Z) E Dfact, they consist of a large number of crystals joined at/ D: X; H7 {. K9 ]8 r" D* H
interfaces, which in single-phase materials are called
0 b% S J$ E* ^& \7 [grain boundaries. These interfaces can, for example, influence6 Y( O+ z1 @# q% C* B9 e
the mechanical and electrical properties of materials.
Q8 r/ b' r. YAt temperatures where the grain boundary diffusion
/ E" \3 m3 R' Z1 ^% j) @rate is low, a small grain size enhances the strength2 z; ], P+ C8 S# d1 O/ |5 I
of a material. However, when the grain boundary diffusion
4 q' T# [/ L; m' D5 S$ u# w& P# Brate is high, the material can exhibit very large elongation% m" h3 f% ^0 x$ K G# _
under a tensile load (superplastic behavior), or2 p3 [& D' j( c$ ^
can exhibit high creep rates under moderate or small& n+ T' N+ i( H$ s
conditions of loading. In demanding high-temperature" K# J. c% d& v" d% C2 t n4 D% \
environments, such as the engine of a modern aircraft,! K9 g, |" q# w9 i8 q6 U0 l
grain boundaries are eliminated so that a complex part,5 }8 r) D- B/ A& T ^
such as a turbine blade, made of a nickel alloy, is a single+ _9 w9 k; i" v1 l0 x* u
crystal. Thus the use of materials for structural purposes1 W, x3 W& N! I
requires an understanding of the behavior of defects in- K+ J; C( b: c( `$ @( W. c) S1 u
solids. This is true for metallic, ceramic, and glassy materials.
8 |' P r* A4 `) UBoth ceramics and glasses were known to ancient civilizations.. o$ C4 ?# H+ K0 m' j
Ceramics were used extensively in pottery and" O; Z& q3 y; b( d; r; B" I
art. The widespread use of ceramics for structural purposes! H3 Q: {& k8 U# q
is largely limited by their brittle behavior. This is
. F; d$ v b9 H) j/ r" P Inow well understood, and schemes have been proposed5 G; _; B6 ] W' E/ i' x$ m
to overcome brittleness by controlling the propagation
5 |1 _% o5 \/ k; X( Dof cracks. In metals, dislocations provide the microscopic& q( V" r, ~8 k) M3 P# e
mechanism that carries energy away from the tip
( G5 l1 ^, z9 b4 b; lof a crack, thereby blunting it. In ceramics, the use of9 H) G9 g3 M4 j- D
phase transformations induced at the tip of a propagating% Y* Z: r; T) z8 P
crack is one analog of dislocations in metals. Other `# O% V/ V% T9 F; V9 v" {0 x
schemes involve the use of bridging elements across
# u, I( [8 m$ u5 \# n9 Ocracks so as to inhibit their opening and hence their
) N- Q; X9 A" z" gpropagation. Still another scheme is to use the frictional
4 F% B/ u! k, {' ?( i2 Adissipation of a sliding fiber embedded in a matrix not# N5 x! f0 E4 |
only to dissipate the energy of crack propagation, but4 a/ |* ^( k7 e. G& v5 @
also, if the crack propagates through the material, to% G% L7 s' I0 P: |+ A! s# `6 [
provide structural integrity. Use of these so-called faulttolerant: O1 L' H2 ]) @* F
materials requires both an understanding of mechanical
0 `9 n2 l, t# r5 _/ ^$ Sproperties and control over the properties of
3 n. M6 G6 C# m1 finterfaces to enable some sliding between the fiber and H: p7 n& k- k/ w
the matrix without loss of adhesion between them. Such* k" S7 C# ^' H1 d* {+ @# D+ F1 N, Z
schemes rely either on composite materials or on microstructures
2 L7 i8 ^ U8 A. y9 W! t; a* Sthat are very well controlled.& \% U# q0 ~0 r/ ^$ S9 x
The widespread use of silicate glasses, ranging from. A2 `4 F$ @: f0 l* I: v
windows to laptop displays, is only possible through the
0 U* N( J5 S% k! M" Z! ]* x5 oelimination of flaws, which are introduced, for example,
3 X& P) R! i6 T8 }$ {. g; `. Sby inhomogeneous cooling. These flaws, which are
4 W' o* ?1 a6 J! `8 Eminute cracks, are eliminated during processing by controlling
8 S9 I+ k# j& i. x7 Bthe cooling conditions, as in a tempered glass,5 ?: S3 e: Z8 ?: B; e& q
and also by introducing compressive strains through9 ~ e9 @7 s Z- B1 H: [6 `3 l
composition modulations.( ^! q' D& b* a4 g- Y8 a: o+ O* }
There are a number of fibers that are available for use
. a" E5 ?9 Q; Dwith ceramics, polymers, and metals to form composite
! @. @5 w* I6 D$ M9 smaterials with specific applications; these include carbon
2 d8 A; G9 Q1 Nfibers, well known for their use in golf clubs and fishing3 U3 i- O% e( e- t: X: }
rods, and silicon carbide or nitride fibers. Optical fibers,3 h/ s4 v& p: X
which are replacing copper wires in communication
. f/ R# m. G J& a$ t! C K( q5 H! atechnologies, owe their widespread use not only to their
1 B% n( ^' M% D# E/ @9 H# c7 Zoptical transparency, but also to improvements in their
4 c; c! S' Q, `1 t% jS332 P. Chaudhari and M. S. Dresselhaus: Materials physics
0 `+ K/ @# P. P3 x* }( Q# PRev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
/ X, W" H: P% z9 u7 z/ S$ vstructural properties. Fibers must withstand mechanical& y8 @/ K( J _
strains introduced during their installation and operation.
: S& I& @! \4 C' M# i5 \The use of composite materials in today’s civilization
# k' y& b+ g( X* P( p% G9 c) |* l) ?is quite widespread, and we expect it to continue as new
, n3 y7 r; H# c- a- O2 Z8 s. oapplications and ‘‘smart’’ materials are developed. An
' |. R: J* b8 `9 p3 [outstanding example of a functional composite product
* j8 t% U& N7 w, z7 S5 n% \comes from the electronics industry. This is a substrate,
; c7 l2 J+ y- Vcalled a package, which carries electronic devices. Substrates
! N" d( F9 ]) a. L- l( f+ I" pare complicated three-dimensionally designed
2 c$ Z4 ]6 v/ ^; K9 }! Y7 Lstructures, consisting of ceramics, polymers, metals,
2 U6 ]. n8 Z+ i* U( a5 T* @; e, Esemiconductors, and insulators. These packages must) |- h) Y( o9 G+ g& O
satisfy not only structural needs but also electrical requirements.( |8 W4 C8 D9 z, C# ]. L0 N! u; p' m
Although we have made great progress over the last
( ^5 Z( ?- d' N' Yhundred years in materials physics, our microscopic understanding
$ J" f% _( ?: u$ F* D) Dof the physics of deformation (particularly5 F5 O- q& B+ D j" i) L
in noncrystalline solids), fracture, wear, and the role of
0 U$ ], |" B; I$ A9 Einternal interfaces is still far from complete. There has
) g S# b* i6 t! B. `, X$ Jbeen considerable progress in computer simulation of4 }' m/ L; i+ N4 o& p
some of these issues. For example, there is now a concerted6 V3 I' K, l# @
effort to model the motion of dislocations, during$ a7 q1 S/ B' J
deformation, in simulations of simple metallic systems.
/ e3 C5 h$ c; |8 ]! \. fWe anticipate that within the next decade, as computational
5 {: B% [- |6 O# y% Ipower continues to increase, many of these problems
) T, ~' ~( J% J! awill become tractable. The ultimate goal is to design
d; g! H. J4 d+ ]3 I' q+ c$ ^a structural component for a set of specified
# i- Q: Y, d/ g2 r, _environmental conditions and for a predictable lifetime.+ M& I/ D: s- v& a w2 @
III. POLYMERS
/ L. G: G! r$ P1 k5 Z: T3 PPolymers, also known as macromolecules, are longchain/ p- Q# U- |# [0 z9 O* Q
molecules in which a molecular unit repeats itself
/ ?* G+ _! V+ e1 r3 o) _8 K: K' zalong the length of the chain. The word polymer was6 o Y! o. l, k1 r) {
coined approximately 165 years ago (from the Greek2 }, e- p4 J& \" h4 r0 i. E- w1 F
polys, meaning many, and meros, parts). However, the
! h% R9 I( O4 j1 Kverification of the structure of polymers, by diffraction
3 e$ S) u" d+ r! h. M2 E) I2 R6 Hand other methods, had to wait, approximately, another/ z" z4 _3 j; K; P- e; M- `
100 years. We now know that the DNA molecule, proteins,* J1 l o: t" ]% t
cellulose, silk, wool, and rubber are some of the
0 S% N! Z% e0 ? i1 K& Z! ~naturally occurring polymers. Synthetic polymers, derived; D F& \5 }1 W7 I5 e
mainly from petroleum and natural gas, became a6 ]0 H7 ]6 k7 k7 C8 z
commodity starting approximately 50 years ago. Polymers
5 i: z- h. Y! W! V) _became widely known to the public when nylon' r' t' w9 Q' R z0 Q, T) m
was introduced as a substitute for silk and, later, when8 f: V: Z3 O- \ T2 _% z! h
Teflon-coated pans became commercially available.
4 f! z2 ^+ M1 o4 D9 ~) S8 oPolymers are now widely used in numerous household
$ @6 q( Q E6 d5 Bapplications. Their industrial use is even more widespread.
" s; j* N9 i# X- c! t6 SMost of the applications associated with polymers
3 z2 h5 P |4 c3 T: a7 O9 Vhave been as structural materials. Since the 1970s it was' N+ v& @/ P! o; [7 x- s2 S
realized that with suitable doping of the polymers, a
0 P A* p8 E' h+ ?) twide variety of physical properties could be achieved,' s3 x$ @* }1 D: |) ]7 I! H
resulting in products ranging from photosensitive materials+ j/ @) M7 ^% K# J7 |& s0 I
to superconductors. The field of materials physics$ C# r* I5 A% }+ E, q3 W
of polymers has grown rapidly from this period onwards.
) p& |8 F: h8 PPolymers are a remarkably flexible class of materials,
! n7 L1 B9 _9 c/ o' N- n, Twhose chemical and physical properties can be modified
9 f' N# ^2 x6 R; d, [6 \' _by molecular design. By substitution of atoms, by adding/ u' x3 U/ j6 s# k5 W
side groups, or by combining (blending) different polymers,
3 w- ^% J: S5 w, A n" Cchemists have created a myriad of materials with
0 O% c5 c( w k( g* Kremarkable, wide ranging, and useful properties. This5 X% f: {3 M. i+ D
research is largely driven by the potential applications of. h5 B1 b8 Q: Q8 I& i# ^
these materials in many diverse areas, ranging from cosmetics" J6 p- t) I F& m) D( Q
to electronics. Compared to most other materials,. ?; ^5 a% I0 E2 `
polymers offer vast degrees of freedom through blending) [1 E8 R5 R, }( ?6 R9 P
and are generally inexpensive to fabricate in large* `: O! }" f N( }( G8 I8 }
volumes. They are light weight and can have very good; [8 e8 ?7 `3 _# E
strength-to-weight ratios.
8 d% M. t, w. ^+ gPolymers have traditionally been divided into five
" t; ~+ A& @3 S/ W: T4 _classes:
O& h- x$ l) `(1) Plastics are materials that are molded and shaped( R' L D; Y$ R% q2 H2 \
by heat and pressure to produce low-density, transparent,: \2 i/ H6 O2 z0 o% |' W
and often tough products, for uses ranging from
5 ]/ B* z8 ~: f( o4 F' j. a0 K Vbeverage bottles to shatterproof windows.2 s/ u$ |# W9 V& r" i+ I
(2) Elastomers are chemically cross-linked or entangled2 \( h b3 Y/ k9 W1 b, k
polymers in which the chains form irregular coils
M" \6 L0 B' ~that straighten out during strain (above their glass transition
+ B% f- O* y2 ?5 B& ktemperatures), thus providing large elongations,' k2 K. i9 j u8 @/ ^
as in natural and synthetic rubbers.
7 _3 c- C/ V- z4 e2 K/ M$ J(3) Fibers, which are spun and woven, are used primarily+ d' E7 P9 g! H. t
in fabrics. About fifty million tons of fibers are produced
: y+ X$ a. T. z1 K- wannually for uses ranging from clothing to drapes.; N% Y2 S' p4 q
Apart from naturally occurring fibers such as silk and2 L# J/ q2 s, n$ m$ k
wool, there are regenerated fibers made from cellulose
. ]& g0 z3 C- k" R1 T5 o. B( ~) Epolymers that make up wood (rayon) and synthetic fibers,; \2 ~ N' K, M: f, `
comprising molecules not found in nature (nylon).8 h% s! @1 Q1 k# @( y7 W
(4) Organic adhesives have been known since antiquity." ?3 T# [* ]1 @) H- n5 D. K, s) i& F A
However, with demanding environments and performance
7 |/ h. B8 E8 Q# y0 `/ srequirements, synthetic adhesives and glues
& L# n( s- P3 z4 L3 X) dhave largely replaced natural ones. The microscopic
. M: x' C1 n$ A6 l9 f# m( [mechanisms of adhesion and the toughness of joints are
4 ^6 J o5 }% O* i- R% jstill debated. There is an increasing trend to use UV2 c1 b! n5 \- v& B, X) t# a! v1 K4 Y
radiation to promote polymerization in adhesives and,
4 b! B" X5 m$ t* Fmore generally, as a method of polymerization and cross4 G+ T7 f, B' N. X
linking in polymers.$ F2 q; R; [) u7 C
(5) Finally, polymers, frequently with additives, are9 `! r( v. r2 G/ [' a" `8 g8 i7 @
used as protective films, such as those found in paints or; |: ?& O! _2 }5 t0 E6 F0 ^) J
varnishes.
$ D1 c/ c, g n$ C+ PPhysicists have played a significant role in explaining7 m+ |% s2 b+ |( ?- p3 r
the physical properties of polymeric materials. However,
5 s9 h. a( G" t, Z# Gthe interest of physicists in polymers accelerated when it+ w2 X; z3 {4 E4 p; t: w0 z8 z
was discovered that polyacetylene could be made conductive! s) X! u# S7 R- c! ^ B! u
by doping. This development was noteworthy
. s& m' I4 C9 `7 c+ ]1 n6 Kfor it opened the possibility of deliberately controlling
4 m! y; M4 ]0 q9 P3 f+ i. Jconductivity in materials that are generally regarded as* X. I) B& j$ i6 z
good insulators. The structure of all conjugated polymers," w# f# R8 S* T9 M8 D: T- M: m9 A" [
as these materials are known, is characterized by a# K4 l/ k1 {* Q* x- h5 k; f
relatively easily delocalized p bond, which, with suitable
; u7 H+ M8 _& H8 S1 ^/ Pdoping, results in effective charge motion by solitons,- k9 b8 ?; {, j* k% R
polarons, or bipolarons. Since the discovery that polymers
: y4 }% N8 V" Dcould be electrical conductors, active research areas6 e% P+ l9 M( ?2 s- I
have developed on the physics of polymer superconductors,
: j7 y2 ]3 ~2 c& C9 \5 V5 z# {ferro- and ferri-magnets, piezoelectrics,
! p7 @5 j8 q7 G5 U6 I3 j( Rferroelectrics, and pyroelectrics. Within the field of4 f1 z* U% v# X- I( P" {$ `5 e" A) u
doped polymers, devices have been built to demonstrate
* I) i; f% Y" }. ]+ ?3 zlight-emitting diodes, photovoltaic cells, and transistors.
/ w, N' t2 X1 i& B4 Z U$ N3 rConjugated polymers have also been investigated extensively. y4 {3 y2 h) ^, a! a- V( e3 j
for their large nonlinear, third-order polarizability,' W3 v# p4 c3 X5 `/ v0 L H
which is of interest to the field of nonlinear op-0 ~% }, p0 |% ^) R" d& q' t+ R1 W
P. Chaudhari and M. S. Dresselhaus: Materials physics S333
/ h% g+ c* B5 Y( \Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
: N( M z$ W- stics. Large nonlinearities are associated with the strong2 a# N: k) Z( @* S$ ]
polarizability of the individual molecules that make up) k; B* G, [* K1 M+ P. Y. p: \
the building blocks of the polymer. Furthermore, the) V3 w+ M: x& T/ I
flexibility of polymer chemistry has allowed the optical1 l$ E8 E( p. i# E) M. {9 a
response of polymers to be tailored by controlling their7 U2 ?6 o# R. k' B: m
molecular structure, through the selective addition of
6 t1 r! H K4 _# F+ |0 U1 Z: Wphotoactive molecules. Hence these materials have been2 z5 z4 T. B- s" ^
widely investigated by physicists and engineers for optical
5 I) U5 V; ^6 O aapplications, such as in holographic displays (dichromated
0 }6 N; U( @$ E: v% s# B9 hgelatin), diffraction gratings, optocouplers, and
% A* V( d- c% x0 C' Jwave guides.
( {9 |) s3 }3 C" [7 oPolymers have long interested physicists for their conformational% Q, {/ m% E3 D) u# Y" K! g n7 X* S
and topological properties. This interest has; E% _* W/ F8 B; J3 r# x
shifted from the conformational behavior of individual0 s! Q) ~* Z- ]% f
molecules to that of a macromolecular assembly, phase" }# \; \3 G7 w- a- p) `
behavior, and a search for universal classes. Block copolymers,
. Y2 M! u& ?, X' o( ?* B& aconsisting of two or more polymers, can give8 o" Q; y5 e) i- k
rise to nanoscale phases, which may, for example, be$ Z7 X9 j5 i; ~% o q# F- k3 ~$ F1 D
present as spheres, rods, or parallel lamallae. The distribution( `: U" g* i# ]' }$ N s1 R
of these phases and their topologies are of current
9 q* C4 E: t+ F6 Ytheoretical and practical interest. Block copolymer- T7 h6 y5 C! D; _$ b
morphologies are also being used as nanoscale templates
Q( r# g o1 T: M( R0 Ofor production of ceramics of unique properties having
% ^/ T, g2 N- `the same morphology.
! H" @+ Q- C# F& a* ^* K cBlock copolymers are also of interest as biomaterials.
/ I. V7 m6 c# [: l( B( QProteins are an example of block copolymers, in which
% D$ A0 U4 C3 z- v X) T5 Fthe two phases form helical coils and sheets. Attempts to
2 t4 F) S/ z# I* Umimic the hierarchical structure present in natural polymers
9 I$ y; a/ u: u. K( v5 n) hhave only been partly successful. The principal difficulty
4 _$ ~1 I6 H1 U& \3 Ehas been to control the length of the polymer3 I! I" X1 H, o% N5 p- J) q q
chains to the precision that Nature demands. Significant$ F& ^' f3 C, k0 M
progress has been made in controlling polymer morphologies( ^! w" A2 W' @& f6 E% `( T! R4 Z- y
with the use of new catalysts. For example,* I/ c8 R2 B% q& r
metallocenes have been used as catalysts to control
! v2 p' L* X# k! G* B8 b Rbranched polymers and organonickel initiators to suppress( \9 Z1 t, o3 x! P1 Q% l _% |+ c
chain transfer and termination, so that polypeptides
& B5 J! a* Z9 w1 Z& |" k/ \1 gwith well-defined sequences and with potential for
9 a- `' k! k. j5 S5 I" {applications in tissue engineering could be made. The$ B+ v9 s. ^% N% \5 v: U8 w
growth of well-controlled polymer chains is an example
, p7 b7 ~" e4 q. m2 M- {, u. F* _. j \of ‘‘living’’ polymerization.4 I ?" \. K, g. k9 B
The static and dynamic arrangement of atoms on the ^2 Y3 A8 [) G! ] G5 [
surfaces and interfaces of polymers is another area of
. C2 E: T/ l2 h5 Y* y; j( ]9 sactive investigation. For example, thin films of polymers,+ H* q6 v, ]' p: j8 [
in which the chain lengths are long compared to the2 d5 z) O; H! |$ h9 O. E) Y3 k
thickness of a film, show unusual physical properties: the
# x) z* J$ K8 V! _! hglass transition temperature for a thin-film polymer decreases
4 \" R5 U: m, @. a5 C- ?significantly, but between solid surfaces polymer
, a' U# Z( [* ]liquids solidify.$ E) l3 h( S% R# O# c( o: ?% L
Even though we have some way to go in making tailored1 |$ s+ w: c0 n9 I
proteinlike structures, polymer research has5 A' a3 e8 ^" K! ~) j. C+ k
played a significant role in the class of materials called$ s9 Z; S1 @% R: K# g) ?+ }/ w
biomaterials. Polymers have been used, for example, to
! n$ j# \& G ~; g* `/ Hproduce artificial skin, for dental fillings that are polymerized
: r" a% \! l' `5 F4 [- win situ by a portable UV lamp, and for highdensity/ A' A/ M. s0 j$ {0 ~ W
polyethylene used in knee prostheses. Physicists; [" w" i; V0 I
play a significant role in these developments, not only
/ z4 I( E: q, V; k3 l& `( Vfor their interest in the materials, but also because of
5 V) P( T3 _- k& s/ u9 s. vtheir familiarity with physical processes that can be used
/ @' q0 H. [. {* ^3 P" eto tailor the properties of polymers. A particularly good
: O+ A4 I8 _/ \: g4 Hexample of this interplay is the recent and rapidly growing
o- \; m+ L7 w8 g2 D# juse of excimer laser radiation to correct corneal abnormalities;7 |3 U) h# N4 v6 J; H& ~( b
using a technology developed from studies
' g- k' G( @8 N0 yof the ablation of polymeric materials for applications in
0 h, r$ V2 V+ Z! |0 p1 U) b' {; |& B% r+ ithe electronics industry, physicists realized that the- a6 W5 ? h6 D8 |
small, yet precisely controlled, ablation of a polymeric
, ?$ G. R5 P. w i8 Fsurface might be useful in shaping the surface of an eye.
9 Z+ t A* `- \/ i# n7 ~IV. ELECTRONIC MATERIALS x! @; u* J% W
The roots of the electronic materials field can be. U" _# n# M, h* g7 i
traced back to Europe in the 1920s, with the advent of- E1 g( S" [) w1 @7 S: b
quantum mechanics and its application to periodic structures9 J1 A$ R5 b0 n0 ~# O3 l
like those occurring in crystals. The early experimental
`! c* u4 h& U" Nfocus was on alkali halides, because these materials
- B2 d2 f4 Z/ Z. E1 D+ A% Tcould be prepared in a controlled way from both a+ E8 `* I! ?. @- }- {* n
structural and a compositional standpoint. The creation2 I; f+ D0 q# G
of a strong academic program in solid-state physics at
) c7 d4 c9 Q8 w+ H: L5 cthe University of Illinois in the 1930s had an important
+ v: ?0 e8 A, t: `" rimpact on the early history of the electronic materials6 A2 F) L1 z" h! f m) }
field in the United States. This knowledgeable human, A% O. ^- x }1 ~
resource played a significant role in mobilizing the national2 a. r5 V* i' x8 n* i9 d
materials program during World War II, especially3 e! o0 b$ Z' t# \1 B
in the development of semiconducting materials
N$ a: @$ q$ A* r' h* s/ qwith enhanced purity, suitable for use in diode detectors
1 U0 ~+ d# h4 I, Oat microwave frequencies for communications applications.3 M" z# C5 m2 _6 W
The availability of these new semiconducting materials
2 j- m& g, |6 g5 n) }0 z$ }in purified, crystalline form soon led to the discovery
1 p- @3 x& z$ W9 l1 gof the transistor, which ushered in the modern* O% E2 I; A1 l, B) _3 f
era of electronics, computers, and communications,
$ K# s0 \$ Y! }* @. c( g& Vwhich is now simply called the ‘‘information age.’’
$ i% G4 l- u, n, ]) l% \Semiconductors have been a central focus for electronic$ y0 |: a. u2 w+ N7 y. x9 l
materials. Quantum-mechanical treatments of a
" }2 B# p, s | ?periodic lattice were successful in laying the groundwork
6 O g7 n# F* Z% }$ A' Vfor describing the electronic band structure, which could
6 @! p4 i) [1 H( d8 v7 z$ ]4 aaccount for electrical conduction by electrons and holes,* a/ U9 L7 a6 f4 S1 u' S: p4 v
carrier transport under the action of forces and fields,. D- R' s1 D" d5 I4 {# Q
and the behavior of early electronic devices. Because of3 w/ K7 F- Q1 N5 U
the interest of industrial laboratories and the Defense
/ w- h( N# f, ^4 WDepartment in the newly emerging field of semiconductor* J8 p v' K8 b- s6 u
electronics, semiconductor physics developed rapidly,; A4 r3 T2 L5 W, r% S
and this focus soon led to the development of the
$ h7 ]. K/ f# t: w- sintegrated circuit and the semiconductor laser.
" w) W6 r* t/ \4 `' z- k2 BThe strong interplay between technological advances
3 B/ y4 I: X- o. V6 nand basic scientific discovery has greatly energized semiconductor
! Y0 ]8 q, r& n" iphysics, by raising challenging fundamental
/ O, p; l, L5 P/ v) f1 c' bquestions and by providing new, better materials and
, V2 o0 F% ?% F/ U8 tdevices, which in turn opened up new research areas.& r# r) w) Y0 t0 D$ w" }& U
For example, the development of molecular-beam epitaxy+ F( c3 W! M8 T
in the 1960s and 1970s led to the ability to control+ r0 |1 F4 O) B6 f/ [: O; D2 Z+ ~0 g
layer-by-layer growth of semiconductor quantum wells0 K7 b$ p' o7 g4 F2 y8 S
and superlattices. The use of modulation doping of the$ I5 e6 x1 b P$ Z
quantum wells, whereby the dopants are introduced
! i; M# ]0 {1 ionly in the barrier regions, led to the possibility of preparing7 _7 h/ y7 j9 W/ {8 Q0 }' C
semiconductors with low-temperature carrier mobilities,
/ g6 Y2 U! d: }+ Vorders of magnitude greater than in the best) B/ a+ G0 K7 I) G# j5 v1 a
bulk semiconductors. These technological advances6 K; Y1 ~7 K# [3 s6 t5 v: f
soon led to the discovery of the quantum Hall effect, the/ ]: l6 r9 R/ `% i" Y' H/ N
fractional quantum Hall effect, and a host of new phenomena,
9 k) ^! T) d- L$ Y6 wsuch as Wigner crystallization, which continue; R, _ z& {; R! Y. ^# E. t$ z
to challenge experimentalists and theorists. Lithographic5 S& q( {) W- K0 u6 u
S334 P. Chaudhari and M. S. Dresselhaus: Materials physics
! O8 [. ~! O, [. w- I. R# vRev. Mod. Phys., Vol. 71, No. 2, Centenary 1999
! m: C [- a0 j4 @and patterning technologies developed for the semiconductor
. p6 i+ i$ F9 G! C& X3 M$ Oindustry have led to the discovery of the quantized% o! @" o; X8 C! h5 C
conductance for one-dimensional semiconductors
# f( u7 _ s' W* Y B c+ `* \and to the fabrication of specially designed semiconductor
/ Z6 Q+ L% I* r# U$ zdevices, in which the transport of a single electron7 P3 U6 W k7 j2 ]
can be controlled and studied. The ever decreasing size0 H$ q# J, G9 g- X% a# p
of electronic devices (now less than 0.2 microns in the
0 w) @( _* J/ A$ F; V% t" Rsemiconductor industry) is greatly stimulating the study
8 {7 k% k$ e4 Y4 D rof mesoscopic physics, in which carriers can be transported
4 J D% O; p0 E) [4 N0 f% J; d+ rballistically without scattering and the effect of* }9 z3 B/ Q* I* Z: y A$ {) Q- [2 S
the electrical leads must be considered as part of the! ~7 @$ b+ d5 D. g( \0 r
electronic system. New materials, such as carbon nanotubes' ?( T$ _( b( c; b8 R
with diameters of 1 nm, have recently been discovered,
) Q4 G; h, E# i4 G1 G( Z" }and junctions between such nanotubes are being
- m7 a- x* O! t& _! R- p+ @considered for possible future electronics applications! t/ y4 B; k% ^
on the nm scale, utilizing their unique one-dimensional
" q& @0 e) q& R3 I; F! J- ~# z3 B2 wcharacteristics.
$ I( l; ^# @( P. V! XThe electronic materials field today is highly focused
% H5 [* F4 J2 V% e7 D" {on the development of new materials with special properties
" r' J: v* @1 u1 f; n3 L2 k2 E8 Z. Bto meet specific needs. Advances in condensedmatter. `* S6 K% c/ \2 T* i0 I
physics offer the possibility of new materials! {+ s9 W3 d! U% U
properties. In photonics, new materials are providing increased) j& w* p( T$ M. [! Y
spectral range for light-emitting diodes, smaller
O6 X1 T0 y3 y& Hand more functional semiconducting lasers, new and improved
5 y F$ C) G6 o# e6 vdisplay materials. The new field of photonic1 ~+ v! ?" P' _/ z8 u
band-gap crystals, based on structures with periodic
3 l1 _: {( g+ G1 M" `variations in the dielectric constant, is just now emerging.
$ e9 L/ z0 r8 U* q6 |" rResearch on optoelectronic materials has been
! R6 B* K* W; z3 H, Z$ O7 J8 ogreatly stimulated by the optical communications industry, `: h2 o# G, o+ |
which was launched by the development of low-loss5 ^5 o! z8 I' O" N2 @, z2 g
optical fibers, amplifiers, and lasers.
3 L. z4 Q/ ~( Y$ S2 s) p; LFerroelectrics have become important for use as capacitors
3 ~- f9 V8 z, i' h* {5 S; R( ^+ K. P! ?and actuators, which are needed in modern robotics
+ S+ C; Z; P* K3 \applications, as are also piezoelectric materials,
& h" K" y0 J3 X5 i& H1 fwhich are critical to the operation of scanning tunneling
( S( }, Z, f I4 lprobes that provide information at the atomic level on$ q# \2 {( `2 F- u9 P% Y% n9 T
structure, stoichiometry, and electronic structure. The5 E0 p9 y* I7 g7 S
technological development of microelectromechanical" I& J) Q5 D% R' U1 q0 o
systems (MEMS), based on silicon and other materials,
8 \8 E& `/ x. L# D/ uis making possible the use of miniature motors and actuators
8 G. ~ G1 j" d- ^at the micrometer level of integrated circuits.
% v% }: w- E" K/ z4 c; iSome of these have already found applications, such as
1 \3 e: P( X( E0 `: Z* Jthe triggering mechanism for the release of airbags in) c/ G) P5 B2 J# V# o1 x" @
automobiles. Such developments are not only important
9 D, K- \, @1 Y' L' k1 L. bto the electronics industry, but are also having great impact
7 [( c+ Z! l- O+ C! Non fields such as astronomy and space science, f9 c, S0 o; I8 \
which are dependent on small, light-weight instruments
5 B4 d- B2 R+ Z1 ^! N" ? {3 m) h+ K5 Hwith enhanced capabilities to gather signals at ever increasing0 z; L, p5 ?1 e% Z! V
data rates and from ever increasing distances6 D# _6 X& z2 F; o, I3 o
from Earth. The developments in new materials and( U9 a5 h4 L; i$ Z. f
low-dimensional fabrication techniques have recently rejuvenated
2 j/ _" z! v" p/ E; }the field of thermoelectricity, where there is o T4 l3 l1 G( p: g) m! O& a
now renewed hope for enhanced thermoelectric performance
9 v2 T) h8 h4 z% t' O- w& Q4 rover a wider temperature range.; M( N9 _! C1 s6 m/ W# T
Research on magnetic materials has been strongly influenced
& q: [: |. R2 c; J4 Eby applications ranging from the development' b3 I& |! ~2 ?3 b2 t2 Q+ n
of soft magnetic materials (by the utilization of rapid! E8 K# \1 s; o0 s3 U9 Y2 q
solidification techniques) to hard magnetic materials' r4 W! a' L* q/ r9 U3 a9 L4 A
such as neodymium-iron-boron for use in permanent9 [( j9 t1 K9 S0 e
magnets. In the 1980s efforts focused on the development. L8 Q& s' L k9 ~& q+ Z2 f
of small magnetic particles for magnetic memory
- e$ D( _6 {/ L1 N* X0 c; hstorage applications. New magnetic materials, especially
U7 C, @! m, }# Bmagnetic nanostructures, are now an extremely active5 ~2 x! D5 u: l6 m9 w$ ]
research field, where the discovery of new phenomena
6 H+ R7 I# e$ Y( D! ^2 isuch as giant magnetoresistance and colossal magnetoresistance8 _3 N& P+ A( a! H5 k7 n
are now being developed for computer memory* k. v; c+ E' W. x/ p; h0 O/ Q
applications.
2 K! ~( ?# j* F+ ^. }The strong interplay between fundamental materials6 h' k; F0 F6 E
physics and applications is also evident in the area of/ X; n" Q0 d4 r, X$ g7 k
superconducting materials. Early use of superconducting
" W9 ]8 V8 \# e7 L# xmaterials was in the fabrication of superconducting magnets,$ ?2 l& g/ {* l: w. ?. `+ X
which in turn promoted understanding of type-II
% O( l/ c' \2 J; E$ {/ M, Lsuperconductors, flux dynamics, and flux pinning phenomena.
. `2 p d7 K7 ?; TThe discovery of the Josephson tunneling effect
- M8 i/ p: |) [" Z. u' ]9 jled to the development of the SQUID (superconducting2 H3 ~5 P w4 c' U1 U& @7 a. g
quantum interference device), which has5 A6 b! k6 y: c# a
become a standard laboratory tool for materials characterization
1 K# i1 A3 {$ h4 X2 S% ]7 Xand for the sensitive measurement of extremely
0 q' W7 v! I9 o3 M1 G' `small magnetic fields, such as the fields associated$ m$ `, |! v. r
with brain stimuli. The discovery of high-Tc
}" L" p/ P* ] [8 Gsuperconductivity in 1986 has revolutionized this field,5 I) \ v0 I( f2 ?' P" H
with much effort being devoted to studies of the mechanism/ k2 T- k6 j! ?. e8 `; d$ D+ w
for high-Tc superconductivity, along with efforts to
; E' ^. U+ r0 n; xdiscover materials with yet higher Tc and critical current
! Y, I) E9 G$ P- i' {# l& mvalues, to improve synthesis methods for the cuprate superconductors,
9 ^( v8 @3 W3 Q' |2 t& Dand to develop applications for these
5 P. X6 D% o8 X2 w2 h: c( W8 W3 }materials to electronics, energy storage, and highmagnetic-2 a9 T$ f' t# F, e5 {7 |9 L
field generation., Q) M8 q' I9 h) {9 S
When viewed from the perspective of time, the developments2 R* a- K7 x. U+ w
in electronic materials have been truly remarkable.
- Z; Y$ t8 N4 [7 K1 ^- A) oThey have generated businesses that approach a9 `# a; |7 P7 ~) W7 w n
trillion dollars, have provided employment to millions of
4 d! }- D) N3 y h$ R. o4 zworkers, either directly and indirectly associated with3 u0 M X; n! ]: E% q7 l+ t- _
these industries, and have enabled us, as humans, to extend
B# O0 ?- w, k1 W4 o0 x9 z- t0 Iour abilities, for example, in information gathering,7 i$ |. A b/ r& u8 x! l/ g. ?% Y; X
communication, and computational capabilities. Science* B; E. _1 v1 A/ P4 k4 U
has been the key to these marvellous developments, and7 \( w/ D* l$ b$ V2 m" J' @
in turn these developments have enabled us, as scientists,
1 j' t- h# s" P. C9 |to explore and understand the subtleties of nature.' y& n3 a. B" N: a+ `: k- U
V. SUMMARY
) J9 D5 p# o" Y" e" z4 AIn this very brief note, we have only touched on some N" y3 ~: Q+ j+ t# h! r
of the advances made in structural, polymeric, and electronic4 ^6 @/ E6 L- D. \6 `/ w
materials over the last century, showing how materials1 z5 z4 S, A/ i: {/ p' n
physics has played a central role in connecting
6 j1 {5 b6 @9 W) R! m' Mscience to technology and, in the process, revolutionized
' c, D: Z/ d, p0 o& ]1 uour lives.8 A7 J, C7 r; a
P. Chaudhari and M. S. Dresselhaus: Materials physics S335+ V) R/ O) S0 d$ a6 U
Rev. Mod. Phys., Vol. 71, No. 2, Centenary 1999 |
|