PHY605 notes Semiconductor Materials.docx

download PHY605 notes Semiconductor Materials.docx

of 39

Transcript of PHY605 notes Semiconductor Materials.docx

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    1/39

    MATERIALS,SEMICONDUCTOR MATERIALS,and MICROELECTRONICS

    Materials science..

    ..is primarily concerned with the search of basic knowledge about the internalstructure, properties, and processing of materials.

    Materials engineering..

    ..is mainly concerned with the use of fundamental and applied knowledge of

    materials so that the materials can be converted into products needed or desired by

    society.

    Materials science and engineering..

    ..combines both materials science and materials engineering.

    Types of aterials

    Most engineering materials are divided into three main or fundamental classes;

    Metallic materials

    Polymeric materials

    Page 1

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    2/39

    Ceramic materials

     Additional application classes;

    Composite materials

    Electronic materials

    Metallic materials..

    ..metals and metal alloys! are inorganic materials that are characteri"ed by high

    thermal and electrical conductivities. E#amples are iron, steel, aluminum, copper.

    Polymeric materials..

    ..are materials consisting of long molecular chains or network of low weight elements

    such as carbon, hydrogen, o#ygen, and nitrogen. Most polymeric materials have low

    electrical conductivities. E#amples are polyethylene, polyvinyl chloride pvc!.

    Ceramic materials..

    ..are materials consisting of compounds of metals and nonmetals. Ceramic materials

    are usually hard and brittle. E#amples are clay products, glass, and pure aluminum

    o#ide that has been compacted and densified.

    Page 2 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    3/39

    Composite materials..

    .. are materials that are mi#tures of two or more materials. E#amples are fiberglass

    reinforcing material in a polyester or epo#y matri#.

    Electronic materials..

    ..are materials used in electronics especially microelectronics. E#amples are silicon,

    gallium arsenide.

    Nanomaterials..

    ..are materials with a characteristic length scale smaller than $%% nm.

     

    Assignent !

    Consider a lig"t#$l#.

    %a& Identify 'ario$s critical coponents of a lig"t#$l#.

    %#& Deterine t"e aterial selected for eac" critical coponent.

    %c& Rationali(e )"y t"e aterial )as selected for eac" coponent.

    Page 3

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    4/39

    Seicond$ctor aterials..

    ..are nearly perfect crystalline solids with small amount of iperfections, such as

    impurity atoms, lattice vacancies, or dislocations, which are sometimes intentionally

    introduced to alter their electrical characteristics

     A summary of the chemical elements involved in the formation of semiconductors.

    &he semiconductors can be eleental, such as Si, *e, and other chemical

    elements from gro$p I+.

    &hey can be also copo$nd, a combination between elements from gro$p III and

    gro$p +, or respectively, fro gro$p II and gro$p +I. 

    Page 4

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    5/39

    E#amples for such combinations are the binary compounds *aAs and nS.

    &here are also several combinations of practical importance, which involve two or

    more elements from the same chemical group.

    'uch alloy seicond$ctors can be #inary e.g. 'i(e !, ternary e.g. Al(aAs !,

    -$aternary e.g. )n(aAsP!, and even pentanary (a)nP'bAs! materials.

    Electronic aterials include insulators, semiconductors, conductors, andsuperconductors.

    &his family of materials has truly revolutionali"ed the world. *rom spark plugs made

    from alumina, and copper wires for electrical transmission to components for

    wireless communications, high powered magnets used in magnetic resonance

    imaging, capacitors, inductors, solar cells, active matri# displays, silicon, and gallium

    arsenide based computer chips, electronic materials are found in countless numbers

    of applications.

    +ew advances in the materials sciences have led to several breakthroughs in the

    developement of new electronic materials. e now have ceramics that are not -ust

    e#cellent insulators, but also semiconductors and superconductors. 'imilarly, we

    now have polymers that are semiconductive and, more recently, a superconductive

    polymer has also been discovered.

    Page 5 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    6/39

    ©2003 Brooks/Cole, a division of Thomson Learning, Inc. Thomson Learning™ is a trademark sed herein nder lic

    Classification of technologically useful electronic materials.

    Page 6 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    7/39

    Page 7 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    8/39

    y alloying multiple compounds, some semiconductor materials are t$na#le, e.g., in

    band gap or lattice constant.

    &he result is ternary, /uaternary, or even /uinary compositions.

    Band gap..

    &ernary compositions allow ad-usting the band gap within the range of the involved

    binary compounds; however, in case of combination of direct and indirect band gap

    materials there is a ratio where indirect band gap prevails, limiting the range usable

    for optoelectronics; e.g. Al(aAs 0E1s are limited to 22% nm by this.

    Lattice constant..

    0attice constants of the compounds also tend to be different, and the lattice

    mismatch against the substrate, dependent on the mi#ing ratio, causes defects in

    amounts dependent on the mismatch magnitude; this influences the ratio of

    achievable radiative3nonradiative recombinations and determines the luminous

    efficiency of the device.

    Band gap and lattice constant..

    4uaternary and higher compositions allow ad-usting simultaneously the band gap

    and the lattice constant, allowing increasing radiant efficiency at wider range of

    wavelengths; for e#ample Al(a)nP is used for 0E1s .

    Materials transparent to the generated wavelength of light are advantageous, as this

    allows more efficient e#traction of photons from the bulk of the material. &hat is, in

    such transparent materials, light production is not limited to -ust the surface.

    Page 8 

    http://en.wikipedia.org/wiki/Band_gaphttp://en.wikipedia.org/wiki/Lattice_constanthttp://en.wikipedia.org/wiki/Light_emitting_diodehttp://en.wikipedia.org/wiki/Lattice_constanthttp://en.wikipedia.org/wiki/Light_emitting_diodehttp://en.wikipedia.org/wiki/Band_gap

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    9/39

    Silicon %Si& and *erani$ %*e&

    )n solid state electronics, either pure silicon or germanium may be used as the

    intrinsic semiconductor  which forms the starting point for fabrication. Each has four

    valence electrons, but germanium will at a given temperature have more free

    electrons and a higher conductivity.

    Silicon is by far the more widely used semiconductor for electronics, partly because

    it can be used at much higher temperatures than germanium.

    Page 9

    http://hyperphysics.phy-astr.gsu.edu/hbase/solids/sili.htmlhttp://hyperphysics.phy-astr.gsu.edu/hbase/solids/intrin.htmlhttp://hyperphysics.phy-astr.gsu.edu/hbase/solids/sili.htmlhttp://hyperphysics.phy-astr.gsu.edu/hbase/solids/sili.htmlhttp://hyperphysics.phy-astr.gsu.edu/hbase/solids/intrin.htmlhttp://hyperphysics.phy-astr.gsu.edu/hbase/solids/sili.html

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    10/39

    Si vs *aAs

    Compound semiconductors have both advantages and disadvantages.

    *or e#ample, galli$ arsenide (aAs! has si# times higher electron mobility thansilicon, which allows faster operation; wider band gap, which allows operation of

    power devices at higher temperatures, and gives lower thermal noise to low power

    devices at room temperature.

    1irect band gap gives compound semiconductors more favorable optoelectronic 

    properties than the indirect band gap of silicon; it can be alloyed to ternary and

    /uaternary compositions, with ad-ustable band gap width, allowing light emission at

    chosen wavelengths, and allowing e.g. matching to wavelengths with lowest losses

    in optical fibers.

    (aAs can be also grown in a semi5insulating form, which is suitable as a lattice5

    matching insulating substrate for (aAs devices.

    Conversely..

    Silicon is robust, cheap, and easy to process.

    whereas..

    *aAs is brittle and e#pensive, and insulation layers cannot be created by -ust

    growing an o#ide layer; (aAs is therefore used only where silicon is not sufficient.

    Page 10 

    http://en.wikipedia.org/wiki/Optoelectronichttp://en.wikipedia.org/wiki/Optoelectronic

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    11/39

    Silicon %Si& vs Silicon Car#ide %SiC&

    'iC devices belong to the so5called wide band gap semiconductor group,

    hen compared to commonly used silicon 'i!, 'iC offers a number of attractivecharacteristics for high voltage power semiconductors.

    Much higher breakdown field strength

    Much higher thermal conductivity

    thus allow creating devices which outperform by far the corresponding 'i ones, and

    enable reaching otherwise unattainable efficiency levels.

    Page 11

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    12/39

    Indi$ Arsenide %InAs&

    http://www.azom.com/article.aspx?ArticleI!"#$$ 

    Description

    )ndium arsenide is a semiconductor material made of arsenic and indi$.

    &he semiconductor has a melting point of 678 9C and appears in the form of grey

    crystals with a cubic structure.

    )t is very similar to gallium arsenide and is a material having a direct bandgap.

    )ndium arsenide is popular for its narrow energy bandgap and high electron mobility.

    Applications

    &he applications of indium arsenide are listed below:

    )ndium arsenide is used to construct infrared detectors for a wavelength range

    of $ ?m. &he detectors are normally photovoltaic photodiodes.

    1etectors that are cryogenically cooled have low noise but )nAs detectors can

    be used in high5power applications at room temperature also.

    1iode lasers are also made using indium arsenide.

    )ndium arsenide and gallium arsenide are similar and it is a direct bandgap

    material.

    )t is used as a terahert" radiation source.

    )t is possible to form /uantum dots in a monolayer of indium arsenide on

    gallium arsenide or indium phosphide

    )t is also possible to form /uantum dots in indium gallium arsenide in the form

    of indium arsenide dots arranged in the gallium arsenide matri#.

    Page 12 

    http://www.azom.com/article.aspx?ArticleID=8355http://www.azom.com/article.aspx?ArticleID=8355

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    13/39

    Toicity of indi$ arsenide, galli$ arsenide, and al$ini$ galli$ arsenide.ana!a ".%ource: #epartment o$ %ygiene& 'ra()ate *c+ool o$ Me(ical *ciences& ,y)s+) -niersity& %igas+i/!)& )!)o!a 812/8582& apan. atana!aeisei.me(.!y)s+)/).ac.p

    (allium arsenide (aAs!, indium arsenide )nAs!, and aluminium gallium arsenideAl(aAs! are semiconductor applications. Although the increased use of these

    materials has raised concerns about occupational e#posure to them, there is little

    information regarding the adverse health effects to workers arising from e#posure to

    these particles. @owever, available data indicate these semiconductor materials can

    be to#ic in animals.

     Although acute and chronic to#icity of the lung, reproductive organs, and kidney are

    associated with e#posure to these semiconductor materials, in particular, chronic

    to#icity should pay much attention owing to low solubility of these materials.

    etween )nAs, (aAs, and Al(aAs, InAs was the most to#ic material to the lung

    followed by (aAs and Al(aAs when given intra5tracheally. &his was probably due to

    difference in the to#icity of the counter5element of arsenic in semiconductor

    materials, such as indium, gallium, or aluminium, and not arsenic itself. )t appeared

    that indium, gallium, or aluminium was to#ic when released from the particles,

    though the physical character of the particles also contributes to to#ic effect.

     Although there is no evidence of the carcinogenicity of )nAs or Al(aAs, (aAs and

    )nP, which are semiconductor materials, showed the clear evidence of carcinogenic

    potential. )t is necessary to pay much greater attention to the human e#posure of

    semiconductor materials.

    Page 13

    http://www.ncbi.nlm.nih.gov/pubmed?term=Tanaka%20A%5BAuthor%5D&cauthor=true&cauthor_uid=15276420http://www.ncbi.nlm.nih.gov/pubmed?term=Tanaka%20A%5BAuthor%5D&cauthor=true&cauthor_uid=15276420

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    14/39

    Direct and Indirect /andgap Seicond$ctor 

    )n a direct #andgap semiconductor, an electron can be promoted from the

    conduction band to the valence band without changing the momentum of theelectron. An e#ample of a direct bandgap semiconductor is (aAs. hen the e#ited

    falls back into the valence band, electrons and holes combine to produce light.

    &hus, electron 0 "ole hν 

    &his is known as radiati'e reco#ination. &hus, direct bandgap materials such as

    (aAs and solid solutions of these e.g. (aAs5AlAs! are used to make light5emitting

    diodes 0E1s! of different colours. &he bandgap of semiconductors can be tuned

    using solid solutions. &he change in bandgap produces a change in the wavelength

    i.e. the fre/uency of the colour  ν) is related to the bandgap E  gas E  g  = hν, where h is

    the Planks constant!. 'ince an optical effect is obtained using an electronic material,

    often the direct bandgap materials are known as optoelectronic materials. Many

    lasers and 0E1s have been developed using these materials. 0E1s that emit light in

    the infrared range are used in optical5fiber communication systems to convert light

    waves into electrical pulses. 1ifferent coloured lasers, such as the newest blue laser

    using (a+, have been developed using direct bandgap materials.

    )n an indirect #andgap semiconductor e.g. 'i, (e, (aP! the electron5hole

    recombination is very efficient and the electrons cannot be promoted to the valence

    band without a change in momentum. As a result, in materials that have an indirect

    bandgap, we cannot get light emission. )nstead, electrons and holes combine to

    produce heat that is dissipated within the material. &hus, electron 0 "ole "eat. 

    &his is known as non1radiati'e reco#ination.

    +ote that both direct and indirect bandgap materials can be doped to form n5type or

    p5type semiconductors.

    Page 14

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    15/39

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    16/39

    Organic Lig"t Eitting Diode %OLED&

    B0E1 Brganic 0ight Emitting 1iodes! is a flat light emitting technology, made by

    placing a series of organic thin films between two conductors. hen electrical

    current is applied, a bright light is emitted. B0E1s can be used to make displays and

    lighting. ecause B0E1s emit light they do not re/uire a backlight and so are thinner 

    and more efficient than 0C1 displays which do re/uire a white backlight!.

    Page 16 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    17/39

    OLED 's LCD

    OLED displays "a'e t"e follo)ing ad'antages o'er LCD displays2

    0ower power consumption

    *aster refresh rate and better contrast

    (reater brightness 5 &he screens are brighter, and have a fuller viewing

    angle

    E#citing displays 5 new types of displays, that we do not have today,

    like ultra5thin, fle#ible or transparent displays

    etter durability 5 B0E1s are very durable and can operate in a

    broader temperature range

    0ighter weight 5 the screen can be made very thin, and can even be

    printed on fle#ible surfaces

    3lei#le and transparent OLED displays

    )t turns out that because B0E1s are thin and simple 5 they can be used to create

    fle#ible and even transparent displays.

    &his is pretty e#citing as it opens up a whole world of possibilities: Curved B0E1 displays, placed on non5flat surfaces

    earable B0E1s

    &ransparent B0E1s embedded in windows

    B0E1s in car windshields

    +ew designs for lamps

     And many more we cannot even imagine today...

    B0E1 video

    +ttps::.yo)t)e.com:atc+;y?9(*00 

    4+ideo %5yo$t$#e&1/enda#le sartp"onehttp:33ceramics.org3ceramic5tech5today3video5new5smartphone5prototype5bends5to5

    meet5consumers5needs

    1t"e 'erge

    Page 17 

    https://www.youtube.com/watch?v=QqyW9vdS0x0https://www.youtube.com/watch?v=QqyW9vdS0x0

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    18/39

    4uantum dot

     A /uantum dot is a seicond$ctor nanostr$ct$re that confines t"e otion of

    conduction band electrons, valence band holes, or e#citons bound pairs of

    conduction band electrons and valence band holes! in all three spatial directions.

    &he confinement can be due to..

    5 electrostatic potentials generated by e#ternal electrodes, doping, strain,

    impurities!

    5 the presence of an interface between different semiconductor materials

    e.g. in core5shell nanocrystal systems!

    5 the presence of the semiconductor surface e.g. semiconductor

    nanocrystal!

    5 ..or a combination of these.

     A /uantum dot has a discrete -$anti(ed energy spectr$.

    &he corresponding wave functions are spatially locali"ed within the /uantum dot, but

    e#tend over many periods of the crystal lattice.

     A /uantum dot contains a small finite number of the order of $5$%%! of conduction

    band electrons, valence band holes, or e#citons, i.e., a finite n$#er of eleentary

    electric c"arges.

    Page 18 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    19/39

    'mall /uantum dots, such as colloidal semiconductor nanocrystals, can be as small

    as 8 to $% nm, corresponding to $% to D% atoms in diameter and a total of $%% to

    $%%,%%% atoms within the /uantum dot volume. 'elf5assembled /uantum dots are

    typically between $% and D% nm in si"e.

    4uantum dots defined by lithographically patterned gate electrodes, or by etching on

    two5dimensional electron gases in semiconductor heterostructures can have lateral

    dimensions e#ceeding $%% nm.

     At $% nm in diameter, nearly = million /uantum dots could be lined up end to end and

    fit within the width of a human thumb.

    Note6  &he above te#t is e#cerpted from the ikipedia article 4uantum dot, which has been

    released under the(+F *ree 1ocumentation 0icense.

    Online so$rce 61

    1 7$ant$ dot slides 5 http:33www.slideshare.net3mcleang$3/uantum5dots

    7$ant$ dots article 61

    http:33nanotechweb.org3cws3article3yournews3=GDD%

    http:33nanotechweb.org3cws3article3tech37G2D=

    Page 19

    http://en.wikipedia.org/wiki/Quantum_dothttp://www.gnu.org/copyleft/fdl.htmlhttp://www.gnu.org/copyleft/fdl.htmlhttp://www.slideshare.net/mcleang1/quantum-dotshttp://nanotechweb.org/cws/article/yournews/37550http://nanotechweb.org/cws/article/tech/47653http://en.wikipedia.org/wiki/Quantum_dothttp://www.gnu.org/copyleft/fdl.htmlhttp://www.slideshare.net/mcleang1/quantum-dotshttp://nanotechweb.org/cws/article/yournews/37550http://nanotechweb.org/cws/article/tech/47653

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    20/39

    Silicon Car#ide Sc"ott8y Diodes

    &he differences in material properties between 'iC and silicon limit the fabrication of

    practical silicon unipolar diodes 'chottky diodes! to a range up to $%%H < $D%H, with

    relatively high on5state resistance and leakage current. Bn the other hand, 'iC

    'chottky barrier diodes '1! can reach a much higher breakdown voltage; )nfineon

    offers products up to $8%%H as discrete and up to $G%%H in modules.

    • Applications 

    • 'erver 

    • &elecom

    • 'olar 

    • FP'

    • PC 'ilverbo#

    • Motor 1rives

    • 0ighting

    3eat$res  /enefits 

    enchmark switching behavior 

    +o reverse recovery charge

    &emperature independent

    switching behavior 

    @igh operating temperature &  - 

    ma# $GD9C!

     

    'ystem efficiency improvement

    compared to 'i diodes

    Ieduced cooling re/uirements

    Enabling higher

    fre/uency3increased power

    density

    @igher system reliability due to

    lower operating temperature

    Ieduced EM)

    •   Diodes

    Page 20 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    21/39

      !  "  n  h  o   m  o #    n  c  t i  o  n  s

      !   $  e  t  e  r  o #    n  c  t i  o  n  s  !   %  e  t  a l &  s  e   m i  c  o  n  d    c  t  o  r

     #    n  c  t i  o  n  s

    Diodes

      !   %  e  t  a l &   '  ( i  d  e &  )  e   m i  c  o  n  d    c  t  o  r  *  +  T ,   %   '  )  *  +  T -

      ! .    n  c  t i  o  n  *  +  T , .  *  +  T -Field-efect

    transistors

      !   $  e  t  e  r  o #    n  c  t i  o  n  B i  "  o l  a  r  T  r  a  n  s i  s  t  o  r  s

    Bipolar junctiontransistor

    s

      !  )  o l  a  r  c  e l l  s  !  /  h  o  t  o  d  e  t  e  c  t  o  r  s  !  /  h  o  t  o l     m i  n  e  s  c  e  n  c  e  !  + l  e  c  t  r  o l     m i  n  e  s  c  e  n  c  e  !  L i  g  h  t &  e   m i  t  t i  n  g  d i  o  d  e  s  !  L  a  s  e  r  d i  o  d  e  s  ! I   m  a  g  e  s  e  n  s  o  r  s

    Optoelectronic

    Devices

    Diodes

    Page 21

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    22/39

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    23/39

    NANOTEC9NOLO*:

    Nanoaterials are defined as materials with at least one e#ternal dimension in the

    si"e range from appro#imately $5$%% nanometers.

    Nanoparticles are ob-ects with all three e#ternal dimensions at the nanoscale.

    Nanotec"nology encompasses the understanding of the fundamental physics,

    chemistry, biology and technology of nanometre5scale ob-ects.

    Nanoparticles can eit+er e..

    5 the naturally occurring

    e.g., volcanic ash, soot from forest fires!

    5 the incidental byproducts of combustion processes

    e.g., welding, diesel engines!

    5 are usually physically and chemically heterogeneous and often termed

    ultrafine particles.

    Engineered nanoparticles

    - are intentionally produced and designed with very specific properties related

    to shape, si"e, surface properties and chemistry.

    - &hese properties are reflected in aerosols, colloids, or powders.

    - Bften, the behavior of nanomaterials may depend more on surface area than

    particle composition itself.

    - Ielative5surface area is one of the principal factors that enhance its reactivity,

    strength and electrical properties.

    Engineered nanoparticles may be bought from commercial vendors or generated via

    e#perimental procedures by researchers in the laboratory.

    e.g., C+&s can be produced by laser ablation, @iPCB high5pressure carbon

    mono#ide, arc discharge, and chemical vapor deposition CH1!!.

    Page 23

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    24/39

    E#amples of engineered nanomaterials include..

    carbon buckeyballs or fullerenes; carbon nanotubes; metal or metal o#ide

    nanoparticles e.g., gold, titanium dio#ide!; /uantum dots, among many others.

    Researc" in t"e icroelectronics and nanotec"nology area includes topics such

    as..

    5 *abrication of new electronic materials and devices.

    5 Computational studies of electronic devices.

    Researc" in nanotec"nology in ot"er field of st$dies include..

    iology

    Medicine

    Environment

    Energy

    Electronics 5Patterning and *abrication

    Photonics

    'ensors

    Material 'ynthesis

    Material Properties and Characteri"ation

    Topics regarding nanotec"nology may cover..

    +ew materials fabrications

    +ew products applications

    Materials Characteri"ation

    Cleanrooms

    @ealth )ssues

    C+&

    B0E1

    4uantum 1ots

    MEM'

    'olar Cells

    Page 24

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    25/39

    @$rom articleA

    Nanotec"nology6 9ealt" iss$es

    Approac"es to Safe Nanotec"nology6 Managing t"e 9ealt" and Safety

    Concerns Associated )it" Engineered Nanoaterials

    &his document reviews what is currently known about nanoparticle toicity,

    process eissions and epos$re assessent, engineering controls, and

    personal protecti'e e-$ipent.

    &his updated version of the document incorporates some of the latest results of

    +)B'@ research, but it is only a starting point. &he document serves a dual purpose:

    it is a summary of +)B'@s current thinking and interim recommendations; and it is a

    re/uest from +)B'@ to occupational safety and health practitioners, researc"ers,

    prod$ct inno'ators and an$fact$rers, eployers, )or8ers, interest gro$p

    e#ers, and t"e general p$#lic to e#change information that will ensure that no

    worker suffers material impairment of safety or health as nanotechnology develops.

    ;otential 9ealt" Concerns

    &he potential for nanomaterials to enter the body is among several factors that

    scientists e#amine in determining whether such materials may pose an occupational

    health ha"ard. +anomaterials have the greatest potential to enter the body through

    the respiratory system if they are airborne and in the form of respirable5si"ed

    particles nanoparticles!. &hey may also come into contact with the skin or be

    ingested.

    ased on results from human and animal studies, airborne nanoparticles can be

    inhaled and deposit in the respiratory tract; and based on animal studies,

    nanoparticles can enter the blood stream, and translocate to other organs.

    E#perimental studies in rats have shown that e/uivalent mass doses of insoluble

    incidental nanoparticles are more potent than large particles of similar composition in

    Page 25 

    http://var/www/apps/conversion/tmp/scratch_5/nano%20-health%20NIOSH.pdfhttp://var/www/apps/conversion/tmp/scratch_5/nano%20-health%20NIOSH.pdfhttp://var/www/apps/conversion/tmp/scratch_5/nano%20-health%20NIOSH.pdfhttp://var/www/apps/conversion/tmp/scratch_5/nano%20-health%20NIOSH.pdf

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    26/39

    causing pulmonary inflammation and lung tumors. Iesults from in vitro cell culture

    studies with similar materials are generally supportive of the biological responses

    observed in animals.

    E#perimental studies in animals, cell cultures, and cell5free systems have shown that

    changes in the chemical composition, crystal structure, and si"e of particles can

    influence their o#idant generation properties and cytoto#icity.

    'tudies in workers e#posed to aerosols of some manufactured or incidental

    microscopic fine! and nanoscale ultrafine! particles have reported adverse lung

    effects including lung function decrements and obstructive and fibrotic lung diseases.

    &he implications of these studies to engineered nanoparticles, which may have

    different particle properties, are uncertain.

    Iesearch is needed to determine the key physical and chemical characteristics of

    nanoparticles that determine their ha"ard potential.

    ;otential Safety Concerns

     Although insufficient information e#ists to predict the fire and e#plosion risk

    associated with powders of nanomaterials, nanoscale combustible material could

    present a higher risk than coarser material with a similar mass concentration given

    its increased particle surface area and potentially uni/ue properties due to the

    nanoscale.

    'ome nanomaterials may initiate catalytic reactions depending on their composition

    and structure that would not otherwise be anticipated based on their chemical

    composition.

    Page 26 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    27/39

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    28/39

    from website!

    MEMS Tec"nology

    https:33www.mems5e#change.org3MEM'3what5is.html

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    29/39

    Bver the past several decades MEM' researchers and developers have

    demonstrated an e#tremely large number of microsensors for almost every possible

    sensing modality including temperature, pressure, inertial forces, chemical species,

    magnetic fields, radiation, etc. Iemarkably, many of these micromachined sensors

    have demonstrated performances e#ceeding those of their macroscale counterparts.

    &hat is, the micromachined version of, for e#ample, a pressure transducer, usually

    outperforms a pressure sensor made using the most precise macroscale level

    machining techni/ues. +ot only is the performance of MEM' devices e#ceptional,

    but their method of production leverages the same batch fabrication techni/ues used

    in the integrated circuit industry < which can translate into low per5device production

    costs, as well as many other benefits. Conse/uently, it is possible to not only achieve

    stellar device performance, but to do so at a relatively low cost level. +ot surprisingly,

    silicon based discrete microsensors were /uickly commercially e#ploited and the

    markets for these devices continue to grow at a rapid rate.

    More recently, the MEM' research and development community has demonstrated a

    number of microactuators including: microvalves for control of gas and li/uid flows;

    optical switches and mirrors to redirect or modulate light beams; independently

    controlled micromirror arrays for displays, microresonators for a number of different

    applications, micropumps to develop positive fluid pressures, microflaps to modulate

    airstreams on airfoils, as well as many others. 'urprisingly, even though these

    microactuators are e#tremely small, they fre/uently can cause effects at the

    macroscale level; that is, these tiny actuators can perform mechanical feats far larger than their si"e would imply. *or e#ample, researchers have placed small

    Page 29

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    30/39

    microactuators on the leading edge of airfoils of an aircraft and have been able to

    steer the aircraft using only these microminiaturi"ed devices.

     A surface micromachined electro5statically5actuated micromotor fabricated by the M+L. &his

    device is an e#ample of a MEM'5based microactuator.

    &he real potential of MEM' starts to become fulfilled when these miniaturi"ed

    sensors, actuators, and structures can all be merged onto a common silicon

    substrate along with integrated circuits i.e., microelectronics!. hile the electronics

    are fabricated using integrated circuit )C! process se/uences e.g., CMB', ipolar,

    or )CMB' processes!, the micromechanical components are fabricated using

    compatible micromachining processes that selectively etch away parts of the

    silicon wafer or add new structural layers to form the mechanical and

    electromechanical devices. )t is even more interesting if MEM' can be merged not

    only with microelectronics, but with other technologies such as photonics,

    nanotechnology, etc. &his is sometimes called Jheterogeneous integration.K Clearly,

    these technologies are filled with numerous commercial market opportunities.

    hile more comple# levels of integration are the future trend of MEM' technology,

    the present state5of5the5art is more modest and usually involves a single discrete

    microsensor, a single discrete microactuator, a single microsensor integrated with

    electronics, a multiplicity of essentially identical microsensors integrated with

    electronics, a single microactuator integrated with electronics, or a multiplicity of

    essentially identical microactuators integrated with electronics. +evertheless, as

    Page 30 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    31/39

    MEM' fabrication methods advance, the promise is an enormous design freedom

    wherein any type of microsensor and any type of microactuator can be merged with

    microelectronics as well as photonics, nanotechnology, etc., onto a single substrate.

     A surface micromachined resonator fabricated by the M+L. &his device can be used as both

    a microsensor as well as a microactuator.

    &his vision of MEM' whereby microsensors, microactuators and microelectronics

    and other technologies, can be integrated onto a single microchip is e#pected to be

    one of the most important technological breakthroughs of the future. &his will enable

    the development of smart products by augmenting the computational ability of

    microelectronics with the perception and control capabilities of microsensors and

    microactuators. Microelectronic integrated circuits can be thought of as the brains

    of a system and MEM' augments this decision5making capability with eyes and

    arms, to allow microsystems to sense and control the environment. 'ensors gather 

    information from the environment through measuring mechanical, thermal, biological,

    chemical, optical, and magnetic phenomena. &he electronics then process the

    information derived from the sensors and through some decision making capability

    direct the actuators to respond by moving, positioning, regulating, pumping, and

    filtering, thereby controlling the environment for some desired outcome or purpose.

    *urthermore, because MEM' devices are manufactured using batch fabrication

    techni/ues, similar to )Cs, unprecedented levels of functionality, reliability, and

    sophistication can be placed on a small silicon chip at a relatively low cost. MEM'technology is e#tremely diverse and fertile, both in its e#pected application areas, as

    Page 31

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    32/39

    well as in how the devices are designed and manufactured. Already, MEM' is

    revolutioni"ing many product categories by enabling complete systems5on5a5chip to

    be reali"ed.

    +anotechnology is the ability to manipulate matter at the atomic or molecular level to

    make something useful at the nano5dimensional scale. asically, there are two

    approaches in implementation: the top5down and the bottom5up. )n the top5down

    approach, devices and structures are made using many of the same techni/ues as

    used in MEM' e#cept they are made smaller in si"e, usually by employing more

    advanced photolithography and etching methods. &he bottom5up approach typically

    involves deposition, growing, or self5assembly technologies. &he advantages of

    nano5dimensional devices over MEM' involve benefits mostly derived from the

    scaling laws, which can also present some challenges as well.

     An array of sub5micron posts made using top5down nanotechnology fabrication methods.

    'ome e#perts believe that nanotechnology promises to:

    a!. allow us to put essentially every atom or molecule in the place and position

    desired < that is, e#act positional control for assembly,

    b!. allow us to make almost any structure or material consistent with the laws of 

    physics that can be specified at the atomic or molecular level; and

    c!. allow us to have manufacturing costs not greatly e#ceeding the cost of the

    re/uired raw materials and energy used in fabrication i.e., massive

    parallelism!.

     Although MEM' and +anotechnology are sometimes cited as separate and distinct

    technologies, in reality the distinction between the two is not so clear5cut. )n fact,

    these two technologies are highly dependent on one another.

    Page 32 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    33/39

    &he well5known scanning t$nneling1tip icroscope %STM& which is used to detect

    individual atoms and molecules on the nanometer scale is a MEM' device.

     A colori"ed image of a scanning5tunneling microscope image of a surface, which is a

    common imaging techni/ue used in nanotechnology.

    'imilarly the atoic force icroscope %A3M& which is used to manipulate the

    placement and position of individual atoms and molecules on the surface of a

    substrate is a MEM' device as well. )n fact, a variety of MEM' technologies are

    re/uired in order to interface with the nano5scale domain.

    0ikewise, many MEM' technologies are becoming dependent on nanotechnologies

    for successful new products. *or e#ample, the crash airbag accelerometers that are

    manufactured using MEM' technology can have their long5term reliability degraded

    due to dynamic in5use stiction effects between the proof mass and the substrate. A

    nanotechnology called 'elf5Assembled Monolayers 'AM! coatings are now

    routinely used to treat the surfaces of the moving MEM' elements so as to prevent

    stiction effects from occurring over the products life.

    Many e#perts have concluded that MEM' and nanotechnology are two different

    labels for what is essentially a technology encompassing highly miniaturi"ed things

    that cannot be seen with the human eye. +ote that a similar broad definition e#ists in

    the integrated circuits domain which is fre/uently referred to as microelectronics

    technology even though state5of5the5art )C technologies typically have devices with

    dimensions of tens of nanometers. hether or not MEM' and nanotechnology are

    one in the same, it is un/uestioned that there are overwhelming mutual

    dependencies between these two technologies that will only increase in time.

    Perhaps what is most important are the common benefits afforded by these

    Page 33

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    34/39

    technologies, including: increased information capabilities; miniaturi"ation of

    systems; new materials resulting from new science at miniature dimensional scales;

    and increased functionality and autonomy for systems.

    Page 34

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    35/39

    Cleanroo

    @$rom esiteA

    Cleanroom +ttp::.a(ancetecllc.com:nanotec+nologyBmicroelectronics.+tml 

    Whether you require a 1,000 square foot Class 100 cleanroom or a fully functional volume

     production fab, Advance!C can address your critical requirements for contamination

    control, code compliance, and process tool fit-up " installation#

    $ur Approach

    Advance!C provides comprehensive cleanroom desi%n and cleanroom construction

    capabilities to serve &anotech and 'emiconductor clients# We understand the technical

    challen%es of these facilities, and deploy the capabilities required to ensure your success#

    Requirements

    GatheringDesign and Engineering

    Construction

    Management

    • (rocess utility

    studies

    • Code compliance

    evaluations

    • Chemical and %as

    stora%e and distribution

     plans

    • *AC, mechanical

    and e+haust systems

    • !stimatin%,

     bud%etin% and schedule

    development

    • (rocess tool

    infrastructure and services

    inte%ration

    • Conceptual desi%n,

     pro%rammin% and layout

    • esi%n for

    constructability and

    maintainability

    • ud%et creation and

    schedule optimi.ation

    • !+perienced,

    salaried (ro/ect and

    Construction ana%ement

    • Clean uild

    (rotocol construction

    • Commissionin%,

    certification and trainin%

    • (rocess tool fit-up

    and hoo-up

    • 'ite safety

    Our Experience

    Advance!C has a proven trac record of addressin% diverse mechanical, architectural and

     process utility requirements of leadin% ed%e &anotech and 'emiconductor cleanrooms#

    Applications

    Design Approach Facility Types

    • Ba 4 chase vs. allroom

    • *an *ilter 5nit **5- vs. Terminal $+6

    • lenm modle, 7sh grid,

    • 849 a""lications las

    •  Trace metals cleanrooms

    ilot lines• $igh volme 1afer fas

    Page 35 

    http://www.advancetecllc.com/nanotechnology_microelectronics.htmlhttp://www.advancetecllc.com/nanotechnology_microelectronics.html

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    36/39

    Design Approach Facility Types

    rod hng T&grid ceilings

    • 8aised access 7oors vs.

    other 7ooring sstems• 8'/9I 1ater sstems

    • $% evalation, design andmanagement

    • )cred e(hast sstems

    •  To(ic gas monitoring and life

    safet

    • )fas, chemical nkersand distrition centers

    •  Test 7oors and :nal

    "ackaging

    • %'C;9 las•  T+%/)+% rooms

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    37/39

    @$rom articleA

    Nanotec"nology %CNT& in Ci'il>Str$ct$ral Engineering

    +anoscience and nanotechnology provide enormous opportunities to engineers theproperties of materials by )or8ing in atoic or olec$lar le'el.

    )t has not only facilitated to o'ercoe any liitations of con'entional

    aterials, but also treendo$sly ipro'ed t"e ec"anical, p"ysical and

    c"eical properties of t"e aterials as well.

    &o develop "ig" perforance, $ltif$nctional, ideal %"ig" strengt", d$ctile,

    crac8 free, d$ra#le& constr$ction aterial, carbon nanotubes C+&s! show

    promising role to odify>en"ance t"e c"aracteristics of t"e con'entional

    constr$ction aterials s$c" as concrete and steel.

    )n the paper, a brief on geometry and mechanical properties, synthesis processes,

    possibilities and findings of different researchers on CNT reinforced coposites is

    presented. )t is also brought out that a crac8 free d$ra#le concrete is possible if

    certain issues such as uniform distribution of C+& in composite and bond behavior of 

    C+& modified concrete can be addressed. *inally, few pre5proof of concepts are

    mentioned where C+&s can play the pivotal role to redefine the scope and ability of

    civil engineering, in general, and structural engineering, in particular.

    Nanoscience +as pae( t+e ay to tailor t+e properties o$ materials ase( on

     partic)lar re>)irement y or!ing in atomic or molec)lar leel. n general&

    nanotec+nology is not an isolate( tec+nology $or certain p)rposes& )t it is an

    enaling tec+nology to ac+iee many goals y engineering a material at nano leel.

    *imilar to t+e $iel(s li!e energy& me(icine& electronics& etc.& nanotec+nology s+os

    remar!ale potentiality o$ its role to play y opening a ne ay to sole many o$ t+e

     perennial prolems ciil engineers (o $ace eery (ay. "ggressie (eelopment o$

    in$rastr)ct)res )sing conentional constr)ctional materials ill e responsile $or

    appro. one/t+ir( o$ gloal arming. t is estimate( t+at per ton pro()ction o$ cement 

    approimately pro()ces one ton o$ C2. %ence& t+ere is an alarming nee( $or

    (eeloping ne constr)ction material +ic+ is smart& e$$icient an( s)stainale. +e

    Page 37 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    38/39

    co)ntries li!e n(ia& +ere grot+ o$ in$rastr)ct)re plays a signi$icant role in t+e

    grot+ o$ t+e co)ntry& engineering o$ green an( smart constr)ction material ill

    enormo)sly +elp to generate p)lic& priate& strategic an( societal goo(s. "mong all

    t+e nano $orms o$ metals an( non/metals& caron nanot)es @CNsA seem to +ae

    t+e most promising role toar(s (eeloping an i(eal @+ig+ strengt+& ()ctile& crac!

    $ree& ()raleA constr)ction material li!e concrete. +e caron nanot)es @CNsA

    attract t+e researc+ers since t+eir (iscoery& eca)se o$ t+eir +ig+er strengt+ an(

    relatiely lo eig+t. +ese nanot)es are )se$)l $or any application +ere

    ro)stness an( $leiility are necessary. )rt+er& nanot)es are also stale )n(er

    etreme c+emical enironments& +ig+ temperat)res an( moist)re as ell. -se o$

    nano engineere( concrete o)l( lea( to consi(erale re()ction in t+e (imensions o$ 

    t+e str)ct)ral memers +ic+ co)l( res)lt in m)c+ less cons)mption o$ cement an(

    t+erey re()ction o$ C2 release an( ma!e t+e orl( s)stainale t+ro)g+ eco/

    $rien(ly pro()cts. )rt+er& caron nanot)es can also e )se( to ma!e nano

    composite steel. nitial researc+ $in(ings reeal t+at t+ey are ao)t 50 times stronger 

    an( 10 times lig+ter t+an conentional steel. "part $rom tec+nical intricacies an( lac! 

    o$ in$ormation& one o$ t+e main ostacles in )sing CNs in constr)ction is cost o$

    CNs as constr)ction materials nee( to e pro()ce( in mass an( s+o)l( e

    reasonaly c+eap. Eoritant cost implications in pro()ction o$ CNs are (iminis+ing 

    ery $ast. or eample& cost o$ in()strial CN as D27&000:l in 1992& D550:l in

    2006 an( D120:l in 2011. t is also pre(icte( t+at t+e price o)l( e as lo as

    D0.5:l in 201314 1F. o ring o)t t+e est $rom caron nanot)es to t+e

    constr)ction in()stry& speci$ically& in )sage o$ constr)ction materials& t+e

    etraor(inary geometrical s+ape& )nparallel mec+anical properties& comple )t

    c+allenging synt+esis processes& an( proale areas o$ applications are essential to

    e !non. +ere$ore& an oerie o$ t+ese aspects o$ caron nanot)es it+ t+e

    c)rrent state o$ !nole(ge is ro)g+t o)t in t+e present paper.

    Page 38 

  • 8/18/2019 PHY605 notes Semiconductor Materials.docx

    39/39