Chp 13 Electrical Properties

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    ISSUESTOADDRESS...

    CHAPTER13:

    ELECTRICALPROPERTIES

    Howareelectricalconductanceandresistance

    characterized?

    Whatarethephysicalphenomenathatdistinguish

    conductors,semiconductors,andinsulators?

    Formetals,howisconductivityaffectedby

    imperfections,T,anddeformation?

    Forsemiconductors,howisconductivityaffected

    byimpurities

    (doping)

    and

    T?

    ScanningelectronmicroscopeimagesofanIC:

    Al

    Si

    (a)(d)

    VIEW

    OF

    AN

    INTEGRATED

    CIRCUIT

    AdotmapshowinglocationofSi(asemiconductor):

    Sishowsupaslightregions.

    0.5mm45m

    (doped)

    (b)

    Alshowsupaslightregions.

    Fig.(a),(b),(c)fromFig.18.0,

    Callister6e.

    Fig.(d)fromFig.18.25,Callister6e.(Fig.18.25iscourtesy

    NickGonzales,NationalSemiconductorCorp.,WestJordan,

    UT.)

    (c)

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    Ohm's Law:V

    =

    I R

    voltagedrop(volts) resistance(Ohms)

    current(amps)

    ELECTRICALCONDUCTION

    VIe-

    A(crosssect.area)

    L

    Resistivity, andConductivity,:geometryindependentformsofOhm'sLaw(recallnormalizationwith)

    V IE:electric resistivit

    LA

    field

    intensity

    (Ohmm)

    J:currentdensity

    I

    conductivity

    Resistance:

    R

    L

    A

    L

    A

    Silver 6.8 x 107

    METALS

    Soda-lime glass 10-10

    CERAMICSconductors

    RoomTvalues(Ohmm)1

    CONDUCTIVITY: COMPARISON

    -14

    Copper 6.0 x 107

    Iron 1.0 x 107

    -4

    SEMICONDUCTORS

    Concrete 10-9

    Aluminum oxide

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    100m

    Cu wire I = 2.5A- +e-

    EX: CONDUCTIVITYPROBLEM

    Whatistheminimumdiameter(D)ofthewiresothat

    V

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    Metalsaregoodconductors

    sincetheirvalencebandisonly

    partiallyfilled.

    Metals: Thermalenergyputs

    manyelectronsinto

    a hi her ener state.

    +-

    -

    CONDUCTION&ELECTRONTRANSPORT

    eeeqn ne =#ofe

    qe =Chargeofe

    =E mobility

    EnergyStates:

    thecasesbelow

    formetalsshow

    thatnearby

    energystates

    Energy

    filled

    emptyband

    s

    Energy

    partlyfilled

    emptyband

    GAPMylevel

    highest

    filledstate

    are

    access ebythermal

    fluctuations.

    filledband

    valenceband

    filledstate

    filledband

    va enceband

    filledstates

    Fermihttp://www.bayarea.net/~kins/

    AboutMe/GIFs/Fermi_2.jpg

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    Insulators:Higherenergystatesnot

    accessible dueto a .

    Semiconductors:Higherenergystates

    separatedbyasmallergap.

    ENERGYSTATES: INSULATORSAND

    SEMICONDUCTORS

    Energy

    filled

    emptyband

    es

    GAP

    Energy

    filled

    emptyband

    es

    GAP?Engineered

    material:Gaps

    aretunable

    moretocome

    filledband

    band

    filled

    sta

    filledband

    va enceband

    filled

    stat

    Insulators: Aparallelplatecapacitorinvolvesaninsulator,ordielectric,between

    two

    metal

    electrodes.

    The

    charge

    density

    buildup

    at

    the

    capacitor

    surface

    is

    related

    to

    thedielectricconstant ofthematerial

    E,Electricfieldstrength(V/m)

    o

    D,charge

    density(C/m2)

    o electricpermittivityinvacuum,

    constant 8.9x1012C Vm

    k,dielectricconstant

    (materialproperty)

    ko electricpermittivity

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    Imperfectionsincreaseresistivitygrainboundaries

    dislocations

    impurityatoms

    Theseacttoscatterelectronssothatthey

    takealessdirectpath.

    METALS: RESISTIVITYVST,IMPURITIES

    vacancies

    Cu+3

    .32at%

    Ni

    Cu+2

    .16at%

    Ni

    eforme

    dCu+

    1.12a

    t%Ni

    3

    4

    5

    6

    esistivity,

    0-8Ohm-m)

    at%Ni

    )](1[ rto TT temperaturecoefficient ofresistivity,o is

    intrinsic(noimpurity)resistivity

    T (C)-200 -100 0

    1R(1

    0

    Cu+.

    Pure

    Cu

    increaseswith:temperature

    wt%impurity

    %CWAdaptedfromFig.18.8,Callister 6e. (Fig.18.8adaptedfromJ.O.Linde,

    Ann.Physik5,p.219(1932);andC.A.WertandR.M.Thomson,Physicsof

    Solids,2nded.,McGrawHillBookCompany,NewYork,1970.)

    Why????

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    Variationinelectricalresistivitywithcompositionforvariouscopperalloyswithsmalllevelsof

    elementaladditions.AlldataareatfixedT(20C).

    xo 1o resistivityofpuremetal

    slope

    x amtofalloy(impurity)addition

    DataforPureSilicon:

    increaseswithT

    oppositetometalsundoped e

    Egap /kT

    Energy

    PURESEMICONDUCTORS: CONDUCTIVITYVST

    Arrheniuseq.!

    filled

    filledvalenceband

    emptyband

    filledstates

    GAP?

    electrons

    cancross

    gapat

    higherT

    e ec r ca con uc v y,

    (Ohm-m)-1

    100

    101

    102

    103

    104

    pure

    material

    Si

    Ge

    GaP

    CdS

    bandgap(eV)

    1.11

    0.67

    2.25

    2.40

    AdaptedfromFig.19.15,Callister5e. (Fig.19.15adapted

    fromG.L.PearsonandJ.Bardeen,Phys.Rev.75,p.865,

    1949.)

    SelectedvaluesfromTable

    18.2,Callister6e.

    50 100 100010-2

    10-1(undoped)

    T(K)

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    CONDUCTIONINTERMSOFELECTRONANDHOLEMIGRATION

    Light(shown),heat,

    ElectricalConductivitygivenby:3

    toexcitee from

    valencebandto

    conductionband

    Conductioncanbeeitherbynegativecarriers,

    nee peh

    #electrons/m 3 electronmobility

    holemobility

    electrons(ntype)and/orpositivecarriers,holes(ptype).

    Electronsmovetowards(+)potentialandholesmoveto()potential

    kT

    Eg

    oe 2

    Arrheniusequation;Why2? Producetwo

    chargecarriers electronandhole

    mxBy

    Tk

    E

    e

    g

    o

    Tk

    E

    o

    g

    1

    2lnln

    1

    2

    Determiningtheactivationenergyforconduction

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    Intrinsicsemiconductors: #ofthermallygeneratedelectrons=

    #of

    holes

    (broken

    bonds)

    INTRINSICVSEXTRINSICCONDUCTION

    x r ns csem con uc ors: mpur esa e o esemiconductorthatcontributetoexcesselectronsorholes.Doping=intentionalimpurities

    Siisthemainmaterialinsemiconductors Largebandgap(1.1eV);allowsSitooperateatwarmertemperatures(150oC) Canformanativeoxide,SiO2,forinsulatingbarriers(importantinfabrication)

    Sicanbemadeintolarge(12inchdia.),highpurity,singlecrystalingots. Czochralski method. Wafersarecutfromtheingot

    DopingofSi Sihas4outershellelectrons ntype:Phosphorous,arsenic(groupV),donateextraelectron ptype:boron(groupIII)forSi

    ntype

    4valenceelectronsofAsallowittobondlikeSi,butthefifthelectronisleftorbitingAs

    site theenergytoreleasethefifthelectronintotheCBissmall

    nee kT

    EEg

    o

    d

    e)(

    Eg isbottomofconductionband

    Ed isthedonorlevelArrheniusequation,again!

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    ptype

    Boron

    has

    only

    3

    valance

    electrons.

    When

    it

    substitutes

    for

    a

    Si

    atoms,

    one

    of

    its

    bonds

    haveamissingelectron(hole)

    Holetunnelsaround,andcanbelibratedbythermalvibrationofSiatoms,fromtheB

    siteintotheVB.

    p eh

    kTE

    o

    a

    e

    ptype

    ntype

    ?type

    ?type

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    Arrheniusplotofelectricalconductivityforanntype

    semiconductoroverawide

    temperaturerange.Atlowtemperatures(high1/T),thematerialisextrinsic.Athightemperatures(low1/T),thematerialisintrinsic.Inbetweenistheexhaustion

    range,inwhichallextra

    electronshavebeenpromoted

    why?

    why?

    CompoundSemiconductors

    GroupIIIVandIIVcompoundsnominallyhave

    theZincBlendstructureandareintrinsic

    semiconductors.Can

    be

    doped,

    like

    Si,

    to

    change

    conduction(extrinsic)

    MXCompounds:GroupIII3+valence,GroupV

    5+valence avg.of4+valenceperatom//

    GroupII2+valence,GroupVI6+valence avg.4

    valenceperatom

    Applications:

    Solarcells

    Lightemittingdiodes(occurswith

    electronholerecombination)

    Higheroperationspeeds,etc.

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    Allowsflowofelectronsinonedirectiononly (e.g.,useful

    toconvert

    alternating

    current

    to

    direct

    current).

    Processing: diffusePintoonesideofaBdopedcrystal.

    Results: - -

    ICDEVICES:PNRECTIFYINGJUNCTION

    Noappliedpotential:

    nonetcurrentflow.

    Forwardbias: carrier

    flowthroughptypeand

    ntyperegions;holesand

    electronsrecombineat

    ++

    +

    +

    -

    -

    --

    -

    ++

    ++

    +

    ---

    --

    p-type n-type+ -

    14

    .

    Reversebias: carrier

    flowawayfrompnjunction;

    carrierconc.greatlyreduced

    atjunction;littlecurrentflow.

    +++

    +

    +

    --- --

    p-type n-type- +

    PN

    Rectifying

    Junction

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    LightEmittingDiode(LED)

    http://electronics.howstuffworks.com/led.htm/printable

    http://spie.org/Images/Graphics/Newsroom/Importe

    d/0695/0695_fig4.jpg

    Bandgapdetermines

    light,viaDeBoglie

    equation=h/(mv)

    TheTransistor

    InventedbyShockley,Bardeen,

    andBrattainin1948.Nobelprize

    in1956.

    Athreeterminaldevicethatacts

    likeasimpleonoffswitch.

    ThebasisofIntegratedCircuits(IC)

    technology

    Computers,cellphones,

    automotivecontrol,etc.

    Ifvoltage(potential)appliedto

    the ate,currentflowsbetween

    thesource

    and

    the

    drain.

    On/offswitch logicswitch,

    go/nogo

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    Howtodoweprocessthematerials?

    Features?

    Controlling

    oxide

    thickness?

    MakingSintype?MakingSiptype?

    FabricatingSingleCrystal,HighPuritySi

    Czochralski method Zonerefining

    http://www.mindfiesta.com/images/article/Metallurgy_clip_image003_0002.gif

    ls CCK /K=segregationcoefficient

    C=concentrationofimpuritiesinsolidand

    liquidMoresoluterejected asTdecreases

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    Cleanrooms

    Featuresbeingmadeare

    submicron

    DUST

    is

    your

    enemy! Candestroyentire

    waferofmulti le rocessors

    Cleanroomclassification

    http://docs.engineeringtoolbox.com/documents/933/cleanroomclass

    particlesizediagramISO.png

    http://zedomax.com/blog/wp

    content/uploads/2009/12/silico

    nwafer.jpg

    http://philip.greenspun.com/images/pcd0094/microdisplaycleanroom

    31.3.jpg

    Turbulentflow Laminarflowhttp://en.wikipedia.org/wiki/Cleanroom

    Oxidation

    Oxidation =growthofanoxidelayerbythereactionofoxygenwiththesubstrate

    Providesdopant maskinganddeviceisolation

    ICtechnologyuses

    Thermalgrownoxidization(dry)

    O2richenvironment,7501100oC,

    largebatchprocess(150+wafers)

    Si+O2 SiO2 Wetoxidation

    Si+H O SiO +2H

    Highergrowthrates,lowoxidedensity(lowerdielectricproperties)

    Selectiveoxidation:Useofsiliconnitridetopreventoxidationinspecificregions

    http://www.semi.org/cms/groups/pu

    blic/documents/web_content/~expor

    t/CTR_032685~1~000086~DC_SNIPPE

    T_LAYOUT/866811.jpg

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    Lithography

    Lithography =processbywhich

    geometricpatternsaretransferredfromamask(reticle)

    toasurfaceofachiptoformthe

    .

    Mooreslaw(1965)

    Linewidth =widthofsmallest

    featureobtainableonSisurface

    (dependent)

    Photoresist (PR)=lightsensitivepolymermaterial Patternsareimprintedusingphotoresist

    Positiveresist =the

    portion

    of

    the

    photoresist that

    is

    exposedtolightbecomessolubletothephotoresistdeveloperandtheportionofthephotoresist thatisunexposedremainsinsolubletothephotoresistdeveloper(exposed,removed)

    Negativeresist =unexposed(uncrosslinked)portionofthephotoresist isdissolvedbythephotoresistdeveloper (exposed,staysput)

    Whytheyellowlight?ICFeatureMaking

    (1) PRspunontowaferandprebaked(driveoffsolvents)(2) Alignmask,usingastepper,overthesubstrate(PR).Maskis

    steppedoverthewaferandexposedtoUV makingseveralpatterns(devices)onasinglewafer(registration)

    (3) Postbake hardenedtheresistthatisexposedtoUV.Regionnotcoveredbyresistisimplantedoretchedaway.

    (4) ResistisstrippedawaybyawetstripperorO2 plasma(ashing).Lithographypatternedmanytimeswithdifferentmasks.

    http://www.anl.gov/Media_Center/ArgonneNow/Fall_2006

    /Center_for_Nanoscale_Materials.html

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    Etching

    Wet:isotropic,undercut Dry:anisotropic,directional

    (Cl andFbasedgasremoval)

    IonImplantation(Doping)

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    pnDiodeFab Steps

    p

    n

    Diode

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    Metallization

    Metallization =growing

    interconnectionsto

    (a)

    connec ev ces

    Lowelectricalresistance,

    goodadhesionto

    dielectricinsulators

    Electromigration =rocessb whichmetal

    atomsdiffusebecauseof

    apotential.

    Not

    good

    a

    materialsresearcharea!

    FilmDeposition

    Tobuildadevice,variousthinmetalorinsulatingfilmsaregrownontopofeachother

    Evaporation

    Sputtering

    Evaporation

    MBE

    Sputtering

    CVD(ALD)

    CVD

    http://www rpl.stanford.edu/user/files/www/ald1.gif

    MBEhttp://www.sandia.gov/media/NewsRel/NR2000/images/jpg/MBE.jpg

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    WireBondingandPackaging

    (a) (b) (c)

    LargelydeterminestheoverallcostofIC

    Massproduced,notindividuallypackaged

    Packages:polymers,metals,ceramics

    Yieldand

    Reliability

    Yield=ratiooffunctionalchipstototal#ofchips ,

    processing

    ReliabilityNodevicehasinfinitelifetime.Statisticalmethodsto

    predictexpectedlifetime

    Failuremechanisms

    Oxidelayers(dielectricbreakdown)

    Lithography(unevenfeaturedefintion)

    Metallayers(poorconnections)

    Lossofpackagehermeticity

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    Electricalconductivity andresistivity are:

    material

    parameters.

    geometryindependent.

    Electrical resistance is:

    SUMMARY

    ageometryandmaterialdependentparameter.

    Conductors,semiconductors, andinsulators...

    differentinwhetherthereareaccessibleenergy

    statesforconductanceelectrons.

    Formetals,conductivityisincreasedby

    reducingdeformation

    reducingimperfections

    decreasingtemperature.

    Forpuresemiconductors,conductivityisincreasedby

    increasingtemperature

    doping(e.g.,addingBtoSi(ptype)orPtoSi(ntype).