Electronic Devices Optoelectronics

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    OPTOELECTRONIC DEVICES

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    Light Emitting

    Diodes

    Red LED White LED

    LED for displays Blue LED LED for traffic light

    LEDs

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    OPTOELECTRONIC DEVICES

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    DIODE LASERS

    Diode lasers have been used for cutting,

    surgery, communication (optical fibre),

    CD writing and reading etc

    http://www.semiconductor-technology.com/projects/iqe/index.htmlhttp://photos4.flickr.com/6933867_7223c5b695.jpg
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    Producing Laser in the

    Lab

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    Optoelectronic devices for

    Photovoltaic Applications

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    Solar Cells

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    Fibre optics Communication

    Transmitter Channel Receiver

    IR - Lasers

    IR-Photodetector

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    Head Mounted Display Applications: Next

    generation head mounted display and virtualreality training

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    n

    nthnppn

    /

    /

    pgand,npassumptionwith the

    ln

    1

    1

    th

    op

    oc

    op

    kTqV

    p

    n

    nn

    p

    p

    op

    kTqV

    th

    opnpopop

    g

    g

    q

    kTV

    IenL

    pL

    qAI

    IeII

    gLLqAgI

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    SOLAR CELLS

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    SOLAR CELLS

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    Finished Solar Cell Cross Section

    SOLAR CELLS

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    SOLAR CELLS

    ocsc

    ocsc

    mm

    VI.max

    VI

    VIfactorFill

    ffP

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    PHOTO DETECTORS

    Quantum efficiency ,

    Q=(Jop/q)/(Pop/h)

    where Jopphotocurrent densityPop- incident optical power density

    GAIN BANDWIDTH AND SIGNAL TO NOISE RATIO OF

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    GAIN, BANDWIDTH AND SIGNAL-TO-NOISE RATIO OF

    AVALANCHE PHOTO DETECTORS

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    Signalto-noise Ratio

    Johnson NoiseRandom thermal motion of the

    carrier

    Shot Noiserandom thermal generation-

    recombination of EHP

    Noise equivalent power (NEP)- is the minimum

    detectable signal that would produce the same rms

    output as the noise

    DetectivityD=1/NEP

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    WAVEGUIDE PHOTO DETECTORS

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    LIGHT EMITTING MATERIALS

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    LIGHT EMITTING MATERIALS

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    FIBER OPTIC COMMUNICATION

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    Light Amplification by Stimulated Emission of Radiation (LASERS)

    kThkTEE een

    n //)(

    1

    2 1212

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    Light Amplification by Stimulated Emission of Radiation (LASERS)

    B12n1(12) = A21n2 +

    B21n2(12)

    Absorption = Spontaneous +

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    B12n1(12) = A21n2 +

    B21n2(12)

    Absorption = Spontaneous +Stimulated

    emission emission)(

    )(

    rateemissionsSpontaneou

    rateemissionStimulated12

    21

    21

    221

    12221

    A

    B

    nA

    nB

    1

    2

    21

    21

    12121

    12221

    )(

    )(

    rateAbsorption

    rateemissionStimulated

    n

    n

    A

    B

    nB

    nB

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    Light Amplification by Stimulated Emission of Radiation (LASERS)

    materiallasertheofindexrefractiveisnwhere

    2

    0 n

    mL

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    SEMICONDUCTOR LASERS

    Population Inversion at a junction

    kTFE

    i

    kTEF

    v

    kTEF

    i

    kTFE

    c

    pivp

    innc

    eneNp

    eneNn

    /)(/)(

    /)(/)(

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    SEMICONDUCTOR LASERS

    gpn

    pn

    EFF

    hFF

    )(

    )(

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    SEMICONDUCTOR LASERS

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    Emission Spectra for p-n junction Lasers

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    m

    d

    dn

    nLn

    or

    d

    dnLLn

    d

    dm

    Lnmor

    n

    mL

    o

    ooo

    oooo

    o

    o

    12

    2

    1

    2

    22

    2

    2

    If we let m=-1, we can calculate the change in

    wavelength o between adjacent modes

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    Heterojunction Lasers

    Basic Semiconductor Lasers

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    Double Heterojunction Laser structure

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    Double -Heterojunction Laser structure

    Separate Confinement and Graded Index Channels

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    Separate Confinement and Graded Index Channels

    Vertical Cavity Surface Emitting Lasers (VCSELs)

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    Vertical Cavity Surface-Emitting Lasers (VCSELs)

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    High Frequency and

    High-Power Devices

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    Tunnel Diode

    IMPATT Diode

    P-N-P-N Diode

    Insulated Gate Bipolar Transistor(IGBT)

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    Tunnel Diode

    Degenerate n-type if n>NC

    Degenerate p-type if p>Nc

    Tunnel Diode

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    Tunnel Diode

    Tunnel Diode Band Diagram

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    Tunnel Diode Band Diagram

    Tunnel Diode Characteristics

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    Tunnel Diode Characteristics

    Impact Avalanche Transit-Time (IMPATT) Diode

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    Impact Avalanche Transit Time (IMPATT) Diode

    Time dependence of the growth and drift of holes in Read Diode

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    Time dependence of the growth and drift of holes in Read Diode

    Lfv

    L

    d 2

    vfor

    1

    2

    1 d

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    The transferred electron mechanism

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    The transferred electron mechanism

    The transferred electron mechanism

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    e t a s e ed e ect o ec a s

    Formation and drift Space Charge Domains

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    p g

    The P-N-P-N Diode

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    Two Transistor Analogy of SCR

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    gy

    )(1ior

    )i(

    But

    21

    21

    2121

    21

    1222

    2111

    COCO

    COCO

    CC

    BCOC

    BCOC

    II

    iII

    iii

    iIiiiIii

    Forward Blocking State

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    g

    The Semiconductor Controlled Rectifier (SCR)

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    ( )

    Application of SCR

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    pp

    Insulated Gate Bipolar Transistor (IGBT)

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    p

    COMFET- Conductivity Modulated FETIGTInsulated Gate Transistor

    IGR- Insulated Gate Rectifier

    GEMFET- Gain Enhanced MOSFET

    BiFET- Bipolar FET

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    Characteristics of IGBT:

    It has very high input impedance like MOSFET

    It has a low input capacitance

    In the ON state , it has low resistance and high

    current handling capability

    It can turn off more easily than SCR