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    Transmitters, Receivers

    Optical WirelessCommunications

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    Optical Communication Systems

    Communication systems with light as the carrierand optical fiberascommunication medium

    Optical fiber is used to contain and guide light waves

    Typically made of glass or plastic

    Propagation of light in atmosphere is impractical

    This is similar to cable guiding electromagnetic waves

    Capacity comparison

    Microwave at 10 GHz

    Light at 100 Tera Hz (1014)

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    Optical Fiber Construction

    Corethin glass center of the fiber

    where light travels.

    Claddingouter optical material

    surrounding the core Buffer Coatingplastic

    coating that protects

    the fiber.

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    Types Of Optical Fiber

    Single-mode step-index Fiber

    Multimode step-index Fiber

    Multimode graded-index Fiber

    n1core

    n2cladding

    noair

    n2cladding

    n1core

    Variable

    n

    noair

    Light

    ray

    Index profile

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    Optical Transmitter LED

    Laser

    Lamp

    Optical ReceiverDetection Techniques:

    Direct Detection

    Coherent Detection

    Photodetectors

    p-i-n

    Avalanche Photo Diode (APD)

    Photo Multiplier Tube (PMT)

    Modulation Techniques

    Transmitters/Receivers

    5

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    LED

    Semiconductor device

    Medium modulation speed

    Incoherent output light

    Mainly used for short range FSO systems (shorter than 1 km)

    Laser

    Highly directional beam profile Used for long range FSO systems

    High modulation speed

    Coherent output light

    Lamp

    Lower efficiency compared to LED and laser Lower cost

    Low modulation speed

    Incoherent output light

    Provides higher power

    Optical Transmitters

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    A semiconductor pn junction device that gives off spontaneous

    optical radiation when subjected to electronic excitation

    The electro-optic conversion process is fairly efficient, thus resulting

    in very little heat compared to incandescent lights

    Mainly used for short-range FSO systems (shorter than 1 km)

    Ultraviolet communications

    Indoor FSO systems

    Optical Transmitters: LED

    Illustration of the radiated

    optical power against driving

    current of an LED

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    LED Types

    Optical Transmitters: LED

    Dome LED

    Edge-Emitting LED

    Planar LED

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    Laser: light amplification by stimulated emitted radiation

    Has highly directional beam profile

    Is used for long range FSO systems

    Has narrow spectral width compared to LED

    Optical Transmitters: Laser

    Laser output power

    against drive current plot

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    Laser Types

    Optical Transmitters: Laser

    Fabry-Perot Laser

    Distributed Feedback Laser Vertical-cavity surface-

    emitting Laser (VCSEL)

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    Hecht: Understanding Fiber

    Optics. (C) 2006 PearsonEducation, Upper Saddle River,

    11

    Distributed Feedback Laser

    Light scatters

    from grating in

    laser substrate

    Limits

    oscillation to

    one wavelength

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    Hecht: Understanding Fiber

    Optics. (C) 2006 PearsonEducation, Upper Saddle River,

    12

    Distributed Bragg reflection

    Grating etched insubstrate

    In plane of activelayer, but outsidelaser zone

    Feedback limits

    oscillation to onewavelength Light scattered

    From here

    into active layer

    Semiconductor covers

    grating layer

    In unpumped region

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    Can be used in FSO communications, not in fiber optics

    Wideband and continuous spectrum Have very high power, but undirected

    The electro-optic process is inefficient, and huge amount of

    energy is dissipated as heat (causes high temperature in lamps) Has very low modulation bandwidth

    Divided as follows

    Carbon button lamp Halogen lamps

    Globar

    Nernst lamp

    Optical Transmitters: Lamp

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    Optical Receivers

    The purpose of the receiver is:

    To convert the optical signal to electrical domain Recover data

    Direct-Detection Receiver:

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    Coherent-Detection Receiver

    For detecting weak signal, coherent detection scheme is applied

    where the signal is mixed with a single-frequency strong localoscillator signal.

    The mixing process converts the weak signal to an intermediate

    frequency (IF) in the RF for improved detection and processing.

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    Optical Receivers

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    Photodetectors

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    A square-law optoelectronic transducer that generates an electrical signal

    proportional to the square of the instantaneous optical field incident on its

    surface

    The ratio of the number of electronhole (eh) pairs generated by a

    photodetector to the incident photons in a given time is termed the quantum

    efficiency,

    Dark current: the current through the photodiode in the absence of light

    Noise-equivalent power (NEP): the minimum input optical power to

    generate photocurrent equal to the root mean square (RMS) noise current ina 1 Hz bandwidth

    Responsivity: photocurrent generated per unit incident optical power

    (W/A)

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    Photodetectors

    p-i-nphotodetector

    Consists ofp- and n-type semiconductor materials separated by a very

    lightly n-doped intrinsic region

    In normal operating conditions, a sufficiently large reverse bias

    voltage is applied across the device

    The reverse bias ensures that the intrinsic region is depleted of any

    charge carriers

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    Photodetectors

    Avalanche Photo-Diode (APD)

    provides an inherent current gain through the process called repeated

    electron

    This culminates in increased sensitivity since the photocurrent is now

    multiplied before encountering the thermal noise associated with the

    receiver circuit

    Multiplication (or gain) factor:

    :the average value of the total output current

    = : the primary unmultipliedphotocurrent

    Typical gain values lie in the range 50300

    Excess noise factor:

    = + 2 1

    1

    : the ratio of the hole impact ionization

    rate to that of electrons

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    AVALANCHE Photodiodes.

    An APD internally amplifies the photocurrentby an avalanche process when a large reverse-

    bias voltage is applied across the active

    region.

    The gain of the APD can be changed by

    changing the reverse-bias voltage.

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    AVALANCHE Photodiode.