01 Optical Concepts

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    Global Professional Services

    ECI Training services

    Optical Concepts

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    Milestones in Optics

    1960 - Laser development

    1966 - Fiber optics development1970 - First fiber production with attenuation of 20 dB/km

    1972 - Production of fiber with attenuation of 4 dB/km

    1976 - Mass production of fiber with attenuation

    of 0.5 dB/km for 1310nm

    1977 - First field trial using fiber optics in Chicago

    1979 - Production of Single Mode fiber with attenuation

    of 0.2dB/km for 1550nm

    1985 - Mass production of Single Mode Fiber

    1991 - Development of optical amplifiers

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    Why Fiber Optics?

    Capacity, Distance, Reliability

    Microwave

    Networks

    FiberOptics

    A communications network is one that conveys / transportsinformation (audio, video, and data) over substantialdistances between customer and network sites

    Twisted Pair

    Coax

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    Network Providers combine the signals from different usersand send them over a single

    transmission

    Basic Network Information Rates

    Examples of information rates for some typical voice,

    video and data services:Video on demand/interactive TV 1.5-6 Mbps

    Video games 1-2 Mbps

    Remote education 1.5-3 Mbps

    Electronic shopping 1.5-6 MbpsData transfer 1-3 Mbps

    Video-conferencing 0.4-2 Mbps

    Voice 64 Kbps

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    The Optical Fiber

    Very thin strands of pure silica

    glass through which laser light

    travels in optical networks

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    The Optical Fiber

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    The Light Theory

    The Quantum nature

    The wavelengthnature

    Vs.

    Of light

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    Energy levels: E1, E2,E3

    E1 E3E2

    Photon

    The Quantum Nature of Light

    When a photon insides on an atom, it transfers its

    energy to an electron within this atom, exciting itto a higher energy level

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    Spontaneous emission

    Absorption

    Energy

    E1

    E2

    E3

    Ground Level

    Excited State Level

    The energy of the photon must be exactly equal to thatrequired to excite the electron to a higher energy level, to be

    absorbedConversely, an electron in an excited state can drop to a lowerenergy state by emitting a photon, with exactly the sameenergy

    This energy equals h, h: Plank constant, : photon frequency

    E3-E2 h32

    Photon Absorption and Emission

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    Spontaneous emission Stimulated emission

    In spontaneous emission:thehigh energy state lifetime is betweennanoseconds to milliseconds

    Instimulated emission:the emitted photon is identical in wavelength,

    phase and direction to the incident photon

    E1 E3E2

    Photon

    E1 E3E2

    Photon

    Photons Behavior

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    Population Inversion : E3 > E2Stimulated emission amplification

    Amplification

    Energy

    E1

    E2

    E3

    The amount of electrons in stimulated level must be higher than

    those in ground level

    Optical Amplification

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    The Wavelength Nature

    Wavelength is the distance between identical points in theadjacent cycles of a waveform signal propagated in space or

    along a wire

    Wavelength is specified in nanometers (units of 10-9 meter)

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    Electromagnetic Spectrum

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    Wavelength Vs Frequency

    The higher the frequency of the signal, the shorter its

    wavelength:= c / f

    c= 299,792,458 m/s

    The standard unit of frequency is Hertz

    If a wave completes one cycle per second, then

    f = 1 Hz

    1 THz = 10 cycles per second

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    Optical Parameters

    Attenuation refers to any reduction in the strength of a signal

    Attenuation occurs with any type of signal, sometimes called

    loss

    A natural consequence of signal transmission over long

    distances

    The extent of attenuation is usually expressed in dB:

    dB = a common unit of measurement for the relative

    difference between two power levels

    dB = 10 log(Pout / Pin ) = 10 log Pout - 10 log Pin

    dBm = a measure of absolute power

    dBm = 10 log P(mw)

    Characteristics of Different Wavelengths

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    Beginningof the 80s

    Beginning

    of the 90s Today

    Characteristics of Different Wavelengthsin Pure Silica Fiber

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    Optical Parameters

    Dispersion refers to the expansion or widening of the

    signal by the time it reaches the receiving end

    Dispersion is due to the fact that different

    wavelengths propagate in different velocities

    Dispersion does not alter the wavelength (frequency)

    but it directly affects the bit rate

    Measured as the amount of delay in picoseconds

    (10 - seconds) per km of fiber per nm change in the

    wavelength

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    Dispersion

    Input pulses

    Output pattern

    Inter-symbol interference

    Puls

    eShapeandAmplitudes

    Distance along fiber

    1 10

    1 0 1

    1 0 1

    111

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    Dispersion Types

    Modal dispersion

    Material dispersionWaveguide dispersion

    Polarization dispersion

    Chromatic Dispersion

    t

    Before After

    t

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    Modal Dispersion

    Depends on the diameter of the core and the critical

    angleSignificant in Multi-mode fibers and not in Single-mode

    fibers

    Input Surface Refraction

    CladdingCore

    Jacket

    t

    1 1

    t

    Pulse entering

    the fiber

    t

    11

    Pulse exiting

    the fiber

    t

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    Chromatic Dispersion

    Material dispersion

    Effect of the fiber material on the propagation velocityof the wave

    Waveguide dispersion relates to the ratio betweencore radius and wavelength

    Input Surface Refraction

    CladdingCore

    Jacket

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    Chromatic Dispersion

    Material dispersion and Waveguide dispersion

    may act in opposite waysFiber is engineered in order to give a resultant

    chromatic dispersion near to zero

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    1

    0

    1 0 1 1 0 1 1 0 1 1 1 1

    2 dB per 100 kmfor 2.5Gps

    Dispersion Penalty

    The dispersion of the

    signal causes attenuation

    Dispersion Penalty

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    Polarization Dispersion

    This kind of dispersion is significant in higher bitrates,

    from 10 GbpsDue to manufacturing imperfections, the non-circular

    core of the fiber may contribute to cause PD

    Caused by several sources: core shape, external

    stress, material properties, older fibers etc.

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    G.653

    G.655

    G.652 /

    G.654

    Fiber ITU-T

    Standard

    l

    nm

    Dispersion

    ps/(nm km)

    Attenuation

    dB/ km

    Zero-Dispersion G.652 1310 0 < 0.5

    Non-Zero-

    Dispersion

    G.655 1550 3 < 0.35

    G.652 1550 18 < 0.4Zero-Dispersion

    Wavelength Vs Dispersion

    O

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    1 0 1 0 1

    Dispersion - Limits How Fast: ps/(nm.km)

    1 0 1

    Attenuation- Limits How Far: dB/km

    1 0 0 0 0

    1 1 1

    Optical Parameters

    The How far and How fast are not only fiber-dependent

    LASER - Light Amplification by Stimulated

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    28 28 O ti l C t

    Typical Transmittance Profile of a Laser Diode

    f1 f1 f1 f1

    Transmittance

    Thefrequencys lasers output is uniform

    LASER- Light Amplification by StimulatedEmission of Radiation