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7/31/2019 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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Typical Transmittance Profile of a Laser Diode
f1 f1 f1 f1
Transmittance
Thefrequencys lasers output is uniform
LASER- Light Amplification by StimulatedEmission of Radiation