Transcript Slide 1

Optical Fibre Amplifiers
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Introduction to Optical Amplifiers
Raman Fibre Amplifier
Brillouin Fibre Amplifier
Doped Fibre Amplifier
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* Introduction
- operate solely in the optical domain with no inter-conversion of
photons to electrons
- can be placed at intervals along a fiber link to provide linear
amplification
- provide better performance over regenerative repeaters which require
optoelectronic devices and electronic circuits:
(a) larger amplification bandwidth (several thousands GHz)
(b) speed bottlenecks from electronics are removed
(c) amplify multiple optical inputs at different wavelengths
simultaneously (WDM).
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* Two main categories of optical amplifiers:
(a) Semiconductor Laser amplifiers (SLAs)
- a laser diode operated below threshold
- amplification is done by stimulated emission from injected
carriers
(b) Fiber amplifiers (FA)
- a fiber section that has a positive medium gain
- fiber is doped with Erbium (1.55 mm) or
Neodymium/Praseodymium (1.3 mm)
- amplification also can be provided by nonlinear effects such
as stimulated Raman scattering or Brillouin scattering
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Types of Optical Amplifiers
Travelling Wave
Semiconductor Laser
Amplifier (SLA)
Angled-facet or tiltedstripe – the reflected
beam at the facet is
physically separated
from the forward beam
Mirror
Fabry-Perot
Semiconductor Laser
Amplifier (SLA)
Buried-facet
or
window facet – the
optical beam spreads
in the transparent
window
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Types of Optical Amplilfiers
Rare-earth dopants (for doped optical
amplifier) or a highly nonlinear
medium (for Raman and Brillouin
optical amplifiers)
Its wavelength is
dependent on the
dopant
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* Optical Amplifier Gain Characteristics
- Traveling wave semiconductor laser amplifier (TWSLA), Erbium
doped fiber and Raman fiber amplifiers provide wide spectral
bandwidth suitable for WDM applications.
- Brillouin fiber amplifier has a very narrow spectral bandwidth
~50MHz and it can be used for channel selection within a WDM
system
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* Applications of Optical Amplifier
(a) In-line Amplifier
- use to compensate for transmission loss and increase the
distance between regenerative repeaters.
(b) Preamplifier
- used as a front-end preamplifier for an optical receiver.
(c) Power Amplifier
- to boost transmitted power and increase the transmission
distance
- as booster of signal level in the local area network
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* Applications of Optical Amplifier (cont.)
(a) In-line Amplifier
(b) Preamplifier
(c) Power Amplifier
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* Merits of TWA
• TWAs have been used more widely than FPAs (particularly for
linear application) because they have
(a) a large optical bandwidth,
(b) high saturation power, and
(c) low polarization sensitivity.
• In particular, TWAs are used as amplifiers in the 1300nm window
and as wavelength converters in the 1550nm region.
* Advantages of SLAs
• able to operate at the 1300nm and 1550nm wavelengths
(simultaneously)
• wide bandwidth, up to 100nm
• can be readily integrated along with other semiconductors and
photonic devices into one monolithic chip called an optoelectronic integrated circuit (OEIC)
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* Drawbacks of SLAs
•
•
•
•
a relatively high crosstalk level
polarization sensitivity
large coupling loss
difficult to produce an active medium with reflectances as low as
10-4 (TWA)
• optical noise
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Basic Concepts
Most optical amplifiers amplify incident light through stimulated
emission – a laser without feedback
The optical gain realized when the amplifier is pumped (optically or
electrically) to achieve population inversion
The optical gain, in general, depends not only on the frequency (or
wavelength) of the incident signal, but also on the local beam
intensity at any point inside the amplifier.
Details of the frequency and intensity dependence of the optical gain
depend on the amplifier medium
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Gain Saturation
The large-signal amplifier gain:
The output saturation power Pouts – the output power for which the
amplifier gain G is reduced by a factor of 2 (or by 3 dB) from its
unsaturated value G0.
By using G = G0/2,
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Gain Saturation
Amplifier gain G as a function of the output power (normalized to the
saturation power)
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Amplifier Noise
The SNR degradation is quantified through a parameter Fn, called the
amplifier noise figure
Consider an amplifier with the gain G such that the output and input
powers are related by Pout = GPin.
The SNR of the input signal is given by
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Amplifier Noise
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Amplifier Noise
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Amplifier Noise
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Basic Concepts
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Raman Gain & Bandwidth
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Raman Gain & Bandwidth
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Amplifier Characteristics
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Amplifier Characteristics
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Amplifier Characteristics
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Amplifier Characteristics
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Amplifier Characteristics
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Amplifier Characteristics
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Amplifier Performance
???
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Amplifier Performance
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Amplifier Performance
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Amplifier Performance
???
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Amplifier Performance
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Amplifier Performance
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Amplifier Performance
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Pumping Requirements
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Pumping Requirements
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Pumping Requirements
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Pumping Requirements
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Pumping Requirements
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Gain Spectrum
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Gain Spectrum
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Theory
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Theory
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Theory
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Theory
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Amplifier Noise
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Amplifier Noise
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Amplifier Noise
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Amplifier Noise
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Multichannel Amplification
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Multichannel Amplification
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Multichannel Amplification
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Multichannel Amplification
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Multichannel Amplification
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Multichannel Amplification
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Multichannel Amplification
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Multichannel Amplification
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Multichannel Amplification
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Distributed-Gain Amplifiers
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Distributed-Gain Amplifiers
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Distributed-Gain Amplifiers
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Optical Preamplification
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Optical Preamplification
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Optical Preamplification
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Optical Preamplification
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Optical Preamplification
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Optical Preamplification
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Optical Preamplification
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Noise Accumulation in Long-Haul Systems
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Noise Accumulation in Long-Haul Systems
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Noise Accumulation in Long-Haul Systems
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Noise Accumulation in Long-Haul Systems
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Noise Accumulation in Long-Haul Systems
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ASE-Induced Timing Jitter
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ASE-Induced Timing Jitter
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ASE-Induced Timing Jitter
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ASE-Induced Timing Jitter
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Accumulated Dispersive and Nonlinear Effects
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WDM-Related Impairments
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WDM-Related Impairments
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