doped optical fibers
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Doped Optical FibersFocused on Erbium-Doped Fibers as Examples
Used as Laser Gain Mediums and Optical Amplifiers
by Ryan McKinney
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Concept
Erbium-Doped Fiber Amplifiers Most important fiber amplifiers in long-range optical fiber
communications.
Efficiently amplify light in the 1.5-m wavelength region,
where telecom fibers have their loss minimum.
Fiber Lasers used with Amplifiers
High-power fiber lasers and particularly amplifiers with
output powers of tens or hundreds of watts; even several
kilowatts from a single fiber.
Very high surface-to-volume ratio and the waveguide
effect,
Avoids thermo-optical problems even with significant heating.
Based on solid-state laser technologies.
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Concept
Raman Amplifiers Optical amplifier based on Raman gain.
Optical gain from stimulated Raman scattering.
Occur in transparent solid media, liquids and gases under the
influence of intense pump light.
Magnitude depends mainly on the optical frequency offset
between pump and signal wave.
Can be fairly strong in optical fibers where substantial optical
intensities can be maintained over long lengths.
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Material Composition & Operation
Typical fiber amplifier works in the 1550 nm band. Consists of a length of fiber doped with Erbium.
Pumped with a laser at 980 nm.
Stimulated emission stimulates more emission
Rapid exponential growth of photons in the doped fiber. Gains of >40 dB (10,000X) possible with power outputs >+20
dBm (100 mW)
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Material Composition & Operation
The most efficient fiber amplifiers have been Erbium-Doped Fiber Amplifiers (EDFAs) operating in the
1550 nm range.
Amplifier emits light energy in a signal wavelength.
Energy supplied to it by photons in a pump wavelength. When stimulated by incoming photons in the signal the
emitted photons stimulate other emissions, so there is an
exponential growth of photons.
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Material Composition & Operation
Why Erbium ions? (Er3+) Erbium ions have quantum levels that allow them to be
stimulated to emit in the 1540nm band,
Band with the least power loss in most silica-based fiber.
Gives them the ability to amplify signals in a band where high-
quality amplifiers are most needed.
Can also be excited by a signal at 800nm or 980nm.
Silica-based fiber can carry these without great losses but
are not in the middle of the signal wavelengths.
Bands are also far enough away from the signal bandsthat it is easy to keep the pump beam and the signal
beam separated.
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Material Composition & Operation
Raman Fiber Amplifiers A high-power pump laser and a WDM or directional
coupler.
Optical amplification occurs in the transmission fiber.
Distributed along the transmission path.
Optical signals are amplified up to 10 dB in the optical
fiber.
Can be combined with EDFAs but fibers used for Raman
amplifiers are not exclusively doped with rare earth ions.
Pump laser has a wavelength of 1535 nm.
Circulator injects light backwards
into the transmission path.
Preferred as transfer of noise from
the pump to the signal is reduced.
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Applications
Erbium-Doped Fiber Amplifiers Light Distance Amplifier.
Overcomes traditional electronic fiber optic repeater limitations.
Digital Signal & Analog Signal Conversion
Repeater Changes and Replacements
Complex Structure & Expenses
EDFA does not have to be replaced if input signal is changed.
Equipment is expansive for optical wavelength division
multiplexing.
Transmitter Amplifier & Optical Receiver Preamplifier Signal transmission distance can be increased to 100-200km
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Applications
High-Power Fiber Lasers & Amplifiers Special General-Purpose Solid-State Lasers
High Potential for High Average Output Power
High Power Efficiency & Beam Quality
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Applications
High-Power Fiber Lasers & Amplifiers Broad Wavelength Tunability
Transitions of rare-earth-doped
crystals/glasses
Transitions with very low oscillator
strength
Long radiative upper-state lifetimes
Good energy storage qualities
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Applications
Raman Fiber Amplifiers Optical Telecommunications
All-Band Wavelength Coverage
In-Line Distributed Signal Amplification
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Issues & Problems
Fiber Amplifiers Most operate on quasi-three-level transitions.
In the unpumped state amplifiers exhibit some
losses caused by the active ions.
Only when a certain excitation level is
exceeded does actual amplification occur.
Quasi-three-level nature also has an increased noise figure.
Can be minimized by certain design optimizations.
Most are not made with polarization-maintaining fibers.
Polarization state of the input is not preserved. Amplification process is normally not polarization-dependent
in telecommunications.
In some cases polarization hole burning can cause problems.
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Issues & Problems
Fiber Lasers Subject to problems with uncontrolled birefringence.
Refractive index depends on polarization or double refraction.
This often changes the polarization state from linear to
elliptical depending on temperature and bending.
May require readjustment of polarization controllers with
temperature changes.
May be acceptable for laboratory use but not for commercial
devices.
Special fibers and fiber devices are often not available withpolarization-maintaining fibers.
Mode locking with nonlinear polarization rotation would not work
with a polarization-maintaining fiber.
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Issues & Problems
Fiber Lasers Devices require pump sources with higher beam
quality and brightness.
Generally increases the price per watt of the pump source.
Very sensitive to optical feedback.
Especially when used as master oscillator power amplifiers.
Backreflected light is even amplified on its way back to the seed
laser.
Fibers consist of glass material where the composition is
often poorly defined. Even the manufacturer may not know the exact composition and
it is not revealed to customers.
Fiber parameters such as the core diameter or refractive index
profile can be uncertain and vary between different samples.
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Issues & Problems
Raman Amplifiers Relatively poor pumping efficiency by comparison.
Require longer gain fibers.
Fast response time creates new sources of noise.
Reacts to minor unwanted inputs other amplifiers may not. More directly couple pump noise to the signal than laser
amplifiers.
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Technological Future
Dense Wavelength Division Multiplexing Pools data from different sources together on an optical
fiber.
80+ separate wavelengths or channels of data can be
multiplexed into a lightstream transmitted on a single
optical fiber.
Each channel carries a time division multiplexed signal.
In a system with each channel
carrying 2.5 Gbps (billion bits per
second), up to 200 billion bitscan be delivered a second by the
optical fiber.
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Technological Future
Developments Within the 12601610 nm Bands Typically fell within ranges absorbed by water.
Tiny amounts of water vapor within fiber glass affected
transmissions.
Fiber amplifiers and diode lasers in development within
this band to expand it as useable bandwidth.
Will allow for even greater ranged of wavelength-division
multiplexing, especially within dense wavelength-division
systems.
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Technological Future
Semiconductor Optical Amplifiers Direct competition with erbium-doped fiber amplifiers.
Compact setup containing only a small semiconductorchip with electrical and fiber connections.
The output powers are significantly smaller.
The gain bandwidth is smaller. Faster reaction to pump or signal input changes.
The noise figure is typically higher.
Often used currently in telecom systems in the form offiber-pigtailed components.
A single, short optical fiber with exposed fiber at one end usedto separate bundles into individual fibers spliced to otherequipment.
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References
RP PHOTONICSENCYCLOPEDIA
HTTP://WWW.RP-PHOTONICS.COM/ENCYCLOPEDIA.HTML
THEFIBEROPTICSASSOCIATIONAMPLIFIERS
HTTP://WWW.THEFOA.ORG/TECH/FIBERAMP.HTM
FIBER-OPTICS.INFOOPTICALAMPLIFIERS
HTTP://WWW.FIBER-
OPTICS.INFO/ARTICLES/OPTICAL_AMPLIFIERS
UNIVERSITYOFSOUTHAMPTONFIBERLASERS
HTTP://WWW.ORC.SOTON.AC.UK/61.HTML
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