Difference between revisions of "Master Oscillator Power Amplifier Pulsed Laser"
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== Master Oscillator with graphene as saturable absorber == | == Master Oscillator with graphene as saturable absorber == | ||
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| + | [http://www.rp-photonics.com/master_laser.html Master Laser] | ||
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| + | A master laser is a single-frequency seed laser which is used for, e.g., injection locking of one or several slave lasers. | ||
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| + | A master laser often generates an optical power which is well below the output power of the complete laser system; the injection-seeded slave lasers may then be high-power lasers. The modest power requirements for the master laser make it possible to realize a very low level of laser noise, which may be more or less transferred to the whole system. Also, a larger range for wavelength tuning may be accomplished. | ||
[[File:MasterOscillator.jpg|500px]] | [[File:MasterOscillator.jpg|500px]] | ||
Revision as of 14:07, 18 June 2015
Contents
MOPA (Master Oscillator Power Amplifier)
The master oscillator produces a highly coherent beam, and an optical amplifier is used to increase the power of the beam while preserving its main properties. The master oscillator has no need to be powerful, and has no need to operate at high efficiency because the efficiency is determined mainly by the power amplifier.
With a MOPA instead of a laser, it can be easier to reach the required performance e.g. in terms of linewidth, wavelength tuning range, beam quality or pulse duration if the required power is very high. This is because various performance aspects are decoupled from the generation of high powers. This gives extra flexibility, e.g. when a gain-switched laser diode is used as a seed laser.
The same aspects apply to other kinds of modulation, e.g. intensity or phase modulation: it may be advantageous to modulate the low-power seed laser, or to use an optical modulator between seed laser and power amplifier, rather than to modulate a high-power device directly. Slower power modulation may be done by adjusting the amplifier's pump power, without significantly affecting e.g. the obtained pulse duration or wavelength.
The combination of an existing laser with an existing amplifier (or an amplifier chain) may be simpler than developing a new laser with higher output power.
The optical intensities are lower in an amplifier, compared with the intracavity intensities in a laser.
However, the MOPA approach can also have disadvantages:
The resulting laser noise tends to be higher, since an amplified source can not reach the shot noise level (→ amplifier noise). Effects of drifts of the seed power may be suppressed, however, if the amplifier is operated in a strongly saturated regime.
A MOPA can be sensitive to back-reflections, which are amplified again before entering the master laser. This feedback sensitivity can often be cured only by placing a Faraday isolator behind the amplifier. Particularly for high-power pulsed devices, this can introduce serious limitations.
Stages of the fiber laser
1st: Master Oscillator (this is the stage that will contain the graphene and will produce the pulsing)
2nd: Single-Mode Power Amplifier
3rd: Double-Clad Power Amplifier
Master Oscillator with graphene as saturable absorber
A master laser is a single-frequency seed laser which is used for, e.g., injection locking of one or several slave lasers.
A master laser often generates an optical power which is well below the output power of the complete laser system; the injection-seeded slave lasers may then be high-power lasers. The modest power requirements for the master laser make it possible to realize a very low level of laser noise, which may be more or less transferred to the whole system. Also, a larger range for wavelength tuning may be accomplished.
Length of fiber
The lengths of Erbium-doped fiber are chosen based on RP Fiber Power simulation:
