Difference between revisions of "Mode-locked Erbium-Ytterbium Doped Fiber Laser"
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[[File:ModeLocking2.jpg|500px]] | [[File:ModeLocking2.jpg|500px]] | ||
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+ | '''The Kerr effect''' | ||
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+ | Nonlinear polarization generated in the medium, which modifies the propagation properties of the light. | ||
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+ | The refractive index for the high intensity light beam is modified according to Δn = n' ∙ I | ||
+ | (with the nonlinear index n' and the optical intensity I). | ||
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+ | Half wave plate rotates polarization so that the fast axis (highest intensity)is in line with the polarizer; | ||
+ | |||
+ | the signal passes through polarizer with the narrowing of the pulse due to extinguishing of the low-intensity tail-modes; | ||
+ | |||
+ | the quarter wave plate turns linearly polarized light into elliptically polarized light so that the non-linear rotation continues: | ||
+ | |||
+ | [[File:KerrOptics.jpg|500px]] |
Revision as of 10:40, 16 June 2015
High Power Pulsed Fiber Lasers
Ring cavity Er-Yb doped fiber laser showing optical bench for Kerr mode locking:
Mode Locking
Mode locking is a technique to create very short periodic pulses by locking modes in phase
Additive-pulse Mode Locking
Nonlinear phase shifts in a single-mode fiber.
Pulses returning from the fiber resonator into the main laser resonator interfere with those pulses which already are in the main resonator.
Constructive interference near the peak of the pulses, but not in the wings, because the latter have acquired different nonlinear phase shifts in the fiber.
Peak of the circulating pulse is enhanced, whereas the wings are attenuated.
The Kerr effect
Nonlinear polarization generated in the medium, which modifies the propagation properties of the light.
The refractive index for the high intensity light beam is modified according to Δn = n' ∙ I (with the nonlinear index n' and the optical intensity I).
Half wave plate rotates polarization so that the fast axis (highest intensity)is in line with the polarizer;
the signal passes through polarizer with the narrowing of the pulse due to extinguishing of the low-intensity tail-modes;
the quarter wave plate turns linearly polarized light into elliptically polarized light so that the non-linear rotation continues: