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“Finding” a Pulse Shape
Jason Taylor May 16, 2005 “The laser cavity finds the pulse that minimizes loss--it's like magic.”
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My Research I investigate the usefulness of laser cavities and laser dynamics for information processing. Kerr Lens Mode-Locked laser cavities
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Project Goals Discover what a KLM laser minimizes
Cavity loss? Population Inversion? Use results to predict good bit representation and/or logical operators Space Time Phase Power
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Kerr-Lens Mode Locked Oscillator
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The Equation GVD SPM This equation describes the evolution of a short pulse over one round trip in a KLM cavity.
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Mode Locking
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Artificial Fast Saturable Absorbers
[Hau00]
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fast saturable absorber
master equation: solution unbounded Siegman, Haus [Hau00]
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Kerr-Lens Mode Locked Laser
Ti:Sapphire KLM oscillators are available commercially—where else would this graphic come from?
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Soliton Effects in Ultrashort Pulses
Group Velocity Dispersion (GVD) Self Phase Modulation (SPM) pulse width New master equation with GVD and SPM: GVD SPM d0 = no SPM Dn = GVD
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Haus’ Master Equation master equation with GVD and SPM: Gain depletion
where
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Numerical Simulation Here we look at the equation properties via numerical simulation.
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Separate into Linear and Non-Linear Operators
where
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Simulation
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Gain, SAM, no GVD, no SPM pulse width frequency
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Gain, SAM, GVD, and SPM pulse width frequency
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What is minimized? Cavity loss? Gain medium population inversion?
Pulse width?
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Haus’ Master Equation master equation with GVD and SPM: Gain depletion
where
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Complex Ginzburg-Landau Equation
master equation with GVD and SPM: GVD SPM Gain depletion where
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Complex Ginzburg-Landau Equation
master equation: soliton like pulse CW solution general CGLE
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Complex Ginzburg-Landau Equation
general CGLE
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Lyapunov Function A good approximate Lyapunov function is known for a
soliton like pulse CW solution A good approximate Lyapunov function is known for a CW stationary solution. No Lyapunov function is known for soliton solutions—too close to chaos. IMHO
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Simplify Equation ignore gain depletion, BW filtering and SAM
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Non-linear Schrodinger Equation
Lyapunov Function: Looks a lot like minimizing the action.
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Numerical Confirmation
Try Lyapunov function in simulator.
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NLSE Lyapunov function on CGLE with gain saturation
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Gain, SAM, GVD, and SPM pulse width frequency
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Zoom in on Hump
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Zoom in on 2nd Hump
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Zoom in on 3rd Hump
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Zoom in on 4th Hump
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Conclusions We found a fractal.
The NLSE approximate Lyapunov function isn’t valid far away from the soliton solution. Is a numerical stability analysis of the CGLE sufficient?
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