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“Finding” a Pulse Shape

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1 “Finding” a Pulse Shape
Jason Taylor May 16, 2005 “The laser cavity finds the pulse that minimizes loss--it's like magic.”

2 My Research I investigate the usefulness of laser cavities and laser dynamics for information processing. Kerr Lens Mode-Locked laser cavities

3 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

4 Kerr-Lens Mode Locked Oscillator

5 The Equation GVD SPM This equation describes the evolution of a short pulse over one round trip in a KLM cavity.

6 Mode Locking

7 Artificial Fast Saturable Absorbers
[Hau00]

8 fast saturable absorber
master equation: solution unbounded Siegman, Haus [Hau00]

9 Kerr-Lens Mode Locked Laser
Ti:Sapphire KLM oscillators are available commercially—where else would this graphic come from?

10 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

11 Haus’ Master Equation master equation with GVD and SPM: Gain depletion
where

12 Numerical Simulation Here we look at the equation properties via numerical simulation.

13 Separate into Linear and Non-Linear Operators
where

14 Simulation

15 Gain, SAM, no GVD, no SPM pulse width frequency

16 Gain, SAM, GVD, and SPM pulse width frequency

17 What is minimized? Cavity loss? Gain medium population inversion?
Pulse width?

18 Haus’ Master Equation master equation with GVD and SPM: Gain depletion
where

19 Complex Ginzburg-Landau Equation
master equation with GVD and SPM: GVD SPM Gain depletion where

20 Complex Ginzburg-Landau Equation
master equation: soliton like pulse CW solution general CGLE

21 Complex Ginzburg-Landau Equation
general CGLE

22 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

23 Simplify Equation ignore gain depletion, BW filtering and SAM

24 Non-linear Schrodinger Equation
Lyapunov Function: Looks a lot like minimizing the action.

25 Numerical Confirmation
Try Lyapunov function in simulator.

26 NLSE Lyapunov function on CGLE with gain saturation

27 Gain, SAM, GVD, and SPM pulse width frequency

28 Zoom in on Hump

29 Zoom in on 2nd Hump

30 Zoom in on 3rd Hump

31 Zoom in on 4th Hump

32 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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