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SOLITONS in space. BEAM PROPAGATION MAXWELL Townes Soliton: solution of an eigenvalue equation (dimensionless form): 2D NONLINEAR SCHROEDINGER EQUATION.

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Presentation on theme: "SOLITONS in space. BEAM PROPAGATION MAXWELL Townes Soliton: solution of an eigenvalue equation (dimensionless form): 2D NONLINEAR SCHROEDINGER EQUATION."— Presentation transcript:

1 SOLITONS in space

2 BEAM PROPAGATION MAXWELL Townes Soliton: solution of an eigenvalue equation (dimensionless form): 2D NONLINEAR SCHROEDINGER EQUATION Normalization: and

3 Scaling parameters: Such that critical power SOLUTION: TOWNES SOLITON (Gaeta) Radius: o Peak Field: o o o 2 2 TOWNES SOLITON AS A “BEAM CLEANER”

4 Simulations with Elliptical Input Beam 4X 3.5 P cr x y z = 0 z = 0.8 z = 1.8 Alexander L. Gaeta Cornell University

5 K. D. Moll, G. Fibich, and A. L. Gaeta, Phys. Rev. Lett. 90, 203902 (2003). Experiments performed in glass aberrated input output input power position intensity

6

7 Some properties of filaments “Conical Emission” Intensity clamp: always the same energy in a filament “Ideal filter”: a distorted beam produces a nice round filament Pattern of filaments – not always random – often in a circle. Very broad spectrum ? ? ? ? ? ?

8 The filaments appear in circle for P > 10 P cr and “super Gaussian” beams Too complicated! SIMPLIFY! Approximation: neglect diffraction Solution: Gaussian Super-Gaussian

9 SIMULATION OF GAETA Data of Olivier Chalus


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