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Published byLynette Roberts Modified over 9 years ago
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SOLITONS in space
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BEAM PROPAGATION MAXWELL Townes Soliton: solution of an eigenvalue equation (dimensionless form): 2D NONLINEAR SCHROEDINGER EQUATION Normalization: and
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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”
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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
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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
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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 ? ? ? ? ? ?
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The filaments appear in circle for P > 10 P cr and “super Gaussian” beams Too complicated! SIMPLIFY! Approximation: neglect diffraction Solution: Gaussian Super-Gaussian
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SIMULATION OF GAETA Data of Olivier Chalus
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