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The Restless Vortex

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Transverse Patterns in Nonlinear Optical Resonators

Part of the book series: Springer Tracts in Modern Physics ((STMP,volume 183))

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Abstract

A single, isolated vortex in a class A or C laser, as described by the CSH equation (2.26), is stationary. However, in the case of a class B laser, the situation is different. Free vortices are not stationary but are in permanent motion. Also, a lattice of vortices experiences permanent self-sustained motion, leading to various oscillation modes.

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References

  1. J. Lega, J.V. Moloney and A.C. Newell, Universal description of laser dynamics near threshold, Physica D 83, 478 (1995).

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  2. K. Staliunas and C.O. Weiss, Nonstationary vortex lattices in large-aperture class B lasers, J. Opt. Soc. Am. B 12, 1142 (1995).

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  3. G. Slekys, K. Staliunas, M.F.H. Tarroja and C.O. Weiss, Cooperative frequency locking and tristability in a class-B laser, Appl. Phys. B 59, 11 (1994).

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© 2003 Springer-Verlag Berlin Heidelberg

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(2003). The Restless Vortex. In: Transverse Patterns in Nonlinear Optical Resonators. Springer Tracts in Modern Physics, vol 183. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-36416-1_7

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  • DOI: https://doi.org/10.1007/3-540-36416-1_7

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  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-540-00434-9

  • Online ISBN: 978-3-540-36416-0

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