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Volumn 57, Issue 5, 1998, Pages 4026-4033

Selection rules for transverse-mode excitation in nonlinear ring and Fabry-Perot resonators

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EID: 0347295314     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.57.4026     Document Type: Article
Times cited : (1)

References (36)
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    • (a) J. Opt. Soc. Am. B 7 (1990) special issue on transverse effects in nonlinear-optical systems, edited by N. B. Abraham and W. J. Firth;(b) Chaos, Solitons and Fractals 4 (8/9) (1994), special issue on nonlinear optical structures, patterns, chaos, edited by L. A. Lugiato and M. S. El Naschie.
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    • A. Gahl, Diplomarbeit, University of Münster, 1992, in German. A copy of the relevant pages can be obtained from the authors.
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    • This simulates the situation in which the beam waist of the incoupled beam is smaller than the beam waist of the fundamental eigenmode of the empty resonator, cf
    • This simulates the situation in which the beam waist of the incoupled beam is smaller than the beam waist of the fundamental eigenmode of the empty resonator, cf. 5. In reality, the excitation of the higher-order modes in the simulations was not exactly cylindrically symmetric, but the (Formula presented) Gauss–Hermite mode was slightly favored (by 2%) to study symmetry breaking effects, cf. 4. However, this point is not important for the present discussion.
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