Abstract
Second-harmonic generation (SHG) is explained in terms of linear phase matching and deploys in non-centrosymmetric crystals. The classification of the SHG processes into type I and type II are well known but the more general vector case has not been studied. Type II SHG is a vector process involving two electric field components at the fundamental frequency and one component at the second-harmonic frequency. It is assumed in the literature that only one component of the second-harmonic field is phase matched but this argument is based upon the magnitude of the linear phases only. For a situation in which linear phase matching is absent the nonlinear phases are important and will balance the linear phases. The full vector theory needs to be investigated therefore.
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References
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© 1999 Springer Science+Business Media Dordrecht
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Bontemps, P., Boardman, A.D. (1999). Full Vector Theory of Fundamental and Second-Harmonic CW Waves. In: Boardman, A.D., Pavlov, L., Tanev, S. (eds) Advanced Photonics with Second-Order Optically Nonlinear Processes. NATO Science Series, vol 61. Springer, Dordrecht. https://doi.org/10.1007/978-94-007-0850-1_8
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DOI: https://doi.org/10.1007/978-94-007-0850-1_8
Publisher Name: Springer, Dordrecht
Print ISBN: 978-0-7923-5316-4
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