Expand this Topic clickable element to expand a topic
Skip to content
Optica Publishing Group

"Cerenkov" configuration Second Harmonic Generation

Not Accessible

Your library or personal account may give you access

Abstract

The use of the largest nonlinear coefficient d33 of LiNbO3 for second harmonic generation (SHG), first demonstrated with a guided wave phase-matched interaction suffering from poor field overlap integrals (1), has been considerably improved by the use of a Cerenkov type configuration : nonlinear polarization having a phase velocity greater than that of light in the waveguide, harmonic radiated into the substrate (2,3).

© 1989 Optical Society of America

PDF Article
More Like This
Cerenkov Second Harmonic Generation of Semiconductor Laser Radiation (λ=1.3 μm) in Ti: LiNbO3 Waveguide

K.S. Buritskii, D.Z. Garbuzov, E.M. Dianov, S.V. Zaitsev, A.V. Ovchinnikov, I.S. Tarasov, V.A. Chernykh, and E.A. Scherbakov
THB10 Nonlinear Guided-Wave Phenomena (NP) 1989

Influence of annealing on the conversion efficiency for SHG by Cerenkov radiation from proton-exchanged LiNbO3 waveguides

G Arvidsson, F Laurell, B Jaskorzynska, J Webjörn, A Loni, R W Keys, and R M De La Rue
THA3 Nonlinear Guided-Wave Phenomena (NP) 1989

Optimization of Optical Second-Harmonic Generation in the Cerenkov-Radiation Scheme

N. Hashizume, T. Kondo, T. Onda, and R. Ito
PTh007 International Quantum Electronics Conference (IQEC) 1992

Select as filters


Select Topics Cancel
© Copyright 2024 | Optica Publishing Group. All rights reserved, including rights for text and data mining and training of artificial technologies or similar technologies.