Second-harmonic imaging of poled silica waveguides

Jesper Arentoft; Kjeld Pedersen; Sergey I. Bozhevolnyi; Martin Kristensen; Ping Yu; Christian Bergenstof Nielsen

doi:10.1063/1.125644

Second-harmonic imaging of poled silica waveguides

Jesper Arentoft, Kjeld Pedersen, Sergey I. Bozhevolnyi, Martin Kristensen, Ping Yu, Christian Bergenstof Nielsen

Aalborg University

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Abstract

Electric-field poled silica-based waveguides are characterized by measurements of second-harmonic generation (SHG) and of the linear electro-optic effect (LEO). A SHG scanning technique allowing for high-resolution imaging of poled devices is demonstrated. Scans along the direction of the poling field show that the second-order optical nonlinearity is located near the interface between differently doped glass layers. Both SHG and LEO measurements indicate that the ratio between the main elements of the second-order nonlinear optical susceptibility tensor, chi(33)((2)) and chi(31)((2)), is significantly smaller than three. (C) 2000 American Institute of Physics.

Original language	English
Journal	Applied Physics Letters
Volume	76
Issue number	1
Pages (from-to)	25-27
ISSN	0003-6951
DOIs	https://doi.org/10.1063/1.125644
Publication status	Published - 2000

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Copyright (2000) American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics.

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GLASS

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title = "Second-harmonic imaging of poled silica waveguides",

abstract = "Electric-field poled silica-based waveguides are characterized by measurements of second-harmonic generation (SHG) and of the linear electro-optic effect (LEO). A SHG scanning technique allowing for high-resolution imaging of poled devices is demonstrated. Scans along the direction of the poling field show that the second-order optical nonlinearity is located near the interface between differently doped glass layers. Both SHG and LEO measurements indicate that the ratio between the main elements of the second-order nonlinear optical susceptibility tensor, chi(33)((2)) and chi(31)((2)), is significantly smaller than three. (C) 2000 American Institute of Physics.",

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note = "Copyright (2000) American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics.",

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T1 - Second-harmonic imaging of poled silica waveguides

AU - Arentoft, Jesper

AU - Pedersen, Kjeld

AU - Bozhevolnyi, Sergey I.

AU - Kristensen, Martin

AU - Yu, Ping

AU - Nielsen, Christian Bergenstof

N1 - Copyright (2000) American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics.

PY - 2000

Y1 - 2000

N2 - Electric-field poled silica-based waveguides are characterized by measurements of second-harmonic generation (SHG) and of the linear electro-optic effect (LEO). A SHG scanning technique allowing for high-resolution imaging of poled devices is demonstrated. Scans along the direction of the poling field show that the second-order optical nonlinearity is located near the interface between differently doped glass layers. Both SHG and LEO measurements indicate that the ratio between the main elements of the second-order nonlinear optical susceptibility tensor, chi(33)((2)) and chi(31)((2)), is significantly smaller than three. (C) 2000 American Institute of Physics.

AB - Electric-field poled silica-based waveguides are characterized by measurements of second-harmonic generation (SHG) and of the linear electro-optic effect (LEO). A SHG scanning technique allowing for high-resolution imaging of poled devices is demonstrated. Scans along the direction of the poling field show that the second-order optical nonlinearity is located near the interface between differently doped glass layers. Both SHG and LEO measurements indicate that the ratio between the main elements of the second-order nonlinear optical susceptibility tensor, chi(33)((2)) and chi(31)((2)), is significantly smaller than three. (C) 2000 American Institute of Physics.

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JO - Applied Physics Letters

JF - Applied Physics Letters

IS - 1

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Second-harmonic imaging of poled silica waveguides

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