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Reflection second harmonic generation on a z-cut congruent lithium niobate crystal

Reflection second harmonic generation on a z-cut congruent lithium niobate crystal
Reflection second harmonic generation on a z-cut congruent lithium niobate crystal
Reflection second harmonic generation experiments were performed on z-cut congruent lithium niobate crystals (LiNbO3) to reveal the interfacial layer symmetry as the crystal is rotated around the z-axis. To suppress the bulk contribution, the fundamental wavelength was selected to be 532 nm resulting in second harmonic generation at a wavelength within the absorption region of the crystal. The polarity of the direction of the y-axis was determined from second harmonic generation data and used to show that this direction also inverts during domain inversion.
1550-235X
205424-[7pp]
Sono, T.J.
75e20011-f3af-4fb3-8dd4-f0cd05a840b3
Scott, J.G.
a5e576f1-39c6-4c3b-a0e2-42e388e9b583
Sones, C.L.
9de9d8ee-d394-46a5-80b7-e341c0eed0a8
Valdivia, C.E.
d9e77b23-1e72-4302-a11c-e6af43f0e518
Mailis, S.
233e0768-3f8d-430e-8fdf-92e6f4f6a0c4
Eason, R.W.
e38684c3-d18c-41b9-a4aa-def67283b020
Frey, J.G.
ba60c559-c4af-44f1-87e6-ce69819bf23f
Danos, L.
c831e137-37b9-42cc-ab8c-49de31038922
Sono, T.J.
75e20011-f3af-4fb3-8dd4-f0cd05a840b3
Scott, J.G.
a5e576f1-39c6-4c3b-a0e2-42e388e9b583
Sones, C.L.
9de9d8ee-d394-46a5-80b7-e341c0eed0a8
Valdivia, C.E.
d9e77b23-1e72-4302-a11c-e6af43f0e518
Mailis, S.
233e0768-3f8d-430e-8fdf-92e6f4f6a0c4
Eason, R.W.
e38684c3-d18c-41b9-a4aa-def67283b020
Frey, J.G.
ba60c559-c4af-44f1-87e6-ce69819bf23f
Danos, L.
c831e137-37b9-42cc-ab8c-49de31038922

Sono, T.J., Scott, J.G., Sones, C.L., Valdivia, C.E., Mailis, S., Eason, R.W., Frey, J.G. and Danos, L. (2006) Reflection second harmonic generation on a z-cut congruent lithium niobate crystal. Physical Review B, 74 (20), 205424-[7pp]. (doi:10.1103/PhysRevB.74.205424).

Record type: Article

Abstract

Reflection second harmonic generation experiments were performed on z-cut congruent lithium niobate crystals (LiNbO3) to reveal the interfacial layer symmetry as the crystal is rotated around the z-axis. To suppress the bulk contribution, the fundamental wavelength was selected to be 532 nm resulting in second harmonic generation at a wavelength within the absorption region of the crystal. The polarity of the direction of the y-axis was determined from second harmonic generation data and used to show that this direction also inverts during domain inversion.

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Published date: 20 November 2006

Identifiers

Local EPrints ID: 46934
URI: http://eprints.soton.ac.uk/id/eprint/46934
ISSN: 1550-235X
PURE UUID: 340bc810-9a40-455e-85df-89300a8e50c6
ORCID for S. Mailis: ORCID iD orcid.org/0000-0001-8100-2670
ORCID for R.W. Eason: ORCID iD orcid.org/0000-0001-9704-2204
ORCID for J.G. Frey: ORCID iD orcid.org/0000-0003-0842-4302

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Date deposited: 24 Jul 2007
Last modified: 16 Mar 2024 02:38

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Contributors

Author: T.J. Sono
Author: J.G. Scott
Author: C.L. Sones
Author: C.E. Valdivia
Author: S. Mailis ORCID iD
Author: R.W. Eason ORCID iD
Author: J.G. Frey ORCID iD
Author: L. Danos

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