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Near-surface modification of the third-order nonlinear susceptibility in thermally poled Infrasil™ glasses
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10.1063/1.1921348
/content/aip/journal/apl/86/18/10.1063/1.1921348
http://aip.metastore.ingenta.com/content/aip/journal/apl/86/18/10.1063/1.1921348
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Bottom: Evolution of the etching rate (normalized to the value in the unpoled region) as a function of the depth under the anode. Top: Built-in electric field distribution versus depth under anode. has been deduced from Eq. (2).

Image of FIG. 2.
FIG. 2.

Bottom: Nonlinear distribution as a function of the depth under the anode. The NL coefficient has been obtained using the method described in Ref. 5. Top: Evolution of the square root of the SH signal.

Image of FIG. 3.
FIG. 3.

Deduced third-order nonlinear susceptibility as a function of the position across the nonlinear region.

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/content/aip/journal/apl/86/18/10.1063/1.1921348
2005-04-27
2014-04-20
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Near-surface modification of the third-order nonlinear susceptibility in thermally poled Infrasil™ glasses
http://aip.metastore.ingenta.com/content/aip/journal/apl/86/18/10.1063/1.1921348
10.1063/1.1921348
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