Optical Frequency Conversion Device with Asymmetric k-dbr Structure

Kazuo Kasaya; Kiyoto Takahata; Hiroshi Yasaka

doi:10.1109/68.205625

Optical Frequency Conversion Device with Asymmetric k-dbr Structure

Kazuo Kasaya, Kiyoto Takahata, Hiroshi Yasaka

RIEC - Information Communication Platforms Division

Nippon Telegraph & Telephone

Research output: Contribution to journal › Article › peer-review

4 Citations (Scopus)

Abstract

An optical-frequency conversion device is fabricated, using monolithically integrated distributed Bragg reflector (DBR) mirrors with different coupling coefficients at the outer sides of the active and the saturable absorber regions. The input-end DBR mirror has higher coupling coefficient than that of the output-end DBR mirror. The converted light is reflected by the input-end DBR mirror and is emitted only from the output end of the device. This device successfully performs optical frequency conversion when the input TM-polarized light.

Original language	English
Pages (from-to)	321-324
Number of pages	4
Journal	IEEE Photonics Technology Letters
Volume	5
Issue number	3
DOIs	https://doi.org/10.1109/68.205625
Publication status	Published - 1993 Mar

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abstract = "An optical-frequency conversion device is fabricated, using monolithically integrated distributed Bragg reflector (DBR) mirrors with different coupling coefficients at the outer sides of the active and the saturable absorber regions. The input-end DBR mirror has higher coupling coefficient than that of the output-end DBR mirror. The converted light is reflected by the input-end DBR mirror and is emitted only from the output end of the device. This device successfully performs optical frequency conversion when the input TM-polarized light.",

author = "Kazuo Kasaya and Kiyoto Takahata and Hiroshi Yasaka",

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AU - Yasaka, Hiroshi

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AB - An optical-frequency conversion device is fabricated, using monolithically integrated distributed Bragg reflector (DBR) mirrors with different coupling coefficients at the outer sides of the active and the saturable absorber regions. The input-end DBR mirror has higher coupling coefficient than that of the output-end DBR mirror. The converted light is reflected by the input-end DBR mirror and is emitted only from the output end of the device. This device successfully performs optical frequency conversion when the input TM-polarized light.

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Optical Frequency Conversion Device with Asymmetric k-dbr Structure

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