Mode reduction, Q loss, gain saturation, and bandfilling modification of the light versus current characteristics of thin (∼0.9 μm) quantum well heterostructure lasers
Data are presented demonstrating the effect that cavity length, and thus Q, has upon quantum well heterostructure edge-emitting laser diodes that are reduced to microcavity thickness. The lasers, with reduced mode density and enhanced spontaneous emission, are defined vertically by a Ag top-contact...
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Veröffentlicht in: | Journal of applied physics 1996-06, Vol.79 (11), p.8829-8831 |
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container_title | Journal of applied physics |
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creator | Evans, P. W. Holonyak, N. Ries, M. J. Chen, E. I. Minervini, A. D. |
description | Data are presented demonstrating the effect that cavity length, and thus Q, has upon quantum well heterostructure edge-emitting laser diodes that are reduced to microcavity thickness. The lasers, with reduced mode density and enhanced spontaneous emission, are defined vertically by a Ag top-contact mirror and a closely spaced (∼0.9 μm) high-contrast AlAs native oxide-GaAs distributed Bragg reflecting bottom mirror. For shorter and shorter diode lengths (700→70 μm, and still lesser mode density) the light versus current (L–I) characteristic below threshold is at first steeper and steeper (amplified stimulated emission), until, at a diode length of ∼100 μm, the loss in Q and insufficient gain are manifest as a downward bend in the L–I curve and a shift to higher threshold current where bandfilling to a higher state (shorter wavelength) contributes more gain. |
doi_str_mv | 10.1063/1.362562 |
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For shorter and shorter diode lengths (700→70 μm, and still lesser mode density) the light versus current (L–I) characteristic below threshold is at first steeper and steeper (amplified stimulated emission), until, at a diode length of ∼100 μm, the loss in Q and insufficient gain are manifest as a downward bend in the L–I curve and a shift to higher threshold current where bandfilling to a higher state (shorter wavelength) contributes more gain.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.362562</identifier><language>eng</language><ispartof>Journal of applied physics, 1996-06, Vol.79 (11), p.8829-8831</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c186t-ccc486ba50060d6f8e67ec6b5763d6b6491b5a54e6744b710be52bd4ead7c36d3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Evans, P. 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For shorter and shorter diode lengths (700→70 μm, and still lesser mode density) the light versus current (L–I) characteristic below threshold is at first steeper and steeper (amplified stimulated emission), until, at a diode length of ∼100 μm, the loss in Q and insufficient gain are manifest as a downward bend in the L–I curve and a shift to higher threshold current where bandfilling to a higher state (shorter wavelength) contributes more gain.</description><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1996</creationdate><recordtype>article</recordtype><recordid>eNotkFtKxEAURBtRcBwFl3A_RzBjd5LuJJ8y-IIREfQ79CuTljy0H4o7cC2uYdbgIlyJrfHnFtwqDkUhdEzwkmCWnZFlxlLK0h00I7iskoJSvItmGKckKaui2kcHzj1hTEiZVTP0eTsqDVarIL0Zh1O4h2507hQ23AzguA-WTwYfFIh4GtN1ZthAPyrTGPnnwtiAbzV0ZtN6eNXWBQcyWKsHD7LllkuvrXHeSDdlI3zx_bHFywq-tv0JvAQ--NDDm-46aHVMj87bWCrYiOUuIg_RXsM7p4_-dY4eLy8eVtfJ-u7qZnW-TiQpmU-klHnJBKcYM6xYU2pWaMkELVimmGB5RQTlNI_vPBcFwULTVKhcc1XIjKlsjhYTV8YOzuqmfram5_a9Jrj-3bgm9bRx9gObxnPm</recordid><startdate>19960601</startdate><enddate>19960601</enddate><creator>Evans, P. 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J.</creatorcontrib><creatorcontrib>Chen, E. I.</creatorcontrib><creatorcontrib>Minervini, A. D.</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Evans, P. W.</au><au>Holonyak, N.</au><au>Ries, M. J.</au><au>Chen, E. I.</au><au>Minervini, A. D.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Mode reduction, Q loss, gain saturation, and bandfilling modification of the light versus current characteristics of thin (∼0.9 μm) quantum well heterostructure lasers</atitle><jtitle>Journal of applied physics</jtitle><date>1996-06-01</date><risdate>1996</risdate><volume>79</volume><issue>11</issue><spage>8829</spage><epage>8831</epage><pages>8829-8831</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><abstract>Data are presented demonstrating the effect that cavity length, and thus Q, has upon quantum well heterostructure edge-emitting laser diodes that are reduced to microcavity thickness. The lasers, with reduced mode density and enhanced spontaneous emission, are defined vertically by a Ag top-contact mirror and a closely spaced (∼0.9 μm) high-contrast AlAs native oxide-GaAs distributed Bragg reflecting bottom mirror. For shorter and shorter diode lengths (700→70 μm, and still lesser mode density) the light versus current (L–I) characteristic below threshold is at first steeper and steeper (amplified stimulated emission), until, at a diode length of ∼100 μm, the loss in Q and insufficient gain are manifest as a downward bend in the L–I curve and a shift to higher threshold current where bandfilling to a higher state (shorter wavelength) contributes more gain.</abstract><doi>10.1063/1.362562</doi><tpages>3</tpages></addata></record> |
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title | Mode reduction, Q loss, gain saturation, and bandfilling modification of the light versus current characteristics of thin (∼0.9 μm) quantum well heterostructure lasers |
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