Ridged wave-guiding high-power semiconductor laser structure with conical gain zone

A technology of tapered gain region and ridge waveguide, which is applied in the field of ridge waveguide high-power semiconductor laser structure, can solve the problems of semiconductor laser maximum output power and beam quality limitation, multiple side modes, etc.
CN1681176AInactive Publication Date: 2005-10-12INST OF SEMICONDUCTORS - CHINESE ACAD OF SCI
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Patent Information

Authority / Receiving Office
CN · China
Patent Type
Applications(China)
Current Assignee / Owner
INST OF SEMICONDUCTORS - CHINESE ACAD OF SCI
Publication Date
2005-10-12
Estimated Expiration
Not applicable · inactive patent

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Abstract

The invention consists of a substrate, an AlGaAs layer that is made on the substrate, an AlGaInPAs active layer that is made on AlGaAs layer, an AlInAs layer that is made on AlGaInPAs active layer, an InP layer that is made on the AlInAs layer and has less area than AlInAs layer, an InGaAs layer that is made on InP layer and forms a ridge shape area with InGaAs layer, a media film layer that is made on both sides of the ridge shape area and AlInAS layer, a p-side electrode layer that is made on top of ridge shape area and media film, a n-side electrode that is made under the substrate.
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Description

technical field

[0001] The invention relates to a semiconductor laser structure, in particular to a ridge waveguide high-power semiconductor laser structure with a tapered gain region. Background technique

[0002] Semiconductor laser refers to a type of laser with semiconductor material as the working substance, also known as semiconductor laser diode, or laser diode for short, and the English abbreviation is LD. Its basic structure consists of three parts, that is, the working substance (active medium) that can generate stimulated emission with high efficiency, the resonant cavity that provides optical feedback, and the driving power supply. Since the resonator length of the semiconductor laser (that is, the length of the active medium) is very short, the only way to obtain the inversion of the number of particles in the active medium of the semiconductor laser to form the laser emission is to effectively inject high-concentration electrons and The injected electrons and ...

Claims

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