JPS56131989A - Semiconductor laser - Google Patents
Semiconductor laserInfo
- Publication number
- JPS56131989A JPS56131989A JP3529680A JP3529680A JPS56131989A JP S56131989 A JPS56131989 A JP S56131989A JP 3529680 A JP3529680 A JP 3529680A JP 3529680 A JP3529680 A JP 3529680A JP S56131989 A JPS56131989 A JP S56131989A
- Authority
- JP
- Japan
- Prior art keywords
- active region
- difference
- thickness
- mode
- refractive index
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/30—Structure or shape of the active region; Materials used for the active region
- H01S5/32—Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/20—Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers
- H01S5/22—Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers having a ridge or stripe structure
- H01S5/223—Buried stripe structure
- H01S5/2238—Buried stripe structure with a terraced structure
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/20—Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers
- H01S5/2054—Methods of obtaining the confinement
- H01S5/2059—Methods of obtaining the confinement by means of particular conductivity zones, e.g. obtained by particle bombardment or diffusion
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/30—Structure or shape of the active region; Materials used for the active region
- H01S5/32—Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures
- H01S5/3201—Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures incorporating bulkstrain effects, e.g. strain compensation, strain related to polarisation
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/30—Structure or shape of the active region; Materials used for the active region
- H01S5/32—Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures
- H01S5/323—Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser
- H01S5/32308—Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser emitting light at a wavelength less than 900 nm
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Optics & Photonics (AREA)
- Geometry (AREA)
- Semiconductor Lasers (AREA)
Abstract
PURPOSE:To realize single-mode oscillation with ease by holding an active layer between two curved parts at the position above the level-difference part of a substrate. CONSTITUTION:When the active region is made to have a difference in thickness, there occurs a large difference in refractive index and thereby the condition for a single mode is narrowed. Therefore, the thickness of the active region is made to be fixed both in a part immediately above the level-difference part and in the flat part thereof or to be smaller by several percents in the bend part thereof, and thus it is made to vary moderately with some curvature. Accordingly, the difference in refractive index between the curved part and flat part of the active region depends only on the thickness of the 1st clad layer located between the active region 10 and the substrate 8, and thus it becomes a small value of the about 10<-5>. Therefore, even when the length between two curved parts is extended to about 5mum, the oscillation of a single horizontal mode is possible. In order to confine electric current effectively in the active region 10, it suffices when a cap layer 13 is formed to be n-GaAs, Zn diffusion 14 is performed and thus a part of a diffused front is formed to reach p-Ga1-xAlxAs 11.
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3529680A JPS56131989A (en) | 1980-03-19 | 1980-03-19 | Semiconductor laser |
US06/224,821 US4392227A (en) | 1980-01-14 | 1981-01-13 | Terraced substrate semiconductor laser |
EP81100192A EP0032401B1 (en) | 1980-01-14 | 1981-01-13 | Semiconductor laser |
CA000368427A CA1154852A (en) | 1980-01-14 | 1981-01-13 | Semiconductor laser |
DE8181100192T DE3171754D1 (en) | 1980-01-14 | 1981-01-13 | Semiconductor laser |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3529680A JPS56131989A (en) | 1980-03-19 | 1980-03-19 | Semiconductor laser |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS56131989A true JPS56131989A (en) | 1981-10-15 |
Family
ID=12437804
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3529680A Pending JPS56131989A (en) | 1980-01-14 | 1980-03-19 | Semiconductor laser |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS56131989A (en) |
-
1980
- 1980-03-19 JP JP3529680A patent/JPS56131989A/en active Pending
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