JPS6450489A - Semiconductor laser - Google Patents
Semiconductor laserInfo
- Publication number
- JPS6450489A JPS6450489A JP20788887A JP20788887A JPS6450489A JP S6450489 A JPS6450489 A JP S6450489A JP 20788887 A JP20788887 A JP 20788887A JP 20788887 A JP20788887 A JP 20788887A JP S6450489 A JPS6450489 A JP S6450489A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- inp
- semiconductor laser
- reduce
- whole length
- 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
- H01S5/305—Structure or shape of the active region; Materials used for the active region characterised by the doping materials used in the laser 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
- H01S5/10—Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
-
- 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
- H01S5/3235—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 longer than 1000 nm, e.g. InP-based 1300 nm and 1500 nm lasers
- H01S5/32391—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 longer than 1000 nm, e.g. InP-based 1300 nm and 1500 nm lasers based on In(Ga)(As)P
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Optics & Photonics (AREA)
- Semiconductor Lasers (AREA)
Abstract
PURPOSE:To reduce an oscillation threshold value and to remarkably widen an application range by a method wherein an active layer is divided in two in a longitudinal direction, and its part is doped with Er atoms. CONSTITUTION:A structure having a barrier layer 3 made of InP, an active layer 4 made of InGaAsP, and an upper barrier layer 5 made InP is provided through a buffer layer 2 on a crystalline substrate 1, and 1 atomic % of Er is contained in the half part 6 of the whole length of the layer. Thus, its threshold current value becomes substantially similar to that of a semiconductor laser which contains no Er. In order to sufficiently perform this effect, it is necessary to set the Er-doping region to a range of 1/4-3/4 of the whole length of the layer. Thus, the wavelength selecting effect is accelerated to reduce its threshold value.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20788887A JPS6450489A (en) | 1987-08-20 | 1987-08-20 | Semiconductor laser |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20788887A JPS6450489A (en) | 1987-08-20 | 1987-08-20 | Semiconductor laser |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6450489A true JPS6450489A (en) | 1989-02-27 |
Family
ID=16547227
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP20788887A Pending JPS6450489A (en) | 1987-08-20 | 1987-08-20 | Semiconductor laser |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6450489A (en) |
-
1987
- 1987-08-20 JP JP20788887A patent/JPS6450489A/en active Pending
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