GB1461199A - Semiconductor laser - Google Patents
Semiconductor laserInfo
- Publication number
- GB1461199A GB1461199A GB1172274A GB1172274A GB1461199A GB 1461199 A GB1461199 A GB 1461199A GB 1172274 A GB1172274 A GB 1172274A GB 1172274 A GB1172274 A GB 1172274A GB 1461199 A GB1461199 A GB 1461199A
- Authority
- GB
- United Kingdom
- Prior art keywords
- layer
- layers
- active layer
- carrier concentration
- concentration
- 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.)
- Expired
Links
- 239000004065 semiconductor Substances 0.000 title abstract 3
- 239000002019 doping agent Substances 0.000 abstract 3
- 229910001218 Gallium arsenide Inorganic materials 0.000 abstract 2
- 238000004519 manufacturing process Methods 0.000 abstract 1
- 239000000758 substrate Substances 0.000 abstract 1
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y20/00—Nanooptics, e.g. quantum optics or photonic crystals
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L33/0004—Devices characterised by their operation
- H01L33/002—Devices characterised by their operation having heterojunctions or graded gap
- H01L33/0025—Devices characterised by their operation having heterojunctions or graded gap comprising only AIIIBV compounds
-
- 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
- H01S5/30—Structure or shape of the active region; Materials used for the active region
- H01S5/34—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
- H01S5/343—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser
- H01S5/34313—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer having only As as V-compound, e.g. AlGaAs, InGaAs
-
- 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
-
- 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
- H01S5/34—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
- H01S5/343—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser
- H01S5/34313—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer having only As as V-compound, e.g. AlGaAs, InGaAs
- H01S5/3432—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer having only As as V-compound, e.g. AlGaAs, InGaAs the whole junction comprising only (AI)GaAs
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Nanotechnology (AREA)
- Power Engineering (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Computer Hardware Design (AREA)
- Life Sciences & Earth Sciences (AREA)
- Biophysics (AREA)
- Manufacturing & Machinery (AREA)
- Crystallography & Structural Chemistry (AREA)
- Semiconductor Lasers (AREA)
Abstract
1461199 Semi-conductor lasers MATSUSHITA ELECTRONICS CORP 15 March 1974 [20 March 1973 (2)] 11722/74 Headings H1C and H1K [Also in Division C4] In a double heterostructure semi-conductor laser the carrier concentration in its active layer 13, with reference to the thickness of this layer, has a maximum at the centre of the layer and parts of the active layer away from the centre have progressively lower carrier concentrations. The carrier concentration change may be of a step-wise character, Fig. 5 (not shown) or may be continuous, Fig. 7c (not shown). In the embodiment of Fig. 3, which is made by the epitaxial growth of layers 12, 13, 14 and 15 on a substrate 11, the active layer 13 is grown as a series of seven layers. In layers two to four, the concentration of Zn dopant in each layer is greater than in the previous layer, to reach a maximum dopant concentration in layer four. From layers four to seven this effect is reversed, to give a symmetrical step-like distribution of carrier concentration. In the embodiment of Fig. 6 the active layer 113 initially comprises three layers 41-43, 42 being Zn-doped GaAs while 41 and 43 are non-doped GaAs. After production by epitaxial growth of the entire element 111-115, it is heat-treated, causing the Zn dopant of layer 42 to diffuse outwards and produce a symmetrical bell-shaped distribution of carrier concentration (Fig. 7c).
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3236373A JPS49122290A (en) | 1973-03-20 | 1973-03-20 | |
JP3236273A JPS49122289A (en) | 1973-03-20 | 1973-03-20 |
Publications (1)
Publication Number | Publication Date |
---|---|
GB1461199A true GB1461199A (en) | 1977-01-13 |
Family
ID=26370916
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB1172274A Expired GB1461199A (en) | 1973-03-20 | 1974-03-15 | Semiconductor laser |
Country Status (3)
Country | Link |
---|---|
CA (1) | CA1009738A (en) |
FR (1) | FR2222773B1 (en) |
GB (1) | GB1461199A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1162673A2 (en) * | 2000-06-08 | 2001-12-12 | Eastman Kodak Company | Method of making an emissive layer for an organic light-emitting device |
CN100448044C (en) * | 2007-02-15 | 2008-12-31 | 华南师范大学 | Semiconductor heterozygote and its lighting transistor |
CN114374146A (en) * | 2020-10-15 | 2022-04-19 | 山东华光光电子股份有限公司 | GaAs-based 915nm/976nm high-power dual-wavelength laser epitaxial wafer and preparation method thereof |
-
1974
- 1974-03-15 GB GB1172274A patent/GB1461199A/en not_active Expired
- 1974-03-15 FR FR7408923A patent/FR2222773B1/fr not_active Expired
- 1974-03-18 CA CA195,291A patent/CA1009738A/en not_active Expired
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1162673A2 (en) * | 2000-06-08 | 2001-12-12 | Eastman Kodak Company | Method of making an emissive layer for an organic light-emitting device |
EP1162673A3 (en) * | 2000-06-08 | 2004-02-04 | Eastman Kodak Company | Method of making an emissive layer for an organic light-emitting device |
CN100448044C (en) * | 2007-02-15 | 2008-12-31 | 华南师范大学 | Semiconductor heterozygote and its lighting transistor |
CN114374146A (en) * | 2020-10-15 | 2022-04-19 | 山东华光光电子股份有限公司 | GaAs-based 915nm/976nm high-power dual-wavelength laser epitaxial wafer and preparation method thereof |
Also Published As
Publication number | Publication date |
---|---|
DE2413493B2 (en) | 1976-02-19 |
FR2222773B1 (en) | 1979-03-23 |
FR2222773A1 (en) | 1974-10-18 |
DE2413493A1 (en) | 1974-10-03 |
CA1009738A (en) | 1977-05-03 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PS | Patent sealed | ||
PE20 | Patent expired after termination of 20 years |
Effective date: 19940314 |