DE1278002C2 - LUMINESCENT DIODE FROM GAAS AS BASIC MATERIAL - Google Patents
LUMINESCENT DIODE FROM GAAS AS BASIC MATERIALInfo
- Publication number
- DE1278002C2 DE1278002C2 DE1966S0101435 DES0101435A DE1278002C2 DE 1278002 C2 DE1278002 C2 DE 1278002C2 DE 1966S0101435 DE1966S0101435 DE 1966S0101435 DE S0101435 A DES0101435 A DE S0101435A DE 1278002 C2 DE1278002 C2 DE 1278002C2
- Authority
- DE
- Germany
- Prior art keywords
- gaas
- conductive zone
- zone
- luminescent diode
- basic material
- 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
- 239000000463 material Substances 0.000 title claims description 3
- 230000005855 radiation Effects 0.000 claims description 8
- 238000010521 absorption reaction Methods 0.000 claims description 6
- 238000004020 luminiscence type Methods 0.000 claims description 5
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 3
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 229910052787 antimony Inorganic materials 0.000 description 1
- WATWJIUSRGPENY-UHFFFAOYSA-N antimony atom Chemical compound [Sb] WATWJIUSRGPENY-UHFFFAOYSA-N 0.000 description 1
- 229910052785 arsenic Inorganic materials 0.000 description 1
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical compound [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 229910052733 gallium Inorganic materials 0.000 description 1
- 229910052738 indium Inorganic materials 0.000 description 1
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical compound [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
- H10H20/00—Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
- H10H20/80—Constructional details
-
- C—CHEMISTRY; METALLURGY
- C09—DYES; PAINTS; POLISHES; NATURAL RESINS; ADHESIVES; COMPOSITIONS NOT OTHERWISE PROVIDED FOR; APPLICATIONS OF MATERIALS NOT OTHERWISE PROVIDED FOR
- C09K—MATERIALS FOR MISCELLANEOUS APPLICATIONS, NOT PROVIDED FOR ELSEWHERE
- C09K11/00—Luminescent, e.g. electroluminescent, chemiluminescent materials
- C09K11/08—Luminescent, e.g. electroluminescent, chemiluminescent materials containing inorganic luminescent materials
- C09K11/74—Luminescent, e.g. electroluminescent, chemiluminescent materials containing inorganic luminescent materials containing arsenic, antimony or bismuth
- C09K11/7492—Arsenides; Nitrides; Phosphides
Landscapes
- Chemical & Material Sciences (AREA)
- Inorganic Chemistry (AREA)
- Engineering & Computer Science (AREA)
- Materials Engineering (AREA)
- Organic Chemistry (AREA)
- Led Devices (AREA)
Description
Die Erfindung betrifft eine Lumineszenzdiode nach dem Oberbegriff des Patentanspruchs.The invention relates to a light emitting diode according to the preamble of the patent claim.
Bekanntlich ist in einer A1MBV-Lumineszenzdiode die Photonenenergie in der η-leitenden Zone meist größer als in der p-leitenden Zone. Das bedeutet, daß im wesentlichen nur die in der p-leitenden Zone erzeugte Lumineszenzstrahlung durch die η-leitende Zone nach außen gelangen kann, ohne stark absorbiert zu werden. Bei üblichen Betriebstemperaturen sind die Absorptionsverluste aber noch so hoch, daß nur wenige Prozent der in der p-leitenden Zone erzeugten Lumineszenzstrahlung die η-leitende Zone durchdringen kann.It is known that in an A 1M B V luminescent diode the photon energy in the η-conducting zone is usually greater than in the p-conducting zone. This means that essentially only the luminescence radiation generated in the p-conductive zone can reach the outside through the η-conductive zone without being strongly absorbed. At normal operating temperatures, however, the absorption losses are still so high that only a few percent of the luminescence radiation generated in the p-conductive zone can penetrate the η-conductive zone.
Zur Verringerung der Absorptionsverluste in der η-leitenden Zone ist es bekannt (J. Appl. Phys., Bd. 36, Nr. 2, 1965, S. 460 bis 461), eine Lumineszenzdiode auf GaAs-GaP-Basis zu verwenden, deren Absorptionsverluste beim Durchgang der in der p-leitenden Zone der Diode entstandenen Lumineszenzstrahlung durch die η-leitende Zone dadurch vermindert sind, daß mittels kontinuierlicher Änderung der Zusammensetzung des halbleitenden Grundmaterials die η-leitende Zone einen mit zunehmendem Abstand von pn-Übergang wachsenden effektiven Bandabstand hat. Hierzu wird auf einem Substrat aus einer Ga(As-P)-Legierung eine GaAs-Schicht epitaktisch abgeschieden.To reduce absorption losses in the In the η-conductive zone, it is known (J. Appl. Phys., Vol. 36, No. 2, 1965, pp. 460 to 461) to have a light-emitting diode To use GaAs-GaP base, whose absorption losses when passing through in the p-type zone of the Diode resulting luminescence radiation are reduced by the η-conductive zone that by means of continuous change in the composition of the semiconducting base material, the η-conductive zone the effective band gap increases with increasing distance from the pn junction. This is done on a Substrate made of a Ga (As-P) alloy, a GaAs layer is deposited epitaxially.
Es ist außerdem bekannt, daß die Intensität der austretenden Strahlung noch dadurch merklich erhöht werden kann, daß man dem η-dotierten Teil der Diode an der Außengrenze eine solche Form, etwa Weierstraß-Geometrie, gibt, daß die Strahlung auf diese Grenzfläche so auftrifft, daß sie praktisch ohne Totalreflexionsverluste nach außen durchtreten kann.It is also known that the intensity of the exiting radiation is noticeably increased as a result can be that the η-doped part of the diode at the outer border has a shape such as Weierstrass geometry, gives that the radiation impinges on this interface in such a way that it is practically without Total reflection losses can pass through to the outside.
Aufgabe der vorliegenden Erfindung ist es, die Lichtausbeute der A1MBV-Lumineszendiode darüber hinaus noch dadurch zu erhöhen, daß die Absorptionsverluste an Lumineszenzstrahlung längs des Weges von ihrer Entstehung am pn-Übergang durch die η-Zone der Diode bis hin zur äußeren Grenzfläche möglichst vermieden werden.The object of the present invention is to further increase the luminous efficiency of the A 1M B V luminescent diode by reducing the absorption losses of luminescent radiation along the path from its formation at the pn junction through the η zone of the diode to the outer interface should be avoided if possible.
Diese Aufgabe wird erfindungsgemäß durch die im kennzeichnenden Teil des Patentanspruchs angegebenen Merkmale gelöst.According to the invention, this object is given by what is stated in the characterizing part of the patent claim Features solved.
In der p-leitenden Zone ist also ein Teil des Galliums durch Indium und ein Teil des Arsens durch Antimon ersetzt. Dadurch und durch die Gegendotierung mit Sn wird in der p-leitenden Zone der Bandabstand verringert, so daß infolge der sprunghaften Änderung der effektiven Bandbreite am pn-Übergang ein größerer Anteil der in dieser Zone erzeugten Lumineszenzstrahlung ohne Absorption die η-leitende Zone durchqueren kann.In the p-conducting zone, therefore, part of the gallium is made up of indium and part of the arsenic is made up of antimony replaced. As a result of this and the counter-doping with Sn, the band gap is established in the p-conductive zone reduced, so that due to the sudden change in the effective bandwidth at the pn junction, a larger one Share of the luminescence radiation generated in this zone cross the η-conductive zone without absorption can.
Claims (1)
Priority Applications (9)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DES101436A DE1257965B (en) | 1966-01-14 | 1966-01-14 | AIIIBA light emitting diode, especially based on GaAs, with high light yield |
| DE1966S0101435 DE1278002C2 (en) | 1966-01-14 | 1966-01-14 | LUMINESCENT DIODE FROM GAAS AS BASIC MATERIAL |
| NL6616658A NL6616658A (en) | 1966-01-14 | 1966-11-25 | |
| GB1311/67A GB1156903A (en) | 1966-01-14 | 1967-01-10 | Improvements in or relating to Luminescent Diodes |
| AT28967A AT266939B (en) | 1966-01-14 | 1967-01-11 | A <III> B <V> luminescent diode |
| CH43167A CH459365A (en) | 1966-01-14 | 1967-01-12 | AIIIBv light emitting diode |
| FR90844A FR1507827A (en) | 1966-01-14 | 1967-01-12 | Light emitting diode |
| SE481/67A SE323144B (en) | 1966-01-14 | 1967-01-12 | |
| JP226967A JPS5132076B1 (en) | 1966-01-14 | 1967-01-13 |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DES101436A DE1257965B (en) | 1966-01-14 | 1966-01-14 | AIIIBA light emitting diode, especially based on GaAs, with high light yield |
| DE1966S0101435 DE1278002C2 (en) | 1966-01-14 | 1966-01-14 | LUMINESCENT DIODE FROM GAAS AS BASIC MATERIAL |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| DE1278002B DE1278002B (en) | 1968-09-19 |
| DE1278002C2 true DE1278002C2 (en) | 1977-11-03 |
Family
ID=25998341
Family Applications (2)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| DES101436A Pending DE1257965B (en) | 1966-01-14 | 1966-01-14 | AIIIBA light emitting diode, especially based on GaAs, with high light yield |
| DE1966S0101435 Expired DE1278002C2 (en) | 1966-01-14 | 1966-01-14 | LUMINESCENT DIODE FROM GAAS AS BASIC MATERIAL |
Family Applications Before (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| DES101436A Pending DE1257965B (en) | 1966-01-14 | 1966-01-14 | AIIIBA light emitting diode, especially based on GaAs, with high light yield |
Country Status (7)
| Country | Link |
|---|---|
| JP (1) | JPS5132076B1 (en) |
| CH (1) | CH459365A (en) |
| DE (2) | DE1257965B (en) |
| FR (1) | FR1507827A (en) |
| GB (1) | GB1156903A (en) |
| NL (1) | NL6616658A (en) |
| SE (1) | SE323144B (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3758875A (en) * | 1970-05-01 | 1973-09-11 | Bell Telephone Labor Inc | Double heterostructure junction lasers |
| GB8715211D0 (en) * | 1987-06-29 | 1987-08-05 | Secr Defence | Lensed photo detector |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR1416939A (en) * | 1963-12-12 | 1965-11-05 | Gen Electric | Improvements in optical transmission processes of alloyed semiconductor light sources |
-
1966
- 1966-01-14 DE DES101436A patent/DE1257965B/en active Pending
- 1966-01-14 DE DE1966S0101435 patent/DE1278002C2/en not_active Expired
- 1966-11-25 NL NL6616658A patent/NL6616658A/xx unknown
-
1967
- 1967-01-10 GB GB1311/67A patent/GB1156903A/en not_active Expired
- 1967-01-12 SE SE481/67A patent/SE323144B/xx unknown
- 1967-01-12 FR FR90844A patent/FR1507827A/en not_active Expired
- 1967-01-12 CH CH43167A patent/CH459365A/en unknown
- 1967-01-13 JP JP226967A patent/JPS5132076B1/ja active Pending
Also Published As
| Publication number | Publication date |
|---|---|
| GB1156903A (en) | 1969-07-02 |
| DE1257965B (en) | 1968-01-04 |
| JPS5132076B1 (en) | 1976-09-10 |
| DE1278002B (en) | 1968-09-19 |
| FR1507827A (en) | 1967-12-29 |
| CH459365A (en) | 1968-07-15 |
| SE323144B (en) | 1970-04-27 |
| NL6616658A (en) | 1967-07-17 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| E77 | Valid patent as to the heymanns-index 1977 | ||
| 8339 | Ceased/non-payment of the annual fee |