JPH03225969A - Manufacture of light-emitting element - Google Patents
Manufacture of light-emitting elementInfo
- Publication number
- JPH03225969A JPH03225969A JP2020695A JP2069590A JPH03225969A JP H03225969 A JPH03225969 A JP H03225969A JP 2020695 A JP2020695 A JP 2020695A JP 2069590 A JP2069590 A JP 2069590A JP H03225969 A JPH03225969 A JP H03225969A
- Authority
- JP
- Japan
- Prior art keywords
- gas
- injection layer
- light
- emitting layer
- hole injection
- 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
- 238000004519 manufacturing process Methods 0.000 title claims description 10
- 239000007789 gas Substances 0.000 claims abstract description 91
- 238000002347 injection Methods 0.000 claims abstract description 52
- 239000007924 injection Substances 0.000 claims abstract description 52
- BLRPTPMANUNPDV-UHFFFAOYSA-N Silane Chemical compound [SiH4] BLRPTPMANUNPDV-UHFFFAOYSA-N 0.000 claims abstract description 24
- 238000000034 method Methods 0.000 claims abstract description 19
- 238000005229 chemical vapour deposition Methods 0.000 claims abstract description 14
- 239000004215 Carbon black (E152) Substances 0.000 claims abstract description 13
- 229930195733 hydrocarbon Natural products 0.000 claims abstract description 13
- 150000002430 hydrocarbons Chemical class 0.000 claims abstract description 13
- 229910003481 amorphous carbon Inorganic materials 0.000 claims abstract description 8
- 239000012535 impurity Substances 0.000 claims abstract description 6
- 239000012495 reaction gas Substances 0.000 claims abstract description 6
- 229910021417 amorphous silicon Inorganic materials 0.000 claims abstract description 4
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 claims abstract description 4
- 239000000758 substrate Substances 0.000 claims description 18
- 229910052990 silicon hydride Inorganic materials 0.000 claims description 15
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 claims description 5
- 238000010030 laminating Methods 0.000 claims description 5
- 239000000203 mixture Substances 0.000 abstract description 6
- 229910052710 silicon Inorganic materials 0.000 abstract description 5
- 229910052739 hydrogen Inorganic materials 0.000 abstract description 3
- 239000010408 film Substances 0.000 description 20
- 239000000463 material Substances 0.000 description 12
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 10
- 230000003287 optical effect Effects 0.000 description 8
- 238000004020 luminiscence type Methods 0.000 description 5
- 239000002194 amorphous carbon material Substances 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 238000005424 photoluminescence Methods 0.000 description 4
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical group [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 2
- 150000001721 carbon Chemical group 0.000 description 2
- 229910052799 carbon Inorganic materials 0.000 description 2
- 239000003086 colorant Substances 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- 101100497957 Caenorhabditis elegans cyn-2 gene Proteins 0.000 description 1
- 229910004613 CdTe Inorganic materials 0.000 description 1
- VGGSQFUCUMXWEO-UHFFFAOYSA-N Ethene Chemical compound C=C VGGSQFUCUMXWEO-UHFFFAOYSA-N 0.000 description 1
- 239000005977 Ethylene Substances 0.000 description 1
- -1 GaAsP Inorganic materials 0.000 description 1
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 238000001311 chemical methods and process Methods 0.000 description 1
- 210000000078 claw Anatomy 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 230000000379 polymerizing effect Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 229910010271 silicon carbide Inorganic materials 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- XOLBLPGZBRYERU-UHFFFAOYSA-N tin dioxide Chemical compound O=[Sn]=O XOLBLPGZBRYERU-UHFFFAOYSA-N 0.000 description 1
- 229910001887 tin oxide Inorganic materials 0.000 description 1
Landscapes
- Led Devices (AREA)
Abstract
Description
【発明の詳細な説明】
A、産業上の利用分野
本発明はアモルファス半導体よりなる発光素子の製造方
法に関するものである。DETAILED DESCRIPTION OF THE INVENTION A. Field of Industrial Application The present invention relates to a method of manufacturing a light emitting device made of an amorphous semiconductor.
B1発明の概要
本発明は、発光層の両面に夫々正孔注入層及び電子注入
層を積層してなる発光素子の製造方法において、
低圧の水素ガスと炭化水素ガスと水素化ケイ素ガスとを
反応ガスとしたプラズマ化学的蒸着法により得られたア
モルファス炭素系膜を発光層として用いると共に、炭化
水素ガスに対する水素化ケイ素ガスの混合比を正孔注入
層〈発光層〈電子注入層の関係とすることによって、発
光層の発光特性が良好であり、しかもこの特性を十分引
き出せるようにしたものである。B1 Summary of the Invention The present invention provides a method for manufacturing a light emitting device in which a hole injection layer and an electron injection layer are laminated on both sides of a light emitting layer, in which low pressure hydrogen gas, hydrocarbon gas, and silicon hydride gas are reacted. An amorphous carbon-based film obtained by a plasma chemical vapor deposition method in the form of a gas is used as a light-emitting layer, and the mixing ratio of silicon hydride gas to hydrocarbon gas is set in the relationship of hole-injection layer <light-emitting layer><electron-injection layer. As a result, the light-emitting layer has good light-emitting properties, and this property can be fully brought out.
C従来の技術
従来、発光材料としては、発光ダイオードの月料である
GaAs、GaAsP、GaP、GaAQAsZnSe
xTe+−x、Znx’ Cd+−xTe、CdTeな
どがある。C. Conventional technology Conventionally, light-emitting materials such as GaAs, GaAsP, GaP, and GaAQAsZnSe, which are used for light-emitting diodes, have been used as light-emitting materials.
Examples include xTe+-x, Znx' Cd+-xTe, and CdTe.
B3発明が解決しようとする課題
しかしながら、このような従来の発光材料にあっては、
例えば、GaPではビーク波長(発光エネルギーがピー
クとなる波長)が698nm、光学的エネルギーギャッ
プが1.76eVというように、ピーク波長、光学的エ
ネルギーギヤ・ツブは、その発光材料に固有のものであ
る。このため発光素材としての発光特性を変えたいとき
は、所要ノ特性を有する発光材料を選択することが必要
となり、ともすると所要のピーク波長、光学的エネルギ
ーギャップに由来する特性を得られない場合が生ずる問
題点があった。B3 Problems to be solved by the invention However, with such conventional luminescent materials,
For example, in GaP, the peak wavelength (the wavelength at which the emission energy peaks) is 698 nm, and the optical energy gap is 1.76 eV.The peak wavelength and optical energy gap are unique to the luminescent material. . Therefore, when you want to change the luminescent properties of a luminescent material, it is necessary to select a luminescent material that has the required properties, and in some cases, you may not be able to obtain the properties derived from the required peak wavelength and optical energy gap. There were some problems that arose.
こうしたことからCVD法を利用してアモルファス炭素
系物質を生成し、これを発光材料に適用することが検討
されている。具体的にはこのアモルファス炭素系物質は
、真空容器内で、基板温度を例えば300℃以下に保ち
、例えば133.3mPa〜6X133.3Paの水素
ガス存在下で高周波電圧または直流電圧を印加してプラ
ズマCVD法(P−CVD法)を行うことにより生成さ
れる。For this reason, it is being considered to generate an amorphous carbon-based material using the CVD method and apply it to a light-emitting material. Specifically, this amorphous carbon-based material is produced by maintaining the substrate temperature at, for example, 300°C or less in a vacuum container and applying a high frequency voltage or DC voltage in the presence of hydrogen gas of, for example, 133.3 mPa to 6 x 133.3 Pa to generate plasma. It is generated by performing the CVD method (P-CVD method).
このような物質よりなる発光材料は、大きな光学的エネ
ルギーギャップを有する(耐熱的には300℃までその
ギャップは変化しない)と共に任意の光学的エネルギー
ギャップ及び発光特性を、CVD法の条件のコントロー
ルにより得られるため、要望に応じた材料が容易に得ら
れるという利点がある。この発光材料よりなる膜は光学
的エネルギーギャップ(Ego)の大小により強力なフ
ォトルミネッセンス(PL)が観察される。第3図にE
goとP Lのピーク値との関係を示す。特にEgoが
30V程度の膜は青白発光することからアモルファスの
特性を生かした大面積の青色発光パネルを実現させる可
能性がある。更に種々のEgoを選択することにより赤
から青までの色をデユーナブルに出す発光素子を作るこ
ともできる。Luminescent materials made of such substances have a large optical energy gap (in terms of heat resistance, the gap does not change up to 300°C), and can have arbitrary optical energy gaps and luminescent properties by controlling the conditions of the CVD method. Therefore, it has the advantage that it is easy to obtain a material that meets your needs. In a film made of this luminescent material, strong photoluminescence (PL) is observed depending on the size of the optical energy gap (Ego). E in Figure 3
The relationship between go and the peak value of P L is shown. In particular, since a film with an Ego of about 30 V emits blue-white light, there is a possibility of realizing a large-area blue light-emitting panel that takes advantage of the amorphous characteristics. Furthermore, by selecting various Ego's, it is also possible to create a light emitting element that repeatedly emits colors from red to blue.
またEgoの大小によるPL強度についても室温観察で
非常に強い発光を示し、大画面を有するフラットパネル
デイスプレィへと応用を広げることのできる発光素子材
料(R,G、83元色を作るもの)として有望なもので
ある。Furthermore, regarding the PL intensity depending on the size of Ego, it shows very strong light emission when observed at room temperature, and is a light emitting element material (one that creates R, G, 83 elemental colors) that can be used to expand its application to flat panel displays with large screens. This is promising.
ところでこのような物質よりなる膜を発光層としたLE
D(Light EmittingDiode)を作
る場合、電子と正孔を発光層に注入する注入層が必要で
あり、この注入層としては、半導体化したp型、n型の
上記のアモルファス炭素系物質を用いることが最良であ
る。しかしながらこの物質を注入層として用いる場合、
目標特性であるEgo>2eV、ρ(抵抗率)≦I06
Ω・cmを有するp型、n型膜を作ることが非常に難し
く、この問題点が上記のアモルファス炭素系物質の発光
素子への適用を妨げている。By the way, LE with a film made of such a substance as a light-emitting layer
When creating a D (Light Emitting Diode), an injection layer is required to inject electrons and holes into the light emitting layer, and as this injection layer, the above-mentioned amorphous carbon-based material of semiconducting p-type or n-type can be used. is the best. However, when using this material as an injection layer,
Target characteristics Ego>2eV, ρ (resistivity)≦I06
It is very difficult to make p-type and n-type films having Ω·cm, and this problem prevents the application of the above-mentioned amorphous carbon-based material to light-emitting devices.
本発明の目的は、任意の光学的エネルギーギャップ及び
発光特性を発光層に付与することができ、しかも発光層
の特性を十分に引き出すことのできる発光素子の製造方
法を提供することにある。An object of the present invention is to provide a method for manufacturing a light-emitting element that can impart arbitrary optical energy gaps and light-emitting characteristics to a light-emitting layer and can fully bring out the characteristics of the light-emitting layer.
E9課題を解決するための手段及び作用本発明は、炭化
水素ガスと水素化ケイ素ガスとn型不純物ガスとを含む
低圧の反応ガスを真空容器内でグロー放電させて分解ガ
スを重合させるプラズマ化学的蒸着法によりp型のアモ
ルファス炭素系膜よりなる正孔注入層を生成する工程と
、低圧の水素ガスと炭化水素ガスと水素化ケイ素ガスと
を反応ガスとし、炭化水素ガスに対する水素化ケイ素ガ
スの混合比を正孔注入層におiJる同混合比よりも大き
くしたプラズマ化学的蒸着法によりアモルファス炭素系
膜よりなる発光層を曲部正孔注入層」二に積層する工程
と、
炭化水素ガスと水素化ケイ素ガスとn型不純物ガスとを
含み、炭化水素ガスに対する水素化ケイ素ガスの混合比
が前記発光層における同混合比よりも大きい反応ガスを
真空容器内でクロー放電させて分解ガスを重合させるプ
ラズマ化学的蒸着法によりn型のアモルファス炭化ケイ
素膜よりなる電子注入層を前記発光層上に積層する工程
とを含むことを特徴とする。E9 Means and operation for solving the problem The present invention is a plasma chemistry method in which a low-pressure reaction gas containing a hydrocarbon gas, a silicon hydride gas, and an n-type impurity gas is glow-discharged in a vacuum container to polymerize a decomposed gas. A process of generating a hole injection layer made of a p-type amorphous carbon film by a selective evaporation method, and using low-pressure hydrogen gas, hydrocarbon gas, and silicon hydride gas as reaction gases, and forming a silicon hydride gas for the hydrocarbon gas. a step of laminating a light-emitting layer made of an amorphous carbon-based film on the curved hole-injection layer by a plasma chemical vapor deposition method in which the mixing ratio of iJ is larger than the same mixing ratio of the hole-injection layer; A reaction gas containing silicon hydride gas, silicon hydride gas, and n-type impurity gas, in which the mixing ratio of silicon hydride gas to hydrocarbon gas is larger than the same mixing ratio in the light emitting layer, is subjected to claw discharge in a vacuum container to produce decomposed gas. The method is characterized in that it includes a step of laminating an electron injection layer made of an n-type amorphous silicon carbide film on the light emitting layer by a plasma chemical vapor deposition method of polymerizing.
また、本発明では、正孔注入層の生成工程における基板
温度を、発光層及び電子注入層の各生成工程における基
板温度以上の大きさにすることが好ましい。Further, in the present invention, it is preferable that the substrate temperature in the step of forming the hole injection layer is higher than the substrate temperature in each step of forming the light emitting layer and the electron injection layer.
F 実施例
第1図は本発明方法により得られた発光素子の実施例を
示す構成図である。第1図中は例えば63cyn2程度
の面積をもつガラス基板、2は酸化錫よりなる透明電極
、3はB”をドーパントした30nm程度の厚さのp型
のアモルファス炭素系膜(以下ra−C:Si、H膜J
という)よりなる正孔注入層、4は300nmの厚さの
a−C:Si、H膜よりなる発光層、5はP5゛をドー
パントした50nm程度の厚さのn型のアモルファス炭
化ケイ素膜(以下ra−3tC膜」という)よりなる電
子注入層、6はアルミニウム電極である。F. Example FIG. 1 is a block diagram showing an example of a light emitting device obtained by the method of the present invention. In FIG. 1, for example, a glass substrate with an area of about 63 cyn2, 2 a transparent electrode made of tin oxide, and 3 a p-type amorphous carbon-based film doped with B'' and having a thickness of about 30 nm (hereinafter ra-C) are shown. Si, H film J
4 is a light-emitting layer made of a-C:Si,H film with a thickness of 300 nm, and 5 is an n-type amorphous silicon carbide film doped with P5' and with a thickness of about 50 nm ( 6 is an aluminum electrode.
各アモルファス薄膜は、真空槽、ガス導入系ガス排気系
あるいは高周波電源(または直流電源)等を具備した一
般的なP−CVD装置により作製することができる。Each amorphous thin film can be produced using a general P-CVD apparatus equipped with a vacuum chamber, a gas introduction system, a gas exhaust system, a high frequency power supply (or a DC power supply), and the like.
ここで発光素子を製造する場合の製造条件の3つの例(
試料1〜3)を以下に挙げる。Here are three examples of manufacturing conditions for manufacturing light emitting devices (
Samples 1 to 3) are listed below.
(+、 )試料1について
■正孔注入層
真空容器内ガス圧力 26.7Pa (0,2To
rr)基 板 温 度 275℃CH4ガ
ス:SiH,ガス
9:1
B2Hoプjス・(CI−14プjス+SiH4ガス)
3:]000
高周波電源電力
0W
(入力電極面積に対し0
] 25 W/am2)
■発
光
層
真空容器内混合ガス(CH,とH2と5iH4)圧力2
6.7Pa (0
To r r)
CI−1,に対する5iI44ガスの混合比12%
基
板
温
度
250°C
高周波電源電力
0W
■電子注入層
真空容器内ガス圧力
26.7Pa(0
’I’orr)
基
板
温
度
506C
CH4ガス:SjH,ガス
3・2
P I(3ガス
(CH,ガス+5iHaガス)
5.8
000
1
高周波電源電力
0W
(入ツノ電極面積に対し0
125 W/crtrす
(2)試料2について
■正孔注入層
H4
iHt
1とした他は試料1と同じ
条件で製造した。(+, ) Regarding sample 1 ■ Hole injection layer gas pressure inside vacuum container 26.7Pa (0.2To
rr) Substrate temperature 275℃ CH4 gas: SiH, gas 9:1 B2Ho gas (CI-14 gas + SiH4 gas)
3:]000 High frequency power source power 0W (0 for input electrode area] 25 W/am2) ■ Light emitting layer mixed gas (CH, H2 and 5iH4) in vacuum container pressure 2
6.7 Pa (0 Torr) Mixing ratio of 5iI44 gas to CI-1: 12% Substrate temperature 250°C High frequency power source power 0W ■Electron injection layer vacuum vessel internal gas pressure 26.7 Pa (0 'I'orr) Substrate Temperature 506C CH4 gas: SjH, gas 3.2 PI (3 gases (CH, gas + 5iHa gas) Regarding ■ Hole injection layer H4 iHt was manufactured under the same conditions as Sample 1 except that it was 1.
■発
光
層
CH4ガスに対するSiH4ガスの混合比を15%とし
た他は試料1と同じ条件で製造した。(2) Light emitting layer This was manufactured under the same conditions as Sample 1 except that the mixing ratio of SiH4 gas to CH4 gas was 15%.
■電子注入層 試料1と同じ条件で製造した。■Electron injection layer It was manufactured under the same conditions as Sample 1.
(3)試料3について ■正孔注入層 Cl44 : S i H4 ■とした他は試料1と同じ 条件で製造した。(3) About sample 3 ■Hole injection layer Cl44: S i H4 Same as sample 1 except for ■ Manufactured under the following conditions.
2
■発光層
CH4ガスに対するSiH4ガスの混合比を25%とし
た他は試料Iと同じ条件で製造した。2 (2) Light-emitting layer This was manufactured under the same conditions as Sample I except that the mixing ratio of SiH4 gas to CH4 gas was 25%.
■電子注入層 試料1と同じ条件で製造した。■Electron injection layer Manufactured under the same conditions as Sample 1.
以上の各試料1〜3について波長とE L強度との関係
を調べたところ第3図に示す関係が得られた。同図中実
線■〜■のグラフは夫々試料1〜3に対応する。このよ
うに良好な発光特性を得るためには、発光層の製膜に用
いるメタンガスに対する水素化ケイ素ガスの混合比は5
〜35%であることが好ましい。ただし正孔注入層、発
光層及び電子注入層の生成工程における、メタンガスに
対する水素化ケイ素ガスの濃度を夫々AP、AL。When the relationship between wavelength and EL intensity was investigated for each of the above samples 1 to 3, the relationship shown in FIG. 3 was obtained. In the same figure, solid lines ■ to ■ correspond to samples 1 to 3, respectively. In order to obtain such good luminescent properties, the mixing ratio of silicon hydride gas to methane gas used for forming the luminescent layer must be 5.
It is preferably 35%. However, in the production steps of the hole injection layer, light emitting layer, and electron injection layer, the concentrations of silicon hydride gas relative to methane gas are AP and AL, respectively.
ANとすると、A p< A I、< A Nとする必
要がある。When AN, it is necessary to satisfy A p < A I and < A N.
その理由は、ケイ素原子の含有量に対する炭素原子の含
有率について、正孔注入層よりも発光層を小さくし、か
つ発光層よりも電子注入層を小さくするためである。The reason for this is to make the light-emitting layer smaller than the hole-injection layer and to make the electron-injection layer smaller than the light-emission layer in terms of the carbon atom content relative to the silicon atom content.
いずれの試料1〜3も目視で十分観察できる発光を示し
、十分な発光特性を有していることが判った。試験に用
いた順方向バイアス電圧は5Vであり、電流密度は20
0mA/cz2であった。また基板温度についてはa−
C:Si、H膜の耐熱性により制限されるが、a−C:
Si、I−1膜は350℃以上に加熱されるとEgoが
低下し、かつ膜厚が小さくなるため、350℃程度が限
界である。It was found that all Samples 1 to 3 exhibited sufficient luminescence that could be observed visually, and had sufficient luminescent properties. The forward bias voltage used in the test was 5V, and the current density was 20
It was 0 mA/cz2. Regarding the substrate temperature, a-
C: Limited by the heat resistance of Si, H film, a-C:
When the Si, I-1 film is heated to 350°C or higher, Ego decreases and the film thickness becomes small, so about 350°C is the limit.
ここで上記の試料1〜3においては、各層を生成する工
程で用いる炭化水素ガスとしてCH4ガスを使用してい
るが、本発明ではCH4ガスに限定されるものではなく
、例えばC2H4ガスを用いてもよい。このようにC2
H4ガスを用いて製造した試料(4〜6)の製造条件を
次に記述する。Here, in the above samples 1 to 3, CH4 gas is used as the hydrocarbon gas used in the process of generating each layer, but the present invention is not limited to CH4 gas, and for example, C2H4 gas may be used. Good too. In this way C2
The manufacturing conditions for samples (4 to 6) manufactured using H4 gas will be described below.
(1)試料4について
■正孔注入層
真空容器内ガス圧力 26.7Pa (0,2To
rr)基 板 温 度 275°CC2H
4ガス:SiH4ガス 9.1
B 2 Hoガス:(C2F(、ガス+5i)Lガス)
3:1000高周波電源電力 10W
(入力電極面積に対し0 、125 W/cm2)■発
光層
真空容器内混合ガス(C2H4とH2とS jH4)圧
力26.7P2L(0,2
Torr)
5
C2H4に対するSiH4ガスの混合比12%
基
板
温
度
250°C
高周波電源電力
0W
■電子注入層
真空容器内ガス圧力
6
7Pa (0
’I’orr)
基
板
温
度
250°C
C2H4ガス
SiH+ガス
3:2
PI43ガス・(C2H4ガス+SiH4ガス)5.8
000
高周波電源電力
0W
(入力電極面積に対し0.125W/cが)(2)試料
5について
■正孔注入層
C7H4: S i H4
1とした他は試料Iと同じ
条件で製造した。(1) Regarding sample 4 ■ Hole injection layer gas pressure inside vacuum container 26.7Pa (0.2To
rr) Substrate temperature 275°CC2H
4 gas: SiH4 gas 9.1 B 2 Ho gas: (C2F (, gas + 5i) L gas)
3:1000 High frequency power supply power 10W (0 to input electrode area, 125 W/cm2) ■ Light emitting layer Mixed gas in vacuum container (C2H4, H2 and S jH4) Pressure 26.7P2L (0.2 Torr) 5 SiH4 to C2H4 Gas mixture ratio 12% Substrate temperature 250°C High frequency power supply power 0W ■Electron injection layer vacuum chamber internal gas pressure 6 7 Pa (0 'I'orr) Substrate temperature 250°C C2H4 gas SiH + gas 3:2 PI43 gas (C2H4 gas + SiH4 gas) 5.8 000 High frequency power source power 0W (0.125W/c for the input electrode area) (2) Regarding sample 5■ Hole injection layer C7H4: Same as sample I except that SiH4 was set to 1 Manufactured under the following conditions.
■発
光
層
6
C2H,ガスに対するSiH4ガスの混合比を15%と
した他は試料1と同じ条件で製造した。(2) Light emitting layer 6 This was manufactured under the same conditions as Sample 1 except that the mixing ratio of SiH4 gas to C2H gas was 15%.
■電子注入層 試料Iと同じ条件で製造した。■Electron injection layer Manufactured under the same conditions as Sample I.
(3)試料6について
■正孔注入層
C2H4: S i H*−’−4・1とした他は試料
1と同じ条件で製造した。(3) Regarding Sample 6 ■ Hole injection layer C2H4: Manufactured under the same conditions as Sample 1 except that S i H*-'-4.1.
■発光層
C2H4ガスに対するSighガスの混合比を25%と
した他は試料1と同じ条件で製造した。(2) Light Emitting Layer The light emitting layer was manufactured under the same conditions as Sample 1 except that the mixing ratio of Sigh gas to C2H4 gas was 25%.
■電子注入層 試料1と同じ条件で製造した。■Electron injection layer It was manufactured under the same conditions as Sample 1.
以」二の各試料4〜6について波長とE L強度との関
係を調へたところ夫々試料1〜3の場合と同等の関係で
あった。このように良好な発光特性を得るためには、発
光層の製膜に用いる水素化ケイ素ガスの濃度(エチレン
ガスに対する濃度(混合比))は2.5〜20%である
ことが好ましい。When the relationship between wavelength and EL intensity was investigated for each of Samples 4 to 6 listed below, it was found that the relationship was the same as that for Samples 1 to 3, respectively. In order to obtain such good luminescent properties, the concentration of silicon hydride gas (concentration (mixing ratio) to ethylene gas) used for forming the luminescent layer is preferably 2.5 to 20%.
いずれの試料4〜6も目視で十分観察できる発光を示し
、試料1〜3の場合と同様に十分な発光特性を有してい
ることが判った。発光試験における条件は試料1〜3と
同じである。It was found that all Samples 4 to 6 exhibited luminescence that could be sufficiently observed visually, and had sufficient luminescence characteristics as in the case of Samples 1 to 3. The conditions in the luminescence test were the same as Samples 1-3.
また上記の全ての試料1〜6に電界をかけたときの発光
エネルギーのピーク値はかなり高かった。In addition, the peak values of luminescence energy when an electric field was applied to all of the above samples 1 to 6 were quite high.
その理由は、上述実施例では、正孔注入層の生成工程に
おける基板温度を、発光層、電子注入層の生成工程にお
ける基板温度よりも高くしているため、発光層及び電子
注入層の生成工程時に正孔注入層内のボロンが発光層内
に拡散されにくいと考えられる。The reason for this is that in the above embodiment, the substrate temperature in the hole injection layer generation step is higher than the substrate temperature in the light emitting layer and electron injection layer generation steps. It is sometimes thought that boron in the hole injection layer is difficult to diffuse into the light emitting layer.
ところでp型のa−C:5iSH膜、1型のaC:Si
、H膜及びn型のa−SiC膜を積層したp−1−n型
セルを作った場合各層間の接合はへテロ接合となるから
、その接合が良好になされるか否か、即ち注入層から発
光層に正孔(電子)がうまく注入されるか否かが問題で
あったが、試料1〜6についてダイオード特性を調べて
みると、良好な特性を示し、接合が良好になされている
ことが判った。By the way, p-type aC:5iSH film, 1-type aC:Si
When a p-1-n type cell is made by laminating a H film and an n-type a-SiC film, the junction between each layer becomes a heterojunction. The problem was whether holes (electrons) were successfully injected from the layer to the light-emitting layer, but when we investigated the diode characteristics of samples 1 to 6, they showed good characteristics and good junctions. It turned out that there was.
G8発明の効果
本発明によれば、P−CVD法により得られたa−C:
SiH膜を正孔注入層及び発光層として用いているため
、大きな光学的エネルギーギトップを有すると共に各層
間におζノる所定の関係を9
保持しながらSiH+ガスの混合量を変えることにより
発光特性をコントロールできるから要望に応じた発光層
が容易に得られる。G8 Effect of the invention According to the invention, a-C obtained by P-CVD method:
Since the SiH film is used as the hole injection layer and the light emitting layer, it has a large optical energy top and can emit light by changing the mixing amount of SiH + gas while maintaining the predetermined relationship between each layer. Since the characteristics can be controlled, a light-emitting layer that meets your needs can be easily obtained.
更にケイ素原子の含有量に対する炭素原子の含有率につ
いて、正孔注入層よりも発光層を小さくし、かつ発光層
よりも電子住人層を小さくしているため、発光層と注入
層とかへテロ接合により結合されていても電子及び正孔
が発光層にうまく注入され、発光層の特性を十分に引き
出すことができ、実用価値の高い発光素子を得ることが
できる。Furthermore, regarding the carbon atom content relative to the silicon atom content, the emissive layer is made smaller than the hole injection layer, and the electron resident layer is made smaller than the emissive layer. Even if the electrons and holes are combined with each other, electrons and holes can be successfully injected into the light emitting layer, the characteristics of the light emitting layer can be fully brought out, and a light emitting device with high practical value can be obtained.
また正孔注入層の生成工程における基板温度を、発光層
、電子注入層の生成工程における基板温度よりも高くし
ているため、正孔注入層内の不純物の発光層への拡散を
防止できるから発光層のダメージが小さく、その特性が
失イつれない。In addition, since the substrate temperature in the hole injection layer generation process is higher than the substrate temperature in the emission layer and electron injection layer generation processes, it is possible to prevent impurities in the hole injection layer from diffusing into the emission layer. The damage to the light emitting layer is small and its characteristics are not lost.
00
第1図は本発明の実施例に係る発光素子を示す構成図、
第2図はダイオードの発光特性を示す特性図、第3図は
アモルファス炭素系膜のEgoとPLとの関係を示す特
性図である。
3 ・正孔注入層、4・・・発光層、5・・電子注入層
。
外2名
第1図
実施例の構成図
1・・・基板
2.6・・・電極
3・・・正孔注入層
4・・・発光層
5・・・電子注入層FIG. 1 is a configuration diagram showing a light emitting element according to an embodiment of the present invention,
FIG. 2 is a characteristic diagram showing the light emitting characteristics of the diode, and FIG. 3 is a characteristic diagram showing the relationship between Ego and PL of the amorphous carbon film. 3. Hole injection layer, 4. Light emitting layer, 5. Electron injection layer. Figure 1 Structure of Example 1...Substrate 2.6...Electrode 3...Hole injection layer 4...Light emitting layer 5...Electron injection layer
Claims (2)
スとを含む低圧の反応ガスを真空容器内でグロー放電さ
せて分解ガスを重合させるプラズマ化学的蒸着法により
p型のアモルファス炭素系膜よりなる正孔注入層を生成
する工程と、 低圧の水素ガスと炭化水素ガスと水素化ケイ素ガスとを
反応ガスとし、炭化水素ガスに対する水素化ケイ素ガス
の混合比を正孔注入層における同混合比よりも大きくし
たプラズマ化学的蒸着法によりアモルファス炭素系膜よ
りなる発光層を前記正孔注入層上に積層する工程と、 炭化水素ガスと水素化ケイ素ガスとn型不純物ガスとを
含み、炭化水素ガスに対する水素化ケイ素ガスの混合比
が前記発光層における同混合比よりも大きい反応ガスを
真空容器内でグロー放電させて分解ガスを重合させるプ
ラズマ化学的蒸着法によりn型のアモルファス炭化ケイ
素膜よりなる電子注入層を前記発光層上に積層する工程
とを含むことを特徴とする発光素子の製造方法。(1) A p-type amorphous carbon-based film is produced using a plasma chemical vapor deposition method in which a low-pressure reaction gas containing hydrocarbon gas, silicon hydride gas, and p-type impurity gas is glow-discharged in a vacuum container and the decomposed gas is polymerized. A step of generating a hole injection layer consisting of low pressure hydrogen gas, hydrocarbon gas, and silicon hydride gas as reaction gases, and adjusting the mixing ratio of silicon hydride gas to hydrocarbon gas to the same mixing ratio in the hole injection layer. a step of laminating a light-emitting layer made of an amorphous carbon-based film on the hole injection layer by a plasma chemical vapor deposition method with a ratio larger than An n-type amorphous silicon carbide film is formed by a plasma chemical vapor deposition method in which a reaction gas in which the mixing ratio of silicon hydride gas to hydrogen gas is larger than the same mixing ratio in the light emitting layer is caused to glow discharge in a vacuum container to polymerize the decomposed gas. A method for manufacturing a light emitting device, comprising the step of laminating an electron injection layer consisting of the following on the light emitting layer.
層及び電子注入層の各生成工程における基板温度以上の
大きさにすることを特徴とする請求項(1)記載の発光
素子の製造方法。(2) Manufacturing the light emitting device according to claim (1), wherein the substrate temperature in the step of forming the hole injection layer is set to be higher than the substrate temperature in each step of forming the light emitting layer and the electron injection layer. Method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2020695A JPH03225969A (en) | 1990-01-31 | 1990-01-31 | Manufacture of light-emitting element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2020695A JPH03225969A (en) | 1990-01-31 | 1990-01-31 | Manufacture of light-emitting element |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03225969A true JPH03225969A (en) | 1991-10-04 |
Family
ID=12034291
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2020695A Pending JPH03225969A (en) | 1990-01-31 | 1990-01-31 | Manufacture of light-emitting element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03225969A (en) |
-
1990
- 1990-01-31 JP JP2020695A patent/JPH03225969A/en active Pending
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| WO2007037343A1 (en) | Diode and photovoltaic element using carbon nanostructure | |
| JPH07263636A (en) | Resistor and manufacturing method thereof | |
| EP0244874A2 (en) | Luminescent material, process for producing it and luminescent semiconductor device using it | |
| JPH07283434A (en) | Diamond light emitting element | |
| JPH0158839B2 (en) | ||
| JPH02260669A (en) | Manufacture of light emitting element | |
| JP2605834B2 (en) | Light emitting device manufacturing method | |
| JPH03225972A (en) | Manufacture of light-emitting element | |
| JPH02109378A (en) | Manufacture of light emitting element | |
| JPH02218181A (en) | Light emitting element | |
| JPH02218180A (en) | Light emitting element | |
| JPH03225971A (en) | Manufacture of light-emitting element | |
| JPH02109379A (en) | Manufacture of light emitting element | |
| JP2508015B2 (en) | Method of manufacturing light emitting material | |
| JPH03225970A (en) | Manufacture of light-emitting element | |
| JPH02218179A (en) | Light emitting element and manufacture of amorphous material layer | |
| JPH02224377A (en) | Manufacture of light emitting element | |
| JP4925147B2 (en) | cathode | |
| JP2015154005A (en) | Iron silicide semiconductor, method for manufacturing iron silicide semiconductor thin film, light-emitting element, and light-receiving element | |
| JPS63213375A (en) | Light emitting element | |
| Chen et al. | Effects of Si, Ge and Ar ion-implantation on EL from Au/Si-rich SiO2/p-Si structure | |
| JPH0652806B2 (en) | Method for manufacturing semiconductor light emitting device | |
| JP2762910B2 (en) | Luminescent material | |
| JPH0758360A (en) | Semiconductor device and manufacturing method thereof | |
| JPS6267884A (en) | light emitting element |