JPH026237B2 - - Google Patents
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- Publication number
- JPH026237B2 JPH026237B2 JP57037381A JP3738182A JPH026237B2 JP H026237 B2 JPH026237 B2 JP H026237B2 JP 57037381 A JP57037381 A JP 57037381A JP 3738182 A JP3738182 A JP 3738182A JP H026237 B2 JPH026237 B2 JP H026237B2
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- Prior art keywords
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- type
- substrate
- semiconductor element
- gaas
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Classifications
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
- H10H29/00—Integrated devices, or assemblies of multiple devices, comprising at least one light-emitting semiconductor element covered by group H10H20/00
- H10H29/10—Integrated devices comprising at least one light-emitting semiconductor component covered by group H10H20/00
-
- 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
- H01S5/02—Structural details or components not essential to laser action
- H01S5/026—Monolithically integrated components, e.g. waveguides, monitoring photo-detectors, drivers
- H01S5/0261—Non-optical elements, e.g. laser driver components, heaters
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- Solid State Image Pick-Up Elements (AREA)
- Semiconductor Lasers (AREA)
Description
【発明の詳細な説明】
発明の技術分野
本発明は、同一基板上に通常の半導体素子と光
半導体素子とを共存させた半導体装置の改良に関
する。DETAILED DESCRIPTION OF THE INVENTION Technical Field of the Invention The present invention relates to an improvement in a semiconductor device in which a normal semiconductor element and an optical semiconductor element coexist on the same substrate.
従来技術と問題点
従来、同一基板上に例えば論理用電界効果半導
体素子と光半導体素子とを形成した半導体装置と
して第1図に見られるものが知られている。BACKGROUND ART Conventionally, the one shown in FIG. 1 is known as a semiconductor device in which, for example, a logic field effect semiconductor element and an optical semiconductor element are formed on the same substrate.
図に於いて、1は半絶縁性GaAs基板、2はn
型GaAs能動層、3はn型GaAs層、4はn型
GaAlAsクラツド層、5はn型GaAs活性層、6
はp型GaAlAsクラツド層、7はp+型GaAsキヤ
ツプ層、8はAuZnからなるp側電極、9は
AuGeからなるドレイン電極、10はAlからなる
ゲート電極、11はAuGeからなるソース電極を
それぞれ示す。尚、QTは電界効果トランジスタ
部分、QLは半導体レーザ部分をそれぞれ示す。 In the figure, 1 is a semi-insulating GaAs substrate, 2 is an n
type GaAs active layer, 3 is n-type GaAs layer, 4 is n-type
GaAlAs clad layer, 5 is n-type GaAs active layer, 6
is a p-type GaAlAs cladding layer, 7 is a p + type GaAs cap layer, 8 is a p-side electrode made of AuZn, and 9 is a p-side electrode made of AuZn.
A drain electrode made of AuGe, 10 a gate electrode made of Al, and 11 a source electrode made of AuGe. Note that QT indicates a field effect transistor portion and QL indicates a semiconductor laser portion.
この装置に図示の極性に電圧を印加すると、矢
印Iで示すように電流が流れる。そして、この電
流はゲート電極10に印加される負電圧に依つて
発生する空乏層の拡がりで制御されるので、前記
負電圧を信号として半導体レーザ部分QLの放射
光を変調することができる。 When a voltage is applied to this device with the polarity shown, a current flows as indicated by arrow I. Since this current is controlled by the expansion of the depletion layer generated by the negative voltage applied to the gate electrode 10, the light emitted from the semiconductor laser portion QL can be modulated using the negative voltage as a signal.
ところで、この従来例では、電界効果トランジ
スタ部分QTと半導体レーザ部分QLとの間の段
差が大(例えば3〜5〔μm〕)である為、電界効
果トランジスタの電極、特にゲート電極のフオト
リソグラフイが困難になり微細加工ができず、ま
た、電流はキヤリヤ濃度が低い能動層2を配線と
して流れる為、配線抵抗が大である。 By the way, in this conventional example, since the step between the field effect transistor part QT and the semiconductor laser part QL is large (for example, 3 to 5 [μm]), the photolithography of the electrodes of the field effect transistor, especially the gate electrode, is difficult. This makes microfabrication difficult, and since the current flows through the active layer 2, which has a low carrier concentration, as a wiring, the wiring resistance is high.
そこで、第2図に見られる構造の装置も提案さ
れている。 Therefore, a device having the structure shown in FIG. 2 has also been proposed.
図に於いて、21はn型GaAs基板、22はn
型GaAlAsクラツド層、23はn型GaAlAs活性
層、24はp型GaAlAsクラツド層、25はn型
GaAs層、26は半絶縁性GaAlAs層、27はn
型GaAs能動層、28は二酸化シリコン絶縁膜、
29はp型不純物拡散領域、30はAuCrからな
るp側電極、31はAuGeNiからなるドレイン電
極、32はAuCrからなるゲート電極、33は
AuGeNiからなるソース電極、34はAuGeNiか
らなるn側電極、QTは電界効果トランジスタ部
分、QLは半導体レーザ部分をそれぞれ示す。 In the figure, 21 is an n-type GaAs substrate, 22 is an n-type GaAs substrate, and 22 is an n-type GaAs substrate.
23 is an n-type GaAlAs active layer, 24 is a p-type GaAlAs clad layer, 25 is an n-type
GaAs layer, 26 is semi-insulating GaAlAs layer, 27 is n
type GaAs active layer, 28 is a silicon dioxide insulating film,
29 is a p-type impurity diffusion region, 30 is a p-side electrode made of AuCr, 31 is a drain electrode made of AuGeNi, 32 is a gate electrode made of AuCr, and 33 is a p-side electrode made of AuCr.
A source electrode made of AuGeNi, 34 an n-side electrode made of AuGeNi, QT a field effect transistor part, and QL a semiconductor laser part.
この装置に於いて、図示の極性に電圧を印加す
ると、矢印I1で示す電流が流れ、それは、ソース
電極33、p側電極30を通り、矢印I2の如く流
れる。そして、この電流もゲート電極32に印加
される負電圧で能動層27中に発生する空乏層の
拡がり如何で制御される。従つて、前記同様、半
導体レーザ部分QLの放射光は変調可能である。 In this device, when a voltage is applied to the illustrated polarity, a current shown by arrow I 1 flows, which passes through the source electrode 33 and the p-side electrode 30 and flows as shown by arrow I 2 . This current is also controlled by how the depletion layer generated in the active layer 27 spreads due to the negative voltage applied to the gate electrode 32. Therefore, as described above, the emitted light of the semiconductor laser portion QL can be modulated.
この従来例に依ると、半導体レーザ部分QLと
電界効果トランジスタ部分QTとの間の段差は解
消され、また、配線抵抗は問題にならないもの
の、別の欠点が発生する。即ち、この装置では、
半絶縁性GaAlAs層26はエピタキシヤル成長法
で形成している為、その比抵抗ρは通常〜103〜4
〔Ω−cm〕程度であつて、余り高くはできない。
従つて、矢印I1で示した電流が破線の矢印で示し
てあるように流れ、半導体レーザ部分QLは正常
に動作しないことになる。尚、因に第1図に見ら
れる半絶縁性GaAs基板1に於ける比抵抗ρは
106〜7〔Ωcm〕を得ることができる。 According to this conventional example, although the step difference between the semiconductor laser portion QL and the field effect transistor portion QT is eliminated and the wiring resistance is not a problem, another drawback occurs. That is, in this device,
Since the semi-insulating GaAlAs layer 26 is formed by epitaxial growth, its specific resistance ρ is usually ~10 3 ~ 4
It is about [Ω-cm] and cannot be made too high.
Therefore, the current indicated by the arrow I1 flows as indicated by the broken line arrow, and the semiconductor laser portion QL does not operate normally. Incidentally, the specific resistance ρ in the semi-insulating GaAs substrate 1 shown in Figure 1 is
10 6 to 7 [Ωcm] can be obtained.
発明の目的
本発明は、高比抵抗の半絶縁性基板上に通常の
半導体素子と半導体レーザ、LEDなどの光半導
体素子とを段差がないように併設し、また、それ
等半導体素子と光半導体素子とを結ぶ配線の抵抗
を低く抑えることができるようにするものであ
る。Purpose of the Invention The present invention provides a structure in which a normal semiconductor element and an optical semiconductor element such as a semiconductor laser or an LED are arranged side by side on a high resistivity semi-insulating substrate so that there is no difference in level between the semiconductor element and the optical semiconductor element. This makes it possible to suppress the resistance of the wiring connecting the device to a low level.
発明の実施例
第3図乃至第7図は本発明一実施例を製造する
工程を説明する為の工程要所に於ける半導体装置
の要部断面図であり、次に、これ等の図を参照し
つつ説明する。Embodiment of the Invention FIGS. 3 to 7 are cross-sectional views of essential parts of a semiconductor device at key points in the process for explaining the manufacturing process of an embodiment of the present invention. I will explain while referring to it.
第3図参照
(1) 半絶縁性GaAs基板31上に厚さ〜6000〔Å〕
の二酸化シリコン膜51を例えばCVD法で形
成する。Refer to Figure 3 (1) On the semi-insulating GaAs substrate 31, the thickness is ~6000 [Å].
A silicon dioxide film 51 is formed by, for example, a CVD method.
(2) 通常のフオト・リソグラフイ技術にて二酸化
シリコン膜51のパターニングを行ない、選択
的に窓を形成する。(2) The silicon dioxide film 51 is patterned using ordinary photolithography technology to selectively form windows.
(3) パターニングされた二酸化シリコン膜51を
マスクとして基板31を深さ7〜8〔μm〕程
度エツチングする。(3) Using the patterned silicon dioxide film 51 as a mask, the substrate 31 is etched to a depth of about 7 to 8 [μm].
第4図参照
(4) 再び二酸化シリコン膜51のパターニングを
行ない、さきに形成した窓を若干拡大する。See FIG. 4 (4) The silicon dioxide film 51 is patterned again to slightly enlarge the previously formed window.
(5) 二酸化シリコン膜51をマスクとしてZnの
拡散を行ない基板31に深さ〜50〔μm〕のp+
(p>1020〔cm-3〕)型配線層32を形成する。(5) Using the silicon dioxide film 51 as a mask, Zn is diffused into the substrate 31 to a depth of ~50 [μm] p +
(p>10 20 [cm -3 ]) type wiring layer 32 is formed.
第5図参照
(6) 二酸化シリコン膜51を除去してから分子ビ
ーム・エピタキシヤル成長法(MBE法)にて
通常の半導体素子に於ける能動層であるn型
GaAs層33を厚さ例えば0.2〔μm〕程度に成
長させる。このときの温度は600〜700〔℃〕、時
間は1〜3〔時間〕であり、また、n型不純物
の濃度は1×1017〔cm-3〕である。Refer to Figure 5 (6) After removing the silicon dioxide film 51, an n-type layer, which is an active layer in a normal semiconductor device, is formed by molecular beam epitaxial growth (MBE).
The GaAs layer 33 is grown to a thickness of, for example, about 0.2 [μm]. The temperature at this time is 600 to 700 [° C.], the time is 1 to 3 [hours], and the concentration of n-type impurity is 1×10 17 [cm −3 ].
この工程中に、p+型配線層32上のn型
GaAs層33にはp型不純物が這い上りn型を
p型に変換する。尚、温度を600〔℃〕として1
時間に於ける這い上り拡散深さは〜0.5〔μm〕
程度である。 During this step, the n - type
P-type impurities creep into the GaAs layer 33 and convert n-type to p-type. In addition, the temperature is 600 [℃] and 1
The creeping diffusion depth in time is ~0.5 [μm]
That's about it.
(7) CVD法に依り二酸化シリコン膜52を形成
し、これをリソグラフイ技術にてパターニング
し、基板31の厚い部分と、段差部と、基板3
1の薄くなされた部分の一部とを覆うものを残
して他を除去する。(7) A silicon dioxide film 52 is formed by the CVD method, and this is patterned by lithography to cover the thick portions of the substrate 31, the stepped portions, and the substrate 3.
1. Leave the part that covers part of the thinned part of 1 and remove the others.
(8) 再びMBE法を適用し、半導体レーザのp側
コンタクト層であるp+型GaAs層34を厚さ例
えば2〜3〔μm〕程度に成長させる。尚、p
型不純物濃度は5×1018〔cm-3〕程度である。(8) Apply the MBE method again to grow the p + type GaAs layer 34, which is the p-side contact layer of the semiconductor laser, to a thickness of, for example, about 2 to 3 [μm]. In addition, p
The type impurity concentration is about 5×10 18 [cm −3 ].
続いて、キヤリア閉じ込め層であるp型
GaAlAs層35を厚さ例えば1〔μm〕程度に
成長させる。尚、p型不純物濃度は1×1017
〔cm-3〕程度である。 Next, the p-type carrier confinement layer
The GaAlAs layer 35 is grown to a thickness of, for example, about 1 [μm]. In addition, the p-type impurity concentration is 1×10 17
It is about [cm -3 ].
続いて活性層であるn型GaAs層36を厚さ
例えば0.2〔μm〕に形成する。尚、n型不純物
濃度は1×1017〔cm-3〕程度である。 Subsequently, an n-type GaAs layer 36 as an active layer is formed to a thickness of, for example, 0.2 [μm]. Note that the n-type impurity concentration is about 1×10 17 [cm −3 ].
続いてキヤリヤ閉じ込め層であるn型
GaAlAs層37を厚さ例えば1〔μm〕程度に
形成する。尚、n型不純物濃度は1×1017〔cm
-3〕程度である。 Next is the n-type carrier confinement layer.
The GaAlAs layer 37 is formed to have a thickness of, for example, about 1 [μm]. In addition, the n-type impurity concentration is 1×10 17 [cm
-3 ].
続いてn側コンタクト層であるn+型GaAs層
38を厚さ例えば1〔μm〕程度に形成する。
尚、n型不純物濃度は1×1018〔cm-3〕程度で
ある。 Subsequently, an n + type GaAs layer 38 serving as an n-side contact layer is formed to a thickness of, for example, about 1 [μm].
Note that the n-type impurity concentration is approximately 1×10 18 [cm −3 ].
これ等の成長は連続的に行なわれる。そし
て、二酸化シリコン膜52上に成長された各層
は多結晶になる。図では、これを記号39で指
示してある。 This growth is continuous. Each layer grown on the silicon dioxide film 52 becomes polycrystalline. In the figure, this is indicated by the symbol 39.
第6図参照
(9) 光半導体素子のn側電極用としてAuGe/Ni
を〜3000〔Å〕程度の厚さに真空蒸着法で形成
する。See Figure 6 (9) AuGe/Ni for the n-side electrode of optical semiconductor devices.
is formed to a thickness of approximately 3000 Å by vacuum evaporation.
(10) 通常のフオト・リソグラフイ技術にて、n+
型GaAs層38上に幅10〔μm〕、長さ300〔μ
m〕のストライプ電極40を形成し、次いで、
温度420〔℃〕、時間1〔分〕の熱処理を窒素雰囲
気中で行なう。(10) Using normal photolithography technology, n +
A layer with a width of 10 [μm] and a length of 300 [μm] is formed on the type GaAs layer 38.
m] stripe electrodes 40 are formed, and then
Heat treatment is performed at a temperature of 420 [° C.] and a time of 1 [minute] in a nitrogen atmosphere.
(11) ストライプ電極40を覆うように幅250〔μ
m〕、長さ310〔μm〕のマスクをフオト・レジ
スト膜で形成し(図示せず)、さきに形成した
各半導体層をエツチングし、p+型GaAs層34
が露出するまで行なう。この時、エツチング液
としてはH2SO4/H2O2/H2O(1/8/1)の
混液を使用することができる。尚、二酸化シリ
コン膜52上の多結晶層のエツチング・レート
は単結晶層のそれと比較して2倍も速いので、
前記エツチング工程で完全に除去されてしま
う。また、エツチングをp+型GaAs層34で停
止させる為の制御はエツチング・レート及び時
間に依つて行なうが、p+型GaAs層34を厚く
形成しておけば、多少オーバ・エツチングにな
つても問題は生じない。(11) Width 250 [μ] so as to cover the stripe electrode 40
m], a mask with a length of 310 [μm] is formed using a photoresist film (not shown), and each of the previously formed semiconductor layers is etched to form a p + type GaAs layer 34.
Continue until exposed. At this time, a mixed solution of H 2 SO 4 /H 2 O 2 /H 2 O (1/8/1) can be used as the etching solution. Incidentally, since the etching rate of the polycrystalline layer on the silicon dioxide film 52 is twice as fast as that of the single crystal layer,
It is completely removed in the etching process. Furthermore, control to stop the etching at the p + type GaAs layer 34 is performed depending on the etching rate and time, but if the p + type GaAs layer 34 is formed thickly, even if the etching is slightly over-etched, No problems arise.
第7図参照
(12) 二酸化シリコン膜52を除去してから、真空
蒸着法にてAuZn膜を厚さ例えば〜3000〔Å〕
程度に形成し、これをパターニングして、基板
31の厚い部分に在るp+型配線層32上のも
の以外は除去し、コンタクト層41を形成し、
次いで、温度450〔℃〕、時間5〔分〕の熱処理を
窒素雰囲気中で行なう。See Figure 7 (12) After removing the silicon dioxide film 52, a AuZn film is deposited to a thickness of, for example, ~3000 [Å] by vacuum evaporation.
The contact layer 41 is formed by patterning the contact layer 41 and removing it except for those on the p + type wiring layer 32 located in the thick part of the substrate 31.
Next, heat treatment is performed at a temperature of 450 [° C.] for a time of 5 [minutes] in a nitrogen atmosphere.
(13) 真空蒸着法にてAuGe/Niを厚さ例えば〜
3000〔Å〕程度に形成し、これをパターニング
してドレイン電極42,ソース電極43を形成
し、次いで、温度420〔℃〕、時間1〔分〕の熱処
理を窒素雰囲気中で行なう。(13) AuGe/Ni is deposited by vacuum evaporation method to a thickness of e.g.
It is formed to a thickness of about 3000 [Å] and patterned to form a drain electrode 42 and a source electrode 43. Next, heat treatment is performed at a temperature of 420 [° C.] for a time of 1 [minute] in a nitrogen atmosphere.
(14) 真空蒸着法にてAlを厚さ例えば〜2000〔Å〕
程度に形成し、これをパターニングしてゲート
電極44を形成する。(14) Deposit Al to a thickness of e.g. ~2000 Å using vacuum evaporation method.
The gate electrode 44 is formed by patterning the gate electrode 44.
このようにして基板31の厚い部分(メサ状
部分)には電界効果トランジスタ部分QTが形
成され、薄い部分(凹所)には半導体レーザ部
分QLが形成される。 In this way, the field effect transistor portion QT is formed in the thick portion (mesa-shaped portion) of the substrate 31, and the semiconductor laser portion QL is formed in the thin portion (recess).
前記実施例では、トランジスタ部分QTとレー
ザ部分QLとはZnを高濃度に拡散して形成したp+
型配線層32に依り電気的に接続されているが、
これに代え、高不純物濃度の単結晶層、例えば
p+(或いはn+)型GaAs層を用いても良い。n+型
GaAs層を使用した場合には、半導体レーザ部分
QLに於ける各層の導電型を反転させるとともに
抵抗性コンタクト形成に用いる電極材料を変えれ
ば良い。尚、レーザに於ける共振器端面を形成す
るには前記工程(11)で形成しても良いが、通常の如
く劈開に依ることもできる。 In the above embodiment, the transistor part QT and the laser part QL are formed by diffusing Zn at a high concentration .
Although electrically connected by the type wiring layer 32,
Alternatively, a single crystal layer with high impurity concentration, e.g.
A p + (or n + ) type GaAs layer may also be used. n + type
When using a GaAs layer, the semiconductor laser part
It is sufficient to invert the conductivity type of each layer in the QL and change the electrode material used to form the resistive contact. Incidentally, the resonator end face in the laser may be formed in the step (11) described above, but it is also possible to use conventional cleavage.
発明の効果
以上の説明で判るように、本発明に依れば、高
比抵抗の半絶縁性単結晶基板を使用しているので
半導体素子と光半導体素子間に流れる電流が側路
する惧れは皆無であり、また、該電流は低抵抗値
の拡散層或いは単結晶層からなる配線層を流れる
ので大出力をとり出すことが容易であり、更にま
た、多層になるので必然的に丈が高くなる光半導
体素子は基板をエツチングして形成した段差の下
方表面に、そして、通常の半導体素子はエツチン
グされていない基板表面即ち段差の上方表面にそ
れぞれ形成されるものであるから両素子の表面が
略一致する高さとなり、リソグラフイを実施する
際の微細パターン形成が容易となる。Effects of the Invention As can be seen from the above explanation, according to the present invention, since a semi-insulating single crystal substrate with high resistivity is used, there is a risk that the current flowing between the semiconductor element and the optical semiconductor element may be bypassed. In addition, since the current flows through a wiring layer made of a low resistance diffusion layer or a single crystal layer, it is easy to extract a large output.Furthermore, since there are multiple layers, the length is inevitably increased. The height of the optical semiconductor element is formed on the surface below the step formed by etching the substrate, and the normal semiconductor element is formed on the unetched surface of the substrate, that is, the surface above the step. have substantially the same height, making it easier to form fine patterns when performing lithography.
第1図及び第2図は従来例の要部断面図、第3
図乃至第7図は本発明一実施例を製造する工程を
説明する為の工程要所に於ける半導体装置の要部
断面図である。
図に於いて、31は段差を有する半絶縁性
GaAs基板、32はp+型配線層、33は能動層で
あるn型GaAs層、34はp側コンタクト層であ
るp+型GaAs層、35はキヤリヤ閉じ込め層であ
るp型GaAlAs層、36は活性層であるn型
GaAs層、37はキヤリヤ閉じ込め層であるn型
GaAlAs層、38はn側コンタクト層であるn+型
GaAs層、40はストライプ電極、41はコンタ
クト層、42はドレイン電極、43はソース電
極、44はゲート電極である。
Figures 1 and 2 are sectional views of the main parts of the conventional example;
7 to 7 are sectional views of essential parts of a semiconductor device at key points in the process for explaining the process of manufacturing an embodiment of the present invention. In the figure, 31 is a semi-insulating material with steps.
32 is a p + type wiring layer, 33 is an n type GaAs layer which is an active layer, 34 is a p + type GaAs layer which is a p side contact layer, 35 is a p type GaAlAs layer which is a carrier confinement layer, and 36 is a GaAs substrate. n-type active layer
GaAs layer, 37 is n-type carrier confinement layer
GaAlAs layer, 38 is n + type which is n side contact layer
40 is a stripe electrode, 41 is a contact layer, 42 is a drain electrode, 43 is a source electrode, and 44 is a gate electrode.
Claims (1)
間に形成された高不純物濃度の拡散層或いは単結
晶層からなる配線層、 前記段差の上方表面に形成された通常の半導体
素子、 前記段差の下方表面に積層され且つ表面が前記
通常の半導体素子の表面と略一致する高さに形成
されると共に前記配線層で該通常の半導体素子と
電気的に結合された光半導体素子 を備えてなることを特徴とする半導体装置。[Claims] 1. A semi-insulating single-crystal substrate having a step on its surface, comprising a diffusion layer or a single-crystal layer with a high impurity concentration formed between the upper surface and the lower surface of the step in the substrate. a wiring layer; a normal semiconductor element formed on the upper surface of the step; a wiring layer laminated on the lower surface of the step; A semiconductor device comprising an optical semiconductor element electrically coupled to the ordinary semiconductor element.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57037381A JPS58154286A (en) | 1982-03-10 | 1982-03-10 | Semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57037381A JPS58154286A (en) | 1982-03-10 | 1982-03-10 | Semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58154286A JPS58154286A (en) | 1983-09-13 |
| JPH026237B2 true JPH026237B2 (en) | 1990-02-08 |
Family
ID=12495941
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57037381A Granted JPS58154286A (en) | 1982-03-10 | 1982-03-10 | Semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58154286A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0285943U (en) * | 1988-12-22 | 1990-07-06 | ||
| JPH03291452A (en) * | 1990-04-04 | 1991-12-20 | Rinnai Corp | Hot water feeding device |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5936263U (en) * | 1982-08-30 | 1984-03-07 | 日本電気株式会社 | semiconductor equipment |
| JPS60201382A (en) * | 1984-03-26 | 1985-10-11 | ロ−ム株式会社 | light emitting display device |
| JPS60251654A (en) * | 1984-05-28 | 1985-12-12 | Fujitsu Ltd | Manufacture of semiconductor device |
| JPS6169169A (en) * | 1984-09-13 | 1986-04-09 | Agency Of Ind Science & Technol | Semiconductor photodetector |
| FR2588701B1 (en) * | 1985-10-14 | 1988-12-30 | Bouadma Noureddine | METHOD FOR PRODUCING AN INTEGRATED LASER-PHOTODETECTOR STRUCTURE |
-
1982
- 1982-03-10 JP JP57037381A patent/JPS58154286A/en active Granted
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0285943U (en) * | 1988-12-22 | 1990-07-06 | ||
| JPH03291452A (en) * | 1990-04-04 | 1991-12-20 | Rinnai Corp | Hot water feeding device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58154286A (en) | 1983-09-13 |
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