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JPH0728079B2 - Method for manufacturing semiconductor laser - Google Patents
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JPH0728079B2 - Method for manufacturing semiconductor laser - Google Patents

Method for manufacturing semiconductor laser

Info

Publication number
JPH0728079B2
JPH0728079B2 JP59153971A JP15397184A JPH0728079B2 JP H0728079 B2 JPH0728079 B2 JP H0728079B2 JP 59153971 A JP59153971 A JP 59153971A JP 15397184 A JP15397184 A JP 15397184A JP H0728079 B2 JPH0728079 B2 JP H0728079B2
Authority
JP
Japan
Prior art keywords
type
layer
gas containing
xalxas
substrate
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 - Fee Related
Application number
JP59153971A
Other languages
Japanese (ja)
Other versions
JPS6134987A (en
Inventor
潤一 西澤
薫 本谷
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Individual
Original Assignee
Individual
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Filing date
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Application filed by Individual filed Critical Individual
Priority to JP59153971A priority Critical patent/JPH0728079B2/en
Publication of JPS6134987A publication Critical patent/JPS6134987A/en
Publication of JPH0728079B2 publication Critical patent/JPH0728079B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S5/00Semiconductor lasers
    • H01S5/30Structure or shape of the active region; Materials used for the active region
    • H01S5/32Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures
    • H01S5/323Structure 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
    • H01S5/32308Structure 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
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/01Manufacture or treatment
    • H10H20/011Manufacture or treatment of bodies, e.g. forming semiconductor layers
    • H10H20/013Manufacture or treatment of bodies, e.g. forming semiconductor layers having light-emitting regions comprising only Group III-V materials

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  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)
  • Semiconductor Lasers (AREA)

Description

【発明の詳細な説明】 [発明の技術分野] 本発明は半導体レーザの製造方法に関する。Description: TECHNICAL FIELD OF THE INVENTION The present invention relates to a method for manufacturing a semiconductor laser.

[先行技術とその問題点] 従来から半導体の薄膜結晶を得るための気相エピタキシ
ー技術として、有機金属気相成長法(以下、MO−CVD法
と呼ぶ)、分子線エピタキシー法(以下、MBE法と呼
ぶ)、原子層エピタキシー法(以下、ALE法と呼ぶ)な
どが知られている。しかし、MO−CVD法はソースとしてI
II族、V族元素を水素ガス等をキャリアとして、同時に
反応室へ導入し、熱分解によって成長させるため、成長
層の品質が悪い。また、単分子層オーダーの制御が困難
である等の欠点がある。また、通常結晶品質を良くため
ために、600℃以上の成長温度が用いられている。
[Prior Art and its Problems] Conventional vapor phase epitaxy techniques for obtaining semiconductor thin film crystals include metal organic chemical vapor deposition (MO-CVD) and molecular beam epitaxy (MBE). Atomic layer epitaxy method (hereinafter referred to as ALE method) and the like are known. However, MO-CVD method
Since the Group II and V elements are simultaneously introduced into the reaction chamber using hydrogen gas as a carrier and are grown by thermal decomposition, the quality of the growth layer is poor. Further, there are drawbacks such that it is difficult to control the order of monomolecular layer. In addition, a growth temperature of 600 ° C. or higher is usually used to improve the crystal quality.

一方、超高真空を利用した結晶成長法としてよく知られ
るMBE法は、物理吸着を第一段階とするために、結晶の
品質は化学反応を利用した気相成長法に劣る。GaAsのよ
うなIII−V族間の化合物半導体を成長する時には、III
族、V族元素をソースとして用い、ソース源自体を成長
室の中に設置している。このため、ソース源を加熱して
得られる放出ガスと蒸発量の制御、および、ソースの補
給が困難であり、成長速度を長時間一定に保つことが困
難である。また、蒸発物の排気など真空装置が複雑にな
る。更には、化合物半導体の化学量論的組成(ストイキ
オメトリー)を精密に制御することが困難で、結局、高
品質の結晶を得ることができない欠点がある。また、混
晶を作るためには、GaAlAsでは約600℃以上にしないと
良好な結晶が得られないこと、GaAsとのヘテロ接合界面
には1〜数原子層に及び凹凸があり良好とはいえないも
のである。
On the other hand, the MBE method, which is well known as a crystal growth method using ultra-high vacuum, is inferior to the vapor phase growth method using a chemical reaction because the physical adsorption is the first step. When growing a III-V compound semiconductor such as GaAs, III
Group and V group elements are used as sources, and the source source itself is installed in the growth chamber. Therefore, it is difficult to control the emission gas and evaporation amount obtained by heating the source source, and to replenish the source, and it is difficult to keep the growth rate constant for a long time. Further, the vacuum device such as evacuation of the evaporated material becomes complicated. Furthermore, it is difficult to precisely control the stoichiometric composition (stoichiometry) of the compound semiconductor, and as a result, high quality crystals cannot be obtained. Also, in order to form a mixed crystal, good crystals cannot be obtained unless the temperature is about 600 ° C. or higher with GaAlAs, and it can be said that the heterojunction interface with GaAs has unevenness of 1 to several atomic layers and is good. There is no such thing.

更にALE法は、T.SuntolaらがU.S.P.No.4058430(1977)
で説明しているように、半導体元素をパルス状に供給
し、基板に付着させることにより結晶を原子層ずつ成長
させるものであるが、半導体の単結晶を成長させること
ができない。即ち、単結晶の薄膜を形成させるために、
同じグループのM.Pessaらが用いた方法は、ALE法でな
く、1984年の米真空協会の論文集(J.Vac.Sci.Techno
l、A2(1984)418)に発表しているように前記MBE法に
よるものである。
For the ALE method, T. Suntola et al., USP No. 4058430 (1977).
As described in (1), a semiconductor element is supplied in a pulsed form and deposited on a substrate to grow a crystal atomic layer by atomic layer, but a semiconductor single crystal cannot be grown. That is, in order to form a single crystal thin film,
The method used by M. Pessa et al. In the same group is not the ALE method but the collection of papers of the American Vacuum Society in 1984 (J. Vac. Sci.
l, A2 (1984) 418), which is based on the MBE method.

このように、MO−CVD法やMBE法では化学量論的組成を満
足する高品質の結晶が低温では得られず、また、単分子
層オーダーで形成することが困難な一方、ALE法では単
結晶が得られない欠点があった。
Thus, the MO-CVD method and MBE method cannot obtain high-quality crystals satisfying the stoichiometric composition at low temperature, and it is difficult to form monolayers, while the ALE method does not There was a drawback that crystals could not be obtained.

[発明の目的] 本発明は上記従来技術の欠点を除き、化学量論的組成を
制御することにより結晶成長層の品質を改善し、基板の
より低温領域での加熱と、単分子量の精度で成長膜を形
成することにより、高品質のヘテロ接合を有する半導体
レーザを製造する方法を提供することを目的とする。
[Object of the Invention] The present invention eliminates the above-mentioned drawbacks of the prior art, improves the quality of the crystal growth layer by controlling the stoichiometric composition, and heats the substrate in a lower temperature region and achieves the accuracy of a single molecular weight. It is an object of the present invention to provide a method for manufacturing a semiconductor laser having a high quality heterojunction by forming a growth film.

[発明の概要] このため本発明は、(1)真空に排気する成長槽内に外
部よりGa、As、Al及びPの各成分元素を含むガス及び不
純物となる成分元素を含むガスをそれぞれ導入する手段
と、n+形GaAs基板を加熱する手段と、前記n+形基板を光
照射する光源とを具備した結晶成長装置を用い、前記成
長槽内を10-7〜10-9Paに排気すると共に、前記n+形基板
を約300〜600℃に加熱し、前記光源より前記n+形基板に
光を照射しながら、Gaを含むガス又は同時にAlを含むガ
スを成長槽内の圧力が10-1〜10-7Paとなる範囲で0.5〜1
0秒間導入し、次いで成長槽内のガスを排気した後、As
を含むガス又は同時にAlを含むガスを成長槽内の圧力が
10-1〜10-7Paとなる範囲で2〜200秒間導入する操作を
繰り返すことにより、前記n+形基板上にn形のGa1-xAlx
As又はGa1-xAlxAs1-yPyを1分子層ずつ成長させる工
程、その上にアンドープのGaAsを形成する工程、さらに
その上にp形のGa1-xAlxAs又はGa1-xAlxAs1-yPyを成長
させる工程、その上に絶縁膜を形成した後、所定個所に
開口部を形成して前記p形層へZnによる不純物拡散を行
ってp+形層を形成する工程、前記p+形層へ合金を蒸着し
てp+形電極を形成する工程、前記n+形基板に合金を蒸着
してn+形電極を形成する工程を順次実行して半導体レー
ザを製造することを特徴とする。
[Summary of the Invention] Therefore, according to the present invention, (1) a gas containing component elements of Ga, As, Al, and P and a gas containing component elements to be impurities are introduced from the outside into a growth tank evacuated to vacuum. And a means for heating the n + -type GaAs substrate, and a light source for irradiating the n + -type substrate with a light source, and the inside of the growth tank is evacuated to 10 −7 to 10 −9 Pa. In addition, while heating the n + -type substrate to about 300 ~ 600 ℃, while irradiating the n + -type substrate with light from the light source, the gas containing Ga or the gas containing Al at the same time as the pressure in the growth tank is increased. 0.5 to 1 in the range of 10 -1 to 10 -7 Pa
It was introduced for 0 seconds, then the gas in the growth tank was exhausted,
Gas containing Al or gas containing Al at the same time
By repeating the operation of introducing for 2 to 200 seconds within the range of 10 -1 to 10 -7 Pa, the n - type Ga 1- xAlx is formed on the n + -type substrate.
Step of growing As or Ga 1- xAlxAs 1- yPy one by one molecular layer, step of forming undoped GaAs thereon, and further growing p - type Ga 1- xAlxAs or Ga 1- xAlxAs 1- yPy step of, after forming an insulating film thereon, forming a p + -type layer by performing impurity diffusion by Zn to the p-type layer to form an opening in a predetermined position, the alloy into the p + -type layer To form a p + -type electrode and a step of depositing an alloy on the n + -type substrate to form an n + -type electrode, thereby sequentially manufacturing a semiconductor laser.

また本発明は、(2)真空に排気する成長槽内に外部よ
りGa、As、Al及びPの各成分元素を含むガス及び不純物
となる成分元素を含むガスをそれぞれ導入する手段と、
n+形GaAs基板を加熱する手段と、前記n+形基板を光照射
する光源とを具備した結晶成長装置を用い、前記成長槽
内を10-7〜10-9Paに排気すると共に、前記n+形基板を約
300〜600℃に加熱し、前記光源より前記n+形基板に光を
照射しながら、Gaを含むガス又は同時にAlを含むガスを
成長槽内の圧力が10-1〜10-7Paとなる範囲で0.5〜10秒
間導入し、次いで成長槽内のガスを排気した後、Asを含
むガス又は同時にAlを含むガスを成長槽内の圧力が10-1
〜10-7Paとなる範囲で2〜200秒間導入する操作を繰返
すことにより、前記n+形基板上にn形のGa1-xAlxAs又は
Ga1-xAlxAs1-yPyを1分子層ずつ成長させる工程、その
上にアンドープのGa1-xAlxAs1-yPy層と、さらにその上
にGaAs層とを繰り返し成長させることによりヘテロ層を
形成させる工程、前記ヘテロ層上にp+形のGa1-xAlxAs又
はGa1-xAlxAs1-yPyを形成した後、その上にp+形GaAs層
を形成する工程、前記p+形のGaAs層上に絶縁膜を形成し
た後、所定個所に開口部を形成する工程、前記開口部よ
り前記p+形層へ合金を蒸着してp+形電極を形成する工
程、前記n+形基板に合金を蒸着してn+形電極を形成する
工程を順次実行して量子井戸構造を有する半導体レーザ
を製造することを特徴とする。
The present invention also provides (2) means for introducing a gas containing each component element of Ga, As, Al, and P and a gas containing a component element that becomes an impurity from the outside into a growth tank evacuated to a vacuum.
Using a crystal growth apparatus equipped with a means for heating an n + -type GaAs substrate and a light source for irradiating the n + -type substrate with light, the inside of the growth tank is evacuated to 10 -7 to 10 -9 Pa, and About n + type substrate
While heating to 300 to 600 ° C. and irradiating the n + -type substrate with light from the light source, a gas containing Ga or a gas containing Al at the same time has a pressure in the growth tank of 10 −1 to 10 −7 Pa. After introducing the gas in the range for 0.5 to 10 seconds, and then exhausting the gas in the growth tank, the gas containing As or the gas containing Al at the same time has a pressure in the growth tank of 10 -1.
10-7 By repeating the operation of introducing 2-200 seconds within an amount of Pa, the n + -type substrate to the n-type Ga 1-x Alx As or
A step of growing Ga 1- xAlxAs 1- yPy one molecular layer at a time, and a step of repeatedly growing an undoped Ga 1- xAlxAs 1- yPy layer and a GaAs layer thereon to form a hetero layer Forming a p + -type Ga 1- xAlxAs or Ga 1- xAlxAs 1 - yPy on the hetero layer and then forming a p + -type GaAs layer thereon, insulating on the p + -type GaAs layer After forming the film, a step of forming an opening at a predetermined place, a step of depositing an alloy from the opening to the p + -type layer to form a p + -type electrode, and an alloy is vapor-deposited on the n + -type substrate. The step of forming an n + -type electrode is sequentially performed to manufacture a semiconductor laser having a quantum well structure.

[発明の実施例] 以下、本発明の実施例を半導体としてGaAsとGa1-xAlxAs
あるいはGa1-xAlxAs1-yPyを用いた場合を例にとり説明
する。
[Examples of the Invention] In the following, examples of the present invention are used as semiconductors for GaAs and Ga 1- x AlxAs.
Alternatively, a case of using Ga 1- xAlxAs 1- yPy will be described as an example.

第1図は本発明の一実施例に係る半導体レーザ製造装置
の構成図を示したもので、1は成長槽で材質はステンレ
ス等の金属、2はゲートバルブ、3は成長槽1を超高真
空に排気するための排気装置、4はTMG(トリメチルガ
リウム)等のGaを含むガスを導入するノズル、5はAsH3
を導入するノズル、6はTMA(トリメチルアルミニウ
ム)等のAlを含むガスを導入するノズル、7はPH3等の
Pを含むガスを導入するノズル、8はGaAsとGa1-xAlxAs
1-yPyへのn型不純物となるH2S等のSを含むガスを導入
するノズル、9はノズル8と同様にp型の不純物となる
TMZ(トリメチル亜鉛)等のZnを含むガスを導入するノ
ズル、10,11,12,13,14,15は前記ノズルを開閉するバル
ブでガス源16(Ga(CH3等)、17(AsH3)、18(TM
A)、19(PH3等)、20(TMZ等)、21(H2S等)との間に
設けられる。22は基板加熱用のヒーターで、石英ガラス
に封入したW(タングステン)線であり、配線は図示省
略してある。23は測温用の熱電対である。24は基板への
光照射用の光源で、水銀ランプ,エキシマレーザ,アル
ゴンイオンレーザ等が使用できる。25は光照射用の窓、
26は成長槽内の圧力を測定するための圧力計、27はGaAs
基板である。
FIG. 1 is a block diagram of a semiconductor laser manufacturing apparatus according to an embodiment of the present invention, in which 1 is a growth tank and the material is a metal such as stainless steel, 2 is a gate valve, 3 is an ultrahigh growth tank 1. An evacuation device for evacuation to a vacuum, 4 a nozzle for introducing a gas containing Ga such as TMG (trimethylgallium), and 5 an AsH 3
Nozzle for introducing, 6 is a nozzle for introducing a gas containing Al such as TMA (trimethylaluminum), 7 is a nozzle for introducing a gas containing P such as PH 3 , 8 is GaAs and Ga 1- xAlxAs
A nozzle for introducing a gas containing S such as H 2 S which becomes an n-type impurity into 1- yPy, and 9 becomes a p-type impurity like the nozzle 8.
Nozzles for introducing a gas containing Zn such as TMZ (trimethylzinc), 10,11,12,13,14,15 are valves for opening and closing the nozzles, and gas sources 16 (Ga (CH 3 ) 3 etc.), 17 ( AsH 3 ), 18 (TM
A), 19 (PH 3 etc.), 20 (TMZ etc.), 21 (H 2 S etc.). Reference numeral 22 is a heater for heating the substrate, which is a W (tungsten) wire enclosed in quartz glass, and the wiring is not shown. 23 is a thermocouple for temperature measurement. 24 is a light source for irradiating the substrate with light, and a mercury lamp, an excimer laser, an argon ion laser, or the like can be used. 25 is a window for light irradiation,
26 is a pressure gauge for measuring the pressure in the growth tank, 27 is GaAs
The substrate.

この構成で、GaAsの成長は、先ず、ゲートバルブ2を開
けて超高真空排気装置3により成長槽1内を10-7〜10-8
pascal(以下、Paと略す)程度に排気する。次に、GaAs
基板27を例えば300〜600℃にヒーター22により加熱した
後に、TMGを成長槽1内の圧力が10-1〜10-7Paとなる範
囲で0.5〜10秒間バルブ8を開けて導入する。次に、そ
のTMGを成長槽1内より排気後、AsH313を成長槽1内の
圧力が10-1〜10-7Paとなる範囲で2〜200秒間バルブ5
を開けて導入する。これにより1分子層が成長できる。
With this structure, the growth of GaAs is carried out by first opening the gate valve 2 and using the ultrahigh vacuum exhaust device 3 to grow the inside of the growth tank 1 to 10 -7 to 10 -8.
Exhaust to about pascal (abbreviated as Pa below). Next, GaAs
After heating the substrate 27 to, for example, 300 to 600 ° C. by the heater 22, TMG is introduced by opening the valve 8 for 0.5 to 10 seconds within the range where the pressure in the growth tank 1 is 10 −1 to 10 −7 Pa. Next, after the TMG is evacuated from the growth tank 1, AsH 3 13 is valved for 2 to 200 seconds within a range where the pressure in the growth tank 1 is 10 -1 to 10 -7 Pa.
Open and install. Thereby, one molecular layer can be grown.

一方、Ga1-xAlxAs1-yPyの成長はGaAsの成長と同じよう
にIII族のGaとAlを導入した後に、V族のAsとPを導入
することによって1分子層が成長できる。
On the other hand, in the growth of Ga 1- xAlxAs 1- yPy, one molecular layer can be grown by introducing Ga and Al of the group III and then introducing As and P of the group V like the growth of GaAs.

また、不純物の添加は、p型ではGaと同時にII族を含む
ガス、n型ではAsと同時に、VI族を含むガスを導入する
ことによってそれぞれp、n型の不純物添加を行なうこ
とができる。
The impurities can be added by introducing a gas containing a group II at the same time as Ga in the p-type and a gas containing a group VI at the same time in the n-type as As, respectively.

ここで、レーザダイオードのヘテロ接合としてのGa1-xA
lxAs1-yPyの組成は、GaAsとの格子定数の補償を行なた
め、x=0.3ではyは0.01程度とすれば良いし、場合に
よっては、Pを含まないGa1-xAlxAsでも良い。
Here, Ga 1- xA as a heterojunction of the laser diode
Since the composition of lxAs 1- yPy compensates the lattice constant with GaAs, y may be set to about 0.01 when x = 0.3, or Ga 1- xAlxAs containing no P may be used in some cases.

また、基板の加熱は、ヒーター22による加熱を説明した
が、赤外線ランプ加熱源とし、これを成長槽1の外に設
けるようにしてもよい。更に、基板の加熱と同時に、Hg
ランプ24による光を成長層に照射するようにしてもよ
い。そうした場合には、成長温度を400℃程度に低下で
きるので、不純物のオートドーピング乃至は相互拡散を
制御することができるようになる。
Further, the heating of the substrate has been described as the heating by the heater 22. However, an infrared lamp heating source may be provided outside the growth tank 1. Furthermore, at the same time as heating the substrate, Hg
The growth layer may be irradiated with light from the lamp 24. In such a case, since the growth temperature can be lowered to about 400 ° C., it becomes possible to control auto-doping of impurities or mutual diffusion.

このように、III−V族ないしはその混晶成分元素を含
むガスを交互に導入し、化学反応によって結晶成長を進
行させることにより、化学量論的組成を完全なものとす
るIII−V族およびその混晶の結晶成長層を1分子層毎
に成長させることができ、従来方法では得られないよう
な高品質の半導体レーザが製造できるようになる。
As described above, the gases containing the III-V group or the mixed crystal component elements thereof are alternately introduced, and the crystal growth is advanced by the chemical reaction to complete the stoichiometric composition. The crystal growth layer of the mixed crystal can be grown for each molecular layer, and a high quality semiconductor laser which cannot be obtained by the conventional method can be manufactured.

第2図は上述第1図の装置を用いて製造する半導体レー
ザの製造過程を示したもので、同図(a)の30はn+(ρ
=1×10-3Ω・cm)のGaAs基板である。この基板30上
に、n形(n=1×1018cm-3)Ga1-xAlxAs1-yPy層31を
ヘテロエピタキシャル成長させる(b)。次いで、その
上にアンドロープのn形GaAs層32を成長させる(c)。
更にその上にp形のGa1-xAlxAs1-yPy層33を成長させる
(d)。このときの成長層の厚さは、Ga1-xAlxAs1-yPy
層31,33を0.5μm、アンドロープのn形GaAs層32を500
〜1000Å程度に形成する。このダブルヘテロ構造の半導
体のp層へSiO2またはSi3N4等の絶縁膜34を全面に形成
したのち、開口部を設ける(e)。次いで、その露出し
たp形Ga1-xAlxAs1-yPy層32へZnによる不純物拡散を行
ない、p+層35を形成する(f)。そのp+層35へAu−Zn、
Ag−Zn等の合金を蒸着してp+電極36を形成する(g)。
次に、n+基板30を100μm程度まで薄くして、An−Ge、A
u−Ge−Ni合金によりn+電極37を形成する(h)。この
ようにしてできたウエハを100μm×200μm程度に壁開
し、ボンディング等によりパッケージ化することによ
り、レーザダイオードが製造できる。
FIG. 2 shows the manufacturing process of the semiconductor laser produced using the apparatus described above Figure 1, 30 in FIG. (A) is n + ([rho
= 1 × 10 −3 Ω · cm) GaAs substrate. An n-type (n = 1 × 10 18 cm −3 ) Ga 1- xAlxAs 1- yPy layer 31 is heteroepitaxially grown on this substrate 30 (b). Then, an andrope n-type GaAs layer 32 is grown thereon (c).
Further thereon, a p - type Ga 1- xAlxAs 1- yPy layer 33 is grown (d). The thickness of the growth layer at this time is Ga 1- xAlxAs 1- yPy
Layers 31 and 33 are 0.5 μm, and n-type GaAs layer 32 is 500
Form ~ 1000Å. An insulating film 34 such as SiO 2 or Si 3 N 4 is formed on the entire surface of the p layer of this double-heterostructure semiconductor, and then an opening is provided (e). Next, impurities are diffused into the exposed p-type Ga 1- xAlxAs 1- yPy layer 32 by Zn to form ap + layer 35 (f). Au-Zn to the p + layer 35,
An alloy such as Ag-Zn is deposited to form the p + electrode 36 (g).
Next, the n + substrate 30 is thinned to about 100 μm, and An-Ge, A
An n + electrode 37 is formed from a u-Ge-Ni alloy (h). The laser diode can be manufactured by opening the thus-formed wafer to a size of about 100 μm × 200 μm and packaging it by bonding or the like.

以上は最も簡単なダブルヘテロ形のレーザダイオードの
製造について説明したが、他の構造のものも前記結晶成
長法により実現できることは言う迄もない。
Although the manufacture of the simplest double-hetero laser diode has been described above, it goes without saying that other structures can be realized by the crystal growth method.

第3図は本発明の別の実施例であって、いわゆる量子井
戸型の半導体レーザの製造過程を示したものである。40
はn+(ρ=1×10-3Ω・cm)のGaAs基板である(a)。
この基板40上にn(n=1×1018cm-3)形Ga1-xAlxAs1-
yPy層41を0.5μm、前述第1図の装置を用いてエピタキ
シャル成長させ(b)。その上にアンドープのGa1-xAlx
As1-yPy層42を形成し(c)、更にその上にGaAs層43を
成長させる(d)。これらの成長層42,43の厚さは約100
Åで、これを交互に繰り返し成長させる(e)。更に、
この成長層42,43を繰り返しに10組のヘテロ層45成長さ
せる(f)。更に、その10組のヘテロ層45の上にp+(p
=1×1018cm-3)形Ga1-xAlxAs1-yPy層46を形成し、そ
の上にp+(p=1×1019cm-3)形GaAs層47を形成する
(g)。このようにして分子層エピタキシャル成長法に
よって成長させたウエハのp+形GaAs層47上へ、SiO2また
はSi3N4膜48を付着させて開孔し(h)、p+層47へはAu
−Zn、Ag−Zn等、n+基板40へはAu−Ge、Au−Ge−Ni等の
合金によりオーミックコンタクト49,50を形成する
(i)。これにより、量子井戸型の半導体レーザが製造
できる。
FIG. 3 shows another embodiment of the present invention, showing a manufacturing process of a so-called quantum well type semiconductor laser. 40
Is a n + (ρ = 1 × 10 −3 Ω · cm) GaAs substrate (a).
On this substrate 40, n (n = 1 × 10 18 cm -3 ) type Ga 1- xAlxAs 1-
A yPy layer 41 of 0.5 μm is epitaxially grown using the apparatus shown in FIG. 1 (b). Undoped Ga 1- x Alx
An As 1- yPy layer 42 is formed (c), and a GaAs layer 43 is further grown thereon (d). The thickness of these growth layers 42,43 is about 100.
Repeat with Å to grow repeatedly (e). Furthermore,
The growth layers 42 and 43 are repeatedly grown to form 10 hetero layers 45 (f). Furthermore, p + (p
= 1 × 10 18 cm -3 ) type Ga 1- xAlxAs 1- yPy layer 46 is formed, and a p + (p = 1 × 10 19 cm -3 ) type GaAs layer 47 is formed thereon (g). An SiO 2 or Si 3 N 4 film 48 is attached and opened on the p + -type GaAs layer 47 of the wafer thus grown by the molecular layer epitaxial growth method (h), and the p + layer 47 is Au.
Ohmic contacts 49, 50 are formed on the n + substrate 40 such as -Zn, Ag-Zn or the like by an alloy such as Au-Ge or Au-Ge-Ni (i). Thereby, a quantum well type semiconductor laser can be manufactured.

[発明の効果] 以上のように本発明によれば、化学量論的組成を満たす
高品質の結晶薄膜を単分子層の精度で成長させることが
でき、ダブルヘテロ構造を有する高品質のGaAs形のレー
ザダイオードが製造できるようになる。
[Effects of the Invention] As described above, according to the present invention, a high-quality crystal thin film satisfying a stoichiometric composition can be grown with the accuracy of a monolayer, and a high-quality GaAs type having a double hetero structure can be obtained. Laser diode can be manufactured.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明の一実施例に係る結晶成長装置の構成
図、第2図および第3図は第1図の装置により製造され
る半導体レーザの製造過程説明図で、第2図(a)〜
(h)はダブルヘテロ形半導体レーザの製造過程説明
図、第3図(a)〜(i)は量子井戸型半導体レーザの
製造過程説明図である。 1……金属、2……ゲートバルブ、3……排気装置、4,
5,6,7,8,9……ノズル、10〜15……バルブ、16〜21……
ガス源、22……ヒーター、23……熱電対、24……光源、
25……窓。
FIG. 1 is a block diagram of a crystal growth apparatus according to an embodiment of the present invention, and FIGS. 2 and 3 are explanatory views of a manufacturing process of a semiconductor laser manufactured by the apparatus of FIG. ) ~
(H) is a manufacturing process explanatory view of a double hetero type semiconductor laser, and FIGS. 3 (a) to (i) are manufacturing process explanatory views of a quantum well type semiconductor laser. 1 ... metal, 2 ... gate valve, 3 ... exhaust device, 4,
5,6,7,8,9 …… Nozzle, 10-15 …… Valve, 16-21 ……
Gas source, 22 ... Heater, 23 ... Thermocouple, 24 ... Light source,
25 ... windows.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 本谷 薫 宮城県仙台市米ヶ袋2丁目1番9号406 (56)参考文献 応用物理 53[6],1984−6,P. 516〜P.520 「化合物半導体デバイス[▲I▼](株 式会社工業調査会,1987年7月15日発行) P.126〜P.131 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Kaoru Motoya 2-9-9 Yonegabukuro, Sendai City, Miyagi 406 (56) References Applied Physics 53 [6], 1984-6, pp. 516-P. 520 “Compound semiconductor devices [▲ I ▼]” (Industry Research Institute of the Stock Company, published on July 15, 1987) P.126 to P.131

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】真空に排気する成長槽内に外部よりGa、A
s、Al及びPの各成分元素を含むガス及び不純物となる
成分元素を含むガスをそれぞれ導入する手段と、n+形Ga
As基板を加熱する手段と、前記n+形基板を光照射する光
源とを具備した結晶成長装置を用い、 前記成長槽内を10-7〜10-9Paに排気すると共に、前記n+
形基板を約300〜600℃に加熱し、前記光源より前記n+
基板に光を照射しながら、Gaを含むガス又は同時にAlを
含むガスを成長槽内の圧力が10-1〜10-7Paとなる範囲で
0.5〜10秒間導入し、次いで成長槽内のガスを排気した
後、Asを含むガス又は同時にAlを含むガスを成長槽内の
圧力が10-1〜10-7Paとなる範囲で2〜200秒間導入する
操作を繰り返すことにより、前記n+形基板上にn形のGa
1-xAlxAs又はGa1-xAlxAs1-yPyを1分子層ずつ成長させ
る工程、 その上にアンドープのGaAsを形成する工程、 さらにその上にp形のGa1-xAlxAs又はGa1-xAlxAs1-yPy
を成長させる工程、 その上に絶縁膜を形成した後、所定個所に開口部を形成
して前記p形層へZnによる不純物拡散を行ってp+形層を
形成する工程、 前記p+形層へ合金を蒸着してp+形電極を形成する工程、 前記n+形基板に合金を蒸着してn+形電極を形成する工
程、 を順次実行して半導体レーザを製造することを特徴とす
る半導体レーザの製造方法。
1. A growth chamber evacuated to a vacuum is supplied with Ga and A from the outside.
a means for introducing a gas containing each elemental element of s, Al, and P and a gas containing an elemental element that becomes an impurity, and n + -type Ga
Using a crystal growth apparatus equipped with a means for heating the As substrate and a light source for irradiating the n + -type substrate with light, the inside of the growth tank is evacuated to 10 -7 to 10 -9 Pa, and the n +
While heating the shaped substrate to about 300 to 600 ° C. and irradiating the n + type substrate with light from the light source, a gas containing Ga or at the same time a gas containing Al is grown at a pressure of 10 −1 to 10 − In the range of 7 Pa
After introducing the gas for 0.5 to 10 seconds and then exhausting the gas in the growth tank, a gas containing As or a gas containing Al at the same time is 2 to 200 in the range where the pressure in the growth tank is 10 -1 to 10 -7 Pa. By repeating the operation of introducing for a second, n-type Ga is formed on the n + -type substrate.
Step of growing 1 - xAlxAs or Ga 1- xAlxAs 1- yPy for each molecular layer, step of forming undoped GaAs thereon, and p - type Ga 1 - xAlxAs or Ga 1- xAlxAs 1- yPy
A step of growing a p + -type layer by forming an opening at a predetermined location and diffusing impurities into the p-type layer by Zn to form a p + -type layer after forming an insulating film on the p + -type layer. A semiconductor laser is manufactured by sequentially performing a step of vapor-depositing an alloy to form ap + -type electrode, and a step of vapor-depositing an alloy onto the n + -type substrate to form an n + -type electrode. Manufacturing method of semiconductor laser.
【請求項2】真空に排気する成長槽内に外部よりGa、A
s、Al及びPの各成分元素を含むガス及び不純物となる
成分元素を含むガスをそれぞれ導入する手段と、n+形Ga
As基板を加熱する手段と、前記n+形基板を光照射する光
源とを具備した結晶成長装置を用い、 前記成長槽内を10-7〜10-9Paに排気すると共に、前記n+
形基板を約300〜600℃に加熱し、前記光源より前記n+
基板に光を照射しながら、Gaを含むガス又は同時にAlを
含むガスを成長槽内の圧力が10-1〜10-7Paとなる範囲で
0.5〜10秒間導入し、次いで成長槽内のガスを排気した
後、Asを含むガス又は同時にAlを含むガスを成長槽内の
圧力が10-1〜10-7Paとなる範囲で2〜200秒間導入する
操作を繰り返すことにより、前記n+形基板上にn形のGa
1-xAlxAs又はGa1-xAlxAs1-yPyを1分子層ずつ成長させ
る工程、 その上にアンドープのGa1-xAlxAs1-yPy層と、さらにそ
の上にGaAs層とを繰り返し成長させることによりヘテロ
層を形成させる工程、 前記ヘテロ層上にp+形のGa1-xAlxAs又はGa1-xAlxAs1-yP
yを形成した後、その上にp+形GaAs層を形成する工程、 前記p+形GaAs層上に絶縁膜を形成した後、所定個所に開
口部を形成する工程、 前記開口部より前記p+形層へ合金を蒸着してp+形電極を
形成する工程、 前記n+形基板に合金を蒸着してn+形電極を形成する工
程、 を順次実行して量子井戸構造を有する半導体レーザを製
造することを特徴とする半導体レーザの製造方法。
2. Ga, A from the outside in a growth tank evacuated to a vacuum
a means for introducing a gas containing each elemental element of s, Al, and P and a gas containing an elemental element that becomes an impurity, and n + -type Ga
Using a crystal growth apparatus equipped with a means for heating the As substrate and a light source for irradiating the n + -type substrate with light, the inside of the growth tank is evacuated to 10 -7 to 10 -9 Pa, and the n +
While heating the shaped substrate to about 300 to 600 ° C. and irradiating the n + type substrate with light from the light source, a gas containing Ga or at the same time a gas containing Al is grown at a pressure of 10 −1 to 10 − In the range of 7 Pa
After introducing the gas for 0.5 to 10 seconds and then exhausting the gas in the growth tank, a gas containing As or a gas containing Al at the same time is 2 to 200 in the range where the pressure in the growth tank is 10 -1 to 10 -7 Pa. By repeating the operation of introducing for a second, n-type Ga is formed on the n + -type substrate.
A step of growing 1 - xAlxAs or Ga 1- xAlxAs 1- yPy by one molecular layer, a hetero layer by repeatedly growing an undoped Ga 1- xAlxAs 1- yPy layer and a GaAs layer thereon. Forming a p + -type Ga 1 - xAlxAs or Ga 1- xAlxAs 1- yP on the hetero layer.
After forming y, a step of forming ap + -type GaAs layer thereon, a step of forming an insulating film on the p + -type GaAs layer, and then forming an opening at a predetermined location, A semiconductor laser having a quantum well structure by sequentially performing a step of depositing an alloy on a + type layer to form ap + type electrode, a step of depositing an alloy on the n + type substrate to form an n + type electrode. A method of manufacturing a semiconductor laser, comprising:
JP59153971A 1984-07-26 1984-07-26 Method for manufacturing semiconductor laser Expired - Fee Related JPH0728079B2 (en)

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Publication number Priority date Publication date Assignee Title
JP2544378B2 (en) * 1987-03-25 1996-10-16 株式会社日立製作所 Optical semiconductor device
JPH07517B2 (en) * 1987-05-30 1995-01-11 松下電器産業株式会社 Semiconductor crystal thin film manufacturing equipment

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
「化合物半導体デバイス[▲I▼(株式会社工業調査会,1987年7月15日発行)P.126〜P.131
応用物理53[6,1984−6,P.516〜P.520

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