JPH0888432A - Production of semiconductor laser - Google Patents

Production of semiconductor laser

Info

Publication number
JPH0888432A
JPH0888432A JP22202094A JP22202094A JPH0888432A JP H0888432 A JPH0888432 A JP H0888432A JP 22202094 A JP22202094 A JP 22202094A JP 22202094 A JP22202094 A JP 22202094A JP H0888432 A JPH0888432 A JP H0888432A
Authority
JP
Japan
Prior art keywords
layer
type
injection region
semiconductor
current 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
Application number
JP22202094A
Other languages
Japanese (ja)
Inventor
Haruo Tanaka
治夫 田中
Yukio Shakuda
幸男 尺田
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.)
Rohm Co Ltd
Original Assignee
Rohm Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Rohm Co Ltd filed Critical Rohm Co Ltd
Priority to JP22202094A priority Critical patent/JPH0888432A/en
Publication of JPH0888432A publication Critical patent/JPH0888432A/en
Priority to US08/892,273 priority patent/US5974069A/en
Priority to US09/392,456 priority patent/US6298079B1/en
Priority to US09/392,459 priority patent/US6274891B1/en
Pending legal-status Critical Current

Links

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
    • H01S5/32341Structure 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 blue laser based on GaN or GaP

Landscapes

  • Semiconductor Lasers (AREA)

Abstract

PURPOSE: To easily control the current injection area even a in semiconductor laser using a gallium nitride-based compound semiconductor by providing an n-type layer, active layer and p-type layer on a substrate, activating a p-type layer in the current injection area of the piled-up semiconductor layers and keeping a p-type layer other than it in an in active state. CONSTITUTION: An n-type low-temperature buffer layer 2, n-type hightemperature buffer layer 3, n-type clad layer 4, active layer 5, and p-type clad layer 6 are formed in sequence on a substrate 1. Next, a p-type contact layer 7 is formed in order to reduce the contact resistance against a p-type electrode. Then, the joint of H with Mg or Zn as dopant for the p-type layer is released and activated to reduce the resistance. That is, the whole substrate in which the semiconductor layers are piled up is put into a furnace of nitrogen atmosphere so as to be heated at 400 to 800 deg.C. Further, an inactivating treatment is applied to the non-injection area of current. Namely, a protection layer 8 is provided on the surface of the semiconductor layer consisting of only current injection area, and it is heated at 400 to 800 deg.C in an atmosphere containing H.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は半導体レーザの製法に関
する。さらに詳しくは、青色発光に好適なチッ化ガリウ
ム系化合物半導体を用いて、電流非注入領域を高抵抗に
して電流注入領域を制御する利得導波構造に適した半導
体レーザに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for manufacturing a semiconductor laser. More specifically, the present invention relates to a semiconductor laser suitable for a gain waveguide structure in which a current non-injection region is made to have high resistance and a current injection region is controlled by using a gallium nitride based compound semiconductor suitable for blue light emission.

【0002】ここにチッ化ガリウム系化合物半導体と
は、III 族元素のGaとV族元素のNとの化合物または
III 族元素のGaの一部がAl、Inなど他のIII 族元
素と置換したものおよび/またはV族元素のNの一部が
P、Asなど他のV族元素と置換した化合物からなる半
導体をいう。
Here, a gallium nitride compound semiconductor is a compound of a group III element Ga and a group V element N or
A semiconductor made of a compound in which a part of Ga of the group III element is replaced with another group III element such as Al and In and / or a part of N of the group V element is replaced with another group V element such as P and As. Say.

【0003】[0003]

【従来の技術】半導体レーザの導波構造として、一般的
には屈折率導波構造と利得導波構造が知られている。屈
折率導波構造は、活性層に平行方向に屈折率差をもた
せ、光を閉じ込めて導波させるもので、高出力動作まで
の単一横モード発振をうることができるが、可干渉性が
高く戻り光誘起ノイズが発生し易い。一方、利得導波構
造は、横方向に屈折率差をもたない構造で、横モードが
不安定でキンクが生じ易いが、縦マルチモード発振をす
るため、戻り光ノイズが小さい。
2. Description of the Related Art As a waveguide structure of a semiconductor laser, a refractive index waveguide structure and a gain waveguide structure are generally known. The refractive index guiding structure has a refractive index difference in the direction parallel to the active layer to confine and guide light, and it is possible to obtain single transverse mode oscillation up to high output operation. High return light-induced noise is likely to occur. On the other hand, the gain waveguide structure is a structure having no refractive index difference in the lateral direction, and the transverse mode is unstable and a kink is likely to occur, but since the longitudinal multimode oscillation occurs, the return light noise is small.

【0004】この利得導波構造の電流注入領域を制御す
る最も簡単な構造としては、図4(a)〜(c)に示さ
れるように、電極をパターン化して電極パターンの下側
のみを電流注入領域とする構造(図4(a)参照)や、
電流注入領域の両側にプロトンなどを打ち込んで高抵抗
化する構造(図4(b)参照)や、電流注入領域の両側
をエッチング除去してメサ型形状にする構造(図4
(c)参照)などが用いられている。なお、図4におい
て、21はたとえばn型GaAs基板で、その上にn型
クラッド層22、活性層23、p型クラッド層24が順
次積層されたダブルヘテロ接合構造の半導体レーザが構
成され、25はp側電極、26はn側電極、27はプロ
トン打込領域である。
The simplest structure for controlling the current injection region of this gain waveguide structure is to pattern the electrodes as shown in FIGS. A structure to be an implantation region (see FIG. 4A),
A structure in which protons are implanted into both sides of the current injection region to increase the resistance (see FIG. 4B), or a structure in which both sides of the current injection region are removed by etching to form a mesa shape (FIG. 4).
(See (c)) is used. In FIG. 4, reference numeral 21 denotes, for example, an n-type GaAs substrate, on which a n-type clad layer 22, an active layer 23, and a p-type clad layer 24 are sequentially laminated to constitute a semiconductor laser having a double heterojunction structure. Is a p-side electrode, 26 is an n-side electrode, and 27 is a proton implantation region.

【0005】一方チッ化ガリウム系化合物半導体を用い
た発光ダイオード(以下、LEDという)が開発され、
従来の赤色、緑色のLEDに加えて青色においても高輝
度のLEDがえられ、半導体レーザにおいても青色の半
導体レーザの開発が要望されている。このチッ化ガリウ
ム系化合物半導体を用いたLEDはp型層のエピタキシ
ャル成長をする際に、GaやNのほかにp型ドーパント
のMgやZnがキャリアガスのH2 や反応ガスのNH3
などのHと結合し易く、ドーパントとしての機能を充分
に果さないため、p型層の成長後アニールによる活性化
処理を施してMgやZnとHとの結合を切り離し低抵抗
化を図っている。
On the other hand, a light emitting diode (hereinafter referred to as LED) using a gallium nitride based compound semiconductor was developed,
In addition to conventional red and green LEDs, LEDs with high brightness in blue can be obtained, and there is a demand for development of blue semiconductor lasers in semiconductor lasers. In the LED using the gallium nitride-based compound semiconductor, when the p-type layer is epitaxially grown, in addition to Ga and N, the p-type dopants Mg and Zn are H 2 as a carrier gas and NH 3 as a reaction gas.
Since it easily binds to H and does not sufficiently function as a dopant, an activation treatment by annealing after growth of the p-type layer is performed to separate the bond between Mg and Zn and H to reduce the resistance. There is.

【0006】[0006]

【発明が解決しようとする課題】従来の電極ストライプ
型構造の半導体レーザでは、電極から離れるにしたがっ
て電極ストライプの幅より電流が拡散して発光に寄与し
ない、もれ電流が多くなり、とくにチッ化ガリウム系化
合物半導体では動作電圧が3V程度なので、もれ電流が
多いと発光に寄与しない電力分も大きくなり、発光効率
が低下するという問題がある。
In the conventional semiconductor laser of the electrode stripe type structure, as the distance from the electrode increases, the current does not contribute to light emission due to the diffusion of the current from the width of the electrode stripe. Since the operating voltage of a gallium-based compound semiconductor is about 3 V, if there is a large amount of leakage current, the amount of electric power that does not contribute to light emission also increases and there is a problem in that the light emission efficiency decreases.

【0007】また電極ストライプ両側の電流非注入領域
にプロトンなどを打ち込んで高抵抗化する方法では、プ
ロトン打込みの装置が大がかりとなり、低コストでの大
量生産には向いていないという問題がある。
Further, in the method of implanting protons or the like into the current non-injection regions on both sides of the electrode stripe to increase the resistance, there is a problem in that a device for implanting protons becomes large in size and is not suitable for mass production at low cost.

【0008】さらにエッチングしてメサ型形状にする方
法は、エッチングするのに時間がかかり、とくにチッ化
ガリウム系化合物半導体層をエッチングするのは困難
で、250℃以上の高温でウェットエッチングをするか
塩素ガス雰囲気下で反応性イオンエッチングをしなけれ
ばならず、作業が大変であるという問題がある。
In the method of further etching into a mesa shape, it takes a long time to perform the etching, and it is particularly difficult to etch the gallium nitride-based compound semiconductor layer. Whether the wet etching is performed at a high temperature of 250 ° C. or higher. Reactive ion etching has to be performed in a chlorine gas atmosphere, and there is a problem that the work is difficult.

【0009】本発明はこのような問題を解決し、無効電
流が少なく、簡単な製法で電流注入領域を制御でき、し
かもチッ化ガリウム系化合物半導体を用いた半導体レー
ザにおいても、電流注入領域を簡単に制御できる半導体
レーザの製法を提供することにある。
The present invention solves such a problem, the reactive current is small, the current injection region can be controlled by a simple manufacturing method, and the current injection region is simple even in a semiconductor laser using a gallium nitride based compound semiconductor. It is to provide a method of manufacturing a semiconductor laser that can be controlled in a stable manner.

【0010】[0010]

【課題を解決するための手段】本発明の半導体レーザの
製法は、(a)基板上に少なくともn型層、活性層およ
びp型層を含み、半導体レーザを構成するチッ化ガリウ
ム系化合物半導体を積層し、(b)該積層された半導体
層の電流注入領域におけるp型層を活性化し、(c)前
記積層された半導体層の電流注入領域以外の領域におけ
るp型層を不活性化状態に維持することを特徴とする。
According to the method of manufacturing a semiconductor laser of the present invention, (a) a gallium nitride based compound semiconductor which comprises at least an n-type layer, an active layer and a p-type layer on a substrate and constitutes a semiconductor laser is provided. And (b) activating the p-type layer in the current injection region of the laminated semiconductor layer, and (c) deactivating the p-type layer in the region other than the current injection region of the laminated semiconductor layer. It is characterized by maintaining.

【0011】前記積層された半導体層がn型バッファ
層、n型クラッド層、活性層、p型クラッド層およびp
型コンタクト層であることが、チッ化ガリウム系化合物
半導体からなる半導体レーザを製造するのに好ましい。
The stacked semiconductor layers are an n-type buffer layer, an n-type clad layer, an active layer, a p-type clad layer and a p-type clad layer.
The type contact layer is preferable for producing a semiconductor laser made of a gallium nitride based compound semiconductor.

【0012】前記半導体層の積層後基板全体の熱処理を
行うことによりp型層の活性化を行い、ついで前記電流
注入領域の表面に保護膜を設けて水素を含む雰囲気中で
熱処理を行うことにより前記電流注入領域以外の領域を
不活性化状態にすることが、電流非注入領域を確実に高
抵抗化することができ、電流注入領域を制御することが
できるため好ましい。
After the semiconductor layers are stacked, the entire substrate is heat-treated to activate the p-type layer, and then a protective film is provided on the surface of the current injection region and heat-treated in an atmosphere containing hydrogen. It is preferable to inactivate the region other than the current injection region because the resistance of the current non-injection region can be surely increased and the current injection region can be controlled.

【0013】前記p型層の活性化のため熱処理をチッ素
雰囲気中、400〜800℃で行うことが、半導体層の
表面に保護膜を設けないで熱処理を行っても、チッ化ガ
リウム系化合物半導体層中のNが蒸発しにくく、簡単な
工程で半導体層の劣化が生じないため好ましい。
The heat treatment for activating the p-type layer is performed at 400 to 800 ° C. in a nitrogen atmosphere, even if the heat treatment is performed without providing a protective film on the surface of the semiconductor layer. N in the semiconductor layer is less likely to evaporate and deterioration of the semiconductor layer does not occur in a simple process, which is preferable.

【0014】前記半導体層の積層後前記電流注入領域の
みに電子線を照射し、前記p型層の該電流注入領域のみ
を活性化することによっても、最も少ない工程数で簡単
に電流注入領域を制御することができるため好ましい。
By irradiating only the current injection region with an electron beam after the semiconductor layers are stacked to activate only the current injection region of the p-type layer, the current injection region can be easily formed with the fewest number of steps. It is preferable because it can be controlled.

【0015】[0015]

【作用】本発明の半導体レーザの製法によれば、チッ化
ガリウム系化合物半導体層のp型層はその成膜工程でド
ーパントのMgやZnがキャリアガスや反応ガス中のH
と結合して不活性化しやすいという性質を利用し、p型
層の電流注入領域のみを熱処理や電子線照射によってア
ニールすることにより、MgやZnと結合したHを分離
して放出しているため低抵抗になり、電流非注入領域は
ドーパントのMgやZnをHと結合させたり、チッ化ガ
リウム系化合物半導体のNを蒸発させてn型化している
ため、ドーパントが動きにくく不活性となったり、p型
不純物が薄められることになり高抵抗となる。
According to the method of manufacturing a semiconductor laser of the present invention, in the p-type layer of the gallium nitride based compound semiconductor layer, Mg or Zn as the dopant is H in the carrier gas or the reaction gas in the film forming process.
By utilizing the property of being easily combined with and deactivating, the current injection region of the p-type layer is annealed by heat treatment or electron beam irradiation to separate and release H combined with Mg and Zn. The resistance becomes low, and the current non-injection region combines the dopants Mg and Zn with H, or vaporizes N in the gallium nitride-based compound semiconductor to make it n-type, which makes the dopant difficult to move and inactive. , P-type impurities are thinned, resulting in high resistance.

【0016】すなわちチッ化ガリウム系化合物半導体の
p型層を成膜したのち、全体を熱処理してp型層の活性
化処理を行ったのち、電流注入領域の表面のみに保護膜
をしてH2 ガスやNH3 ガスなどのHの雰囲気中で熱処
理をすることにより、保護膜のある部分はHの侵入が妨
げられるとともに、半導体層からNなどの蒸発を防止す
ることができるが、保護膜のない部分は半導体層内にH
が侵入し、ドーパントのMgやZnと結合し、不活性化
するとともに、半導体層からNが蒸発してn型化する。
そのため、電流注入領域の表面に保護膜を設けて、Hの
存在する雰囲気で充分熱処理をすることにより電流非注
入領域のみを高抵抗化することができる。
That is, after forming a p-type layer of a gallium nitride-based compound semiconductor, the whole is heat-treated to activate the p-type layer, and then a protective film is formed only on the surface of the current injection region to form H. By performing heat treatment in an atmosphere of H such as 2 gas or NH 3 gas, invasion of H can be prevented in a portion where the protective film is present, and evaporation of N or the like from the semiconductor layer can be prevented. There is no H in the semiconductor layer
Penetrates, combines with the dopants Mg and Zn and becomes inactive, and N evaporates from the semiconductor layer to become n-type.
Therefore, by providing a protective film on the surface of the current injection region and performing sufficient heat treatment in an atmosphere containing H, it is possible to increase the resistance only in the current non-injection region.

【0017】また、p型層のエピタキシャル成長の際の
不活性化を利用し、またはさらに水素雰囲気下でp型層
の不活性化を進めたのちに、電流注入領域のみに電子線
を照射することにより、電子線照射は微細に制御でき、
照射部分のみを高温にしてアニールし、低抵抗化するこ
とができるため、電流注入領域を精度よく制御すること
ができる。
Further, the passivation during the epitaxial growth of the p-type layer is utilized, or after the passivation of the p-type layer is further advanced in a hydrogen atmosphere, the electron beam is irradiated only to the current injection region. The electron beam irradiation can be controlled finely by
Since it is possible to reduce the resistance by annealing only the irradiated portion at a high temperature, it is possible to control the current injection region with high accuracy.

【0018】[0018]

【実施例】つぎに添付図面を参照しながら本発明の半導
体レーザの製法を説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A method of manufacturing a semiconductor laser according to the present invention will be described below with reference to the accompanying drawings.

【0019】図1は本発明の半導体レーザの製法の一実
施例(実施例1)の工程断面説明図、図2は他の実施例
(実施例2)の一工程の断面説明図である。
FIG. 1 is a sectional view showing a process of one embodiment (embodiment 1) of the method for manufacturing a semiconductor laser according to the present invention, and FIG. 2 is a sectional view showing one process of another embodiment (embodiment 2).

【0020】本発明は、前述のようにチッ化ガリウム系
化合物半導体のp型層はそのエピタキシャル成長工程で
ドーパントのMgやZnがHと結合して動きにくくなる
ため、活性化処理をしなければ低抵抗のp型層として機
能しないという知見に基づいてなされたものである。す
なわち、チッ化ガリウム系化合物半導体を用いた半導体
発光素子では、p型層をエピタキシャル成長しただけで
はp型ドーパントがドーパントとして充分機能しないた
め、熱処理または電子線照射をすることにより、ドーパ
ントのMgやZnとHとの結合を切り離して活性化を図
っているが、本発明ではこのドーパントのMgやZnと
Hとの結合による不活性化状態になり易いという性質、
および熱処理によりチッ化ガリウム系化合物半導体から
Nが蒸発してn型化し易いという性質を利用し、電流注
入領域のみのp型層の活性化を行い、電流の非注入領域
のp型層はエピタキシャル成長時に生じた不活性化状態
を維持するかまたはさらにHと結合させて不活性化する
ことにより電流注入領域を制御するものである。
According to the present invention, as described above, in the p-type layer of the gallium nitride based compound semiconductor, the dopants Mg and Zn combine with H in the epitaxial growth process to make it difficult to move. This is based on the finding that it does not function as a p-type layer of resistance. That is, in a semiconductor light emitting device using a gallium nitride-based compound semiconductor, the p-type dopant does not sufficiently function as a dopant only by epitaxially growing the p-type layer, and therefore, the dopant Mg or Zn is not exposed by heat treatment or electron beam irradiation. Although the bond between H and H is cut off for activation, in the present invention, the property that the dopant Mg or Zn and the bond between H and H tend to be inactivated.
By utilizing the property that N is easily evaporated from the gallium nitride based compound semiconductor by heat treatment and becomes n-type by heat treatment, the p-type layer only in the current injection region is activated, and the p-type layer in the current non-injection region is epitaxially grown. The current injection region is controlled by maintaining the inactivated state that sometimes occurs or by further inactivating it by combining with H.

【0021】電流注入領域を活性化し、電流非注入領域
を不活性化する方法としては、p型層の全体を熱処理ま
たは電子線照射などにより活性化したのち電流の非注入
領域のみのp型層のドーパントをHと結合させて不活性
化状態にしたり、チッ化ガリウム系化合物半導体層のN
を蒸発させてn型化し高低抗にする方法と、p型層全体
をp型層のエピタキシャル成長時または成長後の水素雰
囲気下での熱処理により不活性化状態にしておき、電流
注入領域のみのp型層を活性化する方法がある。以下、
具体的な実施例でさらに詳細に説明する。
As a method of activating the current injection region and deactivating the current non-injection region, the entire p-type layer is activated by heat treatment or electron beam irradiation, and then the p-type layer having only the current non-injection region is activated. Is combined with H to bring it into an inactivated state, and N of the gallium nitride-based compound semiconductor layer is combined.
Of the p-type layer by evaporating the n-type to make it have a high resistance, and the whole p-type layer is inactivated by heat treatment in a hydrogen atmosphere during or after the epitaxial growth of the p-type layer, and only the current injection region is p-typed. There is a method of activating the mold layer. Less than,
It will be described in more detail with reference to specific examples.

【0022】実施例1 本実施例は半導体レーザを構成するチッ化ガリウム系化
合物半導体からなる半導体層を基板上に積層したのち、
全体を熱処理によりアニールして活性化し、そののち電
流注入領域の表面のみに保護膜を設けてH2 ガスやNH
3 などHの存在する雰囲気下で熱処理をすることによ
り、保護膜の存在しない半導体層中にHを侵入させてM
gやZnなどのp型ドーパントと結合させるとともに、
チッ化ガリウム系化合物半導体中のNを蒸発させて高抵
抗化し、電流注入領域は保護膜によりHの侵入を防止し
て活性化状態を維持し低抵抗にすることにより電流注入
領域を制御するものである。図1を参照して本発明の製
法を詳細に説明する。
Example 1 In this example, after a semiconductor layer made of a gallium nitride-based compound semiconductor constituting a semiconductor laser was laminated on a substrate,
The whole is annealed and activated by heat treatment, and then a protective film is provided only on the surface of the current injection region to remove H 2 gas and NH.
By heat treatment in an atmosphere containing H such as 3 , H is caused to penetrate into the semiconductor layer without the protective film, and M
While combining with a p-type dopant such as g or Zn,
Controlling the current injection region by evaporating N in the gallium nitride-based compound semiconductor to increase its resistance and preventing the invasion of H by the protective film to maintain the activated state and lower the resistance. Is. The manufacturing method of the present invention will be described in detail with reference to FIG.

【0023】まず、図1(a)に示されるように、サフ
ァイヤ(Al2 3 単結晶)などからなる基板1に40
0〜700℃の低温で有機金属化合物気相成長法(以
下、MOCVD法という)によりキャリアガスH2 とと
もに有機金属化合物ガスであるトリメチルガリウム(以
下、TMGという)、NH3 およびドーパントとしての
SiH4 またはGeH4 、SnH4 、TeH4 などを供
給し、n型のGaNからなる低温バッファ層2を0.0
1〜0.2μm程度形成し、ついで700〜1200℃
の高温で同じ組成のn型GaNからなる高温バッファ層
3を2〜5μm程度形成する。
First, as shown in FIG. 1 (a), a substrate 1 made of sapphire (Al 2 O 3 single crystal) or the like is provided with 40
Trimethylgallium (hereinafter, referred to as TMG) which is an organic metal compound gas, NH 3 and SiH 4 as a dopant together with a carrier gas H 2 by a metal organic compound vapor phase growth method (hereinafter, referred to as MOCVD method) at a low temperature of 0 to 700 ° C. Alternatively, GeH 4 , SnH 4 , TeH 4 or the like is supplied to form the low temperature buffer layer 2 made of n-type GaN with 0.0
1 ~ 0.2μm, then 700 ~ 1200 ℃
The high temperature buffer layer 3 made of n-type GaN having the same composition is formed at a high temperature of about 2 to 5 μm.

【0024】ついで、前述のガスにさらにトリメチルア
ルミニウム(以下、TMAという)の原料ガスを加え、
n型ドーパントのSiなどを含有したn型Alx Ga
1-x N(0<x<1)層を成膜し、ダブルヘテロ接合形
成のためのn型クラッド層4を0.1〜0.3μm程度
形成する。
Then, a source gas of trimethylaluminum (hereinafter referred to as TMA) is further added to the above gas,
n-type Al x Ga containing n-type dopant such as Si
A 1-xN (0 <x <1) layer is formed, and an n-type cladding layer 4 for forming a double heterojunction is formed to have a thickness of about 0.1 to 0.3 μm.

【0025】つぎに、バンドギャップエネルギーがクラ
ッド層のそれよりも小さくなる材料、たとえば前述の原
料ガスのTMAに代えてトリメチルインジウム(以下、
TMIという)を導入し、Gay In1-y N(0<y≦
1)からなる活性層5を0.05〜0.1μm程度形成
する。
Next, a material whose band gap energy is smaller than that of the cladding layer, such as trimethylindium (hereinafter
Introducing TMI), Ga y In 1-y N (0 <y ≦
The active layer 5 composed of 1) is formed to a thickness of about 0.05 to 0.1 μm.

【0026】さらに、n型クラッド層4の形成に用いた
ガスと同じ原料のガスで不純物原料ガスをSiH4 など
に代えてp型不純物としてMgまたはZnをビスシクロ
ペンタジエニルマグネシウム(以下、Cp2 Mgとい
う)またはジメチル亜鉛(以下、DMZn)として加え
て反応管に導入し、p型クラッド層6であるp型Alx
Ga1-x N層を気相成長させる。これによりn型クラッ
ド層4と活性層5とp型クラッド層6とによりダブルヘ
テロ接合が形成される。
Further, the same raw material gas as that used for forming the n-type cladding layer 4 is used, and the impurity raw material gas is replaced with SiH 4 or the like, and Mg or Zn is replaced with biscyclopentadienyl magnesium (hereinafter referred to as Cp 2 Mg) or dimethylzinc (hereinafter referred to as DMZn) and introduced into the reaction tube to form the p-type clad layer 6 of p-type Al x.
The Ga 1-x N layer is vapor-grown. As a result, a double heterojunction is formed by the n-type clad layer 4, the active layer 5, and the p-type clad layer 6.

【0027】ついで、p型電極との接触抵抗を減少させ
るためのp型コンタクト層7を形成するため、前述のバ
ッファ層3と同様のガスで不純物ガスとしてCp2 Mg
またはDMZnを供給してp型のGaN層を0.3〜2
μm程度成長させ、半導体層の積層が完了する。
Next, in order to form the p-type contact layer 7 for reducing the contact resistance with the p-type electrode, the same gas as the buffer layer 3 is used as Cp 2 Mg as an impurity gas.
Alternatively, DMZn may be supplied to form a p-type GaN layer of 0.3 to 2
The growth of about μm is completed, and the stacking of the semiconductor layers is completed.

【0028】つぎにp型層のドーパントであるMgやZ
nとHとの結合を分離して活性化させて抵抗を小さくす
る処理を行う。すなわち、半導体層が積層された基板全
体をチッ素雰囲気中の炉内に入れて400〜800℃、
約1気圧のもとで20〜60分間程度の熱処理をする。
このばあい、熱処理の際に全体の温度が高温になるた
め、チッ化ガリウム系化合物半導体中のNやGa、とく
にNの蒸発が起り易いが、炉内の雰囲気ガスをチッ素に
しているため、その蒸発を防止することができ、蒸発し
易いHのみがMgなどとの結合を切られて蒸発する。な
お、NやGaの蒸発を防止するため、1気圧でなく、2
〜100気圧程度の高圧にしてもHは蒸発し易いため、
確実な活性化処理をすることもできる。このようにチッ
素雰囲気中で行うことにより、表面に保護膜を設けなく
てもNやGaの蒸発を防止することができるため好まし
い。
Next, Mg or Z which is a dopant for the p-type layer
A process of reducing the resistance by separating and activating the bond between n and H is performed. That is, the whole substrate on which the semiconductor layers are stacked is put in a furnace in a nitrogen atmosphere and 400 to 800 ° C.
Heat treatment is performed for about 20 to 60 minutes under about 1 atmosphere.
In this case, N and Ga in the gallium nitride-based compound semiconductor, especially N are easily vaporized because the whole temperature becomes high during the heat treatment, but the atmosphere gas in the furnace is nitrogen. However, only H, which can prevent the evaporation and is easy to evaporate, has its bond with Mg or the like cut off and evaporates. In order to prevent the evaporation of N and Ga, it is not 1 atm but 2
Even if the pressure is about 100 atm, H easily evaporates.
A reliable activation process can also be performed. By carrying out in a nitrogen atmosphere as described above, it is possible to prevent evaporation of N and Ga without providing a protective film on the surface, which is preferable.

【0029】つぎに電流の非注入領域の不活性化処理を
行う(図1(b)参照)。具体的には電流注入領域だけ
の半導体層の表面にSiO2 、Si3 4 、Al2 3
などの保護膜8を0.05〜0.3μm程度設け、H2
ガスやNH3 などのHが存在するガス雰囲気(たとえば
1気圧)下で400〜800℃、20〜60分間の熱処
理を行う。熱処理により雰囲気中のHがp型層の半導体
層中に侵入し、前述のようにドーパントのMgやZnな
どと結合して不活性化し、高抵抗となる。また熱処理中
に半導体層のGaやNが分解して蒸発し易く、とくにN
の方が蒸発し易く、保護膜8のある部分は保護膜によっ
て蒸発が制御されるが、保護膜8のない部分はNが蒸発
し易い。チッ化ガリウム系化合物半導体のp型層からN
が蒸発するとn型化するため、高抵抗になる。その結
果、保護膜8のない電流の非注入領域の高抵抗化が図ら
れる。なお、前述の保護膜8の形成は、CVD法、スパ
ッタ法などによりSiO2 などを表面全体に設け、レジ
スト膜の露光、現像、エッチングなどの通常のフォトリ
ソグラフィ工程により、電流注入領域表面のみの必要部
分だけに保護膜8を設けることができる。
Next, the non-injection region of the current is inactivated (see FIG. 1B). Specifically, SiO 2 , Si 3 N 4 , Al 2 O 3 is formed on the surface of the semiconductor layer only in the current injection region.
A protective film 8 such as 0.05 to 0.3 μm is provided, and H 2
Heat treatment is performed at 400 to 800 ° C. for 20 to 60 minutes in a gas atmosphere (for example, 1 atm) in which gas or H such as NH 3 exists. By the heat treatment, H in the atmosphere penetrates into the semiconductor layer of the p-type layer and is combined with the dopants Mg, Zn and the like to be inactivated, resulting in high resistance. Further, during heat treatment, Ga and N in the semiconductor layer are decomposed and easily vaporized.
Is more likely to evaporate, and the evaporation is controlled by the protective film in the portion with the protective film 8, but N is more easily evaporated in the portion without the protective film 8. From the p-type layer of gallium nitride based compound semiconductor to N
Evaporates to become n-type, resulting in high resistance. As a result, the resistance of the current non-injection region without the protective film 8 can be increased. The protective film 8 described above is formed by depositing SiO 2 or the like on the entire surface by a CVD method, a sputtering method, or the like and performing only a photolithography process such as exposure, development, or etching of the resist film so that only the surface of the current injection region is exposed. The protective film 8 can be provided only on a necessary portion.

【0030】つぎに保護膜8を除去し、レジスト膜を設
けて塩素ガス雰囲気下で反応性イオンエッチングを行う
ことにより積層された半導体層の一部をエッチングして
高温バッファ層3を露出させ、コンタクト層7上の電流
注入領域表面にAuなどからなるp側電極9およびエッ
チングにより露出した高温バッファ層3の表面にAlな
どからなるn側電極10を設け、ダイシングすることに
より半導体レーザチップがえられる(図1(c)参
照)。
Next, the protective film 8 is removed, a resist film is provided, and reactive ion etching is performed in a chlorine gas atmosphere to etch a part of the stacked semiconductor layers to expose the high temperature buffer layer 3, A p-side electrode 9 made of Au or the like is provided on the surface of the current injection region on the contact layer 7, and an n-side electrode 10 made of Al or the like is provided on the surface of the high temperature buffer layer 3 exposed by etching, and the semiconductor laser chip is obtained by dicing. (See FIG. 1C).

【0031】なお電流の非注入領域の高抵抗化が完全に
なされておれば、電極のパターン化は不要で、コンタク
ト層7の表面全面にp側電極を設けることもできる。
If the resistance of the current non-injection region is completely increased, the electrode patterning is unnecessary and the p-side electrode can be provided on the entire surface of the contact layer 7.

【0032】実施例2 本実施例は、p型層のエピタキシャル成長後またはエピ
タキシャル成長後さらにH2 やNH3 ガスなどHの存在
する雰囲気下で熱処理することにより、p型ドーパント
とHとの結合またはチッ化ガリウム系化合物半導体中の
Nの蒸発を促進させて高抵抗化し、そののち電子注入領
域のみに電子線を照射して活性化することにより、電子
注入領域のみを低抵抗化するものである。図2は半導体
層を積層後電流注入領域のみに電子線を照射するときの
模式図である。
Example 2 In this example, after the epitaxial growth of the p-type layer or after the epitaxial growth, heat treatment is performed in an atmosphere containing H such as H 2 or NH 3 gas to bond or chip the p-type dopant and H. The resistance of only the electron injection region is reduced by accelerating the evaporation of N in the gallium bromide-based compound semiconductor to increase the resistance and then activating the electron injection region by irradiating it with an electron beam. FIG. 2 is a schematic diagram when electron beams are irradiated only on the current injection region after the semiconductor layers are stacked.

【0033】電子線照射装置は、たとえば図3に概念図
を示すように、電子銃31、電子線走査ユニット32、
電子線収束系33などからなる通常の電子線照射装置3
9を用いることができるが、マスク製造用またはウェハ
直接描画用の電子線照射装置を用いることが1μm以下
の精度で照射することができ、電流注入領域のみに正確
にアニール処理をすることができるため好ましい。電子
銃31とサファイア基板を保持している電極とのあいだ
には3〜30kV程度の加速電圧が印加され、電子銃3
1より放射される電子ビーム34の径は、電子線収束系
33に印加される電圧により収束され、積層された化合
物半導体層であるウエハ36の表面で1〜100μm程
度となり、ウエハ36に対して垂直に深さ0.1〜1μ
m程度まで浸透し(加速電圧を高くすることにより浸透
深さをさらに深くすることができる)、局部的に半導体
層が400〜800℃程度に上昇して、MgやZnとH
との結合が切られ、Hが放出されて活性化が行われる。
この電子線の照射によるアニールは局部的に行われるた
め、電流注入領域のみ活性化が行われて低抵抗になり、
電流の非注入領域を高抵抗に維持することができる。
The electron beam irradiation apparatus includes an electron gun 31, an electron beam scanning unit 32, and an electron beam scanning unit 32, as shown in the conceptual diagram of FIG.
Ordinary electron beam irradiation device 3 including an electron beam focusing system 33 and the like
No. 9 can be used, but using an electron beam irradiation device for mask production or wafer direct writing enables irradiation with an accuracy of 1 μm or less, and an annealing process can be accurately performed only in the current injection region. Therefore, it is preferable. An acceleration voltage of about 3 to 30 kV is applied between the electron gun 31 and the electrode holding the sapphire substrate.
The diameter of the electron beam 34 radiated from 1 is converged by the voltage applied to the electron beam converging system 33, and becomes about 1 to 100 μm on the surface of the wafer 36 which is a compound semiconductor layer laminated, Vertical depth 0.1 to 1μ
permeation up to about m (the permeation depth can be further increased by increasing the acceleration voltage), the semiconductor layer locally rises to about 400 to 800 ° C., and Mg, Zn and H
The bond with and is cut, H is released, and activation is performed.
Since this annealing by electron beam irradiation is performed locally, only the current injection region is activated and the resistance becomes low,
The non-injection region of the current can be maintained at a high resistance.

【0034】前記各実施例では、チッ化ガリウム系化合
物半導体として、GaNとAlx Ga1-x NとGay
1-y Nの積層膜の例で説明したが、半導体層としては
前述の組成の材料に限定されず、一般にAlp Gaq
1-p-q N(0≦p<1、0<q≦1、0<p+q≦
1)の一般式からなり、たとえば活性層のバンドギャッ
プエネルギーがクラッド層のバンドギャップエネルギー
より小さくなるように組成の比率が選定されるようp、
qを選定し組成量を変化させたものでもよい。また、前
記Alp Gaq In1-p-q NのNの一部または全部をA
sおよび/またはPなどで置換した材料でも同様に本発
明を適用できる。
In each of the above embodiments, GaN, Al x Ga 1-x N, and Ga y I are used as the gallium nitride-based compound semiconductor.
Although the example of the laminated film of n 1 -y N has been described, the semiconductor layer is not limited to the material having the above-described composition, and is generally Al p Ga q I.
n 1-pq N (0 ≦ p <1, 0 <q ≦ 1, 0 <p + q ≦
1), for example, p is selected so that the composition ratio is selected so that the bandgap energy of the active layer is smaller than the bandgap energy of the cladding layer.
It is also possible to select q and change the composition amount. In addition, a part or all of N of Al p Ga q In 1 -pq N is A
The present invention can be similarly applied to a material substituted with s and / or P or the like.

【0035】[0035]

【発明の効果】本発明の半導体レーザの製法によれば、
所定範囲に保護膜を設けてHの存在する雰囲気下で熱処
理をするだけ、または所定範囲に電子線ビームを照射し
てアニールをするだけで電流注入領域を正確に制御する
ことができるため、簡単な工程で電流注入領域と非注入
領域とを正確に区分したストライプ構造の半導体レーザ
をうることができる。その結果、もれ電流が少なく発光
効率の高い半導体レーザを安価にうることができる。
According to the method of manufacturing the semiconductor laser of the present invention,
The current injection region can be accurately controlled by simply providing a protective film in a predetermined range and performing heat treatment in an atmosphere containing H, or by irradiating a predetermined range with an electron beam and annealing. A semiconductor laser having a stripe structure in which a current injection region and a non-injection region are accurately divided can be obtained by various processes. As a result, a semiconductor laser having a small leakage current and a high luminous efficiency can be obtained at low cost.

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

【図1】本発明の半導体レーザの製法の実施例1の工程
断面説明図である。
FIG. 1 is a process cross-sectional explanatory view of a first embodiment of a method for manufacturing a semiconductor laser of the present invention.

【図2】本発明の半導体レーザの製法の実施例2の電子
線照射を示す模式的説明図である。
FIG. 2 is a schematic explanatory view showing electron beam irradiation in Example 2 of the method for producing a semiconductor laser of the present invention.

【図3】電子線照射装置の一例の概略説明図である。FIG. 3 is a schematic explanatory view of an example of an electron beam irradiation device.

【図4】従来の半導体レーザの電流注入領域を制御する
構造の例を示す断面説明図である。
FIG. 4 is a sectional explanatory view showing an example of a structure for controlling a current injection region of a conventional semiconductor laser.

【符号の説明】[Explanation of symbols]

1 基板 3 高温バッファ層 4 n型クラッド層 5 活性層 6 p型クラッド層 7 コンタクト層 8 保護膜 11 電子線 1 substrate 3 high temperature buffer layer 4 n-type clad layer 5 active layer 6 p-type clad layer 7 contact layer 8 protective film 11 electron beam

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 (a)基板上に少なくともn型層、活性
層およびp型層を含み、半導体レーザを構成するチッ化
ガリウム系化合物半導体を積層し、(b)該積層された
半導体層の電流注入領域におけるp型層を活性化し、
(c)前記積層された半導体層の電流注入領域以外の領
域におけるp型層を不活性化状態に維持することを特徴
とする半導体レーザの製法。
1. A laminate of (a) a gallium nitride based compound semiconductor, which comprises at least an n-type layer, an active layer and a p-type layer, and which constitutes a semiconductor laser, on a substrate, and (b) the laminated semiconductor layers. Activate the p-type layer in the current injection region,
(C) A method of manufacturing a semiconductor laser, characterized in that the p-type layer in a region other than the current injection region of the stacked semiconductor layers is maintained in an inactivated state.
【請求項2】 前記積層された半導体層がn型バッファ
層、n型クラッド層、活性層、p型クラッド層およびp
型コンタクト層である請求項1記載の半導体レーザの製
法。
2. The laminated semiconductor layers are an n-type buffer layer, an n-type cladding layer, an active layer, a p-type cladding layer and a p-type cladding layer.
The method for producing a semiconductor laser according to claim 1, wherein the method is a contact layer.
【請求項3】 前記半導体層の積層後基板全体の熱処理
を行うことによりp型層の活性化を行い、ついで前記電
流注入領域の表面に保護膜を設けて水素を含む雰囲気中
で熱処理を行うことにより前記電流注入領域以外の領域
を不活性化状態にする請求項1または2記載の半導体レ
ーザの製法。
3. The p-type layer is activated by heat-treating the entire substrate after the semiconductor layers are laminated, and then a protective film is provided on the surface of the current injection region and heat-treated in an atmosphere containing hydrogen. 3. The method for producing a semiconductor laser according to claim 1, wherein the regions other than the current injection region are thereby inactivated.
【請求項4】 前記p型層の活性化のため熱処理をチッ
素雰囲気中、400〜800℃で行う請求項3記載の半
導体レーザの製法。
4. The method for manufacturing a semiconductor laser according to claim 3, wherein the heat treatment for activating the p-type layer is performed at 400 to 800 ° C. in a nitrogen atmosphere.
【請求項5】 前記半導体層の積層後前記電流注入領域
のみに電子線を照射し、前記p型層の該電流注入領域の
みを活性化する請求項1または2記載の半導体レーザの
製法。
5. The method of manufacturing a semiconductor laser according to claim 1, wherein after the semiconductor layers are stacked, only the current injection region is irradiated with an electron beam to activate only the current injection region of the p-type layer.
JP22202094A 1994-09-16 1994-09-16 Production of semiconductor laser Pending JPH0888432A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP22202094A JPH0888432A (en) 1994-09-16 1994-09-16 Production of semiconductor laser
US08/892,273 US5974069A (en) 1994-09-16 1997-07-14 Semiconductor laser and manufacturing method thereof
US09/392,456 US6298079B1 (en) 1994-09-16 1999-09-09 Gallium nitride type laser for emitting blue light
US09/392,459 US6274891B1 (en) 1994-09-16 1999-09-09 Semiconductor laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22202094A JPH0888432A (en) 1994-09-16 1994-09-16 Production of semiconductor laser

Publications (1)

Publication Number Publication Date
JPH0888432A true JPH0888432A (en) 1996-04-02

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Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0929109A1 (en) * 1998-01-08 1999-07-14 Pioneer Electronic Corporation Method for manufacturing a semiconductor light emitting device
JP2000323751A (en) * 1999-05-10 2000-11-24 Pioneer Electronic Corp Method for manufacturing group III nitride semiconductor device
US6524882B2 (en) 2000-04-04 2003-02-25 Sony Corporation Method of producing p-type nitride based III-V compound semiconductor and method of fabricating semiconductor device using the same
JP2007305744A (en) * 2006-05-10 2007-11-22 Sumitomo Electric Ind Ltd Integrated semiconductor optical device and manufacturing method thereof
DE112005001337B4 (en) 2004-06-10 2010-07-01 Toyoda Gosei Co., Ltd., Nishikasugai-gun Process for producing a FET
JPWO2015129610A1 (en) * 2014-02-26 2017-03-30 学校法人 名城大学 Manufacturing method of npn type nitride semiconductor light emitting device and npn type nitride semiconductor light emitting device

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0929109A1 (en) * 1998-01-08 1999-07-14 Pioneer Electronic Corporation Method for manufacturing a semiconductor light emitting device
JP2000323751A (en) * 1999-05-10 2000-11-24 Pioneer Electronic Corp Method for manufacturing group III nitride semiconductor device
US6524882B2 (en) 2000-04-04 2003-02-25 Sony Corporation Method of producing p-type nitride based III-V compound semiconductor and method of fabricating semiconductor device using the same
DE112005001337B4 (en) 2004-06-10 2010-07-01 Toyoda Gosei Co., Ltd., Nishikasugai-gun Process for producing a FET
US7981744B2 (en) 2004-06-10 2011-07-19 Toyoda Gosei Co., Ltd. Field-effect transistor, semiconductor device, a method for manufacturing them, and a method of semiconductor crystal growth
JP2007305744A (en) * 2006-05-10 2007-11-22 Sumitomo Electric Ind Ltd Integrated semiconductor optical device and manufacturing method thereof
JPWO2015129610A1 (en) * 2014-02-26 2017-03-30 学校法人 名城大学 Manufacturing method of npn type nitride semiconductor light emitting device and npn type nitride semiconductor light emitting device

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