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JPS6118189A - Semiconductor laser array device and manufacture thereof - Google Patents

Semiconductor laser array device and manufacture thereof

Info

Publication number
JPS6118189A
JPS6118189A JP13793084A JP13793084A JPS6118189A JP S6118189 A JPS6118189 A JP S6118189A JP 13793084 A JP13793084 A JP 13793084A JP 13793084 A JP13793084 A JP 13793084A JP S6118189 A JPS6118189 A JP S6118189A
Authority
JP
Japan
Prior art keywords
laser array
layer
array device
thin film
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.)
Pending
Application number
JP13793084A
Other languages
Japanese (ja)
Inventor
Akio Yoshikawa
昭男 吉川
Takashi Sugino
隆 杉野
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP13793084A priority Critical patent/JPS6118189A/en
Publication of JPS6118189A publication Critical patent/JPS6118189A/en
Pending legal-status Critical Current

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  • Semiconductor Lasers (AREA)

Abstract

PURPOSE:To enable realization of a semiconductor laser array device which operates at a low threshold and is fabricated with a high degree of integration in a single crystal growth, by forming an active layer directly above recesses or projections so that the dimensions of the active layer in directions which are respectively parallel to the cavity resonator surface and the semiconductor junction surface are sufficient to provide two oscillation regions. CONSTITUTION:Stripe-shaped grooves are formed in the surface of a p type GaAs substrate 10 by chemical etching. Then, n type GaAs current blocking layers 11, 20 whose film thickness is smaller than the depth of the grooves are formed. A p type GaAs layer 12, a p type clad layer 13, an active layer 14, an n type clad layer 15 and an n type layer 16 are formed on the layers 11, 20. Although current concentrates on and near the part above each groove, as the current comes closer to the GaAs substrate 10, it diverges and flows along both side surfaces of the groove, thereby forming two laser oscillation regions within the groove. Thus, oscillations take place substantially simultaneously at or near a threshold of 70mA, and stable single transverse mode oscillation is obtained. The volume of each chip of this laser array is reduced to about half of that in a conventional laser array having the same number of laser oscillation regions. Thus, it is possible to reduce the size of the laser array device.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、コヒーレント光源として、或いは高出力、高
密度、高輝度光源として、各種電子機器。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention is applicable to various electronic devices as a coherent light source or as a high output, high density, high brightness light source.

光学機器に用いられる半導体レーザアレイ装置に関する
ものである。
The present invention relates to a semiconductor laser array device used in optical equipment.

(従来例の構成とその問題点) 半導体レーザアレイ装置の重要な用途の1つに高出力高
集積光源がある。すなわち、1チツプ内に多数のレーザ
発振領域を持ち、そのそれぞれが互いに近接し、レーザ
光の発振波長、位相等の特性が揃っている必要がある。
(Conventional Structure and its Problems) One of the important uses of semiconductor laser array devices is as a high-output, highly integrated light source. That is, it is necessary to have a large number of laser oscillation regions within one chip, each of which is close to each other, and whose characteristics such as the oscillation wavelength and phase of laser light are uniform.

従来の液相エビタキミャル成長法によシ作製したレーザ
アレイ装置では、基板に1つくシつけのストライプや、
成長エビ層上でのZn拡散やプロトン照射、絶縁膜によ
るストライプを用いるため、゛単位レーザ発振領域の占
めるチップ面積が比較的大きくなシ、多数の発振領域を
適当な大きさのチップに集積するとき、集積度は低い。
Laser array devices fabricated using the conventional liquid phase epitaxial growth method have a single stripe on the substrate,
Since Zn diffusion on the growth layer, proton irradiation, and stripes made of an insulating film are used, the chip area occupied by a unit laser oscillation area is relatively large, and many oscillation areas can be integrated into an appropriately sized chip. When, the degree of integration is low.

まだ、液相エピタキシャル成長法を用いるため、レーザ
光の発振波長のバラツキ等特性のバラツキも大きい。
However, since the liquid phase epitaxial growth method is used, there are large variations in characteristics such as variations in the oscillation wavelength of laser light.

(発明の目的) 本発明は上記欠点に鑑み、レーデ光の発振波長のバラツ
キなどの特性のバラツキが少なく、チップ上にレーザ発
振領域を比較的大きな集積度で集積可能な構造を有する
半導体レーザアレイ装置と、前記半導体レーザアレイ装
置を1回の結晶成長で実現可能な製造方法とを提供する
ものである。
(Object of the Invention) In view of the above-mentioned drawbacks, the present invention provides a semiconductor laser array having a structure that has little variation in characteristics such as variation in the oscillation wavelength of LED light and that allows laser oscillation regions to be integrated on a chip with a relatively large degree of integration. The present invention provides a device and a manufacturing method that can realize the semiconductor laser array device with one crystal growth.

(発明の構成) この目的を達成するために本発明の半導体レーザアレイ
装置は、凹部又は凸部を有する導電性基板上に、前記凹
部又は凸部の高さよりも小さい膜厚で、前記基板とは逆
の導電型を示す薄膜層を持ち、加えて前記薄膜層上に二
重ヘテロ構造を含む多層薄膜を有する。しかも基板上の
凹部又は凸部直上の活性層の共振器面及び半導体接合面
に平行な方向の長さが、2つの発振領域を持つのに十分
な長さで構成される。以上の構成は、1回の結晶成長で
行なわれ、この構成により、特性のバラツキが少なく、
レーデ発振領域を比較的大きな集積度で集積化すること
を可能とする。
(Structure of the Invention) To achieve this object, the semiconductor laser array device of the present invention is provided by forming a film on a conductive substrate having a concave portion or a convex portion with a film thickness smaller than the height of the concave portion or the convex portion. has thin film layers exhibiting opposite conductivity types and additionally has a multilayer thin film containing a double heterostructure on said thin film layers. Moreover, the length of the active layer directly above the recess or projection on the substrate in the direction parallel to the resonator surface and the semiconductor junction surface is sufficient to have two oscillation regions. The above structure is achieved by one-time crystal growth, and with this structure, there is little variation in characteristics.
It is possible to integrate the Rade oscillation region with a relatively large degree of integration.

(実施例の説明) 本発明の半導体レーデアレイ装置について、一実施例を
用いて具体的に説明する。
(Description of Embodiment) The semiconductor radar array device of the present invention will be specifically described using one embodiment.

−例として、導電性基板にp型GaAs基板を用いる。- As an example, a p-type GaAs substrate is used as the conductive substrate.

第1図は本発明の第一の実施例を示す。p型GaAs基
板(キャリア濃度二〜1018i3程度)10の(10
0)面上に、<110)方向に化学エツチングにより、
逆メサ状にストライプ状の溝(凹)を形成する。なお、
溝の深さは1.5μm1溝の幅は10μmとした。次に
有機金属気相エピタキシャル(キャリア濃度:1×10
1−−3程度)を1μmの厚さで形成する。この時、上
記n mGaAs層は、第1図11及び20に示す部分
にしか成長しない。その後、上記n 型GaAs層11
及び2o上に、GaAs基板lOと同じ程度のキャリア
濃度を持つp型GaAs層12.p型Ga1xAZxA
 aクラ22層13゜Ga1−yASAs活性層14(
0≦y < x ) p n型G al xAAx A
 sクラッド層15.n型GaAs層16を形成する。
FIG. 1 shows a first embodiment of the invention. p-type GaAs substrate (carrier concentration about 2 to 1018i3) of 10 (10
0) surface, by chemical etching in the <110) direction,
Form striped grooves (concavities) in an inverted mesa shape. In addition,
The depth of the groove was 1.5 μm and the width of each groove was 10 μm. Next, organometallic vapor phase epitaxial (carrier concentration: 1 × 10
1 to 3) with a thickness of 1 μm. At this time, the nm GaAs layer grows only in the portions shown in FIGS. 11 and 20. After that, the n-type GaAs layer 11
and 2o, a p-type GaAs layer 12 . p-type Ga1xAZxA
a-class 22 layer 13°Ga1-yASAs active layer 14 (
0≦y<x) p n-type Gal xAAx A
s cladding layer 15. An n-type GaAs layer 16 is formed.

MOCVD法による結晶成長条件の一例を以下に示す。An example of crystal growth conditions by the MOCVD method is shown below.

成長速度2μm/時、成長温度770℃。Growth rate: 2 μm/hour, growth temperature: 770°C.

全ガス流量51/分、■族元素に対するV族元素のモル
比40である。
The total gas flow rate was 51/min, and the molar ratio of Group V elements to Group II elements was 40.

この構造に電極を作製して電流を流すと、電流は溝形成
部の上部付近に集中するが、GaAs基板1゜に近づく
につれ、溝の両側面に分岐して流れる。
When an electrode is made in this structure and a current is passed through it, the current is concentrated near the top of the groove forming part, but as it approaches 1° of the GaAs substrate, it branches and flows to both sides of the groove.

その結果、溝の内部で、2つのレーザ発振領域が形成さ
れた。このとき、2つのレーザ発振領域では、70.m
kのしきい値付近でほぼ同時に発振が起こシ、それぞれ
、安定な単−横モード発振が得られた。
As a result, two laser oscillation regions were formed inside the groove. At this time, in the two laser oscillation regions, 70. m
Oscillations occurred almost simultaneously near the threshold value of k, and stable single-transverse mode oscillations were obtained in each case.

通常のレーザアレイ装置では、1つの溝では、溝内での
電流の流し方が本発−明と異なシ、1つのレーザ発振領
域しか得られず、これが基本単位となってレーザアレイ
を構成するが、本発明の場合は、1つの溝で2つのレー
ザ発振領域を持つので、同数のレーザ発振領域を持つレ
ーザアレイを作製すると、チップは約半分の体積となり
、小型化が可能である。
In a normal laser array device, only one laser oscillation region can be obtained with one groove, since the method of flowing current in the groove is different from that of the present invention, and this serves as the basic unit to configure the laser array. However, in the case of the present invention, one groove has two laser oscillation regions, so if a laser array with the same number of laser oscillation regions is manufactured, the chip will have about half the volume, allowing for miniaturization.

第2実施例として、第2図の様に、導電性基板上に凸部
を形成して、同様に半導体レーザアレイ装置を作製した
ところ、上記第1実施例と同様の結果が得られた。
As a second example, a semiconductor laser array device was similarly fabricated by forming a convex portion on a conductive substrate as shown in FIG. 2, and the same results as in the first example were obtained.

なお、凹部(溝)の幅および凸部の幅は8μm以上で2
つのレーデ発振領域を実現できレーザ発振領域を4箇所
以上取シたい場合は、上記第1実施例と第2実施例を基
本単位として組み合わせればよい。
Note that the width of the recess (groove) and the width of the protrusion are 8 μm or more and 2
If four or more laser oscillation regions can be realized and four or more laser oscillation regions are desired, the first embodiment and the second embodiment described above may be combined as a basic unit.

なお、本実施例では、GaAs系+ GaAtAa系半
導体レーザについて述べたが、InP系や他の多元混晶
系を含む化合物半導体を材料とする半導体レーザアレイ
装置についても、本発明を同様に適用することが可能で
おる。さらに、導電性基板にn型基材を用いても、結晶
成長を行なうのに、他の物質供給律速の結晶成長方法、
たとえば、分子線エピタキシャル成長法を用いてもよい
Although this embodiment describes a GaAs + GaAtAa semiconductor laser, the present invention is also applicable to semiconductor laser array devices made of compound semiconductors including InP and other multi-component mixed crystal systems. It is possible. Furthermore, even if an n-type base material is used as the conductive substrate, other material supply rate-limiting crystal growth methods,
For example, molecular beam epitaxial growth may be used.

(発明の効果) 本発明の半導体レーザアレイ装置は、低しきい値動作で
、単−横モード発振する半導体レーザアレイ装置を高集
積化したものを1回の結晶成長で実現できる構造を有す
るものであシ、その実用的効果は著しい。
(Effects of the Invention) The semiconductor laser array device of the present invention has a structure that allows a highly integrated semiconductor laser array device that operates at a low threshold and oscillates in a single transverse mode to be realized by one crystal growth. Yes, its practical effects are remarkable.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、本発明+1”IJ11+1実施例の半導体レ
ーザアレイ装置の断面図、第2図は、第2実施例の断面
図、である。 10−p型GaAs基板、11− n型GaAs電流阻
止層、12・・・p型GaAsバッファ層、13・・・
p型GaAAAsクラッド層、14− GaAtAs活
性層、15”’n型GaAtAsクラッド層、16− 
n型GaAs層、’     20− n型GaAs電 流阻止層、21・・・オーミック電極、22・・・絶縁
膜。 第1図
FIG. 1 is a sectional view of a semiconductor laser array device according to a +1"IJ11+1 embodiment of the present invention, and FIG. 2 is a sectional view of a second embodiment. 10-p-type GaAs substrate, 11-n-type GaAs current Blocking layer, 12...p-type GaAs buffer layer, 13...
p-type GaAAAs cladding layer, 14- GaAtAs active layer, 15'''n-type GaAtAs cladding layer, 16-
n-type GaAs layer, '20- n-type GaAs current blocking layer, 21... Ohmic electrode, 22... Insulating film. Figure 1

Claims (2)

【特許請求の範囲】[Claims] (1)凹部又は凸部を有する導電性基板上に、前記凹部
又は凸部の高さよりも小さい膜厚で、前記基板とは逆の
導電型を示す薄膜層が形成され、さらに前記薄膜層上に
二重ヘテロ構造を含む多層薄膜が形成され、しかも前記
基板上の凹部又は凸部直上の活性層の共振器面及び半導
体接合面に平行な方向の長さが、2つの発振領域を持つ
のに十分な長さであることを特徴とする半導体レーザア
レイ装置
(1) A thin film layer having a thickness smaller than the height of the recesses or projections and having a conductivity type opposite to that of the substrate is formed on a conductive substrate having recesses or projections, and further on the thin film layer. A multilayer thin film including a double heterostructure is formed on the substrate, and the length of the active layer directly above the recess or protrusion on the substrate in the direction parallel to the resonator surface and the semiconductor junction surface has two oscillation regions. A semiconductor laser array device characterized by having a length sufficient for
(2)有機金属気相エピタキシャル成長方法又は分子線
エピタキシャル成長方法を用いて、凹部又は凸部を有す
る導電性基板上に、前記凹部又は凸部の高さよりも小さ
い膜厚で前記基板とは逆の導電型を示す薄膜層を形成し
、その後、前記薄膜層上に二重ヘテロ構造を含む多層薄
膜を形成することを特徴とする半導体レーザアレイ装置
の製造方法。
(2) Using a metal organic vapor phase epitaxial growth method or a molecular beam epitaxial growth method, a conductive substrate having a concave portion or a convex portion is coated with a film having a thickness smaller than the height of the concave portion or convex portion and having a conductivity opposite to that of the substrate. 1. A method for manufacturing a semiconductor laser array device, comprising forming a thin film layer showing a pattern, and then forming a multilayer thin film including a double heterostructure on the thin film layer.
JP13793084A 1984-07-05 1984-07-05 Semiconductor laser array device and manufacture thereof Pending JPS6118189A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13793084A JPS6118189A (en) 1984-07-05 1984-07-05 Semiconductor laser array device and manufacture thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13793084A JPS6118189A (en) 1984-07-05 1984-07-05 Semiconductor laser array device and manufacture thereof

Publications (1)

Publication Number Publication Date
JPS6118189A true JPS6118189A (en) 1986-01-27

Family

ID=15210006

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13793084A Pending JPS6118189A (en) 1984-07-05 1984-07-05 Semiconductor laser array device and manufacture thereof

Country Status (1)

Country Link
JP (1) JPS6118189A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6373685A (en) * 1986-09-17 1988-04-04 Mitsubishi Electric Corp Semiconductor laser array and manufacture thereof
US5031183A (en) * 1990-03-05 1991-07-09 Mcdonnell Douglas Corporation Full aperture semiconductor laser
US5291033A (en) * 1991-05-29 1994-03-01 Eastman Kodak Company Semiconductor light-emitting device having substantially planar surfaces

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57162382A (en) * 1981-03-30 1982-10-06 Sumitomo Electric Ind Ltd Semiconductor laser
JPS5843590A (en) * 1981-09-08 1983-03-14 Sumitomo Electric Ind Ltd Semiconductor laser

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57162382A (en) * 1981-03-30 1982-10-06 Sumitomo Electric Ind Ltd Semiconductor laser
JPS5843590A (en) * 1981-09-08 1983-03-14 Sumitomo Electric Ind Ltd Semiconductor laser

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6373685A (en) * 1986-09-17 1988-04-04 Mitsubishi Electric Corp Semiconductor laser array and manufacture thereof
US5031183A (en) * 1990-03-05 1991-07-09 Mcdonnell Douglas Corporation Full aperture semiconductor laser
US5291033A (en) * 1991-05-29 1994-03-01 Eastman Kodak Company Semiconductor light-emitting device having substantially planar surfaces

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