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JPH0576794B2 - - Google Patents
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JPH0576794B2 - - Google Patents

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Publication number
JPH0576794B2
JPH0576794B2 JP59019602A JP1960284A JPH0576794B2 JP H0576794 B2 JPH0576794 B2 JP H0576794B2 JP 59019602 A JP59019602 A JP 59019602A JP 1960284 A JP1960284 A JP 1960284A JP H0576794 B2 JPH0576794 B2 JP H0576794B2
Authority
JP
Japan
Prior art keywords
layer
type
active layer
semiconductor
thickness
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 - Lifetime
Application number
JP59019602A
Other languages
Japanese (ja)
Other versions
JPS60164379A (en
Inventor
Mitsunori Sugimoto
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.)
NEC Corp
Original Assignee
Nippon Electric 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP1960284A priority Critical patent/JPS60164379A/en
Publication of JPS60164379A publication Critical patent/JPS60164379A/en
Publication of JPH0576794B2 publication Critical patent/JPH0576794B2/ja
Granted 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
    • 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
    • H01S5/20Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers
    • H01S5/2004Confining in the direction perpendicular to the layer structure
    • 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

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Semiconductor Lasers (AREA)

Description

【発明の詳細な説明】 本発明は半導体レーザー特に単一量子井戸構造
半導体レーザーの改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in semiconductor lasers, particularly single quantum well structure semiconductor lasers.

従来例として、AlGaAs/GaAs単一量子井戸
構造半導体レーザーの主要部のエネルギーバンド
図を第1図aに原子配置の模式図を第1図bに示
す。図中、1はn−Alx1Ga1-x1As(x1≠0)から
なるn型キヤリア閉じ込め層、2はGaAsからな
る活性層、3はP−Alx2Ga1-x2As(x2≠0)から
なるP型キヤリア閉じ込め層である。第1図bに
おいて斜線を施した丸はAl原子、斜線のない白
丸はGa原子を表わしている。又、As原子は紙面
に対して垂直方向にずれたところに位置し、ここ
には示していない。図中、AlGaAsのAl濃度は約
0.3の場合である。この図に示される様にAl原子
はかなりクラスター状にかたまつて配置してい
る。このためb図中央の活性層2のGaAsの厚さ
は本来9原子層であるべきところが、10原子層や
11原子層となつている箇所もあることがわかる。
したがつてこの様なAlとGaの混晶のキヤリア閉
じ込め層を用いた量子井戸構造を形成する場合に
は量子井戸層の厚さは必然的に1〜2原子層の厚
さの不均一が膜面内に存在してしまうことにな
る。この様な不均一性は量子化レベルの不均一を
伴うため半導体レーザの利得スペクトルの広がり
を引き起こし閾値電流の増大を招いていた。
As a conventional example, an energy band diagram of the main parts of an AlGaAs/GaAs single quantum well structure semiconductor laser is shown in FIG. 1a, and a schematic diagram of the atomic arrangement is shown in FIG. 1b. In the figure, 1 is an n-type carrier confinement layer made of n-Alx 1 Ga 1-x1 As (x 1 ≠ 0), 2 is an active layer made of GaAs, and 3 is P-Alx 2 Ga 1-x2 As (x 2 ≠0). In FIG. 1b, hatched circles represent Al atoms, and white circles without hatching represent Ga atoms. Furthermore, the As atom is located at a position perpendicular to the plane of the paper and is not shown here. In the figure, the Al concentration of AlGaAs is approximately
This is the case of 0.3. As shown in this figure, the Al atoms are arranged in clusters. Therefore, the thickness of GaAs in the active layer 2 in the center of figure b should originally be 9 atomic layers, but it is 10 atomic layers.
It can be seen that in some places there are 11 atomic layers.
Therefore, when forming a quantum well structure using a carrier confinement layer of such a mixed crystal of Al and Ga, the thickness of the quantum well layer inevitably has a non-uniform thickness of 1 to 2 atomic layers. It ends up existing within the membrane plane. Such non-uniformity is accompanied by non-uniformity in quantization levels, which causes a broadening of the gain spectrum of the semiconductor laser and an increase in threshold current.

本発明の目的は、量子井戸層の膜面内不均一が
無くしたがつて利得スペクトルが狭く、低閾値の
半導体レーザを提供することにある。
An object of the present invention is to provide a semiconductor laser that eliminates in-plane non-uniformity in a quantum well layer, has a narrow gain spectrum, and has a low threshold.

本発明の半導体レーザーは、活性層と、この活
性層を上下にはさみ前記活性層に比し大きな禁制
帯幅を有し2つの元素からなる化合物半導体から
なる第1及び第2半導体層とこの第1及び第2半
導体層と前記活性層からなる3層構造を上下には
さみ前記活性層に比し大きな禁制帯幅を有し、少
なくとも3つ以上の元素からなる化合物半導体か
らなる第3及び第4半導体層とを備え、前記第1
及び第2半導体層の厚みが、それぞれ電子及び正
孔が量子力学的トンネル現象によつて通過できる
程度の厚さになつている。
The semiconductor laser of the present invention includes an active layer, first and second semiconductor layers sandwiching the active layer above and below and made of a compound semiconductor made of two elements and having a larger forbidden band width than the active layer; Third and fourth semiconductor layers sandwiching a three-layer structure consisting of the first and second semiconductor layers and the active layer above and below, having a larger forbidden band width than the active layer, and made of a compound semiconductor made of at least three or more elements. a semiconductor layer;
The thicknesses of the second semiconductor layer and the second semiconductor layer are such that electrons and holes can pass therethrough by quantum mechanical tunneling.

次に図面を参照して本発明を詳細に説明する。 Next, the present invention will be explained in detail with reference to the drawings.

本発明の一実施例の断面図を第2図に示す。図
中、6はn−GaAs基板、7はバツフアー層(n
−GaAs)、8はn型クラツド層(n−
Alx8Ga1-x8As、0.2≦x8≦0.8、厚さ0.5〜3μm)
1はn型キヤリア閉じ込め層(n−Alx1Ga1-x1
As、0.1≦x1≦0.4、x1<x8、厚さ0.05〜0.3μm)、
4はn型AlAs層(厚さ≦20Å)、2は活性層
(nondope GaAs、厚さ≦200Å)、5はP型AlAs
層(厚さ≦20Å)、3はP型キヤリア閉じ込め層
(P−Alx3Ga1-x3As、0.1≦x3≦0.4、厚さ0.05〜
0.3μm)、9はP型クラツド層(P−Alx9Ga1-x9
As、x9>x8、0.2≦x9≦0.8、厚さ0.5〜3μm)、1
0はキヤツプ層(P+−GaAs)、11はSiO2膜、
12はP型電極、13はn型電極、14は電極窓
である。尚、この例ではn型キヤリア閉じ込め層
1が第3半導体層に、n型AlAs層4が第1半導
体層に、P型AlAs層5が第2半導体層に、P型
キヤリア閉じ込め層3が第4半導体層に相当す
る。本実施例では、n型キヤリア閉じ込め層1及
びP型キヤリア閉じ込め層3は光ガイド層として
働くため、光とキヤリアを別々の層で閉じ込める
いわゆるSCH(Separate Confinement
Heterostvucture)構造となつている。本実施例
の活性層近傍のエネルギーバンド図を第3図a
に、原子配置の模式図を第3図bに示す。従来例
と異なる点は、n型AlAs層4及びP型AlAs層5
を備えている点である。第3図bでは第1図bと
同様に斜線丸がAl原子、白丸がGa原子を示して
いる。第3図bで示される様に、n型AlAs層4
及びP型AlAs層5が活性層2を上下にはさんで
いるため活性層2の厚さは膜面内均一に9原子層
となつていることがわかる。したがつて、活性層
2の厚みが均一なため量子化レベルが膜面内で均
一となり利得スペクトルが狭く、低閾値電流発振
が可能となる。又n型AlAs層4及びP型AlAs層
5の厚さが第3図bでは2原子層と薄いため、こ
れらの層をトンネルによつて電子及び正孔が通過
し、活性層2に有効に注入出来る。
A cross-sectional view of one embodiment of the present invention is shown in FIG. In the figure, 6 is an n-GaAs substrate, 7 is a buffer layer (n
-GaAs), 8 is an n-type cladding layer (n-
Alx 8 Ga 1-x8 As, 0.2≦ x8 ≦0.8, thickness 0.5-3μm)
1 is an n-type carrier confinement layer (n-Alx 1 Ga 1-x1
As, 0.1≦ x1 ≦0.4, x1 < x8 , thickness 0.05-0.3μm),
4 is n-type AlAs layer (thickness ≦20 Å), 2 is active layer (nondope GaAs, thickness ≦200 Å), 5 is P-type AlAs
layer (thickness ≦20 Å), 3 is a P-type carrier confinement layer (P-Alx 3 Ga 1-x3 As, 0.1≦x 3 ≦0.4, thickness 0.05~
0.3 μm), 9 is a P-type cladding layer (P-Alx 9 Ga 1-x9
As, x 9 > x 8 , 0.2≦x 9 ≦0.8, thickness 0.5 to 3 μm), 1
0 is the cap layer (P + -GaAs), 11 is the SiO 2 film,
12 is a P-type electrode, 13 is an N-type electrode, and 14 is an electrode window. In this example, the n-type carrier confinement layer 1 is the third semiconductor layer, the n-type AlAs layer 4 is the first semiconductor layer, the P-type AlAs layer 5 is the second semiconductor layer, and the P-type carrier confinement layer 3 is the third semiconductor layer. This corresponds to 4 semiconductor layers. In this embodiment, since the n-type carrier confinement layer 1 and the P-type carrier confinement layer 3 work as light guide layers, so-called SCH (Separate Confinement) that confines light and carriers in separate layers is used.
Heterostuvucture) structure. Figure 3a shows the energy band diagram near the active layer of this example.
A schematic diagram of the atomic arrangement is shown in FIG. 3b. The difference from the conventional example is that the n-type AlAs layer 4 and the p-type AlAs layer 5
The point is that it has the following. In FIG. 3b, as in FIG. 1b, diagonal circles indicate Al atoms, and open circles indicate Ga atoms. As shown in Figure 3b, the n-type AlAs layer 4
It can be seen that since the active layer 2 is sandwiched between the P-type AlAs layer 5 and the active layer 2 above and below, the thickness of the active layer 2 is 9 atomic layers uniformly within the film surface. Therefore, since the thickness of the active layer 2 is uniform, the quantization level is uniform within the film plane, the gain spectrum is narrow, and low threshold current oscillation is possible. In addition, since the thickness of the n-type AlAs layer 4 and the p-type AlAs layer 5 is as thin as two atomic layers in FIG. Can be injected.

次に本実施例の製造方法について説明する。ま
ず最初にn−GaAs基板6上にバツフアー層7、
n型クラツド層8、n型キヤリア閉じ込め層1、
n型AlAs層4、活性層2、P型AlAs層5、P型
キヤリア閉じ込め層3、P型クラツド層9、キヤ
ツプ層10を順次結晶成長する。結晶成長方法は
MBE法、MO−CVD法VPE法等々のいずれの方
法を用いても良い。次にSiO2膜11を形成し、
フオトエツチング法により電極窓14を形成す
る。次にP型電極12及びn型電極13を形成し
オーミツクコンタクトをとる。最後にウエハーか
ら劈開等を用いてペレツトに切出した後ステム等
に融着し電極ワイヤを取付けて完成する。
Next, the manufacturing method of this example will be explained. First, a buffer layer 7 is placed on an n-GaAs substrate 6,
n-type cladding layer 8, n-type carrier confinement layer 1,
An n-type AlAs layer 4, an active layer 2, a p-type AlAs layer 5, a p-type carrier confinement layer 3, a p-type cladding layer 9, and a cap layer 10 are successively crystal-grown. The crystal growth method is
Any method such as MBE method, MO-CVD method, VPE method, etc. may be used. Next, a SiO 2 film 11 is formed,
Electrode windows 14 are formed by photoetching. Next, a P-type electrode 12 and an N-type electrode 13 are formed to establish ohmic contact. Finally, the wafer is cut into pellets using cleavage or the like, then fused to a stem or the like, and electrode wires are attached to complete the pellets.

本実施例においては、SCH構造を用いたが、
これに限らず、例えばGRIN−SCH(Graded−
Index Waveguide Separate−Confinement−
Hetevosructure)構造等を用いても本発明が適
用出来ることは明らかである。又、本実施例では
電極狭窄構造としてSiO2膜ストライプ構造とし
たが、これに限らずプレーナストライプ構造、リ
ツヂ・ウエイブガイド(Ridge Wave guide)構
造、埋め込み構造等いずれの電流狭窄構造を用い
ても本発明が適用出来る。又本実施例では、活性
層にGaAsを用いたが、AlGaAsを用いても効果
が期待される。又、本実施例ではn−GaAs基板
を用いたがこれに限らずP−GaAs基板を用い
て、本実施例の導電型をすべて反対にしても良い
ことは明らかである。又、本実施例ではn側では
n型AlAs層をP側ではP型AlAs層を備えていた
がこれに限らず、AlAsはノンドープあるいは反
対導電型であつても本発明の効果が期待出来る。
又、本実施例ではAlGaAs/GaAs系を材料に用
いていたがこれに限らずAlGaSb/GaSb系等他
の材料を用いても本発明を適用出来ることは明ら
かである。
In this example, the SCH structure was used, but
Not limited to this, for example, GRIN-SCH (Graded-
Index Waveguide Separate−Confinement−
It is clear that the present invention can also be applied to other structures such as Hetevostructure. In addition, in this example, the SiO 2 film stripe structure was used as the electrode confinement structure, but the current confinement structure is not limited to this, and any current confinement structure such as a planar stripe structure, a ridge wave guide structure, or a buried structure can be used. The present invention can be applied. Further, in this embodiment, GaAs was used for the active layer, but the effect is expected to be obtained even if AlGaAs is used. Further, although an n-GaAs substrate is used in this embodiment, it is obvious that the present invention is not limited to this, and a P-GaAs substrate may be used, with all the conductivity types of this embodiment being reversed. Further, in this embodiment, an n-type AlAs layer is provided on the n-side and a p-type AlAs layer is provided on the p-side, but the present invention is not limited to this, and the effects of the present invention can be expected even if the AlAs is non-doped or of the opposite conductivity type.
Furthermore, although AlGaAs/GaAs-based materials are used in this embodiment, it is clear that the present invention can be applied to other materials such as AlGaSb/GaSb-based materials.

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

第1図aは従来例のAlGaAs/GaAs単一量子
井戸構造半導体レーザーの主要部のエネルギーバ
ンド図、第1図bはその原子配置の模式図であ
る。第2図は本発明の一実施例の断面図である。
第3図aは本発明の一実施例の活性層近傍のエネ
ルギーバンド図、第3図bはその原子配置の模式
図である。 図中、1はn型キヤリア閉じ込め層、2は活性
層、3はP型キヤリア閉じ込め層、4はn型
AlAs層、5はP型AlAs層、6はn−GaAs基板、
7はバツフアー層、8はn型クラツド層、9はP
型クラツド層、10はキヤツプ層、11はSiO2
膜、12はP型電極、13はn型電極、14は電
極窓である。
FIG. 1a is an energy band diagram of the main part of a conventional AlGaAs/GaAs single quantum well structure semiconductor laser, and FIG. 1b is a schematic diagram of its atomic arrangement. FIG. 2 is a sectional view of one embodiment of the present invention.
FIG. 3a is an energy band diagram near the active layer of an embodiment of the present invention, and FIG. 3b is a schematic diagram of its atomic arrangement. In the figure, 1 is an n-type carrier confinement layer, 2 is an active layer, 3 is a P-type carrier confinement layer, and 4 is an n-type
AlAs layer, 5 is P-type AlAs layer, 6 is n-GaAs substrate,
7 is a buffer layer, 8 is an n-type cladding layer, 9 is a P
type cladding layer, 10 is the cap layer, 11 is SiO 2
12 is a P-type electrode, 13 is an N-type electrode, and 14 is an electrode window.

Claims (1)

【特許請求の範囲】[Claims] 1 活性層とこの活性層を上下にはさみ前記活性
層に比し、大きな禁制帯幅を有し2つの元素から
なる化合物半導体からなる第1及び第2半導体層
と、この第1及び第2半導体層と前記活性層から
なる量子井戸型3層構造を上下にはさみ前記活性
層に比し大きな禁制帯幅を有し、少なくとも3つ
以上の元素からなる化合物半導体からなる第3及
び第4半導体層を備え、前記第1及び第2半導体
層の厚みが、それぞれ電子及び正孔が量子力学的
トンネル現象によつて通過できる程度の厚さにな
つていることを特徴とする半導体レーザー。
1. an active layer, first and second semiconductor layers sandwiching the active layer above and below and comprising a compound semiconductor made of two elements and having a larger forbidden band width than the active layer; and the first and second semiconductor layers. and third and fourth semiconductor layers sandwiching a quantum well type three-layer structure consisting of the active layer above and below, having a larger forbidden band width than the active layer, and made of a compound semiconductor made of at least three or more elements. A semiconductor laser comprising: the first and second semiconductor layers each having a thickness such that electrons and holes can pass therethrough by a quantum mechanical tunneling phenomenon.
JP1960284A 1984-02-06 1984-02-06 Semiconductor laser Granted JPS60164379A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1960284A JPS60164379A (en) 1984-02-06 1984-02-06 Semiconductor laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1960284A JPS60164379A (en) 1984-02-06 1984-02-06 Semiconductor laser

Publications (2)

Publication Number Publication Date
JPS60164379A JPS60164379A (en) 1985-08-27
JPH0576794B2 true JPH0576794B2 (en) 1993-10-25

Family

ID=12003754

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1960284A Granted JPS60164379A (en) 1984-02-06 1984-02-06 Semiconductor laser

Country Status (1)

Country Link
JP (1) JPS60164379A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
USRE36431E (en) * 1992-02-05 1999-12-07 Mitsui Chemicals, Inc. Semiconductor laser element and laser device using the same element
US5467364A (en) * 1992-02-05 1995-11-14 Mitsui Petrochemical Industries, Ltd. Semiconductor laser element and laser device using the same element
CA2138912C (en) * 1993-12-24 1999-05-04 Shoji Ishizaka Semiconductor laser device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA1137605A (en) * 1979-01-15 1982-12-14 Donald R. Scifres High output power laser

Also Published As

Publication number Publication date
JPS60164379A (en) 1985-08-27

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