JP3147133B2 - Horizontal light receiving element and method of forming the same - Google Patents
Horizontal light receiving element and method of forming the sameInfo
- Publication number
- JP3147133B2 JP3147133B2 JP8634593A JP8634593A JP3147133B2 JP 3147133 B2 JP3147133 B2 JP 3147133B2 JP 8634593 A JP8634593 A JP 8634593A JP 8634593 A JP8634593 A JP 8634593A JP 3147133 B2 JP3147133 B2 JP 3147133B2
- Authority
- JP
- Japan
- Prior art keywords
- light receiving
- layer
- receiving element
- type
- crystal layer
- 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
Links
- 238000000034 method Methods 0.000 title claims description 8
- 239000010410 layer Substances 0.000 claims description 155
- 239000013078 crystal Substances 0.000 claims description 52
- 239000000758 substrate Substances 0.000 claims description 51
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 30
- 230000004888 barrier function Effects 0.000 claims description 6
- 238000005229 chemical vapour deposition Methods 0.000 claims description 6
- 229910052751 metal Inorganic materials 0.000 claims description 6
- 239000002184 metal Substances 0.000 claims description 6
- 239000002344 surface layer Substances 0.000 claims description 6
- 229910000980 Aluminium gallium arsenide Inorganic materials 0.000 claims description 3
- 239000012535 impurity Substances 0.000 claims 6
- 230000004044 response Effects 0.000 description 24
- 230000003287 optical effect Effects 0.000 description 11
- 230000035945 sensitivity Effects 0.000 description 10
- 239000000969 carrier Substances 0.000 description 9
- 230000005684 electric field Effects 0.000 description 8
- 229910001020 Au alloy Inorganic materials 0.000 description 7
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 7
- 239000010931 gold Substances 0.000 description 7
- 238000004519 manufacturing process Methods 0.000 description 6
- 239000004065 semiconductor Substances 0.000 description 6
- 229910000927 Ge alloy Inorganic materials 0.000 description 5
- 239000000463 material Substances 0.000 description 5
- 238000009826 distribution Methods 0.000 description 4
- 239000002994 raw material Substances 0.000 description 4
- RGGPNXQUMRMPRA-UHFFFAOYSA-N triethylgallium Chemical compound CC[Ga](CC)CC RGGPNXQUMRMPRA-UHFFFAOYSA-N 0.000 description 4
- IBEFSUTVZWZJEL-UHFFFAOYSA-N trimethylindium Chemical compound C[In](C)C IBEFSUTVZWZJEL-UHFFFAOYSA-N 0.000 description 4
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 2
- 229910001297 Zn alloy Inorganic materials 0.000 description 2
- RBFQJDQYXXHULB-UHFFFAOYSA-N arsane Chemical compound [AsH3] RBFQJDQYXXHULB-UHFFFAOYSA-N 0.000 description 2
- 229910052785 arsenic Inorganic materials 0.000 description 2
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical compound [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 229910052733 gallium Inorganic materials 0.000 description 2
- 238000002513 implantation Methods 0.000 description 2
- 229910052738 indium Inorganic materials 0.000 description 2
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical compound [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 description 2
- 238000005468 ion implantation Methods 0.000 description 2
- 150000002500 ions Chemical class 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 229910000530 Gallium indium arsenide Inorganic materials 0.000 description 1
- 229910000673 Indium arsenide Inorganic materials 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- RPQDHPTXJYYUPQ-UHFFFAOYSA-N indium arsenide Chemical compound [In]#[As] RPQDHPTXJYYUPQ-UHFFFAOYSA-N 0.000 description 1
- 238000002347 injection Methods 0.000 description 1
- 239000007924 injection Substances 0.000 description 1
- 230000031700 light absorption Effects 0.000 description 1
- JLTRXTDYQLMHGR-UHFFFAOYSA-N trimethylaluminium Chemical compound C[Al](C)C JLTRXTDYQLMHGR-UHFFFAOYSA-N 0.000 description 1
- 238000000927 vapour-phase epitaxy Methods 0.000 description 1
Classifications
-
- C—CHEMISTRY; METALLURGY
- C04—CEMENTS; CONCRETE; ARTIFICIAL STONE; CERAMICS; REFRACTORIES
- C04B—LIME, MAGNESIA; SLAG; CEMENTS; COMPOSITIONS THEREOF, e.g. MORTARS, CONCRETE OR LIKE BUILDING MATERIALS; ARTIFICIAL STONE; CERAMICS; REFRACTORIES; TREATMENT OF NATURAL STONE
- C04B18/00—Use of agglomerated or waste materials or refuse as fillers for mortars, concrete or artificial stone; Treatment of agglomerated or waste materials or refuse, specially adapted to enhance their filling properties in mortars, concrete or artificial stone
- C04B18/04—Waste materials; Refuse
- C04B18/18—Waste materials; Refuse organic
- C04B18/24—Vegetable refuse, e.g. rice husks, maize-ear refuse; Cellulosic materials, e.g. paper, cork
- C04B18/28—Mineralising; Compositions therefor
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02W—CLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO WASTEWATER TREATMENT OR WASTE MANAGEMENT
- Y02W30/00—Technologies for solid waste management
- Y02W30/50—Reuse, recycling or recovery technologies
- Y02W30/91—Use of waste materials as fillers for mortars or concrete
Landscapes
- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Ceramic Engineering (AREA)
- Environmental & Geological Engineering (AREA)
- Civil Engineering (AREA)
- Materials Engineering (AREA)
- Structural Engineering (AREA)
- Organic Chemistry (AREA)
- Light Receiving Elements (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、高感度で応答速度の速
い横型受光素子の構造及びその形成方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a structure of a horizontal light receiving element having high sensitivity and high response speed and a method of forming the same.
【0002】[0002]
【従来の技術】光通信技術や光計測技術の分野では、高
速な応答特性を有する受光素子が必要とされている。受
光素子は構造的に縦型受光素子と横型受光素子に大別さ
れる。2. Description of the Related Art In the fields of optical communication technology and optical measurement technology, a light receiving element having a high-speed response characteristic is required. The light receiving elements are roughly classified into vertical light receiving elements and horizontal light receiving elements.
【0003】縦型受光素子は、受光面に対して例えば垂
直に入射された光信号によって励起された電気的なキャ
リアを、半導体基板に対して垂直方向へ走行させる構造
を有しており、更に、このキャリアを電気信号として出
力するために、半導体基板の表面側に電極が形成される
と共に、半導体基板の内部若しくは裏面にも電極が形成
されることから、半導体基板を平坦化することが困難で
あるという欠点と、絶縁性の基板を利用することができ
ないという問題がある。[0003] The vertical light receiving element has a structure in which an electric carrier excited by an optical signal incident perpendicularly to the light receiving surface, for example, travels in a direction perpendicular to the semiconductor substrate. In order to output the carrier as an electric signal, an electrode is formed on the front surface side of the semiconductor substrate, and an electrode is formed inside or on the back surface of the semiconductor substrate. Therefore, it is difficult to flatten the semiconductor substrate. And the problem that an insulating substrate cannot be used.
【0004】一方、横型受光素子は、受光面に対して例
えば垂直に入射された光信号によって励起された電気的
なキャリアを、半導体基板に対して平行方向へ走行させ
る構造を有しており、更に、キャリアを電気信号として
出力するためには、半導体基板の表面に一対の電極を形
成すればよいので、製造プロセスが簡素化されると同時
に、他の素子を含む集積回路を形成し易い等の利点があ
る。On the other hand, a horizontal light receiving element has a structure in which an electric carrier excited by, for example, an optical signal incident perpendicularly to a light receiving surface travels in a direction parallel to a semiconductor substrate. Furthermore, in order to output the carrier as an electric signal, a pair of electrodes may be formed on the surface of the semiconductor substrate, so that the manufacturing process is simplified and an integrated circuit including other elements is easily formed. There are advantages.
【0005】横型受光素子としては、図8に示す縦断面
構造を有する光伝導型受光素子と、図9に示す縦断面構
造を有するPINフォトダイオード型受光素子と、図1
0に示す縦断面構造を有するMSM型受光素子が知られ
ている。As the horizontal light receiving element, a photoconductive light receiving element having a vertical sectional structure shown in FIG. 8, a PIN photodiode type light receiving element having a vertical sectional structure shown in FIG.
An MSM type light receiving element having a vertical cross-sectional structure shown in FIG.
【0006】図8の光伝導型受光素子は、InP基板上
に結晶成長されたGa0.47In0.53Asの受光層を有す
ると共に、その受光層上に一対のn型オーミック電極が
形成され、約1.7μm以下の波長の光に対して感度を
有する。尚、InP基板の代わりにGaAs基板が適用
され、このGaAs基板上にGaAs結晶の受光層が形
成されると共に、一対のn型オーミック電極が形成され
た光伝導型受光素子もあり、この素子は、約0.9μm
以下の波長の光に対して感度を有する。The photoconductive light-receiving element shown in FIG. 8 has a light-receiving layer of Ga 0.47 In 0.53 As grown on an InP substrate and a pair of n-type ohmic electrodes formed on the light-receiving layer. It has sensitivity to light having a wavelength of 0.7 μm or less. In addition, a GaAs substrate is used instead of the InP substrate, and there is a photoconductive type light receiving element in which a GaAs crystal light receiving layer is formed on the GaAs substrate and a pair of n-type ohmic electrodes are formed. , About 0.9μm
It has sensitivity to light of the following wavelengths.
【0007】図9のPINフォトダイオード型受光素子
は、InP基板上に結晶成長されたGaInAsの受光
層の表層に、n型イオン注入領域とp型イオン注入領域
が形成され、更にn型イオン注入領域上にn型オーミッ
ク電極、p型イオン注入領域上にp型オーミック電極が
夫々形成されている。尚、InP基板に代えてGaAs
基板を適用し、そのGaAs基板上にGaAs結晶の受
光層が形成されると共に、図示の如く一対のn型オーミ
ック電極とp型オーミック電極とが形成され、更にn型
オーミック電極とp型オーミック電極が夫々形成された
ものもある。In the PIN photodiode type light receiving element shown in FIG. 9, an n-type ion implantation region and a p-type ion implantation region are formed on the surface layer of a GaInAs light-receiving layer crystal-grown on an InP substrate. An n-type ohmic electrode is formed on the region, and a p-type ohmic electrode is formed on the p-type ion-implanted region. Incidentally, GaAs is used instead of the InP substrate.
A GaAs crystal light-receiving layer is formed on the GaAs substrate, a pair of n-type ohmic electrodes and a p-type ohmic electrode are formed as shown in the figure, and further, an n-type ohmic electrode and a p-type ohmic electrode are applied. Some are formed respectively.
【0008】図10のMSM型受光素子は、InP基板
上に結晶成長されたGa0.47In0.53As受光層の上面
に、Al0.48Ga0.52Asショットキ障壁増大層が形成
され、更に、そのショットキ障壁増大層の上面に一対の
ショットキ電極が形成されている。即ち、Ga0.47In
0.53As受光層に直接ショットキ接合を形成することが
困難であるので、Al0.48Ga0.52Asショットキ障壁
増大層が形成されている。尚、InP基板に代えてGa
As基板を適用し、このGaAs基板上にGaAs結晶
の受光層が形成される場合には、この受光層に直接ショ
ットキ電極が蒸着される場合が多い。In the MSM type light receiving device shown in FIG. 10, an Al 0.48 Ga 0.52 As Schottky barrier enhancement layer is formed on the upper surface of a Ga 0.47 In 0.53 As light absorption layer crystal-grown on an InP substrate. A pair of Schottky electrodes are formed on the upper surface of the layer. That is, Ga 0.47 In
Since it is difficult to form a Schottky junction directly on the 0.53 As light receiving layer, an Al 0.48 Ga 0.52 As Schottky barrier enhancement layer is formed. In addition, instead of the InP substrate, Ga
When an As substrate is applied and a GaAs crystal light-receiving layer is formed on the GaAs substrate, a Schottky electrode is often directly deposited on the light-receiving layer.
【0009】[0009]
【発明が解決しようとする課題】ところで、横型受光素
子の応答速度は、光信号により励起されたキャリアが電
極に到達するまでの走行時間によって支配され、キャリ
アの走行速度は受光層内の電界強度に依存しており、一
般的には、電界強度が高いほど走行速度が速くなる。図
8に対応する図11の電界強度分布に基づいて更に詳述
すると、例えば電極に印加された電圧(−5Vと+5
V)によって受光層内に生じる電界の強度は受光層の表
層近傍では強く、深部に行くほど弱くなる。したがっ
て、受光素子の応答速度は、深部を走行するキャリアの
走行速度に支配されることとなる。By the way, the response speed of the lateral light receiving element is governed by the transit time until the carrier excited by the optical signal reaches the electrode, and the traveling speed of the carrier depends on the electric field strength in the light receiving layer. In general, the higher the electric field intensity, the higher the traveling speed. More specifically, based on the electric field intensity distribution of FIG. 11 corresponding to FIG. 8, for example, the voltages (−5 V and +5
The intensity of the electric field generated in the light receiving layer due to V) is strong near the surface layer of the light receiving layer and becomes weaker as it goes deeper. Therefore, the response speed of the light receiving element is governed by the traveling speed of the carrier traveling deep.
【0010】そこで、受光素子の応答速度を向上させる
ための手段として、受光層の層厚を薄くすることによっ
て、強電界中を走行するキャリアのみを検出することが
考えられるが、しかし受光層を薄くすると、この受光層
では、入射された光信号を十分に吸収することができな
いので、感度が低下するという問題を招来する。Therefore, as a means for improving the response speed of the light receiving element, it is conceivable to detect only carriers traveling in a strong electric field by reducing the thickness of the light receiving layer. If the thickness is reduced, the light-receiving layer cannot sufficiently absorb the incident optical signal, which causes a problem that the sensitivity is reduced.
【0011】本発明は、このような従来の課題に鑑みて
なされたものであり、高感度で且つ応答速度の優れた横
型受光素子とその形成方法を提供することを目的とす
る。The present invention has been made in view of such conventional problems, and has as its object to provide a horizontal light receiving element having high sensitivity and excellent response speed, and a method of forming the same.
【0012】[0012]
【課題を解決するための手段及び作用】かかる本発明の
目的を達成するために、次の原理に基づいて横型受光素
子を構成した。In order to achieve the object of the present invention, a horizontal light receiving element is constructed based on the following principle.
【0013】即ち、図11と共に説明したように、受光
層中に発生したキャリアの多くは、その受光層の深部
(基板に近い部分)に沿って走行する。よって、受光層
の深部を走行するキャリアの走行速度を高めれば、受光
層の層厚を厚くしても、受光素子の応答速度を向上させ
ることができることとなる。That is, as described with reference to FIG. 11, most of the carriers generated in the light-receiving layer travel along the deep part (the part close to the substrate) of the light-receiving layer. Therefore, if the traveling speed of the carrier traveling deep in the light receiving layer is increased, the response speed of the light receiving element can be improved even if the thickness of the light receiving layer is increased.
【0014】次表は、GaAsと、Ga0.47In0.53A
sと、InAsの各材料の電子移動度と正孔移動度を示
している。The following table shows GaAs and Ga 0.47 In 0.53 A
s, and electron mobility and hole mobility of each material of InAs.
【0015】[0015]
【表1】 [Table 1]
【0016】かかる特性を評価すると、Ga(1-x) In
x Asにおける電子移動度は、xが大きいほど大きくな
る。よって、本発明は、受光層と基板との界面に、xの
大きなGa(1-x) Inx Asの層を形成することによっ
て、受光層の深部に沿って走行する電子の走行速度を向
上(大きく)させ、ひいては受光素子の応答速度の向上
と感度の向上を図った。When these characteristics are evaluated, Ga (1-x) In
electron mobility in x As increases as x increases. Therefore, the present invention improves the traveling speed of electrons traveling along the deep part of the light receiving layer by forming a layer of Ga (1-x) In x As with a large x at the interface between the light receiving layer and the substrate. (Increase), and thus the response speed and sensitivity of the light receiving element are improved.
【0017】又、GaAs基板上にGa(1-x) Inx A
s(但し、x>0.1)を結晶成長させたり、InP基
板上にGa(1-x) Inx As(但し、x>0.6)を結
晶成長させると、基板に対して成長された結晶の格子定
数が大きいために、結晶に圧縮性の歪が発生する。この
圧縮性の歪は、結晶のエネルギーバンドの構造を変化さ
せ、キャリアの走行特性に変化をもたらす。特に、圧縮
性の歪を有する結晶では正孔移動度が大幅に向上し、I
nP基板上にGa0.32In0.68As(1%の歪量に相当
する)を結晶成長させた場合には、InP基板上にGa
0.47In0.53As(無歪)を結晶成長させた場合と比較
して、約3倍の正孔移動度の向上が得られることが知ら
れている(“ELECTRON AND HOLE MOBILITY IN MODULATI
ON DOPEDGaInAs-AlInAs STRAINED LAYER SUPERLATTECE
”K.Hirose,T.Mizutani, Journal of Crystal Growth
vol.81 page130(1987) )。よって、本発明は、基板に
対して圧縮性の歪を有する結晶層を、受光層と基板との
界面に形成することによって、正孔の走行速度を向上さ
せ、ひいては受光素子の応答速度の向上と感度の向上を
図った。Further, Ga (1-x) In x A is formed on a GaAs substrate.
When s (where x> 0.1) is grown or Ga (1-x) In x As (where x> 0.6) is grown on an InP substrate, the crystal is grown on the substrate. Since the crystal lattice constant is large, compressive strain is generated in the crystal. This compressive strain changes the structure of the energy band of the crystal, and changes the running characteristics of the carrier. In particular, in a crystal having compressive strain, the hole mobility is significantly improved, and
When Ga 0.32 In 0.68 As (corresponding to 1% strain) is grown on the nP substrate, Ga
It is known that the hole mobility can be improved about three times as compared with the case where 0.47 In 0.53 As (unstrained) is grown (“ELECTRON AND HOLE MOBILITY IN MODULATI”).
ON DOPEDGaInAs-AlInAs STRAINED LAYER SUPERLATTECE
”K. Hirose, T. Mizutani, Journal of Crystal Growth
vol.81 page130 (1987)). Therefore, the present invention improves the traveling speed of holes by forming a crystal layer having compressive strain with respect to the substrate at the interface between the light receiving layer and the substrate, and thus improves the response speed of the light receiving element. And improved sensitivity.
【0018】本発明の実施態様として、InP基板上
に、Ga(1-x) Inx As(但し、x>0.6)結晶層
を形成すると共に、更に該結晶層上にGa0.47In0.53
As受光層を形成した横型受光素子にあっては、光信号
によって発生されたキャリアが上記Ga(1-x) Inx A
s(但し、x>0.6)結晶層を高速走行するので、応
答速度の向上した受光素子が実現される。As an embodiment of the present invention, a Ga (1-x) In x As (where x> 0.6) crystal layer is formed on an InP substrate, and Ga 0.47 In 0.53 is further formed on the crystal layer.
In the lateral light receiving element having the As light receiving layer, the carrier generated by the optical signal is Ga (1-x) In x A
Since the s (where x> 0.6) crystal layer travels at high speed, a light receiving element with improved response speed is realized.
【0019】又、他の実施態様として、GaAs基板上
に形成されたGa(1-x) Inx As(但し、x>0.
1)結晶層を形成すると共に、更に該結晶層上にGaA
s受光層が形成された横型受光素子にあっては、光信号
によって発生されたキャリアが上記Ga(1-x) Inx A
s(但し、x>0.1)結晶層を高速走行するので、応
答速度の向上した受光素子が実現される。In another embodiment, Ga (1-x) In x As (where x> 0.times.0 ) is formed on a GaAs substrate.
1) A crystal layer is formed, and GaAs is further formed on the crystal layer.
In the lateral light receiving element in which the s light receiving layer is formed, the carrier generated by the optical signal is Ga (1-x) In x A
Since the s (where x> 0.1) crystal layer travels at a high speed, a light receiving element with improved response speed is realized.
【0020】[0020]
【実施例】以下、本発明の一実施例を図面と共に説明す
る。まず、図1に基づいて構造を説明すると、Feをド
ープした半絶縁性のInP基板1に、有機金属気相成長
法を用いて、Ga0.32In0.68Asの結晶層2とGa
0.47In0.53Asの受光層3とが順に形成されている。
ここで、結晶層2と受光層3のガリウム(Ga)原料に
はトリエチルガリウム、インジウム(In)原料にはト
リメチルインジウム、砒素(As)原料にはアルシンが
適用される。そして、製造工程において、トリエチルガ
リウムとトリメチルインジウムの流量比を調節すること
によって、組成の異なる結晶層2と受光層3を成長させ
る。又、結晶層2の厚さは100nm、受光層3の厚さ
は1.5μmとした。An embodiment of the present invention will be described below with reference to the drawings. First, the structure will be described with reference to FIG. 1. On a Fe-doped semi-insulating InP substrate 1, a Ga 0.32 In 0.68 As crystal layer 2 and a Ga 3
The light receiving layer 3 of 0.47 In 0.53 As is formed in order.
Here, gallium (Ga) material for the crystal layer 2 and the light receiving layer 3 is triethylgallium, indium (In) material is trimethylindium, and arsenic (As) material is arsine. Then, in the manufacturing process, the crystal layer 2 and the light receiving layer 3 having different compositions are grown by adjusting the flow ratio of triethylgallium and trimethylindium. The thickness of the crystal layer 2 was 100 nm, and the thickness of the light receiving layer 3 was 1.5 μm.
【0021】更に、結晶成長した受光層3の表面に、一
対のオーミック電極4a,4bが形成されている。尚、
オーミック電極4a,4bは、ゲルマニウムと金の合金
が適用され、相互の電極間隔が4μm、厚さが100n
mの櫛形形状に形成されている。Further, a pair of ohmic electrodes 4a and 4b are formed on the surface of the light receiving layer 3 on which the crystal is grown. still,
For the ohmic electrodes 4a and 4b, an alloy of germanium and gold is applied, the distance between the electrodes is 4 μm, and the thickness is 100 n.
m is formed in a comb shape.
【0022】かかる構造を有する横型受光素子によれ
ば、図7に示すように、例えば、オーミック電極4a,
4bに−5Vと+5Vの電圧を印加した場合に、図示の
如く受光素子内に電界強度分布が発生する。そして、光
信号hνの入射によって内部に発生して受光層3の深部
に達したキャリアは、電子移動度及び正孔移動度の高い
歪層の領域Wを高速走行するので、応答速度の向上した
受光素子が実現される。According to the lateral light receiving element having such a structure, for example, as shown in FIG.
When -5V and + 5V voltages are applied to 4b, an electric field intensity distribution is generated in the light receiving element as shown in the figure. The carriers generated inside by the incidence of the optical signal hν and reaching the deep portion of the light-receiving layer 3 travel at high speed in the region W of the strained layer having high electron mobility and hole mobility, so that the response speed is improved. A light receiving element is realized.
【0023】次に、第2の実施例を図2と共に説明す
る。尚、図2において図1の構成部分に相当する部分を
同一符号で示す。まず、構造を説明すると、これはPI
Nフォトダイオード型受光素子であり、Feをドープし
た半絶縁性のInP基板1に、有機金属気相成長法を用
いて、Ga0.32In0.68Asの結晶層2とGa0.47In
0.53Asの受光層3とが順に形成されている。ここで、
結晶層2と受光層3の原料と製造方法は前記第1の実施
例と同じである。Next, a second embodiment will be described with reference to FIG. In FIG. 2, parts corresponding to those in FIG. 1 are indicated by the same reference numerals. First, to explain the structure, this is PI
This is an N-photodiode type light receiving element, in which a Ga 0.32 In 0.68 As crystal layer 2 and a Ga 0.47 In are formed on a semi-insulating InP substrate 1 doped with Fe by using a metal organic chemical vapor deposition method.
The light receiving layer 3 of 0.53 As is formed in order. here,
The raw materials and manufacturing method of the crystal layer 2 and the light receiving layer 3 are the same as those in the first embodiment.
【0024】更に、結晶成長した受光層3の所定箇所の
表層部分に、Siをイオン注入することによってn型注
入領域5aが形成されると共に、Beをドーピングする
ことによってp型注入領域5bが形成されている。更
に、n型注入領域5a上にn型オーミック電極6a、p
型注入領域5b上にp型オーミック電極6bが夫々形成
されている。尚、n型オーミック電極6aにはゲルマニ
ウムと金の合金等が適用され、p型オーミック電極6b
には亜鉛と金の合金等が適用されている。Further, an n-type implanted region 5a is formed by implanting Si ions into a predetermined portion of the surface layer of the light-receiving layer 3 on which the crystal has been grown, and a p-type implanted region 5b is formed by doping Be. Have been. Further, the n-type ohmic electrodes 6a, p
A p-type ohmic electrode 6b is formed on each of the mold injection regions 5b. Note that an alloy of germanium and gold or the like is applied to the n-type ohmic electrode 6a, and the p-type ohmic electrode 6b
Is applied with an alloy of zinc and gold.
【0025】かかる構造を有するPINフォトダイオー
ド型受光素子にあっても、図7に示すのと同様に、素子
内部に発生して受光層3の深部に達したキャリアは、電
子移動度及び正孔移動度の高い歪層を高速走行するの
で、応答速度の向上した受光素子が実現される。Even in the PIN photodiode type light receiving element having such a structure, the carriers generated inside the element and reaching the deep part of the light receiving layer 3 have the electron mobility and the hole as shown in FIG. Since the vehicle travels at a high speed on the strained layer having high mobility, a light receiving element with improved response speed is realized.
【0026】次に、第3の実施例を図3と共に説明す
る。尚、図3において図1の構成部分に相当する部分を
同一符号で示す。まず、構造を説明すると、これはMS
M型受光素子であり、Feをドープした半絶縁性のIn
P基板1にInPのバッファ層7が形成され、更にバッ
ファ層7上にGa0.61In0.39Asの層8が形成され、
更に層8の上に、有機金属気相成長法を用いて、Ga
0.32In0.68Asの結晶層2とGa0.47In0.53Asの
受光層3とが順に形成されている。ここで、結晶層2と
受光層3の原料と製造方法は前記第1の実施例と同じで
ある。Next, a third embodiment will be described with reference to FIG. In FIG. 3, portions corresponding to the components in FIG. 1 are indicated by the same reference numerals. First, the structure will be described.
This is an M-type light receiving element, which is semi-insulating In doped with Fe.
A buffer layer 7 of InP is formed on the P substrate 1, and a layer 8 of Ga 0.61 In 0.39 As is further formed on the buffer layer 7,
Further, on the layer 8, Ga was grown using metal organic chemical vapor deposition.
A crystal layer 2 of 0.32 In 0.68 As and a light receiving layer 3 of Ga 0.47 In 0.53 As are sequentially formed. Here, the raw materials and manufacturing method of the crystal layer 2 and the light receiving layer 3 are the same as those in the first embodiment.
【0027】更に、受光層3の上面にAl0.48In0.52
Asの層9が形成され、この層9の表面に一対のショッ
トキ電極10a,10bが形成されている。尚、Al
0.48In0.52Asの層9の層厚は約0.1μm、Alの
原料としてトリメチルアルミニウムが適用されている。
又、ショットキ電極10a,10bは、ゲルマニウムと
金の合金が適用され、相互の電極間隔が4μm、厚さが
100nmの櫛形形状に形成されている。Further, Al 0.48 In 0.52
An As layer 9 is formed, and a pair of Schottky electrodes 10 a and 10 b are formed on the surface of the layer 9. In addition, Al
The layer 9 of 0.48 In 0.52 As has a thickness of about 0.1 μm, and trimethyl aluminum is applied as a raw material of Al.
The Schottky electrodes 10a and 10b are made of an alloy of germanium and gold, and are formed in a comb shape with a mutual electrode spacing of 4 μm and a thickness of 100 nm.
【0028】かかる構造を有するMSM型受光素子にあ
っても、図7に示すのと同様に、素子内部に発生して受
光層3の深部に達したキャリアは、電子移動度及び正孔
移動度の高い歪層を高速走行するので、応答速度の向上
した受光素子が実現される。更に、InPバッファ層7
と受光層2の間に、Ga0.61In0.39Asの層8を介在
させたことにより、歪を相殺して結晶性を良好に保つの
に効果がある。Even in the MSM type light receiving element having such a structure, carriers generated inside the element and reaching the deep part of the light receiving layer 3 have electron mobility and hole mobility as shown in FIG. Since the light-emitting element travels at a high speed on a strained layer having a high response speed, a light-receiving element with improved response speed is realized. Further, the InP buffer layer 7
By interposing the Ga 0.61 In 0.39 As layer 8 between the light-receiving layer 2 and the light-receiving layer 2, the strain is canceled and the crystallinity is effectively maintained.
【0029】尚、図3では、InPのバッファ層7が形
成されているが、バッファ層7はこれに限らず任意の構
造のバッファ層を適用してもよい。又、同図では、Ga
0.47In0.53Asの受光層3にAl0.48In0.52Asの
層9を直接形成しているが、かかる層9と受光層3との
間に、AlGaInAsの4元層若しくはこれらの材料
からなる超格子を挿入形成してもよく、かかる構造を挿
入すると応答速度の更なる向上を図ることができる。Although the buffer layer 7 of InP is formed in FIG. 3, the buffer layer 7 is not limited to this, and a buffer layer having an arbitrary structure may be used. In FIG.
A layer 9 of Al 0.48 In 0.52 As is directly formed on the light receiving layer 3 of 0.47 In 0.53 As, and a quaternary layer of AlGaInAs or a superlattice made of these materials is provided between the layer 9 and the light receiving layer 3. May be formed. When such a structure is inserted, the response speed can be further improved.
【0030】次に、第4の実施例を図4と共に説明す
る。まず構造を説明すると、これはGaAs基板を適用
した素子であり、GaAs基板11に、有機金属気相成
長法を用いて、Ga0.84In0.15Asの結晶層12とG
aAsの受光層13とが順に形成されている。ここで、
結晶層12と受光層13のガリウム(Ga)原料にはト
リエチルガリウム、インジウム(In)原料にはトリメ
チルインジウム、砒素(As)原料にはアルシンが適用
される。そして、製造工程において、トリエチルガリウ
ムとトリメチルインジウムの流量比を調節することによ
って、組成の異なる結晶層12と受光層13を成長させ
る。Next, a fourth embodiment will be described with reference to FIG. First, the structure will be described. This is an element using a GaAs substrate. A GaAs substrate 11 is formed on a Ga 0.84 In 0.15 As crystal layer 12 by metalorganic vapor phase epitaxy.
The light-receiving layer 13 of aAs is formed in order. here,
The gallium (Ga) source of the crystal layer 12 and the light receiving layer 13 is triethylgallium, the indium (In) source is trimethylindium, and the arsenic (As) source is arsine. Then, in the manufacturing process, the crystal layer 12 and the light receiving layer 13 having different compositions are grown by adjusting the flow ratio of triethylgallium and trimethylindium.
【0031】更に、結晶成長した受光層13の表面に、
一対のn型オーミック電極14a,14bが形成されて
いる。尚、n型オーミック電極14a,14bは、ゲル
マニウムと金の合金が適用されている。Further, on the surface of the light receiving layer 13 on which the crystal has grown,
A pair of n-type ohmic electrodes 14a and 14b are formed. The n-type ohmic electrodes 14a and 14b are made of an alloy of germanium and gold.
【0032】かかる構造を有する横型受光素子によれ
ば、図7に示したのと同様に、素子内部に発生して受光
層13の深部に達したキャリアは、電子移動度及び正孔
移動度の高い歪層を高速走行するので、応答速度の向上
した受光素子が実現される。According to the lateral light receiving element having such a structure, carriers generated inside the element and reaching the deep portion of the light receiving layer 13 have the same electron mobility and hole mobility as shown in FIG. Since the vehicle travels at a high speed on a high strain layer, a light receiving element with improved response speed is realized.
【0033】次に、第5の実施例を図5と共に説明す
る。尚、図5において図4の構成部分に相当する部分を
同一符号で示す。まず、構造を説明すると、これはPI
Nフォトダイオード型受光素子であり、GaAs基板1
1に、有機金属気相成長法を用いて、Ga0.84In0.15
Asの結晶層12とGaAsの受光層13とが順に形成
されている。ここで、結晶層12と受光層13の原料と
製造方法は前記第4の実施例と同じである。Next, a fifth embodiment will be described with reference to FIG. In FIG. 5, portions corresponding to the components in FIG. 4 are denoted by the same reference numerals. First, to explain the structure, this is PI
N photodiode type light receiving element, GaAs substrate 1
First, using a metal organic chemical vapor deposition method, Ga 0.84 In 0.15
An As crystal layer 12 and a GaAs light receiving layer 13 are sequentially formed. Here, the raw materials and manufacturing method of the crystal layer 12 and the light receiving layer 13 are the same as those of the fourth embodiment.
【0034】更に、結晶成長した受光層13の所定箇所
の表層部分に、Siをイオン注入することによってn型
注入領域15aが形成されると共に、Beをドーピング
することによってp型注入領域15bが形成されてい
る。更に、n型注入領域15a上にn型オーミック電極
16a、p型注入領域15b上にp型オーミック電極1
6bが夫々形成されている。尚、n型オーミック電極1
6aにはゲルマニウムと金の合金等が適用され、p型オ
ーミック電極16bには亜鉛と金の合金等が適用されて
いる。Further, an n-type implanted region 15a is formed by implanting Si ions into a predetermined portion of the surface layer of the light-receiving layer 13 where the crystal has been grown, and a p-type implanted region 15b is formed by doping Be. Have been. Further, the n-type ohmic electrode 16a is provided on the n-type implanted region 15a, and the p-type ohmic electrode 1 is provided on the p-type implanted region 15b.
6b are respectively formed. The n-type ohmic electrode 1
An alloy of germanium and gold is applied to 6a, and an alloy of zinc and gold is applied to the p-type ohmic electrode 16b.
【0035】かかる構造を有するPINフォトダイオー
ド型受光素子にあっても、図7に示すのと同様に、素子
内部に発生して受光層13の深部に達したキャリアは、
電子移動度及び正孔移動度の高い歪層を高速走行するの
で、応答速度の向上した受光素子が実現される。Even in the PIN photodiode type light receiving element having such a structure, carriers generated inside the element and reaching the deep part of the light receiving layer 13 are similar to those shown in FIG.
Since the high-speed traveling through the strained layer having high electron mobility and high hole mobility, a light receiving element with improved response speed is realized.
【0036】次に、第6の実施例を図6と共に説明す
る。尚、図6において図4の構成部分に相当する部分を
同一符号で示す。まず、構造を説明すると、これはMS
M型受光素子であり、GaAs基板11にAl0.3 Ga
0.7 Asのバッファ層17が形成され、更にバッファ層
17上に、有機金属気相成長法を用いて、Ga0.85In
0.15Asの結晶層12とGaAsの受光層13とが順に
形成されている。Next, a sixth embodiment will be described with reference to FIG. In FIG. 6, portions corresponding to the components in FIG. 4 are denoted by the same reference numerals. First, the structure will be described.
This is an M-type light receiving element, and an Al 0.3 Ga
A buffer layer 17 of 0.7 As is formed, and a Ga 0.85 In layer is formed on the buffer layer 17 by metal organic chemical vapor deposition.
A crystal layer 12 of 0.15 As and a light receiving layer 13 of GaAs are sequentially formed.
【0037】更に、受光層13の上面にAlGaAsの
層18が形成され、この層18の表面に一対のショット
キ電極19a,19bが形成されている。Further, an AlGaAs layer 18 is formed on the upper surface of the light receiving layer 13, and a pair of Schottky electrodes 19a and 19b are formed on the surface of the layer 18.
【0038】かかる構造を有するMSM型受光素子にあ
っても、図7に示すのと同様に、素子内部に発生して受
光層13の深部に達したキャリアは、電子移動度及び正
孔移動度の高い歪層を高速走行するので、応答速度の向
上した受光素子が実現される。Even in the MSM type light receiving element having such a structure, the carriers generated inside the element and reaching the deep part of the light receiving layer 13 have the electron mobility and the hole mobility as shown in FIG. Since the light-emitting element travels at a high speed on a strained layer having a high response speed, a light-receiving element with improved response speed is realized.
【0039】更に、GaAs基板11と結晶層12との
間に、Al0.3 Ga0.7 Asのバッファ層17を形成し
たので、光信号によって発生したキャリアを、電子移動
度及び正孔移動度の高い結晶層12に効果的に閉じ込め
ることができる結果、応答速度の向上に寄与する。即
ち、Ga0.85In0.15Asの結晶層12とGaAsの受
光層13のバンドギャップの違いが小さく、光信号によ
って発生したキャリアがこの結晶層12よりも下に漏洩
するという効果を、バッファ層17による大きなバンド
ギャップによって抑止することができるからである。Further, since the buffer layer 17 of Al 0.3 Ga 0.7 As is formed between the GaAs substrate 11 and the crystal layer 12, the carrier generated by the optical signal is transferred to a crystal having a high electron mobility and a high hole mobility. As a result of being able to be effectively confined in the layer 12, it contributes to the improvement of the response speed. That is, the difference in band gap between the crystal layer 12 of Ga 0.85 In 0.15 As and the light-receiving layer 13 of GaAs is small, and the effect that the carriers generated by the optical signal leak below the crystal layer 12 is caused by the buffer layer 17. This is because it can be suppressed by a large band gap.
【0040】[0040]
【発明の効果】以上説明したように本発明によれば、I
nP基板を適用した横型受光素子にあっては、受光層と
該基板との間に電子移動度の大きなGa(1-x) Inx A
s(但し、x>0.6)の結晶層を形成すると共に、こ
の結晶層による圧縮歪によって電子移動度と正孔移動度
を向上させたので、受光層の深部に沿って走行するキャ
リアの走行速度が向上(大きく)なり、受光層を比較的
厚くしても応答速度の向上を図ることができ且つ高感度
を実現することができる。As described above, according to the present invention, I
In a lateral light receiving element using an nP substrate, Ga (1-x) In x A having a large electron mobility is provided between the light receiving layer and the substrate.
Since a crystal layer of s (where x> 0.6) is formed and the electron mobility and the hole mobility are improved by the compressive strain of this crystal layer, the carrier traveling along the deep part of the light receiving layer is improved. Even if the traveling speed is improved (increased) and the light receiving layer is relatively thick, the response speed can be improved and high sensitivity can be realized.
【0041】又、GaAs基板を適用した横型受光素子
にあっては、受光層と該基板との間に電子移動度の大き
なGa(1-x) Inx As(但し、x>0.1)の結晶層
を形成すると共に、この結晶層による圧縮歪によって電
子移動度と正孔移動度を向上させたので、受光層の深部
に沿って走行するキャリアの走行速度が向上(大きく)
なり、受光層を比較的厚くしても応答速度の向上を図る
ことができ且つ高感度を実現することができる。In the case of a lateral light receiving element using a GaAs substrate, Ga (1-x) In x As (where x> 0.1) having a high electron mobility is provided between the light receiving layer and the substrate. And the electron mobility and the hole mobility are improved by the compressive strain caused by the crystal layer, so that the traveling speed of the carrier traveling along the deep part of the light receiving layer is improved (increased).
In other words, even if the light receiving layer is relatively thick, the response speed can be improved and high sensitivity can be realized.
【0042】このように本発明によれば、高感度且つ高
速応答性を有すると共に構造の簡素な横型受光素子を実
現することができるので、極めて高速の光通信システム
に適用したり、極めて高速の計測分野等に適用すること
ができる等の優れた効果を発揮するものである。As described above, according to the present invention, it is possible to realize a horizontal light-receiving element having high sensitivity and high-speed response and having a simple structure. It exhibits excellent effects such as being applicable to the measurement field and the like.
【図1】InP基板を用いた光伝導型の横型受光素子の
一実施例の構造を示す部分断面図である。FIG. 1 is a partial cross-sectional view showing a structure of an embodiment of a photoconductive lateral light receiving element using an InP substrate.
【図2】InP基板を用いたPINフォトダイオード型
の横型受光素子の一実施例の構造を示す部分断面図であ
る。FIG. 2 is a partial cross-sectional view showing the structure of one embodiment of a PIN photodiode type lateral light receiving element using an InP substrate.
【図3】InP基板を用いたMSM型の横型受光素子の
一実施例の構造を示す部分断面図である。FIG. 3 is a partial cross-sectional view showing a structure of an embodiment of an MSM type lateral light receiving element using an InP substrate.
【図4】GaAs基板を用いた光伝導型の横型受光素子
の一実施例の構造を示す部分断面図である。FIG. 4 is a partial cross-sectional view showing a structure of one embodiment of a photoconductive lateral light receiving element using a GaAs substrate.
【図5】GaAs基板を用いたPINフォトダイオード
型の横型受光素子の一実施例の構造を示す部分断面図で
ある。FIG. 5 is a partial cross-sectional view showing the structure of one embodiment of a PIN photodiode type lateral light receiving element using a GaAs substrate.
【図6】GaAs基板を用いたMSM型の横型受光素子
の一実施例の構造を示す部分断面図である。FIG. 6 is a partial cross-sectional view showing the structure of one embodiment of an MSM type lateral light receiving element using a GaAs substrate.
【図7】図1ないし図6に示す実施例の素子内部の電界
分布の概略を示した説明図である。FIG. 7 is an explanatory view schematically showing an electric field distribution inside the device of the embodiment shown in FIGS. 1 to 6;
【図8】光伝導型の横型受光素子の従来例の構造を示す
部分断面図である。FIG. 8 is a partial cross-sectional view showing a structure of a conventional example of a photoconductive horizontal light receiving element.
【図9】PINフォトダイオード型の横型受光素子の従
来例の構造を示す部分断面図である。FIG. 9 is a partial sectional view showing the structure of a conventional example of a PIN photodiode type horizontal light receiving element.
【図10】MSM型の横型受光素子の従来例の構造を示
す部分断面図である。FIG. 10 is a partial cross-sectional view showing the structure of a conventional example of an MSM type horizontal light receiving element.
【図11】図8ないし図10に示す従来例の素子内部の
電界分布の概略をを示した説明図である。FIG. 11 is an explanatory view schematically showing an electric field distribution inside the element of the conventional example shown in FIGS. 8 to 10;
1…InP基板、2…結晶層、3…受光層、4a,4
b,14a,14b…n型オーミック電極、5a,15
a…n型注入領域、5b,15b…p型注入領域、6
a,16a…n型オーミック電極、6b,16b…p型
オーミック電極、7…InP層、8…Ga0.61In0.39
As層、9…Al0.48In0.52As層、10a,10
b,19a,19b…ショットキ電極、17…Al0.3
Ga0.7 As層、18…AlGaAs層。DESCRIPTION OF SYMBOLS 1 ... InP board, 2 ... crystal layer, 3 ... light receiving layer, 4a, 4
b, 14a, 14b... n-type ohmic electrodes, 5a, 15
a: n-type implantation region, 5b, 15b: p-type implantation region, 6
a, 16a ... n-type ohmic electrode, 6b, 16b ... p-type ohmic electrode, 7 ... InP layer, 8 ... Ga 0.61 In 0.39
As layer, 9... Al 0.48 In 0.52 As layer, 10a, 10
b, 19a, 19b: Schottky electrode, 17: Al 0.3
Ga 0.7 As layer, 18... AlGaAs layer.
───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.7,DB名) H01L 31/10 - 31/119 ──────────────────────────────────────────────────続 き Continued on the front page (58) Field surveyed (Int.Cl. 7 , DB name) H01L 31/10-31/119
Claims (13)
nx As(但し、x>0.6)からなる結晶層と、該結
晶層上に形成されたGa0.47In0.53Asからなる受光
層とを有することを特徴とする横型受光素子。 1. Ga (1-x) I formed on an InP substrate
n x As (where, x> 0.6) lateral light receiving element and having a crystal layer composed of, a light receiving layer composed of a formed on the crystal layer Ga 0.47 In 0.53 As.
対する歪量に対する臨界膜厚以下に設定されていること
を特徴とする請求項1に記載の横型受光素子。2. The lateral light receiving device according to claim 1, wherein the thickness of the crystal layer is set to be equal to or less than a critical film thickness with respect to a strain amount with respect to the InP substrate.
ク電極が形成されたことを特徴とする請求項1に記載の
横型受光素子。3. The horizontal light receiving element according to claim 1, wherein an ohmic electrode is formed at a predetermined position on the surface of the light receiving layer.
型の不純物領域が形成され、n型の不純物領域にn型の
オーミック電極、p型の不純物領域にp型のオーミック
電極が形成されることにより、PINフォトダイオード
型構造を有することを特徴とする請求項1に記載の横型
受光素子。4. An n-type and a p-type on a surface layer of a predetermined portion of the light receiving layer.
A n-type impurity region, an n-type ohmic electrode in the n-type impurity region, and a p-type ohmic electrode in the p-type impurity region, thereby having a PIN photodiode type structure. The horizontal light-receiving element according to claim 1.
壁層が形成されると共に、更に該障壁層上に一対のショ
ットキ電極が形成されることにより、MSM型構造を有
することを特徴とする請求項1に記載の横型受光素子。5. An MSM type structure in which a barrier layer made of AlInAs is formed on the light receiving layer and a pair of Schottky electrodes are further formed on the barrier layer. 2. The horizontal light receiving element according to 1.
Inx As(但し、x>0.1)からなる結晶層と、該
結晶層上に形成されたGaAsからなる受光層とを有す
ることを特徴とする横型受光素子。6. Ga (1-x) formed on a GaAs substrate
A horizontal light-receiving element comprising: a crystal layer made of In x As (where x>0.1); and a light-receiving layer made of GaAs formed on the crystal layer.
に対する歪量に対する臨界膜厚以下に設定されているこ
とを特徴とする請求項6に記載の横型受光素子。7. The lateral light receiving device according to claim 6, wherein the thickness of the crystal layer is set to be equal to or less than a critical film thickness with respect to a strain amount with respect to the GaAs substrate.
ク電極が形成されたことを特徴とする請求項6に記載の
横型受光素子。8. The horizontal light receiving element according to claim 6, wherein an ohmic electrode is formed at a predetermined position on the surface of the light receiving layer.
型の不純物領域が形成され、n型の不純物領域にn型の
オーミック電極、p型の不純物領域にp型のオーミック
電極が形成されることにより、PINフォトダイオード
型構造を有することを特徴とする請求項6に記載の横型
受光素子。9. An n-type and a p-type on a predetermined surface layer of the light-receiving layer.
A n-type impurity region, an n-type ohmic electrode in the n-type impurity region, and a p-type ohmic electrode in the p-type impurity region, thereby having a PIN photodiode type structure. The horizontal light receiving element according to claim 6.
障壁層が形成されると共に、更に該障壁層上に一対のシ
ョットキ電極が形成されることにより、MSM型構造を
有することを特徴とする請求項6に記載の横型受光素
子。10. An MSM structure having a barrier layer made of AlGaAs formed on the light receiving layer and a pair of Schottky electrodes formed on the barrier layer. 7. The horizontal light receiving element according to 6.
Asからなるバッファ層と、更に該バッファ層上に形成
されたGa(1-X)InXAs(但し、x>0.1)からなる
結晶層と、更に該結晶層上に形成されたGaAsからな
る受光層とを有することを特徴とする横型受光素子。11. An AlGa film formed on a GaAs substrate.
A buffer layer composed of As, a crystal layer composed of Ga (1-X) In x As (where x> 0.1) further formed on the buffer layer, and a GaAs layer further formed on the crystal layer. A light receiving element comprising: a light receiving layer comprising:
基板上に、Ga(1-x) Inx As(但し、x>0.6)
からなる結晶層と、Ga0.47In0.53Asからなる受光
層とを順に成長させることを特徴とする横型受光素子の
形成方法。12. InP is formed by metal organic chemical vapor deposition.
On the substrate, Ga (1-x) In x As (where x> 0.6)
A method for forming a lateral light receiving element, comprising sequentially growing a crystal layer made of Ga 0.47 In 0.53 As and a light receiving layer made of Ga 0.47 In 0.53 As.
s基板上に、Ga(1-x) Inx As(但し、x>0.
1)からなる結晶層と、GaAsからなる受光層とを順
に成長させることを特徴とする横型受光素子の形成方
法。13. A method of forming GaAs by metal organic chemical vapor deposition.
Ga (1-x) In x As (provided that x> 0.
A method for forming a lateral light receiving element, comprising sequentially growing a crystal layer made of 1) and a light receiving layer made of GaAs.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8634593A JP3147133B2 (en) | 1993-04-13 | 1993-04-13 | Horizontal light receiving element and method of forming the same |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8634593A JP3147133B2 (en) | 1993-04-13 | 1993-04-13 | Horizontal light receiving element and method of forming the same |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH06302843A JPH06302843A (en) | 1994-10-28 |
| JP3147133B2 true JP3147133B2 (en) | 2001-03-19 |
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ID=13884281
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|---|---|---|---|
| JP8634593A Expired - Fee Related JP3147133B2 (en) | 1993-04-13 | 1993-04-13 | Horizontal light receiving element and method of forming the same |
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| Country | Link |
|---|---|
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|---|---|---|---|---|
| US7138697B2 (en) * | 2004-02-24 | 2006-11-21 | International Business Machines Corporation | Structure for and method of fabricating a high-speed CMOS-compatible Ge-on-insulator photodetector |
| JP2006086227A (en) * | 2004-09-14 | 2006-03-30 | Osaka Univ | Light switch |
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|---|---|
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