JPH0677517A - Semiconductor photodetector - Google Patents
Semiconductor photodetectorInfo
- Publication number
- JPH0677517A JPH0677517A JP4250726A JP25072692A JPH0677517A JP H0677517 A JPH0677517 A JP H0677517A JP 4250726 A JP4250726 A JP 4250726A JP 25072692 A JP25072692 A JP 25072692A JP H0677517 A JPH0677517 A JP H0677517A
- Authority
- JP
- Japan
- Prior art keywords
- semiconductor
- layer
- quantum
- polarization light
- type
- 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.)
- Withdrawn
Links
Landscapes
- Light Receiving Elements (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、偏光選択機能を有する
半導体光検出器に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor photodetector having a polarization selection function.
【0002】[0002]
【従来の技術】半導体光検出器は従来結晶基板に不純物
を拡散か、あるいは不純物を打ち込むか、さらには基板
の面に平行な半導体層を結晶成長技術により積層するこ
とによって形成されている。ところが、結晶成長技術の
進歩によって基板の面内方向に量子効果を生じる程度あ
るいはそれ以下の周期の周期的細線構造を形成すること
が可能となった。2. Description of the Related Art A semiconductor photodetector is conventionally formed by diffusing impurities or implanting impurities in a crystal substrate, or by laminating semiconductor layers parallel to the surface of the substrate by a crystal growth technique. However, the progress of crystal growth technology has made it possible to form a periodic thin line structure having a period of a quantum effect in the in-plane direction of the substrate or less.
【0003】図4に従来の半導体光検出器の構造例を示
す。InP基板1上にn型に不純物添加されたInP層
2、不純物添加されていないInGaAs層3、p型に
不純物添加されたInGaAs層4、AuZn金属電極
5を形成する。全ての層を形成し、n型InP層2まで
メサエッチした後、n型InP層2上にAuGeNi金
属電極6を形成する。FIG. 4 shows a structural example of a conventional semiconductor photodetector. On the InP substrate 1, an n-type impurity-doped InP layer 2, an undoped impurity-doped InGaAs layer 3, a p-type impurity-doped InGaAs layer 4, and an AuZn metal electrode 5 are formed. After forming all layers and performing mesa etching to the n-type InP layer 2, the AuGeNi metal electrode 6 is formed on the n-type InP layer 2.
【0004】上記の構造を持つ半導体光検出器にpin
接合に対して逆バイアス電圧を印加しながら、光信号を
pin接合に照射する。i層において光子が吸収され、
電子正孔対が生成される。生成された電子正孔対はpi
n接合に印加された電界によって電極に向かって流れ、
光電流として電極から取り出される。The semiconductor photodetector having the above structure has a pin
An optical signal is applied to the pin junction while applying a reverse bias voltage to the junction. photons are absorbed in the i-layer,
Electron-hole pairs are generated. The generated electron-hole pairs are pi
An electric field applied to the n-junction causes it to flow toward the electrodes,
It is taken out from the electrode as a photocurrent.
【0005】従来の半導体光検出器では特定の偏光光に
対する選択機能を有していないので、その受光感度は入
力光の偏光方向に依存しない。Since the conventional semiconductor photodetector does not have a selection function for specific polarized light, its light receiving sensitivity does not depend on the polarization direction of input light.
【0006】[0006]
【発明が解決しようとする課題】従来の半導体光検出器
は、偏光を選択することができないので、特定の偏光光
を選択的に検出するために検光子等の光学素子を必要と
し、光学装置が複雑になるという欠点があった。Since the conventional semiconductor photodetector cannot select the polarized light, it requires an optical element such as an analyzer to selectively detect the specific polarized light, and the optical device Had the drawback of being complicated.
【0007】本発明の目的は、特定の偏光光に対して選
択的に出力電流を得ることができる半導体光検出器を提
供することにある。An object of the present invention is to provide a semiconductor photodetector which can selectively obtain an output current for a specific polarized light.
【0008】[0008]
【課題を解決するための手段】本発明の第1の半導体光
検出器は、半導体基板上に形成したp型半導体とn型半
導体で構成されたpn接合を有する半導体光検出器にお
いて、前記pn接合の光入射面側に、第1の禁制帯幅の
半導体細線と前記第1の禁制帯幅の半導体細線より広い
第2の禁制帯幅を持つ半導体細線とからなる周期構造を
有し、前記周期構造が面内方向において量子効果を生ず
る程度の周期を持つことを特徴とする。A first semiconductor photodetector according to the present invention is a semiconductor photodetector having a pn junction composed of a p-type semiconductor and an n-type semiconductor formed on a semiconductor substrate. A semiconductor thin line having a first forbidden band width and a semiconductor thin line having a second forbidden band width wider than the semiconductor thin line having the first forbidden band width on the light incident surface side of the junction; It is characterized in that the periodic structure has a period that causes a quantum effect in the in-plane direction.
【0009】本発明の第2の半導体光検出器は、上記第
1の半導体光検出器において、前記p型半導体とn型半
導体の間にi型半導体を形成することによって構成され
るpin接合を有することを特徴とする。A second semiconductor photodetector according to the present invention has a pin junction formed by forming an i-type semiconductor between the p-type semiconductor and the n-type semiconductor in the first semiconductor photodetector. It is characterized by having.
【0010】[0010]
【作用】本発明の原理を図をもとに説明する。図4に示
す従来構成の半導体光検出器では、pin接合に逆バイ
アス電圧を印加し、光信号をi層に照射することによっ
て光電流を得ることができる。図2、図3は、本発明の
半導体光検出器の偏光に関する受光特性を説明するため
の図である。図2は偏光選択層を形成する量子細線の構
造図であり、図3は量子細線の反射率異方性の図を示
す。The principle of the present invention will be described with reference to the drawings. In the semiconductor photodetector with the conventional configuration shown in FIG. 4, a reverse bias voltage is applied to the pin junction and a photocurrent can be obtained by irradiating the i layer with an optical signal. FIG. 2 and FIG. 3 are diagrams for explaining the light receiving characteristics regarding the polarization of the semiconductor photodetector of the present invention. FIG. 2 is a structural view of a quantum wire forming the polarization selection layer, and FIG. 3 is a view of reflectance anisotropy of the quantum wire.
【0011】本発明では、図2に示すように偏光選択層
7がGaAs半導体細線8とInAs半導体細線9とが
量子効果の生じる程度の周期で並んでいる量子細線構造
を有している。量子細線構造は、有機金属気相エピタキ
シアル成長法あるいは有機金属化学気相堆積法あるいは
分子線エピタキシアル成長法によって実現することがで
きる。量子細線構造作製方法の詳細は、例えば、雑誌ア
プライド・フィジックス・レターズ(Applied
Physics Letters)、第50巻、198
7年、824〜826頁に記載された論文「有機金属化
学気相堆積法によって(001)微斜面上に成長した
(AlAs)0.5(GaAs)0.5分数超格子((AlA
s)0.5(GaAs)0.5fractional−lay
er superlattices grown on
(001) vicinal surface by
metal organic chemical v
apor deposition)」に述べられてい
る。半導体細線の周期が量子効果の生じる程度に小さく
なった場合、入射する偏光方向によってバンド端が分離
して観測される。そして、図3に示すように反射率と透
過率が偏光方向によって異なるという光学的異方性を生
じる。詳しく述べると、基板の面方位が(001)面で
あるGaAs基板上で[110]方向に平行なGaAs
細線とInAs細線から形成される量子細線構造では、
InAsの方がGaAsよりも禁制帯幅が狭いため、
[−110]方向にキャリアが閉じ込められる。このキ
ャリア閉じ込め効果により、重い正孔に関与した遷移と
軽い正孔に関与した遷移が分離される。図2において入
射光の電界が[110]に平行な偏光aの場合は長波長
側の重い正孔に関与した遷移が許され、垂直な偏光bの
場合はその遷移が禁止されるためである。そこで、量子
細線構造を半導体光検出器の偏光選択層に用いることが
できる。図3に示す反射率差RDの大きな波長λD を入
射光波長λinに合わせる。このように設計した半導体光
検出器は、偏光方向が[110]に平行な偏光aに対す
る透過率の方が、[110]に垂直な偏光bに対する透
過率よりも小さくなるので、偏光bを選択的に透過でき
る。偏光光bは、pn接合あるいはpin接合部に入射
し、接合部において電子正孔対が生成される。この電子
正孔対は、接合部に印加された逆バイアス電圧によって
発生する光電流として検出される。以上の原理により、
特定方向に偏光成分を持つ光信号を選択的に受光するこ
とが可能となる。In the present invention, as shown in FIG. 2, the polarization selection layer 7 has a quantum thin wire structure in which a GaAs semiconductor thin wire 8 and an InAs semiconductor thin wire 9 are arranged at a period such that a quantum effect occurs. The quantum wire structure can be realized by a metal organic chemical vapor deposition method, a metal organic chemical vapor deposition method, or a molecular beam epitaxial growth method. For details of the quantum wire structure manufacturing method, see, for example, the magazine Applied Physics Letters (Applied).
Physics Letters), Volume 50, 198
7 years, pp. 824-826, "(AlAs) 0.5 (GaAs) 0.5 fractional superlattice ((AlA) grown on (001) vicinal surface by metalorganic chemical vapor deposition.
s) 0.5 (GaAs) 0.5 fractional-lay
er superlattices grown on
(001) vicinal surface by
metal organic chemical v
Apor deposition) ". When the period of the semiconductor wire becomes small enough to cause quantum effect, the band edges are observed separately depending on the incident polarization direction. Then, as shown in FIG. 3, optical anisotropy occurs in which the reflectance and the transmittance differ depending on the polarization direction. More specifically, on a GaAs substrate whose plane orientation is the (001) plane, GaAs parallel to the [110] direction
In the quantum wire structure formed from the wires and the InAs wires,
InAs has a narrower band gap than GaAs,
Carriers are confined in the [-110] direction. Due to this carrier confinement effect, transitions involved in heavy holes and transitions involved in light holes are separated. This is because, in FIG. 2, when the electric field of the incident light is polarized light a parallel to [110], the transition involved in the heavy holes on the long wavelength side is allowed, and in the case of the vertically polarized light b, the transition is prohibited. . Therefore, the quantum wire structure can be used for the polarization selection layer of the semiconductor photodetector. The wavelength λ D having a large reflectance difference RD shown in FIG. 3 is matched with the incident light wavelength λ in . In the semiconductor photodetector designed in this way, the transmittance for the polarized light a whose polarization direction is parallel to [110] is smaller than the transmittance for the polarized light b perpendicular to [110]. Transparently. The polarized light b enters the pn junction or the pin junction, and electron-hole pairs are generated at the junction. This electron-hole pair is detected as a photocurrent generated by the reverse bias voltage applied to the junction. Based on the above principle,
It becomes possible to selectively receive an optical signal having a polarization component in a specific direction.
【0012】[0012]
【実施例】図1に本発明の半導体光検出器の構造例を示
す。InP基板1上にGaAs/InAsの量子細線周
期構造よりなる偏光選択層7、n型に不純物添加された
InP層2、不純物添加されていないInGaAs層
3、p型に不純物添加されたInGaAs層4、AuZ
n金属電極5を形成する。全ての層を形成した後、n型
InP層2までメサエッチした後、n型InP層2上に
AuGeNi金属電極6を形成する。偏光選択層7は図
2に示すように、GaAs半導体細線8とInAs半導
体細線9からなる量子細線周期構造で構成される。図3
に偏光選択層の透過率に偏光依存性を持つ波長λD を示
す。入射光波長λinと波長λD が同じになるように偏光
選択層を設計する。偏光選択層7において量子細線に平
行な偏光光の方が垂直な偏光光よりも透過率が小さいた
め、量子細線に垂直な偏光方向を持つ入力光信号を選択
的に受光することが可能となる。FIG. 1 shows an example of the structure of a semiconductor photodetector of the present invention. A polarization selection layer 7 having a GaAs / InAs quantum wire periodic structure on an InP substrate 1, an n-type doped InP layer 2, an undoped InGaAs layer 3, and a p-type doped InGaAs layer 4. , AuZ
The n metal electrode 5 is formed. After forming all layers, mesa etching is performed up to the n-type InP layer 2, and then an AuGeNi metal electrode 6 is formed on the n-type InP layer 2. As shown in FIG. 2, the polarization selection layer 7 has a quantum wire periodic structure including a GaAs semiconductor wire 8 and an InAs semiconductor wire 9. Figure 3
Shows the wavelength λ D , which has the polarization dependence on the transmittance of the polarization selection layer. The polarization selection layer is designed so that the incident light wavelength λ in and the wavelength λ D are the same. In the polarization selection layer 7, the polarized light parallel to the quantum wire has a smaller transmittance than the polarized light perpendicular to the quantum wire, so that it becomes possible to selectively receive the input optical signal having the polarization direction perpendicular to the quantum wire. .
【0013】以上に述べてきた実施例では、結晶系をI
nGaAsP系としたが、他の結晶系でもよく、偏光選
択層中の量子細線の組成や電極金属材料も上記実施例に
限られるものではない。In the embodiments described above, the crystal system is I
Although the nGaAsP system is used, other crystal systems may be used, and the composition of the quantum wires in the polarization selection layer and the electrode metal material are not limited to those in the above embodiment.
【0014】[0014]
【発明の効果】本発明により、特定の偏光方向の光を選
択的に受光する半導体光検出器を容易に得ることができ
る。According to the present invention, a semiconductor photodetector that selectively receives light of a specific polarization direction can be easily obtained.
【図1】本発明の実施例の構造を示す断面図。FIG. 1 is a sectional view showing a structure of an embodiment of the present invention.
【図2】本発明に用いる偏光選択層を示す斜視図。FIG. 2 is a perspective view showing a polarization selection layer used in the present invention.
【図3】本発明の原理を説明する図。FIG. 3 is a diagram illustrating the principle of the present invention.
【図4】従来の半導体光検出器の構造を示す断面図。FIG. 4 is a sectional view showing the structure of a conventional semiconductor photodetector.
1 InP基板 2 n−InP層 3 i−InGaAs層 4 p−InGaAs層 5 AuZn金属電極層 6 AuGeNi金属電極層 7 偏光選択層 8 GaAs半導体細線 9 InAs半導体細線 1 InP Substrate 2 n-InP Layer 3 i-InGaAs Layer 4 p-InGaAs Layer 5 AuZn Metal Electrode Layer 6 AuGeNi Metal Electrode Layer 7 Polarization Selective Layer 8 GaAs Semiconductor Fine Wire 9 InAs Semiconductor Fine Wire
Claims (2)
型半導体で構成されたpn接合を有する半導体光検出器
において、前記pn接合の光入射面側に、第1の禁制帯
幅の半導体細線と前記第1の禁制帯幅の半導体細線より
広い第2の禁制帯幅を持つ半導体細線とからなる周期構
造を有し、前記周期構造が面内方向において量子効果を
生ずる程度の周期を持つことを特徴とする半導体光検出
器。1. A p-type semiconductor and n formed on a semiconductor substrate.
A semiconductor photodetector having a pn junction composed of a semiconductor of a type, a second thin semiconductor wire having a first forbidden band width and a second semiconductor thin wire having a first forbidden band width on a light incident surface side of the pn junction. 2. A semiconductor photodetector characterized by having a periodic structure composed of a semiconductor thin wire having a forbidden band width, and having a period such that the periodic structure causes a quantum effect in an in-plane direction.
半導体を形成することによって構成されるpin接合を
有することを特徴とする請求項1に記載の半導体光検出
器。2. The semiconductor photodetector according to claim 1, further comprising a pin junction formed by forming an i-type semiconductor between the p-type semiconductor and the n-type semiconductor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4250726A JPH0677517A (en) | 1992-08-26 | 1992-08-26 | Semiconductor photodetector |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4250726A JPH0677517A (en) | 1992-08-26 | 1992-08-26 | Semiconductor photodetector |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0677517A true JPH0677517A (en) | 1994-03-18 |
Family
ID=17212139
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4250726A Withdrawn JPH0677517A (en) | 1992-08-26 | 1992-08-26 | Semiconductor photodetector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0677517A (en) |
-
1992
- 1992-08-26 JP JP4250726A patent/JPH0677517A/en not_active Withdrawn
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
A300 | Application deemed to be withdrawn because no request for examination was validly filed |
Free format text: JAPANESE INTERMEDIATE CODE: A300 Effective date: 19991102 |