JPS593870B2 - light detection element - Google Patents
light detection elementInfo
- Publication number
- JPS593870B2 JPS593870B2 JP49084488A JP8448874A JPS593870B2 JP S593870 B2 JPS593870 B2 JP S593870B2 JP 49084488 A JP49084488 A JP 49084488A JP 8448874 A JP8448874 A JP 8448874A JP S593870 B2 JPS593870 B2 JP S593870B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- semiconductor layer
- space charge
- charge region
- junction
- 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
Links
- 238000001514 detection method Methods 0.000 title description 2
- 239000012535 impurity Substances 0.000 claims description 12
- 239000004065 semiconductor Substances 0.000 claims description 11
- 239000000758 substrate Substances 0.000 claims description 5
- 230000004888 barrier function Effects 0.000 claims description 3
- 230000031700 light absorption Effects 0.000 claims description 2
- 238000009792 diffusion process Methods 0.000 description 9
- 239000000969 carrier Substances 0.000 description 7
- 238000000034 method Methods 0.000 description 3
- 239000003990 capacitor Substances 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 1
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 230000002238 attenuated effect Effects 0.000 description 1
- 230000000903 blocking effect Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
Landscapes
- Light Receiving Elements (AREA)
Description
【発明の詳細な説明】 本発明は半導体光検出器に関するものである。[Detailed description of the invention] The present invention relates to a semiconductor photodetector.
高速の半導体光検出器として、pn接合ダイオードやシ
ョットキー障壁型ダイオードが一般に用いられている。
これらのダイオードでは逆バイアス状態で使用され、光
によつて励起されたキャリアが空間電荷領域を走行する
とき発生する電流を検出するものである。空間電荷領域
中で励起されたキャリアは、ただちに電場によつて加速
され、およそ107−少の飽和速度に達する。従つて、
例へぱ10ミクロンの空間電荷領域を有する時は走行時
間は10−10秒となり、充分高速検出が可能になる。
空間電荷領域以外で光励起されたキャリアは拡散して、
空間電荷領域端に達したものは同様に電場中を走行し信
号に寄与する。この拡散電流はキャリアの寿命が走行時
間に比べはるかに長いため、フォトダイオードの応答速
度を遅くする原因となつている。実際Siダイオードで
GaAsレーザ光やNdド5−プ固体レーザ等の長波長
光を受けるとき、光が吸収されl/8.5に減衰する距
離は40から400ミクロンにも及び空間電荷領域中に
比してはるかに大きくなる。Pn junction diodes and Schottky barrier diodes are generally used as high-speed semiconductor photodetectors.
These diodes are used in a reverse bias state to detect the current generated when carriers excited by light travel in a space charge region. Carriers excited in the space charge region are immediately accelerated by the electric field and reach a saturation velocity of approximately 10<7>. Therefore,
For example, when the space charge region is 10 microns, the travel time is 10-10 seconds, which enables sufficiently high-speed detection.
Photoexcited carriers outside the space charge region diffuse and
Those that reach the edge of the space charge region similarly travel in the electric field and contribute to the signal. This diffusion current is a cause of slowing down the response speed of the photodiode because the lifetime of carriers is much longer than the transit time. In fact, when a Si diode receives long-wavelength light such as GaAs laser light or Nd-doped solid-state laser, the distance at which the light is absorbed and attenuated to l/8.5 is 40 to 400 microns, and the distance is within the space charge region. much larger compared to
このため拡散電流の寄与が大きくなり、超高速パルス光
を忠実に復調することが困10難であつた6これに対し
、不純物濃度を下げて空間電荷領域中を拡げることによ
り拡散電流成分を軽減する方法も考えられるが、走行時
間の方が長くなるため応答速度の改善に限界があり、1
つ使用電圧が高圧になり実用性に欠けてくる。15本発
明は、このような従来のフォトダイオードの有する欠点
を除去し、高速応答する光検出素子を提供することを目
的とする。For this reason, the contribution of the diffusion current increases, making it difficult to faithfully demodulate ultrafast pulsed light6.In contrast, by lowering the impurity concentration and expanding the space charge region, the diffusion current component is reduced. Although it is possible to consider the method of
The voltage used becomes high, making it impractical. 15 An object of the present invention is to eliminate such drawbacks of conventional photodiodes and provide a photodetecting element that responds at high speed.
本発明による光検出素子はpn接合またはショットキー
障壁型フォトダイオードにおいて光吸収20領域のうら
、空間電荷領域以遠に少なくとも空間電荷領域とは逆の
導電型を有する不純物層を設け、空間電荷領域以遠で生
じる光励起キャリアの拡散を阻止することにより応答速
度の高速化を行うものである。The photodetecting element according to the present invention is a pn junction or Schottky barrier type photodiode in which an impurity layer having at least a conductivity type opposite to that of the space charge region is provided behind the light absorption region and beyond the space charge region. The response speed is increased by preventing the diffusion of photoexcited carriers that occur in the process.
25次に本発明の一実施例を図を用いて説明すれば、n
型シリコン基板1のうえにエピタキシャル成長法でp型
不純物層2を形成し層2の表面にp゛不純物層3を環状
に形成しその内部にn″′型不純物層4を形成すること
により第1のpn接合5と第3Q2のpn接合6を有す
る光検出素子が得られる。25 Next, one embodiment of the present invention will be explained using the drawings.
A p-type impurity layer 2 is formed on a type silicon substrate 1 by an epitaxial growth method, a p-type impurity layer 3 is formed in an annular shape on the surface of the layer 2, and an n''-type impurity layer 4 is formed inside the p-type impurity layer 2. A photodetecting element having the pn junction 5 of Q2 and the pn junction 6 of the third Q2 is obtained.
層2は動作状態では空間電荷領域となる領域でその巾は
空間電荷領域が逆バイアス下で層2の境界5に達しない
ように層2の不純物濃度に依存して決定される。たとえ
ば層2の不純物濃度が3×35lo15cm−3のとき
は約10ミクロンの幅とした。これにn型不純物を表面
濃度1013cm−3以上で約1ミクロンの深さまで拡
散してn1層4を形成し100Vまで逆バイアスを印加
できるフオトダイオードを得た。逆バイアスは層2の一
部に高濃度に1P型不純物を拡散した層3とn+層4の
間に負荷抵抗7と電源8を接続して第2のPn接合6の
みに印加する。約100Vの印加により層2はほぼ空間
電荷領域となり、層4の表面から入射した光により励起
されたキヤリアは飽和速度で層2中を走行し、0.2ナ
ノ秒以下の半導体レーザのパルス光を忠実に復調できた
。9は高周波信号を通すためのバイパスコンデンサーで
ある。The layer 2 is a space charge region in the operating state, the width of which is determined depending on the impurity concentration of the layer 2 so that the space charge region does not reach the boundary 5 of the layer 2 under reverse bias. For example, when the impurity concentration of layer 2 is 3x35lo15cm-3, the width is about 10 microns. An n-type impurity was diffused to a depth of about 1 micron at a surface concentration of 1013 cm-3 or higher to form an n1 layer 4, thereby obtaining a photodiode capable of applying a reverse bias of up to 100V. A reverse bias is applied only to the second Pn junction 6 by connecting a load resistor 7 and a power supply 8 between a layer 3 in which a 1P type impurity is diffused at a high concentration in a part of the layer 2 and an n+ layer 4. By applying approximately 100V, layer 2 becomes almost a space charge region, and carriers excited by light incident from the surface of layer 4 travel through layer 2 at a saturation speed, and the pulsed light of the semiconductor laser for less than 0.2 nanoseconds is generated. was able to be faithfully reconstructed. 9 is a bypass capacitor for passing high frequency signals.
層2と層1の間は外部電極10で電気的に短絡されてい
る。このため層1で励起されたキヤリアはPn接合5に
生じている拡散電位のため電子が層2とは逆方向にドリ
フトされて外部電極10により正孔と再結合して消減す
るため層2に流れ込む拡散電流がなくなる。従つて従来
のように遅い拡散電流信号が発生することはなく立下が
りの速いフオトダイオードが得られた。空間電荷領域に
入らずに残つているp層2の部分からの拡散電流は問題
とな出8,.
るが、印加電圧を制御してこの部分を充分薄くすること
により容易に全光電流のl(I)以下にでき応答速度へ
の影響を避けることができた。Layer 2 and layer 1 are electrically short-circuited by external electrode 10. For this reason, carriers excited in layer 1 drift in the opposite direction to layer 2 due to the diffusion potential generated in Pn junction 5, and are recombined with holes by external electrode 10 to be quenched. The inflowing diffusion current disappears. Therefore, a photodiode with a fast fall rate without generating a slow diffusion current signal as in the conventional case was obtained. Diffusion current from the remaining portion of the p-layer 2 that does not enter the space charge region poses a problem. However, by controlling the applied voltage and making this portion sufficiently thin, it was possible to easily reduce the total photocurrent to less than l (I) and avoid affecting the response speed.
本発明による光検出素子は以上に述べたように、フオト
ダイオードの基板として逆導電型不純物層を用いること
により速度の遅い拡散電流を阻止し超高速パルス光の復
調に効果がある。As described above, the photodetecting element according to the present invention is effective in demodulating ultrahigh-speed pulsed light by blocking slow diffusion current by using a reverse conductivity type impurity layer as the substrate of the photodiode.
尚、本発明は実施例以外に各部の導電型を逆にした構成
にしても同様であり、また他の半導体材料にも適応でき
ることは言うまでもない。It goes without saying that the present invention is the same even if the conductivity type of each part is reversed in addition to the embodiments, and can also be applied to other semiconductor materials.
図は、本発明の一実施例をその動作回路と共に説明する
ためのものである。
図中1〜4は半導体であり、1および4と2および3と
は逆導電型である。
したがつて5および6はPn48合を形成する。7は負
荷抵抗、8は電源〜9はバイパスコンデンサ、10は短
絡電極である。The drawings are for explaining one embodiment of the present invention together with its operational circuit. In the figure, 1 to 4 are semiconductors, and 1 and 4 and 2 and 3 are of opposite conductivity type. Therefore, 5 and 6 form a Pn48 bond. 7 is a load resistor, 8 is a power supply, 9 is a bypass capacitor, and 10 is a short-circuit electrode.
Claims (1)
ードにおいて、逆バイアスを印加することにより空間電
荷領域化となし、光吸収に供する半導体層と該半導体層
に接して該半導体層とは逆の導電型を示す不純物を含有
する基板層が存在し、前記半導体層と該基板層とを電気
的に短絡して動作させることを特徴とする光検出素子。1 In a PN junction or Schottky barrier type photodiode, a space charge region is created by applying a reverse bias, and a semiconductor layer used for light absorption and a semiconductor layer in contact with the semiconductor layer exhibit a conductivity type opposite to that of the semiconductor layer. 1. A photodetecting element characterized in that a substrate layer containing impurities is present, and the semiconductor layer and the substrate layer are operated by electrically shorting the semiconductor layer and the substrate layer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP49084488A JPS593870B2 (en) | 1974-07-23 | 1974-07-23 | light detection element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP49084488A JPS593870B2 (en) | 1974-07-23 | 1974-07-23 | light detection element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5112785A JPS5112785A (en) | 1976-01-31 |
| JPS593870B2 true JPS593870B2 (en) | 1984-01-26 |
Family
ID=13832026
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP49084488A Expired JPS593870B2 (en) | 1974-07-23 | 1974-07-23 | light detection element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS593870B2 (en) |
-
1974
- 1974-07-23 JP JP49084488A patent/JPS593870B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5112785A (en) | 1976-01-31 |
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