JPH04326024A - Photoelectric conversion device - Google Patents

Photoelectric conversion device

Info

Publication number
JPH04326024A
JPH04326024A JP9660491A JP9660491A JPH04326024A JP H04326024 A JPH04326024 A JP H04326024A JP 9660491 A JP9660491 A JP 9660491A JP 9660491 A JP9660491 A JP 9660491A JP H04326024 A JPH04326024 A JP H04326024A
Authority
JP
Japan
Prior art keywords
voltage
photoelectric conversion
parallel resonator
current
parallel
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
JP9660491A
Other languages
Japanese (ja)
Inventor
Koji Shinomiya
巧治 篠宮
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP9660491A priority Critical patent/JPH04326024A/en
Publication of JPH04326024A publication Critical patent/JPH04326024A/en
Pending legal-status Critical Current

Links

Landscapes

  • Amplifiers (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Measurement Of Optical Distance (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Abstract

PURPOSE:To enable the picking up of an electric signal alone selectively as obtained by photoelectric conversion of light energy with a specified frequency in a photoelectric conversion device. CONSTITUTION:A parallel resonator 11 which performs a frequency selection and a current-voltage conversion of a photoelectric conversion current with a photoelectric conversion element 1 is provided with a voltage limiter circuit 12 in parallel. Thus, a voltage alone by light with a specified frequency can be picked up selectively by the setting of a resonance frequency of the parallel resonator 11. Thus, also allows the limiting of a voltage generated by the parallel resonator 11 to a moderate level thereby enabling the prevention of malfunction, breakage of a circuit element and the like otherwise caused by the voltage generated by the parallel resonator 11 as it becomes excessive.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】この発明は、カメラなどにおける
光を用いた自動焦点装置,測距装置や遠隔制御装置,通
信装置等に適用される光電変換装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a photoelectric conversion device applied to automatic focusing devices using light in cameras, distance measuring devices, remote control devices, communication devices, and the like.

【0002】0002

【従来の技術】図11は従来の光電変換装置の結線図で
あり、フォトダイオードからなる光電変換素子1のカソ
ードが直流電圧源2の正端子に接続され、この直流電圧
源2の負端子が接地され、光電変換素子1のアノードと
接地との間に電流・電圧変換用の抵抗3が接続され、光
電変換素子1のアノードと出力端子4との間に増幅器5
が設けられている。
2. Description of the Related Art FIG. 11 is a wiring diagram of a conventional photoelectric conversion device, in which the cathode of a photoelectric conversion element 1 consisting of a photodiode is connected to the positive terminal of a DC voltage source 2, and the negative terminal of this DC voltage source 2 is connected to the positive terminal of a DC voltage source 2. A resistor 3 for current/voltage conversion is connected between the anode of the photoelectric conversion element 1 and the ground, and an amplifier 5 is connected between the anode of the photoelectric conversion element 1 and the output terminal 4.
is provided.

【0003】そして、光電変換素子1が光を受光して発
生される光電変換電流は光電変換素子1,抵抗3を通っ
て接地へと流れ、抵抗3の電圧降下により電流・電圧変
換され、この抵抗3の電圧降下が増幅器5により増幅さ
れて出力端子4に出力電圧として現われる。
The photoelectric conversion current generated when the photoelectric conversion element 1 receives light flows to the ground through the photoelectric conversion element 1 and the resistor 3, and is converted into a current and a voltage by the voltage drop across the resistor 3. The voltage drop across the resistor 3 is amplified by the amplifier 5 and appears at the output terminal 4 as an output voltage.

【0004】このとき、直流電圧源2により光電変換素
子1が逆バイアスされているため、光電変換素子1の空
乏層が広がって接合容量が小さくなり、その結果応答性
が良好になって周波数特性が向上する。
At this time, since the photoelectric conversion element 1 is reverse biased by the DC voltage source 2, the depletion layer of the photoelectric conversion element 1 expands and the junction capacitance becomes smaller, resulting in better response and frequency characteristics. will improve.

【0005】[0005]

【発明が解決しようとする課題】しかし、上記した従来
の光電変換装置の場合、光電変換素子1は受光したすべ
ての光エネルギーを電流に変換し、この光電変換素子1
による光電変換電流を抵抗3によって電流・電圧変換し
ているため、太陽光や人工的な照明光などいろいろな周
波数の光を検出することになる。
However, in the case of the conventional photoelectric conversion device described above, the photoelectric conversion element 1 converts all the received light energy into electric current, and the photoelectric conversion element 1
Since the photoelectric conversion current is converted into current and voltage by the resistor 3, light of various frequencies such as sunlight and artificial illumination light can be detected.

【0006】一方、カメラ等の自動焦点装置や測距装置
などでは、光源から所定の変調を加えた特定周波数の信
号光を発し、対象物により反射されてくる信号光を受光
し検出することによって、自動焦点合わせや測距等を行
うが、従来の光電変換装置は上記のように特定周波数の
信号以外の不要な光も一緒に受光してしまうため、所望
の信号光成分だけを取り出すことができないという問題
点があった。
On the other hand, automatic focusing devices such as cameras, distance measuring devices, etc. emit signal light of a specific frequency that has been modulated in a predetermined manner from a light source, and then receive and detect the signal light reflected by an object. , automatic focusing, distance measurement, etc. are performed, but as mentioned above, conventional photoelectric conversion devices receive unnecessary light as well as signals of specific frequencies, making it difficult to extract only the desired signal light component. The problem was that it couldn't be done.

【0007】この発明は、上記のような問題点を解消す
るためになされたもので、特定周波数の光エネルギーを
光電変換して得られる電気信号だけを選択的に取り出せ
るようにすることを目的とする。
[0007] This invention was made to solve the above-mentioned problems, and its purpose is to make it possible to selectively extract only electrical signals obtained by photoelectrically converting optical energy of a specific frequency. do.

【0008】[0008]

【課題を解決するための手段】この発明に係る光電変換
装置は、光を受光して光電変換電流を発生する光電変換
素子と、前記光電変換電流の周波数選択及び電流・電圧
変換を行う並列共振器と、前記並列共振器に並列に接続
された電圧制限回路とを備えたことを特徴としている。
[Means for Solving the Problems] A photoelectric conversion device according to the present invention includes a photoelectric conversion element that receives light and generates a photoelectric conversion current, and a parallel resonance device that performs frequency selection and current/voltage conversion of the photoelectric conversion current. and a voltage limiting circuit connected in parallel to the parallel resonator.

【0009】[0009]

【作用】この発明においては、光電変換素子による光電
変換電流の周波数選択及び電流・電圧変換を行う並列共
振器に、電圧制限回路を並列に設けたため、光電変換素
子により各種の周波数成分を含む種々雑多な外来光を伴
う光を受光しても、並列共振器の共振周波数の設定によ
って特定周波数の光による電圧だけが選択的に取り出さ
れると共に、並列共振器の発生電圧を適度なレベルに制
限することが可能になり、並列共振器の発生電圧が過大
になることによる誤動作や回路素子の破損等が防止され
る。
[Operation] In this invention, a voltage limiting circuit is provided in parallel with the parallel resonator that performs frequency selection of photoelectric conversion current and current/voltage conversion by the photoelectric conversion element. Even when receiving light accompanied by miscellaneous external light, only the voltage due to light at a specific frequency is selectively extracted by setting the resonant frequency of the parallel resonator, and the voltage generated by the parallel resonator is limited to an appropriate level. This makes it possible to prevent malfunctions and damage to circuit elements due to excessive voltage generated by the parallel resonators.

【0010】0010

【実施例】図1はこの発明の光電変換装置の第1の実施
例の結線図である。
DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a wiring diagram of a first embodiment of a photoelectric conversion device according to the present invention.

【0011】ところで、図2はこの発明の背景となる光
電変換装置の結線図であり、上記した図11における抵
抗3に代わり、コイル11aとコンデンサ11bとから
なる並列共振器11が、光電変換素子1のアノードと接
地との間に設けられ、光電変換装置が構成されている。
By the way, FIG. 2 is a wiring diagram of a photoelectric conversion device which is the background of the present invention, and instead of the resistor 3 in FIG. It is provided between the anode of No. 1 and ground, and constitutes a photoelectric conversion device.

【0012】このような光電変換装置をカメラの自動焦
点装置や測距装置等に適用する場合に、信号光用光源と
して、一定周期で輝度が強弱するもの、或いは、一定周
期で点灯,消灯を繰り返すものを使用し、このように周
期を一定とすることによって輝度の強弱或いは点灯,消
灯の周波数が一定となり、一定周波数の信号光を光源か
ら発するようにする。
[0012] When such a photoelectric conversion device is applied to an automatic focusing device of a camera, a distance measuring device, etc., the light source for the signal light may be one whose brightness increases or decreases at regular intervals, or one that turns on and off at regular intervals. By using a repeating device and making the period constant in this way, the intensity of brightness or the frequency of turning on and off becomes constant, and a signal light of a constant frequency is emitted from the light source.

【0013】このとき、並列共振器11の共振周波数が
上記した信号光の周波数などに等しくなるように、コイ
ル11aのインダクタンス,コンデンサ11bの容量を
設定しておく。
At this time, the inductance of the coil 11a and the capacitance of the capacitor 11b are set so that the resonant frequency of the parallel resonator 11 is equal to the frequency of the signal light described above.

【0014】そして、光電変換素子1により各種の周波
数成分を含む種々雑多な外来光と共に上記の光源からの
信号光を受光すると、光電変換素子1による光電変換電
流が並列共振器11を流れるが、並列共振器11の共振
周波数が信号光の周波数と同じ値に設定されているため
、光電変換電流のうち信号光による電流成分に対して並
列共振器11は高インピーダンスとなり、信号光以外の
電流成分に対しては低インピーダンスとなり、並列共振
器11の両端間の電圧降下は信号光以外の電流成分に対
して極めて小さく電圧は発生せず、信号光の電流成分に
対して高インピーダンスの並列共振器11による電圧降
下によって電圧が発生し、増幅器5を介して出力端子4
に信号光の電流成分による出力電圧が現われる。
When the photoelectric conversion element 1 receives the signal light from the light source as well as various miscellaneous external lights containing various frequency components, a photoelectric conversion current by the photoelectric conversion element 1 flows through the parallel resonator 11. Since the resonant frequency of the parallel resonator 11 is set to the same value as the frequency of the signal light, the parallel resonator 11 has a high impedance with respect to the current component due to the signal light in the photoelectric conversion current, and current components other than the signal light The voltage drop across the parallel resonator 11 is extremely small with respect to current components other than the signal light, and no voltage is generated. A voltage is generated due to the voltage drop caused by 11, and is passed through the amplifier 5 to the output terminal 4.
An output voltage due to the current component of the signal light appears.

【0015】ところが、上記したように、並列共振器1
1はその共振周波数と同じ周波数の電流に対しては高イ
ンピーダンスとなり、異なる周波数の電流に対しては低
インピーダンスとなり、このときのインピーダンス変化
は並列共振器11のQによって決定されるが、Qが大き
い場合には、共振時における並列共振器11の両端間電
圧は非常に大きな値になり、誤動作や回路素子の破損な
どを招くおそれがある。
However, as mentioned above, the parallel resonator 1
1 has a high impedance for a current with the same frequency as its resonant frequency, and a low impedance for a current with a different frequency, and the impedance change at this time is determined by the Q of the parallel resonator 11. If it is large, the voltage between both ends of the parallel resonator 11 during resonance becomes a very large value, which may cause malfunction or damage to circuit elements.

【0016】そこでこの発明においては、図1に示すよ
うに、並列共振器11に並列に、アノードが互いに接続
された2個のダイオード12a,12bからなる電圧制
限回路12を接続している。
Therefore, in the present invention, as shown in FIG. 1, a voltage limiting circuit 12 consisting of two diodes 12a and 12b whose anodes are connected to each other is connected in parallel to the parallel resonator 11.

【0017】このように、並列共振器11に並列に電圧
制限回路12を接続することによって、並列共振器11
の発生電圧を適度なレベルに制限することが可能になり
、図1の場合、ダイオードの順方向電圧をVF ,逆方
向のブレークダウン電圧をBVR とすると、電圧制限
回路12により、並列共振器11の発生電圧はVL (
=VF +BVR )に制限される。
In this way, by connecting the voltage limiting circuit 12 in parallel to the parallel resonator 11, the parallel resonator 11
In the case of FIG. 1, if the forward voltage of the diode is VF and the reverse breakdown voltage is BVR, the voltage limiting circuit 12 controls the parallel resonator 11. The generated voltage is VL (
=VF +BVR).

【0018】従って、電圧制限回路12により並列共振
器11の発生電圧を適度に制限できるため、並列共振器
11の発生電圧が過大になることによる誤動作や回路素
子の破損などを防止することができる。
Therefore, since the voltage generated by the parallel resonator 11 can be appropriately limited by the voltage limiting circuit 12, it is possible to prevent malfunctions and damage to circuit elements due to excessive voltage generated by the parallel resonator 11. .

【0019】つぎに、図3ないし図10はこの発明の第
2ないし第9の実施例の一部の結線図であり、図1にお
ける電圧制限回路の変形例である。
Next, FIGS. 3 to 10 are partial wiring diagrams of second to ninth embodiments of the present invention, which are modified examples of the voltage limiting circuit in FIG. 1.

【0020】図3においては、互いに逆方向に並列に接
続された2個のダイオード13a,13bにより電圧制
限回路13を構成しており、このとき並列共振器11の
発生電圧はVF に制限される。
In FIG. 3, a voltage limiting circuit 13 is constituted by two diodes 13a and 13b connected in parallel in opposite directions, and at this time, the voltage generated by the parallel resonator 11 is limited to VF. .

【0021】図4においては、抵抗14aとこれにカソ
ードが接続されたダイオード14bとにより電圧制限回
路14を構成しており、このとき抵抗14aによる電圧
降下分をVR とすると、並列共振器11の発生電圧は
VL1(=VR +VF )またはVL2(=VR +
BVR )に制限される。
In FIG. 4, a voltage limiting circuit 14 is constituted by a resistor 14a and a diode 14b whose cathode is connected to the resistor 14a.If the voltage drop due to the resistor 14a is VR, then the voltage of the parallel resonator 11 is The generated voltage is VL1 (=VR +VF) or VL2 (=VR +
BVR).

【0022】また、図5においては、電圧制限回路を抵
抗15により構成し、図6においては、電圧制限回路を
ダイオード16により構成しており、図5の場合、並列
共振器11の発生電圧は抵抗15の電圧降下分であるV
R に制限され、図6の場合、並列共振器11の発生電
圧はダイオード16の順方向電圧VF または逆方向ブ
レークダウン電圧BVR に制限される。
Further, in FIG. 5, the voltage limiting circuit is composed of a resistor 15, and in FIG. 6, the voltage limiting circuit is composed of a diode 16. In the case of FIG. 5, the voltage generated by the parallel resonator 11 is V which is the voltage drop of the resistor 15
In the case of FIG. 6, the voltage generated by the parallel resonator 11 is limited to the forward voltage VF of the diode 16 or the reverse breakdown voltage BVR.

【0023】一方、図7においては、4個のダイオード
17a,17b,17c,17dを設け、ダイオード1
7aのアノードとダイオード17bのカソードを接続し
、ダイオード17b,17cのアノードを互いに接続し
、ダイオード17cのカソードとダイオード17dのア
ノードを接続して電圧制限回路17を構成しており、こ
のような電圧制限回路17により、並列共振器11の発
生電圧はVL (=2VF +2BVR )に制限され
る。
On the other hand, in FIG. 7, four diodes 17a, 17b, 17c, and 17d are provided, and diode 1
The voltage limiting circuit 17 is configured by connecting the anode of the diode 7a and the cathode of the diode 17b, connecting the anodes of the diodes 17b and 17c to each other, and connecting the cathode of the diode 17c and the anode of the diode 17d. The limiting circuit 17 limits the voltage generated by the parallel resonator 11 to VL (=2VF +2BVR).

【0024】さらに、図8においては、順方向に接続さ
れた3個のダイオード18a,18b,18cの直列回
路と、同様に順方向に接続された3個のダイオード18
d,18e,18fの直列回路とを、互いに逆方向に並
列接続して電圧制限回路18を構成しており、このとき
並列共振器11の発生電圧は3VF 又は3BVR に
制限される。
Furthermore, in FIG. 8, a series circuit of three diodes 18a, 18b, 18c connected in the forward direction, and a series circuit of three diodes 18 similarly connected in the forward direction are shown.
A voltage limiting circuit 18 is constructed by connecting the series circuits d, 18e, and 18f in parallel in opposite directions, and at this time, the voltage generated by the parallel resonator 11 is limited to 3VF or 3BVR.

【0025】また、図9に示すように、図8におけるダ
イオード18a,18bのアノードそれぞれと、ダイオ
ード18d,18eのカソードそれぞれとを接続して電
圧制限回路19を構成してもよく、このときの並列共振
器11の発生電圧は図8の場合と同様に3VF 又は3
BVR に制限される。
Further, as shown in FIG. 9, the voltage limiting circuit 19 may be configured by connecting the anodes of the diodes 18a and 18b and the cathodes of the diodes 18d and 18e in FIG. The voltage generated by the parallel resonator 11 is 3VF or 3 as in the case of FIG.
Limited to BVR.

【0026】さらに、図10においては、互いに逆方向
に並列に接続された2個のダイオード20a,20bの
逆並列回路と、同様の2個のダイオード20c,20d
の逆並列回路とを抵抗20eにより接続して電圧制限回
路20を構成しており、このとき並列共振器11の発生
電圧はVL3(=2VF +VR )又はVL4(=2
BVR +VR )に制限される。
Furthermore, in FIG. 10, an anti-parallel circuit of two diodes 20a and 20b connected in parallel in opposite directions, and two similar diodes 20c and 20d are shown.
A voltage limiting circuit 20 is constructed by connecting the anti-parallel circuit of
BVR +VR).

【0027】従って、上記第2ないし第9の実施例にお
いては、それぞれ第1の実施例と同様の効果を得ること
ができ、各々の電圧制限値が異なることから、制限すべ
きレベルに応じた電圧制限回路を選択すればよい。
Therefore, in the second to ninth embodiments described above, the same effects as in the first embodiment can be obtained, and since each voltage limit value is different, the voltage limit value can be adjusted according to the level to be limited. Just select a voltage limiting circuit.

【0028】なお、上記実施例では光電変換素子として
フォトダイオードを用いた場合について説明したが、光
電変換素子は特にこれに限るものではなく、フォトトラ
ンジスタ,太陽電池など光により超電力を発生するもの
であればよい。
[0028] In the above embodiment, a case was explained in which a photodiode was used as a photoelectric conversion element, but the photoelectric conversion element is not limited to this, and may be a phototransistor, solar cell, or other device that generates superpower by light. That's fine.

【0029】さらに、図1,図3,図6,図7,図8,
図9では、ダイオードの組み合わせの例について示した
が、使用するダイオードの数と接続段数は、制限すべき
設定電圧に応じて適宜選定すればよい。
Furthermore, FIGS. 1, 3, 6, 7, 8,
Although FIG. 9 shows an example of a combination of diodes, the number of diodes used and the number of connected stages may be appropriately selected depending on the set voltage to be limited.

【0030】[0030]

【発明の効果】以上のように、この発明によれば、光電
変換素子による光電変換電流の周波数選択及び電流・電
圧変換を行う並列共振器に、電圧制限回路を並列に設け
たため、並列共振器の共振周波数の設定によって特定周
波数の光による電圧だけを選択的に取り出すことができ
ると共に、電圧制限回路により、並列共振器の発生電圧
を制限して、並列共振器の発生電圧が過大になることに
よる誤動作や回路素子の破損等を防止することができ、
自動焦点装置,測距装置などに好適である。
As described above, according to the present invention, since a voltage limiting circuit is provided in parallel to the parallel resonator that performs frequency selection of the photoelectric conversion current by the photoelectric conversion element and current/voltage conversion, the parallel resonator By setting the resonant frequency of the resonant frequency, it is possible to selectively extract only the voltage due to light of a specific frequency, and the voltage limiting circuit limits the voltage generated by the parallel resonator, thereby preventing the voltage generated by the parallel resonator from becoming excessive. This can prevent malfunctions and damage to circuit elements caused by
Suitable for automatic focusing devices, distance measuring devices, etc.

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

【図1】この発明の光電変換装置の第1の実施例の結線
図である。
FIG. 1 is a wiring diagram of a first embodiment of a photoelectric conversion device of the present invention.

【図2】この発明の背景となる光電変換装置の結線図で
ある。
FIG. 2 is a wiring diagram of a photoelectric conversion device, which is the background of the present invention.

【図3】この発明の第2の実施例の一部の結線図である
FIG. 3 is a partial wiring diagram of a second embodiment of the invention.

【図4】この発明の第3の実施例の一部の結線図である
FIG. 4 is a partial wiring diagram of a third embodiment of the invention.

【図5】この発明の第4の実施例の一部の結線図である
FIG. 5 is a partial wiring diagram of a fourth embodiment of the invention.

【図6】この発明の第5の実施例の一部の結線図である
FIG. 6 is a partial wiring diagram of a fifth embodiment of the invention.

【図7】この発明の第6の実施例の一部の結線図である
FIG. 7 is a partial wiring diagram of a sixth embodiment of the invention.

【図8】この発明の第7の実施例の一部の結線図である
FIG. 8 is a partial wiring diagram of a seventh embodiment of the present invention.

【図9】この発明の第8の実施例の一部の結線図である
FIG. 9 is a partial wiring diagram of an eighth embodiment of the invention.

【図10】この発明の第9の実施例の一部の結線図であ
る。
FIG. 10 is a partial wiring diagram of a ninth embodiment of the present invention.

【図11】従来の光電変換装置の結線図である。FIG. 11 is a wiring diagram of a conventional photoelectric conversion device.

【符号の説明】[Explanation of symbols]

1    光電変換素子 11  並列共振器 12,13,14,17,18,19,20  電圧制
限回路 15  抵抗(電圧制限回路) 16  ダイオード(電圧制限回路)
1 Photoelectric conversion element 11 Parallel resonator 12, 13, 14, 17, 18, 19, 20 Voltage limiting circuit 15 Resistor (voltage limiting circuit) 16 Diode (voltage limiting circuit)

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  光を受光して光電変換電流を発生する
光電変換素子と、前記光電変換電流の周波数選択及び電
流・電圧変換を行う並列共振器と、前記並列共振器に並
列に接続された電圧制限回路とを備えたことを特徴とす
る光電変換装置。
1. A photoelectric conversion element that receives light and generates a photoelectric conversion current, a parallel resonator that selects the frequency of the photoelectric conversion current and performs current/voltage conversion, and a parallel resonator that is connected in parallel to the parallel resonator. A photoelectric conversion device characterized by comprising a voltage limiting circuit.
JP9660491A 1991-04-26 1991-04-26 Photoelectric conversion device Pending JPH04326024A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9660491A JPH04326024A (en) 1991-04-26 1991-04-26 Photoelectric conversion device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9660491A JPH04326024A (en) 1991-04-26 1991-04-26 Photoelectric conversion device

Publications (1)

Publication Number Publication Date
JPH04326024A true JPH04326024A (en) 1992-11-16

Family

ID=14169476

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9660491A Pending JPH04326024A (en) 1991-04-26 1991-04-26 Photoelectric conversion device

Country Status (1)

Country Link
JP (1) JPH04326024A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006333019A (en) * 2005-05-25 2006-12-07 Nippon Telegr & Teleph Corp <Ntt> Photoelectric conversion circuit

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006333019A (en) * 2005-05-25 2006-12-07 Nippon Telegr & Teleph Corp <Ntt> Photoelectric conversion circuit

Similar Documents

Publication Publication Date Title
US5252820A (en) Photoelectric conversion circuit having a tuning circuit and changeover switcher
JPS6024410B2 (en) Photoelectric conversion circuit
FR2701612A1 (en) A method of controlling the power applied to a resonant inverter.
JPH04326024A (en) Photoelectric conversion device
KR940000851B1 (en) Fiber optic receiving circuit
JPH05300042A (en) Photoelectric conversion circuit
US4642453A (en) Apparatus for increasing the dynamic range in an integrating optoelectric receiver
EP0401911B1 (en) Switching device
WO1999003218A1 (en) Data reception circuit for infrared signals
EP0486021B1 (en) Optical receiver
JP2005072924A (en) Photoelectric current and voltage converting circuit
JPH04326023A (en) Photoelectric conversion device
CN220983503U (en) Laser radar
JP2543612B2 (en) Light receiving device
CN107612543A (en) Automatic Power Adjust circuit applied to optic communication
JPS5947249B2 (en) Optical signal receiver
GB2194406A (en) Optical signal receiver circuits
KR200201153Y1 (en) Electtronic relay for preventing over current
SU1425752A1 (en) Device for receiving pulsed signals
CN207490901U (en) Automatic Power Adjust circuit applied to optic communication
JPS60117930A (en) Photo-electric conversion circuit
JPH04282872A (en) Photoelectric conversion circuit
JPS5920299B2 (en) Photoelectric conversion circuit
SU1705751A1 (en) Device for control of grounding
SU1198500A1 (en) Device for protection of a.c.power source