JPH04192568A - Movable photodetector - Google Patents

Movable photodetector

Info

Publication number
JPH04192568A
JPH04192568A JP2326256A JP32625690A JPH04192568A JP H04192568 A JPH04192568 A JP H04192568A JP 2326256 A JP2326256 A JP 2326256A JP 32625690 A JP32625690 A JP 32625690A JP H04192568 A JPH04192568 A JP H04192568A
Authority
JP
Japan
Prior art keywords
vibration
section
elastic deformation
light
receiving element
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
JP2326256A
Other languages
Japanese (ja)
Inventor
Yoshinori Ito
嘉則 伊藤
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.)
Omron Corp
Original Assignee
Omron Corp
Omron Tateisi Electronics Co
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 Omron Corp, Omron Tateisi Electronics Co filed Critical Omron Corp
Priority to JP2326256A priority Critical patent/JPH04192568A/en
Publication of JPH04192568A publication Critical patent/JPH04192568A/en
Pending legal-status Critical Current

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  • Mechanical Optical Scanning Systems (AREA)
  • Light Receiving Elements (AREA)

Abstract

PURPOSE:To obtain a wide detection range and to detect a direction whose optical intensity is largest by a method wherein this photodetector is composed of the following: a scanning part which can be turned in at least two directions by the elastic vibration of an elastic deformation part; and a photodetector chip installed at the scanning part. CONSTITUTION:When a vibration part 5 is vibrated by using a driving source 6, both vibrations in a twist deformation mode and in a bend deformation mode are amplified at an elastic deformation part 2, and a vibration at a turning angle thetaT around the axial center P and a vibration at a turning angle thetaB around a Q-direction are composed at a scanning part 3. As a result, the photodetection direction of a photodetector chip 4 is scanned inside a space at a definite pyramid-shaped solid angle. In addition, an output signal from the photodetector chip 4 is input to a signal processing device. Thereby, light can be detected over a wide range, and it is possible to detect a direction whose photodetection sensitivity is highest.

Description

【発明の詳細な説明】[Detailed description of the invention] 【産業上の利用分野】[Industrial application field]

本発明は、受光方向を連続的に変化させることができる
可動型の受光素子に関する。
The present invention relates to a movable light-receiving element that can continuously change the light-receiving direction.

【背景技術】[Background technology]

従来より用いられている受光素子(フォトトランジスタ
)51を第6図に示す。これは、シリコン基板に形成さ
れた受光素子チップ(図示せず)を素子本体であるリー
ドフレーム52やステム上に実装し、樹脂でモールドし
てレンズ53付きの樹脂ケース54内に納めたり、窓付
きキャップでシールドしたものである。 第7図(a)は、受光素子51の受光方向(指向角φ)
と受光感度(相対感度)との関係の一例を示している。 ここで、指向角φは、第7図(b)に示すように受光素
子51の中心を基準に定められた角度である。このよう
に、受光素子51は、−般に指向性の強い受光感度を有
している。
A conventionally used light receiving element (phototransistor) 51 is shown in FIG. This is done by mounting a light-receiving element chip (not shown) formed on a silicon substrate on a lead frame 52 or stem that is the element body, molding it with resin and housing it in a resin case 54 with a lens 53, or It is shielded with a cap. FIG. 7(a) shows the light receiving direction (direction angle φ) of the light receiving element 51.
An example of the relationship between and light receiving sensitivity (relative sensitivity) is shown. Here, the directivity angle φ is an angle determined with the center of the light receiving element 51 as a reference, as shown in FIG. 7(b). In this way, the light receiving element 51 generally has a highly directional light receiving sensitivity.

【発明が解決しようとする課題】[Problem to be solved by the invention]

受光素子は、上記のように一般に強い指向性を有してい
るため、広い範囲を検出させることができず、広い検出
範囲を得ようとすれば、複雑な光学系を追加し、この光
学系を透過させた光を受光素子へ入射させる必要があり
、全体としての形状が大型化し、また検出範囲の拡大に
も限度があった。あるいは、複数個の受光素子を方向を
異なら−せて配置してもよいが、その場合には受光感度
の低い部分(盲点)をなくそうとすれば、非常に多数の
受光素子が必要となり、全体の形状も大きくならざるを
得なかった。 さらに、受光感度が最大となる方向を検出させようとす
れば、受光素子を機械的な駆動装置の可動部に取付け、
当該駆動装置によって受光素子の受光方向をあらゆる方
向へ変化させなければならず、全体的な形状が大型にな
るという問題があった。 本発明は叙上の従来例の欠点に鑑みてなされたものであ
り、その目的とするところは、指向性を有する受光素子
チップを用いて広い検出範囲を得ることができ、さらに
光強度の最も大きな方向を検出することができる小型の
受光素子を提供することにある。
As mentioned above, the light-receiving element generally has strong directivity, so it cannot detect a wide range.If you want to obtain a wide detection range, you need to add a complicated optical system and use this optical system. It is necessary to make the transmitted light enter the light-receiving element, which increases the overall size and limits the expansion of the detection range. Alternatively, multiple light-receiving elements may be arranged in different directions, but in that case, in order to eliminate areas with low light-receiving sensitivity (blind spots), a very large number of light-receiving elements would be required. The overall shape also had to become larger. Furthermore, in order to detect the direction in which the light receiving sensitivity is maximum, the light receiving element is attached to the movable part of the mechanical drive device.
The light receiving direction of the light receiving element must be changed in all directions by the driving device, and there is a problem in that the overall shape becomes large. The present invention was made in view of the drawbacks of the conventional examples described above, and its purpose is to obtain a wide detection range using a directional light-receiving element chip, and furthermore, to obtain the maximum detection range of light intensity. An object of the present invention is to provide a small-sized light receiving element that can detect large directions.

【課題を解決するための手段】[Means to solve the problem]

本発明の可動型受光素子は、少なくとも2つの弾性変形
モードを有する弾性変形部と、弾性変形部の一端に設け
られた加振部と、前記弾性変形部の各弾性変形モードに
対する共振周波数の振動を加振部に付与するための駆動
源と、弾性変形部の他端に設けられ、加振部に振動が印
加された時に少なくともいずれかの弾性変形モードで弾
性変形部を弾性振動させるように配置され、弾性変形部
の弾性振動によって少なくとも2方向に回動できるよう
になったスキャン部と、スキャン部に設けられた受光素
子チップとからなることを特徴としている。
The movable light receiving element of the present invention includes an elastic deformation section having at least two elastic deformation modes, an excitation section provided at one end of the elastic deformation section, and vibrations at a resonant frequency for each elastic deformation mode of the elastic deformation section. a drive source for applying the vibration to the vibrating part, and a drive source provided at the other end of the elastic deformation part, so as to elastically vibrate the elastic deformation part in at least one of the elastic deformation modes when vibration is applied to the vibration part. It is characterized in that it consists of a scanning section that is arranged so that it can rotate in at least two directions by elastic vibration of an elastically deformable section, and a light-receiving element chip provided in the scanning section.

【作用】[Effect]

弾性変形部の2つの弾性変形モードに対する共振周波数
の振動を加振部に加えると、弾性変形部が両弾性変形モ
ードで弾性振動し、スキャン部が2方向で同時に回動す
る。このため、スキャン部に設けられた受光素子チップ
の受光方向は、一定の角度(立体角)領域内で連続的に
変化し、指向性を有する1個の受光素子チップを用いて
も広い範囲の光を検出させることができる。さらに、指
向性を有する受光素子チップの方向を連続的に変化させ
ることにより、単体で光強度の最も大きな方向(受光感
度が最大となる方向)を検出することができる。 また、スキャン部、弾性変形部及び加振部は、プレート
状に形成することかでき、駆動源としては圧電振動子の
ような小型のアクチュエータを使用することができるの
で、上記のような機能を有する可動型受光素子を小形化
することができる。 さらに、駆動源によって加振部の振幅を変化させれば、
弾性変形部における弾性振動の振幅(スキャン部の回動
角)を変化させることができ、容易に受光領域ないし受
光範囲の大ぎさを調整することもできる。
When vibrations at resonance frequencies for two elastic deformation modes of the elastic deformation section are applied to the vibrating section, the elastic deformation section vibrates elastically in both elastic deformation modes, and the scanning section rotates in two directions simultaneously. For this reason, the light receiving direction of the light receiving element chip provided in the scanning section changes continuously within a certain angular (solid angle) region, and even if one light receiving element chip with directivity is used, it can cover a wide range. Light can be detected. Furthermore, by continuously changing the direction of the light-receiving element chip having directivity, it is possible to detect the direction in which the light intensity is greatest (the direction in which the light-receiving sensitivity is maximum) by itself. In addition, the scanning section, elastic deformation section, and vibration section can be formed into plate shapes, and a small actuator such as a piezoelectric vibrator can be used as the drive source, so the above functions can be achieved. The movable light-receiving element can be downsized. Furthermore, if the amplitude of the vibrating part is changed depending on the driving source,
The amplitude of the elastic vibration in the elastic deformation section (the rotation angle of the scanning section) can be changed, and the size of the light receiving area or the light receiving range can be easily adjusted.

【実施例】【Example】

以下、本発明の実施例を添付図に基づいて詳述する。 第1図(a)(b)に本発明の一実施例を示す。この可
動型受光素子7は、薄板状のプレート1と、圧電振動子
や磁歪振動子等の微小振動を発生する小形の駆動源6と
、フォトダイオードチップ等の受光素子チップ4とから
構成されている。プレート1は、長い細幅の弾性変形部
2の下端に、駆動源6から振動を印加させるための加振
部5が一体に設けられ、弾性変形部2の上端にスキャン
部3が一体に設けられている。ここで、弾性変形部2は
、第1図(a)に示すように軸心Pの回りにねじれ変形
するねじれ変形モードと、第1図(b)に示すように軸
心Pに沿って曲げ変形する曲げ変形モードが可能になっ
ており、ねじれ変形モードの弾性振動についてはfTの
共振周波数を有し、曲げ変形モードの弾性振動について
はfaの共振周波数を有している。スキャン部3は、弾
性変形部2の軸心Pに関してアンバランスな形状に形成
されており、弾性変形部2の軸心Pから離れた部分にウ
ェイト部8が形成されている。したがって、スキャン部
3の重心は、弾性変形部2の軸心Pから外れた位置にあ
り、さらに、弾性変形部2の上端よりも上方に位置して
いる。また、スキャン部3の表面には、指向性の強い1
個の受光素子チップ4が取り付けられている。加振部5
は、圧電振動子等の駆動源6に接着もしくは接合されて
駆動源6に固定されており、スキャン部3は弾性変形部
2によってフリーに支持されている。 加振部5へ高周波振動(例えば、数100 Hz)を加
える圧電振動子等の駆動源6は、駆動回路によって制御
されており、ねじれ変形モードの共振周波数f7及び曲
げ変形モードの共振周波数faの振動を励起される。第
3図に示すものは、この駆動回路9の一例であり、ねじ
れ変形モードの共振周波数fアと一致する周波数の電圧
信号を出力し続けている発振器lOと、発振器10から
出力されている電圧信号を増幅する増幅器11と、曲げ
変形モードの共振周波数f’aと一致する周波数の電圧
信号を出力し続けている発振器12と、この発振器12
から出力されている電圧信号を増幅する増幅器13と、
両増幅器11.13から出力された周波数fTの電圧信
号と周波数faの電圧信号を重畳させて出力するミキシ
ング回路14とから構成されている。 しかして、本発明に係る可動型受光素子7は、上述のよ
うに構成されているので、駆動回路9番こよって駆動源
6を振動させ、この振動を加振部5に印加させて往復振
動させると、スキャン部3に慣性力が作用し、この慣性
力によって弾性変形部2は、慣性力の加わった方向に弾
性変形し振動する。しかも、加振部5に印加される駆動
周波数fの成分が、弾性変形部2のばね剛性や慣性モー
メントの値、プレート7の形状等から決まるねじれ変形
モードの共振周波数fTまたは曲げ変形モードの共振周
波数f8に一致すると、当該モードの弾性振動が弾性変
形部2で増幅され、スキャン部3が大きな回動角で駆動
される。すなわち、駆動周波数f(成分)とスキャン部
3のねじれ変形モードの回動角θ7または曲げ変形モー
ドの回動角θ8との関係は、例えば第2図に示すように
なる。 第2図は、2つの共振周波数がfi<foの場合におけ
る、駆動源6の駆動周波数fとスキャン部3の回動角と
の関係を示しており、横軸が駆動周波数f、縦軸がスキ
ャン部3のねじれ変形モードの回動角θアまたは曲げ変
形モードの回動角θ8を示している。このようにねじれ
変形モードにおける回動角θ7は、駆動周波数fがfT
に等しい時に最大となり、その両側では急激に減衰する
。一方、曲げ変形モードにおける回動角θ8は、駆動周
波数fがfaに等しい時に最大となり、その両側で急激
に減衰する。したがって、圧電振動子のように微小振動
しか行なえないような駆動源6であっても、各弾性変形
モードの共振周波数と等しい周波数で駆動させることに
より、スキャン部3を大きな角度で回動させることがで
きる。 よって、加振部5に印加される電圧にねじれ変形モード
の共振周波数ftが含まれていると、弾性変形部2でね
じれ変形モードの振動が増幅され、スキャン部3は第1
図(a)に示すようにθ1の回動角で軸心Pの回りに回
動させられる。したがって、受光素子チップ4の受光方
向はX方向にスキャンされる。 また、加振部5に印加される電圧に曲げ変形モードの共
振周波数fBか含まれていると、弾性変形部2で曲げ変
形モードの振動が増幅され、スキャン部3は第1図(b
)に示すようにθ8の回動角で軸心Pと直交する方向Q
の回りに回動させられる。 したがって、受光素子チップ4の受光方向はX方向にス
キャンされる。 従って、駆動源6により、ねじれ変形モードの共振周波
数f、をもつ振動と曲げ変形モードの共振周波数f。を
もつ振動とを重ね合わせた振動モードで加振部5を振動
させると、弾性変形部2でねしれ変形モードと曲げ変形
モードの両振動が増幅され、スキャン部3では軸心2回
りの回動角θ、の振動とQ方向の回りの回動角θ、の振
動とが合成される。この結果、受光素子チップ4の受光
方向は、角錐状をした一定の立体角の空間内でスキャン
され、指向性の強い1個の受光素子チップ4を用いて広
い範囲にわたって光を受光ないし検出させることができ
る。さらに、この受光素子チップ4からの出力信号を信
号処理装置(図示せず)へ入力させることにより、最も
光強度の大きな方向(受光感度か最大の方向)を知るこ
とができる。 また、駆動源6に印加する電圧を調整することにより加
振部5の振幅を変化させると、スキャン部3の回動角θ
7もしくはθ3を制御することかできる。すなわち、第
2図の破線で示した曲線は、実線で示した曲線よりも大
きな振幅で加振部5を振動させた場合であり、加振部5
の振幅が大きくなると、スキャン部3の回動角θ7.θ
8も増大する。従って、受光素子チップ4の受光範囲も
印加電圧によって変化させることができる。 なお、上述の説明では、P軸回りの回動運動とQ軸回り
の回動運動を同時に行わせる場合について説明したが、
駆動回路によってP軸回り又はQ軸回りの一方の回動運
動だけを行わせてもよい。 第4図(a) (b)に示すものは本発明の別な実施例
であって、上記可動型受光素子7を用いて検出面15の
角度を検出できるようにしたものである。 すなわち、検圧面15に半導体レーザや発光ダイオード
等の投光素子16を固定し、投光素子16から検出面1
5に垂直な方向へ光を出射させ、スキャン部3及び受光
素子チップ4の角度θと受光素子チップ4の検出信号と
を同期させてあり、受光素子チップ4の受光強度が最大
となった時の角度θから検出面15の角度を知るもので
ある。具体的にいうと、第5図(a)は第4図(a)に
示すようにθ7の回動角でスキャン部3がP軸の回りに
回動運動している時のスキャン部3の角度θを表わして
おり(スキャン部3の非駆動時の方向をθ−〇としてい
る。)、第5図(1))はスキャン部3の角度変化と同
期させて検出されている受光素子チップ4の検出信号の
強度Wの変化を示している。 受光素子チップ4の受光信号の強度Wが最大値Wmax
の時、受光素子チップ4は投光素子16の方向(あるい
は、検出面15と垂直な方向)を向いているから、強度
Wか最大値Wmaxの時のスキャン部3の角度θmを知
れば、検出面15の角度を知ることができる。同様にし
て、第4図(b)のようにQ軸のまわりで回転している
検出面15の角度も知ることができる。 なお、上記のような方法ではスキャン部3の非駆動時の
方向に誤差が含まれる恐れがある場合には、基準方向を
向けて検出面15を配置し、その時検出信号の強度Wが
最大となるスキャン部角度を測定しておけば、当該方向
を基準として検出面15の角度な知ることができ、検出
面15の測定精度を向上させることができる。 なお、本発明の可動型受光素子は、上記実施例に限定さ
れるものでなく、本発明の技術思想を逸脱しない範囲に
おいて種々の設計変更が可能である。例えば、駆動源と
しては、圧電振動子や磁歪振動子等以外にも、高速で微
小振動可能なアクチュエータであればよく、例えば静電
力を用いて微小振動を発生させるアクチュエータを用い
てもよい。また、図示したプレートの形状は一例であっ
て、2種以上の弾性変形モードを得ることができる形状
であれば図示の形状に限らない。 【発明の効果〕 本発明によれば、圧電振動子のような駆動源の振動を弾
性変形部によってスキャン部における少なくとも2方向
の回動運動に変換させることができ、受光素子チップの
受光方向を広い空間領域にわたってスキャニングさせる
ことができる。従って、指向性を有する受光素子チップ
を用いて、複雑な光学系を用いることなく、広い範囲に
おいて光を検出することができる。また、指向性を有す
る単体の受光素子チップを用いて受光感度の最も高い方
向を検出することがでとる。 しかも、本発明によれば、上記のような機能を備えた受
光素子を小型化することができる。 さらに、加振部の振幅を調整することにより、スキャン
部の各スキャン角を変化させることができ、1個の受光
素子によって受光方向を任意の空間領域で走査させるこ
とができる。
Embodiments of the present invention will be described in detail below with reference to the accompanying drawings. An embodiment of the present invention is shown in FIGS. 1(a) and 1(b). This movable light receiving element 7 is composed of a thin plate 1, a small drive source 6 such as a piezoelectric vibrator or a magnetostrictive vibrator that generates minute vibrations, and a light receiving element chip 4 such as a photodiode chip. There is. In the plate 1, an excitation part 5 for applying vibration from a drive source 6 is integrally provided at the lower end of a long narrow elastic deformation part 2, and a scanning part 3 is integrally provided at the upper end of the elastic deformation part 2. It is being Here, the elastic deformation section 2 has a torsional deformation mode in which it twists and deforms around the axis P as shown in FIG. A bending deformation mode is enabled, and the elastic vibration in the torsional deformation mode has a resonance frequency of fT, and the elastic vibration in the bending deformation mode has a resonance frequency of fa. The scan section 3 is formed in an unbalanced shape with respect to the axis P of the elastically deformable section 2, and the weight section 8 is formed in a portion away from the axis P of the elastically deformable section 2. Therefore, the center of gravity of the scanning section 3 is located away from the axis P of the elastically deformable section 2, and is further located above the upper end of the elastically deformable section 2. In addition, on the surface of the scanning unit 3, there is a highly directional 1
A number of light receiving element chips 4 are attached. Vibrating part 5
is fixed to the drive source 6 such as a piezoelectric vibrator by adhesion or bonding, and the scanning section 3 is freely supported by the elastic deformation section 2 . A drive source 6 such as a piezoelectric vibrator that applies high-frequency vibration (for example, several hundred Hz) to the vibrator 5 is controlled by a drive circuit, and has a resonance frequency f7 in a torsional deformation mode and a resonance frequency fa in a bending deformation mode. Excited vibrations. What is shown in FIG. 3 is an example of this drive circuit 9, which includes an oscillator lO that continues to output a voltage signal with a frequency that matches the resonance frequency fa of the torsional deformation mode, and a voltage that is output from the oscillator 10. An amplifier 11 that amplifies a signal, an oscillator 12 that continues to output a voltage signal with a frequency that matches the resonance frequency f'a of the bending deformation mode, and this oscillator 12
an amplifier 13 that amplifies the voltage signal output from the
It consists of a mixing circuit 14 that superimposes the voltage signal of frequency fT output from both amplifiers 11 and 13 and the voltage signal of frequency fa and outputs the superimposed voltage signal. Since the movable light-receiving element 7 according to the present invention is configured as described above, the drive circuit 9 causes the drive source 6 to vibrate, and this vibration is applied to the vibrator 5 to cause reciprocating vibration. When this happens, an inertial force acts on the scanning section 3, and this inertial force causes the elastic deformation section 2 to elastically deform and vibrate in the direction in which the inertial force is applied. Moreover, the component of the driving frequency f applied to the vibrating section 5 is the resonance frequency fT of the torsional deformation mode or the resonance frequency of the bending deformation mode, which is determined by the spring stiffness of the elastic deformation section 2, the value of the moment of inertia, the shape of the plate 7, etc. When the frequency matches f8, the elastic vibration of the mode is amplified by the elastic deformation section 2, and the scanning section 3 is driven at a large rotation angle. That is, the relationship between the drive frequency f (component) and the rotation angle θ7 in the torsional deformation mode or the rotation angle θ8 in the bending deformation mode of the scanning section 3 is as shown in FIG. 2, for example. FIG. 2 shows the relationship between the drive frequency f of the drive source 6 and the rotation angle of the scanning unit 3 when the two resonance frequencies fi<fo, where the horizontal axis is the drive frequency f and the vertical axis is the rotation angle of the scanning unit 3. The rotation angle θa in the torsional deformation mode or the rotation angle θ8 in the bending deformation mode of the scanning section 3 is shown. In this way, the rotation angle θ7 in the torsional deformation mode is determined by the drive frequency f being fT.
It reaches its maximum when it is equal to , and rapidly attenuates on both sides. On the other hand, the rotation angle θ8 in the bending deformation mode reaches a maximum when the drive frequency f is equal to fa, and rapidly attenuates on both sides thereof. Therefore, even if the driving source 6 is a piezoelectric vibrator that can only produce minute vibrations, it is possible to rotate the scanning unit 3 by a large angle by driving it at a frequency equal to the resonance frequency of each elastic deformation mode. I can do it. Therefore, when the voltage applied to the vibrating section 5 includes the resonance frequency ft of the torsional deformation mode, the vibration of the torsional deformation mode is amplified in the elastic deformation section 2, and the scanning section 3
As shown in Figure (a), it is rotated around the axis P at a rotation angle of θ1. Therefore, the light receiving direction of the light receiving element chip 4 is scanned in the X direction. Furthermore, if the voltage applied to the vibrating section 5 includes the resonant frequency fB of the bending deformation mode, the vibration of the bending deformation mode is amplified in the elastic deformation section 2, and the scanning section 3 is
), the direction Q perpendicular to the axis P at a rotation angle of θ8
can be rotated around. Therefore, the light receiving direction of the light receiving element chip 4 is scanned in the X direction. Therefore, the driving source 6 causes vibrations having a resonance frequency f in the torsional deformation mode and a resonance frequency f in the bending deformation mode. When the excitation unit 5 is vibrated in a vibration mode in which vibrations with The vibration at the moving angle θ and the vibration at the rotation angle θ around the Q direction are combined. As a result, the light-receiving direction of the light-receiving element chip 4 is scanned within a pyramid-shaped space of a constant solid angle, and one light-receiving element chip 4 with strong directivity is used to receive or detect light over a wide range. be able to. Furthermore, by inputting the output signal from the light-receiving element chip 4 to a signal processing device (not shown), it is possible to know the direction in which the light intensity is greatest (the direction in which the light-receiving sensitivity is greatest). Furthermore, when the amplitude of the vibrating section 5 is changed by adjusting the voltage applied to the drive source 6, the rotation angle θ of the scanning section 3
7 or θ3 can be controlled. That is, the curve shown by the broken line in FIG.
When the amplitude of θ7. increases, the rotation angle θ7. θ
8 also increases. Therefore, the light receiving range of the light receiving element chip 4 can also be changed by changing the applied voltage. In addition, in the above explanation, the case where the rotational movement around the P-axis and the rotational movement around the Q-axis are performed simultaneously,
The drive circuit may perform rotational movement only around the P axis or around the Q axis. 4(a) and 4(b) show another embodiment of the present invention, in which the angle of the detection surface 15 can be detected using the movable light-receiving element 7. That is, a light emitting element 16 such as a semiconductor laser or a light emitting diode is fixed to the pressure detection surface 15, and the light emitting element 16 is connected to the detection surface 1.
5, and the angle θ of the scanning unit 3 and the light receiving element chip 4 is synchronized with the detection signal of the light receiving element chip 4, and when the light receiving intensity of the light receiving element chip 4 reaches the maximum. The angle of the detection surface 15 is known from the angle θ. Specifically, FIG. 5(a) shows the state of the scanning section 3 when the scanning section 3 is rotating around the P axis at a rotation angle of θ7 as shown in FIG. 4(a). The angle θ is shown (the direction when the scanning unit 3 is not driven is θ−〇), and FIG. 4 shows a change in the strength W of the detection signal of No. 4. The intensity W of the light reception signal of the light receiving element chip 4 is the maximum value Wmax
At this time, the light receiving element chip 4 faces the direction of the light emitting element 16 (or the direction perpendicular to the detection surface 15), so if we know the angle θm of the scanning unit 3 when the intensity W is the maximum value Wmax, The angle of the detection surface 15 can be known. Similarly, the angle of the detection surface 15 rotating around the Q-axis as shown in FIG. 4(b) can also be determined. Note that in the above method, if there is a possibility that an error may be included in the direction of the scanning unit 3 when it is not driven, the detection surface 15 should be placed facing the reference direction, so that the intensity W of the detection signal is at its maximum. By measuring the scanning section angle, the angle of the detection surface 15 can be known with respect to the direction, and the accuracy of measurement of the detection surface 15 can be improved. The movable light-receiving element of the present invention is not limited to the above embodiments, and various design changes can be made without departing from the technical idea of the present invention. For example, the drive source may be any actuator capable of high-speed micro-vibration in addition to piezoelectric vibrators, magnetostrictive vibrators, etc. For example, an actuator that generates micro-vibration using electrostatic force may be used. Further, the illustrated shape of the plate is only an example, and the plate is not limited to the illustrated shape as long as it can obtain two or more types of elastic deformation modes. Effects of the Invention According to the present invention, the vibration of a drive source such as a piezoelectric vibrator can be converted into rotational movement in at least two directions in the scanning section by the elastic deformation section, and the light receiving direction of the light receiving element chip can be changed. Scanning can be performed over a wide spatial area. Therefore, light can be detected in a wide range using a light receiving element chip having directivity without using a complicated optical system. Furthermore, it is possible to detect the direction in which the light receiving sensitivity is highest using a single light receiving element chip having directivity. Moreover, according to the present invention, a light receiving element having the above-mentioned functions can be miniaturized. Further, by adjusting the amplitude of the vibrating section, each scan angle of the scanning section can be changed, and a single light receiving element can scan an arbitrary spatial region in the light receiving direction.

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

第1図(a) (b)は本発明の一実施例であって、第
1図(a)はそのねじれ変形モードを示す斜視図、第1
図(b)はその曲げ変形モードを示す斜視図、第2図は
駆動周波数とスキャン部の回動角との関係を示す図、第
3図は同上の駆動源を駆動させるための駆動回路を示す
ブロック図、第4図(a)(b)は本発明の別な実施例
であって、第4図(a)はそのねじれ変形モードを示す
斜視図、第4図(b)はその曲げ変形モードを示す斜視
図、第5図はスキャン部の角度の変化と受光素子チップ
の検出信号の強度の変化のようすを示す図、第6図は従
来例の概略斜視図、第7図(a)は同上の受光素子の受
光方向(指向角)と受光感度との関係を示す図、第7図
(b)は第7図(a)の指向角の説明図である。 2・・・弾性変形部 3・・・スキャン部 4・・・受光素子チップ 5・・・加振部 6・・・駆動源
FIGS. 1(a) and 1(b) show one embodiment of the present invention, and FIG. 1(a) is a perspective view showing its torsional deformation mode;
Figure (b) is a perspective view showing the bending deformation mode, Figure 2 is a diagram showing the relationship between the drive frequency and the rotation angle of the scanning section, and Figure 3 is a diagram showing the drive circuit for driving the same drive source. The block diagram shown in FIG. 4(a) and FIG. 4(b) are another embodiment of the present invention, in which FIG. 4(a) is a perspective view showing its torsional deformation mode, and FIG. 4(b) is a perspective view showing its bending mode. FIG. 5 is a perspective view showing the deformation mode, FIG. ) is a diagram showing the relationship between the light-receiving direction (directivity angle) and light-receiving sensitivity of the light-receiving element, and FIG. 7(b) is an explanatory diagram of the directivity angle in FIG. 7(a). 2... Elastic deformation part 3... Scanning part 4... Light receiving element chip 5... Vibrating part 6... Drive source

Claims (1)

【特許請求の範囲】[Claims] (1)少なくとも2つの弾性変形モードを有する弾性変
形部と、 弾性変形部の一端に設けられた加振部と、 前記弾性変形部の各弾性変形モードに対する共振周波数
の振動を加振部に付与するための駆動源と、 弾性変形部の他端に設けられ、加振部に振動が印加され
た時に少なくともいずれかの弾性変形モードで弾性変形
部を弾性振動させるように配置され、弾性変形部の弾性
振動によって少なくとも2方向に回動できるようになっ
たスキャン部と、スキャン部に設けられた受光素子チッ
プとからなることを特徴とする可動型受光素子。
(1) an elastic deformation section having at least two elastic deformation modes; an excitation section provided at one end of the elastic deformation section; and a vibration at a resonant frequency for each elastic deformation mode of the elastic deformation section applied to the excitation section. a drive source provided at the other end of the elastic deformation section and arranged to elastically vibrate the elastic deformation section in at least one of the elastic deformation modes when vibration is applied to the vibrating section; 1. A movable light-receiving element comprising a scanning part that can be rotated in at least two directions by elastic vibration, and a light-receiving element chip provided in the scanning part.
JP2326256A 1990-11-27 1990-11-27 Movable photodetector Pending JPH04192568A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2326256A JPH04192568A (en) 1990-11-27 1990-11-27 Movable photodetector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2326256A JPH04192568A (en) 1990-11-27 1990-11-27 Movable photodetector

Publications (1)

Publication Number Publication Date
JPH04192568A true JPH04192568A (en) 1992-07-10

Family

ID=18185741

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2326256A Pending JPH04192568A (en) 1990-11-27 1990-11-27 Movable photodetector

Country Status (1)

Country Link
JP (1) JPH04192568A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100686081B1 (en) * 2006-02-14 2007-02-26 엘지전자 주식회사 Micro Mirror Device and Display Using Same
WO2009093162A1 (en) * 2008-01-24 2009-07-30 Koninklijke Philips Electronics N.V. Sensor device with tilting or orientation-correcting photo sensor for atmosphere creation

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100686081B1 (en) * 2006-02-14 2007-02-26 엘지전자 주식회사 Micro Mirror Device and Display Using Same
WO2009093162A1 (en) * 2008-01-24 2009-07-30 Koninklijke Philips Electronics N.V. Sensor device with tilting or orientation-correcting photo sensor for atmosphere creation
US8471188B2 (en) 2008-01-24 2013-06-25 Koninlijke Philips Electronics N.V. Sensor device with tilting or orientation-correcting photo sensor for atmosphere creation

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