JPS6351569B2 - - Google Patents
Info
- Publication number
- JPS6351569B2 JPS6351569B2 JP2684981A JP2684981A JPS6351569B2 JP S6351569 B2 JPS6351569 B2 JP S6351569B2 JP 2684981 A JP2684981 A JP 2684981A JP 2684981 A JP2684981 A JP 2684981A JP S6351569 B2 JPS6351569 B2 JP S6351569B2
- Authority
- JP
- Japan
- Prior art keywords
- ultrasonic
- cell
- light
- signal
- signal processing
- 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
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/11—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on acousto-optical elements, e.g. using variable diffraction by sound or like mechanical waves
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Description
【発明の詳細な説明】
この発明は電気信号の時間遅延、時間軸伸長、
圧縮、逆転、および、特定区間(時間)信号の抽
出を行う音響光学的電気信号処理器に関するもの
である。[Detailed Description of the Invention] This invention provides time delay, time axis extension, and
The present invention relates to an acousto-optic electrical signal processor that performs compression, inversion, and extraction of specific interval (time) signals.
従来より、レンズ系や超音波光変調器等を使用
して電気信号の実時間処理、すなわち、空間的実
時間積分やフーリエ変換などを行う音響光学的信
号処理装置がある。本発明は、これらの装置に用
いられている音響光学的信号処理部(超音波光変
調器・フーリエ変換光学系・空間フイルタ)の時
間遅延・一時的記憶特性に着目し、これを用い
て、従来、電気回路で構成すると、非常に複雑な
回路と多数の電気部品を必要としたアナログ信号
遅延回路、実時間時間軸変換処理回路を音響光学
的に構成し、簡便な時間遅延・時間軸変換器用信
号処理器を提供することを目的としている。 2. Description of the Related Art Conventionally, there have been acousto-optic signal processing devices that perform real-time processing of electrical signals, such as spatial real-time integration and Fourier transformation, using lens systems, ultrasonic light modulators, and the like. The present invention focuses on the time delay and temporary memory characteristics of the acousto-optic signal processing unit (ultrasonic light modulator, Fourier transform optical system, spatial filter) used in these devices, and uses this to Conventionally, analog signal delay circuits and real-time time axis conversion processing circuits, which required extremely complex circuits and numerous electrical components, were constructed using an acousto-optic system to provide simple time delay and time axis conversion. The purpose is to provide a dexterous signal processor.
この目的のため、本発明では、処理すべき電気
信号を超音波に変換する振動子と、この超音波に
変換された電気信号を時間的に圧縮しつつ検出す
る検出用超音波信号の振動子が、空間的に平行度
良く配置するようにし、超音波伝搬媒質として液
状物質を使用した2つの光超音波信号処理セルを
構成した。また、これら2つのセル間にセル内の
超音波信号を、超音波伝搬方向に伸長、圧縮する
レンズ7A,7Bを配置し、かつ、前記の検出用
超音波信号によつて現われる特定の出力回折光の
みを通過させる光学的空間フイルタ8を設けた。 For this purpose, the present invention includes a transducer that converts an electrical signal to be processed into an ultrasonic wave, and a transducer for a detection ultrasonic signal that detects the electrical signal converted into an ultrasonic wave while compressing it in time. However, two optical ultrasonic signal processing cells were constructed so that they were arranged spatially with good parallelism, and a liquid substance was used as the ultrasonic propagation medium. Further, lenses 7A and 7B are arranged between these two cells to expand and compress the ultrasonic signal in the cell in the ultrasonic propagation direction, and the specific output diffraction that appears by the above-mentioned detection ultrasonic signal is arranged. An optical spatial filter 8 is provided that allows only light to pass through.
つぎに、この発明を図面により具体的に説明す
る。 Next, this invention will be specifically explained with reference to the drawings.
第1図は、本発明の音響光学的電気信号処理器
の構成要素である光超音波信号処理セルおよび、
超音波伸長、圧縮用のレンズ7A,7Bの概略透
視図である。同図に示した2つのセル3,3′は
帯状平面波光(平行なレーザ光)9の通過に十分
な大きさを有する光通過窓5,5′と、前記平面
波光9の進行方向に垂直に超音波を発射する超音
波振動子1,1′、および、この振動子より発射
された超音波を吸収する超音波吸収部材2,2′
より構成されている。また超音波の伝搬媒質には
液状物質4,4′を使用し、容易に長い超音波伝
搬距離を設定することができる。また、レンズ系
は第1のセル3内に存在する超音波信号を超音波
伝搬方向長に伸長または圧縮し、第2のセル3′
に投射する。2つのセル内を進行中の超音波は伝
搬媒質密度の疎密波であるため、これらを横切つ
た前記帯状平面波光9には部分的に位相差が生
じ、レンズで集束すると回折像が現われる。 FIG. 1 shows an optical ultrasound signal processing cell, which is a component of an acousto-optic electric signal processor of the present invention, and
It is a schematic perspective view of lenses 7A and 7B for ultrasonic expansion and compression. The two cells 3 and 3' shown in the figure have light passage windows 5 and 5' that are large enough for passage of the band-shaped plane wave light (parallel laser light) 9, and a light passage window 5 and 5' that is perpendicular to the traveling direction of the plane wave light 9. Ultrasonic transducers 1, 1' that emit ultrasonic waves, and ultrasonic absorbing members 2, 2' that absorb the ultrasonic waves emitted from the transducers.
It is composed of Further, by using liquid substances 4, 4' as the ultrasonic propagation medium, it is possible to easily set a long ultrasonic propagation distance. Further, the lens system expands or compresses the ultrasonic signal existing in the first cell 3 to the length in the ultrasonic propagation direction, and
to project. Since the ultrasonic waves traveling in the two cells are compression waves of the density of the propagation medium, a phase difference occurs partially in the band-shaped plane wave light 9 that traverses them, and when focused by a lens, a diffraction image appears.
第2図は、前記光超音波信号処理セルおよびレ
ンズ系によつて電気信号を回折光に変換する光学
処理系の構成を示している。レーザ光線14は拡
大レンズ系により帯状平面波光に拡大され、第1
のセル3内を通過し、この時セル内の超音波信号
によつて位相変化を受ける。この位相変化を受け
た平面波光は、レンズ系7A,7Bを通過して超
音波進行方向に伸長、あるいは圧縮を受け、第2
のセル3′に入射する。第2のセル内で再び超音
波による位相変調を受けた平面波光はレンズ7C
で収束されて焦点面に配置した光学的空間フイル
タ8面上で結像する。このような場合、超音波信
号がセル3′のみに存在し周波数fの正弦波であ
れば回折像は輝点となり前記光学的空間フイルタ
8の光軸点より距離dだけ離れた場所に発生す
る。光軸点より回折光点の方向は、超音波信号の
進行方向に等しく、dの値は次式で表わされる。 FIG. 2 shows the configuration of an optical processing system that converts electrical signals into diffracted light using the optical ultrasonic signal processing cell and lens system. The laser beam 14 is expanded into band-shaped plane wave light by a magnifying lens system, and the first
The ultrasonic signal passes through the cell 3, and at this time undergoes a phase change due to the ultrasonic signal within the cell. The plane wave light that has undergone this phase change passes through the lens systems 7A and 7B, is expanded or compressed in the direction of ultrasound propagation, and is then
enters cell 3'. The plane wave light that has undergone phase modulation by the ultrasonic wave again in the second cell passes through the lens 7C.
The light is converged at , and an image is formed on an optical spatial filter 8 placed at the focal plane. In such a case, if the ultrasonic signal exists only in the cell 3' and is a sine wave with a frequency f, the diffraction image becomes a bright spot and is generated at a distance d from the optical axis point of the optical spatial filter 8. . The direction of the diffracted light point from the optical axis point is equal to the traveling direction of the ultrasound signal, and the value of d is expressed by the following equation.
d=λFf/v …(1)
λは光源の波長、Fはレンズ7Cの焦点距離、
vは超音波のセル3′中進行速度である。また、
回折光の強度は超音波信号振幅が小さい場合、信
号振幅の自乗に比例することが知られている。 d=λFf/v...(1) λ is the wavelength of the light source, F is the focal length of the lens 7C,
v is the speed at which the ultrasonic wave travels through the cell 3'. Also,
It is known that the intensity of the diffracted light is proportional to the square of the signal amplitude when the ultrasound signal amplitude is small.
つぎに、平面波光が周波数の異なる2つの正弦
波超音波を横切る場合を考える。この2つの超音
波が共に光軸に垂直で、かつ、互いに進行方向が
平行であれば、回折光は各々の超音波周波数を示
すものの他に、各々の周波数の和と差の周波数を
示す2点の場所に現われる。各々の周波数をf1、
f2とすれば、(1)式の場合と同様に、光軸と回折光
点の距離d(+)、d(-)はそれぞれ次式で表わされる。 Next, consider a case where plane wave light crosses two sinusoidal ultrasound waves having different frequencies. If these two ultrasonic waves are both perpendicular to the optical axis and their propagation directions are parallel to each other, the diffracted light will not only indicate the respective ultrasonic frequencies, but also the two frequencies that indicate the sum and difference of each frequency. Appears at the location of the point. Each frequency is f 1 ,
Assuming f 2 , the distances d (+) and d (-) between the optical axis and the diffracted light spot are respectively expressed by the following equations, as in the case of equation (1).
ただしkはレンズ系の拡大縮小率であり、周波
数f1の信号は第1のセル3、同f2は第2のセル
3′に入力されるものとする。回折光の強度は2
つの超音波信号振幅が小さな場合、和・差周波数
ともに、2つの超音波振幅の積の自乗に比例す
る。 Here, k is the enlargement/reduction ratio of the lens system, and the signal of frequency f 1 is input to the first cell 3, and the signal of frequency f 2 is input to the second cell 3'. The intensity of the diffracted light is 2
When two ultrasonic signal amplitudes are small, both the sum and difference frequencies are proportional to the square of the product of the two ultrasonic amplitudes.
以上の事柄より、2つの正弦波超音波の一方
を、処理すべき電気信号で振幅変調し、他方を前
記電気信号の最小周期の数分の一以下の幅を有す
る振幅値一定の矩形パルスで振幅変調すれば、(2)
式で示した、和・差周波数回折光を光学的空間フ
イルタ8で検出し光電変換することによつて前記
電気信号の時間軸を伸長、圧縮または逆転した信
号を得ることができる。この様子を第3図におけ
る本発明の実施例によつて説明する。本実施例は
動作精度と簡便化を考慮して、セル3,3′、レ
ンズ7A,7B,7C、光学的空間フイルタ8を
一体化構造としたものである。セル3に設けられ
た光通過窓5より帯状平面波光9がセル内に入射
する。この時セル3内に超音波信号が存在しなけ
れば、前記平面波光9はそのままセル3を通過
し、レンズ系7A,7Bによつて超音波進行方向
長が拡大もしくは縮小されて第2のセル3′に入
射する。セル3′では、処理すべき電気信号によ
つて振幅変調を受けた周波数f2の正弦波信号が、
電気信号入力端子6′に加えられ、超音波振動子
1′によつて超音波信号11に変換され、セル内
を矢印の方向に進行する。この超音波信号11を
横切ることによつて位相変化を受けた前記帯状平
面波光9は、レンズ7Cによつて収束しf2周波数
回折光を生ずるが、この回折光は光学的空間フイ
ルタ8で遮られ、信号処理器の外部には現われな
い。ここで、セル3に設けられた、第1の電気信
号入力端子6より、前述した、周波数f1の正弦波
信号をパルス振幅変調して加え、セル内にパルス
状の超音波信号を発射すると、第2のセル3′に
おいてこのパルス超音波信号12と空間的に光軸
方向で重なつた部分の前記超音波信号の振幅自乗
値に比例した光強度の(kf1±f2)周波数回折光
が現われる。この回折光は光学的空間フイルタ8
にあらかじめ用意した開口を通過して、信号処理
器外部に放出される。 From the above, one of the two sinusoidal ultrasonic waves is amplitude-modulated with the electrical signal to be processed, and the other is modulated with a constant amplitude rectangular pulse having a width less than a fraction of the minimum period of the electrical signal. If amplitude modulated, (2)
By detecting the sum/difference frequency diffracted light shown by the equation with the optical spatial filter 8 and photoelectrically converting it, it is possible to obtain a signal in which the time axis of the electrical signal is expanded, compressed, or reversed. This situation will be explained with reference to an embodiment of the present invention shown in FIG. In this embodiment, cells 3, 3', lenses 7A, 7B, 7C, and optical spatial filter 8 are integrated in consideration of operational accuracy and simplicity. Band-shaped plane wave light 9 enters into the cell through a light passing window 5 provided in the cell 3. At this time, if no ultrasonic signal exists in the cell 3, the plane wave light 9 passes through the cell 3 as it is, and the length in the ultrasonic traveling direction is expanded or reduced by the lens systems 7A and 7B, and the plane wave light 9 passes through the cell 3 as it is. 3'. In cell 3', a sinusoidal signal of frequency f 2 amplitude-modulated by the electrical signal to be processed is
The signal is applied to the electrical signal input terminal 6', is converted into an ultrasonic signal 11 by the ultrasonic transducer 1', and travels within the cell in the direction of the arrow. The band-shaped plane wave light 9 which has undergone a phase change by crossing this ultrasonic signal 11 is converged by the lens 7C to generate f2 frequency diffracted light, but this diffracted light is blocked by the optical spatial filter 8. and does not appear outside the signal processor. Here, if the above-mentioned sine wave signal of frequency f 1 is pulse amplitude modulated and applied from the first electrical signal input terminal 6 provided in the cell 3, a pulsed ultrasonic signal is emitted into the cell. , (kf 1 ±f 2 ) frequency diffraction of the light intensity proportional to the squared amplitude of the ultrasonic signal in a portion spatially overlapping with this pulsed ultrasonic signal 12 in the optical axis direction in the second cell 3'. Light appears. This diffracted light is filtered through an optical spatial filter 8.
The signal passes through an aperture prepared in advance and is emitted to the outside of the signal processor.
次に超音波信号11と第2のセル3′内に拡大
または縮小されて投射されたパルス超音波信号1
2の相対的な運動について考える。まず、2つの
超音波信号の動きが、第2のセル3′内において
同方向であり、かつ、レンズ系の拡大、縮小率が
1であれば、2つの超音波信号は等価的に第2の
セル3′内を等しい速度で同方向に進行する状態
となる。この時、パルス超音波信号12は、超音
波信号11の特定部分と重なつた状態を保つてセ
ル3′内を進行するため、光学的空間フイルタ8
を通過して得られる和・差周波数回折光は、超音
波信号11の特定部分の値を示す。また、この値
は前記パルス超音波信号12が第1のセル3内に
存在する時間保持され出力されることになる。よ
つて、セル3′に加えた電気信号のサンプルホー
ルドが実現できる。サンプリングの精度を高める
ためには、電気信号の最小周期の数分の1以下に
細いパルス超音波信号を使う必要がある。つぎ
に、セル3,3′の向き、あるいはレンズ系によ
つて、2つの超音波信号が第2のセル3′内で等
価的に等しい速度で互いに反対方向に進行する場
合を考える。この場合第2のセル3′内における
パルス超音波信号12の空間幅が光通過窓5の超
音波伝搬方向幅、および、処理される電気信号の
最小空間周期に比べ十分小さければ、あたかも超
音波信号11をパルス超音波信号12で走査した
形となる。この2つの超音波信号の相対速度は
各々の超音波速度の2倍であり、超音波パルスの
振幅は一定であるから前記走査で得られた信号
は、時間的に処理すべき電気信号を1/2に圧縮し
たものとなる。さらに光通過窓5前面よりレンズ
7Cまでの間に、前記パルス超音波の空間幅程度
の開口を有する光学的固定パターンフイルタを設
置すれば、ゲート機能を有する時間遅延器とな
る。すなわち、前例の時間軸圧縮に使用した、走
査用のパルス超音波をゲート制御用に使用し、パ
ルス超音波が前記光学的固定パターンフイルタの
開口部分に重なつて存在する場合に限り、回折光
が得られる構成となる。この場合、パルス超音波
の幅および周期は任意であり、処理すべき電気信
号の遅延時間は、超音波振動子1より前記固定パ
ターンの開口までの距離(固定パターンを光通過
窓5に投影した場合の距離)をセル3内の超音波
速度で割つた値となる。また、時間遅延と時間軸
圧縮を同時に行うには、前記固定パターンの開口
幅を広げ、パルス超音波を走査用に細くする方法
が考えられる。この場合、時間軸圧縮と時間遅延
はそれぞれ前例と同様の動作で行なわれ、ゲート
機能は無くなる。つぎにレンズ系の拡大、縮小率
を1以外にした場合を考える。第1のセル3内の
パルス超音波信号がレンズ系によつてk倍に拡大
され、第2のセル3′に投射された場合同セル内
でのパルス超音波信号の速度もk倍となるため、
kが1以上の場合、2つの超音波信号が同方向に
進行すればパルス超音波信号12は等価的に、セ
ル3′内において超音波信号11を追い越し走査
することになる。この場合、光学的空間フイルタ
8を通過して得られる光量の時間変化は、セル
3′に加えた電気信号の一部すなわち、2つの超
音波信号11,12の重なり合つている部分を時
間軸逆転し、かつ伸長あるいは圧縮した波形とな
る。k=2の場合は時間軸が逆転し、伸長、圧縮
は行なわれない。また、2つの超音波信号が第2
のセル3′内を等価的に互いに反対方向に進行す
れば、電気信号の時間軸圧縮が行なわれる。さら
に、kが1以下で2つの超音波信号が同方向に進
行する構成にすれば、電気信号の時間軸伸長とな
る。これら、時間軸伸長、圧縮、逆転の処理はレ
ンズ系による拡大、縮小率と、2つのセルの配置
によつて任意に行なうことができる。また、セル
内の超音波減衰による出力誤差を補正するため、
セルに入射する光束の光強度分布を光学的フイル
タで変化させれば、より精度の高い信号処理が期
待できる。この窓の部分に設けられる光学的フイ
ルタには面積形を用いてもよい。この場合には、
シリンドリカルレンズの組合せによつて断面が長
方形となる光束を使うことになりその結果光束の
有効使用率が高まる。 Next, the ultrasonic signal 11 and the pulsed ultrasonic signal 1 are enlarged or reduced and projected into the second cell 3'.
Consider the relative motion of the two. First, if the movements of the two ultrasound signals are in the same direction within the second cell 3' and the magnification/reduction ratio of the lens system is 1, then the two ultrasound signals are equivalent to the second The robots travel in the same direction at the same speed inside the cell 3'. At this time, the pulsed ultrasound signal 12 travels through the cell 3' while keeping a state overlapping with a specific portion of the ultrasound signal 11, so the optical spatial filter 8
The sum/difference frequency diffracted light obtained by passing through the ultrasonic signal 11 indicates the value of a specific portion of the ultrasound signal 11. Further, this value is held and output while the pulsed ultrasonic signal 12 is present in the first cell 3. Therefore, it is possible to sample and hold the electrical signal applied to the cell 3'. In order to improve sampling accuracy, it is necessary to use a thin pulsed ultrasonic signal that is less than a fraction of the minimum period of the electrical signal. Next, consider the case where two ultrasonic signals travel in opposite directions at equivalent speeds within the second cell 3' depending on the orientation of the cells 3, 3' or the lens system. In this case, if the spatial width of the pulsed ultrasonic signal 12 in the second cell 3' is sufficiently small compared to the width of the light passing window 5 in the ultrasonic propagation direction and the minimum spatial period of the electrical signal to be processed, it will appear as if the ultrasonic wave The signal 11 is scanned by the pulsed ultrasonic signal 12. The relative speed of these two ultrasound signals is twice the speed of each ultrasound, and since the amplitude of the ultrasound pulse is constant, the signal obtained by the scanning is equal to the electrical signal to be processed in time. It is compressed to /2. Further, if an optical fixed pattern filter having an aperture as large as the spatial width of the pulsed ultrasound is installed between the front surface of the light passing window 5 and the lens 7C, a time delay device having a gate function can be obtained. That is, the pulsed ultrasound for scanning, which was used for time axis compression in the previous example, is used for gate control, and only when the pulsed ultrasound exists overlapping the opening of the optical fixed pattern filter, the diffracted light is The configuration provides the following. In this case, the width and period of the pulsed ultrasound are arbitrary, and the delay time of the electrical signal to be processed is determined by the distance from the ultrasound transducer 1 to the aperture of the fixed pattern (the distance from the fixed pattern projected onto the light passing window 5). It is the value obtained by dividing the distance in the cell 3 by the ultrasonic velocity within the cell 3. Further, in order to perform time delay and time axis compression at the same time, it is possible to widen the aperture width of the fixed pattern and narrow the pulsed ultrasonic wave for scanning. In this case, time base compression and time delay are performed in the same manner as in the previous example, and the gate function is eliminated. Next, consider the case where the magnification and reduction ratios of the lens system are set to values other than 1. When the pulsed ultrasound signal in the first cell 3 is magnified by k times by the lens system and projected onto the second cell 3', the speed of the pulsed ultrasound signal in the same cell also becomes k times. For,
When k is 1 or more, if the two ultrasonic signals travel in the same direction, the pulsed ultrasonic signal 12 will equivalently pass and scan the ultrasonic signal 11 within the cell 3'. In this case, the temporal change in the amount of light obtained by passing through the optical spatial filter 8 is based on a time axis of a part of the electrical signal applied to the cell 3', that is, the overlapping part of the two ultrasonic signals 11 and 12. The waveform is reversed and expanded or compressed. When k=2, the time axis is reversed and no expansion or compression is performed. Also, the two ultrasonic signals are
If the electrical signals travel equivalently in opposite directions within the cell 3', the time axis of the electrical signal is compressed. Furthermore, if k is 1 or less and the two ultrasonic signals are configured to travel in the same direction, the time axis of the electrical signal will be expanded. These processes of time axis expansion, compression, and reversal can be performed arbitrarily depending on the expansion and reduction ratios of the lens system and the arrangement of the two cells. In addition, in order to correct the output error due to ultrasonic attenuation inside the cell,
If the light intensity distribution of the light beam incident on the cell is changed using an optical filter, more accurate signal processing can be expected. An area type optical filter may be used for the optical filter provided in this window portion. In this case,
The combination of cylindrical lenses allows the use of a light beam with a rectangular cross section, thereby increasing the effective utilization rate of the light beam.
本発明は以上のような構成であり、簡便な本発
明の音響光学的電気信号処理器を用いることによ
つて、電気信号の時間軸伸長、圧縮、逆転、ゲー
ト機能を有する時間遅延、さらに、これら数種の
組合せによる信号処理を実時間でアナログ的に実
行できる効果を有する。 The present invention has the above-described configuration, and by using the simple acousto-optic electric signal processor of the present invention, it is possible to extend the time axis of an electric signal, compress it, reverse it, and time delay having gate functions. It has the effect that signal processing using a combination of these several types can be executed in real time in an analog manner.
第1図は本発明に用いる光超音波信号処理セル
を示す図、第2図は本発明の光学処理系を示す
図、第3図は本発明の1実施例を示す図である。
図中の1,1′は超音波振動子、2,2′は超音
波吸収部材、3,3′はセル、4,4′は液状物
質、5,5′は光透過窓、6,6′は電気信号入力
端子、7A,7B,7C,7Dはレンズ、8は光
学的空間フイルタ、9は帯状平面波光、15は光
学的フイルタ、Aは(f1−f2)周波数回折光輝点
を示す、Bは(f1+f2)周波数回折光輝点を示
す。
FIG. 1 is a diagram showing an optical ultrasound signal processing cell used in the present invention, FIG. 2 is a diagram showing an optical processing system of the present invention, and FIG. 3 is a diagram showing one embodiment of the present invention. In the figure, 1 and 1' are ultrasonic transducers, 2 and 2' are ultrasonic absorption members, 3 and 3' are cells, 4 and 4' are liquid substances, 5 and 5' are light transmission windows, and 6 and 6 ' is an electric signal input terminal, 7A, 7B, 7C, and 7D are lenses, 8 is an optical spatial filter, 9 is a band plane wave light, 15 is an optical filter, and A is a (f 1 - f 2 ) frequency diffraction bright spot. , B indicates a (f 1 +f 2 ) frequency diffraction bright spot.
Claims (1)
部電気信号を受領して振動する1又は複数の超音
波振動子1,1′と、前記超音波振動子が設けら
れた該セルの対面に備えられ前記液状物質中を伝
搬してくる超音波を吸収するための1又は複数の
超音波吸収部材2,2′と、外部からの平行なレ
ーザ光を透過させるため該セルに設けられ、前記
超音波の伝搬経路方向に開かれた形状の光透過窓
5,5′とを有する第1および第2の超音波信号
処理セルと;前記第1および第2の超音波信号処
理セルを透過した光をそれぞれ受ける第1、第3
のレンズ7A,7Cと;該第3のレンズ7Cの焦
点位置に設けられた光学的空間フイルタ8と;前
記第2の超音波信号処理セルの受光窓側に備えら
れると共に、前記第1のレンズ7Aの出力光を受
光して平行なレーザ光線に変換する第2のレンズ
7Bとを備えた音響光学的電気信号処理器であつ
て: 前記外部からの平行なレーザ光が該第1、第2
の超音波信号処理セル内の該超音波伝搬経路に対
して垂直に通過するよう前記超音波振動子がそれ
ぞれ配置されていると共に、前記レーザ平行光線
が第1のセルを通過後、第2のセルに再び平行光
線で入射される間にその光束が広がり又は縮小さ
れるよう該第1および第2のレンズ7A,7Bが
配置されていることを特徴とする音響光学的電気
信号処理器。[Scope of Claims] 1. One or more ultrasonic transducers 1, 1' that are provided on the inner surface of a cell that holds a liquid substance and that vibrate upon receiving an external electrical signal; one or more ultrasonic absorbing members 2, 2' provided on opposite sides of the cell for absorbing ultrasonic waves propagating in the liquid substance; first and second ultrasonic signal processing cells provided in the cells and having light transmission windows 5, 5' opened in the propagation path direction of the ultrasonic waves; the first and second ultrasonic waves; a first and a third receiving the light transmitted through the signal processing cell;
lenses 7A, 7C; an optical spatial filter 8 provided at the focal position of the third lens 7C; and an optical spatial filter 8 provided on the light receiving window side of the second ultrasonic signal processing cell; an acousto-optic electrical signal processor, comprising: a second lens 7B that receives the output light of the laser beam and converts it into a parallel laser beam;
The ultrasonic transducers are respectively arranged so as to pass perpendicularly to the ultrasonic propagation path in the ultrasonic signal processing cell, and after the parallel laser beam passes through the first cell, An acousto-optic electrical signal processor characterized in that the first and second lenses 7A and 7B are arranged so that the light flux is expanded or contracted while being re-injected into the cell as a parallel light beam.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2684981A JPS57142018A (en) | 1981-02-27 | 1981-02-27 | Acoustooptic electric signal processor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2684981A JPS57142018A (en) | 1981-02-27 | 1981-02-27 | Acoustooptic electric signal processor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57142018A JPS57142018A (en) | 1982-09-02 |
| JPS6351569B2 true JPS6351569B2 (en) | 1988-10-14 |
Family
ID=12204717
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2684981A Granted JPS57142018A (en) | 1981-02-27 | 1981-02-27 | Acoustooptic electric signal processor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57142018A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05115162A (en) * | 1991-07-02 | 1993-05-07 | Ebara Corp | Squirrel-cage rotor and fabrication thereof |
-
1981
- 1981-02-27 JP JP2684981A patent/JPS57142018A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05115162A (en) * | 1991-07-02 | 1993-05-07 | Ebara Corp | Squirrel-cage rotor and fabrication thereof |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57142018A (en) | 1982-09-02 |
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