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JPS6351570B2 - - Google Patents
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JPS6351570B2 - - Google Patents

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Publication number
JPS6351570B2
JPS6351570B2 JP2685081A JP2685081A JPS6351570B2 JP S6351570 B2 JPS6351570 B2 JP S6351570B2 JP 2685081 A JP2685081 A JP 2685081A JP 2685081 A JP2685081 A JP 2685081A JP S6351570 B2 JPS6351570 B2 JP S6351570B2
Authority
JP
Japan
Prior art keywords
ultrasonic
cell
electrical signal
acousto
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
Application number
JP2685081A
Other languages
Japanese (ja)
Other versions
JPS57142019A (en
Inventor
Koichiro Myagi
Yoshiaki Shimoda
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.)
Anritsu Corp
Original Assignee
Anritsu 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 Anritsu Corp filed Critical Anritsu Corp
Priority to JP2685081A priority Critical patent/JPS57142019A/en
Publication of JPS57142019A publication Critical patent/JPS57142019A/en
Publication of JPS6351570B2 publication Critical patent/JPS6351570B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/11Devices 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、および、特定区間(時間)信号の抽出を行う
音響光学的な電気信号処理器に関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an acousto-optic electrical signal processor that performs time delay, time axis expansion and compression of electrical signals, 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、実時間時間軸伸長圧縮回路を音響光学
的に構成し、簡便な時間遅延・時間軸伸長圧縮器
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 expansion/compression 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 expansion. The present invention aims to provide a signal processor for a compressor.

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を、空間的に平行度
良く対向、あるいは同方向に配置し、超音波伝搬
媒質として超音波伝搬速度の異なるいくつかの液
体物質を透明仕切板で分離した光超音波信号処理
セルを構成し、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. are arranged spatially facing each other with good parallelism or in the same direction, and constitute an optical ultrasound signal processing cell in which several liquid substances with different ultrasound propagation velocities are separated by a transparent partition plate as ultrasound propagation media, In addition, an optical spatial filter was provided that allows only specific output diffracted light appearing by the detection ultrasonic signal 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3,3′
の概略透視図である。本セルは帯状平面波光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
媒質には伝搬速度の異なる2種類の液状物質4,
4′を透明仕切板10にて分離使用し、容易に長
い超音波伝搬距離を設定することが可能である。
本セル内に進行する2つの超音波は伝搬媒質密度
の疎密波であるため、これ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 optical ultrasonic signal processing cells 3 and 3' which are the components of the acousto-optic electrical signal processor of the present invention.
FIG. This cell has light passing windows 5, 5' having a size sufficient for passage of band-shaped plane wave light 9,
It is composed of ultrasonic transducers 1 and 1' that emit ultrasonic waves perpendicular to the traveling direction of the plane wave light 9, and ultrasonic absorbing members 2 and 2' that absorb the ultrasonic waves emitted from the transducers. There is. In addition, there are two types of liquid substances with different propagation speeds4 as propagation media for ultrasonic waves.
It is possible to easily set a long ultrasonic propagation distance by separating the ultrasonic waves 4' with a transparent partition plate 10.
Since the two ultrasonic waves traveling in this cell 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3,3′
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はレンズ系
により帯状平面波光に拡大され、セル3,3′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、レンズ7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
の時、セル3にのみ超音波信号が存在し、その周
波数がf1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 optical ultrasound signal processing cells 3, 3'
This figure shows the configuration of an optical processing system that converts electrical signals into diffracted light. The laser beam 14 is expanded into band-shaped plane wave light by a lens system, passes through the cells 3 and 3', undergoes a phase change due to the ultrasonic signal in the cell, and is converged by the lens 7 and placed on the focal plane. The image is formed on eight optical spatial filters. At this time, if the ultrasonic signal exists only in the cell 3 and its frequency is a sine wave of f1 , 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. do. 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=λFf1/v1 …(1) λは光源の波長、Fはレンズ7の焦点距離、v1
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 1 /v 1 ...(1) λ is the wavelength of the light source, F is the focal length of the lens 7, v 1
is the traveling speed of the ultrasonic wave in the cell 3. Furthermore, 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、セル3,3′内に各々周波数の異なる
正弦波超音波が存在する場合を考える。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 the case where sinusoidal ultrasonic waves having different frequencies exist in the cells 3 and 3'. 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. Assuming that the respective frequencies are f 1 and 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).

(2)式におけるv2はセル3′内の超音波進行速度
である。また、回折光の強度は、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。
v 2 in equation (2) is the ultrasonic traveling speed within the cell 3'. Furthermore, the intensity of the diffracted light is proportional to the square of the product of two ultrasonic amplitudes, both at the sum and difference frequencies.

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、また、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
号の時間軸伸長、圧縮を実現することができる。
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7、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。処理すべき電気信号によつて振幅
変調を受けた周波数f1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7によつて収束しf1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2の電気信号入力端子
6′より、前述した、周波数f2の正弦波信号をパ
ルス振幅変調して加え、セル内にパルス状で振幅
が一定の超音波信号を発射すると、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
の和および差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。
超音波信号11とパルス超音波信号12はそれぞ
れ速度v1、v2でセル中を進行しているため、セル
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
が速度(v1〜v2)で走査した形となる。この2つ
の超音波信号の相対速度の大きさおよび符号によ
り、超音波パルスの振幅は一定であることから前
記走査で得られた信号は、時間的に処理すべき電
気信号を伸長、圧縮したものとなる。すなわち、
セル3内の超音波進行速度v1より、セル3′の同
速度v2が小さな場合、出力光量の変化は、セル3
の端子6に加えた電気信号の時間軸を伸長した波
形を示す。この時の時間軸伸長率Keはv1、v2
用いて、 Ke=v1/v1−v2(v1>v2) …(3) で表わされる。また、v2がv1より大きな場合、パ
ルス超音波信号12は超音波信号11を追い越し
走査する形となり、時間軸の逆転が生ずる。v1
v2<2v1の場合、伸長逆転であり、2v1<v2の場
合、圧縮逆転となる。v2=2v1の場合には、単に
波形の逆転のみである。次に、第3図に示した構
成とは異なり、2つの振動子1,1′が互いに対
向する形で配置された場合を考える。この場合に
は、時間軸圧縮動作のみが行なわれ、圧縮率Kc
はv1、v2を用いて次式で表わされる。
Based on the above, one of the two sinusoidal ultrasonic waves is amplitude-modulated with the electrical signal to be processed, and the other is amplitude-modulated with a rectangular pulse having a width less than a fraction of the minimum period of the electrical signal. Then, by detecting the sum/difference frequency diffracted light by the optical spatial filter 8 and photoelectrically converting it as shown in equation (2), time axis expansion and compression of the electrical signal can be realized.
This situation will be explained with reference to an embodiment of the present invention shown in FIG. In this embodiment, the cells 3, 3', the lens 7, and the optical spatial filter 8 are integrated in consideration of operational precision and simplicity. Band-shaped plane wave light 9 enters into the cell through a light passing window 5 provided in the cell 3. A sine wave signal of frequency f 1 that has been amplitude-modulated by the electrical signal to be processed is applied to the electrical signal input terminal 6, converted to an ultrasound signal 11 by the ultrasound transducer 1, and transmitted inside the cell. Proceed in the direction of the arrow. The band-shaped plane wave light 9 undergoes a phase change by crossing this ultrasonic signal 11,
It is converged by the lens 7 to produce f 1 frequency diffracted light, but this diffracted light is blocked by the optical spatial filter 8 and does not appear outside the signal processor. here,
The above-mentioned sinusoidal wave signal of frequency f 2 is pulse-amplitude modulated and applied from the second electric signal input terminal 6' provided in the cell 3', and a pulse-like ultrasonic signal with a constant amplitude is generated in the cell. When emitted, a sum of light intensities and a difference frequency diffracted light proportional to the squared amplitude of the ultrasonic signal appear in a portion spatially overlapping with the pulsed ultrasonic signal 12 in the optical axis direction. This diffracted light passes through an aperture prepared in advance in the optical spatial filter 8 and is emitted to the outside of the signal processor.
Since the ultrasonic signal 11 and the pulsed ultrasonic signal 12 are traveling through the cell at velocities v 1 and v 2 respectively, the spatial width of the pulsed ultrasonic signal 12 within the cell is equal to the width of the light passing window 5 in the ultrasonic propagation direction. , and if it is sufficiently small compared to the minimum spatial period of the electrical signal to be processed, then
As if the ultrasonic signal 11 were the pulsed ultrasonic signal 12
is scanned at a speed (v 1 to v 2 ). Since the amplitude of the ultrasound pulse is constant depending on the magnitude and sign of the relative velocity of these two ultrasound signals, the signal obtained by the scanning is an expanded and compressed electrical signal to be processed in time. becomes. That is,
When the ultrasonic traveling speed v 1 in cell 3 is smaller than the same speed v 2 in cell 3', the change in the output light amount is
The waveform of the electric signal applied to the terminal 6 of 2 is shown with the time axis expanded. The time axis expansion rate Ke at this time is expressed as Ke = v1 / v1 - v2 ( v1 > v2 ) (3 ) using v1 and v2 . Furthermore, when v 2 is larger than v 1 , the pulsed ultrasound signal 12 scans past the ultrasound signal 11, causing a reversal of the time axis. v 1
When v 2 < 2v 1 , it is expansion inversion, and when 2v 1 < v 2 , it is compression inversion. In the case of v 2 = 2v 1 , the waveform is simply reversed. Next, consider a case in which two vibrators 1 and 1' are arranged opposite to each other, unlike the configuration shown in FIG. In this case, only the time axis compression operation is performed, and the compression ratio K c
is expressed by the following equation using v 1 and v 2 .

Kc=1+v2/v1 …(4) 以上が時間軸に関する処理動作の説明である
が、さらに、光通過窓5前面よりレンズ7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
口までの距離をセル3内の超音波速度v1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。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。さらに、セルを
第3図に示したような透明仕切板を用いた一体化
構造とせず、第4図に示すような、単体に分離し
て作成し、これらの光軸および超音波進行方向を
一致させて用いる方法等も考えられる。この場合
には、処理すべき電気信号の特性(周波数、周期
等)に合わせたセルを適宜選択して使用可能な長
所がある。
K c = 1 + v 2 / v 1 ...(4) The above is an explanation of the processing operation regarding the time axis, but furthermore, between the front surface of the light passing window 5 and the lens 7, there is an aperture approximately the same as the spatial width of the pulsed ultrasound. If you install an optical fixed pattern filter with
It becomes a time delay device with gate function. 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 varying the distance from the ultrasound transducer 1 to the opening of the fixed pattern with the ultrasound velocity v 1 in the cell 3. The divided value is the value. 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. In order to correct output errors due to ultrasonic attenuation within the cell, more accurate signal processing can be expected if the light intensity distribution of the light beam incident on the cell is changed using an optical filter. An area type optical filter may be used for the optical filter provided in this window portion. In this case, a light beam whose cross section is rectangular is used due to the combination of cylindrical lenses, and as a result, the effective usage rate of the light beam is increased. Furthermore, instead of making the cell an integrated structure using a transparent partition plate as shown in Fig. 3, it was made separately as shown in Fig. 4, and these optical axes and ultrasonic propagation directions were A method of matching and using them may also be considered. In this case, there is an advantage that cells suitable for the characteristics (frequency, period, etc.) of the electrical signal to be processed can be appropriately selected and used.

本発明は以上のような構成であり、簡便な本発
明の音響光学的な電気信号処理器を用いることに
よつて、電気信号の時間軸圧縮、ゲート機能を有
する時間遅延、さらに、これら2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 compress the time axis of electric signals, time delay having a gate function, and further achieve these two types. This has the effect of allowing signal processing to be performed in analog fashion in real time by combining the following.

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

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、第4図
は単体セルによる構成例を示す図である。 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、7はレンズ、8は光学的空間フイルタ、9
は帯状平面波光、10は透明仕切板、11は超音
波信号、12はパルス超音波信号、Aは和周波数
回折光輝点を示す、Bは差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, FIG. 3 is a diagram showing one embodiment of the present invention, and FIG. FIG. 3 is a diagram showing an example of a configuration using a single cell. 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, 7 is a lens, 8 is an optical spatial filter, 9
10 is a band-shaped plane wave light, 10 is a transparent partition plate, 11 is an ultrasound signal, 12 is a pulsed ultrasound signal, A is a sum frequency diffraction bright spot, and B is a difference frequency diffraction bright spot.

Claims (1)

【特許請求の範囲】 1 液状物質をその内部に保つセルの内側面に設
けられ、外部電気信号を受領して振動する1また
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また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
設けられ該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、前記複数の超音波振動子
による当該複数の超音波伝搬経路を所定数で区分
するため(所定数−1)個備えられた透明仕切板
10とを有する超音波信号処理セルと;前記超音
波信号処理セルの出力光を受けるレンズ7と;該
レンズの焦点位置に設けられた光学的空間フイル
タ8とを備えた音響光学的な電気信号処理器であ
つて: 前記レーザ光が該超音波信号処理セルに設けら
れた光透過窓より入射したのち前記複数の超音波
伝搬経路すべてに対して垂直に通過するよう前記
複数のセル中の該超音波振動子がそれぞれ配置さ
れていることを特徴とする音響光学的な電気信号
処理器。 2 前記超音波信号処理セルの透明仕切板10に
より所定数に区分された部分に異なる超音波伝搬
時間を有する液状物質を保つことを特徴とする特
許請求の範囲第1項記載の音響光学的な電気信号
処理器。 3 液状物質をその内部に保つセルの内側面に設
けられ、外部電気信号を受領して振動する1また
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または複数の超音波吸収部材2,2′と、外部
のレーザ平行光線を透過させるため該セルに設け
られ該超音波の伝搬経路長手方向に開かれた形状
の光透過窓5,5′とを有する複数個の超音波信
号処理セルと;前記超音波信号処理セルの出力光
を受けるレンズ7と;該レンズの焦点位置に設け
られた光学的空間フイルタ8とを備えた音響光学
的な電気信号処理器であつて: 前記レーザ光は該複数のセルのそれぞれの光透
過窓から順に直列に通過すると共に、該レーザ光
が前記複数の超音波伝搬経路すべてに対して垂直
に通過するよう前記セル中の振動子がそれぞれ配
置されていることを特徴とする音響光学的な電気
信号処理器。 4 前記複数個の超音波信号処理セルのうち1又
は所望の該セルは他のセル内のそれとは異なる超
音波伝搬時間を有する液状物質をその内部に保つ
ことを特徴とする特許請求の範囲第3項記載の音
響光学的な電気信号処理器。
[Scope of Claims] 1. One or more ultrasonic transducers 1, 1' that are provided on the inner surface of a cell that keeps a liquid substance therein and vibrate upon receiving an external electric signal, and the ultrasonic transducer one or more ultrasonic absorbing members 2, 2' provided on the opposite side of the cell for absorbing ultrasonic waves propagating in the liquid substance, and transmitting parallel laser beams from the outside. The plurality of ultrasonic propagation paths by the plurality of ultrasonic transducers are divided into a predetermined number by light transmission windows 5, 5' provided in the cell and opened in the direction of the propagation path of the ultrasonic waves. an ultrasonic signal processing cell having (predetermined number - 1) transparent partition plates 10; a lens 7 that receives the output light of the ultrasonic signal processing cell; an optical device provided at the focal point of the lens; an acousto-optic electrical signal processor comprising: a spatial filter 8; the laser beam enters through a light transmission window provided in the ultrasonic signal processing cell and then passes through all of the plurality of ultrasonic propagation paths; An acousto-optic electrical signal processor, characterized in that the ultrasonic transducers in the plurality of cells are respectively arranged so as to pass perpendicularly to the cell. 2. The acousto-optic system according to claim 1, characterized in that liquid substances having different ultrasonic propagation times are kept in a predetermined number of sections divided by the transparent partition plate 10 of the ultrasonic signal processing cell. Electrical signal processor. 3. One or more ultrasonic transducers 1, 1' that are provided on the inner surface of a cell that keeps a liquid substance therein and that vibrate upon receiving an external electrical signal, and the cell provided with the ultrasonic transducers. one or more ultrasonic absorbing members 2, 2' provided on opposite sides of the cell for absorbing ultrasonic waves propagating in the liquid substance; a plurality of ultrasonic signal processing cells each having light transmission windows 5, 5' having a shape open in the longitudinal direction of the ultrasonic wave propagation path; a lens 7 for receiving output light from the ultrasonic signal processing cells; and the lens. an acousto-optic electrical signal processor, comprising: an optical spatial filter 8 provided at a focal position of the plurality of cells; An acousto-optic electrical signal processor characterized in that each of the vibrators in the cell is arranged so that the laser beam passes perpendicularly to all of the plurality of ultrasonic propagation paths. 4. Claim 4, wherein one or a desired cell of the plurality of ultrasonic signal processing cells maintains therein a liquid substance having an ultrasonic propagation time different from that in the other cells. 4. The acousto-optic electrical signal processor according to item 3.
JP2685081A 1981-02-27 1981-02-27 Acoustooptic electric signal processor Granted JPS57142019A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2685081A JPS57142019A (en) 1981-02-27 1981-02-27 Acoustooptic electric signal processor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2685081A JPS57142019A (en) 1981-02-27 1981-02-27 Acoustooptic electric signal processor

Publications (2)

Publication Number Publication Date
JPS57142019A JPS57142019A (en) 1982-09-02
JPS6351570B2 true JPS6351570B2 (en) 1988-10-14

Family

ID=12204745

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2685081A Granted JPS57142019A (en) 1981-02-27 1981-02-27 Acoustooptic electric signal processor

Country Status (1)

Country Link
JP (1) JPS57142019A (en)

Also Published As

Publication number Publication date
JPS57142019A (en) 1982-09-02

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