JPS6351568B2 - - Google Patents
Info
- Publication number
- JPS6351568B2 JPS6351568B2 JP1171281A JP1171281A JPS6351568B2 JP S6351568 B2 JPS6351568 B2 JP S6351568B2 JP 1171281 A JP1171281 A JP 1171281A JP 1171281 A JP1171281 A JP 1171281A JP S6351568 B2 JPS6351568 B2 JP S6351568B2
- Authority
- JP
- Japan
- Prior art keywords
- ultrasonic
- cell
- signal
- electrical signal
- acousto
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 230000005540 biological transmission Effects 0.000 claims description 5
- 239000007788 liquid Substances 0.000 claims description 5
- 239000000126 substance Substances 0.000 claims description 5
- 230000001902 propagating effect Effects 0.000 claims 1
- 230000003287 optical effect Effects 0.000 description 25
- 238000002604 ultrasonography Methods 0.000 description 18
- 230000006835 compression Effects 0.000 description 5
- 238000007906 compression Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 3
- 230000006870 function Effects 0.000 description 3
- 238000001514 detection method Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 1
- 230000001934 delay Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000000284 extract Substances 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
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
- G02F1/29—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 position or the direction of light beams, i.e. deflection
- G02F1/33—Acousto-optical deflection devices
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、時間軸圧縮、
および、特定区間(時間)信号の抽出を行なう音
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 compression, and
The present invention also relates to an acousto-optic electrical signal processor that extracts a specific interval (time) signal.
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、実時間時間軸圧縮回路を音響光学的に
構成し、簡便な時間遅延・時間軸圧縮器用信号処
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 base compression circuits, which required extremely complex circuits and numerous electrical components, were constructed using an acousto-optical method, and are now available for simple time delays and time base compressors. The purpose is to provide a 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を、平行度良く対向
配置し、超音波伝搬媒質として液状物質を使用し
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 opposite to each other with good parallelism to constitute an optical ultrasound signal processing cell using a liquid substance as an ultrasound propagation medium, and only a specific output diffracted light appearing by the detection ultrasound signal passes through. An optical spatial filter was provided.
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透過窓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。本セル内に進行中
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 is a schematic perspective view of an optical ultrasound signal processing cell that is a component of the acousto-optic electrical signal processor of the present invention. This cell includes light transmission windows 5, 5' having a size sufficient for passage of band-shaped plane wave light 9, ultrasonic transducers 1, 1' that emit ultrasonic waves perpendicular to the traveling direction of the plane wave light 9, and , an ultrasonic absorbing member 2 that absorbs ultrasonic waves emitted from this vibrator,
2'. Furthermore, by using the liquid substance 4 as the ultrasonic propagation medium, it is possible to easily set a long ultrasonic propagation distance. Since the ultrasonic wave traveling in this cell is a compressional wave of the density of the propagation medium, a phase difference occurs partially in the band-shaped plane wave light 9 that traverses the ultrasonic wave, and a diffraction image appears when focused by a lens.
第2図は、前記光超音波信号処理セルによつて
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、超音波信
号が周波数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 by the optical ultrasonic signal processing cell. The laser beam 14 is expanded into band-shaped plane wave light by a lens system, passes through the cell 3, and at this time undergoes a phase change by the ultrasonic signal within the cell.
The light is converged by the lens 7 and formed into an image on the surface of the optical spatial filter 8 disposed at the focal plane. At this time, if the ultrasonic signal is a sine wave with a frequency f, the diffraction image becomes a bright spot at a distance d from the optical axis point of the optical spatial filter 8.
occurs in a remote location. 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7の焦点距離、v
は超音波のセル中進行速度である。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 7, v
is the speed at which the ultrasound waves travel through the cell. 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内に周波数の異なる2つの正弦
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 a case where two sinusoidal ultrasound waves having different frequencies exist in the cell 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. each frequency
Assuming 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).
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。 In addition, the intensity of the diffracted light is as follows for both the sum and difference frequencies:
It is proportional to the square of the product of two ultrasound 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1/2に圧縮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、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
れた光透過窓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(f1±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加して、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は等しい速度で互いに逆向きにセ
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。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。 From the above, if 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, , shown in equation (2),
By detecting the sum/difference frequency diffracted light with an optical spatial filter 8 and photoelectrically converting it, a signal can be obtained in which the time axis of the electrical signal is compressed to 1/2.
This situation will be explained with reference to an embodiment of the present invention shown in FIG. In this embodiment, the cell 3, lens 7, optical spatial filter 8
It has an integrated structure. Band-shaped plane wave light 9 enters the cell through a light transmission 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 which has undergone a phase change by crossing the ultrasonic signal 11 is converged by the lens 7 to generate 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, from the second electric signal input terminal 6' provided in the cell 3,
When the above-mentioned sine wave signal of frequency f 2 is modulated in pulse amplitude and applied and a pulsed ultrasonic signal is emitted into the cell, the part that spatially overlaps with this pulsed ultrasonic signal 12 in the optical axis direction is (f 1 ±f 2 ) frequency diffracted light with a light intensity proportional to the squared amplitude of the ultrasonic signal appears. 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 in opposite directions through the cell at the same speed, 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. If it is sufficiently smaller than the minimum spatial period of the electrical signal to be processed, it will be as if the ultrasonic signal 11 were scanned by the pulsed ultrasonic signal 12. The relative velocity of these two ultrasound signals is twice the ultrasound velocity, and the amplitude of the ultrasound pulse is constant, so the signal obtained by the scanning is 1/2 the electrical signal to be processed in time. It is compressed into . Furthermore, between the front surface of the light passing window 5 and the lens 7,
If an optical fixed pattern filter having an aperture approximately equal to the spatial width of the pulsed ultrasound is installed, it becomes a time delay device with a 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 ultrasonic waves are arbitrary, and the delay time of the electrical signal to be processed is the value obtained by dividing the distance from the ultrasonic transducer 1 to the opening of the fixed pattern by the ultrasonic velocity within the cell. becomes. Furthermore, in order to simultaneously perform time delay and time axis compression, a method of widening the aperture width of the fixed pattern and narrowing the pulsed ultrasonic wave for scanning may be considered. in this case,
Time axis 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.
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 electrical signal processor of the present invention, it is possible to compress the time axis of electrical signals, time delay having a gate function, and further achieve these two types. This has the effect of allowing combinational signal processing to be performed in analog fashion in real time.
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はセル、4は液状物質、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、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 is a cell, 4 is a liquid substance, 5 is a light transmission window, 6 and 6' are electrical signal input terminals, and 7 is a lens,
8 is an optical spatial filter, 9 is a band plane wave light, A
indicates the (f 1 + f 2 ) frequency diffraction bright spot, B indicates (f 1
−f 2 ) indicates a frequency diffraction bright spot.
Claims (1)
けられ、外部電気信号を受領して振動する複数の
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
伝搬経路に対して直角に通過するよう前記セル中
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電気信号処理器。[Claims] 1. A plurality of ultrasonic transducers 1 and 1' provided on the inner surface of a cell that keeps a liquid substance in a cubic shape and vibrating upon receiving an external electric signal; an ultrasonic absorbing member 2, 2' provided on the opposite side of the cell for absorbing ultrasonic waves propagating in the liquid substance; an ultrasonic signal processing cell having a light transmission window 5 opened in the longitudinal direction of the ultrasonic propagation path; a lens 7 for receiving the output light of the ultrasonic signal processing cell; and a lens 7 provided at the focal point of the lens. an acousto-optic electrical signal processor comprising: an acousto-optic electrical signal processor comprising: an acousto-optic electrical signal processor, wherein the laser light enters the plurality of ultrasonic propagation paths after entering through a light transmission window provided in the ultrasonic signal processing cell; An acousto-optic electrical signal processor, characterized in that the ultrasonic transducers in the cell are arranged so as to pass at right angles to the ultrasonic transducer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1171281A JPS57127320A (en) | 1981-01-30 | 1981-01-30 | Processor of acoustooptic electric signal |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1171281A JPS57127320A (en) | 1981-01-30 | 1981-01-30 | Processor of acoustooptic electric signal |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57127320A JPS57127320A (en) | 1982-08-07 |
| JPS6351568B2 true JPS6351568B2 (en) | 1988-10-14 |
Family
ID=11785648
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1171281A Granted JPS57127320A (en) | 1981-01-30 | 1981-01-30 | Processor of acoustooptic electric signal |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57127320A (en) |
-
1981
- 1981-01-30 JP JP1171281A patent/JPS57127320A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57127320A (en) | 1982-08-07 |
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