JPS6227694B2 - - Google Patents
Info
- Publication number
- JPS6227694B2 JPS6227694B2 JP15545781A JP15545781A JPS6227694B2 JP S6227694 B2 JPS6227694 B2 JP S6227694B2 JP 15545781 A JP15545781 A JP 15545781A JP 15545781 A JP15545781 A JP 15545781A JP S6227694 B2 JPS6227694 B2 JP S6227694B2
- Authority
- JP
- Japan
- Prior art keywords
- ultrasonic
- cell
- light
- wave
- vibrator
- 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
- 239000007788 liquid Substances 0.000 claims description 19
- 230000005540 biological transmission Effects 0.000 claims description 6
- 230000004907 flux Effects 0.000 claims 1
- 230000001902 propagating effect Effects 0.000 claims 1
- 230000003287 optical effect Effects 0.000 description 12
- 238000002604 ultrasonography Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 5
- 230000004397 blinking Effects 0.000 description 4
- 239000000463 material Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000010363 phase shift Effects 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 1
- 230000009471 action Effects 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 230000000737 periodic effect Effects 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
- 230000002123 temporal effect 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
- G02F1/01—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】
この発明は液状物質中における超音波伝搬を用
い、電気信号を時間的変化信号より空間的、すな
わち、位置あるいは距離に対応して変化する信号
に変換し、空間的信号処理を行わせるための音響
光学的信号処理用液体セルに関するものである。DETAILED DESCRIPTION OF THE INVENTION This invention uses ultrasonic propagation in a liquid substance to convert an electrical signal into a signal that changes spatially, that is, in response to position or distance, rather than a temporally changing signal. The present invention relates to an acousto-optic signal processing liquid cell for performing processing.
従来より、光学レンズ系や音響光学的な変調器
を使用した空間的信号処理装置があり、レーダー
信号の圧縮や、実時間スペクトルアナライザ等、
広く利用されている。これら装置の光変調部分に
用いられている超音波光変調器には、光波面の位
相変調作用の他に、超音波伝搬による電気信号の
時間的遅延動作が有り、この2つの特徴を効果的
に組合せることによつて、電気的信号処理では非
常に複雑な装置構成を必要とする積分、アナログ
信号遅延などの処理を簡単かつ高速に実現してい
る。本発明は、この超音波光変調器の改良であつ
て、従来の変調器の基本的な構造である、変調器
内壁の片面に取付けた振動子より変調器内に、単
一方向伝搬する超音波信号を放射する方式を改
め、1つの変調器内に互いに反対方向に進行し、
かつ、振幅波形の等しい2つの超音波信号を発生
させることによつて、従来変調器の2台分の動作
を行い、かつ、2つの超音波信号の時間的、空間
的同期が正確に得られ、さらに回折輝点が自動的
に点滅する音響光学的信号処理用液体セルを提供
することを目的としている。 Traditionally, there have been spatial signal processing devices using optical lens systems and acousto-optic modulators, which are used to compress radar signals, real-time spectrum analyzers, etc.
Widely used. The ultrasonic optical modulator used in the optical modulation part of these devices has a phase modulation effect on the optical wavefront as well as a time delay operation on the electric signal due to ultrasonic propagation, and these two characteristics can be effectively utilized. By combining these, it is possible to easily and quickly realize processes such as integration and analog signal delay, which require extremely complicated device configurations in electrical signal processing. The present invention is an improvement of this ultrasonic optical modulator, in which ultrasonic light propagates in a single direction within the modulator from a vibrator attached to one side of the inner wall of the modulator, which is the basic structure of conventional modulators. The method of emitting sound wave signals has been changed, and the sound waves are transmitted in opposite directions within one modulator.
Moreover, by generating two ultrasonic signals with equal amplitude waveforms, it is possible to perform the operations of two conventional modulators, and to obtain accurate temporal and spatial synchronization of the two ultrasonic signals. Another object of the present invention is to provide a liquid cell for acousto-optic signal processing in which a diffraction bright spot automatically blinks.
この目的のため、本発明では、電気信号を超音
波に変換して液体セル中に放射する振動子に厚み
方向振動子を使用し、この振動子を液体セルに設
けられている光通過窓のほぼ中央に、通過する光
の光軸と振動子面とが平行になるように配置し
た。さらに、この振動子面と対面するセル両壁の
内面に、超音波吸収部材を設置し、セル内に液状
の超音波伝搬媒質を充てんした。 For this purpose, in the present invention, a thickness direction oscillator is used as the oscillator that converts an electric signal into an ultrasonic wave and radiates it into the liquid cell, and this oscillator is inserted into the light passing window provided in the liquid cell. The vibrator was placed approximately in the center so that the optical axis of the light passing therethrough was parallel to the vibrator surface. Further, ultrasonic absorbing members were installed on the inner surfaces of both walls of the cell facing the transducer surface, and the cell was filled with a liquid ultrasonic propagation medium.
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信号処理用液体
セルの実施例における構造を示す図である。直方
体状のセル1の対向する1組の壁面に、1対の光
透過窓2a,2bが設けられ、この窓を光が通過
する。前記セル1内には液状の超音波伝搬媒質3
が充てんされており、この媒質中に超音波を発射
する厚み方向振動子4が、前記光透過窓のほぼ中
央の位置にまたがり、かつ、その振動子面が光の
進行方向と平行になるように配置されている。こ
の振動子は前記光透過窓に張られている透明な
板、およびセル内壁との間に、弾性を持ち液状物
質に対して気密性を有する保持材5により保持さ
れている。前記振動子の振動面に対向する一対の
セル内壁には、振動子より発生した超音波を吸収
する、超音波吸収部材6a,6bが取付けられて
おり、超音波のセル内不要反射波を防止してい
る。前記振動子には電気信号を加える信号入力端
子7が取付けてある。 FIG. 1 is a diagram showing the structure of an embodiment of the acousto-optic signal processing liquid cell of the present invention. A pair of light transmitting windows 2a and 2b are provided on a pair of opposing wall surfaces of the rectangular parallelepiped cell 1, and light passes through these windows. Inside the cell 1 is a liquid ultrasonic propagation medium 3.
A thickness-direction transducer 4 that emits ultrasonic waves into this medium straddles the approximately central position of the light transmission window, and the transducer surface is parallel to the traveling direction of the light. It is located in This vibrator is held between a transparent plate placed on the light transmitting window and the inner wall of the cell by a holding material 5 which is elastic and airtight against liquid substances. Ultrasonic absorption members 6a and 6b are attached to a pair of inner walls of the cell facing the vibration surface of the transducer to absorb ultrasonic waves generated from the transducer, thereby preventing unnecessary reflected waves of ultrasonic waves within the cell. are doing. A signal input terminal 7 for applying an electric signal is attached to the vibrator.
第2図は、セル内の超音波信号8a,8bの動
きと、この超音波による光の回折の状態を示して
いる。セル1の光透過窓2a,2bの超音波進行
方向長さをLとする。超音波の形は、伝搬状態を
明白にするため、正弦波信号を矩形パルスで100
%振幅変調したものとし、正弦波信号の時間周波
数を〔Hz〕、矩形パルスの周期およびパルス幅
をT,W〔m〕とする。前記セル内の超音波伝搬
速度をv〔m/s〕とすれば、前記正弦波信号の
空間的周期TCSは
TCS=v/〔m〕 ……(1)
また、前記パルス周期、パルス幅の空間的長
さ、TS,WSは
TS=T×v〔m〕 ……(2)
WS=W×v〔m〕 ……(3)
となる。 FIG. 2 shows the movement of the ultrasonic signals 8a and 8b within the cell and the state of light diffraction due to the ultrasonic waves. Let L be the length of the light transmitting windows 2a and 2b of the cell 1 in the ultrasonic propagation direction. The shape of the ultrasonic wave is a rectangular pulse of 100 sine wave signals to make the propagation state obvious.
% amplitude modulation, the time frequency of the sine wave signal is [Hz], and the period and pulse width of the rectangular pulse are T, W [m]. If the ultrasonic propagation speed in the cell is v [m/s], then the spatial period T CS of the sine wave signal is T CS = v/[m] ... (1) Also, the pulse period, pulse The spatial lengths of the widths, T S and W S are as follows: T S =T x v [m] ... (2) W S = W x v [m] ... (3).
ここで、L≫WS,L≫TS,TCS≪TS,TCS
≪WSの条件を仮定し、前記光透過窓より前記振
動子面と平行行に平面波光をセル内を通過させれ
ば、セル内で超音波信号により位相変調を受けた
平面波光はレンズ9の作用で収束し、前記レンズ
の焦点面10上に回折輝点を生ずる。前記レンズ
の焦点距離をFとすれば、前記仮定条件より、前
記回折輝点の最も強いもの、すなわち、1次回折
輝点の位置は前記正弦波信号の空間周期TCSを用
いて
d=λF/TCS〔m〕 ……(4)
なる式で与えられる。dは光軸点と回折輝点との
間隔、λは光源波長である。ゆえに、(4)式で与え
られる前記焦点面上の開口を有する光学的フイル
タ10を前焦点面に配置し、このフイルタを通過
した光を光電変換器11で検出すれば、電気信号
で制御した光信号が得られる。なお、(4)式で明ら
かなように回折輝点位置はTCSの値により変化す
るが、超音波信号8a,8bの位置および、動き
に対しては不変である。 Here, L≫W S , L≫T S , T CS ≪T S , T CS
<<Assuming the condition of W S , if plane wave light is passed through the cell in parallel with the transducer surface from the light transmission window, the plane wave light that has been phase modulated by the ultrasonic signal within the cell will pass through the lens 9. The light is converged by the action of , and a diffraction bright spot is produced on the focal plane 10 of the lens. If the focal length of the lens is F, then from the above assumption, the position of the strongest diffraction bright spot, that is, the first-order diffraction bright spot, is determined by d=λF using the spatial period T CS of the sine wave signal. /T CS [m] ...(4) It is given by the formula. d is the distance between the optical axis point and the diffraction bright spot, and λ is the light source wavelength. Therefore, if an optical filter 10 having an aperture on the focal plane given by equation (4) is placed on the front focal plane and the light passing through this filter is detected by the photoelectric converter 11, it can be controlled by an electrical signal. An optical signal is obtained. Note that, as is clear from equation (4), the position of the diffraction bright spot changes depending on the value of T CS , but remains unchanged with respect to the position and movement of the ultrasound signals 8a and 8b.
次に輝点の輝度について考える。従来の超音波
光変調器では超音波の伝搬方向が単一方向である
ため一次元の移動格子と見なせ、超音波の空間的
周期が光透過窓の開口長に比べ十分小さな場合、
輝点の輝度は超音波信号振幅値の自乗に比例し、
超音波強度が一定の場合には輝点の輝度も一定に
なることが知られている。本発明では、同一液体
セル内に振幅、周波数が共に等しい2つの超音波
が存在し、かつ、反対方向に移動しているため、
この2つの超音波を通過した平面光が一点に収束
すれば、各々の超音波を通過した平面波光の位相
変化が時間的に異なり、回折輝点は点滅する。第
3図は輝点の点滅を示す図である。同図aは振動
子4より発射された2つの超音波が1つの連続し
た正弦波形を形成する場合を示し、この瞬間にお
いては、セル全体が一次元格子と見なせるため回
折輝点は最大輝度を示す。同図bは同図aの時刻
より時間が経過し、前記2つの超音波が反対方向
に各々1/4空間周期移動した場合を示している。
この時刻においては、2つの超音波の位相は〔n
+1/2〕空間周期(n;整数)のずれを生じてお
り、各々の超音波を通過した平面波光の位相ずれ
も焦点面上の輝点位置において〔n+1/2〕周期
のずれを生じ、理論上は輝点輝度が零となる。ゆ
えに、本発明による液体セルで得られた回折輝点
は超音波伝搬により自動的に点滅し、その点滅周
期Tfは
Tf=TCS/(4v)〔S〕 ……(5)
で与えられる。 Next, consider the brightness of the bright spot. In conventional ultrasonic optical modulators, the propagation direction of the ultrasonic waves is unidirectional, so it can be regarded as a one-dimensional moving grating, and if the spatial period of the ultrasonic waves is sufficiently small compared to the aperture length of the light transmission window,
The brightness of the bright spot is proportional to the square of the ultrasound signal amplitude value,
It is known that when the ultrasonic intensity is constant, the brightness of the bright spot is also constant. In the present invention, since two ultrasonic waves having the same amplitude and frequency exist in the same liquid cell and are moving in opposite directions,
When the plane light that has passed through these two ultrasound waves converges on one point, the phase change of the plane wave light that has passed through each ultrasound wave is different in time, and the diffraction bright spot blinks. FIG. 3 is a diagram showing blinking of bright spots. Figure a shows a case where two ultrasonic waves emitted from the transducer 4 form one continuous sine waveform. At this moment, the entire cell can be regarded as a one-dimensional grating, so the diffraction bright spot reaches its maximum brightness. show. Figure b shows a case where time has elapsed since the time in figure a, and the two ultrasonic waves have each moved 1/4 spatial period in opposite directions.
At this time, the phases of the two ultrasound waves are [n
+1/2] spatial period (n; integer), and the phase shift of the plane wave light that has passed through each ultrasound also causes a shift of [n + 1/2] period at the bright spot position on the focal plane, Theoretically, the luminance of the bright spot becomes zero. Therefore, the diffraction bright spot obtained by the liquid cell according to the present invention blinks automatically due to ultrasonic propagation, and the blinking period T f is given by T f =T CS /(4v) [S] ...(5) It will be done.
本発明は以上のような構成であり、1枚の振動
子4よりセル1内の液状超音波伝搬媒質3中に放
射された2つの超音波信号が、互いに反対方向に
等しい空間周波数および振幅で伝搬する特徴を有
する。このため、この2つの超音波を通過して位
相変調された平面波光をレンズ9で収束すれば、
各々の超音波を通過した平面波光の周期的な位相
ずれによつて、回折光輝点が自動的に点滅し、こ
の周期はセル1内の超音波速度vと超音波周波数
で決定される性質を有する。ゆえに、本発明に
よる液体セルを使用して音響光学的信号処理装置
を構成すれば、出力光の点滅周波数信号を電気的
フイルタで容易に分離することが可能であり、装
置に対する外来光雑音や、機械的振動等により発
生する光学系の低周波雑音が簡単に排除でき、さ
らに、光電変換後の出力信号を交流信号として取
扱うことが可能である。また、2つの超音波が反
対方向に等速で移動する特徴を、従来の音響光学
的相関器に応用して、パターンの対称性の検出や
中心位置決定などに利用することもできる。 The present invention has the above configuration, and two ultrasonic signals emitted from one transducer 4 into the liquid ultrasonic propagation medium 3 in the cell 1 are transmitted in opposite directions with the same spatial frequency and amplitude. It has the characteristic of propagation. Therefore, if the phase-modulated plane wave light that passes through these two ultrasonic waves is converged by the lens 9,
Due to the periodic phase shift of the plane wave light that has passed through each ultrasonic wave, the diffracted light bright spot automatically blinks, and this period has a property determined by the ultrasonic velocity v in the cell 1 and the ultrasonic frequency. have Therefore, if an acousto-optic signal processing device is configured using the liquid cell according to the present invention, it is possible to easily separate the blinking frequency signal of the output light using an electric filter, and to prevent external optical noise to the device. Low frequency noise in the optical system caused by mechanical vibration etc. can be easily eliminated, and furthermore, the output signal after photoelectric conversion can be handled as an alternating current signal. Furthermore, the characteristic that two ultrasonic waves move in opposite directions at the same speed can be applied to a conventional acousto-optic correlator and used for detecting pattern symmetry, determining the center position, etc.
第1図は本発明の実施例を示す図、第2図は液
体セル内の超音波の動きと、回折輝点位置を示す
図、第3図は回折輝点の点滅を示す図である。
1はセル、2a,2bは光透過窓、3は液状の
超音波伝搬媒質、4は厚み方向振動子、5は保持
材、6a,6bは超音波吸収部材、7は信号入力
端子を示す。
FIG. 1 is a diagram showing an embodiment of the present invention, FIG. 2 is a diagram showing the movement of ultrasonic waves in a liquid cell and the position of a diffraction bright spot, and FIG. 3 is a diagram showing blinking of a diffraction bright spot. 1 is a cell, 2a and 2b are light transmission windows, 3 is a liquid ultrasonic propagation medium, 4 is a thickness direction vibrator, 5 is a holding material, 6a and 6b are ultrasonic absorbing members, and 7 is a signal input terminal.
Claims (1)
前記媒質中に超音波進行波と平面波光とを入射し
て前記平面波光を前記超音波進行波で位相変調さ
せる音響光学的信号処理用液体セルであつて、該
セルの対向する両壁に備えられ平面波光束を該セ
ル内に通過させるための光透過窓2a,2bと;
該光透過窓のほぼ中央にまたがつて配置され、か
つ前記平面波光束の進行方向と平行な振動面を有
する厚み方向振動子4と;該振動子を保持しかつ
該振動子と該セル内壁との間にあつて該超音波伝
搬媒質を二分するための保持材5と;該振動子の
一対の厚み振動面に対向する該セルの各々の内壁
に設えられ前記振動子面より発生し前記超音波伝
搬媒質中を伝搬してきた一対の超音波を吸収消滅
させるための超音波吸収部材6a,6bと;該厚
み方向振動子に駆動用電気信号を供給するための
信号入力端子7とを備えたことを特徴とする音響
光学的信号処理用液体セル。1 contains a liquid ultrasonic propagation medium therein,
A liquid cell for acousto-optic signal processing that inputs an ultrasonic traveling wave and a plane wave light into the medium and modulates the phase of the plane wave light with the ultrasonic traveling wave, the liquid cell being provided on both opposing walls of the cell. light transmission windows 2a, 2b for passing the plane wave light flux into the cell;
a thickness direction oscillator 4 disposed straddling substantially the center of the light transmission window and having a vibrating surface parallel to the traveling direction of the plane wave light beam; a holding member 5 for dividing the ultrasonic propagation medium into two; and a holding member 5 provided on the inner wall of each of the cells facing the pair of thickness vibration surfaces of the vibrator to prevent the ultrasonic wave generated from the vibrator surface. Ultrasonic absorbing members 6a and 6b for absorbing and extinguishing a pair of ultrasonic waves propagating in a sound wave propagation medium; and a signal input terminal 7 for supplying a drive electric signal to the thickness direction vibrator. A liquid cell for acousto-optic signal processing characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15545781A JPS5857110A (en) | 1981-09-30 | 1981-09-30 | Liquid cell for acoustooptic signal processing |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15545781A JPS5857110A (en) | 1981-09-30 | 1981-09-30 | Liquid cell for acoustooptic signal processing |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5857110A JPS5857110A (en) | 1983-04-05 |
| JPS6227694B2 true JPS6227694B2 (en) | 1987-06-16 |
Family
ID=15606458
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15545781A Granted JPS5857110A (en) | 1981-09-30 | 1981-09-30 | Liquid cell for acoustooptic signal processing |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5857110A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2661992B1 (en) * | 1990-05-09 | 1992-08-28 | Aa | ACOUSTO-OPTIC DEFLECTOR. |
-
1981
- 1981-09-30 JP JP15545781A patent/JPS5857110A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5857110A (en) | 1983-04-05 |
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