JPH01149031A - Acoustooptic device - Google Patents

Acoustooptic device

Info

Publication number
JPH01149031A
JPH01149031A JP62309139A JP30913987A JPH01149031A JP H01149031 A JPH01149031 A JP H01149031A JP 62309139 A JP62309139 A JP 62309139A JP 30913987 A JP30913987 A JP 30913987A JP H01149031 A JPH01149031 A JP H01149031A
Authority
JP
Japan
Prior art keywords
light
acousto
incident light
diffraction efficiency
optic
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
JP62309139A
Other languages
Japanese (ja)
Inventor
Toshiro Sakurai
俊郎 櫻井
Fumio Tanaka
文雄 田中
Koichi Kanayama
光一 金山
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP62309139A priority Critical patent/JPH01149031A/en
Publication of JPH01149031A publication Critical patent/JPH01149031A/en
Pending legal-status Critical Current

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  • Spectrometry And Color Measurement (AREA)

Abstract

PURPOSE:To perform accurate measurement which is not affected by the polarized state of light by providing a pulse modulator in a driving part operated to obtain the diffracted light from the incident light and setting a prescribed power so that the diffraction efficiency of vertical linear polarization and that of horizontal linear polarization are equalized. CONSTITUTION:An acoustooptic medium 1, a piezoelectric element 2, a driving part 3 of this element 2, and a modulation input terminal of the pulse modulator are provided. In this case, the output of the driving part 3 is set to a prescribed power so that a diffracted light 5a has the same diffraction efficiency whether an incident light 5 is a vertically linearly polarized light or a horizontally linearly polarized light. Thus, the same diffraction efficiency is obtained in the case of the same intensity of light though the polarized state of the incident light like a laser light is changed, and accurate measurement is possible at the time of trouble point detection of an optical fiber or the like.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、超音波による光の回折、すなわち音響光学効
果を利用した音響光学装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an acousto-optic device that utilizes the diffraction of light caused by ultrasonic waves, that is, the acousto-optic effect.

従来の技術 音響光学素子は二酸化チル/’(TeO2)やモリブデ
ン酸鉛(PbMo、04)などの単結晶またはガラスか
らなる音響光学媒体に圧電素子を装着した基本構成であ
屈折率の疎密によシ回折格子が形成され、ここに一定の
角度(ブラック角)で入射するレーザ光などの光を回折
することができる。超音波の周波数によシ回折角が定ま
シ、超音波の強度によシ回折光の強度が定まるため、こ
れを利用して光の変調ができる。
Conventional technology Acousto-optic elements have a basic structure in which a piezoelectric element is attached to an acousto-optic medium made of single crystal or glass such as tyl dioxide (TeO2) or lead molybdate (PbMo, 04). A diffraction grating is formed, and light such as laser light that is incident thereon at a certain angle (Black angle) can be diffracted. The diffraction angle is determined by the frequency of the ultrasonic wave, and the intensity of the diffracted light is determined by the intensity of the ultrasonic wave, so this can be used to modulate light.

音響光学素子の動作原理を第4図に示す。第4図におい
て、音響光学媒体1の一面に設けた圧電素子2に駆動部
6よシミ完信号を入力し、圧電素子2によシ前記電気信
号を超音波信号に変換し、この超音波信号を音響光学媒
体l中を進光させ、レーザ光などの光5を回折させるも
のである。ここで5aは回折光、5bは透過光である。
The operating principle of the acousto-optic device is shown in FIG. In FIG. 4, a stain completion signal is input from the drive unit 6 to the piezoelectric element 2 provided on one surface of the acousto-optic medium 1, and the piezoelectric element 2 converts the electrical signal into an ultrasonic signal. The beam propagates through an acousto-optic medium l, and diffracts light 5 such as a laser beam. Here, 5a is diffracted light and 5b is transmitted light.

従来この種の音響光学装置は、入射するレーザ光などの
光の偏光状態を一定の直線偏光で使用し回折効率が最も
大きくなるように駆動部6からの入力電力を設定する。
Conventionally, this type of acousto-optic device uses a constant linear polarization state of incident light such as a laser beam, and sets the input power from the drive section 6 so that the diffraction efficiency is maximized.

すなわち、音響光学素子の入力電力と回折効率の関係を
示す第2図において、入射光と回折光で作る平面に垂直
な直線偏光(以下垂直直線偏光という)の場合はAの入
力電力、入射光と回折光で作る平面に平行な直M偏光(
以下水平直線偏光という)の場合はCの入力電力で使用
していた。また、垂直直線偏光および水平直線偏光以外
の入射光5を使う場合、音響光学媒体1の材料として入
射光5の波長による偏光依存性の少ないものを使用して
いた。
That is, in Figure 2, which shows the relationship between input power and diffraction efficiency of an acousto-optic element, in the case of linearly polarized light perpendicular to the plane created by the incident light and diffracted light (hereinafter referred to as vertical linear polarized light), the input power of A, the incident light and direct M polarized light parallel to the plane created by the diffracted light (
In the case of horizontal linearly polarized light (hereinafter referred to as horizontal linear polarization), an input power of C was used. Further, when using incident light 5 other than vertically linearly polarized light and horizontally linearly polarized light, a material with little polarization dependence on the wavelength of the incident light 5 is used as the material for the acousto-optic medium 1.

発明が解決しようとする問題点 このような従来の構成では、入射するレーザ光などの光
の偏光状態が変れば、駆動部6からの入力電力が一定で
あっても回折効率が変わる丸めに、光ファイバーの障害
点検出などを行うための0TDRに音響光学装置を使用
する場合、正確な測定ができないという問題があった。
Problems to be Solved by the Invention In such a conventional configuration, if the polarization state of incident laser light or other light changes, the diffraction efficiency will change even if the input power from the drive unit 6 is constant. When using an acousto-optic device for 0TDR to detect fault points in optical fibers, there is a problem in that accurate measurements cannot be made.

また音響光学媒体1の材料を入射光50波長による偏光
依存性の少ないもので使用する場合、例えば音響光学媒
体1にモリブデン酸鉛を使用し、波長633nmのレー
ザ光を入射するとか、音響光学媒体lに二酸化チルρを
使用し、波長1.3μmのレーザ光を入射するというふ
うに音響光学媒体1の材料および入射光5の波長が制限
されてしまい、装置としての自由度が小さく問題であっ
た。
In addition, when using a material for the acousto-optic medium 1 that has little polarization dependence depending on the wavelength of the incident light, for example, lead molybdate is used for the acousto-optic medium 1 and laser light with a wavelength of 633 nm is incident on the acousto-optic medium 1. Since the material of the acousto-optic medium 1 and the wavelength of the incident light 5 are limited, such as by using chil dioxide ρ for l and injecting a laser beam with a wavelength of 1.3 μm, the degree of freedom of the device is small, which is a problem. Ta.

本発明はこのような問題点を解決するもので、測定精度
に優れ、音響光学媒体の材料と入射光の波長の制限を緩
和できる音響光学装置を提供することを目的とするもの
である。
The present invention solves these problems, and aims to provide an acousto-optic device that has excellent measurement accuracy and can alleviate restrictions on the material of the acousto-optic medium and the wavelength of incident light.

問題点を解決するための手段 この問題点を解決するために本発明は、音響光学素子と
、この音響光学素子を駆動して、入射光から回折光を得
るように動作させる駆動部と、この駆動部に設けたパル
ス変調器とを備え、前記駆動部の出力を、前記音響光学
素子の入射光の偏光状態が入射光と回折光で作る平面に
平行な直線偏光と前記平面に垂直な直線偏光で同等の回
折効率が得られる所定電力に設定したものである。
Means for Solving the Problem In order to solve this problem, the present invention provides an acousto-optic element, a driving section for driving the acousto-optic element to obtain diffracted light from incident light, and a driver for driving the acousto-optic element to obtain diffracted light from incident light. a pulse modulator provided in the drive unit, and the output of the drive unit is configured such that the polarization state of the incident light of the acousto-optic element is a linearly polarized light parallel to a plane formed by the incident light and the diffracted light, and a straight line perpendicular to the plane. This is set to a predetermined power that allows the same diffraction efficiency to be obtained with polarized light.

作用 上記構成によシ、音響光学素子に入射させるレーザ光な
どの光の偏光状態が変わっても、光強度が同じであれば
同等の回折効率が得られるため、0TDRKこの音響光
学装置を使用する場合、光の偏光状態の影響がなく正確
な測定ができ、しかも、音響光学媒体の材料、使用入射
光の波長の制限を緩和することができる。このとき、駆
動部はそのバルヌ変調出力により、光ファイバーなどの
障害点からの反射光のみを回折させるように動作させる
ことができる。
Effect With the above configuration, even if the polarization state of light such as a laser beam incident on the acousto-optic element changes, as long as the light intensity is the same, the same diffraction efficiency can be obtained. In this case, accurate measurements can be made without being affected by the polarization state of the light, and furthermore, restrictions on the material of the acousto-optic medium and the wavelength of the incident light used can be relaxed. At this time, the driving section can be operated to diffract only the reflected light from the failure point, such as the optical fiber, by its Varne modulation output.

実施例 以下本発明の一実施例を図面に基づいて説明する。Example An embodiment of the present invention will be described below based on the drawings.

第1図は本発明の一実施例による音響光学装置を示す原
理構成図、第2図は音響光学素子の入力電力と回折効率
の関係を示す図である。第1図において、1は音響光学
媒体、2は圧電素子、5は入射光、5aは回折光、 5
bは透過光で、第4図と同じである。3は圧電素子2の
駆動部で、パルス変調器が設けられている。4は変調入
力端子である。
FIG. 1 is a diagram showing the principle configuration of an acousto-optic device according to an embodiment of the present invention, and FIG. 2 is a diagram showing the relationship between input power and diffraction efficiency of an acousto-optic element. In FIG. 1, 1 is an acousto-optic medium, 2 is a piezoelectric element, 5 is incident light, 5a is diffracted light, 5
b is transmitted light, which is the same as in FIG. 3 is a drive section for the piezoelectric element 2, and is provided with a pulse modulator. 4 is a modulation input terminal.

この駆動部3の出力は、入射光5が垂直直線偏光でも水
平直線偏光でも回折光5aが同等の回折効率になるよう
に所定電力に設定される。すなわち、第2図から、垂直
直線偏光と水平直線偏光の回折効率が同等なるようにす
るには、入力電力Bの点で音響光学素子を駆動すればよ
いことがわかるので、駆動部3の出力を、このような入
力電力を与える所定電圧に設定する。
The output of the drive unit 3 is set to a predetermined power so that the diffraction efficiency of the diffracted light 5a is the same whether the incident light 5 is vertically linearly polarized light or horizontally linearly polarized light. In other words, from FIG. 2, it can be seen that in order to make the diffraction efficiency of vertically linearly polarized light and horizontally linearly polarized light the same, the acousto-optic element should be driven at the input power B, so the output of the driving section 3 is set to a predetermined voltage that provides such input power.

一方、駆動部3のパルス変調器はパルス変調信号によシ
、音響光学素子は入射光5を回折したシ、透過させたシ
する。
On the other hand, the pulse modulator of the drive unit 3 uses a pulse modulation signal, and the acousto-optic element diffracts and transmits the incident light 5.

第3図は本発明の音響光学装置を使用した探傷装置の一
例を示す。光源11からの入射光はパルス変調信号によ
る非駆動時に音響光学素子12を透過して光ファイバー
13に入射され、光ファイバー13の障害点からの反射
光はパルス変調信号によシ駆動される音響光学素子12
で回折され、この回折光はミラー14で反射して受光器
15で受光され、測定される。このとき、障害点からの
反射光が偏光状態の一定でない光であっても、正確に障
害点の検出が行えるものでおる。
FIG. 3 shows an example of a flaw detection device using the acousto-optic device of the present invention. The incident light from the light source 11 is transmitted through the acousto-optic element 12 and enters the optical fiber 13 when not driven by the pulse modulation signal, and the reflected light from the failure point of the optical fiber 13 is reflected from the acousto-optic element driven by the pulse modulation signal. 12
This diffracted light is reflected by a mirror 14, received by a light receiver 15, and measured. At this time, even if the reflected light from the fault point has an uneven polarization state, the fault point can be detected accurately.

発明の効果 以上のように本発明によれば、入射するレーザ光などの
光の偏光状態が変っても、光の強度が同じであれば、同
等の回折効率が得られ、光ファイバーの障害点検出など
を行うための0TDRに音響光学装置を使用する場合に
、正確な測定が可能である。また従来、偏光依存性のた
め音響光学媒体の材料と入射光の波長が制限されていた
ものも緩和することができる。
Effects of the Invention As described above, according to the present invention, even if the polarization state of incident laser light or other light changes, as long as the intensity of the light is the same, the same diffraction efficiency can be obtained, and it is possible to detect fault points in optical fibers. Accurate measurements are possible when using an acousto-optic device for 0TDR. Furthermore, the conventional limitations on the material of the acousto-optic medium and the wavelength of the incident light due to polarization dependence can be alleviated.

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

第1図は本発明の一実施例の音響光学装置を示す原理構
成図、第2図は音響光学素子の入力電力と回折効率の関
係を示す図、第3図は同音響光学装置を使用した探傷装
置の一例を示す構成図、第4図は従来の音響光学装置の
原理構成図である。 l・・・音響光学媒体、2・・・圧電素子、3・・・駆
動部、4・・・変調入力端子、5・・・入射光、5a・
・・回折光、5b・・・透過光。 代地人    森   本   義   弘第1図 第′2図
Figure 1 is a diagram showing the principle configuration of an acousto-optic device according to an embodiment of the present invention, Figure 2 is a diagram showing the relationship between input power and diffraction efficiency of an acousto-optic element, and Figure 3 is a diagram showing the relationship between the input power and diffraction efficiency of an acousto-optic device. FIG. 4 is a block diagram showing an example of a flaw detection device, and FIG. 4 is a diagram showing the principle structure of a conventional acousto-optic device. l... Acousto-optic medium, 2... Piezoelectric element, 3... Drive unit, 4... Modulation input terminal, 5... Incident light, 5a...
... Diffracted light, 5b... Transmitted light. Representative Yoshihiro Morimoto Figure 1 Figure '2

Claims (1)

【特許請求の範囲】[Claims] 1、音響光学素子と、この音響光学素子を駆動して入射
光から回折光を得るように動作させる駆動部と、この駆
動部に設けたパルス変調器とを備え、前記駆動部の出力
を、前記音響光学素子の入射光の偏光状態が入射光と回
折光で作る平面に平行な直線偏光と前記平面に垂直な直
線偏光で同等の回折効率が得られる所定電力に設定した
音響光学装置。
1. An acousto-optic element, a drive unit that drives the acousto-optic element to obtain diffracted light from incident light, and a pulse modulator provided in the drive unit, and the output of the drive unit is An acousto-optic device in which the polarization state of the incident light of the acousto-optic element is set to a predetermined power such that equivalent diffraction efficiency can be obtained for linearly polarized light parallel to a plane formed by the incident light and diffracted light and linearly polarized light perpendicular to the plane.
JP62309139A 1987-12-07 1987-12-07 Acoustooptic device Pending JPH01149031A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62309139A JPH01149031A (en) 1987-12-07 1987-12-07 Acoustooptic device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62309139A JPH01149031A (en) 1987-12-07 1987-12-07 Acoustooptic device

Publications (1)

Publication Number Publication Date
JPH01149031A true JPH01149031A (en) 1989-06-12

Family

ID=17989373

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62309139A Pending JPH01149031A (en) 1987-12-07 1987-12-07 Acoustooptic device

Country Status (1)

Country Link
JP (1) JPH01149031A (en)

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