JPH0439618A - optical phase modulator - Google Patents
optical phase modulatorInfo
- Publication number
- JPH0439618A JPH0439618A JP2148294A JP14829490A JPH0439618A JP H0439618 A JPH0439618 A JP H0439618A JP 2148294 A JP2148294 A JP 2148294A JP 14829490 A JP14829490 A JP 14829490A JP H0439618 A JPH0439618 A JP H0439618A
- Authority
- JP
- Japan
- Prior art keywords
- piezoelectric vibrator
- optical phase
- phase modulator
- optical fiber
- cylindrical
- 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
Links
Landscapes
- Mechanical Light Control Or Optical Switches (AREA)
- Gyroscopes (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、光ファイバを用いて高精度の計測を行う光フ
ブイバジャイロ等といった光フアイバセンサに用いられ
る、光フアイバ形の光位相変調器に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to an optical fiber-type optical phase modulator used in optical fiber sensors such as optical fiber gyros that perform high-precision measurements using optical fibers. .
従来の技術
従来、このような目的に用いられる光位相変調器として
は、ニオブ酸リチウム等の誘電体基板上に光導波路と電
極とを形成してなる導波路形の光位相変調器と、円柱状
の圧電振動子に光ファイバを巻いた光フアイバ形の光位
相変調器の2種類がある。このうち、光フアイバ形光位
相変調器は、どちらも光ファイバを主要構成要素として
いるため、例えば光フアイバジャイロのような光フアイ
バセンサとの光学的結合が極めて容易であるという、導
波路形光位相変調器にはない優れた特徴をもっている。BACKGROUND OF THE INVENTION Conventionally, optical phase modulators used for such purposes include waveguide-shaped optical phase modulators in which an optical waveguide and electrodes are formed on a dielectric substrate such as lithium niobate, and circular optical phase modulators. There are two types of optical fiber-type optical phase modulators in which an optical fiber is wound around a columnar piezoelectric vibrator. Among these, optical fiber type optical phase modulators are waveguide type optical phase modulators, which are extremely easy to optically couple with optical fiber sensors such as optical fiber gyros because they both have optical fibers as their main component. It has excellent features not found in phase modulators.
また、この光フアイバ形光位相変調器は、構造が簡単で
、製作も容易である利点もある。Further, this optical fiber type optical phase modulator has the advantage of being simple in structure and easy to manufacture.
第3図は前述した従来の光フアイバ形光位相変調器の概
念図であり、図中、符号21は円柱状圧電振動子で、直
径方向に振動する。そして、22は前記円柱状圧電振動
子21の外周にきつく数回巻かれた光ファイバであり、
位相変調しようとする光を前記光ファイバの一方の端か
ら入射させ、他方から位相変調された光を取り出す。ま
た、23と24は変調信号電圧が印加される電極で、こ
れらに変調信号電圧を両電極間に印加すると、圧電撮動
子21は直径方向に振動し、周囲に巻かれた光ファイバ
22に長さ方向の応力と歪を誘起する。したがって、こ
の応力・歪により光ファイバ22の実効屈折率と長さが
わずかに変化するので、光位相変調器を光が通過する時
間が変調信号電圧に対応して変化して、結果的に位相変
調が行われる。FIG. 3 is a conceptual diagram of the conventional optical fiber type optical phase modulator mentioned above. In the figure, reference numeral 21 denotes a cylindrical piezoelectric vibrator, which vibrates in the diameter direction. 22 is an optical fiber tightly wound several times around the outer circumference of the cylindrical piezoelectric vibrator 21;
The light to be phase modulated is inputted from one end of the optical fiber, and the phase modulated light is extracted from the other end. Further, 23 and 24 are electrodes to which a modulation signal voltage is applied, and when a modulation signal voltage is applied between these electrodes, the piezoelectric sensor 21 vibrates in the diametrical direction, and the optical fiber 22 wound around it vibrates. Inducing longitudinal stresses and strains. Therefore, as the effective refractive index and length of the optical fiber 22 change slightly due to this stress and strain, the time it takes for light to pass through the optical phase modulator changes in accordance with the modulation signal voltage, resulting in a phase change. Modulation is performed.
発明が解決しようとする課題
前述したように優れた特徴をもつファイバ形光位相変調
器にも、次のような欠点がある。即ち、従来のファイバ
形光位相変調器は、その形状によって決まる振動モード
の共振周波数がいくつか存在し、そのため変調特性が平
坦ではない。例えば、圧電振動子21に印加する振幅電
圧一定の変調信号の周波数と、光位相変調器を通過する
光の位相変位量の振幅の関係は、第4図のようになるけ
れども、この変調周波数特性曲線には、圧電振動子21
の振動モードに関係した顕著な共振特性が現れている。Problems to be Solved by the Invention Even though the fiber-type optical phase modulator has the excellent features described above, it still has the following drawbacks. That is, in a conventional fiber-type optical phase modulator, there are several resonance frequencies of vibration modes determined by its shape, and therefore the modulation characteristics are not flat. For example, the relationship between the frequency of a modulation signal with a constant amplitude voltage applied to the piezoelectric vibrator 21 and the amplitude of the phase displacement amount of light passing through an optical phase modulator is as shown in FIG. 4, but this modulation frequency characteristic The curve includes a piezoelectric vibrator 21
Remarkable resonance characteristics related to the vibration modes of
つまり、このような平坦ではな−・変調周波数特性では
、任意の波形で光の位相を変調し、高度な信号処理で高
精度の光計測を行うことはできないといった課題がある
。In other words, with such an uneven modulation frequency characteristic, it is impossible to modulate the phase of light with an arbitrary waveform and perform highly accurate optical measurement using advanced signal processing.
本発明の課題は、前述した従来のファイバ形光位相変調
器のこのような欠点をなくし、平坦な光位相変調特性を
実現し、ファイバ形光位相変調器がもつ光フアイバセン
サとの結合が容易で、製作も容易といった優れた特徴を
充分に活用できるファイバ形光位相変調器を得るにある
。The object of the present invention is to eliminate such drawbacks of the conventional fiber-type optical phase modulator mentioned above, to realize flat optical phase modulation characteristics, and to facilitate coupling with the optical fiber sensor that the fiber-type optical phase modulator has. The object of the present invention is to obtain a fiber-type optical phase modulator that can fully utilize its excellent features such as ease of manufacture.
課題を解決するための手段
この課題を達成するための本発明第一の態様によれば、
対称軸あるいは対称面を持たない筒状の圧電振動子の内
・外側に電極を形成し、外周に光ファイバを巻いたこと
を特徴とする光位相変調器が提供される。Means for Solving the Problem According to the first aspect of the present invention for achieving this problem,
An optical phase modulator is provided, in which electrodes are formed on the inner and outer sides of a cylindrical piezoelectric vibrator having no axis of symmetry or plane of symmetry, and an optical fiber is wound around the outer periphery.
また、本発明の第二の態様によれば、外形が円柱状の圧
電振動子の内部に、前記円柱と中心軸を同一とする円柱
状空洞とは異なる空洞を形成されかつ肉厚が均一ではな
い筒状の圧電振動子の内・外側に電極を形成し、同圧電
振動子の外周に光ファイバを巻いたことを特徴とする光
位相変調器が提供される。According to the second aspect of the present invention, a cavity different from the cylindrical cavity having the same central axis as the cylinder is formed inside the piezoelectric vibrator having a cylindrical outer shape, and the wall thickness is not uniform. There is provided an optical phase modulator characterized in that electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator, and an optical fiber is wound around the outer periphery of the piezoelectric vibrator.
さらに、本発明の第三の態様によれば、外形が円柱状の
圧電振動子の内部に、前記円柱と中心軸を同一としない
円柱状空洞を形成した筒状圧電振動子の内・外側に電極
を形成し、同圧電振動子の外周に光ファイバを巻いた光
位相変調器が提供される。Furthermore, according to a third aspect of the present invention, a cylindrical piezoelectric vibrator having a cylindrical outer shape has a cylindrical cavity formed inside the piezoelectric vibrator whose central axis is not the same as the cylinder. An optical phase modulator is provided in which an electrode is formed and an optical fiber is wound around the outer periphery of a piezoelectric vibrator.
本発明の第四の態様によれば、前述した筒状圧電振動子
の壁の長さが一様でない圧電振動子の内・外側に電極を
形成し、同圧電振動子の外周に光ファイバを巻いた光位
相変調器が提供される。According to the fourth aspect of the present invention, electrodes are formed on the inside and outside of the piezoelectric vibrator whose wall length is not uniform, and an optical fiber is attached to the outer periphery of the piezoelectric vibrator. A wound optical phase modulator is provided.
本発明の第五の態様によれば、外形の円柱の中心軸と直
交しない平面で切断した形状の圧電振動子の内・外側に
電極を形成し、同圧電振動子の外周に光ファイバを巻い
た光位相変調器が提供される。According to the fifth aspect of the present invention, electrodes are formed on the inner and outer sides of a piezoelectric vibrator cut along a plane that is not perpendicular to the central axis of the external cylinder, and an optical fiber is wound around the outer circumference of the piezoelectric vibrator. An optical phase modulator is provided.
作用
前述の本発明の各構成により、対称軸や対称面を持たず
、肉厚が不均一な筒状の圧電振動子の内・外側に電極を
形成したものが得られるから、両電極間に振動電圧を印
加すると、対称性が低いので、光の位相変調に関係した
直径方向振動に関しては顕著な共振が起こりにくくなる
。そして、本発明のように、対称性の低い圧電振動子と
して、円柱状の外形を持つ圧電振動子の内側に、外形の
円柱と中心軸を同一とする円柱状空洞とは異なる空洞を
形成した、肉厚が不均一な筒状圧電振動子を用いれば、
顕著な振動モードの共振が現れないという効果が同様に
得られる。さらに、本発明による光位相変調器は、外形
が円柱状なので、製作上の困難が少なく、光ファイバを
巻くことも容易である。本発明による光位相変調器にあ
っては、内側に形成する空洞を、外形の円柱の中心軸と
異なる中心軸を持つ円柱状空洞とすれば、圧電振動子の
製作がさらに容易となる。Effects Each of the configurations of the present invention described above makes it possible to obtain a cylindrical piezoelectric vibrator with electrodes formed on the inside and outside of the cylindrical piezoelectric vibrator, which has no axis of symmetry or plane of symmetry and whose wall thickness is uneven. When an oscillating voltage is applied, significant resonance is less likely to occur with respect to diametrical oscillations associated with optical phase modulation due to the low symmetry. Then, as in the present invention, as a piezoelectric vibrator with low symmetry, a cavity different from a cylindrical cavity having the same central axis as the cylinder of the outer shape is formed inside the piezoelectric vibrator having a cylindrical outer shape. , if a cylindrical piezoelectric vibrator with uneven wall thickness is used,
The effect that no significant vibration mode resonance occurs is similarly obtained. Furthermore, since the optical phase modulator according to the present invention has a cylindrical outer shape, there are few manufacturing difficulties, and it is easy to wind the optical fiber. In the optical phase modulator according to the present invention, if the cavity formed inside is a cylindrical cavity having a central axis different from the central axis of the external cylinder, manufacturing of the piezoelectric vibrator becomes easier.
いい換えると、本発明は、筒状圧電振動子の肉厚を不均
一にすることによって、肉厚に関係した振動モードの共
振を抑えて、平坦な変調周波数特性を得ることができる
。しかし、筒状圧電振動子の直径方向振動モードの共振
には、この他に圧電振動子の長さに関係した共振からの
寄与もある。In other words, in the present invention, by making the wall thickness of the cylindrical piezoelectric vibrator non-uniform, it is possible to suppress the resonance of the vibration mode related to the wall thickness and obtain flat modulation frequency characteristics. However, the resonance of the diametrical vibration mode of the cylindrical piezoelectric vibrator also has a contribution from resonance related to the length of the piezoelectric vibrator.
これを抑えるには、筒状圧電振動子の壁の長さを不均一
にすることが有効である。このような構成は、外形が円
柱状の圧電振動子を、その中心軸と直交しない平面で切
断することによって、容易に得ることができる。To suppress this, it is effective to make the length of the wall of the cylindrical piezoelectric vibrator non-uniform. Such a configuration can be easily obtained by cutting a piezoelectric vibrator having a cylindrical outer shape along a plane that is not perpendicular to its central axis.
実施例
以下、第1図及び第2図を用いて本発明による光フアイ
バ形光位相変調器の実施例の詳細を説明するO
第1図は本発明による光フアイバ形光位相変調器の斜視
図であり、同図の符号11はチタン酸鉛系のセラミック
を用いた外形が円柱の筒状圧電振動子、12は外形の円
柱の中心軸とは異なる中心軸を持つ円柱状空洞である。EXAMPLE Hereinafter, details of an embodiment of an optical fiber type optical phase modulator according to the present invention will be explained using FIGS. 1 and 2. FIG. 1 is a perspective view of an optical fiber type optical phase modulator according to the present invention. The reference numeral 11 in the figure is a cylindrical piezoelectric vibrator with a cylindrical outer shape made of lead titanate ceramic, and the reference numeral 12 is a cylindrical cavity having a central axis different from the central axis of the external cylinder.
筒状圧電振動子の外径は301111で、その外周には
光ファイバ13が3回だけ巻かれている。内側の空洞の
直径は10龍で、外形の円柱の中心軸に対して、71+
11だけ偏心している。また、圧電振動子11の長さ方
向に関していえば、外形の円柱の中心軸と直交しな℃・
平面で切断した形状となっている。圧電振動子11の内
・外側には電極14と16が形成されており、両電極間
に振動電圧を印加することによって、圧電振動子は直径
方向に振動する。The outer diameter of the cylindrical piezoelectric vibrator is 301111, and the optical fiber 13 is wound around the outer circumference only three times. The diameter of the inner cavity is 10 dragons, and the diameter is 71+ with respect to the central axis of the outer cylinder.
It is eccentric by 11. In addition, regarding the length direction of the piezoelectric vibrator 11, it is noted that the longitudinal direction of the piezoelectric vibrator 11 is
It has a shape cut along a plane. Electrodes 14 and 16 are formed on the inside and outside of the piezoelectric vibrator 11, and by applying an oscillating voltage between the two electrodes, the piezoelectric vibrator vibrates in the diametrical direction.
この実施例の圧電振動子11は、内側の円柱状空洞の中
心軸が偏心しているので、肉厚が不均一となっている。In the piezoelectric vibrator 11 of this embodiment, the central axis of the inner cylindrical cavity is eccentric, so the wall thickness is non-uniform.
そして、同圧電振動子11は、長さ方向に関しても、壁
の長さが一様ではなく、顕著な振動モードの共振が現れ
ない形状となっている。このため、このような圧電振動
子に光ファイバを巻いて構成した光位相変調器の変調周
波数特性曲線には、第2図に示すように、顕著な共振特
性が出現せず、平坦な特性が得られる。The piezoelectric vibrator 11 also has a shape in which the length of the wall is not uniform in the longitudinal direction, and no significant vibration mode resonance occurs. Therefore, as shown in Figure 2, the modulation frequency characteristic curve of an optical phase modulator constructed by winding an optical fiber around such a piezoelectric vibrator does not exhibit significant resonance characteristics and has a flat characteristic. can get.
光フアイバジャイロ等において、高精度の信号処理を行
う方式として、セロダイン方式は有効な方式の一つであ
るが、この方式では、鋸歯状波による光位相変調が必要
であり、10μsec〜1m5ecの周期を持つ鋸歯状
波信号での光位相変調が可能な、広い帯域を持った光位
相変調器を使用しなければならない。本発明による光位
相変調器を用いて、この鋸歯状波で光位相変調を実行し
たところ、実用上問題のない変調信号を得ることができ
た。The serodyne method is one of the effective methods for high-precision signal processing in optical fiber gyros, etc., but this method requires optical phase modulation using a sawtooth wave, and has a period of 10 μsec to 1 m5 ec. An optical phase modulator with a wide band that can perform optical phase modulation with a sawtooth signal with When optical phase modulation was performed using this sawtooth wave using the optical phase modulator according to the present invention, it was possible to obtain a modulated signal with no problems in practical use.
発明の効果
以上に説明したように、本発明によれば、光位相変調の
平坦な周波数特性を得ることができるばかりでなく、本
発明のファイバ形光位相変調器は、圧電振動子製作上の
問題も少なく、光ファイバも容易に巻くことができ、フ
ァイバ形光位相変調器が持つ、ファイバとの結合が容易
であるという特徴を失うこともない等の効果がある。Effects of the Invention As explained above, according to the present invention, not only can flat frequency characteristics of optical phase modulation be obtained, but also the fiber-type optical phase modulator of the present invention has advantages in manufacturing piezoelectric vibrators. There are fewer problems, the optical fiber can be easily wound, and there are advantages such as not losing the characteristic of the fiber-type optical phase modulator that it is easy to couple with the fiber.
第1図は本発明による光位相変調器の斜視図、第2図は
本発明にかかる光位相変調器の振幅一定の印加変調信号
に対する変調周波数特性図、第3図は従来のファイバ形
光位相変調器の斜視図、第4図は同光位相変調器の振幅
一定の印加変調信号に対する変調周波数特性図である。
11・・・筒状圧電振動子、12・・・偏心円柱状空洞
、13.22・・・光ファイバ、14.16.23.2
4・・・電極、21・・・円筒状圧電振動子。
代理人の氏名 弁理士 粟 野 重 孝 ほか1名第
図
第
図
第
図
変調周波数
第
図
変調周波数FIG. 1 is a perspective view of an optical phase modulator according to the present invention, FIG. 2 is a modulation frequency characteristic diagram of the optical phase modulator according to the present invention for an applied modulation signal with a constant amplitude, and FIG. 3 is a diagram of a conventional fiber-type optical phase modulator. FIG. 4, a perspective view of the modulator, is a modulation frequency characteristic diagram of the same optical phase modulator with respect to an applied modulation signal of constant amplitude. 11... Cylindrical piezoelectric vibrator, 12... Eccentric cylindrical cavity, 13.22... Optical fiber, 14.16.23.2
4... Electrode, 21... Cylindrical piezoelectric vibrator. Name of agent Patent attorney Shigetaka Awano and one other person Fig. Fig. Fig. Modulation frequency Fig. Modulation frequency
Claims (5)
子の内側と外側に電極を形成し、同圧電振動子の外周に
光ファイバを巻いたことを特徴とする光位相変調器。(1) An optical phase modulator characterized in that electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator having no axis of symmetry or plane of symmetry, and an optical fiber is wound around the outer circumference of the piezoelectric vibrator.
中心軸を同一とする円柱状空洞とは異なる空洞が形成さ
れかつ肉厚が均一ではない筒状の圧電振動子の内・外側
に電極を形成し、同圧電振動子の外周に光ファイバを巻
いたことを特徴とする光位相変調器。(2) Inside the piezoelectric vibrator having a cylindrical outer shape, a cavity different from the cylindrical cavity having the same central axis as the cylinder is formed, and the wall thickness is not uniform. An optical phase modulator characterized in that an electrode is formed on the outside and an optical fiber is wound around the outer periphery of a piezoelectric vibrator.
中心軸を同一としない円柱状空洞を形成した筒状圧電振
動子の内・外側に電極を形成し、同圧電振動子の外周に
光ファイバを巻いたことを特徴とする光位相変調器。(3) Electrodes are formed on the inside and outside of the cylindrical piezoelectric vibrator, which has a cylindrical cavity whose central axis is not the same as that of the cylinder, inside the piezoelectric vibrator whose external shape is cylindrical. An optical phase modulator characterized by having an optical fiber wound around its outer periphery.
子の内・外側に電極を形成し、同圧電振動子の外周に光
ファイバを巻いたことを特徴とする請求項1、請求項2
もしくは請求項3記載の光位相変調器。(4) Claim 1 characterized in that electrodes are formed on the inner and outer sides of the piezoelectric vibrator whose walls are not uniform in length, and an optical fiber is wound around the outer periphery of the piezoelectric vibrator. , claim 2
Or the optical phase modulator according to claim 3.
形状の圧電振動子の内・外側に電極を形成し、同圧電振
動子の外周に光ファイバを巻いたことを特徴とする請求
項2もしくは請求項3記載の光位相変調器。(5) A claim characterized in that electrodes are formed on the inside and outside of a piezoelectric vibrator cut along a plane that is not orthogonal to the central axis of the external cylinder, and an optical fiber is wound around the outer periphery of the piezoelectric vibrator. 4. The optical phase modulator according to claim 2 or claim 3.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2148294A JPH0439618A (en) | 1990-06-05 | 1990-06-05 | optical phase modulator |
| US07/709,879 US5101449A (en) | 1990-06-05 | 1991-06-04 | Optical phase modulator with asymmetric piezoelectric vibrator |
| EP19910109188 EP0460635A3 (en) | 1990-06-05 | 1991-06-05 | Optical phase modulator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2148294A JPH0439618A (en) | 1990-06-05 | 1990-06-05 | optical phase modulator |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0439618A true JPH0439618A (en) | 1992-02-10 |
Family
ID=15449562
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2148294A Pending JPH0439618A (en) | 1990-06-05 | 1990-06-05 | optical phase modulator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0439618A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2008009435A (en) * | 2006-06-28 | 2008-01-17 | Harris Corp | Actuator arrangement for excitation of flexural wave on optical fiber |
-
1990
- 1990-06-05 JP JP2148294A patent/JPH0439618A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2008009435A (en) * | 2006-06-28 | 2008-01-17 | Harris Corp | Actuator arrangement for excitation of flexural wave on optical fiber |
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