JPH04147210A - Optical phase modulator - Google Patents
Optical phase modulatorInfo
- Publication number
- JPH04147210A JPH04147210A JP27393690A JP27393690A JPH04147210A JP H04147210 A JPH04147210 A JP H04147210A JP 27393690 A JP27393690 A JP 27393690A JP 27393690 A JP27393690 A JP 27393690A JP H04147210 A JPH04147210 A JP H04147210A
- Authority
- JP
- Japan
- Prior art keywords
- piezoelectric vibrator
- cylindrical
- phase modulator
- electrodes
- optical fiber
- 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
- 230000003287 optical effect Effects 0.000 title claims abstract description 60
- 239000013307 optical fiber Substances 0.000 claims abstract description 44
- 238000004804 winding Methods 0.000 claims abstract description 3
- 239000000835 fiber Substances 0.000 claims description 3
- 239000000919 ceramic Substances 0.000 abstract description 2
- NKZSPGSOXYXWQA-UHFFFAOYSA-N dioxido(oxo)titanium;lead(2+) Chemical compound [Pb+2].[O-][Ti]([O-])=O NKZSPGSOXYXWQA-UHFFFAOYSA-N 0.000 abstract description 2
- 230000001788 irregular Effects 0.000 abstract 1
- 238000004519 manufacturing process Methods 0.000 description 7
- 238000000034 method Methods 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 241000282472 Canis lupus familiaris Species 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 229910000484 niobium oxide Inorganic materials 0.000 description 1
- URLJKFSTXLNXLG-UHFFFAOYSA-N niobium(5+);oxygen(2-) Chemical compound [O-2].[O-2].[O-2].[O-2].[O-2].[Nb+5].[Nb+5] URLJKFSTXLNXLG-UHFFFAOYSA-N 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 230000001629 suppression Effects 0.000 description 1
Abstract
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
アイバジャイロ等といった光ファイバヤンサに用いられ
る、光フアイバ型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
従来技術による光位相変調器としては、ニオブ酸すチク
ム等の誘電体基板上に光導波路と電極を形成してなる導
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、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、どちらも光ファイバを主要構成要素としている
ため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持つ。また、構造が簡単で、製作も
容易である。Prior Art Conventional optical phase modulators include a waveguide-shaped optical phase modulator in which an optical waveguide and an electrode are formed on a dielectric substrate such as niobium oxide, and a cylindrical piezoelectric vibrator. There are two types of optical fiber type optical phase modulators that are wound with optical fiber. Among these, optical fiber type optical phase modulators are optical waveguide type optical modulators that are extremely easy to optically couple with optical fiber sensors such as optical fiber gyros because both have optical fibers as their main components. It has excellent features not found in phase modulators. Furthermore, the structure is simple and manufacturing is easy.
従来技術による光フアイバ形光位相変調器の構造略図を
第6図に示す。21は円柱状圧電振動子で、動径方向に
振動する。22は光ファイバで円柱状圧電振動子の外周
にきつく数回巻かれている。A schematic structural diagram of a conventional optical fiber type optical phase modulator is shown in FIG. 21 is a cylindrical piezoelectric vibrator that vibrates in the radial direction. An optical fiber 22 is tightly wound several times around the outer circumference of the cylindrical piezoelectric vibrator.
位相変調しようとする光を前記光ファイバーの一力の端
から入射させ、他力から位相変調された光を取り出す。The light to be phase-modulated is input from one end of the optical fiber, and the phase-modulated light is extracted from the other end.
23と24は電極で、これに変調信号電圧を両電極間1
で組方りすると、圧電振動子2】は動径方向に振動し、
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。これにょって、光ファイバ22の実効屈折率
と長さがわずか(″C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。23 and 24 are electrodes, and a modulation signal voltage is applied between the two electrodes.
When assembled, the piezoelectric vibrator 2 vibrates in the radial direction,
This induces longitudinal stress and strain in the optical fiber 22 wound around it. As a result, the effective refractive index and length of the optical fiber 22 change slightly ("C"), so the time it takes for light to pass through the optical phase modulator changes in accordance with the modulation signal voltage, resulting in the phase Modulation is performed.
発明が解決しようとする課題
優れた特徴を持つファイバー形光位相変調器にも、欠点
がある。まず第一に、従来技術によるファイバ形光位相
変調器は、その形状によって決まる振動モートの共振周
波数がいくつか存在し、そのため変調特性が平坦ではな
かった。例えば、圧電振動子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7図のようになる。この変調
周波数特性曲線には、圧電振動子の振動モードに関係し
た顕著な共振特性が現れている。このような特性では、
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不可能である。Problems to be Solved by the Invention Although fiber-type optical phase modulators have excellent features, they also have drawbacks. First of all, in the fiber-type optical phase modulator according to the prior art, there are several resonant frequencies of vibration motes determined by the shape of the fiber-type optical phase modulator, 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 a piezoelectric vibrator and the amplitude of the phase displacement amount of light passing through an optical phase modulator is as shown in FIG. This modulation frequency characteristic curve shows remarkable resonance characteristics related to the vibration mode of the piezoelectric vibrator. With such characteristics,
It is impossible to modulate the phase of light with an arbitrary waveform and perform highly accurate optical measurements using advanced signal processing.
本発明は、従来技術による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持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活かすこ
とを目的としている。The present invention eliminates these drawbacks of conventional fiber-type optical phase modulators, realizes flat optical phase modulation characteristics, and is easy to combine with the optical fiber sensor that fiber-type optical phase modulators have and is easy to manufacture. The purpose is to take advantage of its excellent features such as ease of use.
課題を解決するだめの手段
本発明では、上記のようなファイバ形光位相変調器の欠
点をなくするために、多くとも1本の対称軸か1枚の対
称面しか持たない形状の圧電振動子の表面に、少なくと
も1対の電極を形成し、外周に光ファイバを巻いた光位
相変調器とする。Means for Solving the Problems In the present invention, in order to eliminate the drawbacks of the fiber-type optical phase modulator as described above, a piezoelectric vibrator having a shape having at most one axis of symmetry or one plane of symmetry is used. At least one pair of electrodes is formed on the surface of the optical phase modulator, and an optical fiber is wound around the outer periphery of the optical phase modulator.
特に上記のような光位相変調器は、第一に対称軸あるい
は対称面を持たない筒状の圧電振動子の内側と外側に電
極を形成し、外周に光ファイバを巻いた光位相変調器で
あり、第二に断面形状に対称点あるいは対称軸を持たず
、壁の長さが一様でない筒状圧電振動子の、内側と外側
に電極を形成し、外周に光ファイバを巻いた光位相変調
器であるO
さらに詳しく記せば、第一に外形が円柱状または楕円柱
状または角が丸い角柱状で、肉厚が均一ではない筒状の
圧電振動子の、内側と外側に電極を形成し、外周に光フ
ァイバを巻いた光位相変調器であり、第二に外形が円柱
状または楕円柱状または角が丸い角柱状の圧電振動子の
内部に、前記円柱または楕円柱または角が丸い角柱と、
中心軸または対称軸または対称面を同一としない円柱状
または楕円柱状または角が丸い角柱状空洞を設けた筒状
圧電振動子の、内側と外側に電極を形成し、外周に光フ
ァイバを巻いた光位相変調器であシ、第三に外形が円柱
状または楕円柱状または角が丸い角柱状の圧電振動子の
内部に、円錐または楕円錐または角の丸い角錘の一部を
切りとった形状の空洞を設けた筒状圧電振動子の、内側
と外側に電極を形成し、外周に光ファイバを巻いた光位
相変調器であり、第四に外形が大きさの異なる円柱また
は楕円柱または角が丸い角柱を積み重ねた形状で、内部
に空洞が形成されている筒状の圧電振動子の、内側と外
側に電極を形成し、外周に光ファイバを巻いた光位相変
調器であり、第五に外形が円柱または楕円柱または角が
丸い角柱の一部を切り欠いた形状で、肉厚が均一ではな
い筒状の圧電振動子の、内側と外側に電極を形成し、外
周に光ファイバを巻いた光位相変調器であり、第六に外
形が円柱状または楕円柱状または角が丸い角柱状の筒状
圧電振動子を、前記円柱または楕円柱または角が丸い角
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、内側と外側に電極を形成し、外周に光ファイバを
巻いた光位相変調器である。In particular, the optical phase modulator described above is an optical phase modulator in which electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator that does not have an axis or plane of symmetry, and an optical fiber is wound around the outer circumference. Second, the optical phase is a cylindrical piezoelectric vibrator that has no point or axis of symmetry in its cross-sectional shape and whose walls are not uniform in length, with electrodes formed on the inside and outside, and an optical fiber wrapped around the outside. To describe in more detail, first, electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator whose outer shape is cylindrical, elliptical, or prismatic with rounded corners, and whose wall thickness is not uniform. , an optical phase modulator in which an optical fiber is wound around the outer periphery, and secondly, inside a piezoelectric vibrator whose outer shape is a cylinder, an elliptical cylinder, or a prism with rounded corners, the cylinder, elliptic cylinder, or prism with rounded corners is placed inside the piezoelectric vibrator. ,
Electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator, which has a cylindrical, elliptical, or prismatic cavity with rounded corners that do not have the same central axis, axis of symmetry, or plane of symmetry, and an optical fiber is wound around the outer periphery. It is an optical phase modulator, and thirdly, a piezoelectric vibrator with a cylindrical, elliptical, or prismatic shape with rounded corners has a shape in which a part of a cone, elliptical cone, or square pyramid with rounded corners is cut out. It is an optical phase modulator in which electrodes are formed on the inner and outer sides of a cylindrical piezoelectric vibrator with a cavity, and an optical fiber is wound around the outer periphery. It is an optical phase modulator in which electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator that has a stacked shape of round prisms and a cavity is formed inside, and an optical fiber is wound around the outer circumference. Electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator, which has the shape of a cylinder, an elliptic cylinder, or a rectangular cylinder with rounded corners with a part cut out, and whose wall thickness is not uniform. Electrodes are formed on the inside and outside, and an optical fiber is wound around the outside. Sixthly, a cylindrical piezoelectric vibrator having a cylindrical, elliptical, or prismatic shape with rounded corners is placed in a plane that is not orthogonal to the central axis of the cylinder, elliptical, or prismatic with rounded corners. This is an optical phase modulator in which electrodes are formed on the inside and outside of a cut-shaped piezoelectric vibrator, and an optical fiber is wound around the outer circumference.
作 用
本発明にかかる、対称軸や対称面を多くとも1つしか持
たない圧電振動子の、一対の電極間に振動電圧を印加す
ると、対称性が低いので、顕著な共振が起こりにくい。Function: When an oscillating voltage is applied between a pair of electrodes of a piezoelectric vibrator having at most one axis or plane of symmetry according to the present invention, significant resonance is unlikely to occur because the symmetry is low.
そのため、このような圧電振動子の外周に光ファイバを
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
、顕著な共振特性が出現せず、平坦な特性が得られる。Therefore, the modulation frequency characteristic curve of an optical phase modulator constructed by winding an optical fiber around the outer periphery of such a piezoelectric vibrator does not exhibit significant resonance characteristics, and a flat characteristic is obtained.
特に、電極に特に肉厚が不均一な筒状圧電振動子の内側
と外側に電極を形成したものでは、両電極間に振動電圧
を印加したとき、光の位相変調特性と密接に関係した動
径方向振動に関して顕著な共振が起こりにくくなる。筒
状圧電振動子の動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 particular, when electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator whose wall thickness is particularly uneven, when an oscillating voltage is applied between the two electrodes, a vibration occurs that is closely related to the phase modulation characteristics of light. Significant resonance with respect to radial vibration is less likely to occur. In addition to this, the resonance of the radial 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。こうすることによって、肉厚
に関係した振動モードの共振をさらに抑えることが可能
となり、平坦な変調周波数特性を得ることができた。To suppress this, it is effective to make the length of the wall of the cylindrical piezoelectric vibrator non-uniform. By doing this, it became possible to further suppress the resonance of the vibration mode related to the wall thickness, and it was possible to obtain flat modulation frequency characteristics.
対称性の低い圧電振動子として、円柱状または楕円柱状
または角の丸い角柱状の外形を持ち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、外形が円柱
状または楕円柱状または角の丸い角柱状なのでなので、
光ファイバを巻くことが容易であり、特に円柱の場合に
は製作上の困難が少ない。If a cylindrical piezoelectric vibrator with a cylindrical, elliptical, or rounded prismatic external shape and uneven wall thickness is used as a piezoelectric vibrator with low symmetry, no significant vibration mode resonance will occur. is obtained similarly. Furthermore, since the external shape is cylindrical, elliptical, or prismatic with rounded corners,
It is easy to wind the optical fiber, and there are few manufacturing difficulties, especially in the case of a cylinder.
内側に設ける空洞を、外形の円柱または楕円柱または角
が丸い角柱と、中心軸または対称軸または対称面を同一
としない円柱状または楕円柱状または角が丸い角柱状空
洞とすれば、さらに本発明にかかる圧電振動子の製作が
容易となる。内側に設ける空洞を、円錐または楕円錐ま
たは角の丸い角錘の一部を切りとった形状とした筒状圧
電振動子は、断面形状のみならず長さ方向に対する対称
性も低いので、共振の抑制効果が太きい。また、製作上
特に困難が増すこともない。If the cavity provided inside is a cylindrical, elliptical cylindrical, or prismatic cavity with rounded corners that does not have the same central axis, axis of symmetry, or plane of symmetry as the external cylinder, elliptical cylinder, or prismatic cylinder with rounded corners, the present invention further provides the present invention. This makes it easy to manufacture piezoelectric vibrators. A cylindrical piezoelectric vibrator whose inner cavity is shaped like a partially cut out cone, elliptical cone, or rounded pyramid has low symmetry not only in the cross-sectional shape but also in the length direction, making it difficult to suppress resonance. The effect is strong. Further, there is no particular increase in the difficulty in manufacturing.
肉厚が均一ではない筒状圧電振動子において、外形の円
柱または楕円柱または角が丸い角柱の一部を切り欠いた
形状でとすれば、長さ方向に対する対称性も低下させる
事ができ、容易に大きな共振抑制効果を得ることができ
る。特に、外形が円柱状または楕円柱状または角が丸い
角柱状の筒状圧電振動子を、前記円柱または楕円柱また
は角が丸い角柱の中心軸と直交しない平面で切断した形
状は、製作が非常に容易で、且つ犬き々共振抑制効果を
得ることができる。In a cylindrical piezoelectric vibrator whose wall thickness is not uniform, if the external shape is a circular cylinder, an elliptical cylinder, or a square cylinder with rounded corners with a part cut out, the symmetry in the length direction can be reduced. A large resonance suppression effect can be easily obtained. In particular, it is very difficult to manufacture a cylindrical piezoelectric vibrator whose external shape is a cylinder, an elliptical cylinder, or a prism with rounded corners, cut by a plane that is not perpendicular to the central axis of the cylinder, elliptic cylinder, or rectangular pillar with rounded corners. It is easy to use and can effectively suppress resonance in dogs.
外形が大きさの異なる円柱または楕円柱または角が丸い
角柱を積み重ねた形状で、内部に空洞が形成されている
筒状の圧電振動子を用いれば、大きさの異なる円柱また
は楕円柱または角が丸い角柱が持つそれぞれの共振特性
を、互いに打ち消し合わせることができ、平坦な変調周
波数特性を得ることができる。If you use a cylindrical piezoelectric vibrator whose outer shape is a stack of cylinders or elliptical cylinders of different sizes or square cylinders with rounded corners and a hollow inside, it will be possible to combine cylinders or elliptical cylinders of different sizes or square pillars with rounded corners. The respective resonance characteristics of the round prisms can cancel each other out, and a flat modulation frequency characteristic can be obtained.
実施例
第1図は本発明にかかる光フアイバ型光位相変調器の実
施例の斜視図である。1]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。Embodiment FIG. 1 is a perspective view of an embodiment of an optical fiber type optical phase modulator according to the present invention. 1] is a cylindrical piezoelectric vibrator with a cylindrical outer shape made of lead titanate-based ceramic, and 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30 mmで、外周には光ファ
イバ】3が3回巻かれている。内側の空洞の直径は10
Mで、外形の円柱の中心軸にたいして、7 mm偏心
している。The outer diameter of the cylindrical piezoelectric vibrator is 30 mm, and an optical fiber 3 is wound around the outer circumference three times. The diameter of the inner cavity is 10
M, and is eccentric by 7 mm with respect to the central axis of the external cylinder.
贅だ長さ方向(で関し、外形の円柱の中心軸と直交しな
い平面で切断した形状となっている。筒状圧電振動子1
1の内側と外側には電極14 と15が形成さ′i′し
ており、両電極間に振動電圧を印加することによって、
圧電振動子は動径方向に振動する。The shape is cut along a plane that is not perpendicular to the central axis of the external cylinder. Cylindrical piezoelectric vibrator 1
Electrodes 14 and 15 are formed on the inside and outside of 1, and by applying an oscillating voltage between the two electrodes,
The piezoelectric vibrator vibrates in the radial direction.
この実施例にかかる圧電振動子は、内側の円柱状空洞の
中心軸が偏心しでいるので、肉厚が不均一となっている
。長さ方向に関しても、偏氾・方向とは違う方向(で傾
いた面で切断した形状なので、壁の長さが一様ではなく
、顕著な振動モートの共振が現れない。このため、第2
図に示した良好な光位相変調周波数特性の平坦性を得る
ことができる0
光フアイバー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、七ロダインカ式は鳴動な方式の一つで
ある。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〜]m5eC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力らない。本発明にかかる光
位相変調器を用いて、上記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イハ号を得ること
ができた。In the piezoelectric vibrator according to this embodiment, the central axis of the inner cylindrical cavity is eccentric, so the wall thickness is non-uniform. Regarding the length direction, since the shape is cut with an inclined surface in a direction different from the uneven flooding direction, the length of the wall is not uniform, and the resonance of the vibration mote does not appear.For this reason, the second
As shown in the figure, the good flatness of the optical phase modulation frequency characteristic can be obtained. The Seven Rod Inker method is one of the most effective methods for performing high-precision signal processing in optical fiber gyros and the like. This method requires optical phase modulation using a sawtooth wave, and an optical phase modulator with a wide band that can perform optical phase modulation using a sawtooth wave signal with a period of 10 μsec to ]m5eC must be used. No pressure. When optical phase modulation was carried out using the above-mentioned sawtooth wave using the optical phase modulator according to the present invention, it was possible to obtain a modulation I/H number that poses no problem in practice.
次に、本発明にかかる圧電振動子形状の他の実施例を示
す。第3図は楕円柱状の外形の圧電振動子41 に、こ
の楕円柱と対称面や対称軸が一致しない楕円柱形状の空
洞・12を設け、内側と外側に電極43と44を形成し
た実施例である0肩の部分には切り欠き45 を設けて
おり、楕円柱の高さ方向(で関しての対称性を低くする
事にも配慮している。第4図は、角の丸い三角柱状の圧
電振動子51 の内部に、円錐の一部を切りとった形状
の空洞52 を設け、内側と外側に電極53 と54を
形成した実施例である。このような形状の圧電振動子の
外周に光ファイバを巻いた本発明にかかる光位相変調器
は、あらゆる方向に、肉厚が不均一であり、極めて良好
な変調周波数特性を得ることができる。第5図は、直径
の異なる3個の円柱を、中心軸をずらせて重ねた形状の
圧電振動子61の内部に、円柱状の空洞62を設け、電
極62と63形成した実施例である。光ファイバは、3
個の円柱全てQて所定の回数券いて、光位相変調器を構
成する。この位相変調器に入射した光は、3つの円柱部
分で順次変調される。3つの円柱部分の共振特性が、最
適に打ち消し合うように円柱の大きさが決められており
、これによって良好な変調周波数特性が得られる。Next, other embodiments of the piezoelectric vibrator shape according to the present invention will be shown. FIG. 3 shows an embodiment in which a piezoelectric vibrator 41 having an elliptical external shape is provided with an elliptic cylindrical cavity 12 whose plane of symmetry and axis of symmetry do not coincide with the elliptical cylinder, and electrodes 43 and 44 are formed on the inside and outside. A notch 45 is provided in the shoulder part of the elliptical cylinder to reduce the symmetry in the height direction of the elliptical cylinder. Figure 4 shows a triangular cylinder with rounded corners. This is an embodiment in which a cavity 52 in the shape of a partially cut out cone is provided inside a piezoelectric vibrator 51, and electrodes 53 and 54 are formed on the inside and outside. The optical phase modulator according to the present invention, which is wound with optical fiber, has non-uniform wall thickness in all directions and can obtain extremely good modulation frequency characteristics. This is an embodiment in which a cylindrical cavity 62 is provided inside a piezoelectric vibrator 61 having a shape in which cylinders are stacked with their center axes shifted, and electrodes 62 and 63 are formed.
The optical phase modulator is constructed by applying all the cylinders Q a predetermined number of times. The light incident on this phase modulator is sequentially modulated by the three cylindrical parts. The size of the cylinder is determined so that the resonance characteristics of the three cylinder parts optimally cancel each other out, thereby obtaining good modulation frequency characteristics.
以上にあげた実施例の他にも、本発明の各請求項に記載
された手法を、適機宜組み合わせることによって、いろ
いろ々形状の、変調周波数特性の平坦な光位相変調器を
容易に得ることが可能である。In addition to the embodiments mentioned above, optical phase modulators of various shapes with flat modulation frequency characteristics can be easily obtained by appropriately combining the techniques described in each claim of the present invention. is possible.
発明の効果
以上のよう(・τ本発明は、光位相変調の周波数特性が
平坦なファイバ形光位相変調器を実現することができ、
本発明の構造を持ってすれば、圧N撮動子製作上の問題
も少なく、光ファイバも容易に巻くことができる。贅だ
、ファイバ形光位相変調器が持つ、ファイバとの結合が
容易という特徴を失うこともない。Effects of the Invention As described above (・τ), the present invention can realize a fiber-type optical phase modulator with flat frequency characteristics of optical phase modulation.
With the structure of the present invention, there are fewer problems in manufacturing the pressure-N sensor, and optical fibers can be easily wound. What's more, it does not lose the characteristic of fiber-type optical phase modulators, which is that they can be easily coupled to fibers.
第1図は本発明にかかる光位相変調器の一実施例の斜視
図、第2図は振幅一定の印加変調信号に対する本発明に
かかる光位相変調器の変調周波数特性図、第3図と第4
図と第5図は本発明にかかる光位相変調器の圧電振動子
の実施例の斜視図、第6図は従来技術によるファイバ形
光位相変調器の斜視図、第7図は振幅一定の印加変調信
号に対する、従来技術による光位相変調器の変調周波数
特性図である。
11・・筒状圧電振動子、12 偏心円柱状空洞、1
3・・・光ファイバ、21−・ 円筒状圧電振動子、2
2−・・光ファイバ。
代理人の氏名 弁理士 小鍜治 明 ほか2名第1
図
第2図
変調N我べ
第3図
4−44L極 42稈巴枳?洞
第4図
5に町社披帽庫刺子
第5図
第6図
23賓寝
7・′
ゝ \2,44、−一4
\22えヮフイバFIG. 1 is a perspective view of an embodiment of the 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 FIGS. 4
5 and 5 are perspective views of an embodiment of a piezoelectric vibrator of an optical phase modulator according to the present invention, FIG. 6 is a perspective view of a fiber type optical phase modulator according to the prior art, and FIG. 7 is a perspective view of an embodiment of a piezoelectric vibrator of an optical phase modulator according to the present invention. FIG. 3 is a modulation frequency characteristic diagram of an optical phase modulator according to the prior art with respect to a modulated signal. 11...Cylindrical piezoelectric vibrator, 12 Eccentric cylindrical cavity, 1
3... Optical fiber, 21-- Cylindrical piezoelectric vibrator, 2
2--Optical fiber. Name of agent: Patent attorney Akira Okaji and two others 1st
Figure 2 Modulation N Gabe Figure 3 4-44 L pole 42 Culm bar? In the cave No. 4, Figure 5, the town shrine's hat storehouse, Sashiko, Figure 5, Figure 6, Figure 23, 7.'
Claims (9)
い形状の圧電振動子の表面に、少なくとも1対の電極を
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。(1) A light characterized by forming at least one pair of electrodes on the surface of a piezoelectric vibrator having at most one axis of symmetry or one plane of symmetry, and winding an optical fiber around the outer periphery. Phase modulator.
子の内側と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請求項1記載の光位相変調器。(2) The optical phase modulator according to claim 1, wherein 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 periphery.
長さが一様でない筒状圧電振動子の、内側と外側に電極
を形成し、外周に光ファイバを巻いたことを特徴とする
請求項1記載の光位相変調器。(3) Electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator that does not have a symmetry point or axis of symmetry in its cross-sectional shape and whose wall length is not uniform, and an optical fiber is wound around the outer circumference. The optical phase modulator according to claim 1.
状で、肉厚が均一ではない筒状の圧電振動子の、内側と
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。(4) Electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator whose external shape is cylindrical, elliptical, or prismatic with rounded corners and whose wall thickness is not uniform, and an optical fiber is wound around the outer circumference. Features of optical phase modulator.
状の圧電振動子の内部に、前記円柱または楕円柱または
角が丸い角柱と、中心軸または対称軸または対称面を同
一としない円柱状または楕円柱状または角が丸い角柱状
空洞を設けた筒状圧電振動子の、内側と外側に電極を形
成し、外周に光ファイバを巻いたことを特徴とする請求
項4記載の光位相変調器。(5) Inside a piezoelectric vibrator whose external shape is cylindrical, elliptical, or prismatic with rounded corners, there is a cylindrical shape whose central axis, axis of symmetry, or plane of symmetry is not the same as the cylinder, elliptical, or prismatic with rounded corners. or an optical phase modulator according to claim 4, characterized in that electrodes are formed on the inner and outer sides of a cylindrical piezoelectric vibrator having an elliptical cylinder shape or a prismatic cavity with rounded corners, and an optical fiber is wound around the outer periphery. .
状の圧電振動子の内部に、円錐または楕円錐または角の
丸い角錘の一部を切りとった形状の空洞を設けた筒状圧
電振動子の、内側と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請求項4記載の光位相変
調器。(6) Cylindrical piezoelectric vibration in which a cavity in the shape of a part of a cone, elliptical cone, or rounded pyramid is provided inside a piezoelectric vibrator with a cylindrical, elliptical, or prismatic shape with rounded corners. 5. The optical phase modulator according to claim 4, wherein electrodes are formed on the inside and outside of the child, and an optical fiber is wound around the outer periphery.
部を切り欠いた形状で、肉厚が均一ではない筒状の圧電
振動子の、内側と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。(7) Electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator whose external shape is a cylinder, an elliptic cylinder, or a rectangular cylinder with rounded corners with a part cut out, and whose wall thickness is not uniform. An optical phase modulator characterized by a wound fiber.
状の筒状圧電振動子を、前記円柱または楕円柱または角
が丸い角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、内側と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。(8) A piezoelectric vibrator having a shape obtained by cutting a cylindrical piezoelectric vibrator having a cylindrical, elliptical, or prismatic shape with rounded corners along a plane that is not perpendicular to the central axis of the cylinder, elliptical, or prismatic with rounded corners. , an optical phase modulator characterized by forming electrodes on the inside and outside and having an optical fiber wound around the outside.
が丸い角柱を積み重ねた形状で、内部に空洞が形成され
ている筒状の圧電振動子の、内側と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請求項8
記載の光位相変調器。(9) Electrodes are formed on the inside and outside of a cylindrical piezoelectric vibrator that has a stacked shape of cylinders, elliptical cylinders, or square cylinders with rounded corners of different sizes, and has a cavity inside. Claim 8 characterized in that an optical fiber is wound around the
The optical phase modulator described.
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP27393690A JPH04147210A (en) | 1990-10-11 | 1990-10-11 | 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 |
---|---|---|---|
JP27393690A JPH04147210A (en) | 1990-10-11 | 1990-10-11 | Optical phase modulator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04147210A true JPH04147210A (en) | 1992-05-20 |
Family
ID=17534633
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP27393690A Pending JPH04147210A (en) | 1990-06-05 | 1990-10-11 | Optical phase modulator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04147210A (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
- 1990-10-11 JP JP27393690A patent/JPH04147210A/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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