JPH0534166A - Optical fiber gyro - Google Patents

Optical fiber gyro

Info

Publication number
JPH0534166A
JPH0534166A JP19405091A JP19405091A JPH0534166A JP H0534166 A JPH0534166 A JP H0534166A JP 19405091 A JP19405091 A JP 19405091A JP 19405091 A JP19405091 A JP 19405091A JP H0534166 A JPH0534166 A JP H0534166A
Authority
JP
Japan
Prior art keywords
optical fiber
light
polarization
optical
maintaining
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.)
Granted
Application number
JP19405091A
Other languages
Japanese (ja)
Other versions
JP2514491B2 (en
Inventor
Aritaka Ono
有孝 大野
Shinji Motohara
伸二 本原
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.)
Japan Aviation Electronics Industry Ltd
Original Assignee
Japan Aviation Electronics Industry 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 Japan Aviation Electronics Industry Ltd filed Critical Japan Aviation Electronics Industry Ltd
Priority to JP3194050A priority Critical patent/JP2514491B2/en
Priority to US07/897,748 priority patent/US5187757A/en
Priority to EP92110078A priority patent/EP0520282B1/en
Priority to DE69225639T priority patent/DE69225639T2/en
Publication of JPH0534166A publication Critical patent/JPH0534166A/en
Application granted granted Critical
Publication of JP2514491B2 publication Critical patent/JP2514491B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To obtain a stable gyro output in the inexpensive structure even when the double refraction of a single mode optical fiber is changed by inclining main axes of an optical diverging means and two optical fibers preserving the plane of polarization by 45 deg.. CONSTITUTION:The light reaching a connecting point 23 from a polarizer 13 through an optical fiber coupler 14 which holes the plane of polarization is a lineary-polarized light propagated through one of polarization holding axes 24x and 24y of the coupler 14. The lineary-polarized light emission enters two optical fibers 16b holding the plane of polarization at the connecting point 23 by 45 deg. to a polarization holding axis 25x. As a result of this, the linearly- polarized light is separated into two components of the same intensity of the holding axes 25x and 25y orthogonal to each other and, propagated in the fibers 16b. Even when the double refraction of a single mode optical fiber 16a is changed and a polarization holding axis thereof is changed, one is decreased when the other of the two components is increased, so that the light is constant at all times. Accordingly, the intensity of light reaching a photodetector is made constant.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は光ファイバコイルに右
回り光と左回り光とを伝播させ、これら右回り光と左回
り光との位相差を検出して光ファイバコイルに印加され
るその中心回りの角速度を検出する光ファイバジャイロ
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention propagates clockwise light and counterclockwise light in an optical fiber coil, detects the phase difference between these clockwise light and counterclockwise light, and applies them to the optical fiber coil. The present invention relates to an optical fiber gyro that detects an angular velocity around a center.

【0002】[0002]

【従来の技術】図2に従来の光ファイバジャイロを示
す。光源11からの光は光ファイバカプラなどの光分岐
器12を通り、更に偏光子13を通って所定の偏光方向
の成分のみが取り出され、その偏光子13からの光は光
ファイバカプラなどの光分岐器14で2分配され、その
一方の光は光ファイバコイル16の一端に右回り光とし
て入射され、他方の光は光位相変調器17を通って光フ
ァイバコイル16の他端に左回り光として入射される。
2. Description of the Related Art FIG. 2 shows a conventional optical fiber gyro. The light from the light source 11 passes through an optical branching device 12 such as an optical fiber coupler, and further passes through a polarizer 13 to extract only a component in a predetermined polarization direction. The light from the polarizer 13 is a light such as an optical fiber coupler. The light is split into two by the branching device 14, one light of which is incident on one end of the optical fiber coil 16 as a clockwise light, and the other light passes through the optical phase modulator 17 and is counterclockwise light on the other end of the optical fiber coil 16. Is incident as.

【0003】光ファイバコイル16を伝播した右回り光
と左回り光とは光分岐器14に戻って合成されて干渉
し、その干渉光は偏光子13で所定の偏光方向の成分の
みが取り出され、その偏光子13を通過した光は光分岐
器12で分岐されて光検出器18に入射され、その光の
強度に応じた電気信号に変換される。変調信号発生器1
9からの周期関数、例えば正弦波信号により光位相変調
器17が駆動され、これを通過する光が位相変調され
る。光検出器18の出力は同期検波回路21で変調信号
発生器19からの基準信号により同期検波され、その検
波出力は出力端子22に出力される。
The right-handed light and the left-handed light propagating through the optical fiber coil 16 return to the optical branching device 14 to be combined and interfere with each other, and the interfering light is extracted by the polarizer 13 only in a predetermined polarization direction. The light that has passed through the polarizer 13 is split by the optical splitter 12 and is incident on the photodetector 18, and is converted into an electrical signal corresponding to the intensity of the light. Modulation signal generator 1
The optical phase modulator 17 is driven by the periodic function from 9, for example, a sine wave signal, and the light passing therethrough is phase-modulated. The output of the photodetector 18 is synchronously detected by the synchronous detection circuit 21 by the reference signal from the modulation signal generator 19, and the detected output is output to the output terminal 22.

【0004】光ファイバコイル16に、その軸心回りの
角速度が印加されていない状態では、光ファイバコイル
16を伝播した右回り光と、左回り光との位相差はゼロ
であり、同期検波回路21の出力もゼロであるが、光フ
ァイバコイル16に、その軸心回りの角速度が印加され
ると、これに応じて右回り光と左回り光とに位相差が生
じ、同期検波回路21から、前記印加角速度の方向およ
び大きさに応じた極性およびレベルの出力が生じ、印加
角速度を検出することができる。
When the angular velocity around the axis of the optical fiber coil 16 is not applied, the phase difference between the clockwise light propagating through the optical fiber coil 16 and the counterclockwise light is zero, and the synchronous detection circuit. The output of 21 is also zero, but when an angular velocity around the axis is applied to the optical fiber coil 16, a phase difference occurs between the clockwise light and the counterclockwise light in response to this, and the synchronous detection circuit 21 The output of the polarity and level according to the direction and magnitude of the applied angular velocity is generated, and the applied angular velocity can be detected.

【0005】このように光ファイバジャイロは右回り光
と、左回り光との位相差を検出するものであるが、光フ
ァイバコイル16を伝播中に、偏波状態が変化し、偏光
方向が直角な成分が生じると、光ファイバコイル16に
複屈折性がわずか存在しているため、これら直角な偏光
方向の両光は光ファイバコイル16の伝播速度が異な
り、従って、光分岐器14で合成される右回り光の一方
の偏光成分と、左回り光の他方の偏光成分とが干渉する
と、右回り光と左回り光との位相差を正しく検出するこ
とができなくなる。
As described above, the optical fiber gyroscope detects the phase difference between the clockwise light and the counterclockwise light. However, the polarization state changes during propagation through the optical fiber coil 16, and the polarization direction is right angle. When there is such a component, since the optical fiber coil 16 has a small amount of birefringence, the two lights in the orthogonal polarization directions have different propagation velocities in the optical fiber coil 16 and are thus combined by the optical branching device 14. If one polarization component of the clockwise light and the other polarization component of the counterclockwise light interfere with each other, the phase difference between the clockwise light and the counterclockwise light cannot be correctly detected.

【0006】このような点から従来においては、光ファ
イバコイル16に偏波面保存光ファイバを用いるのが一
般的であった。この場合は光ファイバコイル16を伝播
する右回り光と左回り光との偏光状態が安定に保たれる
ので、ジャイロ性能が安定している。しかしながら、偏
波面保存光ファイバは高価であるため、光ファイバジャ
イロの全体の価格の半分程度にもなる欠点があった。
From this point of view, conventionally, it has been general to use a polarization-maintaining optical fiber for the optical fiber coil 16. In this case, the polarization states of the clockwise light and the counterclockwise light propagating through the optical fiber coil 16 are kept stable, so that the gyro performance is stable. However, since the polarization-maintaining optical fiber is expensive, there is a drawback that it is about half the total price of the optical fiber gyro.

【0007】この問題を解決し、安価で性能の安定した
光ファイバジャイロを、特願平3−158768で提案
した。これは図3に示すように光ファイバコイル16と
して安価なシングルモード光ファイバ16aと、その両
端に接続した余長部の偏波面保存光ファイバ16bとに
より構成し、コイル化の曲げによりシングルモード光フ
ァイバ16aに生じる複屈折性により、偏波面保存光フ
ァイバと同等の偏波保持性をもたせ、曲げが生じない余
長部分に偏波面保存光ファイバ16bを用い偏光状態を
安定に保っている。
An optical fiber gyro that solves this problem and is stable in performance has been proposed in Japanese Patent Application No. 3-158768. As shown in FIG. 3, this is composed of an inexpensive single-mode optical fiber 16a as an optical fiber coil 16 and a polarization-maintaining optical fiber 16b with extra lengths connected to both ends thereof. Due to the birefringence generated in the fiber 16a, the polarization maintaining property equivalent to that of the polarization maintaining optical fiber is provided, and the polarization maintaining optical fiber 16b is used in the extra length portion where bending does not occur to maintain the stable polarization state.

【0008】この構成により、安価でかつ全体を偏波面
保存光ファイバとした場合と同等の安定した光ファイバ
ジャイロが得られる。
With this structure, it is possible to obtain a stable optical fiber gyro which is inexpensive and is equivalent to the case where the whole polarization plane maintaining optical fiber is used.

【0009】[0009]

【発明が解決しようとする課題】しかしながら、図3に
示した光ファイバジャイロにおいては、曲げ応力により
シングルモード光ファイバ16aに生じる複屈折性を利
用しているため、コイルボビンとシングルモード光ファ
イバ16aとの熱膨張の差により生じる熱応力の影響に
より、シングルモード光ファイバ16aに生じている複
屈折性が変化しやすく、光ファイバコイル16における
偏波保持性の変化をまねき、つまり偏波保持軸が変化
し、この結果、偏光子13を通過して光検出器18に至
る干渉光の光量が変化するため、特に温度変化に対し、
光ファイバジャイロの出力変化が生じやすいという問題
がある。
However, in the optical fiber gyro shown in FIG. 3, since the birefringence generated in the single mode optical fiber 16a due to the bending stress is utilized, the coil bobbin and the single mode optical fiber 16a are used. Due to the effect of thermal stress caused by the difference in thermal expansion between the two, the birefringence generated in the single-mode optical fiber 16a is likely to change, which causes a change in polarization maintaining property in the optical fiber coil 16, that is, the polarization maintaining axis is Change, and as a result, the amount of interference light that passes through the polarizer 13 and reaches the photodetector 18 changes.
There is a problem that the output of the optical fiber gyro is likely to change.

【0010】[0010]

【課題を解決するための手段】請求項1の発明によれ
ば、光ファイバコイルをシングルモード光ファイバと、
その両端に接続した2本の偏波面保存光ファイバとによ
り構成し、そのシングルモード光ファイバの曲げ応力に
より生じる複屈折性を利用し、かつ光分岐手段と、光フ
ァイバコイル両端の前記2本の偏波面保存光ファイバと
の接続点において、前記偏波面保存光ファイバと前記光
分岐手段との主軸を互いに45°傾斜させている。
According to the invention of claim 1, the optical fiber coil is a single mode optical fiber,
It is composed of two polarization-maintaining single-mode optical fibers connected to both ends thereof, and utilizes the birefringence caused by bending stress of the single-mode optical fiber. At the connection point with the polarization-maintaining optical fiber, the principal axes of the polarization-maintaining optical fiber and the optical branching means are inclined by 45 ° with respect to each other.

【0011】請求項2の発明によれば、光ファイバコイ
ルをシングルモード光ファイバと、その両端に接続した
2本の偏波面保存光ファイバとにより構成し、そのシン
グルモード光ファイバの曲げ応力により生じる複屈折性
を利用し、かつ光源よりの光を偏光子を通じて光分岐手
段へ入射し、その光分岐手段を偏波面保存光伝送路で構
成し、その光分岐手段と偏光子との主軸を互いに45°
傾斜させている。
According to the invention of claim 2, the optical fiber coil is composed of a single mode optical fiber and two polarization-maintaining optical fibers connected to both ends of the single mode optical fiber, and is generated by bending stress of the single mode optical fiber. Utilizing the birefringence, the light from the light source is incident on the optical branching means through the polarizer, and the optical branching means is constituted by the polarization-maintaining optical transmission line, and the main axes of the optical branching means and the polarizer are mutually 45 °
It is inclined.

【0012】請求項1の発明、請求項2の発明において
も、光ファイバコイルに入射される光は偏波面保存光フ
ァイバの各互いに直交した二つの偏波保存軸のほゞ同一
強度の成分として伝播するため、シングルモード光ファ
イバの部分で複屈折性が変動し、その偏波保存軸方向が
変化しても、前記直角な二成分の偏光子の通過成分は、
一方が減少したとき、他方が増加し、常に一定となり、
干渉光の強度は変化しない。
Also in the inventions of claim 1 and claim 2, the light incident on the optical fiber coil is a component having almost the same intensity of two polarization maintaining axes of the polarization maintaining optical fiber which are orthogonal to each other. Since it propagates, the birefringence fluctuates in the part of the single mode optical fiber, and even if the polarization maintaining axis direction changes, the passing component of the orthogonal two-component polarizer is
When one decreases, the other increases and is always constant,
The intensity of the interference light does not change.

【0013】[0013]

【実施例】図1にこの発明による光ファイバジャイロの
要部を示し、図3と対応した部分に同一符号を付けてあ
る。この発明においては図3と同様に、光ファイバコイ
ル16はシングルモード光ファイバ16aとその両端に
接続された2本の偏波面保存光ファイバ16bとよりな
る。この例では光分岐器14として偏波面保存光ファイ
バカプラを用いた場合である。この偏波面保存光ファイ
バカプラ14と2本の偏波面保存光ファイバ16bとの
接続点23を分離し、かつその端面を拡大して示すよう
に、偏波面保存光ファイバカプラ14の端面における互
いに直交する偏波保持軸24x(X軸)および24y
(Y軸)と、2本の偏波面保存光ファイバ16bの端面
における互いに直交する偏波保持軸25x(X軸)およ
び25y(Y軸)とが軸心まわりに互いにほゞ45°ず
らされている。
DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 shows the essential parts of an optical fiber gyro according to the present invention, and the parts corresponding to those in FIG. In the present invention, as in FIG. 3, the optical fiber coil 16 is composed of a single mode optical fiber 16a and two polarization-maintaining optical fibers 16b connected to both ends thereof. In this example, a polarization maintaining optical fiber coupler is used as the optical branching device 14. The connection point 23 between the polarization-maintaining single-mode fiber coupler 14 and the two polarization-maintaining single-mode optical fibers 16b is separated, and the end face thereof is enlarged. Polarization maintaining axes 24x (X axis) and 24y
(Y axis) and the polarization maintaining axes 25x (X axis) and 25y (Y axis) orthogonal to each other at the end faces of the two polarization-maintaining single-mode fibers 16b are displaced from each other by about 45 ° about the axis. There is.

【0014】このため偏光子13から偏波面保存光ファ
イバカプラ14を通って接続点23に達した光は、偏波
面保存光ファイバカプラ14の偏波保持軸24xまたは
24yのどちらかを伝播してきた直線偏光であって、直
線偏光は接続点23において2本の偏波面保存光ファイ
バ16bにその偏波保持軸25x(X軸)に対して45
°の角度で入射する。この結果、この直線偏光は偏波面
保存光ファイバ16bを2つの直交する偏波保持軸25
x,25yの二つの同一強度の成分に分けられて伝播す
る。つまり、偏波保持軸25x,25yと平行した同一
強度の直線偏光が偏波面保存光ファイバ16bに入射さ
れたことになる。これらが光ファイバコイル16を通
り、更に光ファイバカプラ14を通って偏光子13に戻
った光の偏光子13の通過成分についてみると、熱応力
変動などによりシングルモード光ファイバ16aの複屈
折性が変化して、その偏波保持軸が変化(回動)して
も、上記二つの成分の一方が増加するとき、他方が減少
し、常に一定となり、このため光検出器18に達する光
の強度は一定となり、安定したジャイロ出力が得られ
る。
Therefore, the light that has reached the connection point 23 from the polarizer 13 through the polarization-maintaining optical fiber coupler 14 has propagated through either the polarization-maintaining axis 24x or 24y of the polarization-maintaining optical fiber coupler 14. It is linearly polarized light, and the linearly polarized light is 45 in the two polarization-maintaining optical fibers 16b at the connection point 23 with respect to the polarization maintaining axis 25x (X axis).
Incident at an angle of °. As a result, this linearly polarized light is transmitted through the polarization-maintaining optical fiber 16b through two orthogonal polarization-maintaining axes 25.
It is propagated after being divided into two components of the same intensity x and 25y. That is, the linearly polarized light of the same intensity parallel to the polarization maintaining axes 25x and 25y is incident on the polarization-maintaining optical fiber 16b. Looking at the passing components of the polarizer 13 of the light passing through the optical fiber coil 16 and further back to the polarizer 13 through the optical fiber coupler 14, the birefringence of the single mode optical fiber 16a due to thermal stress fluctuation or the like is observed. Even if the polarization maintaining axis changes (rotates) due to the change, when one of the two components increases, the other decreases and becomes constant, so that the intensity of the light reaching the photodetector 18 increases. Is constant and a stable gyro output is obtained.

【0015】接続点23においては一般には光ファイバ
の融着接続が行われるが、レンズ結合、光ファイバ同士
の光接続などで結合させてもよい。光分岐手段14とし
て光集積回路によるものを用いてもよい。二つの偏波面
保存光ファイバ16bに、その二つの偏波保持軸25
x,25yにそれぞれ平行な同一強さの直線偏光を入射
すればよいから、偏光子13と光分岐手段14との接続
において、偏光子13側の例えば光ファイバの偏波保持
軸と、光分岐手段14側の例えば光ファイバの偏波保持
軸とを互いに45°かたむけて、偏光子13側の一つの
偏波保持軸と平行した直線偏光を光分岐手段14側へ入
射させてもよい。
At the connection point 23, fusion splicing of optical fibers is generally performed, but they may be coupled by lens coupling, optical coupling between optical fibers, or the like. An optical integrated circuit may be used as the optical branching means 14. The two polarization-maintaining optical fibers 16b are connected to the two polarization-maintaining axes 25
Since it suffices to input linearly polarized light of the same intensity parallel to x and 25y respectively, in the connection between the polarizer 13 and the optical branching means 14, for example, the polarization maintaining axis of the optical fiber on the side of the polarizer 13 and the optical branching. For example, linearly polarized light parallel to one polarization maintaining axis on the side of the polarizer 13 may be incident on the side of the optical branching means 14 by making the polarization maintaining axis of the optical fiber on the side of the means 14 side away from each other by 45 °.

【0016】[0016]

【発明の効果】以上述べたように、この発明によれば光
ファイバコイル16をシングルモード光ファイバコイル
と、その両端に接続された2本の偏波面保存光ファイバ
とから構成しているため、安価に構成することができ、
しかも偏波面保存光ファイバに対し、その二つの偏波保
持軸とそれぞれ平行した二つの同一強度の直線偏光を入
射しているため、温度変化によりシングルモード光ファ
イバ16aの複屈折性が変化しても、安定したジャイロ
出力が得られる。
As described above, according to the present invention, the optical fiber coil 16 is composed of the single mode optical fiber coil and the two polarization maintaining optical fibers connected to both ends thereof. Can be configured inexpensively,
Moreover, since two linearly polarized light beams of the same intensity parallel to the two polarization-maintaining axes are incident on the polarization-maintaining optical fiber, the birefringence of the single-mode optical fiber 16a changes due to the temperature change. Also, stable gyro output can be obtained.

【図面の簡単な説明】[Brief description of drawings]

【図1】この発明の実施例の要部を示すブロック図。FIG. 1 is a block diagram showing a main part of an embodiment of the present invention.

【図2】従来の光ファイバジャイロを示すブロック図。FIG. 2 is a block diagram showing a conventional optical fiber gyro.

【図3】先に提案した光ファイバジャイロを示すブロッ
ク図。
FIG. 3 is a block diagram showing the previously proposed optical fiber gyro.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 光源よりの光を光分岐手段にて分配し
て、光ファイバコイルの両端から右回り光および左回り
光として入射し、これら両光をその光ファイバコイル伝
播後に、前記光分岐手段で干渉させ、その干渉光の強度
を電気信号に変換し、その電気信号から前記光ファイバ
コイルの中心回りに印加される角速度を検出する光ファ
イバジャイロにおいて、 前記光ファイバコイルはシングルモード光ファイバとそ
の両端に接続された2本の偏波面保存光ファイバとから
なり、 前記光分岐手段と前記2本の偏波面保存光ファイバとの
主軸が互いに45°傾斜していることを特徴とする光フ
ァイバジャイロ。
1. Light from a light source is distributed by a light branching means and is incident as right-handed light and left-handed light from both ends of an optical fiber coil. In the optical fiber gyro that causes interference by means, converts the intensity of the interference light into an electric signal, and detects the angular velocity applied around the center of the optical fiber coil from the electric signal, the optical fiber coil is a single mode optical fiber. And two polarization-maintaining single-mode optical fibers connected to both ends thereof, wherein the principal axes of the optical branching means and the two polarization-maintaining single-mode optical fibers are inclined by 45 ° with respect to each other. Fiber gyro.
【請求項2】 光源よりの光を偏光子を通じて光分岐手
段に入射して分配し、その分配光を光ファイバコイルに
その両端から右回り光および左回り光として入射し、こ
れら両光をその光ファイバコイル伝播後に、前記光分岐
手段で干渉させ、その干渉光を前記偏光子を通過させた
後、その強度を電気信号に変換し、その電気信号から前
記光ファイバコイルの中心回りに印加される角速度を検
出する光ファイバジャイロにおいて、 前記光ファイバコイルはシングルモード光ファイバとそ
の両端に接続された2本の偏波面保存光ファイバとから
なり、 前記光分岐手段は、偏波面保存光伝送路よりなり、 その光分岐手段と前記偏光子との主軸が互いに45°傾
斜していることを特徴とする光ファイバジャイロ。
2. Light from a light source is incident on a light splitting means through a polarizer to be distributed, and the distributed light is incident on both ends of the optical fiber coil as right-handed light and left-handed light. After propagating through the optical fiber coil, the optical branching means interferes with each other, the interference light is passed through the polarizer, and the intensity thereof is converted into an electric signal, and the electric signal is applied around the center of the optical fiber coil. In the optical fiber gyro for detecting an angular velocity, the optical fiber coil includes a single-mode optical fiber and two polarization-maintaining optical fibers connected to both ends thereof, and the optical branching unit includes a polarization-maintaining optical transmission line. An optical fiber gyro, characterized in that the principal axes of the light branching means and the polarizer are inclined by 45 ° with respect to each other.
JP3194050A 1991-06-28 1991-08-02 Fiber optic gyro Expired - Lifetime JP2514491B2 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP3194050A JP2514491B2 (en) 1991-08-02 1991-08-02 Fiber optic gyro
US07/897,748 US5187757A (en) 1991-06-28 1992-06-12 Fiber optic gyro
EP92110078A EP0520282B1 (en) 1991-06-28 1992-06-15 Fiber optic gyro
DE69225639T DE69225639T2 (en) 1991-06-28 1992-06-15 Optical fiber gyroscope

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3194050A JP2514491B2 (en) 1991-08-02 1991-08-02 Fiber optic gyro

Publications (2)

Publication Number Publication Date
JPH0534166A true JPH0534166A (en) 1993-02-09
JP2514491B2 JP2514491B2 (en) 1996-07-10

Family

ID=16318118

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3194050A Expired - Lifetime JP2514491B2 (en) 1991-06-28 1991-08-02 Fiber optic gyro

Country Status (1)

Country Link
JP (1) JP2514491B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002054933A (en) * 2000-08-14 2002-02-20 Tokimec Inc Optical fiber gyro

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62223614A (en) * 1986-03-26 1987-10-01 Toshiba Corp Optical fiber gyro

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62223614A (en) * 1986-03-26 1987-10-01 Toshiba Corp Optical fiber gyro

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002054933A (en) * 2000-08-14 2002-02-20 Tokimec Inc Optical fiber gyro

Also Published As

Publication number Publication date
JP2514491B2 (en) 1996-07-10

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