Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6310403B2 - - Google Patents
[go: Go Back, main page]

JPS6310403B2 - - Google Patents

Info

Publication number
JPS6310403B2
JPS6310403B2 JP57190395A JP19039582A JPS6310403B2 JP S6310403 B2 JPS6310403 B2 JP S6310403B2 JP 57190395 A JP57190395 A JP 57190395A JP 19039582 A JP19039582 A JP 19039582A JP S6310403 B2 JPS6310403 B2 JP S6310403B2
Authority
JP
Japan
Prior art keywords
polarization
fiber
cladding
core
fibers
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
Application number
JP57190395A
Other languages
Japanese (ja)
Other versions
JPS5979201A (en
Inventor
Shigefumi Masuda
Takeo Iwama
Akira Okamoto
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP57190395A priority Critical patent/JPS5979201A/en
Priority to CA000437093A priority patent/CA1238970A/en
Priority to DE8383305763T priority patent/DE3382205D1/en
Priority to EP83305763A priority patent/EP0107373B1/en
Publication of JPS5979201A publication Critical patent/JPS5979201A/en
Publication of JPS6310403B2 publication Critical patent/JPS6310403B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)

Description

【発明の詳細な説明】 (a) (発明の技術分野) 本発明は一方向の偏波面をそのまま維持して伝
送する所謂偏波面保存光フアイバーの改良に関
す。
DETAILED DESCRIPTION OF THE INVENTION (a) (Technical Field of the Invention) The present invention relates to improvements in so-called polarization-maintaining optical fibers that transmit data while maintaining the plane of polarization in one direction.

(b) 技術の背景 半導体レーザ、半導体受光素子および伝送路と
しての光フアイバーの開発進歩は、従来の電気通
信に代つて幾多の長所を備える所謂光通信技術を
著しく進歩させ、既にその実用化も著しい進展を
見せつつある。
(b) Background of the technology The progress in the development of semiconductor lasers, semiconductor photodetectors, and optical fibers as transmission lines has led to significant advances in so-called optical communication technology, which has many advantages over conventional telecommunications, and has already reached the point where it can be put into practical use. Significant progress is being made.

この際使用されている光フアイバーは、共に石
英材からなるクラツドタイプのもので、中心のコ
アー部と外周のクラツド部との屈折率の相違に基
づく界面全反射を利用して媒体であるレーザ光を
僅少な損失で伝送する。
The optical fibers used in this case are both clad type made of quartz material, and utilize total internal reflection based on the difference in refractive index between the central core and the outer cladding to emit laser light as a medium. Transmit with minimal loss.

この光フアイバーはレーザ光のどの方向の偏波
面も一様に伝送する。
This optical fiber uniformly transmits the polarization plane of laser light in any direction.

一方上記従来の光フアイバーと異なり、特定方
向の偏波面のシングルモードレーザ光はその偏波
面を保持して伝播させるが、他の方向の偏波面の
レーザ光をできるだけ減衰する所謂偏波面保存フ
アイバーも特殊目的のために開発されつつある。
On the other hand, unlike the conventional optical fibers mentioned above, a single mode laser beam with a polarization plane in a specific direction propagates while maintaining that polarization plane, but there are also so-called polarization preserving fibers that attenuate laser beams with polarization planes in other directions as much as possible. It is being developed for special purposes.

このような偏波面保存フアイバーを使用すれば
例えば波長の僅か異なる2個のレーザ光を偏波面
を一致させて該フアイバーの一端に入力させ、他
端より両者の位相差に該当する出力を得て、電気
的に変換することなく光の状態のままへテロダイ
ン検波機能を持たせることができる。
If such a polarization-maintaining fiber is used, for example, two laser beams with slightly different wavelengths can be input into one end of the fiber with their polarization planes matched, and an output corresponding to the phase difference between the two can be obtained from the other end. , it is possible to provide a heterodyne detection function in the optical state without electrical conversion.

更に移動体の運動方向指示や姿勢制御のために
必要とする角速度センサ(ジヤイロ)を、この偏
波面保存フアイバーを使用して感度よく製作する
ことができる。即ち該フアイバーを以て作られた
コイル中を伝播する光波の移相(θ)がコイルの
回転角速度(Ω)に比例してずれる現象(サグナ
ツク効果)を利用して高い精度で該回転角速度が
測定される。
Furthermore, an angular velocity sensor (gyro) required for indicating the movement direction and controlling the attitude of a moving object can be manufactured with high sensitivity using this polarization preserving fiber. That is, the rotational angular velocity can be measured with high precision by utilizing the phenomenon (Sagnatsk effect) in which the phase shift (θ) of a light wave propagating in a coil made of the fiber shifts in proportion to the rotational angular velocity (Ω) of the coil. Ru.

第1図はその原理図を示すもので半導体レーザ
1からの波長λのレーザ光はミラー2で反射して
半径Rのコイル状にN回捲かれた偏波面保存フア
イバーコイル3の一方の端面より実線矢印のよう
に入力され、一方ミラー2を通過したレーザ光は
他方の端面より点線矢印のように入力され、両者
の出力はミラー2にて反射、あるいは通過して合
成され光検知器4によつて電気出力に変換され、
増幅器5を経て記録計6に記録される。
Figure 1 shows a diagram of its principle. Laser light with a wavelength λ from a semiconductor laser 1 is reflected by a mirror 2 and exits from one end face of a polarization-maintaining fiber coil 3 which is wound N times into a coil shape with a radius R. The laser beam is input as shown by the solid line arrow, and the laser beam that has passed through one mirror 2 is inputted from the other end face as shown by the dotted line arrow, and the outputs of both are reflected or passed through the mirror 2 and combined and sent to the photodetector 4. It is then converted into electrical output,
The signal is recorded on a recorder 6 via an amplifier 5.

コイル3が回転角速度Ωで回転した場合に生じ
る光位相差θは所謂サグナツクの式 θ=8π2R2N/λC (Cは光速度) で示され、これに比例する電気出力が記録計6か
ら得られる。
The optical phase difference θ that occurs when the coil 3 rotates at a rotational angular velocity Ω is expressed by the so-called Sagnac equation θ=8π 2 R 2 N/λC (C is the speed of light), and the electrical output proportional to this is expressed by the recorder 6. obtained from.

このように偏波面保存フアイバーは種々特殊な
利用に今後大きい期待が持たれているので、安価
に生産されて特性もよくかつ取り扱いの容易なも
のであることが望ましい。
As described above, polarization preserving fibers have high expectations for various special uses in the future, so it is desirable that they be produced at low cost, have good characteristics, and be easy to handle.

(c) 従来技術と問題点 従来この種偏波面保存フアイバーとして生産さ
れた2例を横断面をもつて第2図イ,ロに示すが
イにあつてはコアー11を取りかこむクラツド1
2が楕円形状に構成されて、これをジヤケツト1
3が囲み構造となつており、製作時の熱歪によつ
て長軸方向、短軸方向を最大、最小とする屈折率
の推移変化を起させて両軸方向の偏波面のレーザ
光を主として伝播させるものであり、ロにあつて
はコアー14を囲むクラツド15に軸心に対称的
に空洞16,16′を設け、同様製作時の熱歪に
よる屈折率の推移変化を起させて同様の特性をも
たしめたものである。
(c) Prior art and problems Two examples of this type of polarization preserving fiber conventionally produced are shown in cross section in Figure 2 A and B. In A, the cladding 1 surrounding the core 11 is shown.
2 is configured in an elliptical shape, and this is the jacket 1.
3 has an enclosing structure, and due to thermal strain during manufacturing, the refractive index changes with the maximum and minimum in the major and minor axis directions, so that the laser beam with polarization planes in both axis directions is mainly In B, cavities 16 and 16' are provided in the cladding 15 surrounding the core 14 symmetrically with respect to the axis, and similar changes in the refractive index due to thermal strain during manufacturing are caused to produce a similar effect. It has special characteristics.

一見して推察されるようにこのような構造のフ
アイバーを生産するのはかなり困難であるのみな
らず、全長を通して均一な特性とすることも頗る
難しい。更にフアイバーとフアイバーとの接続に
際しては、従来のようにセンター合せに加えて断
面形状合せを必要とし、コアー歪が10ミクロンに
満たないフアイバーにこのような断面形状合せは
容易なことではない。
As might be inferred at first glance, it is not only quite difficult to produce a fiber with such a structure, but also extremely difficult to achieve uniform properties throughout its entire length. Furthermore, when connecting fibers, it is necessary to match the cross-sectional shapes in addition to the conventional center alignment, and such cross-sectional shape matching is not easy for fibers whose core strain is less than 10 microns.

更に既述のコイル状となして角速度センサとし
て使用せんとする場合には、捲回に際して生じる
内部応力による屈折率の変動を配慮すれば、捲回
面に対する断面の相対的関係位置を一定に保持す
る必要があり、極めて取り扱いの困難なるのみな
らず、然して特定偏波面出力が他に比し相対的に
大きく、即ちSN比をあげるためには数糎から数
十糎の長さを必要とし、小形化のためにはコイル
状となす必要がある。
Furthermore, if it is to be made into a coil shape and used as an angular velocity sensor as described above, the relative position of the cross section with respect to the winding surface can be kept constant if consideration is given to fluctuations in the refractive index due to internal stress generated during winding. Not only is it extremely difficult to handle, but the specific polarization plane output is relatively large compared to others, that is, in order to increase the S/N ratio, a length of several to several tens of lengths is required. For miniaturization, it is necessary to make it into a coil shape.

第2図ハは横軸にドラム(コイル)径を、縦軸
に偏波面の保存特性を、所定の偏波面を有する光
を入射したとき目的とする偏波面をもつ光とその
他の光のパアーの比で示したもので点線波形で示
すようにフアイバーを捲きつけるドラムの径をあ
る程度大にしなければ偏波面保存特性が維持でき
ず、小形化に不適である。
Figure 2 (c) shows the diameter of the drum (coil) on the horizontal axis and the preservation characteristic of the plane of polarization on the vertical axis. As shown by the dotted line waveform, the polarization preservation characteristic cannot be maintained unless the diameter of the drum around which the fiber is wound is increased to a certain extent, making it unsuitable for miniaturization.

(d) 発明の目的 本発明は従来のこの種フアイバーの欠点を除去
し、通常のフアイバーと同様な工程で生産され、
フアイバー間の接続もセンター合せのみで行い得
る新規な偏波面保存光フアイバーを得ることをそ
の目的とする。
(d) Purpose of the invention The present invention eliminates the drawbacks of conventional fibers of this type, can be produced in the same process as ordinary fibers,
The purpose of this study is to obtain a new polarization-maintaining optical fiber that can connect fibers by simply aligning their centers.

(e) 発明の構成 本発明の上記目的は、石英を素材とし、コア
ー、クラツドおよびジヤケツトの三層よりなり、
コアーとクラツドの屈折率差の比(n1−n2/2n1× 100、ここにn1,n2は夫々コアークラツドの屈折
率)を0.13±0.05%としたフアイバーを直径50〜
200mmのドラムに捲回してなる本発明によるシン
グルモードの偏波面保存フアイバーによつて達成
される。
(e) Structure of the invention The above-mentioned object of the present invention is to provide a jacket made of quartz and composed of three layers: a core, a cladding, and a jacket.
A fiber with a diameter of 50 to
This is achieved by a single mode polarization preserving fiber according to the invention wound on a 200 mm drum.

即ち本発明のフアイバーはコアー、クラツドお
よびジヤケツト共に断面同心円状に構成されてい
る故に、生産工程も従来の偏波面非保存性光フア
イバーと同様であり、フアイバー間の結合もセン
ー合せのみ配慮すればよい。尚±0.05は製造誤差
で、屈折率が一般のフアイバーに比べて小さいの
で、生じるものである。
That is, since the fiber of the present invention has a core, cladding, and jacket each having a concentric circular cross-section, the production process is the same as that for conventional polarization non-maintaining optical fibers, and the coupling between the fibers can be achieved by considering only the center alignment. good. Note that ±0.05 is a manufacturing error that occurs because the refractive index is smaller than that of ordinary fibers.

この光フアイバーは、直線状のままでは偏波面
保存特性を示さないが円筒ドラムに捲きつけるこ
とによつて、光フアイバーの円筒ドラムの軸に対
し、直角方向の部分において、外側が延び、ドラ
ム側が縮む。一方、円筒ドラムの軸に対し水平方
向については、歪が生じないことにより、形状を
方向によつて変化させることとなり、始めて偏波
保存特性を示す。このことはマイクロ波でよく用
いられる矩形円形導波管変換器と同じように考え
ることができる。
This optical fiber does not exhibit polarization preservation characteristics when it is straight, but by winding it around a cylindrical drum, the outside of the optical fiber extends at right angles to the axis of the cylindrical drum, and the drum side extends. Shrink. On the other hand, in the horizontal direction with respect to the axis of the cylindrical drum, since no distortion occurs, the shape changes depending on the direction, and exhibits polarization preservation characteristics for the first time. This can be thought of in the same way as a rectangular-circular waveguide converter often used in microwaves.

勿論従来の通信用光フアイバーも屈曲に際して
微少な屈折率の方向性を生じるが元々偏波面保存
特性についての配慮はなく、伝送損失を可及的小
さくするようコアー、クラツドの屈折率が選ばれ
ており、両者の屈折率の比(n1−n2/2n1×100、こ こにn1,n2は夫々コアー、クラツドの屈折率)
は0.2〜0.5%に及ぶ。
Of course, conventional communication optical fibers also exhibit slight directionality in their refractive index when bent, but originally there was no consideration given to polarization preservation characteristics, and the refractive indices of the core and cladding were selected to minimize transmission loss. The ratio of their refractive indexes (n1−n2/2n1×100, where n1 and n2 are the refractive indexes of the core and cladding, respectively)
ranges from 0.2 to 0.5%.

このようなフアイバーではたとえ屈曲しても偏
波面保存特性は僅少で、例えば既述のジヤイロ用
として使用することができない。
Even if such a fiber is bent, its polarization preservation properties are so small that it cannot be used, for example, for the gyro described above.

本発明のフアイバーにあつてはコアー、クラツ
ドの屈折率差をさらに僅少にし、n1−n2/2n1×100 %を0.13±0.05%となすことによつて第2図ハの
実線に示すように捲きつけるドラムの径が小さい
方がフアイバーのドラム軸に対して垂直方向の歪
が大きくなり、従つて偏波面保存特性はよくな
り、小形化に適している。屈折率の差の僅少とな
ることで屈曲した場合の前述した二方向の歪によ
る屈折率の相対的変化が増大するためである。か
くて目的とする偏波面保存特性を実用し得る値に
まで向上させることができた。
In the fiber of the present invention, the difference in refractive index between the core and the cladding is made even smaller, and n1-n2/2n1×100% is set to 0.13±0.05%, so that the fiber can be wound as shown in the solid line in Fig. 2C. The smaller the diameter of the attached drum, the greater the distortion in the direction perpendicular to the drum axis of the fiber, and therefore the better the polarization preservation characteristic, making it suitable for miniaturization. This is because the relative change in the refractive index due to the above-mentioned strain in the two directions when bent increases due to the small difference in the refractive index. In this way, we were able to improve the desired polarization preservation property to a value that can be put to practical use.

(f) 発明の実施例 第3図は本発明の一実施例をフアイバー横断面
拡大図イ、偏波面保存特性を測定するための構成
ブロツクダイアグラムロ、および該特性曲線ハで
示すものである。
(f) Embodiment of the Invention FIG. 3 shows an embodiment of the invention by an enlarged cross-sectional view of a fiber (a), a block diagram of a structure for measuring polarization preservation characteristics (b), and a characteristic curve (c).

円形断面コアー21、円形断面クラツド22お
よび円形断面ジヤケツト23の三重構造からな
り、コアー21とクラツド22の屈折率の比が
0.13に選ばれた第3図イに示す寸法の光フアイバ
ー24を、同図ロに示すように直径150mmのドラ
ム25に約500米捲回し、その始端に偏光プリズ
ム26、レンズ系27,27′を介して0.78ミク
ロン波長の半導体レーザ光を付与して、コイル内
に直線偏波面のレーザ光を伝播させ、他端よりの
出力光を集光レンズ28および回転検光子29を
介して検知器30に付与し、出力計31を働かせ
る。
It has a triple structure of a circular cross-section core 21, a circular cross-section cladding 22, and a circular cross-section jacket 23, and the ratio of the refractive index of the core 21 and the cladding 22 is
An optical fiber 24 having the dimensions shown in FIG. 3A and selected as 0.13 is wound approximately 500 times around a drum 25 with a diameter of 150 mm as shown in FIG. A semiconductor laser beam with a wavelength of 0.78 microns is applied through the coil to propagate the linearly polarized laser beam inside the coil, and the output light from the other end is passed through the condenser lens 28 and the rotating analyzer 29 to the detector 30. and activates the output meter 31.

検光子29を回転させ到来光の直線偏波面とな
す角度θを横軸に、出力計32の指示(dB)を
横軸にとつた第3図ハに示す特性曲線は、本発明
光フアイバーの良好な偏波面保存性を示してい
る。
The characteristic curve shown in FIG. 3C, in which the horizontal axis is the angle θ formed by rotating the analyzer 29 and the linear polarization plane of the incoming light, and the horizontal axis is the indication (dB) of the output meter 32, is a characteristic curve of the optical fiber of the present invention. It shows good polarization preservation.

(g) 発明の効果 以上説明のように本発明による偏波面保存光フ
アイバーにあつては生産も従来の光フアイバーと
同様に行われ、フアイバー同志の接続もセンター
合せのみでよく、ドラム捲回にも特別の配慮を必
要としない等従来のこの種フアイバーの欠点を除
去した優れた効果を示すものである。
(g) Effects of the Invention As explained above, the polarization preserving optical fiber according to the present invention can be produced in the same manner as conventional optical fibers, and the fibers only need to be connected to each other by center alignment, and there is no need for drum winding. This fiber exhibits an excellent effect that eliminates the drawbacks of conventional fibers of this type, such as requiring no special consideration.

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

第1図は偏波面保存フアイバーを利用した角速
度センサー(ジヤイロ)の構成を示し、第2図
イ,ロは従来使用されて来たこの種フアイバーの
2例を、ハはドラム径と偏波面保存特性を、第3
図は本発明の1実施例を、フアイバー断面イ、偏
波面保存特性測定のための構成ブロツクダイアグ
ラムロ、及びその保存特性曲線ハを示す。 図において11,14,21はフアイバーコア
ー、12,15,22はクラツド、13,23は
ジヤケツト、24は本発明による光フアイバー、
25はドラム、26は偏光プリズム、29は検光
子、30は検知器、31は出力計を示す。
Figure 1 shows the configuration of an angular velocity sensor (gyro) that uses a polarization-preserving fiber, and Figure 2 (a) and (b) show two examples of this type of fiber that have been used in the past, and (c) shows the drum diameter and polarization-preserving fiber. Characteristics, 3rd
The figure shows one embodiment of the present invention, with a fiber cross section (a), a block diagram of a configuration for measuring polarization preservation characteristics (b), and a preservation characteristic curve thereof (c). In the figure, 11, 14, 21 are fiber cores, 12, 15, 22 are claddings, 13, 23 are jackets, 24 is an optical fiber according to the present invention,
25 is a drum, 26 is a polarizing prism, 29 is an analyzer, 30 is a detector, and 31 is an output meter.

Claims (1)

【特許請求の範囲】 1 石英を素材としてコアー、クラツドおよびジ
ヤケツトの同心3重構造よりなり、コアとクラツ
ドの屈折率差の比(n1−n2/2n1×100、ここにn1, n2は夫々コアー、クラツドの屈折率)を0.13±
0.05%としたフアイバーを直径50〜200mmのドラ
ムに捲回してなることを特徴とするシングルモー
ドの偏波面保存光フアイバー。
[Claims] 1. It is made of quartz and has a concentric triple structure of a core, a cladding, and a jacket, and the ratio of the refractive index difference between the core and the cladding (n1-n2/2n1×100, where n1 and n2 are the core and the cladding, respectively). , refractive index of the cladding) is 0.13±
A single-mode polarization-maintaining optical fiber that is made by winding a 0.05% fiber into a drum with a diameter of 50 to 200 mm.
JP57190395A 1982-09-28 1982-10-29 Polarization plane saving optical fiber Granted JPS5979201A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP57190395A JPS5979201A (en) 1982-10-29 1982-10-29 Polarization plane saving optical fiber
CA000437093A CA1238970A (en) 1982-09-28 1983-09-20 Fiber-optic gyro
DE8383305763T DE3382205D1 (en) 1982-09-28 1983-09-27 CIRCULAR WITH OPTICAL THREAD.
EP83305763A EP0107373B1 (en) 1982-09-28 1983-09-27 Fibre optic gyroscope

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57190395A JPS5979201A (en) 1982-10-29 1982-10-29 Polarization plane saving optical fiber

Publications (2)

Publication Number Publication Date
JPS5979201A JPS5979201A (en) 1984-05-08
JPS6310403B2 true JPS6310403B2 (en) 1988-03-07

Family

ID=16257437

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57190395A Granted JPS5979201A (en) 1982-09-28 1982-10-29 Polarization plane saving optical fiber

Country Status (1)

Country Link
JP (1) JPS5979201A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61103329A (en) * 1984-10-26 1986-05-21 Nippon Telegr & Teleph Corp <Ntt> Method and apparatus for giving group delay time difference of optical signal
JPS61143112U (en) * 1985-02-25 1986-09-04
IT1192093B (en) * 1985-07-26 1988-03-31 Carlo Giacomo Someda CIRCULAR TWO-REFLECTOR DIELECTRIC WAVE GUIDE

Also Published As

Publication number Publication date
JPS5979201A (en) 1984-05-08

Similar Documents

Publication Publication Date Title
US11947159B2 (en) Interferometric fibre optic gyroscopes using hollow core optical fibre and methods thereof
US4443698A (en) Sensing device having a multicore optical fiber as a sensing element
CN101387519B (en) Hollow photonic crystal fiber gyroscope
CN114397729B (en) SiN integrated optical chip based on continuous curvature curved waveguide polarizer
CN111121838A (en) Double-core optical fiber Michelson interferometer for inclined grating beam splitting
CN117433500B (en) Polarization mode multiplexing double optical path fiber optic gyroscope based on photonic chip
JPH05241039A (en) Optical fiber having internal partial mirror
CN115824265A (en) Method for reducing temperature sensitivity of scale factor of fiber-optic gyroscope and fiber-optic gyroscope
JPS6385313A (en) Sagnack ring rotaion sensor and method of forming sagnack ring rotation sensor
JPS6310403B2 (en)
JPH11352158A (en) Optical fiber measuring instrument
EP0059644B1 (en) Optical gyroscope
JPS61117411A (en) Optical fiber sensor
JP6539227B2 (en) Electric field detector
CN111141317A (en) Parallel Michelson integrated interferometer based on three-core fiber
JPH065266B2 (en) Optical fiber magnetic field sensor
JPS62291514A (en) Optical-fiber rotating sensor
JPS61233314A (en) Optical element
JPH0371051B2 (en)
JPH0658227B2 (en) Light fiber gyro
JPH0774845B2 (en) Elliptical jacket type polarization-maintaining optical fiber
JP2528094B2 (en) Fiber type polarizer
JPH02103422A (en) Optical fiber acoustic sensor
BUCHHAVE et al. Fiber-Optic Laser Anemometer
JPS6139364Y2 (en)