JPS628034A - Single mode optical fiber eccentricity measuring device - Google Patents
Single mode optical fiber eccentricity measuring deviceInfo
- Publication number
- JPS628034A JPS628034A JP14580085A JP14580085A JPS628034A JP S628034 A JPS628034 A JP S628034A JP 14580085 A JP14580085 A JP 14580085A JP 14580085 A JP14580085 A JP 14580085A JP S628034 A JPS628034 A JP S628034A
- Authority
- JP
- Japan
- Prior art keywords
- mode optical
- optical fiber
- fiber
- single mode
- eccentricity
- 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
- 239000013307 optical fiber Substances 0.000 title claims abstract description 30
- 239000000835 fiber Substances 0.000 abstract description 21
- 238000000034 method Methods 0.000 abstract description 2
- 206010044565 Tremor Diseases 0.000 abstract 3
- 230000008878 coupling Effects 0.000 description 2
- 238000010168 coupling process Methods 0.000 description 2
- 238000005859 coupling reaction Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
- 230000013011 mating Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/33—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
- Light Guides In General And Applications Therefor (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明はシングルモード光ファイバの偏心量を簡易に
且つ精度よく測定することができるシングルモード光フ
ァイバの偏心測定装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a single-mode optical fiber eccentricity measuring device that can easily and accurately measure the eccentricity of a single-mode optical fiber.
[従来の技術]
従来、シングルモード光ファイバの偏心量の測定は、シ
ングルモード光ファイバの断面像を写真にとり、断面像
から作図により求めたり、あるいは断面像を基準に像の
み動かして、即ちイメージシェアリングにより計測して
いた。[Prior Art] Conventionally, the amount of eccentricity of a single-mode optical fiber has been measured by photographing a cross-sectional image of the single-mode optical fiber and drawing it from the cross-sectional image, or by moving only the image based on the cross-sectional image. It was measured by sharing.
[発明が解決しようとする問題点]
しかしながら、上記のシングルモード光ファイバの断面
像を用いる方法では、シングルモード光ファイバ端面の
カットの状態が影響したり、断面を見る時あるいは写真
をとる際には白色光を用いるため、実際の使用波長での
シングルモード光ファイバの真の偏心がわからない。ま
た写真に基づいて求めるので精度がでない。[Problems to be Solved by the Invention] However, in the above-mentioned method using a cross-sectional image of a single-mode optical fiber, the cutting condition of the end face of the single-mode optical fiber may be affected, and when viewing the cross-section or taking a photograph, uses white light, so the true eccentricity of the single-mode optical fiber at the wavelength actually used is unknown. Also, since it is calculated based on photographs, it is not accurate.
[発明の目的]
この発明は以上の従来技術の問題点を解消すべく創案さ
れたものであり、この発明の目的は実際の使用波長での
真の偏心量を簡単に且つ精度よく求めることができるシ
ングルモード光ファイバの偏心測定装置を提供すること
にある。[Object of the Invention] This invention was devised to solve the above-mentioned problems of the prior art, and an object of the invention is to easily and accurately determine the true amount of eccentricity at the wavelength actually used. An object of the present invention is to provide a device for measuring the eccentricity of a single mode optical fiber.
[発明の概要]
上記の目的を達成するために、この発明は、突き合せら
れる一方のシングルモード光ファイバに光を入射するた
めの光源と、もう一方のシングルモード光ファイバから
出射される光の強度を検出するための受光器と、突き合
せられるシングルモード光ファイバの端部を3軸方向に
移動させることができ、且つ回転させることができる駆
動装置とを備えてなるものである。[Summary of the Invention] In order to achieve the above object, the present invention includes a light source for inputting light into one single mode optical fiber to be matched, and a light source for inputting light to one single mode optical fiber to be matched, and a light source for inputting light to the other single mode optical fiber. It is equipped with a light receiver for detecting intensity, and a drive device that can move and rotate the ends of single-mode optical fibers to be matched in three axes.
まず、シングルモード光ファイバの端部を突き合せ、端
部の3軸方向の移動により調心を行なう。First, the ends of single-mode optical fibers are butted together, and alignment is performed by moving the ends in three axial directions.
次いで、一方のシングルモード光ファイバを回転させ受
光強度を測定する。こうすると、回転角により両光ファ
イバの結合状態が変化し受光強度が変動する。受光強度
の変動幅はシングルモード光ファイバの偏心量に応じて
増大し、受光強度の最大値から偏心量を決定できる。Next, one single mode optical fiber is rotated and the received light intensity is measured. In this case, the coupling state of both optical fibers changes depending on the rotation angle, and the received light intensity fluctuates. The fluctuation range of the received light intensity increases according to the eccentricity of the single mode optical fiber, and the eccentricity can be determined from the maximum value of the received light intensity.
[実施例]
以下に、この発明の実施例を添付図面に従って詳述する
。[Examples] Examples of the present invention will be described in detail below with reference to the accompanying drawings.
第1図には偏心測定装置を示す。同図において、1は偏
心量を測定するシングルモード光ファイバ(以下、8M
ファイバと略称する)である。8Mファイバ1,1の突
き合せ端部は微動台2.3によりそれぞれ支持されてい
る。微動台2は8Mファイバ1の突合せ端部をx、y、
z方向に移動させることができる。また、微動台3は、
×、y。FIG. 1 shows an eccentricity measuring device. In the same figure, 1 is a single mode optical fiber (hereinafter referred to as 8M) for measuring eccentricity.
(abbreviated as fiber). The abutted ends of the 8M fibers 1, 1 are supported by fine movement tables 2.3, respectively. The fine movement table 2 moves the butt ends of the 8M fiber 1 in x, y,
It can be moved in the z direction. In addition, the fine movement table 3 is
×, y.
2方向のみならず8Mファイバ1をその中心軸のまわり
に回転させることができる。微動台2とは反対側の8M
ファイバ1の端部には光源としてのレーザーダイオード
4が設けられている。また微動台3とは反対側の8Mフ
ァイバ1の端部には受光器5が設けられている。レーザ
ーダイオード4の出射光の波長は8Mファイバ1の使用
波長となっている。なお、6は突合せ部である。The 8M fiber 1 can be rotated around its central axis as well as in two directions. 8M on the opposite side of fine movement table 2
A laser diode 4 is provided at the end of the fiber 1 as a light source. Further, a light receiver 5 is provided at the end of the 8M fiber 1 on the opposite side from the fine movement table 3. The wavelength of the emitted light from the laser diode 4 is the wavelength used by the 8M fiber 1. Note that 6 is a butt portion.
上記の構成において、偏心測定にあたっては、まず、8
Mファイバ1を切断し、8Mファイバ1゜1の突合せ端
部を微動台2.3にそれぞれセットする。そして、レー
ザーダイオード4から使用波長の光を一方の8Mファイ
バ1に入射し他方の8Mファイバ1からの出射光を受光
器5によりモニタしながら微動台2または3をx、y、
z方向に移動して、突合せ余剰績が最小となるよう調心
する。次に、微動台3により8Mファイバ1の突合せ端
部を回転させつつ受光器5で出射光の強度を測定する。In the above configuration, when measuring eccentricity, first, 8
Cut the M fiber 1, and set the mating ends of the 8M fiber 1°1 on the fine movement table 2.3. Then, the light of the wavelength to be used is inputted from the laser diode 4 into one 8M fiber 1, and while the light emitted from the other 8M fiber 1 is monitored by the receiver 5, the fine movement table 2 or 3 is moved in x, y,
Move in the z direction and align so that the butt surplus is minimized. Next, the abutting ends of the 8M fiber 1 are rotated by the fine movement stage 3, and the intensity of the emitted light is measured by the light receiver 5.
偏心のないSMファイバ同士を突き合せたとき、オフセ
ット量(横ずらし量)と突合せ余剰績との間には第2図
に示す関係がある。また、上記測定より、偏心のある8
Mファイバ1.1では回転によって突合せ部6の結合状
態が変化し、第3図に示すような突合せ余剰績の回転角
依存性が得られる。従って、第3図より8Mファイバ1
の回転時の突合せ余剰績の最大値を測定すれば、第2図
より8Mファイバ1の偏心間が求まる。When SM fibers without eccentricity are butted together, there is a relationship shown in FIG. 2 between the offset amount (lateral shift amount) and the butt surplus. Also, from the above measurements, the eccentric 8
In the M fiber 1.1, the coupling state of the butt portion 6 changes with rotation, and the rotation angle dependence of the butt surplus as shown in FIG. 3 is obtained. Therefore, from Figure 3, 8M fiber 1
By measuring the maximum value of the butt surplus during rotation, the eccentricity of the 8M fiber 1 can be determined from FIG.
なお、上記実施例において、微動台2を固定した支持台
とし、微動台3で調心(x 、 y 、 z方向の移動
)と回転との両方を行なうようにしてもよい。また微動
台3を回転機能だけの回転台とし、微動台2で関心を行
なうようにしてもよい。In the above embodiment, the fine movement table 2 may be a fixed support table, and the fine movement table 3 may perform both alignment (movement in the x, y, and z directions) and rotation. Alternatively, the fine movement table 3 may be a rotary table with only a rotation function, and the fine movement table 2 may be used to perform the desired operation.
[発明の効果]
以上型するに、この発明によれば次のような優れた効果
を発揮する。[Effects of the Invention] In summary, the present invention provides the following excellent effects.
(1) シングルモード光ファイバを突き合せて調心
した後、シングルモード光ファイバに回転を与えて突合
せ余剰績の最大値から偏心量を求める方式であるため、
精度がよく且つ簡易な偏心測定ができる。(1) After aligning the single mode optical fibers by butting them together, the single mode optical fibers are rotated and the amount of eccentricity is determined from the maximum value of the butt surplus.
Eccentricity can be measured easily and with good accuracy.
(り 更に、実際の使用波長における真の偏心量を測定
できる。(In addition, the true amount of eccentricity at the wavelength actually used can be measured.
Cり 既存の装置を用いて容易に且つ安価に構成でき有
用性が高い。C-ri: It can be constructed easily and inexpensively using existing equipment, and is highly useful.
第1図はこの発明に係る偏心測定装置の一実施例を示す
構成図、第2図は偏心のないシングルモード光ファイバ
のオフセット量と突合せ余剰績との関係を示すグラフ、
第3図はこの発明の偏心測定装置により得られる、偏心
のあるシングルモード光ファイバの突合せ余剰績の回転
角依存性を示すグラフである。
図中、1はシングルモード光ファイバ、2.3は微動台
、4はレーザーダイオード、5は受光器、6は突合せ部
である。
特許出願人 日立電線株式会社
代理人弁理士 絹 谷 信 雄l−・渉ブ)
レモード考ファイバ
乙・・“突合t+8
第1図
# 7t・y) V tIJms
177;J転角K (dog、)第2図
第3図FIG. 1 is a configuration diagram showing an embodiment of an eccentricity measuring device according to the present invention, and FIG. 2 is a graph showing the relationship between the offset amount and the matching surplus of a single mode optical fiber without eccentricity.
FIG. 3 is a graph showing the rotation angle dependence of the butt result of an eccentric single mode optical fiber obtained by the eccentricity measuring device of the present invention. In the figure, 1 is a single mode optical fiber, 2 and 3 are fine movement tables, 4 is a laser diode, 5 is a light receiver, and 6 is a butt portion. Patent Applicant: Hitachi Cable Co., Ltd. Representative Patent Attorney Nobuo Kinutani/Watabu)
Remode consideration fiber B..."butt t+8 Figure 1 #7t・y) V tIJms
177; J rotation angle K (dog,) Fig. 2
Figure 3
Claims (1)
ァイバのうちの一方のシングルモード光ファイバに光を
入射するための光源と、他方のシングルモード光ファイ
バから出射される光の強度を検出するための受光器と、
突き合せられる上記シングルモード光ファイバの端部を
支持し、該端部を3軸方向に移動させ且つ回転させるこ
とができる駆動装置とを備えたことを特徴とするシング
ルモード光ファイバの偏心測定装置。A light source for inputting light into one of two single-mode optical fibers whose ends are butted against each other, and for detecting the intensity of light emitted from the other single-mode optical fiber. and a receiver of
A device for measuring the eccentricity of a single-mode optical fiber, comprising a drive device that supports the end portions of the single-mode optical fibers to be butted together, and is capable of moving and rotating the end portions in three axial directions. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14580085A JPS628034A (en) | 1985-07-04 | 1985-07-04 | Single mode optical fiber eccentricity measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14580085A JPS628034A (en) | 1985-07-04 | 1985-07-04 | Single mode optical fiber eccentricity measuring device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS628034A true JPS628034A (en) | 1987-01-16 |
Family
ID=15393441
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14580085A Pending JPS628034A (en) | 1985-07-04 | 1985-07-04 | Single mode optical fiber eccentricity measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS628034A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0987571A3 (en) * | 1998-09-15 | 2001-06-13 | Siemens Aktiengesellschaft | Method of making a fused joint between optical fibres |
-
1985
- 1985-07-04 JP JP14580085A patent/JPS628034A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0987571A3 (en) * | 1998-09-15 | 2001-06-13 | Siemens Aktiengesellschaft | Method of making a fused joint between optical fibres |
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