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JPS6216402B2 - - Google Patents
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JPS6216402B2 - - Google Patents

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Publication number
JPS6216402B2
JPS6216402B2 JP9263684A JP9263684A JPS6216402B2 JP S6216402 B2 JPS6216402 B2 JP S6216402B2 JP 9263684 A JP9263684 A JP 9263684A JP 9263684 A JP9263684 A JP 9263684A JP S6216402 B2 JPS6216402 B2 JP S6216402B2
Authority
JP
Japan
Prior art keywords
optical fiber
optical fibers
received light
light power
optical
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
JP9263684A
Other languages
Japanese (ja)
Other versions
JPS60237409A (en
Inventor
Juji Uematsu
Isao Minamida
Yasuyuki Kato
Juichi Usui
Toshiaki Kakii
Takeshi Yamada
Kazukuni Oosato
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.)
Furukawa Electric Co Ltd
Sumitomo Electric Industries Ltd
NTT Inc
Original Assignee
Furukawa Electric Co Ltd
Nippon Telegraph and Telephone Corp
Sumitomo Electric Industries 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 Furukawa Electric Co Ltd, Nippon Telegraph and Telephone Corp, Sumitomo Electric Industries Ltd filed Critical Furukawa Electric Co Ltd
Priority to JP9263684A priority Critical patent/JPS60237409A/en
Publication of JPS60237409A publication Critical patent/JPS60237409A/en
Publication of JPS6216402B2 publication Critical patent/JPS6216402B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/255Splicing of light guides, e.g. by fusion or bonding
    • G02B6/2551Splicing of light guides, e.g. by fusion or bonding using thermal methods, e.g. fusion welding by arc discharge, laser beam, plasma torch

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Mechanical Coupling Of Light Guides (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は光フアイバ相互を融着接続する際に重
要なゼロ間隔の設定、すなわち接続すべき光フア
イバの端面間隔を0に設定するための方法に関す
る。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) The present invention is a method for setting the zero spacing, which is important when fusion splicing optical fibers, that is, setting the end face spacing of the optical fibers to be connected to zero. Regarding the method.

(従来技術) 光フアイバ相互を融着接続する際の主要な工程
は光フアイバ端部の軸合わせ、光フアイバ端面間
隔の設定、光フアイバ端部の突き合わせ移動、光
フアイバ端部への放電熱供与などであり、他は上
記工程に付随した工程である。
(Prior art) The main steps in fusion splicing optical fibers are alignment of the optical fiber ends, setting of the distance between the optical fiber end faces, butt movement of the optical fiber ends, and provision of discharge heat to the optical fiber ends. etc., and the others are steps incidental to the above steps.

光フアイバの融着接続が全自動化へと移行しつ
つある現状においてもその大要は変わらず、第1
図イ〜トに示す工程がとられる。
Even in the current situation where optical fiber fusion splicing is moving towards full automation, the main point remains the same.
The steps shown in Figures I to B are taken.

以下これについて説明すると、それぞれ外周に
被覆層を有する光フアイバ1A,1Bはその端部
2A,2Bにおいて被覆層が除去されて裸状とな
り、これら端部2A,2Bが適当なカツテイング
手段により切り揃えられる。
To explain this below, the optical fibers 1A and 1B each have a coating layer on the outer periphery, and the coating layer is removed at the end portions 2A and 2B, resulting in a bare state, and these end portions 2A and 2B are trimmed by appropriate cutting means. It will be done.

こうして前処理された光フアイバ端部2A,2
Bは、軸合台のV溝内に嵌めこまれ、これら端部
2A,2Bと連続する光フアイバ1A,1Bの被
覆部が既知のスリツプ式ホルダを介してクランプ
される。
Optical fiber ends 2A, 2 thus pretreated
B is fitted into the V-groove of the shaft mating stand, and the coated portions of the optical fibers 1A, 1B that are continuous with these end portions 2A, 2B are clamped via a known slip-type holder.

これにより光フアイバ端部2A,2Bは一直線
状に並び、その端面3A,3Bが互いに対向す
る。
As a result, the optical fiber ends 2A and 2B are aligned in a straight line, and their end faces 3A and 3B are opposed to each other.

第1図イは上記において光フアイバ1A,1B
の第1次端面間隔G1が設定される状態を略示し
たものであり、この際、光フアイバ端部2A,2
Bはスリツプ式ホルダを介して間隔設定板4の方
向へ移動され、その端面3A,3Bが間隔設定板
4の両面と衝突することにより、0.5mm程度の第
1次端面間隔G1が設定される。
Figure 1A shows optical fibers 1A and 1B in the above
This diagram schematically shows a state in which the primary end face spacing G 1 is set, and in this case, the optical fiber ends 2A, 2
B is moved in the direction of the spacing setting plate 4 via the slip type holder, and its end faces 3A and 3B collide with both sides of the spacing setting plate 4, thereby setting a primary end face spacing G1 of about 0.5 mm. Ru.

つぎに光フアイバ端面3A,3B間から間隔設
定板4が退去し、その後、第1図ロのごとく光フ
アイバ端部2A,2Bがこれらの突き合わせ方向
へ所定量だけ移動され、これにより10μm程度の
第2次端面間隔G2が設定される。
Next, the spacing setting plate 4 is removed from between the optical fiber end faces 3A and 3B, and then, as shown in FIG. A secondary end face spacing G2 is set.

第2端面間隔設定後は、第1図ハのように両光
フアイバ端部2A,2Bの軸合わせ(コア相互を
一致させる)が行なわれるのであり、この軸合わ
せ手段は通常、光フアイバ端部2A,2Bを水平
方向、垂直方向などへ徴動調整することにより行
なわれ、この際、光フアイバ1A,1Bにわたつ
て光信号が通されるのであり、その受光側でのモ
ニタにより最大受光パワーが確認できたとき、コ
ア相互は一致したとみなせる。
After setting the second end face distance, the axes of both the optical fiber ends 2A and 2B are aligned (to align the cores with each other) as shown in FIG. This is done by adjusting the optical fibers 2A and 2B horizontally, vertically, etc. At this time, the optical signal is passed across the optical fibers 1A and 1B, and the maximum received light power is determined by monitoring on the receiving side. When this can be confirmed, the cores can be considered to match each other.

上記によりコア相互が一致した後は、第1図ニ
のごとく一方の光フアイバ端部2Aが他方の光フ
アイバ端部2Bに向けて移動され、かつ、光フア
イバ端面3A,3B相互が突き合わされることに
より端面間隔は一たん0となる。
After the cores are aligned with each other as described above, one optical fiber end 2A is moved toward the other optical fiber end 2B, and the optical fiber end surfaces 3A and 3B are butted against each other, as shown in FIG. 1D. As a result, the distance between the end faces becomes 0.

その後、一方の光フアイバ端部2Bが他方の光
フアイバ端部2Bから離れる方向へ所定量だけ移
動され、これにより10μm程度の第3次端面間隔
G3が設定される。
After that, one optical fiber end 2B is moved by a predetermined amount in a direction away from the other optical fiber end 2B, thereby creating a tertiary end face spacing of about 10 μm.
G 3 is set.

この第3次端面間隔G3は放電を開始するのに
適した間隔であり、この時点において公知の放電
装置、すなわち1対の放電電極5M,5Nを主体
にした放電が第1図ヘのごとく開始され、これと
同時に一方の光フアイバ端部2Aが他方の光フア
イバ端部2Bに向けて再移動され、かくして光フ
アイバ端部2A,2Bはこの際の放電熱(放電時
間1秒程度)と突き合わせ移動(移動量>10μ
m)とにより相互に融着され、第1図トのごとく
接続作業が完了する。
This tertiary end face spacing G 3 is a suitable spacing for starting a discharge, and at this point, a known discharge device, that is, a discharge mainly using a pair of discharge electrodes 5M and 5N, is generated as shown in Fig. 1. At the same time, one optical fiber end 2A is moved again toward the other optical fiber end 2B, and thus the optical fiber ends 2A and 2B absorb the discharge heat at this time (discharge time is about 1 second). Butt movement (travel amount > 10μ)
(m) are fused to each other, and the connection work is completed as shown in Fig. 1 (g).

なお、最近の提案例では第1図イ〜ロの間にお
いて光フアイバ端面3A,3Bのいずれか一方ま
たは両方に光学的なカツプリング特性のあるマツ
チング液(グリセリンをアルコールで溶解したも
の)を塗布し、第1図ハにおける軸合わせのと
き、第2図イのごとくそのマツチング液6より両
光フアイバ端面3A,3Bを光学的に結合して軸
合わせ時の受光パワー感度よく検出できるように
している。
In addition, in a recent proposal, a matching liquid (glycerin dissolved in alcohol) having optical coupling properties is applied to either or both of the optical fiber end faces 3A and 3B between A and B in Figure 1. , during alignment in Figure 1C, the matching liquid 6 optically couples both optical fiber end faces 3A and 3B as shown in Figure 2A, so that the received light power can be detected with high sensitivity during alignment. .

また、第1図ハにおける両光フアイバ1A,1
Bの軸合わせにより、前述の最大受光パワーが検
出できるが、その後の工程である第1図ニにおい
て両光フアイバ端面3A,3Bを相互に接触させ
たとき、すなわち第2図ロのごとく両光フアイバ
2A,2B相互にわたる直線状態を保持しながら
これらの端面3A,3Bを接触させたとき(接触
圧は0とみなす)この時点の受光パワーは両光フ
アイバ1A,1Bのコア相互が直接接触すること
により、前記軸合わせ時の最大受光パワーよりも
上回る。
In addition, both optical fibers 1A, 1 in FIG.
By aligning the axes of B, the aforementioned maximum received light power can be detected, but when the end faces 3A and 3B of both optical fibers are brought into contact with each other in the subsequent step of FIG. 1D, that is, as shown in FIG. When the end faces 3A and 3B of the fibers 2A and 2B are brought into contact with each other while maintaining a straight line between them (contact pressure is assumed to be 0), the received light power at this point is such that the cores of both optical fibers 1A and 1B are in direct contact with each other. This exceeds the maximum received light power during the axis alignment.

したがつて当該受光パワーのピークを検出する
ことにより、光フアイバ端面3A,3Bの間隔が
0となつたことがわかるが、上記ピークはその受
光パワーが増加傾向から減少傾向へと変化したと
きに検出できるのであり、それゆえ、受光パワー
が減少傾向を示す状態を一時的にとらねばならな
い。
Therefore, by detecting the peak of the received light power, it can be seen that the distance between the optical fiber end faces 3A and 3B has become 0, but the peak occurs when the received light power changes from an increasing trend to a decreasing trend. Therefore, it is necessary to temporarily maintain a state in which the received light power shows a decreasing tendency.

すなわち、端面間隔>0(第2図イの状態)、
端面間隔=0(第2図ロの状態)、端面間隔<0
(第2図ハの状態)の操作を介して受光パワーを
増加傾向、ピーク、減少傾向へと変移させるので
あり、この際、第2図ハの端面間隔<0では端面
3A,3Bが強く接触するとともに光フアイバ端
部2A,2B相互が曲がり状態となるので、これ
にともなう損失により受光パワーが減少する。
That is, the end face spacing > 0 (state in Fig. 2 A),
End distance = 0 (state in Figure 2 B), end distance <0
The received light power is changed to an increasing trend, a peak, and a decreasing trend through the operation (state shown in Fig. 2 C). At this time, when the end face spacing is <0 as shown in Fig. 2 C, the end faces 3A and 3B are in strong contact with each other. At the same time, the optical fiber ends 2A and 2B are bent to each other, and the received light power is reduced due to the resulting loss.

その後は第2図ハの状態から第2図ロの端面間
隔=0へもどすべく、光フアイバ端部2A,2B
を所定量だけ反突合方向へ相対移動させる。
Thereafter, in order to return the state shown in FIG. 2C to the end face distance = 0 shown in FIG. 2B, the optical fiber ends 2A and 2B are
is relatively moved by a predetermined amount in the opposite direction.

ところで、上述した端面間隔=0を確認する手
段として、従来、顕微鏡観察によるものがあつた
が、この方法によるときは、端面間が顕微鏡によ
り拡大されるとしても、分解能の低い肉眼で端面
間隔を識別することになるのでバラツキが生じ、
殊にマツチング液を光フアイバ端面に塗布してい
る場合、このようなバラツキ傾向が増す。
By the way, as a means of confirming the above-mentioned end face spacing = 0, conventionally there was a method using a microscope, but when using this method, even if the end face distance is enlarged with a microscope, the end face distance can be determined with the naked eye with low resolution. Since it is necessary to identify, there will be variations,
In particular, when a matching liquid is applied to the end face of an optical fiber, this tendency for variation increases.

一方、前記のごとく受光パワーをモニタしなが
ら端面間隔=0を設定する方法も考えられるが、
この場合も受光パワー測定時に誤差がともない、
また、受光パワーのピークを検出したとしても、
実際に端面間隔が0であるか否かについての確認
が必要であり、これらの点を含めた技術的配慮が
必要となる。
On the other hand, it is also possible to set the end face spacing = 0 while monitoring the received light power as described above.
In this case as well, there is an error when measuring the received light power.
Also, even if the peak of the received light power is detected,
It is necessary to confirm whether the end face spacing is actually 0 or not, and technical considerations including these points are required.

なお、当然のこととして、端面間隔=0が正確
に設定できないときは、放電時の第3次端面間隔
G3にも狂いが生じ、低損失の光フアイバ接続が
期待できなくなる。
As a matter of course, if the end face interval = 0 cannot be set accurately, the tertiary end face interval during discharge
G3 will also go awry, and low-loss optical fiber connections can no longer be expected.

(発明の目的) 本発明は上記の問題点に鑑み、光フアイバ融着
接続時における端面間隔=0の設定が正確に行な
え、当該設定操作の自動化がはかれる方法を提供
しようとするものである。
(Object of the Invention) In view of the above-mentioned problems, the present invention provides a method in which the end face spacing = 0 can be accurately set during optical fiber fusion splicing, and the setting operation can be automated.

(発明の構成) 本発明は、対をなす光フアイバの端部を互いに
対向させた後、これら光フアイバ端部の軸合わ
せ、光フアイバ端面間隔の設定、光フアイバ端部
の突き合わせ移動、光フアイバ端部への放電熱供
与など、所要の工程によりその対をなす光フアイ
バ端部を相互に融着接続する方法において、上記
対をなす光フアイバにわたつて光を通し、当該通
光状態においてこれら光フアイバの端部をその突
合方向へ相対移動させるとともに受光側光フアイ
バにおける測定により最大受光パワーが減少傾向
となるのを検出し、かつ、該検出時点で該光フア
イバ端部の突合移動を停止し、これにより上記光
フアイバの端面相互を接触状態とした後は、受光
パワーを検出している状態においてこれら光フア
イバ端部を反突合方向へ相対移動させる操作と、
これら光フアイバ端部を軸ずれ方向へ相対移動さ
せる操作とを、任意の順序で少なくとも1回ずつ
以上行ない、これにより光フアイバ相互の端面間
隔が0となる状態、および光フアイバ端部相互の
軸ずれ状態をそれぞれつくり、その後、これら光
フアイバ端部を相互に軸合わせすることを特徴と
している。
(Structure of the Invention) The present invention involves, after the ends of a pair of optical fibers are made to face each other, the axes of these optical fiber ends are aligned, the distance between the optical fiber end faces is set, the optical fiber ends are butted and moved, and the optical fibers are brought into contact with each other. In a method of fusion splicing the ends of paired optical fibers to each other by a necessary process such as applying discharge heat to the ends, light is passed across the paired optical fibers, and in the light-passing state, these The ends of the optical fibers are relatively moved in the abutting direction, and a tendency of the maximum received light power to decrease is detected by measurement on the light-receiving optical fiber, and at the time of this detection, the abutting movement of the optical fiber ends is stopped. After the end surfaces of the optical fibers are brought into contact with each other, the ends of the optical fibers are relatively moved in the opposite direction while the received light power is being detected;
These operations of relatively moving the ends of the optical fibers in the direction of axis deviation are performed at least once in any order, thereby creating a state in which the distance between the end faces of the optical fibers becomes 0, and the axis of the ends of the optical fibers. The method is characterized in that a misaligned state is created, and then the ends of these optical fibers are aligned with each other.

(実施例) 以下、本発明方法の実施例につき、図面を参照
して説明する。
(Example) Examples of the method of the present invention will be described below with reference to the drawings.

本発明が前提としている光フアイバ融着接続法
の具体例は前記第1図イ〜トの工程で述べた通り
であり、したがつてこれら全工程にわたる内容は
前掲の記載にゆずり、必要な工程のみ抽出して説
明する。
The specific example of the optical fiber fusion splicing method on which the present invention is based is as described in the steps of FIG. Only the following will be extracted and explained.

本発明において光フアイバ端面3A,3Bの端
面間隔を0に設定するのは、第1図ハの軸合わせ
工程までを終えた後、すなわち第1図ニの時点で
あり、この際の工程を実施するとき、あらかじめ
光フアイバ1A,1Bに備えられた測定手段によ
り受光パワーを測定する。
In the present invention, the distance between the end faces 3A and 3B of the optical fibers is set to 0 after the axis alignment step shown in FIG. At this time, the received light power is measured in advance by measuring means provided in the optical fibers 1A and 1B.

当該測定手段としては既知の透過法、後方散乱
法など、いずれの手段を採用してもよい。
As the measuring means, any known means such as a known transmission method or a backscattering method may be employed.

測定手段の具体的1例を第3図により略述する
と、発信側となる光フアイバ1Aの入射端側には
LED安定化光源またはLD安定化光源など、適当
な光源7を接続し、受信側となる光フアイバ1B
の出射端側にはPDまたはAPDなど、汎用光電力
計とか、高感度光電力計などによる光検出器8を
接続する。
A specific example of the measuring means will be briefly described with reference to FIG.
Connect an appropriate light source 7, such as an LED stabilized light source or LD stabilized light source, to the optical fiber 1B that will be the receiving side.
A photodetector 8 such as a general-purpose optical power meter such as a PD or APD, or a high-sensitivity optical power meter is connected to the output end side of the detector.

さらに光検出器8による測定値が制御器9を介
して光フアイバ用の送り機構10、軸合わせ機構
11などへ入力されるよう、これら各者8,9,
10,11を相互に接続する。
Further, the measurement values from the photodetector 8 are inputted to the optical fiber feeding mechanism 10, alignment mechanism 11, etc. via the controller 9, so that these devices 8, 9,
10 and 11 are connected to each other.

本発明における端面間隔=0の設定時、既述の
測定手段は光源7から光フアイバ1A,1B、光
検出器8へと光信号(光パルス)を送り、該光検
出器8により受光パワーを検出する。
When setting the end face distance = 0 in the present invention, the measurement means described above sends an optical signal (light pulse) from the light source 7 to the optical fibers 1A, 1B and the photodetector 8, and the photodetector 8 measures the received light power. To detect.

つぎに端面間隔を0とする際の操作について説
明する。
Next, the operation for setting the end face interval to 0 will be explained.

第1図ハ、第2図イのごとく光フアイバ端部2
A,2Bの軸合わせを行なつたとき、当該軸合わ
せによる最大受光パワーは第4図のP1となる。
Optical fiber end 2 as shown in Figure 1C and Figure 2B
When the axes A and 2B are aligned, the maximum received light power due to the axis alignment becomes P1 in FIG. 4.

その後、一方の光フアイバ端部2Aを他方の光
フアイバ端部2Bに向けて移動させると、受光パ
ワーが漸増し、かつ、第2図ハのごとく光フアイ
バ端面3A,3Bの間隔が0となつたとき、受光
パワーは第4図のP2で示すごとくピークとなる。
After that, when one optical fiber end 2A is moved toward the other optical fiber end 2B, the received light power gradually increases and the distance between the optical fiber end faces 3A and 3B becomes 0 as shown in FIG. At this time, the received light power reaches a peak as shown at P2 in FIG.

なおも光フアイバ端部2Aを上記の方向へ移動
させると、第2図ハのごとき押しこみ過剰により
受光パワーが第4図のP3にレベルダウンする。
If the optical fiber end 2A is still moved in the above-mentioned direction, the received light power will drop to P3 in FIG. 4 due to excessive pushing as shown in FIG. 2C.

このように受光パワーの増加傾向、減少傾向に
わたる光フアイバ端部2A,2Bの突き合わせを
行なうことにより、受光パワーのピークP2、すな
わち端面間隔=0がわかる。
In this way, by matching the optical fiber ends 2A and 2B over the increasing and decreasing trends of the received light power, the peak P 2 of the received light power, that is, the end face spacing=0, can be determined.

ついで光フアイバ端部2Aをインチングにより
前記とは反対の方向すなわち反突合方向へ移動さ
せると、受光パワーが再度漸増していき、端面間
隔が0となつた時点で受光パワーは第4図P4(=
P2)のごとくピークとなり、したがつてこの時点
で光フアイバ端部2Aの移動を止める。
Next, when the optical fiber end 2A is moved by inching in the opposite direction, that is, in the anti-butting direction, the received light power gradually increases again, and when the end face distance becomes 0, the received light power increases as shown in Fig. 4, P 4 . (=
P 2 ), and therefore the movement of the optical fiber end 2A is stopped at this point.

このP4を検出したとき、見かけ上は第2図ハの
状態から同図ロの状態にもどつているといえる。
When this P4 is detected, it can be said that the state apparently returns from the state shown in Figure 2C to the state shown in Figure 2B.

その後、いずれか一方の光フアイバ端部、例え
ば3Bを軸ずれ方向(光フアイバ軸線と直交する
方向)へ微小移動させる。
After that, one of the optical fiber ends, for example 3B, is slightly moved in the direction of axis deviation (direction perpendicular to the optical fiber axis).

ここで測定誤差以上の受光パワー変化がないと
き、光フアイバ端面3A,3Bがまだ強く接触し
ているのであり、正確に端面間隔が0になつてい
ないといえる。
When there is no change in the received light power greater than the measurement error, it can be said that the optical fiber end faces 3A and 3B are still in strong contact, and the end face distance has not become exactly zero.

換言すると、上記のごとき接触状態であること
により、光フアイバ端部2A,2Bが軸ずれする
ことなく連動し、それゆえ、受光パワーが変化し
なかつたといえる。
In other words, due to the above-mentioned contact state, the optical fiber ends 2A and 2B are interlocked without being axially misaligned, and therefore, it can be said that the received light power does not change.

一方、光フアイバ端面3A,3Bが接触圧ほぼ
0の状態で接触しているとき、つまり端面間隔=
0の精度が高いとき、上記軸ずれ移動により光フ
アイバ端部2A,2B相互が軸ずれし、受光パワ
ーが第4図P5のごとくレベルダウンする。
On the other hand, when the optical fiber end faces 3A and 3B are in contact with each other with almost zero contact pressure, that is, the end face distance =
When the accuracy of 0 is high, the optical fiber ends 2A and 2B are axially deviated from each other due to the above-mentioned axial deviation movement, and the level of the received light power is reduced as shown in FIG. 4, P5 .

したがつて受光パワーP4を検出した後は、既述
の軸ずれ操作により受光パワーP5があらわれるか
否かを検じ、受光パワーに変化がないときは、上
記P5が生じるまで、光フアイバ端部2Aの反突合
方向へのステツプ移動を行なう。
Therefore, after detecting the received light power P 4 , it is checked whether the received light power P 5 appears by the above-mentioned axis shift operation, and if there is no change in the received light power, the light is continued until the above-mentioned P 5 occurs. The fiber end 2A is moved stepwise in the opposite direction.

かくて受光パワーP5の生じた後は、軸ずれ状態
を修正すべく、軸ずれ操作した方向とは反対の方
向へ光フアイバ端部2Bを移動するのであり、こ
れにより第4図P6(=P2=P4)が得られたとき、
光フアイバ端部2A,2Bは軸合わせ状態に復帰
し、端面間隔は前記の操作を経ていることにより
正確な0の状態を呈す。
In this way, after the received light power P5 is generated, the optical fiber end 2B is moved in the opposite direction to the direction in which the axis deviation was operated in order to correct the axis deviation state, and thereby, as shown in Fig. 4 P 6 ( =P 2 =P 4 ) is obtained,
The optical fiber ends 2A and 2B are returned to their axially aligned state, and the distance between the end faces assumes an accurate zero state due to the above-described operation.

なお、上記において光フアイバ端面3A,3B
を突合方向、反突合方向へ、さらには軸ずれ方
向、軸合わせ方向などへ相対移動させるとき、そ
の端部を所定方向へ微小距離ずつステツプ移動さ
せるのがよく、こうすることにより各操作の制御
性が増す。
In addition, in the above, the optical fiber end faces 3A, 3B
When relatively moving in the butting direction, anti-butting direction, or in the axis misalignment direction or alignment direction, it is best to move the end part in small steps in a predetermined direction, and by doing this, each operation can be controlled. Sex increases.

また、光検出器8による前記P1〜P6の受光パワ
ーなど、これら測定値を制御器9へ入力し、さら
に該制御器9から所定の制御信号を送り機構1
0、軸合わせ機構11へ入力することにより、端
面間隔=0の設定が自動的に行なえるようにな
る。
In addition, these measured values, such as the received light power of P 1 to P 6 by the photodetector 8, are input to the controller 9, and further, a predetermined control signal is sent from the controller 9 to the mechanism 1.
By inputting 0 to the axis alignment mechanism 11, it becomes possible to automatically set the end face spacing to 0.

つぎに端面間隔=0を自動設定する際のプログ
ラミングにつき、第5図を参照して説明する。
Next, programming for automatically setting the end face interval=0 will be explained with reference to FIG.

第5図の11番、13番では、Pは読みとつた
受光パワーのうち最大のものを表わし(以下同
じ)、Newは最新の受光パワーを表わし(以下同
じ)、さらにldはNewよりも1つ前の受光パワ
ーを表わすとともにPower( )はx=Power
( )において新しい受光パワーを読みこんでそ
の値をxに代入することを表わす(以下同じ)。
In numbers 11 and 13 in Figure 5, P represents the maximum received light power that has been read out (the same applies below), New represents the latest received light power (the same applies below), and ld is 1 greater than New. It represents the previous received light power and Power ( ) is x = Power
( ) indicates reading the new received light power and substituting that value into x (the same applies below).

12番のZFは光フアイバ端部を突合方へ1ス
テツプずつ移動させることを意味する。
ZF number 12 means to move the optical fiber ends one step at a time toward abutment.

21番のmax(P、New)はPとNewのうち、
値の大きいものを表わす。
The 21st max(P, New) is between P and New,
Represents a large value.

31番のZRは光フアイバ端部を反突合方向へ
1ステツプずつ移動させることを意味する。
No. 31 ZR means to move the optical fiber end in the opposite direction one step at a time.

42番のXは光フアイバ端部を軸ずれ方向へ10
ステツプ移動させることを意味する。
No. 42 X points the end of the optical fiber in the axial direction 10
It means to move by step.

第5図において、11番のPが前記第4図の受
光パワーP1であるとき、つぎに測定値が入力され
るまでP=P1にてNewを保持するが、12番の
ZFが開始されると、そのステツプ移動にともな
い受光パワーが増加するので、13番に示すごと
くldは常に新しいNewに置き換えられ、当該ス
テツプ移動は第4図のP2,P3が検出されるまで行
なわれる。
In Fig. 5, when P at No. 11 is the received light power P 1 in Fig. 4, New is held at P = P 1 until the next measured value is input, but P at No. 12 is
When ZF starts, the received light power increases as the step moves, so ld is always replaced with the new New as shown in number 13, and P 2 and P 3 in Figure 4 are detected as the step moves. It will be carried out until

21番では順次変化する測定値のうち、値の大
きいものをピツクアツプするので、上記ステツプ
移動時における受光パワーのピーク、すなわち第
4図のP3を読みとることとなる。
Since No. 21 picks up the larger value among the sequentially changing measured values, the peak of the received light power at the time of the step movement, that is, P3 in FIG. 4 is read.

22番では、21番で読みこんだP3をNewと
し、このNewがP−0.05dB(Pは測定誤差を確認
するための基準値)と比較演算し、New<P−
0.05dBを満足させないときは測定誤差が大きいと
してNの指令を出し、ZFを再度行なわせる。
In No. 22, P 3 read in No. 21 is set as New, and this New is compared with P-0.05d B (P is the reference value for checking the measurement error), and New<P-
If 0.05d B is not satisfied, it is assumed that the measurement error is large and an N command is issued to perform ZF again.

22番においてNew<P−0.05dBを満足させた
ときはYESが出る。
When New<P-0.05d B is satisfied in No. 22, YES is output.

このYESの指令を受けた31番では、ZRによ
る1ステツプ移動を行ない、32番では該ステツ
プ移動により増加した受光パワーをNewとする。
At No. 31, which receives this YES command, one step movement is performed by ZR, and at No. 32, the received light power increased by this step movement is set as New.

さらに33番では32番のNewが受光パワーの
ピーク(許容誤差0.02dB)であるか否か、すなわ
ちNewが第4図P4の許容誤差の範囲内にあるか否
かをNew≧P−0.02dBにより比較演算し、Nの
ときはP4を検出するまでZRを繰り返し、YESの
ときはその指命を41番へ入力する。
Furthermore, in No. 33, it is determined whether New of No. 32 is the peak of the received light power (tolerance error 0.02dB ), that is, whether New is within the tolerance range of P4 in Figure 4. New≧P− Perform a comparison operation using 0.02d B , and if N, repeat ZR until P 4 is detected, and if YES, input the instruction to number 41.

41番では上記33番でYESが出たときの
Newを受け、さらに42番では41番にNewが入
つたことにより、Xすなわち軸ずれ方向の移動を
行なう。
In number 41, when YES comes out in number 33 above.
In response to New, New is entered in No. 41 at No. 42, and movement in the X, ie, axis deviation direction is performed.

ここで42番のステツプ移動により端面間隔が
0となつているとき、光フアイバ端部相互は軸ず
れを起こすが、これを確認するため、つぎの51
番においてZRを行なう。
Here, when the distance between the end faces becomes 0 due to step movement No. 42, the mutual axes of the ends of the optical fibers will occur, but in order to confirm this, the following
Perform ZR on the turn.

51番で1ステツプ移動を行なつたときの受光
パワーすなわち測定値は52番へNewとして入
り、さらに53番ではそのNewとld(受光パワ
ーのピーク)との差が測定誤差(0.02dB)以上で
あるか否かを比較演算する。
The received light power, that is, the measured value when moving one step at No. 51, enters No. 52 as New, and the difference between New and ld (peak of received light power) at No. 53 is the measurement error (0.02d B ). A comparison operation is performed to determine whether or not the value is greater than or equal to the value.

この53番においてNのときは51番が繰り
返され、YESのときは第4図のP5があつたとし
て、すなわち端面間隔が0であるとして、61番
への微調心(軸合わせ)へ指命を送る。
If this number 53 is N, then number 51 is repeated, and if it is YES, it is assumed that P 5 in Fig. 4 has occurred, that is, the end face spacing is 0, and the instruction is given to fine centering (axis alignment) to number 61. Send your life.

これに基づき61番では光フアイバ端部相互の
軸合わせを行ない、第4図のP6を検出した時点
で、すなわち光フアイバ1A,1Bのコア相互が
一致した時点で軸合わせを完了する。
Based on this, in No. 61, the ends of the optical fibers are aligned with each other, and the alignment is completed when P6 in FIG. 4 is detected, that is, when the cores of the optical fibers 1A and 1B coincide with each other.

なお、本発明の場合、第4図のP3を検出した
後、同図のP4を検出すべき光フアイバ端部の移動
(反突合方向)を省略することがあり、この場合
は軸ずれ方向のステツプ移動と反突合方向のステ
ツプ移動とを交互に行ない、これを必要な回数だ
け繰り返して前記P3,P4等を検出するようにな
る。
In the case of the present invention, after detecting P 3 in Fig. 4, the movement of the optical fiber end (in the opposite direction) that should detect P 4 in Fig. 4 may be omitted, and in this case, the axis misalignment may be omitted. The step movement in the direction and the step movement in the opposite direction are performed alternately, and this is repeated as many times as necessary to detect the above-mentioned P 3 , P 4 , etc.

これを第5図で例えると、同図の31番〜33
番を省略し、51番〜53番のステツプ移動が先
行、41番、42番のステツプ移動を後続するよ
うな、しかもこれら両ステツプ移動を必要回数だ
け繰り返すようなプログラミングを組むようにな
る。
To illustrate this in Figure 5, numbers 31 to 33 in the same figure
By omitting the step numbers 51 to 53, the program is programmed so that the step movements numbered 51 to 53 precede, and the step movements numbered 41 and 42 follow, and both of these step movements are repeated as many times as necessary.

第5図で述べた数値はすべて変更可能である。 All of the values mentioned in FIG. 5 can be changed.

(効果) 以上説明した通り、本発明方法によるときは、
光フアイバ相互にわたる通光状態において所定の
各操作を行なうようにしており、まず、対をなす
光フアイバの端面相互を接触状態にするとき、最
大受光レベルが減少傾向を示すまで光フアイバ端
部の突合移動を行なうから、端面間隔=0の基準
とすべき受光パワーのピークが正確に把握できる
ようになり、その後、端面間隔=0を設定すると
き、光フアイバ端部を反突合方向へ相対移動させ
るだけでなく、軸ずれ方向の相対移動をも行なう
ので、端面間隔=0が確実かつ精度よく設定で
き、あとは軸合わせ操作のみで足りるようにな
る。
(Effects) As explained above, when using the method of the present invention,
Each predetermined operation is performed while the optical fibers are passing through each other. First, when the end surfaces of a pair of optical fibers are brought into contact with each other, the ends of the optical fibers are kept in contact with each other until the maximum light reception level shows a decreasing tendency. Since the butt movement is performed, it is possible to accurately grasp the peak of the received light power that should be used as a reference for the end face spacing = 0. After that, when setting the end face spacing = 0, the optical fiber end is relatively moved in the opposite direction. In addition to the relative movement in the axis misalignment direction, the end face interval = 0 can be set reliably and accurately, and only the axis alignment operation is required.

したがつて光フアイバ相互を融着接続する際の
端面間隔>0の設定も精度よく行なえるようにな
り、ひいては低損失の光フアイバ融着接続が実現
できるようになる。
Therefore, it becomes possible to accurately set the end face spacing >0 when fusion splicing optical fibers to each other, and it becomes possible to achieve low-loss fusion splicing of optical fibers.

また、上記各操作時の受光パワーの測定値を所
定の制御系へ入力することにより、端面間隔=0
を設定する際の自動化も簡易にはかれる。
In addition, by inputting the measured values of the received light power during each of the above operations to a predetermined control system, the end face spacing = 0
You can easily automate the settings.

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

第1図イ〜トは本発明方法が前提としている光
フアイバ融着接続法の工程説明図、第2図イ〜ハ
は端面間隔=0を設定する際の主要工程を拡大し
た説明図、第3図は本発明方法における測定手段
の略示図、第4図は本発明方法における受光パワ
ーの測定値を示した説明図、第5図は本発明方法
を自動化する際のプログラミングをあらわしたフ
ローチヤートである。 1A,1B……光フアイバ、2A,2B……光
フアイバの端部、3A,3B……光フアイバの端
面、6……マツチング液、7……光源、8……光
検出器。
Figures 1 to 1 are explanatory diagrams of the process of the optical fiber fusion splicing method on which the method of the present invention is based; Figure 3 is a schematic diagram of the measuring means in the method of the present invention, Figure 4 is an explanatory diagram showing the measured value of the received light power in the method of the present invention, and Figure 5 is a flowchart showing programming when automating the method of the present invention. It's a chat. 1A, 1B... optical fiber, 2A, 2B... end of optical fiber, 3A, 3B... end face of optical fiber, 6... matching liquid, 7... light source, 8... photodetector.

Claims (1)

【特許請求の範囲】 1 対をなす光フアイバの端部を互いに対向させ
た後、これら光フアイバ端部の軸合わせ、光フア
イバ端面間隔の設定、光フアイバ端部の突き合わ
せ移動、光フアイバ端部への放電熱供与など、所
要の工程によりその対をなす光フアイバ端部を相
互に融着接続する方法において、上記対をなす光
フアイバにわたつて光を通し、当該通光状態にお
いてこれら光フアイバの端部をその突合方向へ相
対移動させるとともに受光側光フアイバにおける
測定により最大受光パワーが減少傾向となるのを
検出し、かつ、該検出時点で該光フアイバ端部の
突合移動を停止し、これにより上記光フアイバの
端面相互を接触状態とした後は、受光パワーを検
出している状態においてこれら光フアイバ端部を
反突合方向へ相対移動させる操作と、これら光フ
アイバ端部を軸ずれ方向へ相対移動させる操作と
を、任意の順序で少なくとも1回ずつ以上行な
い、これにより光フアイバ相互の端面間隔が0と
なる状態、および光フアイバ端部相互の軸ずれ状
態をそれぞれつくり、その後、これら光フアイバ
端部を相互に軸合わせする光フアイバ融着接続法
における光フアイバ端面間隔設定方法。 2 対をなす光フアイバの端部をその突合方向へ
相対移動させるとき、これら光フアイバの端面に
マツチング液を塗布する特許請求の範囲第1項記
載の光フアイバ融着接続法における光フアイバ端
面間隔設定方法。
[Claims] After the ends of a pair of optical fibers are made to face each other, the axes of these optical fiber ends are aligned, the distance between the optical fiber end faces is set, the optical fiber ends are moved to butt each other, and the optical fiber ends are moved. In the method of fusion splicing the ends of the optical fibers forming the pair by a necessary process such as applying discharge heat to relatively moving the end portions of the optical fibers in the abutting direction, detecting a tendency of the maximum received light power to decrease by measurement on the receiving side optical fiber, and stopping the abutting movement of the optical fiber end portions at the time of the detection, After the end surfaces of the optical fibers are brought into contact with each other, the ends of the optical fibers are relatively moved in the opposite direction while the received light power is being detected, and the ends of the optical fibers are moved in the direction of misalignment. The operation of moving the optical fibers relative to each other is performed at least once in any order, thereby creating a state in which the distance between the end faces of the optical fibers becomes 0 and a state in which the ends of the optical fibers are misaligned with each other. A method for setting the spacing between optical fiber end faces in an optical fiber fusion splicing method in which optical fiber ends are aligned with each other. 2. Optical fiber end face spacing in the optical fiber fusion splicing method according to claim 1, in which a matching liquid is applied to the end faces of the optical fibers when the ends of the pair of optical fibers are relatively moved in the abutment direction. Setting method.
JP9263684A 1984-05-09 1984-05-09 Setting method of space between end faces of optical fibers in method for welding and connecting optical fibers Granted JPS60237409A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9263684A JPS60237409A (en) 1984-05-09 1984-05-09 Setting method of space between end faces of optical fibers in method for welding and connecting optical fibers

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9263684A JPS60237409A (en) 1984-05-09 1984-05-09 Setting method of space between end faces of optical fibers in method for welding and connecting optical fibers

Publications (2)

Publication Number Publication Date
JPS60237409A JPS60237409A (en) 1985-11-26
JPS6216402B2 true JPS6216402B2 (en) 1987-04-13

Family

ID=14059928

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9263684A Granted JPS60237409A (en) 1984-05-09 1984-05-09 Setting method of space between end faces of optical fibers in method for welding and connecting optical fibers

Country Status (1)

Country Link
JP (1) JPS60237409A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6082313B2 (en) * 2013-05-23 2017-02-15 日本電信電話株式会社 Distance measuring apparatus and method for optical axis adjustment
JP6082320B2 (en) * 2013-06-05 2017-02-15 日本電信電話株式会社 Optical axis adjusting device and process thereof

Also Published As

Publication number Publication date
JPS60237409A (en) 1985-11-26

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