JPH0361926B2 - - Google Patents
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- Publication number
- JPH0361926B2 JPH0361926B2 JP58218891A JP21889183A JPH0361926B2 JP H0361926 B2 JPH0361926 B2 JP H0361926B2 JP 58218891 A JP58218891 A JP 58218891A JP 21889183 A JP21889183 A JP 21889183A JP H0361926 B2 JPH0361926 B2 JP H0361926B2
- Authority
- JP
- Japan
- Prior art keywords
- fiber
- core
- fibers
- centers
- center
- 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 - Lifetime
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/255—Splicing of light guides, e.g. by fusion or bonding
- G02B6/2555—Alignment or adjustment devices for aligning prior to splicing
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/255—Splicing of light guides, e.g. by fusion or bonding
- G02B6/2551—Splicing of light guides, e.g. by fusion or bonding using thermal methods, e.g. fusion welding by arc discharge, laser beam, plasma torch
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- 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】
本発明は低損失にして高強度なフアイバの融着
接続方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a low-loss, high-strength fiber fusion splicing method.
フアイバ相互を接続する方法として、従来融着
接続方法が用いられている。融着するための熱源
には、対向する電極間の高電圧をかけて起こさせ
た放電や、ガスバーナによる火災、その他高出力
レーザ等が用いられている。一方、コア径の小さ
いフアイバ(光フアイバ)、例えば単一モードフ
アイバの接続にあたつては、その損失を低減する
ために接続される2本のフアイバのコアの中心間
のずれ(軸ずれ量)を最小にする必要がある。 Conventionally, a fusion splicing method has been used to connect fibers to each other. As a heat source for fusing, electric discharge generated by applying a high voltage between opposing electrodes, fire caused by a gas burner, or other high-power lasers are used. On the other hand, when connecting fibers with small core diameters (optical fibers), such as single-mode fibers, in order to reduce loss, the amount of misalignment between the centers of the cores of the two fibers being connected (the amount of axial misalignment) ) must be minimized.
そのため、従来は融着接続の前段階でフアイバ
相互のコア軸を一致させるコアの軸合せを行うと
ともに、融着過程においてコアの軸ずれができる
だけ起こらないような加熱条件を選定するように
している。このような従来の融着接続方法を第1
図を参照して説明する。 For this reason, conventionally, the core axes of the fibers are aligned to match each other before fusion splicing, and heating conditions are selected to prevent core axes from shifting as much as possible during the fusion splicing process. . This conventional fusion splicing method is the first
This will be explained with reference to the figures.
接続すべきフアイバの片方2を固定台3に固定
し、他のフアイバ1を同図に示すz、y、zの各
方向に微動可能な固定台4に固定し、これらフア
イバ1,2を相互に突合わせる。そして、接続前
段階としてコアの軸合せを行うために、光源5か
らの出力光をフアイバ2からフアイバ1に入射さ
せ、フアイバ1および2を透過して受光器6に到
達する光のパワをモニタし、このパワが最大とな
るように固定台4をx、yの2方向に動かして調
整する。この後、放電電極7,8間に高電圧を印
加して放電を起こさせ、この熱によりフアイバ
1,2の端面を溶融し、固定台4をz方向にわず
かに移動させ、適当量フアイバ1をフアイバ2に
押し込んで接続を完了する。ここでは、放電を用
いて融着する方法を例に説明したが、先に述べた
ようにガスバーナの火災で加熱する方法なども同
じ目的で用いられている。 One side 2 of the fibers to be connected is fixed to a fixed base 3, and the other fiber 1 is fixed to a fixed base 4 that can be moved slightly in each of the z, y, and z directions shown in the figure, and these fibers 1 and 2 are connected to each other. Match with. Then, in order to align the cores as a pre-connection step, the output light from the light source 5 is input from the fiber 2 to the fiber 1, and the power of the light transmitted through the fibers 1 and 2 and reaching the optical receiver 6 is monitored. Then, adjust the power by moving the fixed base 4 in two directions, x and y, so that this power becomes maximum. After that, a high voltage is applied between the discharge electrodes 7 and 8 to cause a discharge, and the end faces of the fibers 1 and 2 are melted by this heat, and the fixing table 4 is slightly moved in the z direction to remove an appropriate amount of the fibers 1 and 2. into fiber 2 to complete the connection. Here, a method of fusing using electric discharge has been explained as an example, but as mentioned earlier, a method of heating with a fire from a gas burner is also used for the same purpose.
このような融着接続をおこなう場合、もし、フ
アイバにコア偏心があるとコアは相互に一致して
いてもフアイバの中心は一致していない。第2図
aはこのような接続前における2本のフアイバの
コア中心とフアイバ中心の断面内の位置関係を示
すものである。コア中心11およびフアイバ中心
13が一方のフアイバ2に関するものであり、コ
ア中心12およびフアイバ中心14が他方のフア
イバ1に関するものである。 When performing such fusion splicing, if the fibers have core eccentricity, the centers of the fibers will not coincide even if the cores coincide with each other. FIG. 2a shows the positional relationship in the cross section between the core centers of the two fibers and the fiber centers before such connection. Core center 11 and fiber center 13 relate to one fiber 2, core center 12 and fiber center 14 relate to the other fiber 1.
コア中心11,12は調心によつて完全に一致し
ている。しかし、フアイバのコア偏心がそれぞれ
d1,d2であると、フアイバの中心13,14は必
ずしも一致しない。この状態で融着を行うと、融
着しているフアイバ端間に表面張力が作用し、フ
アイバの中心を一致させるような移動がおこる。
移動方向はフアイバ中心13,14を結ぶ方向
で、軸の移動量Dは一般にフアイバ中心間の初期
距離d12に比例し、D=kd12で与えられる。kは
放電(融着)時の温度や放電(融着)の時間で決
まるもので、ほぼ一定の値である。このような融
着時のフアイバ軸の移動の結果、第2図bに示す
ようにフアイバ中心間が近接し、例えばフアイバ
中心13は13′に、それに対応してコア中心1
1は11′に移る。その結果、融着接続後はコア
中心11′および12間にDの軸ずれが発生し、
接続損失を劣化させることになる。The core centers 11 and 12 are perfectly aligned due to alignment. However, the core eccentricity of the fibers is
When d 1 and d 2 , the fiber centers 13 and 14 do not necessarily coincide. When fusion is performed in this state, surface tension acts between the ends of the fused fibers, causing the fibers to move so as to bring their centers into alignment.
The direction of movement is the direction connecting the fiber centers 13 and 14, and the amount of shaft movement D is generally proportional to the initial distance d 12 between the fiber centers, given by D=kd 12 . k is determined by the temperature during discharge (fusion) and the time of discharge (fusion), and is a substantially constant value. As a result of this movement of the fiber axes during fusion, the fiber centers are brought closer to each other, as shown in FIG.
1 moves to 11'. As a result, after fusion splicing, an axis deviation of D occurs between core centers 11' and 12,
This will degrade the connection loss.
一般的にDの軸ずれが生じている時に発生する
接続損失α(単位dB)は、
α=4.34・2D2/W1 2+W2 2
で与えられる。W1、W2は被接続フアイバ1,2
でそれぞれのスポツトサイズであり、通常の単一
モードフアイバの場合ほぼ5μmである。 In general, the connection loss α (unit: dB) that occurs when the axis of D is misaligned is given by α=4.34·2D 2 /W 1 2 +W 2 2 . W 1 and W 2 are connected fibers 1 and 2
The respective spot size is approximately 5 μm for a typical single mode fiber.
前記、融着中の軸の移動は、コアが偏心してい
るような場合に発生するもので、その大きさは
高々2μmというわずかな量であるが、それでも、
上式から計算する接続損失の値は軸ずれDが1μ
mで0.2dB、2μmで0.7dBとなり、接続損失とし
ては無視できない量となる。 The above-mentioned movement of the axis during fusion occurs when the core is eccentric, and the size of the movement is a small amount of 2 μm at most, but still.
The connection loss value calculated from the above formula is when the axis misalignment D is 1μ
It is 0.2 dB at m and 0.7 dB at 2 μm, which is a non-negligible connection loss.
このような表面張力の影響を低減する(k値を
下げる)ために放電時間を短くしたり放電時温度
を下げるようにパワーを低減すると、接続強度が
低下したり溶融が不十分となり、端面間に気泡が
混入し、逆に接続損失が増大したりして問題とな
る。そのため、強度をある程度満足し、かつ、安
定した接続が行われるような範囲でしか放電時
間、放電パワを低減することができず、偏心率が
2〜3%程度のフアイバの接続になると表面張力
の影響を避けることが困難で、低損失な接続損失
を得ることが難しかつた。 If you reduce the power by shortening the discharge time or lowering the temperature during discharge in order to reduce the effect of surface tension (lower the k value), the connection strength will decrease, melting will be insufficient, and the gap between the end faces will decrease. This causes problems as air bubbles get mixed in and conversely increase connection loss. Therefore, it is only possible to reduce the discharge time and discharge power within a range that satisfies the strength to a certain extent and provides a stable connection, and when connecting fibers with an eccentricity of about 2 to 3%, the surface tension It was difficult to avoid the effects of this, and it was difficult to obtain low connection loss.
特に、高強度な接続を行いたい場合は融着時間
を長くする必要があり、表面張力の影響を下げる
ことは非常に困難であつた。 In particular, when a high-strength connection is desired, it is necessary to increase the fusion time, and it has been extremely difficult to reduce the effects of surface tension.
本発明は、このような表面張力の影響によつて
接続後にコアの軸ずれが残ることを除去するため
に、調心段階でコアの偏心状態やフアイバの中心
間距離を観察し、表面張力によつて移動する軸ず
れ量の分だけ予めコア相互にずれを与えて調心
し、融着時の軸ずれを利用してコアを一致させ、
接続後には軸ずれが残留せず低損失な接続ができ
るようにしたことを特徴とし、その目的とすると
ころは、コアの軸ずれが残留しないフアイバ融着
接続方法を提供することにある。以下、本発明を
図面に示す実施例に基づいて詳細に説明する。 In order to eliminate the core axis misalignment that remains after connection due to the influence of surface tension, the present invention observes the eccentricity of the core and the distance between fiber centers during the alignment stage, and measures the surface tension. Therefore, the cores are aligned by giving a mutual offset in advance by the amount of axis deviation that will be moved, and the cores are aligned using the axis deviation during fusion,
The fiber fusion splicing method is characterized in that no axial misalignment remains after splicing and low-loss splicing can be performed, and the object thereof is to provide a fiber fusion splicing method in which no axial misalignment of the core remains. Hereinafter, the present invention will be described in detail based on embodiments shown in the drawings.
本発明を実施するためには、接続しようとして
いるフアイバ間のコアの状態、フアイバ中心の距
離と方向を求めなければならない。第3図はその
ようなフアイバ中のコアを観察しながら調心し、
接続を行う融着装置の一例を示すものである。 In order to carry out the present invention, it is necessary to determine the state of the cores between the fibers to be connected, as well as the distance and direction of the fiber centers. Figure 3 shows how to align while observing the core in such a fiber.
This figure shows an example of a fusion device that performs the connection.
水平方向(x軸方向)のフアイバの状態は、光
源21でフアイバ1,2をその真下から照らし、
その像を顕微鏡23で観察する。一方垂直方向
(y軸方向)のフアイバの状態は、光源22でフ
アイバ1,2をその真横から照らし、ミラー24
を介してその像を顕微鏡23で観察する。 The state of the fibers in the horizontal direction (x-axis direction) is determined by illuminating the fibers 1 and 2 from directly below with a light source 21.
The image is observed with a microscope 23. On the other hand, to determine the state of the fibers in the vertical direction (y-axis direction), the light source 22 illuminates the fibers 1 and 2 from directly beside them, and the mirror 24
The image is observed through a microscope 23.
フアイバ1,2は第1図と同様、固定台3と、
x、y、zそれぞれ軸に微動可能な固定台4にそ
れぞれ固定しておく。 As in FIG. 1, the fibers 1 and 2 are connected to a fixed base 3,
They are each fixed to a fixed base 4 that can be slightly moved along the x, y, and z axes.
第4図a,bは観察される像を示す図であり、
同図aは垂直方向から観察したものであつて、水
平方向のずれを示す像、同図bは水平方向から観
察したものであつて、垂直方向のずれを示す像で
ある。これらの図に示すように像はフアイバ表面
部とコアの中心部が暗くなつている。したがつて
これらの像から各フアイバの中心位置31,3
2,33,34およびコアの中心位置35,3
6,37,38が求められる。実際には、フアイ
バクラツドのレンズ効果によりコアの観察位置3
5〜38が実際の異なつており、これを補正しな
ければ真の位置は求められないが、ここで説明を
簡単にするため、35〜38を真のコア位置とす
る。まず、調心の際には水平方向についてコア中
心35,36を一致させるように固定台4をx軸
方向に移動する。次いで垂直方向についてコア中
心37,38を一致させるようy軸方向に移動す
る。 Figures 4a and 4b are diagrams showing the observed images,
Figure a is an image observed from the vertical direction and shows the deviation in the horizontal direction, and Figure b is an image observed from the horizontal direction and shows the deviation in the vertical direction. As shown in these figures, the images are dark at the fiber surface and at the center of the core. Therefore, from these images, the center position 31, 3 of each fiber can be determined.
2, 33, 34 and core center position 35, 3
6, 37, 38 are found. In reality, due to the lens effect of the fiber cladding, the core observation position 3
5 to 38 are actually different, and the true position cannot be determined unless this is corrected. However, to simplify the explanation, 35 to 38 are assumed to be the true core positions. First, during alignment, the fixing base 4 is moved in the x-axis direction so that the core centers 35 and 36 are aligned in the horizontal direction. Next, it is moved in the y-axis direction so that the core centers 37 and 38 are aligned in the vertical direction.
この結果、第5図a,bに示すように水平、垂
直方向ともコア軸は一致する。第5図aは水平方
向のずれを示す像、第5図bは垂直方向のずれを
示す像である。従来はこれで調心を完了して接続
を行うわけであるが、この状態では第5図a,b
に示すように、フアイバ中心位置がそれぞれ3
1′,32′,33′,34′で示すようになり、そ
れぞれコアの中心に対してd1x、d2x、d1y、d2yの
ずれがある。これをフアイバの断面内の位置関係
でみると丁度第2図aと同じようになり、フアイ
バ中心間にはd12なるずれが存在する。この状態
で接続すると融着の温度や時間によつて決まる表
面張力による軸の移動D(=kd12)が発生し、接
続損失の劣化がおこる。 As a result, the core axes coincide in both the horizontal and vertical directions, as shown in FIGS. 5a and 5b. FIG. 5a is an image showing the shift in the horizontal direction, and FIG. 5b is an image showing the shift in the vertical direction. Conventionally, this completes the alignment and connects the connection, but in this state, Fig. 5 a and b
As shown in , the fiber center position is 3.
1', 32', 33', and 34', and are shifted by d 1x , d 2x , d 1y , and d 2y from the center of the core, respectively. If we look at this in terms of the positional relationship within the cross section of the fiber, it will be exactly the same as that shown in Figure 2a, and there will be a deviation of d 12 between the fiber centers. If they are connected in this state, the shaft will move D (=kd 12 ) due to surface tension determined by the temperature and time of fusion, resulting in deterioration of connection loss.
第6図はコア観察によつてコアを一致させてか
ら融着接続した時の融着の前後での損失の分布の
一例を比較したもので、用いたフアイバの偏心率
は約3%である。コアの観察自体に誤差があるた
め融着前にもわずかに軸ずれが存在しているが、
融着過程の軸ずれによつてさらに損失が劣化して
いることがわかる。また、第7図はその時のフア
イバ中心の位置の変化から求めたkの値を示した
ものであり、0.2〜0.35に大きな度数が分布して
おり、中心値は0.28である。 Figure 6 shows an example of the loss distribution before and after fusion splicing when the cores are matched by core observation and then fusion spliced.The eccentricity of the fiber used is approximately 3%. . Because there is an error in the observation of the core itself, there is a slight axis misalignment even before welding.
It can be seen that the loss is further deteriorated due to axis misalignment during the fusion process. Moreover, FIG. 7 shows the value of k determined from the change in the position of the fiber center at that time, and large frequencies are distributed from 0.2 to 0.35, with the center value being 0.28.
そこで本発明ではコアを一致させた状態ですぐ
融着をせずその時のフアイバ中心位置のずれd1x、
d2x、d1y、d2yを求め、第8図に示すように
d12/1−k〔ここでd12=√(2x−1x)2+(2y
−1y)2
〕にフアイバ中心が互いに離れるように固定台
4をx軸、y軸方向に移動させる。第8図ではフ
アイバ中心が位置43にある一方のフアイバを固
定し、フアイバ中心が位置44にある他方のフア
イバをそのフアイバ中心が45にくるように移動
する場合を示している。すなわち、2本のフアイ
バのコア中心を位置41に一致させた場合の他方
のフアイバ中心の位置44と一方のフアイバ中心
の位置43とを結ぶ線の延長上にある位置45に
他方のフアイバの中心が来るように他方のフアイ
バを移動させる。その結果、当該他方のフアイバ
のコア中心は位置41から位置42に移動する。
移動する距離はk/1−kd12であり、x軸方向には
k/1−k(d2x−d1x)、y軸方向にはk/1−k(d2
y
−d1y)である。 Therefore, in the present invention, we do not immediately fuse the fibers with the cores aligned, but rather the deviation d 1x of the fiber center position at that time,
Find d 2x , d 1y , and d 2y as shown in Figure 8.
d 12 /1-k [here d 12 =√( 2x − 1x ) 2 + ( 2y
−1y ) 2 ], move the fixing base 4 in the x-axis and y-axis directions so that the fiber centers are separated from each other. FIG. 8 shows a case in which one fiber whose fiber center is at position 43 is fixed, and the other fiber whose fiber center is at position 44 is moved so that its fiber center is at position 45. That is, when the core centers of the two fibers are aligned with position 41, the center of the other fiber is located at position 45, which is an extension of the line connecting the center position 44 of the other fiber and the center position 43 of one fiber. Move the other fiber so that As a result, the core center of the other fiber moves from position 41 to position 42.
The distance traveled is k/1- kd12 , k/1-k( d2x - d1x ) in the x-axis direction, and k/1-k( d2x ) in the y-axis direction.
y −d 1y ).
この時の移動量はd12が通常のフアイバを使用
する限り、高々4〜5μmであるため、kの値に
も依存するがせいぜい2μmまでの値である。 The amount of movement at this time is 4 to 5 μm at most as long as d 12 uses a normal fiber, so it is up to 2 μm at most, although it also depends on the value of k.
この状態で融着を行うと表面張力の効果によつ
てフアイバ中心45−43間で移動か起こるが、
その時の移動量はd12/1−k×kであり、丁度、後
でずらした分の軸ずれを打消す。そのため、融着
接続後のフアイバ中心位置は再び45から44
へ、またコア中心位置は42から41へ移つてコ
ア軸は完全に一致して接続されることになり、そ
の結果、軸ずれ損失の少い、低損失接続が可能と
なる。 If fusion is performed in this state, movement will occur between the fiber centers 45 and 43 due to the effect of surface tension, but
The amount of movement at that time is d 12 /1-k×k, which exactly cancels out the axis deviation caused by the later shift. Therefore, the fiber center position after fusion splicing is again from 45 to 44
Further, the core center position is moved from 42 to 41, and the core axes are connected in perfect alignment, resulting in a low-loss connection with less axis misalignment loss.
実際には、Rの値は第7図のように完全に一定
値ではないため、コアの中心の移動先も41の回
りにばらつくことになるが、何れにしても軸ずれ
損失の少ない低損失接続が可能となる。 In reality, the value of R is not a completely constant value as shown in Figure 7, so the destination of the center of the core will also vary around 41, but in any case, the loss is low with little axis misalignment loss. Connection is now possible.
なお、Rの値は先に示した例の場合は、ほぼそ
の中心値0.28にすればよいが、この値は前に説明
したように融着の際の条件、温度や時間に依存す
るもので、装置によつてそれぞれ異なると思わ
れ、装置毎に予めいくつかの接続を行い、その時
のフアイバ中心の移動を第7図と同様に測定して
決定しておくことが望ましい。 In addition, in the case of the example shown earlier, the value of R should be approximately the central value of 0.28, but as explained earlier, this value depends on the conditions, temperature, and time during fusion. , which may differ depending on the device, it is desirable to make several connections for each device in advance and measure and determine the movement of the fiber center at that time in the same manner as shown in FIG.
このように表面張力によつて移動する軸ずれ量
を予め与えて調心すれば、表面張力の影響がかな
り大きいような融着条件、例えば融着時間を長く
したような場合でも接続後のコア軸を一致させる
ことができ、融着時間を短くした時のような不安
定な接続が行われたり、強度が低下するといつた
弊害をおこさず低損失な接続が可能となる。 In this way, if the amount of axial deviation that moves due to surface tension is given in advance for alignment, even if the influence of surface tension is quite large, such as when the welding time is long, the core after joining can be adjusted. The axes can be aligned, and low-loss connections can be made without causing problems such as unstable connections when shortening the fusion time or weakening of the welding strength.
なお、コアの観察方法については、ここでは顕
微鏡による目視観察を例に説明してきたが、実際
にはフアイバの中心のずれ量の検出や、またそれ
に応じたコアの軸ずれの与え方については正確さ
が必要である。これは、第9図に示すように顕微
鏡にTVカメラのような撮像装置51と、撮像信
号からコアの中心、フアイバ中心を検出し、接続
すべき2本のフアイバ間のそれらの相対位置関係
を求める画像処理装置52、およびその結果をも
とに固定台4の移動を制御する制御装置53を設
けることによつて容易に実現でき、また、これに
よつて自動的に調心を完了させ、融着接続を行う
ことも可能である。 The core observation method has been explained here using visual observation using a microscope as an example, but in reality, it is difficult to accurately detect the amount of deviation of the fiber center and how to give the core axis deviation accordingly. It is necessary to As shown in FIG. 9, this method uses an imaging device 51 such as a TV camera on a microscope, detects the center of the core and the center of the fiber from the imaging signal, and calculates the relative positional relationship between the two fibers to be connected. This can be easily realized by providing the desired image processing device 52 and a control device 53 that controls the movement of the fixed base 4 based on the result, and thereby automatically completes the alignment. It is also possible to perform fusion splicing.
また、フアイバの軸合わせおよび移動手順につ
いては、第2図および第8図において、説明の簡
単のため先に2つのコア中心の軸合わせを行い、
次に表面張力による軸ずれを考慮した補正分
k/1−kd12の移動を行う方法で説明していたが、
第4図に示すように2つのフアイバを設置し、そ
れぞれのフアイバのコア偏心および2つのフアイ
バ間のコア中心のずれを測定し、コア中心を一致
させた時のフアイバ中心にずれ量d12をコア偏心
状態(d1x、d1y、d2x、d2y)より求め、次に前記
k/1−kd12とコア中心のずれ量とのベクトル和を
演算して、その演算結果をもとに一つの工程でフ
アイバの移動を行うこともできる。 Regarding the fiber axis alignment and movement procedure, in FIGS. 2 and 8, for ease of explanation, first align the two core centers,
Next, we explained the method of moving the correction amount k/1 - kd 12 to account for the axis misalignment due to surface tension, but as shown in Figure 4, two fibers are installed, and the core eccentricity of each fiber is Then, measure the deviation of the core centers between the two fibers, find the deviation d 12 of the fiber center from the core eccentricity state (d 1x , d 1y , d 2x , d 2y ) when the core centers are aligned, and calculate the following: It is also possible to calculate the vector sum of the above-mentioned k/1-kd 12 and the deviation amount of the core center, and move the fiber in one step based on the calculation result.
また、フアイバの観察についても第3図のよう
な光源と顕微鏡の設置による方法以外にも、コア
中心、およびフアイバ中心の識別が可能である方
法であればその何れであつてもかまわないことは
いうまでもない。 Furthermore, regarding the observation of the fiber, in addition to the method using a light source and microscope as shown in Figure 3, any method that allows the identification of the core center and fiber center may be used. Needless to say.
以上説明したように本発明によれば、接続すべ
きフアイバのコア中心位置およびフアイバ中心位
置を検出できる装置を用いてコアの調心を行つた
上、さらに、融着時の表面張力によつて生ずる軸
ずれを予め相互のコアに与えておくので、融着接
続によつて完全なコア軸の合わせを行うことがで
き、コア偏心の大きなフアイバであつても十分融
着時間を長くするような融着条件を採用すること
ができ、低損失でかつ高強度な接続が可能とな
る。 As explained above, according to the present invention, core alignment is performed using a device that can detect the core center position of the fibers to be connected and the fiber center position, and furthermore, the core centering is performed using a device that can detect the core center position of the fiber to be connected and the fiber center position. Since the axis misalignment that occurs is given to the mutual cores in advance, the core axes can be perfectly aligned by fusion splicing, and even if the fiber has a large core eccentricity, the fusion time can be sufficiently long. It is possible to adopt fusion bonding conditions, and a low-loss and high-strength connection is possible.
第1図は従来の光パワモニタ法を用いた調心と
融着接続の方法を説明する説明図、第2図は従来
の調心方法でコア軸合せを行つた時の融着接続時
の軸ずれの説明図、第3図は本発明の接続方法を
実施するコア観察形の融着装置の一例を示す概略
構成図、第4図a,b、第5図a,bは観察され
たフアイバ像のコア中心、フアイバ中心位置を示
す図、第6図は融着時の表面張力に起因して生じ
た軸ずれによるフアイバの損失劣化の一例を示す
図、第7図はフアイバ融着時の表面張力による軸
移動係数kの分布例を示す図、第8図は本発明に
よる調心方法を行つた時、コア、フアイバ中心の
相互関係を示す説明図、第9図は第3図の自動化
を具現する装置の概略構成図である。
1,2……フアイバ、3,4……固定台、7,
8……放電電極、21,22……照明用光源、2
3……顕微鏡、31〜34,31′〜34′……フ
アイバ中心線、35〜38……コア中心線、4
1,42……コア中心、43,44,45……フ
アイバ中心、51……撮像装置、52……画像処
理装置、53……固定台制御装置。
Figure 1 is an explanatory diagram explaining the alignment and fusion splicing method using the conventional optical power monitoring method, and Figure 2 is an illustration of the axis during fusion splicing when core alignment is performed using the conventional alignment method. FIG. 3 is a schematic configuration diagram showing an example of a core observation type fusion splicing device implementing the connection method of the present invention, FIGS. 4 a, b, and 5 a, b are diagrams of observed fibers. Figure 6 shows an example of fiber loss and deterioration due to axis misalignment caused by surface tension during fusion. Figure 7 shows the position of the core center and fiber center of the image. A diagram showing an example of the distribution of the axis movement coefficient k due to surface tension, FIG. 8 is an explanatory diagram showing the mutual relationship between the core and fiber center when performing the alignment method according to the present invention, and FIG. 9 is an automation diagram of FIG. 3. 1 is a schematic configuration diagram of a device that embodies this. 1, 2...Fiber, 3, 4...Fixing base, 7,
8... Discharge electrode, 21, 22... Light source for illumination, 2
3... Microscope, 31-34, 31'-34'... Fiber center line, 35-38... Core center line, 4
1, 42... core center, 43, 44, 45... fiber center, 51... imaging device, 52... image processing device, 53... fixed base control device.
Claims (1)
線状につき合わせて相互のコア中心を一致させた
ときに生じるフアイバ中心相互のずれを検出し、 そのときのフアイバ中心相互を結ぶ線の延長線
上で前記ずれがより大きくなる方向に、後に行う
融着工程で前記ずれに応じて発生するフアイバ中
心間の予測される軸ずれ量だけ余分にずれを与え
た後、 熱源を用いてフアイバ端相互を溶融接続するこ
とを特徴とするフアイバ融着接続方法。[Scope of Claims] 1. Detect the deviation of the fiber centers that occurs when the fiber ends of two fibers to be connected are aligned in a straight line and their mutual core centers coincide, and detect the mutual deviation of the fiber centers at that time. After applying an extra misalignment in the direction in which the misalignment becomes larger on the extension line of the connecting line by the amount of axis misalignment expected between the fiber centers that will occur in accordance with the misalignment in the subsequent fusion process, using a heat source. A fiber fusion splicing method characterized in that the fiber ends are fused and spliced to each other.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP21889183A JPS60111205A (en) | 1983-11-21 | 1983-11-21 | Fiber fusion connecting method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP21889183A JPS60111205A (en) | 1983-11-21 | 1983-11-21 | Fiber fusion connecting method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60111205A JPS60111205A (en) | 1985-06-17 |
| JPH0361926B2 true JPH0361926B2 (en) | 1991-09-24 |
Family
ID=16726917
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP21889183A Granted JPS60111205A (en) | 1983-11-21 | 1983-11-21 | Fiber fusion connecting method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60111205A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60195504A (en) * | 1984-03-17 | 1985-10-04 | Fujikura Ltd | Welding and connecting device of single mode fiber |
| JP4457873B2 (en) | 2004-11-30 | 2010-04-28 | 住友電気工業株式会社 | Optical fiber fusion splicing device and fusion splicing method |
| JP4856506B2 (en) * | 2006-09-14 | 2012-01-18 | 本田技研工業株式会社 | Vehicle seat belt device |
| CN110716264A (en) * | 2019-09-12 | 2020-01-21 | 北京工业大学 | A kind of soft glass optical fiber fusion splicing method |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4557556A (en) * | 1983-10-28 | 1985-12-10 | At&T Bell Laboratories | Method of fabricating an optical attenuator by fusion splicing of optical fibers |
-
1983
- 1983-11-21 JP JP21889183A patent/JPS60111205A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60111205A (en) | 1985-06-17 |
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