JPS63168606A - Splicing method for optical fiber - Google Patents

Splicing method for optical fiber

Info

Publication number
JPS63168606A
JPS63168606A JP17887A JP17887A JPS63168606A JP S63168606 A JPS63168606 A JP S63168606A JP 17887 A JP17887 A JP 17887A JP 17887 A JP17887 A JP 17887A JP S63168606 A JPS63168606 A JP S63168606A
Authority
JP
Japan
Prior art keywords
optical fiber
optical fibers
splicing
amount
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
Application number
JP17887A
Other languages
Japanese (ja)
Inventor
Tadashi Haibara
灰原 正
Noboru Kawasaki
登 川崎
Mitsuru Miyauchi
宮内 充
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.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone Corp
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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP17887A priority Critical patent/JPS63168606A/en
Publication of JPS63168606A publication Critical patent/JPS63168606A/en
Pending legal-status Critical Current

Links

Landscapes

  • Mechanical Coupling Of Light Guides (AREA)

Abstract

PURPOSE:To obtain a splicing part of small loss by setting the extent of forcing-in of optical fibers to <=10mum in the case of fusion-splicing between optical fibers of less eccentricity. CONSTITUTION:Single mode optical fibers are put along V grooves to face each other and are forced in and spliced while heated and fused by discharge heating. In this method, the extent of forcing-in for splicing is set to <=10mum when the extent of eccentricity of optical fiber cores of optical fibers is <=0.5%. Thus, fixing V grooves are used and only clads are aligned to splice optical fibers with a small loss of about 0.01dB average, and therefore, the quality of an optical fiber communication line is improved and the splicing device is simplified.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、単一モード光ファイバを低損失で接続する方
法に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a method for splicing single mode optical fibers with low loss.

(従来の技術) 従来、単一モード光ファイバを融着接続するに際しては
、第2図の当該光ファイバの断面図に示すように、コア
1の中心2が、クラッド3の中心4からε=δ/R=2
%程度ずれていたので、第3図に示すように、X方向、
Y方向およびこれらに直角なZ方向に可動の■溝5.5
′に光ファイバ6.6′を沿わせた後、V溝5,5′を
移動してコア1,1′相互を軸合わせした後、放電電極
7.7′の放電8によって当該光ファイバ6.6′を加
熱し、光ファイバを突き当てて、さらに押し込んで融着
接続を行っていた。
(Prior Art) Conventionally, when fusion splicing a single mode optical fiber, the center 2 of the core 1 is separated from the center 4 of the cladding 3 by ε= δ/R=2
%, so as shown in Figure 3, the X direction,
■Groove 5.5 movable in the Y direction and the Z direction perpendicular to these
After aligning the optical fiber 6.6' along the V-grooves 5, 5' and aligning the cores 1, 1' with each other, the optical fiber 6. .6' was heated, the optical fiber was butted against it, and the fiber was further pushed in to perform fusion splicing.

このとき、第4図に当該光ファイバの押し込み量と接続
損失の関係を示すように、押し込み量は20μm程度が
最良とされていた(Y−Kato et、al。
At this time, as shown in FIG. 4, which shows the relationship between the amount of push-in of the optical fiber and the connection loss, it was thought that the best push-in amount was about 20 μm (Y-Kato et al.

”Arc−fusion splicing of s
ingle−mode fibers 1: Opti
mum 5plice conditions” Ap
pl、 Opt、 21pp、 1332−1336.
1982)。
”Arc-fusion splicing of s
ingle-mode fibers 1: Opti
mum 5price conditions” Ap
pl, Opt, 21pp, 1332-1336.
1982).

このように偏心率の大きな場合、光ファイバの押し込み
量の大小によって接続損失が変動する理由としては、融
着接続時のコアの変形が考えられる。第5図に光ファイ
バの押し込み量を変化させた場合のコアの変形の様子を
示す。第5図(a)は偏心が2%の光ファイバの融着接
続時に光ファイバの端面が接触した直後のコア1.1′
およびクラッド3.3′の状態を示すが、コア1,1′
相互は直線的に接続されている。しかし光ファイバの押
し込み量が小さな場合には、表面張力によって、クラッ
ド3,3′の外径が合致するので、第5図(b)に示す
ようにコアの先端が極度に変形し、接続損失が増加する
。一方、光ファイバの押し込み量が大きな場合には、表
面張力の影響は小さいが、第5図(c)に示すようにコ
アが波形に変形して接続損失が増加する。従って、光フ
ァイバの押し込み量を適切に選ぶ必要があった。
In the case of such a large eccentricity, deformation of the core during fusion splicing is considered to be the reason why the splice loss varies depending on the amount of pushing of the optical fiber. FIG. 5 shows how the core deforms when the amount of push of the optical fiber is changed. Figure 5(a) shows the core 1.1' immediately after the end surfaces of the optical fibers come into contact during fusion splicing of optical fibers with eccentricity of 2%.
and cladding 3.3', but core 1,1'
They are connected to each other in a straight line. However, when the optical fiber is pushed in only a small amount, the outer diameters of the claddings 3 and 3' match due to surface tension, resulting in extreme deformation of the tip of the core as shown in Figure 5(b), resulting in splice loss. increases. On the other hand, when the optical fiber is pushed in by a large amount, the influence of surface tension is small, but the core is deformed into a waveform as shown in FIG. 5(c), and the splice loss increases. Therefore, it was necessary to appropriately select the amount of push-in of the optical fiber.

このように、偏心の大きな光ファイバも接続可能とする
ためには、光ファイバ軸合わせ用の■溝もx、y、z方
向に可動式とせねばならず、装置化にあたって機構が複
雑化するという欠点を有するとともに、この光ファイバ
の押し込み量の範囲では、接続損失を0.07dB程度
にすることしかできないという欠点があった。
In order to be able to connect optical fibers with large eccentricities, the grooves for aligning the optical fiber axes must also be movable in the x, y, and z directions, which complicates the mechanism when building equipment. Another disadvantage is that within the range of the amount of pushing of the optical fiber, the splice loss can only be reduced to about 0.07 dB.

また従来の技術においては、偏心の小さな光ファイバは
、製造技術上、困難であったので、偏心の大きな光ファ
イバを接続することを念頭に置き、光ファイバの押し込
み量を一率20μm程度に決めていた。したがって、偏
心の小さな光ファイバもやむなく過大に押し込んでしま
い、接続損失を大きくしていまうという欠点があった。
In addition, with conventional technology, it was difficult to manufacture optical fibers with small eccentricities, so keeping in mind the connection of optical fibers with large eccentricities, the amount of push-in of the optical fibers was determined at a rate of about 20 μm. was. Therefore, even optical fibers with small eccentricities are unavoidably pushed in excessively, resulting in an increase in connection loss.

したがって、従来技術によっては、光ファイバ通信線路
の構築上、中継距離がある程度制限されるという欠点が
あった。
Therefore, depending on the conventional technology, there has been a drawback that the relay distance is limited to some extent due to the construction of the optical fiber communication line.

(発明が解決しようとする問題点) 本発明は、偏心量の小さな単一モード光ファイバを低損
失に接続するための最適な光ファイバの押し込み量を明
かにし、極めて低損失な接続部を実現するための光ファ
イバ接続方法を提供することにある。
(Problems to be Solved by the Invention) The present invention clarifies the optimal optical fiber push amount to connect single-mode optical fibers with small eccentricity with low loss, and realizes extremely low-loss connections. The object of the present invention is to provide an optical fiber connection method for

(問題点を解決するための手段) 本発明は、偏心量0.5%以下の単一モード光ファイバ
をその外径の軸合わせのみで、コアの軸合わせを積極的
に行わないで融着接続するに際し、接続すべき1対の光
ファイバ相互の端面同志が突き当たった後、当該光ファ
イバの押し込み量を10μm以下とする。
(Means for Solving the Problems) The present invention fuses a single mode optical fiber with an eccentricity of 0.5% or less by aligning its outer diameter only, without actively aligning its core. When connecting, after the end surfaces of a pair of optical fibers to be connected abut each other, the amount of pushing of the optical fibers is set to 10 μm or less.

従来の光ファイバの接続方法では、光ファイバの押し込
み量の設定値を20μmとしていた点が異なる。
The difference is that in the conventional optical fiber connection method, the set value for the amount of pushing of the optical fiber is 20 μm.

(実施例) 第1図は本発明の詳細な説明する図であって、偏心の小
さな(ε=0.5%)光ファイバの押し込み量と接続損
失の関係を示す実験データである。
(Example) FIG. 1 is a diagram for explaining the present invention in detail, and shows experimental data showing the relationship between the pushing amount and splicing loss of an optical fiber with small eccentricity (ε=0.5%).

なお、このデータは単一モード光ファイバを固定のV溝
に沿わせて、コアの調心をすることなく接続したもので
ある。第1図に示すように、光ファイバの押し込み量を
10μm以下とすることで接続損失を平均0.01dB
程度にすることができ、従来の光ファイバ融着接続方法
による接続損失0.07dBの177にすることが可能
となる。これは偏心の小さな(例えばε=0.5%)光
ファイバでは、第1図に示すように、光ファイバの押し
込み量が小さくても、表面張力によるコアの変形が少な
いので、接続損失を小さくすることが可能であるからで
ある。
Note that this data is based on a single mode optical fiber connected along a fixed V-groove without aligning the core. As shown in Figure 1, by setting the optical fiber push depth to 10 μm or less, the splice loss can be reduced to 0.01 dB on average.
It is possible to reduce the splice loss to 177, which is 0.07 dB by the conventional optical fiber fusion splicing method. For optical fibers with small eccentricity (epsilon = 0.5%, for example), as shown in Figure 1, even if the optical fiber is pushed in a small amount, the core deformation due to surface tension is small, so the splice loss can be reduced. This is because it is possible to do so.

したがって、光ファイバ通信線路構築上の制限がほとん
どなくなり、大幅な中継距離の増大が可能となる。
Therefore, there are almost no restrictions on the construction of optical fiber communication lines, and it becomes possible to significantly increase the relay distance.

また、従来の光ファイバ融着接続方法による可動V溝を
使用せずとも、前述のような低損失接続が可能であるの
で、装置構成も単純になるという利点もある。
Furthermore, since the above-described low-loss splicing is possible without using the movable V-groove of the conventional optical fiber fusion splicing method, there is also the advantage that the device configuration is simple.

以上説明したように、本発明の光ファイバ接続方法によ
れば、偏心の小さな光ファイバ(ε=0.5%以下)を
融着接続する際に、当該光ファイバの押し込み量を10
μm以下とすることで、可動V溝を使用してコアの軸合
わせをすることなく、固定V溝を使用して、クラッドの
軸合わせのみでも平均0.01dB程度の低損失接続が
可能となるので、光ファイバ通信線路の品質向上と接続
装置の簡易化を達成できる利点がある。
As explained above, according to the optical fiber splicing method of the present invention, when fusion splicing optical fibers with small eccentricity (ε=0.5% or less), the pushing amount of the optical fibers is reduced to 10
By setting the diameter to less than μm, it is possible to achieve a low-loss connection of about 0.01 dB on average by using a fixed V-groove and aligning the cladding without aligning the core using a movable V-groove. Therefore, there are advantages in that the quality of the optical fiber communication line can be improved and the connection device can be simplified.

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

第1図は本発明の詳細な説明するだめの光ファイバの押
し込み量と接続損失の関係を示す図、第2図はコアの偏
心を示す概略図、第3図は従来の光ファイバ融着接続方
法の説明図、笛鳴図は従来の光ファイバ融着接続方法に
よる光ファイバの押し込み量と接続損失の関係を示す図
、第5図(a)。 (b)、 (C1は従来の光ファイバ融着接続時に光フ
ァイバの押し込み量を変化させた場合のコアの変形の様
子を示す図である。 1.1′・・・コア    2・・・コアの中心3.3
′クラツド   4・・・クラッドの中心5.5′・・
・可動V溝  6,6′・・・光ファイバ7.7′・・
・放電電極  8・・・放電特許出願人   日本電信
電話株式会社第1図 f7pイバ°の押り込〃ス(メ慴) 第2図 第3図 紅 打 美
Fig. 1 is a diagram showing the relationship between the pushing amount of the optical fiber and the splicing loss for detailed explanation of the present invention, Fig. 2 is a schematic diagram showing the eccentricity of the core, and Fig. 3 is a diagram of the conventional optical fiber fusion splicing. Fig. 5(a) is an explanatory diagram of the method, and a whistle diagram is a diagram showing the relationship between the amount of pushing of the optical fiber and the splicing loss in the conventional optical fiber fusion splicing method. (B), (C1 is a diagram showing how the core deforms when the amount of pushing of the optical fiber is changed during conventional optical fiber fusion splicing. 1.1'...Core 2...Core center of 3.3
'Clad 4...Center of clad 5.5'...
・Movable V groove 6,6'...Optical fiber 7.7'...
・Discharge electrode 8... Discharge patent applicant Nippon Telegraph and Telephone Corporation Fig. 1 F7P lever push-in location (method) Fig. 2 Fig. 3 Beniuchi

Claims (1)

【特許請求の範囲】[Claims] 1、単一モード光ファイバをV溝に沿わせて互いに対向
させ、放電加熱によって該光ファイバ相互を加熱溶融さ
せるとともに、互いに押し込み接続する方法において、
当該光ファイバコアの偏心量が0.5%以下の光ファイ
バに対して、接続時の押し込み量を10μm以下とする
ことを特徴とする光ファイバ接続方法。
1. A method in which single mode optical fibers are placed facing each other along a V-groove, the optical fibers are heated and melted by discharge heating, and the optical fibers are pressed and connected to each other,
An optical fiber connecting method, characterized in that for an optical fiber whose optical fiber core has an eccentricity of 0.5% or less, the pushing amount at the time of connection is 10 μm or less.
JP17887A 1987-01-06 1987-01-06 Splicing method for optical fiber Pending JPS63168606A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17887A JPS63168606A (en) 1987-01-06 1987-01-06 Splicing method for optical fiber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17887A JPS63168606A (en) 1987-01-06 1987-01-06 Splicing method for optical fiber

Publications (1)

Publication Number Publication Date
JPS63168606A true JPS63168606A (en) 1988-07-12

Family

ID=11466752

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17887A Pending JPS63168606A (en) 1987-01-06 1987-01-06 Splicing method for optical fiber

Country Status (1)

Country Link
JP (1) JPS63168606A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008003170A (en) * 2006-06-20 2008-01-10 Fujikura Ltd Method and apparatus for fusion splicing optical fiber

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008003170A (en) * 2006-06-20 2008-01-10 Fujikura Ltd Method and apparatus for fusion splicing optical fiber
JP4610524B2 (en) * 2006-06-20 2011-01-12 株式会社フジクラ Optical fiber fusion splicing method and apparatus

Similar Documents

Publication Publication Date Title
US6321006B2 (en) Optical fiber having an expanded mode field diameter and method of expanding the mode field diameter of an optical fiber
EP0144136B1 (en) Method for fabricating an optical attenuator by fusion splicing of optical fibres
EP0207980B1 (en) Fiber-lens optical coupler
JP3615735B2 (en) Manufacture of collimators using optical fibers welded and connected to optical elements of considerable cross section
US5588087A (en) Overlapping fusion attenuator
JPH03504052A (en) Optical waveguide connection
JP3158105B2 (en) Manufacturing method of core diffused optical fiber
JPS60243605A (en) Attenuator for optical fiber and manufacture thereof
JPH03100603A (en) Method of manufacturing fused optical fiber coupler
JPH01169408A (en) Inspecting method for optical fiber connecting part
JP2005284150A (en) Method of manufacturing core-expanded optical fiber, optical fiber, and optical connector
US20030108307A1 (en) Optical attenuator employing a fusion splice
EP0487151B1 (en) Low-reflection termination of an optical fibre
JPS63168606A (en) Splicing method for optical fiber
JP2619130B2 (en) Single Mode Optical Fiber Interconnection Method
JPS62184403A (en) Fusion splicing method for optical fiber
JPS6240685B2 (en)
JP3095511B2 (en) Polarization-maintaining optical fiber coupler
JP3344061B2 (en) Optical fiber fusion splicing method
JP2584651B2 (en) Optical fiber fusion splicing method
JPH0498206A (en) Optical fiber terminal optical connector
JPS63304209A (en) Method for branching and joining optical fiber circuit and branching and joining connector
JP2805533B2 (en) Fiber fusion type optical branch coupler
JPH0659150A (en) Connection structure of optical fiber
JPH01295208A (en) Optical fiber mode matching device