JPS6212885B2 - - Google Patents
Info
- Publication number
- JPS6212885B2 JPS6212885B2 JP8223982A JP8223982A JPS6212885B2 JP S6212885 B2 JPS6212885 B2 JP S6212885B2 JP 8223982 A JP8223982 A JP 8223982A JP 8223982 A JP8223982 A JP 8223982A JP S6212885 B2 JPS6212885 B2 JP S6212885B2
- Authority
- JP
- Japan
- Prior art keywords
- optical fiber
- light
- connection
- optical
- measuring
- 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
Links
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
- G01M11/35—Testing of optical devices, constituted by fibre optics or optical waveguides in which light is transversely coupled into or out of the fibre or waveguide, e.g. using integrating spheres
-
- 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
- G02B6/26—Optical coupling means
-
- 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
- G02B6/36—Mechanical coupling means
- G02B6/38—Mechanical coupling means having fibre to fibre mating means
- G02B6/3801—Permanent connections, i.e. wherein fibres are kept aligned by mechanical means
- G02B6/3803—Adjustment or alignment devices for alignment prior to splicing
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Mechanical Coupling Of Light Guides (AREA)
Description
【発明の詳細な説明】
この発明は例えば光通信網における電柱上やマ
ンホール内で使用することを可能とする光フアイ
バ接続損失の測定方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring optical fiber connection loss that can be used, for example, on utility poles or in manholes in optical communication networks.
光フアイバケーブルを使用する光通信が実用に
供されるに従い、布設された光フアイバケーブル
内の光フアイバをマンホール内や電柱上で接続す
る必要が多数生じている。このような接続工事に
おいて、接続損失を測定しながら接続を行なうの
が通常の方法である。従来、このために第1図に
示すような構成をとつていた。即ち光源1と、接
続すべき光フアイバ2A,2Bと、受光器3とを
用いる。通常光源の設置場所イと光フアイバの接
続場所ロと受光器3の設置場所ハとは異なり、こ
れらは数100m以上離れるのが常である。近年光
フアイバケーブルの細径軽量性を生かして、ケー
ブルの布設単長が伸びるに従い、これら場所イ,
ロ,ハ間の距離は長くなる傾向にある。
As optical communication using optical fiber cables is put into practical use, there is a growing need to connect optical fibers in installed optical fiber cables in manholes or on utility poles. In such connection work, the usual method is to perform the connection while measuring the connection loss. Conventionally, for this purpose, a configuration as shown in FIG. 1 has been adopted. That is, a light source 1, optical fibers 2A and 2B to be connected, and a light receiver 3 are used. Unlike the installation location (a) of the light source, the connection location (b) of the optical fiber, and the installation location (c) of the light receiver 3, these locations are usually separated by several hundred meters or more. In recent years, taking advantage of the small diameter and light weight of optical fiber cables, as the length of cable installation has increased, these locations have become more and more
The distance between b and c tends to be longer.
このような構成で接続損失を測定するには従来
においては、まず第2図aに示すように光源1か
らの光を光フアイバ2Aに通し、接続場所ロで光
フアイバ2Aより出射される光パワーQ1
(dBm)を受光器3により測定する。次に第2図
bに示すように接続場所ロで、光フアイバ2A,
2Bを接続したのち、場所ハで光フアイバ2Bか
ら出射される光パワーQ2(dBm)を測定する。
こゝで光フアイバ2Bの単位長当りの損失αB
(dB/Km)が予め測定されてあり、かつ光フアイ
バ2Bの長さl(m)が知られている。この時の
接続損失は
Q1−Q2−αB・l/1000 (dB)
で求まる。 Conventionally, to measure splice loss with such a configuration, first, as shown in Figure 2a, the light from light source 1 is passed through optical fiber 2A, and the optical power emitted from optical fiber 2A at the splicing location B is measured. Q1
(dBm) is measured by the optical receiver 3. Next, as shown in FIG. 2b, at the connection location RO, the optical fiber 2A,
After connecting optical fiber 2B, the optical power Q 2 (dBm) emitted from optical fiber 2B is measured at location C.
Here, the loss per unit length of optical fiber 2B α B
(dB/Km) has been measured in advance, and the length l (m) of the optical fiber 2B is known. The connection loss at this time is found as Q 1 −Q 2 −α B ·l/1000 (dB).
以上説明したように、従来法で接続損失を測定
するには、光源の設置場所イと、接続場所ロと、
受光器の設置場所ハとが互に遠く離れていた。こ
のため、工事に従事する要員が多くかかり、工事
費の上昇をまねくという欠点がある。また、交通
量の多い場所等では同時にイ,ロ,ハの3ケ所を
専有することが困難であり、工事の施行が困難で
あるという欠点もある。また、この従来の方法で
は光フアイバ2Aの損失を測定しなければならな
かつた。 As explained above, in order to measure splice loss using the conventional method, the light source installation location A, the connection location B,
The photoreceiver installation locations C and C were far apart from each other. For this reason, there is a drawback that a large number of personnel are required to work on the construction, leading to an increase in construction costs. Another disadvantage is that it is difficult to monopolize three locations (A, B, and C) at the same time in areas with heavy traffic, making it difficult to carry out construction work. Furthermore, in this conventional method, it was necessary to measure the loss of the optical fiber 2A.
この発明は光フアイバを曲げ、その曲げ部分に
光を照射することによりその光フアイバ内に光を
入射させ、仮接続工程と本接続工程とを行ない、
これら2回の接続工程における光フアイバ接続部
からのもれ光パワーを測定することを特徴とし、
その目的は接続する場所で光フアイバの接続損失
を測定することを可能とし、これに伴い接続工事
費の低減、簡便な接続工事方法の低減を可能とし
ようとするものである。
This invention bends an optical fiber, irradiates the bent portion with light to allow light to enter the optical fiber, and performs a temporary connection process and a main connection process,
It is characterized by measuring the leakage optical power from the optical fiber connection part in these two connection steps,
The purpose is to make it possible to measure the splice loss of optical fibers at the location where they are connected, thereby reducing the cost of splicing and simplifying the method of splicing.
第3図にこの発明の測定方法の構成を示す。こ
の発明においては接続場所ロに光源1が設けら
れ、またこの場所ロに受光器3が用意される。
FIG. 3 shows the configuration of the measuring method of the present invention. In this invention, a light source 1 is provided at a connection location RO, and a light receiver 3 is provided at this location RO.
この発明による接続損失の測定法においては第
4図aに示すように、光フアイバ2Aを曲げ治具
により曲げ、その曲げ部2Aaに光源1からの光
を照射することで、光フアイバ2Aに光を入射さ
せる。曲げ部2Aaは接続場所ロで形成され、光
フアイバ2Aの接続端から、数m程度離れた個所
とされる。この長さは接続場所の環境により、あ
まり長くできない状況も起きるが、できれば2m
以上が好ましい。また、この曲げ部2Aaは以下
の工程中において固定して光源1と光フアイバ2
Aとの結合効率が変化しないようにする。光源1
として半導体レーザや気体レーザ、白色ランプ、
キセノンランプ等が考えられ、連続光でもパルス
状発光でもよい。 In the method for measuring splice loss according to the present invention, as shown in FIG. is incident. The bent portion 2Aa is formed at the connection location B, and is located several meters away from the connection end of the optical fiber 2A. This length may not be very long depending on the environment of the connection location, but if possible it is 2m.
The above is preferable. In addition, this bent portion 2Aa is fixed during the following steps to connect the light source 1 and the optical fiber 2.
The coupling efficiency with A should not change. light source 1
As semiconductor lasers, gas lasers, white lamps,
A xenon lamp or the like may be used, and continuous light or pulsed light may be used.
光源1と光フアイバ2Aとの結合効率は、光フ
アイバ2Aが複覆されていると非常に小さくな
る。光フアイバ2Aに色づけ被覆がなされている
と、さらに結合効率は小さくなる。被覆光フアイ
バをその許容曲げ半径内で曲げて実験した結果、
−40dB程度の結合が可能であつた。この値は光
源1と曲げ部2Aaとの幾何学形状や、被覆材
料、被覆の色等に依存するが、この程度の結合が
期待できる。 The coupling efficiency between the light source 1 and the optical fiber 2A becomes extremely small when the optical fiber 2A is doubled over. If the optical fiber 2A is coated with a colored coating, the coupling efficiency will be further reduced. As a result of an experiment by bending a coated optical fiber within its allowable bending radius,
Coupling of about -40dB was possible. Although this value depends on the geometric shape of the light source 1 and the bent portion 2Aa, the coating material, the coating color, etc., this level of coupling can be expected.
光フアイバ2Aの接続端からの光出力P1を受光
器3で測定する。 The optical receiver 3 measures the optical output P 1 from the connecting end of the optical fiber 2A.
その後、第4図bに示すように光フアイバ2A
と2Bを仮接続し(仮接続工程)、その仮接続部
からのもれ光のパワーP2を測定する。この測定を
正しく行うには例えば光フアイバの軸にそつて受
光器3を動かすことにより測定する。第4図a,
bでの各測定に用いる受光器3は同一のもので
も、異なるものでも良い。第4図bに受光器3を
動かす方向を矢印A−A′で示す。 After that, as shown in FIG. 4b, the optical fiber 2A is
and 2B (temporary connection process), and measure the power P2 of the light leaking from the temporary connection. This measurement can be carried out correctly, for example, by moving the receiver 3 along the axis of the optical fiber. Figure 4a,
The light receivers 3 used for each measurement in b may be the same or different. In FIG. 4b, the direction in which the light receiver 3 is moved is indicated by an arrow A-A'.
次に第4図cに示すように、光フアイバ2Bを
仮接続部に近い所で短尺BSと長尺BLとに切断す
る。図では仮接続部からαmのところで光フアイ
バ2Bを切断しているが、このαは1〜2m程度
である。この切断後、上記仮接続状態で短尺の光
フアイバBSの端面より出射される光パワー出力
P3を測定する。光フアイバ2Bが当初lmであれ
ば、この切断により本接続される長尺の光フアイ
バBLは(l−α)mとなる。 Next, as shown in FIG. 4c, the optical fiber 2B is cut into a short length BS and a long length BL near the temporary connection part. In the figure, the optical fiber 2B is cut at a distance αm from the temporary connection, but this α is about 1 to 2 m. After this disconnection, the optical power output is emitted from the end face of the short optical fiber BS in the above temporarily connected state.
Measure P3 . If the optical fiber 2B is initially lm, the length of the long optical fiber BL to be finally connected by this cutting becomes (l-α)m.
P3の測定後、第4図dに示すように仮接続した
所を切断し、光フアイバ2Aと、(l−α)mと
なつた光フアイバ2B、つまり長尺の光フアイバ
BLとを再び接続する(本接続工程)。その後、第
4図eに示すように接続部からのもれ光のパワー
P4を、第4図bに示した方法と同一の方法により
測定する。 After measuring P 3 , as shown in Fig. 4d, the temporary connection is cut, and the optical fiber 2A and the optical fiber 2B (l-α)m, that is, the long optical fiber
Connect to BL again (main connection process). After that, as shown in Figure 4e, the power of the leaking light from the connection part is
P 4 is measured by the same method as shown in Figure 4b.
以上の作業により、本接続の接続損失Lを次の
ようにして求める。 Through the above operations, the connection loss L of this connection is determined as follows.
L=−10 log10(1−KP4/P1) (dB)(1)
である。Kは受光器3と光フアイバ2A,2Bと
の距離等に依存する値である。仮接続の接続損失
L′は
L′=−10 log10K(1−KP2/P1) (dB) (2)
ともとまるが、L′はまた
L′=−10 log10(P3/P1) (dB) (3)
と表わされる。式(2)と式(3)からKをもとめ、式(1)
に代入することで、Lは次式となる。L=-10 log 10 (1-KP 4 /P 1 ) (dB) (1). K is a value that depends on the distance between the light receiver 3 and the optical fibers 2A, 2B, etc. Connection loss of temporary connection
L' is also L'=-10 log 10 K(1-KP 2 /P 1 ) (dB) (2), but L' is also L'=-10 log 10 (P 3 /P 1 ) (dB ) (3). Find K from equations (2) and (3), and use equation (1)
By substituting into , L becomes the following formula.
L=−10 log〔1−(P1−P3)P4/P1P2〕
(dB)(4)
なお、光源1と光フアイバ2Aとの結合効率を
上げるため、第5図、第6図に示す方法が考えら
れる。第3図、第4図では曲げ部2Aaは半回の
曲げであるが、第5図に示すようにn回の波状曲
げ及び第6図に示すようにn回のコイル状曲げが
考えられる。第5図はn=3の波状曲げ、第6図
はn=2のコイル状曲げである。L=-10 log [1-( P1 - P3 ) P4 / P1P2 ]
(dB) (4) In order to increase the coupling efficiency between the light source 1 and the optical fiber 2A, the methods shown in FIGS. 5 and 6 can be considered. In FIGS. 3 and 4, the bent portion 2Aa is bent half a time, but as shown in FIG. 5, n times of wavy bending and as shown in FIG. 6, n times of coiled bending are possible. FIG. 5 shows wavy bending with n=3, and FIG. 6 shows coiled bending with n=2.
また、接続部からのもれ光を受光器3で測定す
る方法として、第4図に示すようにA−A′方向
に受光器3を移動させる他に、第7図に示すよう
に光フアイバ2A,2Bを軸とするらせんに沿つ
たB−B′方向に受光器3を移動させることも可能
である。或は第12図に示すように接続部の近傍
において光フアイバ2A,2Bに沿つて複数の受
光器3を配列し、これら受光器3の出力を加算し
てもよい。更にこれら受光器3の配列を第13図
に示すように光フアイバの周面において複数列設
け、これらのすべて受光器の出力を加算してもよ
い。 In addition, as a method for measuring the leakage light from the connection part with the optical receiver 3, in addition to moving the optical receiver 3 in the A-A' direction as shown in FIG. It is also possible to move the light receiver 3 in the BB' direction along a spiral with 2A and 2B as axes. Alternatively, as shown in FIG. 12, a plurality of light receivers 3 may be arranged along the optical fibers 2A, 2B near the connection portion, and the outputs of these light receivers 3 may be added. Furthermore, as shown in FIG. 13, these light receivers 3 may be arranged in a plurality of rows on the circumferential surface of the optical fiber, and the outputs of all these light receivers may be added.
また、この発明の方法にもとずく、接続損失測
定装置は、曲げ治具と、受光器と、必要に応じて
受光器を光フアイバの軸にそつて移動させる機構
とからなる。曲げ治具は、例えば第8図に示すよ
うに円柱4の周面に周方向に沿つて光フアイバ2
Aをそわせるものである。第6図に示したコイル
状曲げにするには、例えば円柱4の回りに光フア
イバ2Aを巻きつけることで可能である。また、
第5図に示した波状曲げとするには、第9図に示
すように等間隔で平行に配された複数の円柱4A
〜4Eに対し、その円柱4を順次ジグザグに光フ
アイバ2Aを通すと供にその円柱の周面にそわせ
る。または第10図に示すように平行に配された
半円柱状突起5A〜5Dのある板6に光フアイバ
2Aを押しつけることで波状曲げが可能となる。
受光器3を光フアイバの軸にそつて移動させる機
構は、受光器をモータ等で移動させれば実現でき
る。 Further, a splice loss measuring device based on the method of the present invention includes a bending jig, a light receiver, and a mechanism for moving the light receiver along the axis of the optical fiber as necessary. For example, as shown in FIG.
This is to make A move away. The coiled bending shown in FIG. 6 can be achieved, for example, by winding the optical fiber 2A around the cylinder 4. Also,
In order to achieve the wavy bending shown in FIG. 5, a plurality of cylinders 4A are arranged in parallel at equal intervals as shown in FIG.
4E, the optical fiber 2A is sequentially passed through the cylinder 4 in a zigzag manner and aligned with the circumferential surface of the cylinder. Alternatively, as shown in FIG. 10, by pressing the optical fiber 2A against a plate 6 having semi-cylindrical protrusions 5A to 5D arranged in parallel, it is possible to bend the optical fiber 2A in a wavy manner.
The mechanism for moving the light receiver 3 along the axis of the optical fiber can be realized by moving the light receiver with a motor or the like.
以上の説明では単心光フアイバを例にとつた。
しかし、第11図に示すような複数心の光フアイ
バでも、曲げ部で入射する光の波長をそれぞれ変
え、各々の光フアイバに異なる波長の光を入射さ
せ、受光部でフイルターにより分離させることで
接続損失の同時測定が可能である。なお第11図
の7は被覆である。光パワーP1,P2,P3の測定は
前記の順に限らない。例えば光パワーP3を測定
後、光フアイバー2Aと光フアイバBSとを切離
した時に光パワーP1を測定してもよい、また光パ
ワ−P3を測定後、光パワーP2を測定してよい。 In the above explanation, a single optical fiber was used as an example.
However, even with a multi-core optical fiber as shown in Figure 11, it is possible to change the wavelength of the incident light at each bent part, to make light of different wavelengths enter each optical fiber, and to separate them using a filter at the light receiving part. Simultaneous measurement of splice loss is possible. Note that 7 in FIG. 11 is a coating. The measurement of the optical powers P 1 , P 2 , and P 3 is not limited to the above order. For example, after measuring the optical power P3 , the optical power P1 may be measured when the optical fiber 2A and the optical fiber BS are separated, or after measuring the optical power P3 , the optical power P2 may be measured. good.
以上説明したように、この発明の方法は光フア
イバを曲げ、その曲げ部分に光を照射することで
光フアイバ内に光を入射させ、仮接続工程を行つ
た後、一方の光フアイバを仮接続点より短尺と長
尺とに切断し、その後、その短尺のものを離し、
長尺のものを本接続する2回の接続を行い、それ
ぞれにおける光フアイバ接続部からのもれ、及び
仮接続状態での短尺のものの端面からの光パワー
を測定するものであるから、接続する場所で光フ
アイバの接続損失を測定することができ、工事に
必要な要員数の減少、接続損失を算出するための
連絡の不要等の利点があり、工事費の著しい低下
し、工事作業の著しい簡素化が図れる。
As explained above, the method of the present invention involves bending an optical fiber, irradiating the bent portion with light to allow light to enter the optical fiber, performing a temporary connection process, and then temporarily connecting one optical fiber. Cut it into short pieces and long pieces from the point, then separate the short pieces,
The purpose is to make two connections, including the final connection of a long item, and measure the leakage from the optical fiber connection at each time, as well as the optical power from the end face of the short item in the tentatively connected state. Optical fiber splice loss can be measured on-site, which has the advantage of reducing the number of personnel required for construction and eliminating the need for communication to calculate splice loss, resulting in a significant reduction in construction costs and a significant reduction in construction work. It can be simplified.
第1図は従来の接続損失測定のための構成図、
第2図は従来の接続損失測定法の測定順を示す
図、第3図はこの発明の接続損失測定法のための
構成図、第4図はこの発明の接続損失測定法の測
定順を示す図、第5図及び第6図はそれぞれ光フ
アイバの曲げ部の他の例を示す斜視図、第7図は
もれ光の測定における受光器の移動方向の他の例
を示す図、第8図乃至第10図はそれぞれ光フア
イバの曲げ治具の例を示す斜視図、第11図は複
数心の光フアイバ心線を示す斜視図、第12図は
フアイバ接続部からのもれ光を測定する他の例を
示す図、第13図は第12図の変形例を示す図で
ある。
1:光源、2:光フアイバ、3:受光器、4:
円柱、6:突起板、7:被覆。
Figure 1 is a configuration diagram for conventional connection loss measurement.
Figure 2 is a diagram showing the measurement order of the conventional splice loss measurement method, Figure 3 is a block diagram for the splice loss measurement method of the present invention, and Figure 4 is a diagram showing the measurement order of the splice loss measurement method of the present invention. 5 and 6 are respectively perspective views showing other examples of the bent portion of the optical fiber, FIG. 7 is a view showing other examples of the moving direction of the light receiver in measuring leakage light, and FIG. Figures 10 to 10 are perspective views showing an example of an optical fiber bending jig, Figure 11 is a perspective view showing a multi-core optical fiber, and Figure 12 is a measurement of leakage light from the fiber connection. FIG. 13 is a diagram showing a modification of FIG. 12. 1: Light source, 2: Optical fiber, 3: Light receiver, 4:
Cylinder, 6: projection plate, 7: covering.
Claims (1)
げ部に光を照射することにより光フアイバAに光
を入射させ、その光フアイバAの端面より出射す
る光パワーP1を測定する第1工程と、 前記光フアイバAの端面と接続されるべき光フ
アイバBの端面とを仮接続し、その仮接続部から
のもれ光のパワーP2を測定する第2工程と、 その仮接続状態で光フアイバBをその仮接続部
に近い所で短尺BSと長尺BLとの2本に切断し、
短尺の光フアイバBSの端面から出射する光パワ
ーP3を測定する第3工程と、 その後、光フアイバAと短尺光フアイバBSと
の仮接続部を離し、再び光フアイバAと長尺の光
フアイバBLとを本接続し、その本接続部からの
もれ光のパワーP4を測定する第4工程とを備え、
光フアイバAと長尺の光フアイバBLとの接続損
失L(dB)を、 L=−10 log10〔1−(P1−P3)P4/P
1P2〕 の式により算出する光フアイバ接続損失測定方
法。[Claims] 1. By bending the optical fiber A and irradiating the bent portion of the optical fiber A with light, the light enters the optical fiber A, and the optical power P 1 emitted from the end face of the optical fiber A is determined. a first step of measuring; a second step of temporarily connecting the end face of the optical fiber A and the end face of the optical fiber B to be connected, and measuring the power P2 of the light leaking from the temporary joint; In the temporarily connected state, the optical fiber B is cut into two pieces, a short BS and a long BL, near the temporary connection part,
A third step of measuring the optical power P 3 emitted from the end face of the short optical fiber BS, and then separating the temporary connection between the optical fiber A and the short optical fiber BS, and connecting the optical fiber A and the long optical fiber again. A fourth step of making a main connection with the BL and measuring the power P 4 of the leaking light from the main connection part,
The connection loss L (dB) between optical fiber A and long optical fiber BL is L=-10 log 10 [1-(P 1 -P 3 )P 4 /P
1 P 2 ] A method for measuring optical fiber connection loss calculated by the formula:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8223982A JPS58198015A (en) | 1982-05-14 | 1982-05-14 | Method for measuring of connection loss of optical fiber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8223982A JPS58198015A (en) | 1982-05-14 | 1982-05-14 | Method for measuring of connection loss of optical fiber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58198015A JPS58198015A (en) | 1983-11-17 |
| JPS6212885B2 true JPS6212885B2 (en) | 1987-03-23 |
Family
ID=13768856
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8223982A Granted JPS58198015A (en) | 1982-05-14 | 1982-05-14 | Method for measuring of connection loss of optical fiber |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58198015A (en) |
Families Citing this family (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0145343B1 (en) * | 1983-11-18 | 1988-05-18 | Nippon Telegraph And Telephone Corporation | Optical fibre test method and apparatus for performing the method |
| US4743086A (en) * | 1984-12-03 | 1988-05-10 | Polaroid Corporation | Coupling device for forming optically efficient end-to-end optical fiber connections |
| JPS61204535A (en) * | 1984-12-24 | 1986-09-10 | Sumitomo Electric Ind Ltd | Inspecting device for optical fiber |
| CA1273816A (en) * | 1985-05-24 | 1990-09-11 | Masatoshi Kaneshi | Method of the measurement of light from an optical cable and arrangement therefor |
| EP0582831B1 (en) * | 1992-07-30 | 1998-03-18 | Siemens Aktiengesellschaft | Procedure and device for making measurements on optical waveguides |
| DE59307929D1 (en) * | 1992-10-20 | 1998-02-12 | Siemens Ag | Method and device for measurements on several optical fibers |
| JP2007225961A (en) * | 2006-02-24 | 2007-09-06 | Nippon Telegr & Teleph Corp <Ntt> | Optical fiber connection method |
-
1982
- 1982-05-14 JP JP8223982A patent/JPS58198015A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58198015A (en) | 1983-11-17 |
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