JPH037061B2 - - Google Patents
Info
- Publication number
- JPH037061B2 JPH037061B2 JP4637881A JP4637881A JPH037061B2 JP H037061 B2 JPH037061 B2 JP H037061B2 JP 4637881 A JP4637881 A JP 4637881A JP 4637881 A JP4637881 A JP 4637881A JP H037061 B2 JPH037061 B2 JP H037061B2
- Authority
- JP
- Japan
- Prior art keywords
- optical fiber
- measured
- single mode
- optical
- core
- 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
- G01M11/33—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
- Light Guides In General And Applications Therefor (AREA)
Description
【発明の詳細な説明】
本発明は単一モード光フアイバの評価装置に関
する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a single mode optical fiber evaluation device.
従来単一モード光フアイバは特に通信用として
長距離の伝送線に利用されている。この単一モー
ド光フアイバは使用波長と同程度の太さのコア
に、該コアに比し屈折率が稍々小さい被覆材を被
覆したものである。このような単一モード光フア
イバは、その通信品質にかかわる重要特性とし
て、コアの直径、コアと被覆材との屈折率差、単
一モード光フアイバとしての使用限界波長である
シングル・モード・リミツトがあげられる。これ
らの特性は光フアイバ同士の結合、素子との結合
等においてもその結合効率に影響する。従つてこ
れらの特性は使用前に予め評価する必要がある。
この評価方法として従来、コア径及び屈折率差は
フアイバをグリセリン等の液体に浸漬して横から
顕微鏡で測定する方法が用いられている。しかし
実際の光フアイバの断面の屈折率分布は第1図に
示すようにプリフオームの段階での屈折率分布が
曲線Aであるのに対し、フアイバの段階では曲線
Bの如くなつているので、前記顕微鏡での測定は
正確な値を得ることが困難である。またシング
ル・モード・リミツトの測定は、モノクロメータ
を用いて被測定光フアイバの一端より順次波長を
変えて光を入射し、他端に現われるシングル・モ
ード・パターンをテレビジヨンカメラにて観察
し、その輝度分布の変化により測定している。と
ころがこの方法は第2図の曲線No.1〜No.4で示す
如く、被測定光フアイバの長さ(図の横軸に示
す)により測定値(図の縦軸に示す)が変りこれ
も正確な測定が困難である。本発明はこれらの欠
点を除去するために案出されたものである。 Traditionally, single mode optical fibers have been used in long distance transmission lines, particularly for communication purposes. This single mode optical fiber has a core having a thickness comparable to the wavelength used and coated with a coating material whose refractive index is slightly smaller than that of the core. The important characteristics of such a single mode optical fiber that affect its communication quality are the diameter of the core, the difference in refractive index between the core and the coating material, and the single mode limit, which is the limit wavelength for use as a single mode optical fiber. can be given. These characteristics also affect the coupling efficiency in coupling between optical fibers, coupling with elements, and the like. Therefore, these properties must be evaluated before use.
Conventionally, the core diameter and refractive index difference have been evaluated by dipping the fiber in a liquid such as glycerin and measuring it from the side using a microscope. However, as shown in Fig. 1, the refractive index distribution in the cross section of an actual optical fiber is curve A at the preform stage, but curve B at the fiber stage. It is difficult to obtain accurate values when measuring with a microscope. To measure the single mode limit, use a monochromator to sequentially change the wavelength of light from one end of the optical fiber to be measured, and observe the single mode pattern that appears at the other end with a television camera. It is measured by changes in the brightness distribution. However, with this method, as shown by curves No. 1 to No. 4 in Figure 2, the measured value (shown on the vertical axis of the figure) changes depending on the length of the optical fiber to be measured (shown on the horizontal axis of the figure). Accurate measurement is difficult. The present invention has been devised to eliminate these drawbacks.
このため本発明の単一モード光フアイバの評価
装置においては被測定光フアイバを2分し、その
2分した光フアイバのそれぞれの一方の端面同士
をある間隔を設けて対向せしめて接続することが
できる光コネクタと、一方の被測定光フアイバに
切替えて接続される発光波長が異なる2つの光源
と、他方の被測定光フアイバに接続する光パワー
メータとにより構成されたことを特徴とするもの
である。 Therefore, in the single-mode optical fiber evaluation apparatus of the present invention, it is possible to divide the optical fiber to be measured into two and connect the two halves by placing one end face of each of the two halves facing each other with a certain distance between them. The device is characterized in that it consists of an optical connector that can be used, two light sources with different emission wavelengths that are switched and connected to one optical fiber to be measured, and an optical power meter that is connected to the other optical fiber to be measured. be.
以下添付図面に基づいて本発明の実施例につき
詳細に説明する。 Embodiments of the present invention will be described in detail below based on the accompanying drawings.
第3図に実施例の構造図を示す。図において符
号1および2は被測定用の光フアイバ、3は光コ
ネクタ、4は光源、5は光パワーメータである。
そして光コネクタは第4図に示す如く光フアイバ
1および2の対向面にある間隔を与えるため、各
光フアイバを保持している中子6および7の端面
間にリング状のスペーサ8を挿入できるようにな
つている。なお中子6,7はソケツト9の中のア
ダブター10により光フアイバ同士の光軸を一致
させるように案内され、袋ナツト11,11′に
より結合される。また光源4は第3図の如く4a
及び4bの2つの光源を有し、切換機構(図示省
略)により光フアイバ1にそれぞれ単独に光を入
射できるようになつており、2つの光源4a,4
bは出射する光の波長を異にしている。 FIG. 3 shows a structural diagram of the embodiment. In the figure, reference numerals 1 and 2 are optical fibers to be measured, 3 is an optical connector, 4 is a light source, and 5 is an optical power meter.
In order to provide a certain distance between the opposing surfaces of the optical fibers 1 and 2 in the optical connector as shown in FIG. 4, a ring-shaped spacer 8 can be inserted between the end surfaces of the cores 6 and 7 that hold each optical fiber. It's becoming like that. The cores 6 and 7 are guided by an adapter 10 in the socket 9 so that the optical axes of the optical fibers coincide with each other, and are connected by cap nuts 11 and 11'. In addition, the light source 4 is 4a as shown in Figure 3.
It has two light sources 4a and 4b, and is configured so that light can be input independently into the optical fiber 1 by a switching mechanism (not shown).
b has a different wavelength of emitted light.
次にこのように構成された本実施例装置の作用
について説明する。先ず装置に被測定光フアイバ
1および2をセツトしたのち、一方の光源4aに
より光を投射し、パワーメータ5に入力する値
L1を読み取る。次いで光源を4bに切換え、パ
ワーメータ5に入力する値L2を読み取る。 Next, the operation of the apparatus of this embodiment configured as described above will be explained. First, after setting the optical fibers 1 and 2 to be measured in the device, one of the light sources 4a projects light, and the value input to the power meter 5 is calculated.
Read L 1 . Next, the light source is switched to 4b, and the value L2 input to the power meter 5 is read.
一般に単一モード光フアイバを間隔Dに設けて
接続し一方の光フアイバより波長λの光を入射し
たとき他方の光フアイバに現われるパワー損失L
(λ)は、一方の光フアイバより出る光がガウス
分布をしているものと仮定すると次の近似式で示
される。 In general, when single mode optical fibers are connected with a spacing D and light of wavelength λ is input from one optical fiber, the power loss L that appears in the other optical fiber
(λ) is expressed by the following approximate expression, assuming that the light emitted from one optical fiber has a Gaussian distribution.
L(λ)=−10log(4/(4+λD/πW2(λ))2)
……(1)
但しW(λ)はビームウエスト
またビームウエストW(λ)は
W(λ)=A(0.65+1.619/V1.5+2.879/V6)
……(2)
但しAはコアの半径
Vは次式による
V=2πAn0√2/λ ……(3)
但しn0はコアの屈折率
Δ=n0 2−n2/2n0 2
nはクラツドの屈折率
この(2)式と(3)式を(1)式に挿入し、波長λ1、λ2に
おけるパワーメータの測定値L(λ1)、L(λ2)を
与えるとAとΔを計算することができる。L(λ)=−10log(4/(4+λD/πW 2 (λ)) 2 )
...(1) However, W (λ) is the beam waist and the beam waist W (λ) is W (λ) = A (0.65 + 1.619 / V 1.5 + 2.879 / V 6 )
...(2) However, A is the radius of the core and V is according to the following formula: V=2πAn 0 √2/λ ...(3) However, n 0 is the refractive index of the core Δ=n 0 2 −n 2 /2n 0 2 n is the refractive index of the cladding. Inserting equations (2) and (3) into equation (1) and giving the measured values L(λ 1 ) and L(λ 2 ) of the power meter at wavelengths λ 1 and λ 2 , A and Δ can be calculated.
このAとΔを次式のカツトオフ条件の(4)式に入
れるとシングル・モード・リミツトλcが算出され
る。 By inserting A and Δ into the following cutoff condition (4), the single mode limit λ c is calculated.
λc=2πAn√2/2.405≒5.3781A√ ……(4)
第3図に示した実施例装置を用いて第2図に示
した光フアイバを測定し、前記の(4)式により計算
した結果を第2図に○印で示した。N0はそれぞ
れ従来法で測定したものに対応するものである。
(4)式より本実施例装置を用いた場合、測定値は光
フアイバの長さに無関係であることがわかる。λ c =2πAn√2/2.405≒5.3781A√ ...(4) The optical fiber shown in FIG. 2 was measured using the example device shown in FIG. 3, and calculated using the above equation (4). The results are shown in Figure 2 with a circle. N 0 corresponds to those measured by the conventional method.
From equation (4), it can be seen that when the device of this embodiment is used, the measured value is independent of the length of the optical fiber.
以上説明した如く本発明の単一モード光フアイ
バの評価装置は単一モード光フアイバの特性の正
確な測定値を得ることを可能としたものである。 As explained above, the single mode optical fiber evaluation apparatus of the present invention makes it possible to obtain accurate measured values of the characteristics of a single mode optical fiber.
第1図は単一モード光フアイバのコアの屈折率
分布を示した説明図、第2図は従来の測定方法に
よる単一モード光フアイバのシングルモードリミ
ツトの測定値及び本発明による評価装置を用いた
測定値を示した線図、第3図は本発明にかかる実
施例の単一モード光フアイバの評価装置の概略説
明図、第4図はその光コネクタの断面図である。
1,2……光フアイバ、3……光コネクタ、4
……光源、5……パワーメータ、6,7……中
子、8……スペーサ。
Fig. 1 is an explanatory diagram showing the refractive index distribution of the core of a single mode optical fiber, and Fig. 2 shows the measured value of the single mode limit of the single mode optical fiber by the conventional measurement method and the evaluation device according to the present invention. A line diagram showing the measured values used, FIG. 3 is a schematic explanatory diagram of a single mode optical fiber evaluation apparatus according to an embodiment of the present invention, and FIG. 4 is a sectional view of the optical connector. 1, 2...Optical fiber, 3...Optical connector, 4
... light source, 5 ... power meter, 6, 7 ... core, 8 ... spacer.
Claims (1)
フアイバのそれぞれの一方の端面同士をある間隔
を設けて対向せしめて接続することができる光コ
ネクタと、一方の被測定光フアイバに切替えて接
続される発光波長が異なる2つの光源と、他方の
被測定光フアイバに接続する光パワーメータとに
より構成されたことを特徴とする単一モード光フ
アイバの評価装置。1 Divide the optical fiber to be measured into two, and switch to an optical connector that can connect one end face of each of the two halves to face each other with a certain interval, and one optical fiber to be measured. 1. A single mode optical fiber evaluation device comprising two connected light sources having different emission wavelengths and an optical power meter connected to the other optical fiber to be measured.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4637881A JPS57161529A (en) | 1981-03-31 | 1981-03-31 | Evaluating device for single mode optical fiber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4637881A JPS57161529A (en) | 1981-03-31 | 1981-03-31 | Evaluating device for single mode optical fiber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57161529A JPS57161529A (en) | 1982-10-05 |
| JPH037061B2 true JPH037061B2 (en) | 1991-01-31 |
Family
ID=12745474
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4637881A Granted JPS57161529A (en) | 1981-03-31 | 1981-03-31 | Evaluating device for single mode optical fiber |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57161529A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5262639A (en) * | 1992-04-15 | 1993-11-16 | Norscan Instruments Ltd. | Fiber optic cable monitoring method and apparatus including moisture detection and bending loss detection |
| CN103884493B (en) * | 2014-03-11 | 2016-06-29 | 国家电网公司 | Cable fast tester |
| CN105973575A (en) * | 2016-06-28 | 2016-09-28 | 成都启源电子信息技术有限公司 | Insertion misalignment loss control system for optical fiber connector |
-
1981
- 1981-03-31 JP JP4637881A patent/JPS57161529A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57161529A (en) | 1982-10-05 |
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