JPH076867B2 - Optical fiber structure measurement method - Google Patents

Optical fiber structure measurement method

Info

Publication number
JPH076867B2
JPH076867B2 JP61012155A JP1215586A JPH076867B2 JP H076867 B2 JPH076867 B2 JP H076867B2 JP 61012155 A JP61012155 A JP 61012155A JP 1215586 A JP1215586 A JP 1215586A JP H076867 B2 JPH076867 B2 JP H076867B2
Authority
JP
Japan
Prior art keywords
fiber
light
measurement
optical fiber
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 - Lifetime
Application number
JP61012155A
Other languages
Japanese (ja)
Other versions
JPS62170832A (en
Inventor
享 井上
保次 服部
徹 茗荷谷
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.)
Sumitomo Electric Industries Ltd
Original Assignee
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 Sumitomo Electric Industries Ltd filed Critical Sumitomo Electric Industries Ltd
Priority to JP61012155A priority Critical patent/JPH076867B2/en
Publication of JPS62170832A publication Critical patent/JPS62170832A/en
Publication of JPH076867B2 publication Critical patent/JPH076867B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Testing Of Optical Devices Or Fibers (AREA)
  • Light Guides In General And Applications Therefor (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の構造を測定する方法に関する。The present invention relates to a method for measuring the structure of an optical fiber.

<従来の技術> 近年、通信用光フアイバの主流はグレーデツド・インデ
ツクス型フアイバから第7図に示すシングル・モードフ
アイバ(SMフアイバ)に移つている。SMフアイバは図中
に示すようにコア径が約10μmと小さいため、コア1が
偏心していると接続時の伝送損失が大きくなる。このた
め、SMフアイバの外径及び偏心に対する要求精度は厳し
いものになりつつある。それにつれて、光フアイバ構造
測定の精度に対する要求も高まつており、高精度な測定
法の開発が望まれている。尚、第1図中2はクラツド、
3は1次被覆、4は2次被覆である。
<Prior Art> In recent years, the mainstream of optical fibers for communication has shifted from the graded index type fiber to the single mode fiber (SM fiber) shown in FIG. As shown in the figure, the SM fiber has a small core diameter of about 10 μm, so if the core 1 is eccentric, the transmission loss at the time of connection increases. Therefore, the required accuracy for the outer diameter and eccentricity of the SM fiber is becoming severe. Along with this, there is a high demand for the accuracy of optical fiber structure measurement, and development of a highly accurate measurement method is desired. Incidentally, 2 in FIG. 1 is a cladding,
3 is a primary coating and 4 is a secondary coating.

光フアイバ構造測定方法の従来例として第8図にITVを
用いた測定法を示す。同図に示すように被測定フアイバ
5の端面5aが対物レンズ6で拡大されてITVカメラ7に
よつて観測され、モニタに映し出される。この時のITV
の輝度レベルの分布を基に、フアイバ径、コア径、フア
イバ非円率、コア非円率、コア偏心率等が評価される。
照明光として2種のものが用いられる。その1つはコア
測定用のもので、コア入射用光源8から出射し、ダミー
フアイバ9、被測定フアイバ5を伝搬し、その端面5aか
ら出射する。一方、他の1つはクラツド測定用のもの
で、反射光用光源10から出射され、ハーフミラー11で反
射されレンズ6を経て被測定フアイバの端面5aで反射す
ることとなる。このように1本の光フアイバの測定にお
いて、コア測定にはフアイバ透過光を用い、クラツド測
定にはフアイバ端面反射光を用いていた。
As a conventional example of the optical fiber structure measuring method, Fig. 8 shows the measuring method using ITV. As shown in the figure, the end surface 5a of the fiber 5 to be measured is magnified by the objective lens 6, observed by the ITV camera 7, and displayed on the monitor. ITV at this time
The fiber diameter, core diameter, fiber non-circularity, core non-circularity, core eccentricity, etc. are evaluated based on the distribution of the luminance level of.
Two types of illumination light are used. One of them is for core measurement, which is emitted from the core incidence light source 8, propagates through the dummy fiber 9 and the measured fiber 5, and is emitted from the end face 5a. On the other hand, the other one is for the cladding measurement, which is emitted from the reflected light source 10, reflected by the half mirror 11, passed through the lens 6, and reflected by the end face 5a of the fiber to be measured. Thus, in the measurement of one optical fiber, the fiber transmitted light was used for the core measurement, and the fiber end face reflected light was used for the cladding measurement.

<発明が解決しようとする問題点> 上述した従来の測定方法では、測定値が光軸の微小なず
れ或いは光軸に対する被測定フアイバ端の傾き等の影響
を受けやすく、測定精度の向上が困難であつた。
<Problems to be Solved by the Invention> In the above-described conventional measuring method, it is difficult to improve the measurement accuracy because the measured value is easily affected by a slight deviation of the optical axis or the inclination of the fiber end to be measured with respect to the optical axis. It was.

本発明は上記従来技術の問題点を解消して測定精度を向
上させると共に光入射効率を向上させた光フアイバ構造
測定方法を提供することを目的とする。
SUMMARY OF THE INVENTION It is an object of the present invention to provide a method for measuring an optical fiber structure which solves the above-mentioned problems of the prior art, improves the measurement accuracy, and improves the light incidence efficiency.

<問題点を解決するための手段> 斯かる目的を達成する本発明の構成は光ファイバの端面
をレンズで拡大して観察することにより、該光ファイバ
の構造を測定すると共に、照明光としてファイバ透過光
を用いてコア及びクラッドを測定する光ファイバ構造測
定法において、前記ファイバ透過光は、光ファイバに密
着した光散乱性物質を通過してクラッド内に入射したも
のであることを特徴とする。
<Means for Solving Problems> The structure of the present invention that achieves such an object is to measure the structure of an optical fiber by observing the end face of the optical fiber by enlarging it with a lens and measuring the fiber as illumination light. In an optical fiber structure measuring method for measuring a core and a clad by using transmitted light, the fiber transmitted light is characterized by being incident on the inside of the clad after passing through a light scattering substance in close contact with the optical fiber. .

<作用> 一般に、光が伝搬するのは光フアイバのコア部だけと思
われがちであるが、実際には短い距離であればクラツド
部でも光の伝搬が可能である。この性質を利用して本発
明ではコア測定のみならず、クラツド測定をもフアイバ
透過光により行うようにしたものである。
<Operation> Generally, it is thought that light propagates only in the core portion of the optical fiber, but actually, the light can propagate even in the cladding portion if the distance is short. Utilizing this property, in the present invention, not only the core measurement but also the cladding measurement is performed by the fiber transmitted light.

<実施例> 以下、本発明の実施例について図面を参照して詳細に説
明する。尚、前述した従来技術と同一部分については同
一番号を付して説明を省略する。
<Example> Hereinafter, an example of the present invention will be described in detail with reference to the drawings. It should be noted that the same parts as those of the above-mentioned conventional technique are designated by the same reference numerals and the description thereof will be omitted.

第1図に本発明の一実施例を示す。同図に示されるよう
に被測定フアイバ5の上方における、その端面5aに近接
した位置にクラツド測定用光源12が設置されており、該
光源12から出射した光が被測定フアイバ5のクラツドに
入射すると、この中を伝搬して被測定フアイバ端面5aか
ら出射し、ITVカメラ7によりフアイバ透過光として観
察される。これによりクラツドについての構造が評価さ
れる。コア測定については前述したコア入射用光源8に
より照明されるので、コア測定及びクラツド測定がいず
れもフアイバ透過光により照明されて行えることとな
る。尚、観測はITVカメラ7に限るものでなく、肉眼に
よるものであつても良い。
FIG. 1 shows an embodiment of the present invention. As shown in the figure, a light source 12 for cladding measurement is installed above the fiber 5 to be measured and close to its end face 5a, and the light emitted from the light source 12 is incident on the cladding of the fiber 5 to be measured. Then, the light propagates through this and exits from the fiber end face 5a to be measured, and is observed by the ITV camera 7 as fiber transmitted light. This evaluates the structure for the cladding. Since the core measurement is illuminated by the above-mentioned core incidence light source 8, both the core measurement and the cladding measurement can be performed by illuminating with the fiber transmitted light. It should be noted that the observation is not limited to the ITV camera 7, but may be performed with the naked eye.

クラッドに光を入射させる方法としては、第2図に示す
ように、フアイバ被覆13を除去した被測定フアイバ5に
光散乱性物質14を密着させ、この光散乱物質14に図中矢
印で示すように光を照射して通過させて、クラツド内に
入射させて伝搬させる方法である。光散乱性物質14とし
ては、光を散乱させることのできる物質、例えばスリガ
ラス、メンデイングテープ、ビニールテープ等が用いら
れる。
As shown in FIG. 2, the light is incident on the clad. As shown in FIG. It is a method of irradiating and passing light on and then making it enter the cladding and propagating. As the light-scattering substance 14, a substance capable of scattering light, for example, frosted glass, mending tape, vinyl tape or the like is used.

上記構成を有する本実施例では次の効果を奏する。The present embodiment having the above configuration has the following effects.

即ち、光軸に対するフアイバ端面の傾斜角がθである場
合において、クラツド測定のための照射光としてフアイ
バ端面反射光を用いる方法を第3図に、またフアイバ透
過光を用いる方法を第4図に比較して示す。両図に示さ
れるように照光明としてレンズ6に入射する光の光軸か
らのずれは、第3図に示す方法が2θであるのに対し第
4図に示す方法では(θ′−θ)である。ここでθ′は
下式で表される。従つて、例えばθ=3゜, 但し、nはフアイバの屈折率、 n′は空気の屈折率である。
That is, when the inclination angle of the fiber end face with respect to the optical axis is θ, the method of using the fiber end face reflected light as the irradiation light for the cladding measurement is shown in FIG. 3, and the method of using the fiber transmitted light is shown in FIG. It shows in comparison. As shown in both figures, the deviation of the light incident on the lens 6 as the illumination light from the optical axis is 2θ in the method shown in FIG. 3, whereas it is (θ′−θ) in the method shown in FIG. Is. Here, θ ′ is expressed by the following equation. Therefore, for example, θ = 3 °, However, n is the refractive index of fiber and n'is the refractive index of air.

n=1.4,n′=1の場合においては、2θ=6゜,
(θ′−θ)=1.2゜となり2θ>(θ′−θ)であ
る。一般に、2θ>(θ′−θ)であり、本実施例のよ
うにフアイバ透過光を用いる方が、フアイバ端面反射光
を用いる従来よりも、フアイバ端面からレンズ6に入射
する照明光の光軸からのずれが小さいこととなる。この
ことは、レンズの収差等の影響を考えると、レンズに入
射する光はレンズ中央部に光軸と平行に入射することが
望ましいので、従つて、フアイバ端面反射光を用いる場
合よりもフアイバ透過光を用いる場合の方が、より歪の
ない像が得られ、正確な測定を行えることを意味する。
また、フアイバ端面反射光を用いる場合には反射光用光
源10から発射された光がフアイバ端面できれいに結像さ
れていなければならないこと及びコア測定にはフアイバ
透過光を用いていることなどから言つても、測定精度向
上のために、クラツド測定にもフアイバ透過光を用いる
ことが望しい。
In the case of n = 1.4 and n ′ = 1, 2θ = 6 °,
(Θ'-θ) = 1.2 ° and 2θ>(θ'-θ). In general, 2θ> (θ′−θ), and the optical axis of the illumination light incident on the lens 6 from the fiber end surface is smaller when using the fiber transmitted light as in the present embodiment than when using the fiber end surface reflected light. The deviation from is small. This means that considering the effects of lens aberration, etc., it is desirable that the light entering the lens enter the center of the lens parallel to the optical axis. When light is used, it means that a more distortion-free image can be obtained and accurate measurement can be performed.
Also, when using the fiber end face reflected light, the light emitted from the reflected light source 10 must be imaged cleanly on the fiber end face, and the fact that fiber transmitted light is used for core measurement etc. In particular, it is desirable to use the fiber transmitted light for the cladding measurement in order to improve the measurement accuracy.

また、第5図及び第6図に示されるように、フアイバ端
面にきずBが存在する場合に、従来の測定法では光が外
向きに反射して、測定不能となる場合が多かつたが、フ
アイバ透過光を用いるときずの影響も少ないため測定が
可能となり、測定の効率化を計ることができる。
Further, as shown in FIGS. 5 and 6, when a flaw B is present on the fiber end face, the conventional measurement method often causes light to be reflected outward, which makes measurement impossible. Since the influence when using the fiber transmitted light is small, the measurement can be performed and the measurement efficiency can be improved.

次に、下表を参照して、フアイバ透過光を用いた本発明
とフアイバ端面反射光を用いた従来法によりクラツド測
定した結果について照明する。測定はクラツドについて
直径(μm)と偏心率(%)を各々10回づつ測定し、こ
れらの値の標準偏差を求めて結果として表にまとめたも
のである。下表−1に示すように、いずれの結果につい
ても、本発明の方が標準偏 差が小さく、つまりばらつきが小さく、このことから精
度良く測定することができることが判る。
Next, referring to the table below, the results of the cladding measurement according to the present invention using the transmitted light from the fiber and the conventional method using the reflected light from the fiber end surface are illuminated. For the measurement, the diameter (μm) and the eccentricity (%) of the cladding were measured 10 times each, and the standard deviations of these values were obtained and summarized in the table as a result. As shown in Table 1 below, for all the results, the present invention has a standard deviation. The difference is small, that is, the variation is small, which shows that accurate measurement can be performed.

<発明の効果> 以上、実施例に基づいて具体的に説明したように本発明
ではフアイバ透過光を照明光として、コアのみならずク
ラツドをも測定するので、照明光がレンズ中央を光軸と
平行に通過し易く、このため、歪のない像を観測して正
確な測定を行うことができる。
<Effects of the Invention> As described above in detail with reference to the embodiments, in the present invention, not only the core but also the cladding is measured by using the fiber transmitted light as the illumination light. Therefore, the illumination light has the lens center as the optical axis. It is easy to pass in parallel, so that an image without distortion can be observed and accurate measurement can be performed.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明を実施するための装置構成の1例を示す
説明図、第2図はクラツドへ光を入射させる方法につい
ての斜視図、第3図は端面反射光を用いて照明する場合
の照明光の光路を示す説明図、第4図はフアイバ透過光
を用いて照明する場合の照明光の光路を示す説明図、第
5図はキズのあるフアイバ端面の斜視図、第6図は第5
図中のA−A線断面図、第7図はSMフアイバの横断面
図、第8図は従来の光フアイバ構造測定方法の説明図で
ある。 図面中、 5は被測定フアイバ、 6はレンズ、 7はITVカメラ、 8,12は光源、 9はダミーフアイバ、 13はフアイバ被覆、 14は光散乱性物質である。
FIG. 1 is an explanatory diagram showing an example of a device configuration for carrying out the present invention, FIG. 2 is a perspective view of a method of making light incident on a cladding, and FIG. 3 is a case of illuminating using end face reflected light. 4 is an explanatory view showing the optical path of the illumination light, FIG. 4 is an explanatory view showing the optical path of the illumination light in the case of illuminating using fiber transmitted light, FIG. 5 is a perspective view of the fiber end surface with scratches, and FIG. 6 is Fifth
7 is a cross-sectional view of the SM fiber, and FIG. 8 is an explanatory view of a conventional optical fiber structure measuring method. In the drawing, 5 is a fiber to be measured, 6 is a lens, 7 is an ITV camera, 8 and 12 are light sources, 9 is a dummy fiber, 13 is a fiber coating, and 14 is a light scattering substance.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】光ファイバの端面をレンズで拡大して観察
することにより、該光ファイバの構造を測定すると共
に、照明光としてファイバ透過光を用いてコア及びクラ
ッドを測定する光ファイバ構造測定法において、前記フ
ァイバ透過光は、光ファイバに密着した光散乱性物質を
通過してクラッド内に入射したものであることを特徴と
する光ファイバ構造測定法。
1. An optical fiber structure measuring method for measuring the structure of the optical fiber by observing the end face of the optical fiber by enlarging it with a lens and measuring the core and the clad by using fiber transmitted light as illumination light. 2. The optical fiber structure measuring method as set forth in claim 1, wherein the light transmitted through the fiber is incident on the inside of the clad after passing through a light-scattering substance in close contact with the optical fiber.
JP61012155A 1986-01-24 1986-01-24 Optical fiber structure measurement method Expired - Lifetime JPH076867B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61012155A JPH076867B2 (en) 1986-01-24 1986-01-24 Optical fiber structure measurement method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61012155A JPH076867B2 (en) 1986-01-24 1986-01-24 Optical fiber structure measurement method

Publications (2)

Publication Number Publication Date
JPS62170832A JPS62170832A (en) 1987-07-27
JPH076867B2 true JPH076867B2 (en) 1995-01-30

Family

ID=11797570

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61012155A Expired - Lifetime JPH076867B2 (en) 1986-01-24 1986-01-24 Optical fiber structure measurement method

Country Status (1)

Country Link
JP (1) JPH076867B2 (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51144253A (en) * 1975-06-06 1976-12-11 Nec Corp Photo-fiber check method
JPS6161031A (en) * 1984-09-03 1986-03-28 Hitachi Cable Ltd Optical fiber dimension measurement method using a video analyzer

Also Published As

Publication number Publication date
JPS62170832A (en) 1987-07-27

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