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JP2945131B2 - Optical fiber preform refractive index measurement method - Google Patents

Optical fiber preform refractive index measurement method

Info

Publication number
JP2945131B2
JP2945131B2 JP33735490A JP33735490A JP2945131B2 JP 2945131 B2 JP2945131 B2 JP 2945131B2 JP 33735490 A JP33735490 A JP 33735490A JP 33735490 A JP33735490 A JP 33735490A JP 2945131 B2 JP2945131 B2 JP 2945131B2
Authority
JP
Japan
Prior art keywords
optical fiber
fiber preform
refractive index
refraction angle
distribution
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 - Fee Related
Application number
JP33735490A
Other languages
Japanese (ja)
Other versions
JPH04204229A (en
Inventor
富夫 畔蒜
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.)
Fujikura Ltd
Original Assignee
Fujikura 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 Fujikura Ltd filed Critical Fujikura Ltd
Priority to JP33735490A priority Critical patent/JP2945131B2/en
Publication of JPH04204229A publication Critical patent/JPH04204229A/en
Application granted granted Critical
Publication of JP2945131B2 publication Critical patent/JP2945131B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 [産業上の利用分野] この発明は、光ファイバ母材の屈折率分布測定方法に
関するものである。
Description: TECHNICAL FIELD The present invention relates to a method for measuring the refractive index distribution of an optical fiber preform.

[従来の技術] 第5図に、従来の屈折率分布測定系を模型的に示した
(上が側面図で下が平面図)。
[Prior Art] FIG. 5 schematically shows a conventional refractive index distribution measuring system (an upper side view and a lower side plan view).

20は光源、22は入射側の光学系、24は出射側の光学
系、26は光ビームの位置などの検出装置、28は解析装置
である。
20 is a light source, 22 is an optical system on the incident side, 24 is an optical system on the emitting side, 26 is a detecting device for detecting the position of a light beam, and 28 is an analyzing device.

被測定母材10は、クラッドとほぼ同等の屈折率を持つ
マッチングオイル16に浸しておく。
The base material 10 to be measured is immersed in a matching oil 16 having a refractive index substantially equal to that of the clad.

その軸(これをx軸とする)に対して垂直なz方向
(矢印30参照)から光ビーム32を入射して、出射する光
ビームの屈折角φを、上記検出装置26,解析装置28によ
り求める。
The light beam 32 is incident from the z direction (see arrow 30) perpendicular to the axis (this is the x axis), and the refraction angle φ of the emitted light beam is determined by the detection device 26 and the analysis device 28. Ask.

光ビーム32の入射位置をy方向に順次移動して、屈折
角φの分布を求める。
The incident position of the light beam 32 is sequentially moved in the y direction to obtain the distribution of the refraction angle φ.

屈折角分布から、計算により屈折率分布を求める。 The refractive index distribution is calculated from the refractive angle distribution by calculation.

[発明が解決しようとする課題] 光ファイバ母材10はマッチングオイル16に浸すのは、
大気中では、媒質である空気と被測定体である石英系光
ファイバ母材との屈折率の違いが大きすぎるため、屈折
角φが大きすぎて精度のよい測定ができないためであ
る。
[Problems to be Solved by the Invention] The optical fiber preform 10 is immersed in the matching oil 16
In the atmosphere, the difference in refractive index between the air as the medium and the quartz optical fiber preform as the object to be measured is too large, so that the refraction angle φ is too large to perform accurate measurement.

そこで屈折角φが余り大きくならないように、光ファ
イバ母材のクラッド部材14とほぼ同等の屈折率を持つマ
ッチングオイル16を用いている。しかし、マッチングオ
イルは飽和脂肪酸などを材料とするものが多く、高価で
あり、測定後の除去が困難であった。
Therefore, a matching oil 16 having a refractive index substantially equal to that of the clad member 14 of the optical fiber preform is used so that the refraction angle φ does not become too large. However, many of the matching oils are made of saturated fatty acids or the like, and are expensive and difficult to remove after the measurement.

また最近のように光ファイバ母材が大型になると、マ
ッチングオイルに浸すための取扱が、非常に困難にな
る。
In addition, when the optical fiber preform becomes large recently, handling for immersion in matching oil becomes very difficult.

[課題を解決するための手段] 第1図のように、光ファイバ母材10のコア部分12とそ
の近傍のクラッド部分14aの範囲についてだけ、前記光
ビームの入射による方法によって屈折角分布を求める。
[Means for Solving the Problems] As shown in FIG. 1, a refraction angle distribution is obtained by a method based on the incidence of the light beam only in the range of the core portion 12 of the optical fiber preform 10 and the cladding portion 14a in the vicinity thereof. .

それから外側のクラッド部分14bについては推定によ
り補完して、全体の屈折角分布を求める。
Then, the outer cladding portion 14b is complemented by estimation to obtain the entire refraction angle distribution.

[その説明] 光ファイバ母材10は、同心円状に配置されたコア部分
12とクラッド部分14とからなる。
[Description] The optical fiber preform 10 has a core portion arranged concentrically.
12 and a clad portion 14.

コア部分12とクラッド部分14との外径の比は、シング
ルモード光ファイバの場合、約13程度である。
The ratio of the outer diameter of the core portion 12 to the outer diameter of the clad portion 14 is about 13 in the case of a single mode optical fiber.

また通常、クラッド部分14は平坦な屈折率分布を有し
ている。
Usually, the clad portion 14 has a flat refractive index distribution.

以上の事実から、光ファイバ母材の内部屈折率分布測
定のためには、母材の中心付近の、コア部分12とその近
傍のクラッド部分14aのみを測定すれば、ほとんどすべ
てについて知ることとができ、その外側のクラッド部分
14bについては、コア近傍のクラッド部分14aとほぼ同じ
と推定してよい。
From the above facts, for measuring the internal refractive index distribution of the optical fiber preform, it is possible to know almost everything by measuring only the core portion 12 and the cladding portion 14a near the center of the preform. Can, its outer cladding part
About 14b, it may be presumed that it is almost the same as the cladding part 14a near the core.

また、第2図に示すように、光ファイバ母材の中央付
近においては、大気中で測定した場合とマッチングオイ
ル中で測定した場合の、屈折角の大きさにほとんど違い
はない(中央を外れた部分では、大気中の屈折角は非常
に大きくなる。
In addition, as shown in FIG. 2, near the center of the optical fiber preform, there is almost no difference in the magnitude of the refraction angle between when measured in air and when measured in matching oil (outside the center). In those areas, the refraction angle in the atmosphere becomes very large.

したがって、マッチングオイルの中に光ファイバ母材
を浸さずに、大気中で母材の中央部だけを測定しても、
十分な精度をもって母材全体の屈折率分布が得られるこ
とになる。
Therefore, even if only the central part of the preform is measured in the air without immersing the optical fiber preform in the matching oil,
The refractive index distribution of the entire base material can be obtained with sufficient accuracy.

なお、クラッド/コア比が13であるならば、測定範囲
yは、光ファイバ母材10の直径の15%程度までとすれば
よいことが分かっている。
It is known that if the clad / core ratio is 13, the measurement range y may be up to about 15% of the diameter of the optical fiber preform 10.

第3図は、測定装置の模型的説明図であり、マッチン
グオイル16の無い点が、従来の第5図の場合と相違して
いる。なお、この場合も、側面図と平面図を併記した。
FIG. 3 is a schematic explanatory view of a measuring device, which differs from the conventional case of FIG. 5 in that the matching oil 16 is not provided. In this case, the side view and the plan view are also shown.

第4図の実線部分は、この装置で測定した屈折角分布
の一例である。
The solid line in FIG. 4 is an example of the refraction angle distribution measured by this apparatus.

なお、この場合は、直径に対して約20%の部分を測定
した。
In this case, about 20% of the diameter was measured.

残りの破線部分は、光ビームの堆積を数値計算によっ
て推定し、実線部分と接続して補完したものである。
The remaining broken line portion is obtained by estimating the deposition of the light beam by numerical calculation and connecting the solid line portion to complement it.

このようにして、屈折角分布が求められると、その後
は従来の場合同様に、計算により、屈折率分布を求める
ことができる。
After the refraction angle distribution is obtained in this way, the refraction index distribution can be obtained by calculation in the same manner as in the conventional case.

[発明の作用効果] 光ファイバ母材のコア部分とその近傍のクラッド部分
の範囲についてだけ、屈折角分布を求め、それから外側
のクラッド部分については推定により補完して全体の屈
折角分布を求めるようにしたので、 (1)上記のように、マッチングオイルを用いないで、
大気中で測定しても、十分な精度が得られる。
[Function and Effect of the Invention] The refractive angle distribution is obtained only for the core portion of the optical fiber preform and the range of the cladding portion near the core portion, and then the outer cladding portion is complemented by estimation to obtain the entire refractive angle distribution. (1) As mentioned above, do not use matching oil,
Even when measured in the atmosphere, sufficient accuracy can be obtained.

(2)そのために、マッチングオイルの使用に伴う上記
の問題(特に大型母材の場合の取扱困難、測定後の洗浄
など)が解消される。
(2) As a result, the above-mentioned problems associated with the use of the matching oil (particularly difficult handling in the case of a large base material, washing after measurement, etc.) are solved.

なお、この発明の方法により、従来の方法で40分程度
かかっていた測定を、ほぼ同程度の精度を確保したま
ま、5分で完了することができた。
According to the method of the present invention, the measurement, which took about 40 minutes by the conventional method, could be completed in 5 minutes while securing approximately the same accuracy.

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

第1〜4図はこの発明の実施例にかかるもので、第1図
は屈折角の測定範囲の説明図、 第2図は大気中とマッチングオイル中で測定した屈折角
の大きさの違いを示す説明図、 第3図は測定装置の模型的説明図、 第4図は屈折角分布図、 第5図は従来技術の模型的説明図。 10:光ファイバ母材、12:コア部分 14:クラッド部分、20:光源 22,24:光学系 26:角度、位置の検出装置 28:解析装置
1 to 4 relate to an embodiment of the present invention. FIG. 1 is an explanatory diagram of a measurement range of a refraction angle, and FIG. 2 is a diagram showing a difference in a refraction angle measured in the atmosphere and in a matching oil. FIG. 3 is a model explanatory view of a measuring apparatus, FIG. 4 is a refraction angle distribution diagram, and FIG. 5 is a model explanatory view of a prior art. 10: optical fiber preform, 12: core part 14: clad part, 20: light source 22, 24: optical system 26: angle and position detection device 28: analysis device

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】光ファイバ母材に、その軸(x軸)に対し
て垂直のz方向から光ビームを入射して、出射する光ビ
ームの屈折角を測定するとともに、前記光ビームの入射
位置をy方向に順次移動することにより、前記屈折角の
分布を求め、その屈折角分布から屈折率分布を求める、
光ファイバ母材の屈折率測定方法において、 前記光ファイバ母材のコア部分とその近傍のクラッド部
分の範囲についてだけ、前記光ビームの入射による方法
によって屈折角分布を求め、それから外側のクラッド部
分については推定により補完して全体の屈折角分布を求
める、光ファイバ母材の屈折率測定方法。
1. A light beam is incident on an optical fiber preform from a z-direction perpendicular to its axis (x-axis), the refraction angle of an outgoing light beam is measured, and the incident position of the light beam is measured. Are sequentially moved in the y-direction to determine the distribution of the refraction angle, and determine the refractive index distribution from the refraction angle distribution.
In the method for measuring the refractive index of the optical fiber preform, only for the core portion of the optical fiber preform and the range of the clad portion in the vicinity thereof, the refraction angle distribution is obtained by the method by incidence of the light beam, and then the outer clad portion is obtained. Is a method for measuring the refractive index of an optical fiber preform, which obtains the entire refraction angle distribution by complementing by estimation.
JP33735490A 1990-11-30 1990-11-30 Optical fiber preform refractive index measurement method Expired - Fee Related JP2945131B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP33735490A JP2945131B2 (en) 1990-11-30 1990-11-30 Optical fiber preform refractive index measurement method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP33735490A JP2945131B2 (en) 1990-11-30 1990-11-30 Optical fiber preform refractive index measurement method

Publications (2)

Publication Number Publication Date
JPH04204229A JPH04204229A (en) 1992-07-24
JP2945131B2 true JP2945131B2 (en) 1999-09-06

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ID=18307833

Family Applications (1)

Application Number Title Priority Date Filing Date
JP33735490A Expired - Fee Related JP2945131B2 (en) 1990-11-30 1990-11-30 Optical fiber preform refractive index measurement method

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Country Link
JP (1) JP2945131B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3735063B2 (en) * 2001-12-13 2006-01-11 古河電気工業株式会社 Optical fiber preform refractive index measurement method

Also Published As

Publication number Publication date
JPH04204229A (en) 1992-07-24

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