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JPH0136050B2 - - Google Patents
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JPH0136050B2 - - Google Patents

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Publication number
JPH0136050B2
JPH0136050B2 JP5949380A JP5949380A JPH0136050B2 JP H0136050 B2 JPH0136050 B2 JP H0136050B2 JP 5949380 A JP5949380 A JP 5949380A JP 5949380 A JP5949380 A JP 5949380A JP H0136050 B2 JPH0136050 B2 JP H0136050B2
Authority
JP
Japan
Prior art keywords
fiber
groups
optical fiber
distribution
concentration 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
Application number
JP5949380A
Other languages
Japanese (ja)
Other versions
JPS56155827A (en
Inventor
Toshito Hosaka
Yasuji Oomori
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.)
NTT Inc
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 JP5949380A priority Critical patent/JPS56155827A/en
Publication of JPS56155827A publication Critical patent/JPS56155827A/en
Publication of JPH0136050B2 publication Critical patent/JPH0136050B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M11/00Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
    • G01M11/30Testing of optical devices, constituted by fibre optics or optical waveguides
    • G01M11/37Testing of optical devices, constituted by fibre optics or optical waveguides in which light is projected perpendicularly to the axis of the fibre or waveguide for monitoring a section thereof

Landscapes

  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • General Physics & Mathematics (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Testing Of Optical Devices Or Fibers (AREA)

Description

【発明の詳細な説明】 本発明は、光フアイバ中のOH基の濃度分布の
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 the concentration distribution of OH groups in an optical fiber.

従来、光フアイバ中のOH基の濃度分布の測定
には、赤外分光計による波長2.73μmでのOH基に
よる強い光吸収を測定する方法が用いられて来
た。この方法では、光源としてSiCランプを使用
し、回折格子型分光器によりOH基の基本吸収波
長である2.73μmの単色光を得ている。そして、
この光をCaF2製のレンズ系で平行束とした後に、
1mm厚の円板状に切り出して研磨した測定試料に
垂直に入射させる。測定試料を通過した光束をコ
ア径約60μmの低OH多モードステツプ型光フア
イバ(約30cm長)でとらえ、InSb光検出器に導
き、ここで検出した信号を電流増幅した後、ロツ
クイン増幅器に入力する。フアイバ用母材の径方
向のOH基分布を測定するにあたつては、試料移
動台を用いて、測定試料を入射光束と垂直方向に
50μm間隔で移動させながら透過光強度分布を測
定し、これよりOH基の濃度分布を求める。この
方法の欠点として、0.1ppm以下の微少なOH基の
測定が困難であること、コアとクラツドとの境界
で屈折率が急激に変化していることに起因する光
透過強度分布の乱れが存在すること等が挙げられ
る。
Conventionally, the concentration distribution of OH groups in an optical fiber has been measured by a method of measuring strong light absorption by OH groups at a wavelength of 2.73 μm using an infrared spectrometer. In this method, a SiC lamp is used as a light source, and a monochromatic light of 2.73 μm, which is the fundamental absorption wavelength of OH groups, is obtained using a diffraction grating spectrometer. and,
After converting this light into a parallel beam using a CaF 2 lens system,
The light is applied perpendicularly to the measurement sample, which has been cut into a 1 mm thick disc and polished. The light flux that has passed through the measurement sample is captured by a low-OH multimode step optical fiber (about 30 cm long) with a core diameter of about 60 μm, guided to an InSb photodetector, where the detected signal is amplified by current and then input to a lock-in amplifier. do. When measuring the OH group distribution in the radial direction of the fiber base material, a sample moving stage is used to move the measurement sample in the direction perpendicular to the incident light flux.
The transmitted light intensity distribution is measured while moving at 50 μm intervals, and the OH group concentration distribution is determined from this. The disadvantages of this method are that it is difficult to measure minute OH groups of 0.1 ppm or less, and that there is a disturbance in the light transmission intensity distribution due to the rapid change in the refractive index at the boundary between the core and the cladding. Examples include:

本発明の目的は、上述した欠点を除去し、光フ
アイバの長さに比例して測定精度が向上する特長
を有する光フアイバの伝送損失測定系を利用して
OH基による吸収損失を求め、さらに光フアイバ
中のOH基の濃度分布を導出し、以て微少なOH
基の測定を行うことのできる方法を提案すること
にある。
An object of the present invention is to eliminate the above-mentioned drawbacks and utilize an optical fiber transmission loss measurement system that has the feature that measurement accuracy improves in proportion to the length of the optical fiber.
The absorption loss due to OH groups is determined, and the concentration distribution of OH groups in the optical fiber is derived.
The object of the present invention is to propose a method that can perform measurements of groups.

以下図面について本発明を詳細に説明する。 The invention will be explained in detail below with reference to the drawings.

本発明では、同一母材から製造された種々の規
格化導波路幅(または規格化周波数)(以下では
V値という)を有する単一モード光フアイバを用
いるが、かかる光フアイバを製造するための線引
き装置の一例を第1図に示す。第1図において、
1は光フアイバ用母材、2は抵抗加熱炉、3はフ
アイバ外径測定部、4は被覆装置、5はキヤプス
タン、6は光フアイバ、7は巻き取り装置、8は
フアイバ外径制御回路、9は母材送り装置であ
る。第1図より明らかなように光フアイバ用母材
1は母材送り装置9により徐々に抵抗加熱炉2に
送られる。抵抗加熱炉2で約2000℃に加熱された
母材先端は軟化し、粘性が低下してくびれフアイ
バとなりキヤプスタン5によつて引き出される。
線引きされたフアイバ6は巻き取り装置7に装着
したドラムに巻き取られる。また、光フアイバ6
の強度を保つために被覆装置4によつてウレタン
およびシリコンがフアイバ6のガラス表面に被覆
される。光フアイバ6の外径の制御はフアイバ外
径測定部3でフアイバ6の外径を読み取り、フア
イバ外径制御回路8において、測定値を、設定値
と比較してフアイバの巻き取り速度を制御するこ
とにより行なつている。
In the present invention, single mode optical fibers having various standardized waveguide widths (or standardized frequencies) (hereinafter referred to as V values) manufactured from the same base material are used. An example of a wire drawing device is shown in FIG. In Figure 1,
1 is a base material for optical fiber, 2 is a resistance heating furnace, 3 is a fiber outer diameter measuring section, 4 is a coating device, 5 is a capstan, 6 is an optical fiber, 7 is a winding device, 8 is a fiber outer diameter control circuit, 9 is a base material feeding device. As is clear from FIG. 1, the optical fiber preform 1 is gradually fed to the resistance heating furnace 2 by the preform feeder 9. The tip of the base material heated to about 2000° C. in the resistance heating furnace 2 is softened and its viscosity is reduced to become a constricted fiber and drawn out by the capstan 5.
The drawn fiber 6 is wound onto a drum attached to a winding device 7. In addition, optical fiber 6
A coating device 4 coats the glass surface of the fiber 6 with urethane and silicon to maintain its strength. To control the outer diameter of the optical fiber 6, a fiber outer diameter measuring section 3 reads the outer diameter of the fiber 6, and a fiber outer diameter control circuit 8 compares the measured value with a set value to control the winding speed of the fiber. This is done by doing this.

次に本発明の1実施例について述べる。外径12
mm、合成クラツド径5mm、コア径0.7mmおよび屈
折率差0.2%の母材1を母材送り装置9に装着し、
上述の方法により加熱溶融して27m/分の線引き
速度で外径100μmのフアイバ6を約500m製造す
る。次に巻き取り速度を23m/分にし、外径
120μmのフアイバ6を500m製造する。このよう
な工程を繰り返して行ない、フアイバ外径が
100μm〜200μmまで20μmづつ変化している6本
のフアイバを製造する。このようにして製造した
フアイバはコア径が約5μm〜10μmであり、OH
基の吸引損失波長である1.38μmでのV値は2.4以
下になるよう設計される。ここで、 V=2π/λa√1 22 2 (1) であり、2aはコア径、n1はコアに屈折率、n2
クラツドの屈折率、λは波長である。そして、V
<2.4としたため伝搬するモードは基本モードの
みとなる。
Next, one embodiment of the present invention will be described. Outer diameter 12
A base material 1 with a synthetic cladding diameter of 5 mm, a core diameter of 0.7 mm, and a refractive index difference of 0.2% is mounted on the base material feeding device 9,
Approximately 500 m of fiber 6 having an outer diameter of 100 μm is produced by heating and melting by the above-described method at a drawing speed of 27 m/min. Next, set the winding speed to 23 m/min, and
Manufacture 500m of 120μm fiber 6. By repeating this process, the outer diameter of the fiber becomes
Six fibers are produced varying in 20 μm steps from 100 μm to 200 μm. The fiber produced in this way has a core diameter of about 5 μm to 10 μm, and has an OH
The V value at 1.38 μm, which is the original absorption loss wavelength, is designed to be 2.4 or less. Here, V=2π/λa√ 1 22 2 (1) where 2a is the core diameter, n 1 is the refractive index of the core, n 2 is the refractive index of the cladding, and λ is the wavelength. And V
Since <2.4, the only mode that propagates is the fundamental mode.

次にこれらのフアイバのOH基による吸収損失
およびコアの屈折率分布の測定を行なう。第2図
は上述の方法により線引かれた種々のフアイバ
の、波長1.38μmでのOH基による吸収損失
[dB/Km]をV値に対して示したものである。
また、第3図は上述のフアイバのコアの屈折率分
布を示したものであり、第4図はこのフアイバに
おける距離r/aでの基本モードのパワー分布P
(r)を種々のV値に対して示したものである。
Next, we will measure the absorption loss due to OH groups of these fibers and the refractive index distribution of the core. FIG. 2 shows the absorption loss [dB/Km] due to OH groups at a wavelength of 1.38 μm for various fibers drawn by the above-mentioned method versus the V value.
Moreover, FIG. 3 shows the refractive index distribution of the core of the fiber mentioned above, and FIG. 4 shows the power distribution P of the fundamental mode at the distance r/a in this fiber.
(r) is shown for various V values.

OH基による吸収損失(第2図)およびコアの
屈折率分布(第3図)は既存の測定装置により容
易に測定できる。また基本モードのパワー分布P
(r)(第4図)はコアの屈折率分布から計算され
る。しかして、フアイバ中のOH基の濃度分布は
第2図および第4図から以下のような計算により
導出される。
Absorption loss due to OH groups (Figure 2) and core refractive index distribution (Figure 3) can be easily measured using existing measurement equipment. Also, the power distribution of the fundamental mode P
(r) (FIG. 4) is calculated from the refractive index distribution of the core. Therefore, the concentration distribution of OH groups in the fiber can be derived from FIGS. 2 and 4 by the following calculation.

光フアイバ断面におけるOH基の濃度分布は母
材の作製工程で決定され線引き工程はOH基の濃
度分布にほとんど影響しない。従つて、同一母材
から得た種々のV値を有する光フアイバにおい
て、光フアイバ断面におけるOH基の濃度分布は
各光フアイバで相似形となる。すなわち、各光フ
アイバにおいてコア径を基準にとり半径方向の距
離を規格化すれば、各光フアイバにおけるOH基
濃度分布は同一になる。さらに、本実施例で述べ
ているように、種々のV値の光フアイバを得るた
め、コア径を変化させる場合、コア径の変化率と
同じ割合で光フアイバの外径も変化している。従
つて、フアイバ断面を半径方向に等間隔で分割す
る場合、分割数を同じにすれば各分割された領域
でのOH基の濃度は種々のV値を有する光フアイ
バで同一になる。
The concentration distribution of OH groups in the cross section of the optical fiber is determined by the process of manufacturing the base material, and the drawing process has little effect on the concentration distribution of OH groups. Therefore, in optical fibers having various V values obtained from the same base material, the concentration distribution of OH groups in the optical fiber cross section will be similar in each optical fiber. That is, if the distance in the radial direction of each optical fiber is normalized based on the core diameter, the OH group concentration distribution in each optical fiber will be the same. Furthermore, as described in this embodiment, when changing the core diameter in order to obtain optical fibers with various V values, the outer diameter of the optical fiber is also changed at the same rate as the rate of change of the core diameter. Therefore, when the fiber cross section is divided at equal intervals in the radial direction, if the number of divisions is the same, the concentration of OH groups in each divided region will be the same for optical fibers having various V values.

まず、フアイバの断面を半径方向に等間隔に区
分する。分割数は10とする。それぞれの領域での
求めるべきOH基の濃度をC1、C2、…、C10とす
る。V=2.0のときのフアイバ断面中のHE11モー
ドの全パワーを1と規格化すると、それぞれの領
域でのパワーは第4図より求めることができ、そ
の値をP1,1、P2,1、…、P10,1とする。V=2.0のと
きのOH基による吸収損失は第2図から求めるこ
とができ、その値をl1とすると、V=2.0について
次式が成立する。
First, the cross section of the fiber is divided into equal intervals in the radial direction. The number of divisions is 10. The concentrations of OH groups to be determined in each region are assumed to be C 1 , C 2 , ..., C 10 . If the total power of the HE 11 mode in the fiber cross section when V = 2.0 is normalized to 1, the power in each region can be found from Figure 4, and the values can be expressed as P 1,1 , P 2, 1 ,...,P 10,1 . The absorption loss due to the OH group when V=2.0 can be determined from FIG. 2, and if that value is l1 , then the following equation holds true for V=2.0.

Q×(C1P1,1+C2P2,1+…+C10P10,1)=l1 (2) ただしQは比例定数であり、波長1.38μmでは
Q=65である。ここでQは1ppm当りのOH基に
起因する吸収損失値を与え、1.38μmに生じるOH
基の吸収ピークでは65dB/kmの損失値になる。
以下同様にして、種々のV値(V<2.4)につい
て下記の式 Q×(C1P1,2+C2P2,2+…+C10P10,2)=l2 Q×(C1P1,3+C2P2,3+…+C10P10,3)=l3 〓 Q×(C1P1,10+C2P2,10+…+C10P10,10)=l10 が成立するので、10行10列の連立方程式より、
OH基濃度C1、C2、…、C10を導出することがで
きる。ただし分割数は10に限らず、またフアイバ
は上述以外のすべてのフアイバに適用できる。使
用するOH基の吸収波長も1.38μmに限らず、
0.94μmおよび1.24μm等の波長も使用可能であ
る。
Q×(C 1 P 1,1 +C 2 P 2,1 +…+C 10 P 10,1 )=l 1 (2) However, Q is a proportionality constant, and at a wavelength of 1.38 μm, Q=65. Here, Q gives the absorption loss value due to OH groups per 1 ppm, and the OH generated at 1.38 μm
The original absorption peak results in a loss value of 65 dB/km.
Similarly, for various V values (V<2.4), the following formula Q×(C 1 P 1,2 +C 2 P 2,2 +…+C 10 P 10,2 )=l 2 Q×(C 1 P 1,3 +C 2 P 2,3 +…+C 10 P 10,3 )=l 3 〓 Q×(C 1 P 1,10 +C 2 P 2,10 +…+C 10 P 10,10 )= l 10 holds, so from the 10 rows and 10 columns of simultaneous equations,
The OH group concentrations C 1 , C 2 , ..., C 10 can be derived. However, the number of divisions is not limited to 10, and the fibers can be applied to all fibers other than those mentioned above. The absorption wavelength of the OH group used is not limited to 1.38μm,
Wavelengths such as 0.94 μm and 1.24 μm can also be used.

第5図はこのようにして導出したフアイバ中の
OH濃度分布を示したものである。第5図より、
本発明によれば10ppb程度の微小OH濃度の精密
測定が可能であることがわかる。なお、OH基に
よる吸収は1.38μmでは非常に強いので、10ppb以
下の測定も十分可能である。
Figure 5 shows the fibers derived in this way.
This shows the OH concentration distribution. From Figure 5,
It can be seen that according to the present invention, precise measurement of minute OH concentrations of about 10 ppb is possible. Note that since absorption by OH groups is very strong at 1.38 μm, measurement of 10 ppb or less is fully possible.

以上説明したように、本発明の光フアイバ中の
OH基濃度分布の測定方法によれば、OH基の吸
収損失値をデータとして使用しているが、かかる
吸収損失値は光フアイバ長に比例して測定精度が
向上するので、微少なOH基濃度の測定が可能で
あるという利点がある。また、本発明方法により
測定したOH基濃度分布を光フアイバの製造プロ
セスに帰還してそのプロセスを制御することによ
つて、層の低OH化に寄与することができる。
As explained above, in the optical fiber of the present invention,
According to the measurement method of OH group concentration distribution, the absorption loss value of OH group is used as data, but the measurement accuracy of such absorption loss value improves in proportion to the optical fiber length, so it is difficult to detect minute OH group concentration. It has the advantage that it is possible to measure Further, by feeding back the OH group concentration distribution measured by the method of the present invention to the optical fiber manufacturing process and controlling that process, it is possible to contribute to lowering the OH of the layer.

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

第1図は本発明を実施するための線引き装置の
概略図、第2図はOH基による吸収損失のV値依
存性を示すグラフ、第3図はコアの屈折率分布を
示すグラフ、第4図は基本モードの電力分布をV
値をパラメータとして示すグラフ、第5図は導出
されたフアイバ中のOH濃度分布を示すグラフで
ある。 1……フアイバ用母材、2……抵抗加熱炉、3
……フアイバ外径測定部、4……被覆装置、5…
…キヤプスタン、6……フアイバ、7……巻き取
り装置、8……フアイバ外径制御回路、9……母
材送り装置。
Fig. 1 is a schematic diagram of a drawing apparatus for carrying out the present invention, Fig. 2 is a graph showing the V value dependence of absorption loss due to OH groups, Fig. 3 is a graph showing the refractive index distribution of the core, and Fig. 4 is a graph showing the V value dependence of absorption loss due to OH groups. The figure shows the fundamental mode power distribution V
A graph showing the values as parameters, FIG. 5 is a graph showing the derived OH concentration distribution in the fiber. 1...Fiber base material, 2...Resistance heating furnace, 3
...Fiber outer diameter measuring section, 4...Coating device, 5...
... Capstan, 6 ... Fiber, 7 ... Winding device, 8 ... Fiber outer diameter control circuit, 9 ... Base material feeding device.

Claims (1)

【特許請求の範囲】[Claims] 1 光通信用伝送媒体である光フアイバ中のOH
基の濃度分布の測定方法において、同一母材から
作製した種々の規格化導波路幅の単一モード光フ
アイバについて、OH基による吸収損失の実測値
と屈折率分布の実測値に基いて計算されたパワー
分布とを用いてOH基濃度を未知数とした方程式
を作り、これを解くことによつてOH基濃度分布
を求めることを特徴とする光フアイバ中のOH基
濃度分布の測定方法。
1 OH in optical fiber, which is a transmission medium for optical communication
In the method for measuring the concentration distribution of OH groups, calculations are made based on the measured values of absorption loss due to OH groups and the measured values of the refractive index distribution for single mode optical fibers with various standardized waveguide widths made from the same base material. A method for measuring the OH group concentration distribution in an optical fiber, characterized in that the OH group concentration distribution is determined by creating an equation with the OH group concentration as an unknown quantity using the calculated power distribution and solving the equation.
JP5949380A 1980-05-07 1980-05-07 Measuring method for oh group concentration distribution in optical fiber Granted JPS56155827A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5949380A JPS56155827A (en) 1980-05-07 1980-05-07 Measuring method for oh group concentration distribution in optical fiber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5949380A JPS56155827A (en) 1980-05-07 1980-05-07 Measuring method for oh group concentration distribution in optical fiber

Publications (2)

Publication Number Publication Date
JPS56155827A JPS56155827A (en) 1981-12-02
JPH0136050B2 true JPH0136050B2 (en) 1989-07-28

Family

ID=13114863

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5949380A Granted JPS56155827A (en) 1980-05-07 1980-05-07 Measuring method for oh group concentration distribution in optical fiber

Country Status (1)

Country Link
JP (1) JPS56155827A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103630510A (en) * 2013-11-29 2014-03-12 浙江工业大学 Method for qualitatively determining hydroxyl free radicals in gas-phase reaction system
CN115372357B (en) * 2022-08-19 2024-04-12 中国科学院上海光学精密机械研究所 System and method for monitoring and purifying gaseous OH in hollow fiber in real time

Also Published As

Publication number Publication date
JPS56155827A (en) 1981-12-02

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