JPS628105A - Polarization maintaining optical fiber - Google Patents
Polarization maintaining optical fiberInfo
- Publication number
- JPS628105A JPS628105A JP60148014A JP14801485A JPS628105A JP S628105 A JPS628105 A JP S628105A JP 60148014 A JP60148014 A JP 60148014A JP 14801485 A JP14801485 A JP 14801485A JP S628105 A JPS628105 A JP S628105A
- Authority
- JP
- Japan
- Prior art keywords
- refractive index
- stress
- fiber
- polarization
- optical fiber
- 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.)
- Granted
Links
Classifications
-
- 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
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/105—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type having optical polarisation effects
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
- Glass Compositions (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、偏波保持性に優れた偏波保持光ファイバに関
する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a polarization-maintaining optical fiber with excellent polarization-maintaining properties.
第1図(a)、(b)は偏波保持光ファイバの構造の一
例を示したものであり応力付与型偏波保持光ファイバと
呼ばれるものである。第1図で1はコア部、2は応力付
与部、3はクラッド部であり、応力付与部2とクラッド
部3の熱膨張係数の差によって、光の伝播するコア部1
に応力が付与されるものであり、この結果コア部1内で
は、応力の付与される方向とそれと直交する方向とで屈
折率がわずかに異なることとなり、したがってそれぞれ
の方向に対応する伝播光の偏波面が保持されることとな
る。FIGS. 1(a) and 1(b) show an example of the structure of a polarization-maintaining optical fiber, which is called a stress-applied polarization-maintaining optical fiber. In FIG. 1, 1 is a core section, 2 is a stress applying section, and 3 is a cladding section.Due to the difference in coefficient of thermal expansion between the stress applying section 2 and the cladding section 3, the core section 1
As a result, within the core portion 1, the refractive index differs slightly between the direction in which the stress is applied and the direction perpendicular to it, and therefore the propagating light in each direction differs. The plane of polarization will be maintained.
従来、応力付与部2の材料としては、S!02にBz
Oz 、Qe 02 、P20S 、F、等ノウちの1
種以上を添加した組成のガラス素材が使用されていた。Conventionally, the material for the stress applying portion 2 has been S! Bz on 02
Oz, Qe 02, P20S, F, etc.
A glass material with a composition in which more than one species was added was used.
しかしながら、このような組成のガラス素材よりなる応
力付与部2を有する偏波保持光ファイバにあっては、そ
の偏波保持性の点で次のような問題があった。However, the polarization-maintaining optical fiber having the stress applying portion 2 made of a glass material having such a composition has the following problems in terms of its polarization-maintaining property.
一般に、第1図で示したような応力付与型幅波
□保持光ファイバの場合、その偏波保持力B(モー
iド複屈折率と呼ばれる)は、一般に次式(1)で
・:表わされる。In general, a stress-applying wide wave as shown in Figure 1 is used.
□In the case of a maintaining optical fiber, its polarization maintaining power B (mode
The i-do birefringence index is generally expressed by the following formula (1).
Bゲ(α2−α3 )・T−Co ・・・・・・
(1)(IEEE、Vow、 LT−2,No、5
.PP。B game (α2-α3)・T-Co...
(1) (IEEE, Vow, LT-2, No, 5
.. P.P.
650−662.1984.0ct)ここで、α2、α
3は応力付与部2及びクラッド部3の熱膨張係数、王は
応力付与部2をなすガラス素材の固化温度、 coは構
造で決まる定数である。したがって、(1)式より、固
化温度Tが高いほど、また、熱膨張係数差(α2−α3
)が大きいほどBが大きくなることになる。650-662.1984.0ct) Here, α2, α
3 is the coefficient of thermal expansion of the stress-applying portion 2 and the cladding portion 3, 〇 is the solidification temperature of the glass material forming the stress-applying portion 2, and co is a constant determined by the structure. Therefore, from equation (1), the higher the solidification temperature T, the higher the difference in thermal expansion coefficient (α2−α3
) is larger, B becomes larger.
ところが、応力付与部2をなすガラス素材が8203を
添加したガラス素材の場合、熱膨張係数は大きくなるが
、ガラスの固化温度が低下するため、得られる付与応力
は期待するほど高くならないという欠点があった。また
、Qe 02 、 P205を添加した場合、軟化温度
低下の点ではやや改善されるが、屈折率値がコアより高
くなり易いため、応力付与部2のガラス素材としては不
適切であった。このため、従来の偏波保持光ファイバで
は、その偏波保持性が不十分であるという問題があった
。However, when the glass material forming the stress applying part 2 is a glass material to which 8203 is added, the thermal expansion coefficient increases, but the solidification temperature of the glass decreases, so the resulting applied stress is not as high as expected. there were. Further, when Qe 02 and P205 are added, although the softening temperature is slightly improved, the refractive index value tends to be higher than that of the core, so it is not suitable as a glass material for the stress applying part 2. For this reason, conventional polarization-maintaining optical fibers have a problem in that their polarization-maintaining properties are insufficient.
そこで本発明にあっては、応力付与部をなすガラス素材
として少なくとも5モル%のAjPO4を含む5fOz
ガラス素材を採用することにより、応力付与部のガラス
素材の固化温度を高めるとともにその屈折率を低下せし
めコア部のガラス素材の屈折率よりも高くなる不都合を
解決し、優れた偏波保持性を有するようにした。Therefore, in the present invention, 5fOz containing at least 5 mol% of AjPO4 is used as the glass material forming the stress applying part.
By using a glass material, the solidification temperature of the glass material in the stress-applying part is raised and its refractive index is lowered, solving the problem of the refractive index being higher than that of the glass material in the core part, and achieving excellent polarization maintenance. It was made to have.
以下、本発明の詳細な説明する。The present invention will be explained in detail below.
AjPO4は、ベルリナイトとも呼ばれ、Al2O2と
Pz Osとをほぼ等吊混合してガラス化することなど
により得られるものである。このAJP04自体の固化
温度は、1850℃±50℃と極めて高く、また熱膨張
係数も20X10−!/℃で、Si 02の10倍程度
の値である。さらに、AJ POA自体の屈折率は1.
436 (0,63μm)であり、5iOz (1,
458)よりわずかに小さい値を有するも゛のである。AjPO4 is also called Berlinite, and is obtained by mixing Al2O2 and PzOs in substantially equal proportions and vitrifying the mixture. The solidification temperature of AJP04 itself is extremely high at 1850°C±50°C, and its thermal expansion coefficient is 20X10-! /°C, which is about 10 times that of Si 02. Furthermore, the refractive index of AJ POA itself is 1.
436 (0,63μm) and 5iOz (1,
458).
次に、このAjPO4を含むSiO2ガラス素材の特性
を知るために、VAD法によってSiO2中にAjPO
4を添加(実際はAl2O2とP2O5を同量添加)し
たガラス素材を製造し、該ガラス素材の屈折率値、熱膨
張係数および固化温度の変化を測定した。第2図はAl
POaの添加量と屈折率の関係を、また第3図はAjP
O4の添加量と熱膨張係数の関係を、さらに第4図はA
jPO4の添加量と同化温度との関係を示したものであ
る。第2図からAjPO4を添加した場合、20モル%
程度添加しても、屈折率はSiO2とほとんど差がない
くわずかに低い値となる)ことがわかった。また第3図
から熱膨張係数値は、20モル%の添加で5fOzの約
4倍となり、同量の8203を添加した場合より大きな
値となった。Next, in order to understand the characteristics of this SiO2 glass material containing AjPO4, AjPO4 was added into SiO2 by the VAD method.
A glass material to which 4 was added (actually, the same amount of Al2O2 and P2O5 were added) was manufactured, and changes in the refractive index value, thermal expansion coefficient, and solidification temperature of the glass material were measured. Figure 2 shows Al
Figure 3 shows the relationship between the amount of POa added and the refractive index.
Figure 4 shows the relationship between the amount of O4 added and the coefficient of thermal expansion.
This figure shows the relationship between the amount of jPO4 added and the assimilation temperature. From Figure 2, when AjPO4 is added, 20 mol%
It was found that even if SiO2 is added to a certain degree, the refractive index becomes a slightly lower value with almost no difference from that of SiO2. Moreover, from FIG. 3, the thermal expansion coefficient value was about four times that of 5 fOz when 20 mol % was added, which was larger than when the same amount of 8203 was added.
さらに、第4図からAj PO4S i 02混合系ガ
ラスの固化温度は、20モル%の添加で約1690℃と
なり、B2O3を20モル%含むSiO2ガラスよりも
約100℃以上高くなっている。Furthermore, from FIG. 4, the solidification temperature of the Aj PO4S i 02 mixed glass is about 1690° C. when 20 mol% is added, which is about 100° C. or more higher than that of SiO2 glass containing 20 mol% B2O3.
よって、熱膨張係数の値と、応力付与部の同化温度の上
昇の効果により、従来の8203を用いた偏波保持ファ
イバと同等以上の特性を得るためにはAjPO<の含有
量は少なくとも5モル%以上とすることが必要であ゛す
、好ましくは5〜50モル%の範囲で決められる。5モ
ル%未満であれば、応力付与部として必要な熱膨張係数
が得られず、また50モル%以上では、クラッド部との
固化温度の差が大きくなりすぎ、線引工程に困難が生ず
る。Therefore, due to the value of the thermal expansion coefficient and the effect of increasing the assimilation temperature of the stress-applying part, the content of AjPO< should be at least 5 mol in order to obtain properties equivalent to or better than that of a polarization-maintaining fiber using conventional 8203. % or more, preferably in the range of 5 to 50 mol %. If it is less than 5 mol %, the thermal expansion coefficient necessary for the stress applying part cannot be obtained, and if it is 50 mol % or more, the difference in solidification temperature with the cladding part becomes too large, causing difficulty in the wire drawing process.
次に、AjPO4を20モル%添加したガラス素材を用
いて第1図(a)に示した構造の偏波保持光ファイバを
製造した。この偏波保持ファイバの路光は、コア径9.
6μm、外径200μm。Next, a polarization-maintaining optical fiber having the structure shown in FIG. 1(a) was manufactured using a glass material to which 20 mol% of AjPO4 was added. The path light of this polarization maintaining fiber has a core diameter of 9.
6μm, outer diameter 200μm.
カットオフ波長1.35μm、コア比屈折率差0゜35
%、応力付与部比屈折率−0,1%であり、本ファイバ
のモード複屈折率Bは1.5X10′3゜また直交する
モード間のクロストークは一45dB(波長1.55μ
m、ファイバ長3触)であった。この値は、同じ構造の
偏波保持ファイバで応力付与部をS io2 B203
(20モル%)とした場合に比べて、Bが約5倍、
またクロストークで20dB改良されていた。また本フ
ァイバの損失値は波長1.56μmで0.20dB/F
aであり、極めて低損失なものであった。これはAlP
O4が特に吸収損失等を引き起こす原因にならないため
と考えられる。Cutoff wavelength 1.35 μm, core relative refractive index difference 0°35
%, the relative refractive index of the stress-applying part is -0.1%, and the mode birefringence B of this fiber is 1.5X10'3°, and the crosstalk between orthogonal modes is -45 dB (wavelength: 1.55 μ).
m, fiber length 3 cm). This value is based on the polarization maintaining fiber with the same structure and the stress applying part as S io2 B203
(20 mol%), B is about 5 times more,
There was also a 20dB improvement in crosstalk. In addition, the loss value of this fiber is 0.20 dB/F at a wavelength of 1.56 μm.
a, and the loss was extremely low. This is AlP
This is thought to be because O4 does not particularly cause absorption loss.
さらに、第1図(a)、(b)の構造で、応力付与部を
コアガラスに接近させ、応力付与を大きくした偏波保持
ファイバを製造した結果、B=3゜0X10−3.クロ
ストーク−55dB(3触艮)の偏波保持ファイバが得
られた。この場合、直交する2つの偏波モードのうち一
方は伝播しなくなり、いわゆる単一偏波ファイバが実現
された。Furthermore, as a result of manufacturing a polarization-maintaining fiber with the structure shown in FIGS. 1(a) and 1(b) in which the stress-applying portion was brought closer to the core glass and the stress applied was increased, B=3°0X10-3. A polarization-maintaining fiber with a crosstalk of -55 dB (3 samples) was obtained. In this case, one of the two orthogonal polarization modes no longer propagates, resulting in a so-called single polarization fiber.
以上説明したように、本発明のガラス素材を使用した場
合、固化温度が高く、また屈折率も3i02とほぼ同程
度のため、偏波保持力に優れた偏波保持光ファイバを容
易に得られる利点がある。As explained above, when the glass material of the present invention is used, the solidification temperature is high and the refractive index is almost the same as 3i02, so it is possible to easily obtain a polarization-maintaining optical fiber with excellent polarization-maintaining power. There are advantages.
また、本発明のガラス素材は損失増の原因とならないた
め、低損失でかつ偏波保持力の高いファイバを容易に得
られる利点がある。Further, since the glass material of the present invention does not cause an increase in loss, it has the advantage that a fiber with low loss and high polarization holding power can be easily obtained.
したがって、本発明の偏波保持ファイバを光波通信、あ
るいはコヒーレント光通信9等の伝送媒体として十分に
使用できる利点があるほか、回転センサ、等各種計測用
としても優れた特性が期待できる。Therefore, the polarization maintaining fiber of the present invention has the advantage of being fully usable as a transmission medium for light wave communication or coherent optical communication 9, etc., and can also be expected to have excellent characteristics for various measurement applications such as rotation sensors.
第1図(a)および(b)はいずれも偏波保持光ファイ
バの構造を示す概略断面図、
第2図はAlPOa添加量と屈折率の関係を示すグラフ
、第3図はAj PO4添加量と熱膨張係数の関係を示
すグラフ、第4図はAlPOa添加量と同化温度の関係
を示すグラフである。
1・・・・・・コア部、2・・・・・・応力付与部、3
・・・・・・クラッド部。
C0)
(b)
fHa図Figures 1 (a) and (b) are both schematic cross-sectional views showing the structure of a polarization-maintaining optical fiber, Figure 2 is a graph showing the relationship between AlPOa doping amount and refractive index, and Figure 3 is Aj PO4 doping amount. FIG. 4 is a graph showing the relationship between the amount of AlPOa added and the assimilation temperature. 1...Core part, 2...Stress applying part, 3
・・・・・・Clad part. C0) (b) fHa diagram
Claims (1)
与部及びクラッド部よりなる偏波保持光ファイバにおい
て、 該応力付与部が5モル%以上のAlPO_4を含むSi
O_2ガラス素材よりなることを特徴とする偏波保持光
ファイバ。[Claims] A polarization-maintaining optical fiber comprising a core portion for propagating light, a stress applying portion applying stress to the core portion, and a cladding portion, wherein the stress applying portion is made of Si containing 5 mol% or more of AlPO_4.
A polarization-maintaining optical fiber characterized by being made of O_2 glass material.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60148014A JPH0623805B2 (en) | 1985-07-05 | 1985-07-05 | Polarization-maintaining optical fiber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60148014A JPH0623805B2 (en) | 1985-07-05 | 1985-07-05 | Polarization-maintaining optical fiber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS628105A true JPS628105A (en) | 1987-01-16 |
| JPH0623805B2 JPH0623805B2 (en) | 1994-03-30 |
Family
ID=15443176
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60148014A Expired - Lifetime JPH0623805B2 (en) | 1985-07-05 | 1985-07-05 | Polarization-maintaining optical fiber |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0623805B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4978377A (en) * | 1988-12-09 | 1990-12-18 | Alcatel N.V. | Method of assembling a fiber optic preform from discrete preformed elements |
| US7430353B2 (en) * | 2005-06-29 | 2008-09-30 | Fujikura Ltd. | Polarization-maintaining optical fiber and optical fiber gyro |
-
1985
- 1985-07-05 JP JP60148014A patent/JPH0623805B2/en not_active Expired - Lifetime
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4978377A (en) * | 1988-12-09 | 1990-12-18 | Alcatel N.V. | Method of assembling a fiber optic preform from discrete preformed elements |
| US7430353B2 (en) * | 2005-06-29 | 2008-09-30 | Fujikura Ltd. | Polarization-maintaining optical fiber and optical fiber gyro |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0623805B2 (en) | 1994-03-30 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |