JPS62283303A - Absolute single polarizing plane maintaining optical fiber - Google Patents

Absolute single polarizing plane maintaining optical fiber

Info

Publication number
JPS62283303A
JPS62283303A JP61124663A JP12466386A JPS62283303A JP S62283303 A JPS62283303 A JP S62283303A JP 61124663 A JP61124663 A JP 61124663A JP 12466386 A JP12466386 A JP 12466386A JP S62283303 A JPS62283303 A JP S62283303A
Authority
JP
Japan
Prior art keywords
refractive index
axis direction
optical fiber
cladding
jacket
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.)
Pending
Application number
JP61124663A
Other languages
Japanese (ja)
Inventor
Takeyoshi Takuma
詫摩 勇悦
Hiroshi Kajioka
博 梶岡
Tatsuya Kumagai
達也 熊谷
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.)
Hitachi Cable Ltd
Original Assignee
Hitachi Cable 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 Hitachi Cable Ltd filed Critical Hitachi Cable Ltd
Priority to JP61124663A priority Critical patent/JPS62283303A/en
Publication of JPS62283303A publication Critical patent/JPS62283303A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/105Light 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)

Abstract

PURPOSE:To provide the titled optical fiber which exhibits the absolute single polarizing plane maintaining characteristic even if the fiber is not bent by using a support having the refractive index equal to the refractive index of a clad and determining the refractive index distribution of an elliptical jacket in such a manner that the refractive index is equal in the minor axis direction and has the low refractive index in the major axis direction. CONSTITUTION:The elliptical jacket 3 consists of SiO2 glass added with P2O5 and B2O3 and has a large coefft. of thermal expansion. The amt. of the B2O3 to be added is large in the major axis direction (X-axis direction) thereof and the jacket has the refractive index n1 lower than the refractive index n0 of the clad 2 in said direction. The jacket has the refractive index n0 equal to the refractive index of the clad 2 in the minor axis (Y-axis direction). The fiber exhibiting the absolute single polarizing plane maintaining characteristic to propagate only the polarization mode in the single direction is thus obtd. even if the fiber is not bent.

Description

【発明の詳細な説明】 3、発明の詳細な説明 [産業上の利用分野] 本発明は絶対単一偏波面保存光ファイバに係り、特に曲
げを必要とせずに絶対単一偏波面保存特性を示す楕円ジ
ャケット型ファイバに関するものである。
[Detailed Description of the Invention] 3. Detailed Description of the Invention [Field of Industrial Application] The present invention relates to an absolutely single polarization maintaining optical fiber, which has absolute single polarization maintaining characteristics without particularly requiring bending. The present invention relates to an elliptical jacket type fiber shown in FIG.

[従来の技術] 従来の絶対単一偏波面保存光ファイバでは一般に直交す
る2つの偏波モードの曲げ損失特性に差を持たせ、一方
の偏波モードのみを減衰させていた。すなわち、2つの
偏波モードにそれぞれ異なるカットオフ波長を設定した
偏波面保存光ファイバを直径数cmでコイル状に巻回し
、一方の偏波モードの曲げ損失を数10dB/−程度、
他方の偏波モードの曲げ損失を数dB/lk以下として
実質的に一つの偏波モードのみが伝播されるようにして
いた。
[Prior Art] In a conventional absolutely single polarization maintaining optical fiber, the bending loss characteristics of two orthogonal polarization modes are generally made different, and only one polarization mode is attenuated. That is, a polarization-maintaining optical fiber with different cutoff wavelengths set for two polarization modes is wound into a coil with a diameter of several centimeters, and the bending loss of one polarization mode is approximately several tens of dB/-.
The bending loss of the other polarization mode is set to several dB/lk or less so that substantially only one polarization mode is propagated.

[発明が解決しようとする問題点1 従って、この種の絶対単一偏波面保存光ファイバは主に
コイル型の光フアイバ偏光子としては用いられたが、次
のような問題点を有していた。
[Problem to be solved by the invention 1 Therefore, although this type of absolutely single polarization maintaining optical fiber has been mainly used as a coil type optical fiber polarizer, it has the following problems. Ta.

■ 各偏波モードに所定の曲げ損失を与えるための曲げ
半径はこれら偏波モードのカットオフ波長の差により決
定されるので、小型のコイル型偏光子を得ようとすると
それに適した光ファイバを用意しなければならず、歩留
りが悪い。
■ The bending radius to give a predetermined bending loss to each polarization mode is determined by the difference in the cutoff wavelengths of these polarization modes, so if you are trying to obtain a small coil-type polarizer, you need to select an optical fiber suitable for it. It has to be prepared and the yield is poor.

■ 一定の曲げを印加する必要があるので長尺の絶対単
一偏波面保存光ファイバを実現することが不可能であり
、その結果コヒーレント通信用として用いることができ
ない。
■ Since it is necessary to apply a certain bending force, it is impossible to realize a long absolutely single polarization maintaining optical fiber, and as a result, it cannot be used for coherent communications.

■ カットオフ波長の差が大きな光ファイバを用いるこ
とが望ましいが、このような光ファイバを製造する際の
歩留りが悪い。
(2) It is desirable to use optical fibers with a large difference in cutoff wavelength, but the yield when manufacturing such optical fibers is poor.

かくして、本発明の目的は上記従来技術の問題点を解消
し、曲げを印加しなくても絶対単一偏波面保存特性を示
す絶対単一偏波面保存光ファイバを提供することにある
SUMMARY OF THE INVENTION Thus, an object of the present invention is to solve the above-mentioned problems of the prior art and to provide an absolutely single polarization maintaining optical fiber that exhibits an absolutely single polarization maintaining characteristic without applying bending.

[問題点を解決するための手段] 本発明の絶対単一偏波面保存光ファイバは上記目的を達
成するために、コアを中心としてその外周部に順次クラ
ッド、楕円ジャケット及びサボーl−が設(プられてい
る4層構造の偏波面保存光ファイバにおいて、上記サポ
ートが上記クラッドと等しい屈折率を有すると共に上記
楕円ジャケットの屈折率分布をその円周方向に分割して
楕円の短軸方向では上記クラッドと等しく且つ長軸方向
では上記クラッドより低い屈折率を有するようにしたも
のである。
[Means for Solving the Problems] In order to achieve the above object, the absolutely single polarization maintaining optical fiber of the present invention has a cladding, an elliptical jacket, and a sabot l- arranged in sequence around the core and around the outer periphery. In a polarization-maintaining optical fiber with a four-layer structure, the support has a refractive index equal to that of the cladding, and the refractive index distribution of the elliptical jacket is divided in the circumferential direction, so that in the short axis direction of the ellipse, the support has a refractive index equal to that of the cladding. It has a refractive index equal to that of the cladding and lower than that of the cladding in the major axis direction.

[作 用コ 以上のような構成とすることにより、楕円の長軸方向で
はW型の屈折率分布が、短軸方向ではMC(マツチド 
クラッド)型の屈折率分布がそれぞれ形成される。
[Function] With the above configuration, a W-shaped refractive index distribution is created in the long axis direction of the ellipse, and an MC (matshidden) refractive index distribution is created in the short axis direction of the ellipse.
A cladding type refractive index distribution is formed respectively.

一般に、W型の屈折率分布を有する光ファイバでは基本
モードにカットオフ波長が存在し、一方MC型の屈折率
分布を有する光ファイバでは基本モードにカットオフ波
長が存在しないことが知られている。
Generally, it is known that an optical fiber with a W-shaped refractive index distribution has a cutoff wavelength in its fundamental mode, whereas an optical fiber with an MC-shaped refractive index distribution has no cutoff wavelength in its fundamental mode. .

従って、本発明のファイバにおいてはその基本モードに
楕円の長軸方向ではカットオフ波長が存在し、短軸方向
では存在しないことになる。すなわち、短軸方向の偏波
モードのみを伝播する絶対単一偏波領域が存在する。
Therefore, in the fiber of the present invention, the fundamental mode has a cutoff wavelength in the long axis direction of the ellipse, but does not exist in the short axis direction. That is, there is an absolutely single polarization region in which only the polarization mode in the short axis direction is propagated.

[実施例] 以下、本発明の実施例を添付図面に従って説明する。[Example] Embodiments of the present invention will be described below with reference to the accompanying drawings.

第1図(a>(b)(c)はそれぞれ本発明の一実施例
に係る絶対単一偏波面保存光ファイバの横断面図、X軸
方向の屈折率分布図及びY軸方向の屈折率分布図である
。図中、1はGeS添加された5102ガラスからなる
コアであり、このコア1の外周部にこれを囲繞するよう
に純粋5i02ガラスからなるクラッド2が設けられて
いる。さらに、クラッド2の外周部にこれを囲繞するよ
うに楕円ジャケット3が設けられている。この楕円ジャ
ケット3はP2O5及びB2O3を添加した5102ガ
ラスからなり大きな熱膨張係数を有すると共にその長軸
力゛向(X軸方向)においてはB2O3の添加口が大き
く第1図(b)の如くクラッド2の屈折率n。
FIG. 1 (a>(b) and (c) are a cross-sectional view, a refractive index distribution diagram in the X-axis direction, and a refractive index in the Y-axis direction, respectively, of an absolutely single polarization maintaining optical fiber according to an embodiment of the present invention. It is a distribution diagram. In the figure, 1 is a core made of 5102 glass doped with GeS, and a cladding 2 made of pure 5i02 glass is provided on the outer periphery of this core 1 so as to surround it.Furthermore, An elliptical jacket 3 is provided on the outer periphery of the cladding 2 so as to surround it.The elliptical jacket 3 is made of 5102 glass added with P2O5 and B2O3 and has a large coefficient of thermal expansion and has a large thermal expansion coefficient ( In the X-axis direction), the B2O3 doping port is large and the refractive index of the cladding 2 is n, as shown in FIG. 1(b).

より低い屈折率n1を右し、短軸方向(Y軸方向)にお
いては第1図(C)の如くクラッド2と等しい屈折率n
oを有している。
In the short axis direction (Y-axis direction), the refractive index n is equal to that of the cladding 2 as shown in FIG. 1(C).
It has o.

さらに、この楕円ジャケット3の外周部にこれを囲繞す
るように純粋SiO2ガラスからなりクラッド2と等し
い屈折率noを有するサポート4が設けられている。
Further, a support 4 made of pure SiO2 glass and having a refractive index no equal to that of the cladding 2 is provided at the outer circumference of the elliptical jacket 3 so as to surround it.

次に、本実施例の作用を述べる。Next, the operation of this embodiment will be described.

まず、X軸方向は第1図(b)のようにW型の屈折率分
布を有している。ここでコア1とクラッド2の階段状屈
折率分布をこれと等価的なステップ型分布(ESI)に
買ぎ換え、この681分布と楕円ジャケット3及びサポ
ート4から構成されるW型ファイバのU−■特性を第2
図に示す。Uは等価的なコア内における正規化横方向位
相定数でこのW型ファイバの固有方程式を解くことによ
り得られ、■は等価的なコアと楕円ジャケット3から決
定される正規化周波数である。
First, the X-axis direction has a W-shaped refractive index distribution as shown in FIG. 1(b). Here, the stepped refractive index distribution of the core 1 and cladding 2 is replaced with an equivalent stepped index distribution (ESI), and the U- ■Second characteristics
As shown in the figure. U is obtained by solving the characteristic equation of this W-shaped fiber with the normalized transverse phase constant in the equivalent core, and ■ is the normalized frequency determined from the equivalent core and elliptical jacket 3.

なお、上記の681分布におけるコア半径a。Note that the core radius a in the above 681 distribution.

及び比屈折率差Δ。はコア1とクラッド2の階段状屈折
率分布をF (r)としたとぎそれぞれ以下の(1)式
及び(2)式により表わされる。
and relative refractive index difference Δ. are expressed by the following equations (1) and (2), respectively, where F (r) is the stepped refractive index distribution of the core 1 and the cladding 2.

Δ8=(Δや+△−) 5: F (r) dr/ a
 o−tz)ただし、Δや及びΔ−はそれぞれコア1と
クラッド2の比屈折率差、クラッド2と楕円ジャケット
3の比屈折率差を示している。
Δ8=(Δ or +Δ-) 5: F (r) dr/a
o-tz) However, Δ, and Δ- indicate the relative refractive index difference between the core 1 and the cladding 2, and the relative refractive index difference between the cladding 2 and the elliptical jacket 3, respectively.

さらに、plはU=■の関係を、p2はU=V[(Δ 
−Δ−)/Δ ]“4の関係をそれぞれ示ee す直線であり、この直線j2とLPo1モード及びLP
11モードの各特性曲線との交点P及びQのV値V1及
びV2の間の領域が単一モード動作域となる。そして、
正規化周波数■がこの■1以下の領域では漏洩波モード
で高損失となり、■2以上の領域では多モード動作域と
なる。
Furthermore, pl represents the relationship U=■, and p2 represents the relationship U=V[(Δ
−Δ−)/Δ ] “4, and this straight line j2 and LPo1 mode and LP
The region between the V values V1 and V2 of the intersection points P and Q with the respective characteristic curves of the 11 modes becomes a single mode operating region. and,
In the region where the normalized frequency (2) is less than or equal to (1), high loss occurs in the leaky wave mode, and in the region (2 or more), the normalized frequency is in the multimode operating region.

一方、Y軸方向は第1図(C)のようにMC型の屈折率
分布を有しており、この方向では一般に知られるように
基本モードのカットオフ波長が存在せず、正規化周波数
Vが2.405以下の範囲において単一モード伝播が行
なわれる。
On the other hand, the Y-axis direction has an MC-type refractive index distribution as shown in FIG. Single mode propagation occurs in the range where is 2.405 or less.

従って、正規化周波数Vがv1以下で且、つ2、405
以下の範囲に動作■値■3を設定すれば、X軸方向の偏
波モードは漏洩波モードで高損失となり、Y軸方向の偏
波モードは導波モードで低損失となる。すなわち、Y軸
方向の偏波モードのみを伝播する絶対単一偏波面保存光
ファイバが実現される。
Therefore, if the normalized frequency V is less than or equal to v1, and 2,405
If the operating value ■3 is set in the following range, the polarization mode in the X-axis direction is a leaky wave mode and has high loss, and the polarization mode in the Y-axis direction is a guided mode and has low loss. In other words, an absolutely single polarization-maintaining optical fiber that propagates only the polarization mode in the Y-axis direction is realized.

なお、X@力方向偏波した漏洩波モードの減衰定数は等
価的なコアの屈折率、楕円ジャケット3の屈折率及び長
軸径により任意に設計することができる。
Note that the attenuation constant of the leaky wave mode polarized in the X@force direction can be arbitrarily designed based on the equivalent refractive index of the core, the refractive index of the elliptical jacket 3, and the major axis diameter.

[発明の効果] 以上説明したように本発明によれば、次の如き優れた効
果を発揮する。
[Effects of the Invention] As explained above, according to the present invention, the following excellent effects are exhibited.

(1)  曲げを印加しなくても単一方向の偏波モード
のみを伝播する絶対単一偏波面保存特性を示すファイバ
が実現される。
(1) A fiber exhibiting absolute single polarization preserving characteristics that propagates only a polarization mode in a single direction without applying bending can be realized.

(2)  短尺で用いれば、光ファイバとの接続が容易
であると共に小型で信頼性の高い光フアイバ型偏光子を
構成することができる。
(2) When used in a short length, it is possible to construct an optical fiber type polarizer that is easy to connect to an optical fiber, and is small and highly reliable.

(3)  長尺で用いれば、コヒーレント通信用伝送路
として利用でき、伝送可能な情報ωの飛躍的な増大化を
達成することができる。
(3) If a long length is used, it can be used as a transmission path for coherent communication, and the amount of information ω that can be transmitted can be dramatically increased.

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

第1図(a)〜(C)はそれぞれ本発明の一実施例に係
る絶対単一偏波面保存光ファイバの横断面図、X軸方向
の屈折率分布図及びY軸方向の屈折率分布図、第2図は
実施例のX軸方向のU−■特性を示す特性図である。 図中、1はコア、2はクラッド、3は楕円ジャケット、
4はサポートである。
FIGS. 1(a) to (C) are a cross-sectional view, a refractive index distribution diagram in the X-axis direction, and a refractive index distribution diagram in the Y-axis direction, respectively, of an absolutely single polarization-maintaining optical fiber according to an embodiment of the present invention. , FIG. 2 is a characteristic diagram showing the U-■ characteristic in the X-axis direction of the example. In the figure, 1 is the core, 2 is the cladding, 3 is the oval jacket,
4 is support.

Claims (1)

【特許請求の範囲】[Claims] コアを中心としてその外周部に順次クラッド、楕円ジャ
ケット及びサポートが設けられている4層構造の偏波面
保存光ファイバにおいて、上記サポートが上記クラッド
と等しい屈折率を有すると共に上記楕円ジャケットの屈
折率分布をその円周方向に分割して楕円の短軸方向では
上記クラッドと等しく且つ長軸方向では上記クラッドよ
り低い屈折率を有するようにしたことを特徴とする絶対
単一偏波面保存光ファイバ。
In a polarization-maintaining optical fiber having a four-layer structure in which a cladding, an elliptical jacket, and a support are sequentially provided on the outer periphery of a core, the support has a refractive index equal to that of the cladding, and the elliptical jacket has a refractive index distribution. An absolutely single polarization-maintaining optical fiber characterized in that it has a refractive index equal to that of the cladding in the short axis direction of the ellipse and lower than that of the cladding in the long axis direction by dividing the ellipse in the circumferential direction.
JP61124663A 1986-05-31 1986-05-31 Absolute single polarizing plane maintaining optical fiber Pending JPS62283303A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61124663A JPS62283303A (en) 1986-05-31 1986-05-31 Absolute single polarizing plane maintaining optical fiber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61124663A JPS62283303A (en) 1986-05-31 1986-05-31 Absolute single polarizing plane maintaining optical fiber

Publications (1)

Publication Number Publication Date
JPS62283303A true JPS62283303A (en) 1987-12-09

Family

ID=14890974

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61124663A Pending JPS62283303A (en) 1986-05-31 1986-05-31 Absolute single polarizing plane maintaining optical fiber

Country Status (1)

Country Link
JP (1) JPS62283303A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5915004B2 (en) * 1981-12-18 1984-04-07 房雄 矢野 "Ko" kneading device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5915004B2 (en) * 1981-12-18 1984-04-07 房雄 矢野 "Ko" kneading device

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