JPS62272205A - Polarizing plane maintaining optical fiber - Google Patents
Polarizing plane maintaining optical fiberInfo
- Publication number
- JPS62272205A JPS62272205A JP61114826A JP11482686A JPS62272205A JP S62272205 A JPS62272205 A JP S62272205A JP 61114826 A JP61114826 A JP 61114826A JP 11482686 A JP11482686 A JP 11482686A JP S62272205 A JPS62272205 A JP S62272205A
- Authority
- JP
- Japan
- Prior art keywords
- axis direction
- refractive index
- optical fiber
- clad
- polarization
- 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
Links
- 239000013307 optical fiber Substances 0.000 title claims abstract description 24
- 230000010287 polarization Effects 0.000 claims abstract description 24
- 238000009826 distribution Methods 0.000 claims abstract description 10
- 238000005253 cladding Methods 0.000 claims description 22
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 abstract description 21
- 235000012239 silicon dioxide Nutrition 0.000 abstract description 17
- 239000011521 glass Substances 0.000 abstract description 15
- 229910052681 coesite Inorganic materials 0.000 abstract description 4
- 229910052906 cristobalite Inorganic materials 0.000 abstract description 4
- 239000000377 silicon dioxide Substances 0.000 abstract description 4
- 229910052682 stishovite Inorganic materials 0.000 abstract description 4
- 229910052905 tridymite Inorganic materials 0.000 abstract description 4
- 230000002093 peripheral effect Effects 0.000 abstract 2
- 238000010791 quenching Methods 0.000 abstract 2
- 230000000171 quenching effect Effects 0.000 abstract 2
- 239000010453 quartz Substances 0.000 description 13
- 239000000835 fiber Substances 0.000 description 12
- 230000008033 biological extinction Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 5
- 230000003287 optical effect Effects 0.000 description 5
- 230000005540 biological transmission Effects 0.000 description 4
- 230000008878 coupling Effects 0.000 description 4
- 238000010168 coupling process Methods 0.000 description 4
- 238000005859 coupling reaction Methods 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 3
- 238000004804 winding Methods 0.000 description 3
- 208000025174 PANDAS Diseases 0.000 description 2
- 208000021155 Paediatric autoimmune neuropsychiatric disorders associated with streptococcal infection Diseases 0.000 description 2
- 240000004718 Panda Species 0.000 description 2
- 235000016496 Panda oleosa Nutrition 0.000 description 2
- 238000005452 bending Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 238000004891 communication Methods 0.000 description 1
- 230000008602 contraction Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 239000006185 dispersion Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000000644 propagated effect Effects 0.000 description 1
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)
Abstract
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]
本発明は偏波面保存光ファイバに係り、特に消光比特性
の向上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 a polarization-maintaining optical fiber, and particularly to improvement of extinction ratio characteristics.
[従来の技術]
従来、偏波面保存光ファイバとしては第5図及び第6図
にそれぞれ示すような楕円ジャケット型ファイバやパン
ダ型ファイバが用いられていた。[Prior Art] Conventionally, elliptical jacket type fibers and panda type fibers as shown in FIGS. 5 and 6 have been used as polarization maintaining optical fibers.
楕円ジャケット型ファイバではクラッド51を内包する
楕円ジャケット52が、またパンダ型ファイバではクラ
ッド61を内包するサポート62内で且つクラッド61
の両側に設けられた応力付与部材63がそれぞれBある
いはPを添加したSio2ガラス等の大きな熱膨張係数
を有する材質から形成され、これによりコア53及び6
4に異方性の応力が加えられるように構成されている。In the elliptical jacket type fiber, the elliptical jacket 52 containing the cladding 51 is inside the support 62 containing the cladding 61 and in the panda type fiber.
The stress applying members 63 provided on both sides of the cores 53 and 6 are each made of a material having a large coefficient of thermal expansion, such as Sio2 glass added with B or P.
The structure is such that an anisotropic stress is applied to 4.
その結果、コア53及び64に複屈折性が生じ、2つの
直交偏波モード間にエネルギー結合が抑制されて一つの
偏波モードのみが伝播されるようになる。As a result, birefringence occurs in the cores 53 and 64, energy coupling between the two orthogonal polarization modes is suppressed, and only one polarization mode is propagated.
[発明が解決しようとする問題点]
しかしながら、一般に光ファイバを製造する際には長手
方向の屈折率変動や径変動の発生が避は難く、その結果
2つの直交偏波モード間にエネルギー結合が生じ、高い
消光比を1qることができなかった。従って、このよう
な偏波面保存光ファイバを高精度光計測システムに適用
するとシステムの機能低下を招いてしまう。[Problems to be Solved by the Invention] However, in general, when manufacturing optical fibers, it is difficult to avoid variations in the refractive index and diameter in the longitudinal direction, and as a result, energy coupling occurs between two orthogonal polarization modes. Therefore, it was not possible to obtain a high extinction ratio of 1q. Therefore, if such a polarization-maintaining optical fiber is applied to a high-precision optical measurement system, the functionality of the system will deteriorate.
そこで、直交偏波モード間にエネルギー結合を生じさせ
ない目的でファイバの複屈折率を大きくすると、今度は
偏波分散が大きくなり、一旦モード結合が発生した場合
には大きなパルス拡がりを生じるようになるので、特に
長距離伝送システムには適さなくなる。Therefore, if the birefringence of the fiber is increased in order to prevent energy coupling between orthogonal polarization modes, polarization dispersion will increase, and once mode coupling occurs, large pulse broadening will occur. This makes it particularly unsuitable for long-distance transmission systems.
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、消光比の優れた偏波面保存光ファイバを提供するこ
とにある。Thus, an object of the present invention is to solve the problems of the above-mentioned prior art and to provide a polarization-maintaining optical fiber with an excellent extinction ratio.
[問題点を解決するための手段]
本発明の偏波面保存光ファイバは上記目的を達成するた
めに、コアの外周部にこれを囲繞するようにクラッドが
設けられると共にクラッドの外周部にこれを囲繞するよ
うに楕円ジャケットが設けられている偏波面保存光ファ
イバにおいて、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、楕円の長軸方向では上記クラッドよ
り低く且つ短軸方向では上記クラッドより高い屈折率を
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 polarization-maintaining optical fiber of the present invention is provided with a cladding around the outer periphery of the core, and a cladding is provided on the outer periphery of the cladding. In a polarization maintaining optical fiber having a surrounding elliptical jacket, the refractive index distribution of the elliptical jacket is divided in the circumferential direction, and the refractive index distribution of the elliptical jacket is lower than the cladding in the major axis direction of the ellipse and above the cladding in the minor axis direction. It has a higher refractive index than the cladding.
[作 用]
以上のように楕円ジャケットの屈折率分布をその円周方
向に分割することにより、楕円ジャケットはコアに異方
性の応力を付与するのみでなく、2つの直交偏波モード
の伝播特性を直接具なったものとさせる機能を有するこ
とになる。[Function] By dividing the refractive index distribution of the elliptical jacket in the circumferential direction as described above, the elliptical jacket not only applies anisotropic stress to the core, but also suppresses the propagation of two orthogonal polarization modes. It has the function of directly realizing the characteristics.
具体的には楕円ジャケットの長軸方向においてはクラッ
ドより低く、短軸方向においてはクラッドより高い屈折
率を持たせることによって、長軸方向の偏波モードのカ
ットオフ波長は長く、短軸方向の偏波モードのカットオ
フ波長は短くなる。Specifically, by making the elliptical jacket have a refractive index lower than that of the cladding in the major axis direction and higher than that of the cladding in the minor axis direction, the cutoff wavelength of the polarization mode in the major axis direction is long, and the cutoff wavelength of the polarization mode in the minor axis direction is long. The cutoff wavelength of the polarization mode becomes shorter.
従って、この偏波面保存光ファイバに曲げを加えたりマ
イクルベンディングを生じさせれば、容易に絶対単一偏
波ファイバを構成することができる。Therefore, by bending or microbending this polarization maintaining optical fiber, an absolutely single polarization fiber can be easily constructed.
なお、コアに応力を加えて複屈折性を生じさせるために
楕円ジャケットの楕円率は10%以上とすることが好ま
しい。Note that the ellipticity of the elliptical jacket is preferably 10% or more in order to generate birefringence by applying stress to the core.
[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
に係る偏波面保存光ファイバの横断面図。FIGS. 1(a), 1(b), and 1(c) are cross-sectional views of a polarization-maintaining optical fiber according to an embodiment of the present invention, respectively.
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Geが添加された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5i(h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8203を添加した5i0
2ガラスからなり大きな熱膨張係数を有すると共にその
長軸方向(X軸方向)においてはB2O3の添加量が大
きく第1図(b)の如くクラッド2の屈折率noより低
い屈折率n1を有し、短軸方向(Y軸方向)においては
P2O5の添加量が大きく第1図(C)の如くクラッド
2の屈折* n oより高い屈折率n2を有している。They are a refractive index distribution diagram in the X-axis direction and a refractive index distribution diagram in the Y-axis direction. In the figure, reference numeral 1 denotes a core made of 5102 glass doped with Ge, and a cladding 2 made of pure 5i (h glass) is provided around the outer periphery of the core 1. An elliptical jacket 3 is provided around the outer periphery of the 5i0 to which P2O5 and 8203 are added.
2 glass has a large coefficient of thermal expansion, and in its major axis direction (X-axis direction), the amount of B2O3 added is large, and as shown in FIG. 1(b), it has a refractive index n1 lower than the refractive index no of the cladding 2. In the minor axis direction (Y-axis direction), the amount of P2O5 added is large, and as shown in FIG. 1(C), the refractive index n2 is higher than the refraction *no of the cladding 2.
さらに、この楕円ジャケット3の外周部にこれを囲I!
するように純粋5102ガラスからなるサポート4が設
けられている。Furthermore, this is enclosed on the outer periphery of this oval jacket 3!
A support 4 made of pure 5102 glass is provided to do so.
このような構成の偏波面保存光ファイバは次のようにし
て製造される。The polarization maintaining optical fiber having such a configuration is manufactured as follows.
まず、第2図に示すように石英管5の内面上にP2O5
−8202添加5i02ガラス層6をP2O5添加固を
大きくしてMCVD法により堆積させる。このとき、石
英管5は回転させないので図面の上下方向からのみ加熱
し石英管5の内面上部及び下部に堆積させる。First, as shown in FIG. 2, P2O5 is placed on the inner surface of the quartz tube 5.
-8202 doped 5i02 glass layer 6 is deposited by MCVD with increased P2O5 doping. At this time, since the quartz tube 5 is not rotated, the quartz tube 5 is heated only from the top and bottom directions in the drawing, and is deposited on the upper and lower inner surfaces of the quartz tube 5.
次に、石英管5をその円周方向に90”回転させてから
この石英管5内面の上部及び下部、すなわちまだ積層さ
れていない部分にP2O5−8203添加SiO2ガラ
ス層7を今度はB2O3添加はを大きくしてMCVD法
により堆積させる。この場合も石英管5は回転させず固
定したまま堆積を行なう。Next, the quartz tube 5 is rotated 90'' in the circumferential direction, and then a P2O5-8203-doped SiO2 glass layer 7 is applied to the upper and lower parts of the inner surface of the quartz tube 5, that is, the parts that have not yet been laminated. The quartz tube 5 is enlarged and deposited by the MCVD method.In this case as well, the quartz tube 5 is kept fixed without being rotated.
その侵、クラッド付きコアロッド(図示せず)をこの石
英管5内に挿入し、減圧しながら石英管5を収縮(カラ
ブス)させて、ガラス層7が長軸方向に、ガラスFIJ
6が短軸方向に位置する楕円ジャケット部を形成し、光
フアイバ母材を得る。そして、コア部の屈折率分布を測
定し、所望のカットオフ波長となるようにさらに石英管
をオーバージャケットするかあるいは線引外径を調整し
ながら光フアイバ化を行なった。To prevent this, a core rod with a cladding (not shown) is inserted into the quartz tube 5, and the quartz tube 5 is contracted (carabous) while reducing the pressure, so that the glass layer 7 is aligned in the longitudinal direction of the glass FIJ.
An elliptical jacket portion with 6 located in the minor axis direction is formed to obtain an optical fiber preform. Then, the refractive index distribution of the core portion was measured, and the quartz tube was further overjacketed or the outer diameter of the wire was adjusted to form an optical fiber so as to obtain the desired cutoff wavelength.
このようにして、コア1/クラツド2の屈折率差が0.
7%、楕円ジャケット3の長軸方向の屈折率がクラッド
2に対して−0,2%、短軸方向の屈折率がクラッド2
に対して+0.2%の偏波面保存光ファイバを製造した
。In this way, the refractive index difference between core 1 and cladding 2 is reduced to 0.
7%, the refractive index in the major axis direction of the elliptical jacket 3 is -0.2% with respect to the cladding 2, and the refractive index in the minor axis direction is the same as that of the cladding 2.
A polarization-maintaining optical fiber of +0.2% with respect to the above was manufactured.
この光ファイバのカットオフ波長を測定したところ、長
軸方向(X軸方向)の偏波モードでは1.15μs、短
軸方向(Y軸方向)の偏波モードでは1.0μsであっ
た。When the cutoff wavelength of this optical fiber was measured, it was 1.15 μs in the polarization mode in the long axis direction (X-axis direction) and 1.0 μs in the polarization mode in the short axis direction (Y-axis direction).
さらに、絶対単一偏波ファイバを構成するために、製造
された光ファイバを径30am+のコイル状に約100
m巻いてその光損失波長特性を測定したところ、第3図
のように波長1.3−帯において2つの直交偏波モード
間に大きな減衰量の差を生じ、−45dBの消光比特性
が得られた。すなわち、この波長帯で実質的に絶対単一
偏波伝送を行なうことが可能となった。Furthermore, in order to construct an absolutely single polarization fiber, the manufactured optical fiber was coiled into a coil with a diameter of 30 am+.
When we measured the optical loss wavelength characteristics after winding it with m windings, we found that there was a large difference in attenuation between the two orthogonal polarization modes in the 1.3-wavelength band, as shown in Figure 3, and an extinction ratio characteristic of -45 dB was obtained. It was done. In other words, it has become possible to perform substantially absolute single polarization transmission in this wavelength band.
なお、上記実施例では円形断面を有する石英管5の内面
にP2O5−8203添加5ithガラス層6及び7を
堆積した後、これらの収縮時にガラス層6及び7を楕円
断面形状に変化させたが、第4図に示すような楕円断面
を有する石英管15の内面にP2O5−8203添加5
i02ガラス層16及び17を堆積させてもよい。In the above example, after depositing the P2O5-8203-added 5ith glass layers 6 and 7 on the inner surface of the quartz tube 5 having a circular cross section, the glass layers 6 and 7 were changed into an elliptical cross-sectional shape when they were shrunk. P2O5-8203 is added to the inner surface of the quartz tube 15 having an elliptical cross section as shown in FIG.
i02 glass layers 16 and 17 may be deposited.
さらに、絶対単一偏波ファイバを構成する場合、上述し
たように本発明の偏波面保存光ファイバをコイル状に巻
り代わりに、ファイバの外周部にプラスチックの被覆を
施し、その収縮によるマイクロベンディングを利用する
こともできる。Furthermore, when constructing an absolutely single-polarized fiber, instead of winding the polarization-maintaining optical fiber of the present invention into a coil as described above, the outer periphery of the fiber is coated with plastic, and micro-bending is caused by the contraction of the fiber. You can also use
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。As explained above, according to the present invention, the following excellent effects are exhibited.
(1) 極めて高い消光比特性が得られ、実質的に絶
対単一偏波伝送を行なうことができる。(1) Extremely high extinction ratio characteristics can be obtained, and substantially absolute single polarization transmission can be performed.
(り 従って、本発明の偏波面保存光ファイバを偏波や
位相を利用する光通信システム及び光計測システム等に
適用することにより、システムの機能向上及び精度向上
を図ることが可能となる。また、長距離伝送システムに
も適したものである。(Thus, by applying the polarization-maintaining optical fiber of the present invention to optical communication systems, optical measurement systems, etc. that utilize polarization and phase, it is possible to improve the functionality and accuracy of the system. , it is also suitable for long-distance transmission systems.
第1図(a)〜(C)はそれぞれ本発明の一実施例に係
る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図は実施例のファイバの!lJ造方法を説明するた
めの断面図、第3図は実施例のファイバをコイル化した
ときの光損失波長特性図、第4図は他の実施例の製造方
法を示す断面図、第5図及び第6図はそれぞれ一般的な
偏波面保存光ファイバの横断面図である。
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. 1A to 1C are cross-sectional views of polarization-maintaining optical fibers according to embodiments of the present invention. A refractive index distribution diagram in the X-axis direction and a refractive index distribution diagram in the Y-axis direction,
Figure 2 shows the example fiber! A cross-sectional view for explaining the LJ manufacturing method, FIG. 3 is an optical loss wavelength characteristic diagram when the fiber of the example is coiled, FIG. 4 is a cross-sectional view showing the manufacturing method of another example, and FIG. and FIG. 6 are cross-sectional views of general polarization-maintaining optical fibers. In the figure, 1 is the core, 2 is the cladding, 3 is the oval jacket,
4 is support.
Claims (2)
設けられると共にクラッドの外周部にこれを囲繞するよ
うに楕円ジャケットが設けられている偏波面保存光ファ
イバにおいて、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、楕円の長軸方向では上記クラッドよ
り低く且つ短軸方向では上記クラッドより高い屈折率を
有するようにしたことを特徴とする偏波面保存光ファイ
バ。(1) In a polarization maintaining optical fiber in which a cladding is provided around the outer periphery of the core and an elliptical jacket is provided around the outer periphery of the cladding, the refractive index of the elliptical jacket is 1. A polarization-maintaining optical fiber characterized in that the distribution is divided in the circumferential direction of the ellipse, and the refractive index is lower than that of the cladding in the major axis direction of the ellipse and higher than that of the cladding in the minor axis direction.
ることを特徴とする特許請求の範囲第1項記載の偏波面
保存光ファイバ。(2) The polarization-maintaining optical fiber according to claim 1, wherein the elliptical jacket has an ellipticity of 10% or more.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61114826A JPS62272205A (en) | 1986-05-21 | 1986-05-21 | Polarizing plane maintaining optical fiber |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61114826A JPS62272205A (en) | 1986-05-21 | 1986-05-21 | Polarizing plane maintaining optical fiber |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62272205A true JPS62272205A (en) | 1987-11-26 |
Family
ID=14647654
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61114826A Pending JPS62272205A (en) | 1986-05-21 | 1986-05-21 | Polarizing plane maintaining optical fiber |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62272205A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0414369A2 (en) * | 1989-07-17 | 1991-02-27 | Minnesota Mining And Manufacturing Company | Single-mode, single-polarization optical fiber |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5915004B2 (en) * | 1981-12-18 | 1984-04-07 | 房雄 矢野 | "Ko" kneading device |
-
1986
- 1986-05-21 JP JP61114826A patent/JPS62272205A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5915004B2 (en) * | 1981-12-18 | 1984-04-07 | 房雄 矢野 | "Ko" kneading device |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0414369A2 (en) * | 1989-07-17 | 1991-02-27 | Minnesota Mining And Manufacturing Company | Single-mode, single-polarization optical fiber |
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