JPS5834405A - Polarization preserving optical fiber - Google Patents
Polarization preserving optical fiberInfo
- Publication number
- JPS5834405A JPS5834405A JP56133741A JP13374181A JPS5834405A JP S5834405 A JPS5834405 A JP S5834405A JP 56133741 A JP56133741 A JP 56133741A JP 13374181 A JP13374181 A JP 13374181A JP S5834405 A JPS5834405 A JP S5834405A
- Authority
- JP
- Japan
- Prior art keywords
- glass
- core
- rod
- thermal expansion
- 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.)
- Pending
Links
Abstract
Description
【発明の詳細な説明】
本発明は光通信、光センサ等で用いられる偏光保存光フ
ァイバに関ずろものである。偏光を保存したまま光を導
波する光ファイバは、光ヘテロダイン通信、フ・Tイバ
ジャイロ、圧カセンザ等に使用される将来性の高い光伝
送路である。従来開発されてきた偏光保存光ファイバは
、コア形を楕円形にし、かつ、クラッド層も楕円形にし
、コアに加わる応力を光フアイバ断面内の2力向(以後
X方向とX方向ど呼ぶ)で異フJ、るようにし、コアガ
ラスに複屈折性を持たせろことによって行l工っ゛〔い
た。コアを(イイ円形にする方j去は、ファイバとレー
ザとの結合やファイバ同士の結合損失の増大を招き、し
かも本方法は偏光保イr性を高める効果が低く、偏光保
存光ファイバを得る方法としては得策ではない。クジッ
ドム5を7隋円形にし、コアに加わる応力なX方向とX
方向で異なるようにする方法は、コアを円形にするため
、ファイバとt/−ヂとの結合やファイバ同士の結合損
失は増大せず、かつ偏光保存性を高める効果は高いが、
X方向とX方向で大きな応力差を発生させるために、コ
アとクラッド層間に大ぎな熱膨張係截の差を設けた、け
ればならない。大きな熱膨張係数の差を設けるためには
、コアに大量のゲルマニウムやリン等のドーパントを混
入させる必要があり、散乱損失が増加する問題があった
。したがって、本発明の目的は、レーザとの結合やファ
イバ同士の結合損失が増大ぜず、かつ散乱損失が小さい
偏光保存光ファイバを提供することにある。本発明の溝
或は、ガラス棒の両側に、前記ガラス棒より熱膨張係数
の大きい2本のガラス棒が前記ガラス棒と平行に接し、
かつ前記3本のガラス棒がガラス管によって被覆されて
いることを特徴とする偏光保存光ファイバである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a polarization-maintaining optical fiber used in optical communications, optical sensors, and the like. Optical fibers that guide light while preserving polarization are promising optical transmission lines for use in optical heterodyne communications, fiber optic gyros, pressure sensors, and the like. Conventionally developed polarization-maintaining optical fibers have an elliptical core and an elliptical cladding layer, and the stress applied to the core is distributed in two directions (hereinafter referred to as the X direction and the X direction) within the cross section of the optical fiber. Therefore, they were able to achieve this by making the core glass have birefringence. Making the core circular causes an increase in the coupling loss between the fiber and the laser and the coupling loss between the fibers, and this method is less effective in improving polarization preservation, making it difficult to obtain a polarization preservation optical fiber. It is not a good idea as a method.The Kuzidom 5 is made into a 7-circular shape, and the stress applied to the core is
The method of making the core different in direction does not increase the coupling loss between the fiber and t/-d or the coupling loss between the fibers, and is highly effective in improving polarization preservation, since the core is made circular.
In order to generate a large stress difference between the X direction and the X direction, a large difference in thermal expansion coefficient must be provided between the core and the cladding layer. In order to provide a large difference in thermal expansion coefficient, it is necessary to mix a large amount of dopant such as germanium or phosphorus into the core, which poses the problem of increased scattering loss. Therefore, an object of the present invention is to provide a polarization-maintaining optical fiber that does not increase coupling loss with a laser or fiber-to-fiber coupling and has low scattering loss. In the groove of the present invention, on both sides of the glass rod, two glass rods having a larger coefficient of thermal expansion than the glass rod are in contact with the glass rod in parallel,
The polarization-maintaining optical fiber is characterized in that the three glass rods are covered with a glass tube.
次に図面を用いて本発明を実施例により説明する。Next, the present invention will be explained by examples using the drawings.
@1図(alは本発明の一実施例を説明する図であり、
これは光ファイバの中心軸に対し垂直な面に1・5ける
本実施例の断面形状を示し、11はコア、12はクラッ
ド層、13は高熱膨張係数ガラス棒、14はガラス被覆
、15は空隙、16は対称軸Xであり、第1図の(1)
)は第1図の(a)に示された光ファイバの対称軸16
上での屈折率分布を示し、21はコア、22は高熱膨張
係数ガラス棒、23はガラス被覆、24は中心線、25
は屈折率を示す縦i11+、26は径方向を示す横軸で
ある。本実施例では、コア11に酸化ゲルマニウムを約
1チ含む石英ガラス、クラッド層12に創イ詐石英ガラ
ス、高熱膨張係数ガラス棒13に酸化硼素を約5チ含む
石英ガラスを使用した。これらのガラス棒な第1図の(
a)に示すように、3本沿わせ接している部分を融着し
、さらにガラス被覆14を被覆する。この場合、空隙1
5が保たれるように、ガラス被覆14の管内圧を外圧に
対し10順水柱圧程度高め19000程度に加熱する。@Figure 1 (al is a diagram explaining one embodiment of the present invention,
This shows the cross-sectional shape of this example at 1.5 in a plane perpendicular to the central axis of the optical fiber, where 11 is a core, 12 is a cladding layer, 13 is a high thermal expansion coefficient glass rod, 14 is a glass coating, and 15 is a The air gap 16 is the axis of symmetry X, which is (1) in Figure 1.
) is the axis of symmetry 16 of the optical fiber shown in FIG.
The refractive index distribution above is shown, 21 is the core, 22 is a high thermal expansion coefficient glass rod, 23 is a glass coating, 24 is a center line, 25
is the vertical axis i11+ indicating the refractive index, and 26 is the horizontal axis indicating the radial direction. In this embodiment, the core 11 was made of quartz glass containing about 1 tem of germanium oxide, the cladding layer 12 was made of fused silica glass, and the high coefficient of thermal expansion glass rod 13 was made of quartz glass containing about 5 oz. of boron oxide. These glass rods are shown in Figure 1 (
As shown in a), the parts where the three wires are in contact with each other are fused and then covered with a glass coating 14. In this case, void 1
The internal pressure of the glass coating 14 is raised by about 10 water column pressure to about 19,000, so that the pressure within the tube of the glass coating 14 is maintained at about 19,000.
すると高熱膨張係数ガラス棒13は高温状態から常温に
冷却する際に強く収縮し、コアガラス11は対称軸】6
のX方向に張力を受けるが、対称軸16と直角のX方向
には空隙15があるために張力を受けない。このためコ
アガラス11は光弾性効果により対称軸116のX方向
の屈折率が対称軸16と直角なX方向の屈折率より小さ
くなり、複屈折性ガラスになる。上記複屈折性により、
偏光保存性ファイバが得られる。本実施例では、コアは
円形に保たれてもかかわらずコア11に含有される酸化
ゲルマニウム、濃度が約1チと低いため、散乱損失が小
さい偏光保存性光ファイバが得られる。上記実施例にお
いて、ガラス材料として石英系ガラスを使用したが多成
分ガラスを用いても良い。Then, the high coefficient of thermal expansion glass rod 13 contracts strongly when it is cooled from a high temperature state to room temperature, and the core glass 11 has an axis of symmetry]6
However, since there is a gap 15 in the X direction perpendicular to the axis of symmetry 16, no tension is applied. Therefore, the refractive index of the core glass 11 in the X direction of the axis of symmetry 116 becomes smaller than the refractive index in the X direction perpendicular to the axis of symmetry 16 due to the photoelastic effect, and the core glass 11 becomes birefringent glass. Due to the above birefringence,
A polarization preserving fiber is obtained. In this example, although the core is kept circular, the germanium oxide concentration contained in the core 11 is as low as about 1,000 nm, so that a polarization-maintaining optical fiber with low scattering loss can be obtained. In the above embodiments, silica-based glass was used as the glass material, but multi-component glass may also be used.
上記実施例においては、コアガラス棒11、高熱膨張係
数ガラス棒とも円柱の形状であったが、その断面形状は
角形でも良い。以上説明したように、本発明によれば、
コアが円形に保たれているため、レーザとの結合や光フ
アイバ同士の結合損失が増大せず、また大きな複屈折性
が得られるにもかかわらずコアの純度が比較的高いため
、散乱損失が小さい偏光保存光ファイバが得られる。In the above embodiment, both the core glass rod 11 and the high thermal expansion coefficient glass rod have a cylindrical shape, but their cross-sectional shape may be rectangular. As explained above, according to the present invention,
Because the core is kept circular, coupling losses with the laser and between optical fibers do not increase, and despite the large birefringence, the relatively high purity of the core reduces scattering losses. A small polarization-maintaining optical fiber is obtained.
第1図は本発明の一実施例を説明する図であり、図の(
a)は光ファイバの断面形状を示す図、図の(b)は(
a)の対称軸X方向の屈折率分布を示す図である。
な寸6図面1で使用した符号はそれぞれ以下のものを示
す。
11・・・・・・二fア、12・・・・・・クラッド層
、13・・・・・・ 5−
高熱膨張係数ガラス棒、14・・・・・・ガラス被覆、
15・・・・・・空隙、16・・・・・・対称軸、21
・・・・・・コア、22・・・・・・高熱膨fBk係数
ガシス棒、23・・・・・・ガラス被層、24・・・・
・・中心線、25・・・・・・屈折率を表わす縦軸、2
6・・・・・・径方向を表わす横++i+1゜G−FIG. 1 is a diagram illustrating an embodiment of the present invention.
(a) is a diagram showing the cross-sectional shape of the optical fiber, (b) is (
It is a figure which shows the refractive index distribution of the symmetry axis X direction of a). 6. The symbols used in Drawing 1 indicate the following. 11... 2f a, 12... cladding layer, 13... 5- high thermal expansion coefficient glass rod, 14... glass coating,
15...Gap, 16...Axis of symmetry, 21
... Core, 22 ... High thermal expansion fBk coefficient gasis rod, 23 ... Glass coating, 24 ...
...Center line, 25...Vertical axis representing refractive index, 2
6... Horizontal direction representing radial direction++i+1°G-
Claims (1)
ガラス棒の両側に、前記ガラス棒より熱膨張係数の大き
い2本のガラス棒が前記ガラス棒と平行に接1−1かつ
前記3本のガラス棒がガラス管によって被覆されている
ことを特徴とする偏光保存光ファイバ。In optical fibers that guide light while preserving polarization,
Two glass rods having a larger coefficient of thermal expansion than the glass rod are connected in parallel to the glass rod on both sides of the glass rod 1-1, and the three glass rods are covered with a glass tube. polarization preserving optical fiber.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56133741A JPS5834405A (en) | 1981-08-26 | 1981-08-26 | Polarization preserving optical fiber |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56133741A JPS5834405A (en) | 1981-08-26 | 1981-08-26 | Polarization preserving optical fiber |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5834405A true JPS5834405A (en) | 1983-02-28 |
Family
ID=15111831
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP56133741A Pending JPS5834405A (en) | 1981-08-26 | 1981-08-26 | Polarization preserving optical fiber |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5834405A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0543208A (en) * | 1991-08-16 | 1993-02-23 | Agency Of Ind Science & Technol | Continuous production of fibrous silicon compound |
US5318761A (en) * | 1991-07-18 | 1994-06-07 | Sumitomo Metal Industries, Ltd. | Process for preparing silicon carbide powder for use in semiconductor equipment |
-
1981
- 1981-08-26 JP JP56133741A patent/JPS5834405A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5318761A (en) * | 1991-07-18 | 1994-06-07 | Sumitomo Metal Industries, Ltd. | Process for preparing silicon carbide powder for use in semiconductor equipment |
JPH0543208A (en) * | 1991-08-16 | 1993-02-23 | Agency Of Ind Science & Technol | Continuous production of fibrous silicon compound |
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