JPS6131842B2 - - Google Patents
Info
- Publication number
- JPS6131842B2 JPS6131842B2 JP53100744A JP10074478A JPS6131842B2 JP S6131842 B2 JPS6131842 B2 JP S6131842B2 JP 53100744 A JP53100744 A JP 53100744A JP 10074478 A JP10074478 A JP 10074478A JP S6131842 B2 JPS6131842 B2 JP S6131842B2
- Authority
- JP
- Japan
- Prior art keywords
- optical
- light beam
- dimensional
- optical fiber
- curved surfaces
- 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
Links
Landscapes
- Optical Couplings Of Light Guides (AREA)
Description
【発明の詳細な説明】
この発明は光フアイバ通信用光回路、特に1本
の光フアイバからの光ビームを複数の光フアイバ
へ分配するための光分配器に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical circuit for optical fiber communication, and more particularly to an optical splitter for distributing a light beam from one optical fiber to a plurality of optical fibers.
光フアイバ通信は適用領域の広い将来性の高い
伝送システムとして期待され、実用化のための開
発が進められている。光フアイバ通信の有効な適
用領域のひとつに、工場、プラント内等の通信回
線やコンピユータ間をつなぐ通信回線等がある。
これらの回線においては中央の制御部から数多く
の端末機器へ信号を送ることが多い。したがつて
これらの回線に光フアイバ通信を適用するため
に、1本の光フアイバからの光ビームを多数の光
フアイバへ分岐する光分配器が必要になる。従来
このような機能を実現するために、複数の光フア
イバを束ねて加熱延引し、テーパ状の結合部を形
成したものがあるが、この方法は寸法の小さな光
フアイバの加工をともなうので、要求される加工
精度が厳しく、多数の光フアイバへの分配比を等
しくしたり、任意の比率に設定したりすることが
かなり困難で製作が難しいという欠点が避けがた
かつた。一方、この欠点を除去するために、一方
向にのみ2乗関数で近似される屈折率分布をつけ
た1次元集束性光伝送体と複数の曲面を組み合わ
せて、1次元集束性光伝送体の集束方向と直角な
方向にひろがつた光ビームを、この方向に集束作
用を持つように配置された複数の曲面により分割
集束する光分配器が考案されているが、この光分
配器は曲面での光の屈折を利用しているために曲
面が露出する構造をとらざるを得ず、ほこりや湿
気や汚れ等による特性劣化が生じやすく、信頼性
の点に問題があつた。 Optical fiber communication is expected to be a promising transmission system with a wide range of applications, and development for practical use is progressing. One of the effective application areas of optical fiber communication is communication lines within factories, plants, etc., and communication lines connecting computers.
In these lines, signals are often sent from a central control unit to a large number of terminal devices. Therefore, in order to apply optical fiber communication to these lines, an optical splitter that branches a light beam from one optical fiber into multiple optical fibers is required. Conventionally, in order to achieve this function, multiple optical fibers were bundled and heated and drawn to form a tapered joint, but this method involved processing small-sized optical fibers, so it did not meet the requirements. The processing precision required is very strict, and it is quite difficult to equalize or set the distribution ratio to a large number of optical fibers at an arbitrary ratio, making it difficult to manufacture. On the other hand, in order to eliminate this drawback, a one-dimensional convergent optical transmitter with a refractive index distribution approximated by a square function in only one direction and a plurality of curved surfaces are combined to create a one-dimensional convergent optical transmitter. An optical splitter has been devised that splits and focuses a light beam that spreads in a direction perpendicular to the focusing direction using multiple curved surfaces arranged to have a focusing effect in this direction. Because it utilizes the refraction of light, it is forced to have a structure in which curved surfaces are exposed, and its characteristics tend to deteriorate due to dust, moisture, dirt, etc., which poses problems in terms of reliability.
この発明の目的は、製作が容易でかつ信頼性の
高い光フアイバ通信用の光分配器を提供すること
にある。 An object of the present invention is to provide an optical splitter for optical fiber communication that is easy to manufacture and has high reliability.
この発明によれば、中心面に垂直な方向にその
平面からの距離の2乗にほぼ比例して減少する屈
折率分布を有する1次元集束性光伝送体と、複数
の2次元的な曲面からなる反射面と、3本以上の
光フアイバとを含む反射型光分配器が得られる。 According to the present invention, there is provided a one-dimensional convergent optical transmitter having a refractive index distribution that decreases in a direction perpendicular to a central plane in approximately proportion to the square of the distance from the plane, and a plurality of two-dimensional curved surfaces. A reflective optical distributor including a reflective surface and three or more optical fibers is obtained.
この発明では、従来の1次元集束性光伝送体と
曲面を組み合わせた光分配器における曲面での屈
折のかわりに反射を用いることにより、構成部品
の数を減らして製作を容易にし、かつ信頼性を高
めている。すなわち、1本の光フアイバから出射
した光ビームを1次元集束性光伝送体に導きその
光の集束方向と直角な方向に光ビーム径ひろげ
る。そこに複数の2次元的な曲面からなる反射面
を配置し、ひろがつた光ビームを分割するととも
に集束しながらもとの1次元集束性光伝送体中へ
折り返し、その入射端面に設置した複数の光フア
イバへ別々に結合することにより、光ビームの分
配機能を実現している。この発明では、各光学素
子は互いに平面で接着されるので製作は容易であ
る。しかし光学素子の表面での光ビームの屈折を
利用していないので、ほこりや湿気や汚れ等によ
る特性の劣化は全くなく信頼性が高い。 In this invention, by using reflection instead of refraction on a curved surface in an optical distributor that combines a conventional one-dimensional focusing optical transmitter and a curved surface, the number of component parts is reduced, manufacturing is easy, and reliability is improved. is increasing. That is, a light beam emitted from one optical fiber is guided to a one-dimensional convergent light transmission body, and the diameter of the light beam is expanded in a direction perpendicular to the direction of convergence of the light. A plurality of reflecting surfaces consisting of two-dimensional curved surfaces are placed there, and the expanding light beam is split and focused while being returned back into the original one-dimensional focusing optical transmitter. The optical beam distribution function is realized by coupling the optical fibers separately to each other. In this invention, each optical element is bonded to each other on a plane, so manufacturing is easy. However, since the refraction of the light beam on the surface of the optical element is not used, there is no deterioration in characteristics due to dust, moisture, dirt, etc., and the reliability is high.
以下、図面を参照してこの発明を詳しく説明す
る。 Hereinafter, the present invention will be explained in detail with reference to the drawings.
第1図はこの発明の第1の実施例の斜視図、第
2図、第3図は光ビームの集束の様子を示すため
の平面図、断面図をそれぞれ示す。x,y,z軸
を図示のように定める。この実施例は、y方向に
のみ中心から周辺に向かつて距離のほぼ2乗に比
例して減少する屈折率分布を有する1次元集束性
光伝送体1の入射端面11に入射光フアイバ21
および第1から第4の出射光フアイバ22〜25
の端部を設置し、その出射端面12に第1から第
4の部分円柱3〜6をその中心軸がy軸に平行に
なるように接着固定し、その表面に金を蒸着して
2次元的な曲面からなる反射膜60を形成したも
のである。1次元集束性光伝送体1は、良く知ら
れたイオン交換法を用いてガラス平板に所望の屈
折率分布をつけたもので、そのz軸方向の長さは
異軸入射光ビームのy方向蛇行ピツチの約1/4に
選んでいる。 FIG. 1 is a perspective view of a first embodiment of the present invention, and FIGS. 2 and 3 are a plan view and a sectional view, respectively, showing how the light beam is focused. Define the x, y, and z axes as shown. In this embodiment, an input optical fiber 21 is connected to an input end surface 11 of a one-dimensional convergent optical transmission body 1 having a refractive index distribution that decreases in proportion to the square of the distance from the center to the periphery only in the y direction.
and first to fourth output optical fibers 22 to 25
The first to fourth partial cylinders 3 to 6 are adhesively fixed to the output end surface 12 so that their central axes are parallel to the y-axis, and gold is deposited on the surface to create a two-dimensional structure. A reflective film 60 having a curved surface is formed. The one-dimensional focusing optical transmitter 1 is a flat glass plate with a desired refractive index distribution using the well-known ion exchange method, and its length in the z-axis direction is the same as the y-direction of the different-axis incident light beam. It is selected to be approximately 1/4 of the meandering pitch.
最初にy方向について考えると入射光フアイバ
21から出射した入射光ビーム31は、1次元集
束性光伝送体1でy方向に集束されこの方向には
ほぼ平行な光ビームになつて第1から第4の部分
円柱3〜6の表面に形成された反射膜60へ入射
する。反射膜60はy方向には収束作用をもたな
いので入射光ビーム31はほぼ平行なまま折り返
されてもとの1次元集束性光伝送体1へ入射し、
そこでy方向に集束されて第1から第4の分配光
ビーム32〜35に変換され、第1から第4の出
射光フアイバ22〜25へそれぞれ入射する。光
ビームは1次元集束性光伝送体1をz軸方向にそ
のy方向蛇行ピツチの約半分の長さだけか通過す
るので1次元集束性光伝送体1の入射端面11で
入射光ビーム31と分配光ビーム32〜35のy
方向の光ビーム径はほぼ等しくなる。次にx方向
での光ビームの様子について考える、1次元集束
性光伝送体1はx方向には集束作用を持たないの
で、入射光ビーム31はひろがりながら反射膜6
0に入射し、そこで分割・集束されながら折り返
され第1から第4の分配光ビーム32〜35に変
換され、第1から第4の出射光フアイバ22〜2
5に分配されて入射する。。前述したように、y
方向には光ビーム径はほとんど変わらず、x方向
には個々の部分円柱3,4,5,6の各々の反射
膜60により別々に集束されるので、この光分配
器では挿入損失を小さくできる。光ビームがひろ
がつたところへ分配用の光学素子を配置している
ので、その形状等に対してはそれ程きびしい工作
精度等は要求されず、分配比を任意の値に設定す
ることが可能であつた。すなわち、ひろがつた光
ビームの強度分布を考慮して部分円柱3〜6の大
きさを決めることにより、各分配光フアイバ22
〜25への分配比を所望の値に設定することがで
きた。このように分配用の光学素子の形状が比較
的大きいことや、1次元集束性光伝送体1と部分
円柱3〜6を平面で互いに接着固定できること等
からこの光分配器の製作は容位であつた。さら
に、この光分配器は光学素子表面での光の屈折に
よらず反射膜60による反射を利用しているの
で、光ビームが空気中に出ることはなく、表面の
汚れや湿気やほこり等による特性の劣化は全くな
く、信頼性の高いものであつた。 First, considering the y-direction, the incident light beam 31 emitted from the incident optical fiber 21 is focused in the y-direction by the one-dimensional focusing optical transmitter 1 and becomes a light beam substantially parallel to this direction. The light is incident on the reflective film 60 formed on the surfaces of the partial cylinders 3 to 6 of No. 4. Since the reflective film 60 does not have a convergence effect in the y direction, the incident light beam 31 is turned back while remaining almost parallel and enters the original one-dimensional convergent light transmission body 1.
There, it is focused in the y direction and converted into first to fourth distributed light beams 32 to 35, which enter the first to fourth output optical fibers 22 to 25, respectively. Since the light beam passes through the one-dimensional convergent optical transmitter 1 in the z-axis direction for approximately half the length of the meandering pitch in the y-direction, it is separated from the incident light beam 31 at the incident end surface 11 of the one-dimensional convergent optical transmitter 1. y of distributed light beams 32-35
The light beam diameters in both directions are approximately equal. Next, consider the state of the light beam in the x direction.Since the one-dimensional focusing optical transmitter 1 does not have a focusing effect in the
0, where it is split and focused while being turned back and converted into the first to fourth distributed light beams 32 to 35, which are then transmitted to the first to fourth output optical fibers 22 to 2.
It is distributed into 5 parts and enters the field. . As mentioned above, y
In the x direction, the light beam diameter hardly changes, and in the x direction, it is focused separately by the reflective film 60 of each of the partial cylinders 3, 4, 5, and 6, so this optical splitter can reduce insertion loss. . Since the optical element for distribution is placed where the light beam spreads, the shape etc. do not require very strict machining precision, and the distribution ratio can be set to any value. It was hot. That is, by determining the size of the partial cylinders 3 to 6 in consideration of the intensity distribution of the diffused light beam, each distribution optical fiber 22
It was possible to set the distribution ratio to ~25 to a desired value. Because the shape of the distributing optical element is relatively large and the one-dimensional convergent light transmitter 1 and the partial cylinders 3 to 6 can be adhesively fixed to each other on a flat surface, it is possible to manufacture this optical distributor with ease. It was hot. Furthermore, since this optical splitter utilizes reflection by the reflective film 60 instead of refraction of light on the surface of the optical element, the light beam does not go into the air, and the light beam is not affected by surface dirt, moisture, dust, etc. There was no deterioration in characteristics at all, and the reliability was high.
第4図はこの発明の第2の実施例の平面図をあ
らわす。この実施例では第1の実施例で用いた複
数の部分用柱の表面につけた反射膜60を、分割
された第1から第4の曲面42〜45を持つ透明
体40の表面につけた反射膜61でおきかえたも
のである。これらの曲面は、反射膜61の各々の
曲面で分割、集束、反射された第1から第4の分
配光ビーム32〜35の中心の軌跡が中心軸50
にほぼ平行になるように定めた。こうすることに
より第1から第4の出射光フアイバ22〜25を
互いに平行にならべることができ、光分配器の製
作がより容易になつた。また中心軸50に近い第
2、第3の曲面43,44が見込む角度を中心軸
50から遠い第1、第4の曲面42,45が見込
む角度より小さくすることにより、入射光フアイ
バ21が集束型フアイバのときのようにひろがつ
たところでのx−z面内の光ビームの強度の角度
分布が角度の大きいところ程小さいような場合に
も第1から第4の出射光フアイバ22〜25への
分配比をほぼ等しくすることができた。透明体4
0は、必要な曲面を持つ金型を作り、そこへ透明
プラスチツク材料を流し込んで固化するという方
法を用いて作つた。以上、述べたように、この実
施例でも製作が容易で信頼性の高い光分配器が得
られた。 FIG. 4 shows a plan view of a second embodiment of the invention. In this embodiment, the reflective film 60 applied to the surface of the plurality of partial pillars used in the first example is the same as the reflective film 60 applied to the surface of the transparent body 40 having the divided first to fourth curved surfaces 42 to 45. It was replaced in 61. These curved surfaces are such that the locus of the centers of the first to fourth distributed light beams 32 to 35 that are split, focused, and reflected by each curved surface of the reflective film 61 is aligned with the central axis 50.
It was set so that it was almost parallel to. By doing so, the first to fourth output optical fibers 22 to 25 can be arranged parallel to each other, making it easier to manufacture the optical distributor. In addition, by making the angle observed by the second and third curved surfaces 43 and 44 near the central axis 50 smaller than the angle observed by the first and fourth curved surfaces 42 and 45 far from the central axis 50, the incident optical fiber 21 is focused. Even in the case where the angular distribution of the intensity of the light beam in the x-z plane is smaller as the angle is larger, as in the case of a type fiber, the light beam is transmitted to the first to fourth output optical fibers 22 to 25. We were able to make the distribution ratios almost equal. transparent body 4
0 was made by creating a mold with the necessary curved surface, pouring transparent plastic material into it, and letting it solidify. As described above, in this example as well, an optical distributor that was easy to manufacture and had high reliability was obtained.
この発明は上記の望ましい実施例のほかにいく
つかの変形が可能である。光ビームを分割、集束
するための2次曲面としては円柱面の一部に限ら
ず、半円柱面、放物筒の曲面である放物柱面、あ
るいは他の特殊な曲面等も利用できる。1次元集
束性光伝送体としてガラス製だけでなくプラスチ
ク等に重合拡散を利用して屈折率分布をつけたも
のも用いることができる。プラスチツク製1次元
集束性光伝送体の場合には、その一方の端面を直
接複数に分割された曲面に成形することもでき
る。1次元集束性光伝送体のz軸方向の長さはy
方向蛇行ピツチの1/4の奇数倍であればこの実施
例と同様な効果が期待できる。その場合にその長
さを長くすればする程光ビームのx方向のひろが
りは大きくなるので分配数が多い場合には都合が
良い。また、適当なスペーサを用いることにより
1/4ピツチ4より長くすることも短かくすること
もできる。分配数は実施例に示した4に限らず、
もつと多くてももつと少なくても良い。入出射の
光フアイバと1次元集束性光伝送体の間には屈折
率整合材を用いてそこでの反射損失を減少させる
ことができる。 This invention can be modified in several ways in addition to the preferred embodiments described above. The quadratic curved surface for dividing and focusing the light beam is not limited to a part of a cylindrical surface, but may also be a semi-cylindrical surface, a parabolic cylinder surface that is a curved surface of a paraboloid, or other special curved surfaces. As the one-dimensional focusing light transmitting body, it is possible to use not only glass but also plastic or the like with a refractive index distribution using polymerization diffusion. In the case of a plastic one-dimensional focusing light transmission body, one end surface thereof can be directly formed into a curved surface divided into a plurality of parts. The length of the one-dimensional focusing optical transmitter in the z-axis direction is y
If it is an odd number multiple of 1/4 of the direction meandering pitch, the same effect as this embodiment can be expected. In this case, the longer the length, the greater the spread of the light beam in the x direction, which is convenient when the number of distributions is large. Also, by using an appropriate spacer
It can be made longer or shorter than 1/4 pitch 4. The number of distributions is not limited to 4 as shown in the example,
It's okay to have more or less. A refractive index matching material can be used between the input/output optical fiber and the one-dimensional focusing optical transmission body to reduce reflection loss there.
第1図はこの発明の第1の実施例の斜視図、第
2図はその平面図、第3図はその断面図、第4図
はこの発明の第2の実施例の平面図をそれぞれあ
らわす。
図において、1……1次元集束性光伝送体、3
〜6……部分円柱、11,12……端面、21〜
25……光フアイバ、31〜35……光ビーム、
40……透明体、42〜45……曲面、50……
中心軸、60,61……反射膜を、それぞれあら
わす。
FIG. 1 is a perspective view of a first embodiment of this invention, FIG. 2 is a plan view thereof, FIG. 3 is a sectional view thereof, and FIG. 4 is a plan view of a second embodiment of this invention. . In the figure, 1... one-dimensional focusing optical transmission body, 3
~6...Partial cylinder, 11,12...End face, 21~
25...Optical fiber, 31-35...Light beam,
40...Transparent body, 42-45...Curved surface, 50...
Central axis, 60, 61 . . . represent reflective films, respectively.
Claims (1)
面からの距離の2乗にほぼ比例して減少する屈折
率分布を有し前記中心軸にほぼ垂直な入射端面及
び出射端面を有する1次元集束性光伝送体と、そ
の出射端面に近接して設置され前記垂直な方向に
平行な軸を有する複数の2次元的な曲面からなる
反射面と、前記入射端面に端部を設置された3本
以上の光フアイバとを含むことを特徴とする反射
型光分配器。1. A one-dimensional lens having a refractive index distribution that decreases in a direction perpendicular to a central plane including the central axis in approximately proportion to the square of the distance from the central plane, and having an entrance end surface and an exit end surface that are approximately perpendicular to the central axis. a convergent light transmitter; a reflective surface made of a plurality of two-dimensional curved surfaces installed close to the output end face thereof and having axes parallel to the perpendicular direction; 1. A reflective optical splitter comprising at least one optical fiber.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10074478A JPS5528029A (en) | 1978-08-17 | 1978-08-17 | Reflection type light distributor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10074478A JPS5528029A (en) | 1978-08-17 | 1978-08-17 | Reflection type light distributor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5528029A JPS5528029A (en) | 1980-02-28 |
| JPS6131842B2 true JPS6131842B2 (en) | 1986-07-23 |
Family
ID=14282049
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10074478A Granted JPS5528029A (en) | 1978-08-17 | 1978-08-17 | Reflection type light distributor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5528029A (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS55105207A (en) * | 1979-02-06 | 1980-08-12 | Matsushita Electric Ind Co Ltd | Optical branching and coupling device |
| US4993796A (en) * | 1979-08-14 | 1991-02-19 | Kaptron, Inc. | Fiber optics communication modules |
| JPS57198423A (en) * | 1981-06-01 | 1982-12-06 | Nippon Sheet Glass Co Ltd | Planar type optical demultiplexer and multiplexer |
| JPS5863914A (en) * | 1981-09-28 | 1983-04-16 | カプトロン・インコ−ポレ−テツド | Optical fiber communication equipment |
| US4813759A (en) * | 1983-08-25 | 1989-03-21 | The Babcock & Wilcox Company | Fiber optic high and low level alarms |
| US6198864B1 (en) * | 1998-11-24 | 2001-03-06 | Agilent Technologies, Inc. | Optical wavelength demultiplexer |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5114348A (en) * | 1974-07-26 | 1976-02-04 | Nippon Selfoc Co Ltd | ICHIHOKOSHUSOKUSEIHIKARIDENSOTAIOSONAETA HIKARIBIIMUHENKANKI |
| JPS5379553A (en) * | 1976-12-24 | 1978-07-14 | Toshiba Corp | Light distributor |
-
1978
- 1978-08-17 JP JP10074478A patent/JPS5528029A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5528029A (en) | 1980-02-28 |
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