JPH0451804B2 - - Google Patents

Info

Publication number
JPH0451804B2
JPH0451804B2 JP1863386A JP1863386A JPH0451804B2 JP H0451804 B2 JPH0451804 B2 JP H0451804B2 JP 1863386 A JP1863386 A JP 1863386A JP 1863386 A JP1863386 A JP 1863386A JP H0451804 B2 JPH0451804 B2 JP H0451804B2
Authority
JP
Japan
Prior art keywords
dispersion
light
optical
wavelength
grating
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 - Lifetime
Application number
JP1863386A
Other languages
Japanese (ja)
Other versions
JPS62201407A (en
Inventor
Masataka Shirasaki
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP1863386A priority Critical patent/JPS62201407A/en
Priority to CA000528106A priority patent/CA1280921C/en
Priority to DE8787101177T priority patent/DE3773687D1/en
Priority to EP87101177A priority patent/EP0231874B1/en
Priority to US07/008,346 priority patent/US4747655A/en
Publication of JPS62201407A publication Critical patent/JPS62201407A/en
Publication of JPH0451804B2 publication Critical patent/JPH0451804B2/ja
Granted 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
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means
    • G02B6/28Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
    • G02B6/293Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
    • G02B6/29304Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating by diffraction, e.g. grating
    • G02B6/29305Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating by diffraction, e.g. grating as bulk element, i.e. free space arrangement external to a light guide
    • G02B6/2931Diffractive element operating in reflection
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/10Beam splitting or combining systems
    • G02B27/1006Beam splitting or combining systems for splitting or combining different wavelengths
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/10Beam splitting or combining systems
    • G02B27/1086Beam splitting or combining systems operating by diffraction only
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/04Prisms
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means
    • G02B6/28Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
    • G02B6/293Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
    • G02B6/29379Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device
    • G02B6/2938Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device for multiplexing or demultiplexing, i.e. combining or separating wavelengths, e.g. 1xN, NxM

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Diffracting Gratings Or Hologram Optical Elements (AREA)
  • Optical Communication System (AREA)

Description

【発明の詳細な説明】 〔概要〕 光路上の回折格子間に、頂角が60°で階段状に
形成された分散分割格子を設置した、各波長チヤ
ネル内の透過帯域(バンド)幅の広い光波長合分
波器を提起する。
[Detailed description of the invention] [Summary] A dispersion splitting grating formed in a stepped manner with an apex angle of 60° is installed between the diffraction gratings on the optical path, and the transmission band width in each wavelength channel is wide. Introducing an optical wavelength multiplexer/demultiplexer.

〔産業上の利用分野〕 本発明は光通信システムを構成する光波長合分
波器に関する。
[Industrial Application Field] The present invention relates to an optical wavelength multiplexer/demultiplexer constituting an optical communication system.

波長多重通信は波長の異なる光(各波長チヤネ
ル)毎にそれぞれ別個の情報をのせ、それらを1
つの光路に合成し、光フアイバを通して伝送する
という方法がとられている。
Wavelength multiplexing communication carries separate information for each wavelength of light (each wavelength channel) and combines them into one
A method is used in which the light is combined into two optical paths and transmitted through an optical fiber.

従つて、受信側では合成された光を各波長チヤ
ネル毎に分解し、それぞれの光に重畳されている
情報を取り出す必要がある。
Therefore, on the receiving side, it is necessary to decompose the combined light into each wavelength channel and extract the information superimposed on each light.

このようなシステムにおいては、複数の波長の
光を合成したり、あるいは合成された光を波長別
に分解するための光波長合分波器が用いられてい
る。
In such a system, an optical wavelength multiplexer/demultiplexer is used to combine light of a plurality of wavelengths or to separate the combined light into wavelengths.

以上のような波長多重光通信システムの構成に
おいては、光波長合分波器内の回折格子の波長分
散に起因する狭帯域の問題を解決して、各波長チ
ヤネル内の透過帯域幅を広くすることが重要であ
る。
In the configuration of the wavelength division multiplexing optical communication system as described above, the narrow band problem caused by the wavelength dispersion of the diffraction grating in the optical wavelength multiplexer/demultiplexer is solved and the transmission bandwidth within each wavelength channel is widened. This is very important.

〔従来の技術〕[Conventional technology]

第2図は従来例の回折格子を用いた光波長合分
波器の側断面図である。
FIG. 2 is a side sectional view of a conventional optical wavelength multiplexer/demultiplexer using a diffraction grating.

ここでは、説明の便宜上入出力関係は分波の場
合について説明する。
Here, for convenience of explanation, the case where the input/output relationship is split will be described.

図において、入力用光フアイバ21より入力さ
れた光は、レンズ24で平行光になり回折格子2
2で反射される。
In the figure, the light input from the input optical fiber 21 is turned into parallel light by the lens 24, and the diffraction grating 2
It is reflected by 2.

回折格子22によつて波長分散された光は、レ
ンズ24を透過することにより、それぞれの波長
毎に設けられた出力用光フアイバアレイ23の各
光フアイバの上に集光し、ここより出力される。
The light wavelength-dispersed by the diffraction grating 22 passes through the lens 24 and is focused onto each optical fiber of the output optical fiber array 23 provided for each wavelength, from which it is output. Ru.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

それぞれの波長毎に設けられた出力用光フアイ
バが開口している範囲は、出力用光フアイバアレ
イの各光フアイバの間隔に対して比較的狭く、出
力用光フアイバに入る光は、同一波長帯域にある
光のごく狭い波長帯域の光になるという欠点があ
る。
The opening range of the output optical fibers provided for each wavelength is relatively narrow compared to the spacing between each optical fiber in the output optical fiber array, and the light entering the output optical fibers is in the same wavelength band. The disadvantage is that it produces light in a very narrow wavelength band.

〔問題点を解決するための手段〕[Means for solving problems]

第1図は本発明による回折格子と分散分割格子
を用いた光波長合分波器の側断面図である。
FIG. 1 is a side sectional view of an optical wavelength multiplexer/demultiplexer using a diffraction grating and a dispersion splitting grating according to the present invention.

図において、1は光フアイバ、2は第1の回折
格子、3は分散分割格子、4は第2の回折格子、
5は光フアイバアレイ、6,7,8,9はレンズ
である。
In the figure, 1 is an optical fiber, 2 is a first diffraction grating, 3 is a dispersion splitting grating, 4 is a second diffraction grating,
5 is an optical fiber array, and 6, 7, 8, and 9 are lenses.

上記問題点の解決は、1本の光フアイバ1から
複数本の光フアイバからなる光フアイバアレイ5
に至る光路上に、2個の回折格子2,4と、該2
個の回折格子間に側断面が頂角60°の2等辺三角
形で構成された溝が配列された階段型反射面を有
する分散分割格子3が設置され、該分散分割格子
3への光の入射方向は該分散分割格子の溝を構成
する片側の斜面に平行であり、出射方向は他側の
斜面に平行である光波長合分波器により達成され
る。
The solution to the above problem is to convert the single optical fiber 1 into an optical fiber array 5 consisting of a plurality of optical fibers.
There are two diffraction gratings 2 and 4 on the optical path leading to
A dispersion splitting grating 3 having a step-shaped reflecting surface in which grooves each having a side cross section composed of isosceles triangles with an apex angle of 60° are arranged is installed between the diffraction gratings, and the incidence of light to the dispersion splitting grating 3 is This is achieved by an optical wavelength multiplexer/demultiplexer whose direction is parallel to one side of the slope constituting the grooves of the dispersion dividing grating, and whose output direction is parallel to the other side of the slope.

さらに、前期分散分割格子3上に集光するよう
に、集光レンズ7,8を設置し、前記回折格子の
波長分散によつて生ずる集光点の移動が、分散分
割格子3を形成する面、すなわち分散分割格子3
の稜線を含む面と、入射光に垂直な面とが交わる
直線に平行であるように調整する。
Furthermore, condensing lenses 7 and 8 are installed so as to condense the light onto the dispersion splitting grating 3, and the movement of the focusing point caused by the wavelength dispersion of the diffraction grating is caused by the surface forming the dispersion splitting grating 3. , that is, dispersion splitting grid 3
Adjust so that it is parallel to the straight line that intersects the plane containing the ridgeline of the plane and the plane perpendicular to the incident light.

〔作用〕[Effect]

以下本発明においても従来例と同様に、説明の
便宜上入出力関係は分波の場合について説明する
ことにする。
In the following, in the present invention, as in the conventional example, for convenience of explanation, the input/output relationship will be explained in the case of demultiplexing.

第3図は本発明の分散分割格子の形状と機能を
説明する斜視図である。
FIG. 3 is a perspective view illustrating the shape and function of the dispersion dividing grid of the present invention.

図において、分散分割格子は直交座標xyzのy
面に刻まれた頂角60°の階段状に形成された格子
で、溝の斜面Bに平行に、溝の斜面Aに入射した
光は、2度反射して、溝の斜面Bより溝の斜面A
に平行に出射することができる。
In the figure, the dispersion dividing grid is y in Cartesian coordinates xyz
The grating is formed in the shape of steps with an apex angle of 60° carved into the surface, and light incident on the slope A of the groove parallel to the slope B of the groove is reflected twice and is reflected from the slope B of the groove into the groove. Slope A
It can be emitted parallel to.

なお、x′,y′の方位は、 x′の方位(2-1/2,2-1/2,0), y′の方位(−2-1/2,2-1/2,0), と決める。 Note that the directions of x′ and y′ are the direction of x′ (2 -1/2 , 2 -1/2 , 0) and the direction of y′ (−2 -1/2 , 2 -1/2 , 0 ), decide.

いま、入射光をK1、反射間の中間光をLM、出
射光をKOとし、x軸と溝の方向がx軸となす角
をθとすると、分散分割格子はつぎの限定条件を
充たす必要がある。
Now, let K 1 be the incident light, L M be the intermediate light between reflections, K O be the outgoing light, and let θ be the angle between the x-axis and the direction of the groove, then the dispersion splitting grating satisfies the following limiting conditions. There is a need.

(1) 格子を形成する面はy軸。(1) The plane forming the lattice is the y-axis.

(2) 頂角が60°の多数の溝を有する。(2) It has many grooves with an apex angle of 60°.

(3) θ=Tan-1(2-1/2)≒35.3°. (4) 入射光K1の方位(2-1/2,−2-1/2,0). (5) 中間光KMの方位(0,0,1). (6) 出射光KOの方位(2-1/2,2-1/2,0). 上記の条件(2),(3)と等価な表現をすると、つぎ
のようになる。
(3) θ=Tan -1 (2 -1/2 )≒35.3°. (4) Direction of incident light K 1 (2 -1/2 , -2 -1/2 , 0). (5) Direction of intermediate light K M (0,0,1). (6) Direction of output light K O (2 -1/2 , 2 -1/2 , 0). The expression equivalent to conditions (2) and (3) above is as follows.

(2)′,(3)′溝の斜面A,Bはそれぞれつぎの方位
をもつ。すなわち、 斜面Aの方位(−2-1,2-1,2-1/2), 斜面Bの方位(2-1,2-1,−2-1/2). となる。
The slopes A and B of the (2)′ and (3)′ grooves have the following orientations, respectively. That is, the direction of slope A (-2 -1 , 2 -1 , 2 -1/2 ), and the direction of slope B (2 -1 , 2 -1 , -2 -1/2 ). becomes.

ここで、各部の方位をまとめるとつぎのように
なる。
Here, the orientation of each part is summarized as follows.

K1:(2-1/2,−2-1/2,0), KM:(0,0,1), KO:(2-1/2,2-1/2,0), A:(−2-1,2-1,2-1/2), B:(2-1,2-1,−2-1/2). 以上の(1)〜(6)の限定条件を充たし、さらにつぎ
の条件を適用する。
K 1 : (2 -1/2 , −2 -1/2 , 0), K M : (0, 0, 1), K O : (2 -1/2 , 2 -1/2 , 0), A: (-2 -1 , 2 -1 , 2 -1/2 ), B: (2 -1 , 2 -1 , -2 -1/2 ). The above limiting conditions (1) to (6) are satisfied, and the following conditions are also applied.

(7) 入射側回折格子の分散方向をz方向とする。(7) The dispersion direction of the incident side diffraction grating is the z direction.

(8) 分散分割格子上に集光する。(8) Focus the light onto the dispersive splitting grating.

このような条件の下に、分散分割格子の作用を
要約するとつぎのようになる。
Under these conditions, the action of the dispersion splitting grid can be summarized as follows.

(1) 出射側の分散方向はz方向に垂直となる。す
なわち、y′方向である。
(1) The dispersion direction on the output side is perpendicular to the z direction. That is, in the y′ direction.

(2) 分散分割格子における2度の反射とも入射角
は45°となる。
(2) The angle of incidence is 45° for both reflections at the dispersion splitting grating.

(3) 入射時のz方向偏光は、A面でP偏光、B面
でS偏光となるために、出射時にはy′方向偏光
となる。
(3) Since the z-direction polarized light upon incidence becomes P-polarized light on the A plane and S-polarized light on the B-plane, it becomes y′-direction polarized light upon exit.

(4) 同様に、入射時のx′方向偏光は、出射時にz
方向偏光となる。
(4) Similarly, x′-direction polarization at the time of incidence is polarized in the z′ direction at the time of exit.
It becomes directional polarized light.

(5) この分散分割格子への入射位置が図示のよう
に−z方向へ移動した場合、同一の溝に入射す
る範囲においては出射位置がy′の方向へ移動す
る。入射位置がさらに−z方向へ移動し、つぎ
の溝の領域に入ると出射位置は不連続的に変化
し、以下同様にして周期的な動きを示す。
(5) When the input position to this dispersion dividing grating moves in the -z direction as shown in the figure, the output position moves in the y' direction within the range where the light enters the same groove. When the incident position further moves in the -z direction and enters the next groove area, the output position changes discontinuously, and thereafter shows periodic movement in the same manner.

(6) なお、この分散分割格子は溝の深さ程度の誤
差範囲内でレンズの焦点面に置くことが可能で
ある。
(6) Note that this dispersion dividing grating can be placed on the focal plane of the lens within an error range of about the depth of the groove.

第4図(1)〜(4)は本発明による光波長合分波器内
の各部における光の位置を示す図である。
FIGS. 4(1) to 4(4) are diagrams showing the positions of light at various parts within the optical wavelength multiplexer/demultiplexer according to the present invention.

2個の回折格子を同一チヤネル内において波長
分散を打ち消すように構成すれば、光フアイバよ
りの入射時の1点が(第4図(1))、第1の回折格
子で1方向に拡がり(第4図(2))、分散分割格子
で波長チヤネル毎に第4図(2)の方向と垂直に拡が
り(第4図(3))、つぎの第2の回折格子で波長チ
ヤネル毎に1点となる(第4図(4))。
If two diffraction gratings are configured to cancel wavelength dispersion within the same channel, one point at the time of incidence from the optical fiber (Fig. 4 (1)) will spread in one direction at the first diffraction grating ( (Fig. 4(2)), spread perpendicularly to the direction of Fig. 4(2) for each wavelength channel with a dispersion splitting grating (Fig. 4(3)), and spread 1 per wavelength channel with a second diffraction grating (Fig. 4(3)). It becomes a point (Figure 4 (4)).

このようにして波長チヤネル内の波長依存性を
なくすことができる。
In this way, wavelength dependence within the wavelength channel can be eliminated.

〔実施例〕〔Example〕

本発明の実施例を第1図に従つて説明する。 An embodiment of the present invention will be described with reference to FIG.

光フアイバ1から入力された光は、レンズ6を
透過して平行光になり、第1の回折格子2に入
り、ここで反射される。
Light input from the optical fiber 1 passes through the lens 6, becomes parallel light, enters the first diffraction grating 2, and is reflected there.

第1の回折格子2における反射によつて波長別
に分離された光はレンズ7を透過して分散分割格
子3上に集光される。
The light separated into wavelengths by reflection on the first diffraction grating 2 is transmitted through the lens 7 and focused onto the dispersion splitting grating 3.

分散分割格子3上に集光された光は、回折格子
2の波長分散を反映して線分となり、格子により
この線分は波長チヤネル毎の線分に分割される。
The light focused on the dispersion splitting grating 3 becomes a line segment reflecting the wavelength dispersion of the diffraction grating 2, and this line segment is divided into line segments for each wavelength channel by the grating.

分散分割格子3で反射された光はレンズ8を透
過して平行光となり、第2の回折格子4に入り、
ここで反射される。
The light reflected by the dispersion splitting grating 3 passes through the lens 8, becomes parallel light, enters the second diffraction grating 4,
It is reflected here.

第2の回折格子4は第1の回折格子2と波長分
散の大きさが等しく、同一チヤネル内においてこ
れらが打ち消されるように構成する。
The second diffraction grating 4 is configured to have the same wavelength dispersion as the first diffraction grating 2, and to cancel them within the same channel.

従つて、レンズ9を透過することにより、各波
長帯域毎に設けた光フアイバアレイ5の各光フア
イバ上に集光された光は、同一波長帯域の光の中
の広い帯域の光が含まれており、波長が変動して
も光信号を光フアイバアレイ5の各光フアイバに
出力することができる。
Therefore, the light that passes through the lens 9 and is focused onto each optical fiber of the optical fiber array 5 provided for each wavelength band includes a wide band of light within the same wavelength band. Therefore, even if the wavelength changes, the optical signal can be output to each optical fiber of the optical fiber array 5.

第5図(1),(2)はそれぞれ従来例と本発明による
光波長合分波器の損失と波長の関係を示す透過特
性図である。
FIGS. 5(1) and 5(2) are transmission characteristic diagrams showing the relationship between loss and wavelength of the optical wavelength multiplexer/demultiplexer according to the conventional example and the present invention, respectively.

図において、V,U型の各曲線は各チヤネルを
示し、本発明による第5図(2)は各チヤネル毎の波
長依存はU型になり、透過帯域幅が広くなつてい
ることが示されている。
In the figure, V- and U-shaped curves indicate each channel, and FIG. 5 (2) according to the present invention shows that the wavelength dependence of each channel is U-shaped, and the transmission bandwidth is widened. ing.

この実施例においては、回折格子に反射型を用
いたが、これの代わりに透過型を用いても同様の
効果が得られる。
In this embodiment, a reflection type diffraction grating is used, but the same effect can be obtained by using a transmission type instead.

〔発明の効果〕〔Effect of the invention〕

以上詳細に説明したように本発明によれば、波
長チヤネル内の透過帯域幅の広い光波長合分波器
が得られる。
As described in detail above, according to the present invention, an optical wavelength multiplexer/demultiplexer with a wide transmission band width within a wavelength channel can be obtained.

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

第1図は本発明による回折格子と分散分割格子
を用いた光波長合分波器の側断面図、第2図は従
来例の回折格子を用いた光波長合分波器の側断面
図、第3図は本発明の分散分割格子の形状と機能
を説明する斜視図である。第4図(1)〜(4)は本発明
による光波長合分波器内の各部における光の位置
を示す図、第5図(1),(2)はそれぞれ従来例と本発
明による光波長合分波器の損失と波長の関係を示
す透過特性図である。 図において、1は光フアイバ、2は第1の回折
格子、3は分散分割格子、4は第2の回折格子、
5は光フアイバアレイ、6,7,8,9はレン
ズ、である。
FIG. 1 is a side sectional view of an optical wavelength multiplexer/demultiplexer using a diffraction grating and dispersion splitting grating according to the present invention, and FIG. 2 is a side sectional view of an optical wavelength multiplexer/demultiplexer using a conventional diffraction grating. FIG. 3 is a perspective view illustrating the shape and function of the dispersion dividing grid of the present invention. Figures 4 (1) to (4) are diagrams showing the positions of light in each part of the optical wavelength multiplexer/demultiplexer according to the present invention, and Figures 5 (1) and (2) are diagrams showing the positions of light in each part of the optical wavelength multiplexer/demultiplexer according to the present invention, and Figures 5 (1) and (2) are diagrams showing the optical positions of the conventional example and the present invention, respectively. FIG. 2 is a transmission characteristic diagram showing the relationship between loss and wavelength of a wavelength multiplexer/demultiplexer. In the figure, 1 is an optical fiber, 2 is a first diffraction grating, 3 is a dispersion splitting grating, 4 is a second diffraction grating,
5 is an optical fiber array, and 6, 7, 8, and 9 are lenses.

Claims (1)

【特許請求の範囲】 1 1本の光フアイバ1から複数本の光フアイバ
からなる光フアイバアレイ5に至る光路上に、 2個の回折格子2,4と、該2個の回折格子間
に側断面が頂角60°の2等辺三角形で構成された
溝が配列された階段型反射面を有する分散分割格
子3が設置され、 該分散分割格子3への光の入射方向は該分散分
割格子の溝を構成する片側の斜面に平行であり、
出射方向は他側の斜面に平行であることを特徴と
する光波長合分波器。 2 前記分散分割格子3上に、該分散分割格子を
形成する面に集光するように2つの集光レンズ
7,8が設置され、 前記回折格子の波長分散によて生ずる集光点の
移動が、該分散分割格子を形成する面と、入射光
に垂直な面とが交わる直線に平行であることを特
徴とする特許請求の範囲第1項記載の光波長合分
波器。
[Claims] 1. On the optical path from one optical fiber 1 to an optical fiber array 5 consisting of a plurality of optical fibers, there are two diffraction gratings 2 and 4, and a side wall between the two diffraction gratings. A dispersion splitting grating 3 having a step-shaped reflective surface in which grooves each having a cross section composed of an isosceles triangle with an apex angle of 60° are arranged is installed, and the direction of incidence of light to the dispersion splitting grating 3 is set according to the direction of the dispersion splitting grating 3. parallel to the slope on one side of the groove,
An optical wavelength multiplexer/demultiplexer characterized in that the output direction is parallel to the slope on the other side. 2. Two condensing lenses 7 and 8 are installed on the dispersion splitting grating 3 so as to focus the light on the surface forming the dispersion splitting grating, and the movement of the focusing point caused by the wavelength dispersion of the diffraction grating 2. The optical wavelength multiplexer/demultiplexer according to claim 1, wherein the wavelength multiplexer/demultiplexer is parallel to a straight line that intersects a plane forming the dispersion splitting grating and a plane perpendicular to the incident light.
JP1863386A 1986-01-30 1986-01-30 Optical wavelength multiplexer/demultiplexer Granted JPS62201407A (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP1863386A JPS62201407A (en) 1986-01-30 1986-01-30 Optical wavelength multiplexer/demultiplexer
CA000528106A CA1280921C (en) 1986-01-30 1987-01-26 Optical wavelength compounding/dividing device
DE8787101177T DE3773687D1 (en) 1986-01-30 1987-01-28 OPTICAL WAVELENGTH MULTIPLEXER / -DEMULTIPLEXER.
EP87101177A EP0231874B1 (en) 1986-01-30 1987-01-28 Optical wavelength compounding/dividing device
US07/008,346 US4747655A (en) 1986-01-30 1987-01-29 Optical wavelength compounding/dividing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1863386A JPS62201407A (en) 1986-01-30 1986-01-30 Optical wavelength multiplexer/demultiplexer

Publications (2)

Publication Number Publication Date
JPS62201407A JPS62201407A (en) 1987-09-05
JPH0451804B2 true JPH0451804B2 (en) 1992-08-20

Family

ID=11977016

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1863386A Granted JPS62201407A (en) 1986-01-30 1986-01-30 Optical wavelength multiplexer/demultiplexer

Country Status (1)

Country Link
JP (1) JPS62201407A (en)

Also Published As

Publication number Publication date
JPS62201407A (en) 1987-09-05

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