JPS6325631A - Waveguide type optical switch - Google Patents
Waveguide type optical switchInfo
- Publication number
- JPS6325631A JPS6325631A JP16803086A JP16803086A JPS6325631A JP S6325631 A JPS6325631 A JP S6325631A JP 16803086 A JP16803086 A JP 16803086A JP 16803086 A JP16803086 A JP 16803086A JP S6325631 A JPS6325631 A JP S6325631A
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- refractive index
- light
- intersection
- optical switch
- 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
- 230000003287 optical effect Effects 0.000 title claims description 12
- 238000009826 distribution Methods 0.000 claims abstract description 10
- 230000001902 propagating effect Effects 0.000 claims description 3
- 239000006185 dispersion Substances 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 238000004458 analytical method Methods 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、光導波路中を伝搬する光の進行方向を制御す
る導波型光スイッチに関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a waveguide optical switch that controls the traveling direction of light propagating in an optical waveguide.
導波型光スイッチとして、従来よりX交差型の導波路に
電極を設け、交差部の中心線に沿って導波光の光路をさ
えぎるように屈折率の低い領域を電気的に生じさせ、導
波光を全反射させることによ逆光路を変えるものがある
。この型の光スィッチは構造が簡単で非常に小型にする
ことができると云う特徴がある。Conventionally, as a waveguide type optical switch, an electrode is provided in an X-crossing waveguide, and a region with a low refractive index is electrically created to block the optical path of the guided light along the center line of the intersection. There are some devices that change the backlight path by total reflection. This type of optical switch has a simple structure and can be made very compact.
以下に上記従来技術を図面を用いて説明する。The above-mentioned conventional technology will be explained below with reference to the drawings.
第6図は平面図でちり、図において1,2は直線導波路
であり、基板3上に交差点4で交差して形成され、その
交差部5に長さ方向に沿って電極6が設けである。FIG. 6 is a plan view. In the figure, 1 and 2 are straight waveguides, which are formed on the substrate 3 so as to intersect at an intersection 4, and electrodes 6 are provided along the length direction at the intersection 5. be.
このような構成の光スィッチてよると、電圧を電極6に
印加しないときには、直線導波路1(又は2)の入口1
a(又は2a)から入力した光が出口1b(又は2b)
から出力される状態(以下クロス状態と云う。)となる
ように導波路部の交差角φを選択しである。According to the optical switch having such a configuration, when no voltage is applied to the electrode 6, the entrance 1 of the straight waveguide 1 (or 2)
Light input from a (or 2a) exits exit 1b (or 2b)
The crossing angle φ of the waveguide section is selected so that the output state (hereinafter referred to as a cross state) is achieved.
そして、電極4に電圧を印加したときに電極部分の屈折
率全下げて光を全反射させ、入口1a(又は2a)から
入力した光を出口2b(又はIb)に出力させている(
以下バー状態と云う。)。When a voltage is applied to the electrode 4, the refractive index of the electrode portion is completely lowered to cause total reflection of the light, and the light input from the entrance 1a (or 2a) is outputted to the exit 2b (or Ib).
This will be referred to as the bar state below. ).
しかし、上記クロス状態において良いクロストークを得
ることは難しく交差角を8°程度以上とすることが必要
であった。ところが、この場合屈折率を低くした電極部
分へ入射す・る角度が大きくなるために動作電圧が高く
なるという欠点がある。However, it is difficult to obtain good crosstalk in the above-mentioned cross state, and it is necessary to set the crossing angle to about 8° or more. However, in this case, there is a drawback that the operating voltage becomes high because the angle of incidence on the electrode portion with a low refractive index becomes large.
交差角φが比較的大きい場合(4°以上)にこのクロス
トークが生じる原因は、第7図に示す如く導波路が交差
部5に入ってきた場所において急激に光の閉じ込めが悪
くなるために回折が生じるためである。すなわち、導波
光7は交差部5に入つたところで回折し、大部分は導波
光7aとして進むが、わずかに不要光7b、7cが生じ
、このうちの不要光7bの方向の回折光が導波路の導波
光となってクロストークが生じてしまうことになる。The reason why this crosstalk occurs when the crossing angle φ is relatively large (4° or more) is that light confinement suddenly deteriorates at the place where the waveguide enters the crossing part 5, as shown in FIG. This is because diffraction occurs. That is, the guided light 7 is diffracted when it enters the intersection 5, and most of it travels as guided light 7a, but a small amount of unnecessary light 7b and 7c is generated, and among these, the diffracted light in the direction of the unnecessary light 7b passes through the waveguide. As a result, crosstalk will occur.
本発明は、2本の導波路を交差させてその導波路中を伝
搬する光の進行方向全制御する導波型光スイッチにおい
て、高屈折率部と低屈折率部とより成る導波路を交差さ
せて交差部へ入射する入射光の界分布を適切に定めて回
折角を制御することを特徴とする。The present invention provides a waveguide type optical switch that completely controls the traveling direction of light propagating in the waveguides by crossing two waveguides. The diffraction angle is controlled by appropriately determining the field distribution of the incident light incident on the intersection.
以上の構成によると、交差部において散乱源が生じない
ように屈折率を大きくしたことにより、交差部での回折
角は小さくなって交差部に入射した光は洩れが少なく所
定の導波路に進み、クロストークが低減されることにな
る。According to the above configuration, by increasing the refractive index to prevent scattering sources from occurring at the intersection, the diffraction angle at the intersection becomes small, and the light incident on the intersection proceeds to the designated waveguide with little leakage. , crosstalk will be reduced.
以下に本発明の実施例を図面を用いて説明する0第1図
は第1実施例を示す導波路の平面図、第2図はこの導波
路を2つ交差させた状態の平面図であり、図において、
8は導波路であり、高屈折率部9と低屈折率部10を非
対称に設けた構造となっている。Embodiments of the present invention will be explained below with reference to the drawings. 0. FIG. 1 is a plan view of a waveguide showing the first embodiment, and FIG. 2 is a plan view of two waveguides intersecting each other. , In the figure,
A waveguide 8 has a structure in which a high refractive index section 9 and a low refractive index section 10 are provided asymmetrically.
このような構造の導波管8を2本人力側で高屈折率部9
が互に向い合うようにして交差点11で交差させ、その
交差部12は散乱源が生じないように高屈折率部9とし
ておき、図示しないが電極を設けておく。Two waveguides 8 having such a structure are manually connected to the high refractive index section 9.
They are made to face each other and intersect at an intersection 11, and the intersection 12 is made into a high refractive index section 9 so as not to generate a scattering source, and an electrode (not shown) is provided therein.
以上の構成による本実施例の作用を以下に説明する。な
おこの作動原理を第3図の説明図に示す。The operation of this embodiment with the above configuration will be explained below. The principle of this operation is shown in the explanatory diagram of FIG.
導波路8−2aに入力さnた光は、交差点11を通9、
導波路8−2bに入射されるが、このとき、光の界分布
13−2が高屈折率部9に片寄って存在しているために
導波路8−1bの中にはほとんど存在せずに、導波路8
−2bへの漏れ込みが少ない。このためにクロストーク
が低減することになる。The light input to the waveguide 8-2a passes through the intersection 11 9,
The light is incident on the waveguide 8-2b, but at this time, because the field distribution 13-2 of the light is biased toward the high refractive index portion 9, almost no light exists in the waveguide 8-1b. , waveguide 8
-Leakage into 2b is small. This will reduce crosstalk.
第4図は第2実施例に示す導波路の平面図、第5図はこ
の導波路を2つ交差させた状態の平面図であり、図にお
いて、14は導波管であシ、中央に高屈折率部15を設
けその周囲を低屈折率部16とした構成となっている。FIG. 4 is a plan view of the waveguide shown in the second embodiment, and FIG. 5 is a plan view of two waveguides intersecting each other. In the figure, 14 is a waveguide. It has a structure in which a high refractive index section 15 is provided and a low refractive index section 16 is provided around it.
このような構成の導波管14を2本交差点17で交差さ
せ、さらに高屈折率部15の幅が交差点17に近付くに
従って狭くなって行く構造としておき、交差部18は散
乱源が生じないように高屈折率部15の−様なものとし
ておく。本実施例においても図示はしないが交差部に電
極を設けておく。Two waveguides 14 having such a configuration are made to intersect at an intersection 17, and the width of the high refractive index portion 15 becomes narrower as it approaches the intersection 17, and the intersection 18 is designed to prevent scattering sources from occurring. The high refractive index portion 15 is assumed to be similar to -. In this embodiment as well, although not shown, electrodes are provided at the intersections.
以上の構成によると、光の界分布の幅をω、光する。し
たがってωが大きい根回折角は小さくなり、高屈折率部
15を狭くすることによってω全増大することができ、
これによってクロストークが低減することになる。According to the above configuration, the width of the light field distribution is ω. Therefore, the root diffraction angle where ω is large becomes small, and by narrowing the high refractive index portion 15, ω can be totally increased.
This will reduce crosstalk.
以上説明した本発明によると、82M解析法を用いて以
下の条件全解析した。基板屈折率2,14、光の波数1
.3μm導波路幅8μm、導波路部の屈3 × 10
折率2.14+(−5の値のときに、角度φ6× 10
=4.6° において、従来の一12dBから一15d
Bへと改善することができる。According to the present invention described above, the following conditions were all analyzed using the 82M analysis method. Substrate refractive index 2.14, light wave number 1
.. When the 3 μm waveguide width is 8 μm and the refractive index of the waveguide part is 3 × 10 and the refractive index is 2.14 + (-5, the angle φ6 × 10 = 4.6°, the conventional -12 dB to -15 d
It can be improved to B.
第1図は本発明の第1実施例に用いる導波路の平面図、
第2図は導波路全交差させた状態の平面図、第3図は界
分布の状態を示す説明図、第4図は第2実施例に用いる
導波路の平面図、第5図は導波路を交差させた状態の平
面図、第6図は従来列の平面図、第7図は光の洩れ状態
を示す平面図である。
8・・・導波路 9・・・高屈折率部 10・・・低屈
折率部 11・・・交差点 12・・・交差部特許出願
人 沖電気工業株式会社
代理人弁理士 金 倉 喬 二第1笑施例の導
波路の平面図
鏑 1 亘
導波路を交差させた平面図 界分布ヶ示ス説明図
舖 2 ■ 輔 3 国
第2実施例の導波路の平面図
輔 41
2b Ib
従来例の平面図
閲 6112
14−2b 14−4b
導波路を交差させた平面図
紬 5 l
光の洩れを示す平面図
輔 7 図FIG. 1 is a plan view of a waveguide used in the first embodiment of the present invention,
Fig. 2 is a plan view of the waveguides with all of them intersecting, Fig. 3 is an explanatory diagram showing the state of field distribution, Fig. 4 is a plan view of the waveguide used in the second embodiment, and Fig. 5 is the waveguide. 6 is a plan view of a conventional row, and FIG. 7 is a plan view showing a state of light leakage. 8... Waveguide 9... High refractive index section 10... Low refractive index section 11... Intersection 12... Intersection Patent applicant Oki Electric Industry Co., Ltd. Representative patent attorney Takashi Kanakura Second 1 Plan view of the waveguide of the second embodiment 1 Plan view of crossed waveguides Explanatory diagram showing field distribution 2 ■ 3 Plan view of the waveguide of the second embodiment 41 2b Ib Conventional example View of the plan view of 6112 14-2b 14-4b Plan view of intersecting waveguides 5 l Plan view showing light leakage 7 Figure
Claims (1)
光の進行方向を制御する導波型光スイッチにおいて、 高屈折率部と低屈折率部とより成る導波路を交差させ、
その交差部に入射する入射光の界分布を適切に定めて回
折角を制御することを特徴とする導波型光スイッチ。 2、特許請求の範囲第1項において、導波路の屈折率を
導波路の中心軸に対して非対称とし、交差点以降におい
て互の光の界分布の重なりを小さくしたことを特徴とす
る導波型光スイッチ。 3、特許請求の範囲第1項において、導波路の膜厚、屈
折率または幅を交差部の近傍で小さくし導波光の界分布
を広げることに回折角を小さくしたことを特徴とする導
波型光スイッチ。 4、特許請求の範囲第1項において、交差部の屈折率を
高くしたことを特徴とする導波型光スイッチ。[Claims] A waveguide optical switch that controls the traveling direction of light propagating in the waveguides by intersecting one or two waveguides, comprising a high refractive index section and a low refractive index section. Cross the waveguides,
A waveguide optical switch is characterized in that the field distribution of incident light incident on the intersection is appropriately determined to control the diffraction angle. 2. A waveguide type according to claim 1, characterized in that the refractive index of the waveguide is asymmetrical with respect to the central axis of the waveguide, and the overlap of mutual light field distributions after the intersection is reduced. light switch. 3. A waveguide according to claim 1, characterized in that the film thickness, refractive index, or width of the waveguide is reduced near the intersection to widen the field distribution of the guided light and to reduce the diffraction angle. type optical switch. 4. A waveguide optical switch according to claim 1, characterized in that the refractive index of the intersection portion is increased.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16803086A JPS6325631A (en) | 1986-07-18 | 1986-07-18 | Waveguide type optical switch |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP16803086A JPS6325631A (en) | 1986-07-18 | 1986-07-18 | Waveguide type optical switch |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6325631A true JPS6325631A (en) | 1988-02-03 |
Family
ID=15860518
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP16803086A Pending JPS6325631A (en) | 1986-07-18 | 1986-07-18 | Waveguide type optical switch |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6325631A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2002023264A1 (en) * | 2000-09-18 | 2002-03-21 | Ngk Insulators, Ltd. | Optical device |
US6961493B2 (en) | 2001-04-18 | 2005-11-01 | Ngk Insulators, Ltd. | Optical device |
-
1986
- 1986-07-18 JP JP16803086A patent/JPS6325631A/en active Pending
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2002023264A1 (en) * | 2000-09-18 | 2002-03-21 | Ngk Insulators, Ltd. | Optical device |
EP1319973A1 (en) * | 2000-09-18 | 2003-06-18 | Ngk Insulators, Ltd. | Optical device |
EP1319973A4 (en) * | 2000-09-18 | 2004-07-14 | Ngk Insulators Ltd | Optical device |
US7184631B2 (en) | 2000-09-18 | 2007-02-27 | Ngk Insulators, Ltd. | Optical device |
US6961493B2 (en) | 2001-04-18 | 2005-11-01 | Ngk Insulators, Ltd. | Optical device |
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