JPH0358033A - Waveguide type optical device - Google Patents

Waveguide type optical device

Info

Publication number
JPH0358033A
JPH0358033A JP19267989A JP19267989A JPH0358033A JP H0358033 A JPH0358033 A JP H0358033A JP 19267989 A JP19267989 A JP 19267989A JP 19267989 A JP19267989 A JP 19267989A JP H0358033 A JPH0358033 A JP H0358033A
Authority
JP
Japan
Prior art keywords
refractive index
optical
waveguide
thin film
optical waveguide
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.)
Granted
Application number
JP19267989A
Other languages
Japanese (ja)
Other versions
JP2613942B2 (en
Inventor
Yasuhisa Tanizawa
谷澤 靖久
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP1192679A priority Critical patent/JP2613942B2/en
Publication of JPH0358033A publication Critical patent/JPH0358033A/en
Application granted granted Critical
Publication of JP2613942B2 publication Critical patent/JP2613942B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/29Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the position or the direction of light beams, i.e. deflection
    • G02F1/31Digital deflection, i.e. optical switching
    • G02F1/313Digital deflection, i.e. optical switching in an optical waveguide structure
    • G02F1/3132Digital deflection, i.e. optical switching in an optical waveguide structure of directional coupler type

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  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Integrated Circuits (AREA)

Abstract

PURPOSE:To decrease crosstalks and to improve an extinction ratio by forming a thin film having the refractive index higher than the refractive index of optical waveguides and a thin film having the refractive index lower than the refractive index of the optical waveguides between an input side end face and electrodes. CONSTITUTION:A buffer layer 3 consisting of SiO2 is formed at 3000Angstrom on the surface of a waveguide substrate 1 in order to decrease the absorption loss of TM mode light on the electrodes and to make low voltage operation and the electrodes 4 consisting of CrAu are formed atop this layer. The Si thin film 6 (900Angstrom ) having the refractive index higher than the refractive index of the optical waveguides 2 and the SiO2 thin film 5 (2000Angstrom ) having the refractive index lower than the refractive index of the optical wave guides 2 are formed over the entire surface of the region (about 5mm length) on the surface of the substrate 1 between the substrate 1 and the part formed of the input side end face fixed with a constant polarization optical fiber 7 and the electrodes 4. The above-mentioned film thicknesses sufficiently attenuate only the TE mode and do not attenuate the TM mode. The crosstalks are decreased in this way and the extinction ratio is increased.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明はスイッチングや変調機能を有する導波路型光デ
バイスに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a waveguide type optical device having switching and modulation functions.

[従来の技術コ 導波路型光デバイスは強誘電体や半導体材料からなる基
板に光導波路となる屈折率の高い部分を形成し,この光
導波路の上部または近傍に電極を形或し,外部から電圧
を印加することによりスイッチングや光変調を行う光デ
バイスである。
[Conventional technology] In a waveguide type optical device, a high-refractive-index portion that serves as an optical waveguide is formed on a substrate made of a ferroelectric or semiconductor material, and an electrode is formed on or near the optical waveguide. It is an optical device that performs switching and optical modulation by applying voltage.

第2図は従来のこの種の光デバイスの一例を示したもの
であって.電気光学効果を有する強誘電体であるLiH
bO,基板1に導波路パターンをTiで形成し.これを
熱拡散して光導波路2を形成した後,さらにこの光導波
路2の上部あるいは近傍に金属膜により電極4を設け,
上記の機能をもたせた導波路型光デバイスがすでに数多
く研究・開発されている。
Figure 2 shows an example of a conventional optical device of this type. LiH, a ferroelectric material with electro-optic effect
bO, a waveguide pattern is formed on the substrate 1 using Ti. After thermally diffusing this to form an optical waveguide 2, an electrode 4 is further provided with a metal film on or near the optical waveguide 2.
Many waveguide type optical devices having the above functions have already been researched and developed.

これらの導波路型光デバイスは光導波路の上部または近
傍に設けられた電極に電圧を印加し,光導波路に電界を
発生させ,基板のもつ電気光学効果により光導波路の屈
折率を変化させることにより,導波光の伝播定数や位相
を変化させ,所望のスイッチングや光変調機能を得るも
のである。このとき,一般には光導波路の屈折率変化は
基板の電気光学定数により定まり,これは基板の結晶軸
の方向と発生電界により異なる。
These waveguide-type optical devices apply a voltage to an electrode provided on or near the optical waveguide, generate an electric field in the optical waveguide, and change the refractive index of the optical waveguide using the electro-optic effect of the substrate. , by changing the propagation constant and phase of guided light to obtain desired switching and optical modulation functions. At this time, the refractive index change of the optical waveguide is generally determined by the electro-optical constant of the substrate, which varies depending on the direction of the crystal axis of the substrate and the generated electric field.

このため,従来,導波路型光デバイスを設計する場合,
同じ電界強度に対して最も大きく屈折率が変化するよう
に基板の結晶軸と電圧を印加したときの電界発生方向を
定め,これに合わせて導波光の偏波方向が所望の偏光状
態になるように半導体レーザからの直線偏光を定偏波光
ファイバなどを用いて保存して,これをそのまま光導波
路に入射し,導波路基板内でスイッチングや光変調させ
ていた。
For this reason, conventionally, when designing a waveguide type optical device,
The crystal axis of the substrate and the direction of electric field generation when voltage is applied are determined so that the refractive index changes the most for the same electric field strength, and the polarization direction of the guided light is adjusted accordingly to the desired polarization state. In the past, linearly polarized light from a semiconductor laser was stored using a polarization constant optical fiber, etc., and then input directly into an optical waveguide, where it was switched and optically modulated within the waveguide substrate.

例えば,2板L i N b O sを用いたT1拡散
導波路型光スイッチでは.基板表面(全反射面)に光の
電界成分が垂直な導波光(TMモード光)に対して基板
表面に垂直な方向に電界を発生させると,このときの電
気光学定数はL i N b O s結晶がもつ最も大
きい値となり(ri3−2。7〜3.1).低電圧でス
イッチング動作をさせることができる。
For example, in a T1 diffused waveguide optical switch using two plates L i N b O s. When an electric field is generated in a direction perpendicular to the substrate surface for guided light (TM mode light) whose electric field component is perpendicular to the substrate surface (total reflection surface), the electro-optical constant at this time is L i N b O This is the largest value that the s crystal has (ri3-2.7 to 3.1). Switching operation can be performed at low voltage.

[発明が解決しようとする課題] 上述した従来の導波路型光デバイスは,光導波路の導波
光が所望の偏光状態となるように9半導体レーザからの
光を第2図に示すように定偏波光ファイバ7で偏波方向
を保存し.定偏波光ファイバ7の偏波保存方向を光導波
路2の偏波方向に合わせて光学的に結合させている。
[Problems to be Solved by the Invention] The conventional waveguide type optical device described above polarizes the light from the nine semiconductor lasers at a constant polarization as shown in FIG. 2 so that the guided light in the optical waveguide has a desired polarization state. The polarization direction is preserved in the wave optical fiber 7. The polarization-maintaining direction of the polarization-constant optical fiber 7 is matched with the polarization direction of the optical waveguide 2 and optically coupled.

ところが,こうした方法だけで光導波路の導波光の偏光
状態を定めようとすると,定偏波光ファイバの偏波消光
比(主軸を伝播する直線偏光と主紬と直交紬を伝播する
光の割合)が低かったり.また.定偏波光ファイバの偏
波消光比が高くても,定偏波光ファイバの偏波保存方向
と光導波路の偏波方向との角度にずれが生じていると,
光導波路の導波先に所望の偏光と直交する偏光が保存す
ることになり,スイッチング特性や光変調特性が劣化し
てしまうという欠点がある。
However, if we try to determine the polarization state of guided light in an optical waveguide using only these methods, the polarization extinction ratio (ratio of linearly polarized light propagating through the main axis and light propagating through the main axis and the orthogonal axis) of the polarization-controlled optical fiber becomes It was low. Also. Even if the polarization extinction ratio of the polarization-controlled optical fiber is high, if there is a misalignment between the polarization preservation direction of the polarization-controlled optical fiber and the polarization direction of the optical waveguide,
This has the drawback that polarized light orthogonal to the desired polarized light is stored at the waveguide end of the optical waveguide, resulting in deterioration of switching characteristics and optical modulation characteristics.

すなわち,光スイッチにおいては所望の偏光状態をもつ
導波光は完全にスイッチングされるが,直交する偏光は
完全にスイッチングされないので,その分がクロストー
クとなる。また.光変調器においては,所望の偏光状態
と直交する偏光は発生電界により完全には動作しないた
め,変調時の消光比が劣化してしまう。例えば,先述の
2板L i H b 0 3を用いたTi拡散導波路型
光スイッチでは,基板表面゜に電界成分が水平な偏光状
態の導波光(TEモード光)に対しては.電気光学定数
がr ss− 1.1 〜1.4となり,TMモード光
に対するスイッチング電圧では十分なスイッチングがな
されず,この分がクロストークとなる。
That is, in an optical switch, guided light having a desired polarization state is completely switched, but orthogonal polarized light is not completely switched, resulting in crosstalk. Also. In an optical modulator, polarized light perpendicular to the desired polarization state does not operate perfectly due to the generated electric field, resulting in a degradation of the extinction ratio during modulation. For example, in the Ti diffused waveguide optical switch using the two plates L i H b 0 3 described above, for guided light (TE mode light) whose electric field component is in a horizontal polarization state at the substrate surface. The electro-optical constant is r ss-1.1 to 1.4, and the switching voltage for TM mode light does not provide sufficient switching, resulting in crosstalk.

本発明は従来のもののこのような課題を解決し,ストロ
ークを低減し消光比を高めた導波路型光デバイスを提供
するものである。
The present invention solves these problems of the conventional devices and provides a waveguide type optical device that reduces the stroke and increases the extinction ratio.

[課題を解決するための手段] 本発明の導波路型光デバイスは,光導波路の入力側には
光導波路基板表面の光導波路端と電極が形成された部分
の間に光導波路よりも屈折率の低い第1層の薄膜が被膜
され,さらに第1層の薄膜の上面に光導波路よりも屈折
率の高い第2層の薄膜が光導波路の幅よりも広い幅で形
成されていることを特徴としている。
[Means for Solving the Problems] The waveguide type optical device of the present invention has a refractive index higher than that of the optical waveguide on the input side of the optical waveguide between the end of the optical waveguide on the surface of the optical waveguide substrate and the portion where the electrode is formed. A first layer thin film with a low refractive index is coated, and a second layer thin film having a higher refractive index than the optical waveguide is formed on the top surface of the first layer thin film with a width wider than the width of the optical waveguide. It is said that

これは.定偏波光ファイバから光導波路に光を入射する
際に,定偏波光ファイバの偏波消光比が低かったり.あ
るいは定偏波光ファイバの偏波保存方向と光導波路の全
反射面の間に角度ずれが生じ,所望の偏光状態でない光
が光導波路に入射されても,光導波路と上記のjN2層
の薄膜との間に′1s1層を介して位相整合による結合
を不要光に対してのみ起こさせ,この不要光を第2層に
逃がすことができる。ここで.第2層の薄膜の幅を光導
波路の幅よりも広くしておけば、いったん第2層の薄膜
に結合した光は薄膜内で横方向に広がり再び光導波路に
結合することは′ない。
this is. When inputting light from a constant polarization optical fiber to an optical waveguide, the polarization extinction ratio of the constant polarization optical fiber may be low. Alternatively, even if an angular misalignment occurs between the polarization preserving direction of the polarization-controlled optical fiber and the total reflection surface of the optical waveguide, and light that is not in the desired polarization state enters the optical waveguide, the optical waveguide and the above jN2 layer thin film During this time, coupling by phase matching can be caused only for unnecessary light through the '1s1 layer, and this unnecessary light can be released to the second layer. here. If the width of the second layer thin film is made wider than the width of the optical waveguide, the light once coupled to the second layer thin film will spread laterally within the thin film and will not be coupled to the optical waveguide again.

位相整合による結合の条件は,光導波路2第1,2層の
それぞれの屈折率と第1.2各層の薄膜に依存し、導波
光の偏光状態によって異なるので9これらの条件を適当
に設定することにより,不要光のみを除去することがで
きる。
The conditions for coupling by phase matching depend on the refractive index of each of the first and second layers of the optical waveguide 2 and the thin films of the first and second layers, and vary depending on the polarization state of the guided light, so these conditions should be set appropriately. By doing so, only unnecessary light can be removed.

[実施例] 次に,本発明について図面を参照して説明する。[Example] Next, the present invention will be explained with reference to the drawings.

第1図は本発明を2×2導波路型光スイッチに適用した
ときの一実施例の斜視図で,1は強誘電体であるLiN
bO3のZ板であり,図に示すような方向性結合器のパ
ターンをTi膜により形或し.これを1050℃,8時
間熱拡散し,光導波路2を形成する。Z板LiNbO,
基板を用いた光スイッチや光変調器では.光導波路への
入射光の偏光状態を,その電界成分が基板表面に対して
垂直になるようにし,(TMモード光)光導波路に外部
から電界を発生させて動作させたとき.最も基板のもつ
電気光学効果が大きくなり,低電圧でスイッチングや光
変調などの動作を行うことができる。
FIG. 1 is a perspective view of an embodiment of the present invention applied to a 2×2 waveguide type optical switch, and 1 is a ferroelectric LiN
It is a Z plate of bO3, and a directional coupler pattern as shown in the figure is formed using a Ti film. This is thermally diffused at 1050° C. for 8 hours to form the optical waveguide 2. Z plate LiNbO,
In optical switches and optical modulators using substrates. When the polarization state of the light incident on the optical waveguide is set so that its electric field component is perpendicular to the substrate surface, (TM mode light) the optical waveguide is operated by generating an external electric field. The electro-optic effect of the substrate is the greatest, and operations such as switching and optical modulation can be performed with low voltage.

このとき1光導波路に電界を発生させるための電極4を
直線光導波路上部に設けると電極を構成な金属膜による
吸収が起き9導波光の損失が大きくなるので,これを防
ぐため,通常導波路基板1の表面にLiNb03より屈
折率の低いSt02膜をバッファ層3として,該バッフ
ァ層3を介して電極4を形威する。ここでは,導波路基
板1のらなるバッファ層3を被膜し,その上面にCrA
uにより電極4を形成している。
At this time, if an electrode 4 for generating an electric field in the optical waveguide 1 is provided on the top of the straight optical waveguide, absorption by the metal film composing the electrode will occur, increasing the loss of the guided light. An St02 film having a lower refractive index than LiNb03 is used as a buffer layer 3 on the surface of the substrate 1, and an electrode 4 is formed through the buffer layer 3. Here, a buffer layer 3 consisting of a waveguide substrate 1 is coated, and a CrA
The electrode 4 is formed by u.

一方.導波路基板1の端面ば研磨されており.光導波路
2の入出力端面には,光ファイバが光学的に光導波路2
と結合,固着されている。ここで,光スイッチの入力側
(光源側)は半導体レーザからの偏光状態を保持し,光
導波路2の導波光の偏光状態をTMモード光とするため
定偏波光ファイバ7が用いられており.光導波路2との
結合の際も偏波保存方向が導波路基板1の表面と垂直に
なるよウに角度調整されている。以上述べた光スイッチ
の構成は従来の光スイッチの構成と共通している。
on the other hand. The end face of the waveguide substrate 1 is polished. An optical fiber is optically connected to the input/output end face of the optical waveguide 2.
It is combined and fixed with. Here, on the input side (light source side) of the optical switch, a polarization constant optical fiber 7 is used to maintain the polarization state from the semiconductor laser and to change the polarization state of the guided light in the optical waveguide 2 to TM mode light. When coupling with the optical waveguide 2, the angle is also adjusted in such a manner that the polarization preservation direction is perpendicular to the surface of the waveguide substrate 1. The configuration of the optical switch described above is common to that of a conventional optical switch.

本発明の光スイッチでは,上述の導波路基板1の定偏波
光ファイバ7が固着された入力側端面と、電極4が形成
されている部分の間の基板表面の領域全体(約5關長)
に,光導波路よりも屈折率の低いSin.薄115と,
光導波路よりも屈折率の高いSL薄膜6を被膜している
。ここでこのSin.とSiの薄膜を被膜した領域で,
本実施例では,光導波路2を伝播する導波光(TMモー
ド)と直交する偏光状態をもつTEモード光(電界成分
が基板表面に平行な導波光)を減衰させる必要がある。
In the optical switch of the present invention, the entire region (approximately 5 angles) of the substrate surface between the input side end face of the waveguide substrate 1 to which the polarization-controlled optical fiber 7 is fixed and the portion where the electrode 4 is formed
In addition, Sin. has a lower refractive index than the optical waveguide. Thin 115 and
It is coated with an SL thin film 6 having a higher refractive index than the optical waveguide. Here this Sin. In the area coated with a thin film of Si,
In this embodiment, it is necessary to attenuate TE mode light (guided light whose electric field component is parallel to the substrate surface) having a polarization state perpendicular to the guided light (TM mode) propagating through the optical waveguide 2.

Sin.とS1の薄膜のそれぞれの膜厚εTEモードの
減衰量との関係は第3図に示されるとおりである。ここ
ではTEモードのみを十分減衰させ,TMモードに対し
ては減衰しない次に,従来の光スイッチと本発明の構成
を用いた光スイッチのスイッチング特性評優結果につい
て説明する。第4図(a) (b)はそれぞれ従来の光
スイッチと本発明による光スイッチのスイッチング特性
を示している。第4図からわかるように。従来の光スイ
ッチでは入力側の定偏光ファイバ7のもつ偏波消光比が
約15〜20dBであり,また光導波路2と定偏波光フ
ァイバ7の結合や固着時の偏波方向の角度合わせのずれ
(約1度)から,光導波路2を伝播する導波光のTM/
TE偏波消光比は10〜15dB程度となり,電極4に
電圧を印加しスイッチングさせたとて,TMモード光は
約5.5vの電圧印加時でも約20dB程度しかクロス
トークを低下させることができない。これは約5.5v
電圧印加時でもTEモードに対する電気光学的効果が小
さいため( r s3=(LI8)4 ss”) . 
T Eモードがほとんどスイッチング動作しておらず.
しかも導波光の偏波消光比が約10〜15dBと低いた
めに十分なスイッチングをしていない。TE七−ドの影
響を受けこれがクロストーク分となるからである。
Sin. The relationship between the film thickness ε of the thin film S1 and the attenuation amount of the TE mode is as shown in FIG. Here, only the TE mode is sufficiently attenuated, and the TM mode is not attenuated.Next, the evaluation results of the switching characteristics of the conventional optical switch and the optical switch using the configuration of the present invention will be explained. FIGS. 4(a) and 4(b) show the switching characteristics of a conventional optical switch and an optical switch according to the present invention, respectively. As can be seen from Figure 4. In a conventional optical switch, the polarization extinction ratio of the input-side polarized optical fiber 7 is about 15 to 20 dB, and there is also a difference in the angle alignment of the polarization direction when the optical waveguide 2 and the polarized optical fiber 7 are coupled or fixed. (approximately 1 degree), the TM/ of the guided light propagating through the optical waveguide 2
The TE polarization extinction ratio is about 10 to 15 dB, and even when a voltage is applied to the electrode 4 for switching, the crosstalk of TM mode light can only be reduced by about 20 dB even when a voltage of about 5.5 V is applied. This is about 5.5v
Even when voltage is applied, the electro-optical effect on the TE mode is small (rs3=(LI8)4ss").
TE mode is hardly switching.
Moreover, since the polarization extinction ratio of the guided light is as low as about 10 to 15 dB, sufficient switching is not performed. This is because it is affected by the TE7-code and becomes a crosstalk component.

一方本発明の構成の光スイッチでは。Si02,Si薄
膜を被膜した5uの長さの領域でTEモードが約10d
Bの減衰をしているため. 5.5 V電圧印加時にT
Eモードが十分スイッチングしていなくても,導波光の
偏波消光比が20〜25dBと改善されているため,ス
イッチング動作時のクロストークは30dBと大幅に低
下している。
On the other hand, in the optical switch configured according to the present invention. The TE mode is about 10d in a 5u long region coated with Si02, Si thin film.
Because B is attenuated. T when 5.5 V voltage is applied
Even if the E mode is not sufficiently switched, the polarization extinction ratio of the guided light is improved to 20 to 25 dB, so crosstalk during switching operation is significantly reduced to 30 dB.

[発明の効果コ 以上説明したように本発明は.導波路型光デバイスの基
板表面の入力側端面と電極が形成されている部分との間
に,光導波路よりも屈折率の低い第1層の薄膜とその上
面に光導波路よりも屈折率が高くかつ光導波路の幅より
も広い範囲にわたって第2層の薄膜を被膜することによ
り.実際に光導波路基板内でスイッチングや光変調を行
う所望の偏光状態をもつ導波光以外の導波光を減衰させ
,クロストークを低減したり消光比を高めたりできる効
果がある。
[Effects of the Invention] As explained above, the present invention has... Between the input side end face of the substrate surface of the waveguide type optical device and the part where the electrode is formed, there is a first layer thin film having a lower refractive index than the optical waveguide, and a first layer thin film having a refractive index higher than the optical waveguide on the upper surface. And by coating a second layer of thin film over a wider area than the width of the optical waveguide. This has the effect of attenuating guided light other than the guided light with the desired polarization state that is actually used for switching and optical modulation within the optical waveguide substrate, reducing crosstalk and increasing the extinction ratio.

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

第1図は本発明の導波路型光デバイスの一実施例の斜視
図.第2図は従来の導波路型光デバイスの一例の斜視図
.第3図は導波路基板上面に被膜した2層の薄膜にS1
02とStを用いた場合の膜厚と導波光の減衰との関係
を示す図,第4図(a) (b)は従来の導波路型デバ
イスと本発明による光スイッチのスイッチング特性を示
す図である。 記号の説明:1・・・導波路基板、2・・・光導波路,
3・・・バッファ層,4・・・電極,5・・・Sin2
薄膜,6・・・St薄膜,7・・・定偏波光ファイバ、
8・・・シングルモード光ファイバ。 第1図 11M路屡板 第2図 第3図 Sj膜厚(A) 第4図
FIG. 1 is a perspective view of an embodiment of the waveguide type optical device of the present invention. Figure 2 is a perspective view of an example of a conventional waveguide type optical device. Figure 3 shows the two-layer thin film S1 coated on the top surface of the waveguide substrate.
4(a) and 4(b) are diagrams showing the switching characteristics of a conventional waveguide type device and an optical switch according to the present invention. It is. Explanation of symbols: 1... Waveguide substrate, 2... Optical waveguide,
3... Buffer layer, 4... Electrode, 5... Sin2
Thin film, 6... St thin film, 7... Constant polarization optical fiber,
8...Single mode optical fiber. Fig. 1 11M road board Fig. 2 Fig. 3 Sj film thickness (A) Fig. 4

Claims (1)

【特許請求の範囲】[Claims] 1、基板表面に光導波路と該光導波路の上部または近傍
に電極が形成され、前記基板に形成された光導波路の入
出力端面には光ファイバが光学的に結合している導波路
型光デバイスにおいて、前記光導波路の入力側には光導
波路基板表面の光導波路端と前記電極が形成された部分
との間に光導波路よりも屈折率の低い第1層の薄膜が被
膜され、さらに第1層の薄膜の上面に前記光導波路より
も屈折率の高い第2層の薄膜が前記光導波路の幅よりも
広い幅で形成されていることを特徴とする導波路型光デ
バイス。
1. A waveguide type optical device in which an optical waveguide is formed on the surface of a substrate and an electrode is formed on or near the optical waveguide, and an optical fiber is optically coupled to the input/output end face of the optical waveguide formed on the substrate. In the input side of the optical waveguide, a first layer thin film having a refractive index lower than that of the optical waveguide is coated between the optical waveguide end of the surface of the optical waveguide substrate and the portion where the electrode is formed, and a first layer thin film having a refractive index lower than that of the optical waveguide is coated. A waveguide-type optical device characterized in that a second layer thin film having a higher refractive index than the optical waveguide is formed on an upper surface of the layer thin film, and has a width wider than the width of the optical waveguide.
JP1192679A 1989-07-27 1989-07-27 Waveguide type optical device Expired - Lifetime JP2613942B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1192679A JP2613942B2 (en) 1989-07-27 1989-07-27 Waveguide type optical device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1192679A JP2613942B2 (en) 1989-07-27 1989-07-27 Waveguide type optical device

Publications (2)

Publication Number Publication Date
JPH0358033A true JPH0358033A (en) 1991-03-13
JP2613942B2 JP2613942B2 (en) 1997-05-28

Family

ID=16295244

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1192679A Expired - Lifetime JP2613942B2 (en) 1989-07-27 1989-07-27 Waveguide type optical device

Country Status (1)

Country Link
JP (1) JP2613942B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5483609A (en) * 1993-07-09 1996-01-09 Nec Corporation Optical device with mode absorbing films deposited on both sides of a waveguide
JPH0980364A (en) * 1995-09-13 1997-03-28 Nec Corp Waveguide type optical device

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5313198B2 (en) * 2010-03-30 2013-10-09 住友大阪セメント株式会社 Waveguide polarizer

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5632601A (en) * 1979-08-24 1981-04-02 Matsushita Electric Works Ltd Method of illuminating stair and illuminator
JPS62133428A (en) * 1985-12-05 1987-06-16 Nippon Telegr & Teleph Corp <Ntt> Optical switch

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5632601A (en) * 1979-08-24 1981-04-02 Matsushita Electric Works Ltd Method of illuminating stair and illuminator
JPS62133428A (en) * 1985-12-05 1987-06-16 Nippon Telegr & Teleph Corp <Ntt> Optical switch

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5483609A (en) * 1993-07-09 1996-01-09 Nec Corporation Optical device with mode absorbing films deposited on both sides of a waveguide
JPH0980364A (en) * 1995-09-13 1997-03-28 Nec Corp Waveguide type optical device

Also Published As

Publication number Publication date
JP2613942B2 (en) 1997-05-28

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