JPS58142320A - Waveguide type optical switch - Google Patents
Waveguide type optical switchInfo
- Publication number
- JPS58142320A JPS58142320A JP2279282A JP2279282A JPS58142320A JP S58142320 A JPS58142320 A JP S58142320A JP 2279282 A JP2279282 A JP 2279282A JP 2279282 A JP2279282 A JP 2279282A JP S58142320 A JPS58142320 A JP S58142320A
- Authority
- JP
- Japan
- Prior art keywords
- lens
- waveguide
- optical
- light
- crystal
- 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
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL 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
- G02F1/00—Devices 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
- G02F1/29—Devices 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
- G02F1/31—Digital deflection, i.e. optical switching
- G02F1/313—Digital deflection, i.e. optical switching in an optical waveguide structure
- G02F1/3137—Digital deflection, i.e. optical switching in an optical waveguide structure with intersecting or branching waveguides, e.g. X-switches and Y-junctions
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Integrated Circuits (AREA)
Abstract
Description
【発明の詳細な説明】 (1)発明の技術分野 不発#iは導波路形光スイッチに関する。[Detailed description of the invention] (1) Technical field of the invention Misfiring #i relates to a waveguide type optical switch.
(2)技術の背景
近年通信システムにお妙る伝送ts体として光を用いる
揚台が多くなった。これに元信号が一気傷号に比して優
れ九通信特性を示すからである。このような光通信シス
テムの斃展に伴いea+xデバイスが提案され改良が加
えられている。このような各種デバイスの中で特に不発
aAに導波路形光スイッチに言反する。(2) Background of the technology In recent years, there has been an increase in the number of platforms that use light as a transmission medium for communication systems. This is because the original signal exhibits better communication characteristics than the original signal. With the expansion of such optical communication systems, ea+x devices have been proposed and improved. Among these various devices, the unfired aA is particularly contradictory to the waveguide type optical switch.
(3) 従来技術と間融点
第1図に一般的な導波路形光スィッチ0基本構成を示す
平自図である。本−において、参照番号11flそれぞ
れ光7アイパーを示し、これら光7アづパー11の間に
導波路形光スイッチ10が挿入される。元スイッチ1O
fl’l[錦電体結晶例えはニオブ酸リチウムからなり
、その表面層内に2本の光導波路12−1および12−
2が交差して形成される。例えばチタンの拡散によって
形成される。さらに、その交差の部分に平板状の電極対
14および14’が配置される。(3) Prior art and melting point FIG. 1 is a plan view showing the basic configuration of a general waveguide type optical switch. In this case, reference numeral 11fl indicates seven optical eyelets, and a waveguide type optical switch 10 is inserted between these optical seven eyeers 11. Original switch 1O
fl'l [The brocade crystal is made of lithium niobate, and has two optical waveguides 12-1 and 12- in its surface layer.
2 are formed by crossing each other. For example, it is formed by diffusion of titanium. Furthermore, a flat electrode pair 14 and 14' is arranged at the intersection.
今、入力元Pが融水するように照射されたものとすると
、#入力光Pは元ファイバー11”(左下)→光導波路
12−1→光ファイバー11(右上)の経路管通って出
力光Pok得る。この揚台、電極対14.14’には電
圧<V>が印加されておらず、これらの間の電界は零で
ある。ところが、電極対14 、 l 4’に電圧(V
)を印加して、これらの間に電界を生じさせると、今F
ILは、前記入力光Pが1元ファイバー11(左下)→
光導波路12−1→光導波路12−2→光7アイパー1
1(右下)の経路を通って出力光P。を得る。ここに出
力光P。はスイッチをその1箇スルーで通夕抜けた光を
表わし、出力光P。はスイッチでスイッチされ九yt、
を表わす。このような元スイッチの一使朗例を挙けると
入力Jjt、Pに乗っているアドレス信号を出力光〜で
検出して、そのアドレスが本スイッチのものであれば、
スイッチを動作させ、入力光Pを出力光P。へ導き、光
信号tスイッチさぜることができ、電子交1sfI1.
にとって代わることができる。Now, assuming that the input source P is irradiated so as to melt water, the #input light P passes through the path pipe of original fiber 11" (lower left) → optical waveguide 12-1 → optical fiber 11 (upper right) and outputs light P. On this platform, no voltage <V> is applied to the electrode pair 14, 14', and the electric field between them is zero. However, a voltage (V) is applied to the electrode pair 14, 14'.
) to create an electric field between them, now F
In IL, the input light P is connected to a single fiber 11 (bottom left) →
Optical waveguide 12-1 → Optical waveguide 12-2 → Optical 7 Eyeper 1
Output light P passes through path 1 (bottom right). get. Here is the output light P. represents the light that passes through one switch, and the output light P. is switched with a switch and nine yt,
represents. To give a good example of the use of such an original switch, if the address signal on the inputs Jjt and P is detected by the output light ~, and the address belongs to the main switch,
Operate the switch to convert input light P to output light P. The optical signal t switch can be guided to the electronic exchange 1sfI1.
can be replaced.
總1rkJに示した光スイッチには未だ樵々改良すべき
点が多々ある。本発明においては1%に、Cれら改良す
べき点の中で消光比に着目する。すなわち、従来の元ス
イッチでは消光比を十分に大きく探れず、光スィッチと
しての性能上改良を景するところであった。The optical switch shown in 1rkJ still has many points to be improved. In the present invention, attention is paid to the extinction ratio of 1% among the points to be improved. In other words, with the conventional original switch, it was not possible to find a sufficiently large extinction ratio, and there was a need for improvement in terms of performance as an optical switch.
@2図は導波路形光スイッチの消光比91rこついて貌
明するためのグラフである。本グラフにおいて機軸には
電極対14 、14’ (第11)への印加電圧■【採
シ、縦軸には出力光〜2.〜の出カパワーPWt採る。Figure @2 is a graph to clarify the extinction ratio 91r of a waveguide type optical switch. In this graph, the mechanical axis shows the voltage applied to the electrode pair 14, 14' (11th), and the vertical axis shows the output light ~2. Take the output power PWt of ~.
横軸上のswは、光スィッチのスイッチ切替時を示す。sw on the horizontal axis indicates the switching time of the optical switch.
本グ27申記号P。onnススルーモード0出カツ切t
−表わし”(,1offはスルーモードを停止したとき
の出力パワーを表わす。又、記号P。。7.はスイッチ
モードを停止したときの出カー量ワー1ゎし’ %!J
on ’ %)o工はスイッチモード時の出力ノリ−を
表わす。本グラフ中特に点線のカーブy。onIa、従
来における特性に係り、実線のカーツー。n線後述する
本発明に係る特性である。消光比は本グラフ中の出カバ
従米におけるこの1iIに1例えば12.6 dBであ
る。Book 27 Monkey symbol P. onn through mode 0 cutoff
-Representation"(,1off represents the output power when the through mode is stopped. Also, the symbol P.7. is the output power when the switch mode is stopped. %!J
on' %)o represents the output flow in switch mode. In this graph, especially the dotted curve y. onIa, regarding the conventional characteristics, the solid line is CAR2. This is a characteristic related to the present invention for the n-line, which will be described later. The extinction ratio is, for example, 12.6 dB per 1iI of the output power in this graph.
第211に示すグラフにおいて、従来の特性(点線のカ
ーブ)でにスイッチ効率が悪く、前記のレベル差t−R
’からRC)ように引き上げ消光比の改良′t−纏るこ
とが望まれている。In the graph shown in No. 211, the switching efficiency is poor with the conventional characteristics (dotted line curve), and the level difference t-R
It is desired to improve the extinction ratio by increasing the extinction ratio from ' to RC).
(4) 発明の目的
本発明は上述した消光比の不良に鎌み、消光比の大幅な
改善11gJ侍し得る導波路形光スイッチを提案する仁
とを目的とするものである。(4) Object of the Invention The object of the present invention is to solve the problem of the above-mentioned poor extinction ratio and to propose a waveguide type optical switch that can significantly improve the extinction ratio by 11 gJ.
(5)発明の構成
上記の目的は、入力元が電極対に向って集束するような
光集束形の#膜状レンズを光導波路上に構成することに
より達成される。(5) Structure of the Invention The above object is achieved by configuring a light-focusing type film-like lens on an optical waveguide so that an input source is focused toward a pair of electrodes.
(6)発明の実施例 以下本発明の実施例t−図面によp親切する。(6) Examples of the invention Embodiments of the present invention will be described below with reference to the drawings.
第3図は本発明に基づく一夾&!I例を示す斜視地であ
る。本−において、参照瞥号31が本発明の特徴tな1
薄膜状−レンズであり、光集束形でるる。Figure 3 shows Ichikyo &! based on the present invention. This is a perspective view showing Example I. In this book, reference number 31 is a feature of the present invention.
Thin film-like lens, light focusing type.
その他の構成については、歓略に飲明級みでめ2.。For other configurations, please feel free to ask me if you have any questions. .
すなわち番照査号33がgk肪電体結晶であり、(の表
面!kV3には5Z差して2本の九番波路32−1およ
び32−2(第1−の12−1および12−2)が形成
される。その交差部分には平板上・の亀&#a 4 、
34’ (第1−の14.14’)が設けられる。
。That is, the number reference number 33 is a gk adielectric crystal, and the surface of is formed.At the intersection, a turtle on a flat plate &#a4,
34'(1-14.14') is provided.
.
レンズ31框−示する位置に飄がれる。その位litは
、入力元Pが電極対34および34′に向って集束する
ような位置でるる。Lens 31 frame - swivels to the position shown. The position lit is such that the input source P is focused towards the electrode pair 34 and 34'.
このようなレンズ効果を与えることによって。By giving a lens effect like this.
所期の目的は達成される。夾験例で示せば、既述の@2
図のグラフ中、実−のカーブへ。。で示すとおりでTo
り、レベル差は従来のR′からRに増大する。数値で表
わすと、既述の消光比12.6dBから15.5 dB
に引き上けられる。たたし、このよ5なレンズ効果の付
与によって、如何に消元比の改良がなされ友かについて
の理論的な静軸は現段階で扛明らかではない。いずれに
しても、デバイス上は、かようなレンズを光導波路上に
形成しておけに消光比は増大できる。The intended purpose is achieved. If you show it with a trial example, the above @2
In the graph shown in the figure, go to the actual curve. . As shown in To
As a result, the level difference increases from the conventional R' to R. Expressed numerically, the extinction ratio is from 12.6 dB to 15.5 dB.
be lifted up. However, the theoretical static axis as to how the extinction ratio is improved by adding such a lens effect is not clear at this stage. In any case, the extinction ratio can be increased by forming such a lens on the optical waveguide of the device.
前述したレンズ効果を生じさせるためには、単にレンズ
31を設けただりでは不十分でToシ、屈折率KIII
して一定の条件が必要である。これt−5tt4図會参
照して説明する。i84図は琳3図の2イン4−4で切
断した断FB−である。ここにレンズ31の屈折率t
nl s光導波路32−1の屈折率【nss強誘電体結
晶33のそれをnlとすると、ns>nl>ns
なる関係に設定する。そうすると、ii4図に矢印をも
って示すごとく、入力光Pの一部は光導波路32−1よ
りレンズ31内に吸い上けられ(nl〉nl)、レンズ
の集束作用を受けて再び元の光導波路32−1円に戻る
。なお1強酵電体結晶33内で特に光導波路32−1中
に光を閉じ込めるべくnt>nso胸係を要する。In order to produce the above-mentioned lens effect, simply providing the lens 31 is insufficient; however, the refractive index KIII is insufficient.
Certain conditions are required. This will be explained with reference to Figure t-5tt4. Figure i84 is a 2-in 4-4 section FB- of Figure Rin3. Here, the refractive index t of the lens 31
The refractive index of the nl s optical waveguide 32-1 [nss, where nl is that of the ferroelectric crystal 33, is set to the relationship ns>nl>ns. Then, as shown by the arrow in Figure ii4, a part of the input light P is sucked up from the optical waveguide 32-1 into the lens 31 (nl>nl), and is returned to the original optical waveguide 32 after receiving the focusing action of the lens. - Return to 1 yen. Note that in order to confine light particularly in the optical waveguide 32-1 within the one-strong electrolyte crystal 33, a nt>nso coupling is required.
(7) 発明の詳細
な説明したように本発明によれは、消光比の同上がwJ
侍される導波路形九ス1クチが夫玩嘔れる。(7) As described in detail, according to the present invention, the extinction ratio is equal to wJ
The waveguide-shaped nine crosses that are served by the attendant are drowning in pain.
累1図に一般的な導波路彩光スイッチのi仝楕成會示す
平■図、@2&Jは導肢路形元スイッチの消光比%性に
ついて12明するためのグン7.絽3図に本発明に基づ
〈一実施例を示す斜視図、第4−は1143図の2イン
4−4で切断した断面−である。
31・・・IIIII状レンズ、32−1.32−2・
・光導波路、33・・・強酵亀体結晶、34.34’・
・・lIE&対。
特許出願人
富士通株式会社
特許出願代塩入
弁理士 青 木 朗
弁理士 画 舘 和 之
弁理士 内 1)幸 男
弁理士 山 口 昭 之
第1図
第2図
)W v→Figure 1 shows the i-ellipse formation of a general waveguide chromatic switch, and @2&J shows Gun 7. Figure 3 is a perspective view showing one embodiment of the present invention, and Figure 4 is a cross section taken at 2-in 4-4 in Figure 1143. 31...III-shaped lens, 32-1.32-2.
・Optical waveguide, 33...strongly fermented turtle crystal, 34.34'・
...lIE&vs. Patent applicant Fujitsu Ltd. Patent application agent Akira Shioiri, patent attorney Patent attorney Akira Aoki Illustrations Kazuyuki Tate Patent attorney 1) Yukio Patent attorney Akira Yamaguchi (Figure 1, Figure 2) W v →
Claims (1)
の光導波路と、前記の交差Os分に択一的に電界を形成
する平板状の電極対とを有し、#電界の有無に応じてそ
れぞれ前記光導波路を伝搬する光の光路を一方の皺先導
波路から他方の該光導波路ヘスイッチし又は皺光會スイ
ッチしないようにし九等波路形元スイッチにおいて、前
記強誘電体結晶の表WJIIi上に光集束形の薄膜状レ
ンズを形成し、ここに該薄膜状レンズはこれt通過した
前記光が前記電極対に集束する位置に配置され、且つ前
記薄膜状レンズ、光等波路および強誘電体結晶の各屈折
率をそれぞれn1*nff1、および幻とすると、これ
らの間の関係がns>nt>n婁 に設定されることを特徴とする導波路形光スイッチ。[Claims] 1. Two optical waveguides formed to intersect within the surface layer of a ferroelectric crystal, and a pair of flat electrodes that selectively form an electric field at the intersection Os. # Switches the optical path of light propagating through the optical waveguide from one wrinkle-guided waveguide to the other optical waveguide depending on the presence or absence of an electric field, or prevents the wrinkle-guided waveguide from switching. , a light-focusing thin film lens is formed on the surface WJIIi of the ferroelectric crystal, the thin film lens is disposed at a position where the light passing through the lens is focused on the electrode pair; A waveguide shape characterized in that, assuming that the refractive indices of the shaped lens, the optical wave path, and the ferroelectric crystal are respectively n1*nff1 and phantom, the relationship between them is set to ns>nt>nru. light switch.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2279282A JPS58142320A (en) | 1982-02-17 | 1982-02-17 | Waveguide type optical switch |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2279282A JPS58142320A (en) | 1982-02-17 | 1982-02-17 | Waveguide type optical switch |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS58142320A true JPS58142320A (en) | 1983-08-24 |
Family
ID=12092525
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2279282A Pending JPS58142320A (en) | 1982-02-17 | 1982-02-17 | Waveguide type optical switch |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58142320A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60147716A (en) * | 1984-01-11 | 1985-08-03 | Nec Corp | Optical transmitter of extinction ratio control |
JPS6285228A (en) * | 1985-10-09 | 1987-04-18 | Tokyo Inst Of Technol | Y-branch selective optical waveguide |
-
1982
- 1982-02-17 JP JP2279282A patent/JPS58142320A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60147716A (en) * | 1984-01-11 | 1985-08-03 | Nec Corp | Optical transmitter of extinction ratio control |
JPS6285228A (en) * | 1985-10-09 | 1987-04-18 | Tokyo Inst Of Technol | Y-branch selective optical waveguide |
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