JPS6150293B2 - - Google Patents
Info
- Publication number
- JPS6150293B2 JPS6150293B2 JP7686180A JP7686180A JPS6150293B2 JP S6150293 B2 JPS6150293 B2 JP S6150293B2 JP 7686180 A JP7686180 A JP 7686180A JP 7686180 A JP7686180 A JP 7686180A JP S6150293 B2 JPS6150293 B2 JP S6150293B2
- Authority
- JP
- Japan
- Prior art keywords
- refractive index
- optical waveguide
- waveguide film
- low refractive
- film
- 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
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/35—Optical coupling means having switching means
- G02B6/3536—Optical coupling means having switching means involving evanescent coupling variation, e.g. by a moving element such as a membrane which changes the effective refractive index
-
- 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
- G02F1/315—Digital deflection, i.e. optical switching based on the use of controlled internal reflection
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/35—Optical coupling means having switching means
- G02B6/354—Switching arrangements, i.e. number of input/output ports and interconnection types
- G02B6/3544—2D constellations, i.e. with switching elements and switched beams located in a plane
- G02B6/3546—NxM switch, i.e. a regular array of switches elements of matrix type constellation
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/35—Optical coupling means having switching means
- G02B6/3596—With planar waveguide arrangement, i.e. in a substrate, regardless if actuating mechanism is outside the substrate
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Mechanical Light Control Or Optical Switches (AREA)
- Optical Integrated Circuits (AREA)
Description
【発明の詳細な説明】
本発明は、薄膜光導波路を利用した複数入力、
複数出力の薄膜光スイツチ回路に関するものであ
る。DETAILED DESCRIPTION OF THE INVENTION The present invention provides multiple inputs using thin film optical waveguides,
This invention relates to a thin film optical switch circuit with multiple outputs.
従来、光導波路を利用した複数入力、複数出力
の薄膜光スイツチ回路では、その構成要素の1入
力2出力もしくは2入力2出力の光スイツチ素子
に電気光学効果または音響光学効果による光の偏
向を用いている。しかしこれらの光スイツチ素子
では、偏向角が高々2゜以下と小さい。従つてこ
れらの素子を組み合わせて複数入力、複数出力の
光スイツチ回路を構成しようとすると、偏向角が
小さいので、著しく長い導波膜を要し、形状が大
きくなるとともに、伝搬損失も無視できなくなる
という欠点があつた。 Conventionally, in multi-input, multi-output thin film optical switch circuits using optical waveguides, light deflection using the electro-optic effect or acousto-optic effect is used for the 1-input, 2-output or 2-input, 2-output optical switch elements that are the constituent elements. ing. However, in these optical switch elements, the deflection angle is as small as 2° or less. Therefore, if you try to combine these elements to construct an optical switch circuit with multiple inputs and multiple outputs, the deflection angle is small, so you will need an extremely long waveguide film, which will increase the size and cause propagation loss to become non-negligible. There was a drawback.
本発明はこれらの欠点を解決するため、光導波
路の等価屈折率を変えることにより、従来に比べ
て大きい偏向角が得られる光スイツチ素子を用
い、これを構成要素とした複数入力、複数出力の
薄膜光スイツチ回路を提供するものである。以下
図面により本発明を詳細に説明する。 In order to solve these drawbacks, the present invention uses an optical switch element that can obtain a larger deflection angle than conventional ones by changing the equivalent refractive index of the optical waveguide, and uses this element as a component for multiple inputs and multiple outputs. A thin film optical switch circuit is provided. The present invention will be explained in detail below with reference to the drawings.
第1図は本発明の薄膜光スイツチ回路の構成要
素の2入力2出力の光スイツチ素子の斜視図であ
る。第2図は該光スイツチ素子の断面図である。
この光スイツチ素子は、特願昭55−003474「薄膜
型光偏向素子」に記載のものと同様であるが、簡
単にその構造と動作を説明する。 FIG. 1 is a perspective view of a two-input, two-output optical switch element that is a component of the thin film optical switch circuit of the present invention. FIG. 2 is a sectional view of the optical switch element.
This optical switch element is similar to that described in Japanese Patent Application No. 55-003474 "Thin Film Type Optical Deflection Element", and its structure and operation will be briefly explained.
基板1の上に光導波膜2を所定の厚みに積層す
る。第1図に示すように、以下の説明上、光導波
膜2の面内にxy直交座標軸およびこれらに垂直
にz軸をとる。光導波膜2のx軸方向に直線状の
低屈折率領域2′を形成し、その上に中間層3
(第1図および第2図では空気層にしてある)を
介してxy面に平行な底面を有する可動誘電体片
4を設ける。可動誘電体片をz軸方向に上下させ
るため、可動誘電体片4と機械的に接続した誘電
体片駆動部5(たとえば圧電バイモルフ)と、さ
らに誘電体片駆動部5と電気的に接続した駆動回
路6を設ける。基板1、光導波膜2、低屈折率領
域2′、中間層3、可動誘電体片4の屈折率をそ
れぞれn1、n2、n2′、n3、n4とし、n2>n2′>n4>
(n1、n3)の関係を満たすようにする。第1図に示
すように、光導波膜2中の低屈折率領域2′に導
光波7および7′が入射すると、これらは入射角
度θに応じて低屈折率領域2′で全反射または透
過する。ここで低屈折率領域2′の屈折率分布は
ステツプ型でもグレーテツド型でもよいが、第1
図はグレーテツド型の場合(y軸方向にグレーテ
ツド型になつている。)で、光偏向が低屈折率領
域2′の中央で生じている。この場合、前記の屈
折率n2′は、低屈折率領域2′のy軸方向の中心の
値である。さてここで、第2図に示す可動誘電体
片4と光導波膜2との距離l3と、低屈折率領域
2′における全反射条件の関係を考える。距離l3
が光導波膜2の膜厚より大きいときの光導波膜2
および低屈折率領域2′の中心の等価屈折率をν
0およびν0′とする。またl3が光導波膜2の膜厚
より十分に小さいときの光導波膜2および低屈折
率領域2′の中心の等価屈折率をνおよびν′とす
る。等価屈折率ν0、ν0′、ν、ν′は前記特願
昭55−003474に記載の固有方程式で求められる。
この固有方程式によればν0、ν0′、ν、ν′の
間にはν′/ν>ν0′/ν0なる関係がある。そ
こで導波光7および7′の低屈折率領域2′への入
射角θが
ν′/ν>cosθ>ν0′/ν0 ……(1)
を満足するようにとる。このようにすると、l3が
前述のように大きい場合、すなわち可動誘電体片
4を光導波膜2から遠ざけた場合には、全反射条
件が満足されて、入射導波光7は全反射して出力
導波光8となり、入射導波光7′もまた全反射し
て出力導光波8′となる。 An optical waveguide film 2 is laminated on a substrate 1 to a predetermined thickness. As shown in FIG. 1, for the following explanation, x and y orthogonal coordinate axes and a z axis perpendicular to these are taken within the plane of the optical waveguide film 2. A linear low refractive index region 2' is formed in the x-axis direction of the optical waveguide film 2, and an intermediate layer 3 is formed thereon.
A movable dielectric piece 4 having a bottom parallel to the xy plane is provided via an air layer (which is shown as an air layer in FIGS. 1 and 2). In order to move the movable dielectric piece up and down in the z-axis direction, a dielectric piece drive unit 5 (for example, a piezoelectric bimorph) is mechanically connected to the movable dielectric piece 4, and a dielectric piece drive unit 5 is electrically connected to the dielectric piece drive unit 5. A drive circuit 6 is provided. The refractive indices of the substrate 1, optical waveguide film 2, low refractive index region 2', intermediate layer 3, and movable dielectric piece 4 are respectively n 1 , n 2 , n 2 ', n 3 , and n 4 , and n 2 > n 2 ′>n 4 >
The relationship (n 1 , n 3 ) should be satisfied. As shown in FIG. 1, when the guided waves 7 and 7' are incident on the low refractive index region 2' in the optical waveguide film 2, they are totally reflected or transmitted in the low refractive index region 2' depending on the incident angle θ. do. Here, the refractive index distribution of the low refractive index region 2' may be either a step type or a graded type.
The figure shows a case of a graded type (graded type in the y-axis direction), where light deflection occurs at the center of the low refractive index region 2'. In this case, the refractive index n 2 ' is the value at the center of the low refractive index region 2' in the y-axis direction. Now, consider the relationship between the distance l 3 between the movable dielectric piece 4 and the optical waveguide film 2 shown in FIG. 2, and the total reflection condition in the low refractive index region 2'. distance l 3
is larger than the film thickness of the optical waveguide film 2.
and the equivalent refractive index at the center of the low refractive index region 2' is ν
0 and ν 0 '. Further, when l 3 is sufficiently smaller than the film thickness of the optical waveguide film 2, the equivalent refractive indexes at the center of the optical waveguide film 2 and the low refractive index region 2' are assumed to be ν and ν'. The equivalent refractive indices ν 0 , ν 0 ', ν, ν' are determined by the characteristic equations described in the above-mentioned Japanese Patent Application No. 55-003474.
According to this characteristic equation, there is a relationship between ν 0 , ν 0 ', ν, and ν' such that ν'/ν>ν 0 '/ν 0 . Therefore, the incident angle θ of the guided light beams 7 and 7' into the low refractive index region 2' is set so as to satisfy ν'/ν>cosθ>ν 0 '/ν 0 (1). In this way, when l 3 is large as described above, that is, when the movable dielectric piece 4 is moved away from the optical waveguide film 2, the total reflection condition is satisfied and the incident guided wave light 7 is totally reflected. The output guided wave 8 becomes the output guided wave 8, and the incident guided wave 7' is also totally reflected to become the output guided wave 8'.
一方、l3が前述のように十分に小さい場合、す
なわち可動誘電体片4を光導波膜2に近づけた場
合には、全反射条件が満足されなくなり、入射導
波光7は低屈折率領域2′を透過して出力導波光
8′となり、入射導波光7′もまた透過して出力導
波光8となる。 On the other hand, when l 3 is sufficiently small as described above, that is, when the movable dielectric piece 4 is brought close to the optical waveguide film 2, the total internal reflection condition is no longer satisfied, and the incident guided light 7 passes through the low refractive index region 2. The incident guided light 7' also passes through and becomes the output guided light 8.
この場合の出力導波光8および8′の分岐角度
は第1図から明らかなように2θで与えられる。
分岐角度2θは、光導波膜2と低屈折率領域2′
の比屈折率差n2−n2′/n2を2%とすると20゜以
上の
角度が得られ、この程度の比屈折率差は、特開昭
54−161350「薄膜光素子の製造方法」および特開
昭53−71845「光導波薄膜とその作製法」によれ
ば簡単に得られる。実際にこのようなスイツチ素
子を駆動するには、駆動回路6から駆動信号を誘
電体駆動部5に送り、可動誘電体片4を上下させ
る。 In this case, the branching angle of the output guided beams 8 and 8' is given by 2θ, as is clear from FIG.
The branching angle 2θ is between the optical waveguide film 2 and the low refractive index region 2'.
If the relative refractive index difference n 2 - n 2 '/n 2 is 2%, an angle of 20° or more can be obtained, and this degree of relative refractive index difference was
54-161350 "Method for manufacturing thin-film optical devices" and JP-A-53-71845 "Optical waveguide thin film and method for manufacturing the same". To actually drive such a switch element, a drive signal is sent from the drive circuit 6 to the dielectric drive section 5 to move the movable dielectric piece 4 up and down.
前述したような光スイツチ素子は、第3図に示
すようなスイツチ動作を行う。スイツチをオン状
態にした(可動誘電体片4を光導波膜2および低
屈折率領域2′に近づけた)場合には、第3図a
に示すように入力端子と出力端子〓〓が接続
し、入力端子と出力端子〓〓が接続する。一
方、オフ状態にした(可動誘電体片4を光導波膜
2および低屈折率領域2′から遠ざけた)場合に
は、第3図bに示すように入力端子と出力端子
〓〓が接続し、入力端子は出力端子〓〓と接続
する。このようなスイツチ9は、再配置閉そく型
の2×2スイツチである。再配置型とは、入力端
子と出力端子が必ずどれかに1対1で接続するも
のを言い、閉そく型とは、ある入力端子と出力端
子の接続が他の入力端子の接続に影響を与えるも
のを言う。 The optical switch element as described above performs a switch operation as shown in FIG. When the switch is turned on (the movable dielectric piece 4 is brought close to the optical waveguide film 2 and the low refractive index region 2'), as shown in FIG.
As shown in the figure, the input terminal and the output terminal 〓〓 are connected, and the input terminal and the output terminal 〓〓 are connected. On the other hand, when the movable dielectric piece 4 is placed in the off state (the movable dielectric piece 4 is moved away from the optical waveguide film 2 and the low refractive index region 2'), the input terminal and the output terminal 〓〓 are connected as shown in Fig. 3b. , the input terminal is connected to the output terminal 〓〓. Such a switch 9 is a 2×2 switch of the relocation block type. A relocation type refers to one in which input terminals and output terminals are always connected one to one, and a block type refers to one in which the connection of one input terminal and output terminal affects the connection of other input terminals. say something
再配置閉そく型2×2スイツチ9を基本単位と
すれば、再配置閉そく型N×Nスイツチは、N
(N−1)/2個の2×2スイツチ9で構成でき
ることが知られている。その構成法は、第4図に
示すようにダイヤモンド構造にするか、または第
5図に示すようにトライアングル構造にすればよ
い。いずれの例も7×7スイツチの例である。 If the relocation block type 2x2 switch 9 is the basic unit, the relocation block type NxN switch is N
It is known that it can be configured with (N-1)/2 2×2 switches 9. The structure may be a diamond structure as shown in FIG. 4 or a triangular structure as shown in FIG. Both examples are examples of 7x7 switches.
第4図および第5図に示すN×Nスイツチは、
第1図に示す2×2光スイツチ素子を用いれば、
構成できる。第6図は第4図に示すダイヤモンド
構造のN×N光スイツチの構成を示したものであ
る。説明の便宜上、図のようにxy直交座標軸を
とる。 The N×N switch shown in FIGS. 4 and 5 is
If the 2×2 optical switch element shown in Fig. 1 is used,
Can be configured. FIG. 6 shows the structure of the diamond-structured N.times.N optical switch shown in FIG. 4. For convenience of explanation, xy orthogonal coordinate axes are used as shown in the figure.
光導波膜2中に(N+1)本の直線状の低屈折
率領域2′を、それぞれの低屈折率領域2′の中心
線がy=−nd(n=0、1、……、N)に一致
し、かつ左側端部はxy座標軸の第3象限内にあ
るようにする。ここにdは第6図に示すように相
隣る低屈折率領域2′の中心間の距離とする。 There are (N+1) linear low refractive index regions 2' in the optical waveguide film 2, and the center line of each low refractive index region 2' is y=-nd (n=0, 1, ..., N). and the left end is within the third quadrant of the xy coordinate axes. Here, d is the distance between the centers of adjacent low refractive index regions 2' as shown in FIG.
また任意の低屈折率領域2′上にある端子と、
この低屈折率領域2′と相隣る低屈折率領域2′上
にあり、かつ前記端子と最短距離にある端子との
端子間のx軸方向の距離をlとし、右側端部は、
(N+1)本の低屈折率領域2′のx座標が、l=
d/tanθ(θは(1)式を満たす)として(N−
1)lより十分大きくとればよい。 In addition, a terminal located on an arbitrary low refractive index region 2',
The distance in the x-axis direction between this low refractive index region 2' and a terminal located on the adjacent low refractive index region 2' and at the shortest distance from the terminal is l, and the right end portion is
The x-coordinates of (N+1) low refractive index regions 2' are l=
As d/tanθ (θ satisfies equation (1)), (N-
1) It is sufficient if it is sufficiently larger than l.
これらの低屈折率領域2′上に、x、yを座標
軸とする座標〔2(n1−1)l、2(n2−1)
d〕、ここでNが奇数のときn1=1、2、……、
(N+1)/2、n2=1、2、……、(N−1)/
2、Nが偶数のときn1=1、2、……、N/2、
n2=1、2、……、N/2、およびx、yを座標
軸とする座標〔2(n1−1)l、2n2d〕、ここで
Nが奇数のときn1=1、2、……、(N−1)/
2、n2=1、2、……、(N−1)/2、Nが偶
数のときn1=1、2、……、N/2、n2=1、
2、……、N/2−1で表わされる合計N(N−
1)/2個の位置に、低屈折率領域2′および光
導波膜2をともに覆うに足る十分大きな底面を有
する可動誘電体片4を中間層3を介して設置す
る。このような構成をとると、第6図の場合では
入力端子〜に入射した導波光に対して、〓〓
〜〓〓を出力端子とする7×7再配置閉そく型薄
膜光スイツチ回路が形成される。ここで、入出力
の端子番号は、第6図に示すように、x軸に近い
方から順に,,……,〓〓,〓〓,……とつけ
る。第6図では、−〓〓,−〓〓,−〓
〓,−〓〓,−〓〓,−〓〓,−〓〓の
接続例を示している。図中一重丸はオン状態、二
重丸はオフ状態を表わす。接続は、与えられた接
続対−〓〓(ここには,,……,,〓
〓は〓〓,〓〓,……′である。)の中で|a−
a′|が最も大きいものから順に行えばよい。なぜ
なら、|a−a′|の大きい接続程、光路の選択が
限定されるからである。 On these low refractive index regions 2', coordinates [2(n 1 -1)l, 2(n 2 -1) with x and y as coordinate axes]
d], where N is an odd number, n 1 = 1, 2, ...,
(N+1)/2, n 2 = 1, 2, ..., (N-1)/
2. When N is an even number, n 1 = 1, 2, ..., N/2,
n 2 = 1, 2, ..., N/2, and coordinates with x and y as coordinate axes [2(n 1 -1)l, 2n 2 d], where when N is an odd number, n 1 = 1, 2,..., (N-1)/
2, n 2 = 1, 2, ..., (N-1)/2, when N is an even number, n 1 = 1, 2, ..., N/2, n 2 = 1,
2,..., the total N(N-
1) A movable dielectric piece 4 having a sufficiently large bottom surface to cover both the low refractive index region 2' and the optical waveguide film 2 is installed at the intermediate layer 3 at the /2 position. If such a configuration is adopted, in the case of Fig. 6, for the guided light incident on the input terminal ~, 〓〓
A 7×7 rearranged block type thin film optical switch circuit is formed with ~〓〓 as an output terminal. Here, the input/output terminal numbers are numbered in order from the one closest to the x-axis, as shown in FIG. 6. In Figure 6, −〓〓, −〓〓, −〓
Connection examples of 〓, −〓〓, −〓〓, −〓〓, and −〓〓 are shown. In the figure, a single circle represents an on state, and a double circle represents an off state. A connection is a given connection pair −〓〓 (here, ,...,,〓
〓 is 〓〓, 〓〓, ...'. ) in |a-
It is sufficient to perform the steps in order starting from the one with the largest a′|. This is because the selection of the optical path becomes more limited as |a−a′| becomes larger.
第7図は第5図に示すトライアングル構造のN
×N再配置閉そく型薄膜光スイツチの構成を示
す。光導波膜2中にN本の直線状の低屈折率領域
2′をそれぞれの低屈折率領域2′の中心線がy=
nd(n=0、……、N−1)に一致するように
形成する。かつこられの端部は、右側端部のx座
標が(n−1)lより大きく、左側端部のx座標
が−(n−1)lより小さいようにする。これら
の低屈折率領域2′上に、x、yを座標軸とする
座標〔(n1−1)l−2 l(n2−1)(n1−1)
d〕、ここでn1=1、2、……、N−1、n2=
1、2、……、n1で表わされるN(N−1)/2
個の位置に、低屈折率領域2′および光導波膜2
を、ともに覆うに足る十分大きな底面を有する可
動誘電体片を中間層3を介して設置する。このよ
うな構成をとつても、第7図の入力端子〜に
対して〓〓〜〓〓を出力端子とする7×7再配置
閉そく型薄膜光スイツチ回路が形成される。ここ
で入出力端子番号は、第7図に示すように、x軸
から最も遠いものから順に,,……,〓〓,
〓〓,……とつける。第7図では第6図と同様に
−〓〓,−〓〓,−〓〓,−〓〓,−
〓〓,−〓〓,−〓〓の接続例を示す。接続
は、入力端子の端子番号の最も大きなものから順
に行うか、または出力端子の端子番号の最も大き
なものから順に行えばよい。なぜなら入力端子番
号の大きい接続の組み合わせ、または出力端子番
号の大きい接続の組み合わせ程、光路の選択が限
定されるからである。 Figure 7 shows the N of the triangle structure shown in Figure 5.
The configuration of a ×N rearrangement block type thin film optical switch is shown. N linear low refractive index regions 2' are formed in the optical waveguide film 2 so that the center line of each low refractive index region 2' is y=
nd (n=0, . . . , N-1). In addition, the x-coordinate of the right-hand end is larger than (n-1)l, and the x-coordinate of the left-hand end is smaller than -(n-1)l. On these low refractive index regions 2', coordinates with x and y as coordinate axes [(n 1 -1) l-2 l (n 2 -1) (n 1 -1)
d], where n 1 = 1, 2, ..., N-1, n 2 =
1, 2, ..., N(N-1)/2 represented by n 1
The low refractive index region 2' and the optical waveguide film 2 are located at
A movable dielectric piece having a sufficiently large bottom surface to cover both is installed via the intermediate layer 3. Even with this configuration, a 7.times.7 rearranged block type thin film optical switch circuit is formed in which the input terminals shown in FIG. 7 are connected to the output terminals . Here, the input/output terminal numbers are as shown in Figure 7, in order from the one farthest from the x-axis.
Add 〓〓,... In Figure 7, as in Figure 6, −〓〓, −〓〓, −〓〓, −〓〓, −
A connection example of 〓〓, −〓〓, and −〓〓 is shown. The connections may be made in order from the input terminal with the largest terminal number, or in order from the largest output terminal number. This is because the selection of optical paths is more limited as the combination of connections with larger input terminal numbers or the combination of connections with larger output terminal numbers.
第6図および第7図では7×7の例を示した
が、前述した構成法によれば、一般的にN×N再
配置閉そく型スイツチが形成し得る。これらの薄
膜光スイツチ回路は、特開昭53−71845「光導波
膜とその作製法」および特開昭54−161350「薄膜
光素子を製造方法」によれば、簡単に作製し得る
ものである。 Although a 7.times.7 example is shown in FIGS. 6 and 7, an N.times.N relocation block type switch can generally be formed by the construction method described above. These thin-film optical switch circuits can be easily manufactured according to JP-A-53-71845 ``Optical waveguide film and its manufacturing method'' and JP-A-54-161350 ``Method for manufacturing thin-film optical devices''. .
以上説明したように、本発明の薄膜光スイツチ
回路は、光導波膜中に簡単に作製し得るN本の平
行な低屈折率領域の上部に、可動誘電体片を設置
する構造であり、構造が簡単で作製が容易であ
り、N×Nスイツチ回路が同一基板上に作製でき
る。また回路の基本スイツチ素子の偏向角が大き
いので、スイツチ構成の密度を上げることができ
る。従つて本発明の薄膜光スイツチ回路を光通信
および光情報処理分野に応用すれば、製造コスト
の低減化および装置の小型化にきわめて有効であ
る。 As explained above, the thin film optical switch circuit of the present invention has a structure in which a movable dielectric piece is installed above N parallel low refractive index regions that can be easily fabricated in an optical waveguide film. It is simple and easy to manufacture, and N×N switch circuits can be manufactured on the same substrate. Also, since the deflection angle of the basic switch elements of the circuit is large, the density of the switch arrangement can be increased. Therefore, if the thin film optical switch circuit of the present invention is applied to the fields of optical communications and optical information processing, it will be extremely effective in reducing manufacturing costs and downsizing devices.
第1図は2×2光スイツチ素子の斜視図、第2
図は2×2光スイツチ素子の断面図、第3図は2
×2スイツチの接続状態を示す図、第4図および
第5図はN×Nスイツチの構成を示す図、第6図
および第7図はN×N薄膜型光スイツチの構成を
示す図である。
1……基板、2……光導波膜、2′……低屈折
率領域、3……中間層、4……可動誘電体片、5
……可動誘電体片駆動部、6……駆動回路、7…
…入射導波光、8……出力導波光、8′……出力
導波光、9……2×2スイツチ。
Figure 1 is a perspective view of a 2x2 optical switch element, Figure 2
The figure is a cross-sectional view of a 2x2 optical switch element, and Figure 3 is a cross-sectional view of a 2x2 optical switch element.
4 and 5 are diagrams showing the configuration of an N×N switch, and FIGS. 6 and 7 are diagrams showing the configuration of an N×N thin-film optical switch. . DESCRIPTION OF SYMBOLS 1... Substrate, 2... Optical waveguide film, 2'... Low refractive index region, 3... Intermediate layer, 4... Movable dielectric piece, 5
...Movable dielectric piece drive unit, 6...Drive circuit, 7...
...Incoming waveguide light, 8...Output waveguide light, 8'...Output waveguide light, 9...2x2 switch.
Claims (1)
な基板上に、屈折率n2を有する光導波膜が所定の
厚みに積層され、前記光導波膜中にxy直交座標
軸をとつた場合に、前記光導波膜中にNを正の整
数として(N+1)本の直線状の屈折率n2′を有
する低屈折率領域2′が設けられdを相隣る低屈
折率領域2′の中心間の距離とし、前記低屈折率
領域2′のそれぞれの中心線がy=−nd(n=
0、1、……、N)で表わされる(N+1)本の
直線に一致し、かつそれらの左側端部が前記座標
軸の第3象限内にあり、前記低屈折率領域2′の
前記導波光に対する全反射角度をθとして、任意
の低屈折率領域2′上にある端子と、この低屈折
率領域2′と相隣る低屈折率領域2′上にあり、か
つ前記端子と最短距離にある端子との端子間のx
軸方向の距離をlとし、l=d/tanθとし、前
記(N+1)本の低屈折率領域2′の右側端部の
x座標が(N−1)lより大なるように設置され
n1、n2を正の整数として前記低屈折率領域の上部
のx、yを座標軸とする座標〔2(n1−1)l、
(2n2−1)d〕、ここでNが奇数のときn1=1、
2、……、(N+1)/2、n2=1、2、……、
(N−1)/2、Nが偶数のときn1=1、2、…
…、N/2、n2=1、2、……、N/2および
x、yを座標軸とする座標〔(2n1−1)l、
2n2d〕、ここでNが奇数のときn1=1、2、…
…、(N−1)/2、n2=1、2、……、(N−
1)/2、Nが偶数のときn1=1、2、……、
N/2、n2=1、2、……、N/2−1で表わさ
れる合計N(N−1)/2個のそれぞれの位置
に、屈折率n3なる中間層を介して屈折率n4を有
し、かつ導波膜に平行で、前記低屈折率領域2′
およびその周囲の光導波膜を覆うに足る十分広い
底面を有する可動誘電体片が設置され、かつこの
可動誘電体片と前記光導波膜との距離l3が光導波
膜の膜厚より大きいときの前記光導波膜および低
屈折率領域2′の中心の等価屈折率をν0および
ν0′とし、前記距離l3が光導波膜の膜厚より十分
に小さいときの前記光導波膜および低屈折率領域
2′の中心の等価屈折率をνおよびν′とし、
ν′/ν>cosθ>ν0′/ν0なる関係を満足し、
前記屈折率n1、n2、n2′、n3、n4の間にn2>n2′>
n4>(n1、n3)なる関係が満足されていることを特
徴とする薄膜光スイツチ回路。 2 導波光に対して透明で屈折率n1を有する平滑
な基板上に、屈折率n2を有する光導波膜が所定の
厚みに積層され、前記光導波膜中にxy直交座標
軸をとつた場合に、前記光導波膜中にNを正の整
数としてN本の直線状の屈折率n2′を有する低屈
折率領域2′が設けられ、dを相隣る前記低屈折
率領域2′の中心間の距離とし、前記低屈折率領
域2′のそれぞれの中心線がy=nd(n=0、
1、……、N−1)で表わされるN本の直線に一
致し、かつ前記低屈折率領域2′の導波光に対す
る全反射角度をθとして、任意の低屈折率領域
2′上にある端子とこの低屈折率領域2′と相隣る
低屈折率領域2′上にあり、かつ前記端子と最短
距離にある端子との端子間のx軸方向の距離をl
とし、l=d/tanθとし、N本の前記低屈折率
領域2′の右側端部のx座標が(n−1)lより
大きく、左側端部のx座標が−(n−1)lより
小さいように設置され、前記低屈折率領域2′の
上部の前記x、yを座標軸とする座標〔(n1−
1)l−2 l(n2−1)、(n−1)d〕、ここ
でn1=1、2、……、N−1、n2=1、2、…
…、n1で表わされるN(N−1)/2個の位置
に、屈折率n3なる中間層を介して、屈折率n4を有
し、かつ光導波膜に平行で、前記低屈折率領域
2′およびその周囲の光導波膜を覆うに足る十分
に広い底面を有する可動誘電体片が設置され、か
つこの可動誘電体片と前記光導波膜との距離l3が
光導波膜の膜厚より大きいときの前記光導波膜お
よび低屈折率領域2′の中心の等価屈折率をν0
およびν0′とし、前記距離l3が光導波膜の膜厚よ
り十分に小さいときの前記光導波膜および低屈折
率領域2′の中心の等価屈折率をνおよびν′と
し、ν′/ν>cosθ>ν0′/ν0なる関係を満足
し、さらに前記屈折率n11、n2、n2′、n3、n4間に
n2>n2′>n4>(n1、n3)なる関係が満足されている
ことを特徴とする薄膜光スイツチ回路。[Claims] 1. An optical waveguide film having a refractive index n 2 is laminated to a predetermined thickness on a smooth substrate that is transparent to guided light and has a refractive index n 1 , and xy When the orthogonal coordinate axes are taken, (N+1) linear low refractive index regions 2' having a refractive index n 2 ' are provided in the optical waveguide film, where N is a positive integer, and d is the adjacent low refractive index region 2'. Let the distance between the centers of the refractive index regions 2' be y=-nd(n=
0, 1, . Assuming that the total reflection angle for x between certain terminals
The distance in the axial direction is l, l = d/tanθ, and the x-coordinate of the right end of the (N+1) low refractive index regions 2' is set to be larger than (N-1)l.
Coordinates [ 2 ( n 1 -1)l,
(2n 2 -1)d], where N is an odd number, n 1 = 1,
2,..., (N+1)/2, n 2 = 1, 2,...,
(N-1)/2, when N is an even number, n 1 = 1, 2,...
..., N/2, n 2 = 1, 2, ..., N/2 and coordinates with x, y as the coordinate axes [(2n 1 -1)l,
2n 2 d], where N is an odd number, n 1 = 1, 2,...
..., (N-1)/2, n 2 = 1, 2, ..., (N-
1)/2, when N is an even number, n 1 = 1, 2,...
At each of a total of N(N-1)/2 positions represented by N/2, n 2 = 1, 2, ..., N/2-1, a refractive index is applied via an intermediate layer with a refractive index of n 3 . n 4 and parallel to the waveguide film, the low refractive index region 2'
and a movable dielectric piece having a sufficiently wide bottom surface to cover the surrounding optical waveguide film is installed, and the distance l3 between this movable dielectric piece and the optical waveguide film is greater than the film thickness of the optical waveguide film. Let ν 0 and ν 0 ' be the equivalent refractive index at the center of the optical waveguide film and the low refractive index region 2', and the optical waveguide film and the low refractive index when the distance l 3 is sufficiently smaller than the film thickness of the optical waveguide film and the low refractive index region 2'. Let the equivalent refractive index at the center of the refractive index region 2' be ν and ν',
Satisfying the relationship ν′/ν>cosθ>ν 0 ′/ν 0 ,
Between the refractive index n 1 , n 2 , n 2 ′, n 3 , n 4 , n 2 >n 2 ′>
A thin film optical switch circuit characterized in that the following relationship is satisfied: n 4 >(n 1 , n 3 ). 2. When an optical waveguide film having a refractive index n 2 is laminated to a predetermined thickness on a smooth substrate that is transparent to guided light and has a refractive index n 1 , and xy orthogonal coordinate axes are set in the optical waveguide film. , N linear low refractive index regions 2' having a refractive index n 2 ' are provided in the optical waveguide film, where N is a positive integer, and d is the number of adjacent low refractive index regions 2'. The distance between the centers is y=nd (n=0,
1, . The distance in the x-axis direction between the terminal and a terminal located on the low refractive index region 2' adjacent to this low refractive index region 2' and located at the shortest distance from the terminal is l.
and l=d/tanθ, the x-coordinate of the right end of the N low refractive index regions 2' is larger than (n-1)l, and the x-coordinate of the left end is -(n-1)l The coordinates [(n 1 −
1) l-2 l(n 2 -1), (n-1) d], where n 1 = 1, 2, ..., N-1, n 2 = 1, 2, ...
..., at N(N-1)/2 positions represented by n 1 , have a refractive index n 4 through an intermediate layer with a refractive index n 3 , and are parallel to the optical waveguide film and have the low refractive index. A movable dielectric piece having a sufficiently wide bottom surface to cover the index area 2' and the optical waveguide film around it is installed, and the distance l 3 between this movable dielectric piece and the optical waveguide film is equal to the distance of the optical waveguide film. The equivalent refractive index at the center of the optical waveguide film and the low refractive index region 2' when it is larger than the film thickness is ν 0
and ν 0 ′, and when the distance l 3 is sufficiently smaller than the film thickness of the optical waveguide film, the equivalent refractive index at the center of the optical waveguide film and the low refractive index region 2′ is ν and ν′, and ν′/ The relationship ν>cosθ>ν 0 ′/ν 0 is satisfied, and furthermore, between the refractive indices n 11 , n 2 , n 2 ′, n 3 , n 4
A thin film optical switch circuit characterized in that the following relationship is satisfied: n 2 > n 2 ′ > n 4 > (n 1 , n 3 ).
Priority Applications (7)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7686180A JPS574010A (en) | 1980-06-07 | 1980-06-07 | Thin film optical switch circuit |
| US06/222,650 US4365862A (en) | 1980-01-18 | 1981-01-05 | Optical switch |
| GB8100575A GB2070271B (en) | 1980-01-18 | 1981-01-09 | Optical switch |
| CA000368445A CA1155934A (en) | 1980-01-18 | 1981-01-13 | Optical switch |
| NLAANVRAGE8100175,A NL185037C (en) | 1980-01-18 | 1981-01-15 | OPTICAL SWITCH AND OPTICAL SWITCH CHAIN. |
| FR8100809A FR2475239B1 (en) | 1980-01-18 | 1981-01-16 | |
| DE3101415A DE3101415A1 (en) | 1980-01-18 | 1981-01-17 | OPTICAL SWITCH |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7686180A JPS574010A (en) | 1980-06-07 | 1980-06-07 | Thin film optical switch circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS574010A JPS574010A (en) | 1982-01-09 |
| JPS6150293B2 true JPS6150293B2 (en) | 1986-11-04 |
Family
ID=13617424
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7686180A Granted JPS574010A (en) | 1980-01-18 | 1980-06-07 | Thin film optical switch circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS574010A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01103816U (en) * | 1987-12-28 | 1989-07-13 |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN107678097B (en) * | 2016-08-01 | 2019-11-12 | 华为技术有限公司 | Optical Switches and Optical Switching Systems |
| WO2025032677A1 (en) * | 2023-08-07 | 2025-02-13 | 日本電信電話株式会社 | Optical switch |
-
1980
- 1980-06-07 JP JP7686180A patent/JPS574010A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01103816U (en) * | 1987-12-28 | 1989-07-13 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS574010A (en) | 1982-01-09 |
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