JP2000241838A - Digital thermo-optic optical switch - Google Patents

Digital thermo-optic optical switch

Info

Publication number
JP2000241838A
JP2000241838A JP11040246A JP4024699A JP2000241838A JP 2000241838 A JP2000241838 A JP 2000241838A JP 11040246 A JP11040246 A JP 11040246A JP 4024699 A JP4024699 A JP 4024699A JP 2000241838 A JP2000241838 A JP 2000241838A
Authority
JP
Japan
Prior art keywords
optical waveguide
optical
branch
heater
thin 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.)
Granted
Application number
JP11040246A
Other languages
Japanese (ja)
Other versions
JP3478751B2 (en
Inventor
Naoki Oba
直樹 大庭
Takashi Kurihara
栗原  隆
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.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone 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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP04024699A priority Critical patent/JP3478751B2/en
Publication of JP2000241838A publication Critical patent/JP2000241838A/en
Application granted granted Critical
Publication of JP3478751B2 publication Critical patent/JP3478751B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related 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
    • G02F1/01Devices 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 intensity, phase, polarisation or colour 
    • G02F1/0147Devices 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 intensity, phase, polarisation or colour  based on thermo-optic effects
    • 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
    • G02F1/3137Digital deflection, i.e. optical switching in an optical waveguide structure with intersecting or branching waveguides, e.g. X-switches and Y-junctions
    • 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
    • G02F2201/00Constructional arrangements not provided for in groups G02F1/00 - G02F7/00
    • G02F2201/12Constructional arrangements not provided for in groups G02F1/00 - G02F7/00 electrode
    • G02F2201/122Constructional arrangements not provided for in groups G02F1/00 - G02F7/00 electrode having a particular pattern
    • 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
    • G02F2202/00Materials and properties
    • G02F2202/02Materials and properties organic material
    • G02F2202/022Materials and properties organic material polymeric
    • G02F2202/023Materials and properties organic material polymeric curable

Abstract

PROBLEM TO BE SOLVED: To provide a digital thermooptic optical switch which permits to obtain the performance equivalent to standard with small operation power and is also reduced in power consumption of an optical cross-connect system and an optical add-drop multiplexer. SOLUTION: This is a digital thermooptic optical switch formed of a Y- branching optical waveguide consisting of a linear optical waveguide 11, a tapered optical waveguide 12, and a branching optical waveguide 13, and a thin film heater 15 along the Y-branching optical waveguide. In this case, the thin film heater 15 part in an area B along the tapered optical waveguide 12 is formed to be gradually tapered in width (maximum width W1 → minimum width W0) from the linear optical wveguide 11 side toward the branching optical waveguide 13.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、波長多重( WD
M) 光通信等の光通信及び光信号処理において光路切り
替えに用いられる光導波路型光スイッチに関し、特にデ
ジタル熱光学光スイッチに関する。
The present invention relates to a wavelength division multiplexing (WD)
M) An optical waveguide type optical switch used for optical path switching in optical communication such as optical communication and optical signal processing, and particularly to a digital thermo-optical switch.

【0002】[0002]

【従来の技術】光導波路型熱光学光スイッチは、可動部
分が無く、挿入損失が低く、小型で集積化が容易なた
め、波長多重通信網のクロスコネクトやアドドロップマ
ルチプレクサ(ADM)用光スイッチ用として有望視さ
れている。この光導波路型熱光学光スイッチの中でもデ
ジタル熱光学光スイッチは、スイッチ特性が波長や偏光
や動作電力に対して原理的に低依存である利点が着目さ
れ、各機関で活発な研究開発が進められている(参考文
献1:N.Ooba et al.,“Low Loss 1×8 digital optica
l switch and tunable arrayed-waveguide grating mul
tiplexer using a silicone resin waveguide ”,Proc.
7th Int Plastic Opt. Fibres Conf.,Berlin,P.303,199
8 )。
2. Description of the Related Art An optical waveguide type thermo-optical switch has no moving parts, has a low insertion loss, is small in size, and can be easily integrated. Promising for use. Among these optical waveguide type thermo-optical switches, digital thermo-optical switches are noted for their advantage that their switch characteristics are basically low dependent on wavelength, polarization and operating power. (Reference 1: N. Ooba et al., “Low Loss 1 × 8 digital optica
l switch and tunable arrayed-waveguide grating mul
tiplexer using a silicone resin waveguide ”, Proc.
7th Int Plastic Opt.Fibres Conf., Berlin, P.303,199
8).

【0003】デジタル熱光学光スイッチの動作には、大
きい熱光学屈折率変化が必要とされるので、コア・クラ
ッド共に熱光学定数の大きい高分子光導波路材料が主に
用いられている。
Since the operation of the digital thermo-optical switch requires a large change in the thermo-optical refractive index, a polymer optical waveguide material having a large thermo-optical constant is mainly used for both the core and the clad.

【0004】従来の一般的なデジタル熱光学光スイッチ
の構造を図4の平面図に示す。入力光導波路としての直
線光導波路11とテーパー光導波路12及び分岐光導波
路13及び出力光導波路14からなるY分岐光導波路に
沿って、薄膜ヒーター15はその垂直方向にほぼ一定間
隔をおいて配置されている。図4中、薄膜ヒーター15
に電流を供給するリードは省略している。2本の分岐光
導波路13は、互いにモード結合しながら徐々に離れて
いくテーパードヴェロシティーカップラーをなしてい
る。
FIG. 4 is a plan view showing the structure of a conventional general digital thermo-optical switch. Along the Y-branch optical waveguide composed of the linear optical waveguide 11, the taper optical waveguide 12, the branch optical waveguide 13, and the output optical waveguide 14 as the input optical waveguide, the thin film heaters 15 are arranged at substantially constant intervals in the vertical direction. ing. 4, the thin film heater 15
The lead for supplying current to the power supply is omitted. The two branch optical waveguides 13 form a tapered velocity coupler that gradually separates while being mode-coupled to each other.

【0005】一対の薄膜ヒーター15のいずれか一方を
加熱することで、熱光学効果により2つの分岐光導波路
13の屈折率を非対称とすると、テーパードヴェロシテ
ィーカップラーにおける基本モード光は、出力光導波路
14側では高屈折率側に集中する。このため、直線光導
波路11に入射した基本モード光が高次モードに結合し
なければ、高屈折率側の出力光導波路14に導かれ、こ
のデバイスは分岐スイッチとして動作する(参考文献
2:W.K.Burns,et al., “Mode conversion in planar-
dielectric separating waveguides”,IEEE j.Quantum
Electron.,Vol.QE-11,p.32,1975)。
If one of the pair of thin film heaters 15 is heated to make the refractive index of the two branch optical waveguides 13 asymmetric by the thermo-optic effect, the fundamental mode light in the tapered velocity coupler is output from the output optical waveguide 14. The side concentrates on the high refractive index side. Therefore, if the fundamental mode light incident on the linear optical waveguide 11 is not coupled to a higher-order mode, it is guided to the output optical waveguide 14 on the high refractive index side, and this device operates as a branch switch (Ref. 2: WKBurns). , et al., “Mode conversion in planar-
dielectric separating waveguides ”, IEEE j.Quantum
Electron., Vol. QE-11, p. 32, 1975).

【0006】デジタル熱光学光スイッチにおいて、より
高い分岐比を得るためには、分岐角を小さくする、また
は大きな屈折率差を分岐光導波路13に与えることが必
要となる。分岐角を小さくすると加熱領域である分岐光
導波路13が長くなる。20dBを越える消光比を得る
ためには、一般に分岐角0.1度程度となり、10mm
程度の分岐光導波路13や薄膜ヒーター15が必要とな
る(参考文献3:W.Horsthuis et al.,"PACKAGED POLYM
ERIC 1×8 DIGITAL OPTICAL SWITCHES", Proc.21st Eu
r.Conf.Opt.Comm.,Brussels,Th.L.3,4,p.1059, 199
5)。
In order to obtain a higher branching ratio in the digital thermo-optical switch, it is necessary to reduce the branching angle or to provide a large difference in refractive index to the branching optical waveguide 13. When the branch angle is reduced, the length of the branch optical waveguide 13 that is the heating region becomes longer. In order to obtain an extinction ratio exceeding 20 dB, the branch angle is generally about 0.1 degree, and 10 mm
A small amount of the branch optical waveguide 13 and the thin film heater 15 are required (Reference 3: W. Horsthuis et al., "PACKAGED POLYM"
ERIC 1 × 8 DIGITAL OPTICAL SWITCHES ", Proc. 21st Eu
r.Conf.Opt.Comm., Brussels, Th.L.3,4, p.1059,199
Five).

【0007】しかし、高分子光導波路の場合、導波路自
体の導波損失が10mmで0.5dB程度見込まれるの
で、スイッチが長くなると損失増加をまねく問題が生じ
る。
However, in the case of the polymer optical waveguide, the waveguide loss of the waveguide itself is expected to be about 0.5 dB at 10 mm, so that there is a problem that the loss increases when the switch is long.

【0008】また、大きな屈折率差を分岐光導波路13
に与えた場合、薄膜ヒーター15の直線光導波路11側
の端点において、モード変換による過剰損失が生じる。
これを防ぐためには、図4のAで示すように、薄膜ヒー
ター15を徐々にコア(光導波路)12に近づけている
領域が必要となる。
Further, a large difference in the refractive index is caused by the branch optical waveguide 13.
, Excessive loss due to mode conversion occurs at the end point of the thin-film heater 15 on the side of the linear optical waveguide 11.
In order to prevent this, a region where the thin film heater 15 is gradually approached to the core (optical waveguide) 12 is required as shown by A in FIG.

【0009】[0009]

【発明が解決しようとする課題】このように、従来のデ
ジタル熱光学光スイッチでは、コアと薄膜ヒーターの距
離を変えてコア部分の加熱量を制御している。しかし、
この従来方法では、加熱量を小さくしたい部分では、ス
イッチ動作に関与しないコアから離れた領域を加熱して
いることになり、加熱電力効率を下げている。そこで、
このようなデジタル熱光学光スイッチでは、加熱効率を
上げて、消費電力をさらに下げることが課題となってい
る。
As described above, in the conventional digital thermo-optical switch, the heating amount of the core portion is controlled by changing the distance between the core and the thin film heater. But,
In this conventional method, in a portion where the amount of heating is desired to be reduced, a region which is not involved in the switching operation and is away from the core is heated, and the heating power efficiency is reduced. Therefore,
In such a digital thermo-optical switch, it has been a problem to increase the heating efficiency and further reduce the power consumption.

【0010】本発明の目的は、上述のような従来技術の
課題を解決し、小さい動作電力で同等の性能を得ること
ができ、光クロスコネクトシステムや光アドドロップマ
ルチプレクサの低電力化を図ったデジタル熱光学光スイ
ッチを提供することにある。
An object of the present invention is to solve the above-mentioned problems of the prior art, achieve the same performance with a small operating power, and reduce the power of an optical cross-connect system and an optical add / drop multiplexer. A digital thermo-optical switch is provided.

【0011】[0011]

【課題を解決するための手段】上記目的を達成するた
め、請求項1の発明は、直線光導波路及びテーパー光導
波路及び分岐光導波路からなるY分岐光導波路と、該Y
分岐光導波路に沿う薄膜ヒーターとにより構成されるデ
ジタル熱光学光スイッチにおいて、前記薄膜ヒーターの
一部が前記直線光導波路側から前記分岐光導波路側へ向
けて徐々にその幅が細くなる形状、およびその厚さが薄
くなる形状の少なくともいずれかの形状を有することを
特徴とする。
In order to achieve the above object, the present invention is directed to a Y-branch optical waveguide comprising a linear optical waveguide, a tapered optical waveguide, and a branch optical waveguide;
In a digital thermo-optical switch configured by a thin film heater along a branch optical waveguide, a shape in which a part of the thin film heater gradually narrows in width from the straight optical waveguide side toward the branch optical waveguide side, and It is characterized in that it has at least one of the shapes whose thickness is reduced.

【0012】ここで、好ましくは、前記薄膜ヒーターの
前記一部は、前記テーパー光導波路に沿う部分である。
Here, preferably, the part of the thin film heater is a part along the tapered optical waveguide.

【0013】また、好ましくは、前記Y分岐光導波路
が、アクリル系高分子、または紫外線硬化エポキシ樹
脂、またはシリコーン樹脂、またはポリイミドのいずれ
か、またはそれらの組み合わせによって作られている。
Preferably, the Y-branch optical waveguide is made of an acrylic polymer, an ultraviolet curable epoxy resin, a silicone resin, or a polyimide, or a combination thereof.

【0014】[0014]

【発明の実施の形態】図面を参照して、本発明の実施の
形態を詳細に説明する。
Embodiments of the present invention will be described in detail with reference to the drawings.

【0015】まず、本発明の原理を説明する。抵抗率ρ
の金属薄膜で出来ている厚さT、幅Wのストリップ状の
薄膜電熱ヒーターに電流iを流した時、単位面積当たり
の発熱量は、
First, the principle of the present invention will be described. Resistivity ρ
When a current i is passed through a strip-shaped thin-film electric heater having a thickness T and a width W made of a metal thin film of

【0016】[0016]

【数1】 (Equation 1)

【0017】となる。光導波路の厚さに比べてヒーター
の幅が同程度以上の場合、ヒーターの上昇温度は、単位
面積当たりの発熱量に比例すると近似できる。ここか
ら、薄膜ヒーターの幅、または厚さを変化させること
で、ヒーターの上昇温度を場所により変化させることが
できることがわかる。
## EQU1 ## When the width of the heater is equal to or greater than the thickness of the optical waveguide, the temperature rise of the heater can be approximated as being proportional to the amount of heat generated per unit area. From this, it can be seen that by changing the width or thickness of the thin film heater, the temperature at which the heater rises can be changed depending on the location.

【0018】(第1の実施形態)図1は、本発明の一実
施形態のデジタル熱光学光スイッチの構成を示す平面図
である。図1において、図4の従来例と同様の構成要素
には同一符号を付してある。すなわち、入力光導波路と
しての直線光導波路11とテーパー光導波路12及び分
岐光導波路13及び出力光導波路14からなるY分岐光
導波路に沿って、薄膜ヒーター15はその垂直方向にほ
ぼ一定間隔をおいて配置されている。2本の分岐光導波
路13は、互いにモード結合しながら徐々に離れていく
テーパードヴェロシティーカップラーをなしている。
(First Embodiment) FIG. 1 is a plan view showing a configuration of a digital thermo-optical switch according to an embodiment of the present invention. 1, the same components as those of the conventional example of FIG. 4 are denoted by the same reference numerals. That is, along the Y-branch optical waveguide composed of the linear optical waveguide 11 as an input optical waveguide, the tapered optical waveguide 12, the branch optical waveguide 13, and the output optical waveguide 14, the thin film heaters 15 are arranged at substantially constant intervals in the vertical direction. Are located. The two branch optical waveguides 13 form a tapered velocity coupler that gradually separates while being mode-coupled to each other.

【0019】テーパー光導波路12が形成されている図
1のBの領域では、直線光導波路11側へ向けて薄膜ヒ
ーター15の幅Wを徐々に太くすることで(最小幅W0
→最大幅W1 )、発熱量を減らし、従来ヒーターを遠ざ
けていたのと同じ効果を得ている。例えば、ヒーター1
5の左端で1/10の発熱量とするには、
In the region of FIG. 1B where the tapered optical waveguide 12 is formed, the width W of the thin-film heater 15 is gradually increased toward the linear optical waveguide 11 (minimum width W 0).
→ The maximum width W 1 ), the amount of heat generation is reduced, and the same effect as that obtained by keeping the heater away from the conventional one is obtained. For example, heater 1
To make the calorific value of 1/10 at the left end of 5,

【0020】[0020]

【数2】 (Equation 2)

【0021】とすればよい。この時、B領域のヒーター
15の全体の発熱量若しくは加熱電力P1 は、ヒーター
15の幅を、
[0021] At this time, the entire heat generation amount or heating power P 1 of the heater 15 in the region B is determined by the width of the heater 15.

【0022】[0022]

【数3】 (Equation 3)

【0023】B領域のヒーター15の長さをLとして、Assuming that the length of the heater 15 in the region B is L,

【0024】[0024]

【数4】 (Equation 4)

【0025】である。ただし、P0 は、従来の幅W0
ヒーターの発熱量若しくは加熱電力、
## EQU1 ## Here, P 0 is the calorific value or heating power of the conventional heater of width W 0 ,

【0026】[0026]

【数5】 (Equation 5)

【0027】である。## EQU1 ##

【0028】上式(4)から、本実施形態のB領域にお
ける発熱量若しくは加熱電力P1 は、従来型の発熱量若
しくは加熱電力P0 に比べ約半分になることがわかる。
分岐光導波路13が形成されている図1のC部分を含む
ヒーター15全体でも2割以上の加熱電力の減少が見込
まれる。
From the above equation (4), it can be seen that the heating value or heating power P 1 in the B region of this embodiment is about half of the heating value or heating power P 0 of the conventional type.
A reduction in heating power of more than 20% is expected for the entire heater 15 including the portion C in FIG. 1 where the branch optical waveguide 13 is formed.

【0029】なお、本発明を適用するY分岐光導波路
は、例えば、アクリル系高分子、または紫外線硬化エポ
キシ樹脂、またはシリコーン樹脂、またはポリイミドの
いずれか、またはそれらの組み合わせによって作成する
のが好ましい。
The Y-branch optical waveguide to which the present invention is applied is preferably made of, for example, an acrylic polymer, an ultraviolet-curable epoxy resin, a silicone resin, or a polyimide, or a combination thereof.

【0030】(第2の実施形態)図2は、本発明の他の
実施形態のデジタル熱光学光スイッチの構成を示し、薄
膜ヒーターの厚みを制御して発熱量を変化させた例を示
す平面図と側面図である。図2の(a)の平面図、図2
の(b)の側面図に示すように、テーパー光導波路12
が形成されているBの領域では、直線光導波路11側へ
向けて徐々にヒーター15の厚みTを厚くすることで
(最小厚みT0 →最大厚みT1 )、発熱量P1 を減ら
し、従来のヒーターを光導波路から遠ざけていたのと同
じ効果を得ている。たとえば、ヒーター左端で1/10
の発熱量とするには、
(Second Embodiment) FIG. 2 shows a configuration of a digital thermo-optical switch according to another embodiment of the present invention, in which a thickness of a thin film heater is controlled to change an amount of generated heat. It is a figure and a side view. FIG. 2A is a plan view of FIG.
(B), as shown in the side view of FIG.
In the region B where is formed, the thickness T of the heater 15 is gradually increased toward the straight optical waveguide 11 side (minimum thickness T 0 → maximum thickness T 1 ) to reduce the calorific value P 1. Has the same effect as moving the heater away from the optical waveguide. For example, 1/10 at the left end of the heater
The calorific value of

【0031】[0031]

【数6】 T1 =10T0 …(6) とすればよい。この時、B領域のヒーター全体の発熱量
若しくは加熱電力P1 は、従来の厚さT0 のヒーターに
比べ約1/4になる。C領域部分を含むヒーター全体で
も3割以上の加熱電力の減少が見込まれる。
T 1 = 10T 0 (6) At this time, the calorific value or heating power P 1 of the entire heater in the region B is about 4 of that of the conventional heater having the thickness T 0 . A reduction in heating power of 30% or more is expected for the entire heater including the region C.

【0032】[0032]

【実施例】次に、本発明の実施例を具体的に説明する。Next, embodiments of the present invention will be described specifically.

【0033】(第1の実施例)屈折率1.489の重水
素シリコーン樹脂をコアに、屈折率1.485の重水素
化シリコーン樹脂をクラッドに用いて、シリコン基板上
にY分岐光導波路を作製した。シリコーン樹脂光導波路
の作成方法は、本願発明者らが提案した「熱光学デバイ
ス」(特開平10−319445号公報)の作成方法に
準じた。
First Embodiment A Y-branch optical waveguide is formed on a silicon substrate by using a deuterated silicone resin having a refractive index of 1.489 as a core and a deuterated silicone resin having a refractive index of 1.485 as a clad. Produced. The method for producing the silicone resin optical waveguide was in accordance with the method for producing a "thermo-optical device" (JP-A-10-319445) proposed by the present inventors.

【0034】コア断面サイズは8μm×8μm、下層ク
ラッド厚、コア上の上部クラッド厚は、それぞれ14μ
m、12μmとした。導波路上に金薄膜をスパッター法
で形成し、フォトリソグラフィー及びドライエッチング
法を用いて図1示す形状のストリップ状の薄膜抵抗ヒー
ターを作製した。ここで、W0 =20μm、W1 =60
μmである。
The cross-sectional size of the core is 8 μm × 8 μm, the thickness of the lower cladding, and the thickness of the upper cladding on the core are each 14 μm.
m and 12 μm. A gold thin film was formed on the waveguide by a sputtering method, and a strip-shaped thin film resistance heater having the shape shown in FIG. 1 was manufactured by using photolithography and dry etching. Here, W 0 = 20 μm and W 1 = 60
μm.

【0035】比較のため図4に示す一定幅20μmのヒ
ーターを備えた形状の従来型光スイッチも同様にして作
製した。
For comparison, a conventional optical switch having a heater having a constant width of 20 μm as shown in FIG. 4 was similarly manufactured.

【0036】波長1.55μmのLD光源(図示しな
い)及び2つの光パワーメータ(図示しない)をそれぞ
れ幹側コア11、分岐側コア14に接続してスイッチ特
性を測定した。2つの分岐出力の比、即ち消光比が30
dBを越えるのに必要なヒーター加熱電力は、従来型1
60mWに対して本発明の光スイッチは120mWであ
った。これにより、本発明を適用することで加熱効率を
上げ、消費電力を下げることが可能であることが確認さ
れた。
An LD light source (not shown) having a wavelength of 1.55 μm and two optical power meters (not shown) were connected to the trunk core 11 and the branch core 14, respectively, and the switch characteristics were measured. The ratio of the two branch outputs, ie the extinction ratio is 30
Heater heating power required to exceed dB is 1
The optical switch of the present invention was 120 mW compared to 60 mW. Thereby, it was confirmed that the heating efficiency can be increased and the power consumption can be reduced by applying the present invention.

【0037】(第2の実施例)上記の本発明の第1の実
施例と同構造のY分岐光導波路を作製し、この上に、図
3に示すように金属マスク18を光導波路16から離し
て設置したスパッター装置を用いて、膜厚変化のある金
属薄膜17を堆積した。ここで、19はスパッター装置
のスパッターターゲットである。さらに、フォトリソグ
ラフィー及びドライエッチング法を用いて図2に示す形
状のストリップ状の薄膜抵抗ヒーターを作製した。ここ
で、T0 =0.05μm、T1 =0.6μmとなった。
(Second Embodiment) A Y-branch optical waveguide having the same structure as that of the first embodiment of the present invention is manufactured, and a metal mask 18 is formed on the Y-branch optical waveguide 16 as shown in FIG. A metal thin film 17 having a change in film thickness was deposited by using a sputtering apparatus which was separately installed. Here, 19 is a sputter target of the sputter device. Further, a strip-shaped thin-film resistance heater having the shape shown in FIG. 2 was manufactured by using photolithography and dry etching. Here, T 0 = 0.05 μm and T 1 = 0.6 μm.

【0038】上記の第1の実施例と同様の方法で消光比
を測定した。消光比が30dB以上となるヒーター加熱
電力は、100mWであった。これにより、本発明を適
用することで加熱効率を上げ、消費電力を下げることが
可能であることが確認された。
The extinction ratio was measured in the same manner as in the first embodiment. The heater heating power at which the extinction ratio became 30 dB or more was 100 mW. Thereby, it was confirmed that the heating efficiency can be increased and the power consumption can be reduced by applying the present invention.

【0039】[0039]

【発明の効果】以上説明したように、本発明によれば、
従来のものより小さい動作電力で同等の性能を得ること
ができ、光クロスコネクトシステムや光アドドロップマ
ルチプレクサの低電力化が図れるという効果が得られ
る。
As described above, according to the present invention,
The same performance can be obtained with an operating power smaller than that of the conventional one, and the effect of reducing the power of the optical cross-connect system and the optical add / drop multiplexer can be obtained.

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

【図1】本発明の第1の実施形態におけるヒーター幅を
変化させたY分岐デジタル熱光学光スイッチの構成を示
す平面図である。
FIG. 1 is a plan view showing a configuration of a Y-branch digital thermo-optical switch in which a heater width is changed according to a first embodiment of the present invention.

【図2】本発明の第2の実施形態におけるヒーター厚を
変化させたY分岐デジタル熱光学光スイッチの構成を示
す平面図(a)と側面図(b)である。
FIG. 2 is a plan view (a) and a side view (b) showing a configuration of a Y-branch digital thermo-optical switch in which a heater thickness is changed according to a second embodiment of the present invention.

【図3】本発明の実施例で用いたスパッター薄膜堆積装
置の概略図である。
FIG. 3 is a schematic view of a sputter thin film deposition apparatus used in an embodiment of the present invention.

【図4】従来のY分岐デジタル熱光学光スイッチの構成
を示す平面図である。
FIG. 4 is a plan view showing a configuration of a conventional Y-branch digital thermo-optical switch.

【符号の説明】[Explanation of symbols]

11 直線光導波路 12 テーパー光導波路 13 分岐光導波路 14 出力光導波路 15 薄膜ヒーター 16 光導波路 17 堆積した金属薄膜 18 マスク 19 スパッターターゲット DESCRIPTION OF SYMBOLS 11 Straight optical waveguide 12 Taper optical waveguide 13 Branch optical waveguide 14 Output optical waveguide 15 Thin film heater 16 Optical waveguide 17 Metal thin film deposited 18 Mask 19 Sputter target

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 直線光導波路及びテーパー光導波路及び
分岐光導波路からなるY分岐光導波路と、該Y分岐光導
波路に沿う薄膜ヒーターとにより構成されるデジタル熱
光学光スイッチにおいて、 前記薄膜ヒーターの一部が前記直線光導波路側から前記
分岐光導波路側へ向けて徐々にその幅が細くなる形状、
およびその厚さが薄くなる形状の少なくともいずれかの
形状を有することを特徴とするデジタル熱光学光スイッ
チ。
1. A digital thermo-optical switch comprising: a Y-branch optical waveguide including a linear optical waveguide, a taper optical waveguide, and a branch optical waveguide; and a thin-film heater along the Y-branch optical waveguide. A portion whose width gradually narrows from the straight optical waveguide side toward the branch optical waveguide side,
And a digital thermo-optical switch having at least one of a shape whose thickness is reduced.
【請求項2】 前記薄膜ヒーターの前記一部は、前記テ
ーパー光導波路に沿う部分であることを特徴とする請求
項1に記載のデジタル熱光学光スイッチ。
2. The digital thermo-optical switch according to claim 1, wherein the part of the thin film heater is a part along the tapered optical waveguide.
【請求項3】 前記Y分岐光導波路が、アクリル系高分
子、または紫外線硬化エポキシ樹脂、またはシリコーン
樹脂、またはポリイミドのいずれか、またはそれらの組
み合わせによって作られていることを特徴とする請求項
1または2に記載のデジタル熱光学光スイッチ。
3. The Y-branch optical waveguide is made of an acrylic polymer, an ultraviolet curable epoxy resin, a silicone resin, or a polyimide, or a combination thereof. Or the digital thermo-optical switch according to 2.
JP04024699A 1999-02-18 1999-02-18 Digital thermo-optic light switch Expired - Fee Related JP3478751B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP04024699A JP3478751B2 (en) 1999-02-18 1999-02-18 Digital thermo-optic light switch

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP04024699A JP3478751B2 (en) 1999-02-18 1999-02-18 Digital thermo-optic light switch

Publications (2)

Publication Number Publication Date
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JP3478751B2 JP3478751B2 (en) 2003-12-15

Family

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Country Link
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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003100516A1 (en) * 2002-05-28 2003-12-04 Optun (Bvi) Ltd. Device and method of dynamic optical spot conversion
WO2005045489A3 (en) * 2003-07-02 2005-06-30 Du Pont Y-branch-based thermo-optic digital optical switches and variable optical attenuators with non-uniform heating
CN100390590C (en) * 2004-10-21 2008-05-28 复旦大学 Multimode interference heat optical switch
EP2015116A3 (en) * 2007-07-12 2010-01-13 NEC Corporation Silicon structure, in particular including an optical waveguide, and method of manufacturing the same

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003100516A1 (en) * 2002-05-28 2003-12-04 Optun (Bvi) Ltd. Device and method of dynamic optical spot conversion
WO2005045489A3 (en) * 2003-07-02 2005-06-30 Du Pont Y-branch-based thermo-optic digital optical switches and variable optical attenuators with non-uniform heating
JP2007524863A (en) * 2003-07-02 2007-08-30 イー・アイ・デュポン・ドウ・ヌムール・アンド・カンパニー Y-branch thermo-optic digital optical switch and variable optical attenuator using non-uniform heating
US7302141B2 (en) 2003-07-02 2007-11-27 E.I. Du Pont De Nemors And Company Y-branch-based thermo-optic digital optical switches and variable optical attenuators with non-uniform heating
CN100412616C (en) * 2003-07-02 2008-08-20 纳幕尔杜邦公司 Y-branch-based thermo-optic digital optical switches and variable optical attenuators with non-uniform heating
CN100390590C (en) * 2004-10-21 2008-05-28 复旦大学 Multimode interference heat optical switch
EP2015116A3 (en) * 2007-07-12 2010-01-13 NEC Corporation Silicon structure, in particular including an optical waveguide, and method of manufacturing the same

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