JPS62212631A - Optical multiplexer and demultiplexer - Google Patents
Optical multiplexer and demultiplexerInfo
- Publication number
- JPS62212631A JPS62212631A JP61054938A JP5493886A JPS62212631A JP S62212631 A JPS62212631 A JP S62212631A JP 61054938 A JP61054938 A JP 61054938A JP 5493886 A JP5493886 A JP 5493886A JP S62212631 A JPS62212631 A JP S62212631A
- Authority
- JP
- Japan
- Prior art keywords
- refractive index
- optical
- waveguide
- grooves
- wavelength
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 46
- 230000000737 periodic effect Effects 0.000 claims abstract description 21
- 239000000758 substrate Substances 0.000 claims abstract description 16
- 230000000694 effects Effects 0.000 claims abstract description 7
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 claims 1
- 238000009792 diffusion process Methods 0.000 claims 1
- 229910052719 titanium Inorganic materials 0.000 claims 1
- 239000010936 titanium Substances 0.000 claims 1
- 229920001296 polysiloxane Polymers 0.000 abstract 1
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 230000003993 interaction Effects 0.000 description 3
- 230000005540 biological transmission Effects 0.000 description 2
- 239000006185 dispersion Substances 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 229910052814 silicon oxide Inorganic materials 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は波長多重光伝送に必要とされる光合波分波器に
関し、特に単一モード光伝送系に用いられる光集積回路
化に適した波長可変形の光合波分波器に関する。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to an optical multiplexer/demultiplexer required for wavelength multiplexed optical transmission, and is particularly suitable for optical integrated circuits used in single mode optical transmission systems. This invention relates to a variable wavelength optical multiplexer/demultiplexer.
従来、光合波分波器の一つとして、誘電体基板上に2本
の非対称な光導波路を形成し、これら2つの光導波路の
伝搬定数が特定波長で同一となるようにパラメータを設
定した同方向性結合を利用したものが知られている。Conventionally, as an optical multiplexer/demultiplexer, two asymmetrical optical waveguides are formed on a dielectric substrate, and parameters are set so that the propagation constants of these two optical waveguides are the same at a specific wavelength. One that utilizes directional coupling is known.
上述した従来の光合波分波器は、分波する波長の中心値
は、2つの光導波路の屈折率分布と寸法のみによって設
定されてしまうため、合波分波回路の設計における自由
度が乏しいという問題がある。In the conventional optical multiplexer/demultiplexer described above, the center value of the wavelength to be demultiplexed is set only by the refractive index distribution and dimensions of the two optical waveguides, so there is little freedom in designing the multiplexer/demultiplexer circuit. There is a problem.
本発明の光合波分波器は、任意の波長の入射光のみを−
の光導波路から取り出すことを可能とするものである。The optical multiplexer/demultiplexer of the present invention allows only incident light of an arbitrary wavelength to be -
This makes it possible to extract the light from the optical waveguide.
本発明の光合波分波器は、強誘電体基板に形成した2つ
の非対称光導波路間に、これらと平行に周期的に屈折率
の異なる溝を形成してこれを屈折率の周期的摂動として
構成するとともに、各光導波路には電気光学効果を生起
させる電極を配設した構成としている。The optical multiplexer/demultiplexer of the present invention forms grooves with periodically different refractive indexes in parallel between two asymmetric optical waveguides formed on a ferroelectric substrate, and uses this as a periodic perturbation of the refractive index. In addition, each optical waveguide is provided with an electrode that produces an electro-optic effect.
次に、本発明を図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.
第1図は本発明の一実施例の斜視図、第2図はその■■
線に沿う断面図である。Fig. 1 is a perspective view of one embodiment of the present invention, and Fig. 2 is its
It is a sectional view along a line.
図示のように所定厚さのL i N b Osで形成し
た強誘電体基板1の表面には、Tiを熱拡散して非対称
な、つまり断面寸法の異なる2本の光導波路2.3を形
成している。ここでは、各光導波路2.3は夫々テーバ
状またはこれに近い形状に構成している。また、前記強
誘電体基板1の表面上には酸化シリコン等からなるバッ
ファ層4を形成し、この上面でかつ前記光導波路2.3
上の位置には電極5.6を形成している。ここでは、こ
れら電極5,6は前記光導波路2,3の長さ方向に適宜
間隔おいて夫々2個の電極を配設している。As shown in the figure, on the surface of a ferroelectric substrate 1 made of L i N b Os with a predetermined thickness, Ti is thermally diffused to form two optical waveguides 2.3 which are asymmetrical, that is, have different cross-sectional dimensions. are doing. Here, each optical waveguide 2.3 is configured to have a tapered shape or a shape close to this. A buffer layer 4 made of silicon oxide or the like is formed on the surface of the ferroelectric substrate 1, and the optical waveguide 2.3 is formed on the upper surface of the buffer layer 4.
Electrodes 5.6 are formed at the upper position. Here, two electrodes 5 and 6 are respectively arranged at appropriate intervals in the length direction of the optical waveguides 2 and 3.
これら電極5.6には基板1との間に電圧が印加され、
この電圧に応じた電気光学効果によって前記光導波路2
.3の夫々の屈折率が変化できるように構成している。A voltage is applied between these electrodes 5.6 and the substrate 1,
Due to the electro-optic effect according to this voltage, the optical waveguide 2
.. The structure is such that the refractive index of each of the three lenses can be changed.
一方、前記強誘電体基板1表面の前記光導波路2.3の
間には、長さ方向に所定ピッチ八を有する複数個の矩形
状の溝8を形成しかつこの溝8内に前記バッファ層4を
充填させた構成の屈折率の周期的摂動7を形成している
。即ち、この溝8によりこの部分の屈折率が低減され、
他の基板1との間で周期的な屈折率の凹凸が構成され、
これが屈折率の周期的摂動として機能することになる。On the other hand, a plurality of rectangular grooves 8 having a predetermined pitch in the longitudinal direction are formed between the optical waveguides 2 and 3 on the surface of the ferroelectric substrate 1, and the buffer layer is formed in the grooves 8. A periodic perturbation 7 of the refractive index having a configuration filled with 4 is formed. That is, the refractive index of this part is reduced by this groove 8,
A periodic refractive index unevenness is formed between the substrate 1 and the other substrate 1,
This functions as a periodic perturbation of the refractive index.
この構成において、今光導波路3の一端に入力光■、が
入射され、光導波路2,3の他端に出力光Ox、Oxが
夫々出力されるものとする。ここで、前記入力光はλ8
.λ2・・・λ9のN波長の光からなり、出力光0□は
その中からλ7の光のみが分波された場合を示している
。出力光O1は他の波長の光が出力されていることは言
うまでもない。In this configuration, it is assumed that the input light (1) is incident on one end of the optical waveguide 3, and the output lights Ox, Ox are outputted on the other ends of the optical waveguides 2 and 3, respectively. Here, the input light is λ8
.. It consists of light of N wavelengths λ2...λ9, and the output light 0□ shows the case where only the light of λ7 is demultiplexed. It goes without saying that the output light O1 is light of other wavelengths.
次に、前記構成の光合波分波器の動作原理を説明する。Next, the operating principle of the optical multiplexer/demultiplexer having the above configuration will be explained.
第3図は2つの光導波路2.3の夫々の導波モードの分
散特性d、、d、を示し、Cは真空中の光速度、ncl
n! + n3は夫々基板1.導波路2、導波路
3の屈折率である。いま、波長λ7゜即ち角周波数ω、
(−2πC/λ7)の入射光に着目すると、2つの導波
路の伝搬定数β2.β。Figure 3 shows the dispersion characteristics d, , d, of the respective waveguide modes of the two optical waveguides 2.3, where C is the speed of light in vacuum, ncl
n! +n3 are respectively substrates 1. This is the refractive index of waveguide 2 and waveguide 3. Now, the wavelength λ7°, that is, the angular frequency ω,
Focusing on the incident light of (-2πC/λ7), the propagation constant β2 of the two waveguides. β.
の間に、
Δβ=β、−β2 ・・・・ (1)
たけ位相差が生じ、2つの導波モード間の相互作用は非
常に小さい。そこで、
Δβ=に=Δ/2π・・・ (2)
だけの位相差を屈折率の周期摂動により供給することに
より、2つの導波モードで有効に相互作用し、2つの導
波モード間で周期的な電力の移行が行われる。During this time, a phase difference of Δβ=β, −β2 (1) occurs, and the interaction between the two waveguide modes is very small. Therefore, by supplying a phase difference of Δβ==Δ/2π... (2) by periodic perturbation of the refractive index, the two waveguide modes interact effectively, and the two waveguide modes Periodic power transitions occur.
したがって、2つの導波路2.3間の結合係数と相互作
用長の積が(2m+1)Xπ/2になるように屈折率の
周期的摂動7を設計すれば、位相整合条件が満たされて
いる波長λ7の人力光のみを入射光導波路3に結合して
いる他の導波路2から取り出すことができる。この場合
、結合係数と相互作用長の積が上記式を満足しない場合
には、電極5.6に電圧を印加して条件を満足させれば
よい。Therefore, if the periodic perturbation 7 of the refractive index is designed so that the product of the coupling coefficient and the interaction length between the two waveguides 2.3 is (2m+1)Xπ/2, the phase matching condition is satisfied. Only the human power light with wavelength λ7 can be taken out from the other waveguide 2 coupled to the input optical waveguide 3. In this case, if the product of the coupling coefficient and the interaction length does not satisfy the above equation, a voltage may be applied to the electrode 5.6 to satisfy the condition.
この構成によれば、基板1の2つの光導波路2゜3間に
周期的な溝8を形成し、この溝8による周期的な屈折率
の凹凸、即ち屈折率の周期的摂動7を形成することによ
り、導波モード間の位相整合条件を満足させ、特定波長
の入射光のみを−の導波路から取り出すことができる。According to this configuration, periodic grooves 8 are formed between the two optical waveguides 2.3 of the substrate 1, and the grooves 8 form periodic irregularities in the refractive index, that is, periodic perturbations 7 in the refractive index. By doing so, it is possible to satisfy the phase matching condition between the waveguide modes and extract only the incident light of a specific wavelength from the negative waveguide.
また、電極5゜6に適宜電圧を印加することにより、整
合条件を満たす波長を変化でき、取り出す光の波長を変
えることができる。この光合波分波器は見方を変えれば
波長スイッチ素子であると考えることもできる。Further, by applying an appropriate voltage to the electrodes 5.6, the wavelength that satisfies the matching condition can be changed, and the wavelength of the light to be extracted can be changed. From a different perspective, this optical multiplexer/demultiplexer can be thought of as a wavelength switching element.
ここで、屈折率の周期的摂動は、第4図に符号7Aで示
すようにバッファ層4に形成した周期的な溝8Aで構成
してもよく、この溝8Aにおける屈折率を他の部分より
も低くすることにより周期的な屈折率の凹凸を形成し、
これにより前例と同様の効果を得ることができる。Here, the periodic perturbation of the refractive index may be formed by periodic grooves 8A formed in the buffer layer 4, as shown by reference numeral 7A in FIG. By lowering the refractive index, periodic irregularities in the refractive index are formed.
With this, the same effect as the previous example can be obtained.
なお、光導波路をテーパ構造にすることにより、分波波
長帯域の制jIIが可能となり、また偏光依存性を除去
することも可能となる。Note that by forming the optical waveguide into a tapered structure, it is possible to control the demultiplexed wavelength band, and it is also possible to eliminate polarization dependence.
以上説明したように本発明は、2つの非対称光導波路間
に周期的に屈折率の異なる溝からなる屈折率の周期的摂
動を構成するとともに、各光導波路には電気光学効果を
生起させる電極を配設しているので、2つの光4波路に
おける導波モード間の位相整合条件を満足させ、特定波
長の入射光のみを−の導波路から取り出すことができる
とともに、電極に適宜電圧を印加することにより、整合
条件を満たす波長を変化でき、取り出す光の波長を変え
ることができる。As explained above, the present invention constitutes a periodic perturbation of the refractive index consisting of grooves with periodically different refractive indexes between two asymmetrical optical waveguides, and each optical waveguide is provided with an electrode that produces an electro-optic effect. This allows it to satisfy the phase matching conditions between the waveguide modes in the two four-wavelength optical waveguides, extract only the incident light of a specific wavelength from the negative waveguide, and apply an appropriate voltage to the electrodes. By doing so, the wavelength that satisfies the matching condition can be changed, and the wavelength of the light to be extracted can be changed.
第1図は本発明の一実施例の斜視図、第2図は第1図の
on線に沿う断面図、第3図は導波モードの分散特性を
示す図、第4図は変形例の断面図で第2図と同様の図で
ある。
1・・・強誘電体基板、2.3・・・光導波路、4・・
・バッファ層、5.6・・・電極、7,7A・・・屈折
率の周期的摂動、8,8A・・・溝。FIG. 1 is a perspective view of one embodiment of the present invention, FIG. 2 is a sectional view taken along the on line in FIG. 1, FIG. 3 is a diagram showing the dispersion characteristics of the waveguide mode, and FIG. FIG. 2 is a sectional view similar to FIG. 2; 1... Ferroelectric substrate, 2.3... Optical waveguide, 4...
- Buffer layer, 5.6... Electrode, 7,7A... Periodic perturbation of refractive index, 8,8A... Groove.
Claims (4)
2つの非対称な光導波路を備える光合波分波器において
、前記2つの光導波路間に、これらと平行に周期的に屈
折率の異なる溝を形成してこれを屈折率の周期的摂動と
して構成するとともに、各光導波路には電気光学効果を
生起させる電極を配設したことを特徴とする光合波分波
器。(1) In an optical multiplexer/demultiplexer equipped with two asymmetrical optical waveguides formed by thermal diffusion of titanium or the like on a ferroelectric substrate, there is a periodic difference in refractive index between the two optical waveguides in parallel with them. An optical multiplexer/demultiplexer characterized in that grooves are formed to constitute periodic perturbations in the refractive index, and each optical waveguide is provided with an electrode that produces an electro-optic effect.
形成して屈折率の周期的摂動を構成してなる特許請求の
範囲第1項記載の光合波分波器。(2) The optical multiplexer/demultiplexer according to claim 1, wherein a plurality of grooves at a predetermined pitch are formed on the surface of a ferroelectric substrate to constitute a periodic perturbation of the refractive index.
所定ピッチの複数個の溝を形成して屈折率の周期的摂動
を構成してなる特許請求の範囲第1項記載の光合波分波
器。(3) Optical multiplexing according to claim 1, wherein a plurality of grooves at a predetermined pitch are formed on the surface of a buffer layer provided on the surface of a ferroelectric substrate to constitute periodic perturbation of the refractive index. Duplexer.
求の範囲第1項記載の光合波分波器。(4) The optical multiplexer/demultiplexer according to claim 1, which comprises two optical waveguides formed in a tapered shape.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61054938A JPS62212631A (en) | 1986-03-14 | 1986-03-14 | Optical multiplexer and demultiplexer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61054938A JPS62212631A (en) | 1986-03-14 | 1986-03-14 | Optical multiplexer and demultiplexer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62212631A true JPS62212631A (en) | 1987-09-18 |
Family
ID=12984578
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61054938A Pending JPS62212631A (en) | 1986-03-14 | 1986-03-14 | Optical multiplexer and demultiplexer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62212631A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5274487A (en) * | 1989-12-29 | 1993-12-28 | Fujitsu Limited | Photonic switching system |
KR100403673B1 (en) * | 2001-12-12 | 2003-10-30 | 한국전자통신연구원 | Method for forming on a fiber two thin conductive films isolated electrically each other |
KR100420951B1 (en) * | 2002-04-17 | 2004-03-02 | 한국전자통신연구원 | Poled fibers, a method for fabricating a poled fiber, and dispersion compensator |
-
1986
- 1986-03-14 JP JP61054938A patent/JPS62212631A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5274487A (en) * | 1989-12-29 | 1993-12-28 | Fujitsu Limited | Photonic switching system |
KR100403673B1 (en) * | 2001-12-12 | 2003-10-30 | 한국전자통신연구원 | Method for forming on a fiber two thin conductive films isolated electrically each other |
KR100420951B1 (en) * | 2002-04-17 | 2004-03-02 | 한국전자통신연구원 | Poled fibers, a method for fabricating a poled fiber, and dispersion compensator |
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