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JPH01102435A - Optical modulator - Google Patents

Optical modulator

Info

Publication number
JPH01102435A
JPH01102435A JP26039087A JP26039087A JPH01102435A JP H01102435 A JPH01102435 A JP H01102435A JP 26039087 A JP26039087 A JP 26039087A JP 26039087 A JP26039087 A JP 26039087A JP H01102435 A JPH01102435 A JP H01102435A
Authority
JP
Japan
Prior art keywords
superconductor
extra
high frequencies
optical modulator
optical
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
Application number
JP26039087A
Other languages
Japanese (ja)
Inventor
Noriaki Tsukada
塚田 紀昭
Taku Noguchi
卓 野口
Kazuyoshi Kojima
一良 児島
Kyozo Kanemoto
恭三 金本
Kunio Ookawa
大川 訓生
Tetsuya Takami
高見 哲也
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP26039087A priority Critical patent/JPH01102435A/en
Publication of JPH01102435A publication Critical patent/JPH01102435A/en
Pending legal-status Critical Current

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  • Optical Integrated Circuits (AREA)

Abstract

PURPOSE:To decrease frequency dispersion and to enable modulation up to extra-high frequencies by using a superphotoconductor as an electrode material in order to change the coupling constant between two light guides by an electro- optic effect. CONSTITUTION:The conventional normal conductor is changed to a superconductor and is then used as a microwave strip line 23 which constitutes a part of an optical modulator. The oxide superconductor of a recently discovered La-Ba-Cu-O system or Y-Ba-Cu-O system which is a ceramic system of the critical temp. Tc=90K class grows as a single crystal on a perovskite type dielectric substrate (for example, SrTiO3 or LiNbO3), etc.). The microwave strip line 23 formed of the superconductor is the extremely small frequency distribution to frequencies below the gap energy intrinsic to the superconductor and has the excellent capability as the transmission line for extra-high frequencies. For example, the oxide superconductor of the Y-Ba-Cu-O system has 30meV gap energy and is capable of transmitting the extra-high frequencies up to about 10<12>Hz; therefore, the light modulation by the extra-high frequencies in 10<12>Hz order is possible.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は光変調器に関し、特に進行波型先方向性結合
器を用いた高速光変調器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an optical modulator, and more particularly to a high-speed optical modulator using a traveling wave type forward coupler.

〔従来の技術〕[Conventional technology]

第2図は例えば、アイイーイーイー ジャーナル オブ
 クワオンタム エレクトロニクス(IHRI! Jo
urnal of Quantum I!1ectro
nica ) Qf!−16巻、754真に示された従
来の進行波型光変調器の構成図であり、図において、l
はLiNbO5誘電体基板、2a、  2bは基板1に
Ti拡散することにより形成された光導波路、3は光導
波路2a、2b上に形成されたAJI電極、4a、4b
はそれぞれマイクロ波進行波の入力リード線、出力リー
ド線、5a、5bはそれぞれ入力光、出力光である。
Figure 2 shows, for example, the International Journal of Quantum Electronics (IHRI! Jo
Urnal of Quantum I! 1electro
nica ) Qf! This is a configuration diagram of a conventional traveling wave optical modulator shown in Vol. 16, 754, and in the figure, l
is a LiNbO5 dielectric substrate, 2a and 2b are optical waveguides formed by diffusing Ti on the substrate 1, 3 is an AJI electrode formed on the optical waveguides 2a and 2b, 4a and 4b
are an input lead wire and an output lead wire for microwave traveling waves, respectively, and 5a and 5b are input light and output light, respectively.

次に動作について説明する。Next, the operation will be explained.

入力光5aは常に一定強度の連続(cw)光であり、進
行波マイクロ波信号がない時にはcw光が入射された光
導波路2aの出力端にそのまま送り出される。マイクロ
波進行波が入力リード線4aから入力されたとき、この
マイクロ波と同期して進行する入射光の一部が、誘電体
基板1の電気光学効果により他の光導波路2b側に結合
される。
The input light 5a is always continuous (cw) light with a constant intensity, and when there is no traveling wave microwave signal, it is sent out as it is to the output end of the optical waveguide 2a into which the cw light is input. When a traveling microwave wave is input from the input lead wire 4a, a part of the incident light traveling in synchronization with the microwave is coupled to the other optical waveguide 2b side due to the electro-optic effect of the dielectric substrate 1. .

つまり、マイクロ波信号に対応した変調光が光導波路2
bの出力として得られる。
In other words, the modulated light corresponding to the microwave signal is transmitted through the optical waveguide 2.
It is obtained as the output of b.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来の光変調器は以上のように構成されているので、変
調速度はマイクロ波の進行するAjl電極の周波数分散
特性によって律則されるため、変調周波数は最高5〜1
0GHzに制限されていた。
Since the conventional optical modulator is configured as described above, the modulation speed is determined by the frequency dispersion characteristics of the Ajl electrode through which the microwave propagates, so the modulation frequency is at most 5 to 1.
It was limited to 0GHz.

この発明は上記のような問題点を解消するためになされ
たもので、超高速の光変調を行うことのできる光変調器
を得ることを目的とする。
The present invention was made to solve the above-mentioned problems, and an object of the present invention is to obtain an optical modulator that can perform ultra-high-speed optical modulation.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る光変調器は、マイクロ波伝幡用電橿とし
て、超伝導電極を用いたものである。
The optical modulator according to the present invention uses a superconducting electrode as a microwave propagation cable.

〔作用〕[Effect]

この発明における光変調器は、マイクロ波伝幡用電極と
して、超伝導電極を用いたので、周波数分散を非常に小
さくでき、超高周波数(THzオーダ)まで変調が可能
となる。
Since the optical modulator of the present invention uses a superconducting electrode as the electrode for microwave propagation, frequency dispersion can be made very small, and modulation up to extremely high frequencies (THz order) is possible.

〔実施例〕〔Example〕

以下、この発明の一実施例を図について説明する。 An embodiment of the present invention will be described below with reference to the drawings.

第1図はこの発明の一実施例による光変調器の構成図で
ある0図において、21は電気光学効果ををするペロブ
スカイト型構造の強誘電体基板、2a、2bはこの基板
21上にTi拡散等で形成された光導波路、23は超伝
導電極、4 a *  4 bはそれぞれマイクロ波の
入力リード線、出力リード線、5a、5bはそれぞれ入
力光、出力光である。
FIG. 1 is a block diagram of an optical modulator according to an embodiment of the present invention. In FIG. An optical waveguide formed by diffusion etc., 23 is a superconducting electrode, 4a*4b are microwave input lead wires and output lead wires, respectively, and 5a and 5b are input light and output light, respectively.

動作原理は従来例で述べた、進行波型光方向性結合器を
用いた進行波型光変調器と同様である。
The operating principle is the same as that of the traveling wave optical modulator using the traveling wave optical directional coupler described in the conventional example.

本発明の本質は、光変調器の一部を構成するマイクロ波
ストリップ線路23として、従来の常伝導Ba−Cu−
0系酸化物超伝導体はペロブスカイト型誘電体基板(例
えば5rTiO*やLiNb0り等)上に単結晶成長す
る。また、超伝導体で形成されたマイクロ波ストリップ
線路23は超伝導体固有のギャップエネルギー以下の周
波数に対して周波数分散が非常に小さく、超高周波の伝
送線としての能力に優れている0例えば、上記Y−Ba
−Cu−0系酸化物趨伝導体のギャップエネルギーは3
0meVもあり、約THz (10”Hz)までの超高
周波の伝送が可能であり、このため、THzオーダにお
ける超高周波による光変調が可能となる。
The essence of the present invention is that the conventional normal conduction Ba-Cu-
The 0-based oxide superconductor is grown as a single crystal on a perovskite dielectric substrate (for example, 5rTiO*, LiNb0, etc.). In addition, the microwave strip line 23 made of a superconductor has very small frequency dispersion for frequencies below the gap energy inherent in superconductors, and has excellent performance as an ultra-high frequency transmission line.For example, Above Y-Ba
-The gap energy of Cu-0 based oxide trend conductor is 3
0 meV, it is possible to transmit ultra-high frequencies up to about THz (10''Hz), and therefore optical modulation using ultra-high frequencies on the THz order becomes possible.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明の光変調器によれば、マイクロ
波ストリップ線路電極として超伝導体を用いたので、T
l1zオーダにおける超高周波による光変調が可能とな
る効果がある。
As described above, according to the optical modulator of the present invention, since a superconductor is used as the microwave strip line electrode, T
This has the effect of making it possible to perform optical modulation using ultra-high frequencies on the l1z order.

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

第1図はこの発明の一実施例による光変調器の構成図、
第2図は従来の光変調器の構成図である。 1は誘電体基板、2a、2bは光導波路、3は電極、4
a、4bはそれぞれマイクロ波の人、出力リード線、5
a、5bはそれぞれ人、出力光、21はペロブスカイト
型結晶構造を有する誘電体基板、23はマイクロ波スト
リップ線路としての高温超伝導薄膜電極である。 なお図中同一符号は同−又は相当部分を示す。
FIG. 1 is a configuration diagram of an optical modulator according to an embodiment of the present invention;
FIG. 2 is a block diagram of a conventional optical modulator. 1 is a dielectric substrate, 2a and 2b are optical waveguides, 3 is an electrode, 4
a, 4b are microwave connectors, output lead wires, 5
21 is a dielectric substrate having a perovskite crystal structure, and 23 is a high temperature superconducting thin film electrode as a microwave strip line. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (2)

【特許請求の範囲】[Claims] (1)誘電体基板と、該誘電体基板上に形成された2つ
の光導波路と、該2つの光導波路間の結合定数を進行波
によって変化させる進行波型光方向性結合器とを備えた
光変調器において、上記2つの光導波路間の結合定数を
電気光学効果により変化させるための電極材料として、
超伝導体を使用したことを特徴とする光変調器。
(1) A dielectric substrate, two optical waveguides formed on the dielectric substrate, and a traveling wave optical directional coupler that changes the coupling constant between the two optical waveguides by a traveling wave. In the optical modulator, as an electrode material for changing the coupling constant between the two optical waveguides by electro-optic effect,
An optical modulator characterized by using a superconductor.
(2)上記誘電体基板として、LiNbO_3、SrT
iO_3等のペロブスカイト型構造を有する結晶を用い
、上記超伝導電極としてLa−Ba−Cu−O系あるい
はY−Ba−Cu−O系の酸化物超伝導体を使用したこ
とを特徴とする特許請求の範囲第1項記載の光変調器。
(2) As the dielectric substrate, LiNbO_3, SrT
A patent claim characterized in that a crystal having a perovskite structure such as iO_3 is used, and a La-Ba-Cu-O-based or Y-Ba-Cu-O-based oxide superconductor is used as the superconducting electrode. The optical modulator according to the range 1 above.
JP26039087A 1987-10-15 1987-10-15 Optical modulator Pending JPH01102435A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26039087A JPH01102435A (en) 1987-10-15 1987-10-15 Optical modulator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26039087A JPH01102435A (en) 1987-10-15 1987-10-15 Optical modulator

Publications (1)

Publication Number Publication Date
JPH01102435A true JPH01102435A (en) 1989-04-20

Family

ID=17347254

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26039087A Pending JPH01102435A (en) 1987-10-15 1987-10-15 Optical modulator

Country Status (1)

Country Link
JP (1) JPH01102435A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6498358B1 (en) 2001-07-20 2002-12-24 Motorola, Inc. Structure and method for fabricating an electro-optic system having an electrochromic diffraction grating
US6855992B2 (en) 2001-07-24 2005-02-15 Motorola Inc. Structure and method for fabricating configurable transistor devices utilizing the formation of a compliant substrate for materials used to form the same
US6885065B2 (en) 2002-11-20 2005-04-26 Freescale Semiconductor, Inc. Ferromagnetic semiconductor structure and method for forming the same
US6965128B2 (en) 2003-02-03 2005-11-15 Freescale Semiconductor, Inc. Structure and method for fabricating semiconductor microresonator devices
US6992321B2 (en) 2001-07-13 2006-01-31 Motorola, Inc. Structure and method for fabricating semiconductor structures and devices utilizing piezoelectric materials
US7045815B2 (en) 2001-04-02 2006-05-16 Freescale Semiconductor, Inc. Semiconductor structure exhibiting reduced leakage current and method of fabricating same
US7342276B2 (en) 2001-10-17 2008-03-11 Freescale Semiconductor, Inc. Method and apparatus utilizing monocrystalline insulator

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7045815B2 (en) 2001-04-02 2006-05-16 Freescale Semiconductor, Inc. Semiconductor structure exhibiting reduced leakage current and method of fabricating same
US6992321B2 (en) 2001-07-13 2006-01-31 Motorola, Inc. Structure and method for fabricating semiconductor structures and devices utilizing piezoelectric materials
US6498358B1 (en) 2001-07-20 2002-12-24 Motorola, Inc. Structure and method for fabricating an electro-optic system having an electrochromic diffraction grating
US6855992B2 (en) 2001-07-24 2005-02-15 Motorola Inc. Structure and method for fabricating configurable transistor devices utilizing the formation of a compliant substrate for materials used to form the same
US7342276B2 (en) 2001-10-17 2008-03-11 Freescale Semiconductor, Inc. Method and apparatus utilizing monocrystalline insulator
US6885065B2 (en) 2002-11-20 2005-04-26 Freescale Semiconductor, Inc. Ferromagnetic semiconductor structure and method for forming the same
US6965128B2 (en) 2003-02-03 2005-11-15 Freescale Semiconductor, Inc. Structure and method for fabricating semiconductor microresonator devices

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