JP2001274624A - Microwave oscillator - Google Patents
Microwave oscillatorInfo
- Publication number
- JP2001274624A JP2001274624A JP2000086163A JP2000086163A JP2001274624A JP 2001274624 A JP2001274624 A JP 2001274624A JP 2000086163 A JP2000086163 A JP 2000086163A JP 2000086163 A JP2000086163 A JP 2000086163A JP 2001274624 A JP2001274624 A JP 2001274624A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- microwave
- microwave oscillator
- oscillator
- magnetic pole
- 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
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
- Inductance-Capacitance Distribution Constants And Capacitance-Resistance Oscillators (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、YIG(イットリウム
・鉄・ガーネット)等のフェリ磁性薄膜を利用したマイ
クロ波発振器に関わる。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a microwave oscillator using a ferrimagnetic thin film such as YIG (yttrium / iron / garnet).
【0002】[0002]
【従来の技術】GGG(ガドリニウム・ガリウム・ガー
ネット)等の非磁性基板上に液相エピタキシャル成長さ
せたYIG単結晶磁性薄膜を所要の形状に加工したフェ
リ磁性薄膜静磁波共振子に、外部から直流磁界を印加す
ると静磁波が励起し、マイクロ波能動素子(例えばGa
As FET等)と結合させることでマイクロ波出力を
得るマイクロ波発振器が提案されている。図2に、従来
技術によるマイクロ波発振器の構造断面図を示す。静磁
波共振子1を配したマイクロ波回路基板2を、パーマロ
イ等のヨーク3内に固定し、磁極4と変調コイル5によ
って静磁波共振子に直流磁界を印加してマイクロ波出力
を得る構造となっている。一般的にヨーク3、磁極4お
よび変調コイル5を総称して磁気回路と呼んでいる。ま
た、マイクロ波出力の周波数は、変調コイル5に流す電
流により直流磁界の大きさを変化させることによって制
御する。2. Description of the Related Art An external DC magnetic field is applied to a ferrimagnetic thin-film magnetostatic wave resonator formed by processing a YIG single-crystal magnetic thin film formed on a nonmagnetic substrate such as GGG (gadolinium / gallium / garnet) into a required shape by liquid phase epitaxial growth. Is applied, a magnetostatic wave is excited, and a microwave active element (for example, Ga
A microwave oscillator that obtains a microwave output by being combined with an As FET or the like has been proposed. FIG. 2 shows a structural sectional view of a microwave oscillator according to the prior art. A structure in which a microwave circuit board 2 on which a magnetostatic wave resonator 1 is disposed is fixed in a yoke 3 made of permalloy or the like, and a magnetic field 4 and a modulation coil 5 apply a DC magnetic field to the magnetostatic wave resonator to obtain a microwave output. Has become. Generally, the yoke 3, the magnetic pole 4, and the modulation coil 5 are collectively called a magnetic circuit. The frequency of the microwave output is controlled by changing the magnitude of the DC magnetic field by the current flowing through the modulation coil 5.
【0003】[0003]
【発明が解決しようとする課題】しかし、前述の構造の
マイクロ波発振器は、ヨーク3内においてマイクロ波回
路基板上の空洞部分6によって空洞共振が発生し、延い
ては発振停止等の発振器特性劣化を生ずるという問題が
あった。図4は、従来技術によるマイクロ波発振器の発
振出力の周波数特性を示したものである。約8.9〜
9.1GHzにおいて発振停止の現象が見られた。この
問題を解決する手段として、磁極4やヨーク3の形状お
よび寸法を変えて、空洞部分の体積ならびに回路基板と
の結合を変えることで、空洞共振周波数を発振器の動作
周波数帯域外に変化させるといった方法が考えられる
が、それに伴って直流磁界の強度や分布等の磁気回路磁
気特性の変化が生じ、設計が複雑化および困難となる。However, in the microwave oscillator having the above-described structure, cavity resonance occurs in the yoke 3 due to the hollow portion 6 on the microwave circuit board, and as a result, oscillator characteristics are deteriorated such as oscillation stop. There is a problem that FIG. 4 shows the frequency characteristics of the oscillation output of a microwave oscillator according to the prior art. About 8.9 ~
At 9.1 GHz, a phenomenon of oscillation stop was observed. As a means for solving this problem, changing the shape and dimensions of the magnetic pole 4 and the yoke 3 to change the volume of the cavity and the coupling with the circuit board to change the cavity resonance frequency to outside the operating frequency band of the oscillator. Although a method is conceivable, the magnetic characteristics of the magnetic circuit, such as the intensity and distribution of the DC magnetic field, change, and the design becomes complicated and difficult.
【0004】[0004]
【課題を解決するための手段】そこで、前記空洞共振を
制御するために、磁極およびヨーク形状は変えずに磁極
の周りに金属リングを配し、空洞部分の体積ならびに回
路基板との結合を変えることで、発振器の動作周波数帯
域外に空洞共振周波数を変化させ、発振特性の劣化を防
ぐ方法を見い出した。この金属リングの形状および寸法
は、発振器の動作周波数帯域と空洞共振周波数により最
適値を求める。また、このようにして配置された金属リ
ングによって磁気特性が劣化してはならないので、本発
明の第2の目的は空洞共振制御を磁気特性の劣化無く行
うことである。そのため、前記金属リングとしては非磁
性金属を用いれば、磁界分布や磁界強度を劣化させるこ
と無く空洞共振の制御を行うことができる。この非磁性
金属の材質には、例えば、Al、BS、Cuを用いるこ
とができる。In order to control the cavity resonance, a metal ring is arranged around the magnetic pole without changing the shape of the magnetic pole and the yoke to change the volume of the cavity and the coupling with the circuit board. As a result, they found a method of changing the cavity resonance frequency outside the operating frequency band of the oscillator to prevent deterioration of the oscillation characteristics. The optimum shape and size of the metal ring are determined based on the operating frequency band of the oscillator and the cavity resonance frequency. Further, since the magnetic characteristics must not be deteriorated by the metal ring arranged in this way, a second object of the present invention is to perform cavity resonance control without deterioration of the magnetic characteristics. Therefore, if a non-magnetic metal is used as the metal ring, it is possible to control the cavity resonance without deteriorating the magnetic field distribution and the magnetic field strength. As the material of the nonmagnetic metal, for example, Al, BS, Cu can be used.
【0005】[0005]
【実施例】図1は本発明の実施例を示す図である。従来
の発振器の構造に加えて、非磁性金属リング7を磁極4
の周りに配した構造で、動作周波数帯が約8.1〜9.
7GHzの9GHz帯発振器を作製した。この金属リン
グの形状寸法は、発振器の動作周波数帯域と空洞共振周
波数から最適化し、リング径をヨークの内寸法と同じφ
24mm、高さを6mmとした。また金属リングの材質
にはAlを用いた。この発振器の発振出力の周波数特性
を図3に示す。動作周波数帯8.1〜9.7GHzにわ
たって、従来構造での空洞共振による発振停止現象は見
られず、良好な発振出力が得られた。FIG. 1 is a diagram showing an embodiment of the present invention. In addition to the conventional oscillator structure, the nonmagnetic metal ring 7 is
, And the operating frequency band is about 8.1-9.
A 9 GHz band oscillator of 7 GHz was manufactured. The shape and dimensions of this metal ring are optimized from the operating frequency band of the oscillator and the cavity resonance frequency, and the ring diameter is the same as the inner dimension of the yoke.
The height was 24 mm and the height was 6 mm. Al was used as the material of the metal ring. FIG. 3 shows the frequency characteristics of the oscillation output of this oscillator. Over the operating frequency band of 8.1 to 9.7 GHz, no oscillation stop phenomenon due to cavity resonance in the conventional structure was observed, and a good oscillation output was obtained.
【0006】[0006]
【発明の効果】本発明によれば、非磁性金属リングを磁
極の周りに配することで、空洞共振周波数を制御できる
ので、発振停止等無く安定した発振出力を得ることがで
きた。また、非磁性金属を用いたので磁気特性を劣化さ
せること無く容易に発振特性の安定化が図れた。According to the present invention, the cavity resonance frequency can be controlled by disposing the non-magnetic metal ring around the magnetic pole, so that a stable oscillation output can be obtained without stopping the oscillation. In addition, the use of a non-magnetic metal facilitated stabilization of oscillation characteristics without deteriorating magnetic characteristics.
【図1】本発明による実施例を示す構造断面図。FIG. 1 is a structural sectional view showing an embodiment according to the present invention.
【図2】従来技術によるマイクロ波発振器の構造断面
図。FIG. 2 is a structural sectional view of a microwave oscillator according to the related art.
【図3】実施例によるマイクロ波発振器の発振出力の周
波数特性図。FIG. 3 is a frequency characteristic diagram of an oscillation output of the microwave oscillator according to the embodiment.
【図4】従来技術によるマイクロ波発振器の発振出力の
周波数特性図。FIG. 4 is a frequency characteristic diagram of an oscillation output of a microwave oscillator according to the related art.
1 静磁波共振子 2 マイクロ波回路基板 3 ヨーク 4 磁極 5 変調コイル 6 空洞部分 7 非磁性金属リング DESCRIPTION OF SYMBOLS 1 Magnetostatic wave resonator 2 Microwave circuit board 3 Yoke 4 Magnetic pole 5 Modulation coil 6 Hollow part 7 Nonmagnetic metal ring
Claims (2)
子に直流磁界を印加するための磁極ならびに変調コイル
からなる磁気回路を有した構造のマイクロ波発振器にお
いて、前記磁極の周りに非磁性金属リングを配置するこ
とを特徴としたマイクロ波発振器。1. A microwave oscillator having a magnetic pole for applying a DC magnetic field to a magnetostatic wave element disposed on a microwave circuit board and a magnetic circuit comprising a modulation coil, wherein a nonmagnetic metal is provided around the magnetic pole. A microwave oscillator characterized by placing a ring.
いて、前記非磁性金属リングの材質はAlまたはBSま
たはCuであることを特徴とするマイクロ波発振器。2. The microwave oscillator according to claim 1, wherein the material of the nonmagnetic metal ring is Al, BS, or Cu.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2000086163A JP2001274624A (en) | 2000-03-27 | 2000-03-27 | Microwave oscillator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2000086163A JP2001274624A (en) | 2000-03-27 | 2000-03-27 | Microwave oscillator |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JP2001274624A true JP2001274624A (en) | 2001-10-05 |
Family
ID=18602376
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2000086163A Pending JP2001274624A (en) | 2000-03-27 | 2000-03-27 | Microwave oscillator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2001274624A (en) |
-
2000
- 2000-03-27 JP JP2000086163A patent/JP2001274624A/en active Pending
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