JPS5949649B2 - Materials for dielectric resonators - Google Patents

Materials for dielectric resonators

Info

Publication number
JPS5949649B2
JPS5949649B2 JP52096602A JP9660277A JPS5949649B2 JP S5949649 B2 JPS5949649 B2 JP S5949649B2 JP 52096602 A JP52096602 A JP 52096602A JP 9660277 A JP9660277 A JP 9660277A JP S5949649 B2 JPS5949649 B2 JP S5949649B2
Authority
JP
Japan
Prior art keywords
dielectric
materials
temperature
porcelain
dielectric resonators
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
Application number
JP52096602A
Other languages
Japanese (ja)
Other versions
JPS5430499A (en
Inventor
俊一郎 河島
正光 西田
一朗 上田
宏 大内
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP52096602A priority Critical patent/JPS5949649B2/en
Publication of JPS5430499A publication Critical patent/JPS5430499A/en
Publication of JPS5949649B2 publication Critical patent/JPS5949649B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は誘電体共振器用材料、特にBaO、ZnO、N
b2O5、CaOおよびZrO2の成分で構成される誘
電体共振器用材料に関するものであり、素体の無負荷Q
と誘電率εが大きく、かつ共振周波数の温度安定度γf
に優れたマイクロ波用誘電体共振器を構成することので
きる材料を提供しようとするものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides materials for dielectric resonators, particularly BaO, ZnO, N
This relates to dielectric resonator materials composed of b2O5, CaO, and ZrO2 components, and the unloaded Q of the element body is
and the dielectric constant ε is large, and the temperature stability of the resonance frequency γf
The purpose of this invention is to provide a material that can constitute a microwave dielectric resonator with excellent properties.

従来から、マイクロ波領域において、誘電体はマイクロ
波回路のインピーダンス整合や、誘電体共振器などに応
用されてきている。
Conventionally, in the microwave region, dielectric materials have been applied to impedance matching of microwave circuits, dielectric resonators, and the like.

近年、特に、マイクロ波回路の集積化の技術が進歩する
にともない、発振器の周波数の安定化などに、高誘電率
、低損失、低価格の誘電体磁器を使用して小形化するこ
とが積極的に進められている。従来、これらの誘電体と
しては、BaO−TiO2系磁器、およびその一部を他
の元素で置換した磁器、さらには誘電率が負の温度変化
をもつTiO2と正の誘電率の温度変化をもつ誘電体磁
器とを組合わせたものを使用する場合が多い。しかし、
これらは、誘電体損失が大きかつたり、誘電率の温度変
化のばらつきが大きかつたり、共振周波数の安定度が大
きすぎたりして、実用上問題が多い。
In recent years, especially as the integration technology of microwave circuits has progressed, there has been an active effort to use dielectric ceramics with high dielectric constant, low loss, and low cost to stabilize the frequency of oscillators and to miniaturize them. progress is being made. Conventionally, these dielectric materials include BaO-TiO2-based porcelain, porcelain in which part of it is replaced with other elements, and TiO2, which has a negative dielectric constant that changes with temperature, and TiO2, which has a positive dielectric constant that changes with temperature. A combination of dielectric ceramic and dielectric ceramic is often used. but,
These have many practical problems, such as large dielectric loss, large variations in temperature change in dielectric constant, and too high stability of resonance frequency.

出願人において、これらの欠点のない材料について、種
々検討した結果、一般式xBa0−yZn0・ZNb2
O5で表わされる組成において、0.5≦X≦0.75
、0.1≦y≦0.3、0.1≦z≦0.3(ただしx
+y+z=1)の範囲内にある組成の磁器が、優れた誘
電体マイノロ波共振器になることを見出した(特願昭5
1−110274号)。
As a result of various studies conducted by the applicant regarding materials that do not have these drawbacks, the general formula xBa0-yZn0・ZNb2
In the composition represented by O5, 0.5≦X≦0.75
, 0.1≦y≦0.3, 0.1≦z≦0.3 (where x
+y+z=1) found that porcelain with a composition within the range of
1-110274).

しかしながら、これは共振周波数の温度安定度γfがか
なり大きいものであり、その安定度を向上させるための
研究を進めた。本発明はその結果にもとづくものである
。本発明にかかる誘電体共振器用材料は、BaO、Zn
O、およびNb2O5に、さらにCaOとZrO2とを
加えることによつて、無負荷Q(Qu)と誘電率εを低
下させることなく、共振周波数の温度安定度γfを向上
させることができたものである。
However, the temperature stability γf of the resonant frequency is quite large, and research has been carried out to improve this stability. The present invention is based on that result. The dielectric resonator material according to the present invention includes BaO, Zn
By further adding CaO and ZrO2 to O and Nb2O5, it was possible to improve the temperature stability γf of the resonant frequency without reducing the no-load Q (Qu) and the dielectric constant ε. be.

その特徴とするところは、(11)(y、BaO−yZ
n0・ZNb205)+WCa0−ZrO2なる組成式
において、0.5≦X≦0.75、0.1≦y≦0.3
、0.1≦z≦0.3、x+y+z=1、0<w≦0.
9の範囲内にある組成を有することを特徴とする。以下
、実施例にもとづいて、本発明を説明する。まずBaC
O3,CaCO3,ZNO,Nb2O5およびZrO2
の出発原料を各組成に応じて秤量し、めのうボールを備
え、かつゴム内張りしたボールミルで、純水とともに湿
式混合した。
Its characteristics are (11) (y, BaO-yZ
In the composition formula n0・ZNb205)+WCa0−ZrO2, 0.5≦X≦0.75, 0.1≦y≦0.3
, 0.1≦z≦0.3, x+y+z=1, 0<w≦0.
It is characterized by having a composition within the range of 9. Hereinafter, the present invention will be explained based on Examples. First, BaC
O3, CaCO3, ZNO, Nb2O5 and ZrO2
The starting materials were weighed according to each composition and wet-mixed with pure water in a ball mill equipped with an agate ball and lined with rubber.

この混合物を乾燥させてから、空気中において1200
゜Cで5時時間仮焼した後、前記ボールミルで湿式粉砕
した。粉砕泥しようをボールミルから取出して乾燥させ
た後、圧力700kg/Cwiで直径256の円板に成
形し、それを空気中において1460〜136d’Cの
範囲内の温度で2時間焼成して、下表に示す組成の磁器
を得た。それから、各磁器から、それぞれ直径5−、厚
さ2−の寸法の円板形磁器の試料を切出し、それをマイ
クロ波用誘電体共振器に使用して、トラツブ法により共
振周波数を測定し、この共振周波数(ほぼ11GHz)
と直径とから誘電率εを、また帯域反射法により無負荷
Q(Qu)を測定した。
This mixture was dried and then placed in air for 1200 min.
After calcining at °C for 5 hours, it was wet-pulverized in the ball mill. After taking out the crushed slurry from the ball mill and drying it, it was formed into a disk with a diameter of 256 at a pressure of 700 kg/Cwi, which was then fired in air at a temperature within the range of 1460 to 136 d'C for 2 hours. Porcelain having the composition shown in the table was obtained. Then, a disk-shaped porcelain sample with dimensions of 5 mm in diameter and 2 mm in thickness was cut out from each piece of porcelain, and used in a dielectric resonator for microwaves, and the resonant frequency was measured by the Trutub method. This resonant frequency (approximately 11 GHz)
The dielectric constant ε was measured from the and the diameter, and the no-load Q (Qu) was measured using the band reflection method.

共振周波数の温度安定度γfは、温度槽に各試料を入れ
、−30゜Cから+ 700Cの温度変化におけるトラ
ツプ周波数の変化を測定して求めた。その結果を下表に
示す。表より明らかなように、本発明の誘電体磁器用材
料はマイクロ波領域において、無負荷Qが大きく、誘電
率が比較的大きく、さらに共振周波数の ・温度安定度
の改善された優れたものであることがわかる。
The temperature stability γf of the resonance frequency was determined by placing each sample in a temperature bath and measuring the change in trap frequency as the temperature changed from -30°C to +700C. The results are shown in the table below. As is clear from the table, the dielectric ceramic material of the present invention has a large no-load Q, a relatively large dielectric constant, and is excellent in resonance frequency and temperature stability in the microwave region. I understand that there is something.

本発明の範囲外の組成の試料6,7,8は、磁器への焼
結がよくなく、誘電体共振器として利用するに十分な機
械的強度をもつ磁器とならず、また、同じく試料12で
は無負荷Qが小さく、共振周波数の温度変化が大きいの
で、本発明の範囲から除いた。なお、本発明にかかる磁
器は、低周波領域においても誘電損失が小さく、かつ誘
電率の温度変化が小さいので、磁器コンデンサ用として
も優れた材料であることを確認した。
Samples 6, 7, and 8 with compositions outside the scope of the present invention did not sinter well into porcelain, and did not have sufficient mechanical strength to be used as a dielectric resonator. In this case, the no-load Q is small and the temperature change in the resonant frequency is large, so it is excluded from the scope of the present invention. Furthermore, it was confirmed that the porcelain according to the present invention has a small dielectric loss even in the low frequency range and a small temperature change in the dielectric constant, so it is an excellent material for ceramic capacitors.

Claims (1)

【特許請求の範囲】[Claims] 1 一般式(1−w)(xBaO・yZnO・zNb_
2O_5)+wCaO・ZrO_2で表わされる組成に
おいて、0.5≦X≦0.75,0.1≦y≦0.3,
0.1≦z≦0.3,x+y+z=1,0<w≦0.9
の範囲内にある組成であることを特徴とする誘電体共振
器用材料。
1 General formula (1-w) (xBaO・yZnO・zNb_
In the composition represented by 2O_5)+wCaO・ZrO_2, 0.5≦X≦0.75, 0.1≦y≦0.3,
0.1≦z≦0.3, x+y+z=1,0<w≦0.9
A dielectric resonator material characterized by having a composition within the range of .
JP52096602A 1977-08-11 1977-08-11 Materials for dielectric resonators Expired JPS5949649B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP52096602A JPS5949649B2 (en) 1977-08-11 1977-08-11 Materials for dielectric resonators

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP52096602A JPS5949649B2 (en) 1977-08-11 1977-08-11 Materials for dielectric resonators

Publications (2)

Publication Number Publication Date
JPS5430499A JPS5430499A (en) 1979-03-06
JPS5949649B2 true JPS5949649B2 (en) 1984-12-04

Family

ID=14169414

Family Applications (1)

Application Number Title Priority Date Filing Date
JP52096602A Expired JPS5949649B2 (en) 1977-08-11 1977-08-11 Materials for dielectric resonators

Country Status (1)

Country Link
JP (1) JPS5949649B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61169053U (en) * 1985-04-10 1986-10-20
JPS63160983U (en) * 1987-04-08 1988-10-20
JPH0411981Y2 (en) * 1986-02-14 1992-03-24

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5085540A (en) * 1973-12-03 1975-07-10

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5085540A (en) * 1973-12-03 1975-07-10

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61169053U (en) * 1985-04-10 1986-10-20
JPH0411981Y2 (en) * 1986-02-14 1992-03-24
JPS63160983U (en) * 1987-04-08 1988-10-20

Also Published As

Publication number Publication date
JPS5430499A (en) 1979-03-06

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