JPS58217465A - High frequency dielectric ceramic composition - Google Patents

High frequency dielectric ceramic composition

Info

Publication number
JPS58217465A
JPS58217465A JP57098876A JP9887682A JPS58217465A JP S58217465 A JPS58217465 A JP S58217465A JP 57098876 A JP57098876 A JP 57098876A JP 9887682 A JP9887682 A JP 9887682A JP S58217465 A JPS58217465 A JP S58217465A
Authority
JP
Japan
Prior art keywords
high frequency
ceramic composition
dielectric ceramic
weight
dielectric constant
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
JP57098876A
Other languages
Japanese (ja)
Other versions
JPS6259076B2 (en
Inventor
之雄 樋口
勝部 正嘉
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing 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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP57098876A priority Critical patent/JPS58217465A/en
Publication of JPS58217465A publication Critical patent/JPS58217465A/en
Publication of JPS6259076B2 publication Critical patent/JPS6259076B2/ja
Granted legal-status Critical Current

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Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 この発明は高誘電率で高10Q値を有する高周波用誘電
体磁器組成物に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high frequency dielectric ceramic composition having a high dielectric constant and a high 10Q value.

最近数鴬以下の波長、すなわちマイクロ波、ミリ波(以
下マイクロ波と総称する)を取り扱う高周波回路の技術
の進展に伴な(へ、回路の小形化が図かられCいる。
Recently, with the advancement of technology for high-frequency circuits that handle wavelengths less than a few digits, that is, microwaves and millimeter waves (hereinafter collectively referred to as microwaves), efforts have been made to miniaturize circuits.

この高周波回路には従来より空洞共1凱アンテナなどが
使用されて竜へるが、これらはマイクロ波の波長と同程
度の大きさし・こなるため、小形化への障害となって(
^た。この問題を解決するために。
Conventionally, this high-frequency circuit uses single-cavity antennas, but since these antennas are about the same size as the microwave wavelength, they are an obstacle to miniaturization (
^Ta. to solve this problem.

波長そのもあを短縮すると(へう方法が考えられ・Cき
たが、これを実現するには誘電体磁器を使用する方法が
ある。
A method has been considered to shorten the wavelength itself, but one way to achieve this is to use dielectric ceramics.

このような材料とし°CはTiO2系のものがよく使用
されCおシ、たとえばCaTi0.−MgTiO,−L
a、0j−2TiO,、、、BaO−TiO2などの誘
電体磁器で共振器が構成され”で1へる。しかしながら
、これらの材料ではマイクロ波で使用するときに要求さ
れる特性、すなわち、高誘電率であること、高−へQ値
を有すること、誘電率の温度変化特性が安定し°CLn
ることなどをすべ゛C満足させ得る十分な結果が得られ
゛〔層ない。
For such materials, TiO2-based materials are often used, such as CaTi0. -MgTiO, -L
The resonator is constructed of dielectric ceramics such as a, 0j-2TiO, ..., BaO-TiO2. However, these materials do not have the characteristics required when used in microwaves, that is, It has a high dielectric constant, a high Q value, and the temperature change characteristics of the dielectric constant are stable °CLn
However, it is not possible to obtain sufficient results to satisfy all of the above requirements.

したがって、この発明は上述した従来の欠点を解消した
高周波用誘電体磁器組成物を提°供することを目的とす
る。
Therefore, it is an object of the present invention to provide a high frequency dielectric ceramic composition that eliminates the above-mentioned conventional drawbacks.

またこの発明は高い誘電率を有する高周波用誘電体磁器
組成物を提供することを目的とする。
Another object of the present invention is to provide a high frequency dielectric ceramic composition having a high dielectric constant.

さらにこの発明は組成比率を変化させることたより、H
POを中心11CL、−C任意の誘電率の温度変化率を
有する高周波用誘電体磁器組成物を提供することを目的
とする。
Furthermore, since this invention changes the composition ratio, H
It is an object of the present invention to provide a high frequency dielectric ceramic composition having a dielectric constant of PO, 11CL, -C and an arbitrary temperature change rate.

すなわち、この発明の要旨とするところは、T”h22
〜43重量%、zr0238〜58重量4、SnO!9
〜26重量%を主成分とし、これにNiOを10i量チ
以下、 Ta、O,を5重量%以下含有してなるもので
ある。
That is, the gist of this invention is that T"h22
~43wt%, zr0238~58wt4, SnO! 9
-26% by weight as a main component, and further contains NiO in an amount of 10i or less, and Ta, O, in an amount of 5% by weight or less.

上記した組成範囲に限定した理由は次のとおりである。The reason for limiting the composition to the above composition range is as follows.

すなわち、Tie、が22重量%未満では誘電率(ε)
が低下し、43重量%を越えると誘電率の温度係数(T
C)がプラス側で大きくなりすぎる。
That is, when Tie is less than 22% by weight, the dielectric constant (ε)
decreases, and when it exceeds 43% by weight, the temperature coefficient of dielectric constant (T
C) becomes too large on the plus side.

またZrO,が38重tts未満になり、ある覧へは5
8重量%を越えると誘電率の温度係数(TC)がプラス
側で大きくなシすざる。またSnO,が9重量%未満で
は誘電率の温度係数(TO)がプラス側で大きくなりす
ぎるとともにQが低下し、26重量%を越えると誘電率
の温度係数(TC)がマイナス側で犬きくなシすぎる。
Also, ZrO, becomes less than 38 times tts, and in some cases 5
If it exceeds 8% by weight, the temperature coefficient (TC) of the dielectric constant becomes large on the positive side. Furthermore, if SnO is less than 9% by weight, the temperature coefficient of dielectric constant (TO) becomes too large on the positive side and Q decreases, and if it exceeds 26% by weight, the temperature coefficient of dielectric constant (TC) becomes too large on the negative side. That's too much.

次に添加物のうちNiOが10重量%を越えるとQが低
下し、またTa、O,が5重量%を越えるとQが低下す
る。特にTa、O,は結晶成長を均一にさせる働きがあ
るため、結晶内の格子不整の増加を抑制し、その結果Q
を改善する効果を有する。
Next, when NiO among the additives exceeds 10% by weight, Q decreases, and when Ta, O, exceeds 5% by weight, Q decreases. In particular, Ta, O, have the function of making crystal growth uniform, so they suppress the increase in lattice misalignment within the crystal, resulting in Q
It has the effect of improving.

以下、この発明を実施例に従って詳述する。Hereinafter, this invention will be explained in detail according to examples.

原料として高純度のTie、、ZrO!、SnO,、N
iO,Ta、05を用IQ、第1表の組成比率の磁器が
得られるように秤量し、16時時間式混合した、次いで
脱水、乾燥し、得られた混食原料を250011.F/
dの圧力で直径1211厚み61EIの円板に成形した
。引きつづき成形物を自′然算囲気中1560t−の温
度で6時間焼成し・C磁器試料を得た。
High purity Tie, ZrO as a raw material! ,SnO,,N
iO, Ta, 05 were weighed to obtain porcelain with the composition ratio shown in Table 1, and mixed for 16 hours, then dehydrated and dried. F/
It was molded into a disk with a diameter of 1211 and a thickness of 61 EI under a pressure of d. Subsequently, the molded product was fired for 6 hours at a temperature of 1560 tons in a natural atmosphere to obtain a C porcelain sample.

各磁器試料につ覧へr25t”、7GI(zにおける誘
電率(ε)、Q、および共振周波数の温度係数(TC)
の各電気的特性を測定し、その結果を第1表に表わした
。
For each porcelain sample, the dielectric constant (ε) at 7GI (z), Q, and the temperature coefficient (TC) of the resonant frequency are listed.
The electrical characteristics of each were measured and the results are shown in Table 1.

第1表中※印はこの発明範囲外のものであり。Items marked with * in Table 1 are outside the scope of this invention.

それ以外はすべてこの発明範囲内のものである。Everything else is within the scope of this invention.

第   1   表 第1表の誘電率(ε)とQの値は誘電体共振法によシ測
定したものである。またTCは共振周波数(fo)の温
度変化率を表わしたもので、測定は+25℃〜+85℃
の温度範囲で測定した。
Table 1 The dielectric constant (ε) and Q values in Table 1 were measured by the dielectric resonance method. In addition, TC represents the temperature change rate of the resonant frequency (fo), and the measurement is from +25℃ to +85℃.
Measured over a temperature range of

共振周波数(f)の温度変化率(TC(fo))は次式
より求めたもので、誘電率(ε)の温度変化率(T(X
ε)〕と温度変化による磁器の線膨張率(α)とからな
っている。   TC(f )=J4’TC(t)−a
また、試料番号13につしへて結晶粒径および抗折強度
を測定したところ、結晶粒径5〜10μm。
The temperature change rate (TC(fo)) of the resonant frequency (f) was obtained from the following formula, and the temperature change rate (T(X) of the dielectric constant (ε))
ε)] and the coefficient of linear expansion of porcelain due to temperature change (α). TC(f)=J4'TC(t)-a
Further, when the crystal grain size and bending strength of sample number 13 were measured, the crystal grain size was 5 to 10 μm.

抗折強度1200JCF/dであり、 Ta、06を含
有させることによつ゛C結晶粒径が小さく1強度の大き
い磁器が得られて(八る。
It has a bending strength of 1200 JCF/d, and by containing Ta, 06, a porcelain with a small crystal grain size and a high strength can be obtained.

なお、試料番号4,10にり亀^ては焼結が不可能であ
ったため、電気的特性の測定は行わなかった。
Incidentally, since sintering was impossible for sample numbers 4 and 10, electrical characteristics were not measured.

上記した実施例から明らかなようにこの発明によれば、
共振周波数の温度係数(TC)が0のときにお1へて、
Qが7800もの大きな値のものが得られ′〔いる。ま
た組成比率を変えることによj5 NPOを中心にして
任意の共振周波数の温度係数(TC)が得られて蔦^る
ため、高周波回路に組込んだとき他の電子部品との温度
補償作用を持たせることができる。したがつ゛C1高周
波領域で使用する誘電体共振器やアンテナ、ある1へは
基板などに有用な高周波用誘電体磁器組成物を提供する
ことができる。
As is clear from the above embodiments, according to the present invention,
When the temperature coefficient (TC) of the resonant frequency is 0, it becomes 1,
One with a Q value as large as 7,800 was obtained. In addition, by changing the composition ratio, a temperature coefficient (TC) of an arbitrary resonance frequency can be obtained centering on j5 NPO, so when incorporated into a high frequency circuit, the temperature compensation effect with other electronic components can be improved. You can have it. Therefore, it is possible to provide a high frequency dielectric ceramic composition useful for dielectric resonators, antennas, substrates, etc. used in the C1 high frequency region.

特許出願人 株式会社村田製作所patent applicant Murata Manufacturing Co., Ltd.

Claims (1)

【特許請求の範囲】 T1(h 22〜452〜45重量%238〜58重量
膚。 8n0.9〜26重量%を主成分とし、これにNiOを
10重、11以下、 Ta2O,を5重畳係以下添加含
有してなる高周波用誘電体磁器組成物。
[Claims] T1 (h 22-452-45% by weight 238-58% by weight. 8n0.9-26% by weight as the main component, with 10 times NiO, 11 or less times, and 5 times Ta2O). A high frequency dielectric ceramic composition comprising the following additives.
JP57098876A 1982-06-08 1982-06-08 High frequency dielectric ceramic composition Granted JPS58217465A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57098876A JPS58217465A (en) 1982-06-08 1982-06-08 High frequency dielectric ceramic composition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57098876A JPS58217465A (en) 1982-06-08 1982-06-08 High frequency dielectric ceramic composition

Publications (2)

Publication Number Publication Date
JPS58217465A true JPS58217465A (en) 1983-12-17
JPS6259076B2 JPS6259076B2 (en) 1987-12-09

Family

ID=14231369

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57098876A Granted JPS58217465A (en) 1982-06-08 1982-06-08 High frequency dielectric ceramic composition

Country Status (1)

Country Link
JP (1) JPS58217465A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3615785A1 (en) * 1985-05-10 1986-11-13 Murata Manufacturing Co., Ltd., Nagaokakyo, Kyoto DIELECTRIC CERAMIC COMPOSITION FOR HIGH FREQUENCIES
JPH02192460A (en) * 1988-06-20 1990-07-30 Sanyo Electric Co Ltd Dielectric porcelain composition for microwave
JPH0375268A (en) * 1989-08-11 1991-03-29 Sanyo Electric Co Ltd Production of dielectric ceramic composition for microwave

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3615785A1 (en) * 1985-05-10 1986-11-13 Murata Manufacturing Co., Ltd., Nagaokakyo, Kyoto DIELECTRIC CERAMIC COMPOSITION FOR HIGH FREQUENCIES
JPH02192460A (en) * 1988-06-20 1990-07-30 Sanyo Electric Co Ltd Dielectric porcelain composition for microwave
JPH0375268A (en) * 1989-08-11 1991-03-29 Sanyo Electric Co Ltd Production of dielectric ceramic composition for microwave

Also Published As

Publication number Publication date
JPS6259076B2 (en) 1987-12-09

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