JPS5851406A - High frequency dielectric porcelain composition - Google Patents

High frequency dielectric porcelain composition

Info

Publication number
JPS5851406A
JPS5851406A JP56150078A JP15007881A JPS5851406A JP S5851406 A JPS5851406 A JP S5851406A JP 56150078 A JP56150078 A JP 56150078A JP 15007881 A JP15007881 A JP 15007881A JP S5851406 A JPS5851406 A JP S5851406A
Authority
JP
Japan
Prior art keywords
dielectric constant
weight
high frequency
frequency dielectric
frequency
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
JP56150078A
Other languages
Japanese (ja)
Other versions
JPS6113326B2 (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 JP56150078A priority Critical patent/JPS5851406A/en
Publication of JPS5851406A publication Critical patent/JPS5851406A/en
Publication of JPS6113326B2 publication Critical patent/JPS6113326B2/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1へQ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 Q value of 1.

最近数1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)を取プ扱う高周波回路の技術
の進展に俸なり1回路の小形化が図かられている。
Recent advances in technology for high-frequency circuits that handle wavelengths of less than 1, ie, microwaves and millimeter waves (hereinafter collectively referred to as microwaves), have led to miniaturization of circuits.

この高周波回路には従来よシ空胴共振器、アンテナなど
が使用されているが、これらはマイクロ波の波長と同程
度の大きさになる丸め、小形化への障害となってiQた
。この問題を解決する丸めK。
Conventionally, cavity resonators, antennas, etc. have been used in this high-frequency circuit, but these have become an obstacle to rounding and downsizing to the same size as the microwave wavelength. Rounding K solves this problem.

波長そのものを短縮するという方法が考えられ”Cき九
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。
One possible method is to shorten the wavelength itself, but one way to achieve this is to use dielectric ceramics.

このよう逐材料としてはTlO2系のものがよく使用さ
れており、たとえばCaTl0.−MtTiO,−La
、O,、−2,TiO,、Ba0−Tie、などの誘電
体磁器で共振器が構成されてIQ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、高覧へq値を有
すること、誘電率の温度変化特性が安定してζ^ること
などをすべて満足させ得る十分な結果が得られ°C1へ
なIn。
As such materials, TlO2-based materials are often used, such as CaTl0. -MtTiO, -La
, O, , -2, TiO, , Ba0-Tie, etc., the resonator is constructed with IQ. However, these materials do not meet the characteristics required when used in microwaves, such as having a high dielectric constant, having a high q value, and having a stable temperature change characteristic of the dielectric constant. Sufficient results were obtained to satisfy all the conditions.

このような要求に答えるために、 Tie、 −flr
og−8nO,を生成分とし、 ZnO,Co、O,ま
たはZnQ。
To answer such requests, Tie, -flr
og-8nO, as the product, ZnO, Co, O, or ZnQ.

NiOを添加含有させたものが提案された。しかしNP
O(誘電率の温度変化率がotsであるとj^う意味)
 ”t” 70HM f)周波数におけるq値が6oo
α7000とそれぞれ小さな値のものしか得られてぃ1
^し九がって、この発明は上述し九従来の欠点を解消し
、MPOKお(^て高いQ値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。
A material containing NiO was proposed. However, N.P.
O (meaning that the temperature change rate of dielectric constant is ots)
"t" 70HM f) q value at frequency is 6oo
α7000 and only small values were obtained.1
Therefore, it is an object of the present invention to eliminate the above-mentioned nine conventional drawbacks and to provide a dielectric ceramic composition for high frequency use that has MPOK and a high Q value.

またこの発明は高覧へ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弯化させることに、より、
NPOを中心にし゛〔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, by making the composition ratio curved, this invention
The object of the present invention is to provide a dielectric ceramic composition for high frequency use having an arbitrary dielectric constant and temperature change rate, mainly based on NPO.

すなわち、この発明の要旨とするところは、’f’ 1
0122〜45重量(4,Zr0,38〜58重量e4
.5nO19〜26重量−を主成分とし、これ[ZnO
を7重量−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 'f' 1
0122~45 weight (4, Zr0, 38~58 weight e4
.. The main component is 5nO19-26% by weight, and this [ZnO
It contains up to 7 parts by weight of Ta, O, and up to 5 parts by weight.

上記した組成範囲に限定した理由は次のとおシである。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(ξ)
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。tたZr01が3
8重量−未満になシ、ある亀へは58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ぎ
る。また8nO,が9重量−未満では誘電率の温度係数
(TC)がプラス側で大きくな抄すざるとともに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゛大きくなりすぎる。
That is, when Tie is less than 22wt, the dielectric constant (ξ)
decreases and exceeds 43% by weight, the temperature coefficient of dielectric constant (T
C) becomes too large on the plus side. t Zr01 is 3
It should not be less than 8% by weight, but for some turtles, if it exceeds 58% by weight, the temperature coefficient (TC) of the dielectric constant is too large on the plus side. Furthermore, when 8nO is less than 9% by weight, the temperature coefficient of permittivity (TC) is on the positive side, and the Q decreases with a large reduction, and when it exceeds 26% by weight, the temperature coefficient of permittivity (TC)
becomes too large on the negative side.

次に添加物のうちZnOが7重量優を越えると誘電率、
Qが低下し* 17jTa20.が5重量−を越えると
Qが低下する一41K”tOs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 ZnO among the additives exceeds 7% by weight, the dielectric constant
Q decreases * 17jTa20. If the value exceeds 5wt, Q decreases.41K"tOs has the function of making the crystal growth uniform, so it suppresses the increase in lattice misalignment within the crystal,
As a result, it has the effect of improving Q.

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,、8nO1,
ZrxO9τa、Osを用1八、第1表の組成比率の磁
器が得られるように秤量し、16時時間式混合しな。次
論で脱水、乾燥し、得られ先混合原料を2500#/d
の圧力で直径12−1厚み61mの円板に成形した。引
きつづき成形物を自然雰囲気中1560℃の温度で3時
間焼成して磁器試料を得た。
High purity Tie, ZrO, 8nO1, as a raw material
ZrxO9τa, Os was weighed to obtain porcelain having the composition ratio shown in Table 1, and mixed for 16 hours. In the next step, dehydrate and dry the resulting mixed raw material at 2500#/d.
It was molded into a disk with a diameter of 12-1 and a thickness of 61 m at a pressure of . Subsequently, the molded product was fired in a natural atmosphere at a temperature of 1560° C. for 3 hours to obtain a porcelain sample.

各磁器試料にり層て25r:、70HHにおける誘電率
(番 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表に表わし喪。
The electrical properties of the dielectric constant (Q) and temperature coefficient (TC) of the resonant frequency at 25R and 70HH were measured for each porcelain sample, and the results are shown in Table 1.

第1表中察印はこの発明範囲外のものであ如。The seals 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.

また第1表中には参考例として、  Tie、 −Zr
Ol−8nO,の主成分に、 ZnO,NiOまたはZ
nO。
Also, in Table 1, as reference examples, Tie, -Zr
The main components of Ol-8nO, ZnO, NiO or Z
nO.

Co、Os を添加したものにり(^て同様に電気的特
性を測定し、その結果も示した。     、第1表の
誘電率<1)とqの値は誘電体共振法により測定し丸も
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、#J定は+25C〜+85′Cの温
度範囲で測定した。
The electrical properties were similarly measured and the results are also shown for the materials doped with Co and Os. The dielectric constant <1 in Table 1 and the value of q were measured by the dielectric resonance method. It is something. Further, TC represents the temperature change rate of the resonance frequency (fo), and #J constant was measured in the temperature range of +25C to +85'C.

共振周波数(fo)の温1度変化率〔TC(fo)〕は
次式より求めたもので、誘電率(g)の温度変化率(T
C(t)〕と温度変化による磁器の線膨張率(ff)と
からなって−^る。   TC(fo)=−%TC(@
)−aまた。試料番号13と参考例1につ(へて結晶粒
径および抗折強度を測定したところ、試料番号13のも
のは結晶粒径5〜10μm、抗折強度1200に/d、
参考例1のものは結晶粒径10〜30μm。
The temperature change rate of the resonant frequency (fo) [TC(fo)] is calculated from the following formula, and the temperature change rate of the dielectric constant (g) (T
C(t)] and the linear expansion coefficient (ff) of porcelain due to temperature change. TC(fo)=-%TC(@
)-a again. When we measured the crystal grain size and bending strength of sample number 13 and reference example 1, sample number 13 had a crystal grain size of 5 to 10 μm, a bending strength of 1200/d,
The crystal grain size of Reference Example 1 was 10 to 30 μm.

抗折強度900KI/dであり、 Ta1O1を含有さ
せることによって結晶粒径が小さく1強度の太き−へ磁
器が得られる。
It has a bending strength of 900 KI/d, and by containing Ta1O1, a thick porcelain with a small crystal grain size and a strength of 1 can be obtained.

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のときにお鬼^て、
従来公知の組成のものにくらべて誘電率が高<、Qの大
きな値のものが得られて亀^る。
As is clear from the above embodiments, according to the present invention,
When the temperature coefficient (TC) of the resonant frequency is 0,
Compared to conventionally known compositions, a material with a higher dielectric constant and a larger value of Q can be obtained.

また組成比率を変えることによりypoを中心にし゛C
任意の共振周波数の温度係数(TC)が得られて論るた
め、高周波回路に組み込んだとき他の電子部品との温度
補償作用を持九せることかできる。
In addition, by changing the composition ratio, ypo is the main
Since the temperature coefficient (TC) of any resonant frequency can be obtained, it is possible to have a temperature compensation effect with other electronic components when incorporated into a high frequency circuit.

したがって、高周波領域で使用する誘電体共振器やアン
テナ、ある(^は基板などに有用な高周波用誘電体磁自
組成物を提供することができる。
Therefore, it is possible to provide a high-frequency dielectric magnetic composition useful for dielectric resonators, antennas, substrates, etc. used in high-frequency regions.

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】[Claims] Tie、22〜45重量%−zrOt38〜58重i1
%、8nO1? −26Jit*を主成分とし、j#L
&cZn*1量%以丁、 Ta、O,を5重量−以下添
加含有し°Cなる高周波用誘電体磁器組成物7
Tie, 22-45 wt%-zrOt38-58 wt i1
%, 8nO1? −26Jit* as the main component, j#L
High-frequency dielectric ceramic composition 7 containing Zn*1% by weight or less, Ta, O, added at 5% by weight or less at °C
JP56150078A 1981-09-22 1981-09-22 High frequency dielectric porcelain composition Granted JPS5851406A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56150078A JPS5851406A (en) 1981-09-22 1981-09-22 High frequency dielectric porcelain composition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56150078A JPS5851406A (en) 1981-09-22 1981-09-22 High frequency dielectric porcelain composition

Publications (2)

Publication Number Publication Date
JPS5851406A true JPS5851406A (en) 1983-03-26
JPS6113326B2 JPS6113326B2 (en) 1986-04-12

Family

ID=15489030

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56150078A Granted JPS5851406A (en) 1981-09-22 1981-09-22 High frequency dielectric porcelain composition

Country Status (1)

Country Link
JP (1) JPS5851406A (en)

Cited By (2)

* 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
JPH0233421U (en) * 1988-08-24 1990-03-02

Cited By (2)

* 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
JPH0233421U (en) * 1988-08-24 1990-03-02

Also Published As

Publication number Publication date
JPS6113326B2 (en) 1986-04-12

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