JPS6229010A - Dielectric ceramic composition for high frequency - Google Patents

Dielectric ceramic composition for high frequency

Info

Publication number
JPS6229010A
JPS6229010A JP60167954A JP16795485A JPS6229010A JP S6229010 A JPS6229010 A JP S6229010A JP 60167954 A JP60167954 A JP 60167954A JP 16795485 A JP16795485 A JP 16795485A JP S6229010 A JPS6229010 A JP S6229010A
Authority
JP
Japan
Prior art keywords
weight
dielectric
high frequency
ceramic composition
dielectric ceramic
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
JP60167954A
Other languages
Japanese (ja)
Other versions
JPH056764B2 (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 JP60167954A priority Critical patent/JPS6229010A/en
Priority to US06/861,239 priority patent/US4665041A/en
Priority to DE19863615785 priority patent/DE3615785A1/en
Priority to FR868606762A priority patent/FR2581639B1/en
Publication of JPS6229010A publication Critical patent/JPS6229010A/en
Publication of JPH056764B2 publication Critical patent/JPH056764B2/ja
Granted legal-status Critical Current

Links

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】 〔産業上の利用分野〕 この発明は、マイクロ波やミリ波等の高周波領域におい
て高誘電率で高いQ値を有する高周波用誘電体磁器組成
物に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a high frequency dielectric ceramic composition having a high dielectric constant and a high Q value in a high frequency region such as microwaves and millimeter waves.

〔従来の技術〕[Conventional technology]

マイクロ波やミリ波等の高周波領域において、誘電体磁
器は誘電体共振器やMrC用誘電体基板等に広く利用さ
れている。
In high frequency regions such as microwaves and millimeter waves, dielectric ceramics are widely used for dielectric resonators, dielectric substrates for MrC, and the like.

従来、この種の誘電体磁器として例えばT i Oz−
ZrOz −5nOz −ZnO−NiO系の材料が知
られている(特公昭55−34526号公報)。
Conventionally, as this type of dielectric porcelain, for example, T i Oz-
ZrOz -5nOz -ZnO-NiO based materials are known (Japanese Patent Publication No. 34526/1983).

しかしながら上記材料のQ値は、IGHzで25000
.4GHzで12000.7GHzで7000のレベル
であった。そのため、例えば低い周波数(例えば800
MHz)でハイパワーの回路の誘電体共振器等に使用し
ようとしても、発熱が大きくて温度不安定となって使用
することはできない。また、4GHzや10GHz近辺
の誘電体共振器としてもQ値が低くて使用することがで
きない場合がある。
However, the Q value of the above material is 25000 at IGHz.
.. The level was 12000 at 4GHz and 7000 at 7GHz. Therefore, for example low frequencies (e.g. 800
Even if an attempt is made to use it as a dielectric resonator in a high-power circuit (MHz), it generates a large amount of heat and becomes unstable in temperature, making it unusable. Furthermore, there are cases where the Q value is so low that it cannot be used as a dielectric resonator near 4 GHz or 10 GHz.

そコテ、Ti1t −ZrOz  Snug −ZnO
−N f O糸材料(DZnOまたはNi0(7)代わ
りにTazO。
So, Ti1t -ZrOz Snug -ZnO
-NfO yarn material (TazO instead of DZnO or NiO(7)).

を添加することによってQ値の改善を図った高周波用誘
電体磁器組成物が、特開昭58−51406号公報及び
特開昭58−217465号公報にそれぞれ提案されて
いる。前者における誘電体磁器組成物は、TfOz 2
2〜43 N!−%、Zr0゜38〜58重量%、Sn
0,9〜26重量%を主成分としてこれにZnOを7重
量%以下、Ta、O。
High-frequency dielectric ceramic compositions in which the Q value is improved by adding are proposed in JP-A-58-51406 and JP-A-58-217465, respectively. The dielectric ceramic composition in the former is TfOz 2
2~43 N! -%, Zr0゜38~58wt%, Sn
The main component is 0.9 to 26% by weight, and 7% by weight or less of ZnO, Ta, and O.

を5重量%以下添加したものであり、後者のそれは、前
者のZnoO代わりにNiOを10重量%以下添加した
ものである。
In the latter case, 10% by weight or less of NiO was added instead of ZnoO in the former.

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

上記公報開示の材料においては、Q値は改善されるもの
のそれでも7GHzにおいて最大の値が8000程度止
まりである。また焼結性に更に改善の余地がある。
In the material disclosed in the above publication, although the Q value is improved, the maximum value is still only about 8000 at 7 GHz. There is also room for further improvement in sinterability.

したがってこの発明は、更にQ値及び焼結性の改善を図
っ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 dielectric ceramic composition for high frequency use that further improves the Q value and sinterability.

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

この発明の高周波用誘電体磁器組成物は、TiO,22
〜43重量%、Zr0g 38〜58重量%、5nOt
9〜26重量%を主成分とし、これにZnOを7重量%
以下、NiOを10重量%以下、Sb*Osを7重量%
以下添加含有してなるもの、  である。
The dielectric ceramic composition for high frequency of this invention is TiO, 22
~43% by weight, Zr0g 38-58% by weight, 5nOt
The main component is 9 to 26% by weight, and 7% by weight of ZnO.
Below, NiO is 10% by weight or less, Sb*Os is 7% by weight.
The following additives are included.

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.

即ち、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(TC)
が+側で大きくなり過ぎる。
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 (TC) decreases.
becomes too large on the + side.

またZrO,が38重量%未満になり、あるいは58重
量%を越えると誘電率の温度係数(TC)が+側で大き
くなり過ぎる。またSnugが9重量%未満では誘電率
′)一度係数(To)が1側で大きくなり過ぎると共に
Qが低下し、26重量%を越えると誘電率の温度係数(
TC)が−側で大きくなり過ぎる。
Further, when ZrO is less than 38% by weight or exceeds 58% by weight, the temperature coefficient (TC) of the dielectric constant becomes too large on the + side. Furthermore, when Snug is less than 9% by weight, the coefficient (To) of the dielectric constant becomes too large on the 1 side and the Q decreases, and when it exceeds 26% by weight, the temperature coefficient of the dielectric constant (To)
TC) becomes too large on the - side.

次に添加物の内、ZnOが7重量%を越えると誘電率及
びQが低下し、NiOが10重重篤を越える、あるいは
s b、 o 、が7重量%を越えるとQが低下し、い
ずれも実用に供さなくなる。
Next, among the additives, when ZnO exceeds 7% by weight, the dielectric constant and Q decrease, and when NiO exceeds 10% by weight or s b, o exceeds 7% by weight, Q decreases. will no longer be of practical use.

〔実施例〕〔Example〕

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Ti0z 、ZrO2、SnO2、
Zn0SNips 5bzOsを用い、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、得られた混合原料を2500
 Kg 7cm”の圧力で直径12mm、厚み6a+n
+の円板に成形した。引続き成形物を自然雰囲気中13
50〜1450℃の温度で4時間焼成して磁器試料を得
た。
High purity TiOz, ZrO2, SnO2,
Zn0SNips 5bzOs was weighed and mixed for 16 hours to obtain porcelain having the composition ratio shown in Table 1. Next, the mixed raw material obtained by dehydration and drying was heated to 2500
Kg 7cm” pressure, diameter 12mm, thickness 6a+n
It was molded into a + disc. Continue molding in natural atmosphere 13
Porcelain samples were obtained by firing at a temperature of 50-1450°C for 4 hours.

各磁器試料について25℃、7GHzにおける誘電率(
ε)、Q及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表に表した。
Dielectric constant (at 25℃, 7GHz) for each ceramic sample
ε), Q, and temperature coefficient (TC) of resonance frequency were measured, and the results are shown in Table 1.

第1表中*印はこの発明の範囲外のものであり、それ以
外は全てこの発明の範囲内のものである。
Items marked with * in Table 1 are outside the scope of this invention, and all others are within the scope of this invention.

(以下余白) 第1表の誘電率(ε)とQの値は誘電体共振法により測
定したものである。またTCは共振周波数(fo)の温
度変化率を表したもので、測定は+25℃〜+85℃の
温度範囲で測定した。
(Left space below) The dielectric constant (ε) and Q values in Table 1 were measured by the dielectric resonance method. Further, TC represents the temperature change rate of the resonance frequency (fo), and the measurement was performed in a temperature range of +25°C to +85°C.

共振周波数(fo)の温度変化率[TC(f。Temperature change rate of resonant frequency (fo) [TC(f.

)]は次式より求めたもので、誘電率(ε)の温度変化
率(TC(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。
)] is obtained from the following formula, which is the temperature change rate (TC(ε)) of the dielectric constant (ε) and the coefficient of linear expansion of porcelain due to temperature change (α
).

TC(fo )=’ATC(ε)−α また、試料番号16について結晶粒径及び抗折強度を測
定したところ、結晶粒径5〜lOμm、抗折強度120
0 Kg 7cm2であり、5bzOsを含有させるこ
とによって結晶粒径が小さく、強度の大きい磁器が得ら
れている。
TC(fo)='ATC(ε)-α In addition, when the crystal grain size and bending strength were measured for sample number 16, the crystal grain size was 5 to 10 μm, and the bending strength was 120 μm.
0 Kg 7 cm2, and by containing 5bzOs, a porcelain with small crystal grain size and high strength is obtained.

尚、試料番号7.14.23につい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 it was impossible to sinter sample number 7.14.23, the electrical characteristics were not measured.

比較のために、この発明にかかる試料番号16のものと
、従来例のTie、−ZrO2−3nOw−ZnO−N
jO系のものについて、Qと周波数との関係を図面に示
した。
For comparison, sample number 16 according to the present invention and conventional example Tie, -ZrO2-3nOw-ZnO-N
The relationship between Q and frequency for the jO system is shown in the drawing.

なお、Ti0z −ZrO2−3nO,−ZnO−Nj
O系の組成は次のものからなる。Ti0z:38重量%
、Zr0z  : 48重量%、5nOz:14重量%
からなる主成分に、ZnO:1.0重量%、NjO:0
.5重量%加えたもの。
In addition, Ti0z -ZrO2-3nO, -ZnO-Nj
The O-based composition consists of the following: Ti0z: 38% by weight
, Zr0z: 48% by weight, 5nOz: 14% by weight
The main components are ZnO: 1.0% by weight, NjO: 0
.. Added 5% by weight.

図から明らかなように、この発明によるものは低い周波
数になるほどQの改善効果が大きい。
As is clear from the figure, in the device according to the present invention, the lower the frequency, the greater the effect of improving Q.

〔発明の効果〕〔Effect of the invention〕

上述した実施例から明らかなようにこの発明においては
、添加物をZnON1O−3bzOsの3成分とするこ
とにより、焼結性は安定し、かつ高Qのものが得られた
。例えばQ値は、7 G H2%TC#Oで8700と
、従来にない大きな値が得られた。
As is clear from the examples described above, in this invention, by using the three components of ZnON1O-3bzOs as additives, a product with stable sinterability and high Q was obtained. For example, the Q value of 7 GH2% TC#O was 8700, which was an unprecedentedly large value.

つまりこの発明の材料においては、結晶粒子が従来のも
のに比べて小さくかつ大きさが均一になっており、上記
添加物系は結晶成長を均一に、かつ結晶内の格子不整の
生成を抑制する効果を持っている。
In other words, in the material of this invention, the crystal grains are smaller and more uniform in size than in conventional materials, and the additive system described above makes crystal growth uniform and suppresses the formation of lattice misalignment within the crystal. It has an effect.

またこの発明の材料では、低い周波数になるほどQの改
善効果が大きい。これは、低い周波数になるほどユニッ
トが大型になるが、上記添加物系によって焼結性が改善
されて大型ユニットも均一に焼結したためである。例え
ば、この発明の材料のQ値は、IGHzで38000.
4GHzで16000.7GHzで8700となってお
り、これは上述した従来のTiO□−ZrOz−3nO
□−ZnO−NiO系材料のQ値に比べて、それぞれの
周波数において52%増、33%増及び24%増となっ
ている。
Furthermore, with the material of the present invention, the lower the frequency, the greater the effect of improving Q. This is because the lower the frequency, the larger the unit, but the additive system improved the sinterability and even the large unit was sintered uniformly. For example, the Q value of the material of this invention is 38000.
It is 16000 at 4GHz and 8700 at 7GHz, which is higher than the conventional TiO□-ZrOz-3nO mentioned above.
Compared to the Q value of the □-ZnO-NiO-based material, the Q values are increased by 52%, 33%, and 24% at each frequency.

それゆえこの発明によれば、例えば自動車電話の基地局
チャンネルフィルタ用誘電体共振器等の低周波数(例え
ば800MHz)で高パワーの分野への用途が拡大する
。また、4GHz、10GHzの衛星放送用誘電体共振
器等の高い周波数領域においても、これまでの超高Q材
に比べればQは小さいものの、誘電率(ε)が約38と
大きいため、これまで使用できなかった分野への用途の
拡大も期待できる。
Therefore, according to the present invention, the application can be expanded to the field of low frequency (for example, 800 MHz) and high power, such as dielectric resonators for base station channel filters of mobile telephones. In addition, even in high frequency ranges such as dielectric resonators for satellite broadcasting at 4 GHz and 10 GHz, although the Q is lower than that of conventional ultra-high Q materials, the dielectric constant (ε) is large at approximately 38, so It is also expected that the application will expand to areas where it could not be used.

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

図面は、この発明の実施例にかかる材料(試料番号16
)と、従来例のTiO2−ZrO!−3nOz−ZnO
−NiO系材料のQと周波数の関係を示す図である。
The drawings show material (sample number 16) according to the embodiment of this invention.
) and the conventional TiO2-ZrO! -3nOz-ZnO
FIG. 3 is a diagram showing the relationship between Q and frequency of -NiO-based materials.

Claims (1)

【特許請求の範囲】[Claims] (1)TiO_222〜43重量%、ZrO_238〜
58重量%、SnO_29〜26重量%を主成分とし、
これにZnOを7重量%以下、NiOを10重量%以下
、Sb_2O_5を7重量%以下添加含有してなる高周
波用誘電体磁器組成物。
(1) TiO_222~43% by weight, ZrO_238~
58% by weight, SnO_29-26% by weight as the main component,
A high-frequency dielectric ceramic composition containing ZnO in an amount of 7% by weight or less, NiO in an amount of 10% by weight or less, and Sb_2O_5 in an amount of 7% by weight or less.
JP60167954A 1985-05-10 1985-07-29 Dielectric ceramic composition for high frequency Granted JPS6229010A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP60167954A JPS6229010A (en) 1985-07-29 1985-07-29 Dielectric ceramic composition for high frequency
US06/861,239 US4665041A (en) 1985-05-10 1986-05-08 Dielectric ceramic composition for high frequencies
DE19863615785 DE3615785A1 (en) 1985-05-10 1986-05-10 DIELECTRIC CERAMIC COMPOSITION FOR HIGH FREQUENCIES
FR868606762A FR2581639B1 (en) 1985-05-10 1986-05-12 HIGH FREQUENCY DIELECTRIC CERAMIC COMPOSITION

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60167954A JPS6229010A (en) 1985-07-29 1985-07-29 Dielectric ceramic composition for high frequency

Publications (2)

Publication Number Publication Date
JPS6229010A true JPS6229010A (en) 1987-02-07
JPH056764B2 JPH056764B2 (en) 1993-01-27

Family

ID=15859122

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60167954A Granted JPS6229010A (en) 1985-05-10 1985-07-29 Dielectric ceramic composition for high frequency

Country Status (1)

Country Link
JP (1) JPS6229010A (en)

Also Published As

Publication number Publication date
JPH056764B2 (en) 1993-01-27

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