JPS5884179A - Microwave dielectric ceramic composition - Google Patents

Microwave dielectric ceramic composition

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Publication number
JPS5884179A
JPS5884179A JP56181488A JP18148881A JPS5884179A JP S5884179 A JPS5884179 A JP S5884179A JP 56181488 A JP56181488 A JP 56181488A JP 18148881 A JP18148881 A JP 18148881A JP S5884179 A JPS5884179 A JP S5884179A
Authority
JP
Japan
Prior art keywords
composition
dielectric
dielectric ceramic
ceramic composition
weight
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
JP56181488A
Other languages
Japanese (ja)
Other versions
JPS6410467B2 (en
Inventor
一明 遠藤
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.)
FDK Corp
Original Assignee
FDK Corp
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 FDK Corp filed Critical FDK Corp
Priority to JP56181488A priority Critical patent/JPS5884179A/en
Publication of JPS5884179A publication Critical patent/JPS5884179A/en
Publication of JPS6410467B2 publication Critical patent/JPS6410467B2/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】 本発明は、BaO−TiO2系の誘電体材料に、アンチ
モ゛ンまたはニオブの酸化物を少量添加することによっ
て、マイクロ波共振特性を大幅に向上させた誘電体磁器
組成物に関するものである。−周知のように、マイクロ
波立体回路素子の大きさは、通常使用される電磁波の波
長が基準となっている。誘電体を用いたマイクロ波回路
を伝播する電磁波の波長は、通常誘電体の誘電率をεと
し、真空中の波長をλ0とすると、λ0/ρ7となり、
誘電率εが大きいほど回路の小型化を図ることができる
。近年、マイクロ波やミリ波等の高周波領域での回路の
小型化に伴い、高誘電率、低損失、高安定性の誘電体材
料の開発が強く要望されている。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides a dielectric ceramic composition in which microwave resonance characteristics are significantly improved by adding a small amount of antimony or niobium oxide to a BaO-TiO2-based dielectric material. It is about things. - As is well known, the size of microwave three-dimensional circuit elements is based on the wavelength of electromagnetic waves normally used. The wavelength of electromagnetic waves propagating in a microwave circuit using a dielectric is usually λ0/ρ7, where the permittivity of the dielectric is ε and the wavelength in vacuum is λ0.
The larger the dielectric constant ε, the more compact the circuit can be. In recent years, with the miniaturization of circuits in high frequency regions such as microwaves and millimeter waves, there has been a strong demand for the development of dielectric materials with high dielectric constant, low loss, and high stability.

従来、BaO・nTiO2系誘電体材料は、高誘電率、
低損失で、共振周波数温度係数の小さい材料として誘電
体磁器組成物いられている。しかしながら、更に低い損
失と高い安定性が要求される場合には、従来のBaO・
n T i 02系誘電体材料では特性的に不十分であ
った。
Conventionally, BaO/nTiO2-based dielectric materials have a high dielectric constant,
Dielectric ceramic compositions are used as materials with low loss and a small resonant frequency temperature coefficient. However, when lower loss and higher stability are required, conventional BaO・
The nT i 02-based dielectric material had insufficient characteristics.

また、この系の材料で損失を低(・抑えようとすると、
焼成温度を1300〜+ aooCと高くするか、ホッ
トプレス焼成を行なわねばならないなど、展進は容易で
なかった。
In addition, if you try to reduce the loss with this type of material,
Progress was not easy, as the firing temperature had to be raised to 1300~+aooC or hot press firing had to be carried out.

本発明の目的は、従来のBaO・TlO2系誘電体材料
の特性を更に一層改善し、より低い損失とより高い安定
性を発現しうるようなマイクロ波用圧電磁器組成物を提
供することにある。
An object of the present invention is to provide a microwave piezoelectric ceramic composition that can further improve the properties of conventional BaO/TlO2-based dielectric materials and exhibit lower loss and higher stability. .

本発明は、fja O・TiO2系誘電体材料に対して
0.1〜0.7重量%の5b20aまたはNbaOaを
添加することによって、マイクロ波やミリ波等高周波領
域における電気的特性を著しく改善できることを知得し
、それに基づき完成されたものである。
The present invention provides that by adding 0.1 to 0.7% by weight of 5b20a or NbaOa to an fja O/TiO2-based dielectric material, electrical characteristics in high frequency ranges such as microwaves and millimeter waves can be significantly improved. It has been completed based on this knowledge.

以下、更に詳しく本発明について説明する。The present invention will be explained in more detail below.

ベースとなるHaO−Ti 02系誘電体材料の組成は
、酸化バリウム(Bad)が15〜25モル%に対し、
酸化チタン(Ti02)が75〜85モル係含まれ6組
成である。そして、本発明は、このベースとなるBaO
・n T i 02に対して、酸化アンチモン(Sb2
0a)または酸化ニオブ(Nb206)をOj〜0.7
重量%添付した組成物である。、 製°法的には、従来同様の粉末成形法であってよい。す
なわち、仮焼粉体に有機バインダーを加えて造粒し、所
定形状に加圧成形してから焼成すればよい一焼成温度は
、従来のものより、50〜100C低くてよい。焼成時
の雰囲気は大気中でもよいが、酸素中で行なえばより緻
密な磁器を得ることができる。
The composition of the base HaO-Ti 02 dielectric material is 15 to 25 mol% of barium oxide (Bad),
It contains 75 to 85 moles of titanium oxide (Ti02) and has a composition of 6. The present invention is based on this base BaO
・For n T i 02, antimony oxide (Sb2
0a) or niobium oxide (Nb206) from Oj to 0.7
% by weight of the composition. The manufacturing method may be a conventional powder molding method. That is, the calcination temperature, which is sufficient to add an organic binder to the calcined powder, granulate it, press-form it into a predetermined shape, and then sinter it, may be 50 to 100 C lower than that of the conventional one. The atmosphere during firing may be in the air, but a more dense porcelain can be obtained if the firing is performed in oxygen.

ベースとなるBaO−TiO2系誘電体材料の組成を、
BaO= 15〜25モル%、Ti 02= 75〜8
5モル%とした理由は、Ba0O量が25モル%を超え
るとQ (= 1 / tanδ)が低下し、またBa
0O量が15モル%未満ではQの低下は比較的少ないが
、温度係数が太き(なり実用に適さなくなるからである
。しかし、この系の組成物はBa0O量を約18.2モ
ル%、TiO2の量を約81.2モル%とするのが最も
好ましい。また、5baOaやN b 205の添加量
を0.1〜0.7重量%としたのは、Q、1重ft%以
上添加することによって添加しない場合よりも約20%
程度Qが向上し、明らかな添加効果がでてくるし、0.
7重量%を超えるとQが急激に減少し、温度係数も大き
くなるからである。これら数値限定の根拠については、
以下に述べる実験例の記載からもより一層明らかとなる
であろう。
The composition of the base BaO-TiO2 dielectric material is
BaO=15-25 mol%, Ti02=75-8
The reason for setting it to 5 mol% is that when the Ba0O amount exceeds 25 mol%, Q (= 1 / tan δ) decreases, and BaO
If the amount of 0O is less than 15 mol%, the decrease in Q is relatively small, but the temperature coefficient becomes large (which makes it unsuitable for practical use.However, in this type of composition, the amount of Ba0O is about 18.2 mol%, It is most preferable that the amount of TiO2 is about 81.2 mol%.The reason why the amount of 5baOa and Nb205 added is 0.1 to 0.7% by weight is because Q, 1% by weight or more is added. Approximately 20% more than without addition
The grade Q is improved, a clear addition effect appears, and 0.
This is because if it exceeds 7% by weight, Q will decrease rapidly and the temperature coefficient will also increase. Regarding the basis for these numerical limitations,
This will become clearer from the experimental examples described below.

実験例1゜ BaOO3,TiO2,5b203の各原料をそれぞれ
秤量して11種類の組成の異なる材料を得た。これら材
料をそれぞれボールミルにより湿式混合した後、これを
乾燥し、850〜1200Cの温度で6時間仮焼する。
Experimental Example 1 Each raw material of BaOO3, TiO2, and 5b203 was weighed to obtain 11 types of materials with different compositions. These materials are wet mixed using a ball mill, then dried and calcined at a temperature of 850 to 1200 C for 6 hours.

この後、再度ボールミルにて微粉砕した後、乾燥し、こ
れにポリビニルアルコール等の結合剤を加えて造粒し、
1000〜aoooKP/dの圧力にて201itφ、
 2011m+高の円柱状に成形する。この成形体を1
200〜1+ooUの温度で6時間焼成した後、111
11φX5m11の円柱に加工して11種類の試料(3
1〜S目)を得た。
After that, it is finely ground again in a ball mill, dried, and granulated by adding a binder such as polyvinyl alcohol to it.
201itφ at a pressure of 1000~aoooKP/d,
Form into a cylindrical shape with a height of 2011m+. This molded body is 1
After baking for 6 hours at a temperature of 200-1+ooU, 111
Processed into 11φ x 5m11 cylinders, 11 types of samples (3
1 to S) were obtained.

測定は、誘電体共振法により誘電率ε、誘電体損失ta
nδ、共振周波数の温度係数fO・TK(pPm/l:
、−40〜+80C)を求めたものである。測定周波数
は約6.5 GHzである。各試料の組成と電気的特性
を牙1表に示す。なお、ここで、Q=1/lanδであ
り、本口は本発明の範囲外の組成を示している。また、
試料番号81〜S6につし・では、矛1図にグラフとし
て掲げた。
The dielectric constant ε and dielectric loss ta are measured using the dielectric resonance method.
nδ, temperature coefficient of resonance frequency fO・TK (pPm/l:
, -40 to +80C). The measurement frequency is approximately 6.5 GHz. The composition and electrical properties of each sample are shown in Table 1. Note that here, Q=1/lan δ, and the main mouth indicates a composition outside the scope of the present invention. Also,
Sample numbers 81 to S6 are shown as graphs in Figure 1.

矛1表 5b20aを添加する場合は、矛1図からも判るように
、前記添加範囲の内、とりわけその添加量が0.5重量
係近傍、すなわち0.4〜0.6重量%が好ましい。0
06重量%近傍では、Qは極大をもち、しかも共振周波
数の温度係数は零に非常に近くなるからである。
When adding Table 5b20a, it is preferable that the amount added be around 0.5% by weight, that is, 0.4 to 0.6% by weight, within the above-mentioned addition range, as can be seen from Figure 1. 0
This is because at around 0.06% by weight, Q has a maximum and the temperature coefficient of the resonance frequency becomes very close to zero.

実験例2゜ Nb2O6についても実験例1と同様の手法により7種
の試料(Nl−N7)を製作し、測定を行なった。結果
を矛2表に示す。また、試料番号N1〜N6については
矛2図にその特性をグラフにして示した。
Experimental Example 2 Regarding Nb2O6, seven types of samples (Nl-N7) were prepared in the same manner as in Experimental Example 1, and measurements were performed. The results are shown in Table 2. Further, the characteristics of sample numbers N1 to N6 are shown in graph form in Figure 2.

矛2表 N b 206を添加する場合は、矛2図からも判るよ
うに、前記添加範囲の内、とりわけその添加量が086
重量重量%、すなわち0.5〜0.7重量%が好ましい
。0.6重量%前後では、Qはかなり大きく、しかも共
振周波数の温度係数は零に非常に近(なるからである。
When adding 206, as shown in Figure 2, within the above addition range, especially the addition amount is 086.
% by weight, i.e. 0.5-0.7% by weight is preferred. This is because at around 0.6% by weight, Q is quite large and the temperature coefficient of the resonance frequency is very close to zero.

本発明は、゛上記のように、本来高誘電率で損失が小さ
いとい5 BaO・TiO2系誘電体材料に、極<少量
のアンチモンまたはニオブの酸化物を添加することによ
って、更に一段と損失を小さく、換言するとQを大きく
することができ(無添加の場合に比し20%以上Qを大
きくできる)、また、共振周波数の温度係数を低く抑え
られるばかりでなく、添加量によってその温度係数の値
をコントロールすることも可能であり、そのうえ、焼成
温度を下げることができるため製造も容易となるなど数
々のすぐれた効果を奏しうるものである。
The present invention further reduces loss by adding a very small amount of antimony or niobium oxide to the BaO/TiO2 dielectric material, which originally has a high dielectric constant and low loss, as described above. In other words, it is possible to increase Q (Q can be increased by 20% or more compared to the case without additives), and not only can the temperature coefficient of the resonance frequency be kept low, but also the value of the temperature coefficient can be changed depending on the amount of addition. It is also possible to control the firing temperature, and in addition, the firing temperature can be lowered, making manufacturing easier.

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

牙1図は2BaO・9Ti02に対する5b203の添
加効果を示すグラフ、矛2図は2 Ba0・9TiO4
に対するNb2O5の添加効果を示すグラフである。 第1図 f;b20B  4、Mol(wt’A)1M2図
Figure 1 is a graph showing the effect of adding 5b203 to 2BaO・9Ti02, Figure 2 is a graph showing the effect of adding 5b203 to 2BaO・9TiO2.
2 is a graph showing the effect of adding Nb2O5 to Figure 1 f; b20B 4, Mol (wt'A) 1M2 figure

Claims (1)

【特許請求の範囲】 1、  Ba0= 15〜25モル係、Ti02=75
〜85モル%なる組成の誘電体材料眞対して、同期体表
で?V族矛5周期の元素の酸化物を0.1〜0.7重量
係添加してなるマイクロ波用誘電体磁器組成物。 2、 添加物が8b20aである特許請求の範囲矛1項
記載の組成物。 3、添加物がNb2O6である特許請求の範囲矛1項記
載の組成物。
[Claims] 1. Ba0=15-25 molar ratio, Ti02=75
In contrast to a dielectric material with a composition of ~85 mol%, in the synchronous body table? A dielectric ceramic composition for use in microwaves, in which 0.1 to 0.7 weight percent of an oxide of an element in five periods of group V is added. 2. The composition according to claim 1, wherein the additive is 8b20a. 3. The composition according to claim 1, wherein the additive is Nb2O6.
JP56181488A 1981-11-12 1981-11-12 Microwave dielectric ceramic composition Granted JPS5884179A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56181488A JPS5884179A (en) 1981-11-12 1981-11-12 Microwave dielectric ceramic composition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56181488A JPS5884179A (en) 1981-11-12 1981-11-12 Microwave dielectric ceramic composition

Publications (2)

Publication Number Publication Date
JPS5884179A true JPS5884179A (en) 1983-05-20
JPS6410467B2 JPS6410467B2 (en) 1989-02-21

Family

ID=16101629

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56181488A Granted JPS5884179A (en) 1981-11-12 1981-11-12 Microwave dielectric ceramic composition

Country Status (1)

Country Link
JP (1) JPS5884179A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6051662A (en) * 1983-08-27 1985-03-23 アルプス電気株式会社 Dielectric material
JPS62165804A (en) * 1986-01-16 1987-07-22 日本特殊陶業株式会社 Dielectric ceramic composition for high frequency
JPS62165805A (en) * 1986-01-16 1987-07-22 日本特殊陶業株式会社 Dielectric ceramic composition for high frequency
JPS6340212A (en) * 1986-08-06 1988-02-20 アルプス電気株式会社 Dielectric ceramic composition for microwave
JPS63168906A (en) * 1986-12-27 1988-07-12 株式会社住友金属セラミックス Dielectric ceramic composition for microwave
JP2007153710A (en) * 2005-12-07 2007-06-21 Tdk Corp Dielectric porcelain composition and electronic component

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0353384U (en) * 1989-09-30 1991-05-23

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6051662A (en) * 1983-08-27 1985-03-23 アルプス電気株式会社 Dielectric material
JPS62165804A (en) * 1986-01-16 1987-07-22 日本特殊陶業株式会社 Dielectric ceramic composition for high frequency
JPS62165805A (en) * 1986-01-16 1987-07-22 日本特殊陶業株式会社 Dielectric ceramic composition for high frequency
JPS6340212A (en) * 1986-08-06 1988-02-20 アルプス電気株式会社 Dielectric ceramic composition for microwave
JPS63168906A (en) * 1986-12-27 1988-07-12 株式会社住友金属セラミックス Dielectric ceramic composition for microwave
JP2007153710A (en) * 2005-12-07 2007-06-21 Tdk Corp Dielectric porcelain composition and electronic component

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Publication number Publication date
JPS6410467B2 (en) 1989-02-21

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