JPH0829981B2 - High frequency dielectric ceramic composition - Google Patents
High frequency dielectric ceramic compositionInfo
- Publication number
- JPH0829981B2 JPH0829981B2 JP61257743A JP25774386A JPH0829981B2 JP H0829981 B2 JPH0829981 B2 JP H0829981B2 JP 61257743 A JP61257743 A JP 61257743A JP 25774386 A JP25774386 A JP 25774386A JP H0829981 B2 JPH0829981 B2 JP H0829981B2
- Authority
- JP
- Japan
- Prior art keywords
- dielectric
- composition
- ceramic composition
- dielectric constant
- high 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.)
- Expired - Lifetime
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- Compositions Of Oxide Ceramics (AREA)
- Inorganic Insulating Materials (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は高周波用の誘電体磁器組成物に関するもので
ある。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a high frequency dielectric ceramic composition.
(従来の技術) 近年、自動車電話、パーソナル無線機の実用化、マイ
クロ波回路のIC化への発展、ガン発振器への応用等マイ
クロ波領域で誘電体磁器が広く利用されている。この様
な高周波用誘電体磁器は主に共振器に用いられるが、そ
こに要求される特性としては、(1)誘電体中では波長
が に短縮されるので小型化の要求に対して誘電率が大きい
事(2)高周波での誘電損失が小さいこと、(3)共振
周波数の温度に対する変化が少ないこと、即ち誘電率の
温度依存性が小さくかつ安定であること、以上の3特性
が挙げられる。(Prior Art) In recent years, dielectric ceramics have been widely used in the microwave region, such as the practical use of car telephones and personal radios, the development of ICs for microwave circuits, and the application to gun oscillators. Such high-frequency dielectric porcelain is mainly used for resonators, and the characteristics required therefor are (1) The dielectric constant is large to meet the demand for miniaturization (2) The dielectric loss at high frequencies is small, and (3) The change in resonance frequency with temperature is small, that is, the dielectric constant has temperature dependence. It must be small and stable, and the above three characteristics can be mentioned.
従来、この種の誘電体磁器としては、例えばBaO−TiO
2系材料、ReO−BaO−TiO2系材料及び(BaSr)(ZrTi)O3
系材料などが知られている。Conventionally, as a dielectric ceramic of this type, for example, BaO-TiO
2 material, ReO-BaO-TiO 2 based materials and (BaSr) (ZrTi) O 3
System materials are known.
(発明が解決しようとする問題点) しかしながら、BaO−TiO2系材料では誘電率がεr=3
8〜40と高く、また誘電損失はtanδ<2.00×10-4と小さ
いが、単一相では共振周波数の温度係数τf=0のもの
が得がたく、組成変化に対する誘電率及び誘電率の温度
依存性の変化も大きいため、高い誘電率、低い誘電損失
を維持したまま共振周波数の温度係数(τf)を安定に
小さく制御することが困難である。また、ReO〜BaO−Ti
O2系では誘電率はεr=40〜60と非常に高く、また共振
周波数の温度係数τf=0のものも得られるが、誘電損
失はtanδ>5.0×10-4と大きい。さらに(BaSr)(ZrTi)
O3系では誘電損失はtanδ<2.00×10-4と小さく、共振
周波数の温度係数τf=0のものも得られるが、誘電率
がεr=29〜35と非常に小さい。尚、上記誘電率(ε
r)及び誘電損失(tanδ)は半同軸共振器法により500
〜600MHzで測定した。このように、上記の何れの材料に
おいても高周波用誘電体材料に要求される前記3特性を
共に充分には満足していない。(Problems to be Solved by the Invention) However, in the BaO-TiO 2 system material, the dielectric constant is εr = 3.
It is as high as 8 to 40, and the dielectric loss is small as tan δ <2.00 × 10 -4 , but it is difficult to obtain a resonance frequency temperature coefficient τf = 0 in a single phase. Since the change in dependency is large, it is difficult to stably control the temperature coefficient (τf) of the resonance frequency to be small while maintaining a high dielectric constant and a low dielectric loss. In addition, ReO ~ BaO-Ti
The O 2 system has a very high dielectric constant of εr = 40 to 60 and a temperature coefficient τf = 0 of the resonance frequency can be obtained, but the dielectric loss is large as tan δ> 5.0 × 10 −4 . Furthermore (BaSr) (ZrTi)
In the O 3 system, the dielectric loss is small as tan δ <2.00 × 10 −4, and the one having the temperature coefficient τf = 0 of the resonance frequency can be obtained, but the dielectric constant is very small as εr = 29 to 35. The dielectric constant (ε
r) and dielectric loss (tan δ) are 500 by the semi-coaxial resonator method.
Measured at ~ 600 MHz. As described above, none of the above-mentioned materials sufficiently satisfy the three characteristics required for the high-frequency dielectric material.
(問題点を解決するための手段) 本発明は上記の現状に鑑み鋭意研究の結果、酸化スト
ロンチウム(SrO)、酸化ニッケル(NiO)、酸化ニオブ
(Nb2O5)から成る混合組成を主体とし、この主成分に
対し、酸化カルシウム(CaO)、酸化チタンから成る混
合組成を加えることによって得られる組成式(1) (1-X)Sr(Ni1/3Nb2/3)O3・XCaTiO3 ……(1) 但し、0<X≦0.6 で表わされる磁器組成物が高周波用として、高い誘電率
を有しかつ低い誘電損失を維持すると共に、共振周波数
の温度依存性が小さくかつ安定な特性を示すことを知見
し、本発明に至った。(Means for Solving Problems) As a result of intensive research in view of the above-mentioned present situation, the present invention mainly includes a mixed composition of strontium oxide (SrO), nickel oxide (NiO), and niobium oxide (Nb 2 O 5 ). , A composition formula (1) obtained by adding a mixed composition of calcium oxide (CaO) and titanium oxide to this main component (1) (1-X) Sr (Ni1 / 3Nb2 / 3) O 3 · XCaTiO 3 …… (1) However, the ceramic composition represented by 0 <X ≦ 0.6 has a high dielectric constant and maintains a low dielectric loss for high frequencies, and exhibits a stable temperature dependence and a small temperature dependence of the resonance frequency. This has led to the present invention.
本発明における組成式(1)で示される磁器組成物は
それ自体、Sr(Ni1/3Nb2/3)O3に対し、CaTiO3が固溶して
なるペロブスカイト型結晶構造の単一相であって、Sr
O、NiO、Nb2O5の組成比およびCaOとTiO2の組成は組成式
(1)に示す各々の割合からなるものであって、これら
の比率がはずれると、ペロブスカイト型結晶構造がくず
れ単一相でなくなると同時に、優れた誘電体特性が劣化
する。The porcelain composition represented by the composition formula (1) in the present invention is itself a single phase of a perovskite type crystal structure in which CaTiO 3 is formed as a solid solution with Sr (Ni1 / 3Nb2 / 3) O 3. , Sr
The composition ratio of O, NiO, Nb 2 O 5 and the composition of CaO and TiO 2 are composed of the respective ratios shown in the composition formula (1). If these ratios are deviated, the perovskite type crystal structure is broken. At the same time, it loses the excellent dielectric properties at the same time.
なお、組成式(1)においてX値は0<X≦0.6範囲
であり、X>0.6では誘電損失が大きくQ値が低下する
とともに誘電率の温度係数が大きくなる。特に好ましい
X値は0.1≦X≦0.5である。In the composition formula (1), the X value is in the range of 0 <X ≦ 0.6. When X> 0.6, the dielectric loss is large and the Q value is low, and the temperature coefficient of the dielectric constant is large. Particularly preferable X value is 0.1 ≦ X ≦ 0.5.
実施例 試料の作成 高純度の炭酸ストロンチウム(SrCO3)、酸化ニッケ
ル(NiO)、酸化ニオブ(Nb2O5)および炭酸カルシウム
(CaCO3)、酸化チタン(TiO2)を用いて、X値が第1
表の組成欄に示す割合となるように秤量し、めのう玉石
を用いて一昼夜湿式混合した。この混合物を乾燥したの
ち1,300℃で2時間仮焼を行ない、さらに約1重量%の
バインダーを加えてから整粒し、得られた粉末を約800K
g/cm2の圧力で成形し、それを1,400℃〜1,700℃の範囲
の温度で2時間空気中において焼成した。Example Preparation of sample Using high-purity strontium carbonate (SrCO 3 ), nickel oxide (NiO), niobium oxide (Nb 2 O 5 ), calcium carbonate (CaCO 3 ), and titanium oxide (TiO 2 ) First
It was weighed so as to have the ratio shown in the composition column of the table, and wet-mixed all day and night using agate boulders. After drying this mixture, it is calcined at 1,300 ° C for 2 hours, further added about 1% by weight of binder, and then sized. The powder obtained is about 800K.
It was molded at a pressure of g / cm 2 and calcined in air at a temperature in the range of 1,400 ° C to 1,700 ° C for 2 hours.
特性の測定 得られた試料について誘電体円柱共振器法(ポストレ
ゾネータ法)によって共振周波数4.5〜9GHzにて誘電
率,誘電損失及び共振周波数の温度係数を測定した。結
果は第1表に示す。Measurement of characteristics The dielectric constant, the dielectric loss, and the temperature coefficient of the resonance frequency of the obtained sample were measured by the dielectric cylinder resonator method (post-resonator method) at the resonance frequency of 4.5 to 9 GHz. The results are shown in Table 1.
第1表から明らかなようにCaTiO3を含まないNo.1のサ
ンプルでは誘電率が小さく、またX>0.6のNo.8のサン
プルでは誘電率は大きいが誘電損失が大きいためにQ値
が小さく、共振周波数の温度係数も大きいものであっ
た。これに対し、本発明のサンプルNo.2〜7はいずれも
優れた誘電特性を示し、誘電率30以上、Q値2200以上、
|τf|が80以下の特性が得られ、特に0.1≦X≦0.5の範
囲では誘電率30以上、Q値2300以上、|τf|33以下の優
れた特性を示した。 As is clear from Table 1, the sample No. 1 containing no CaTiO 3 has a small dielectric constant, and the sample No. 8 with X> 0.6 has a large dielectric constant but a large dielectric loss, resulting in a small Q value. The temperature coefficient of the resonance frequency was also large. On the other hand, Sample Nos. 2 to 7 of the present invention all show excellent dielectric properties, having a dielectric constant of 30 or more, a Q value of 2200 or more,
A characteristic of | τf | of 80 or less was obtained, and particularly in the range of 0.1 ≦ X ≦ 0.5, excellent characteristics of dielectric constant of 30 or more, Q value of 2300 or more, and | τf | 33 or less were exhibited.
(発明の効果) 以上詳述した通り本発明の高周波用誘電体磁器組成物
はSrO,NiO,Nb2O5から成るペロブスカイト型結晶構造の
磁器組成物に対し、CaO,TiO2から成る同様の結晶構造の
磁器組成物を特定の割合で固溶させ、単一相のペロブス
カイト型結晶を形成させることによって高周波に対して
高い誘電率、低い誘電損失および共振周波数の温度係数
の小さい特性が得られる。それによって共振器あるいは
回路基板材料としての用途に対し満足したものが得られ
ると同時に小型化も可能とすることができる。(Effects of the Invention) As described in detail above, the high-frequency dielectric ceramic composition of the present invention has the same composition of CaO and TiO 2 as the ceramic composition of perovskite type crystal structure of SrO, NiO and Nb 2 O 5 . By forming a single-phase perovskite-type crystal by forming a solid solution of a porcelain composition having a crystal structure, it is possible to obtain high dielectric constant, low dielectric loss, and low temperature coefficient of resonance frequency for high frequencies. . As a result, it is possible to obtain a material that is satisfactory for use as a resonator or a circuit board material, and at the same time, it is possible to reduce the size.
Claims (1)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61257743A JPH0829981B2 (en) | 1986-10-29 | 1986-10-29 | High frequency dielectric ceramic composition |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61257743A JPH0829981B2 (en) | 1986-10-29 | 1986-10-29 | High frequency dielectric ceramic composition |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63112461A JPS63112461A (en) | 1988-05-17 |
| JPH0829981B2 true JPH0829981B2 (en) | 1996-03-27 |
Family
ID=17310483
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61257743A Expired - Lifetime JPH0829981B2 (en) | 1986-10-29 | 1986-10-29 | High frequency dielectric ceramic composition |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0829981B2 (en) |
-
1986
- 1986-10-29 JP JP61257743A patent/JPH0829981B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63112461A (en) | 1988-05-17 |
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