JP2950672B2 - Dielectric porcelain composition - Google Patents

Dielectric porcelain composition

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Publication number
JP2950672B2
JP2950672B2 JP4007449A JP744992A JP2950672B2 JP 2950672 B2 JP2950672 B2 JP 2950672B2 JP 4007449 A JP4007449 A JP 4007449A JP 744992 A JP744992 A JP 744992A JP 2950672 B2 JP2950672 B2 JP 2950672B2
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JP
Japan
Prior art keywords
composition
sample
dielectric
range
resonance frequency
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JP4007449A
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Japanese (ja)
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JPH05198210A (en
Inventor
智広 鶴田
洋一郎 横谷
公一 釘宮
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Panasonic Holdings Corp
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Matsushita Electric Industrial Co Ltd
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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、マイクロ波、ミリ波帯
などの高周波領域において使用される誘電体共振器、及
び誘電体フィルター等に好適な誘電体磁器組成物に関す
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a dielectric ceramic composition suitable for a dielectric resonator and a dielectric filter used in a high frequency region such as a microwave and a millimeter wave band.

【0002】[0002]

【従来の技術】従来から高周波領域において、回路のイ
ンピーダンス整合、誘電体共振器、及びフィルター等に
誘電体が応用されているが、近年通信の高周波化及び高
密度化に対応するため、無負荷Qが大きく、かつ温度変
化による共振周波数の変動が小さい誘電体が求められて
いる。
2. Description of the Related Art Conventionally, dielectrics have been applied to impedance matching of circuits, dielectric resonators, filters, and the like in the high-frequency region. There is a need for a dielectric having a large Q and a small variation in resonance frequency due to a temperature change.

【0003】BaO−MgO−Ta2 5 系の複合ペロ
ブスカイト型組成物は、既存の材料の中で高い無負荷Q
を有する材料のひとつとして知られるが、共振周波数の
温度変化率に問題があった。
A composite perovskite composition based on BaO—MgO—Ta 2 O 5 has a high unloaded Q value among existing materials.
However, there is a problem with the temperature change rate of the resonance frequency.

【0004】これに対し共振周波数の温度変化率の低減
を図った組成として、BaO−MgO−Ta2 5 系の
MgOの一部を、NiOで置き換えた組成系(特開昭6
0−216407号公報)、及びBaO−MgO−Ta
2 5 系のMgOの一部を、CoOで置き換えた組成系
などが提案されている(特開昭61−8804号公
報)。
On the other hand, as a composition for reducing the temperature change rate of the resonance frequency, a composition system in which a part of MgO of BaO—MgO—Ta 2 O 5 is replaced by NiO (Japanese Patent Laid-Open No.
0-216407) and BaO-MgO-Ta
Some of the 2 O 5 system MgO, such as composition system was replaced with CoO has been proposed (JP 61-8804 JP).

【0005】[0005]

【発明が解決しようとする課題】しかしながら、前記従
来から提案されているこれらのMgOへのNiO,Co
Oの置換組成系は、共振周波数の温度変化率の低減がは
かれる一方で、無負荷Qの低下の問題点を有していた。
However, NiO and Co are added to the above-mentioned conventionally proposed MgO.
The substitutional composition system of O has a problem that the unloaded Q is reduced while the temperature change rate of the resonance frequency is reduced.

【0006】本発明は、前記従来の問題点を解決するた
め、BaO−MgO−Ta2 5 系系の複合ペロブスカ
イト型組成物において、高い無負荷Qを保ちながら共振
周波数の温度変化率の低減を図れる誘電体磁器組成物を
提供することを目的とする。
In order to solve the above-mentioned conventional problems, the present invention provides a BaO-MgO-Ta 2 O 5 based composite perovskite-type composition, which is capable of reducing the temperature change rate of the resonance frequency while maintaining a high no-load Q. It is an object of the present invention to provide a dielectric porcelain composition capable of achieving the following.

【0007】[0007]

【課題を解決するための手段】前記目的を達成するた
め、本発明の第1番目の誘電体磁器組成物は、一般式B
1-X-Y (Mg1-Z CoZ X TaY n で表わされ、
0.01≦z≦0.45の範囲にあるzに対し、0.13≦x≦0.1
9、0.31≦y≦0.37、かつ0.4800≦x+y≦0.4998の範
囲にある(ただしnは任意の数)という構成を備えたも
のである。
In order to achieve the above object, the first dielectric porcelain composition of the present invention has a general formula B
a 1-XY (Mg 1- Z Co Z) is represented by X Ta Y O n,
For z in the range of 0.01 ≦ z ≦ 0.45, 0.13 ≦ x ≦ 0.1
9, which has a configuration in which 0.31 ≦ y ≦ 0.37 and 0.4800 ≦ x + y ≦ 0.4998 (where n is an arbitrary number).

【0008】また本発明の第2番目の誘電体磁器組成物
は、一般式Ba1-X-Y (Mg1-Z NiZ X TaY n
で表わされ、0.01≦z≦0.40の範囲にあるzに対し、0.
12≦x≦0.18、0.32≦y≦0.38、かつ0.4800≦x+y≦
0.4998の範囲にある(ただしnは任意の数)という構成
を備えたものである。
[0008] The second dielectric ceramic composition of the present invention have the general formula Ba 1-XY (Mg 1- Z Ni Z) X Ta Y O n
And for z in the range 0.01 ≦ z ≦ 0.40, 0.
12 ≦ x ≦ 0.18, 0.32 ≦ y ≦ 0.38, and 0.4800 ≦ x + y ≦
It has a configuration that is in the range of 0.4998 (where n is an arbitrary number).

【0009】さらに本発明の第3番目の誘電体磁器組成
物は、一般式Ba1-X-Y (Mg1-Z- V CoZ NiV X
TaY n で表わされ、0.01≦z+v≦0.40、z>0 、
かつv>0 の範囲にあるzとvに対し、 0.13 ≦x≦0.
18 0.32 ≦y≦0.37かつ0.4800≦x+y≦0.4998の範囲
にある(ただしnは任意の数)という構成を備えたもの
である。
Further, a third dielectric ceramic composition of the present invention has a general formula of Ba 1 -XY (Mg 1 -Z- V Co Z Ni V ) X
Ta Y O n represented by, 0.01 ≦ z + v ≦ 0.40 , z> 0,
And for z and v in the range of v> 0, 0.13 ≦ x ≦ 0.
18 0.32 ≦ y ≦ 0.37 and 0.4800 ≦ x + y ≦ 0.4998 (where n is an arbitrary number).

【0010】[0010]

【作用】前記本発明の第1〜第3番目の誘電体磁器組成
物の構成によれば、組成式Ba 1-X-Y (Mg1-Z-V Co
Z NiV X TaY n で表わされる誘電体磁器組成物
であってかつ特定のz+v、x、yの範囲とすることに
より、高い無負荷Qを有し、共振周波数の温度変化率:
τf の小さい磁器を得ることができる。
The first to third dielectric ceramic compositions of the present invention
According to the composition of the product, the composition formula Ba 1-XY(Mg1-ZVCo
ZNiV)XTaYOnDielectric porcelain composition represented by
And a specific range of z + v, x, y
It has a higher no-load Q and the temperature change rate of the resonance frequency:
τfIt is possible to obtain a small porcelain.

【0011】[0011]

【実施例】【Example】

実施例1 出発原料として、化学的に高純度なBaCO3 ,Mg
O,CoO,Ta2 5 を使用し、表1〜表3に示され
た所定の組成に秤量を行い、これをボールミルを用い湿
式混合処理した。
Example 1 Chemically high purity BaCO 3 , Mg
O, CoO, using Ta 2 O 5, performs a weighing a predetermined composition shown in Table 1 to Table 3, which was wet-mixing treatment using a ball mill.

【0012】この混合物を乾燥し、800℃で2時間仮
焼成を行った後、この仮焼成粉をさらにボールミルで粉
砕し、脱水乾燥後に粘結材としてポリビニルアルコール
を適当量加え、1ton/cm2 の圧力を加えて、直径
8mm、厚み4mmの円板に成形した。
This mixture is dried and calcined at 800 ° C. for 2 hours. The calcined powder is further pulverized by a ball mill, and after dehydration and drying, an appropriate amount of polyvinyl alcohol is added as a binder and 1 ton / cm 2. To form a disk having a diameter of 8 mm and a thickness of 4 mm.

【0013】この成形体を1500〜1550℃で12
時間本焼成を行い磁器試料を得た。尚、焼成は高温にお
ける成分の蒸発を考慮して、同一組成の仮焼成粉体で十
分に充填された白金容器中に成形体試料を入れた状態で
行った。
The molded body is heated at 1500 to 1550 ° C. for 12 hours.
The sintering was performed for a time to obtain a porcelain sample. The calcination was carried out in a state in which the molded body sample was placed in a platinum container sufficiently filled with a preliminarily calcined powder having the same composition in consideration of the evaporation of components at a high temperature.

【0014】得られた各磁器試料について、10GHz
の周波数における比誘電率: εr 、無負荷Q値: Q、及
び−50℃〜50℃における共振周波数の温度変化率:
τf (ppm/ ℃) を測定した。結果を表1〜表3に示す。
For each porcelain sample obtained, 10 GHz
Dielectric constant at the frequency of: ε r , unloaded Q value: Q, and temperature change rate of the resonance frequency at −50 ° C. to 50 ° C .:
τ f (ppm / ° C.) was measured. The results are shown in Tables 1 to 3.

【0015】[0015]

【表1】 [Table 1]

【0016】[0016]

【表2】 [Table 2]

【0017】[0017]

【表3】 [Table 3]

【0018】表1〜表3から明かなようにx+y<0.48
の組成では焼結性が悪く、x+y>0.4998の組成ではQ
が著しく小さくなるが、0.48≦x+y≦0.4998の範囲で
は高いQ値と小さなτf が得られた。尚、本実施例の試
料No.33 は特開昭61-8804 号公報中の試料No.1と同一組
成、同じく本実施例の試料No.44 は同公開公報の試料N
o.2と、本実施例の試料No.59 は同公開公報の試料No.5
と同一組成である。これらBaとBa以外の組成比が
1:1の従来組成では、本実施例による組成域における
ものに比べQ値が著しく小さかった。
As is clear from Tables 1 to 3, x + y <0.48
Is poor in sinterability with the composition x, and Q
Was significantly reduced, but a high Q value and a small τ f were obtained in the range of 0.48 ≦ x + y ≦ 0.4998. The sample No. 33 of this example had the same composition as the sample No. 1 in JP-A-61-8804, and the sample No. 44 of this example was also the sample N of the publication.
o.2 and Sample No. 59 of this example are the same as Sample No. 5 of the publication.
And the same composition. In the conventional composition having a composition ratio of Ba and other than Ba of 1: 1, the Q value was significantly smaller than that in the composition range according to the present example.

【0019】またx<0.13、z<0.01ではτf が大き
く、y<0.31、z>0.45の組成ではQ値が低下するため
に実用的ではない。本実施例による組成範囲ではいずれ
の組成でもQ値が20000 以上で且つ、共振周波数の温度
変化率が3ppm/ ℃以下と非常に良好な電気的特性を有し
ている。
When x <0.13 and z <0.01, τ f is large, and when the composition is y <0.31 and z> 0.45, the Q value decreases, which is not practical. In the composition range according to the present embodiment, the Q value is 20,000 or more and the temperature change rate of the resonance frequency is 3 ppm / ° C. or less, which is a very good electrical characteristic.

【0020】実施例2 出発原料として、化学的に高純度なBaCO3 ,Mg
O,NiO,Ta2 5 を使用した。次に表4〜表6に
示された所定の組成に秤量を行い、これをボールミルを
用い湿式混合処理した。以下実施例1と同様の方法で供
試試料を得た。
Example 2 As a starting material, chemically pure BaCO 3 , Mg
O, NiO and Ta 2 O 5 were used. Next, a predetermined composition shown in Tables 4 to 6 was weighed, and the mixture was wet-mixed using a ball mill. Hereinafter, test samples were obtained in the same manner as in Example 1.

【0021】表4〜表6に各組成毎の周波数10GHz
における比誘電率: εr 、無負荷Q値: Q、及び−50
℃〜50℃における共振周波数の温度変化率: τf (ppm
/ ℃) を示す。
Tables 4 to 6 show a frequency of 10 GHz for each composition.
Relative permittivity at ε r , unloaded Q value: Q, and −50
Temperature change rate of resonance frequency between ℃ and 50 ℃: τ f (ppm
/ ° C).

【0022】[0022]

【表4】 [Table 4]

【0023】[0023]

【表5】 [Table 5]

【0024】[0024]

【表6】 [Table 6]

【0025】表4〜表6から明かなようにx+y<0.48
の組成では焼結性が悪く、x+y>0.4998の組成ではQ
が著しく小さくなり0.48≦x+y≦0.4998の範囲では高
いQ値と小さなτf が得られた。尚、本実施例の試料N
o.131は特開昭60-216407 号公報中の試料No.1と同一組
成、同じく本実施例の試料No.143は同公報の試料No.2
と、本実施例の試料No.158は同公報の試料No.5と同一組
成である。これらBaとBa以外の組成比が1:1の従
来組成では本実施例による組成域におけるものに比べQ
値が著しく小さかった。
As is clear from Tables 4 to 6, x + y <0.48
Is poor in sinterability with the composition x, and Q
Was significantly reduced, and a high Q value and a small τ f were obtained in the range of 0.48 ≦ x + y ≦ 0.4998. In addition, the sample N of the present example
o.131 has the same composition as sample No. 1 in JP-A-60-216407, and similarly, sample No. 143 of this example is sample No. 2 of the same publication.
The sample No. 158 of this example has the same composition as the sample No. 5 of the publication. In the conventional composition in which the composition ratio of Ba and other than Ba is 1: 1, Q is larger than that in the composition range according to the present embodiment.
The values were significantly smaller.

【0026】またx<0.12、z<0.01ではτf が大き
く、y<0.32、z>0.40の組成ではQ値が低下するため
に実用的ではない。本実施例による組成範囲では、いず
れの組成でもQ値が20000 以上で且つ、共振周波数の温
度変化率が3ppm/ ℃以下と非常に良好な電気的特性を有
していた。
Further, when x <0.12 and z <0.01, τ f is large, and when the composition is y <0.32 and z> 0.40, the Q value is lowered, so that it is not practical. In the composition range according to the present embodiment, the Q value was 20,000 or more, and the temperature change rate of the resonance frequency was 3 ppm / ° C. or less, which was a very good electrical characteristic.

【0027】実施例3 出発原料として、純度99.9%以上のBaCO3 ,M
gO,CoO,NiO,Ta2 5 を使用した。次に表
7〜表9に示された組成とするための秤量を行い、これ
をボールミルを用い湿式混合処理した。以下実施例1と
同様の方法で供試試料を得た。
Example 3 As a starting material, BaCO 3 , M having a purity of 99.9% or more was used.
gO, was used CoO, NiO, the Ta 2 O 5. Next, weighing was performed to obtain the compositions shown in Tables 7 to 9, and this was subjected to wet mixing using a ball mill. Hereinafter, test samples were obtained in the same manner as in Example 1.

【0028】表7〜表9に各組成毎の周波数10GHz
における比誘電率: εr 、無負荷Q値: Q、及び−50
℃〜50℃における共振周波数の温度変化率: τf (ppm
/ ℃) を示す。
Tables 7 to 9 show a frequency of 10 GHz for each composition.
Relative permittivity at ε r , unloaded Q value: Q, and −50
Temperature change rate of resonance frequency between ℃ and 50 ℃: τ f (ppm
/ ° C).

【0029】[0029]

【表7】 [Table 7]

【0030】[0030]

【表8】 [Table 8]

【0031】[0031]

【表9】 [Table 9]

【0032】表7〜表9から明かなように、各電気特性
は実施例1及び2と同様の挙動を示す。またCoとNi
の組成比に応じてCo,Ni各単体時の特性の中間的な
特性を示す。すなわちCoとNiの比を調製することに
より任意のεr に対して必要なτf を制御することがで
きる。
As is clear from Tables 7 to 9, each electric characteristic shows the same behavior as in Examples 1 and 2. Co and Ni
Shows the intermediate characteristics of the characteristics of each of Co and Ni alone depending on the composition ratio. That is, by adjusting the ratio of Co and Ni, it is possible to control τ f required for an arbitrary ε r .

【0033】以上説明した通り、誘電体磁器を用いた高
周波デバイスではデバイス自体から生じる温度依存性を
有する場合もあり、この場合、デバイスに必要な磁器の
誘電率を保ちながら誘電体の温度依存性で全体としての
温度依存性を補償する必要がある。ゆえに任意のεr
対しτf を制御することは、温度依存性のない高周波デ
バイスを設計するうえで極めて有用なこととなる。した
がって本発明はこの技術分野でとくに有効であると考え
られる。
As described above, a high-frequency device using a dielectric porcelain may have a temperature dependency caused by the device itself. In this case, the temperature dependency of the dielectric while maintaining the permittivity of the porcelain required for the device may be maintained. It is necessary to compensate for the temperature dependency as a whole. Therefore, controlling τ f for an arbitrary ε r is extremely useful in designing a high-frequency device having no temperature dependence. Therefore, the present invention is considered to be particularly effective in this technical field.

【0034】[0034]

【発明の効果】以上説明した通り本発明によれば、組成
式Ba1-X-Y (Mg1-Z-V CoZ Ni V X TaY n
で表わされる誘電体磁器組成物で特定のz+v、x、y
の範囲とし、とくに0.4800≦x+y≦0.4998の範囲とし
たことにより、高い無負荷Q値と小さい共振周波数の温
度変化率を同時に満足する誘電体磁器を得ることが可能
となる。
As described above, according to the present invention, the composition
Formula Ba1-XY(Mg1-ZVCoZNi V)XTaYOn
Specific z + v, x, y in the dielectric ceramic composition represented by
, Especially 0.4800 ≦ x + y ≦ 0.4998
As a result, high unloaded Q value and low resonance frequency
Dielectric porcelain that simultaneously satisfies the rate of change
Becomes

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭61−8804(JP,A) 特開 昭63−19706(JP,A) 特開 昭63−152815(JP,A) 特開 平3−5357(JP,A) 特開 平4−4509(JP,A) 特開 平3−171507(JP,A) (58)調査した分野(Int.Cl.6,DB名) H01B 3/12 312 C04B 35/495 H01G 4/12 415 H01P 11/00 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-61-8804 (JP, A) JP-A-63-19706 (JP, A) JP-A-63-152815 (JP, A) 5357 (JP, A) JP-A-4-4509 (JP, A) JP-A-3-171507 (JP, A) (58) Fields investigated (Int. Cl. 6 , DB name) H01B 3/12 312 C04B 35/495 H01G 4/12 415 H01P 11/00

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】一般式Ba1-X-Y (Mg1-Z CoZ X
Y n で表わされ、0.01≦z≦0.45の範囲にあるzに
対し、0.13≦x≦0.19、0.31≦y≦0.37、かつ0.4800≦
x+y≦0.4998の範囲にある誘電体磁器組成物(ただし
nは任意の数)。
1. The general formula Ba 1 -XY (Mg 1 -Z Co Z ) X T
represented by a Y O n, to z in the range of 0.01 ≦ z ≦ 0.45, 0.13 ≦ x ≦ 0.19,0.31 ≦ y ≦ 0.37, and 0.4800 ≦
A dielectric ceramic composition in the range of x + y ≦ 0.4998 (where n is an arbitrary number).
【請求項2】一般式Ba1-X-Y (Mg1-Z NiZ X
Y n で表わされ、0.01≦z≦0.40の範囲にあるzに
対し、0.12≦x≦0.18、0.32≦y≦0.38、かつ0.4800≦
x+y≦0.4998の範囲にある誘電体磁器組成物(ただし
nは任意の数)。
2. The general formula Ba 1 -XY (Mg 1 -Z Ni Z ) X T
represented by a Y O n, to z in the range of 0.01 ≦ z ≦ 0.40, 0.12 ≦ x ≦ 0.18,0.32 ≦ y ≦ 0.38, and 0.4800 ≦
A dielectric ceramic composition in the range of x + y ≦ 0.4998 (where n is an arbitrary number).
【請求項3】一般式Ba1-X-Y (Mg1-Z-V CoZ Ni
V X TaY n で表わされ、0.01≦z+v≦0.40、z
>0 、かつv>0 の範囲にあるzとvに対し、0.13 ≦
x≦0.18, 0.32 ≦y≦0.37かつ0.4800≦x+y≦0.49
98の範囲にある誘電体磁器組成物(ただしnは任意の
数)。
3. A compound of the formula Ba 1 -XY (Mg 1 -ZV Co Z Ni)
V) represented by X Ta Y O n, 0.01 ≦ z + v ≦ 0.40, z
> 0 and for z and v in the range v> 0, 0.13 ≤
x ≦ 0.18, 0.32 ≦ y ≦ 0.37 and 0.4800 ≦ x + y ≦ 0.49
A dielectric ceramic composition in the range of 98 (where n is an arbitrary number).
JP4007449A 1992-01-20 1992-01-20 Dielectric porcelain composition Expired - Fee Related JP2950672B2 (en)

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