JPH06203631A - Dielectric porcelain composition - Google Patents

Dielectric porcelain composition

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Publication number
JPH06203631A
JPH06203631A JP4361286A JP36128692A JPH06203631A JP H06203631 A JPH06203631 A JP H06203631A JP 4361286 A JP4361286 A JP 4361286A JP 36128692 A JP36128692 A JP 36128692A JP H06203631 A JPH06203631 A JP H06203631A
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JP
Japan
Prior art keywords
composition
value
dielectric
region
oxide
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.)
Pending
Application number
JP4361286A
Other languages
Japanese (ja)
Inventor
Michiaki Tsurumi
通昭 鶴見
Ryoji Takeishi
良治 武石
Kazuaki Endo
一明 遠藤
Yasue Ishiguro
靖江 石黒
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FDK Corp
Original Assignee
FDK Corp
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Filing date
Publication date
Application filed by FDK Corp filed Critical FDK Corp
Priority to JP4361286A priority Critical patent/JPH06203631A/en
Publication of JPH06203631A publication Critical patent/JPH06203631A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】 【目的】 誘電率が高く、かつ共振周波数の温度係数τ
f が0ppm /℃近傍に調整可能な誘電体材料であり、さ
らにマイクロ波領域において実用可能な無負荷Q値を有
する高誘電率のマイクロ波誘電体材料を提供する。 【構成】 酸化鉛、酸化カルシウム、酸化ジルコニウム
及び酸化スズからなる誘電体磁器組成物であって、各成
分の組成比が、一般式(Pbm Ca1-m )(Sn1-o
o )O3 で表したとき、m及びoがm−o平面におい
て下記のa,b,c,dを頂点とする領域内にある(た
だし、o=1.0の線上を除く)。 a; m=0.7 o=1.0 b; m=0.78 o=1.0 c; m=0.94 o=0.25 d; m=0.9 o=0.25
(57) [Abstract] [Purpose] High permittivity and temperature coefficient of resonance frequency τ
Disclosed is a microwave dielectric material having a high dielectric constant, which is a dielectric material whose f can be adjusted to around 0 ppm / ° C. and which has a practically unloaded Q value in the microwave region. [Composition] A dielectric ceramic composition comprising lead oxide, calcium oxide, zirconium oxide, and tin oxide, wherein the composition ratio of each component is represented by the general formula (Pb m Ca 1-m ) (Sn 1-o Z
r o ) O 3 , m and o are in the region having the following a, b, c, and d as vertices in the m-o plane (except on the line of o = 1.0). a; m = 0.7 o = 1.0 b; m = 0.78 o = 1.0 c; m = 0.94 o = 0.25 d; m = 0.9 o = 0.25

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、主にマイクロ波領域に
おいて用いる、酸化鉛、酸化カルシウム、酸化ジルコニ
ウム及び酸化スズからなる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 composed mainly of lead oxide, calcium oxide, zirconium oxide and tin oxide used in the microwave region.

【0002】[0002]

【従来の技術】自動車電話や携帯電話など、マイクロ波
を利用した移動体通信装置などに用いられるマイクロ波
誘電体には、高い誘電率を有し機器の小型化に役立つ
こと、 高い周波数帯域においても使用できるよう、大きな無
負荷Q値を有すること、 使用環境(特に温度)において誘電特性が変化しない
ことが要求され、これら3つの要件が同時に達成されて
いなければならない。
2. Description of the Related Art Microwave dielectrics used in mobile communication devices using microwaves, such as car phones and mobile phones, have a high dielectric constant and are useful for downsizing equipment. In order to be able to use it, it is required to have a large unloaded Q value, and the dielectric characteristics should not change in the usage environment (especially temperature), and these three requirements must be achieved at the same time.

【0003】誘電体内で電磁波の波長は1/√εr に短
くなるため、誘電率の増加は通信装置の小型化に役立
つ。通信量の増大は使用周波数帯を次第に押し上げ、回
線当たりの周波数領域を狭くし、小型化による重量の制
約は通信時間の確保を困難にする。従って、共振周波数
の安定性と、大きな無負荷Q値が必要となる。
Since the wavelength of the electromagnetic wave is shortened to 1 / √ε r in the dielectric body, the increase of the dielectric constant is useful for downsizing the communication device. The increase in communication volume gradually raises the frequency band used, narrows the frequency range per line, and the weight restriction due to miniaturization makes it difficult to secure communication time. Therefore, stability of the resonance frequency and a large unloaded Q value are required.

【0004】このような特性を有する高誘電率マイクロ
波誘電体として、BaO−TiO2−La系(ここで、
LaはNd、Smなどのランタノイド系酸化物)からな
り、比誘電率が90前後でその温度係数の小さなものが
得られている。
As a high dielectric constant microwave dielectric having such characteristics, a BaO--TiO 2 --La system (here,
La is made of lanthanoid oxide such as Nd and Sm), and has a relative dielectric constant of about 90 and a small temperature coefficient.

【0005】しかしながら、近年のマイクロ波を利用し
た通信機器の小型化への動きは、比誘電率が90前後の
BaO−TiO2 −La系の従来材を越える特性を必要
としている。同時に大きな無負荷Q値を有し、かつ小さ
な温度係数を有する材料が必要とされている。このよう
な特性を有する組成物として、特開平4−192209
号公報に記載された磁器組成物がある。この磁器組成物
は、組成式 (Pb1-x Cax )Zr1-y Sny 3 で表したとき、x及びyが、x−y平面で下記の点A,
B,C,Dを頂点とする四角形の領域内にあるものであ
る。 A;x=0.3 y=0.0 B;x=0.5 y=0.0 C;x=0.4 y=0.6 D;x=0.25 y=0.6 しかし、この領域内の磁器組成物は、比誘電率が110
前後にすぎず、従来材の特性をはるかに上回るものとは
言いがたい。
However, the recent movement toward miniaturization of communication equipment using microwaves requires characteristics exceeding the BaO—TiO 2 —La type conventional material having a relative dielectric constant of about 90. At the same time, there is a need for a material that has a large unloaded Q value and a small temperature coefficient. A composition having such characteristics is disclosed in JP-A-4-192209.
There is a porcelain composition described in the publication. When this porcelain composition is represented by the composition formula (Pb 1-x Ca x ) Zr 1-y Sn y O 3 , x and y are the following points A on the xy plane:
It is in a rectangular area having B, C, and D as vertices. A; x = 0.3 y = 0.0 B; x = 0.5 y = 0.0 C; x = 0.4 y = 0.6 D; x = 0.25 y = 0.6 The porcelain composition in this region has a relative dielectric constant of 110.
It is just before and after, and it is hard to say that it far exceeds the characteristics of conventional materials.

【0006】一方、上記3つの特性を同時に満足させる
ため、多種組成物の一体焼結や張り合わせも試みられて
いるが、こうして得られる組成物は均一性等に問題があ
り未だ実用化されていない。
On the other hand, in order to satisfy the above three characteristics at the same time, it has been attempted to integrally sinter and bond various compositions, but the composition thus obtained has a problem in uniformity and has not yet been put to practical use. .

【0007】[0007]

【発明が解決しようとする課題】本発明の目的は、かか
る従来材に比べてさらに誘電率が高く、かつ共振周波数
の温度係数τf が0ppm /℃近傍に調整可能な誘電体材
料であり、さらにマイクロ波領域において実用可能な無
負荷Q値を有する高誘電率のマイクロ波誘電体材料を提
供することにある。
An object of the present invention is to provide a dielectric material having a higher permittivity than that of the conventional material and having a temperature coefficient τ f of the resonance frequency which can be adjusted to around 0 ppm / ° C. Another object of the present invention is to provide a microwave dielectric material having a high dielectric constant and an unloaded Q value that can be practically used in the microwave region.

【0008】[0008]

【課題を解決するための手段】本発明者等は、上記特開
平4−192209号公報において、「マイクロ波誘電
体として望ましい特性が得られない」とされた領域にお
いて、さらに検討を進めた。具体的には、一般式 (Pbm Ca1-m )(Sn1-o Zro )O3 で表される組成物について、SnとZrの組成比を所定
の値としてPbとCaの比を変化させていった場合、共
振周波数の温度係数τf は、Pbの比率が高くなるに従
い負の値から±0をとおり正の値となり再び±0を横切
り負の値になる傾向がある、ことを発見した(図2参
照)。このτf が正の値から再び±0を横切り負の値に
至る付近のPbとCaの比率における比誘電率は、Pb
の比率が高くなるに従いさらに増加する傾向にある、こ
とを発見した(図3参照)。この場合、Pbの比率が高
くなるに従い無負荷Q値は減少傾向にあるが(図4参
照)、比較的低周波領域に用いるマイクロ波誘電体フィ
ルター等にあっては、十分に許容できる範囲にある、こ
とが分かった。本発明は、かかる事実の発見に基づいて
完成されたものである。
DISCLOSURE OF THE INVENTION The inventors of the present invention further studied in the above-mentioned Japanese Unexamined Patent Publication (Kokai) No. 4-192209, where "a desirable characteristic as a microwave dielectric cannot be obtained." Specifically, for a composition represented by the general formula (Pb m Ca 1-m ) (Sn 1-o Zr o ) O 3 , the composition ratio of Sn and Zr is set as a predetermined value, and the ratio of Pb and Ca is When changing, the temperature coefficient τ f of the resonance frequency tends to become a positive value from a negative value to ± 0 and cross a ± 0 value again to become a negative value as the ratio of Pb increases. Was discovered (see FIG. 2). The relative permittivity in the ratio of Pb and Ca near the point where τ f crosses ± 0 again and reaches a negative value again is Pb.
It has been found that the higher the ratio of (3), the more it tends to increase (see FIG. 3). In this case, the unloaded Q value tends to decrease as the Pb ratio increases (see FIG. 4), but in the microwave dielectric filter used in a relatively low frequency region, the value is within a sufficiently allowable range. I found out that there is. The present invention has been completed based on the discovery of such facts.

【0009】したがって、本発明の誘電体磁器組成物
は、酸化鉛、酸化カルシウム、酸化ジルコニウム及び酸
化スズからなる誘電体磁器組成物であって、各成分の組
成比が、一般式 (Pbm Ca1-m )(Sn1-o Zro )O3 で表したとき、m及びoがm−o平面において下記の
a,b,c,dを頂点とする領域内にある(ただし、o
=1.0の線上を除く)ことを特徴としている。 a; m=0.7 o=1.0 b; m=0.78 o=1.0 c; m=0.94 o=0.25 d; m=0.9 o=0.25
Therefore, the dielectric porcelain composition of the present invention is a dielectric porcelain composition comprising lead oxide, calcium oxide, zirconium oxide and tin oxide, and the composition ratio of each component is represented by the general formula (Pb m Ca 1-m ) (Sn 1-o Zr o ) O 3 , m and o are in the region having a, b, c, and d as vertices below in the m-o plane (provided that o is
= Except for the line of 1.0). a; m = 0.7 o = 1.0 b; m = 0.78 o = 1.0 c; m = 0.94 o = 0.25 d; m = 0.9 o = 0.25

【0010】上記のa,b,c,dを頂点とする領域内
(ただし、o=1.0の線上を除く)においてさらに好
ましい領域は、下記のa’,b’,c’,d’を頂点と
する領域又は/及びe,f,g,hを頂点とする領域
(ただし、o=1.0の線上を除く)である。 a’; m=0.745 o=1.0 b’; m=0.76 o=1.0 c’; m=0.875 o=0.5 d’; m=0.865 o=0.5 e; m=0.905 o=0.325 f; m=0.92 o=0.325 g; m=0.925 o=0.275 h; m=0.91 o=0.275
More preferable regions within the above-mentioned regions having a, b, c and d as vertices (except on the line of o = 1.0) are the following a ', b', c ', d'. Is a region having vertices or / and regions having vertices e, f, g and h (except on the line of o = 1.0). a '; m = 0.745 o = 1.0 b'; m = 0.76 o = 1.0 c '; m = 0.875 o = 0.5 d'; m = 0.865 o = 0 .5 e; m = 0.905 o = 0.325 f; m = 0.92 o = 0.325 g; m = 0.925 o = 0.275 h; m = 0.91 o = 0.275

【0011】[0011]

【作用】一般式PbZrO3 で表されるジルコン酸鉛の
ペブスカイト構造を基本として、Pbの一部のサイトを
Caで置換し、Zrの一部のサイトをSnで置換した磁
器組成物であって、上記組成範囲からなる本発明の誘電
体磁器組成物は、マイクロ波領域において従来材をはる
かに上回る特性を現出する。すなわち、上記組成範囲か
らなる誘電体磁器組成物は、比誘電率が100以上で、
かつ共振周波数の温度係数τf が100ppm /℃より小
さく、さらに無負荷Q値がマイクロ波領域で大きい、と
いう特徴を併せ持っている。
A porcelain composition based on the perovskite structure of lead zirconate represented by the general formula PbZrO 3, in which some sites of Pb are replaced by Ca and some sites of Zr are replaced by Sn. The dielectric ceramic composition of the present invention having the above composition range exhibits characteristics far superior to conventional materials in the microwave region. That is, the dielectric ceramic composition having the above composition range has a relative dielectric constant of 100 or more,
Moreover, the temperature coefficient τ f of the resonance frequency is smaller than 100 ppm / ° C., and the unloaded Q value is large in the microwave region.

【0012】 なお、(Pbm Ca1-m )(Sn1-o Zro )O3 で表される本発明の一部イオンを、Pb,Caサイトイ
オンのCaの一部若しくは全部をSr,Ba又はMgの
一種以上で、及び/又はSn,ZrサイトイオンのZr
の一部若しくは全部をTi又はHfの一種以上で置換し
ても、本発明の磁器組成物の特性と類似の傾向が期待で
き、高誘電率領域において比誘電率の温度係数τf が0
ppm /℃近傍に調整可能である。
It should be noted that some of the ions of the present invention represented by (Pb m Ca 1-m ) (Sn 1-o Zr o ) O 3 are used as Pb and Ca site ions, and some or all of Ca is Sr, One or more of Ba or Mg, and / or Zr of Sn, Zr site ion
Even if a part or all of the above is replaced with one or more of Ti or Hf, a tendency similar to the characteristics of the porcelain composition of the present invention can be expected, and the temperature coefficient τ f of relative permittivity in the high permittivity region is 0.
It can be adjusted to around ppm / ° C.

【0013】本発明において、組成物の一般式 (Pbm Ca1-m )(Sn1-o Zro )O3 を一般式 (Pbm Ca1-m X (Sn1-o Zro )O3 で表したとき、xが0.94≦x≦1.06の範囲にあ
れば、磁器組成物のペロブスカイト構造の骨格を阻害し
ないため、実用可能な誘電特性が保持され、かかる範囲
の組成物も本発明の組成物の範囲に含まれる。
In the present invention, the composition of the general formula (Pb m Ca 1-m ) (Sn 1-o Zr o ) O 3 is represented by the general formula (Pb m Ca 1-m ) x (Sn 1-o Zr o ). When represented by O 3 , if x is in the range of 0.94 ≦ x ≦ 1.06, it does not hinder the skeleton of the perovskite structure of the porcelain composition, so that practical dielectric properties are maintained and the composition in this range is maintained. Products are also included in the scope of the composition of the present invention.

【0014】[0014]

【実施例】出発原料として純度99.8%以上の、酸化
鉛(PbO)、炭酸カルシウム(CaCO3 )、酸化ス
ズ(SnO2 )及び酸化ジルコニウム(ZnO2 )を用
い、表1に示す組成比となるように秤量する。秤量した
これらの粉体をボールミルで20時間湿式混合(媒体は
純水を使用)する。これを乾燥後、ふた付きマグネシア
匣鉢に詰め、大気雰囲気中700℃〜1,000℃の温
度で3時間程度仮焼する。仮焼粉を再びボールミルで2
0時間湿式粉砕する。粉砕粉を乾燥後、バインダー(ポ
リビニルアルコール)を適量添加して練合し、35メッ
シュのふるいを通して整粒する。次に、3ton/cm2 の成
形圧で円板状(14φ、厚さ7mm)に成形する。この成
形体を600℃で1時間熱処理して脱脂後、ふた付きマ
グネシア匣鉢中で共粉に埋め込み、大気雰囲気中組成に
応じて850℃〜1,550℃の温度で3時間焼成す
る。焼成物の表面に鉛蒸散がある場合には、表面を研削
して取り除く。
EXAMPLES Lead oxide (PbO), calcium carbonate (CaCO 3 ), tin oxide (SnO 2 ) and zirconium oxide (ZnO 2 ) having a purity of 99.8% or higher were used as starting materials, and the composition ratios shown in Table 1 were used. Weigh so that These weighed powders are wet mixed with a ball mill for 20 hours (pure water is used as a medium). After this is dried, it is packed in a magnesia sagger with a lid and calcined in an air atmosphere at a temperature of 700 ° C to 1,000 ° C for about 3 hours. Calcination powder again in the ball mill 2
Wet mill for 0 hours. After the pulverized powder is dried, an appropriate amount of binder (polyvinyl alcohol) is added and kneaded, and the mixture is sized through a 35-mesh sieve. Next, it is molded into a disk shape (14φ, thickness 7 mm) with a molding pressure of 3 ton / cm 2 . This molded body is heat-treated at 600 ° C. for 1 hour to be degreased, then embedded in co-powders in a magnesia sagger with a lid, and fired for 3 hours at a temperature of 850 ° C. to 1,550 ° C. depending on the composition in the air atmosphere. If lead evaporates on the surface of the fired product, remove the surface by grinding.

【0015】得られた焼結体の誘電特性をHakki-Colema
らの方法により測定し、比誘電率εr 、無負荷Q値を求
めた(ここで、無負荷Q値は共振周波数(f)とおよそ
反比例の関係にあるため、以下明細書中では、これをか
けあわせQf値で示す)。共振周波数は2〜7GHzで
あった。共振周波数温度係数τf は、25℃の共振周波
数を基準にして、−30℃と80℃のときの共振周波数
温度係数を平均して求めた。これらの結果を表1に示
す。
The dielectric properties of the obtained sintered body were measured by Hakki-Colema
The relative permittivity ε r and the unloaded Q value were determined by the method described above (here, since the unloaded Q value and the resonance frequency (f) are approximately inversely proportional, Is shown as Qf value). The resonance frequency was 2 to 7 GHz. The resonance frequency temperature coefficient τ f was obtained by averaging the resonance frequency temperature coefficients at −30 ° C. and 80 ° C. with reference to the resonance frequency of 25 ° C. The results are shown in Table 1.

【0016】[0016]

【表1】 [Table 1]

【0017】なお、酸化スズ(SnO2 )は組成物の焼
成を阻害する場合もあり、このような場合には、CaS
nO3 の形で添加しても、酸化物を出発原料とした場合
と同様の特性を期待できる。
Note that tin oxide (SnO 2 ) may interfere with the firing of the composition. In such a case, CaS
Even when added in the form of nO 3 , the same characteristics as when an oxide is used as a starting material can be expected.

【0018】表1から明らかなように、本発明の組成範
囲にある組成物(実施例1〜10)では、比誘電率が1
00以上と高く、Qf値が800以上の値を示し、かつ
共振周波数温度係数の絶対値が100ppm /℃以下であ
り、マイクロ波用誘電体組成物として優れた特性を有す
ることが分かる。これに対し、本発明の組成範囲外にあ
る組成物(比較例11〜21)では、比誘電率が100
以下であるか、Qf値が700以下であるか、共振周波
数温度係数の絶対値が100ppm /℃を越えるかのいず
れかであり、マイクロ波用誘電体組成物として望ましい
ものとは言えない。
As is apparent from Table 1, in the compositions within the composition range of the present invention (Examples 1 to 10), the relative dielectric constant was 1.
It is as high as 00 or more, the Qf value is 800 or more, and the absolute value of the resonance frequency temperature coefficient is 100 ppm / ° C. or less, and it is understood that the dielectric composition for microwaves has excellent characteristics. On the other hand, in the compositions outside the composition range of the present invention (Comparative Examples 11 to 21), the relative dielectric constant was 100.
It is either less than or equal to, the Qf value is less than or equal to 700, or the absolute value of the temperature coefficient of the resonance frequency exceeds 100 ppm / ° C., which is not desirable as a dielectric composition for microwaves.

【0019】図1は本発明の誘電体磁器組成物の組成範
囲を示すグラフであり、斜線で示した領域が本発明の組
成範囲である。なお、図に示した番号は表1の番号と対
応する。
FIG. 1 is a graph showing the composition range of the dielectric ceramic composition of the present invention, and the shaded region is the composition range of the present invention. The numbers shown in the figure correspond to the numbers in Table 1.

【0020】図2は組成と共振周波数温度係数τf との
関係を示すグラフであり、組成式 (Pbm Ca1-m )(Sn1-o Zro )O3 において、oを所定の値としmを種々変化させた組成物
における共振周波数温度係数τf の変化の様子を示す。
図2から分かるように、共振周波数温度係数τfは、m
が0.6〜0.7付近より小さいときは負の値を示し、
mが0.6〜0.7近傍で±0を横切り、さらにmが増
すと正の値となってmの増加とともに次第にその値を増
してピークに達したのち、再び±0を横切って負の値と
なる傾向を示すことが分かる。
FIG. 2 is a graph showing the relationship between the composition and the temperature coefficient τ f of the resonance frequency. In the composition formula (Pb m Ca 1-m ) (Sn 1-o Zr o ) O 3 , o is a predetermined value. Shows the changes in the resonance frequency temperature coefficient τ f in the compositions in which m is variously changed.
As can be seen from FIG. 2, the resonance frequency temperature coefficient τ f is m
Shows a negative value when is less than around 0.6 to 0.7,
m crosses ± 0 in the vicinity of 0.6 to 0.7, and when m further increases, it becomes a positive value and gradually increases as m increases and reaches a peak, then crosses ± 0 again and becomes negative. It can be seen that there is a tendency that the value becomes.

【0021】図3は組成と比誘電率εr との関係を示す
グラフであり、図2において説明したと同様に、oを所
定の値としmを種々変化させた組成物における比誘電率
εrの変化の様子を示す。図2の共振周波数温度係数τ
f が±0から正の値を示しピークに達し再び±0を横切
る辺りに対応する領域では、比誘電率εr はmの増加と
ともにさらに増加を続けピークに達したのち漸次減少し
ていく傾向がある。かかる領域で、εr は概ね100以
上の高い値を示していることが分かる。
FIG. 3 is a graph showing the relationship between the composition and the relative permittivity ε r . Similarly to the case described with reference to FIG. 2, the relative permittivity ε of the composition in which m is variously changed with the predetermined value of o. This shows how r changes. Resonance frequency temperature coefficient τ in FIG.
In the region where f shows a positive value from ± 0, reaches a peak, and crosses ± 0 again, the relative permittivity ε r continues to increase as m increases, reaches a peak, and then gradually decreases. There is. It can be seen that ε r exhibits a high value of approximately 100 or more in this region.

【0022】図4は組成とQf値との関係を示すグラフ
であり、oを所定の値としmを種々変化させた組成物に
おけるQf値の変化の様子を示す。図4から分かるよう
に、mが0.7 以上の領域で、Qf値は減少傾向にある
が、なおQf値は高い値を示し、マイクロ波領域に用い
る誘電体として許容できる値を示す範囲のあることが分
かる。
FIG. 4 is a graph showing the relationship between the composition and the Qf value, and shows how the Qf value changes in a composition in which o is a predetermined value and m is variously changed. As can be seen from FIG. 4, the Qf value tends to decrease in the region where m is 0.7 or more, but the Qf value still shows a high value, and there is a range in which the value is acceptable as a dielectric used in the microwave region. I understand.

【0023】このような事実から、τf の絶対値が10
0ppm /℃以下、εr が100以上及びQf値が800
以上の値を同時に示す組成領域を選定することにより、
優れたマイクロ波誘電体組成物を得ることができること
が分かる。
From these facts, the absolute value of τ f is 10
0ppm / ℃ or less, ε r is 100 or more and Qf value is 800
By selecting the composition region showing the above values at the same time,
It can be seen that an excellent microwave dielectric composition can be obtained.

【0024】[0024]

【発明の効果】本発明にかかる誘電体磁器組成物は、酸
化鉛、酸化カルシウム、酸化ジルコニウム及び酸化スズ
からなり、その組成比を所定範囲に限定してなるので、
比誘電率が高く、かつ共振周波数温度係数τf の小さな
高誘電率材であり、高周波帯域にも用いることができ
る。本発明の誘電体磁器組成物を誘電体共振器や基板な
どに用いることにより、マイクロ波用通信機のさらなる
小型化を実現することができる等その工業的価値は大き
いものである。
The dielectric ceramic composition according to the present invention comprises lead oxide, calcium oxide, zirconium oxide and tin oxide, and its composition ratio is limited to a predetermined range.
It is a high dielectric constant material having a high relative permittivity and a small resonance frequency temperature coefficient τ f , and can be used in a high frequency band. By using the dielectric ceramic composition of the present invention for a dielectric resonator, a substrate, etc., it is possible to realize further miniaturization of a microwave communication device, and its industrial value is great.

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

【図1】本発明の誘電体磁器組成物の組成範囲を示すグ
ラフ。
FIG. 1 is a graph showing a composition range of a dielectric ceramic composition of the present invention.

【図2】組成と共振周波数温度係数τf との関係を示す
グラフ。
FIG. 2 is a graph showing the relationship between composition and resonance frequency temperature coefficient τ f .

【図3】組成と比誘電率εr との関係を示すグラフ。FIG. 3 is a graph showing the relationship between composition and relative permittivity ε r .

【図4】組成とQf値との関係を示すグラフ。FIG. 4 is a graph showing the relationship between composition and Qf value.

【手続補正書】[Procedure amendment]

【提出日】平成5年9月3日[Submission date] September 3, 1993

【手続補正1】[Procedure Amendment 1]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0010[Correction target item name] 0010

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0010】 上記のa,b,c,dを頂点とする領域
内(ただし、o=1.0の線上を除く)においてさらに
好ましい領域は、下記のa’,b’,c’,d’を頂点
とする領域又は/及びe,f,g,hを頂点とする領域
(ただし、o=1.0の線上を除く)である。 a’; m=0.745 o=1.0 b’; m=0.76 o=1.0 c’; m=0.875 o=0.5 d’; m=0.865 o=0.5 e; m=0.905 o=0.325 f; m=0.92 o=0.325 g; m=0.925 o=0.275 h; m=0.91 o=0.275これらa’,b’,c’,d’を頂点とする領域内と
e,f,g,hを頂点とする領域内では、特に共振周波
数の温度係数τが0近辺にあり、共振周波数の温度変
化を小さくおさえることができ好ましい。
Within the above-mentioned region having a, b, c, and d as vertices (except on the line of o = 1.0), more preferable regions are the following a ′, b ′, c ′, and d ′. Is a region having vertices or / and regions having vertices e, f, g and h (except on the line of o = 1.0). a '; m = 0.745 o = 1.0 b'; m = 0.76 o = 1.0 c '; m = 0.875 o = 0.5 d'; m = 0.865 o = 0 .5 e; m = 0.905 o = 0.325 f; m = 0.92 o = 0.325 g; m = 0.925 o = 0.275 h; m = 0.91 o = 0.275 In the area with these a ', b', c ', d'as vertices
Resonance frequency is especially high in the region with vertices e, f, g, and h.
The temperature coefficient τ f of the number is near 0,
This is preferable because it can be suppressed to be small.

【手続補正2】[Procedure Amendment 2]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0011[Correction target item name] 0011

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0011】[0011]

【作用】 一般式PbZrOで表されるジルコン酸鉛
のペブスカイト構造を基本として、Pbの一部のサイト
をCaで置換し、Zrの一部のサイトをSnで置換した
磁器組成物であって、上記組成範囲からなる本発明の誘
電体磁器組成物は、マイクロ波領域において従来材をは
るかに上回る特性を現出する。すなわち、上記組成範囲
からなる誘電体磁器組成物は、比誘電率が100以上
で、かつ共振周波数の温度係数τ の絶対値が100p
pm/℃以下、さらに無負荷Q値がマイクロ波領域で大
きい(具体的にはQf値が800以上)、という特徴を
併せ持っている。
A porcelain composition based on the perovskite structure of lead zirconate represented by the general formula PbZrO 3 in which some sites of Pb are replaced by Ca and some sites of Zr are replaced by Sn. The dielectric ceramic composition of the present invention having the above composition range exhibits characteristics far superior to conventional materials in the microwave region. That is, the dielectric ceramic composition having the above composition range has a relative dielectric constant of 100 or more and an absolute value of the temperature coefficient τ f of the resonance frequency of 100 p.
It also has the characteristics that it is pm / ° C. or less and that the unloaded Q value is large in the microwave region (specifically, the Qf value is 800 or more) .

【手続補正3】[Procedure 3]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0019[Correction target item name] 0019

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0019】 上記表1に示した実施例1〜10及び比
較例11〜21の組成物の組成をグラフ上にプロットす
ると図1に示したようになる。ここで、図に示した番号
が表1に示した番号に対応している。そして、表1に示
した誘電特性値から分かるように、実施例1〜10の組
成物では、共振周波数の温度係数τの絶対値が100
ppm/℃以下、比誘電率εが100以上、無負荷Q
値(Qf値)が800以上の特性値を同時に満たし、ま
たこれらの誘電特性の限界値に対しτ,ε,Qf値
は余裕がある。そこで、これら実施例1〜10の組成を
含み、実施例1〜10の組成に近い範囲、即ち、図1の
a,b,c,dを結ぶ線で囲んだ領域を定め(a,b,
c,dにおけるm及びoの値は上述した値と同じ。)、
本発明の組成物の組成領域とした。
Examples 1 to 10 and ratios shown in Table 1 above
Plot the composition of the compositions of Comparative Examples 11-21 on a graph
Then, it becomes as shown in FIG. Where the numbers shown in the figure
Corresponds to the number shown in Table 1. And shown in Table 1
As can be seen from the dielectric property values obtained,
In the product, the absolute value of the temperature coefficient τ f of the resonance frequency is 100.
ppm / ° C or less, relative permittivity ε r of 100 or more, no load Q
The value (Qf value) simultaneously satisfies the characteristic value of 800 or more,
The τ f , ε r , and Qf values for the limit values of these dielectric properties
Can afford. Therefore, the compositions of Examples 1 to 10 are
In the range close to the composition of Examples 1 to 10, that is, in FIG.
A region surrounded by a line connecting a, b, c, d is defined (a, b,
The values of m and o in c and d are the same as those described above. ),
The compositional area of the composition of the present invention was defined as this.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 石黒 靖江 東京都港区新橋5丁目36番11号 富士電気 化学株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Yasue Ishiguro 5-36-11 Shimbashi, Minato-ku, Tokyo Fuji Electric Chemical Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】酸化鉛、酸化カルシウム、酸化ジルコニウ
ム及び酸化スズからなる誘電体磁器組成物であって、各
成分の組成比が、一般式 (Pbm Ca1-m )(Sn1-o Zro )O3 で表したとき、m及びoがm−o平面において下記の
a,b,c,dを頂点とする領域内にある(ただし、o
=1.0の線上を除く)ことを特徴とする誘電体磁器組
成物。 a; m=0.7 o=1.0 b; m=0.78 o=1.0 c; m=0.94 o=0.25 d; m=0.9 o=0.25
1. A dielectric ceramic composition comprising lead oxide, calcium oxide, zirconium oxide and tin oxide, wherein the composition ratio of each component is represented by the general formula (Pb m Ca 1-m ) (Sn 1-o Zr o ) When represented by O 3 , m and o are in the region having the following a, b, c, and d as vertices in the m-o plane (provided that o is
= Except 1.0 on the line). a; m = 0.7 o = 1.0 b; m = 0.78 o = 1.0 c; m = 0.94 o = 0.25 d; m = 0.9 o = 0.25
JP4361286A 1992-12-30 1992-12-30 Dielectric porcelain composition Pending JPH06203631A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4361286A JPH06203631A (en) 1992-12-30 1992-12-30 Dielectric porcelain composition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4361286A JPH06203631A (en) 1992-12-30 1992-12-30 Dielectric porcelain composition

Publications (1)

Publication Number Publication Date
JPH06203631A true JPH06203631A (en) 1994-07-22

Family

ID=18472954

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4361286A Pending JPH06203631A (en) 1992-12-30 1992-12-30 Dielectric porcelain composition

Country Status (1)

Country Link
JP (1) JPH06203631A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10861516B2 (en) 2018-07-17 2020-12-08 Samsung Electronics Co., Ltd. Semiconductor memory device and operating method of semiconductor memory device
CN115417670A (en) * 2022-09-28 2022-12-02 昆明理工大学 High-dielectric-constant ceramic with high-entropy design at B site and preparation method thereof
CN115872735A (en) * 2022-11-18 2023-03-31 广东工业大学 Zirconium tin hafnate lanthanum lead ceramic and preparation method and energy storage application thereof

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10861516B2 (en) 2018-07-17 2020-12-08 Samsung Electronics Co., Ltd. Semiconductor memory device and operating method of semiconductor memory device
US11342011B2 (en) 2018-07-17 2022-05-24 Samsung Electronics Co., Ltd. Semiconductor memory device and operating method of semiconductor memory device to reduce duty errors
CN115417670A (en) * 2022-09-28 2022-12-02 昆明理工大学 High-dielectric-constant ceramic with high-entropy design at B site and preparation method thereof
CN115417670B (en) * 2022-09-28 2023-03-10 昆明理工大学 High-dielectric-constant ceramic with high-entropy design at B site and preparation method thereof
CN115872735A (en) * 2022-11-18 2023-03-31 广东工业大学 Zirconium tin hafnate lanthanum lead ceramic and preparation method and energy storage application thereof
CN115872735B (en) * 2022-11-18 2024-01-16 广东工业大学 Zirconium tin hafnium lanthanum lead acid ceramic, preparation method and energy storage application thereof

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