JPH0680564B2 - High dielectric constant dielectric ceramic composition - Google Patents

High dielectric constant dielectric ceramic composition

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Publication number
JPH0680564B2
JPH0680564B2 JP60238337A JP23833785A JPH0680564B2 JP H0680564 B2 JPH0680564 B2 JP H0680564B2 JP 60238337 A JP60238337 A JP 60238337A JP 23833785 A JP23833785 A JP 23833785A JP H0680564 B2 JPH0680564 B2 JP H0680564B2
Authority
JP
Japan
Prior art keywords
dielectric
temperature
ceramic composition
dielectric constant
composition
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
Application number
JP60238337A
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Japanese (ja)
Other versions
JPS6297205A (en
Inventor
宣雄 横江
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Kyocera Corp
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Kyocera Corp
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Publication date
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Priority to JP60238337A priority Critical patent/JPH0680564B2/en
Publication of JPS6297205A publication Critical patent/JPS6297205A/en
Publication of JPH0680564B2 publication Critical patent/JPH0680564B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は磁器コンデンサ、特に低温焼成ができる積層型
磁器コンデンサの高誘電率系誘電体磁器組成物に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial application] The present invention relates to a high dielectric constant dielectric ceramic composition of a ceramic capacitor, particularly a laminated ceramic capacitor capable of low temperature firing.

〔従来の技術〕[Conventional technology]

従来、一般に積層型磁器コンデンサは表面に内部電極が
塗布されたシート状のBaTiO3(チタン酸バリウム)を主
成分とする誘電体を複数枚積層するとともに各シートの
内部電極を交互に並列に一対の外部接続用電極に接続
し、これを焼結一体化することにより形成されている。
このような積層型磁器コンデンサは近年のエレクトロニ
クスの進展に伴い電子部品の小型化が急速に進行し、広
範な電子回路に使用されるようになってきている。
Conventionally, generally, a laminated porcelain capacitor is formed by laminating a plurality of sheet-like dielectrics containing BaTiO 3 (barium titanate) as a main component with internal electrodes coated on the surface and alternately pairing the internal electrodes of each sheet in parallel. It is formed by connecting it to the external connection electrode and sintering and integrating it.
Such multilayer ceramic capacitors have been rapidly used in a wide variety of electronic circuits due to rapid miniaturization of electronic parts with the recent progress of electronics.

しかしながら、この従来のBaTiO3を主成分とする誘電体
材料は1250℃〜1350℃の高温で焼成する必要があり、こ
の材料を積層型磁器コンデンサの誘電体として使用した
場合、内部電極は前記誘電体の焼成温度にて溶融するこ
となく、かつ酸化することがない高価な貴金属であるパ
ラジウム(融点1555℃)またはその合金が使用されるこ
とから、特に静電容量が大きいものでは内部電極数が大
となりコスト高となるため、上記従来の積層型磁器コン
デンサは容量効率が高く、その他誘電的特性に優れかつ
高信頼性にあるにも拘わらず価格面がその進展に大きな
障害となっていた。従って銀(融点960℃)、銅(融点1
083℃)などの安価な金属を内部電極として使用するた
めには、低温とりわけ950℃以下で焼結する高誘電率の
誘電体材料が強く望まれていた。
However, this conventional BaTiO 3 -based dielectric material must be fired at a high temperature of 1250 ° C to 1350 ° C, and when this material is used as the dielectric of a laminated ceramic capacitor, the internal electrodes are Since expensive precious metal palladium (melting point 1555 ° C) or its alloy that does not melt at the firing temperature of the body and does not oxidize is used, the number of internal electrodes is particularly large for those with large capacitance. Since the cost is large and the cost is high, the conventional multilayer ceramic capacitor has high capacity efficiency, excellent dielectric properties, and high reliability, but the price is a major obstacle to its progress. Therefore, silver (melting point 960 ℃), copper (melting point 1
In order to use an inexpensive metal such as (083 ° C.) as an internal electrode, a dielectric material having a high dielectric constant that is sintered at a low temperature, particularly at 950 ° C. or lower, has been strongly desired.

近年、高誘電率系誘電体において、1000℃以下の低温で
焼結できる磁器組成物としていくつかの提案がなされて
いる。それらは低温で焼結できる強誘電体として、Pb(F
e1/2Nb1/2)O3、Pb(Fe2/3W1/3)O3、Pb(Mg1/2W1/2)O3、Pb
(Zn1/3Nb2/3)O3、Pb(Mg1/3Nb2/3)O3、Pb(Ni1/3Nb2/3)
O3、およびPbTiO3のうち二成分または三成分を組合せ、
室温における所望の誘電特性を得ようとしたものであ
る。しかしながら、これらは比誘電率が大きい場合は、
誘電損失が大きかったり、あるいは絶縁抵抗が小さいな
どの欠点を有していた。更には、合成成分がいずれも強
誘電体であることからキュリー温度およびキュリー温度
近くの低い温度域での誘電損失が極めて大きいという原
理的な欠点を避けることができない。
In recent years, several proposals have been made as a porcelain composition which can be sintered at a low temperature of 1000 ° C. or less in a high dielectric constant type dielectric. They are Pb (F
e 1/2 Nb 1/2 ) O 3 , Pb (Fe 2/3 W 1/3 ) O 3 , Pb (Mg 1/2 W 1/2 ) O 3 , Pb
(Zn 1/3 Nb 2/3 ) O 3 , Pb (Mg 1/3 Nb 2/3 ) O 3 , Pb (Ni 1/3 Nb 2/3 )
A combination of two or three components of O 3 and PbTiO 3 ,
It is intended to obtain desired dielectric properties at room temperature. However, when the relative dielectric constant is large,
It has drawbacks such as large dielectric loss and small insulation resistance. Furthermore, since the synthetic components are all ferroelectrics, the theoretical defect that the dielectric loss is extremely large in the Curie temperature and a low temperature region near the Curie temperature cannot be avoided.

因みに特開昭52-21699号公報に開示された〔SrxPb1-xTi
O3A〔Pb(Mg1/2W1/2)O31-Aにおいて×=0〜0.10,A
=0.35〜0.50なる組成物が実用化され、上記組成物の誘
電体粉末が市販されている。しかしながら、この組成系
においては1000℃以下の低温度で焼結でき、かつ優れた
絶縁抵抗等を有する利点はあるものの誘電損失が1.5%
程度であり、積層型磁器コンデンサとして適用する場
合、誘電損失が少なくとも1%以下であるという条件を
満足しない。
Incidentally, it was disclosed in Japanese Patent Laid-Open No. 52-21699 [Sr x Pb 1-x Ti
O 3 ] A [Pb (Mg 1/2 W 1/2 ) O 3 ] 1-A × = 0 to 0.10, A
= 0.35-0.50 has been put into practical use, and dielectric powders of the above composition are commercially available. However, this composition system has the advantages that it can be sintered at a low temperature of 1000 ° C or less and that it has excellent insulation resistance, but the dielectric loss is 1.5%.
However, when applied as a laminated ceramic capacitor, the condition that the dielectric loss is at least 1% or less is not satisfied.

〔発明の目的〕[Object of the Invention]

本発明は前記欠点に鑑み種々の実験の結果案出されたも
のであって、強誘電体であるPb(Fe1/2Nb1/2)O3に対し
て、これと同一結晶構造のペロブスカイト構造を有する
低温度で焼結できる常誘電体であるBa(Cr1/2Nb1/2)O3
固溶させることによりPb(Fe1/2Nb1/2)O3が本来有する誘
電特性を改質し誘電損失が小さく絶縁抵抗が大きい、更
には比誘電率の温度依存性が良好な優れた高誘電率系誘
電体磁器組成物を提供することにある。
The present invention has been devised as a result of various experiments in view of the above-mentioned drawbacks, and for Pb (Fe 1/2 Nb 1/2 ) O 3 which is a ferroelectric substance, a perovskite having the same crystal structure as that of Pb (Fe 1/2 Nb 1/2 ) O 3 . Dielectric property of Pb (Fe 1/2 Nb 1/2 ) O 3 originally obtained by solid solution of Ba (Cr 1/2 Nb 1/2 ) O 3 which is a paraelectric material with a structure that can be sintered at low temperature An object of the present invention is to provide an excellent high-dielectric-constant dielectric porcelain composition that has improved characteristics and has a small dielectric loss, a large insulation resistance, and a good temperature dependence of the relative dielectric constant.

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

本発明の高誘電率系誘電体磁器組成物は組成式がPb(Fe
1/2-xSmxNb1/2)O3で表される組成物において、×が0.02
1≦×≦0.070の範囲にあることを特徴とするものであ
る。
The high dielectric constant dielectric ceramic composition of the present invention has a composition formula of Pb (Fe
In the composition represented by 1 / 2-x Sm x Nb 1/2 ) O 3 , x is 0.02
It is characterized by being in the range of 1 ≦ × ≦ 0.070.

なお、Xの範囲を上記の範囲に限定した理由は、磁器コ
ンデンサ、特に積層型磁器コンデンサとして要求される
誘電特性、即ち比誘電率が7500以上、誘電損失が1.00
%、絶縁抵抗が3.0×1011Ω・cm以上かつ比誘電率の温
度依存性が良好であらねばならないという誘電特性のい
ずれかを満足しないためであり、0.021>Xの場合、比
誘電率が7500未満、かつ比誘電率の温度依存性が大き
く、X>0.070の場合、比誘電率が7500未満、絶縁抵抗
が3.0×1011Ω・cm未満といずれも誘電特性を満足しな
いためである。
The reason why the range of X is limited to the above range is that the dielectric characteristics required for a porcelain capacitor, particularly a laminated porcelain capacitor, that is, the relative dielectric constant is 7500 or more and the dielectric loss is 1.00.
%, The insulation resistance is 3.0 × 10 11 Ω · cm or more, and the temperature dependence of the relative permittivity must be good. Either of the dielectric properties must be satisfied. If 0.021> X, the relative permittivity is This is because the dielectric properties are less than 7500 and the temperature dependence of the relative permittivity is large, and when X> 0.070, the relative permittivity is less than 7500 and the insulation resistance is less than 3.0 × 10 11 Ω · cm, which do not satisfy the dielectric properties.

〔実施例〕〔Example〕

次に本発明を実施例に基づき説明する。 Next, the present invention will be described based on examples.

出発原料としてPbO2,Fe2O3,Nb2O5,およびSm2O3を第1
表の組成比となる様にそれぞれ秤量し、分散剤および分
散媒とともにボールミルにて湿式混合した後、この原料
スラリーを乾燥し、950℃の温度で3時間仮焼した。次
いでこの仮焼物を粗砕後、振動ミルにて微粉砕し、得ら
れた平均粒径0.7〜0.8μmの微粉末にポリビニルアルコ
ールを重量で約1%添加して顆粒状に造粒した後、約90
0Kg/cm2の圧力で直径約12mm、厚さ1.0mmの円板状に成形
した。この円板状成形体のポリビニルアルコールを500
℃にて焼失せしめた後、900℃〜950℃の温度で2時間、
酸素を含む雰囲気で焼成した。
PbO 2 , Fe 2 O 3 , Nb 2 O 5 , and Sm 2 O 3 were the first starting materials.
Each was weighed so as to have the composition ratio shown in the table, wet-mixed with a dispersant and a dispersion medium in a ball mill, and then this raw material slurry was dried and calcined at a temperature of 950 ° C. for 3 hours. Then, this calcined product was roughly crushed and then finely crushed with a vibration mill, and about 1% by weight of polyvinyl alcohol was added to the obtained fine powder having an average particle size of 0.7 to 0.8 μm to form granules. About 90
It was formed into a disk shape having a diameter of about 12 mm and a thickness of 1.0 mm at a pressure of 0 Kg / cm 2 . Polyvinyl alcohol of this disk-shaped molded body is 500
After burning out at ℃, 2 hours at a temperature of 900 ℃ ~ 950 ℃,
It was fired in an atmosphere containing oxygen.

最後に、得られた円板状焼成体の上下両面に銀電極を80
0℃にて焼付けた。同様にして強誘電体であるPb(Fe2/3W
1/3)O3に、同じ強誘電体であるPb(Fe1/2Nb1/2)O3を固溶
させた組成式がPb(Fe2/3W1/3)x(Fe1/2Nb1/2)1-xO3で表
され、X=0.5の誘電体磁器組成物を比較例とした。こ
うして得た円板状のコンデンサ試料の諸特性を第1表に
示す。
Finally, 80 silver electrodes were formed on the upper and lower surfaces of the obtained disc-shaped fired body.
It was baked at 0 ° C. Similarly, the ferroelectric substance Pb (Fe 2/3 W
The composition formula of Pb (Fe 1/2 Nb 1/2 ) O 3 which is the same ferroelectric substance in 1/3 ) O 3 as a solid solution is Pb (Fe 2/3 W 1/3 ) x (Fe 1 A dielectric ceramic composition represented by / 2 Nb 1/2 ) 1-x O 3 and having X = 0.5 was used as a comparative example. Various characteristics of the disk-shaped capacitor sample thus obtained are shown in Table 1.

但し、表中の比誘電率は1.0KHz、1.0Vrmsの入力信号を
用いてキャパシタンスブリッジにて測定した室温での静
電容量値と試料の寸法から計算した値を示し、誘電損失
(tanδ)は室温での1.0KHx1.0Vrmsの入力信号における
測定値を示す。また絶縁抵抗は、絶縁抵抗計にて直流電
圧250Vを印加して1分後の値と試料の寸法から体積抵抗
率(Ω・cm)を計算した値を示し、比誘電率の温度特性
は、−30℃、+25℃、+85℃の各温度において上記と同
様の条件にて静電容量を測定し、+25℃での静電容量に
対する各温度での静電容量の変化率を算出し、ε-30
ε25およびε85/ε25として示した。
However, the relative permittivity in the table shows the value calculated from the capacitance value at room temperature measured by the capacitance bridge using the input signal of 1.0 KHz and 1.0 Vrms and the sample size, and the dielectric loss (tan δ) is Measured value at input signal of 1.0KHx1.0Vrms at room temperature. The insulation resistance is a value obtained by applying a DC voltage of 250 V with an insulation resistance tester after 1 minute and the volume resistivity (Ω · cm) calculated from the dimensions of the sample. The temperature characteristic of the relative permittivity is Measure the capacitance under the same conditions as above at each temperature of -30 ℃, + 25 ℃, and + 85 ℃, and calculate the rate of change of the capacitance at each temperature with respect to the capacitance at + 25 ℃. -30 /
It is shown as ε 25 and ε 85 / ε 25 .

第1表から明らかなように、試料番号1は比誘電比率が
小さく、比誘電率の温度依存性が極めて大きく、試料番
号12は比誘電率が小さく、かつ絶縁抵抗が低くなってい
る。また比較例では誘電損失が極めて大きく、絶縁抵抗
も極めて低く、いずれも実用的な誘電特性が得られてい
ない。
As is clear from Table 1, Sample No. 1 has a small relative permittivity and extremely large temperature dependence of the relative permittivity, and Sample No. 12 has a small relative permittivity and a low insulation resistance. Further, in the comparative examples, the dielectric loss is extremely large and the insulation resistance is extremely low, and practical dielectric characteristics are not obtained in any of the examples.

それに対し、本発明の請求範囲内の誘電体磁器組成物は
比誘電率が8250〜16760と十分大きく、誘電損失(Tan
δ)も0.13〜0.57と小さく、絶縁抵抗(Ω・cm)は5.8
×1011〜3.3×1012と非常に大きくかつ前述の比誘電率
の温度特性も良好でいずれも優れた誘電特性を有してい
るが、とりわけ試料番号5乃至8がより望ましいことが
理解される。
On the other hand, the dielectric ceramic composition within the scope of the claims of the present invention has a sufficiently high relative dielectric constant of 8250 to 16760, and thus the dielectric loss (Tan
δ) is as small as 0.13 to 0.57, and the insulation resistance (Ω · cm) is 5.8.
It is very large as × 10 11 to 3.3 × 10 12 and the temperature characteristics of the above-mentioned relative permittivity are good, and all have excellent dielectric characteristics, but it is understood that sample numbers 5 to 8 are more preferable. It

〔発明の効果〕〔The invention's effect〕

本発明の請求範囲内の誘電体磁器組成物は、比誘電率、
誘電損失(Tanδ)、絶縁抵抗(Ω・cm)、比誘電率の
温度特性のいずれの特性においても満足し得るものであ
る。
The dielectric ceramic composition within the scope of the present invention has a relative permittivity,
All of the dielectric loss (Tanδ), insulation resistance (Ω · cm), and relative dielectric constant temperature characteristics are satisfactory.

また、本発明において、焼成温度が900℃〜950℃の範囲
で焼成することができ、かつ焼結磁器の誘電特性を全て
満足するものであることから、銀および銅などの安価な
金属を内部電極とする積層型磁器コンデンサの誘電体磁
器として十分実用性のあることが理解される。
Further, in the present invention, since the firing temperature can be fired in the range of 900 ° C to 950 ° C, and all the dielectric characteristics of the sintered porcelain are satisfied, inexpensive metals such as silver and copper can be used internally. It is understood that it is sufficiently practical as a dielectric porcelain of a laminated porcelain capacitor used as an electrode.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】組成式が、 Pb(Fe1/2-xSmx Nb1/2)O3 で表される組成物において、×が0.021≦×≦0.070の範
囲にあることを特徴とする高誘電率系誘電体磁器組成
物。
1. A composition represented by Pb (Fe 1 / 2-x Sm x Nb 1/2 ) O 3 wherein x is in the range of 0.021 ≦ × ≦ 0.070. High dielectric constant dielectric ceramic composition.
JP60238337A 1985-10-23 1985-10-23 High dielectric constant dielectric ceramic composition Expired - Lifetime JPH0680564B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60238337A JPH0680564B2 (en) 1985-10-23 1985-10-23 High dielectric constant dielectric ceramic composition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60238337A JPH0680564B2 (en) 1985-10-23 1985-10-23 High dielectric constant dielectric ceramic composition

Publications (2)

Publication Number Publication Date
JPS6297205A JPS6297205A (en) 1987-05-06
JPH0680564B2 true JPH0680564B2 (en) 1994-10-12

Family

ID=17028701

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60238337A Expired - Lifetime JPH0680564B2 (en) 1985-10-23 1985-10-23 High dielectric constant dielectric ceramic composition

Country Status (1)

Country Link
JP (1) JPH0680564B2 (en)

Also Published As

Publication number Publication date
JPS6297205A (en) 1987-05-06

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