JPH0680467A - Dielectric ceramic composition - Google Patents

Dielectric ceramic composition

Info

Publication number
JPH0680467A
JPH0680467A JP4230939A JP23093992A JPH0680467A JP H0680467 A JPH0680467 A JP H0680467A JP 4230939 A JP4230939 A JP 4230939A JP 23093992 A JP23093992 A JP 23093992A JP H0680467 A JPH0680467 A JP H0680467A
Authority
JP
Japan
Prior art keywords
composition
dielectric ceramic
dielectric
ceramic composition
resonance 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.)
Pending
Application number
JP4230939A
Other languages
Japanese (ja)
Inventor
Takuya Fujimaru
琢也 藤丸
Takehiko Yoneda
毅彦 米田
Hiromi Tokunaga
裕美 徳永
Hiromitsu Tagi
宏光 多木
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP4230939A priority Critical patent/JPH0680467A/en
Publication of JPH0680467A publication Critical patent/JPH0680467A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To produce a dielectric magnetic composition having excellent characteristics such as high dielectric constant (60-110), high no-load Q (>=2000) and low resonance frequency temperature factor (tauf) (<=100ppm/ deg.C) in dielectric resonators and electronic equipment used in microwave band. CONSTITUTION:A dielectric ceramic composition expressed by the formula xBaO.yTiO2.zNd2O3.tSm2O3.wBi2O3 having mole fractions in the following ranges: 0.06<=(x)<=0.155, 0.69<=(y)<=0.80, 0.05<=(z)<=0.18, 0<(t)<=0.07, 0<(w)<=0.05 [(x)+(y)+(z)+(t)+(w)=1]. In this composition, one or more kinds of Al2O3 and ZrO2, etc., may be added as additives or a part of Ba of the dielectric ceramic composition may be replaced with other element. The purity of Sm2O3 and Nd2O3 required is >=70wt.%.

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、誘電体共振器及び電子
機器に使用される誘電体基板等の材料として利用される
誘電体磁器組成物に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a dielectric ceramic composition used as a material for a dielectric resonator and a dielectric substrate used for electronic equipment.

【0002】[0002]

【従来の技術】従来、高周波領域において、誘電体はマ
イクロ波回路のインピーダンス整合や、誘電体共振器等
に応用されてきている。特に、近年マイクロ波回路の集
積化の技術が進歩するに伴い、バンドパスフィルタや発
振器の周波数安定化等に、高誘電率、低損失の誘電体磁
器を用いた誘電体共振器を使用して小型化することが積
極的に進められており、高誘電率で無負荷Qが大きく、
共振周波数温度係数(τf)が小さく、かつ、それぞれ
の特性を広範囲に変化させることができる誘電体磁器組
成物が要求されている。
2. Description of the Related Art Heretofore, in the high frequency region, dielectrics have been applied to impedance matching of microwave circuits, dielectric resonators and the like. In particular, as the technology for integrating microwave circuits has advanced in recent years, a dielectric resonator using a dielectric ceramic with a high dielectric constant and low loss is used for frequency stabilization of bandpass filters and oscillators. The miniaturization is being actively promoted, the high dielectric constant and the large unloaded Q,
There is a demand for a dielectric porcelain composition having a small resonance frequency temperature coefficient (τf) and capable of varying the respective characteristics in a wide range.

【0003】そこで、これらの誘電体材料としては、B
aO−TiO2系誘電体磁器〔H.M.O,Bryan,Jr.,Thomso
n,Jr.and J.K.Plourde:J.Am.Ceram.Soc.57(1974)450〕
及びその一部を他の元素で置換したもの、更には、共振
周波数温度係数(τf)を調整するため、負の値を持つ
TiO2と正の値を持つ誘電体磁器やガラスと組み合わ
せた物が利用されてきている。
Therefore, as these dielectric materials, B
aO-TiO 2 system dielectric ceramic [HMO, Bryan, Jr., Thomso
n, Jr.and JK Plourde: J.Am.Ceram.Soc.57 (1974) 450)
And a part of which is replaced with another element, and further, in order to adjust the resonance frequency temperature coefficient (τf), a combination of TiO 2 having a negative value and a dielectric ceramic or glass having a positive value. Has been used.

【0004】[0004]

【発明が解決しようとする課題】しかしながら上記従来
の材料では、誘電率、無負荷Qが低く、又、共振周波数
温度係数(τf)が高い等、実用上使用し難く、種々問
題点があった。この問題点を解決するためにBaO−T
iO2−Nd23系誘電体磁器組成物(特公昭60−4
1633号公報)やBaO−TiO2−Nd23−Bi2
3系誘電体磁器組成物(特公昭59−51091号公
報)等が提案されたが、前者は、共振周波数温度係数
(τf)が大きく、又、後者は比誘電率に対して無負荷
Qが低い等、要求される特性の多様化に応じるためには
未だ満足できるものではなかった。
However, the above-mentioned conventional materials have various problems such as low permittivity and no-load Q, high resonance frequency temperature coefficient (τf), and the like, which are difficult to use in practice. . In order to solve this problem, BaO-T
iO 2 -Nd 2 O 3 based dielectric ceramic composition (JP-B 60-4
1633 JP) or BaO-TiO 2 -Nd 2 O 3 -Bi 2
O 3 -based dielectric ceramic compositions (Japanese Patent Publication No. 59-51091) and the like have been proposed. The former has a large resonance frequency temperature coefficient (τf), and the latter has no load Q with respect to the relative dielectric constant. It was not yet satisfactory to meet the diversification of required characteristics such as low.

【0005】本発明は、上記従来の問題点を解決するも
ので、誘電率、無負荷Qを高く、共振周波数温度係数
(τf)が小さく、且つ、要求される特性の多様化に応
じるために、誘電率、無負荷Q、共振周波数温度係数
(τf)を広範囲に変化させることができる誘電体磁器
組成物を提供することを目的とする。
The present invention solves the above-mentioned problems of the prior art, and has a high permittivity and a no-load Q, a small resonance frequency temperature coefficient (τf), and a required diversification of characteristics. , A dielectric constant, a no-load Q, and a temperature coefficient (τf) of a resonance frequency can be varied over a wide range.

【0006】[0006]

【課題を解決するための手段】この目的を達成する本発
明の誘電体磁器組成物は、組成式が、 xBaO・yTiO2・zNd23・tSm23・wB
23 で表され、それぞれのモル分率が、0.06≦x≦0.
155、0.69≦y≦0.80、0.05≦z≦0.
18、0<t≦0.07、0<w≦0.05(但し、x
+y+z+t+w=1)の範囲にある構成からなり、
尚、前記誘電体磁器組成物100重量部にAl23,F
23,SnO2,ZnO,NiO,MnO,CuO,
CoO,SiO2,ZrO2の一種又は二種以上を3重量
部以下添加してもよく、更に、これら前記誘電体磁器組
成物のBa元素の一部をモル分率で20mol%以下S
r,Ca,Mg等の元素の一種又は二種以上で置換した
構成でもよい。更に、これら前記誘電体磁器組成物中の
Sm23,Nd23の純度が70wt%以上であり不純物
の化学成分が他の稀土類からなる構成を有していてもよ
い。
The dielectric ceramic composition of the present invention which achieves this object has a composition formula of xBaO.yTiO 2 .zNd 2 O 3 .tSm 2 O 3 .wB
i 2 O 3 and the mole fraction of each is 0.06 ≦ x ≦ 0.
155, 0.69≤y≤0.80, 0.05≤z≤0.
18, 0 <t ≦ 0.07, 0 <w ≦ 0.05 (however, x
+ Y + z + t + w = 1) in the range,
Al 2 O 3 , F was added to 100 parts by weight of the dielectric ceramic composition.
e 2 O 3 , SnO 2 , ZnO, NiO, MnO, CuO,
One or two or more of CoO, SiO 2 , and ZrO 2 may be added in an amount of 3 parts by weight or less, and a part of the Ba element in the dielectric ceramic composition may be contained in a mole fraction of 20 mol% or less S
A configuration in which one or more elements such as r, Ca, and Mg are substituted may be used. Furthermore, the purity of Sm 2 O 3 and Nd 2 O 3 in the dielectric ceramic composition may be 70 wt% or more, and the chemical composition of impurities may be composed of other rare earth.

【0007】[0007]

【作用】この構成によって、 (1)BaO−TiO2−Nd23−Sm23−Bi2
3系誘電体磁器組成物を用いることにより、マイクロ波
領域における誘電率、無負荷Qが高く、又、共振周波数
温度係数(τf)が小さい誘電体磁器を得ることができ
る。 (2)Al23やZrO2等を前記誘電体磁器組成物に
添加することにより、焼結性が改善されると共に誘電率
のバラツキを低く抑えることができる。特にZrO2
ついては誘電体磁器の機械的強度をも大幅に向上させる
ことができる。 (3)前記誘電体磁器組成物中のBa元素をSr,C
a,Mg等の元素に一部置換しても、Ba元素と同等の
特性を持つことができ、応用範囲を拡げることができ
る。 (4)Sm23,Nd23の純度に関しては、低純度品
であっても高純度品に近い特性を持つことができ、応用
範囲を拡げることができる。
[Action] This configuration, (1) BaO-TiO 2 -Nd 2 O 3 -Sm 2 O 3 -Bi 2 O
By using the 3- based dielectric porcelain composition, it is possible to obtain a dielectric porcelain having a high dielectric constant and a no-load Q in the microwave region and a small resonance frequency temperature coefficient (τf). (2) By adding Al 2 O 3 or ZrO 2 to the dielectric ceramic composition, the sinterability can be improved and the variation in the dielectric constant can be suppressed low. Especially with respect to ZrO 2 , the mechanical strength of the dielectric ceramics can be greatly improved. (3) Ba element in the dielectric ceramic composition is Sr, C
Even if it is partially replaced with an element such as a or Mg, it can have the same characteristics as the Ba element and the application range can be expanded. (4) Regarding the purity of Sm 2 O 3 and Nd 2 O 3 , even a low-purity product can have characteristics close to those of a high-purity product, and the range of applications can be expanded.

【0008】[0008]

【実施例】以下本発明を実施例に基づいて、更に詳細に
説明する。
EXAMPLES The present invention will be described in more detail based on the following examples.

【0009】原料として、工業原料であるBaCO3
TiO2,Sm23,Nd23,Bi 23,Al23
Fe23,SnO2,ZnO,NiO,MnO,Cu
O,CoO,SiO2,ZrO2を使用する。Sm23
Nd23については、純度65、70、80、90、9
9.9wt%品を準備した。
As a raw material, BaCO which is an industrial raw material3
TiO2, Sm2O3, Nd2O3, Bi 2O3, Al2O3
Fe2O3, SnO2, ZnO, NiO, MnO, Cu
O, CoO, SiO2, ZrO2To use. Sm2O3
Nd2O3For purity 65, 70, 80, 90, 9
A 9.9 wt% product was prepared.

【0010】上記原料粉末を所定の組成になるよう秤量
した後、メノウボールを備えたウレタン内張りのボール
ミルに純水と共に入れ、湿式混合をした。この混合物を
十分乾燥した後、400kg/cm2の圧力でペレット状に
成形し、該成形体を大気中で900〜1000℃の温度
範囲で仮焼した。その後、該仮焼物を純水と共に前記と
同様な構造を有するボールミルに入れ湿式混合をした。
得られた粉砕物を脱水乾燥した後、該粉末に有機バイン
ダーとして濃度3w/v%のポリビニルアルコール溶液
を8v/w%添加して造粒した後、32メッシュのふる
いを用い整粒した。整粒粉体を金型と油圧プレスを用い
て成形圧力800kg/cm2で直径20mm、厚み8〜1
2mmのペレット状に成形した。該成形体を組成に応じ
て1200〜1550℃の温度範囲で2〜3時間焼成し
目的とする誘電体磁器を得た。得られた誘電体磁器を誘
電体共振器として使用し、無負荷Q、及び共振周波数温
度係数(τf)を測定した。誘電率は、共振周波数と誘
電体磁器の大きさより計算で求めた。共振周波数は2〜
4GHzであった。共振周波数温度係数(τf)は、−
25〜50℃の温度範囲で測定した。
The above raw material powders were weighed so as to have a predetermined composition, put into a urethane-lined ball mill equipped with agate balls together with pure water, and wet-mixed. After sufficiently drying this mixture, it was formed into pellets at a pressure of 400 kg / cm 2 , and the formed body was calcined in the temperature range of 900 to 1000 ° C in the atmosphere. Then, the calcined product was put in a ball mill having the same structure as above together with pure water and wet-mixed.
The obtained pulverized product was dehydrated and dried, and then 8 v / w% of a polyvinyl alcohol solution having a concentration of 3 w / v% was added to the powder as an organic binder for granulation, followed by sizing with a 32 mesh sieve. Using a die and a hydraulic press, the sized powder is molded at a pressure of 800 kg / cm 2 with a diameter of 20 mm and a thickness of 8 to 1.
It was molded into 2 mm pellets. The molded body was fired in a temperature range of 1200 to 1550 ° C. for 2 to 3 hours depending on the composition to obtain a target dielectric ceramic. The obtained dielectric porcelain was used as a dielectric resonator, and the unloaded Q and the resonance frequency temperature coefficient (τf) were measured. The permittivity was calculated from the resonance frequency and the size of the dielectric ceramic. Resonance frequency is 2
It was 4 GHz. The resonance frequency temperature coefficient (τf) is −
It measured in the temperature range of 25-50 degreeC.

【0011】(実施例1)各組成成分の配合割合(モル
分率)に対する比誘電率や無負荷Qの依存性について確
認した。その結果を図1、図2に示す。
Example 1 The dependence of the relative dielectric constant and the unloaded Q on the blending ratio (molar fraction) of each composition component was confirmed. The results are shown in FIGS. 1 and 2.

【0012】図1(a),(b)は、BaOのモル分率
(x)に対するこれらの依存性を示したものであり、図
2(a),(b)はTiO2のモル分率(y)に対する
これらの依存性、図3(a)はNd23のモル分率
(z)に対する比誘電率の依存性、図3(b)はSm2
3のモル分率(t)に対する比誘電率の依存性、図4
(a),(b)はBi23のモル分率(w)に対する無
負荷Q、共振周波数温度係数(τf)の依存性を示す。
FIGS. 1 (a) and 1 (b) show these dependences on the BaO mole fraction (x), and FIGS. 2 (a) and 2 (b) show the TiO 2 mole fraction. These dependences on (y), FIG. 3 (a) is the dependence of the relative permittivity on the mole fraction (z) of Nd 2 O 3 , and FIG. 3 (b) is Sm 2
Dependence of relative permittivity on mole fraction (t) of O 3 , FIG.
(A) and (b) show the dependence of the unloaded Q and the resonance frequency temperature coefficient (τf) on the mole fraction (w) of Bi 2 O 3 .

【0013】尚、上記各モル分率に対する依存性を確認
する際は、モル分率を変化させる原料以外の原料は、本
発明の範囲内において一定とした。
When confirming the dependence on each of the above-mentioned mole fractions, the raw materials other than the raw material for changing the mole fraction were made constant within the scope of the present invention.

【0014】又、図示方法としては、試料に対応する特
性値(対象成分組成点における組成数はN=20)をプ
ロットし、該領域をグラフ上に領域指定して行なった。
図1、図2より明らかなように、本発明の誘電体磁器組
成物からなる誘電体磁器は、マイクロ波領域の周波数に
おいて、比誘電率、無負荷Qが大きく、共振周波数温度
係数(τf)は小さいことがわかる。尚、判定基準とし
ては、無負荷Q≧2000、比誘電率≧60、共振周波
数温度係数(τf)≦100ppm/℃とした。 判定理
由としては、無負荷Qについては、2000未満の場合
高周波フィルタに使用したとき、挿入損失が大きく使用
困難なためである。又、回路基板として使用しても、発
熱等回路に悪影響を及ぼすからである。比誘電率につい
ては、60以上ないと周波数1〜2GHz帯において誘
電体共振器の寸法が5mm以上となり小型化の流れから外
れる。共振周波数温度係数(τf)が100ppm/℃
を 超えると回路上に形成された共振器の共振周波数
が、温度によってシフトし、回路上のマッチングが取れ
なくなるからである。
As a method of illustration, a characteristic value corresponding to the sample (the composition number at the composition point of the target component is N = 20) was plotted, and the area was designated on the graph.
As is clear from FIGS. 1 and 2, the dielectric porcelain composed of the dielectric porcelain composition of the present invention has a large relative permittivity and no load Q at a frequency in the microwave region, and has a resonance frequency temperature coefficient (τf). It turns out that is small. In addition, as criteria for determination, no load Q ≧ 2000, relative permittivity ≧ 60, and resonance frequency temperature coefficient (τf) ≦ 100 ppm / ° C. The reason for the determination is that, when the unloaded Q is less than 2000, the insertion loss is large and it is difficult to use when used for a high frequency filter. Moreover, even if it is used as a circuit board, it has a bad influence on the circuit such as heat generation. Regarding the relative permittivity, if it is 60 or more, the size of the dielectric resonator becomes 5 mm or more in the frequency band of 1 to 2 GHz, which is out of the trend of miniaturization. Resonance frequency temperature coefficient (τf) is 100ppm / ℃
This is because, when the value exceeds, the resonance frequency of the resonator formed on the circuit shifts due to temperature, and matching on the circuit cannot be achieved.

【0015】又、モル分率(x)及びモル分率(y)が
それぞれ0.155以上及び0.69以下では、焼成時
にBi23が蒸発してしまい、特性が劣化してしまうの
でモル分率(x)及びモル分率(y)はそれぞれ0.1
55以下及び0.69以上がよい。
Further, when the mole fraction (x) and the mole fraction (y) are 0.155 or more and 0.69 or less, respectively, Bi 2 O 3 is evaporated during firing and the characteristics are deteriorated. The mole fraction (x) and the mole fraction (y) are each 0.1
It is preferably 55 or less and 0.69 or more.

【0016】(実施例2)次に、xBaO・yTiO2
・zNd23・tSm23・wBi23の組成式からな
る誘電体磁器組成物の組成モル分率が、x=0.12
2,y=0.69,z=0.141,t=0.052,
w=0.005となるように調整した組成物100重量
部に、Al23,ZrO2を所定量添加し、その添加効
果を確認した。その結果を図5,6に示す。
(Example 2) Next, xBaO.yTiO 2
· ZNd 2 O 3 · tSm 2 O 3 · wBi 2 O 3 composition mole fraction of a dielectric ceramic composition having a composition formula, x = 0.12
2, y = 0.69, z = 0.141, t = 0.052
A predetermined amount of Al 2 O 3 and ZrO 2 was added to 100 parts by weight of the composition adjusted so that w = 0.005, and the effect of the addition was confirmed. The results are shown in FIGS.

【0017】図5(a),(b)は添加量(重量部)に
対する比誘電率の変動係数(%)及び無負荷Qの依存性
を示したものであり、図6は、ZrO2の添加量(重量
部)に対する3点曲げ強度(kg/ cm2 )の依存性を示し
たものである。
5 (a) and 5 (b) show the dependence of the coefficient of variation (%) of the relative permittivity and the unloaded Q on the added amount (parts by weight), and FIG. 6 shows that of ZrO 2 . It shows the dependence of the three-point bending strength (kg / cm 2 ) on the added amount (parts by weight).

【0018】図5(a),(b)から明らかなように、
焼結性の改善からの波及効果と思われる誘電率のバラツ
キの減少が認められる。添加量が3重量部を超えると結
晶粒界近傍に生成するガラス層の増大のためと思われる
無負荷Qの低下を引き起こす。特にZrO2については
図6から明らかなように、機械的強度の著しい増加が認
められる。しかし3重量部を超えると図5(a),(b)に
示すように無負荷Qが低下する傾向がある。尚、Al2
3とZrO2の混合比の影響はあまり認められなかっ
た。又、上記組成の組成モル分率を本発明の範囲内で変
化させて同様に実験を行なったが、同様の結果が得られ
た。
As is apparent from FIGS. 5 (a) and 5 (b),
A decrease in the variation of the dielectric constant, which is considered to be a ripple effect from the improvement of the sinterability, is recognized. When the addition amount exceeds 3 parts by weight, the no-load Q is lowered, which is considered to be due to an increase in the glass layer formed near the crystal grain boundaries. Especially for ZrO 2 , as is clear from FIG. 6, a remarkable increase in mechanical strength is observed. However, when it exceeds 3 parts by weight, the no-load Q tends to decrease as shown in FIGS. 5 (a) and 5 (b). Al 2
The effect of the mixing ratio of O 3 and ZrO 2 was not so noticeable. Further, the same experiment was conducted by changing the composition mole fraction of the above composition within the range of the present invention, and similar results were obtained.

【0019】(実施例3)次に、実施例2と同一の組成
比の試料を用い、Ba元素をSr,Ca,Mgに所定割
合で置換させた組成物を用い、比誘電率、無負荷Qの依
存性を確認した。その結果を図7(a),(b)に示
す。図7(a),(b)から明らかなように、Sr,C
a,Mgの置換率が20mol%以上では、一部比誘電
率、無負荷Qの低下する傾向があることがわかる。尚、
Sr,Ca,Mgを単一、又は混合して置換させても同
様の結果が得られた。
(Example 3) Next, using a sample having the same composition ratio as in Example 2 and using a composition in which Ba element was replaced by Sr, Ca, and Mg at a predetermined ratio, a relative permittivity and no load were applied. The dependency of Q was confirmed. The results are shown in FIGS. 7 (a) and 7 (b). As is clear from FIGS. 7A and 7B, Sr, C
It can be seen that when the substitution rate of a and Mg is 20 mol% or more, there is a tendency that the relative permittivity and the unloaded Q partially decrease. still,
Similar results were obtained when Sr, Ca, and Mg were replaced alone or as a mixture.

【0020】(実施例4)次に、実施例2と同一の組成
比の試料を用い、Sm23,Nd23の純度の比誘電率
に対する影響について確認した。その結果を図8に示
す。
(Example 4) Next, using a sample having the same composition ratio as in Example 2, the effect of the purity of Sm 2 O 3 and Nd 2 O 3 on the relative dielectric constant was confirmed. The result is shown in FIG.

【0021】図8(a)は、Sm23の純度(wt%)の
影響を示し、図8(b)はNd23の純度(wt%)の影
響を示す。
FIG. 8A shows the influence of the purity (wt%) of Sm 2 O 3 , and FIG. 8B shows the influence of the purity (wt%) of Nd 2 O 3 .

【0022】図8(a),(b)から明らかなように、
Sm23,Nd23の純度が70wt%未満のときに比誘
電率の低下を起こす傾向があることがわかる。従って、
このことから工業的に精製された原料であれば十分使用
に耐えると言える。
As is apparent from FIGS. 8 (a) and 8 (b),
It can be seen that when the purity of Sm 2 O 3 and Nd 2 O 3 is less than 70 wt%, the relative dielectric constant tends to decrease. Therefore,
From this, it can be said that industrially refined raw materials can be sufficiently used.

【0023】(実施例5)次に、組成式xBaO・yT
iO2・zNd23・tSm23・wBi23の組成モ
ル分率を、 0.06≦x≦0.155 0.69≦y≦0.80 0.05≦z≦0.18 0<t≦0.07 0<w≦0.05 (但し、x+y+z+t+w=1) の範囲で変化させた場合、及び従来例の組成比の組成物
について、比誘電率に対する無負荷Q、共振周波数温度
係数(τf)の関係を確認した。その結果を図9
(a),(b)に示す。
(Example 5) Next, the composition formula xBaO.yT
The composition mole fraction of iO 2 · zNd 2 O 3 · tSm 2 O 3 · wBi 2 O 3 is 0.06 ≦ x ≦ 0.155 0.69 ≦ y ≦ 0.80 0.05 ≦ z ≦ 0. 18 0 <t ≤ 0.07 0 <w ≤ 0.05 (however, x + y + z + t + w = 1) When changing in the range, and for the composition of the composition ratio of the conventional example, no load Q with respect to relative permittivity, resonance The relationship between frequency temperature coefficient (τf) was confirmed. The result is shown in Figure 9.
Shown in (a) and (b).

【0024】図9(a)は、各誘電体磁器組成物の比誘
電率に対する無負荷Qの依存性を、図9(b)は同じく
共振周波数温度係数(τf)の依存性を示す。
FIG. 9A shows the dependence of the unloaded Q on the relative permittivity of each dielectric ceramic composition, and FIG. 9B shows the dependence of the resonance frequency temperature coefficient (τf).

【0025】図9(a),(b)から明らかなように従
来例と比較すると、本発明のほうが比誘電率に対して高
い無負荷Q及び低い共振周波数温度係数(τf)を得る
ことができる。
As is apparent from FIGS. 9 (a) and 9 (b), in comparison with the conventional example, the present invention can obtain a higher unloaded Q and a lower resonance frequency temperature coefficient (τf) with respect to the relative permittivity. it can.

【0026】[0026]

【発明の効果】以上のように本発明は、 (1)BaO−TiO2−Nd23−Sm23−Bi2
3系組成物を用いることにより、マイクロ波領域におけ
る誘電率、無負荷Qが高く、又、共振周波数温度係数
(τf)が小さい誘電体磁器を得ることができる。 (2)Al23やZrO2等を添加することにより、焼
結性が改善されると共に誘電率のバラツキを低く抑える
ことができる。特にZrO2については誘電体磁器の機
械的強度をも大幅に向上させることができる。 (3)BaをSr,Ca,Mgに一部置換しても、Ba
と同等の特性を持つことができ、原料の多様化に対応で
きる。 (4)Sm23,Nd23は、低純度品であっても高純
度品に近い特性を持つことができる、優れた誘電体磁器
組成物を提供するものである。
The present invention as described above, according to the present invention is, (1) BaO-TiO 2 -Nd 2 O 3 -Sm 2 O 3 -Bi 2 O
By using the 3- based composition, it is possible to obtain a dielectric porcelain having a high dielectric constant and a no-load Q in the microwave region and a small resonance frequency temperature coefficient (τf). (2) By adding Al 2 O 3 or ZrO 2 or the like, it is possible to improve sinterability and suppress variations in dielectric constant to a low level. Especially with respect to ZrO 2 , the mechanical strength of the dielectric ceramics can be greatly improved. (3) Even if Ba is partially replaced with Sr, Ca, Mg, Ba
It can have the same characteristics as, and can cope with the diversification of raw materials. (4) Sm 2 O 3 and Nd 2 O 3 provide an excellent dielectric porcelain composition that can have characteristics close to those of a high-purity product even if it is a low-purity product.

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

【図1】(a)は本発明の第1の実施例における誘電体
磁器組成物の主要組成物の特性図 (b)は本発明の第1の実施例における誘電体磁器組成
物の主要組成物の特性図
1A is a characteristic diagram of a main composition of a dielectric ceramic composition according to a first embodiment of the present invention, and FIG. 1B is a main composition of a dielectric ceramic composition according to a first embodiment of the present invention. Characteristic diagram of object

【図2】(a)は本発明の第1の実施例における誘電体
磁器組成物の主要組成物の特性図 (b)は本発明の第1の実施例における誘電体磁器組成
物の主要組成物の特性図
FIG. 2 (a) is a characteristic diagram of the main composition of the dielectric ceramic composition in the first embodiment of the present invention. FIG. 2 (b) is a main composition of the dielectric ceramic composition in the first embodiment of the present invention. Characteristic diagram of object

【図3】(a)は本発明の第1の実施例における誘電体
磁器組成物の主要組成物の特性図 (b)は本発明の第1の実施例における誘電体磁器組成
物の主要組成物の特性図
FIG. 3A is a characteristic diagram of a main composition of a dielectric ceramic composition according to the first embodiment of the present invention, and FIG. 3B is a main composition of a dielectric ceramic composition according to the first embodiment of the present invention. Characteristic diagram of object

【図4】(a)は本発明の第1の実施例における誘電体
磁器組成物の主要組成物の特性図 (b)は本発明の第1の実施例における誘電体磁器組成
物の主要組成物の特性図
FIG. 4A is a characteristic diagram of a main composition of a dielectric ceramic composition according to the first embodiment of the present invention, and FIG. 4B is a main composition of a dielectric ceramic composition according to the first embodiment of the present invention. Characteristic diagram of object

【図5】(a)は本発明の第2の実施例における誘電体
磁器組成物の第2成分の添加効果を示す特性図 (b)は本発明の第2の実施例における誘電体磁器組成
物の第2成分の添加効果を示す特性図
5 (a) is a characteristic diagram showing the effect of adding the second component of the dielectric ceramic composition in the second embodiment of the present invention. FIG. 5 (b) is a dielectric ceramic composition in the second embodiment of the present invention. Characteristic diagram showing the effect of adding the second component of the product

【図6】本発明の第2の実施例における誘電体磁器組成
物の第2成分の添加効果を示す特性図
FIG. 6 is a characteristic diagram showing the effect of adding the second component of the dielectric ceramic composition in the second example of the present invention.

【図7】(a)は本発明の第3の実施例における誘電体
磁器組成物の特性図 (b)は本発明の第3の実施例における誘電体磁器組成
物の特性図
7A is a characteristic diagram of a dielectric ceramic composition according to a third embodiment of the present invention, and FIG. 7B is a characteristic diagram of a dielectric ceramic composition according to a third embodiment of the present invention.

【図8】(a)は本発明の第4の実施例における誘電体
磁器組成物のSm23の純度の比誘電率に対する影響の
特性図 (b)は本発明の第4の実施例における誘電体磁器組成
物のNd23の純度の比誘電率に対する影響の特性図
FIG. 8A is a characteristic diagram of the influence of the Sm 2 O 3 purity of the dielectric ceramic composition of the fourth embodiment of the present invention on the relative dielectric constant. FIG. 8B is the fourth embodiment of the present invention. Of the influence of the Nd 2 O 3 purity of the dielectric ceramic composition on the relative permittivity in

【図9】(a)は本発明の第5の実施例における誘電体
磁器組成物と従来例の組成物の特性比較図 (b)は本発明の第5の実施例における誘電体磁器組成
物と従来例の組成物の特性比較図
9 (a) is a characteristic comparison diagram of the dielectric ceramic composition in the fifth embodiment of the present invention and the composition of the conventional example, and FIG. 9 (b) is a dielectric ceramic composition in the fifth embodiment of the present invention. Comparison chart of properties of conventional and conventional compositions

───────────────────────────────────────────────────── フロントページの続き (72)発明者 多木 宏光 大阪府門真市大字門真1006番地 松下電器 産業株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Hiromitsu Taki 1006 Kadoma, Kadoma City, Osaka Prefecture Matsushita Electric Industrial Co., Ltd.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】組成式が、xBaO・yTiO2・zNd2
3・tSm23・wBi23からなる誘電体磁器組成
物であって、その組成範囲をモル分率で表したときそれ
ぞれ、 0.06≦x≦0.155 0.69≦y≦0.80 0.05≦z≦0.18 0<t≦0.07 0<w≦0.05 (但し、x+y+z+t+w=1) の範囲にあることを特徴とする誘電体磁器組成物。
1. The composition formula is xBaO.yTiO 2 .zNd 2
A dielectric ceramic composition comprising O 3 · tSm 2 O 3 · wBi 2 O 3 , wherein when the composition range is expressed by a mole fraction, 0.06 ≦ x ≦ 0.155 0.69 ≦ y A dielectric ceramic composition characterized by being in the range of ≦ 0.80 0.05 ≦ z ≦ 0.18 0 <t ≦ 0.07 0 <w ≦ 0.05 (where x + y + z + t + w = 1).
【請求項2】誘電体磁器組成物の100重量部に対し、
Al23,Fe23,SnO2,ZnO,NiO,Mn
O,CuO,CoO,SiO2,ZrO2の一種又は二種
以上を3重量部以下添加したことを特徴とする請求項1
に記載の誘電体磁器組成物。
2. With respect to 100 parts by weight of the dielectric ceramic composition,
Al 2 O 3 , Fe 2 O 3 , SnO 2 , ZnO, NiO, Mn
O, claim characterized CuO, CoO, and it has added SiO 2, of ZrO 2 one or more kinds of 3 parts by weight or less 1
The dielectric porcelain composition described in 1.
【請求項3】Baの一部をモル分率で20mol%以下S
r,Ca,Mgの一種又は二種以上で置換したことを特
徴とする請求項1又2の内いずれか1に記載の誘電体磁
器組成物。
3. A part of Ba has a molar fraction of 20 mol% or less S
The dielectric ceramic composition according to any one of claims 1 and 2, which is substituted with one or more of r, Ca, and Mg.
【請求項4】Sm23,Nd23の純度が70wt%以上
であり不純物の化学成分が他の稀土類からなることを特
徴とする請求項1又2の内いずれか1に記載の誘電体磁
器組成物。
4. The method according to claim 1, wherein the purity of Sm 2 O 3 and Nd 2 O 3 is 70 wt% or more and the chemical component of impurities is other rare earth. The dielectric ceramic composition of.
JP4230939A 1992-08-31 1992-08-31 Dielectric ceramic composition Pending JPH0680467A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4230939A JPH0680467A (en) 1992-08-31 1992-08-31 Dielectric ceramic composition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4230939A JPH0680467A (en) 1992-08-31 1992-08-31 Dielectric ceramic composition

Publications (1)

Publication Number Publication Date
JPH0680467A true JPH0680467A (en) 1994-03-22

Family

ID=16915676

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4230939A Pending JPH0680467A (en) 1992-08-31 1992-08-31 Dielectric ceramic composition

Country Status (1)

Country Link
JP (1) JPH0680467A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6331499B1 (en) * 1998-06-04 2001-12-18 Sumitomo Special Metals Co., Ltd. Microwave dielectric ceramic composition
KR100444224B1 (en) * 2001-11-13 2004-08-16 삼성전기주식회사 Dielectric Ceramic Compositions
JP2009126742A (en) * 2007-11-22 2009-06-11 Tdk Corp Dielectric porcelain composition and electronic component
JP2010235327A (en) * 2009-03-30 2010-10-21 Tdk Corp Dielectric ceramic composition
JP2010235325A (en) * 2009-03-30 2010-10-21 Tdk Corp Dielectric ceramic composition

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6331499B1 (en) * 1998-06-04 2001-12-18 Sumitomo Special Metals Co., Ltd. Microwave dielectric ceramic composition
KR100444224B1 (en) * 2001-11-13 2004-08-16 삼성전기주식회사 Dielectric Ceramic Compositions
JP2009126742A (en) * 2007-11-22 2009-06-11 Tdk Corp Dielectric porcelain composition and electronic component
JP2010235327A (en) * 2009-03-30 2010-10-21 Tdk Corp Dielectric ceramic composition
JP2010235325A (en) * 2009-03-30 2010-10-21 Tdk Corp Dielectric ceramic composition

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