JPS6236064A - Dielectric ceramic composition for microwave - Google Patents
Dielectric ceramic composition for microwaveInfo
- Publication number
- JPS6236064A JPS6236064A JP60172922A JP17292285A JPS6236064A JP S6236064 A JPS6236064 A JP S6236064A JP 60172922 A JP60172922 A JP 60172922A JP 17292285 A JP17292285 A JP 17292285A JP S6236064 A JPS6236064 A JP S6236064A
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- mol
- dielectric
- microwave
- ceramic composition
- dielectric ceramic
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Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
利用産業分野
この発明は、マイクロ波用誘電体磁器組成物に係り、比
誘電率εrが大きく、マイクロ波帯における誘電損失が
小さく、かつ組成を適当に選択することにより誘電率の
温度係数を比較的広範囲に選択することができるマイク
ロ波用誘電体磁器組成物に関する。DETAILED DESCRIPTION OF THE INVENTION Field of Application This invention relates to a dielectric ceramic composition for microwave use, which has a large relative dielectric constant εr, a small dielectric loss in the microwave band, and which has The present invention relates to a microwave dielectric ceramic composition whose temperature coefficient of dielectric constant can be selected over a relatively wide range.
背景技術
近年、誘電材料として、1つの新しい利用展開が始まっ
ている。それは、従来のコンデンサー等の応用とは異な
った概念の誘電体共振器である。BACKGROUND ART In recent years, a new development in the use of dielectric materials has begun. It is a dielectric resonator with a different concept from conventional applications such as capacitors.
一般に、誘電体が電磁波の伝播媒体であることを利用し
たものであり、誘電体中の電磁波の波長が真空中のそれ
と比べ、1/Jεrになることに着目し、これを積極的
に利用して回路素子の小型化を計ったものでおる。In general, it takes advantage of the fact that dielectrics are propagation media for electromagnetic waves, and it focuses on the fact that the wavelength of electromagnetic waves in dielectrics is 1/Jεr compared to that in vacuum, and actively utilizes this. This design is designed to reduce the size of circuit elements.
従来のマイクロ波帯の回路素子は、導波管や空洞共振器
であったが、近年の目覚ましい発展を見せる衛星通信や
移動通信手段等の通信システム中で用いるには、大型で
かつ重く不適当であり、これらマイクロ波帯が使用され
る部品1回路素子の小型化、信頼性の向上が特に求めら
れていた。Conventional microwave band circuit elements have been waveguides and cavity resonators, but they are large, heavy and unsuitable for use in communication systems such as satellite communication and mobile communication means, which have seen remarkable progress in recent years. Therefore, there has been a particular demand for miniaturization and improved reliability of component single circuit elements in which these microwave bands are used.
かかるマイクロ波用誘電体材料としては、Ca Ti
Os Mo T、03系、(Zr、 Sn) TyO
t系、Ba2 Ti9010系やBaO−Nd203−
Ti02系、BaOSm2O3Ti0t系がよく知られ
ている。Such microwave dielectric materials include CaTi
Os Mo T, 03 series, (Zr, Sn) TyO
t series, Ba2 Ti9010 series and BaO-Nd203-
Ti02 series and BaOSm2O3Ti0t series are well known.
Ca丁L 03−MgTi Os系材料は、低損失で誘
電率の温度係数も小さいが、比誘電率は20と小さい。Ca Ding L 03-MgTiOs-based material has low loss and a small temperature coefficient of dielectric constant, but has a small dielectric constant of 20.
また、(Zr、 Sn) That系やBa2 Tig
O10系材料は同様に低損失、低温度係数であるが、
比誘電率は40程度である。In addition, (Zr, Sn) That series and Ba2 Tig
O10-based materials also have low loss and low temperature coefficient, but
The dielectric constant is about 40.
また、BaONd2O3Ti02系、BaO−5n20
3−TLO2系材料系材比誘電率が60〜80と大きく
、低温度係数であるが、マイクロ波帯での誘電損失は5
GH2程度でQ=1000以下と小さい。In addition, BaONd2O3Ti02 system, BaO-5n20
3-TLO2-based materials have a high relative dielectric constant of 60 to 80 and a low temperature coefficient, but the dielectric loss in the microwave band is 5.
It is small at about GH2 and Q=1000 or less.
しかし、今日ではざらに低損失材料が求められており、
BaOSm203TLOe系は、Ba ONd 203
Ti 02系に比べ、同程度の比誘電率(εr =80
)を有しかつ低損失であるが、Sm2O3を原料に用い
るため、材料コストが高く、また、大量に使用するには
、原料供給に不安があり、合接安定して供給されるのは
困難である。However, today there is a strong demand for low-loss materials.
BaOSm203TLOe series is BaONd203
Compared to the Ti02 system, it has a similar dielectric constant (εr = 80
) and have low loss, but since Sm2O3 is used as a raw material, the material cost is high, and when used in large quantities, there is concern about raw material supply, making it difficult to stably supply the welding material. It is.
発明の目的
この発明は、上述の問題点に鑑み、高誘電率であり、誘
電率の温度係数を比較的自由に選択でき、かつマイクロ
波用誘電材料として、従来材料よりざらに低損失であり
、より安価なマイクロ波帯用誘電材料を目的としている
。Purpose of the Invention In view of the above-mentioned problems, this invention has a high dielectric constant, allows the temperature coefficient of the dielectric constant to be selected relatively freely, and has a much lower loss than conventional materials as a dielectric material for microwaves. The aim is to create a cheaper dielectric material for the microwave band.
発明の構成と効果
この発明は、マイクロ波用誘電体材料に要求される諸特
性を満足する誘電体磁器組成物を目的に種々検討した結
果、BaO−La2O3” TiO2a 5nap系材
料が、高誘電率、低誘電損失であり、誘電率の温度係数
がその組成の選択により設定でき、マイクロ波帯用誘電
材料に最適であり、ざらに資源的に豊富な元素よりなる
磁器組成物であるため従来材料より安価に提供できるこ
とを知見したものである。Structure and effect of the invention As a result of various studies aimed at creating a dielectric ceramic composition that satisfies various properties required for dielectric materials for microwaves, the present invention has revealed that a BaO-La2O3'' TiO2a 5nap-based material has a high dielectric constant. It has low dielectric loss, and the temperature coefficient of dielectric constant can be set by selecting its composition, making it ideal as a dielectric material for microwave bands.As it is a porcelain composition made of elements that are abundant in resources, it is different from conventional materials. This is based on the knowledge that it can be provided at a lower price.
すなわち、この発明は、
基本組成式を、XBa0−yl、、1203・zTL0
2・wSn02 と表わし、
x十y+z+w= 100モル%としたとき、組成範囲
を限定する記号x、y、z、wが下記式を満足すること
を特徴とするマイクロ波用誘電体磁器組成物であり、
0<x≦17.5 モル%
12.5≦y≦35.0 モル%
52.5≦z≦71.5 モル%
0<w≦5.0 モル%
さらには、基本組成式を、XBaO・’/LazO3・
Z TLO2−WSn02 φV PbOと表わし、x
+y+z+w= 100モル%としたとき、組成範囲を
限定する記号x、y、z、w、vが下記式を満足するこ
とを特徴とするマイクロ波用誘電体磁器組成物である。That is, in this invention, the basic compositional formula is
2.wSn02, and when xy+z+w=100 mol%, the symbols x, y, z, and w that limit the composition range satisfy the following formula: Yes, 0<x≦17.5 mol% 12.5≦y≦35.0 mol% 52.5≦z≦71.5 mol% 0<w≦5.0 mol% Furthermore, the basic composition formula is XBaO・'/LazO3・
Z TLO2-WSn02 φV PbO, x
When +y+z+w=100 mol%, the dielectric ceramic composition for microwaves is characterized in that the symbols x, y, z, w, and v that limit the composition range satisfy the following formula.
0<x≦17゜5 モル%
12.5≦y≦35.0 モル%
52.5≦z≦17.5 モル%
0<w≦5.0 モル%
x+y+z+w= 100モル%に対して、O<VS2
.0 モル%
組成の限定理由
この発明による誘電体磁器組成物は、
BaO会L1203 ” TLOe−Sn02あるいは
BaO−La203・Ti Ot・Sn Ot・PbO
からなるが、その組成範囲は以下のとおりである。0<x≦17゜5 mol% 12.5≦y≦35.0 mol% 52.5≦z≦17.5 mol% 0<w≦5.0 mol% <VS2
.. 0 mol% Reason for limiting the composition The dielectric ceramic composition according to the present invention is composed of: BaO-La203・TiOt・SnOt・PbO
The composition range is as follows.
BaOは、17.5モル%を越えると、共振周波数の温
度係数が、300ppm/’Cをこえて実用上不適当な
ため、17.5モル%以下の含有とする。If BaO exceeds 17.5 mol%, the temperature coefficient of the resonance frequency will exceed 300 ppm/'C, which is inappropriate for practical use, so the content is set to 17.5 mol% or less.
La2O3が35モル%を越え、12.5モル%未満、
TiO2が71.5モル%を越え、52.5モル%未満
の場合、磁器組成物の焼結性が悪くなり、高密度な焼結
体が得られず、Q値の低下を招来し、マイクロ波用誘電
材料として不適当なため、La2O212,5〜35.
0モル%、TiO,,52,5〜71.5モル%に限定
する。La2O3 is more than 35 mol% and less than 12.5 mol%,
If TiO2 exceeds 71.5 mol% and is less than 52.5 mol%, the sinterability of the ceramic composition will deteriorate, making it impossible to obtain a high-density sintered body, resulting in a decrease in Q value, and micro La2O212.5-35. is unsuitable as a wave dielectric material.
0 mol%, TiO, 52.5 to 71.5 mol%.
Sn O2は、5モル%を越えると、誘電率の低下とQ
値の低下を招来し、マイクロ波用誘電材料として不適当
なため、5モル%以下の含有とする。When SnO2 exceeds 5 mol%, the dielectric constant decreases and the Q
Since it causes a decrease in the value and is unsuitable as a dielectric material for microwaves, the content is limited to 5 mol% or less.
PbOは、Ba0−Li2O2・且02・SnO2系誘
電体磁器組成物の焼結性の改善に有効なほか、誘電率及
び誘電損失の改善に有効でおるが、7モル%を越える含
有は、Q値が低下し実用上不適当なため、1モル%以下
の含有とする。PbO is effective in improving the sinterability of Ba0-Li2O2 and 02-SnO2-based dielectric ceramic compositions, as well as in improving the dielectric constant and dielectric loss, but if the content exceeds 7 mol%, the Q Since the value decreases and it is not suitable for practical use, the content should be 1 mol% or less.
実施例
純度99.5%以上のTLO2,BaC0:+ 、 S
T+02. L1203 。Example TLO2 with purity of 99.5% or more, BaC0: +, S
T+02. L1203.
PbOを用いて、第1表に示す種々の組成(試斜陽17
〜15は本発明範囲外)に配合し、ボールミルにて5時
間の混合を行なった後、これを乾燥して1ioo℃、1
時間の仮焼を行ない、その後、仮焼粉を粉砕し、バイン
ダーを添加して成形した後、さらに脱バインダーし、1
300℃〜1500℃の温度条件で焼結し、外径17n
vnX高さ10mmの円柱状焼結体を作製した。Using PbO, various compositions shown in Table 1 (test slope 17
-15 is outside the scope of the present invention), mixed in a ball mill for 5 hours, dried and heated at 1iooC.
Calcination is performed for several hours, then the calcined powder is crushed, a binder is added and molded, and the binder is removed.
Sintered under temperature conditions of 300℃ to 1500℃, outer diameter 17n
A cylindrical sintered body with a vnX height of 10 mm was produced.
得られた焼結体について、25℃、 5.5(3)(
Z程度の条件下で、比誘電率εrとQ@を測定し、さら
に共振周波数の温度係数τfを測定した。測定結果は、
組成と共に第1表に示す。The obtained sintered body was heated at 25°C, 5.5(3)(
Under conditions of approximately Z, the relative dielectric constant εr and Q@ were measured, and the temperature coefficient τf of the resonance frequency was also measured. The measurement results are
It is shown in Table 1 along with the composition.
第1表から明らかなように、この発明による°誘電体磁
器組成物は、共振周波数の温度係数が広くとることがで
き、低損失でかつ高透磁率を示し、マイクロ波用誘電体
材料に最適なことが分る。As is clear from Table 1, the dielectric ceramic composition according to the present invention can have a wide temperature coefficient of resonance frequency, exhibits low loss and high magnetic permeability, and is ideal as a dielectric material for microwaves. I understand something.
以下余白Below margin
Claims (1)
_2と表わし、 x+y+z+w=100モル%としたとき、組成範囲を
限定する記号x、y、z、wが下記式を満足することを
特徴とするマイクロ波用誘電体磁器組成物。 0<x≦17.5モル% 12.5≦y≦35.0モル% 52.5≦z≦71.5モル% 0<w≦5.0モル% 2、基本組成式を、 xBaO・yLa_2O_3・zTiO_2・wSnO
_2、vPbOと表わし、 x+y+z+w=100モル%としたとき、組成範囲を
限定する記号x、y、z、w、vが下記式を満足するこ
とを特徴とするマイクロ波用誘電体磁器組成物。 0<x≦17.5モル% 12.5≦y≦35.0モル% 52.5≦z≦71.5モル% 0<w≦5.0モル% x+y+z+w=100モル%に対して、 0<v≦7.0モル%[Claims] 1. The basic compositional formula is xBaO・yLa_2O_3・zTiO_2・wSnO
_2, and when x+y+z+w=100 mol%, symbols x, y, z, and w that limit the composition range satisfy the following formula. 0<x≦17.5 mol% 12.5≦y≦35.0 mol% 52.5≦z≦71.5 mol% 0<w≦5.0 mol% 2. The basic compositional formula is xBaO・yLa_2O_3・zTiO_2・wSnO
A dielectric ceramic composition for microwave use, which is expressed as _2, vPbO, and when x+y+z+w=100 mol%, symbols x, y, z, w, and v that limit the composition range satisfy the following formula. 0<x≦17.5 mol% 12.5≦y≦35.0 mol% 52.5≦z≦71.5 mol% 0<w≦5.0 mol% For x+y+z+w=100 mol%, 0 <v≦7.0 mol%
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60172922A JPS6236064A (en) | 1985-08-05 | 1985-08-05 | Dielectric ceramic composition for microwave |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60172922A JPS6236064A (en) | 1985-08-05 | 1985-08-05 | Dielectric ceramic composition for microwave |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6236064A true JPS6236064A (en) | 1987-02-17 |
JPH022822B2 JPH022822B2 (en) | 1990-01-19 |
Family
ID=15950840
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP60172922A Granted JPS6236064A (en) | 1985-08-05 | 1985-08-05 | Dielectric ceramic composition for microwave |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6236064A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6427108A (en) * | 1987-07-22 | 1989-01-30 | Matsushita Electric Ind Co Ltd | Dielectric porcelain compound |
-
1985
- 1985-08-05 JP JP60172922A patent/JPS6236064A/en active Granted
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6427108A (en) * | 1987-07-22 | 1989-01-30 | Matsushita Electric Ind Co Ltd | Dielectric porcelain compound |
Also Published As
Publication number | Publication date |
---|---|
JPH022822B2 (en) | 1990-01-19 |
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