JPS59228310A - Microwave dielectric porcelain composition - Google Patents

Microwave dielectric porcelain composition

Info

Publication number
JPS59228310A
JPS59228310A JP10403783A JP10403783A JPS59228310A JP S59228310 A JPS59228310 A JP S59228310A JP 10403783 A JP10403783 A JP 10403783A JP 10403783 A JP10403783 A JP 10403783A JP S59228310 A JPS59228310 A JP S59228310A
Authority
JP
Japan
Prior art keywords
dielectric
microwave dielectric
porcelain composition
dielectric porcelain
composition ratio
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.)
Granted
Application number
JP10403783A
Other languages
Japanese (ja)
Other versions
JPH04321B2 (en
Inventor
一明 遠藤
健次 藤本
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.)
FDK Corp
Original Assignee
FDK Corp
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 FDK Corp filed Critical FDK Corp
Priority to JP10403783A priority Critical patent/JPS59228310A/en
Publication of JPS59228310A publication Critical patent/JPS59228310A/en
Publication of JPH04321B2 publication Critical patent/JPH04321B2/ja
Granted legal-status Critical Current

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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】 本発明は、Ba  (Co、Nbz) Oj−Ba  
(Z”/aN b−/、) 0.系のマイクロ波用誘電
体磁器組成物に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides Ba (Co, Nbz) Oj-Ba
(Z''/aN b-/,) 0. The present invention relates to a dielectric ceramic composition for microwave use.

近年、マイクロ波を利用した自動車電話や衛星放送の受
信器において、誘電体材料を用いIこ共振器やフィルタ
等が用いられている。このような用途で使用される誘電
体材料は、高誘電率、低損失、高安定であることが要望
される。しhXしながら従来使用されている3aQ−T
tQ系あるいはZr O,−Sn Oz−Ti O,系
誘電体材料は、誘電損失が充分に小さいとは言えず、ま
た温度安定性も充分に満足しうるちのではなかつた。特
に、回路技術の向上管に伴い誘電体材料を組込んだ装置
全体として高性能化(例えば高度の温度安定性)が追求
されていくなかで、使用する誘電体材料は、周辺の回路
部分等の温度特性との兼ね合いで、それに適した温度補
償を行なえるような特性を持つことが要求されている。
In recent years, resonators, filters, and the like made of dielectric materials have been used in car telephones and satellite broadcasting receivers that utilize microwaves. Dielectric materials used in such applications are required to have a high dielectric constant, low loss, and high stability. 3aQ-T, which is conventionally used while
The tQ-based or Zr 2 O, -SnOz-Ti 2 O, based dielectric materials cannot be said to have sufficiently small dielectric loss, nor do they have sufficiently satisfactory temperature stability. In particular, as circuit technology improves, the overall performance of devices incorporating dielectric materials (e.g., high temperature stability) is sought after, and the dielectric materials used in the peripheral circuit parts, etc. It is required to have characteristics that can perform temperature compensation suitable for the temperature characteristics.

本発明の目的は、これら従来の誘電体材料の特性を更に
一層改善し、より高い誘電率、より低い損失を呈し、か
つ共振周波数の温度係数を自由に調整しうるようなマイ
クロ波用誘電体磁器組成物を提供することにある。
The purpose of the present invention is to further improve the properties of these conventional dielectric materials, to create a microwave dielectric material that exhibits a higher dielectric constant, lower loss, and can freely adjust the temperature coefficient of the resonant frequency. An object of the present invention is to provide a porcelain composition.

本発明ハ、B a  (Co、N b、、、) O,と
Ba(Zn、7゜N bH) Oshの固溶体とするこ
とによって、得られた誘電体材料のマイクロ波(ミリ波
等も含む)における電気的特性が著しく改善されるとと
もに、その組成割合を変化させることによって共振周波
数の湿度係数を所望の値に自由に調整しうるという事実
の知得に基づき完成されたものである。
In the present invention, by forming a solid solution of B a (Co, N b,...) O and Ba (Zn, 7°N bH) O ) was completed based on the knowledge that the electrical characteristics of the resonant frequency were significantly improved and that the humidity coefficient of the resonant frequency could be freely adjusted to a desired value by changing the composition ratio.

以下、本発明について更に詳しく説明する。The present invention will be explained in more detail below.

本発明は、B a  (G 0IAN 11%) Os
とBa(Znt/。
The present invention provides B a (G 0 IAN 11%) Os
and Ba(Znt/.

N b、A) Ohとの固溶体からなる誘電体磁器組成
物である。そして、その固溶体の組成割合は、全く任意
であってよい。ここで組成を一般式(1%式%) 0、で表わしたとき、組成比×の値が増大するにつれ共
振周波数の温度係数τ(は負側(約−10ppm/℃)
から正側(約+30ppIIl/℃)マチはぼ直線的に
変化する。従って、実際には誘電体材料を用いた共振器
やフィルタが組込まれる装置側からの要求によって、そ
れに最適な温度係数となるよう上記×の値を定めること
になる。
A dielectric ceramic composition consisting of a solid solution with N b, A) Oh. The composition ratio of the solid solution may be completely arbitrary. Here, when the composition is expressed by the general formula (1% formula %) 0, as the value of composition ratio x increases, the temperature coefficient τ of the resonance frequency becomes negative (about -10 ppm/℃)
The gusset changes almost linearly from the positive side (approximately +30 ppIIl/°C). Therefore, in reality, the value of x is determined to provide the optimum temperature coefficient depending on the requirements of the device in which the resonator or filter using the dielectric material is installed.

製法的には従来同様の粉末成形法であってよい。すなわ
ち、仮焼粉体に有機結合剤を加えて造粒し、所定形状に
加圧成形してから焼成すればよい。
The manufacturing method may be a conventional powder molding method. That is, the calcined powder may be granulated by adding an organic binder, pressure-molded into a predetermined shape, and then fired.

本発明は、前述ノ如り、B a  (Cr Oy、N 
bys’) OaとB a  (Z nHN b〃) 
OBとの@溶体とすることによって、誘電損失が充分に
小さく、しかも共振周波数の温度係数を負側から正側ま
で広い範囲で自由に調整できるものであるが、より好ま
しい組成比×の値は0.15  (X (0,75であ
る。
As mentioned above, the present invention provides B a (Cr Oy, N
bys') Oa and B a (Z nHN b〃)
By forming an @ solution with OB, the dielectric loss is sufficiently small and the temperature coefficient of the resonant frequency can be freely adjusted in a wide range from the negative side to the positive side, but the more preferable value of composition ratio x is 0.15 (X (0.75).

この範囲内であれば、共振周波数の温度係数τfは−5
〜+20(ppm/℃)の範囲内に収めることができる
からである。これは装置側からの要求に基づくもので、
通常、この範囲内の任意の値に調整でき、しかち低損失
のものが望まれるからである。
Within this range, the temperature coefficient τf of the resonant frequency is -5
This is because it can be kept within the range of ~+20 (ppm/°C). This is based on a request from the equipment side.
This is because it is generally desired that the value can be adjusted to any value within this range and that the loss is low.

次に実験例について述べる。Next, an experimental example will be described.

実施例 1100℃で6時間焼成して得られたBa  (Cod
N l)%) Oaと3a  (ZnxNby、) O
aの各原料粉体をそれぞれ秤量配合し、ボールミルによ
り40時間微粉砕し乾燥する。これにポリビニルアルコ
ール等の有機結合剤を加えて造粒し、1000〜300
0kQ/Cfの圧力で成形する。次に、この成形体を1
350〜1500℃の温度で2〜40時間焼成する。こ
の焼成品を直径12111+11φ、高さ5.5mmの
円柱に加工することによって、それぞれ組成の異なる7
種類の試料を得た。そして、誘電体共振器法により、誘
電率ε、誘電体1員失tanδ、共振周波数の温度係数
τfを測定した。Ill定)周波数は約6.5G HZ
である。
Example 1 Ba (Cod) obtained by firing at 100°C for 6 hours
N l)%) Oa and 3a (ZnxNby,) O
The raw material powders in a were weighed and blended, pulverized in a ball mill for 40 hours, and dried. Add an organic binder such as polyvinyl alcohol to this, granulate it, and
Molding is performed at a pressure of 0 kQ/Cf. Next, this molded body is
Bake at a temperature of 350-1500°C for 2-40 hours. By processing this fired product into cylinders with a diameter of 12111 + 11φ and a height of 5.5 mm, 7
Various samples were obtained. Then, the dielectric constant ε, the dielectric one-member loss tan δ, and the temperature coefficient τf of the resonance frequency were measured by the dielectric resonator method. Ill constant) frequency is approximately 6.5G HZ
It is.

各試料の組成比Xと電気的特性を第1表に示す。Table 1 shows the composition ratio X and electrical characteristics of each sample.

なお、ここで、Q = 1/ tanδであり、τ(の
単位はppm/ ℃である。また*m1よ、より望まし
い組成比の場合を示して0る。組成比Xに対する共振周
波数の温度係数のグラフを図面に示す。この図面からも
明らかなように、Ba  (Z n N bJ Osの
組成比Xの値が増大するにつれて、共振周波数の温度係
数τ(は1勺−101111)1117℃から約+30
  ppm/℃まで負側hXら1狽11ニはぼ直線的に
変化する。ま1.=、誘電率とも組l戊比Xの増大に伴
って若干大きくなる傾向にある。
Note that here, Q = 1/tan δ, and the unit of τ( is ppm/°C. Also, *m1 indicates the case of a more desirable composition ratio. Temperature coefficient of resonance frequency with respect to composition ratio X The graph of is shown in the drawing.As is clear from this drawing, as the value of the composition ratio Approximately +30
The negative side hX, 1, and 11 changes almost linearly up to ppm/°C. 1. Both the dielectric constant and the dielectric constant tend to increase slightly as the set ratio X increases.

これに対しQは中間部分(0,3(x (0,7)で若
干低下する傾向があるが、し)ずれにせよ6000以上
の良好な値となる。それ故、組成比×の(直を変えるだ
けで共振周波数温度係数を広(1範囲にわたって自由に
調整することができるのである。
On the other hand, Q tends to decrease slightly in the middle part (0, 3 (x (0, 7)), but it has a good value of 6000 or more regardless of the deviation. The resonant frequency temperature coefficient can be freely adjusted over a wide range (one range) by simply changing the .

本発明は上Y(Dように、B a  (Coy、N 1
+=A) 08とB a  (Z n、、N b、、>
 o、との固溶体とづ°ることによって、マイクロ波帯
において誘電率を大きく、誘電損失を極めて小さくする
ことができるとともに、共振周波数の温度係数を負側力
\ら正側に至る広い範囲にわたって自由にhXつ容易に
調整でき、それ故、この誘電体材料h〜らなるマイクロ
波共振器やフィルタと組込んだ装置の温度安定性を著し
く向上させることができるなど、数々のづぐれた効果を
奏しうるちのである。
The present invention is based on the above Y(D, B a (Coy, N 1
+=A) 08 and B a (Z n,, N b,, >
By forming a solid solution with o, it is possible to increase the dielectric constant and extremely reduce dielectric loss in the microwave band, and also to increase the temperature coefficient of the resonant frequency over a wide range from the negative side force to the positive side. It has many outstanding effects, such as being able to freely adjust the dielectric material and therefore significantly improving the temperature stability of devices incorporated with microwave resonators and filters made of this dielectric material. It is Uchino who plays.

【図面の簡単な説明】[Brief explanation of the drawing]

図面は、B a  (Z n/l、N b2/、) o
、の組成比×の変化に対Jる共振周波数の湿度係数でf
の変化を示1−図である。 特許出願人   富士電気化学株式会社代  理  人
       尾  股  行  離間       
  茂  見     槙同      荒 木 友之
助 #L べ 几 X
The drawing is B a (Z n/l, N b2/,) o
, is the humidity coefficient of the resonant frequency with respect to the change in the composition ratio x of
Fig. 1 shows the changes in . Patent Applicant: Fuji Electrochemical Co., Ltd.
Shigeru Makido Araki Tomonosuke #L Be Rin X

Claims (1)

【特許請求の範囲】[Claims] 1、  B a  (G O,lIN b%)  Os
とB a  (Z n、、N b、、)  ONとの固
溶体からなることを特徴とするマイクロ波用誘電体磁器
組成物。
1, B a (G O, IN b%) Os
A dielectric ceramic composition for microwave use, comprising a solid solution of B a (Z n,, N b,,) ON.
JP10403783A 1983-06-10 1983-06-10 Microwave dielectric porcelain composition Granted JPS59228310A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10403783A JPS59228310A (en) 1983-06-10 1983-06-10 Microwave dielectric porcelain composition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10403783A JPS59228310A (en) 1983-06-10 1983-06-10 Microwave dielectric porcelain composition

Publications (2)

Publication Number Publication Date
JPS59228310A true JPS59228310A (en) 1984-12-21
JPH04321B2 JPH04321B2 (en) 1992-01-07

Family

ID=14370023

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10403783A Granted JPS59228310A (en) 1983-06-10 1983-06-10 Microwave dielectric porcelain composition

Country Status (1)

Country Link
JP (1) JPS59228310A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62198006A (en) * 1986-02-25 1987-09-01 宇部興産株式会社 Dielectric porcelain compound
JPH03171506A (en) * 1989-08-11 1991-07-25 Sanyo Electric Co Ltd Dielectric porcelain composite for microwave
JPH05298922A (en) * 1992-04-22 1993-11-12 Oki Electric Ind Co Ltd Dielectric ceramic for microwave

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4630735B2 (en) * 2004-12-28 2011-02-09 東京レーダー株式会社 Radio station distance measurement method

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4915759A (en) * 1972-06-01 1974-02-12
JPS5335453A (en) * 1976-09-14 1978-04-01 Matsushita Electric Ind Co Ltd Dielectric resonator

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4915759A (en) * 1972-06-01 1974-02-12
JPS5335453A (en) * 1976-09-14 1978-04-01 Matsushita Electric Ind Co Ltd Dielectric resonator

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62198006A (en) * 1986-02-25 1987-09-01 宇部興産株式会社 Dielectric porcelain compound
JPH03171506A (en) * 1989-08-11 1991-07-25 Sanyo Electric Co Ltd Dielectric porcelain composite for microwave
JPH05298922A (en) * 1992-04-22 1993-11-12 Oki Electric Ind Co Ltd Dielectric ceramic for microwave

Also Published As

Publication number Publication date
JPH04321B2 (en) 1992-01-07

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