JPH0567589B2 - - Google Patents

Info

Publication number
JPH0567589B2
JPH0567589B2 JP62206439A JP20643987A JPH0567589B2 JP H0567589 B2 JPH0567589 B2 JP H0567589B2 JP 62206439 A JP62206439 A JP 62206439A JP 20643987 A JP20643987 A JP 20643987A JP H0567589 B2 JPH0567589 B2 JP H0567589B2
Authority
JP
Japan
Prior art keywords
mol
temperature coefficient
composition
tio
bao
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
JP62206439A
Other languages
Japanese (ja)
Other versions
JPS6451372A (en
Inventor
Minoru Saito
Kazutoshi Ayusawa
Matsue Nakayama
Toyosaku Sato
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.)
Oki Electric Industry Co Ltd
Original Assignee
Oki Electric Industry 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 Oki Electric Industry Co Ltd filed Critical Oki Electric Industry Co Ltd
Priority to JP62206439A priority Critical patent/JPS6451372A/en
Publication of JPS6451372A publication Critical patent/JPS6451372A/en
Publication of JPH0567589B2 publication Critical patent/JPH0567589B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Compositions Of Oxide Ceramics (AREA)
  • Inorganic Insulating Materials (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

(産業上の利用分野) この発明は、マイクロ波用の誘電体磁器組成物
に関するものである。 (従来の技術) マイクロ波回路用の誘電体共振器や温度補償用
磁器コンデンサなどでは、誘電体磁器組成物とし
て、比誘電率(εr)および無負荷Q(Qu)が大き
く、共振周波数の温度係数(τf)が0を中心にし
て正または負の任意の温度系数が得られることが
必要とされている。 従来、かかる誘電体磁器組成物としては、
BaO・TaO2系、MgTiO3・CaO系、ZrO2
SnO2・TiO2系などが使用されていた。 (発明が解決しようとする問題点) しかし、これらの誘電体磁器組成物を用いて誘
電体共振器やコンデンサンを製造した場合は、そ
の温度係数(τf)が0pmm/℃付近ではその比誘
電率(εr)が20〜40と小さく、その結果、誘電体
共振器などの小形化が不可能であるという欠点が
あつた。 この発明は上記の点に鑑みなされたもので、温
度係数が0付近においても比誘電率(εr)および
無負荷Qが大きく、かつ組成変化によつて広範囲
に温度係数(τf)を変化させることのできる誘電
体磁器組成物を提供することを目的とする。 (問題点を解決するための手段) この発明の誘電体磁器組成物は、(BaO)・
(TiO2x系組成物、酸化サマリウム(Sm2O3)お
よび酸化イツテルビウム(Yb2O3)からなる誘電
体磁器組成物であつて、酸化物換算で BaO:15.0〜18.1モル% TiO2:61.8〜70.3モル% Sm2O3:5〜19モル% Yb2O3:0.5〜12モル% の組成範囲としたことを特徴とするものである。 (作用) 上記のような誘電体磁器組成物は、共振周波数
の温度係数(τf)が0付近でも比誘電率(εr)お
よび無負荷Q(Qu)が大きく、かつ組成変化によ
つて広範囲に温度係数(τf)が変化する。 (実施例) 以下この発明の実施例を説明する。 出発原料として化学的に高純度の炭酸バリウム
(BaCO3)、二酸化チタン(TiO2)、酸化サマリウ
ム(Sm2O3)および酸化イツテルビウム
(Yb2O3)を第1表および第2表に示す組成比率
にて混合し、空気中において1060℃2時間仮焼し
た。
(Industrial Application Field) This invention relates to a dielectric ceramic composition for microwave use. (Prior art) In dielectric resonators for microwave circuits, ceramic capacitors for temperature compensation, etc., dielectric ceramic compositions have large relative permittivity (ε r ) and no-load Q (Qu), and the resonance frequency is low. It is necessary to obtain an arbitrary temperature coefficient whose temperature coefficient (τ f ) is positive or negative around 0. Conventionally, such dielectric ceramic compositions include:
BaO・TaO 2 series, MgTiO 3・CaO series, ZrO 2
SnO 2 and TiO 2 systems were used. (Problem to be solved by the invention) However, when dielectric resonators and capacitors are manufactured using these dielectric ceramic compositions, when the temperature coefficient (τ f ) is around 0 pmm/°C, the ratio decreases. The dielectric constant (ε r ) is as small as 20 to 40, and as a result, it has the disadvantage that it is impossible to miniaturize dielectric resonators and the like. This invention was made in view of the above points, and the relative permittivity (ε r ) and no-load Q are large even when the temperature coefficient is near 0, and the temperature coefficient (τ f ) can be varied over a wide range by changing the composition. It is an object of the present invention to provide a dielectric ceramic composition that can (Means for solving the problem) The dielectric ceramic composition of the present invention has (BaO).
A dielectric ceramic composition consisting of a ( TiO 2 ) 2 : 61.8 to 70.3 mol% Sm2O3 : 5 to 19 mol% Yb2O3 : 0.5 to 12 mol%. (Function) The dielectric ceramic composition described above has a large relative dielectric constant (ε r ) and no-load Q (Qu) even when the temperature coefficient (τ f ) of the resonance frequency is around 0, and the The temperature coefficient (τ f ) changes over a wide range. (Example) Examples of the present invention will be described below. Chemically high-purity barium carbonate (BaCO 3 ), titanium dioxide (TiO 2 ), samarium oxide (Sm 2 O 3 ) and ytterbium oxide (Yb 2 O 3 ) are used as starting materials in Tables 1 and 2. They were mixed at the composition ratio shown and calcined in air at 1060°C for 2 hours.

【表】【table】

【表】 得られた仮焼物をポツトミルで純水とともに湿
式粉砕し、脱水乾燥後バインダを添加し造粒し32
メツシユのフルイを通して整粒した。得られた造
粒粉は金型と油圧プレスを用いて成形圧力1〜
3ton/cm2で直径16mmφ厚さ9mmの円板状の成形体
とした。そして、この成形体を高純度のアルミナ
厘に入れ、1260℃〜1450℃2時間の焼成条件で焼
成し、誘導体磁器組成物を得た。 得られた磁器組成物についてハツキ・コールマ
ン法により比誘電率(εr)および無負荷Q(Qu)
を測定した。また、共振周波数の温度係数(τf
は下記(1)式に従つて20℃における共振周波数を基
準にして−30℃〜70℃の温度範囲における値から
求めた。それらの結果を第2表に示す。これらの
測定における共振周波数は3〜5GHzであつた。 τf=f(70)−f(−30)/f(20)・1/△T(ppm
/℃)…(1) ただし、 f(20):20℃における共振周波数 f(−30):−30℃における共振周波数 f(70):70℃における共振周波数 △T:測定温度差、ここでは70+30=100℃ 第2表において、*印を付した試料番号のもの
は本発明の範囲外の比較例であり、それ以外の試
料が本発明範囲内の実施例である。 第1表及び第2表の結果によれば、(BaO)・
(TiO2xが75モル%未満ならびに87モル%を超え
ると無負荷Q(Qu)が小さく、比誘電率(εr)も
小さくなり不適当である。また、Sm2O3が5モ
ル%未満ならびに19モル%を超えると無負荷Q
(Qu)が小さくなり比誘電率(εr)も小さくなり
不適当である。さらに、Yb2O3が0.5モル%未満
ならびに12モル%を超えると無負荷Q(Qu)が小
さく、εrも小さくなり不適当である。 したがつて、実用的にみて、(BaO)・(TiO2
×:75〜87モル%、Sm2O3:5〜19モル%、
Yb2O3:0.5〜12モル%の範囲が適当である。こ
こで、(BaO)・(TiO2xのxは3.8〜4.2であるこ
とから、BaO:15.0〜18.1モル%、TiO2:61.8〜
70.3モル%、Sm2O3:5〜19モル%、Yb2O3:0.5
〜12モル%の範囲が適当である。 また、前記第2表によれば、本発明の磁器組成
物は、共振周波数の温度係数(τf)が0付近で大
きな比誘電率(εr)と無負荷Q(Qu)が得られて
いることが分り、さらに組成変化によつて広範囲
に温度係数が変化することが分る。 (発明の効果) 以上のように、この発明の誘電体磁器組成物
は、マイクロ波領域において、共振周波数の温度
係数が0付近においても無負荷Qおよび比誘電率
が大きく、空に組成変化によつて広範囲に温度係
数τfを変化させることができる。よつて、マイク
ロ波誘電体共振器あるいは温度補償用コンデンサ
などの誘電体磁器組成物として利用してそれらの
小型化を図ることができ、その工業的価値は大で
ある。
[Table] The obtained calcined product was wet-pulverized with pure water in a pot mill, and after dehydration and drying, a binder was added and granulated.
The grains were sized through a mesh sieve. The obtained granulated powder is molded using a mold and a hydraulic press under a molding pressure of 1~
A disc-shaped molded product with a diameter of 16 mm and a thickness of 9 mm was made at 3 ton/cm 2 . Then, this molded body was placed in a high-purity alumina pot and fired under firing conditions of 1260°C to 1450°C for 2 hours to obtain a dielectric ceramic composition. The relative dielectric constant (ε r ) and unloaded Q (Qu) of the obtained porcelain composition were determined by the Hatsuki-Coleman method.
was measured. Also, the temperature coefficient of the resonant frequency (τ f )
was determined from values in the temperature range of -30°C to 70°C based on the resonance frequency at 20°C according to equation (1) below. The results are shown in Table 2. The resonant frequency in these measurements was 3-5 GHz. τ f = f(70)-f(-30)/f(20)・1/△T(ppm
/℃)...(1) However, f(20): Resonance frequency at 20℃ f(-30): Resonance frequency at -30℃ f(70): Resonance frequency at 70℃ △T: Measured temperature difference, here 70+30=100°C In Table 2, the sample numbers marked with * are comparative examples outside the scope of the present invention, and the other samples are examples within the scope of the present invention. According to the results in Tables 1 and 2, (BaO)・
(TiO 2 ) If x is less than 75 mol% or exceeds 87 mol%, the unloaded Q (Qu) will be small and the relative permittivity (ε r ) will also be small, making it unsuitable. In addition, if Sm 2 O 3 is less than 5 mol% or exceeds 19 mol%, the unloaded Q
(Qu) becomes small and the relative dielectric constant (ε r ) also becomes small, which is inappropriate. Furthermore, if Yb 2 O 3 is less than 0.5 mol % or exceeds 12 mol %, the unloaded Q (Qu) will be small and ε r will also be small, which is inappropriate. Therefore, from a practical point of view, (BaO)・(TiO 2 )
× : 75 to 87 mol% , Sm2O3 : 5 to 19 mol%,
Yb 2 O 3 : A range of 0.5 to 12 mol% is appropriate. Here, since x of (BaO)/(TiO 2 ) x is 3.8 to 4.2, BaO: 15.0 to 18.1 mol%, TiO 2 : 61.8 to
70.3 mol% , Sm2O3 : 5-19 mol%, Yb2O3 : 0.5
A range of 12 mol % is suitable. Further, according to Table 2, the ceramic composition of the present invention has a large relative dielectric constant (ε r ) and no-load Q (Qu) when the temperature coefficient (τ f ) of the resonance frequency is around 0. It is found that the temperature coefficient changes over a wide range due to changes in composition. (Effects of the Invention) As described above, the dielectric ceramic composition of the present invention has a large no-load Q and a large relative dielectric constant even when the temperature coefficient of the resonant frequency is near 0 in the microwave region, and is susceptible to compositional changes in the microwave region. Therefore, the temperature coefficient τ f can be varied over a wide range. Therefore, it can be used as a dielectric ceramic composition for microwave dielectric resonators, temperature compensation capacitors, etc. to reduce their size, and its industrial value is great.

Claims (1)

【特許請求の範囲】 1 (BaO)・(TiO2x系組成物、酸化サマリウ
ム(Sm2O3)および酸化イツテルビウム
(Yb2O3)からなる誘電体磁器組成物であつて、
酸化物換算で BaO:15.0〜18.1モル% TiO2:61.8〜70.3モル% Sm2O3:5〜19モル% Yb2O3:0.5〜12モル% の組成範囲としたことを特徴とする誘電体磁器組
成物。
[Scope of Claims] 1 A dielectric ceramic composition comprising a (BaO)/(TiO 2 ) x -based composition, samarium oxide (Sm 2 O 3 ) and ytterbium oxide (Yb 2 O 3 ),
A dielectric characterized by having a composition range of BaO: 15.0 to 18.1 mol%, TiO 2 : 61.8 to 70.3 mol%, Sm 2 O 3 : 5 to 19 mol%, Yb 2 O 3 : 0.5 to 12 mol%, in terms of oxides. Body porcelain composition.
JP62206439A 1987-08-21 1987-08-21 Dielectric porcelain composition Granted JPS6451372A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62206439A JPS6451372A (en) 1987-08-21 1987-08-21 Dielectric porcelain composition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62206439A JPS6451372A (en) 1987-08-21 1987-08-21 Dielectric porcelain composition

Publications (2)

Publication Number Publication Date
JPS6451372A JPS6451372A (en) 1989-02-27
JPH0567589B2 true JPH0567589B2 (en) 1993-09-27

Family

ID=16523395

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62206439A Granted JPS6451372A (en) 1987-08-21 1987-08-21 Dielectric porcelain composition

Country Status (1)

Country Link
JP (1) JPS6451372A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009053808A (en) 2007-08-24 2009-03-12 Fuji Xerox Co Ltd Image forming apparatus, authentication information management method, and program

Also Published As

Publication number Publication date
JPS6451372A (en) 1989-02-27

Similar Documents

Publication Publication Date Title
JPS6118283B2 (en)
JP2974829B2 (en) Microwave dielectric porcelain composition
US5432135A (en) Dielectric ceramic composition for high frequency
JPH0255884B2 (en)
JP2501649B2 (en) Microwave dielectric ceramics
JPH0567589B2 (en)
JPH0742165B2 (en) Microwave dielectric ceramics
JP2731940B2 (en) Dielectric ceramics for microwave
JP3243874B2 (en) Dielectric porcelain composition
JPH0415963B2 (en)
JPS6112865B2 (en)
JPS5951095B2 (en) dielectric porcelain composition
JPH0785363B2 (en) Microwave dielectric ceramics
JPH0571538B2 (en)
JPH0567588B2 (en)
JPH0256305B2 (en)
JPH0415962B2 (en)
JPH06325620A (en) Dielectric ceramic composition
JPS6054269B2 (en) dielectric porcelain composition
JPS63291866A (en) Porcelaneous composition
KR950008599B1 (en) Composition of deelectric substance
JPH0460072B2 (en)
JPH0563882B2 (en)
JPS62187161A (en) Dielectric ceramic composition
JPH06102572B2 (en) High frequency dielectric ceramic composition