JPH107457A - Dielectric porcelain composition - Google Patents
Dielectric porcelain compositionInfo
- Publication number
- JPH107457A JPH107457A JP8157831A JP15783196A JPH107457A JP H107457 A JPH107457 A JP H107457A JP 8157831 A JP8157831 A JP 8157831A JP 15783196 A JP15783196 A JP 15783196A JP H107457 A JPH107457 A JP H107457A
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- dielectric
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- tio
- dielectric ceramic
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Abstract
(57)【要約】
【課題】 共振周波数の温度係数τf ができるだけ零に
近く,Q×f値が大きく,しかも誘電率εr が大きい誘
電体磁器組成物を提供することる。
【解決手段】 誘電体磁器組成物は,一般式a・CaO
−b・La2 O3 −c・TiO2 (但し,a,b,cの
単位はモル%で示され,10.0≦a≦25.0,1
8.0≦b≦34.0,50.6≦c≦70.0,a+
b+c=100モル%)で示される化学組成を有し,図
1においてABCDEFに囲まれた斜線範囲内にある。
[PROBLEMS] To provide a dielectric ceramic composition having a temperature coefficient τ f of a resonance frequency as close to zero as possible, a large Q × f value, and a large dielectric constant ε r . SOLUTION: The dielectric ceramic composition has a general formula a · CaO.
-B · La 2 O 3 -c · TiO 2 ( where, a, b, units of c is represented by mol%, 10.0 ≦ a ≦ 25.0,1
8.0 ≦ b ≦ 34.0, 50.6 ≦ c ≦ 70.0, a +
b + c = 100 mol%), and is within the hatched area surrounded by ABCDEF in FIG.
Description
【0001】[0001]
【発明の属する技術分野】本発明は,主にマイクロ波帯
域用の通信や放送機器に使用される誘電体磁器組成物に
関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a dielectric porcelain composition mainly used for communication and broadcasting equipment for a microwave band.
【0002】[0002]
【従来の技術】近年,通信技術の進歩により,自動車電
話や携帯電話,PHSなどの移動体通信システム,GP
S(Global Positioning System)が急速に普及してい
る。そのため通信に利用される周波数帯域が拡大し,マ
イクロ波帯域での利用が盛んになっている。2. Description of the Related Art In recent years, with the advance of communication technology, mobile communication systems such as car phones, mobile phones, PHSs,
S (Global Positioning System) is rapidly spreading. For this reason, the frequency band used for communication has been expanded, and the use in the microwave band has become active.
【0003】以前はこのマイクロ波帯域で使用される回
路には,空洞共振器,アンテナ等の使用が主流であっ
た。しかしこれら部品は,マイクロ波の波長と同程度の
大きさになるため,部品の小型化は不可能であった。In the past, circuits used in the microwave band mainly used a cavity resonator, an antenna and the like. However, the size of these components is almost the same as the wavelength of microwaves, so that miniaturization of the components was not possible.
【0004】これに対し,近年マイクロ波フィルタや発
信器の周波数安定化回路に,誘電体共振器を用いること
による回路部品の小型化が一般的となっている。On the other hand, in recent years, it has become common to reduce the size of circuit components by using a dielectric resonator for a frequency stabilizing circuit of a microwave filter or a transmitter.
【0005】このような誘電体共振器に用いられる誘電
体材料に要求される特性は,使用周波数帯域における誘
電体材料の誘電率εr が大きいこと,共振周波数の温度
係数τf ができるだけ零に近いこと,マイクロ波帯域で
の誘電損失tanδ(=1/Q)が小さいことが挙げら
れる。尚マイクロ波帯域での誘電損失tanδの大小
は,一般的にQ×fの形で表現される(fはそのときの
共振周波数)。そのため以下Q×fの表現を用いる。[0005] properties such required for dielectric materials used in the dielectric resonator, dielectric constant epsilon r of the dielectric material in the used frequency band is large, the temperature coefficient tau f is possible zero resonant frequency Closeness and small dielectric loss tan δ (= 1 / Q) in the microwave band. The magnitude of the dielectric loss tan δ in the microwave band is generally expressed in the form of Q × f (f is the resonance frequency at that time). Therefore, the expression of Q × f is used below.
【0006】これまで,マイクロ波用,或いは温度補償
用コンデンサの誘電体磁器組成物としては,Ba(Mg
1/3 Ta2/3 )O3 系,Ba(Zn1/3 Ta2/3 )O3
系,Ba2 Ti9 O20系,ZrO2 −SnO2 −TiO
2 系,BaO−希土類−TiO2 系,(Pb,Ca)Z
rO3 系等の材料が知られている。Hitherto, Ba (Mg) has been used as a dielectric ceramic composition for microwave or temperature compensating capacitors.
1/3 Ta 2/3 ) O 3 system, Ba (Zn 1/3 Ta 2/3 ) O 3
System, Ba 2 Ti 9 O 20 system, ZrO 2 -SnO 2 -TiO
2 system, BaO-rare earth-TiO 2 system, (Pb, Ca) Z
Materials such as rO 3 are known.
【0007】一方,移動体通信に用いられる周波数帯域
は年々高周波側に移行し,かつ細分化している。そのよ
うな移動体通信用に用いられる誘電体フィルタ用の誘電
体材料に要求される特性は,前述のように大きなεr を
有することもさることながら,むしろ高いQ×fを有す
ることも重要となってくる。On the other hand, the frequency band used for mobile communication shifts to the high frequency side year by year and is subdivided. Characteristics required for the dielectric material of such a mobile dielectric filter used for communication while also monkey have a large epsilon r as described above, also important to have a rather high Q × f It becomes.
【0008】[0008]
【発明が解決しようとする課題】しかし,これまでに開
示されている組成の材料では,マイクロ波帯域におい
て,Q×fが大きい程誘電率εr が小さく,εr が大き
いほどQ×fが小さいという傾向があった。例えば,B
a2 Ti9 O20系材料ではQ×f=40000〜600
00GHz(1GHz換算)であるがεr は35〜40
程度であり,BaO−希土類−TiO2 系材料ではεr
=75〜100であるもののQ×fは高々10000程
度である。このようにQ×fが20000GHzを越
え,かつεr が40を越える材料は存在しなかった。[SUMMARY OF THE INVENTION However, in the material of the composition has been previously disclosed, in the microwave band, as the Q × f is large dielectric constant epsilon r is small, epsilon higher r is large Q × f is There was a tendency to be small. For example, B
a × Ti = 40000-600 for a 2 Ti 9 O 20 material
00 GHz (1 GHz conversion), but ε r is 35-40
Ε r for BaO-rare earth-TiO 2 based materials
Although Q = 75-100, Q × f is at most about 10,000. Thus Q × f exceeds the 20000GHz, and epsilon r is the material exceeding 40 was not present.
【0009】しかし,一方では,前述のように移動体通
信に使用される周波数帯域の細分化にともない,更に高
Q×fを有し,かつ高いεr を備えた材料が望まれてい
る。However, on the other hand, as described above, as the frequency band used for mobile communication is subdivided, a material having a higher Q × f and a higher ε r is desired.
【0010】そこで,本発明の技術的課題は,共振周波
数の温度係数τf ができるだけ零に近く,Q×f値が大
きく,しかも誘電率εr が大きい誘電体磁器組成物を提
供することにある。It is an object of the present invention to provide a dielectric ceramic composition having a temperature coefficient τ f of the resonance frequency as close to zero as possible, a large Q × f value, and a large dielectric constant ε r. is there.
【0011】[0011]
【課題を解決するための手段】上記の課題を解決するた
めに,本発明者らは,CaO,La2 O3 ,TiO2を
適当量混合して誘電体磁器組成物を合成することによ
り,共振周波数の温度係数τf が零に近く,Q×f値が
大きく,しかも誘電率εr が比較的大きな誘電体磁器材
料が得られることを見出した。Means for Solving the Problems In order to solve the above problems, the present inventors mixed CaO, La 2 O 3 , and TiO 2 in an appropriate amount to synthesize a dielectric ceramic composition. It has been found that a dielectric ceramic material having a temperature coefficient τ f of the resonance frequency close to zero, a large Q × f value, and a relatively large dielectric constant ε r can be obtained.
【0012】即ち,本発明によれば,一般式a・CaO
−b・La2 O3 −c・TiO2 (ただし,a,b,c
の単位はモル%で示され,10.0≦a≦25.0,1
8.0≦b≦34.0,50.6≦c≦70.0,a+
b+c=100モル%)で示される化学組成を有し,図
1におけるABCDEFに囲まれた斜線範囲内にあるこ
とを特徴とする誘電体磁器組成物が得られる。That is, according to the present invention, the general formula a.CaO
−b · La 2 O 3 −c · TiO 2 (however, a, b, c
Is expressed in mol%, 10.0 ≦ a ≦ 25.0,1
8.0 ≦ b ≦ 34.0, 50.6 ≦ c ≦ 70.0, a +
(b + c = 100 mol%), and a dielectric porcelain composition characterized by being within the hatched area surrounded by ABCDEF in FIG. 1 is obtained.
【0013】[0013]
【発明の実施の形態】以下,本発明の実施の形態につい
て説明する。Embodiments of the present invention will be described below.
【0014】図1は本発明の誘電体磁器組成物の範囲を
示す三角図である。FIG. 1 is a triangular diagram showing the range of the dielectric ceramic composition of the present invention.
【0015】本発明の誘電体磁器組成物は,一般式がa
・CaO−b・La2 O3 −c・TiO2 (ただし,
a,b,cの単位はモル%で示され,10.0≦a≦2
5.0,18.0≦b≦34.0,50.6≦c≦7
0.0,a+b+c=100モル%)で示される化学組
成を有する。The dielectric ceramic composition of the present invention has a general formula of a
・ CaO-b ・ La 2 O 3 −c ・ TiO 2 (However,
The units of a, b, and c are represented by mol%, and 10.0 ≦ a ≦ 2
5.0, 18.0 ≦ b ≦ 34.0, 50.6 ≦ c ≦ 7
0.0, a + b + c = 100 mol%).
【0016】図1において,本発明の誘電体磁器組成物
は,ABCDEFに囲まれた斜線範囲内にある。ここで
各点を(a,b,c)の三角座標で示すと,A=(1
2.0,18.0,70.0),B=(25.0,1
8.0,57.0),C=(25.0,24.4,5
0.6),D=(15.4,34.0,50.6),E
=(10.0,34.0,56.0),F=(10.
0,20.0,70.0)である。In FIG. 1, the dielectric ceramic composition of the present invention is in a hatched area surrounded by ABCDEF. Here, when each point is represented by triangular coordinates of (a, b, c), A = (1
2.0, 18.0, 70.0), B = (25.0, 1
8.0, 57.0), C = (25.0, 24.4, 5)
0.6), D = (15.4, 34.0, 50.6), E
= (10.0, 34.0, 56.0), F = (10.
0, 20.0, 70.0).
【0017】この範囲内の誘電体磁器組成物は,共振周
波数の温度係数τf が零に近く,Q×f=20000G
Hz以上であり,しかも,誘電率εr >40である。The dielectric ceramic composition within this range has a temperature coefficient τ f of resonance frequency close to zero and Q × f = 20,000 G
Hz or more, and the dielectric constant ε r > 40.
【0018】次に,本発明の実施の形態による誘電体磁
器組成物の製造の具体例について説明する。Next, a specific example of the production of the dielectric ceramic composition according to the embodiment of the present invention will be described.
【0019】まず,CaCO3 ,La2 O3 ,TiO2
の各粉末を各組成に応じて秤量した後,純水を用いてジ
ルコニアボールにて樹脂製のボールミルで20時間湿式
混合し,混合物を得た。この混合物を乾燥させた後,大
気中にて1200℃程度の温度で約4時間仮焼し,仮焼
物を得た。次に,仮焼物を上記ボールミルで湿式粉砕
(混合を兼ねる)した後,乾燥,造粒した。これを,直
径15mm,厚さ約6mmの円盤状に成形し,1300
〜1600℃の温度で約2時間焼結することによって下
記表1及び図2に示す組成の誘電体磁器を得た。なお下
記表1での組成は,a・CaO−b・La2 O3 −c・
TiO2 (a+b+c=100モル%)のように表わし
た。First, CaCO 3 , La 2 O 3 , TiO 2
Were weighed according to the respective compositions, and wet-mixed with pure water using zirconia balls in a resin ball mill for 20 hours to obtain a mixture. After drying this mixture, it was calcined in the atmosphere at a temperature of about 1200 ° C. for about 4 hours to obtain a calcined product. Next, the calcined product was wet-pulverized (also serving as mixing) by the ball mill, and then dried and granulated. This was formed into a disk having a diameter of 15 mm and a thickness of about 6 mm.
By sintering at a temperature of about 1600 ° C. for about 2 hours, a dielectric ceramic having the composition shown in Table 1 and FIG. 2 was obtained. Note the composition of the following Table 1, a · CaO-b · La 2 O 3 -c ·
It was represented as TiO 2 (a + b + c = 100 mol%).
【0020】次に,各組成の誘電体磁器について,誘電
体共振器法により,誘電率εr ,Q×f値,共振周波数
の温度係数τf を測定した。共振周波数の温度係数τf
は+20〜+60℃の温度範囲での共振周波数fの差よ
り次数1式によって求めた。Next, the dielectric constant ε r , the Q × f value, and the temperature coefficient τ f of the resonance frequency were measured for the dielectric ceramics of each composition by the dielectric resonator method. Temperature coefficient of resonance frequency τ f
Was determined from the difference of the resonance frequencies f in the temperature range of +20 to + 60 ° C. by the following equation 1.
【0021】[0021]
【数1】 (Equation 1)
【0022】それらの測定結果を表1に示した。なお,
共振周波数は3.0〜4.5GHzであった。Table 1 shows the measurement results. In addition,
The resonance frequency was 3.0 to 4.5 GHz.
【0023】[0023]
【表1】 [Table 1]
【0024】上記表1から明らかなように,本発明にお
けるCaO−La2 O3 −TiO2組成範囲において,
τf <10ppm/℃,Q×f>15000GHzが得
られている。また,εr >40であり,既存の高Q材よ
り大きな値となっている(以上,試料1,3,5,6,
7,8,10,12,14)。As is apparent from Table 1 above, in the composition range of CaO—La 2 O 3 —TiO 2 according to the present invention,
τ f <10 ppm / ° C., Q × f> 15000 GHz are obtained. In addition, ε r > 40, which is a value larger than that of the existing high Q material (above, samples 1, 3, 5, 6,
7, 8, 10, 12, 14).
【0025】一般に高Qの材料としては,例えば移動体
通信基地局用フィルタとして使用される観点から,概ね
|τf |<10ppm/℃,Q×f>15000GHz
であることが要求される。しかし,CaOが25モル%
を超えるとτf <10ppm/℃となり(比較試料
2),またCaOが10モル%を下回ると実用上十分緻
密な焼結体が得られないため(比較試料11)本発明の
範囲から除外される。Generally, as a high-Q material, for example, from the viewpoint of being used as a filter for a mobile communication base station, | τ f | <10 ppm / ° C., Q × f> 15000 GHz
Is required. However, 25 mol% of CaO
If it exceeds τ f <10 ppm / ° C. (Comparative Sample 2), and if CaO is less than 10 mol%, a sufficiently dense sintered body cannot be obtained for practical use (Comparative Sample 11), which is excluded from the scope of the present invention. You.
【0026】また,La2 O3 が34.0モル%を超え
るとQ×f<15000GHzとなり(比較試料1
3),La2 O3 が18モル%を下回るとτf >10p
pm/℃,Q×f<15000GHzとなるため(比較
試料4)が本発明の範囲から除外される。When La 2 O 3 exceeds 34.0 mol%, Q × f <15000 GHz (Comparative Sample 1).
3) When La 2 O 3 is less than 18 mol%, τ f > 10 p
pm / ° C., Q × f <15000 GHz (Comparative Sample 4) is excluded from the scope of the present invention.
【0027】また,TiO2 が70モル%を超えるとQ
×f<15000GHzとなり(比較資料9),TiO
2 が50.6モル%を下回るとτf >10ppm/℃と
なるため(比較試料15)本発明の範囲から除外され
る。When TiO 2 exceeds 70 mol%, Q
× f <15000 GHz (Comparative Data 9), TiO
If 2 is less than 50.6 mol%, τ f > 10 ppm / ° C. (Comparative Sample 15), which is excluded from the scope of the present invention.
【0028】尚,高Qの材料としてはQ×f>2000
0GHzであれば尚望ましいが,本発明における試料は
全てQ×f>20000GHzである。Incidentally, as a high Q material, Q × f> 2000
Although 0 GHz is more preferable, all the samples in the present invention have Q × f> 20,000 GHz.
【0029】[0029]
【発明の効果】以上に説明した通り,本発明によれば,
共振周波数の温度係数τf が零に近く,Q×f値が大き
く,しかも誘電率εr が比較的大きな誘電体磁器組成物
が得られる。As described above, according to the present invention,
A dielectric ceramic composition having a temperature coefficient τ f of the resonance frequency close to zero, a large Q × f value, and a relatively large dielectric constant ε r can be obtained.
【図1】本発明の誘電体磁器組成物の組成範囲を示す三
角図であり,ABCDEFで囲まれた境界線を含む斜線
部が本発明の範囲である。FIG. 1 is a triangular diagram showing a composition range of a dielectric ceramic composition of the present invention, and a hatched portion including a boundary surrounded by ABCDEF is the range of the present invention.
【図2】本発明の実施の形態による誘電体磁器組成物の
組成範囲を示す三角図である。FIG. 2 is a triangular diagram showing a composition range of a dielectric ceramic composition according to an embodiment of the present invention.
1,3,5,6,7,8,10,12,14 表1の
試料番号に対応した本発明の試料 2,4,9,11,13,15 表1の試料番号に対
応した比較試料1,3,5,6,7,8,10,12,14 Samples of the present invention corresponding to the sample numbers in Table 1 2,4,9,11,13,15 Comparative samples corresponding to the sample numbers in Table 1
Claims (1)
・TiO2 (但し,a,b,cの単位はモル%で示さ
れ,10.0≦a≦25.0,18.0≦b≦34.
0,50.6≦c≦70.0,a+b+c=100モル
%)で示される化学組成を有し,図1においてABCD
EFに囲まれた斜線範囲内にあることを特徴とする誘電
体磁器組成物。1. A general formula a · CaO-b · La 2 O 3 -c
TiO 2 (however, the unit of a, b, and c is shown by mol%, and 10.0 ≦ a ≦ 25.0, 18.0 ≦ b ≦ 34.
0,50.6 ≦ c ≦ 70.0, a + b + c = 100 mol%), and ABCD in FIG.
A dielectric porcelain composition characterized by being in a hatched area surrounded by EF.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8157831A JPH107457A (en) | 1996-06-19 | 1996-06-19 | Dielectric porcelain composition |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8157831A JPH107457A (en) | 1996-06-19 | 1996-06-19 | Dielectric porcelain composition |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH107457A true JPH107457A (en) | 1998-01-13 |
Family
ID=15658290
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8157831A Withdrawn JPH107457A (en) | 1996-06-19 | 1996-06-19 | Dielectric porcelain composition |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH107457A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2002047059A (en) * | 2000-07-31 | 2002-02-12 | Kyocera Corp | Glass ceramic sintered body and wiring board using the same |
| GB2402937B (en) * | 2002-03-21 | 2006-06-28 | Council Scient Ind Res | Microwave dielectric ceramic composition,method of manufacture thereof and devices comprising the same |
-
1996
- 1996-06-19 JP JP8157831A patent/JPH107457A/en not_active Withdrawn
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2002047059A (en) * | 2000-07-31 | 2002-02-12 | Kyocera Corp | Glass ceramic sintered body and wiring board using the same |
| GB2402937B (en) * | 2002-03-21 | 2006-06-28 | Council Scient Ind Res | Microwave dielectric ceramic composition,method of manufacture thereof and devices comprising the same |
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