JP2579138B2 - Microwave dielectric composition - Google Patents
Microwave dielectric compositionInfo
- Publication number
- JP2579138B2 JP2579138B2 JP7148789A JP14878995A JP2579138B2 JP 2579138 B2 JP2579138 B2 JP 2579138B2 JP 7148789 A JP7148789 A JP 7148789A JP 14878995 A JP14878995 A JP 14878995A JP 2579138 B2 JP2579138 B2 JP 2579138B2
- Authority
- JP
- Japan
- Prior art keywords
- dielectric
- temperature coefficient
- composition
- resonance frequency
- tio
- 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.)
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
- H01B3/00—Insulators or insulating bodies characterised by the insulating materials; Selection of materials for their insulating or dielectric properties
- H01B3/02—Insulators or insulating bodies characterised by the insulating materials; Selection of materials for their insulating or dielectric properties mainly consisting of inorganic substances
- H01B3/12—Insulators or insulating bodies characterised by the insulating materials; Selection of materials for their insulating or dielectric properties mainly consisting of inorganic substances ceramics
-
- C—CHEMISTRY; METALLURGY
- C04—CEMENTS; CONCRETE; ARTIFICIAL STONE; CERAMICS; REFRACTORIES
- C04B—LIME, MAGNESIA; SLAG; CEMENTS; COMPOSITIONS THEREOF, e.g. MORTARS, CONCRETE OR LIKE BUILDING MATERIALS; ARTIFICIAL STONE; CERAMICS; REFRACTORIES; TREATMENT OF NATURAL STONE
- C04B35/00—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products
- C04B35/01—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics
- C04B35/46—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics based on titanium oxides or titanates
- C04B35/462—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics based on titanium oxides or titanates based on titanates
- C04B35/465—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics based on titanium oxides or titanates based on titanates based on alkaline earth metal titanates
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P7/00—Resonators of the waveguide type
- H01P7/10—Dielectric resonators
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- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Ceramic Engineering (AREA)
- Manufacturing & Machinery (AREA)
- Materials Engineering (AREA)
- Structural Engineering (AREA)
- Organic Chemistry (AREA)
- Inorganic Chemistry (AREA)
- Inorganic Insulating Materials (AREA)
- Compositions Of Oxide Ceramics (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、誘電損失が小さく、共
振周波数の温度係数が良好なマイクロ波用誘電体磁気組
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 microwave dielectric magnetic composition having a small dielectric loss and a good temperature coefficient of resonance frequency.
【0002】[0002]
【従来の技術】最近、無線電話機、自動車電話機等の移
動通信、衛星放送、衛星通信等に周波数帯域300MHz
〜300GHz のマイクロ波を利用した通信システムが著
しく発展している。かかるニューメディアの実用化のた
め、共振器、帯域通過(又は阻止)フィルタ及びマイク
ロ波集積回路(MIC)等にマイクロ波用誘電体セラミ
ックの応用が大きく増加している。このマイクロ波用誘
電体を通信システムに応用する場合、(1)誘電体内に
おいてマイクロ波の波長は誘電率の1/2乗に反比例す
るので、部品の小型化のためには誘電率が大きくなけれ
ばならず、(2)誘電損失は周波数に比例して増加する
ので、高性能化のためにはQ値(即ち、誘電損失の逆
数)が大きくなければならず、(3)誘電体共振器の共
振周波数の温度係数が小さくなければならない〔ワーシ
ング(W. Wersing)のElectronic Ceramics (B.C.H. Stee
le編著)、67頁、アメリカ合衆国ニューヨーク州所在の
Elsevier Sci, Pub, Co, (1991) 参照〕。なお、通信シ
ステムに用いているマイクロ波用誘電体は、経時変化が
小さく、熱伝導率が大きく、かつ機械的強度が良好でな
ければならない。今まで開発された誘電体としては、B
a(M+2 1/3 M+5 2/3 )O3 (M+2=Mg,Zn,M+5
=Ta,Nb)系、Ba2 Ti9 O20系及び(Zr,S
n)TiO4 系を挙げることができる。前記類型の誘電
体は誘電率が40以下であるが、誘電損失が低い。また
他の例としては、BaO−Sm2 O3 −TiO2 系、
(Ba,Pb)O−Nd2 O3 −TiO2 系及び(P
b,Ca)ZrO3 系を挙げることができるが、この誘
電体の誘電損失は比較的に大きい(Qxfo(GHz) <1
0,000)が、誘電率が80以上であると知られてい
る〔前記ワーシング文献;及びJ. Kato, JEE, Sep., 11
4-118(1991) 参照〕。2. Description of the Related Art Recently, a frequency band of 300 MHz has been used for mobile communications, such as radio telephones and automobile telephones, satellite broadcasting, and satellite communications.
Communication systems using microwaves of up to 300 GHz have been remarkably developed. For the practical use of such new media, applications of dielectric ceramics for microwaves to resonators, band-pass (or blocking) filters, microwave integrated circuits (MICs), and the like have been greatly increased. When this microwave dielectric is applied to a communication system, (1) the wavelength of the microwave in the dielectric is inversely proportional to the 乗 power of the dielectric constant. (2) Since the dielectric loss increases in proportion to the frequency, the Q value (that is, the reciprocal of the dielectric loss) must be large for high performance, and (3) the dielectric resonator The temperature coefficient of the resonant frequency must be low [Werthing Electronic Ceramics (BCH Stee
le), 67 pages, New York, USA
Elsevier Sci, Pub, Co, (1991)]. The microwave dielectric used in the communication system must have a small change with time, a high thermal conductivity, and a good mechanical strength. As the dielectrics developed so far, B
a (M +2 1/3 M +5 2/3 ) O 3 (M +2 = Mg, Zn, M +5
= Ta, Nb), Ba 2 Ti 9 O 20 and (Zr, S
n) TiO 4 system can be mentioned. This type of dielectric has a dielectric constant of 40 or less, but has a low dielectric loss. As another example, BaO—Sm 2 O 3 —TiO 2 system,
(Ba, Pb) O—Nd 2 O 3 —TiO 2 and (P
b, Ca) ZrO 3 system, but the dielectric loss of this dielectric is relatively large (Qxfo (GHz) <1
000) is known to have a dielectric constant of 80 or more [the above-mentioned Worthing reference; and J. Kato, JEE, Sep., 11].
4-118 (1991)].
【0003】[0003]
【発明が解決しようとする課題】一般的に誘電率が大き
い材料は、誘電体内部の双極子の欠陥等により誘電損失
と共振周波数の温度係数が増加するが、マイクロ波用誘
電体は、共振周波数の温度係数が優先的に±10ppm/℃
程度に安定しなければ応用することができない。(S
r,Ca)TiO3 の場合、2GHz での誘電率は255
〜170程で非常に高いが、共振周波数の温度係数が+
1670〜+800ppm/℃であるため、実用上非常に大
きい問題点がある。一方、Nd(Mg1/2 Ti1/2 )O
3 の場合には、誘電率は24程で低いが、Qxfo(GH
z) が65000程で非常に高く、また共振周波数の温
度係数は−53ppm/℃程である。したがって、本発明の
目的は、誘電率が30以上で大きいながらも、誘電損失
が小さいマイクロ波用誘電体組成物を提供することであ
る。本発明の他の目的は、共振周波数の温度係数を0pp
m/℃を中心として+又は−の方向に必要に応じて容易に
調節できるマイクロ波用誘電体組成物を提供することで
ある。Generally, a material having a large dielectric constant has an increase in dielectric loss and a temperature coefficient of a resonance frequency due to a defect of a dipole inside the dielectric. Temperature coefficient of frequency is preferentially ± 10ppm / ℃
If it is not stable enough, it cannot be applied. (S
In the case of (r, Ca) TiO 3 , the dielectric constant at 2 GHz is 255
It is very high at about 170, but the temperature coefficient of the resonance frequency is +
Since it is 1670 to +800 ppm / ° C., there is a very large problem in practical use. On the other hand, Nd (Mg 1/2 Ti 1/2 ) O
In the case of 3 , the dielectric constant is as low as about 24, but Qxfo (GH
z) is as high as about 65000, and the temperature coefficient of the resonance frequency is about -53 ppm / ° C. Therefore, an object of the present invention is to provide a microwave dielectric composition having a small dielectric loss while having a large dielectric constant of 30 or more. Another object of the present invention is to set the temperature coefficient of the resonance frequency to 0 pp.
An object of the present invention is to provide a microwave dielectric composition that can be easily adjusted in the + or-direction around m / C as needed.
【0004】[0004]
【課題を解決するための手段】前記のような本発明の目
的は、下記組成式で示されるマイクロ波用誘電体磁気組
成物を提供することによって達成される。 (1−y)(Sr1-x Cax )TiO3 ・yNd(Mg
1/2 Ti1/2 )O3 式中、0.01≦x≦1.0、0.3≦y≦0.6であ
る。本発明による誘電体磁気組成物は、例えば、SrC
O3 ,CaCO3 ,Nd2O3 ,TiO2 及びMgOを
出発物質として用いて当該分野で公知にされている通常
の方法で処理することにより製造できる。具体的に説明
すると、SrCO3,CaCO3 ,Nd2 O3 ,TiO2
及びMgOを所定の組成比で混合して得た粉末を大気
中、例えば1,050℃の温度で約10時間か焼した後
粉砕し、更に1,200〜1,300℃で充分な時間、
例えば6時間再びか焼してペロブスカイト構造を有する
固溶体を合成する。この合成粉末をよく粉砕した後、例
えば直径10mm、厚さ1〜2mmの円板型試片に加圧成形
して、大気中、例えば1,500〜1,650℃の温度
で2時間〜6時間焼結することにより製造できる。この
際、焼結温度はMgOの含量が増加するにつれ高くな
る。焼結後試片の収縮率は12〜20%である。The above objects of the present invention can be attained by providing a dielectric magnetic composition for microwaves represented by the following composition formula. (1-y) (Sr 1 -x Ca x) TiO 3 · yNd (Mg
1/2 Ti 1/2 ) O 3 In the formula, 0.01 ≦ x ≦ 1.0 and 0.3 ≦ y ≦ 0.6. The dielectric magnetic composition according to the present invention comprises, for example, SrC
It can be prepared by using O 3 , CaCO 3 , Nd 2 O 3 , TiO 2 and MgO as starting materials and treating in a usual manner known in the art. Specifically, SrCO 3 , CaCO 3 , Nd 2 O 3 , TiO 2
And a powder obtained by mixing MgO at a predetermined composition ratio is calcined in the air, for example, at a temperature of 1,050 ° C. for about 10 hours, and then pulverized, and further at 1,200 to 1,300 ° C. for a sufficient time,
For example, the solution is calcined again for 6 hours to synthesize a solid solution having a perovskite structure. After this synthetic powder is pulverized well, it is pressed into a disk-shaped specimen having a diameter of, for example, 10 mm and a thickness of 1 to 2 mm, and is heated in air at a temperature of, for example, 1,500 to 1,650 ° C. for 2 hours to 6 hours. It can be manufactured by sintering for a time. At this time, the sintering temperature increases as the content of MgO increases. After the sintering, the shrinkage of the specimen is 12 to 20%.
【0005】焼結試片の誘電率、Q値及び共振周波数の
温度計数等の誘電特性は公知にされている誘電体共振技
法により測定することができる。The dielectric properties of the sintered specimen, such as the dielectric constant, Q value, and temperature counting of the resonance frequency, can be measured by a known dielectric resonance technique.
【0006】[0006]
【作用】本発明によるマイクロ波用誘電体磁気組成物
は、誘電率は約30〜60、Qxfo(GHz) が約9,5
00〜50,000、共振周波数の温度係数(TCF)
が約−60〜+60ppm/℃であって、前記の通りマイク
ロ波用誘電体セラミックスが要求する通信システムに適
した形で利用できる。尚、本発明のマイクロ波用誘電体
磁気組成物は、SrTiO3 ,CaTiO3及びNd
(Mg1/2 Ti1/2 )O3 を主成分とするペロブスカイ
ト型固溶体であって、各成分の組成範囲は後記表1の試
料組成例に示す通りである。かかる範囲の組成を有する
誘電体組成物は、共振周波数の温度係数が約±60ppm/
℃であるため、そのまま又は添加剤を少量添加すること
によって、誘電損失が小さく、かつ温度特性が良好なマ
イクロ波誘電体磁気を得ることができる。The dielectric magnetic composition for microwaves according to the present invention has a dielectric constant of about 30 to 60 and a Qxfo (GHz) of about 9.5.
00 to 50,000, temperature coefficient of resonance frequency (TCF)
Is about −60 to +60 ppm / ° C., and can be used in a form suitable for a communication system required by dielectric ceramics for microwaves as described above. Incidentally, the dielectric magnetic composition for microwaves of the present invention comprises SrTiO 3 , CaTiO 3 and Nd.
This is a perovskite-type solid solution containing (Mg 1/2 Ti 1/2 ) O 3 as a main component, and the composition range of each component is as shown in a sample composition example in Table 1 below. A dielectric composition having a composition in such a range has a temperature coefficient of resonance frequency of about ± 60 ppm /
Since the temperature is ° C, microwave dielectric magnetism having small dielectric loss and good temperature characteristics can be obtained as it is or by adding a small amount of an additive.
【0007】本発明の誘電体磁気組成物の特性は、Sr
TiO3 及びCaTiO3 の量により大きく変化する。
SrTiO3 及びCaTiO3 の含量が増加するに従っ
て誘電率は30〜60範囲で次第に増加するが、Qxf
o(GHz) は大きく減少し、共振周波数の温度係数は図1
に示す通り、−から+に漸進的に変化する。特に、Sr
TiO3 及びCaTiO3 の含量が0.4〜0.5モル
付近では誘電率が41〜48、Qxfo(GHz) が30,
000以上、共振周波数の温度係数が10ppm/℃以下で
ある優れたマイクロ波用誘電体磁気を製造することがで
きる。一方、SrTiO3 及びCaTiO3 の含量を少
量調節することによって、同一製造条件下で共振周波数
の温度係数を0ppm/℃を中心として自由に+と−に制御
することができる。The characteristics of the dielectric magnetic composition of the present invention are as follows: Sr
It changes greatly depending on the amount of TiO 3 and CaTiO 3 .
As the content of SrTiO 3 and CaTiO 3 increases, the dielectric constant gradually increases in the range of 30 to 60, but Qxf
o (GHz) is greatly reduced, and the temperature coefficient of the resonance frequency is
As shown in FIG. In particular, Sr
When the content of TiO 3 and CaTiO 3 is around 0.4 to 0.5 mol, the dielectric constant is 41 to 48, Qxfo (GHz) is 30,
An excellent dielectric magnetism for microwaves having a temperature coefficient of the resonance frequency of not less than 000 and not more than 10 ppm / ° C. can be manufactured. On the other hand, by adjusting the contents of SrTiO 3 and CaTiO 3 in a small amount, the temperature coefficient of the resonance frequency can be freely controlled to be + or − around 0 ppm / ° C. under the same manufacturing conditions.
【0008】[0008]
【実施例】以下、本発明を実施例により更に詳しく説明
する。しかし、本発明はこの実施例により限定されるの
ではない。純度99.9%のSrCO3 ,CaCO3 ,
Nd2 O3 ,TiO2 及びMgOを下記表1に示した組
成になるように各原料を正確に秤量した後、互いに混合
した。混合粉末を大気中の1,050℃で約10時間か
焼した後粉砕し、更に1,200〜1,300℃で6時
間か焼してペロブスカイト構造を有する固溶体を合成し
た。合成粉末をよく粉砕した後、直径10mm、厚さ1〜
2mmの円板型試片に加圧成形して、大気中、1,500
〜1,650℃で2時間〜6時間焼結した。焼結後、試
片は12〜20%程収縮した。焼結試片の両面を研磨紙
(#3000まで)でよく研磨した後、導波管中に入れ
て誘電体共振技法で誘電率、Q値及び共振周波数の温度
係数を測定した。この際、測定周波数は8〜12GHz で
あり、測定温度範囲は−15〜85℃であった。各試片
のマイクロ波誘電特性を表1に示した。The present invention will be described below in more detail with reference to examples. However, the present invention is not limited by this embodiment. 99.9% pure SrCO 3 , CaCO 3 ,
Nd 2 O 3 , TiO 2 and MgO were accurately weighed so as to have the compositions shown in Table 1 below, and then mixed together. The mixed powder was calcined at 1,050 ° C. in the air for about 10 hours and then pulverized, and further calcined at 1,200 to 1,300 ° C. for 6 hours to synthesize a solid solution having a perovskite structure. After crushing the synthetic powder well, the diameter is 10mm, thickness is 1 ~
It is press-formed into a 2 mm disk-shaped specimen,
Sintered at 1,1,650 ° C. for 2 to 6 hours. After sintering, the specimen shrunk by about 12 to 20%. After the both sides of the sintered specimen were polished well with abrasive paper (up to # 3000), they were placed in a waveguide, and the dielectric constant, the Q value, and the temperature coefficient of the resonance frequency were measured by a dielectric resonance technique. At this time, the measurement frequency was 8 to 12 GHz, and the measurement temperature range was -15 to 85 ° C. Table 1 shows the microwave dielectric properties of each specimen.
【0009】[0009]
【表1】 [Table 1]
【0010】前記表1に示す通り、誘電特性はNd(M
g1/2 Ti1/2 )O3 の量によっては大きな変化がない
が、SrTiO3 及びCaTiO3 の量によって大きく
変化している。即ち、SrTiO3 及びCaTiO3 の
含量が増加するに従って、誘電率は30〜60の範囲で
徐々増加する一方、Qxfo(GHz) は大きく減少し、共
振周波数の温度係数は−から+に漸進的に変化すること
が分かる。As shown in Table 1, the dielectric properties are Nd (M
g 1/2 Ti 1/2 ) O 3 , there is no significant change, but the amount greatly changes depending on the amounts of SrTiO 3 and CaTiO 3 . That is, according to the content of SrTiO 3 and CaTiO 3 is increased, whereas the dielectric constant is gradually increased in the range of 30~60, Qxfo (GHz) is greatly reduced, the temperature coefficient of resonant frequency - progressively from + It can be seen that it changes.
【0011】[0011]
【発明の効果】本発明によると、SrTiO3 、CaT
iO3 及びNd(Mg1/2 Ti1/2 )O3 を主成分とす
るペロブスカイト型固溶体からなる、マイクロ波用誘電
体磁気組成物の共振周波数の温度係数が、従来の誘電体
磁気組成物とは異なり±60ppm/℃であって、そのまま
又は添加剤を少量添加することによって、誘電損失が小
さく、かつ温度特性が良好なマイクロ波誘電体磁気を形
成することができる。According to the present invention, SrTiO 3 , CaT
The temperature coefficient of the resonant frequency of a dielectric magnetic composition for microwaves composed of a perovskite-type solid solution containing iO 3 and Nd (Mg 1/2 Ti 1/2 ) O 3 as main components is smaller than that of a conventional dielectric magnetic composition. Unlike this, it is ± 60 ppm / ° C., and by itself or by adding a small amount of an additive, it is possible to form a microwave dielectric magnet having small dielectric loss and excellent temperature characteristics.
【図1】本発明による誘電体共振器の組成変化による共
振周波数の温度係数特性を示したグラフである。FIG. 1 is a graph showing a temperature coefficient characteristic of a resonance frequency according to a composition change of a dielectric resonator according to the present invention.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 尹 錫 珍 大韓民国ソウル特別市蘆原区上渓洞6番 地 住公アパート203棟810号 (72)発明者 中村 哲郎 神奈川県横浜市緑区藤ガ丘2−41−21 藤ガ丘宿舎403 (72)発明者 伊藤 満 神奈川県横浜市緑区桜台33−7 桜台コ ートビレッジ1−11 (72)発明者 孫 正 鎬 大韓民国大邱広域市大鳳1洞187番地6 号 (56)参考文献 特開 平8−217535(JP,A) 特開 平4−118807(JP,A) 特開 昭63−138605(JP,A) ──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Yun Sin Jin 203, 810, Janggyeong-dong, Sewon-dong, Awon-gu, Seoul, Republic of Korea (72) Inventor Tetsuro Nakamura Fujiga, Midori-ku, Yokohama-shi, Kanagawa Oka 2-41-21 Fujigaoka Dormitory 403 (72) Inventor Mitsuru Mitsuru 33-7 Sakuradai, Midori-ku, Yokohama-shi, Kanagawa Prefecture 1-11 Sakuradai Court Village 1-11 (72) Inventor Masaho Son 1 Daepo 1-dong, Daegu, Republic of Korea 187 No. 6 (56) References JP-A-8-217535 (JP, A) JP-A-4-118807 (JP, A) JP-A-63-138605 (JP, A)
Claims (1)
体組成物。 (1−y)(Sr1-x Cax )TiO3 ・yNd(Mg
1/2 Ti1/2 )O3 式中、0.01≦x≦1.0、0.3≦y≦0.6であ
る。1. A microwave dielectric composition represented by the following composition formula: (1-y) (Sr 1 -x Ca x) TiO 3 · yNd (Mg
1/2 Ti 1/2 ) O 3 In the formula, 0.01 ≦ x ≦ 1.0 and 0.3 ≦ y ≦ 0.6.
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KR1019940015403A KR960012729B1 (en) | 1994-06-30 | 1994-06-30 | Dielectric composition for microwave frequencies |
KR15403/1994 | 1994-06-30 |
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JPH0817244A JPH0817244A (en) | 1996-01-19 |
JP2579138B2 true JP2579138B2 (en) | 1997-02-05 |
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ID=19386803
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KR960012729B1 (en) | 1996-09-24 |
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