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JP5458927B2 - High frequency dielectric ceramic, method for manufacturing the same, and high frequency circuit element using the same - Google Patents
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JP5458927B2 - High frequency dielectric ceramic, method for manufacturing the same, and high frequency circuit element using the same - Google Patents

High frequency dielectric ceramic, method for manufacturing the same, and high frequency circuit element using the same Download PDF

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JP5458927B2
JP5458927B2 JP2010029619A JP2010029619A JP5458927B2 JP 5458927 B2 JP5458927 B2 JP 5458927B2 JP 2010029619 A JP2010029619 A JP 2010029619A JP 2010029619 A JP2010029619 A JP 2010029619A JP 5458927 B2 JP5458927 B2 JP 5458927B2
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孝史 河野
正孝 山永
敦 岡部
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Description

本発明は、マイクロ波及びミリ波等の高周波域で使用される高周波回路素子を構成する部材として好適な高周波用誘電体磁器に関する。このような高周波用誘電体磁器の例としては、例えば、誘電体共振器、誘電体導波路および誘電体アンテナなどの構成部材である誘電体ブロックや誘電体基板、さらには各種高周波回路素子において使用される基板及び支持部材などが挙げられる。高周波回路素子は、例えば、高周波域の通信機器などの電子装置を構成する。   The present invention relates to a high frequency dielectric ceramic suitable as a member constituting a high frequency circuit element used in a high frequency region such as a microwave and a millimeter wave. Examples of such high-frequency dielectric ceramics are used in dielectric blocks, dielectric substrates, and various high-frequency circuit elements, which are components such as dielectric resonators, dielectric waveguides, and dielectric antennas. And a substrate and a supporting member. The high-frequency circuit element constitutes an electronic device such as a communication device in a high-frequency range, for example.

誘電体共振器の最も基本的なものとして、同軸誘電体共振器が挙げられる。この同軸誘電体共振器では、誘電体磁器からなるブロックに貫通孔を設け、該貫通孔が開口するブロックの一面(開放面)だけは誘電体磁器の表面そのままの状態とし、誘電体磁器の他の表面及び貫通孔内面には導体膜を形成している。   The most basic dielectric resonator is a coaxial dielectric resonator. In this coaxial dielectric resonator, a through-hole is provided in a block made of dielectric ceramic, and only one surface (open surface) of the block in which the through-hole opens is left as it is. A conductor film is formed on the surface and the inner surface of the through hole.

また、平面型高周波回路素子である誘電体導波路の最も基本的なものとして、マイクロストリップ線路が挙げられる。このマイクロストリップ線路では、誘電体磁器基板の表裏両面のうち一方の面にストリップ導体を設け、誘電体磁器基板の他方の面に接地導体膜を設けている。   A microstrip line is the most basic dielectric waveguide that is a planar high-frequency circuit element. In this microstrip line, a strip conductor is provided on one of the front and back surfaces of the dielectric ceramic substrate, and a ground conductor film is provided on the other surface of the dielectric ceramic substrate.

以上の同軸誘電体共振器およびマイクロストリップ線路を用いて誘電体共振器制御型マイクロ波発信器を構成することができる。このマイクロ波発信器では、同軸誘電体共振器を誘電体磁器からなる支持部材を介して誘電体磁器基板に取り付け、同軸誘電体共振器の外部に漏れ出る電磁界を利用して、同軸誘電体共振器と誘電体磁器基板に設けたマイクロストリップ線路との結合をとる。   A dielectric resonator control type microwave transmitter can be configured using the above coaxial dielectric resonator and microstrip line. In this microwave oscillator, a coaxial dielectric resonator is attached to a dielectric ceramic substrate via a support member made of a dielectric ceramic, and an electromagnetic field leaking out of the coaxial dielectric resonator is utilized. The resonator is coupled to the microstrip line provided on the dielectric ceramic substrate.

この種の高周波回路においては、電界が支持部材を介して漏れるのを抑制することによって、無負荷Qの高い共振系が構成される。このため、支持部材の材料としては、比誘電率が低く誘電損失(tanδ)が小さい(すなわちQm×f。が大きい:ここでQmは材料の損失係数)ものを使用する必要がある。このため、従来、支持部材の材料としては、比誘電率εrが約7で、Qm×f。が約150000GHzのフォルステライト(MgSiO)が採用されていた。また、誘電体磁器基板の材料としては、主として比誘電率εrが約10で、Qm×f。が200000GHz以上のアルミナ磁器(Al)が採用されていた(例えば、特許文献1参照)。しかし、これらの材料では、共振周波数の温度係数τが−30〜−70ppm/℃となりやすいため、高周波回路の用途が制限されている。また、これら材料は不純物が混入すると、生成相の構成及び電気特性が大きく変動する等の問題がある。 In this type of high-frequency circuit, a resonance system with a high unloaded Q is configured by suppressing the electric field from leaking through the support member. Therefore, it is necessary to use a material for the support member that has a low relative dielectric constant and a small dielectric loss (tan δ) (that is, Qm × f is large: where Qm is a material loss coefficient). For this reason, conventionally, as a material of the support member, the relative dielectric constant εr is about 7, and Qm × f. Was forsterite (Mg 2 SiO 4 ) of about 150,000 GHz. In addition, as a material for the dielectric ceramic substrate, the relative permittivity εr is mainly about 10 and Qm × f. Alumina ceramics (Al 2 O 3 ) of 200000 GHz or higher have been employed (see, for example, Patent Document 1). However, in these materials, the temperature coefficient τ f of the resonance frequency tends to be −30 to −70 ppm / ° C., so that the use of the high frequency circuit is limited. In addition, when these materials are mixed with impurities, there is a problem that the structure of the generated phase and the electrical characteristics greatly vary.

また、フォルステライト(MgSiO)に酸化チタン(TiO)を加えた誘電体磁器組成物(非特許文献1参照)が提案されている。しかし、この誘電体磁器組成物では、酸化チタン(TiO)の添加とともに共振周波数の温度係数τが徐々にプラス側へシフトしているものの、酸化チタン30wt%添加でも共振周波数の温度係数τが−62ppm/℃と負で大きい値であるため、これに基づく誘電体磁器は実用的ではない。 Further, a dielectric ceramic composition (see Non-Patent Document 1) in which titanium oxide (TiO 2 ) is added to forsterite (Mg 2 SiO 4 ) has been proposed. However, in this dielectric ceramic composition, although the temperature coefficient τ f of the resonance frequency is gradually shifted to the positive side with the addition of titanium oxide (TiO 2 ), the temperature coefficient τ of the resonance frequency is added even when 30 wt% of titanium oxide is added. Since f is a negative and large value of −62 ppm / ° C., a dielectric ceramic based on this is not practical.

一方、誘電体導波路を構成する誘電体磁器基板の材料としては、一般的にはテフロン(登録商標)、アルミナ磁器(Al)が採用されている。しかし、これらの材料は共振周波数の温度係数τが−30〜−70ppm/℃となりやすいため、高周波回路の用途が制限されている。 On the other hand, Teflon (registered trademark) and alumina porcelain (Al 2 O 3 ) are generally used as materials for the dielectric ceramic substrate constituting the dielectric waveguide. However, since these materials tend to have a temperature coefficient τ f of the resonance frequency of −30 to −70 ppm / ° C., the use of the high frequency circuit is limited.

また、比誘電率εr=24、Qm×f。=350000GHz、共振周波数の温度係数τ=0ppm/℃の誘電体を平面型フィルタに適用した開発例(非特許文献2)があるが、今後の更なる高周波化の要請に対応するためには、やはり比誘電率εrが約12以下で、Qm×f。が50000GHz以上で、しかも共振周波数f。の温度係数τの絶対値が30ppm/℃以下であることが必要である。 Further, relative dielectric constant εr = 24, Qm × f. There is a development example (Non-patent Document 2) in which a dielectric having a temperature coefficient of τ f = 0 ppm / ° C. is applied to a planar filter (Non-patent Document 2), but in order to meet the demand for further higher frequency in the future The relative dielectric constant εr is about 12 or less and Qm × f. Is 50000 GHz or more and the resonance frequency f. It is necessary that the absolute value of the temperature coefficient τ f is 30 ppm / ° C. or less.

また、高周波領域になるほど、表皮効果の影響が大きくなり、例えば、導体としてAgを用いた場合には、1〜3GHzの領域で、表皮深さは1.18〜2.04μmとなる(非特許文献3)。   Further, the higher the frequency region, the greater the influence of the skin effect. For example, when Ag is used as the conductor, the skin depth is 1.18 to 2.04 μm in the region of 1 to 3 GHz (non-patented). Reference 3).

特開昭62−103904号公報JP-A-62-103904

Journal of the European Ceramic Society(第23巻(2003)第2575頁、表3参照)Journal of the European Ceramic Society (Vol. 23 (2003), page 2575, see Table 3) A Ka−band Diplexer Using Planar TE Mode Dielectric Resonators with Plastic Package(Metamorphosis,No.6,pp.38−39(2001))A Ka-band Diplexer Using Planar TE Mode Dielectric Resonators with Plastic Package (Metamorphosis, No. 6, pp. 38-39 (2001)) 理科年表 平成19年度版Science chronology 2007 edition

以上のような従来の高周波用誘電体磁器が有する技術的課題に鑑みて、本発明者らは、誘電体磁器の組成を適切なものにすること、および、誘電体磁器の相対密度を適切なものとすることにより、高周波領域の電気特性が優れたものになり製造が容易になるという知見を得た。そして、本発明はこの知見に基づいてなされたものである。   In view of the technical problems of the conventional high-frequency dielectric ceramics as described above, the present inventors have made the composition of the dielectric ceramics appropriate, and appropriately set the relative density of the dielectric ceramics. As a result, it has been found that the electrical characteristics in the high-frequency region are excellent and the manufacture is facilitated. And this invention is made | formed based on this knowledge.

すなわち、本発明の目的は、高周波領域での電気特性に優れ製造が容易な高周波用誘電体磁器およびその製造方法を提供することにある。   That is, an object of the present invention is to provide a high-frequency dielectric ceramic having excellent electrical characteristics in a high-frequency region and easy to manufacture, and a method for manufacturing the same.

本発明の他の目的は、そのような高周波用誘電体磁器を構成部材として用いた高周波回路素子を提供することにある。   Another object of the present invention is to provide a high-frequency circuit element using such a high-frequency dielectric ceramic as a constituent member.

本発明によれば、以上の如き目的のうちのいずれかを達成するものとして、組成式
a(Sn,Ti)O−bMgSiO−cMgTi−dMgSiO
で表され、前記組成式におけるa、b、c、及びd(ただし、a、b、c、及びdはモル%である)がそれぞれ4≦a≦37、34≦b≦92、2≦c≦15、及び2≦d≦15の範囲内にあり、ここでa+b+c+d=100である主成分と、ZrOからなる添加成分とを含んでなり、該添加成分は前記主成分100重量部に対して3.0〜12.0重量部添加されていることを特徴とする高周波用誘電体磁器、が提供される。
According to the present invention, the composition formula a (Sn, Ti) O 2 —bMg 2 SiO 4 —cMgTi 2 O 5 —dMgSiO 3 is achieved as one of the above objects.
A, b, c, and d (where a, b, c, and d are mol%) in the composition formula are 4 ≦ a ≦ 37, 34 ≦ b ≦ 92, and 2 ≦ c, respectively. ≦ 15 and 2 ≦ d ≦ 15, where a + b + c + d = 100, and an additive component composed of ZrO 2 , the additive component with respect to 100 parts by weight of the principal component A high-frequency dielectric porcelain characterized in that 3.0 to 12.0 parts by weight is added.

本発明においては、前記高周波用誘電体磁器は、相対密度が95%以上であり、比誘電率εが7.5〜12.0であり、Qm×f。値が50000GHz以上であり、共振周波数f。の温度係数τが−0〜+0ppm/℃である。
Oite The present onset bright, the high-frequency dielectric ceramic is a relative density of 95% or more, a relative dielectric constant epsilon r is from 7.5 to 12.0, Qm × f. The value is 50000 GHz or more and the resonance frequency f. Temperature coefficient tau f of - 3 is 0~ + 3 0ppm / ℃.

また、本発明によれば、以上の如き目的のうちのいずれかを達成するものとして、上記の高周波用誘電体磁器を製造する方法であって、SnO、TiO及びMgSiOの所定量を混合し仮焼した後に粉砕したものを出発原料として用い、該出発原料100重量部に対してZrOを焼結助剤として3.0〜12.0重量部添加して得られた粉末に有機バインダを添加して成形し、焼成することを特徴とする、高周波用誘電体磁器の製造方法、が提供される。 In addition, according to the present invention, there is provided a method for manufacturing the above-described high frequency dielectric ceramic, which achieves any one of the above-described objects, and includes SnO 2 , TiO 2 and Mg 2 SiO 4 . Powder obtained by mixing 3.0 to 12.0 parts by weight of ZrO 2 as a sintering aid with respect to 100 parts by weight of the starting material, using a pulverized powder after mixing and calcining a fixed amount There is provided a method for producing a dielectric ceramic for high frequency, characterized in that an organic binder is added to, molded and fired.

また、本発明によれば、以上の如き目的のうちのいずれかを達成するものとして、上記の高周波用誘電体磁器からなる部材を含むことを特徴とする高周波回路素子、が提供される。   In addition, according to the present invention, there is provided a high-frequency circuit element characterized by including a member made of the above-described high-frequency dielectric porcelain, in order to achieve any of the above objects.

本発明によれば、高周波領域での電気特性に優れ製造が容易な高周波用誘電体磁器が提供され、とくに、比誘電率εrが7.5〜12.0であり、Qm×f。値が十分に大きく、さらに共振周波数f。の温度係数τの絶対値が30ppm/℃以下であり、比較的低い温度で焼成可能な高周波用誘電体磁器が提供される。この高周波用誘電体磁器を構成部材として用いることで、特性が良好で良好な加工性と小型化容易性との両方の特長を備えた高周波回路素子が提供される。 ADVANTAGE OF THE INVENTION According to this invention, the dielectric ceramic for high frequency which is excellent in the electrical property in a high frequency area | region and is easy to manufacture is provided, especially, the dielectric constant (epsilon) r is 7.5-12.0, Qm * f. The value is sufficiently large, and the resonance frequency f. An absolute value of the temperature coefficient τ f of the high frequency dielectric ceramic is 30 ppm / ° C. or less, and can be fired at a relatively low temperature. By using this high-frequency dielectric ceramic as a constituent member, a high-frequency circuit element having excellent characteristics, both good workability and ease of miniaturization is provided.

高周波回路素子の一例である誘電体共振器制御型マイクロ波発信器の模式的断面図である。It is a typical sectional view of a dielectric resonator control type microwave transmitter which is an example of a high frequency circuit element. 高周波回路素子の一例である同軸誘電体共振器の模式的斜視図である。It is a typical perspective view of the coaxial dielectric resonator which is an example of a high frequency circuit element. 高周波回路素子の一例であるマイクロストリップ線路の模式的斜視図である。It is a typical perspective view of the microstrip line which is an example of a high frequency circuit element. 平面型高周波回路素子を構成する種々のマイクロストリップ線路のパターンを示す模式的平面図である。It is a typical top view which shows the pattern of the various microstrip line | wires which comprise a planar high frequency circuit element. 本発明の高周波用誘電体磁器のX線回折図である。FIG. 3 is an X-ray diffraction diagram of a high frequency dielectric ceramic according to the present invention.

本発明の高周波用誘電体磁器の主成分は、組成式a(Sn,Ti)O−bMg2Si
O4−cMgTi−dMgSiOで表され、前記組成式におけるa、b、c、及
びd(ただし、a、b、c、及びdはモル%である)がそれぞれ4≦a≦37、34≦b
≦92、2≦c≦15、及び2≦d≦15の範囲内にあり、ここでa+b+c+d=10
0である。本発明の高周波用誘電体磁器の添加成分は、ZrOからなる。この添加成分主成分100重量部に対して3.0〜12.0重量部添加されている。
The main component of the high frequency dielectric ceramic of the present invention is a composition formula a (Sn, Ti) O 2 —bMg 2 Si.
O4-cMgTi represented by 2 O 5 -dMgSiO 3, a in the formula, b, c, and d (provided that, a, b, c, and d are mol%), respectively 4 ≦ a ≦ 37, 34 ≦ b
≦ 92, 2 ≦ c ≦ 15, and 2 ≦ d ≦ 15, where a + b + c + d = 10
0. The additive component of the high frequency dielectric ceramic of the present invention is made of ZrO 2 . 3.0 to 12.0 parts by weight is added to 100 parts by weight of this additive component main component.

本発明の高周波用誘電体磁器は、とくに、図5のX線回折図に示されるように、チタン酸スズ((Sn,Ti)O)、フォルステライト(MgSiO)、マグネシウムチタネート(MgTi)、及びステアタイト(MgSiO)を主生成相とする。前記(Sn,Ti)Oとしては、(Sn0.8Ti0.2)O及び(Sn0.2Ti0.8)Oが知られている。このうち(Sn0.8Ti0.2)Oは、(Sn0.2Ti0.8)Oよりも、焼結が容易で、且つτも制御しやすい特徴がある。尚、図5では、主生成相のみ表れており、添加成分ZrOは微量であるため表れていない。 As shown in the X-ray diffraction diagram of FIG. 5, the high frequency dielectric ceramic of the present invention has tin titanate ((Sn, Ti) O 2 ), forsterite (Mg 2 SiO 4 ), magnesium titanate ( MgTi 2 O 5 ) and steatite (MgSiO 3 ) are the main production phases. As the (Sn, Ti) O 2 , (Sn 0.8 Ti 0.2 ) O 2 and (Sn 0.2 Ti 0.8 ) O 2 are known. Among these, (Sn 0.8 Ti 0.2 ) O 2 has characteristics that it is easier to sinter and more easily controls τ f than (Sn 0.2 Ti 0.8 ) O 2 . In FIG. 5, only the main production phase appears, and the additive component ZrO 2 does not appear because the amount is small.

本発明の高周波用誘電体磁器は、Qm×f。が50000GHz以上と高い値を示すことから、誘電損失が非常に小さい高周波用誘電体磁器及びこれを用いた高周波回路素子の提供が容易になる。また、本発明の高周波用誘電体磁器は、共振周波数の温度係数τの絶対値が0ppm/℃以下であることから、温度による特性への影響の少ない高周波用誘電体磁器及びこれを用いた高周波回路素子の提供が容易になる。しかも、本発明の高周波用誘電体磁器は、比誘電率εrが7.5〜12.0であることから、加工性の向上と小型化との両方の特長を備えた高周波回路素子の提供が容易になる。 The high frequency dielectric ceramic of the present invention is Qm × f. Shows a high value of 50000 GHz or more, it is easy to provide a high frequency dielectric ceramic having a very low dielectric loss and a high frequency circuit element using the same. The high frequency dielectric ceramic according to the present invention has an absolute value of the temperature coefficient τ f of the resonance frequency of 30 ppm / ° C. or less. It is easy to provide the high-frequency circuit element. Moreover, since the dielectric ceramic for high frequency according to the present invention has a relative dielectric constant εr of 7.5 to 12.0, it is possible to provide a high-frequency circuit element having both features of improved workability and downsizing. It becomes easy.

さらに、本発明の高周波用誘電体磁器は、添加成分ZrOの添加量が主成分100重量部に対して3.0〜12.0重量部であり且つ相対密度が95%以上であるため、上記Qm×f。、τ及びεrに関する特性が良好であり且つ製造時の焼成に際して接触するジルコニア(ZrO)やアルミナ(Al)などからなる敷板と反応することなく高い歩留まりで製造される。従って、高周波回路素子の提供が容易になる。このような高周波回路素子の一例として、図2に示されるような同軸誘電体共振器が挙げられる。ここでは、外形寸法10.6mm×10.6mm×12mm(軸長)の誘電体磁器のブロックに、軸長方向に沿って穴径3mmの円筒形貫通孔を設け、該貫通孔が開口するブロックの一面(開放面)だけは誘電体磁器の表面(セラミックス面)そのままの状態とし、誘電体磁器の他の表面及び貫通孔内面にはAg導体からなる導体膜を形成している。 Furthermore, in the high frequency dielectric ceramic of the present invention, the additive component ZrO 2 is added in an amount of 3.0 to 12.0 parts by weight with respect to 100 parts by weight of the main component and the relative density is 95% or more. Qm × f above. , Τ f and ε r have good characteristics and are manufactured at a high yield without reacting with a base plate made of zirconia (ZrO 2 ), alumina (Al 2 O 3 ), or the like that is contacted during firing during manufacturing. Accordingly, it is easy to provide a high-frequency circuit element. An example of such a high frequency circuit element is a coaxial dielectric resonator as shown in FIG. Here, a block in which a cylindrical through hole having a hole diameter of 3 mm is provided along the axial length direction in a block of a dielectric ceramic having an outer dimension of 10.6 mm × 10.6 mm × 12 mm (axial length), and the through hole is opened. Only one surface (open surface) of the dielectric ceramic is left as it is (ceramic surface), and a conductor film made of an Ag conductor is formed on the other surface of the dielectric ceramic and the inner surface of the through hole.

本発明の高周波用誘電体磁器における組成の限定理由を説明する。主成分の組成式a(Sn,Ti)O−bMgSiO−cMgTi−dMgSiOにおいて、aが4未満では、共振周波数の温度係数τが−30ppm/℃より小さくなり(すなわち、温度係数τの絶対値が30ppm/℃より大きくなり)、好ましくない。aが37を超えると、比誘電率εrが12.0より大きくなり、好ましくない。aのより好ましい範囲は、18≦a≦36である。この範囲内であれば、共振周波数の温度係数τの絶対値が20ppm/℃以下となる。bが34未満では、比誘電率εrが12.0より大きくなり、好ましくない。bが92を超えると、共振周波数の温度係数τが−30ppm/℃より小さくなり(すなわち、温度係数τの絶対値が30ppm/℃より大きくなり)、好ましくない。bのより好ましい範囲は、34≦b≦68である。この範囲であれば、共振周波数の温度係数τの絶対値が30ppm/℃以下となる。cが2未満では、共振周波数の温度係数τが−30ppm/℃より小さくなり(すなわち、温度係数τの絶対値が30ppm/℃より大きくなり)、好ましくない。cが15を超えると、比誘電率εrが12.0より大きくなり、好ましくない。dが2未満では、共振周波数の温度係数τが−30ppm/℃より小さくなり(すなわち、温度係数τの絶対値が30ppm/℃より大きくなり)、好ましくない。dが15を超えると、比誘電率εrが12.0より大きくなり好ましくない。 The reason for limiting the composition of the high frequency dielectric ceramic according to the present invention will be described. In the main component composition formula a (Sn, Ti) O 2 -bMg 2 SiO 4 -cMgTi 2 O 5 -dMgSiO 3 , if a is less than 4, the temperature coefficient τ f of the resonance frequency becomes smaller than −30 ppm / ° C. ( That is, the absolute value of the temperature coefficient τ f is greater than 30 ppm / ° C.), which is not preferable. When a exceeds 37, the relative dielectric constant εr becomes larger than 12.0, which is not preferable. A more preferable range of a is 18 ≦ a ≦ 36. Within this range, the absolute value of the temperature coefficient τ f of the resonance frequency is 20 ppm / ° C. or less. If b is less than 34, the relative dielectric constant εr becomes larger than 12.0, which is not preferable. If b exceeds 92, the temperature coefficient τ f of the resonance frequency becomes smaller than −30 ppm / ° C. (that is, the absolute value of the temperature coefficient τ f becomes larger than 30 ppm / ° C.), which is not preferable. A more preferable range of b is 34 ≦ b ≦ 68. Within this range, the absolute value of the temperature coefficient τ f of the resonance frequency is 30 ppm / ° C. or less. If c is less than 2, the temperature coefficient τ f of the resonance frequency becomes smaller than −30 ppm / ° C. (that is, the absolute value of the temperature coefficient τ f becomes larger than 30 ppm / ° C.), which is not preferable. When c exceeds 15, the relative dielectric constant εr becomes larger than 12.0, which is not preferable. If d is less than 2, the temperature coefficient τ f of the resonance frequency becomes smaller than −30 ppm / ° C. (that is, the absolute value of the temperature coefficient τ f becomes larger than 30 ppm / ° C.), which is not preferable. If d exceeds 15, the relative dielectric constant εr becomes larger than 12.0, which is not preferable.

後述の実施例で示されるように、本発明の高周波用誘電体磁器における組成範囲内で主成分の組成式におけるモル比a、b、c及びdを適宜変更することで、共振周波数f。の温度係数τの絶対値が30ppm/℃以下すなわちτが零に近い範囲内で十分大きなQm値を実現しつつ、比誘電率εrを7.5〜12.0の範囲の所望値に調整することが可能である。 As shown in the examples described later, the resonance frequency f is obtained by appropriately changing the molar ratios a, b, c, and d in the composition formula of the main component within the composition range in the high frequency dielectric ceramic of the present invention. Of being the absolute value of the temperature coefficient tau f can be regarded a sufficiently large Qm value within a range close to zero is 30 ppm / ° C. or less i.e. tau f, the relative dielectric constant εr in the desired value in the range of 7.5 to 12.0 It is possible to adjust.

また、主成分100重量部に対する添加成分ZrOの添加量が3.0重量部未満では、1350℃以下とくに1300℃以下の比較的低温の焼成で相対密度を95%以上とすることが難しく、良好なQm×f。値が得難くなるので、好ましくない。一方、主成分100重量部に対する添加成分ZrOの添加量が12.0重量部を超えると、良好なQm×f。値及びεrが得難くなり、且つ共振周波数の温度係数τが−30ppm/℃より小さくなり(すなわち、温度係数τの絶対値が30ppm/℃より大きくなり)、好ましくない。 Further, when the additive amount of the additive component ZrO 2 with respect to 100 parts by weight of the main component is less than 3.0 parts by weight, it is difficult to make the relative density 95% or more by firing at a relatively low temperature of 1350 ° C. or less, particularly 1300 ° C. or less, Good Qm × f. Since it becomes difficult to obtain a value, it is not preferable. On the other hand, when the addition amount of the additive component ZrO 2 with respect to 100 parts by weight of the main component exceeds 12.0 parts by weight, good Qm × f. It is difficult to obtain the value and εr, and the temperature coefficient τ f of the resonance frequency becomes smaller than −30 ppm / ° C. (that is, the absolute value of the temperature coefficient τ f becomes larger than 30 ppm / ° C.).

本発明の高周波用誘電体磁器の製造方法の一実施形態は次の通りである。SnO、TiO、及びMgSiOを所定量ずつ、アルコール等の溶媒とともに湿式混合する。続いて溶媒を除去した後、1000〜1150℃で仮焼して粉砕し、出発原料粉末を得る。 An embodiment of the method for manufacturing a high frequency dielectric ceramic according to the present invention is as follows. SnO 2 , TiO 2 , and Mg 2 SiO 4 are wet-mixed in predetermined amounts together with a solvent such as alcohol. Subsequently, after removing the solvent, it is calcined at 1000 to 1150 ° C. and pulverized to obtain a starting raw material powder.

この出発原料粉末に、ZrOを焼結助剤として所定量添加して、アルコール等の溶媒とともに湿式混合する。続いて溶媒を除去して得られた粉末にポリビニルアルコールの如き有機バインダを添加し、混合して均質にし、乾燥、解砕した後、成形密度が2.0〜2.4g/cm、好ましくは2.2〜2.4g/cmになるように加圧成形する。得られた成形物を空気の如き酸素含有ガス雰囲気下にて1200〜1350℃で焼成することにより上記組成式で表される主成分とZrOからなる添加成分とを含み、該添加成分が前記主成分100重量部に対して3.0〜12.0重量部添加されており、相対密度が95%以上である高周波用誘電体磁器を得ることができる。 A predetermined amount of ZrO 2 is added to this starting material powder as a sintering aid, and wet mixed with a solvent such as alcohol. Subsequently, an organic binder such as polyvinyl alcohol is added to the powder obtained by removing the solvent, and after mixing, homogenizing, drying and crushing, the molding density is preferably 2.0 to 2.4 g / cm 3 , preferably Is pressure-molded so as to be 2.2 to 2.4 g / cm 3 . The obtained molded product is fired at 1200 to 1350 ° C. in an oxygen-containing gas atmosphere such as air, and contains the main component represented by the above composition formula and an additive component composed of ZrO 2 , 3.0 to 12.0 parts by weight is added to 100 parts by weight of the main component, and a high frequency dielectric ceramic having a relative density of 95% or more can be obtained.

後述の実施例で示されるように、SnO及びTiOを当モル量用いることができる。この場合、とくに、前記生成相(Sn,Ti)Oは、(Sn0.8Ti0.2)Oであることが好ましい。 As shown in the examples described below, equimolar amounts of SnO 2 and TiO 2 can be used. In this case, in particular, the generated phase (Sn, Ti) O 2 is preferably (Sn 0.8 Ti 0.2 ) O 2 .

このようにして得られた高周波用誘電体磁器は、必要により適当な形状およびサイズに加工することができる。   The high-frequency dielectric ceramic thus obtained can be processed into an appropriate shape and size if necessary.

本発明の高周波用誘電体磁器は、例えば、外部に銀や銅等の導体からなる膜または配線などを形成することにより、図2のような同軸型誘電体共振器やこれを利用した同軸型誘電体フィルタ等の高周波回路素子を構成するのに利用することが可能である。本発明の高周波用誘電体磁器であって板状のものは、銀や銅等の導体配線を形成することにより、各種高周波回路のための誘電体配線基板として利用することができる。   The high frequency dielectric porcelain of the present invention includes a coaxial dielectric resonator as shown in FIG. 2 and a coaxial type using the same, for example, by forming a film or wiring made of a conductor such as silver or copper outside. It can be used to construct a high-frequency circuit element such as a dielectric filter. The plate-shaped high frequency dielectric ceramic of the present invention can be used as a dielectric wiring board for various high frequency circuits by forming a conductor wiring such as silver or copper.

また、出発原料粉末にZrOを焼結助剤として所定量添加し、低融点ガラスを添加し、その後ポリビニルブチラール等のバインダ樹脂、フタル酸ジブチル等の可塑剤、及びトルエン等の有機溶剤と混合し、ドクターブレード法等によるシート成形を行い、得られたシートと導体シートとを積層化し、一体焼成することにより、積層型誘電体フィルタや積層型の誘電体配線基板等の積層型の高周波回路素子を得ることができる。 In addition, a predetermined amount of ZrO 2 is added to the starting material powder as a sintering aid, a low melting glass is added, and then mixed with a binder resin such as polyvinyl butyral, a plasticizer such as dibutyl phthalate, and an organic solvent such as toluene. Then, by forming a sheet by the doctor blade method, etc., laminating the obtained sheet and the conductor sheet and firing them integrally, a laminated high frequency circuit such as a laminated dielectric filter or a laminated dielectric wiring board An element can be obtained.

なお、本発明の高周波用誘電体磁器を構成する元素であるSn、Mg、Si、及びTi、並びにZrOの原料としては、SnO、TiO、MgSiO、ZrOの他に、MgO、SiO等の酸化物を用いることもでき、さらには焼成時に酸化物となる硝酸塩、炭酸塩、水酸化物、塩化物、有機金属化合物等を使用することもできる。 Incidentally, Sn is an element constituting the high-frequency dielectric ceramic of the present invention, Mg, Si, and Ti, as well as the of ZrO 2 raw material, in addition to SnO 2, TiO 2, Mg 2 SiO 4, ZrO 2, Oxides such as MgO and SiO 2 can also be used, and nitrates, carbonates, hydroxides, chlorides, organometallic compounds and the like that become oxides upon firing can also be used.

なお、本発明の高周波用誘電体磁器は、その構成元素がO、Sn、Mg、Si、及びTi、並びにZrであるが、例えば粉砕ボールや原料粉末の不純物に由来するCa、Ba、Ni、Fe、Cr、P、Na等が不純物として混入してもよい。   The high-frequency dielectric ceramic according to the present invention includes O, Sn, Mg, Si, and Ti, and Zr as constituent elements. For example, Ca, Ba, Ni, Fe, Cr, P, Na, etc. may be mixed as impurities.

また、本発明の高周波用誘電体磁器は、低誘電率および高Qm値が求められるものであれば、種々の高周波回路素子の構成部材として使用できる。そのような例の1つとして、図1に示されるような誘電体共振器制御型マイクロ波発信器における構成部材が挙げられる。このマイクロ波発信器では、同軸誘電体共振器1を誘電体磁器からなる支持部材2を介して誘電体磁器基板3に取り付け、同軸誘電体共振器1の外部に漏れ出る電磁界Hを利用して、同軸誘電体共振器1と誘電体磁器基板3に設けたマイクロストリップ線路のストリップ導体4との結合をとる。符号5は、電磁シールド機能を発揮する金属ケースを示す。このマイクロ波発信器において、本発明の高周波用誘電体磁器は、図2に関し説明したような同軸誘電体共振器1の誘電体ブロックとして、支持部材2として、さらには誘電体磁器基板3として、それぞれ使用することができる。図3に、マイクロストリップ線路の詳細を示す。マイクロストリップ線路では、誘電体磁器基板6(上記誘電体磁器基板3に相当)の表面にストリップ導体7を設け、誘電体磁器基板6の裏面に接地導体膜8を設けている。ストリップ導体7の材料としては、Pd、Cu、Au、Agが例示される。   The high frequency dielectric ceramic according to the present invention can be used as a constituent member of various high frequency circuit elements as long as a low dielectric constant and a high Qm value are required. One example is a component in a dielectric resonator-controlled microwave transmitter as shown in FIG. In this microwave oscillator, a coaxial dielectric resonator 1 is attached to a dielectric ceramic substrate 3 via a support member 2 made of a dielectric ceramic, and an electromagnetic field H leaking out of the coaxial dielectric resonator 1 is used. Thus, the coaxial dielectric resonator 1 and the microstrip line strip conductor 4 provided on the dielectric ceramic substrate 3 are coupled. Reference numeral 5 denotes a metal case that exhibits an electromagnetic shielding function. In this microwave oscillator, the high frequency dielectric ceramic according to the present invention is used as a dielectric block of the coaxial dielectric resonator 1 as described with reference to FIG. 2 as a support member 2 and further as a dielectric ceramic substrate 3. Each can be used. FIG. 3 shows details of the microstrip line. In the microstrip line, the strip conductor 7 is provided on the surface of the dielectric ceramic substrate 6 (corresponding to the dielectric ceramic substrate 3), and the ground conductor film 8 is provided on the back surface of the dielectric ceramic substrate 6. Examples of the material of the strip conductor 7 include Pd, Cu, Au, and Ag.

本発明の高周波用誘電体磁器が構成部材として使用される高周波回路素子の他の例としては、図4の(a)〜(i)にそれぞれ示されるような平面型高周波回路素子が挙げられる。これらの平面型高周波回路素子9は、マイクロストリップ線路と同様に、誘電体磁器基板6の表面にストリップ導体7を設け、誘電体磁器基板6の裏面に接地導体膜を設けている。誘電体磁器基板6の表面には、ストリップ導体7と同一の材料により、各種パターン状の導体膜が形成されており、該導体膜によりそれぞれの素子の機能を発揮する。図4において、(a)の素子はインタディジタルキャパシタであり、(b)の素子はスパイラルインダクタであり、(c)の素子は分岐回路であり、(d)の素子は方向性結合器であり、(e)の素子は電力分配合成器であり、(f)の素子は低域通過フィルタであり、(g)の素子は帯域通過フィルタであり、(h)の素子はリング共振器であり、(i)の素子はパッチアンテナである。   Other examples of the high-frequency circuit element in which the high-frequency dielectric ceramic of the present invention is used as a constituent member include planar high-frequency circuit elements as shown in FIGS. 4A to 4I, respectively. These planar high-frequency circuit elements 9 are provided with a strip conductor 7 on the surface of the dielectric ceramic substrate 6 and a ground conductor film on the back surface of the dielectric ceramic substrate 6 in the same manner as the microstrip line. Various patterns of conductive films are formed on the surface of the dielectric ceramic substrate 6 with the same material as that of the strip conductors 7, and the functions of the respective elements are exhibited by the conductive films. In FIG. 4, the element (a) is an interdigital capacitor, the element (b) is a spiral inductor, the element (c) is a branch circuit, and the element (d) is a directional coupler. The element (e) is a power distribution synthesizer, the element (f) is a low-pass filter, the element (g) is a band-pass filter, and the element (h) is a ring resonator. , (I) is a patch antenna.

以下、実施例及び比較例により、本発明を更に説明する。   Hereinafter, the present invention will be further described with reference to Examples and Comparative Examples.

[実施例1]
SnOを4.8mol%、TiOを4.8mol%、MgSiOを90.5mol%となるように所定量を秤量し(表1参照)、これらをエタノール及びZrOボールとともにボールミルに入れ、12時間湿式混合した。その後、溶液を脱媒後、1100℃で2時間仮焼し、粉砕した。この仮焼粉を出発原料として用い、仮焼粉100重量部に対して3.0重量部のZrOを添加し、これらをエタノール及びZrOボールとともにボールミルに入れ、12時間湿式混合した。その後、溶液を脱媒し、更に適量のポリビニルアルコール(PVA)溶液を加えて乾燥した後、直径20mm、厚み8.2mmのペレットに成形し、空気雰囲気下において、1250℃で2時間焼成した。
[Example 1]
Predetermined amounts were weighed so that SnO 2 was 4.8 mol%, TiO 2 was 4.8 mol%, and Mg 2 SiO 4 was 90.5 mol% (see Table 1), and these were mixed with ethanol and ZrO 2 balls in a ball mill. And wet mixed for 12 hours. Then, after removing the solution, it was calcined at 1100 ° C. for 2 hours and pulverized. Using this calcined powder as a starting material, 3.0 parts by weight of ZrO 2 was added to 100 parts by weight of calcined powder, and these were placed in a ball mill together with ethanol and ZrO 2 balls and wet mixed for 12 hours. Thereafter, the solution was removed, and an appropriate amount of polyvinyl alcohol (PVA) solution was added and dried. Then, the pellet was formed into a pellet having a diameter of 20 mm and a thickness of 8.2 mm, and baked at 1250 ° C. for 2 hours in an air atmosphere.

こうして得られた高周波用誘電体磁器(表1参照)につき、アルキメデス法を用いて相
対密度を測定したところ、96%であった。
The relative density of the thus obtained high frequency dielectric ceramic (see Table 1) was measured using the Archimedes method and found to be 96%.

更に、この高周波用誘電体磁器を、直径16.7mm及び厚み7.8mmの大きさに加工した後、誘電共振法による測定で、共振周波数5.9〜6.5GHzにおけるQm×f。値、比誘電率εr、および共振周波数の温度係数τを求めた。その結果を表1に示す。 Furthermore, after processing this high frequency dielectric ceramic to a size of 16.7 mm in diameter and 7.8 mm in thickness, Qm × f at a resonance frequency of 5.9 to 6.5 GHz is measured by a dielectric resonance method. The value, the relative dielectric constant εr, and the temperature coefficient τ f of the resonance frequency were obtained. The results are shown in Table 1.

得られた高周波用誘電体磁器についてX線回折分析を行ったところ、図5に示されるように、主生成相はチタン酸スズ((Sn0.8Ti0.2)O)、フォルステライト(MgSiO)、マグネシウムチタネート(MgTi)、及びステアタイト(MgSiO)の結晶相から構成されていることが確認された。また、得られた高周波用誘電体磁器について蛍光X線分析を行ったところ、ZrOの存在が確認された。 When X-ray diffraction analysis was performed on the obtained dielectric ceramic for high frequency, as shown in FIG. 5, the main production phase was tin titanate ((Sn 0.8 Ti 0.2 ) O 2 ), forsterite. It was confirmed that it was composed of crystal phases of (Mg 2 SiO 4 ), magnesium titanate (MgTi 2 O 5 ), and steatite (MgSiO 3 ). Further, when X-ray fluorescence analysis was performed on the obtained high frequency dielectric ceramic, the presence of ZrO 2 was confirmed.

一方、上記の出発原料粉末100重量部に対して、ZrOを焼結助剤として3.0重量部添加し、更にPVA2.75重量部、セロゾール1重量部、及び分散剤1重量部を添加してスプレー顆粒を作製した。このスプレー顆粒を用いて、グリーン密度が2.3g/cmになるように成形し、その後1250℃×2時間の空気雰囲気条件下で焼成した。かくして得られた高周波用誘電体磁器を構成部材として用いて、図2に示されるような同軸誘電体共振器を作製した。該同軸誘電体共振器の大きさは、軸長12mm、外形(大略矩形状の開放面の一辺の長さ)10.6mm、穴径3mmであった。 On the other hand, with respect to 100 parts by weight of the above starting material powder, 3.0 parts by weight of ZrO 2 is added as a sintering aid, and 2.75 parts by weight of PVA, 1 part by weight of cellosol, and 1 part by weight of dispersant are added. A spray granule was prepared. Using this spray granule, the green density was molded to 2.3 g / cm 3 , and then fired under an air atmosphere condition of 1250 ° C. × 2 hours. A coaxial dielectric resonator as shown in FIG. 2 was fabricated using the high frequency dielectric ceramic thus obtained as a constituent member. The coaxial dielectric resonator had a shaft length of 12 mm, an outer shape (a length of one side of a substantially rectangular open surface) of 10.6 mm, and a hole diameter of 3 mm.

得られた同軸誘電体共振器について、共振周波数2GHzで無負荷Q値を評価した。その結果、同軸誘電体共振器としての無負荷Q値は1250であった。このように、本発明に係る高周波用誘電体磁器を使用することにより、優れた高周波特性を有する同軸誘電体共振器が得られた。   The obtained coaxial dielectric resonator was evaluated for an unloaded Q value at a resonance frequency of 2 GHz. As a result, the unloaded Q value as a coaxial dielectric resonator was 1250. Thus, the coaxial dielectric resonator which has the outstanding high frequency characteristic was obtained by using the dielectric ceramic for high frequencies which concerns on this invention.

[実施例2〜18]
SnO、TiO、及びMgSiOを表1に示した配合比になるように所定量を秤量し、実施例1と同条件で混合し、仮焼し、粉砕した。この仮焼粉を出発原料として用い、表1に示した配合量になるようにZrOを所定量秤量して混合し、実施例1と同様にしてバインダ添加及び成形などを行い、空気雰囲気下において表1に示されるような温度にて2時間焼成して、高周波用誘電体磁器を作製し、実施例1と同様な方法で特性を評価した。その結果を表1に示す。
[Examples 2 to 18]
A predetermined amount of SnO 2 , TiO 2 , and Mg 2 SiO 4 was weighed so as to have a mixing ratio shown in Table 1, mixed under the same conditions as in Example 1, calcined, and pulverized. Using this calcined powder as a starting material, a predetermined amount of ZrO 2 was weighed and mixed so as to have the blending amount shown in Table 1, and the binder was added and molded in the same manner as in Example 1, and then in an air atmosphere Were fired at a temperature as shown in Table 1 for 2 hours to produce a high frequency dielectric ceramic, and the characteristics were evaluated in the same manner as in Example 1. The results are shown in Table 1.

[比較例1〜12]
SnO、TiO、及びMgSiOを表1に示した配合比になるように所定量を秤量し、実施例1と同条件で混合し、仮焼し、粉砕した。この仮焼粉を出発原料として用い、表2に示した配合量になるようにZrOを所定量秤量して混合し、実施例1と同様にしてバインダ添加及び成形を行い、空気雰囲気下において表2に示されるような温度にて2時間焼成して、高周波用誘電体磁器を作製し、実施例1と同様な方法で特性を評価した。その結果を表2に示す。
[Comparative Examples 1 to 12]
A predetermined amount of SnO 2 , TiO 2 , and Mg 2 SiO 4 was weighed so as to have a mixing ratio shown in Table 1, mixed under the same conditions as in Example 1, calcined, and pulverized. Using this calcined powder as a starting material, a predetermined amount of ZrO 2 was weighed and mixed so as to have the blending amount shown in Table 2, and the binder was added and molded in the same manner as in Example 1, and in an air atmosphere A high frequency dielectric ceramic was produced by firing at a temperature as shown in Table 2 for 2 hours, and the characteristics were evaluated in the same manner as in Example 1. The results are shown in Table 2.

Figure 0005458927
Figure 0005458927

Figure 0005458927
Figure 0005458927

以上のように、本発明の高周波用誘電体磁器は、低誘電率且つ高Q値であり温度特性に優れるため、例えば、マイクロ波及びミリ波などの高周波領域で使用される集積回路等の高周波回路素子の構成部材として最適である。   As described above, since the dielectric ceramic for high frequency of the present invention has a low dielectric constant and a high Q value and excellent temperature characteristics, for example, a high frequency such as an integrated circuit used in a high frequency region such as a microwave and a millimeter wave is used. It is optimal as a component for circuit elements.

1・・・同軸誘電体共振器
2・・・支持部材
3・・・誘電体磁器基板
4・・・ストリップ導体
5・・・金属ケース
H・・・電磁界
6・・・誘電体磁器基板
7・・・ストリップ導体
8・・・接地導体膜
9・・・平面高周波回路
DESCRIPTION OF SYMBOLS 1 ... Coaxial dielectric resonator 2 ... Support member 3 ... Dielectric ceramic substrate 4 ... Strip conductor 5 ... Metal case H ... Electromagnetic field 6 ... Dielectric ceramic substrate 7 ... Strip conductor 8 ... Grounding conductor film 9 ... Plane high-frequency circuit

Claims (3)

組成式a(Sn,Ti)O−bMgSiO−cMgTi−dMgSiO
で表され、前記組成式におけるa、b、c、及びd(ただし、a、b、c、及びdはモル%である)がそれぞれ4≦a≦37、34≦b≦92、2≦c≦15、及び2≦d≦15の範囲内にあり、ここでa+b+c+d=100である主成分と、ZrOからなる添加成分とを含んでなり、該添加成分は前記主成分100重量部に対して3.0〜12.0重量部添加されており、相対密度が95%以上であり、比誘電率εrが7.5〜12.0であり、Qm×f。値が50000GHz以上であり、共振周波数f。の温度係数τ が−30〜+30ppm/℃であることを特徴とする高周波用誘電体磁器。
Composition formula a (Sn, Ti) O 2 —bMg 2 SiO 4 —cMgTi 2 O 5 —dMgSiO 3
A, b, c, and d (where a, b, c, and d are mol%) in the composition formula are 4 ≦ a ≦ 37, 34 ≦ b ≦ 92, and 2 ≦ c, respectively. ≦ 15 and 2 ≦ d ≦ 15, where a + b + c + d = 100, and an additive component composed of ZrO 2 , the additive component with respect to 100 parts by weight of the principal component 3.0 to 12.0 parts by weight , the relative density is 95% or more, the relative dielectric constant εr is 7.5 to 12.0, and Qm × f. The value is 50000 GHz or more and the resonance frequency f. High-frequency dielectric ceramic temperature coefficient tau f of characterized in that it is a -30~ + 30ppm / ℃.
請求項に記載の高周波用誘電体磁器を製造する方法であって、SnO、TiO及びMgSiOの所定量を混合し仮焼した後に粉砕したものを出発原料として用い、該出発原料100重量部に対してZrOを焼結助剤として3.0〜12.0重量部添加して得られた粉末に有機バインダを添加して成形し、焼成することを特徴とする高周波用誘電体磁器の製造方法。 A method for producing a dielectric ceramic for high frequency according to claim 1 , wherein a predetermined amount of SnO 2 , TiO 2 and Mg 2 SiO 4 is mixed and calcined and then pulverized as a starting material. For high frequency, characterized in that an organic binder is added to a powder obtained by adding 3.0 to 12.0 parts by weight of ZrO 2 as a sintering aid with respect to 100 parts by weight of the raw material, followed by firing. A method of manufacturing a dielectric ceramic. 請求項に記載の高周波用誘電体磁器からなる部材を含むことを特徴とする高周波回路素子。 A high-frequency circuit element comprising a member comprising the high-frequency dielectric ceramic according to claim 1 .
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