JPS60132402A - Electrode forming method of dielectric element for high frequency - Google Patents
Electrode forming method of dielectric element for high frequencyInfo
- Publication number
- JPS60132402A JPS60132402A JP58239905A JP23990583A JPS60132402A JP S60132402 A JPS60132402 A JP S60132402A JP 58239905 A JP58239905 A JP 58239905A JP 23990583 A JP23990583 A JP 23990583A JP S60132402 A JPS60132402 A JP S60132402A
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- high frequency
- dielectric
- dielectric element
- forming method
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P7/00—Resonators of the waveguide type
- H01P7/04—Coaxial resonators
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
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】
(産業上の利用分野)
不発明は、通信機器等に用いられる同軸共振器等の皮膜
強度が高くまたQ値が大きい高周波用誘電体素子の電極
形成方法に関する。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a method for forming electrodes of high-frequency dielectric elements having high film strength and a large Q value, such as coaxial resonators used in communication equipment and the like.
(従来例の構成とその問題点)
VHF帯もしくはUHF帯で用いられるフづルタとして
は同軸共振器等があり、これらにはQ値の高い誘電体素
子が用いられている。該誘電体素子のQ%性を最大限に
引き出すには、デバイス関係及び電極を検討する必要が
ある。特に電極は共振器の寿命に深い関係があシ、電極
皮膜−誘電体素手表面間の界面状態に依存している。(Structure of conventional example and its problems) Coaxial resonators and the like are examples of filters used in the VHF band or UHF band, and dielectric elements with a high Q value are used in these filters. In order to maximize the Q% property of the dielectric element, it is necessary to consider device relationships and electrodes. In particular, the electrode has a close relationship with the life of the resonator, and it depends on the state of the interface between the electrode film and the surface of the dielectric bare hand.
従来同軸構造の誘電体の内周面及び外周面に第1図の如
く銀電極やメッキによる銅電極を形成させたものがある
。前者は、銀ペースト全誘電体に塗布し焼付けしたもの
であるが、その電極厚と共振器の無負荷Qの関係を、第
2図に示す。ここでQITlは実測値、Q、は理論値、
Eは電極厚み、δは表皮厚さでおる。δについては次式
で与えられる◇ここで、fは共振周波数、μは透磁率(
4X10”−7H/ m )、σは電極金属の電気伝導
度、πは円周率でおる。これより、銀電極を用いた場合
の電極必要厚みをめると、共振周波数Y 900 MJ
(zとした場合、δ(表皮厚)は2.1μmとなる。Q
の劣化を少なくするには第2図よシ、電極厚は21μm
以上は必要となる。この必要電極厚みを得るには、少な
くとも、3回以上の塗布焼付を行なわなければならなく
、非常に工数がかかる。また接着強度に関しては、鎖中
に含まれるガラスフリット量に比例するが、ガラスフリ
ット量とQ値は反比例の関係にある。第3図にガラスフ
リット量とQ値、接着強度の関係を示す。これによると
、高いQ値を満たすには、ガラスフリット量をl、 Q
mo1%以下にしなければならず、その為接着強度が
500g r/an2以下とな9、該誘電体共振器は振
動等の条件に弱く、寿命が短かい等の欠点が生じる。Conventionally, as shown in FIG. 1, silver electrodes or plated copper electrodes are formed on the inner and outer peripheral surfaces of a dielectric having a coaxial structure. In the former case, silver paste was applied to the entire dielectric material and baked, and the relationship between the electrode thickness and the no-load Q of the resonator is shown in FIG. Here, QITl is the measured value, Q is the theoretical value,
E is the electrode thickness, and δ is the skin thickness. δ is given by the following formula ◇Here, f is the resonant frequency and μ is the magnetic permeability (
4X10"-7H/m), σ is the electrical conductivity of the electrode metal, and π is the circumference. From this, when the required electrode thickness is included when using a silver electrode, the resonant frequency Y 900 MJ
(If z, δ (skin thickness) is 2.1 μm.Q
To reduce the deterioration of the electrode, as shown in Figure 2, the electrode thickness should be 21 μm.
The above is necessary. In order to obtain this required electrode thickness, coating and baking must be performed at least three times, which requires a large number of man-hours. Furthermore, the adhesive strength is proportional to the amount of glass frit contained in the chain, but the amount of glass frit and the Q value are inversely proportional. FIG. 3 shows the relationship between the amount of glass frit, Q value, and adhesive strength. According to this, in order to satisfy a high Q value, the amount of glass frit should be l, Q
The mo of the dielectric resonator must be kept at 1% or less, and therefore the adhesive strength is 500 g r/an2 or less.
メッキによる銅電極形成方法(特願昭53−157’1
2号)があるが、これは電極と誘電体表面との接着強度
が非常に弱く、ヒートサイクル試験等で電極が剥離する
などの欠点がある。接着強度を上げるにはエツチング等
で誘電体表面の表面粗さを粗くする方法があるが、第4
図に示すように、粗くすれば共振器の無負荷Qが劣化す
るという問題点がある。ここでQmは実測値、Q(は理
論値、ρは表面粗さく平均値)、δは表皮厚である。Copper electrode formation method by plating (Japanese Patent Application No. 53-157'1)
There is No. 2), but this has the disadvantage that the adhesive strength between the electrode and the dielectric surface is very weak, and the electrode peels off during heat cycle tests and the like. There is a method of increasing the surface roughness of the dielectric material by etching etc. to increase the adhesive strength, but the fourth method is
As shown in the figure, there is a problem that if the roughness is made, the no-load Q of the resonator deteriorates. Here, Qm is a measured value, Q (is a theoretical value, ρ is an average value of surface roughness), and δ is a skin thickness.
(発明の目的)
本発明は高周波用誘電体素子の電極に於いて、電極と誘
電体表面との接着強度が強く、Q値の劣化が少ない電極
形成方法を提供するものである。(Objective of the Invention) The present invention provides a method for forming an electrode of a high frequency dielectric element, in which the adhesive strength between the electrode and the dielectric surface is strong and the Q value is less deteriorated.
(発明の構成)
不発明は上記目的を達成するため、高周波用誘電体素子
表面に電極を形成後、熱間静水圧プレスするものである
。(Structure of the Invention) In order to achieve the above object, the invention is to form an electrode on the surface of a high-frequency dielectric element and then perform hot isostatic pressing.
(実施列の説明)
実施例−1
試料としては、B a T r 40 q系セラミック
を用い、第1図に示す如<’、TEMλ/4共振器とし
た。同軸構造の誘電体1の内周部2、外周部3、及び両
端面4.5に銀電極6を薄く塗布し、800℃−10分
焼付けを行なった。電極厚は15μmとした。該素子を
Arガス中200℃〜700℃、200〜2000 k
g、7cm2にて熱間静水圧プレスする。然る後に該素
子の片端面4を除去し、第5図、第6図に示す各緒特性
を調べた。(Description of Examples) Example 1 A B a T r 40 q ceramic was used as a sample, and a TEMλ/4 resonator was used as shown in FIG. Silver electrodes 6 were thinly coated on the inner circumferential portion 2, outer circumferential portion 3, and both end surfaces 4.5 of the dielectric body 1 having a coaxial structure, and baked at 800° C. for 10 minutes. The electrode thickness was 15 μm. The element was heated in Ar gas at 200°C to 700°C and 200 to 2000k.
g, hot isostatic pressing at 7 cm2. Thereafter, one end surface 4 of the element was removed, and the characteristics shown in FIGS. 5 and 6 were examined.
実施例−2
試料としては実施例−1と同一素子を用い、該素子をH
Fl0ωt%液にて10分エツチング処理を行なった。Example-2 The same element as in Example-1 was used as a sample, and the element was heated to H
Etching treatment was performed for 10 minutes using Fl0ωt% solution.
該素子に無電解銅メッキにて4μm銅膜を形成後、電解
銅メッキにて10μm、計14μmの銅電極を形成させ
る。該素子fArガス中700℃−1000に97cm
2にて熱間静水圧プレスし、然る後に片端面4を除去す
る。該素子の緒特性を表に示す。After forming a 4 μm copper film on the element by electroless copper plating, a copper electrode of 10 μm, total 14 μm, was formed by electrolytic copper plating. The element fAr gas at 700℃-1000℃ 97cm
2, hot isostatic pressing is performed, and then one end surface 4 is removed. The characteristics of the device are shown in the table.
表
以上の結果よシ本発明による電極形成方法は、従来の方
法に比べて電極接着強度が強く、Qの劣化が少ない高周
波用誘電体素子を提供する事が可能となった。As can be seen from the results shown in the table, the electrode forming method according to the present invention has a stronger electrode adhesion strength than conventional methods, and it is possible to provide a high frequency dielectric element with less Q deterioration.
尚本実施例では、銀、銅を用いたが金や他の電極でも同
等の結果が得られた。又、熱間静水圧プレスでは、Ar
ガスを用いたが、耐熱性オイル等(但し、使用温度はm
ax 800℃)を用いても同等の結果が得られた。In this example, silver and copper were used, but similar results were obtained with gold and other electrodes. In addition, in hot isostatic pressing, Ar
Gas was used, but heat-resistant oil, etc. (however, the operating temperature was m
Equivalent results were obtained using a temperature of 800° C.).
(発明の効果)
本発明により、従来の方法(焼付け、メッキ等)に比べ
て、Q値の劣化を少なくシ、電極の接着強度を強くする
事ができ、高周波用誘電体素子としての信頼性が向上し
た。以上のことから、本発明は誘電体共振器等の各種機
器への応用についても適用されることは明白である。(Effects of the invention) Compared to conventional methods (baking, plating, etc.), the present invention can reduce the deterioration of the Q value and increase the adhesive strength of the electrode, improving reliability as a dielectric element for high frequencies. has improved. From the above, it is clear that the present invention is also applicable to various devices such as dielectric resonators.
第1図(a)は本発明の一実施例を説明するだめの、同
軸型共振器の断面図であり、(b)は(a)のA −A
’断面図、第2図は銀型極厚と共振器の無負荷Qの関係
を示す図、第3図は銀電極中のガラスフリット成分含有
量と電極接着強度及び共振器無負荷Qの関係を示す図、
第4図は誘電体素子表面粗さと共振器の無負荷Qの関係
を示す図、第5図、第6図は熱間静水圧プレス条件と電
極接着強度及び共振器の無負荷Qの関係を示す図である
。
1・・・誘電体、2・・・内周部、3・・・外周部、4
.5・・・端面、6・・・電極。
第1図
(a) ・ (b)
第2図
t/6
tjJ3図
1 2 3 4
S1○2系庁ラス刀ツト量(mo!、’lo)第4図
、f/g
第5図
H,1,P圧力(km7c rr4 )第6図
H1P圧力(kg/cm2)FIG. 1(a) is a cross-sectional view of a coaxial resonator for explaining one embodiment of the present invention, and FIG. 1(b) is a sectional view taken along A-A in FIG.
' Cross-sectional view, Figure 2 is a diagram showing the relationship between the silver mold thickness and the no-load Q of the resonator, and Figure 3 is the relationship between the glass frit component content in the silver electrode, electrode adhesion strength, and the no-load Q of the resonator. A diagram showing
Figure 4 shows the relationship between the surface roughness of the dielectric element and the no-load Q of the resonator, and Figures 5 and 6 show the relationship between the hot isostatic pressing conditions, electrode bonding strength, and the no-load Q of the resonator. FIG. 1... Dielectric, 2... Inner peripheral part, 3... Outer peripheral part, 4
.. 5... End face, 6... Electrode. Figure 1 (a) / (b) Figure 2 t/6 tjJ3 Figure 1 2 3 4 S1○2 agency last cut amount (mo!, 'lo) Figure 4, f/g Figure 5 H, 1, P pressure (km7c rr4) Figure 6 H1P pressure (kg/cm2)
Claims (2)
付によ多形成させた後、熱間静水圧プレスする事を特徴
とする高周波用誘電体素子の電極形成方法。(1) A method for forming electrodes of a high frequency dielectric element, which comprises forming electrodes on the surface of the high frequency dielectric element by full plating or baking, followed by hot isostatic pressing.
徴とする特許請求の範囲第(1)項記載の高周波用誘電
体素子の電極形成方法。(2) A method for forming an electrode of a high frequency dielectric element according to claim (1), wherein the electrode is made of Ag, Cu, or Au.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58239905A JPS60132402A (en) | 1983-12-21 | 1983-12-21 | Electrode forming method of dielectric element for high frequency |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58239905A JPS60132402A (en) | 1983-12-21 | 1983-12-21 | Electrode forming method of dielectric element for high frequency |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60132402A true JPS60132402A (en) | 1985-07-15 |
| JPS6366081B2 JPS6366081B2 (en) | 1988-12-19 |
Family
ID=17051592
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58239905A Granted JPS60132402A (en) | 1983-12-21 | 1983-12-21 | Electrode forming method of dielectric element for high frequency |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60132402A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04284003A (en) * | 1991-03-13 | 1992-10-08 | Matsushita Electric Ind Co Ltd | Planar dielectric filter |
-
1983
- 1983-12-21 JP JP58239905A patent/JPS60132402A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04284003A (en) * | 1991-03-13 | 1992-10-08 | Matsushita Electric Ind Co Ltd | Planar dielectric filter |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6366081B2 (en) | 1988-12-19 |
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