JPH0641386Y2 - Monolithic crystal filter - Google Patents

Monolithic crystal filter

Info

Publication number
JPH0641386Y2
JPH0641386Y2 JP14624788U JP14624788U JPH0641386Y2 JP H0641386 Y2 JPH0641386 Y2 JP H0641386Y2 JP 14624788 U JP14624788 U JP 14624788U JP 14624788 U JP14624788 U JP 14624788U JP H0641386 Y2 JPH0641386 Y2 JP H0641386Y2
Authority
JP
Japan
Prior art keywords
vibrator
slope
oscillator
mcf
crystal filter
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
JP14624788U
Other languages
Japanese (ja)
Other versions
JPH0266028U (en
Inventor
宏 中谷
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing 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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP14624788U priority Critical patent/JPH0641386Y2/en
Publication of JPH0266028U publication Critical patent/JPH0266028U/ja
Application granted granted Critical
Publication of JPH0641386Y2 publication Critical patent/JPH0641386Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【考案の詳細な説明】 〔産業上の利用分野〕 本考案は水晶振動子のような圧電単結晶の円板型ATカッ
ト厚みすべり振動子を複数段縦接続してなるモノリシッ
ククリスタルフィルタに関するものである。
[Detailed Description of the Invention] [Industrial field of application] The present invention relates to a monolithic crystal filter formed by vertically connecting a plurality of stages of a piezoelectric single crystal disk-type AT-cut thickness sliding oscillator such as a quartz oscillator. is there.

〔従来の技術〕[Conventional technology]

従来、モノリシッククリスタルフィルタ(以下、MCFと
いう)にはATカット厚みすべり水晶振動子が広く用いら
れている。ATカットは、水晶の結晶面の一つであるXZ面
をX軸を中心に約35°傾けて切り出したものであり、常
温付近で周波数温度特性が良いという特性を有してい
る。
Conventionally, AT-cut thickness sliding crystal units have been widely used for monolithic crystal filters (hereinafter referred to as MCF). The AT cut is obtained by cutting out the XZ plane, which is one of the crystal planes of quartz, with an inclination of about 35 ° around the X axis, and has a characteristic that the frequency-temperature characteristic is good near room temperature.

このようなATカット厚みすべり振動子において、第5図
のように円板状振動子20の表面に入,出力用電極21,22
を分割形成し、裏面に接地用電極23を形成することによ
り、2重モード振動子が得られることが知られている。
2重モード振動子は、それ単体では充分な減衰量のフィ
ルタが得難いため、第6図のように結合コンデンサ24を
介して2段またはそれ以上に縦接続することが多い。
In such an AT cut thickness sliding oscillator, as shown in FIG.
It is known that a dual mode oscillator can be obtained by separately forming and forming the ground electrode 23 on the back surface.
Since it is difficult to obtain a filter having a sufficient attenuation amount by itself, the dual mode oscillator is often connected in two or more stages in series via the coupling capacitor 24 as shown in FIG.

〔考案が解決しようとする課題〕[Problems to be solved by the device]

上記のように振動子を多段接続してフィルタを構成する
場合、同一厚み、同一直径の振動子を使用することにな
るが、これでは輪郭モードのスプリアスも同一周波数で
生じるため、これらスプリアスが強め合って大きな不要
レスポンスとなってしまうという問題があった。
When constructing a filter by connecting oscillators in multiple stages as described above, oscillators with the same thickness and diameter are used.However, since spurious in contour mode also occurs at the same frequency, these spurs are intensified. There was a problem that it would result in a large unnecessary response.

そこで、本考案の目的は、多段縦接続時に輪郭モードの
スプリアスを抑制できるMCFを提供することにある。
Then, the objective of this invention is providing the MCF which can suppress the spurious of a contour mode at the time of multistage vertical connection.

〔課題を解決するための手段〕[Means for Solving the Problems]

上記目的を達成するために、本考案は、周端部に斜面を
形成した圧電単結晶の円板型ATカット厚みすべり振動子
に複数対の電極を形成し、この振動子を複数段縦接続し
てなるMCFにおいて、各段の振動子の斜面を異なる形状
としたことを特徴とするものである。
In order to achieve the above-mentioned object, the present invention forms a plurality of pairs of electrodes on a piezoelectric single crystal disk-type AT-cut thickness-sliding vibrator with a beveled surface at the peripheral edge, and connects the vibrators in multiple stages in a vertical direction. The MCF is characterized in that the slopes of the vibrators at each stage have different shapes.

〔作用〕[Action]

即ち、周波数が数MHz以上の円板型ATカット厚みすべり
振動子の場合には、振動変位を中央部に集中させてエネ
ルギー閉じ込め効率を向上させ、かつ振動子の周端部に
おける支持損失を減ずるために、円板の周端部が漸次薄
肉となるように斜面研磨している。この斜面形状によっ
て輪郭モードのスプリアス周波数が変化する。本考案は
この性質を利用し、異なる斜面形状を持った振動子を多
段縦接続することにより、輪郭モード周波数を分散さ
せ、スプリアスを抑制するものである。
That is, in the case of a disk-type AT-cut thickness-sliding oscillator with a frequency of several MHz or higher, the vibration displacement is concentrated in the central part to improve the energy trapping efficiency and reduce the supporting loss at the peripheral edge of the oscillator. For this reason, the peripheral surface of the disc is gradually polished so that the peripheral end portion becomes thinner. This slope shape changes the spurious frequency of the contour mode. Utilizing this property, the present invention disperses contour mode frequencies and suppresses spurious by vertically connecting transducers having different slope shapes in multiple stages.

〔実施例〕〔Example〕

第1図は本考案にかかるMCFの一例を示す。 FIG. 1 shows an example of the MCF according to the present invention.

図面において、1は水晶,ニオブ酸リチウム,タンタル
酸リチウムなどの圧電単結晶よりなる円板型ATカット厚
みすべり振動子であり、この振動子1の周端部には、エ
ネルギー閉じ込め効率を向上させかつ振動子1の周端部
における支持損失を減ずるために、斜面1aがベベル加工
されている。振動子1の表面には入力用電極2と出力用
電極3とが分割形成され、裏面中央部には入,出力用電
極2,3と対応する部位に接地用電極4が形成されてい
る。上記電極2,4と電極3,4とで2対の電極対が構成さ
れ、変位分布が伝播軸方向に関し線対称な対称モードと
点対称な斜対称モードとの2重モード振動子が実現され
る。
In the drawing, reference numeral 1 is a disk-type AT-cut thickness-sliding vibrator made of a piezoelectric single crystal such as quartz, lithium niobate, or lithium tantalate. The peripheral end portion of the vibrator 1 improves energy trapping efficiency. Moreover, in order to reduce the support loss at the peripheral end of the vibrator 1, the sloped surface 1a is beveled. An input electrode 2 and an output electrode 3 are separately formed on the front surface of the vibrator 1, and a ground electrode 4 is formed at a portion corresponding to the input and output electrodes 2 and 3 at the center of the back surface. Two pairs of electrodes are constituted by the electrodes 2 and 4 and the electrodes 3 and 4, and a dual mode oscillator having a symmetric mode in which the displacement distribution is line symmetrical with respect to the propagation axis direction and a point symmetric oblique symmetric mode is realized. It

振動子1の周端部に導出された各電極2,3,4の取り出し
部にはそれぞれ支持線5,6,7が電気的に接続され、これ
ら支持線はステム8に固定された外部接続用端子9,10,1
1に接続されている。上記振動子1はステム8に被着さ
れたキャップ12内に収容され、気密封止されている。
Support wires 5, 6 and 7 are electrically connected to the lead-out portions of the electrodes 2, 3 and 4 led out to the peripheral end of the vibrator 1, and these support wires are fixed to the stem 8 by an external connection. For terminals 9,10,1
Connected to 1. The vibrator 1 is housed in a cap 12 attached to the stem 8 and hermetically sealed.

上記振動子1は単体で使用すると充分な減衰量のMCFが
得られないので、通常は第6図のように複数段縦接続し
てなる。本考案では、複数の振動子1を縦接続する場合
に、各段の振動子の周端部の斜面形状が異なるものを使
用している。
Since the oscillator 1 cannot obtain a sufficient MCF when used alone, it is usually made up of a plurality of stages connected vertically as shown in FIG. In the present invention, when a plurality of vibrators 1 are vertically connected, the vibrators of the respective stages having different sloped shapes at the peripheral ends are used.

即ち、第2図は上記振動子1の断面図であり、直径は
d、中央部の厚みはt、周端部斜面1aの角度はθ、斜
面1aの幅はw1となっている。
That is, FIG. 2 is a cross-sectional view of the vibrator 1, where the diameter is d, the thickness of the central portion is t, the angle of the peripheral end slope 1a is θ 1 , and the width of the slope 1a is w 1 .

第3図は他の振動子1′を示し、直径dおよび厚みtは
第2図のものと等しいが、斜面1bの角度θは第2図の
ものより大きく、斜面1bの幅w2は第2図のものより狭
い。
FIG. 3 shows another transducer 1 ', whose diameter d and thickness t are the same as those in FIG. 2, but the angle θ 2 of the slope 1b is larger than that of FIG. 2 and the width w 2 of the slope 1b is It is narrower than that of FIG.

第4図はさらに他の振動子1″を示し、この場合には直
径dおよび厚みtは第2図,第3図のものと等しいが、
斜面1cの形状がテーパ面ではなく曲面である点で相違し
ている。
FIG. 4 shows yet another transducer 1 ″, in which case the diameter d and the thickness t are the same as in FIGS. 2 and 3,
The difference is that the shape of the inclined surface 1c is not a tapered surface but a curved surface.

第2図〜第4図に例示されるように、斜面形状の異なる
振動子を組み合わせて多段縦接続すると、斜面形状の違
いによって輪郭モードのスプリアス周波数を分散させる
ことができ、スプリアスの少ないMCFが得られる。
As illustrated in FIGS. 2 to 4, when oscillators having different slope shapes are combined and connected in multiple stages in a vertical manner, spurious frequencies in the contour mode can be dispersed due to the difference in slope shape, and an MCF with less spurious noise can be obtained. can get.

なお、第2図〜第4図は振動子の代表的な形状を例示し
たに過ぎず、この他にも斜面形状の異なる振動子は考え
られる。本考案で斜面形状とは、上記のように斜面の角
度,幅および斜面の曲率等を含む概念である。
It should be noted that FIGS. 2 to 4 merely exemplify the typical shape of the vibrator, and other vibrators having different slope shapes are also conceivable. In the present invention, the slope shape is a concept including the angle and width of the slope and the curvature of the slope as described above.

また、本考案はタンダム型MCFのほかに、混成型MCFにも
適用できる。
Further, the present invention can be applied not only to the tandem type MCF but also to the mixed type MCF.

〔考案の効果〕[Effect of device]

以上の説明で明らかなように、本考案によれば振動子を
多段接続することによって減衰特性に優れ、振動子の周
端部に斜面を設けることによってエネルギー閉じ込め効
率が向上することは勿論、各振動子の斜面形状を相違さ
せることによって、スプリアスの少ないMCFを得ること
ができる。
As is clear from the above description, according to the present invention, it is possible to enhance the damping characteristics by connecting the vibrators in multiple stages, and to improve the energy trapping efficiency by providing the inclined surface at the peripheral end of the vibrators. By changing the slope shape of the oscillator, it is possible to obtain an MCF with less spurious.

【図面の簡単な説明】[Brief description of drawings]

第1図は本考案にかかるMCFの一例の断面図、第2図は
その振動子の一例の横断面図、第3図は振動子の他の例
の横断面図、第4図は振動子のさらに他の例の横断面
図、第5図は従来の振動子の正面図、第6図は振動子を
複数段縦接続したフィルタの回路図である。 1,1′,1″…振動子、1a,1b,1c…斜面、2…入力用電
極、3…出力用電極、4…接地用電極。
1 is a cross-sectional view of an example of the MCF according to the present invention, FIG. 2 is a cross-sectional view of an example of the vibrator, FIG. 3 is a cross-sectional view of another example of the vibrator, and FIG. 4 is a vibrator. FIG. 5 is a cross-sectional view of yet another example of FIG. 5, FIG. 5 is a front view of a conventional vibrator, and FIG. 6 is a circuit diagram of a filter in which a plurality of vibrators are vertically connected. 1,1 ′, 1 ″ ... Oscillator, 1a, 1b, 1c ... Slope, 2 ... Input electrode, 3 ... Output electrode, 4 ... Ground electrode.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】周端部に斜面を形成した圧電単結晶の円板
型ATカット厚みすべり振動子に複数対の電極を形成し、
この振動子を複数段縦接続してなるモノリシッククリス
タルフィルタにおいて、 各段の振動子の斜面を異なる形状としたことを特徴とす
るモノリシッククリスタルフィルタ。
1. A plurality of pairs of electrodes are formed on a disk-shaped AT-cut thickness sliding oscillator of a piezoelectric single crystal having a beveled surface at its peripheral end.
A monolithic crystal filter in which a plurality of stages of these oscillators are vertically connected, in which the slopes of the oscillators in each stage have different shapes.
JP14624788U 1988-11-09 1988-11-09 Monolithic crystal filter Expired - Lifetime JPH0641386Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14624788U JPH0641386Y2 (en) 1988-11-09 1988-11-09 Monolithic crystal filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14624788U JPH0641386Y2 (en) 1988-11-09 1988-11-09 Monolithic crystal filter

Publications (2)

Publication Number Publication Date
JPH0266028U JPH0266028U (en) 1990-05-18
JPH0641386Y2 true JPH0641386Y2 (en) 1994-10-26

Family

ID=31415557

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14624788U Expired - Lifetime JPH0641386Y2 (en) 1988-11-09 1988-11-09 Monolithic crystal filter

Country Status (1)

Country Link
JP (1) JPH0641386Y2 (en)

Also Published As

Publication number Publication date
JPH0266028U (en) 1990-05-18

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