JP3102872B2 - Ultra-thin piezoelectric vibrator - Google Patents

Ultra-thin piezoelectric vibrator

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Publication number
JP3102872B2
JP3102872B2 JP02172114A JP17211490A JP3102872B2 JP 3102872 B2 JP3102872 B2 JP 3102872B2 JP 02172114 A JP02172114 A JP 02172114A JP 17211490 A JP17211490 A JP 17211490A JP 3102872 B2 JP3102872 B2 JP 3102872B2
Authority
JP
Japan
Prior art keywords
electrode
piezoelectric
ultra
piezoelectric block
concave
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 - Fee Related
Application number
JP02172114A
Other languages
Japanese (ja)
Other versions
JPH0461507A (en
Inventor
孝夫 森田
修 石井
武文 黒崎
Original Assignee
東洋通信機株式会社
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 東洋通信機株式会社 filed Critical 東洋通信機株式会社
Priority to JP02172114A priority Critical patent/JP3102872B2/en
Priority to US07/809,512 priority patent/US5235240A/en
Priority to DE69124339T priority patent/DE69124339T2/en
Priority to PCT/JP1991/000615 priority patent/WO1991019351A1/en
Priority to EP91908864A priority patent/EP0484545B1/en
Priority to KR1019910700781A priority patent/KR920702898A/en
Publication of JPH0461507A publication Critical patent/JPH0461507A/en
Application granted granted Critical
Publication of JP3102872B2 publication Critical patent/JP3102872B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は基本波振動によって数10乃至数100MHzに及ぶ
高い共振周波数を得ることのできる超薄肉圧電振動子に
関する。
Description: TECHNICAL FIELD The present invention relates to an ultra-thin piezoelectric vibrator capable of obtaining a high resonance frequency ranging from several tens to several hundreds MHz by fundamental wave vibration.

(従来の技術) 近年、各種電子機器、通信機器においては、高周波化
と高い周波数安定度の要求が厳しくなっているが、従来
より圧電デバイス(振動子、フィルタ)として多用され
てきた一般のATカット水晶振動子は温度−周波数特性は
極めて優れているもののその共振周波数は板厚に反比例
するため、製造技術及び機械的強度の観点より40MHz程
度が限界であった。
(Prior Art) In recent years, demands for higher frequency and higher frequency stability have become strict in various electronic devices and communication devices, but general ATs which have been frequently used as piezoelectric devices (vibrators and filters) have been used in the past. Although the cut-quartz resonator has excellent temperature-frequency characteristics, its resonance frequency is inversely proportional to the plate thickness. Therefore, the limit is about 40 MHz from the viewpoint of manufacturing technology and mechanical strength.

又、ATカット水晶振動子の高調波成分を抽出して基本
波共振周波数の奇数倍の周波数を得る所謂オーバートー
ン発振手段も広く用いられているが、発振回路にコイル
を含むLC同調回路を必要とするため発振回路を半導体集
積回路化する上で不都合がある上、容量比が大きく、且
つインピーダンスレベルが高い為発振が困難になる場合
があるという欠陥があった。
A so-called overtone oscillator that extracts the harmonic component of the AT-cut crystal oscillator and obtains a frequency that is an odd multiple of the fundamental wave resonance frequency is also widely used. Therefore, there are disadvantages in that the oscillation circuit is disadvantageous in forming a semiconductor integrated circuit, and oscillation is sometimes difficult due to a large capacitance ratio and a high impedance level.

一方、インタディジタル・トランスジューサ電極の電
極指ピッチによって共振周波数が決定される弾性表面波
共振子は、フォトリソグラフィ技術の進歩によって1GHz
程度の出力まで可能となってはきたが、これに使用し得
る圧電基板の温度−周波数特性がATカット水晶に比して
著しく劣るという問題があった。
On the other hand, surface acoustic wave resonators whose resonance frequency is determined by the electrode finger pitch of the interdigital transducer
Although it has been possible to achieve an output of about the same degree, there has been a problem that the temperature-frequency characteristics of a piezoelectric substrate that can be used for this are significantly inferior to AT-cut quartz.

上述の如き問題を解決するため、従来より第4図
(a)(b)に示すごとき圧電共振子が研究されてい
る。
In order to solve the above-mentioned problems, piezoelectric resonators as shown in FIGS. 4A and 4B have been studied.

即ち、この圧電共振子はATカット水晶ブロック1の片
面の中央部に機械加工又はエッチングによって凹陥部2
を形成するとともに、凹陥部2の底面に位置する振動部
3の厚さを、例えば100MHzの基本波共振周波数を得んと
するならば約17μmとする。
That is, this piezoelectric resonator is formed by machining or etching a concave portion 2 in the center of one side of the AT-cut quartz block 1.
Is formed, and the thickness of the vibrating portion 3 located on the bottom surface of the concave portion 2 is set to about 17 μm in order to obtain a fundamental wave resonance frequency of, for example, 100 MHz.

凹陥部2を形成した結果、凹陥部2側のブロック面に
は、超薄板状の振動部3の周縁部に厚肉の環状囲繞部
(リブ)4が前記振動部3と一体的に形成され超薄板状
の振動部を機械的に支持する。
As a result of the formation of the concave portion 2, a thick annular surrounding portion (rib) 4 is formed integrally with the vibrating portion 3 on the peripheral surface of the ultra-thin plate-shaped vibrating portion 3 on the block surface on the concave portion 2 side. This mechanically supports the ultra-thin vibrating part.

上述した如き構造を有する圧電素板の凹陥内側壁を含
む全面に導体膜5を付着すると共に、その対向面側の振
動部3の表面に部分電極6及びこれから延びる電極リー
ド7を真空蒸着等の手法を用いて付着すれば、共振周波
数の極めて高い圧電共振子を得ることができる。
The conductor film 5 is adhered to the entire surface including the concave inner side wall of the piezoelectric element having the above-described structure, and the partial electrode 6 and the electrode lead 7 extending therefrom are formed on the surface of the vibrating portion 3 on the opposite surface side by vacuum evaporation or the like. If the piezoelectric resonator is attached using a technique, a piezoelectric resonator having an extremely high resonance frequency can be obtained.

圧電素板の凹陥内壁を含む全面に導体膜5を付着する
主な理由は、精密なマスクを用いた特殊な蒸着技法によ
り部分的に導体膜を形成することが煩雑で生産効率を低
下せしめるからであるが、その反面、凹陥部2部全体が
導体膜5で覆われているために前記部分電極6から延び
る電極リード7との間にコンデンサが形成されて圧電共
振子全体の容量比が増大し、周波数の変動し得る幅が小
さくなるという問題を生ずる。
The main reason for attaching the conductive film 5 to the entire surface including the inner wall of the concave portion of the piezoelectric element is that forming the conductive film partially by a special deposition technique using a precise mask is complicated and reduces the production efficiency. However, on the other hand, since the entire recess 2 is covered with the conductive film 5, a capacitor is formed between the electrode lead 7 extending from the partial electrode 6 and the capacitance ratio of the entire piezoelectric resonator increases. However, there arises a problem that the width in which the frequency can vary becomes small.

即ち、部分電極6から延びる電極リード7に充分な導
電性を与えるために電極リード部面積を大きくすると、
振動部板厚が超薄であることに起因して大容量Cを構成
する。大容量Cが形成されると、第5図に示す圧電共振
子の等価回路における並列容量COが増大して、圧電共振
子の容量比γ=C0/C1が増大するため、斯かるタイプの
共振子は電圧制御水晶発振器(VCXO)の如く所定の範囲
内で発振周波数を変動せしめる必要のある発振回路への
適用が制限を受けるであろうし、又多重モードフィルタ
素子に適用せんとしても比較的広いパスバンドを要求さ
れた場合には対応が困難であるという欠陥が予測され
る。
That is, if the area of the electrode lead portion is increased in order to give sufficient conductivity to the electrode lead 7 extending from the partial electrode 6,
The large capacity C is formed due to the ultra-thin thickness of the vibrating part. When the large capacitance C is formed, the parallel capacitance C O in the equivalent circuit of the piezoelectric resonator shown in FIG. 5 increases, and the capacitance ratio γ = C 0 / C 1 of the piezoelectric resonator increases. Resonators of this type will have limited application to oscillator circuits that need to vary the oscillation frequency within a certain range, such as voltage controlled crystal oscillators (VCXOs), and even if they are not applied to multimode filter elements. If a relatively wide passband is required, a defect is expected that it is difficult to respond.

斯かる不具合を解決する為、全面電極のリードに対応
する部分に導体膜を付着しないようにする手法も考えら
れるが、そのためにはマスクを使用した蒸着が必要とな
り、蒸着にマスクを要しないという全面電極構成のメリ
ットを完全に損なう結果を招来する。
In order to solve such a problem, a method of preventing the conductive film from being attached to a portion corresponding to the lead of the entire surface electrode can be considered. However, for that purpose, vapor deposition using a mask is required, and a mask is not required for vapor deposition. This results in completely deteriorating the merits of the full-surface electrode configuration.

(発明の目的) 本発明は超薄板圧電共振子において予測される上述し
た如き問題点に鑑みてなされたものであって、水晶等の
圧電ブロック表面に形成した凹陥部底面を超薄板状の圧
電振動部とした超薄肉圧電振動子において、前記超薄肉
の振動部を介して電極と電極リードパターンとが相対面
する結果、コンデンサを形成し共振子の並列容量を増大
させることに起因して発生する種々の不都合を解消する
ことができる超薄肉圧電振動子を提供することを目的と
する。
(Objects of the Invention) The present invention has been made in view of the above-mentioned problems expected in an ultra-thin piezoelectric resonator, and has a concave bottom formed on the surface of a piezoelectric block made of quartz or the like. In the ultra-thin piezoelectric vibrator used as the piezoelectric vibrating portion, the electrode and the electrode lead pattern face each other through the ultra-thin vibrating portion, thereby forming a capacitor and increasing the parallel capacitance of the resonator. It is an object of the present invention to provide an ultra-thin piezoelectric vibrator that can eliminate various inconveniences caused by the vibration.

(発明の概要) 上記の目的を達成するため本発明に係る超薄肉圧電振
動子は、超薄肉の振動部の一面に形成する電極から伸び
る電極リードパターンのうち厚肉の環状囲繞部に対応す
る部分を他の部分より充分に幅広としたことを特徴とす
る。
(Summary of the Invention) In order to achieve the above object, an ultra-thin piezoelectric vibrator according to the present invention includes a thick annular surrounding portion of an electrode lead pattern extending from an electrode formed on one surface of an ultra-thin vibrating portion. It is characterized in that the corresponding part is sufficiently wider than the other parts.

(発明の実施例) 以下、添付図面に示した好適な実施例に基づいて本発
明を詳細に説明する。
Hereinafter, the present invention will be described in detail based on preferred embodiments shown in the accompanying drawings.

実施例の説明に先立って、本発明の理解を助ける為本
発明の基礎となる超薄肉圧電振動子が何故にその凹陥部
に全面電極を、その対向面側に部分電極を設ける如き電
極構成を採用するかについて少しく解説する。
Prior to the description of the embodiments, in order to assist the understanding of the present invention, an electrode configuration such that the ultra-thin piezoelectric vibrator serving as the basis of the present invention is provided with a full-surface electrode in its concave portion and a partial electrode on its opposing surface side I will explain a little about whether to adopt.

第1に真空蒸着技術の観点から前述した如き圧電基板
凹陥側振動部に部分電極を、又該電極から前記凹陥の内
側壁及び段差を越えて幅の狭い電極リードを延長するこ
とは、圧電基板を水平面に対し傾けて蒸着を行なう等の
面倒な手法を用いればとも角、極めて困難であって電極
リードの導通確保に不安がある為、該面を全面電極とし
いずれかの部分で必ず導通を確保し得るようにしたもの
である。
First, from the viewpoint of the vacuum deposition technique, extending a partial electrode to the piezoelectric substrate recess side vibrating portion as described above, and extending a narrow electrode lead from the electrode over the inner wall and the step of the piezoelectric substrate, It is extremely difficult to use a troublesome method such as performing evaporation by inclining the electrode with respect to the horizontal plane, and it is extremely difficult to secure conduction of the electrode leads. It is something that can be secured.

第2に斯かるタイプの共振子は元来デバイスの超小型
化を目的とし、圧電基板のサイズは例えば3mm×3mm以下
としたい。然りとすれば、一枚の圧電ウェハー上にバッ
チ処理で一挙に多数のチップを形成し、最後にこれを個
々のチップに切断する製法を採用する。この場合、上述
したタイプの電極構成を採用すれば、ウェハーの一面に
は単に導体膜の全面蒸着を行なえば足り、フォトマスク
或はフォトリソグラフ用マスクの微妙な位置合わせを要
しないので、生産効率、歩留りを向上し、コストを低減
することができる。
Secondly, this type of resonator originally aims at miniaturization of the device, and the size of the piezoelectric substrate is desired to be, for example, 3 mm × 3 mm or less. In other words, a method is adopted in which a large number of chips are formed all at once in a batch process on one piezoelectric wafer, and the chips are finally cut into individual chips. In this case, if an electrode configuration of the type described above is employed, it is sufficient to simply deposit a conductor film over the entire surface of the wafer, and fine alignment of a photomask or photolithographic mask is not required. Thus, the yield can be improved and the cost can be reduced.

以上の如き理由により、従来から研究されていた超薄
肉圧電振動子は凹陥側表面に全面電極を付着することを
基本とするものであることに留意されたい。
For the above reasons, it should be noted that the ultra-thin piezoelectric vibrator which has been studied in the past is basically based on attaching the entire surface electrode to the concave side surface.

しかしながら、上述した如き電極構成を用いれば、前
記振動部の板厚が極めて小さいこともあって該部表裏の
全面電極と、電極リード部との間に大容量のキャパシタ
が構成され、その結果共振器の容量比が大きくなり、種
々の不都合を生ずること前述の通りである。
However, when the electrode configuration as described above is used, a large-capacity capacitor is formed between the entire surface electrodes on the front and back sides of the vibrating portion and the electrode lead portion because the thickness of the vibrating portion is extremely small. As described above, the capacity ratio of the container becomes large, causing various inconveniences.

この問題を解決するため、本発明に係る超薄肉圧電振
動子は以下の如き電極構造をとる。
To solve this problem, the ultra-thin piezoelectric vibrator according to the present invention has the following electrode structure.

第1図は本発明の基本的構成を示す平面図であって、
超薄板圧電ブロック1の凹陥2側に形成した全面電極と
対向する面上の対向電極6より延びる電極リード7の環
状囲繞部4に対応する部分7aの幅員を幅広にしたもので
ある。
FIG. 1 is a plan view showing a basic configuration of the present invention,
The width of a portion 7a corresponding to the annular surrounding portion 4 of the electrode lead 7 extending from the counter electrode 6 on the surface facing the entire surface electrode formed on the concave 2 side of the ultra-thin piezoelectric block 1 is made wider.

斯くの如く振動部3上に位置する電極リード部分7bの
幅員を必要最小限に極限しながらも、環状囲繞部4の裏
面上に位置する電極リード部分7aの幅員を幅広とする理
由は、振動部3はその肉厚が極めて小さく、該部表裏両
面に夫々広面積の導体膜が対向して存在すれば大なる容
量のキャパシタを構成するのに対して、環状囲繞部4は
その肉厚が大であって仮にその表裏に導体膜が存在して
もさほど大なる容量を有することがなく、共振子の容量
比には重大な影響を与えないと考えられるからである。
また、細い電極リード部分7bの長さを極限することによ
ってオーミックなロスを低減できるからである。
The reason why the width of the electrode lead portion 7a located on the back surface of the annular surrounding portion 4 is widened while the width of the electrode lead portion 7b located on the vibration portion 3 is minimized as described above is because vibration The portion 3 has a very small thickness, and a large-capacity capacitor is formed if a large-area conductive film is present on both the front and back surfaces of the portion, whereas the annular surrounding portion 4 has a small thickness. This is because even if the conductor film is present on the front and back surfaces, the capacitance is not so large, and the capacitance ratio of the resonator is not considered to be significantly affected.
Also, by limiting the length of the thin electrode lead portion 7b, ohmic loss can be reduced.

なお、上述した如き超薄肉圧電振動子は第2図に示す
如くその凹陥2側を例えばセラミクスを焼結した皿型パ
ッケージ8の内底面に設けて導体膜10に対面する如く収
納し、前記凹陥2側全面電極5を環状囲繞部4一縁表面
において前記導体膜10と導電性接着剤11で接着固定する
と共に前記導体膜10を介してパッケージの外部リード端
子12と接続する。一方、部分電極6から延びる電極リー
ド7の幅広部7aについてはこれをパッケージ外壁のリー
ド端子13と接続しているパッケージ8内壁段差部に設け
た導体パッド14とボンディングワイヤ15にて接続するの
に利用するに好都合である。
In addition, as shown in FIG. 2, the ultra-thin piezoelectric vibrator as described above is provided with its recess 2 side on the inner bottom surface of a dish-shaped package 8 in which ceramics is sintered, for example, and is housed so as to face the conductive film 10. The entire surface electrode 5 on the side of the recess 2 is adhered and fixed to the conductor film 10 with a conductive adhesive 11 on one edge surface of the annular surrounding portion 4 and connected to the external lead terminal 12 of the package via the conductor film 10. On the other hand, the wide part 7a of the electrode lead 7 extending from the partial electrode 6 is connected to the conductor pad 14 provided on the step part on the inner wall of the package 8 which is connected to the lead terminal 13 on the outer wall of the package by the bonding wire 15. It is convenient to use.

以上、本発明を圧電振動子に適用した場合について説
明したが、本発明は超薄板多重モードフィルタにも同様
に適用可能である。多重モードフィルタのうち最も多用
されている2重モード圧電フィルタは周知の如く圧電基
板の一主面(この場合は凹陥2側)の全面電極5をアー
ス電極とし、その対向面に分割近接電極16を設け、これ
ら両電極に交番電界を印加して、両電極間に音響結合を
生ぜしめ、その結果励起する共振周波数の相異なる2つ
の振動モードを利用してバンドパスフィルタを構成する
ものである。
As described above, the case where the present invention is applied to the piezoelectric vibrator has been described. However, the present invention can be similarly applied to an ultra-thin multi-mode filter. As is well known, the most frequently used dual mode piezoelectric filter among the multimode filters is that the whole surface electrode 5 on one main surface (in this case, the recess 2 side) of the piezoelectric substrate is used as a ground electrode and the divided proximity electrode 16 is provided on the opposite surface. And an alternating electric field is applied to both electrodes to generate acoustic coupling between the two electrodes. As a result, a band-pass filter is constructed using two vibration modes having different resonance frequencies to be excited. .

このようなフィルタ素子も又等価並列容量COが大きく
なると、即ち容量比γが大きくなると実現可能なバンド
幅が減少することは周知である。従って、第3図に示す
如く分割電極16、16から引出すリードの内前記振動部3
表面に付する部分17、17は細く、環状囲繞部4表面上に
おける部分17a,17aは幅広にすればよい。
It is well known that the filter bandwidth of such a filter element also decreases as the equivalent parallel capacitance C O increases, that is, as the capacitance ratio γ increases. Therefore, as shown in FIG.
The portions 17, 17 attached to the surface may be thin, and the portions 17a, 17a on the surface of the annular surrounding portion 4 may be wide.

斯くすることによって数10乃至100MHzの共振周波数を
基本波振動によって得る振動子或はこの周波数をほぼ中
心周波数とするフィルタ素子を超小型に形成し、しかも
これらの特性、殊に共振周波数の可変幅、フィルタのバ
ンド幅を十分大きな値に確保することができる。
In this way, a vibrator that obtains a resonance frequency of several tens to 100 MHz by the fundamental vibration or a filter element having this frequency as a center frequency is formed in a very small size, and these characteristics, particularly, the variable width of the resonance frequency are formed. , The bandwidth of the filter can be secured to a sufficiently large value.

(発明の効果) 本発明は以上説明した如く構成するものであるから、
超薄肉圧電振動子或はフィルタ素子の容量比を低い値に
押え、振動子にあっては共振周波数の可変幅を充分に確
保し、又フィルタ素子にあっては、広いパスバンドを与
える上で著しい効果がある。更に、共振子振動部表面の
リード面積が電極のそれに比して小なることから、不要
波の発生も少ないと云う効果を併せ持つものである。
(Effect of the Invention) Since the present invention is configured as described above,
The capacitance ratio of the ultra-thin piezoelectric vibrator or the filter element is kept at a low value, the variable width of the resonance frequency is sufficiently secured for the vibrator, and a wide pass band is provided for the filter element. Has a remarkable effect. Further, since the lead area on the surface of the resonator vibrating part is smaller than that of the electrode, the effect of generating unnecessary waves is also reduced.

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

第1図本発明に係る超薄肉圧電振動子の一例を示す平面
図、第2図は本発明に係る超薄肉圧電振動子のパッケー
ジ手法の一例を示す断面図、第3図は本発明を適用した
超薄板多重モードフィルタ素子の実施例を示す平面図、
第4図(a)及び(b)は夫々従来から研究されていた
超薄板圧電共振子の構造を示す斜視図及びそのX−X断
面図、第5図は共振子の等価回路図である。 1……超薄板圧電ブロック、2……凹陥、3……振動
部、4……環状囲繞部、5……全面電極、6……部分電
極、7……電極リード、7a……幅広部、7b……狭幅部
FIG. 1 is a plan view showing an example of an ultra-thin piezoelectric vibrator according to the present invention, FIG. 2 is a cross-sectional view showing an example of a packaging method of the ultra-thin piezoelectric vibrator according to the present invention, and FIG. Plan view showing an embodiment of an ultra-thin plate multi-mode filter element to which
4 (a) and 4 (b) are a perspective view and a sectional view taken along the line XX, respectively, showing the structure of an ultra-thin plate piezoelectric resonator which has been studied conventionally, and FIG. 5 is an equivalent circuit diagram of the resonator. . 1 ... ultra-thin plate piezoelectric block, 2 ... recess, 3 ... vibrating part, 4 ... annular surrounding part, 5 ... full-surface electrode, 6 ... partial electrode, 7 ... electrode lead, 7a ... wide part , 7b …… narrow part

フロントページの続き (56)参考文献 特開 昭62−185403(JP,A) 特開 昭61−3514(JP,A) 特開 昭61−3513(JP,A) 特開 昭58−219810(JP,A) (58)調査した分野(Int.Cl.7,DB名) H03H 9/00 - 9/215 H03H 9/54 - 9/60 Continuation of front page (56) References JP-A-62-185403 (JP, A) JP-A-61-3514 (JP, A) JP-A-61-3513 (JP, A) JP-A-58-219810 (JP, A) , A) (58) Field surveyed (Int. Cl. 7 , DB name) H03H 9/00-9/215 H03H 9/54-9/60

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】圧電ブロックの片面に凹陥を設けることに
より、該凹陥の底面に超薄肉の振動部と、該振動部周縁
を支持する厚肉の環状囲繞部とを一体的に形成し、前記
圧電ブロックの凹陥側には全面電極を形成し、前記凹陥
と対向する前記圧電ブロックの対向面には部分電極及び
これから前記圧電ブロック端縁に延びる電極リードを設
け、該電極リードのうち前記環状囲繞部表面に付着する
部分を他の部分より幅が広い幅広部としたことを特徴と
する超薄肉圧電振動子。
1. A concave portion is provided on one surface of a piezoelectric block, so that an ultra-thin vibrating portion and a thick annular surrounding portion supporting the peripheral portion of the vibrating portion are integrally formed on the bottom surface of the concave portion, A whole surface electrode is formed on the concave side of the piezoelectric block, and a partial electrode and an electrode lead extending from the piezoelectric block to the edge of the piezoelectric block are provided on the opposing surface of the piezoelectric block facing the concave. An ultra-thin piezoelectric vibrator characterized in that a portion attached to the surface of the surrounding portion is a wide portion wider than other portions.
【請求項2】圧電ブロックの片面に凹陥を設けることに
より、該凹陥の底面に超薄肉の振動部と、該振動部周縁
を支持する厚肉の環状囲繞部とを一体的に形成し、前記
圧電ブロックの凹陥側には全面電極を形成し、前記凹陥
と対向する前記圧電ブロックの対向面には部分電極及び
これから前記圧電ブロック端縁に延びる電極リードを設
け、該電極リードのうち前記環状囲繞部表面に付着する
部分を他の部分より幅が広い幅広部とし、前記圧電ブロ
ックの凹陥がパッケージの内底面に設けた導電膜と対面
する如く前記圧電ブロックを前記パッケージに収納し、
前記圧電ブロックの全面電極を前記環状囲繞部の一縁表
面において前記導電膜と導電性接着剤で接着固定し、前
記電極リードの前記幅広部と前記パッケージ内に設けた
導体パッドとをボンディングワイヤにて接続したことを
特徴とする超薄肉圧電振動子。
2. An ultra-thin vibrating portion and a thick annular surrounding portion for supporting the peripheral portion of the vibrating portion are integrally formed on the bottom surface of the concave portion by providing a concave portion on one surface of the piezoelectric block. A whole surface electrode is formed on the concave side of the piezoelectric block, and a partial electrode and an electrode lead extending from the piezoelectric block to the edge of the piezoelectric block are provided on the opposing surface of the piezoelectric block facing the concave. The portion attached to the surrounding portion surface is a wide portion wider than other portions, and the piezoelectric block is housed in the package such that the recess of the piezoelectric block faces the conductive film provided on the inner bottom surface of the package,
The whole surface electrode of the piezoelectric block is adhered and fixed to the conductive film with a conductive adhesive on one edge surface of the annular surrounding portion, and the wide portion of the electrode lead and the conductive pad provided in the package are bonded to a bonding wire. An ultra-thin piezoelectric vibrator characterized in that the piezoelectric vibrator is connected by connecting.
JP02172114A 1990-05-25 1990-06-29 Ultra-thin piezoelectric vibrator Expired - Fee Related JP3102872B2 (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP02172114A JP3102872B2 (en) 1990-06-29 1990-06-29 Ultra-thin piezoelectric vibrator
US07/809,512 US5235240A (en) 1990-05-25 1991-05-09 Electrodes and their lead structures of an ultrathin piezoelectric resonator
DE69124339T DE69124339T2 (en) 1990-05-25 1991-05-09 ELECTRODE AND ELECTRODE LINE STRUCTURE OF A PIEZOELECTRIC RESONATOR MADE OF AN ULTRA-THIN LAYER
PCT/JP1991/000615 WO1991019351A1 (en) 1990-05-25 1991-05-09 Structure of electrode and lead thereof of ultra thin plate piezoelectric resonator
EP91908864A EP0484545B1 (en) 1990-05-25 1991-05-09 Structure of electrode and lead thereof of ultra thin plate piezoelectric resonator
KR1019910700781A KR920702898A (en) 1990-05-25 1991-07-25 Electrode and electrode lead structure of ultra-thin piezoelectric resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP02172114A JP3102872B2 (en) 1990-06-29 1990-06-29 Ultra-thin piezoelectric vibrator

Publications (2)

Publication Number Publication Date
JPH0461507A JPH0461507A (en) 1992-02-27
JP3102872B2 true JP3102872B2 (en) 2000-10-23

Family

ID=15935816

Family Applications (1)

Application Number Title Priority Date Filing Date
JP02172114A Expired - Fee Related JP3102872B2 (en) 1990-05-25 1990-06-29 Ultra-thin piezoelectric vibrator

Country Status (1)

Country Link
JP (1) JP3102872B2 (en)

Also Published As

Publication number Publication date
JPH0461507A (en) 1992-02-27

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