JPS59117310A - Elastic surface wave resonator - Google Patents

Elastic surface wave resonator

Info

Publication number
JPS59117310A
JPS59117310A JP22492182A JP22492182A JPS59117310A JP S59117310 A JPS59117310 A JP S59117310A JP 22492182 A JP22492182 A JP 22492182A JP 22492182 A JP22492182 A JP 22492182A JP S59117310 A JPS59117310 A JP S59117310A
Authority
JP
Japan
Prior art keywords
surface wave
elastic surface
electrode
piezoelectric substrate
surface acoustic
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.)
Pending
Application number
JP22492182A
Other languages
Japanese (ja)
Inventor
Taiji Yamamoto
泰司 山本
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric 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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP22492182A priority Critical patent/JPS59117310A/en
Publication of JPS59117310A publication Critical patent/JPS59117310A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/25Constructional features of resonators using surface acoustic waves

Landscapes

  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)

Abstract

PURPOSE:To obtain an elastic surface wave resonator with small size and low cost without adhering especially an absorbing band by forming a drawing-out electrode pad of an interdigitating electrode to both ends in the propagating direction of an elastic surface wave on a piezoelectric substrate. CONSTITUTION:Each electrode finger of the interdigitating electrode 12 is connected alternately to conductors 21, 22 and the leads 21, 22 pass respectively through both sides of the elastic surface wave propagating path and are connected to the drawing-out electrode pads 25, 26 formed at both ends of the elastic surface wave propagating path on the piezoelectric substrate 11. Electrodes 13, 14 are grating electrodes arranged at an equal interval on the elastic surface wave propagating path. Thus, it is not necessary to widen the width of the piezoelectric substrate 11 to form the electrode pads 25, 26, and since an unnecessary elastic surface wave is absorbed by the electrode pads 25, 26 and lead wires connected thereto, no special absorbing band is required. Thus, miniaturization and low cost are realized.

Description

【発明の詳細な説明】 本発明は、弾性表面波共振子の構造に関する。[Detailed description of the invention] The present invention relates to the structure of a surface acoustic wave resonator.

従来の弾性表面波共振子は、例えば第1図に示すように
、圧電基板11の長手方向のほぼ中央に交差指電極12
を形成し、その両側にグレーデインク電極13.14を
等間隔で配列し、交差指電極12の各電極指は一軍おき
に引出し用のパッド15または16に接続している。上
記引出し用の電極パッド15.16は、図示のように弾
性表面波の伝搬路(交差指電極120′電極指に対して
直角な方向)の両側に設けられている。そして、上記弾
性表面波の伝搬路の両端部には、吸収帯17.18を付
着させて、不要な弾性表面波を減衰させている。従って
、上述の従来の共振子は、吸収帯17.18を付着させ
る手数および余分な長さを必要とし、また、引出し用電
極パッド15.16を形成するために圧電基板110幅
を広(しなければならないという欠点がある。このため
、従来のこの棟共振子は、コストが増大する。
For example, as shown in FIG. 1, a conventional surface acoustic wave resonator has an interdigital electrode 12 approximately in the longitudinal center of a piezoelectric substrate 11.
, and grade ink electrodes 13 and 14 are arranged at regular intervals on both sides, and each electrode finger of the interdigital electrode 12 is connected to a lead-out pad 15 or 16 every other group. The lead-out electrode pads 15 and 16 are provided on both sides of the surface acoustic wave propagation path (in the direction perpendicular to the electrode fingers of the interdigital electrode 120') as shown in the figure. Absorption bands 17 and 18 are attached to both ends of the surface acoustic wave propagation path to attenuate unnecessary surface acoustic waves. Therefore, the above-mentioned conventional resonator requires labor and extra length to attach the absorption bands 17, 18, and also requires widening the piezoelectric substrate 110 to form the lead-out electrode pads 15, 16. Therefore, the cost of the conventional ridge resonator increases.

本発明の目的は、上述の従来の欠点を解決し、圧電基板
の面積を縮少し、かつ吸収帯を特別に付着させない小形
かつ低コストの弾性表面波共振子を提供することにある
SUMMARY OF THE INVENTION An object of the present invention is to solve the above-mentioned conventional drawbacks, reduce the area of a piezoelectric substrate, and provide a small and low-cost surface acoustic wave resonator in which no absorption band is specifically attached.

本発明の共振子は、圧電基板上に交差指電極が形成され
た弾性表面波共振子において、前記圧電基板上の弾性表
面波伝搬方向の両端部に前記交差指電極の引出し用電極
パッドを形成したことを特徴とする。
The resonator of the present invention is a surface acoustic wave resonator in which interdigital electrodes are formed on a piezoelectric substrate, in which electrode pads for leading out the interdigital electrodes are formed at both ends of the piezoelectric substrate in the surface acoustic wave propagation direction. It is characterized by what it did.

次に、本発明について、図面を参照して詳細に説明する
Next, the present invention will be explained in detail with reference to the drawings.

第2図は、本発明の一実施例を示す平面図であリ、第1
図に示した従来例と同等の特性を有する共振子である。
FIG. 2 is a plan view showing one embodiment of the present invention;
This resonator has characteristics equivalent to the conventional example shown in the figure.

すなわち、交差指電極12の各電極指は、一本おきに導
線21.22に接続され、4肪21.22は、それぞれ
弾性表面波伝搬路の両仙」を迫って引出し用電極パッド
25.26に接代される。引出し用電極パッド25.2
6は、圧電基板11上の弾性表面波伝搬路の両端部に形
成されている。勿論クレーディング電極13.14は、
従来と同体旋父差指′直極12の両(Ullに等間隔で
配列され−(いる。従って、本呆施例では、電極バッド
25.26乞形成するために圧α基板110幅を広くす
る必要がなく、基板面積を小とすることかできる。そし
て、不一安な弾性表面波は、電極パッド25.26およ
びこれらに接続されるリード線によって吸収されるから
第1図に示した従来例と同様な特性を有する。
That is, each electrode finger of the interdigital electrode 12 is connected to the conducting wire 21.22 every other time, and the four fingers 21.22 are connected to the lead-out electrode pad 25. 26. Extraction electrode pad 25.2
6 are formed at both ends of the surface acoustic wave propagation path on the piezoelectric substrate 11. Of course, the cladding electrodes 13 and 14 are
Conventionally, the co-rotating index finger's straight poles 12 are arranged at equal intervals on both sides of the straight pole 12. Therefore, in this embodiment, the width of the pressure α substrate 110 is widened in order to form the electrode pads 25, 26. There is no need to do this, and the board area can be reduced.In addition, the unstable surface acoustic waves are absorbed by the electrode pads 25 and 26 and the lead wires connected to these, as shown in Figure 1. It has the same characteristics as the conventional example.

第3区は、本発明の他の実施例を示す平面図であり、ク
レーディング電極を持たない共振子に適、「□」した場
合を示す。この場合も引出し用の′電極パッド25.2
6は、弾性表面波伝搬路の両端部に配置され、交差指電
極12の各電極指は1本おきに弾性表面波伝搬路の両側
の導線を介してそれぞれit@!、パッド25.26に
接続されている。電極パッド25.26およびこれらに
接続されるリード線は不要なZ+i性表面波を吸収する
役割りも果す。
The third section is a plan view showing another embodiment of the present invention, and shows the case of "□" suitable for a resonator without a cladding electrode. In this case as well, the electrode pad 25.2 for extraction
6 are arranged at both ends of the surface acoustic wave propagation path, and every other electrode finger of the interdigital electrode 12 is connected to it@! via conductive wires on both sides of the surface acoustic wave propagation path. , connected to pads 25, 26. The electrode pads 25, 26 and the lead wires connected thereto also serve to absorb unnecessary Z+i surface waves.

から、吸収帯をl特別に設ける必要はない。また、圧電
基板110幅は狭(てすむという効果がある。
Therefore, there is no need to provide a special absorption band. Further, the piezoelectric substrate 110 has the effect of being narrow.

以上のように、本発明においては、交差指電極を電気的
に引出すための電極パッドを圧電基板上の弾性表面波伝
搬方向の両端部く形成して、該電極パッドおよびこれに
接続されるリード線によって不要な弾性表面波を吸収さ
せるように構成したから、特別な吸収帯を設けないで従
来と同様な特性を得ることができる。本発明によればt
f&パッドを形成するために圧電基板の幅を広げる必要
がないから小面積の圧電基板で足りる。また吸収帯を付
着させる手数が不要であり、小形安価に提供される効果
がある。
As described above, in the present invention, electrode pads for electrically drawing out the interdigital electrodes are formed at both ends of the surface acoustic wave propagation direction on the piezoelectric substrate, and the electrode pads and the leads connected thereto are formed at both ends of the piezoelectric substrate in the surface acoustic wave propagation direction. Since the structure is configured so that unnecessary surface acoustic waves are absorbed by the wire, the same characteristics as conventional ones can be obtained without providing a special absorption band. According to the invention t
Since there is no need to increase the width of the piezoelectric substrate to form the f&pad, a piezoelectric substrate with a small area is sufficient. Further, there is no need to attach an absorption band, and the device can be provided in a small size and at low cost.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の弾性表面波共振子の一例を示す平面図、
第2図は本発明の一実旋例を示す平面図、第3図は本発
明の他の実施例を示す平面図である。 図において、11・・・圧電基板、12・−・交差指電
極、13.14・・・グレーディング電極、15.16
゜25.26・・・′磁極バッド、17.18・−・吸
収帯、21.22・・・導線。 代理人 弁理士住田俊宗
FIG. 1 is a plan view showing an example of a conventional surface acoustic wave resonator.
FIG. 2 is a plan view showing one practical example of the present invention, and FIG. 3 is a plan view showing another embodiment of the present invention. In the figure, 11... piezoelectric substrate, 12... interdigital electrode, 13.14... grading electrode, 15.16
゜25.26...'magnetic pole pad, 17.18...absorption band, 21.22...conductor wire. Agent: Patent attorney Toshimune Sumita

Claims (1)

【特許請求の範囲】[Claims] 圧電基板上に交差指電極が形成された弾性表面波共振子
において、前記圧電基板上の弾性表面波伝搬方向の両、
端部に前記交差指電極の引出し用電極パッドを形成した
ことを特徴とする弾性表面波共振子。
In a surface acoustic wave resonator in which interdigital electrodes are formed on a piezoelectric substrate, both sides of the surface acoustic wave propagation direction on the piezoelectric substrate,
A surface acoustic wave resonator characterized in that an electrode pad for leading out the interdigital electrodes is formed at an end portion.
JP22492182A 1982-12-23 1982-12-23 Elastic surface wave resonator Pending JPS59117310A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22492182A JPS59117310A (en) 1982-12-23 1982-12-23 Elastic surface wave resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22492182A JPS59117310A (en) 1982-12-23 1982-12-23 Elastic surface wave resonator

Publications (1)

Publication Number Publication Date
JPS59117310A true JPS59117310A (en) 1984-07-06

Family

ID=16821249

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22492182A Pending JPS59117310A (en) 1982-12-23 1982-12-23 Elastic surface wave resonator

Country Status (1)

Country Link
JP (1) JPS59117310A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61113421U (en) * 1984-12-27 1986-07-17
EP0189123A2 (en) * 1985-01-18 1986-07-30 Siemens Aktiengesellschaft Acoustic-wave filter
EP0451078A1 (en) * 1990-04-03 1991-10-09 Institut De Recherches De La Siderurgie Francaise (Irsid) Sampler for blast furnace

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61113421U (en) * 1984-12-27 1986-07-17
EP0189123A2 (en) * 1985-01-18 1986-07-30 Siemens Aktiengesellschaft Acoustic-wave filter
EP0451078A1 (en) * 1990-04-03 1991-10-09 Institut De Recherches De La Siderurgie Francaise (Irsid) Sampler for blast furnace

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