JPS6334348Y2 - - Google Patents

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Publication number
JPS6334348Y2
JPS6334348Y2 JP11027686U JP11027686U JPS6334348Y2 JP S6334348 Y2 JPS6334348 Y2 JP S6334348Y2 JP 11027686 U JP11027686 U JP 11027686U JP 11027686 U JP11027686 U JP 11027686U JP S6334348 Y2 JPS6334348 Y2 JP S6334348Y2
Authority
JP
Japan
Prior art keywords
surface acoustic
electrodes
electrode fingers
electrode
different
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
Application number
JP11027686U
Other languages
Japanese (ja)
Other versions
JPS6275630U (en
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 filed Critical
Priority to JP11027686U priority Critical patent/JPS6334348Y2/ja
Publication of JPS6275630U publication Critical patent/JPS6275630U/ja
Application granted granted Critical
Publication of JPS6334348Y2 publication Critical patent/JPS6334348Y2/ja
Expired legal-status Critical Current

Links

Description

【考案の詳細な説明】 本考案は弾性表面波装置の構造に関するもの
で、特に分波器等として用いるのに適した弾性表
面波装置に関するものである。
[Detailed Description of the Invention] The present invention relates to the structure of a surface acoustic wave device, and particularly to a surface acoustic wave device suitable for use as a duplexer or the like.

弾性表面波装置は、圧電性の基板上に交叉櫛形
電極を設けて弾性表面波を励振させるものであ
る。交叉櫛形電極によつて励振される弾性表面波
は、交叉櫛形電極の電極指の長手方向に対して直
角の方向に伝播するが、電極の端部ではこれと伝
播方向の異なる弾性表面波が励振される。この弾
性表面波の伝播方向は、電極指の長手方向に直角
の方向から一定の角度を有しており、周波数も電
極指の間隔によつて定まる中心周波数とは異なつ
たものである。
A surface acoustic wave device excites surface acoustic waves by providing interdigitated electrodes on a piezoelectric substrate. The surface acoustic waves excited by the interdigitated electrodes propagate in a direction perpendicular to the longitudinal direction of the electrode fingers of the interdigitated electrodes, but surface acoustic waves with a different propagation direction are excited at the ends of the electrodes. be done. The propagation direction of this surface acoustic wave has a certain angle from the direction perpendicular to the longitudinal direction of the electrode fingers, and the frequency is also different from the center frequency determined by the spacing between the electrode fingers.

この現象は次の理由によるものである。弾性表
面波を交叉櫛形電極で励振する場合、弾性表面波
は交叉櫛形電極の電極指の長手方向に直角な方向
と平行な方向との成分によつて伝播方向が決定さ
れる。通常の交叉櫛形電極では直角方向の成分が
大部分であるので電極指の長手方向に直角の方向
に伝播するが、端部では平行方向の成分が強くな
るので異なる伝播方向となるものである。このこ
とから、直角方向の成分と平行方向の成分とを合
成して任意の周波数の弾性表面波を電極指の長手
方向に直角な方向からある角度をもつて伝播させ
ることができる。
This phenomenon is due to the following reasons. When a surface acoustic wave is excited by a crossed comb electrode, the propagation direction of the surface acoustic wave is determined by components in a direction perpendicular to and parallel to the longitudinal direction of the electrode fingers of the crossed comb electrode. In a normal crossed comb electrode, most of the components are in the perpendicular direction, so the propagation occurs in a direction perpendicular to the longitudinal direction of the electrode fingers, but at the ends, the parallel component becomes stronger, so the propagation direction is different. Therefore, by combining the orthogonal component and the parallel component, surface acoustic waves of any frequency can be propagated at a certain angle from a direction perpendicular to the longitudinal direction of the electrode fingers.

考案者は、上記の現象を利用して交叉櫛形電極
に周期性を特たせることを考え、これによつて周
期波源を形成して伝播方向の異なる弾性表面波を
強める方法を考えた。交叉櫛形電極に周期性を持
たせると、特定の周波数において弾性表面波の電
極指の長手方向に平行な方向の成分が強くなり、
それによつてその周波数の弾性表面波が中心周波
数のものと異なる一定の方向に伝播することを利
用するものである。
The inventor considered making use of the above-mentioned phenomenon to make the interdigitated comb-shaped electrodes feature periodicity, and devised a method to thereby form a periodic wave source and intensify surface acoustic waves propagating in different directions. When the interdigitated electrodes are given periodicity, the component of the surface acoustic wave in the direction parallel to the longitudinal direction of the electrode fingers becomes stronger at a specific frequency.
This makes use of the fact that surface acoustic waves of that frequency propagate in a fixed direction different from that of the center frequency.

電極に周期性を持たせるためには次の方法があ
る。交叉櫛形電極を並列に分割して複数の交叉櫛
形電極が電極指の長手方向に複数個配置させ、こ
れによつて長手方向に周期を有する波源を持たせ
るものである。それぞれの交叉櫛形電極はそれら
の電極指の間隔で決定される中心周波数の弾性表
面波を励振する電極となるが、これらの集合体と
しては一定の幅を有する波源が繰返して配置され
たことになる。
There are the following methods to give periodicity to the electrodes. The intersecting comb electrodes are divided in parallel and a plurality of intersecting comb electrodes are arranged in the longitudinal direction of the electrode fingers, thereby providing a wave source having a period in the longitudinal direction. Each intersecting comb-shaped electrode becomes an electrode that excites surface acoustic waves with a center frequency determined by the spacing between the electrode fingers, but as a collection of these, a wave source with a certain width is repeatedly arranged. Become.

上記のように周期性を有する交叉櫛形電極に入
力電気信号が加わると弾性表面波が励振される。
交叉櫛形電極の電極指の間隔によつて中心周波数
は決まるが、中心周波数とは異なる周波数の弾性
表面波が分割された交叉櫛形電極の各部分から発
生し、中心周波数の弾性表面波の伝播方向と異な
る一定の方向に伝播して行く。
As described above, when an input electrical signal is applied to the interdigitated interdigitated electrodes having periodicity, a surface acoustic wave is excited.
The center frequency is determined by the spacing between the electrode fingers of the interdigitated electrode, but surface acoustic waves with a frequency different from the center frequency are generated from each section of the intersected interdigitated electrode, and the propagation direction of the surface acoustic wave of the center frequency It propagates in a certain direction different from that of

このように、周期波源によつて特定の周波数の
弾性表面波を特定の方向に伝播させることができ
るが、この弾性表面波の波源の周期を適当に選択
することによつてその周波数と伝播方向を任意に
とることができる。これを利用して、特定の周波
数の信号を取り出しまたは除去することができ
る。
In this way, a surface acoustic wave of a specific frequency can be propagated in a specific direction by a periodic wave source, but by appropriately selecting the period of the surface acoustic wave wave source, the frequency and propagation direction can be changed. can be taken arbitrarily. This can be used to extract or remove signals of specific frequencies.

本考案は、上記の原理を利用して、従来になか
つた弾性表面波装置によつて、分波器等として利
用価値の高い装置を得ることを目的とする。
The object of the present invention is to utilize the above-mentioned principle to obtain a device with high utility value as a duplexer, etc., using a surface acoustic wave device that has not existed in the past.

本考案による弾性表面波装置を図面に従つて説
明する。
A surface acoustic wave device according to the present invention will be explained according to the drawings.

第1図は本考案の一実施例を示す部分平面図で
ある。入力電極のみを示してあるが、実際の装置
においては基板は広い面積を有し、所定の位置に
出力電極を具えている。圧電体の基板21上に交
叉櫛形電極24a〜24hが並列に配置されてい
る。すなわち、すべての電極指が入力電極のパツ
ドに接続されている。交叉櫛形電極24a〜24
dは同じ電極指の対向する幅W1を有しており、
交叉櫛形電極24e〜24hにおけるその幅W2
と異なるようにしてある。これによつて交叉櫛形
電極24a〜24dの部分と交叉櫛形電極24e
〜24hの部分とでは周期が異なつた構造とな
る。
FIG. 1 is a partial plan view showing an embodiment of the present invention. Although only input electrodes are shown, in an actual device, the substrate has a wide area and includes output electrodes at predetermined positions. Cross-comb electrodes 24a to 24h are arranged in parallel on a piezoelectric substrate 21. That is, all electrode fingers are connected to the pads of the input electrodes. Cross-comb electrodes 24a-24
d have opposite widths W 1 of the same electrode fingers,
The width W 2 of the crossed comb-shaped electrodes 24e to 24h
It is made to be different. As a result, the portions of the crossed comb electrodes 24a to 24d and the crossed comb electrode 24e
The period between 24h and 24h is different from each other.

交叉櫛形電極24a〜24hによつて電極(波
源)は周期性を有するようになるが、単一の周期
ではなく電極24a〜24dの部分と電極24e
〜24hの部分で異なる周期の部分が形成され
る。中心周波数は全体にわたつて同じであるが、
周期が異なることによつて電極24a〜24dの
部分から電極指の長手方向に対して直角の方向か
ら一定の角度をもつて伝播する中心周波数と異な
る周波数の弾性表面波と、電極24e〜24hの
部分から電極指の長手方向に対して直角の方向か
ら一定の角度をもつて伝播する中心周波数と異な
る周波数の弾性表面波がそれぞれ励振される。そ
れらの二種の弾性表面波は周波数及び伝播方向が
異なる。これは、二つの部分で周期性が異なるの
で前記の二方向の成分の現れ方が異なり、これに
よつて周波数、伝播方向が異なるようになる。
Although the electrodes (wave sources) have periodicity due to the interdigitated electrodes 24a to 24h, they do not have a single period but a portion of the electrodes 24a to 24d and the electrode 24e.
Portions with different periods are formed in the portion from 24h to 24h. The center frequency is the same throughout, but
Due to the different periods, surface acoustic waves of a frequency different from the center frequency propagating from the electrodes 24a to 24d at a constant angle from a direction perpendicular to the longitudinal direction of the electrode fingers, and the surface acoustic waves of the electrodes 24e to 24h. Surface acoustic waves having a frequency different from the center frequency are excited from each part, which propagate at a constant angle from a direction perpendicular to the longitudinal direction of the electrode fingers. The two types of surface acoustic waves differ in frequency and propagation direction. This is because the two parts have different periodicities, so the components in the two directions appear differently, and as a result, the frequencies and propagation directions differ.

なお、第1図では出力電極は図示されていない
が、圧電基板21は交叉櫛形電極24の電極指の
長手方向に直角な方向だけでなくその両側に広が
りを有している。そして中心周波数の弾性表面波
の伝播方向と異なる方向の所定の位置に出力電極
が二つ以上形成されている。
Although the output electrodes are not shown in FIG. 1, the piezoelectric substrate 21 extends not only in a direction perpendicular to the longitudinal direction of the electrode fingers of the interdigitated electrodes 24 but also on both sides thereof. Two or more output electrodes are formed at predetermined positions in a direction different from the propagation direction of the surface acoustic wave of the center frequency.

中心周波数と周波数及び伝播方向の異なるそれ
ぞれの弾性表面波は、入力信号にそれぞれの周波
数の信号が印加されたときにその周波数の弾性表
面波を所定の方向に励振する。この伝播方向は交
叉櫛形電極の電極指の間隔と前記の周期によつて
決定される。
When a signal of each frequency is applied to the input signal, each surface acoustic wave having a different center frequency, frequency, and propagation direction excites the surface acoustic wave of that frequency in a predetermined direction. This direction of propagation is determined by the spacing between the electrode fingers of the interdigitated electrodes and the period.

本考案は上記の例のみに限られるものではな
く、周期の変化を三通り以上にする等種々の変形
をなすことができる。また、交叉櫛形電極の中心
周波数を各交叉櫛形電極ごとに変化させても良
い。このようにして、周波数の異なつた弾性表面
波を、異つた方向に励振し、これを出力電極で電
気信号に変換することができる。
The present invention is not limited to the above example, and can be modified in various ways, such as changing the period in three or more ways. Furthermore, the center frequency of the intersecting comb electrodes may be changed for each intersecting comb electrode. In this way, surface acoustic waves with different frequencies can be excited in different directions and converted into electrical signals at the output electrode.

本考案による弾性表面波装置は分波器等として
利用できる。第2図のように、入力電極25に対
してその交叉櫛形電極の電極指の長手方向に直角
な方向から所定の角度を有する方向に出力電極2
6,27を設ける。出力電極26は中心周波数の
弾性表面波の伝播方向からθ1だけ角度を有する方
向に、出力電極27はθ2だけ角度を有する方向に
設けられている。出力電極26と出力電極27は
異なる周波数の所定の弾性表面波のみに応答する
ようにしたものである。
The surface acoustic wave device according to the present invention can be used as a duplexer, etc. As shown in FIG. 2, the output electrode 2 is oriented at a predetermined angle from the direction perpendicular to the longitudinal direction of the electrode fingers of the interdigitated electrode 25 with respect to the input electrode 25.
6, 27 are provided. The output electrode 26 is provided in a direction having an angle of θ 1 from the propagation direction of the surface acoustic wave at the center frequency, and the output electrode 27 is provided in a direction having an angle of θ 2 from the propagation direction of the surface acoustic wave of the center frequency. The output electrode 26 and the output electrode 27 are designed to respond only to predetermined surface acoustic waves of different frequencies.

このように、中心周波数と異なつた一定の周波
数の弾性表面波の伝播方向に出力電極を設けて受
信できるので選択度の良好な精度の高い弾性表面
波装置が得られる。入力電極の周期の変化を多く
してそれに応じた出力電極を多数設けてそれぞれ
の周波数成分を取り出すこともできる。また、逆
に一定の周波数の弾性表面波を除去することも可
能となり、これらを組み合わせることによつて
種々の装置ができる。
In this way, since the output electrode can be provided in the propagation direction of the surface acoustic wave having a certain frequency different from the center frequency to receive the surface acoustic wave, a highly accurate surface acoustic wave device with good selectivity can be obtained. It is also possible to increase the change in the period of the input electrode and provide a correspondingly large number of output electrodes to extract each frequency component. Conversely, it is also possible to remove surface acoustic waves of a certain frequency, and by combining these, various devices can be created.

このように、本考案による弾性表面波装置は波
源に周期性を持たせるだけでなく、周期性に変化
をつけることによつて周波数特性を変化させるこ
とができる。しかも、複数な装置が不要で電極の
構造と配置のみによつてそれがなし得る。したが
つて、製造も容易で小型化できる長所も有してい
る。
In this way, the surface acoustic wave device according to the present invention can not only provide periodicity to the wave source, but also change the frequency characteristics by varying the periodicity. Furthermore, this can be achieved only by the structure and arrangement of the electrodes without the need for multiple devices. Therefore, it also has the advantage of being easy to manufacture and miniaturized.

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

第1図は本考案の実施例の部分平面図、第2図
は本考案の他の実施例の平面図を示す。 21……圧電基板、24……交叉櫛形電極、2
5……入力電極、26,27……出力電極。
FIG. 1 is a partial plan view of an embodiment of the present invention, and FIG. 2 is a plan view of another embodiment of the present invention. 21...Piezoelectric substrate, 24...Cross comb electrode, 2
5... Input electrode, 26, 27... Output electrode.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 交叉櫛形電極を並列に分割した複数の交叉櫛形
電極から成る周期波源を有する弾性表面波装置に
おいて、該周期波源を構成する交叉櫛形電極の一
部をなす複数の交叉櫛形電極の電極指の対向する
幅が他の部分の複数の交叉櫛形電極の電極指の対
向する幅と異なるように形成され、電極指の間隔
によつて決まる電極指の長手方向に直角な方向に
伝播する中心周波数の弾性表面波と異なる二以上
の周波数の弾性表面波を該中心周波数の弾性表面
波の伝播方向と異なる方向に励振することを特徴
とする弾性表面波装置。
In a surface acoustic wave device having a periodic wave source consisting of a plurality of intersecting comb electrodes formed by dividing intersecting comb electrodes in parallel, the electrode fingers of the plurality of intersecting comb electrodes forming a part of the intersecting comb electrodes constituting the periodic wave source are opposed to each other. an elastic surface whose width is different from the opposing widths of the electrode fingers of a plurality of interdigitated electrodes in other parts, and whose center frequency propagates in a direction perpendicular to the longitudinal direction of the electrode fingers determined by the spacing of the electrode fingers; 1. A surface acoustic wave device that excites surface acoustic waves having two or more frequencies different from waves in a direction different from the propagation direction of the surface acoustic waves having the center frequency.
JP11027686U 1986-07-18 1986-07-18 Expired JPS6334348Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11027686U JPS6334348Y2 (en) 1986-07-18 1986-07-18

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11027686U JPS6334348Y2 (en) 1986-07-18 1986-07-18

Publications (2)

Publication Number Publication Date
JPS6275630U JPS6275630U (en) 1987-05-14
JPS6334348Y2 true JPS6334348Y2 (en) 1988-09-12

Family

ID=30989147

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11027686U Expired JPS6334348Y2 (en) 1986-07-18 1986-07-18

Country Status (1)

Country Link
JP (1) JPS6334348Y2 (en)

Also Published As

Publication number Publication date
JPS6275630U (en) 1987-05-14

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