JP2000286674A - Surface acoustic wave filter device and resonator - Google Patents

Surface acoustic wave filter device and resonator

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Publication number
JP2000286674A
JP2000286674A JP11090979A JP9097999A JP2000286674A JP 2000286674 A JP2000286674 A JP 2000286674A JP 11090979 A JP11090979 A JP 11090979A JP 9097999 A JP9097999 A JP 9097999A JP 2000286674 A JP2000286674 A JP 2000286674A
Authority
JP
Japan
Prior art keywords
surface acoustic
acoustic wave
face
electrode
piezoelectric substrate
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.)
Withdrawn
Application number
JP11090979A
Other languages
Japanese (ja)
Inventor
Yasubumi Horio
保文 堀尾
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.)
NGK Insulators Ltd
Original Assignee
NGK Insulators 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 NGK Insulators Ltd filed Critical NGK Insulators Ltd
Priority to JP11090979A priority Critical patent/JP2000286674A/en
Publication of JP2000286674A publication Critical patent/JP2000286674A/en
Withdrawn legal-status Critical Current

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  • Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)

Abstract

PROBLEM TO BE SOLVED: To reduce the adverse influence of reflected waves from the end faces of a surface acoustic wave filter device. SOLUTION: The end faces 10 and 11 of a crystal substrate 1 are mirror finished and the distances between an input-side converter 2 and the end face 10 and between an output-side converter 4 and the end face 11 in the propagating direction of surface acoustic waves are respectively set at an integer multiple the half wavelength of a fundamental surface acoustic wave. Thus, the conversion efficiency of the surface acoustic waves are rather improved further, because the phases of reflected waves from the end phases 10 and 11 become the same as that of a main wave and the main wave does not receive the adverse influence of the reflected waves.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、弾性表面波の反射
波のメイン波に対する悪影響を軽減する弾性表面波フィ
ルタ装置及び共振器に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a surface acoustic wave filter device and a resonator for reducing an adverse effect of a reflected surface acoustic wave on a main wave.

【0002】[0002]

【従来の技術】従来、弾性表面波フィルタ装置及び共振
器において弾性表面波の端面反射波のメイン波への悪影
響を軽減させるために、基板の端部に吸音剤が塗布され
ている。
2. Description of the Related Art Conventionally, in a surface acoustic wave filter device and a resonator, a sound absorbing agent is applied to an end portion of a substrate in order to reduce an adverse effect of an end surface reflected wave of a surface acoustic wave on a main wave.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、このよ
うな吸音剤を塗布した場合、弾性表面波の伝播方向に素
子の寸法が増大し(実際には約0.5〜1mm)、製品
の小型化の要請に反する。
However, when such a sound absorbing agent is applied, the size of the element increases in the propagation direction of the surface acoustic wave (actually, about 0.5 to 1 mm), and the size of the product is reduced. Contrary to the request.

【0004】吸音剤を塗布する代わりに基板の端部を荒
らすことによって反射波の悪影響を軽減させることも考
えられるが、このような狭い範囲を荒らすことは困難で
ある。
[0004] Instead of applying a sound absorbing agent, it is conceivable to reduce the adverse effect of the reflected wave by roughening the edge of the substrate, but it is difficult to roughen such a narrow range.

【0005】本発明の目的は、簡単な構成で端面反射波
の悪影響を軽減させることができる弾性表面波フィルタ
装置及び共振器を提供することである。
An object of the present invention is to provide a surface acoustic wave filter device and a resonator which can reduce the adverse effect of the end face reflected wave with a simple configuration.

【0006】[0006]

【課題を解決するための手段】本発明のうち請求項1記
載の弾性表面波フィルタ装置は、端面を鏡面研磨した圧
電性基板と、この圧電性基板上に形成され、電気信号が
外部から入力され、この電気信号を弾性表面波に変換す
る入力側変換器と、前記水晶基板の表面上に形成され、
前記入力側変換器で励振された弾性表面波を電気信号に
変換し、この電気信号を外部に出力する出力側変換器と
を具え、λを基本弾性表面波の伝播波長とした場合、前
記入力側変換器とそれに近接する前記圧電性基板の端面
との間の弾性表面波の伝播方向の距離を(k+1/2)
λ(k=0,1,2,...)とし、前記出力側変換器
とそれに近接する前記圧電性基板の端面との間の弾性表
面波の伝播方向の距離を(l+1/2)(l=0,1,
2,...)λとしたことを特徴とするものである。
According to a first aspect of the present invention, there is provided a surface acoustic wave filter device comprising: a piezoelectric substrate having an end face mirror-polished; and a piezoelectric substrate formed on the piezoelectric substrate, wherein an electric signal is inputted from the outside. An input converter for converting the electric signal into a surface acoustic wave, and formed on the surface of the quartz substrate,
An output converter for converting the surface acoustic wave excited by the input-side converter into an electric signal, and outputting the electric signal to the outside, wherein λ is the propagation wavelength of the basic surface acoustic wave; The distance in the propagation direction of the surface acoustic wave between the side transducer and the end face of the piezoelectric substrate adjacent to the transducer is (k + /).
λ (k = 0, 1, 2,...), and the distance in the propagation direction of the surface acoustic wave between the output-side converter and the end face of the piezoelectric substrate adjacent thereto is (l + /) ( l = 0,1,
2,. . . ) Λ.

【0007】入力側変換器とそれに近接する端面との間
の弾性表面波の伝播方向の距離及び出力側変換器とそれ
に近接する端面との間の弾性表面波の伝播方向の距離を
それぞれそのように設定することによって、端面反射波
の位相がメイン波の位相と同一になるので、メイン波は
端面反射波の悪影響が及ぼされず、むしろ弾性表面波の
変換効率が更に向上する。
The distance in the propagation direction of the surface acoustic wave between the input-side transducer and the end face close to the input-side transducer and the distance in the direction of propagation of the surface acoustic wave between the output-side transducer and the end face close to the input side transducer are respectively set as follows. Since the phase of the end-face reflected wave becomes the same as the phase of the main wave, the adverse effect of the end-face reflected wave is not exerted on the main wave, but the conversion efficiency of the surface acoustic wave is further improved.

【0008】本発明のうち請求項2記載の弾性表面波フ
ィルタ装置は、前記端面の表面粗さを0〜0.2μmと
したことを特徴とするものである。このような表面粗さ
にすることによって、端面反射波が入力側変換器及び出
力側変換器に有効に反射されるようになる。
In the surface acoustic wave filter device according to a second aspect of the present invention, the end surface has a surface roughness of 0 to 0.2 μm. With such a surface roughness, the end face reflected wave is effectively reflected by the input-side converter and the output-side converter.

【0009】本発明のうち請求項3記載の弾性表面波フ
ィルタ装置は、前記圧電性基板を単結晶材料で構成した
ことを特徴とするものである。このような単結晶材料で
構成することによって、端面を良好に鏡面研磨すること
ができる。
The surface acoustic wave filter device according to a third aspect of the present invention is characterized in that the piezoelectric substrate is made of a single crystal material. The end face can be satisfactorily mirror-polished by using such a single crystal material.

【0010】本発明のうち請求項4記載の共振器は、端
面を鏡面研磨した圧電性基板と、この圧電性基板上に形
成された複数の電極指を有する正電極と、前記圧電性基
板上に形成された複数の電極指を有する負電極とを具
え、λを基本弾性表面波の伝播波長とした場合、一方の
端面とそれに最も近接する前記正電極又は負電極の電極
指との間の弾性表面波の伝播方向の距離を(m+1/
2)λ(m=0,1,2,...)とし、他方の端面と
それに最も近接する前記正電極又は負電極の電極指との
間の弾性表面波の伝播方向の距離を(n+1/2)λ
(n=0,1,2,...)としたことを特徴とするも
のである。
According to a fourth aspect of the present invention, there is provided a resonator according to the fourth aspect of the present invention, wherein the piezoelectric substrate has a mirror-polished end face, a positive electrode having a plurality of electrode fingers formed on the piezoelectric substrate, and And a negative electrode having a plurality of electrode fingers formed in the case where λ is the propagation wavelength of the basic surface acoustic wave, between one end face and the electrode finger of the positive electrode or the negative electrode closest to it. The distance in the propagation direction of the surface acoustic wave is (m + 1 /
2) λ (m = 0, 1, 2,...), And the distance in the propagation direction of the surface acoustic wave between the other end face and the electrode finger of the closest positive electrode or negative electrode is (n + 1). / 2) λ
(N = 0, 1, 2,...).

【0011】一方の端面とそれに最も近接する正電極又
は負電極の電極指との間の弾性表面波の伝播方向の距離
及び他方の端面とそれに最も近接する正電極又は負電極
の電極指との間の弾性表面波の伝播方向の距離をそのよ
うに設定することによって、端面反射波の位相がメイン
波の位相と同一になるので、メイン波は端面反射波の悪
影響が及ぼされず、むしろ弾性表面波の変換効率が更に
向上する。
The distance in the propagation direction of the surface acoustic wave between one end face and the electrode finger of the closest positive electrode or negative electrode, and the distance between the other end face and the electrode finger of the closest positive or negative electrode. By setting the distance in the propagation direction of the surface acoustic wave between them, the phase of the end-face reflected wave becomes the same as the phase of the main wave, so that the main wave is not adversely affected by the end-face reflected wave. Wave conversion efficiency is further improved.

【0012】本発明のうち請求項5記載の共振器は、前
記端面の表面粗さを0〜0.2μmとしたことを特徴と
するものである。このような表面粗さにすることによっ
て、端面反射波が入力側変換器及び出力側変換器に有効
に反射されるようになる。
The resonator according to claim 5 of the present invention is characterized in that the end face has a surface roughness of 0 to 0.2 μm. With such a surface roughness, the end face reflected wave is effectively reflected by the input-side converter and the output-side converter.

【0013】本発明のうち請求項6記載の共振器は、前
記圧電性基板を単結晶材料で構成したことを特徴とする
ものである。このような単結晶材料で構成することによ
って、端面を良好に鏡面研磨することができる。
According to a sixth aspect of the present invention, in the resonator, the piezoelectric substrate is made of a single crystal material. The end face can be satisfactorily mirror-polished by using such a single crystal material.

【0014】[0014]

【発明の実施の形態】本発明による弾性表面波フィルタ
装置及び共振器を、図面を参照して詳細に説明する。図
1は、本発明による弾性表面波フィルタ装置の実施の形
態を示す図である。単結晶材料である水晶基板1の表面
上に、入力側変換器2と、シールド電極3と、出力側変
換器4とを、弾性表面波の伝播方向に沿って順に形成す
る。
DESCRIPTION OF THE PREFERRED EMBODIMENTS A surface acoustic wave filter device and a resonator according to the present invention will be described in detail with reference to the drawings. FIG. 1 is a diagram showing an embodiment of a surface acoustic wave filter device according to the present invention. An input-side converter 2, a shield electrode 3, and an output-side converter 4 are sequentially formed on the surface of a quartz substrate 1 that is a single crystal material along the propagation direction of surface acoustic waves.

【0015】入力側変換器2を、正電極5及び負電極6
と、これら正電極5及び負電極6の電極指間に配置した
短絡型浮き電極7とを有する一方向性変換器とする。こ
れら正電極5、負電極6及び短絡型浮き電極7の弾性表
面波の伝播方向における電極指の幅をそれぞれλ/12
に設定する。ここで、λを基本弾性表面波の波長とす
る。正電極5及び負電極6の各電極指をそれぞれλのピ
ッチで形成し、正電極5の電極指とそれに隣接する負電
極6の電極指との中心間距離をλ/2に設定する。ま
た、短絡型浮き電極7の電極指を、それに隣接する正電
極5の電極指と負電極6の電極指の中間位置から弾性表
面波の伝播方向の上流側にλ/12だけ偏位するように
配置して、非対称構造に基づく一方向性を高める。本実
施の形態では、入力側変換器2の電極の対数を例えば4
0対に設定するが、この対数は、要求されるフィルタ特
性に応じて適宜最適条件に設定することができる。
The input-side converter 2 includes a positive electrode 5 and a negative electrode 6.
And a short-circuit type floating electrode 7 disposed between the electrode fingers of the positive electrode 5 and the negative electrode 6. The width of the electrode finger in the propagation direction of the surface acoustic wave of the positive electrode 5, the negative electrode 6, and the short-circuit type floating electrode 7 is set to λ / 12, respectively.
Set to. Here, λ is the wavelength of the basic surface acoustic wave. The electrode fingers of the positive electrode 5 and the negative electrode 6 are formed at a pitch of λ, and the center distance between the electrode finger of the positive electrode 5 and the electrode finger of the negative electrode 6 adjacent thereto is set to λ / 2. Further, the electrode finger of the short-circuit type floating electrode 7 is shifted by λ / 12 from the intermediate position between the electrode finger of the positive electrode 5 and the electrode finger of the negative electrode 6 adjacent thereto to the upstream side in the propagation direction of the surface acoustic wave. To enhance the unidirectionality based on the asymmetric structure. In the present embodiment, the number of electrodes of the input-side converter 2 is set to, for example, 4
Although the number of pairs is set to 0, the logarithm can be set to an optimum condition as appropriate according to the required filter characteristics.

【0016】出力側変換器4も、正電極8及び負電極9
と、これら正電極8及び負電極9の電極指間に配置した
短絡型浮き電極10とを有する一方向性変換器とする。
これら正電極8、負電極9及び短絡型浮き電極10の弾
性表面波の伝播方向における電極指の幅をそれぞれλ/
12に設定する。ここで、λを基本弾性表面波の波長と
する。正電極8及び負電極9の各電極指をそれぞれλの
ピッチで形成し、正電極8の電極指とそれに隣接する負
電極9の電極指との中心間距離をλ/2に設定する。ま
た、短絡型浮き電極10の電極指を、それに隣接する正
電極5の電極指と負電極6の電極指の中間位置から弾性
表面波の伝播方向の下流側にλ/12だけ偏位するよう
に配置して、非対称構造に基づく一方向性を高める。本
実施の形態では、入力側変換器2の電極の対数を例えば
40対に設定する。
The output converter 4 also includes a positive electrode 8 and a negative electrode 9.
And a short-circuit type floating electrode 10 disposed between the electrode fingers of the positive electrode 8 and the negative electrode 9.
The width of the electrode finger in the propagation direction of the surface acoustic wave of each of the positive electrode 8, the negative electrode 9, and the short-circuit type floating electrode 10 is λ /
Set to 12. Here, λ is the wavelength of the basic surface acoustic wave. Each electrode finger of the positive electrode 8 and the negative electrode 9 is formed at a pitch of λ, and the center distance between the electrode finger of the positive electrode 8 and the electrode finger of the adjacent negative electrode 9 is set to λ / 2. Further, the electrode finger of the short-circuit type floating electrode 10 is shifted from the intermediate position between the electrode finger of the positive electrode 5 and the electrode finger of the negative electrode 6 adjacent thereto by λ / 12 toward the downstream side in the propagation direction of the surface acoustic wave. To enhance the unidirectionality based on the asymmetric structure. In the present embodiment, the number of pairs of electrodes of the input-side converter 2 is set to, for example, 40 pairs.

【0017】本実施の形態では、水晶基板1の端面1
1,12がそれぞれ鏡面研磨され、入力側変換器2とそ
れに近接する水晶基板1の端面11との間の弾性表面波
の伝播方向の距離を(k+1/2)λ(k=0,1,
2,...)とし、出力側変換器4とそれに近接する水
晶基板1の端面12との間の弾性表面波の伝播方向の距
離を(l+1/2)(l=0,1,2,...)λとす
る。なお、端面11,12の表面粗さを0〜0.2μm
とする。
In the present embodiment, the end face 1 of the quartz substrate 1
1 and 12 are mirror-polished, and the distance in the propagation direction of the surface acoustic wave between the input-side transducer 2 and the end face 11 of the quartz substrate 1 adjacent thereto is set to (k + /) λ (k = 0, 1,
2,. . . ), And the distance in the propagation direction of the surface acoustic wave between the output-side converter 4 and the end face 12 of the quartz substrate 1 adjacent thereto is (l + /) (l = 0, 1, 2,...) Λ. And The surface roughness of the end faces 11 and 12 is 0 to 0.2 μm.
And

【0018】本実施の形態の動作を説明する。端面1
1,12によって反射された反射波は、入力側変換器2
と端面11との間の弾性表面波の伝播方向の距離及び出
力側変換器4と端面12との間の弾性表面波の伝播方向
の距離を基本弾性表面波の波長の整数倍にその半波長を
加えた距離設定されているので、その位相がメイン波の
位相と同一になり、メイン波は端面反射波の悪影響が及
ぼされず、むしろ弾性表面波の変換効率が更に向上す
る。
The operation of the embodiment will be described. End face 1
The reflected waves reflected by the input-side converter 2
The distance in the direction of propagation of the surface acoustic wave between the end surface 11 and the distance in the direction of propagation of the surface acoustic wave between the output-side converter 4 and the end surface 12 is set to an integral multiple of the wavelength of the basic surface acoustic wave. Is added, the phase becomes the same as the phase of the main wave, and the main wave is not adversely affected by the end-face reflected wave, but the conversion efficiency of the surface acoustic wave is further improved.

【0019】図2は、本発明による共振器の実施の形態
を示す図である。この共振器は、水晶基板21と、λを
基本弾性表面波の伝播波長とした場合に、λのピッチで
水晶基板21上に周期的に形成され、弾性表面波の伝播
方向の幅がλ/12の複数の電極指を有する正電極22
と、同様にλのピッチで水晶基板上に周期的に形成さ
れ、弾性表面波の伝播方向の幅がλ/12の複数の電極
指を有し、各電極指が正電極22の電極指とλ/2の中
心間距離を以てそれぞれ位置する負電極23とを具え
る。
FIG. 2 is a diagram showing an embodiment of the resonator according to the present invention. This resonator is periodically formed on the quartz substrate 21 at a pitch of λ, where λ is the propagation wavelength of the basic surface acoustic wave, and the width in the propagation direction of the surface acoustic wave is λ / Positive electrode 22 having twelve electrode fingers
Similarly, a plurality of electrode fingers are formed periodically on the quartz substrate at a pitch of λ, and the width of the surface acoustic wave in the propagation direction is λ / 12, and each electrode finger is in contact with the electrode finger of the positive electrode 22. and negative electrodes 23 respectively located with a center distance of λ / 2.

【0020】本実施の形態では、水晶基板21の端面2
4,25がそれぞれ鏡面研磨され、端面24とそれに最
も近接する正電極22の電極指26との間の弾性表面波
の伝播方向の距離を(m+1/2)λ(m=0,1,
2,...)とし、端面25とそれに最も近接する正電
極22の電極指27との間の弾性表面波の伝播方向の距
離を(l+1/2)(l=0,1,2,...)λとす
る。なお、端面24,25の表面粗さを0〜0.2μm
とする。
In this embodiment, the end face 2 of the quartz substrate 21
4 and 25 are mirror-polished, and the distance in the direction of propagation of the surface acoustic wave between the end face 24 and the electrode finger 26 of the positive electrode 22 closest to the end face 24 is (m +)) λ (m = 0, 1,
2,. . . ), And the distance in the propagation direction of the surface acoustic wave between the end face 25 and the electrode finger 27 of the positive electrode 22 closest to the end face 25 is (l + /) (l = 0, 1, 2,...) Λ. I do. In addition, the surface roughness of the end faces 24 and 25 is 0 to 0.2 μm.
And

【0021】本実施の形態の動作を説明する。端面2
4,25によって反射された反射波は、端面24と電極
指26との間の弾性表面波の伝播方向の距離及び端面2
5と電極指27との間の弾性表面波の伝播方向の距離を
基本弾性表面波の波長の整数倍にその半波長を加えた距
離設定されているので、その位相がメイン波の位相と同
一になり、メイン波は端面反射波の悪影響が及ぼされ
ず、むしろ弾性表面波の変換効率が更に向上する。
The operation of the embodiment will be described. End face 2
The reflected waves reflected by the end faces 2 and 25 are the distance in the propagation direction of the surface acoustic wave between the end face 24 and the electrode finger 26 and the end face 2
Since the distance in the propagation direction of the surface acoustic wave between 5 and the electrode finger 27 is set to a distance obtained by adding half the wavelength to an integral multiple of the wavelength of the basic surface acoustic wave, the phase is the same as the phase of the main wave. The main wave is not adversely affected by the end face reflected wave, but the conversion efficiency of the surface acoustic wave is further improved.

【0022】本発明は上記実施の形態に限定されるもの
ではなく、幾多の変更及び変形が可能である。例えば、
弾性表面波フィルタ装置の入力側変換器及び出力側変換
器を、従来既知の任意の変換器とすることができる。ま
た、他の構造の共振器に対しても本発明を適用すること
ができる。
The present invention is not limited to the above-described embodiment, and many modifications and variations are possible. For example,
The input side converter and the output side converter of the surface acoustic wave filter device can be any conventionally known converters. The present invention can be applied to a resonator having another structure.

【0023】さらに、圧電性基板として水晶基板を用い
たが、ほう酸リチウム(Li2 4 7 のような他の単
結晶材料で構成することもできる。
Furthermore, although a quartz substrate is used as the piezoelectric substrate, it may be made of another single crystal material such as lithium borate (Li 2 B 4 O 7 ).

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

【図1】本発明による弾性表面波フィルタ装置の実施の
形態を示す図である。
FIG. 1 is a diagram showing an embodiment of a surface acoustic wave filter device according to the present invention.

【図2】本発明による共振器の実施の形態を示す図であ
る。
FIG. 2 is a diagram showing an embodiment of a resonator according to the present invention.

【符号の説明】[Explanation of symbols]

1,21 水晶基板、2 入力側変換器、3 シールド
電極、4 出力側変換器、5,8,22 正電極、6,
9,23 負電極、7,10 短絡型浮き電極、11,
12,24,25 端面、26,27 電極指
1,21 crystal substrate, 2 input side converter, 3 shield electrode, 4 output side converter, 5,8,22 positive electrode, 6,6
9,23 Negative electrode, 7,10 Short-circuit type floating electrode, 11,
12, 24, 25 end face, 26, 27 electrode finger

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】端面を鏡面研磨した圧電性基板と、この圧
電性基板上に形成され、電気信号が外部から入力され、
この電気信号を弾性表面波に変換する入力側変換器と、
前記水晶基板の表面上に形成され、前記入力側変換器で
励振された弾性表面波を電気信号に変換し、この電気信
号を外部に出力する出力側変換器とを具え、 λを基本弾性表面波の伝播波長とした場合、前記入力側
変換器とそれに近接する前記圧電性基板の端面との間の
弾性表面波の伝播方向の距離を(k+1/2)λ(k=
0,1,2,...)とし、前記出力側変換器とそれに
近接する前記圧電性基板の端面との間の弾性表面波の伝
播方向の距離を(l+1/2)(l=0,1,
2,...)λとしたことを特徴とする弾性表面波フィ
ルタ装置。
1. A piezoelectric substrate having an end surface mirror-polished, and an electric signal formed on the piezoelectric substrate and externally inputted,
An input-side converter for converting the electric signal into a surface acoustic wave,
An output-side converter formed on the surface of the quartz substrate and converting a surface acoustic wave excited by the input-side converter into an electric signal, and outputting the electric signal to the outside; Assuming that the propagation wavelength of the wave is a wave, the distance in the propagation direction of the surface acoustic wave between the input-side converter and the end face of the piezoelectric substrate adjacent thereto is (k + /) λ (k =
0, 1, 2,. . . ), And the distance in the propagation direction of the surface acoustic wave between the output-side converter and the end face of the piezoelectric substrate adjacent thereto is (l + /) (l = 0, 1,
2,. . . A) a surface acoustic wave filter device characterized by λ.
【請求項2】前記端面の表面粗さを0〜0.2μmとし
たことを特徴とする請求項1記載の弾性表面波フィルタ
装置。
2. The surface acoustic wave filter device according to claim 1, wherein the surface roughness of said end face is 0 to 0.2 μm.
【請求項3】前記圧電性基板を単結晶材料で構成したこ
とを特徴とする請求項1又は2記載の弾性表面波フィル
タ装置。
3. The surface acoustic wave filter device according to claim 1, wherein the piezoelectric substrate is made of a single crystal material.
【請求項4】端面を鏡面研磨した圧電性基板と、この圧
電性基板上に形成された複数の電極指を有する正電極
と、前記圧電性基板上に形成された複数の電極指を有す
る負電極とを具え、 λを基本弾性表面波の伝播波長とした場合、一方の端面
とそれに最も近接する前記正電極又は負電極の電極指と
の間の弾性表面波の伝播方向の距離を(m+1/2)λ
(m=0,1,2,...)とし、他方の端面とそれに
最も近接する前記正電極又は負電極の電極指との間の弾
性表面波の伝播方向の距離を(n+1/2)λ(n=
0,1,2,...)としたことを特徴とする共振器。
4. A piezoelectric substrate having an end surface mirror-polished, a positive electrode having a plurality of electrode fingers formed on the piezoelectric substrate, and a negative electrode having a plurality of electrode fingers formed on the piezoelectric substrate. When λ is the propagation wavelength of the basic surface acoustic wave, the distance in the propagation direction of the surface acoustic wave between one end surface and the electrode finger of the closest positive electrode or negative electrode is (m + 1). / 2) λ
(M = 0, 1, 2,...), And the distance in the propagation direction of the surface acoustic wave between the other end face and the electrode finger of the closest positive electrode or negative electrode is (n ++ 1). λ (n =
0, 1, 2,. . . ).
【請求項5】前記端面の表面粗さを0〜0.2μmとし
たことを特徴とする請求項4記載の共振器。
5. The resonator according to claim 4, wherein said end face has a surface roughness of 0 to 0.2 μm.
【請求項6】前記圧電性基板を単結晶材料で構成したこ
とを特徴とする請求項4又は5記載の共振器。
6. The resonator according to claim 4, wherein said piezoelectric substrate is made of a single crystal material.
JP11090979A 1999-03-31 1999-03-31 Surface acoustic wave filter device and resonator Withdrawn JP2000286674A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11090979A JP2000286674A (en) 1999-03-31 1999-03-31 Surface acoustic wave filter device and resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11090979A JP2000286674A (en) 1999-03-31 1999-03-31 Surface acoustic wave filter device and resonator

Publications (1)

Publication Number Publication Date
JP2000286674A true JP2000286674A (en) 2000-10-13

Family

ID=14013648

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11090979A Withdrawn JP2000286674A (en) 1999-03-31 1999-03-31 Surface acoustic wave filter device and resonator

Country Status (1)

Country Link
JP (1) JP2000286674A (en)

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