JPH06303090A - Piezoelectric filter - Google Patents
Piezoelectric filterInfo
- Publication number
- JPH06303090A JPH06303090A JP11379993A JP11379993A JPH06303090A JP H06303090 A JPH06303090 A JP H06303090A JP 11379993 A JP11379993 A JP 11379993A JP 11379993 A JP11379993 A JP 11379993A JP H06303090 A JPH06303090 A JP H06303090A
- Authority
- JP
- Japan
- Prior art keywords
- filter
- piezoelectric
- single crystal
- filter element
- 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.)
- Pending
Links
- 239000013078 crystal Substances 0.000 claims abstract description 22
- 239000000758 substrate Substances 0.000 claims abstract description 17
- 230000009977 dual effect Effects 0.000 claims description 10
- 239000000919 ceramic Substances 0.000 abstract description 10
- 230000008878 coupling Effects 0.000 abstract description 2
- 238000010168 coupling process Methods 0.000 abstract description 2
- 238000005859 coupling reaction Methods 0.000 abstract description 2
- 229910012463 LiTaO3 Inorganic materials 0.000 abstract 4
- 238000010586 diagram Methods 0.000 description 5
- 239000010453 quartz Substances 0.000 description 4
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 4
- 239000000463 material Substances 0.000 description 2
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 229910010293 ceramic material Inorganic materials 0.000 description 1
- 238000003776 cleavage reaction Methods 0.000 description 1
- 238000013016 damping Methods 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229920001296 polysiloxane Polymers 0.000 description 1
- 229910052573 porcelain Inorganic materials 0.000 description 1
- 230000007017 scission Effects 0.000 description 1
Landscapes
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は二重モード構造の圧電フ
ィルタに関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a piezoelectric filter having a dual mode structure.
【0002】[0002]
【従来の技術】近年、通信機などの市場では、広帯域で
かつ周波数の温度変化が小さいMHz帯のフィルタの要
求が高まっている。従来、MHz帯で使用されるフィル
タとして、スプリアス特性が良好で製造の容易な二重モ
ードフィルタが知られている。このフィルタの材料とし
ては、圧電セラミックスあるいは水晶を用いたものがあ
る。2. Description of the Related Art In recent years, in the market of communication devices and the like, there is an increasing demand for a filter in the MHz band which has a wide band and a small frequency change with temperature. Conventionally, as a filter used in the MHz band, a dual mode filter having a good spurious characteristic and easy to manufacture is known. As a material of this filter, there is one using piezoelectric ceramics or crystal.
【0003】[0003]
【発明が解決しようとする課題】しかしながら、圧電セ
ラミックスを用いた二重モードフィルタでは、実用温度
範囲(−20℃〜80℃)における周波数の温度変化が
大きいため、高精度のフィルタを得にくい欠点がある。
一方、水晶を用いた二重モードフィルタでは、周波数の
温度変化を非常に小さく抑えることができるが、その反
面、帯域幅が狭過ぎ、市場の要求に応えきれない。そこ
で、本発明の目的は、広帯域でかつ周波数の温度変化が
小さい高精度の二重モードフィルタを提供することにあ
る。However, in the dual mode filter using the piezoelectric ceramics, the temperature change of the frequency in the practical temperature range (-20 ° C to 80 ° C) is large, and it is difficult to obtain a highly accurate filter. There is.
On the other hand, a dual-mode filter using a crystal can suppress the temperature change in frequency very small, but on the other hand, its bandwidth is too narrow to meet the market demand. Therefore, an object of the present invention is to provide a high-precision dual-mode filter that has a wide band and a small frequency temperature change.
【0004】[0004]
【課題を解決するための手段】上記目的を達成するた
め、本発明の圧電フィルタは、LiTaO3 単結晶より
なる厚みすべり振動モードの圧電基板を用い、この圧電
基板に二重モード構造の振動電極を設けたものである。In order to achieve the above object, the piezoelectric filter of the present invention uses a thickness shear vibration mode piezoelectric substrate made of a LiTaO 3 single crystal, and the piezoelectric substrate has a dual mode structure vibration electrode. Is provided.
【0005】[0005]
【作用】圧電単結晶であるLiTaO3 単結晶は圧電セ
ラミックスに比べて周波数の温度変化が小さく、水晶に
比べて電気機械結合係数が大きい。そのため、LiTa
O3 単結晶を用いた圧電フィルタは、圧電セラミックス
を用いたフィルタに比べて温度特性に優れ、水晶を用い
たフィルタに比べて広帯域となるという利点がある。ま
た、LiTaO3 単結晶は不要振動が励振されやすく、
スプリアスが大きくなりやすい。そこで、振動モードと
して、他の振動モードに比べてスプリアスが小さい厚み
すべり振動モードを用いている。The single crystal of LiTaO 3 which is a piezoelectric single crystal has a smaller frequency change in frequency than the piezoelectric ceramic and has a larger electromechanical coupling coefficient than that of quartz. Therefore, LiTa
The piezoelectric filter using the O 3 single crystal has an advantage that it has better temperature characteristics than a filter using piezoelectric ceramics and has a wider band than a filter using quartz. Moreover, in LiTaO 3 single crystal, unnecessary vibration is easily excited,
Spurious tends to grow. Therefore, as the vibration mode, the thickness-shear vibration mode having smaller spurious than other vibration modes is used.
【0006】LiTaO3 単結晶のX板は、Y軸から−
57°にへき開面があるため、カット時の加工性が良
い。また、温度係数も良好であり、ロールオフ特性や群
遅延特性などの特性も良好であるため、X板のY軸から
−57°±0.5°の角度で切り出したものが望まし
い。The LiTaO 3 single crystal X plate has a −
Since it has a cleavage plane at 57 °, it has good workability during cutting. Further, since the temperature coefficient is good and the characteristics such as roll-off characteristics and group delay characteristics are also good, it is desirable to cut out the X plate at an angle of −57 ° ± 0.5 ° from the Y axis.
【0007】[0007]
【実施例】図1は本発明にかかる圧電フィルタの一例を
示す。この圧電フィルタは、フィルタ素子1と、フィル
タ素子1を収容したケース10と、ケース20の開口部
を閉鎖するカバー30とで構成されている。FIG. 1 shows an example of a piezoelectric filter according to the present invention. This piezoelectric filter includes a filter element 1, a case 10 that houses the filter element 1, and a cover 30 that closes an opening of the case 20.
【0008】フィルタ素子1は、図2に示されるよう
に、1枚の圧電基板2に厚みすべり振動の二重モード共
振子を2個形成したものであり、圧電基板2としては図
3のようにLiTaO3 単結晶のX板をY軸から−57
°±0.5°の角度で切り出したものを用いている。圧
電基板2の表面の両端部には入力用(または出力用)の
端子電極3と出力用(または入力用)の端子電極4とが
形成され、表面の中央部寄りの位置には端子電極3,4
と導通する振動電極5,6が夫々形成されている。ま
た、振動電極5,6の近傍には、夫々対をなす振動電極
7,8が隣接して形成され、これら振動電極7,8は互
いに導通している。圧電基板2の裏面には、振動電極
5,7と対向する幅広な振動電極9と、振動電極6,8
と対向する幅広な振動電極10とが形成され、これら振
動電極9,10はアース用の端子電極11を介して導通
している。As shown in FIG. 2, the filter element 1 is formed by forming two thickness-shear vibration dual mode resonators on one piezoelectric substrate 2. As shown in FIG. The LiTaO 3 single crystal X plate was placed at -57 from the Y axis.
The one cut out at an angle of ± 0.5 ° is used. An input (or output) terminal electrode 3 and an output (or input) terminal electrode 4 are formed at both ends of the surface of the piezoelectric substrate 2, and the terminal electrode 3 is provided at a position near the center of the surface. , 4
Vibrating electrodes 5 and 6 are formed so as to be electrically connected to each other. Further, in the vicinity of the vibrating electrodes 5, 6, paired vibrating electrodes 7, 8 are formed adjacent to each other, and these vibrating electrodes 7, 8 are electrically connected to each other. On the back surface of the piezoelectric substrate 2, a wide vibrating electrode 9 facing the vibrating electrodes 5, 7 and vibrating electrodes 6, 8 are provided.
A wide vibrating electrode 10 is formed so as to face with the vibrating electrodes 9 and 10 and are electrically connected to each other through a grounding terminal electrode 11.
【0009】ケース20はアルミナ磁器のようなセラミ
ックス材料よりなり、その上面にはフィルタ素子1を収
容する凹所21が形成されている。ケース20の両端部
および中央部の外周面および凹所21の内面には、引出
電極22,23,24が幅方向に形成されている。フィ
ルタ素子1はケース20の凹所21に収容されるととも
に、導電性接着剤(図示せず)で固定される。この時、
フィルタ素子1の入力用(または出力用)端子電極3、
出力用(または入力用)の端子電極4、アース用の端子
電極11は、夫々ケース20の引出電極22,23,2
4と接続される。図4は上記圧電フィルタの等価回路で
ある。なお、フィルタ素子1の少なくとも振動部には、
スプリアスを低減し、トップ波形およびG.D.T.特
性を改善するため、シリコーンゲルなどのダンピング材
(図示せず)が塗布されている。The case 20 is made of a ceramic material such as alumina porcelain, and a recess 21 for accommodating the filter element 1 is formed on the upper surface thereof. Lead electrodes 22, 23, 24 are formed in the width direction on the outer peripheral surfaces of both ends and the central portion of the case 20 and on the inner surface of the recess 21. The filter element 1 is housed in the recess 21 of the case 20 and fixed by a conductive adhesive (not shown). At this time,
Input (or output) terminal electrode 3 of the filter element 1,
The output (or input) terminal electrode 4 and the grounding terminal electrode 11 are respectively the extraction electrodes 22, 23, 2 of the case 20.
4 is connected. FIG. 4 is an equivalent circuit of the piezoelectric filter. In addition, at least the vibrating portion of the filter element 1,
Reduces spurious, top waveform and G.I. D. T. A damping material (not shown) such as silicone gel is applied to improve the characteristics.
【0010】次表は、圧電セラミックス(PZT)、水
晶およびLiTaO3 単結晶のX板(Y−57°)を用
いた二重モードフィルタの、3dB帯域幅と周波数偏差
(−20℃〜60℃)とを示したものである。The following table shows a 3 dB bandwidth and a frequency deviation (-20 ° C to 60 ° C) of a dual mode filter using a piezoelectric ceramics (PZT), quartz and a LiTaO 3 single crystal X plate (Y-57 °). ) And is shown.
【表1】 上表から明らかなように、LiTaO3 のX板は3dB
帯域幅では最も広帯域であり、周波数の温度変化では水
晶にはやや劣るものの、圧電セラミックスに比べて4倍
高精度である。[Table 1] As is clear from the above table, the LiTaO 3 X plate has 3 dB.
It has the widest bandwidth and is slightly inferior to quartz in the temperature change of frequency, but is four times more accurate than piezoelectric ceramics.
【0011】図5は図1に示される二重モードフィルタ
のフィルタ特性、図6はそのトップ波形とG.D.T特
性を示す。図から明らかなように、スプリアスが非常に
少なく、トップ波形が丸く、良好なロールオフ特性が得
られるとともに、G.D.T.特性の偏差も小さい良好
なフィルタ特性が得られることが分かる。FIG. 5 shows the filter characteristics of the dual mode filter shown in FIG. 1, and FIG. 6 shows its top waveform and G.I. D. The T characteristic is shown. As is clear from the figure, the spurious response is extremely small, the top waveform is round, and good roll-off characteristics are obtained. D. T. It can be seen that a good filter characteristic with a small characteristic deviation can be obtained.
【0012】上記実施例では、圧電基板としてLiTa
O3 単結晶のX板のY軸から−57°±0.5°の角度
で切り出したものを用いたが、これに限るものではな
く、例えばY軸から−50°や−58°の角度で切り出
したものなど、他のカット角のものを用いても同様なフ
ィルタ特性を得ることが可能である。また、本発明の二
重モードフィルタの電極形状は、図2に示されるものに
限らず、図7あるいは図8のような形状としてもよい。
さらに、本発明は上記のような2素子形の二重モードフ
ィルタに限らず、1素子形あるいは3素子以上の二重モ
ードフィルタであってもよい。In the above embodiment, LiTa is used as the piezoelectric substrate.
An X plate of an O 3 single crystal cut out at an angle of −57 ° ± 0.5 ° from the Y axis was used, but the present invention is not limited to this, and for example, an angle of −50 ° or −58 ° from the Y axis. Similar filter characteristics can be obtained by using other cut angles such as those cut out in. Further, the electrode shape of the dual mode filter of the present invention is not limited to that shown in FIG. 2, and may be a shape as shown in FIG. 7 or 8.
Furthermore, the present invention is not limited to the two-element type dual-mode filter as described above, and may be a one-element type or three-element or more dual-mode filter.
【0013】[0013]
【発明の効果】以上の説明で明らかなように、本発明の
圧電フィルタは、圧電基板としてLiTaO3 単結晶よ
りなる厚みすべり振動モード基板を用いて二重モード構
造としたので、圧電セラミックスや水晶を用いたフィル
タに比べて帯域幅が広く、しかも周波数の温度変化が圧
電セラミックスより小さく、高精度のフィルタを得るこ
とができる。As is apparent from the above description, since the piezoelectric filter of the present invention has the dual mode structure by using the thickness shear vibration mode substrate made of LiTaO 3 single crystal as the piezoelectric substrate, the piezoelectric ceramic or the crystal is used. A band width is wider than that of the filter using, and the temperature change of frequency is smaller than that of the piezoelectric ceramics, and a highly accurate filter can be obtained.
【図1】本発明にかかる圧電フィルタの一例の斜視図で
ある。FIG. 1 is a perspective view of an example of a piezoelectric filter according to the present invention.
【図2】フィルタ素子の正面図および背面図である。FIG. 2 is a front view and a rear view of a filter element.
【図3】圧電基板のカット角を示す図である。FIG. 3 is a diagram showing a cut angle of a piezoelectric substrate.
【図4】圧電フィルタの等価回路図である。FIG. 4 is an equivalent circuit diagram of a piezoelectric filter.
【図5】圧電フィルタのフィルタ特性図である。FIG. 5 is a filter characteristic diagram of a piezoelectric filter.
【図6】圧電フィルタのトップ波形図とG.D.T特性
図である。6 is a top waveform diagram of a piezoelectric filter and G.I. D. It is a T characteristic diagram.
【図7】フィルタ素子の他の例の正面図および背面図で
ある。FIG. 7 is a front view and a rear view of another example of the filter element.
【図8】フィルタ素子のさらに他の例の正面図および背
面図である。FIG. 8 is a front view and a rear view of still another example of the filter element.
1 フィルタ素子 2 圧電基板 1 Filter element 2 Piezoelectric substrate
Claims (2)
動モードの圧電基板を用い、この圧電基板に二重モード
構造の振動電極を設けたことを特徴とする圧電フィル
タ。1. A piezoelectric filter comprising a piezoelectric substrate of a thickness shear vibration mode made of a LiTaO 3 single crystal, and a vibration electrode having a dual mode structure provided on the piezoelectric substrate.
57°±0.5°の角度で切り出されたものであること
を特徴とする圧電フィルタ。2. The piezoelectric filter according to claim 1, wherein the piezoelectric substrate is from the Y axis of an X plate of LiTaO 3 single crystal.
A piezoelectric filter characterized by being cut out at an angle of 57 ° ± 0.5 °.
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11379993A JPH06303090A (en) | 1993-04-15 | 1993-04-15 | Piezoelectric filter |
DE69415202T DE69415202T2 (en) | 1993-04-15 | 1994-04-13 | Piezoelectric filter |
EP94105729A EP0620640B1 (en) | 1993-04-15 | 1994-04-13 | Piezoelectric filter |
US08/227,631 US5608362A (en) | 1993-04-15 | 1994-04-14 | Piezoelectric filter using LiTaO3 substrate |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11379993A JPH06303090A (en) | 1993-04-15 | 1993-04-15 | Piezoelectric filter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH06303090A true JPH06303090A (en) | 1994-10-28 |
Family
ID=14621376
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11379993A Pending JPH06303090A (en) | 1993-04-15 | 1993-04-15 | Piezoelectric filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH06303090A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2002067424A1 (en) * | 2001-02-19 | 2002-08-29 | Matsushita Electric Industrial Co., Ltd. | Piezoelectric vibrator, ladder-type filter using this piezoelectric vibrator and double-mode piezoelectric filter |
US6621194B1 (en) | 1999-11-15 | 2003-09-16 | Matsushita Electric Industrial Co., Ltd. | Piezoelectric element having thickness shear vibration and mobile communication device using the same |
-
1993
- 1993-04-15 JP JP11379993A patent/JPH06303090A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6621194B1 (en) | 1999-11-15 | 2003-09-16 | Matsushita Electric Industrial Co., Ltd. | Piezoelectric element having thickness shear vibration and mobile communication device using the same |
WO2002067424A1 (en) * | 2001-02-19 | 2002-08-29 | Matsushita Electric Industrial Co., Ltd. | Piezoelectric vibrator, ladder-type filter using this piezoelectric vibrator and double-mode piezoelectric filter |
US6992424B2 (en) | 2001-02-19 | 2006-01-31 | Matsushita Electric Industrial Co., Ltd. | Piezoelectric vibrator ladder-type filter using piezoeletric vibrator and double-mode piezolectric filter |
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