JPH11136082A - Piezoelectric element - Google Patents
Piezoelectric elementInfo
- Publication number
- JPH11136082A JPH11136082A JP29511997A JP29511997A JPH11136082A JP H11136082 A JPH11136082 A JP H11136082A JP 29511997 A JP29511997 A JP 29511997A JP 29511997 A JP29511997 A JP 29511997A JP H11136082 A JPH11136082 A JP H11136082A
- Authority
- JP
- Japan
- Prior art keywords
- coupling coefficient
- electromechanical coupling
- piezoelectric element
- piezoelectric
- elastic wave
- 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
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は移動体通信などに広
く用いられている圧電体素子の構造と製造方法に関する
ものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a structure and a manufacturing method of a piezoelectric element widely used in mobile communication and the like.
【0002】[0002]
【従来の技術】PHS(Personal Handy Phone System)を
初めとする、移動体通信システムでは、数多くのセラミ
ックス電子部品、半導体、などが使われている。中で
も、フィルターには圧電体セラミックスが主に使われて
いる。BACKGROUND OF THE INVENTION beginning with PHS (P ersonal H andy Phone S ystem), in a mobile communication system, a number of ceramic electronic components, semiconductors, and the like are used. Among them, piezoelectric ceramics are mainly used for filters.
【0003】[0003]
【発明が解決しようとする課題】前記圧電材料にはそれ
ぞれ固有の特性がある。電気エネルギーから圧電エネル
ギーへの変換効率を表す電気機械結合係数k2は、LiN
bO3は5〜20%と大きく、LiTaO3は0.5〜8%である。一
般にk2が大きいほど、電気信号による弾性波は誘起さ
れやすくなる。一方、弾性波の伝搬減衰率は、LiTaO
3でほぼゼロであるのに対し、LiNbO3では0.04dB/λ
と、水晶の100倍程度と大きい。伝搬減衰率は圧電体素
子の挿入損失の増大に直接効いてくるもので、小さいほ
ど有利であることは言うまでもない。従って、LiNb
O3、LiTaO3のセラミックス、LiNb1-xTaxO
3の混相系セラミックスでは、充分な圧電素子の変換効
率を満たすことができず、いまだ十分に圧電セラミック
スの利点を活かした素子構造の提供はなされていなかっ
た。The above-mentioned piezoelectric materials have their own characteristics. Electromechanical coupling coefficient k 2 representing the conversion efficiency from electrical energy to the piezoelectric energy, LiN
bO 3 is as large as 5 to 20%, and LiTaO 3 is 0.5 to 8%. In general, as k 2 is larger, an elastic wave due to an electric signal is more likely to be induced. On the other hand, the propagation attenuation rate of the elastic wave is LiTaO
3 is almost zero, whereas 0.04 dB / λ for LiNbO 3
And it is about 100 times larger than crystal. The propagation attenuation rate directly affects the insertion loss of the piezoelectric element, and it goes without saying that the smaller the propagation attenuation rate, the more advantageous. Therefore, LiNb
O 3, LiTaO 3 of ceramics, LiNb 1-x Ta x O
The three- phase ceramics cannot satisfy a sufficient conversion efficiency of the piezoelectric element, and an element structure utilizing the advantages of the piezoelectric ceramic has not yet been provided.
【0004】[0004]
【課題を解決するための手段】本発明の圧電体素子は、
少なくともLiTaO3結晶を含む圧電性セラミックス
A上にLiTaO3より電気機械結合係数の大きい圧電
性セラミックスBが形成され、さらにその上に弾性波送
信用及び受信用電極が形成された構成を有する。According to the present invention, there is provided a piezoelectric element comprising:
A piezoelectric ceramic B having a larger electromechanical coupling coefficient than LiTaO 3 is formed on a piezoelectric ceramic A containing at least a LiTaO 3 crystal, and an electrode for transmitting and receiving an elastic wave is further formed thereon.
【0005】また、前記構成においては、圧電性セラミ
ックスBが、少なくともLiNbO3、Li2B4O7、Zn
O、AlN、Ta2O5、Pb-Nd-Ti-Mn-In-O、Pb-
Zn-Ti-O、KNbO3から選ばれる一つの材料であるこ
とが望ましい。In the above structure, the piezoelectric ceramic B is made of at least LiNbO 3 , Li 2 B 4 O 7 , Zn
O, AlN, Ta 2 O5, Pb-Nd-Ti-Mn-In-O, Pb-
Zn-Ti-O, it is desirable that one material selected from the KNbO 3.
【0006】また、前記構成においては、圧電性セラミ
ックスBが、薄膜であることが望ましい。In the above structure, the piezoelectric ceramic B is preferably a thin film.
【0007】また、前記構成においては、圧電性セラミ
ックスBの厚みが、1λ(ただし、λは弾性波の波長を
示す)より薄いことが望ましい。In the above structure, it is desirable that the thickness of the piezoelectric ceramic B is smaller than 1λ (where λ indicates the wavelength of the elastic wave).
【0008】[0008]
【発明の実施の形態】前記のように、圧電性材料におい
て、電気機械結合係数k2と、弾性波の伝搬減衰率は、
相反する関係にある。そこで、本発明者らは、弾性波の
励振・受信部分には電気機械結合係数k2の大きい材料
を用い、弾性波の伝搬部分には、電気機械結合係数k2
の小さい、すなわち伝搬減衰率の小さい材料を用いれ
ば、単一材料の圧電体素子に比べて、挿入損失も少ない
のではと考え、実験的に検証を進めた。DESCRIPTION OF THE PREFERRED EMBODIMENTS As described above, in a piezoelectric material, the electromechanical coupling coefficient k 2 and the propagation attenuation rate of an elastic wave are:
There are conflicting relationships. The present inventors, using a material having a large electromechanical coupling coefficient k 2 is the excitation and reception portion of the elastic wave, the propagation part of the acoustic wave, the electromechanical coupling coefficient k 2
Therefore, it was considered that the insertion loss was small when a material having a small propagation loss, that is, a material having a small propagation attenuation rate was used as compared with a piezoelectric element made of a single material.
【0009】そこで、図1に示すようなLiTaO3単
結晶基板1上に、LiNbO3薄膜2を1μm堆積し
て、薄膜2の上に。弾性波送信用櫛型電極3と弾性波受
信用櫛型電極4をアルミニウムで形成してSAW素子を
作製し、挿入損失を測定して、薄膜2のない場合と比較
した。比較結果を表1に示す。動作中心周波数は、30
0MHzとした。Therefore, a LiNbO 3 thin film 2 is deposited to a thickness of 1 μm on a LiTaO 3 single crystal substrate 1 as shown in FIG. The SAW element was manufactured by forming the elastic wave transmitting comb electrode 3 and the elastic wave receiving comb electrode 4 from aluminum, and the insertion loss was measured and compared with the case without the thin film 2. Table 1 shows the comparison results. The operating center frequency is 30
0 MHz.
【0010】[0010]
【表1】 [Table 1]
【0011】この結果、挿入損失は、LiTaO3基板
1の低いままでほとんど変わらず、電気機械結合係数k
2は、LiNbO3膜2を基板1の上に堆積することで、
2倍以上に増えることがわかった。As a result, the insertion loss hardly changes while the LiTaO 3 substrate 1 remains low, and the electromechanical coupling coefficient k
2 is to deposit a LiNbO 3 film 2 on the substrate 1,
It was found to increase more than twice.
【0012】[0012]
【発明の効果】以上のように本発明によれば、LiNb
O3、LiTaO3のセラミックス、LiNb1-xTaxO
3の混相系セラミックスにおいても、充分な圧電素子の
変換効率を満たすことができ、圧電セラミックスの利点
を十分に活かした素子構造を提供することが出来る。As described above, according to the present invention, LiNb
O 3, LiTaO 3 of ceramics, LiNb 1-x Ta x O
Even with the mixed-phase ceramics of 3 , the sufficient conversion efficiency of the piezoelectric element can be satisfied, and an element structure fully utilizing the advantages of the piezoelectric ceramic can be provided.
【図1】SAW素子の断面構造概略図FIG. 1 is a schematic sectional view of a SAW element.
1 LiTaO3基板 2 LiNbO3膜 3 送信用櫛型電極 4 受信用櫛型電極Reference Signs List 1 LiTaO 3 substrate 2 LiNbO 3 film 3 Comb electrode for transmission 4 Comb electrode for reception
Claims (4)
性セラミックスA上にLiTaO3より電気機械結合係
数の大きい圧電性セラミックスBが形成され、さらにそ
の上に弾性波送信用あるいは受信用電極が形成された圧
電体素子。1. A piezoelectric ceramic B having a larger electromechanical coupling coefficient than LiTaO 3 is formed on a piezoelectric ceramic A containing at least a LiTaO 3 crystal, and an electrode for transmitting or receiving an elastic wave is formed thereon. Piezoelectric element.
iNbO3、Li2B4O7、ZnO、AlN、Ta2O5、Pb-
Nd-Ti-Mn-In-O、Pb-Zn-Ti-O、KNbO3から選
ばれる1つあるいは複数から構成されることを特徴とす
る請求項1に記載の圧電体素子。2. The piezoelectric ceramic B has at least L
iNbO 3, Li 2 B 4 O 7, ZnO, AlN, Ta 2 O5, Pb-
Nd-Ti-Mn-In- O, Pb-Zn-Ti-O, the piezoelectric element according to claim 1, characterized in that they are composed of one or more selected from the KNbO 3.
求項1に記載の圧電体素子。3. The piezoelectric element according to claim 1, wherein the piezoelectric ceramic B is a thin film.
(ただし、λは弾性波の波長を示す)より薄い請求項1
に記載の圧電体素子。4. The piezoelectric ceramic B has a thickness of 1λ.
(1) where λ represents the wavelength of an elastic wave.
3. The piezoelectric element according to item 1.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29511997A JPH11136082A (en) | 1997-10-28 | 1997-10-28 | Piezoelectric element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29511997A JPH11136082A (en) | 1997-10-28 | 1997-10-28 | Piezoelectric element |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH11136082A true JPH11136082A (en) | 1999-05-21 |
Family
ID=17816542
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP29511997A Pending JPH11136082A (en) | 1997-10-28 | 1997-10-28 | Piezoelectric element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH11136082A (en) |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2002095941A1 (en) * | 2001-05-21 | 2002-11-28 | Microtechnology Centre Management Limited | Surface acoustic wave device |
WO2002095940A1 (en) * | 2001-05-21 | 2002-11-28 | Microtechnology Centre Management Limited | Surface acoustic wave sensor |
WO2005050836A1 (en) * | 2003-11-19 | 2005-06-02 | Murata Manufacturing Co., Ltd. | End surface reflection surface acoustic wave device and its manufacturing method |
AU2002308401B2 (en) * | 2001-05-21 | 2005-08-04 | Mnt Innovations Pty Ltd | Surface acoustic wave sensor |
WO2022230723A1 (en) * | 2021-04-30 | 2022-11-03 | 株式会社村田製作所 | Elastic wave device |
-
1997
- 1997-10-28 JP JP29511997A patent/JPH11136082A/en active Pending
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2002095941A1 (en) * | 2001-05-21 | 2002-11-28 | Microtechnology Centre Management Limited | Surface acoustic wave device |
WO2002095940A1 (en) * | 2001-05-21 | 2002-11-28 | Microtechnology Centre Management Limited | Surface acoustic wave sensor |
AU2002308401B2 (en) * | 2001-05-21 | 2005-08-04 | Mnt Innovations Pty Ltd | Surface acoustic wave sensor |
US7027921B2 (en) | 2001-05-21 | 2006-04-11 | Microtechnology Centre Management Limited | Surface acoustic wave sensor |
WO2005050836A1 (en) * | 2003-11-19 | 2005-06-02 | Murata Manufacturing Co., Ltd. | End surface reflection surface acoustic wave device and its manufacturing method |
JPWO2005050836A1 (en) * | 2003-11-19 | 2007-06-14 | 株式会社村田製作所 | End surface reflection type surface acoustic wave device and method of manufacturing the same |
WO2022230723A1 (en) * | 2021-04-30 | 2022-11-03 | 株式会社村田製作所 | Elastic wave device |
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