Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0748626B2 - Frequency adjustment method for surface acoustic wave device - Google Patents
[go: Go Back, main page]

JPH0748626B2 - Frequency adjustment method for surface acoustic wave device - Google Patents

Frequency adjustment method for surface acoustic wave device

Info

Publication number
JPH0748626B2
JPH0748626B2 JP63187704A JP18770488A JPH0748626B2 JP H0748626 B2 JPH0748626 B2 JP H0748626B2 JP 63187704 A JP63187704 A JP 63187704A JP 18770488 A JP18770488 A JP 18770488A JP H0748626 B2 JPH0748626 B2 JP H0748626B2
Authority
JP
Japan
Prior art keywords
film
acoustic wave
surface acoustic
frequency
wave device
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 - Fee Related
Application number
JP63187704A
Other languages
Japanese (ja)
Other versions
JPH0236608A (en
Inventor
和志 橋本
嘉朗 藤原
清 佐藤
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP63187704A priority Critical patent/JPH0748626B2/en
Priority to US07/384,829 priority patent/US4978879A/en
Priority to DE68921811T priority patent/DE68921811T2/en
Priority to EP89307660A priority patent/EP0353073B1/en
Publication of JPH0236608A publication Critical patent/JPH0236608A/en
Publication of JPH0748626B2 publication Critical patent/JPH0748626B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

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

Description

【発明の詳細な説明】 〔概要〕 弾性表面波素子の発振周波数を調整するための方法に関
し、 特に高周波素子の周波数調整を容易かつ高精度化するこ
とを目的とし、 リチウムタンタレート単結晶のX軸廻りにZ軸方向へ36
度回転させたY板から切り出した基板の表面に、トラン
スジューサと、屈折率が1.46±0.01の二酸化シリコン膜
とを設けた弾性表面波素子において、 該二酸化シリコン膜の上に五酸化タンタル膜を積層せし
め、該基板の弾性表面波の周波数が所定値となる厚さに
該五酸化タンタル膜を積層することを特徴とする。
The present invention relates to a method for adjusting the oscillation frequency of a surface acoustic wave device, and particularly for the purpose of facilitating the frequency adjustment of a high-frequency device and improving the accuracy thereof. 36 around the axis in the Z-axis direction
In a surface acoustic wave device in which a transducer and a silicon dioxide film having a refractive index of 1.46 ± 0.01 are provided on the surface of a substrate cut out from a Y plate rotated by a degree, a tantalum pentoxide film is laminated on the silicon dioxide film. At the very least, the tantalum pentoxide film is laminated in such a thickness that the surface acoustic wave frequency of the substrate becomes a predetermined value.

〔産業上の利用分野〕[Industrial application field]

本発明は、VHF,UHF周波数帯域において信号処理等に使
用される弾性表面波素子、特にその周波数調整方法に関
する。
The present invention relates to a surface acoustic wave device used for signal processing and the like in the VHF and UHF frequency bands, and particularly to a frequency adjusting method thereof.

近年の情報処理機器,通信機器の高速化に伴って、これ
らの装置中で使用される周波数は、高周波へ移行してい
る。また、高周波における基準信号の発生,フィルタリ
ング等が必要となる。
With the recent increase in the speed of information processing equipment and communication equipment, the frequencies used in these devices are shifting to high frequencies. In addition, it is necessary to generate and filter a reference signal at a high frequency.

これらの用途に弾性表面波素子が使用されているが、周
波数の高精度化が要求されている前記機器において、該
素子の高精度化および安定化が望まれている。
The surface acoustic wave element is used for these purposes, and in the above-mentioned equipment that requires high frequency accuracy, high accuracy and stabilization of the element are desired.

弾性表面波素子を用いたフィルタの挿入損失や比帯域
幅,VCOとしての周波数可変幅の点で、大きな結合係数を
もつにも係わらず比較的温度係数の優れたリチウムタン
タレート(LiTaO3)の基板、特にリチウムタンタレート
単結晶のX軸廻りにZ軸方向へ36度回転させたY板(36
°Y−XLiTaO3板)から切り出した基板を利用した素子
は、極めて有用であり、トランスジューサが形成された
前記36°Y−XLiTaO3板上に二酸化シリコン(SiO2)を
積層し、温度特性を改善する試みがなされている。
The lithium tantalate (LiTaO 3 ) has a relatively high temperature coefficient despite its large coupling coefficient in terms of insertion loss, specific bandwidth, and frequency variable width as VCO using a surface acoustic wave element. Substrate, especially Y-plate (36) rotated in the Z-axis direction about the X-axis of the lithium tantalate single crystal by 36 degrees
A device using a substrate cut out from (Y-XLiTaO 3 plate) is extremely useful, and silicon dioxide (SiO 2 ) is laminated on the 36-Y-XLiTaO 3 plate on which the transducer is formed to obtain temperature characteristics. Attempts have been made to improve.

かかる弾性表面波素子は、電極の膜厚および電極幅なら
びにSiO2の膜厚変化等によって、周波数にばらつきを生
じるため、その周波数調整が必要となる。
In such a surface acoustic wave element, the frequency varies depending on the film thickness and the electrode width of the electrode, the change in the film thickness of SiO 2 , and the like, so that the frequency adjustment is required.

〔従来の技術〕[Conventional technology]

第4図は弾性表面波素子の概略構成を示す平面図(イ)
とその断面図(ロ)、第5図(イ),(ロ)は36°Y−
XLiTaO3板の説明図である。
FIG. 4 is a plan view showing the schematic structure of the surface acoustic wave device (a).
And its cross-sectional view (b) and Fig. 5 (a) and (b) are 36 ° Y-
XLiTaO 3 is an explanatory view of a plate.

第4図において、第5図に示すようなリチウムタンタレ
ート単結晶のX軸廻りにZ軸方向へ36度回転させたY板
(ウエーハ)1から、基板3を切り出した弾性表面波素
子2は、基板3の上面にトランジューサ、即ち駆動電極
4とその駆動電極4を挟む一対の反射電極5とを形成し
てなる。
In FIG. 4, a surface acoustic wave device 2 obtained by cutting a substrate 3 from a Y plate (wafer) 1 rotated about the X axis of a lithium tantalate single crystal by 36 degrees in the Z axis direction as shown in FIG. A transducer, that is, a drive electrode 4 and a pair of reflective electrodes 5 sandwiching the drive electrode 4 are formed on the upper surface of the substrate 3.

従来、かかる素子2の周波数調整方法は、電極4,5をエ
ッチングして薄くする、または電極4,5の一部をトリミ
ングする、あるいは基板3の電極間をエッチングする方
法であった。
Conventionally, such a frequency adjusting method for the element 2 has been a method in which the electrodes 4 and 5 are thinned by etching, a part of the electrodes 4 and 5 is trimmed, or between the electrodes of the substrate 3 is etched.

そして、弾性表面波素子2の温度特性を改善するため、
第4図(ロ)に一点鎖線で示すようにSiO2膜6を形成し
た弾性表面波素子、即ち屈折率が1.46±0.01のSiO2膜6
を形成した弾性表面波素子では、紫外線を照射してSiO2
膜6を変質させる周波数調整方法が報告されている。
Then, in order to improve the temperature characteristics of the surface acoustic wave element 2,
4 (b) to the surface acoustic wave device formed of the SiO 2 film 6 as indicated by the dashed line, i.e. SiO 2 with a refractive index of 1.46 ± 0.01 film 6
In the surface acoustic wave elements formed a is irradiated with ultraviolet rays SiO 2
A frequency adjustment method for modifying the membrane 6 has been reported.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

以上説明したように、電極または電極間の圧電体基板を
エッチングする従来の周波数調整方法は、トランジュー
サを構成する電極パターンが微細化されると困難とな
り、高性能の所定周波数に対して効率的かつ高精度に調
整できないという問題点があった。
As described above, the conventional frequency adjusting method for etching the electrodes or the piezoelectric substrate between the electrodes becomes difficult when the electrode pattern forming the transducer is miniaturized, and is efficient for a high-performance predetermined frequency. Moreover, there is a problem that the adjustment cannot be performed with high accuracy.

さらに、SiO2膜を被着した温度特性改善素子において、
SiO2膜に紫外線を照射する従来方法は、周波数の調整と
同時に温度特性も変化するという問題点があった。
Furthermore, in the temperature characteristic improving element with the SiO 2 film deposited,
The conventional method of irradiating the SiO 2 film with ultraviolet rays has a problem that the temperature characteristic changes simultaneously with the adjustment of the frequency.

〔課題を解決するための手段〕[Means for Solving the Problems]

表面波の周波数調整を容易かつ高精度にすることを目的
とした本発明方法は、その実施例を示す第1図によれ
ば、 リチウムタンタレート単結晶のX軸廻りにZ軸方向へ36
度回転させたY板から切り出した基板3の表面に、トラ
ンスジューサ(駆動電極4と反射電極5)と、屈折率が
1.46±0.01の二酸化シリコン膜6とを設けた弾性表面波
素子11において、 二酸化シリコン膜6の上に五酸化タンタル膜12を積層せ
しめ、基板3の弾性表面波の周波数が所定値となる厚さ
に五酸化タンタル膜12を積層することである。
According to FIG. 1 showing an embodiment, the method of the present invention aimed at facilitating the frequency adjustment of the surface wave is shown in FIG. 1 and shows that the lithium tantalate single crystal is rotated around the X axis in the Z axis direction.
On the surface of the substrate 3 cut out from the Y plate rotated once, the transducer (driving electrode 4 and reflecting electrode 5) and the refractive index
In a surface acoustic wave element 11 provided with a silicon dioxide film 6 of 1.46 ± 0.01, a tantalum pentoxide film 12 is laminated on the silicon dioxide film 6 so that the frequency of the surface acoustic wave of the substrate 3 becomes a predetermined value. Is to stack the tantalum pentoxide film 12.

〔作用〕[Action]

36°Y−XLiTaO3板を伝播する音速をv1,屈折率が1.46
±0.01の二酸化シリコン膜を伝播する音速をv2,電子ビ
ーム蒸着法によって被着し二酸化シリコンより比重の大
きい五酸化シリコン膜を伝播する音速をv3としたとき、
それらの音速間には v1>v2>v3 の関係が成立する。
The sound velocity propagating through the 36 ° Y-XLiTaO 3 plate is v 1 , and the refractive index is 1.46.
When the velocity of sound propagating in a silicon dioxide film of ± 0.01 is v 2 , and the velocity of sound propagating in a silicon pentoxide film having a specific gravity larger than that of silicon dioxide deposited by the electron beam evaporation method is v 3 ,
The relationship of v 1 > v 2 > v 3 is established between these sound velocities.

従って、36°Y−XLiTaO3板より切り出した基板の表面
にトランスジューサを形成し、その上に温度特性改善用
二酸化シリコン膜を形成したとき、該トランスジューサ
の駆動電極に適当な電流を印加して発生する弾性表面波
の速度は、二酸化シリコン膜を形成しないものより遅く
なり、さらに二酸化シリコン膜の上に五酸化シリコン膜
を形成した素子の弾性表面波の音速は、さらに遅くな
る。
Therefore, when a transducer is formed on the surface of a substrate cut out from a 36 ° Y-XLiTaO 3 plate and a silicon dioxide film for improving temperature characteristics is formed thereon, an appropriate current is applied to the drive electrode of the transducer to generate The velocity of the surface acoustic wave generated becomes slower than that of the case where the silicon dioxide film is not formed, and the acoustic velocity of the surface acoustic wave of the element in which the silicon pentoxide film is formed on the silicon dioxide film becomes further slower.

従って、温度特性を改善し、かつ、発振周波数が所望値
より高くなるように二酸化シリコン膜を形成したのち、
適当厚さの五酸化シリコン膜を二酸化シリコン膜に積層
形成した弾性表面波素子は、五酸化シリコン膜の厚さ選
択によって、温度特性を損なうことなく、発振周波数を
所望値に調整可能となる。
Therefore, after improving the temperature characteristics and forming the silicon dioxide film so that the oscillation frequency becomes higher than the desired value,
In the surface acoustic wave device in which a silicon pentoxide film having an appropriate thickness is laminated on a silicon dioxide film, the oscillation frequency can be adjusted to a desired value without damaging the temperature characteristics by selecting the thickness of the silicon pentoxide film.

〔実施例〕〔Example〕

以下に、図面を用いて本発明による弾性表面波素子の周
波数調整方法を説明する。
The frequency adjusting method of the surface acoustic wave device according to the present invention will be described below with reference to the drawings.

第1図は本発明の実施例による弾性表面波素子の模式断
面図、第2図は第1図の五酸化タンタル膜の厚さと発振
周波数の変化率との関係を示す図、第3図は第1図の五
酸化タンタル膜に替えて積層した酸化シリコン膜の厚さ
と発振周波数との関係を示す図である。
FIG. 1 is a schematic cross-sectional view of a surface acoustic wave device according to an embodiment of the present invention, FIG. 2 is a diagram showing the relationship between the thickness of the tantalum pentoxide film and the rate of change of oscillation frequency, and FIG. It is a figure which shows the relationship between the thickness of the silicon oxide film laminated | stacked instead of the tantalum pentoxide film of FIG. 1, and an oscillation frequency.

第1図において、弾性表面波素子11は、36°Y−XLiTaO
3板より切り出した基板3の上面の中央に駆動電極4を
形成し、駆動電極4の左方および右方位置に反射電極5
を形成し、その上に屈折率が1.46±0.01の二酸化シリコ
ン(SiO2)膜6をプラズマCVDにより積層形成したの
ち、周波数調整のため適当厚さの五酸化タンタル(Ta2O
5)膜12を、SiO2膜6の上に電子ビーム蒸着法により積
層してなる。ただし、素子11の温度特性改善のため被着
したSiO2膜6の厚さは、本実施例において3.75μmであ
る。
In FIG. 1, the surface acoustic wave element 11 is 36 ° Y-XLiTaO.
The drive electrode 4 is formed at the center of the upper surface of the substrate 3 cut out from the three plates, and the reflective electrode 5 is provided at the left and right positions of the drive electrode 4.
Is formed, and a silicon dioxide (SiO 2 ) film 6 having a refractive index of 1.46 ± 0.01 is laminated thereon by plasma CVD, and then tantalum pentoxide (Ta 2 O 5) having an appropriate thickness is formed for frequency adjustment.
5 ) The film 12 is laminated on the SiO 2 film 6 by the electron beam evaporation method. However, the thickness of the SiO 2 film 6 deposited for improving the temperature characteristics of the element 11 is 3.75 μm in this embodiment.

第2図において、縦軸は弾性表面波素子の発振周波数の
変化率、横軸は弾性表面波素子のSiO2膜に積層したTa2O
5膜の厚さ(Å)であり、厚さ50ÅのTa2O5膜12を被着し
発振周波数f0=175.75MHzまたは176.04MHzとした弾性表
面波素子11は、周波数変化率が−0.29%程度であるのに
対し、厚さ100ÅのTa2O5膜12を被着し発振周波数f0=17
5.98MHzまたは175.76MHzとした弾性表面波素子11は、周
波数変化率が−0.58%程度となる。
In FIG. 2, the vertical axis represents the rate of change in the oscillation frequency of the surface acoustic wave device, and the horizontal axis represents Ta 2 O laminated on the SiO 2 film of the surface acoustic wave device.
The surface acoustic wave device 11 having a thickness of 5 films (Å) and a Ta 2 O 5 film 12 having a thickness of 50 Å and an oscillation frequency f 0 = 175.75 MHz or 176.04 MHz has a frequency change rate of −0.29. %, While a 100 Å-thick Ta 2 O 5 film 12 was applied and the oscillation frequency f 0 = 17.
The surface acoustic wave device 11 having 5.98 MHz or 175.76 MHz has a frequency change rate of about −0.58%.

Ta2O5膜12をSiO2膜6に積層した弾性表面波素子11、例
えばTa2O5膜12を積層せしめることによって周波数を0.1
%だけ調整した素子11は、25℃における周波数を基準と
し、±25℃に冷却または加熱する、即ち0℃に冷却また
は50℃に加熱したときの周波数変化率が、±250ppm程度
である。
The Ta 2 O 5 film 12 of SiO 2 film 6 surface acoustic wave element 11 laminated on the frequency by allowed to laminating example the Ta 2 O 5 film 12 0.1
The element 11 adjusted by% has a frequency change rate of about ± 250 ppm when it is cooled or heated to ± 25 ° C., that is, when it is cooled to 0 ° C. or heated to 50 ° C. with reference to the frequency at 25 ° C.

第3図において、縦軸は弾性表面波素子の発振周波数
(MHz)、横軸は弾性表面波素子のSiO2膜に積層した酸
化シリコン膜(SiOx)の厚さ(Å)であり、厚さ3.75μ
mのSiO2膜6を形成し発振周波数が178.0MHzの弾性表面
波素子は、SiO2膜6の上に厚さ2000ÅのSiOx膜を形成し
たとき発振周波数は約1.36MHz(0.76%)だけ低下する
ようになる。
In FIG. 3, the vertical axis is the oscillation frequency (MHz) of the surface acoustic wave device, and the horizontal axis is the thickness (Å) of the silicon oxide film (SiO x ) laminated on the SiO 2 film of the surface acoustic wave device. 3.75μ
SiO 2 film 6 is formed oscillation frequency surface acoustic wave device 178.0MHz of m, the oscillation frequency when forming the SiO x film having a thickness of 2000Å on the SiO 2 film 6 is approximately 1.36MHz (0.76%) only Will start to decline.

そこで、SiOx膜を形成することによって発振周波数が17
8.0MHzであった弾性表面波素子の発振周波数を177MHzに
調整する、即ち発振周波数を0.56%だけ低下させるに
は、厚さ1500ÅのSiOx膜を積層すればよいことが分か
る。
Therefore, by forming a SiO x film, the oscillation frequency is increased to 17
It can be seen that a SiO x film having a thickness of 1500 Å can be laminated to adjust the oscillation frequency of the surface acoustic wave device which was 8.0 MHz to 177 MHz, that is, to reduce the oscillation frequency by 0.56%.

そこで、Ta2O5膜12を積層し周波数調整した弾性表面波
素子Aの温度特性と、Ta2O5膜12に変えてSiO2膜を積層
した弾性表面波素子Bの温度特性を比較する測定を行っ
た。
Therefore, the temperature characteristics of the surface acoustic wave element A in which the Ta 2 O 5 film 12 is laminated and the frequency is adjusted are compared with the temperature characteristics of the surface acoustic wave element B in which the SiO 2 film is laminated instead of the Ta 2 O 5 film 12. The measurement was performed.

Ta2O5膜12またはTa2O5膜12に変わるSiO2膜の積層による
周波数調整量は0.1%とした素子A,Bの周波数特性は、25
℃を測定の基準温度とし、基準温度に対し−25℃即ち0
℃と+25℃即ち50℃における周波数変化率とを実測し
た。
The frequency characteristics of the elements A and B were 25% when the frequency adjustment amount was 0.1% by stacking the Ta 2 O 5 film 12 or the SiO 2 film that was replaced with the Ta 2 O 5 film 12.
℃ is the standard temperature of the measurement, -25 ℃ to the standard temperature or 0
The frequency change rate at + 25 ° C. or + 25 ° C., that is, 50 ° C. was measured.

その実測結果によれば、50℃における素子AおよびBの
周波数変化率は共に30ppmであり、0℃における素子A
の周波数変化率が約50ppmであるのに対し、0℃におけ
る素子Bの周波数変化率は約120ppmとなり、素子Aは素
子Bより優れていることが実証された。
According to the measurement results, the frequency change rates of the elements A and B at 50 ° C. are both 30 ppm, and the element A at 0 ° C.
The frequency change rate of element B is about 50 ppm, whereas the frequency change rate of element B at 0 ° C. is about 120 ppm, demonstrating that element A is superior to element B.

なお、前記素子A,Bの周波数特性において温度の変化量
を大きくしたとき、+側の変化に対し素子A,Bの差異は
殆ど変わらないが、−側の変化に対し素子A,Bの差異に
よる優劣は拡大するようになる。
When the amount of change in temperature is increased in the frequency characteristics of the elements A and B, the difference between the elements A and B hardly changes with respect to the + side change, but the difference between the elements A and B with respect to the − side change. The superiority and inferiority due to will expand.

〔発明の効果〕〔The invention's effect〕

以上説明したように本発明方法によれば、トランスジュ
ーサ(電極)および基板に手を加えることなく、Ta2O5
膜を適当な厚さに積層させる、例えば発振周波数を測定
しながらその発振周波数が所定値となるようにTa2O5
を積層させるまたは、温度特性を良くするSiO2膜を形成
した時点で測定した発振周波数より設定した所定厚さに
Ta2O5膜を被着することによって、表面波の周波数調整
が可能となり、特に高周波素子の生産性が向上し、か
つ、周波数特性に優れた素子を提供できるようにした効
果がある。
As described above, according to the method of the present invention, Ta 2 O 5 can be used without touching the transducer (electrode) and the substrate.
When the film is laminated to have an appropriate thickness, for example, the Ta 2 O 5 film is laminated so that the oscillation frequency becomes a predetermined value while measuring the oscillation frequency, or when the SiO 2 film for improving the temperature characteristic is formed. From the measured oscillation frequency to the specified thickness set
By depositing the Ta 2 O 5 film, the frequency of the surface wave can be adjusted, and in particular, the productivity of the high frequency element can be improved and an element having excellent frequency characteristics can be provided.

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

第1図は本発明の実施例による弾性表面波素子の模式断
面図 第2図は第1図の五酸化タンタル膜の厚さと発振周波数
の変化率との関係を示す図 第3図は第1図の五酸化タンタル膜に替えて積層した酸
化シリコン膜の厚さと発振周波数との関係を示す図 第4図は弾性表面波素子の概略を示す図 第5図は36°Y−XLiTaO3板の説明図 である。 図中において、 1は36°Y−XLiTaO3板 3は素子基板 4,5は電極 6は二酸化シリコン膜 11は弾性表面波素子 12は五酸化タンタル膜 を示す。
FIG. 1 is a schematic cross-sectional view of a surface acoustic wave device according to an embodiment of the present invention. FIG. 2 is a diagram showing the relationship between the thickness of the tantalum pentoxide film in FIG. 1 and the rate of change of oscillation frequency. The figure which shows the relationship between the thickness and the oscillation frequency of the silicon oxide film laminated instead of the tantalum pentoxide film of the figure. The figure 4 shows the outline of the surface acoustic wave element. The figure 5 shows the 36 ° Y-XLiTaO 3 plate. It is an explanatory diagram. In the figure, 1 is a 36 ° Y-XLiTaO 3 plate 3, 3 is an element substrate, 4,5 is an electrode 6, silicon dioxide film 11 is a surface acoustic wave element 12 is a tantalum pentoxide film.

フロントページの続き (56)参考文献 特開 昭58−33310(JP,A) 特開 昭61−77407(JP,A) 特公 昭55−5924(JP,B2)Continuation of the front page (56) References JP-A-58-33310 (JP, A) JP-A-61-77407 (JP, A) JP-B-55-5924 (JP, B2)

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】リチウムタンタレート単結晶のX軸廻りに
Z軸方向へ36度回転させたY板から切り出した基板
(3)の表面に、トランスジューサ(4と5)と、屈折
率が1.46±0.01の二酸化シリコン膜(6)とを設けた弾
性表面波素子において、 該二酸化シリコン膜(6)の上に五酸化タンタル膜(1
2)を積層せしめ、該基板(3)の弾性表面波の周波数
が所定値となる厚さに該五酸化タンタル膜(12)を積層
すること、を特徴とする弾性表面波素子の周波数調整方
法。
1. A transducer (4 and 5) having a refractive index of 1.46 ± on a surface of a substrate (3) cut out from a Y plate rotated around the X axis of a lithium tantalate single crystal by 36 degrees in the Z axis direction. In a surface acoustic wave element provided with a silicon dioxide film (6) of 0.01, a tantalum pentoxide film (1) is formed on the silicon dioxide film (6).
2) is laminated, and the tantalum pentoxide film (12) is laminated to a thickness such that the frequency of the surface acoustic wave of the substrate (3) becomes a predetermined value, and a method for adjusting the frequency of a surface acoustic wave element. .
JP63187704A 1988-07-27 1988-07-27 Frequency adjustment method for surface acoustic wave device Expired - Fee Related JPH0748626B2 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP63187704A JPH0748626B2 (en) 1988-07-27 1988-07-27 Frequency adjustment method for surface acoustic wave device
US07/384,829 US4978879A (en) 1988-07-27 1989-07-25 Acoustic surface wave element
DE68921811T DE68921811T2 (en) 1988-07-27 1989-07-27 Surface acoustic wave arrangements.
EP89307660A EP0353073B1 (en) 1988-07-27 1989-07-27 Acoustic surface wave devices

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63187704A JPH0748626B2 (en) 1988-07-27 1988-07-27 Frequency adjustment method for surface acoustic wave device

Publications (2)

Publication Number Publication Date
JPH0236608A JPH0236608A (en) 1990-02-06
JPH0748626B2 true JPH0748626B2 (en) 1995-05-24

Family

ID=16210703

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63187704A Expired - Fee Related JPH0748626B2 (en) 1988-07-27 1988-07-27 Frequency adjustment method for surface acoustic wave device

Country Status (1)

Country Link
JP (1) JPH0748626B2 (en)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04258008A (en) * 1991-02-12 1992-09-14 Murata Mfg Co Ltd Surface acoustic wave device
DE10302633B4 (en) * 2003-01-23 2013-08-22 Epcos Ag SAW device with improved temperature response
WO2005083881A1 (en) 2004-03-02 2005-09-09 Murata Manufacturing Co., Ltd. Surface acoustic wave device
CN101741342A (en) 2004-03-29 2010-06-16 株式会社村田制作所 Boundary Acoustic Wave Device
TWI381060B (en) * 2008-08-12 2013-01-01 Univ Tatung High frequency surface acoustic wave elements and their substrates
JP5724262B2 (en) 2010-09-16 2015-05-27 株式会社村田製作所 Electronic components
CN115781946B (en) * 2022-11-29 2024-06-04 山东大学 Compression type high-temperature piezoelectric sensitive cutting type lithium niobate crystal, preparation and application

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS555924A (en) * 1978-06-27 1980-01-17 Ito Kogaku Kogyo Kk Composition for coating formed plastic material
JPS5833310A (en) * 1981-08-21 1983-02-26 Hitachi Ltd Surface acoustic wave device
JPS6177407A (en) * 1984-09-22 1986-04-21 Japan Radio Co Ltd Manufacture of layered structure surface acoustic wave element

Also Published As

Publication number Publication date
JPH0236608A (en) 1990-02-06

Similar Documents

Publication Publication Date Title
US4456850A (en) Piezoelectric composite thin film resonator
US5894647A (en) Method for fabricating piezoelectric resonators and product
JP4039322B2 (en) Piezoelectric filter, duplexer, composite piezoelectric resonator and communication device, and frequency adjustment method of piezoelectric filter
EP0034351B1 (en) Surface acoustic wave device
JP2783550B2 (en) Surface acoustic wave oscillator
JPH0748626B2 (en) Frequency adjustment method for surface acoustic wave device
JPS6357966B2 (en)
JPH02295211A (en) Energy shut-up type surface acoustic wave element
US7320164B2 (en) Method of manufacturing an electronic component
JP2000278078A (en) Piezoelectric resonator
JP2000165188A (en) Piezoelectric resonator
JP4196641B2 (en) Ultra-thin piezoelectric device and manufacturing method thereof
JPH0640611B2 (en) Piezoelectric thin film resonator
JPH02295212A (en) Surface acoustic wave resonator
JPH0131728B2 (en)
JP2000196404A (en) Piezoelectric resonator
JPH0316409A (en) Surface acoustic wave device and manufacture thereof
CN119232109B (en) Filter chip, filter chip fabrication method and filter device
EP0594117B1 (en) Piezoelectric filter and its production method
JPS63120508A (en) Manufacture of piezoelectric resonator
JPS5829211A (en) Thin film piezoelectric oscillator
JP3276826B2 (en) Surface acoustic wave device
JPS60116217A (en) Composite resonator
JPH0230207A (en) Crystal resonator and its manufacture
JPS6346605B2 (en)

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees