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
JP7624796B2 - Ladder Filters and Multiplexers - Google Patents
[go: Go Back, main page]

JP7624796B2 - Ladder Filters and Multiplexers - Google Patents

Ladder Filters and Multiplexers Download PDF

Info

Publication number
JP7624796B2
JP7624796B2 JP2019084531A JP2019084531A JP7624796B2 JP 7624796 B2 JP7624796 B2 JP 7624796B2 JP 2019084531 A JP2019084531 A JP 2019084531A JP 2019084531 A JP2019084531 A JP 2019084531A JP 7624796 B2 JP7624796 B2 JP 7624796B2
Authority
JP
Japan
Prior art keywords
region
piezoelectric substrate
insulating layer
ladder
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.)
Active
Application number
JP2019084531A
Other languages
Japanese (ja)
Other versions
JP2020182130A (en
Inventor
直輝 柿田
均 月舘
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.)
Taiyo Yuden Co Ltd
Original Assignee
Taiyo Yuden Co 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 Taiyo Yuden Co Ltd filed Critical Taiyo Yuden Co Ltd
Priority to JP2019084531A priority Critical patent/JP7624796B2/en
Publication of JP2020182130A publication Critical patent/JP2020182130A/en
Application granted granted Critical
Publication of JP7624796B2 publication Critical patent/JP7624796B2/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

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

Description

本発明はラダー型フィルタおよびマルチプレクサに関し、例えば櫛型電極を有するラダー型フィルタおよびマルチプレクサに関する。 The present invention relates to a ladder-type filter and a multiplexer, for example, to a ladder-type filter and a multiplexer having comb-type electrodes.

スマートフォン等の通信機器に用いられる弾性波共振器として、弾性表面波共振器が知られている。弾性表面波共振器を形成する圧電基板を支持基板に接合することが知られている。支持基板と圧電基板との間に酸化シリコン膜を設けることが知られている(例えば特許文献1)。弾性表面波共振器において共振周波数と反共振周波数とで周波数温度係数が異なることが知られている(例えば特許文献2)。 Surface acoustic wave resonators are known as acoustic wave resonators used in communication devices such as smartphones. It is known that a piezoelectric substrate forming a surface acoustic wave resonator is bonded to a support substrate. It is known that a silicon oxide film is provided between the support substrate and the piezoelectric substrate (e.g., Patent Document 1). It is known that the frequency temperature coefficients of the resonant frequency and the anti-resonant frequency in a surface acoustic wave resonator are different (e.g., Patent Document 2).

特開2015-73331号公報JP 2015-73331 A 特開2017-152868号公報JP 2017-152868 A

ラダー型フィルタにおいて、フィルタを所望の特性とすること求められる。例えば、通過帯域の高周波端と低周波端との周波数温度係数を独立に設定することが求められている。 In ladder filters, it is required to give the filter the desired characteristics. For example, it is required to set the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband independently.

本発明は、上記課題に鑑みなされたものであり、通過帯域の高周波端と低周波端との周波数温度係数を独立に設定することを目的とする。 The present invention has been developed in consideration of the above problems, and aims to set the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband independently.

本発明は、支持基板と、前記支持基板上に直接または間接的に接合され、第1領域における平均厚さは第2領域における平均厚さより大きく、酸化シリコンを主成分とする絶縁層と、前記絶縁層上に直接または間接的に接合され、弾性定数の温度係数の符号が前記絶縁層の弾性定数の温度係数の符号と反対であり、タンタル酸リチウム基板である圧電基板と、前記第1領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、第1端子と第2端子との間に直列に接続された、ラダー型フィルタを形成する直列共振器と、前記第2領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、前記第1端子と前記第2端子との間における前記直列共振器が設けられた線路に一端が接続され、他端がグランドに接続された、前記ラダー型フィルタを形成する並列共振器と、を備え、前記並列共振器のうち少なくとも1つの並列共振器の一端は、前記直列共振器のうち2つの直列共振器の間における前記線路に接続され、前記第1領域および前記第2領域における前記圧電基板の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であり、前記第1領域および前記第2領域における前記絶縁層の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であるラダー型フィルタである。 The present invention relates to a piezoelectric substrate comprising: a support substrate; an insulating layer bonded directly or indirectly to the support substrate, the insulating layer having an average thickness in a first region greater than an average thickness in a second region, the insulating layer being mainly composed of silicon oxide; a piezoelectric substrate bonded directly or indirectly to the insulating layer, the insulating layer having a temperature coefficient of elastic constant whose sign is opposite to that of the temperature coefficient of elastic constant of the insulating layer, the piezoelectric substrate being a lithium tantalate substrate; a series resonator provided on the piezoelectric substrate in the first region, the series resonator having a pair of comb electrodes and connected in series between a first terminal and a second terminal , the series resonator forming a ladder-type filter ; and a series resonator provided on the piezoelectric substrate in the second region, the series resonator having a pair of comb electrodes, and a parallel resonator forming the ladder-type filter , the parallel resonator having one end connected to a line on which the series resonator is provided between the first terminal and the second terminal and the other end connected to ground, wherein one end of at least one of the parallel resonators is connected to the line between two of the series resonators, the thickness of the piezoelectric substrate in the first region and the second region is not more than twice the average pitch of the electrode fingers of the pair of comb electrodes, and the thickness of the insulating layer in the first region and the second region is not more than twice the average pitch of the electrode fingers of the pair of comb electrodes.

上記構成において、前記第1領域における前記圧電基板の平均厚さは、前記第2領域における前記圧電基板の平均厚さより小さい構成とすることができる。 In the above configuration, the average thickness of the piezoelectric substrate in the first region can be smaller than the average thickness of the piezoelectric substrate in the second region.

上記構成において、前記第1領域における前記圧電基板の平均厚さと前記第2領域における前記圧電基板の平均厚さはしい構成とすることができる。
In the above configuration, the average thickness of the piezoelectric substrate in the first region and the average thickness of the piezoelectric substrate in the second region can be equal .

本発明は、支持基板と、前記支持基板上に直接または間接的に接合され、酸化シリコンを主成分とする絶縁層と、前記絶縁層上に直接または間接的に接合され、第1領域における平均厚さは第2領域における平均厚さより小さく、弾性定数の温度係数の符号が前記絶縁層の弾性定数の温度係数の符号と反対であり、タンタル酸リチウム基板である圧電基板と、前記第1領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、第1端子と第2端子との間に直列に接続された、ラダー型フィルタを形成する直列共振器と、前記第2領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、前記第1端子と前記第2端子との間における前記直列共振器が設けられた線路に一端が接続され、他端がグランドに接続された、前記ラダー型フィルタを形成する並列共振器と、を備え、前記並列共振器のうち少なくとも1つの並列共振器の一端は、前記直列共振器のうち2つの直列共振器の間における前記線路に接続され、前記第1領域および前記第2領域における前記圧電基板の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であり、前記第1領域および前記第2領域における前記絶縁層の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であるラダー型フィルタである。 The present invention relates to a piezoelectric substrate comprising: a support substrate; an insulating layer bonded directly or indirectly onto the support substrate, the insulating layer being mainly composed of silicon oxide; a piezoelectric substrate bonded directly or indirectly onto the insulating layer, the insulating layer having an average thickness in a first region smaller than an average thickness in a second region, the insulating layer having a temperature coefficient of elastic constant whose sign is opposite to that of the temperature coefficient of elastic constant of the insulating layer, the piezoelectric substrate being a lithium tantalate substrate; a series resonator formed on the piezoelectric substrate in the first region, the series resonator having a pair of comb electrodes and connected in series between a first terminal and a second terminal , the series resonator forming a ladder-type filter ; and a series resonator formed on the piezoelectric substrate in the second region, the series resonator having a pair of comb electrodes, and a parallel resonator forming the ladder-type filter , the parallel resonator having one end connected to a line on which the series resonator is provided between the first terminal and the second terminal and the other end connected to ground, wherein one end of at least one of the parallel resonators is connected to the line between two of the series resonators, the thickness of the piezoelectric substrate in the first region and the second region is not more than twice the average pitch of the electrode fingers of the pair of comb electrodes, and the thickness of the insulating layer in the first region and the second region is not more than twice the average pitch of the electrode fingers of the pair of comb electrodes.

上記構成において、前記第1領域における前記絶縁層の平均厚さと前記第2領域における前記絶縁層の平均厚さとは等しい構成とすることができる。
In the above configuration, the average thickness of the insulating layer in the first region and the average thickness of the insulating layer in the second region may be equal .

本発明は、支持基板と、前記支持基板上に直接または間接的に接合され、第1領域における弾性定数の温度係数は第2領域における弾性定数の温度係数と同じ符号でありかつ絶対値が大きく、酸化シリコンを主成分とする絶縁層と、前記絶縁層上に直接または間接的に接合され、弾性定数の温度係数の符号が前記絶縁層の弾性定数の温度係数の符号と反対であり、タンタル酸リチウム基板である圧電基板と、前記第1領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、第1端子と第2端子との間に直列に接続された、ラダー型フィルタを形成する直列共振器と、前記第2領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、前記第1端子と前記第2端子との間に並列に接続された、前記ラダー型フィルタを形成する並列共振器と、を備え、前記第1領域および前記第2領域における前記圧電基板の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であり、前記第1領域および前記第2領域における前記絶縁層の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であるラダー型フィルタである。 The present invention is a ladder-type filter comprising: a supporting substrate; an insulating layer bonded directly or indirectly to the supporting substrate, the insulating layer having a temperature coefficient of elastic constant in a first region that has the same sign as and has a larger absolute value than the temperature coefficient of elastic constant in a second region, the insulating layer being mainly composed of silicon oxide; a piezoelectric substrate bonded directly or indirectly to the insulating layer, the insulating layer having a temperature coefficient of elastic constant that is opposite in sign to the temperature coefficient of elastic constant of the insulating layer, the piezoelectric substrate being a lithium tantalate substrate; a series resonator formed on the piezoelectric substrate in the first region, the series resonator having a pair of comb electrodes and connected in series between a first terminal and a second terminal , the series resonator forming the ladder-type filter ; and a parallel resonator formed on the piezoelectric substrate in the second region, the series resonator having a pair of comb electrodes and connected in parallel between the first terminal and the second terminal, the parallel resonator forming the ladder-type filter, the parallel resonator having a pair of comb electrodes and connected in parallel between the first terminal and the second terminal, wherein the thickness of the piezoelectric substrate in the first region and the second region is equal to or less than twice the average pitch of the electrode fingers of the pair of comb electrodes, and the thickness of the insulating layer in the first region and the second region is equal to or less than twice the average pitch of the electrode fingers of the pair of comb electrodes.

上記構成において、前記第1領域における前記絶縁層の平均厚さと前記第2領域における前記絶縁層の平均厚さとは等しく、前記第1領域における前記圧電基板の平均厚さと前記第2領域における前記圧電基板の平均厚さは等しい構成とすることができる。
In the above configuration, the average thickness of the insulating layer in the first region and the average thickness of the insulating layer in the second region can be equal, and the average thickness of the piezoelectric substrate in the first region and the average thickness of the piezoelectric substrate in the second region can be equal .

上記構成において、前記ラダー型フィルタは、前記直列共振器および前記並列共振器以外の共振器を有さないラダー型フィルタである構成とすることができる。 In the above configuration, the ladder-type filter may be a ladder-type filter that does not have any resonators other than the series resonators and the parallel resonators.

本発明は、上記ラダー型フィルタを含むマルチプレクサである。
The present invention is a multiplexer including the above ladder-type filter.

本発明によれば、通過帯域の高周波端と低周波端との周波数温度係数を独立に設定することができる。 According to the present invention, the frequency temperature coefficients of the high and low frequency ends of the passband can be set independently.

図1(a)は実施例1に係るラダー型フィルタの回路図、図1(b)は、ラダー型フィルタの通過特性を示す模式図である。FIG. 1A is a circuit diagram of a ladder-type filter in accordance with a first embodiment, and FIG. 1B is a schematic diagram showing the pass characteristic of the ladder-type filter. 図2(a)は、実施例1における弾性波共振器の平面図、図2(b)は、図2(a)のA-A断面図であるFIG. 2A is a plan view of the elastic wave resonator in the first embodiment, and FIG. 2B is a cross-sectional view taken along line AA of FIG. 図3(a)および図3(b)は、それぞれ実験およびシミュレーションに用いた弾性波共振器の断面図である。3A and 3B are cross-sectional views of acoustic wave resonators used in the experiments and simulations, respectively. 図4(a)および図4(b)は、共振周波数および反共振周波数のTCFの実験およびシミュレーション結果を示す図である。4(a) and 4(b) are diagrams showing experimental and simulation results of the TCF of the resonant and anti-resonant frequencies. 図5は、実施例1に係るフィルタの平面図である。FIG. 5 is a plan view of the filter according to the first embodiment. 図6は、実施例1に係るフィルタの断面図である。FIG. 6 is a cross-sectional view of the filter according to the first embodiment. 図7(a)および図7(b)は、それぞれ実施例1の変形例1および2に係るフィルタの断面図である。7A and 7B are cross-sectional views of filters according to first and second modifications of the first embodiment, respectively. 図8(a)および図8(b)は、それぞれ実施例1の変形例3および4に係るフィルタの断面図である。8A and 8B are cross-sectional views of filters according to third and fourth modifications of the first embodiment, respectively. 図9は、実施例2に係るデュプレクサの回路図である。FIG. 9 is a circuit diagram of a duplexer according to the second embodiment.

以下、図面を参照し本発明の実施例について説明する。 The following describes an embodiment of the present invention with reference to the drawings.

図1(a)は実施例1に係るラダー型フィルタの回路図、図1(b)は、ラダー型フィルタの通過特性を示す模式図である。図1(a)に示すように、ラダー型フィルタは、直列共振器S1からS4および並列共振器P1からP3を備えている。直列共振器S1からS4は、入力端子Tin(第1端子)と出力端子Tout(第2端子)との間に直列に接続されている。並列共振器P1からP3は入力端子Tinと出力端子Toutとの間に並列に接続されている。並列共振器P1からP3の一端はグランド端子Tgに接続されている。直列共振器および並列共振器の個数は適宜設定できる。 Figure 1(a) is a circuit diagram of a ladder-type filter according to the first embodiment, and Figure 1(b) is a schematic diagram showing the pass characteristics of the ladder-type filter. As shown in Figure 1(a), the ladder-type filter includes series resonators S1 to S4 and parallel resonators P1 to P3. The series resonators S1 to S4 are connected in series between the input terminal Tin (first terminal) and the output terminal Tout (second terminal). The parallel resonators P1 to P3 are connected in parallel between the input terminal Tin and the output terminal Tout. One end of the parallel resonators P1 to P3 is connected to the ground terminal Tg. The number of series resonators and parallel resonators can be set appropriately.

図1(b)に示すように、ラダー型フィルタは、通過帯域48および阻止帯域49を有するバンドパスフィルタとして機能する。直列共振器S1からS4の共振周波数frsは通過帯域48の中央部に位置し、反共振周波数fasは通過帯域48より高周波数側の阻止帯域49に位置する。並列共振器P1からP3の反共振周波数fapは通過帯域48の中央部に位置し、共振周波数frpは通過帯域48より低周波数側の阻止帯域49に位置する。通過帯域48の高周波端は直列共振器S1からS4の反共振周波数fasにより定まり、通過帯域48の低周波端は並列共振器P1からP3の共振周波数frpにより定まる。 As shown in FIG. 1(b), the ladder filter functions as a bandpass filter having a passband 48 and a stopband 49. The resonant frequency frs of the series resonators S1 to S4 is located in the center of the passband 48, and the anti-resonant frequency fas is located in the stopband 49 on the higher frequency side of the passband 48. The anti-resonant frequency fap of the parallel resonators P1 to P3 is located in the center of the passband 48, and the resonant frequency frp is located in the stopband 49 on the lower frequency side of the passband 48. The high-frequency end of the passband 48 is determined by the anti-resonant frequency fas of the series resonators S1 to S4, and the low-frequency end of the passband 48 is determined by the resonant frequency frp of the parallel resonators P1 to P3.

通過帯域48の温度変化を小さくするためには、直列共振器S1からS4の反共振周波数fasの周波数温度係数を小さくしかつ並列共振器P1からP3の共振周波数frpの周波数温度係数を小さくすることが求められる。また、通過帯域の幅を変えないためには、直列共振器S1からS4の反共振周波数fasの周波数温度係数と、並列共振器P1からP3の共振周波数frpの周波数温度係数と、を略等しくすることが求められる。 To reduce the temperature change of the passband 48, it is necessary to reduce the frequency temperature coefficient of the anti-resonant frequency fas of the series resonators S1 to S4 and the frequency temperature coefficient of the resonant frequency frp of the parallel resonators P1 to P3. Also, to keep the width of the passband unchanged, it is necessary to make the frequency temperature coefficient of the anti-resonant frequency fas of the series resonators S1 to S4 and the frequency temperature coefficient of the resonant frequency frp of the parallel resonators P1 to P3 approximately equal.

図2(a)は、実施例1における弾性波共振器の平面図、図2(b)は、図2(a)のA-A断面図である。電極指の配列方向をX方向、電極指の延伸方向をY方向、支持基板および圧電基板の積層方向をZ方向とする。X方向、Y方向およびZ方向は、圧電基板の結晶方位のX軸方向およびY軸方向とは必ずしも対応しない。圧電基板が回転YカットX伝搬基板の場合、X方向は結晶方位のX軸方向となる。 Figure 2(a) is a plan view of the elastic wave resonator in Example 1, and Figure 2(b) is a cross-sectional view taken along the line A-A in Figure 2(a). The arrangement direction of the electrode fingers is the X direction, the extension direction of the electrode fingers is the Y direction, and the stacking direction of the support substrate and piezoelectric substrate is the Z direction. The X direction, Y direction, and Z direction do not necessarily correspond to the X-axis direction and Y-axis direction of the crystal orientation of the piezoelectric substrate. When the piezoelectric substrate is a rotated Y-cut X-propagation substrate, the X direction is the X-axis direction of the crystal orientation.

図2(a)および図2(b)に示すように、支持基板10上に絶縁層11が接合されている。絶縁層11上に圧電基板12が接合されている。絶縁層11は支持基板10上に直接接合されていてもよいし、接合層等を介し間接的に接合されていてもよい。圧電基板12は絶縁層11上に直接接合されていてもよいし、接合層等を介し間接的に接合されていてもよい。圧電基板12上に弾性波共振器20が設けられている。弾性波共振器20はIDT(Inter Digital Transducer)22および反射器24を有する。反射器24はIDT22のX方向の両側に設けられている。IDT22および反射器24は、圧電基板12上の金属膜14により形成される。 2(a) and 2(b), an insulating layer 11 is bonded onto a support substrate 10. A piezoelectric substrate 12 is bonded onto the insulating layer 11. The insulating layer 11 may be bonded directly onto the support substrate 10, or may be bonded indirectly via a bonding layer or the like. The piezoelectric substrate 12 may be bonded directly onto the insulating layer 11, or may be bonded indirectly via a bonding layer or the like. An elastic wave resonator 20 is provided on the piezoelectric substrate 12. The elastic wave resonator 20 has an IDT (Inter Digital Transducer) 22 and a reflector 24. The reflectors 24 are provided on both sides of the IDT 22 in the X direction. The IDT 22 and the reflector 24 are formed by a metal film 14 on the piezoelectric substrate 12.

IDT22は、対向する一対の櫛型電極18を備える。櫛型電極18は、複数の電極指15と、複数の電極指15が接続されたバスバー16と、を備える。一対の櫛型電極18の電極指15が交差する領域が交差領域25である。交差領域25の長さが開口長である。一対の櫛型電極18は、交差領域25の少なくとも一部において電極指15がほぼ互い違いとなるように、対向して設けられている。交差領域25において複数の電極指15が励振する弾性波は、主にX方向に伝搬する。一対の櫛型電極18のうち一方の櫛型電極の電極指15のピッチがほぼ弾性波の波長λとなる。弾性波の波長λはほぼ電極指15の2本分のピッチとなる。反射器24は、IDT22の電極指15が励振した弾性波(弾性表面波)を反射する。これにより弾性波はIDT22の交差領域25内に閉じ込められる。 The IDT 22 includes a pair of comb electrodes 18 facing each other. The comb electrodes 18 include a plurality of electrode fingers 15 and a bus bar 16 to which the plurality of electrode fingers 15 are connected. The region where the electrode fingers 15 of the pair of comb electrodes 18 intersect is the intersection region 25. The length of the intersection region 25 is the aperture length. The pair of comb electrodes 18 are provided facing each other so that the electrode fingers 15 are almost alternated in at least a part of the intersection region 25. The elastic wave excited by the plurality of electrode fingers 15 in the intersection region 25 propagates mainly in the X direction. The pitch of the electrode fingers 15 of one of the pair of comb electrodes 18 is approximately the wavelength λ of the elastic wave. The wavelength λ of the elastic wave is approximately the pitch of two electrode fingers 15. The reflector 24 reflects the elastic wave (surface acoustic wave) excited by the electrode fingers 15 of the IDT 22. As a result, the elastic wave is confined within the intersection region 25 of the IDT 22.

圧電基板12は、単結晶タンタル酸リチウム(LiTaO)基板、単結晶ニオブ酸リチウム(LiNbO)基板または単結晶水晶基板であり、例えば回転YカットX伝搬タンタル酸リチウム基板または回転YカットX伝搬ニオブ酸リチウム基板である。絶縁層11は、例えば酸化シリコン(SiO)を主成分とするアモルファスおよび/または多結晶層である。絶縁層11は、酸化シリコンを主成分とし、弗素等の不純物を含んでいてもよい。絶縁層11の弾性定数の温度係数の符号は圧電基板12の弾性定数の温度係数の符号の反対である。これにより、弾性波共振器の周波数温度係数を小さくできる。 The piezoelectric substrate 12 is a single crystal lithium tantalate (LiTaO 3 ) substrate, a single crystal lithium niobate (LiNbO 3 ) substrate, or a single crystal quartz substrate, for example a rotated Y-cut X-propagation lithium tantalate substrate or a rotated Y-cut X-propagation lithium niobate substrate. The insulating layer 11 is, for example, an amorphous and/or polycrystalline layer mainly composed of silicon oxide (SiO 2 ). The insulating layer 11 is mainly composed of silicon oxide and may contain impurities such as fluorine. The sign of the temperature coefficient of the elastic constant of the insulating layer 11 is opposite to the sign of the temperature coefficient of the elastic constant of the piezoelectric substrate 12. This allows the frequency temperature coefficient of the elastic wave resonator to be reduced.

支持基板10は、圧電基板12のX方向の線膨張係数より小さな線膨張係数を有する。これにより、弾性波共振器の周波数温度係数を小さくできる。支持基板10は、例えばサファイア基板、アルミナ基板、シリコン基板または炭化シリコン基板である。サファイア基板はr面、c面またはa面を上面とする単結晶酸化アルミニウム(Al)基板である。アルミナ基板は多結晶酸化アルミニウム(Al)基板である。シリコン基板は単結晶または多結晶シリコン(Si)基板である。炭化シリコン基板は単結晶または多結晶炭化シリコン(SiC)基板である。 The support substrate 10 has a linear expansion coefficient smaller than that of the piezoelectric substrate 12 in the X direction. This allows the frequency temperature coefficient of the elastic wave resonator to be small. The support substrate 10 is, for example, a sapphire substrate, an alumina substrate, a silicon substrate, or a silicon carbide substrate. The sapphire substrate is a single crystal aluminum oxide (Al 2 O 3 ) substrate with the r-plane, c-plane, or a-plane as the upper surface. The alumina substrate is a polycrystalline aluminum oxide (Al 2 O 3 ) substrate. The silicon substrate is a single crystal or polycrystalline silicon (Si) substrate. The silicon carbide substrate is a single crystal or polycrystalline silicon carbide (SiC) substrate.

金属膜14は、例えばアルミニウム(Al)、銅(Cu)またはモリブデン(Mo)を主成分とする膜であり、例えばアルミニウム膜、銅膜またはモリブデン膜である。電極指15と圧電基板12との間にTi(チタン)膜またはCr(クロム)膜等の密着膜が設けられていてもよい。密着膜は電極指15より薄い。電極指15を覆うように絶縁膜が設けられていてもよい。絶縁膜は保護膜または温度補償層として機能する。 The metal film 14 is a film whose main component is, for example, aluminum (Al), copper (Cu) or molybdenum (Mo), for example, an aluminum film, a copper film or a molybdenum film. An adhesive film such as a Ti (titanium) film or a Cr (chromium) film may be provided between the electrode fingers 15 and the piezoelectric substrate 12. The adhesive film is thinner than the electrode fingers 15. An insulating film may be provided so as to cover the electrode fingers 15. The insulating film functions as a protective film or a temperature compensation layer.

支持基板10の厚さは例えば50μmから500μmである。絶縁層11の厚さT1は、例えば0.1μmから10μmであり、例えば弾性波の波長λ以下である。圧電基板12の厚さT2は例えば0.5μmから20μmであり、例えば弾性波の波長λ以下である。弾性波の波長λは例えば1μmから6μmである。2本の電極指15を1対としたときの対数は例えば20対から300対である。IDT22のデュティ比は、電極指15の太さ/電極指15のピッチであり、例えば30%から80%である。IDT22の開口長は例えば10λから50λである。 The thickness of the support substrate 10 is, for example, 50 μm to 500 μm. The thickness T1 of the insulating layer 11 is, for example, 0.1 μm to 10 μm, and is, for example, equal to or less than the wavelength λ of the elastic wave. The thickness T2 of the piezoelectric substrate 12 is, for example, 0.5 μm to 20 μm, and is, for example, equal to or less than the wavelength λ of the elastic wave. The wavelength λ of the elastic wave is, for example, 1 μm to 6 μm. When two electrode fingers 15 are considered as one pair, the number of pairs is, for example, 20 pairs to 300 pairs. The duty ratio of the IDT 22 is the thickness of the electrode finger 15/the pitch of the electrode finger 15, and is, for example, 30% to 80%. The aperture length of the IDT 22 is, for example, 10λ to 50λ.

支持基板10として圧電基板12より線膨張係数の小さい材料を用いると、温度変化により電極指15のピッチの変化が小さくなり周波数温度係数の変化が小さくなる。さらに、圧電基板12と絶縁層11の弾性定数の温度係数の正負の符号を反対とする。これにより、周波数温度係数がさらに小さくなる。 When a material with a smaller linear expansion coefficient than the piezoelectric substrate 12 is used as the support substrate 10, the change in pitch of the electrode fingers 15 due to temperature change is smaller, and the change in the frequency temperature coefficient is also smaller. Furthermore, the positive and negative signs of the temperature coefficients of the elastic constants of the piezoelectric substrate 12 and the insulating layer 11 are reversed. This further reduces the frequency temperature coefficient.

[実験およびシミュレーション]
圧電基板12および絶縁層11の厚さT1およびT2を変え、共振周波数frおよび反共振周波数の周波数温度係数(TCF:Temperature Coefficient of Frequency)を測定およびシミュレーションした。図3(a)および図3(b)は、それぞれ実験およびシミュレーションに用いた弾性波共振器の断面図である。
[Experiments and Simulations]
The temperature coefficient of frequency (TCF) of the resonant frequency fr and the anti-resonant frequency was measured and simulated by changing the thicknesses T1 and T2 of the piezoelectric substrate 12 and the insulating layer 11. Figures 3(a) and 3(b) are cross-sectional views of the acoustic wave resonators used in the experiment and the simulation, respectively.

図3(a)に示すように、実験では、絶縁層11と圧電基板12との間に接合層13が設けられている。弾性波共振器20の作製方法について説明する。支持基板10上に絶縁層11をCVD(Chemical Vapor Deposition)法を用い成膜する。絶縁層11上に接合層13を成膜する。接合層13と圧電基板12とを表面活性化法を用い接合する。絶縁層11として酸化シリコン膜を用いると圧電基板との接合強度が弱いため、接合層13を設けている。CMP(Chemical Mechanical Polishing)法を用い圧電基板12の上面を所望の厚さとする。圧電基板12上にIDT22および反射器24を金属膜14を用い形成する。 As shown in FIG. 3(a), in the experiment, a bonding layer 13 is provided between the insulating layer 11 and the piezoelectric substrate 12. The method of manufacturing the elastic wave resonator 20 will be described. The insulating layer 11 is formed on the support substrate 10 using a CVD (Chemical Vapor Deposition) method. The bonding layer 13 is formed on the insulating layer 11. The bonding layer 13 and the piezoelectric substrate 12 are bonded using a surface activation method. If a silicon oxide film is used as the insulating layer 11, the bonding strength with the piezoelectric substrate is weak, so the bonding layer 13 is provided. The upper surface of the piezoelectric substrate 12 is made to the desired thickness using a CMP (Chemical Mechanical Polishing) method. The IDT 22 and the reflector 24 are formed on the piezoelectric substrate 12 using a metal film 14.

弾性波共振器20の作製条件は以下である。
支持基板10:サファイア基板
絶縁層11:厚さがT1の酸化シリコン層
接合層13:厚さが10nmの酸化アルミニウム層
圧電基板12:厚さがT2の42°YカットX伝搬タンタル酸リチウム基板
金属膜14:厚さが500nmのアルミニウム膜
電極指15のピッチ×2:5μm(弾性波の波長λ)
電極指15の対数(本数×2):100対
デュティ比:50%
開口長:100μm(20λ)
The conditions for fabricating the acoustic wave resonator 20 are as follows.
Support substrate 10: sapphire substrate Insulating layer 11: silicon oxide layer with thickness T1 Bonding layer 13: aluminum oxide layer with thickness 10 nm Piezoelectric substrate 12: 42° Y-cut X-propagation lithium tantalate substrate with thickness T2 Metal film 14: aluminum film with thickness 500 nm Pitch of electrode fingers 15×2: 5 μm (wavelength λ of elastic wave)
Number of pairs of electrode fingers 15 (number of fingers x 2): 100 pairs Duty ratio: 50%
Opening length: 100μm (20λ)

図3(b)に示すように、シミュレーションでは、支持基板10は減衰材46上に設けられている。支持基板10上に絶縁層11が設けられ、絶縁層11上に圧電基板12が設けられている。圧電基板12上に電極指15が設けられている。圧電基板12上には電極指15を覆うように空気層44が設けられている。電極指15のピッチはλ/2である。X方向の幅をλとし、X方向の境界条件を周期境界条件とした。Y方向の幅をλ/32とし、Y方向の境界条件を周期境界条件とした。その他のシミュレーション条件は実験と同じである。 As shown in FIG. 3(b), in the simulation, the support substrate 10 is provided on the damping material 46. An insulating layer 11 is provided on the support substrate 10, and a piezoelectric substrate 12 is provided on the insulating layer 11. Electrode fingers 15 are provided on the piezoelectric substrate 12. An air layer 44 is provided on the piezoelectric substrate 12 so as to cover the electrode fingers 15. The pitch of the electrode fingers 15 is λ/2. The width in the X direction is λ, and the boundary condition in the X direction is a periodic boundary condition. The width in the Y direction is λ/32, and the boundary condition in the Y direction is a periodic boundary condition. The other simulation conditions are the same as in the experiment.

図4(a)および図4(b)は、共振周波数および反共振周波数のTCFの実験およびシミュレーション結果を示す図である。横軸は圧電基板12の厚さT2/λであり縦軸はTCFである。圧電基板12の厚さT2を0.2λ、0.4λおよび0.6λとし、絶縁層11の厚さT1を0.2λ、0.4λおよび0.6λとした。ドットは測定点およびシミュレーション点であり、曲線は近似曲線である。T1=0.2λ、0.4λおよび0.6λの測定点からT1=0.1λの推定線を実線で図示している。 Figures 4(a) and 4(b) show experimental and simulation results for the TCF of the resonant frequency and anti-resonant frequency. The horizontal axis is the thickness T2/λ of the piezoelectric substrate 12, and the vertical axis is the TCF. The thickness T2 of the piezoelectric substrate 12 was set to 0.2λ, 0.4λ, and 0.6λ, and the thickness T1 of the insulating layer 11 was set to 0.2λ, 0.4λ, and 0.6λ. The dots represent measurement and simulation points, and the curves are approximation curves. The estimated line of T1 = 0.1λ from the measurement points of T1 = 0.2λ, 0.4λ, and 0.6λ is shown as a solid line.

図4(a)および図4(b)を比較すると、反共振周波数faのTCFは共振周波数frのTCFよりマイナス側に位置する。圧電基板12の厚さT2が小さくなると、TCFはプラスの方向に変化する。T2が0.6λと0.4λの間のTCFの差より、T2が0.4λと0.2λとの間のTCFの差が大きい。絶縁層11の厚さT1が大きくなるとTCFはプラスの方向に変化する。 Comparing Figures 4(a) and 4(b), the TCF of the anti-resonant frequency fa is located on the negative side of the TCF of the resonant frequency fr. When the thickness T2 of the piezoelectric substrate 12 decreases, the TCF changes in the positive direction. The difference in TCF between T2 of 0.4λ and 0.2λ is greater than the difference in TCF between T2 of 0.6λ and 0.4λ. When the thickness T1 of the insulating layer 11 increases, the TCF changes in the positive direction.

タンタル酸リチウムと酸化シリコンとでは弾性定数の温度係数の正負の符号が反対である。電極指15が励振した弾性表面波のエネルギーは主に圧電基板12と絶縁層11内に存在する。圧電基板12を薄くすると、絶縁層11内に含まれる弾性表面波のエネルギーが大きくなりTCFがプラスの方向に変化する。絶縁層11を厚くすると、絶縁層11内に含まれる弾性表面波のエネルギーが大きくなりTCFがプラスの方向に変化する。このように、圧電基板12の厚さT1と絶縁層11の厚さT2を適宜設定することで、ラダー型フィルタの通過帯域の高周波端のTCFと低周波端のTCFを独立に設定できる。 The positive and negative signs of the temperature coefficient of the elastic constant are opposite for lithium tantalate and silicon oxide. The energy of the surface acoustic wave excited by the electrode fingers 15 exists mainly in the piezoelectric substrate 12 and the insulating layer 11. When the piezoelectric substrate 12 is made thinner, the energy of the surface acoustic wave contained in the insulating layer 11 increases and the TCF changes in the positive direction. When the insulating layer 11 is made thicker, the energy of the surface acoustic wave contained in the insulating layer 11 increases and the TCF changes in the positive direction. In this way, by appropriately setting the thickness T1 of the piezoelectric substrate 12 and the thickness T2 of the insulating layer 11, the TCF at the high-frequency end and the TCF at the low-frequency end of the pass band of the ladder filter can be set independently.

例えば、シミュレーション結果を例に、直列共振器では、T1=0.6λおよびT2=0.4λとすると、直列共振器の反共振周波数fasのTCFは約-5ppm/Kである。並列共振器では、T1=0.2λおよびT2=0.4λとすると、並列共振器の共振周波数frpのTCFは約-5ppm/Kである。このように、直列共振器と並列共振器とで圧電基板12の厚さT2を略等しくし、直列共振器の絶縁層11の厚さT1を並列共振器の絶縁層11の厚さT1より大きくすると、直列共振器の反共振周波数fasのTCFと並列共振器の共振周波数frpのTCFを略等しくかつ0に近づけることができる。 For example, using simulation results as an example, when T1 = 0.6λ and T2 = 0.4λ in a series resonator, the TCF of the anti-resonant frequency fas of the series resonator is approximately -5 ppm/K. When T1 = 0.2λ and T2 = 0.4λ in a parallel resonator, the TCF of the resonant frequency frp of the parallel resonator is approximately -5 ppm/K. In this way, by making the thickness T2 of the piezoelectric substrate 12 of the series resonator and the parallel resonator approximately the same and making the thickness T1 of the insulating layer 11 of the series resonator greater than the thickness T1 of the insulating layer 11 of the parallel resonator, the TCF of the anti-resonant frequency fas of the series resonator and the TCF of the resonant frequency frp of the parallel resonator can be made approximately equal and close to 0.

別の例では、直列共振器では、T1=0.4λおよびT2=0.2λとすると、直列共振器の反共振周波数fasのTCFは約-10ppm/Kである。並列共振器では、T1=0.4λおよびT2=0.6λとすると、並列共振器の共振周波数frpのTCFは約-10ppm/Kである。直列共振器と並列共振器とで絶縁層11の厚さT1を略等しくし、直列共振器の圧電基板12の厚さT2を並列共振器の圧電基板12の厚さT2より小さくすると、直列共振器の反共振周波数fasのTCFと並列共振器の共振周波数frpのTCFを略等しくかつ0に近づけることができる。 In another example, for a series resonator, if T1 = 0.4λ and T2 = 0.2λ, the TCF of the anti-resonant frequency fas of the series resonator is approximately -10 ppm/K. For a parallel resonator, if T1 = 0.4λ and T2 = 0.6λ, the TCF of the resonant frequency frp of the parallel resonator is approximately -10 ppm/K. If the thickness T1 of the insulating layer 11 of the series resonator and the parallel resonator is approximately the same and the thickness T2 of the piezoelectric substrate 12 of the series resonator is smaller than the thickness T2 of the piezoelectric substrate 12 of the parallel resonator, the TCF of the anti-resonant frequency fas of the series resonator and the TCF of the resonant frequency frp of the parallel resonator can be approximately the same and approach 0.

図5は、実施例1に係るフィルタの平面図である。図5に示すように、圧電基板12上に弾性波共振器20および配線26が設けられている。弾性波共振器20は直列共振器S1からS4および並列共振器P1からP3を含む。配線26はパッドPin、PoutおよびPgを含む。パッドPin、PoutおよびPgはそれぞれ入力端子Tin、出力端子Toutおよびグランド端子Tgに電気的に接続されている。直列共振器S1からS4は、配線26を介しパッドPinとPoutとの間に直列に接続され、並列共振器P1からP3は、配線26を介しパッドPinとPoutとの間に並列に接続されている。並列共振器P1からP3は領域50に設けられ、直列共振器S1からS4は、領域52に設けられている。 Figure 5 is a plan view of the filter according to the first embodiment. As shown in Figure 5, an elastic wave resonator 20 and a wiring 26 are provided on a piezoelectric substrate 12. The elastic wave resonator 20 includes series resonators S1 to S4 and parallel resonators P1 to P3. The wiring 26 includes pads Pin, Pout, and Pg. The pads Pin, Pout, and Pg are electrically connected to the input terminal Tin, the output terminal Tout, and the ground terminal Tg, respectively. The series resonators S1 to S4 are connected in series between the pads Pin and Pout via the wiring 26, and the parallel resonators P1 to P3 are connected in parallel between the pads Pin and Pout via the wiring 26. The parallel resonators P1 to P3 are provided in an area 50, and the series resonators S1 to S4 are provided in an area 52.

図6は、実施例1に係るフィルタの断面図である。図6に示すように、領域50および52における圧電基板12の平均厚さはそれぞれT2pおよびT2sである。領域50と52との間の支持基板10の上面に段差が設けられている。領域50における絶縁層11の平均厚さT1pは領域52における絶縁層11の平均厚さT1sより小さい。圧電基板12の平均厚さT2pとT2sは略等しい。領域50と52と間の圧電基板12の上面には段差はなく略平面である。 Figure 6 is a cross-sectional view of the filter according to Example 1. As shown in Figure 6, the average thicknesses of the piezoelectric substrate 12 in regions 50 and 52 are T2p and T2s, respectively. A step is provided on the upper surface of the support substrate 10 between regions 50 and 52. The average thickness T1p of the insulating layer 11 in region 50 is smaller than the average thickness T1s of the insulating layer 11 in region 52. The average thicknesses T2p and T2s of the piezoelectric substrate 12 are approximately equal. The upper surface of the piezoelectric substrate 12 between regions 50 and 52 has no step and is approximately flat.

実施例1によれば、直列共振器S1からS4が設けられた領域52(第1領域)における絶縁層11の平均厚さT1sと並列共振器P1からP3が設けられた領域50(第2領域)における絶縁層11の平均厚さT1pが異なる。これにより、通過帯域の高周波端と低周波端の周波数温度係数を独立に設定できる。 According to the first embodiment, the average thickness T1s of the insulating layer 11 in the region 52 (first region) where the series resonators S1 to S4 are provided is different from the average thickness T1p of the insulating layer 11 in the region 50 (second region) where the parallel resonators P1 to P3 are provided. This allows the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband to be set independently.

領域52における絶縁層の平均厚さT1sは、領域50における絶縁層11の平均厚さT1pより大きい。これにより、通過帯域の高周波端と低周波端の周波数温度係数を近づけることができる。T1sはT1pの1.1倍以上が好ましく、1.5倍以上がより好ましい。T1sはT1pの3倍以下が好ましい。 The average thickness T1s of the insulating layer in region 52 is greater than the average thickness T1p of the insulating layer 11 in region 50. This allows the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband to be closer together. T1s is preferably 1.1 times or more, and more preferably 1.5 times or more, of T1p. T1s is preferably 3 times or less of T1p.

領域52における圧電基板12の平均厚さT2sと領域50における圧電基板12の平均厚さT2pは製造誤差を許容する程度に略等しい。これにより、通過帯域の高周波端と低周波端の周波数温度係数を近づけることができる。 The average thickness T2s of the piezoelectric substrate 12 in region 52 and the average thickness T2p of the piezoelectric substrate 12 in region 50 are approximately equal to a degree that allows for manufacturing errors. This allows the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband to be brought closer together.

[実施例1の変形例1]
図7(a)は、実施例1の変形例1に係るフィルタの断面図である。図7(a)に示すように、支持基板10絶縁層11との界面に凸部54および凹部56が設けられている。領域50および52おける凹部56における絶縁層11の厚さT4pおよびT4sは略等しい。領域50および52における凸部54の高さT5pおよびT5sは互いに異なる。T5pはT5sより大きい。これにより、領域50における絶縁層11の平均厚さT1pは領域52における絶縁層11の平均厚さT1sより小さくなる。その他の構成は実施例1と同じであり説明を省略する。
[Modification 1 of Example 1]
7A is a cross-sectional view of a filter according to a first modified example of the first embodiment. As shown in FIG. 7A, a convex portion 54 and a concave portion 56 are provided at the interface between the support substrate 10 and the insulating layer 11. The thicknesses T4p and T4s of the insulating layer 11 at the concave portions 56 in the regions 50 and 52 are substantially equal. The heights T5p and T5s of the convex portions 54 in the regions 50 and 52 are different from each other. T5p is greater than T5s. As a result, the average thickness T1p of the insulating layer 11 in the region 50 is smaller than the average thickness T1s of the insulating layer 11 in the region 52. The other configurations are the same as those of the first embodiment, and therefore description thereof will be omitted.

実施例1の変形例1のように、凸部54の高さを異ならせることで絶縁層11の平均厚さT1pとT1sとを異ならせてもよい。なお、絶縁層11の平均厚さT1pおよびT1sは、絶縁層11の平面視における単位面積当たりの体積により算出できる。 As in Variation 1 of Example 1, the height of the protrusions 54 may be varied to make the average thicknesses T1p and T1s of the insulating layer 11 different. The average thicknesses T1p and T1s of the insulating layer 11 can be calculated from the volume per unit area of the insulating layer 11 in a plan view.

[実施例1の変形例2]
図7(b)は、実施例1の変形例2に係るフィルタの断面図である。図7(b)に示すように、支持基板10の上面および圧電基板12の上面の領域50と52との間には段差はなく略平面である。領域50と52との間における絶縁層11の上面に段差が設けられている。T2pはT2sより大きく、T1pはT1sより小さい。その他の構成は実施例1と同じであり説明を省略する。
[Modification 2 of Example 1]
Fig. 7B is a cross-sectional view of a filter according to Modification 2 of Example 1. As shown in Fig. 7B, there is no step between regions 50 and 52 on the upper surface of the support substrate 10 and the upper surface of the piezoelectric substrate 12, and the upper surface is substantially flat. A step is provided on the upper surface of the insulating layer 11 between regions 50 and 52. T2p is larger than T2s, and T1p is smaller than T1s. The other configurations are the same as those of Example 1, and therefore description thereof will be omitted.

実施例1の変形例2のように、領域52における圧電基板12の平均厚さT2sと領域50における圧電基板12の平均厚さT2pとは互いに異なる。こにより、通過帯域の高周波端と低周波端の周波数温度係数を独立に設定できる。 As in the second modification of the first embodiment, the average thickness T2s of the piezoelectric substrate 12 in the region 52 is different from the average thickness T2p of the piezoelectric substrate 12 in the region 50. This allows the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband to be set independently.

また、領域52における絶縁層11の平均厚さT1sは、領域50における絶縁層11の平均厚さT1pより大きく、かつ領域52における圧電基板12の平均厚さT2sは、領域50における圧電基板12の平均厚さT2pより小さい。これにより、通過帯域の高周波端と低周波端の周波数温度係数をより近づけることができる。T2pはT2sの1.1倍以上が好ましく、1.5倍以上がより好ましい。T2pはT2sの3倍以下が好ましい。 The average thickness T1s of the insulating layer 11 in region 52 is greater than the average thickness T1p of the insulating layer 11 in region 50, and the average thickness T2s of the piezoelectric substrate 12 in region 52 is smaller than the average thickness T2p of the piezoelectric substrate 12 in region 50. This allows the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband to be closer together. T2p is preferably 1.1 times or more than T2s, and more preferably 1.5 times or more. T2p is preferably 3 times or less than T2s.

[実施例1の変形例3]
図8(a)は、実施例1の変形例3に係るフィルタの断面図である。図8(a)に示すように、圧電基板12の上面の領域50と52との間には段差はなく略平面である。領域50と52との間における支持基板10の上面および絶縁層11の上面に段差が設けられている。T2pはT2sより大きく、T1pはT1sと略等しい。その他の構成は実施例1と同じであり説明を省略する。
[Modification 3 of Example 1]
Fig. 8(a) is a cross-sectional view of a filter according to Modification 3 of Example 1. As shown in Fig. 8(a), there is no step between areas 50 and 52 on the upper surface of the piezoelectric substrate 12, which is substantially flat. Steps are provided on the upper surface of the support substrate 10 and the upper surface of the insulating layer 11 between areas 50 and 52. T2p is larger than T2s, and T1p is substantially equal to T1s. The other configurations are the same as those of Example 1, and therefore description thereof will be omitted.

実施例1の変形例3のように、領域52における絶縁層11の平均厚さT1sは、領域50における絶縁層11の平均厚さT1pと製造誤差程度に略等しく、かつ領域52における圧電基板12の平均厚さT2sは、領域50における圧電基板12の平均厚さT2pより小さい。これにより、通過帯域の高周波端と低周波端の周波数温度係数をより近づけることができる。 As in the third modification of the first embodiment, the average thickness T1s of the insulating layer 11 in the region 52 is approximately equal to the average thickness T1p of the insulating layer 11 in the region 50 within the manufacturing error range, and the average thickness T2s of the piezoelectric substrate 12 in the region 52 is smaller than the average thickness T2p of the piezoelectric substrate 12 in the region 50. This makes it possible to bring the frequency temperature coefficients of the high-frequency end and the low-frequency end of the pass band closer together.

[実施例1の変形例4]
図8(b)は、実施例1の変形例4に係るフィルタの断面図である。図8(b)に示すように、領域50の支持基板10と圧電基板12との間に絶縁層11pが設けられ、領域52の支持基板10と圧電基板12との間に絶縁層11sが設けられている。T2pはT2sと略等しく、T1pはT1sと略等しい。絶縁層11pの弾性定数の温度係数と絶縁層11sの弾性定数の温度係数とは異なる。例えば絶縁層11sの弗素濃度は絶縁層11pの弗素濃度より高い。例えば、絶縁層11pには意図的に弗素を添加しておらず、絶縁層11sに5原子%程度の弗素を添加する。その他の構成は実施例1と同じであり説明を省略する。
[Fourth Modification of the First Embodiment]
FIG. 8B is a cross-sectional view of a filter according to a fourth modified example of the first embodiment. As shown in FIG. 8B, an insulating layer 11p is provided between the support substrate 10 and the piezoelectric substrate 12 in the region 50, and an insulating layer 11s is provided between the support substrate 10 and the piezoelectric substrate 12 in the region 52. T2p is approximately equal to T2s, and T1p is approximately equal to T1s. The temperature coefficient of the elastic constant of the insulating layer 11p is different from the temperature coefficient of the elastic constant of the insulating layer 11s. For example, the fluorine concentration of the insulating layer 11s is higher than that of the insulating layer 11p. For example, fluorine is not intentionally added to the insulating layer 11p, and about 5 atomic % of fluorine is added to the insulating layer 11s. The other configurations are the same as those of the first embodiment, and a description thereof will be omitted.

酸化シリコン内の弗素濃度が高くなると弾性定数の温度係数の変化量が大きくなる。よって、領域52の絶縁層11sの弗素濃度を領域50の絶縁層11pの弗素濃度より高くする。これにより、通過帯域の高周波端と低周波端の周波数温度係数をより近づけることができる。 When the fluorine concentration in silicon oxide increases, the amount of change in the temperature coefficient of the elastic constant increases. Therefore, the fluorine concentration of insulating layer 11s in region 52 is made higher than the fluorine concentration of insulating layer 11p in region 50. This makes it possible to bring the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband closer together.

実施例1の変形例4によれば、領域52における絶縁層11sの弾性定数の温度係数と領域50における絶縁層11pの弾性定数の温度係数とは互いに異なる。これにより、通過帯域の高周波端と低周波端の周波数温度係数を独立に設定できる。 According to the fourth modification of the first embodiment, the temperature coefficient of the elastic constant of the insulating layer 11s in the region 52 is different from the temperature coefficient of the elastic constant of the insulating layer 11p in the region 50. This allows the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband to be set independently.

領域52における絶縁層11sの弾性定数の温度係数は領域50における絶縁層11pの弾性定数の温度係数と同じ符号でありかつ絶対値が大きい。これにより、通過帯域の高周波端と低周波端の周波数温度係数をより近づけることができる。 The temperature coefficient of the elastic constant of the insulating layer 11s in region 52 has the same sign as the temperature coefficient of the elastic constant of the insulating layer 11p in region 50 and has a larger absolute value. This makes it possible to bring the frequency temperature coefficients of the high-frequency end and the low-frequency end of the passband closer together.

実施例1およびその変形例1から3において、領域50と52とで絶縁層11の弾性定数の温度係数を異ならせてもよい。領域52における絶縁層11の弾性定数の温度係数は領域50における絶縁層11の弾性定数の温度係数と同じ符号でありかつ絶対値が大きいことが好ましい。 In the first embodiment and its first to third modifications, the temperature coefficient of the elastic constant of the insulating layer 11 may be different between regions 50 and 52. It is preferable that the temperature coefficient of the elastic constant of the insulating layer 11 in region 52 has the same sign as the temperature coefficient of the elastic constant of the insulating layer 11 in region 50 and has a larger absolute value.

実施例1およびその変形例において、弾性表面波のエネルギーは圧電基板12の表面と表面から2λ程度の深さとの間に主に存在する。そこで、領域50および52における圧電基板の平均厚さT2pおよびT2sを、電極指15の平均ピッチの2倍以下とし、領域50および52における絶縁層11の平均厚さT1pおよびT1sを、電極指15の平均ピッチの2倍以下とする。これにより、弾性表面波のエネルギーが圧電基板12および絶縁層11の両方に分布する。よって、圧電基板12および絶縁層11の厚さを設定することでTCFを設定できる。T2p、T2s、T1pおよびT1sは、電極指15の平均ピッチの1.5倍以下が好ましく、1.2倍以下がより好ましい。T2p、T2s、T1pおよびT1sは、電極指15の平均ピッチの0.2倍以上が好ましい。 In the first embodiment and its modified example, the energy of the surface acoustic wave is mainly present between the surface of the piezoelectric substrate 12 and a depth of about 2λ from the surface. Therefore, the average thicknesses T2p and T2s of the piezoelectric substrate in the regions 50 and 52 are set to be less than twice the average pitch of the electrode fingers 15, and the average thicknesses T1p and T1s of the insulating layer 11 in the regions 50 and 52 are set to be less than twice the average pitch of the electrode fingers 15. This distributes the energy of the surface acoustic wave to both the piezoelectric substrate 12 and the insulating layer 11. Therefore, the TCF can be set by setting the thicknesses of the piezoelectric substrate 12 and the insulating layer 11. T2p, T2s, T1p, and T1s are preferably 1.5 times or less, more preferably 1.2 times or less, of the average pitch of the electrode fingers 15. T2p, T2s, T1p, and T1s are preferably 0.2 times or more of the average pitch of the electrode fingers 15.

IDT22がSH(Shear Horizontal)を励振するとき、バルク波が生成されやすい。圧電基板12が36°以上かつ48°以下回転Yカットタンタル酸リチウム基板のとき、SH波が励振される。このとき、圧電基板12の厚さが弾性波の波長λ以下のとき、すなわち電極指15のピッチの平均値に2倍以下のとき、損失が抑制される。また、支持基板10の上面から圧電基板12の上面までの距離が電極指15のピッチの平均値に4倍以下のとき、損失が抑制される。 When the IDT 22 excites SH (Shear Horizontal), bulk waves are likely to be generated. When the piezoelectric substrate 12 is a Y-cut lithium tantalate substrate rotated 36° or more and 48° or less, SH waves are excited. At this time, when the thickness of the piezoelectric substrate 12 is equal to or less than the wavelength λ of the elastic wave, that is, when it is equal to or less than twice the average pitch of the electrode fingers 15, loss is suppressed. In addition, when the distance from the top surface of the support substrate 10 to the top surface of the piezoelectric substrate 12 is equal to or less than four times the average pitch of the electrode fingers 15, loss is suppressed.

弾性波が支持基板10に漏れないように、支持基板10の音響インピーダンスは圧電基板12の音響インピーダンスより高い(すなわち支持基板10の音速は圧電基板12の音速より速い)ことが好ましい。また、絶縁層11内に弾性波が伝搬するため絶縁層11の音響インピーダンスは圧電基板12および支持基板10の音響インピーダンスより低い(すなわち絶縁層11の音速は圧電基板12および支持基板10の音速より遅い)ことは好ましい。図3(a)の接合層13としては、酸化アルミニウム、窒化アルミニウムまたは窒化シリコンを用いることができる。接合層13の厚さは1nm以上かつ10nm以下である。 To prevent the elastic wave from leaking to the support substrate 10, it is preferable that the acoustic impedance of the support substrate 10 is higher than that of the piezoelectric substrate 12 (i.e., the sound velocity of the support substrate 10 is faster than that of the piezoelectric substrate 12). In addition, since the elastic wave propagates within the insulating layer 11, it is preferable that the acoustic impedance of the insulating layer 11 is lower than that of the piezoelectric substrate 12 and the support substrate 10 (i.e., the sound velocity of the insulating layer 11 is slower than that of the piezoelectric substrate 12 and the support substrate 10). Aluminum oxide, aluminum nitride, or silicon nitride can be used as the bonding layer 13 in FIG. 3(a). The thickness of the bonding layer 13 is 1 nm or more and 10 nm or less.

図9は、実施例2に係るデュプレクサの回路図である。図9に示すように、共通端子Antと送信端子Txとの間に送信フィルタ40が接続されている。共通端子Antと受信端子Rxとの間に受信フィルタ42が接続されている。送信フィルタ40は、送信端子Txから入力された高周波信号のうち送信帯域の信号を送信信号として共通端子Antに通過させ、他の周波数の信号を抑圧する。受信フィルタ42は、共通端子Antから入力された高周波信号のうち受信帯域の信号を受信信号として受信端子Rxに通過させ、他の周波数の信号を抑圧する。送信フィルタ40および受信フィルタ42の少なくとも一方を実施例1およびその変形例のフィルタとすることができる。 Figure 9 is a circuit diagram of a duplexer according to the second embodiment. As shown in Figure 9, a transmission filter 40 is connected between the common terminal Ant and the transmission terminal Tx. A reception filter 42 is connected between the common terminal Ant and the reception terminal Rx. The transmission filter 40 passes a signal in the transmission band among the high-frequency signals input from the transmission terminal Tx to the common terminal Ant as a transmission signal, and suppresses signals of other frequencies. The reception filter 42 passes a signal in the reception band among the high-frequency signals input from the common terminal Ant to the reception terminal Rx as a reception signal, and suppresses signals of other frequencies. At least one of the transmission filter 40 and the reception filter 42 can be a filter according to the first embodiment and its modified examples.

マルチプレクサとしてデュプレクサを例に説明したがトリプレクサまたはクワッドプレクサでもよい。 Although a duplexer has been used as an example of a multiplexer, a triplexer or quadplexer may also be used.

以上、本発明の実施例について詳述したが、本発明はかかる特定の実施例に限定されるものではなく、特許請求の範囲に記載された本発明の要旨の範囲内において、種々の変形・変更が可能である。 Although the embodiments of the present invention have been described in detail above, the present invention is not limited to these specific embodiments, and various modifications and variations are possible within the scope of the gist of the present invention as described in the claims.

10 支持基板
11、11p、11s 絶縁層
12 圧電基板
13 接合層
15 電極指
18 櫛型電極
20 弾性波共振器
22 IDT
50、52 領域
REFERENCE SIGNS LIST 10 Support substrate 11, 11p, 11s Insulating layer 12 Piezoelectric substrate 13 Bonding layer 15 Electrode finger 18 Interdigital electrode 20 Acoustic wave resonator 22 IDT
50, 52 Area

Claims (9)

支持基板と、
前記支持基板上に直接または間接的に接合され、第1領域における平均厚さは第2領域における平均厚さより大きく、酸化シリコンを主成分とする絶縁層と、
前記絶縁層上に直接または間接的に接合され、弾性定数の温度係数の符号が前記絶縁層の弾性定数の温度係数の符号と反対であり、タンタル酸リチウム基板である圧電基板と、
前記第1領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、第1端子と第2端子との間に直列に接続された、ラダー型フィルタを形成する直列共振器と、
前記第2領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、前記第1端子と前記第2端子との間における前記直列共振器が設けられた線路に一端が接続され、他端がグランドに接続された、前記ラダー型フィルタを形成する並列共振器と、
を備え、
前記並列共振器のうち少なくとも1つの並列共振器の一端は、前記直列共振器のうち2つの直列共振器の間における前記線路に接続され、
前記第1領域および前記第2領域における前記圧電基板の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であり、前記第1領域および前記第2領域における前記絶縁層の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であるラダー型フィルタ。
A support substrate;
an insulating layer that is directly or indirectly bonded to the support substrate, the insulating layer having an average thickness in a first region greater than an average thickness in a second region, and that is mainly composed of silicon oxide;
a piezoelectric substrate that is directly or indirectly bonded onto the insulating layer, the piezoelectric substrate having a temperature coefficient of elastic constant that is opposite in sign to the temperature coefficient of elastic constant of the insulating layer, the piezoelectric substrate being a lithium tantalate substrate;
a series resonator that is provided on the piezoelectric substrate in the first region, has a pair of comb-shaped electrodes, and is connected in series between a first terminal and a second terminal to form a ladder-type filter ;
a parallel resonator forming the ladder-type filter, the parallel resonator having a pair of comb-shaped electrodes and one end connected to a line on which the series resonator is provided between the first terminal and the second terminal and the other end connected to ground , the parallel resonator being provided on the piezoelectric substrate in the second region ;
Equipped with
one end of at least one of the parallel resonators is connected to the line between two of the series resonators;
A ladder-type filter, wherein a thickness of the piezoelectric substrate in the first region and the second region is less than or equal to twice the average pitch of the electrode fingers of the pair of comb electrodes, and a thickness of the insulating layer in the first region and the second region is less than or equal to twice the average pitch of the electrode fingers of the pair of comb electrodes.
前記第1領域における前記圧電基板の平均厚さは、前記第2領域における前記圧電基板の平均厚さより小さい請求項1に記載のラダー型フィルタ。 2. The ladder-type filter according to claim 1, wherein an average thickness of the piezoelectric substrate in the first region is smaller than an average thickness of the piezoelectric substrate in the second region. 前記第1領域における前記圧電基板の平均厚さと前記第2領域における前記圧電基板の平均厚さは等しい請求項1に記載のラダー型フィルタ。 2. The ladder-type filter according to claim 1, wherein an average thickness of the piezoelectric substrate in the first region is equal to an average thickness of the piezoelectric substrate in the second region. 支持基板と、
前記支持基板上に直接または間接的に接合され、酸化シリコンを主成分とする絶縁層と、
前記絶縁層上に直接または間接的に接合され、第1領域における平均厚さは第2領域における平均厚さより小さく、弾性定数の温度係数の符号が前記絶縁層の弾性定数の温度係数の符号と反対であり、タンタル酸リチウム基板である圧電基板と、
前記第1領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、第1端子と第2端子との間に直列に接続された、ラダー型フィルタを形成する直列共振器と、
前記第2領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、前記第1端子と前記第2端子との間における前記直列共振器が設けられた線路に一端が接続され、他端がグランドに接続された、前記ラダー型フィルタを形成する並列共振器と、
を備え、
前記並列共振器のうち少なくとも1つの並列共振器の一端は、前記直列共振器のうち2つの直列共振器の間における前記線路に接続され、
前記第1領域および前記第2領域における前記圧電基板の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であり、前記第1領域および前記第2領域における前記絶縁層の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であるラダー型フィルタ。
A support substrate;
an insulating layer that is directly or indirectly bonded to the support substrate and is mainly composed of silicon oxide;
a piezoelectric substrate bonded directly or indirectly onto the insulating layer, the piezoelectric substrate having an average thickness in a first region smaller than an average thickness in a second region, a temperature coefficient of elastic constant having a sign opposite to that of the insulating layer, the piezoelectric substrate being a lithium tantalate substrate;
a series resonator that is provided on the piezoelectric substrate in the first region, has a pair of comb-shaped electrodes, and is connected in series between a first terminal and a second terminal to form a ladder-type filter ;
a parallel resonator forming the ladder-type filter, the parallel resonator having a pair of comb-shaped electrodes and one end connected to a line on which the series resonator is provided between the first terminal and the second terminal and the other end connected to ground , the parallel resonator being provided on the piezoelectric substrate in the second region ;
Equipped with
one end of at least one of the parallel resonators is connected to the line between two of the series resonators;
A ladder-type filter, wherein a thickness of the piezoelectric substrate in the first region and the second region is less than or equal to twice the average pitch of the electrode fingers of the pair of comb electrodes, and a thickness of the insulating layer in the first region and the second region is less than or equal to twice the average pitch of the electrode fingers of the pair of comb electrodes.
前記第1領域における前記絶縁層の平均厚さと前記第2領域における前記絶縁層の平均厚さとは等しい請求項4に記載のラダー型フィルタ。 5. The ladder-type filter according to claim 4, wherein an average thickness of the insulating layer in the first region is equal to an average thickness of the insulating layer in the second region. 支持基板と、
前記支持基板上に直接または間接的に接合され、第1領域における弾性定数の温度係数は第2領域における弾性定数の温度係数と同じ符号でありかつ絶対値が大きく、酸化シリコンを主成分とする絶縁層と、
前記絶縁層上に直接または間接的に接合され、弾性定数の温度係数の符号が前記絶縁層の弾性定数の温度係数の符号と反対であり、タンタル酸リチウム基板である圧電基板と、
前記第1領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、第1端子と第2端子との間に直列に接続された、ラダー型フィルタを形成する直列共振器と、
前記第2領域における前記圧電基板上に設けられ、一対の櫛型電極を有し、前記第1端子と前記第2端子との間に並列に接続された、前記ラダー型フィルタを形成する並列共振器と、
を備え、
前記第1領域および前記第2領域における前記圧電基板の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であり、前記第1領域および前記第2領域における前記絶縁層の厚さは、前記一対の櫛型電極の電極指の平均ピッチの2倍以下であるラダー型フィルタ。
A support substrate;
an insulating layer that is directly or indirectly bonded to the support substrate, the temperature coefficient of elastic constant in the first region having the same sign as the temperature coefficient of elastic constant in the second region and a larger absolute value, and that is mainly composed of silicon oxide;
a piezoelectric substrate that is directly or indirectly bonded onto the insulating layer, the piezoelectric substrate having a temperature coefficient of elastic constant that is opposite in sign to the temperature coefficient of elastic constant of the insulating layer, the piezoelectric substrate being a lithium tantalate substrate;
a series resonator that is provided on the piezoelectric substrate in the first region, has a pair of comb-shaped electrodes, and is connected in series between a first terminal and a second terminal to form a ladder-type filter ;
a parallel resonator forming the ladder filter, the parallel resonator being provided on the piezoelectric substrate in the second region, the parallel resonator having a pair of comb-shaped electrodes and connected in parallel between the first terminal and the second terminal;
Equipped with
A ladder-type filter, wherein a thickness of the piezoelectric substrate in the first region and the second region is less than or equal to twice the average pitch of the electrode fingers of the pair of comb electrodes, and a thickness of the insulating layer in the first region and the second region is less than or equal to twice the average pitch of the electrode fingers of the pair of comb electrodes.
前記第1領域における前記絶縁層の平均厚さと前記第2領域における前記絶縁層の平均厚さとは等しく、
前記第1領域における前記圧電基板の平均厚さと前記第2領域における前記圧電基板の平均厚さは等しい請求項6に記載のラダー型フィルタ。
an average thickness of the insulating layer in the first region and an average thickness of the insulating layer in the second region are equal;
7. The ladder-type filter according to claim 6, wherein an average thickness of the piezoelectric substrate in the first region is equal to an average thickness of the piezoelectric substrate in the second region.
前記ラダー型フィルタは、前記直列共振器および前記並列共振器以外の共振器を有さないラダー型フィルタである請求項1から7のいずれか一項に記載のラダー型フィルタ。 8. The ladder-type filter according to claim 1, wherein the ladder-type filter does not include any resonator other than the series resonator and the parallel resonator. 請求項1から8のいずれか一項に記載のラダー型フィルタを含むマルチプレクサ。 A multiplexer comprising the ladder filter according to any one of claims 1 to 8.
JP2019084531A 2019-04-25 2019-04-25 Ladder Filters and Multiplexers Active JP7624796B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2019084531A JP7624796B2 (en) 2019-04-25 2019-04-25 Ladder Filters and Multiplexers

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2019084531A JP7624796B2 (en) 2019-04-25 2019-04-25 Ladder Filters and Multiplexers

Publications (2)

Publication Number Publication Date
JP2020182130A JP2020182130A (en) 2020-11-05
JP7624796B2 true JP7624796B2 (en) 2025-01-31

Family

ID=73023541

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2019084531A Active JP7624796B2 (en) 2019-04-25 2019-04-25 Ladder Filters and Multiplexers

Country Status (1)

Country Link
JP (1) JP7624796B2 (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20230412142A1 (en) * 2020-11-16 2023-12-21 Qorvo Us, Inc. Piezoelectric layer arrangements in acoustic wave devices and related methods
WO2022220155A1 (en) 2021-04-16 2022-10-20 株式会社村田製作所 Elastic wave device
US12244300B2 (en) * 2021-05-17 2025-03-04 Taiyo Yuden Co., Ltd. Ladder-type filter and multiplexer
CN216390939U (en) * 2021-10-28 2022-04-26 深圳飞骧科技股份有限公司 XBAR filter
CN116073791B (en) * 2023-02-15 2025-11-07 上海馨欧集成微电有限公司 Longitudinally leaking surface acoustic wave filter

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009022410A1 (en) 2007-08-14 2009-02-19 Fujitsu Limited Elastic boundary wave device
WO2012086639A1 (en) 2010-12-24 2012-06-28 株式会社村田製作所 Elastic wave device and production method thereof

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008078739A (en) * 2006-09-19 2008-04-03 Fujitsu Media Device Kk Elastic wave device and filter
FR2947398B1 (en) * 2009-06-30 2013-07-05 Commissariat Energie Atomique DEVICE RESONANT TO GUIDED ACOUSTIC WAVES AND METHOD OF MAKING THE DEVICE
JP6497018B2 (en) * 2014-09-30 2019-04-10 株式会社村田製作所 Duplexer and manufacturing method thereof
JP6494545B2 (en) * 2016-02-23 2019-04-03 太陽誘電株式会社 Duplexer
JP6748010B2 (en) * 2017-03-21 2020-08-26 太陽誘電株式会社 Method of manufacturing acoustic wave device

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009022410A1 (en) 2007-08-14 2009-02-19 Fujitsu Limited Elastic boundary wave device
WO2012086639A1 (en) 2010-12-24 2012-06-28 株式会社村田製作所 Elastic wave device and production method thereof

Also Published As

Publication number Publication date
JP2020182130A (en) 2020-11-05

Similar Documents

Publication Publication Date Title
JP7624796B2 (en) Ladder Filters and Multiplexers
JP4419961B2 (en) Boundary acoustic wave device
JP4894911B2 (en) Boundary acoustic wave filter
JP7433873B2 (en) Acoustic wave resonators, filters, and multiplexers
WO2018168836A1 (en) Acoustic wave element, acoustic wave filter device, and multiplexer
US6933810B2 (en) Surface acoustic wave device with lithium tantalate on a sapphire substrate and filter using the same
CN115360994B (en) Trapezoidal filters and multiplexers
US11569433B2 (en) Acoustic wave resonator, filter, and multiplexer
JP2004343168A (en) Filter device and duplexer using the same
CN114070257B (en) Acoustic wave devices, filters and multiplexers
JP2019201345A (en) Acoustic wave resonator, filter and multiplexer
JP7656487B2 (en) Ladder Filters and Multiplexers
US12476616B2 (en) Filter and multiplexer
US12249973B2 (en) Acoustic wave device, filter, and multiplexer
JP2023124332A (en) Acoustic wave devices, filters and multiplexers
US20250175141A1 (en) Acoustic wave device
JP7188412B2 (en) Acoustic wave device and composite filter device
CN120074419A (en) Elastic wave device, filter, multiplexer and wafer
US20240162881A1 (en) Acoustic wave device, filter, and multiplexer
JP7657515B2 (en) Ladder Filters and Multiplexers
CN118202573A (en) Filter device
JP7484045B2 (en) Filters and Multiplexers
JP7713805B2 (en) Acoustic Wave Devices, Filters and Multiplexers
US12615029B2 (en) Acoustic wave device, filter, multiplexer, and wafer
JP2025006298A (en) Acoustic Wave Devices, Filters, and Multiplexers

Legal Events

Date Code Title Description
A621 Written request for application examination

Free format text: JAPANESE INTERMEDIATE CODE: A621

Effective date: 20220323

A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20230315

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20230411

A521 Request for written amendment filed

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20230607

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20230912

A521 Request for written amendment filed

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20231110

A02 Decision of refusal

Free format text: JAPANESE INTERMEDIATE CODE: A02

Effective date: 20240206

A521 Request for written amendment filed

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20240501

A911 Transfer to examiner for re-examination before appeal (zenchi)

Free format text: JAPANESE INTERMEDIATE CODE: A911

Effective date: 20240510

A912 Re-examination (zenchi) completed and case transferred to appeal board

Free format text: JAPANESE INTERMEDIATE CODE: A912

Effective date: 20240816

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20250121

R150 Certificate of patent or registration of utility model

Ref document number: 7624796

Country of ref document: JP

Free format text: JAPANESE INTERMEDIATE CODE: R150