WO2023190697A1 - Elastic wave device - Google Patents

Elastic wave device Download PDF

Info

Publication number
WO2023190697A1
WO2023190697A1 PCT/JP2023/012836 JP2023012836W WO2023190697A1 WO 2023190697 A1 WO2023190697 A1 WO 2023190697A1 JP 2023012836 W JP2023012836 W JP 2023012836W WO 2023190697 A1 WO2023190697 A1 WO 2023190697A1
Authority
WO
WIPO (PCT)
Prior art keywords
piezoelectric layer
electrodes
electrode
wave device
elastic wave
Prior art date
Application number
PCT/JP2023/012836
Other languages
French (fr)
Japanese (ja)
Inventor
和則 井上
勝己 鈴木
Original Assignee
株式会社村田製作所
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 株式会社村田製作所 filed Critical 株式会社村田製作所
Publication of WO2023190697A1 publication Critical patent/WO2023190697A1/en

Links

Images

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/15Constructional features of resonators consisting of piezoelectric or electrostrictive material
    • H03H9/17Constructional features of resonators consisting of piezoelectric or electrostrictive material having a single resonator
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/25Constructional features of resonators using surface acoustic waves

Definitions

  • the present invention relates to an elastic wave device.
  • acoustic wave devices including a piezoelectric layer made of lithium niobate or lithium tantalate are known.
  • Patent Document 1 discloses a support in which a cavity is formed, a piezoelectric substrate provided on the support so as to overlap with the cavity, and a piezoelectric substrate provided on the piezoelectric substrate so as to overlap with the cavity.
  • An acoustic wave device is provided with an IDT (Interdigital Transducer) electrode provided, and a plate wave is excited by the IDT electrode, wherein an edge of the cavity portion is provided with a plate wave excited by the IDT electrode.
  • An elastic wave device is disclosed that does not include a straight portion extending parallel to the propagation direction of the wave.
  • Patent Document 2 discloses a supporting member having a recessed portion on its upper surface, and a supporting member having an upper surface and a lower surface, and is provided on the supporting member so as to cover the recessed portion of the supporting member, and the supporting member is provided with a recessed portion of the supporting member.
  • a piezoelectric thin film having a portion located in a hollow space, and an IDT electrode provided on the upper surface of the piezoelectric thin film and having a plurality of electrode fingers, the plate is in S0 mode or SHO mode. It utilizes waves, and is provided on the upper surface or the lower surface of the piezoelectric thin film in a portion of the piezoelectric thin film located above the hollow space, and extends in the direction in which the electrode fingers of the IDT electrode extend.
  • An elastic wave device is disclosed in which a plurality of grooves are provided.
  • Patent Document 1 describes an example of a method for forming a cavity, in which a piezoelectric substrate is formed with a frame made of a thin film made of SiO 2 , SiN, etc. on a piezoelectric body, and a support substrate is arranged under the frame. The method is described.
  • Patent Document 2 describes that after forming a sacrificial layer on a piezoelectric substrate, a supporting layer is provided to cover the sacrificial layer, and then a supporting substrate is bonded to the supporting layer. Further, Patent Document 2 describes that a piezoelectric substrate is made thinner to form a piezoelectric thin film, that an etching hole is formed in the piezoelectric thin film, and that a sacrificial layer is removed from the etching hole by wet etching. . This creates a hollow space within the support layer.
  • An object of the present invention is to provide an elastic wave device whose element size can be reduced.
  • the elastic wave device of the present invention includes a support member having a cavity on one main surface, a piezoelectric layer provided on the one main surface of the support member so as to cover the cavity, and at least one of the piezoelectric layers.
  • a functional electrode is provided on the main surface so that at least a portion thereof overlaps with the cavity when viewed from the thickness direction of the piezoelectric layer.
  • the piezoelectric layer has a width smaller than the thickness of the piezoelectric layer in a region that overlaps with the cavity and is not provided with the functional electrode when viewed from the thickness direction, and one main surface of the piezoelectric layer.
  • a crack is provided that communicates from one main surface to the other main surface.
  • FIG. 1 is a cross-sectional view schematically showing an example of the elastic wave device of the present invention.
  • FIG. 2 is a plan view schematically showing an example of the elastic wave device of the present invention.
  • FIG. 3 is a cross-sectional view schematically showing an example of the process of forming a sacrificial layer on a piezoelectric substrate.
  • FIG. 4 is a plan view schematically showing an example of the process of forming a sacrificial layer on a piezoelectric substrate.
  • FIG. 5 is a cross-sectional view schematically showing an example of the process of forming the intermediate layer.
  • FIG. 6 is a cross-sectional view schematically showing an example of the process of bonding the support substrate to the intermediate layer.
  • FIG. 1 is a cross-sectional view schematically showing an example of the elastic wave device of the present invention.
  • FIG. 2 is a plan view schematically showing an example of the elastic wave device of the present invention.
  • FIG. 3 is a cross-section
  • FIG. 7 is a cross-sectional view schematically showing an example of the process of thinning the piezoelectric substrate.
  • FIG. 8 is a cross-sectional view schematically showing an example of the process of forming a crack.
  • FIG. 9 is a cross-sectional view schematically showing an example of the process of forming functional electrodes and wiring electrodes.
  • FIG. 10 is a plan view schematically showing an example of the process of forming functional electrodes and wiring electrodes.
  • FIG. 11 is a cross-sectional view schematically showing an example of the process of removing the protective electrode and the sacrificial layer.
  • FIG. 12 is a cross-sectional view schematically showing an example of a state in which a protective resist for forming etching holes is provided.
  • FIG. 13 is a cross-sectional view schematically showing an example of a state during etching.
  • FIG. 14 is a side view schematically showing an example of the portion indicated by XIV in FIG. 13.
  • FIG. 15 is a side view schematically showing an example of a piezoelectric layer in a portion where a crack is provided.
  • FIG. 16 is a plan view schematically showing an example of a piezoelectric layer in a portion where a crack is provided.
  • FIG. 17 is a cross-sectional view schematically showing another example of the elastic wave device of the present invention.
  • FIG. 18 is a schematic perspective view showing the appearance of an example of an elastic wave device that utilizes bulk waves in thickness shear mode.
  • FIG. 19 is a plan view showing the electrode structure on the piezoelectric layer of the acoustic wave device shown in FIG. 18.
  • FIG. 20 is a cross-sectional view of a portion taken along line AA in FIG. 18.
  • FIG. 21 is a schematic front sectional view for explaining Lamb waves propagating through a piezoelectric film of an acoustic wave device.
  • FIG. 22 is a schematic front sectional view for explaining a thickness shear mode bulk wave propagating through a piezoelectric layer of an elastic wave device.
  • FIG. 23 is a diagram showing the amplitude direction of the bulk wave in the thickness shear mode.
  • FIG. 24 is a diagram showing an example of the resonance characteristics of the elastic wave device shown in FIG. 18.
  • FIG. 20 is a cross-sectional view of a portion taken along line AA in FIG. 18.
  • FIG. 21 is a schematic front sectional view for explaining Lamb waves propagating through a piezoelectric film of an acoustic wave device.
  • FIG. 25 is a diagram showing the relationship between d/2p and the fractional band as a resonator of an acoustic wave device, where p is the distance between the centers of adjacent electrodes and d is the thickness of the piezoelectric layer.
  • FIG. 26 is a plan view of another example of an elastic wave device that utilizes bulk waves in thickness shear mode.
  • FIG. 27 is a reference diagram showing an example of the resonance characteristics of the elastic wave device shown in FIG. 18.
  • FIG. 28 is a diagram showing the relationship between the fractional band and the amount of phase rotation of spurious impedance normalized by 180 degrees as the magnitude of spurious when a large number of elastic wave resonators are configured according to the present embodiment. It is.
  • FIG. 29 is a diagram showing the relationship between d/2p, metallization ratio MR, and fractional band.
  • FIG. 30 is a diagram showing a map of fractional bands with respect to Euler angles (0°, ⁇ , ⁇ ) of LiNbO 3 when d/p is brought as close to 0 as possible.
  • FIG. 31 is a partially cutaway perspective view for explaining an example of an elastic wave device that uses Lamb waves.
  • the acoustic wave device of the present invention includes a piezoelectric layer made of lithium niobate or lithium tantalate, a first electrode and a first electrode facing each other in a direction crossing the thickness direction of the piezoelectric layer. 2 electrodes.
  • a bulk wave in a thickness shear mode such as a primary thickness shear mode is used.
  • the first electrode and the second electrode are adjacent electrodes, and when the thickness of the piezoelectric layer is d and the distance between the centers of the first electrode and the second electrode is p, d/ p is set to be 0.5 or less.
  • the Q value can be increased even when miniaturization is promoted.
  • Lamb waves are used as plate waves. Then, resonance characteristics due to the Lamb wave described above can be obtained.
  • FIG. 1 is a cross-sectional view schematically showing an example of the elastic wave device of the present invention.
  • FIG. 2 is a plan view schematically showing an example of the elastic wave device of the present invention. Note that FIG. 1 is an example of a cross-sectional view of the elastic wave device shown in FIG. 2 taken along line II.
  • the elastic wave device 10 shown in FIGS. 1 and 2 includes a support member 20, a piezoelectric layer 21, and a functional electrode 22.
  • the support member 20 has a cavity 23 on one main surface (the upper main surface in FIG. 1).
  • the piezoelectric layer 21 is provided on one main surface of the support member 20 so as to cover the cavity 23.
  • the functional electrode 22 is provided on at least one main surface of the piezoelectric layer 21.
  • the functional electrode 22 is provided on one main surface (the upper main surface in FIG. 1) of the piezoelectric layer 21.
  • the functional electrode 22 is provided so that at least a portion thereof overlaps with the cavity 23 when viewed from the thickness direction of the piezoelectric layer 21 (Z direction in FIGS. 1 and 2).
  • the functional electrode 22 may be provided so that the entirety thereof overlaps with the cavity 23, or a part of the functional electrode 22 may be provided so as to overlap with the cavity 23. .
  • the piezoelectric layer 21 has a width smaller than the thickness of the piezoelectric layer 21 in a region that overlaps the cavity 23 and is not provided with the functional electrode 22 when viewed from the thickness direction, and has one main surface ( A crack 24 is provided that communicates from the upper main surface (in FIG. 1) to the other main surface (lower main surface in FIG. 1).
  • a crack 24 having a minute width is provided at the outer circumference of the membrane portion 21M, which is a part of the piezoelectric layer 21. Therefore, even if a cavity is formed by removing the sacrificial layer, for example, the etching solution for removing the sacrificial layer can enter the cracks 24, so there is no need to form etching holes. As a result, the element size can be reduced.
  • the portion of the piezoelectric layer located in the region overlapping with the cavity when viewed from the thickness direction is also referred to as a "membrane portion.”
  • the width of the crack 24 (the length indicated by W 24 in FIG. 1) is smaller than the thickness of the piezoelectric layer 21 (the length indicated by T 21 in FIG. 1).
  • the width of the crack 24 means the width in a cross section along the thickness direction.
  • the thickness of the piezoelectric layer 21 means the dimension in the thickness direction.
  • the length of the crack 24 (the length indicated by L24 in FIG. 2) is not particularly limited. Note that the length of the crack 24 means the dimension of the crack 24 in the extending direction.
  • the support member 20 may have an intermediate layer 41 (also referred to as an insulating layer or a bonding layer) on one main surface on which the piezoelectric layer 21 is provided.
  • the support member 20 includes a support substrate 42 and an intermediate layer 41 provided between the support substrate 42 and the piezoelectric layer 21.
  • the support substrate 42 is made of silicon (Si), for example.
  • the intermediate layer 41 is made of silicon oxide (SiO x ) such as silicon dioxide (SiO 2 ), for example.
  • the piezoelectric layer 21 is made of, for example, lithium niobate (LiNbO x ) or lithium tantalate (LiTaO x ). In that case, the piezoelectric layer 21 may be composed of LiNbO 3 or LiTaO 3 .
  • the functional electrode 22 is, for example, an IDT electrode provided on one main surface of the piezoelectric layer 21. Note that a wiring electrode 26 such as a two-layer wiring is connected to the functional electrode 22.
  • the elastic wave device of the present invention is manufactured, for example, by the following method.
  • FIG. 3 is a cross-sectional view schematically showing an example of the process of forming a sacrificial layer on a piezoelectric substrate.
  • FIG. 4 is a plan view schematically showing an example of the process of forming a sacrificial layer on a piezoelectric substrate.
  • an inorganic sacrificial layer 40A is formed on the piezoelectric substrate 31.
  • an organic sacrificial layer 40B is formed on the piezoelectric substrate 31.
  • an organic sacrificial layer 40B is formed on the short side of an inorganic sacrificial layer 40A.
  • the sacrificial layer 40 is formed on the piezoelectric substrate 31.
  • the piezoelectric substrate 31 for example, a substrate made of LiNbO 3 or LiTaO 3 is used.
  • the material for the inorganic sacrificial layer 40A an appropriate inorganic material that can be removed by etching, which will be described later, is used.
  • an appropriate inorganic material that can be removed by etching which will be described later, is used.
  • ZnO or the like is used.
  • the inorganic sacrificial layer 40A can be formed, for example, by the following method. First, a ZnO film is formed by sputtering. Thereafter, resist coating, exposure and development are performed in this order. Next, wet etching is performed to form a pattern of the inorganic sacrificial layer 40A. Note that the inorganic sacrificial layer 40A may be formed by other methods.
  • the material of the organic sacrificial layer 40B an appropriate resin material that can be deformed by heat treatment, which will be described later, is used.
  • FIG. 5 is a cross-sectional view schematically showing an example of the process of forming the intermediate layer.
  • the surface of the intermediate layer 41 is planarized.
  • the intermediate layer 41 for example, a SiO 2 film or the like is formed.
  • the intermediate layer 41 can be formed by, for example, a sputtering method.
  • the intermediate layer 41 can be planarized by, for example, chemical mechanical polishing (CMP).
  • FIG. 6 is a cross-sectional view schematically showing an example of the process of bonding the support substrate to the intermediate layer.
  • a support substrate 42 is bonded to the intermediate layer 41. Thereby, the support member 20 is formed.
  • FIG. 7 is a cross-sectional view schematically showing an example of the process of thinning the piezoelectric substrate.
  • the piezoelectric substrate 31 is thinned. As a result, the piezoelectric layer 21 is formed.
  • the piezoelectric substrate 31 can be thinned by, for example, a smart cut method, polishing, or the like.
  • FIG. 8 is a cross-sectional view schematically showing an example of the process of forming a crack.
  • Heat treatment is performed on the support member 20 on which the piezoelectric layer 21 is formed. Since the organic sacrificial layer 40B expands or contracts due to heat, the membrane portion 21M is deformed. As a result, as shown in FIG. 8, a crack 24 is formed on the short side of the sacrificial layer 40.
  • FIG. 9 is a cross-sectional view schematically showing an example of the process of forming functional electrodes and wiring electrodes.
  • FIG. 10 is a plan view schematically showing an example of the process of forming functional electrodes and wiring electrodes.
  • a functional electrode 22 and a wiring electrode 26 are formed on one main surface of the piezoelectric layer 21.
  • the functional electrode 22 and the wiring electrode 26 can be formed by, for example, a lift-off method.
  • a protective electrode 28 on the cracked portion in order to protect the crack during the process flow.
  • FIG. 11 is a cross-sectional view schematically showing an example of the process of removing the protective electrode and the sacrificial layer.
  • the protective electrode 28 is removed by a method such as etching.
  • the sacrificial layer 40 is removed using the cracks 24.
  • the organic sacrificial layer 40B and the inorganic sacrificial layer 40A are removed by a method such as etching.
  • a cavity 23 is formed in the support member 20.
  • the elastic wave device 10 is obtained.
  • the cracks 24 are formed in the piezoelectric layer 21 instead of forming etching holes for removing the sacrificial layer 40 in the piezoelectric layer 21, so the element size can be reduced.
  • FIG. 12 is a cross-sectional view schematically showing an example of a state in which a protective resist for forming etching holes is provided.
  • the areas other than those where etching holes are to be formed are covered with a protective resist 50.
  • FIG. 13 is a cross-sectional view schematically showing an example of a state during etching.
  • etching holes 51 in the piezoelectric layer 21 even dry etching does not require chemical reaction conditions, so it must be performed under ion milling conditions. Therefore, during etching, the protective resist 50 is also etched.
  • FIG. 14 is a side view schematically showing an example of the portion indicated by XIV in FIG. 13.
  • the protective resist 50 is also etched during dry etching. Therefore, as shown in FIG. 14, uniform vertical streaks 52 are generated along the thickness direction (Z direction) of the piezoelectric layer 21 on the side surface of the piezoelectric layer 21 in the portion where the etching hole 51 is formed.
  • FIG. 15 is a side view schematically showing an example of a piezoelectric layer in a portion where a crack is provided.
  • FIG. 16 is a plan view schematically showing an example of a piezoelectric layer in a portion where a crack is provided.
  • FIG. 15 shows the side surface of the piezoelectric layer 21
  • FIG. 16 shows the surface layer of the piezoelectric layer 21.
  • the piezoelectric layer 21 has cracks in the piezoelectric layer 21 in the thickness direction in addition to the cracks 24 in an area that overlaps the cavity 23 when viewed from the thickness direction of the piezoelectric layer 21 and is not provided with the functional electrode 22. It is preferable that no holes (for example, etching holes 51, etc.) passing through are provided. For example, it is preferable that uniform vertical stripes 52 along the thickness direction of the piezoelectric layer 21 do not exist on the side surfaces of the piezoelectric layer 21 .
  • the cracks 24 are preferably provided in a region that overlaps with the outer peripheral edge of the cavity 23, as shown in FIG. In this case, the element area can be minimized.
  • the crack 24 is preferably provided only in a region that overlaps with the outer periphery of the cavity 23, and more preferably only in a part of the region that overlaps with the outer periphery of the cavity 23.
  • the cracks 24 are not provided in a region overlapping with the functional electrode 22 that straddles the outer peripheral edge of the cavity 23, as shown in FIG. In this case, the influence on the function of the element can be reduced.
  • the number, shape, size, etc. of the cracks 24 are not particularly limited. When a plurality of cracks 24 are provided, the shape, size, etc. of the cracks 24 viewed from the thickness direction of the piezoelectric layer 21 may be the same, or may be partially or completely different.
  • the method for forming the crack 24 is not limited to the method using the sacrificial layer 40.
  • the cavity 23 does not need to penetrate the support member 20 in the thickness direction, but may do so.
  • the cavity 23 may be provided so as to penetrate the intermediate layer 41 in the thickness direction, or may be provided so as not to penetrate the intermediate layer 41 in the thickness direction.
  • a cavity 23 may be provided therein.
  • FIG. 17 is a cross-sectional view schematically showing another example of the elastic wave device of the present invention.
  • the cavity 23 may penetrate the support member 20 in the thickness direction.
  • the support member 20 includes an intermediate layer 41 and a support substrate 42 .
  • a method for forming the membrane portion 21M of the piezoelectric layer 21 having the functional electrode 22 is, for example, using a bonded substrate in which a piezoelectric substrate is bonded to a support substrate via an intermediate layer.
  • Examples include a method in which a layer including functional electrodes and wiring electrodes is formed in advance by a method such as lift-off, and then the support substrate on the back surface of the portion corresponding to the membrane portion 21M is removed, and then the intermediate layer is removed.
  • FIG. 18 is a schematic perspective view showing the appearance of an example of an elastic wave device that utilizes bulk waves in thickness shear mode.
  • FIG. 19 is a plan view showing the electrode structure on the piezoelectric layer of the acoustic wave device shown in FIG. 18.
  • FIG. 20 is a cross-sectional view of a portion taken along line AA in FIG. 18.
  • the acoustic wave device 1 has a piezoelectric layer 2 made of, for example, LiNbO 3 .
  • the piezoelectric layer 2 may be made of LiTaO 3 .
  • the cut angle of LiNbO 3 or LiTaO 3 is, for example, a Z cut, but may also be a rotational Y cut or an X cut.
  • the propagation directions of Y propagation and X propagation are ⁇ 30°.
  • the thickness of the piezoelectric layer 2 is not particularly limited, but in order to effectively excite the thickness shear mode, it is preferably 50 nm or more and 1000 nm or less.
  • the piezoelectric layer 2 has a first main surface 2a and a second main surface 2b that face each other.
  • Electrode 3 and an electrode 4 are provided on the first main surface 2a of the piezoelectric layer 2, on the first main surface 2a of the piezoelectric layer 2, an electrode 3 and an electrode 4 are provided.
  • electrode 3 is an example of a "first electrode”
  • electrode 4 is an example of a "second electrode”.
  • the plurality of electrodes 3 are the plurality of first electrode fingers connected to the first busbar electrode 5.
  • the plurality of electrodes 4 are a plurality of second electrode fingers connected to the second busbar electrode 6.
  • the plurality of electrodes 3 and the plurality of electrodes 4 are interposed with each other. Electrode 3 and electrode 4 have a rectangular shape and have a length direction.
  • the electrode 3 and the adjacent electrode 4 face each other in a direction perpendicular to this length direction.
  • Electrodes 3 and 4 constitute an IDT (Interdigital Transducer) electrode.
  • the length direction of the electrodes 3 and 4 and the direction perpendicular to the length direction of the electrodes 3 and 4 are both directions that intersect the thickness direction of the piezoelectric layer 2. Therefore, it can be said that the electrode 3 and the adjacent electrode 4 face each other in the direction intersecting the thickness direction of the piezoelectric layer 2. Further, the length direction of the electrodes 3 and 4 may be replaced with the direction perpendicular to the length direction of the electrodes 3 and 4 shown in FIGS. 18 and 19. That is, in FIGS.
  • the electrodes 3 and 4 may be extended in the direction in which the first busbar electrode 5 and the second busbar electrode 6 are extended. In that case, the first busbar electrode 5 and the second busbar electrode 6 will extend in the direction in which the electrodes 3 and 4 extend in FIGS. 18 and 19.
  • a plurality of pairs of structures in which an electrode 3 connected to one potential and an electrode 4 connected to the other potential are adjacent to each other are provided in a direction perpendicular to the length direction of the electrodes 3 and 4.
  • the expression “electrode 3 and electrode 4 are adjacent” does not mean that electrode 3 and electrode 4 are arranged so as to be in direct contact with each other, but when electrode 3 and electrode 4 are arranged with a gap between them.
  • the center-to-center distance between the electrodes 3 and 4, that is, the pitch, is preferably in the range of 1 ⁇ m or more and 10 ⁇ m or less. Note that the center-to-center distance between the electrodes 3 and 4 refers to the center of the width dimension of the electrode 3 in the direction orthogonal to the length direction of the electrode 3, and the width dimension of the electrode 4 in the direction orthogonal to the length direction of the electrode 4.
  • the distance between the center of refers to the average value of the distance between the centers of adjacent electrodes 3 and 4 among 1.5 or more pairs of electrodes 3 and 4.
  • the width of the electrodes 3 and 4, that is, the dimension in the opposing direction of the electrodes 3 and 4 is preferably in the range of 150 nm or more and 1000 nm or less.
  • the direction perpendicular to the length direction of the electrodes 3 and 4 is the direction perpendicular to the polarization direction of the piezoelectric layer 2.
  • “orthogonal” is not limited to strictly orthogonal, but approximately orthogonal (for example, the angle between the direction orthogonal to the length direction of the electrodes 3 and 4 and the polarization direction is 90° ⁇ 10°) But that's fine.
  • a support substrate 8 is laminated on the second main surface 2b side of the piezoelectric layer 2 with an intermediate layer (also called a bonding layer) 7 interposed therebetween.
  • the intermediate layer 7 and the support substrate 8 have a frame-like shape, and have openings 7a and 8a, as shown in FIG. Thereby, a cavity 9 is formed.
  • the cavity 9 is provided so as not to hinder the vibration of the excitation region C (see FIG. 19) of the piezoelectric layer 2. Therefore, the support substrate 8 is laminated on the second main surface 2b with the intermediate layer 7 interposed therebetween at a position that does not overlap with the portion where at least one pair of electrodes 3 and 4 are provided. Note that the intermediate layer 7 may not be provided. Therefore, the support substrate 8 can be laminated directly or indirectly on the second main surface 2b of the piezoelectric layer 2.
  • the intermediate layer 7 is made of silicon oxide, for example. However, other than silicon oxide, an appropriate insulating material such as silicon oxynitride or alumina can be used.
  • the support substrate 8 is made of Si. The plane orientation of the Si surface on the piezoelectric layer 2 side may be (100), (110), or (111). Preferably, Si has a high resistivity of 4 k ⁇ or more. However, the support substrate 8 can also be constructed using an appropriate insulating material or semiconductor material.
  • Examples of materials for the support substrate 8 include aluminum oxide, lithium tantalate, lithium niobate, piezoelectric materials such as crystal, alumina, magnesia, sapphire, silicon nitride, aluminum nitride, silicon carbide, zirconia, cordierite, mullite, and starch.
  • Various ceramics such as tite and forsterite, dielectrics such as diamond and glass, semiconductors such as gallium nitride, etc. can be used.
  • an AC voltage is applied between the plurality of electrodes 3 and the plurality of electrodes 4. More specifically, an AC voltage is applied between the first busbar electrode 5 and the second busbar electrode 6.
  • d/p is 0. It is considered to be 5 or less. Therefore, the bulk wave in the thickness shear mode is effectively excited, and good resonance characteristics can be obtained. More preferably, d/p is 0.24 or less, in which case even better resonance characteristics can be obtained.
  • the distance p between the centers of the adjacent electrodes 3 and 4 is the average distance between the centers of the adjacent electrodes 3 and 4.
  • the elastic wave device 1 of this embodiment has the above configuration, even if the logarithm of the electrodes 3 and 4 is reduced in an attempt to achieve miniaturization, the Q value is unlikely to decrease. This is because the resonator does not require reflectors on both sides and has little propagation loss. Further, the reason why the reflector is not required is because the bulk wave in the thickness shear mode is used. The difference between the Lamb wave used in a conventional elastic wave device and the thickness-shear mode bulk wave will be explained with reference to FIGS. 21 and 22.
  • FIG. 21 is a schematic front sectional view for explaining Lamb waves propagating through a piezoelectric film of an acoustic wave device.
  • the elastic wave device described in Patent Document 1 Japanese Patent Publication No. 2012-257019
  • waves propagate in the piezoelectric film 201 as indicated by arrows.
  • the first main surface 201a and the second main surface 201b are opposite to each other, and the thickness direction connecting the first main surface 201a and the second main surface 201b is the Z direction. It is.
  • the X direction is the direction in which the electrode fingers of the IDT electrodes are lined up.
  • the Lamb wave the wave propagates in the X direction as shown.
  • the piezoelectric film 201 vibrates as a whole, but since the wave propagates in the X direction, reflectors are placed on both sides to obtain resonance characteristics. Therefore, wave propagation loss occurs, and when miniaturization is attempted, that is, when the number of logarithms of electrode fingers is reduced, the Q value decreases.
  • FIG. 22 is a schematic front cross-sectional view for explaining a thickness-shear mode bulk wave propagating through a piezoelectric layer of an elastic wave device.
  • the waves connect the first main surface 2a and the second main surface 2b of the piezoelectric layer 2. It propagates almost in the Z direction, and resonates. That is, the X-direction component of the wave is significantly smaller than the Z-direction component. Since resonance characteristics are obtained by the propagation of waves in the Z direction, a reflector is not required. Therefore, no propagation loss occurs when propagating to the reflector. Therefore, even if the number of electrode pairs consisting of electrodes 3 and 4 is reduced in an attempt to promote miniaturization, the Q value is unlikely to decrease.
  • FIG. 23 is a diagram showing the amplitude direction of the bulk wave in the thickness shear mode. As shown in FIG. 23, the amplitude direction of the bulk wave in the thickness shear mode is opposite between the first region 451 included in the excitation region C of the piezoelectric layer 2 and the second region 452 included in the excitation region C.
  • FIG. 23 schematically shows a bulk wave when a voltage is applied between electrode 3 and electrode 4 such that electrode 4 has a higher potential than electrode 3.
  • the first region 451 is a region of the excitation region C between a virtual plane VP1 that is perpendicular to the thickness direction of the piezoelectric layer 2 and bisects the piezoelectric layer 2, and the first main surface 2a.
  • the second region 452 is a region of the excitation region C between the virtual plane VP1 and the second principal surface 2b.
  • the elastic wave device 1 As mentioned above, in the elastic wave device 1, at least one pair of electrodes consisting of the electrode 3 and the electrode 4 are arranged, but since the wave is not propagated in the X direction, the elastic wave device 1 is made up of the electrodes 3 and 4. There does not necessarily have to be a plurality of pairs of electrodes. That is, it is only necessary that at least one pair of electrodes be provided.
  • the electrode 3 is an electrode connected to a hot potential
  • the electrode 4 is an electrode connected to a ground potential.
  • the electrode 3 may be connected to the ground potential
  • the electrode 4 may be connected to the hot potential.
  • at least one pair of electrodes is an electrode connected to a hot potential or an electrode connected to a ground potential, as described above, and no floating electrode is provided.
  • FIG. 24 is a diagram showing an example of the resonance characteristics of the elastic wave device shown in FIG. 18. Note that the design parameters of the elastic wave device 1 that obtained this resonance characteristic are as follows.
  • Intermediate layer 7 silicon oxide film with a thickness of 1 ⁇ m.
  • Support substrate 8 Si substrate.
  • the length of the excitation region C is a dimension along the length direction of the electrodes 3 and 4 of the excitation region C.
  • the distances between the electrode pairs made up of the electrodes 3 and 4 were all equal in multiple pairs. That is, the electrodes 3 and 4 were arranged at equal pitches.
  • d/p is preferably 0.5 or less, More preferably it is 0.24 or less. This will be explained with reference to FIG. 25.
  • FIG. 25 is a diagram showing the relationship between d/2p and the fractional band as a resonator of an acoustic wave device, where p is the distance between the centers of adjacent electrodes and d is the thickness of the piezoelectric layer.
  • the at least one pair of electrodes may be one pair, and in the case of one pair of electrodes, the above p is the distance between the centers of adjacent electrodes 3 and 4. Furthermore, in the case of 1.5 or more pairs of electrodes, the average distance between the centers of adjacent electrodes 3 and 4 may be set to p.
  • the thickness d of the piezoelectric layer if the piezoelectric layer 2 has thickness variations, a value obtained by averaging the thicknesses may be adopted.
  • FIG. 26 is a plan view of another example of an elastic wave device that utilizes bulk waves in thickness-shear mode.
  • a pair of electrodes including an electrode 3 and an electrode 4 are provided on the first main surface 2a of the piezoelectric layer 2.
  • K in FIG. 26 is the intersection width.
  • the number of pairs of electrodes may be one. Even in this case, if the above-mentioned d/p is 0.5 or less, bulk waves in the thickness shear mode can be excited effectively.
  • the metallization ratio MR of the adjacent electrodes 3 and 4 satisfies MR ⁇ 1.75(d/p)+0.075. In that case, spurious can be effectively reduced. This will be explained with reference to FIGS. 27 and 28.
  • FIG. 27 is a reference diagram showing an example of the resonance characteristics of the elastic wave device shown in FIG. 18.
  • a spurious signal indicated by arrow B appears between the resonant frequency and the anti-resonant frequency.
  • d/p 0.08 and the Euler angles of LiNbO 3 (0°, 0°, 90°).
  • the metallization ratio MR was set to 0.35.
  • the metallization ratio MR will be explained with reference to FIG. 19.
  • the area surrounded by the dashed line C becomes the excitation region.
  • This excitation region is the region where the electrode 3 overlaps the electrode 4 when the electrode 3 and the electrode 4 are viewed in a direction perpendicular to the length direction of the electrodes 3 and 4, that is, in a direction in which they face each other. and a region between electrodes 3 and 4 where electrodes 3 and 4 overlap.
  • the area of the electrodes 3 and 4 in the excitation region C with respect to the area of this excitation region becomes the metallization ratio MR. That is, the metallization ratio MR is the ratio of the area of the metallized portion to the area of the excitation region.
  • MR may be the ratio of the metallized portion included in all the excitation regions to the total area of the excitation regions.
  • FIG. 28 is a diagram showing the relationship between the fractional band and the amount of phase rotation of spurious impedance normalized by 180 degrees as the magnitude of spurious when a large number of elastic wave resonators are configured according to the present embodiment. It is. Note that the specific band was adjusted by variously changing the thickness of the piezoelectric layer and the dimensions of the electrode. Further, although FIG. 28 shows the results when a Z-cut piezoelectric layer made of LiNbO 3 is used, the same tendency is obtained when piezoelectric layers with other cut angles are used.
  • the spurious is as large as 1.0.
  • the fractional band exceeds 0.17, that is, exceeds 17%, a large spurious with a spurious level of 1 or more will affect the pass band even if the parameters that make up the fractional band are changed. Appear within. That is, as in the resonance characteristic shown in FIG. 27, a large spurious signal indicated by arrow B appears within the band. Therefore, it is preferable that the fractional band is 17% or less. In this case, by adjusting the thickness of the piezoelectric layer 2, the dimensions of the electrodes 3 and 4, etc., the spurious can be reduced.
  • FIG. 29 is a diagram showing the relationship between d/2p, metallization ratio MR, and fractional band.
  • various elastic wave devices having different d/2p and MR were constructed and the fractional bands were measured.
  • the hatched area on the right side of the broken line D in FIG. 29 is the area where the fractional band is 17% or less.
  • FIG. 30 is a diagram showing a map of fractional bands with respect to Euler angles (0°, ⁇ , ⁇ ) of LiNbO 3 when d/p is brought as close to 0 as possible.
  • the hatched areas in FIG. 30 are areas where a fractional band of at least 5% can be obtained, and the range of the area can be approximated by the following equations (1), (2), and (3). ).
  • ...Formula (1) (0° ⁇ 10°, 20° to 80°, 0° to 60° (1-( ⁇ -50) 2 /900) 1/2 ) or (0° ⁇ 10°, 20° to 80°, [180 °-60° (1-( ⁇ -50) 2 /900) 1/2 ] ⁇ 180°)
  • ...Formula (2) (0° ⁇ 10°, [180°-30° (1-( ⁇ -90) 2 /8100) 1/2 ] ⁇ 180°, arbitrary ⁇ ) ...Formula (3) Therefore, the Euler angle range of formula (1), formula (2), or formula (3) above is preferable because the fractional band can be made sufficiently wide.
  • FIG. 31 is a partially cutaway perspective view for explaining an example of an elastic wave device that utilizes Lamb waves.
  • the elastic wave device 81 has a support substrate 82.
  • the support substrate 82 is provided with an open recess on the upper surface.
  • a piezoelectric layer 83 is laminated on the support substrate 82 .
  • An IDT electrode 84 is provided on the piezoelectric layer 83 above the cavity 9 .
  • Reflectors 85 and 86 are provided on both sides of the IDT electrode 84 in the elastic wave propagation direction.
  • the outer peripheral edge of the cavity 9 is shown by a broken line.
  • the IDT electrode 84 includes a first busbar electrode 84a, a second busbar electrode 84b, an electrode 84c as a plurality of first electrode fingers, and an electrode 84d as a plurality of second electrode fingers.
  • the plurality of electrodes 84c are connected to the first busbar electrode 84a.
  • the plurality of electrodes 84d are connected to the second busbar electrode 84b.
  • the plurality of electrodes 84c and the plurality of electrodes 84d are interposed with each other.
  • the elastic wave device 81 by applying an alternating current electric field to the IDT electrode 84 on the cavity 9, a Lamb wave as a plate wave is excited. Since the reflectors 85 and 86 are provided on both sides, the resonance characteristic due to the Lamb wave described above can be obtained.
  • the elastic wave device of the present invention may utilize plate waves such as Lamb waves.

Abstract

This elastic wave device 10 comprises: a support member 20 that has a cavity 23 on one of the two main surfaces thereof; a piezoelectric layer 21 that is provided on the one main surface of the support member 20 so as to cover the cavity 23; and function electrodes 22 that are provided on at least one of the two main surfaces of the piezoelectric layer 21 such that at least some of the function electrodes 22 overlie the cavity 23 as viewed in the thickness direction of the piezoelectric layer 21. In the piezoelectric layer 21, cracks 24 are provided in a region which overlies the cavity 23 when viewed in the thickness direction of the piezoelectric layer 21 and in which the function electrodes 22 are not provided. The cracks 24 have a width smaller than the thickness of the piezoelectric layer 21 and continuously extend from the one main surface of the piezoelectric layer 21 to the other main surface thereof.

Description

弾性波装置elastic wave device
 本発明は、弾性波装置に関する。 The present invention relates to an elastic wave device.
 従来、ニオブ酸リチウム又はタンタル酸リチウムからなる圧電層を備える弾性波装置が知られている。 Conventionally, acoustic wave devices including a piezoelectric layer made of lithium niobate or lithium tantalate are known.
 特許文献1には、空洞部が形成された支持体と、上記支持体の上に上記空洞部と重なるように設けられている圧電基板と、上記圧電基板の上に上記空洞部と重なるように設けられているIDT(Interdigital Transducer)電極と、を備え、上記IDT電極により板波が励振される弾性波装置であって、上記空洞部の端縁部は、上記IDT電極により励振される板波の伝搬方向と平行に延びる直線部を含まない、弾性波装置が開示されている。 Patent Document 1 discloses a support in which a cavity is formed, a piezoelectric substrate provided on the support so as to overlap with the cavity, and a piezoelectric substrate provided on the piezoelectric substrate so as to overlap with the cavity. An acoustic wave device is provided with an IDT (Interdigital Transducer) electrode provided, and a plate wave is excited by the IDT electrode, wherein an edge of the cavity portion is provided with a plate wave excited by the IDT electrode. An elastic wave device is disclosed that does not include a straight portion extending parallel to the propagation direction of the wave.
 特許文献2には、上面に凹部が設けられている支持部材と、上面及び下面を有し、上記支持部材の凹部を覆うように上記支持部材上に設けられており、上記支持部材の凹部からなる中空空間上に位置している部分を有する、圧電薄膜と、上記圧電薄膜の上記上面に設けられており、複数本の電極指を有するIDT電極と、を備え、S0モード又はSH0モードの板波を利用しており、上記圧電薄膜の上記中空空間上に位置している部分において、上記圧電薄膜の上記上面又は上記下面に設けられており、上記IDT電極の上記電極指が延びる方向に延びている複数本の溝が設けられている、弾性波装置が開示されている。 Patent Document 2 discloses a supporting member having a recessed portion on its upper surface, and a supporting member having an upper surface and a lower surface, and is provided on the supporting member so as to cover the recessed portion of the supporting member, and the supporting member is provided with a recessed portion of the supporting member. A piezoelectric thin film having a portion located in a hollow space, and an IDT electrode provided on the upper surface of the piezoelectric thin film and having a plurality of electrode fingers, the plate is in S0 mode or SHO mode. It utilizes waves, and is provided on the upper surface or the lower surface of the piezoelectric thin film in a portion of the piezoelectric thin film located above the hollow space, and extends in the direction in which the electrode fingers of the IDT electrode extend. An elastic wave device is disclosed in which a plurality of grooves are provided.
特開2012-257019号公報Japanese Patent Application Publication No. 2012-257019 特開2017-224890号公報JP2017-224890A
 特許文献1には、空洞部を形成する方法の一例として、圧電体上にSiOやSiN等からなる薄膜で枠を形成した圧電基板を形成し、枠下に支持基板を配して形成する方法が記載されている。 Patent Document 1 describes an example of a method for forming a cavity, in which a piezoelectric substrate is formed with a frame made of a thin film made of SiO 2 , SiN, etc. on a piezoelectric body, and a support substrate is arranged under the frame. The method is described.
 また、特許文献2には、圧電基板上に犠牲層を形成した後、犠牲層を覆うように支持層を設け、その後、支持層に支持基板を接合することが記載されている。さらに、特許文献2には、圧電基板を薄くして圧電薄膜とすること、圧電薄膜にエッチング用孔を形成すること、ウェットエッチングにより、エッチング用孔から犠牲層を除去することが記載されている。これにより、支持層内に中空空間が形成される。 Further, Patent Document 2 describes that after forming a sacrificial layer on a piezoelectric substrate, a supporting layer is provided to cover the sacrificial layer, and then a supporting substrate is bonded to the supporting layer. Further, Patent Document 2 describes that a piezoelectric substrate is made thinner to form a piezoelectric thin film, that an etching hole is formed in the piezoelectric thin film, and that a sacrificial layer is removed from the etching hole by wet etching. . This creates a hollow space within the support layer.
 しかしながら、空洞部と重なる部分の圧電層にエッチング用孔等の貫通穴が設けられている弾性波装置では、貫通穴の分だけ余計な面積が必要になるため、素子サイズが大きくなりやすいという問題がある。 However, in acoustic wave devices in which through-holes such as etching holes are provided in the piezoelectric layer in the portion that overlaps with the cavity, an extra area is required for the through-holes, which tends to increase the element size. There is.
 本発明は、素子サイズを小さくできる弾性波装置を提供することを目的とする。 An object of the present invention is to provide an elastic wave device whose element size can be reduced.
 本発明の弾性波装置は、空洞部を一方主面に有する支持部材と、上記空洞部を覆うように上記支持部材の上記一方主面に設けられた圧電層と、上記圧電層の少なくとも一方の主面に、上記圧電層の厚み方向から見て少なくとも一部が上記空洞部と重なるように設けられた機能電極と、を備える。上記圧電層には、上記厚み方向から見て上記空洞部と重なり、かつ、上記機能電極が設けられていない領域において、上記圧電層の厚みよりも幅が小さく、上記圧電層の一方の主面から他方の主面に連通する亀裂が設けられている。 The elastic wave device of the present invention includes a support member having a cavity on one main surface, a piezoelectric layer provided on the one main surface of the support member so as to cover the cavity, and at least one of the piezoelectric layers. A functional electrode is provided on the main surface so that at least a portion thereof overlaps with the cavity when viewed from the thickness direction of the piezoelectric layer. The piezoelectric layer has a width smaller than the thickness of the piezoelectric layer in a region that overlaps with the cavity and is not provided with the functional electrode when viewed from the thickness direction, and one main surface of the piezoelectric layer. A crack is provided that communicates from one main surface to the other main surface.
 本発明によれば、素子サイズを小さくできる弾性波装置を提供することができる。 According to the present invention, it is possible to provide an elastic wave device whose element size can be reduced.
図1は、本発明の弾性波装置の一例を模式的に示す断面図である。FIG. 1 is a cross-sectional view schematically showing an example of the elastic wave device of the present invention. 図2は、本発明の弾性波装置の一例を模式的に示す平面図である。FIG. 2 is a plan view schematically showing an example of the elastic wave device of the present invention. 図3は、圧電基板上に犠牲層を形成する工程の一例を模式的に示す断面図である。FIG. 3 is a cross-sectional view schematically showing an example of the process of forming a sacrificial layer on a piezoelectric substrate. 図4は、圧電基板上に犠牲層を形成する工程の一例を模式的に示す平面図である。FIG. 4 is a plan view schematically showing an example of the process of forming a sacrificial layer on a piezoelectric substrate. 図5は、中間層を形成する工程の一例を模式的に示す断面図である。FIG. 5 is a cross-sectional view schematically showing an example of the process of forming the intermediate layer. 図6は、中間層に支持基板を接合する工程の一例を模式的に示す断面図である。FIG. 6 is a cross-sectional view schematically showing an example of the process of bonding the support substrate to the intermediate layer. 図7は、圧電基板を薄化する工程の一例を模式的に示す断面図である。FIG. 7 is a cross-sectional view schematically showing an example of the process of thinning the piezoelectric substrate. 図8は、亀裂を形成する工程の一例を模式的に示す断面図である。FIG. 8 is a cross-sectional view schematically showing an example of the process of forming a crack. 図9は、機能電極及び配線電極を形成する工程の一例を模式的に示す断面図である。FIG. 9 is a cross-sectional view schematically showing an example of the process of forming functional electrodes and wiring electrodes. 図10は、機能電極及び配線電極を形成する工程の一例を模式的に示す平面図である。FIG. 10 is a plan view schematically showing an example of the process of forming functional electrodes and wiring electrodes. 図11は、保護電極及び犠牲層を除去する工程の一例を模式的に示す断面図である。FIG. 11 is a cross-sectional view schematically showing an example of the process of removing the protective electrode and the sacrificial layer. 図12は、エッチング用孔を形成するための保護レジストが設けられた状態の一例を模式的に示す断面図である。FIG. 12 is a cross-sectional view schematically showing an example of a state in which a protective resist for forming etching holes is provided. 図13は、エッチング中の状態の一例を模式的に示す断面図である。FIG. 13 is a cross-sectional view schematically showing an example of a state during etching. 図14は、図13においてXIVで示す部分の一例を模式的に示す側面図である。FIG. 14 is a side view schematically showing an example of the portion indicated by XIV in FIG. 13. 図15は、亀裂が設けられた部分の圧電層の一例を模式的に示す側面図である。FIG. 15 is a side view schematically showing an example of a piezoelectric layer in a portion where a crack is provided. 図16は、亀裂が設けられた部分の圧電層の一例を模式的に示す平面図である。FIG. 16 is a plan view schematically showing an example of a piezoelectric layer in a portion where a crack is provided. 図17は、本発明の弾性波装置の別の一例を模式的に示す断面図である。FIG. 17 is a cross-sectional view schematically showing another example of the elastic wave device of the present invention. 図18は、厚み滑りモードのバルク波を利用する弾性波装置の一例の外観を示す略図的斜視図である。FIG. 18 is a schematic perspective view showing the appearance of an example of an elastic wave device that utilizes bulk waves in thickness shear mode. 図19は、図18に示す弾性波装置の圧電層上の電極構造を示す平面図である。FIG. 19 is a plan view showing the electrode structure on the piezoelectric layer of the acoustic wave device shown in FIG. 18. 図20は、図18中のA-A線に沿う部分の断面図である。FIG. 20 is a cross-sectional view of a portion taken along line AA in FIG. 18. 図21は、弾性波装置の圧電膜を伝搬するラム波を説明するための模式的正面断面図である。FIG. 21 is a schematic front sectional view for explaining Lamb waves propagating through a piezoelectric film of an acoustic wave device. 図22は、弾性波装置の圧電層を伝播する厚み滑りモードのバルク波を説明するための模式的正面断面図である。FIG. 22 is a schematic front sectional view for explaining a thickness shear mode bulk wave propagating through a piezoelectric layer of an elastic wave device. 図23は、厚み滑りモードのバルク波の振幅方向を示す図である。FIG. 23 is a diagram showing the amplitude direction of the bulk wave in the thickness shear mode. 図24は、図18に示す弾性波装置の共振特性の一例を示す図である。FIG. 24 is a diagram showing an example of the resonance characteristics of the elastic wave device shown in FIG. 18. 図25は、隣り合う電極の中心間距離をp、圧電層の厚みをdとした場合のd/2pと、弾性波装置の共振子としての比帯域との関係を示す図である。FIG. 25 is a diagram showing the relationship between d/2p and the fractional band as a resonator of an acoustic wave device, where p is the distance between the centers of adjacent electrodes and d is the thickness of the piezoelectric layer. 図26は、厚み滑りモードのバルク波を利用する弾性波装置の別の一例の平面図である。FIG. 26 is a plan view of another example of an elastic wave device that utilizes bulk waves in thickness shear mode. 図27は、図18に示す弾性波装置の共振特性の一例を示す参考図である。FIG. 27 is a reference diagram showing an example of the resonance characteristics of the elastic wave device shown in FIG. 18. 図28は、本実施形態に従って、多数の弾性波共振子を構成した場合の比帯域と、スプリアスの大きさとしての180度で規格化されたスプリアスのインピーダンスの位相回転量との関係を示す図である。FIG. 28 is a diagram showing the relationship between the fractional band and the amount of phase rotation of spurious impedance normalized by 180 degrees as the magnitude of spurious when a large number of elastic wave resonators are configured according to the present embodiment. It is. 図29は、d/2pと、メタライゼーション比MRと、比帯域との関係を示す図である。FIG. 29 is a diagram showing the relationship between d/2p, metallization ratio MR, and fractional band. 図30は、d/pを限りなく0に近づけた場合のLiNbOのオイラー角(0°,θ,ψ)に対する比帯域のマップを示す図である。FIG. 30 is a diagram showing a map of fractional bands with respect to Euler angles (0°, θ, ψ) of LiNbO 3 when d/p is brought as close to 0 as possible. 図31は、ラム波を利用する弾性波装置の一例を説明するための部分切り欠き斜視図である。FIG. 31 is a partially cutaway perspective view for explaining an example of an elastic wave device that uses Lamb waves.
 以下、本発明の弾性波装置について説明する。 Hereinafter, the elastic wave device of the present invention will be explained.
 本発明の弾性波装置は、第1、第2及び第3の態様において、ニオブ酸リチウム又はタンタル酸リチウムからなる圧電層と、圧電層の厚み方向に交差する方向において対向する第1電極及び第2電極とを備える。 In the first, second and third aspects, the acoustic wave device of the present invention includes a piezoelectric layer made of lithium niobate or lithium tantalate, a first electrode and a first electrode facing each other in a direction crossing the thickness direction of the piezoelectric layer. 2 electrodes.
 第1の態様では、厚み滑り1次モード等の厚み滑りモードのバルク波が利用されている。また、第2の態様では、第1電極及び前記第2電極は隣り合う電極同士であり、圧電層の厚みをd、第1電極及び第2電極の中心間距離をpとした場合、d/pが0.5以下とされている。それによって、第1及び第2の態様では、小型化を進めた場合であっても、Q値を高めることができる。 In the first aspect, a bulk wave in a thickness shear mode such as a primary thickness shear mode is used. Further, in the second aspect, the first electrode and the second electrode are adjacent electrodes, and when the thickness of the piezoelectric layer is d and the distance between the centers of the first electrode and the second electrode is p, d/ p is set to be 0.5 or less. Thereby, in the first and second aspects, the Q value can be increased even when miniaturization is promoted.
 また、第3の態様では、板波としてのラム波が利用される。そして、上記ラム波による共振特性を得ることができる。 Furthermore, in the third aspect, Lamb waves are used as plate waves. Then, resonance characteristics due to the Lamb wave described above can be obtained.
 以下、図面を参照しつつ、本発明の具体的な実施形態を説明することにより、本発明を明らかにする。 Hereinafter, the present invention will be clarified by describing specific embodiments of the present invention with reference to the drawings.
 以下に示す図面は模式的なものであり、その寸法、縦横比の縮尺等は実際の製品とは異なる場合がある。 The drawings shown below are schematic, and their dimensions, aspect ratios, etc. may differ from the actual product.
 なお、本明細書に記載の各実施形態は、例示的なものであり、異なる実施形態間において、構成の部分的な置換又は組み合わせが可能である。また、各実施形態を特に区別しない場合、単に「本発明の弾性波装置」という。 Note that each embodiment described in this specification is an illustrative example, and parts of the configurations can be partially replaced or combined between different embodiments. In addition, unless there is a particular distinction between the embodiments, they will simply be referred to as "the elastic wave device of the present invention."
 図1は、本発明の弾性波装置の一例を模式的に示す断面図である。図2は、本発明の弾性波装置の一例を模式的に示す平面図である。なお、図1は、図2に示す弾性波装置のI-I線に沿った断面図の一例である。 FIG. 1 is a cross-sectional view schematically showing an example of the elastic wave device of the present invention. FIG. 2 is a plan view schematically showing an example of the elastic wave device of the present invention. Note that FIG. 1 is an example of a cross-sectional view of the elastic wave device shown in FIG. 2 taken along line II.
 図1及び図2に示す弾性波装置10は、支持部材20と、圧電層21と、機能電極22と、を備える。 The elastic wave device 10 shown in FIGS. 1 and 2 includes a support member 20, a piezoelectric layer 21, and a functional electrode 22.
 支持部材20は、空洞部23を一方主面(図1では上側の主面)に有する。 The support member 20 has a cavity 23 on one main surface (the upper main surface in FIG. 1).
 圧電層21は、空洞部23を覆うように支持部材20の一方主面に設けられている。 The piezoelectric layer 21 is provided on one main surface of the support member 20 so as to cover the cavity 23.
 機能電極22は、圧電層21の少なくとも一方の主面に設けられている。図1及び図2に示す例では、圧電層21の一方の主面(図1では上側の主面)に機能電極22が設けられている。 The functional electrode 22 is provided on at least one main surface of the piezoelectric layer 21. In the example shown in FIGS. 1 and 2, the functional electrode 22 is provided on one main surface (the upper main surface in FIG. 1) of the piezoelectric layer 21.
 機能電極22は、圧電層21の厚み方向(図1及び図2ではZ方向)から見て少なくとも一部が空洞部23と重なるように設けられている。圧電層21の厚み方向から見て、機能電極22の全部が空洞部23と重なるように設けられていてもよく、機能電極22の一部が空洞部23と重なるように設けられていてもよい。 The functional electrode 22 is provided so that at least a portion thereof overlaps with the cavity 23 when viewed from the thickness direction of the piezoelectric layer 21 (Z direction in FIGS. 1 and 2). When viewed from the thickness direction of the piezoelectric layer 21, the functional electrode 22 may be provided so that the entirety thereof overlaps with the cavity 23, or a part of the functional electrode 22 may be provided so as to overlap with the cavity 23. .
 圧電層21には、厚み方向から見て空洞部23と重なり、かつ、機能電極22が設けられていない領域において、圧電層21の厚みよりも幅が小さく、圧電層21の一方の主面(図1では上側の主面)から他方の主面(図1では下側の主面)に連通する亀裂24が設けられている。 The piezoelectric layer 21 has a width smaller than the thickness of the piezoelectric layer 21 in a region that overlaps the cavity 23 and is not provided with the functional electrode 22 when viewed from the thickness direction, and has one main surface ( A crack 24 is provided that communicates from the upper main surface (in FIG. 1) to the other main surface (lower main surface in FIG. 1).
 図1及び図2に示す弾性波装置10では、圧電層21の一部であるメンブレン部21Mの外周部に、微小な幅を有する亀裂24が設けられている。したがって、例えば犠牲層を除去することにより空洞部を形成する場合であっても、犠牲層を除去するためのエッチング液が亀裂24に浸入できるため、エッチング用孔を形成する必要がなくなる。その結果、素子サイズを小さくすることができる。 In the elastic wave device 10 shown in FIGS. 1 and 2, a crack 24 having a minute width is provided at the outer circumference of the membrane portion 21M, which is a part of the piezoelectric layer 21. Therefore, even if a cavity is formed by removing the sacrificial layer, for example, the etching solution for removing the sacrificial layer can enter the cracks 24, so there is no need to form etching holes. As a result, the element size can be reduced.
 本明細書では、厚み方向から見て空洞部と重なる領域に位置する圧電層の部分を「メンブレン部」とも称する。 In this specification, the portion of the piezoelectric layer located in the region overlapping with the cavity when viewed from the thickness direction is also referred to as a "membrane portion."
 上記のとおり、亀裂24の幅(図1中、W24で示す長さ)は、圧電層21の厚み(図1中、T21で示す長さ)よりも小さい。なお、亀裂24の幅とは、厚み方向に沿った断面における幅を意味する。また、圧電層21の厚みとは、厚み方向の寸法を意味する。 As mentioned above, the width of the crack 24 (the length indicated by W 24 in FIG. 1) is smaller than the thickness of the piezoelectric layer 21 (the length indicated by T 21 in FIG. 1). Note that the width of the crack 24 means the width in a cross section along the thickness direction. Moreover, the thickness of the piezoelectric layer 21 means the dimension in the thickness direction.
 亀裂24の長さ(図2中、L24で示す長さ)は、特に限定されない。なお、亀裂24の長さとは、亀裂24の延伸方向の寸法を意味する。 The length of the crack 24 (the length indicated by L24 in FIG. 2) is not particularly limited. Note that the length of the crack 24 means the dimension of the crack 24 in the extending direction.
 支持部材20は、圧電層21が設けられた一方主面に中間層41(絶縁層、接合層ともいう)を有してもよい。例えば、支持部材20は、支持基板42と、支持基板42及び圧電層21の間に設けられた中間層41とを含む。 The support member 20 may have an intermediate layer 41 (also referred to as an insulating layer or a bonding layer) on one main surface on which the piezoelectric layer 21 is provided. For example, the support member 20 includes a support substrate 42 and an intermediate layer 41 provided between the support substrate 42 and the piezoelectric layer 21.
 支持基板42は、例えば、シリコン(Si)からなる。 The support substrate 42 is made of silicon (Si), for example.
 中間層41は、例えば、二酸化ケイ素(SiO)等の酸化ケイ素(SiO)からなる。 The intermediate layer 41 is made of silicon oxide (SiO x ) such as silicon dioxide (SiO 2 ), for example.
 圧電層21は、例えば、ニオブ酸リチウム(LiNbO)又はタンタル酸リチウム(LiTaO)からなる。その場合、圧電層21は、LiNbO又はLiTaOから構成されてもよい。 The piezoelectric layer 21 is made of, for example, lithium niobate (LiNbO x ) or lithium tantalate (LiTaO x ). In that case, the piezoelectric layer 21 may be composed of LiNbO 3 or LiTaO 3 .
 機能電極22は、例えば、圧電層21の一方の主面に設けられたIDT電極である。なお、機能電極22には、2層配線等の配線電極26が接続されている。 The functional electrode 22 is, for example, an IDT electrode provided on one main surface of the piezoelectric layer 21. Note that a wiring electrode 26 such as a two-layer wiring is connected to the functional electrode 22.
 本発明の弾性波装置は、例えば、以下の方法により製造される。 The elastic wave device of the present invention is manufactured, for example, by the following method.
 まず、図3~図11を参照して、本発明の弾性波装置の製造方法の一例について説明する。 First, an example of the method for manufacturing an elastic wave device of the present invention will be described with reference to FIGS. 3 to 11.
 図3は、圧電基板上に犠牲層を形成する工程の一例を模式的に示す断面図である。図4は、圧電基板上に犠牲層を形成する工程の一例を模式的に示す平面図である。 FIG. 3 is a cross-sectional view schematically showing an example of the process of forming a sacrificial layer on a piezoelectric substrate. FIG. 4 is a plan view schematically showing an example of the process of forming a sacrificial layer on a piezoelectric substrate.
 図3及び図4に示すように、まず、無機物の犠牲層40Aを圧電基板31上に形成する。 As shown in FIGS. 3 and 4, first, an inorganic sacrificial layer 40A is formed on the piezoelectric substrate 31.
 続いて、有機物の犠牲層40Bを圧電基板31上に形成する。図3及び図4に示す例では、無機物の犠牲層40Aの短辺側に有機物の犠牲層40Bを形成している。 Subsequently, an organic sacrificial layer 40B is formed on the piezoelectric substrate 31. In the example shown in FIGS. 3 and 4, an organic sacrificial layer 40B is formed on the short side of an inorganic sacrificial layer 40A.
 以上により、圧電基板31上に犠牲層40が形成される。 Through the above steps, the sacrificial layer 40 is formed on the piezoelectric substrate 31.
 圧電基板31としては、例えば、LiNbO又はLiTaO等からなる基板が用いられる。 As the piezoelectric substrate 31, for example, a substrate made of LiNbO 3 or LiTaO 3 is used.
 無機物の犠牲層40Aの材料としては、後述するエッチングにより除去され得る適宜の無機材料が用いられる。例えば、ZnO等が用いられる。 As the material for the inorganic sacrificial layer 40A, an appropriate inorganic material that can be removed by etching, which will be described later, is used. For example, ZnO or the like is used.
 無機物の犠牲層40Aは、例えば、以下の方法により形成することができる。まず、スパッタリング法によりZnO膜を形成する。その後、レジスト塗布、露光及び現像をこの順に行う。次に、ウェットエッチングを行うことにより、無機物の犠牲層40Aのパターンを形成する。なお、無機物の犠牲層40Aは、他の方法により形成されてもよい。 The inorganic sacrificial layer 40A can be formed, for example, by the following method. First, a ZnO film is formed by sputtering. Thereafter, resist coating, exposure and development are performed in this order. Next, wet etching is performed to form a pattern of the inorganic sacrificial layer 40A. Note that the inorganic sacrificial layer 40A may be formed by other methods.
 有機物の犠牲層40Bの材料としては、後述する熱処理により変形し得る適宜の樹脂材料が用いられる。 As the material of the organic sacrificial layer 40B, an appropriate resin material that can be deformed by heat treatment, which will be described later, is used.
 図5は、中間層を形成する工程の一例を模式的に示す断面図である。 FIG. 5 is a cross-sectional view schematically showing an example of the process of forming the intermediate layer.
 図5に示すように、犠牲層40を覆うように中間層41を形成した後、中間層41の表面を平坦化する。 As shown in FIG. 5, after forming the intermediate layer 41 to cover the sacrificial layer 40, the surface of the intermediate layer 41 is planarized.
 中間層41として、例えば、SiO膜等が形成される。中間層41は、例えば、スパッタリング法等により形成することができる。中間層41の平坦化は、例えば、化学的機械研磨(CMP)等により行うことができる。 As the intermediate layer 41, for example, a SiO 2 film or the like is formed. The intermediate layer 41 can be formed by, for example, a sputtering method. The intermediate layer 41 can be planarized by, for example, chemical mechanical polishing (CMP).
 図6は、中間層に支持基板を接合する工程の一例を模式的に示す断面図である。 FIG. 6 is a cross-sectional view schematically showing an example of the process of bonding the support substrate to the intermediate layer.
 図6に示すように、中間層41に支持基板42を接合する。これにより、支持部材20が形成される。 As shown in FIG. 6, a support substrate 42 is bonded to the intermediate layer 41. Thereby, the support member 20 is formed.
 図7は、圧電基板を薄化する工程の一例を模式的に示す断面図である。 FIG. 7 is a cross-sectional view schematically showing an example of the process of thinning the piezoelectric substrate.
 図7に示すように、圧電基板31を薄化する。これにより、圧電層21が形成される。圧電基板31の薄化は、例えば、スマートカット法、研磨等により行うことができる。 As shown in FIG. 7, the piezoelectric substrate 31 is thinned. As a result, the piezoelectric layer 21 is formed. The piezoelectric substrate 31 can be thinned by, for example, a smart cut method, polishing, or the like.
 図8は、亀裂を形成する工程の一例を模式的に示す断面図である。 FIG. 8 is a cross-sectional view schematically showing an example of the process of forming a crack.
 圧電層21が形成された支持部材20に対して熱処理を行う。熱により有機物の犠牲層40Bが膨張又は収縮するため、メンブレン部21Mが変形する。その結果、図8に示すように、犠牲層40の短辺側に亀裂24がクラックとして形成される。 Heat treatment is performed on the support member 20 on which the piezoelectric layer 21 is formed. Since the organic sacrificial layer 40B expands or contracts due to heat, the membrane portion 21M is deformed. As a result, as shown in FIG. 8, a crack 24 is formed on the short side of the sacrificial layer 40.
 図9は、機能電極及び配線電極を形成する工程の一例を模式的に示す断面図である。図10は、機能電極及び配線電極を形成する工程の一例を模式的に示す平面図である。 FIG. 9 is a cross-sectional view schematically showing an example of the process of forming functional electrodes and wiring electrodes. FIG. 10 is a plan view schematically showing an example of the process of forming functional electrodes and wiring electrodes.
 図9及び図10に示すように、圧電層21の一方主面上に、機能電極22及び配線電極26を形成する。機能電極22及び配線電極26は、例えば、リフトオフ法等により形成することができる。 As shown in FIGS. 9 and 10, a functional electrode 22 and a wiring electrode 26 are formed on one main surface of the piezoelectric layer 21. The functional electrode 22 and the wiring electrode 26 can be formed by, for example, a lift-off method.
 この際、工程流動中のクラックを保護するため、クラック部分に保護電極28を形成することが好ましい。 At this time, it is preferable to form a protective electrode 28 on the cracked portion in order to protect the crack during the process flow.
 図11は、保護電極及び犠牲層を除去する工程の一例を模式的に示す断面図である。 FIG. 11 is a cross-sectional view schematically showing an example of the process of removing the protective electrode and the sacrificial layer.
 図11に示すように、エッチング等の方法により保護電極28を除去する。 As shown in FIG. 11, the protective electrode 28 is removed by a method such as etching.
 また、図11に示すように、亀裂24を利用して、犠牲層40を除去する。具体的には、エッチング等の方法により有機物の犠牲層40B及び無機物の犠牲層40Aを除去する。無機物の犠牲層40Aの材料がZnOである場合、例えば、酢酸、リン酸及び水の混合溶液(酢酸:リン酸:水=1:1:10)を用いたウェットエッチングにより無機物の犠牲層40Aを除去することができる。 Furthermore, as shown in FIG. 11, the sacrificial layer 40 is removed using the cracks 24. Specifically, the organic sacrificial layer 40B and the inorganic sacrificial layer 40A are removed by a method such as etching. When the material of the inorganic sacrificial layer 40A is ZnO, for example, the inorganic sacrificial layer 40A is wet etched using a mixed solution of acetic acid, phosphoric acid, and water (acetic acid: phosphoric acid: water = 1:1:10). Can be removed.
 犠牲層40が除去されることで、支持部材20に空洞部23が形成される。 By removing the sacrificial layer 40, a cavity 23 is formed in the support member 20.
 以上により、弾性波装置10が得られる。 Through the above steps, the elastic wave device 10 is obtained.
 上記の方法では、犠牲層40を除去するためのエッチング用孔を圧電層21に形成する代わりに、亀裂24を圧電層21に形成するため、素子サイズを小さくすることができる。 In the above method, the cracks 24 are formed in the piezoelectric layer 21 instead of forming etching holes for removing the sacrificial layer 40 in the piezoelectric layer 21, so the element size can be reduced.
 なお、圧電層21にエッチング用孔を形成しようとする場合、適切なウェットエッチング液が存在しないため、ドライエッチングによりエッチング孔を形成する必要がある。 Note that when attempting to form an etching hole in the piezoelectric layer 21, it is necessary to form the etching hole by dry etching since an appropriate wet etching solution does not exist.
 図12は、エッチング用孔を形成するための保護レジストが設けられた状態の一例を模式的に示す断面図である。 FIG. 12 is a cross-sectional view schematically showing an example of a state in which a protective resist for forming etching holes is provided.
 図12に示すように、エッチング用孔を形成する箇所以外は、保護レジスト50で覆われている。 As shown in FIG. 12, the areas other than those where etching holes are to be formed are covered with a protective resist 50.
 図13は、エッチング中の状態の一例を模式的に示す断面図である。 FIG. 13 is a cross-sectional view schematically showing an example of a state during etching.
 図13に示すように、圧電層21にエッチング用孔51を形成する場合、ドライエッチングであっても化学反応的な条件がないため、イオンミリング的な条件で行う必要がある。そのため、エッチングの際には、保護レジスト50もエッチングされる。 As shown in FIG. 13, when forming etching holes 51 in the piezoelectric layer 21, even dry etching does not require chemical reaction conditions, so it must be performed under ion milling conditions. Therefore, during etching, the protective resist 50 is also etched.
 図14は、図13においてXIVで示す部分の一例を模式的に示す側面図である。 FIG. 14 is a side view schematically showing an example of the portion indicated by XIV in FIG. 13.
 上記のとおり、ドライエッチング中には、保護レジスト50もエッチングされる。そのため、図14に示すように、エッチング用孔51が形成された部分の圧電層21の側面には、圧電層21の厚み方向(Z方向)に沿って一様な縦筋52が発生する。 As described above, the protective resist 50 is also etched during dry etching. Therefore, as shown in FIG. 14, uniform vertical streaks 52 are generated along the thickness direction (Z direction) of the piezoelectric layer 21 on the side surface of the piezoelectric layer 21 in the portion where the etching hole 51 is formed.
 図15は、亀裂が設けられた部分の圧電層の一例を模式的に示す側面図である。図16は、亀裂が設けられた部分の圧電層の一例を模式的に示す平面図である。 FIG. 15 is a side view schematically showing an example of a piezoelectric layer in a portion where a crack is provided. FIG. 16 is a plan view schematically showing an example of a piezoelectric layer in a portion where a crack is provided.
 図15には、圧電層21の側面が示されており、図16には、圧電層21の表層が示されている。 FIG. 15 shows the side surface of the piezoelectric layer 21, and FIG. 16 shows the surface layer of the piezoelectric layer 21.
 圧電層21に設けられる亀裂24は、表層に応力が集中し、結晶軸のすべりによって、亀裂の起点が発生し、その後、圧電層の面内に存在する引張応力によって広がる。そのため、図15に示すように、亀裂24が設けられた部分の圧電層21の側面には、圧電層21の厚み方向(Z方向)に蛇行する縦筋53と、圧電層21の厚み方向(Z方向)に沿った縦筋の無いへき開面54とが混在することが好ましい。縦筋53は、クラックの起点付近に発生するものであり、圧電層21の厚み方向に蛇行している。一方、へき開面54には、縦筋53が存在しない。 In the cracks 24 provided in the piezoelectric layer 21, stress is concentrated on the surface layer, a starting point of the crack is generated due to the slippage of the crystal axis, and then it spreads due to the tensile stress existing in the plane of the piezoelectric layer. Therefore, as shown in FIG. 15, on the side surface of the piezoelectric layer 21 at the portion where the crack 24 is provided, there are vertical stripes 53 that meander in the thickness direction (Z direction) of the piezoelectric layer 21 and It is preferable that cleavage planes 54 without vertical stripes along the Z direction) coexist. The vertical stripes 53 occur near the starting point of the crack, and meander in the thickness direction of the piezoelectric layer 21 . On the other hand, the vertical stripes 53 are not present on the cleavage plane 54.
 弾性波装置10において、圧電層21には、圧電層21の厚み方向から見て空洞部23と重なり、かつ、機能電極22が設けられていない領域において、亀裂24以外に圧電層21を厚み方向に貫通する穴(例えば、エッチング用孔51等)が設けられていないことが好ましい。例えば、圧電層21の側面には、圧電層21の厚み方向に沿った一様な縦筋52が存在しないことが好ましい。 In the acoustic wave device 10, the piezoelectric layer 21 has cracks in the piezoelectric layer 21 in the thickness direction in addition to the cracks 24 in an area that overlaps the cavity 23 when viewed from the thickness direction of the piezoelectric layer 21 and is not provided with the functional electrode 22. It is preferable that no holes (for example, etching holes 51, etc.) passing through are provided. For example, it is preferable that uniform vertical stripes 52 along the thickness direction of the piezoelectric layer 21 do not exist on the side surfaces of the piezoelectric layer 21 .
 圧電層21を厚み方向から見たとき、亀裂24は、図2に示すように、空洞部23の外周縁と重なる領域に設けられていることが好ましい。この場合、素子面積を最も小さくすることができる。亀裂24は、空洞部23の外周縁と重なる領域のみに設けられていることが好ましく、空洞部23の外周縁と重なる領域の一部のみに設けられていることがより好ましい。 When the piezoelectric layer 21 is viewed from the thickness direction, the cracks 24 are preferably provided in a region that overlaps with the outer peripheral edge of the cavity 23, as shown in FIG. In this case, the element area can be minimized. The crack 24 is preferably provided only in a region that overlaps with the outer periphery of the cavity 23, and more preferably only in a part of the region that overlaps with the outer periphery of the cavity 23.
 圧電層21を厚み方向から見たとき、亀裂24は、図2に示すように、空洞部23の外周縁を跨ぐ機能電極22と重なる領域に設けられていないことが好ましい。この場合、素子の機能に与える影響を小さくすることができる。 When the piezoelectric layer 21 is viewed from the thickness direction, it is preferable that the cracks 24 are not provided in a region overlapping with the functional electrode 22 that straddles the outer peripheral edge of the cavity 23, as shown in FIG. In this case, the influence on the function of the element can be reduced.
 亀裂24の数、形状、大きさ等は特に限定されない。複数の亀裂24が設けられている場合、圧電層21の厚み方向から見た亀裂24の形状、大きさ等は、それぞれ同じでもよく、一部又は全部が異なってもよい。 The number, shape, size, etc. of the cracks 24 are not particularly limited. When a plurality of cracks 24 are provided, the shape, size, etc. of the cracks 24 viewed from the thickness direction of the piezoelectric layer 21 may be the same, or may be partially or completely different.
 亀裂24を形成する方法は、犠牲層40を用いる方法に限定されない。 The method for forming the crack 24 is not limited to the method using the sacrificial layer 40.
 空洞部23は、支持部材20を厚み方向に貫通しなくてもよく、貫通してもよい。支持部材20が中間層41と支持基板42とを含む場合、例えば、中間層41を厚み方向に貫通するように空洞部23が設けられていてもよく、中間層41を厚み方向に貫通しないように空洞部23が設けられていてもよい。 The cavity 23 does not need to penetrate the support member 20 in the thickness direction, but may do so. When the support member 20 includes the intermediate layer 41 and the support substrate 42, for example, the cavity 23 may be provided so as to penetrate the intermediate layer 41 in the thickness direction, or may be provided so as not to penetrate the intermediate layer 41 in the thickness direction. A cavity 23 may be provided therein.
 図17は、本発明の弾性波装置の別の一例を模式的に示す断面図である。 FIG. 17 is a cross-sectional view schematically showing another example of the elastic wave device of the present invention.
 図17に示す弾性波装置10Aのように、空洞部23は、支持部材20を厚み方向に貫通してもよい。図17に示す例では、支持部材20が中間層41と支持基板42とを含む。 As in the elastic wave device 10A shown in FIG. 17, the cavity 23 may penetrate the support member 20 in the thickness direction. In the example shown in FIG. 17 , the support member 20 includes an intermediate layer 41 and a support substrate 42 .
 図17に示す弾性波装置10Aにおいて、圧電層21の一方の主面から他方の主面に連通する亀裂24が設けられていると、圧電層21の表裏で圧力差が発生した場合に機械的強度が高くなる。 In the elastic wave device 10A shown in FIG. 17, if a crack 24 communicating from one main surface of the piezoelectric layer 21 to the other main surface is provided, mechanical damage occurs when a pressure difference occurs between the front and back surfaces of the piezoelectric layer 21. Increases strength.
 図17に示す弾性波装置10Aの製造に際して、機能電極22を有する圧電層21のメンブレン部21Mを形成する方法としては、例えば、中間層を介して圧電基板を支持基板と接合した貼り合わせ基板において、予めリフトオフ等の工法で機能電極及び配線電極を含む層を形成した後、メンブレン部21Mに相当する箇所の裏面の支持基板を除去した後、中間層を除去する方法等が挙げられる。 When manufacturing the acoustic wave device 10A shown in FIG. 17, a method for forming the membrane portion 21M of the piezoelectric layer 21 having the functional electrode 22 is, for example, using a bonded substrate in which a piezoelectric substrate is bonded to a support substrate via an intermediate layer. Examples include a method in which a layer including functional electrodes and wiring electrodes is formed in advance by a method such as lift-off, and then the support substrate on the back surface of the portion corresponding to the membrane portion 21M is removed, and then the intermediate layer is removed.
 その他、本発明の弾性波装置を製造する方法は、本発明の範囲内において、種々の応用、変形を加えることが可能である。 In addition, the method for manufacturing an acoustic wave device of the present invention can be applied and modified in various ways within the scope of the present invention.
 以下において、亀裂が設けられていない弾性波装置を例として用いて、厚み滑りモード及び板波を利用する弾性波装置の詳細を説明する。なお、以下においては、機能電極がIDT電極である場合の例を用いて説明する。 In the following, details of an elastic wave device that utilizes a thickness-shear mode and a plate wave will be explained using an example of an elastic wave device in which no cracks are provided. Note that the following description uses an example in which the functional electrode is an IDT electrode.
 図18は、厚み滑りモードのバルク波を利用する弾性波装置の一例の外観を示す略図的斜視図である。図19は、図18に示す弾性波装置の圧電層上の電極構造を示す平面図である。図20は、図18中のA-A線に沿う部分の断面図である。 FIG. 18 is a schematic perspective view showing the appearance of an example of an elastic wave device that utilizes bulk waves in thickness shear mode. FIG. 19 is a plan view showing the electrode structure on the piezoelectric layer of the acoustic wave device shown in FIG. 18. FIG. 20 is a cross-sectional view of a portion taken along line AA in FIG. 18.
 弾性波装置1は、例えば、LiNbOからなる圧電層2を有する。圧電層2は、LiTaOからなるものであってもよい。LiNbO又はLiTaOのカット角は、例えばZカットであるが、回転Yカット又はXカットであってもよい。好ましくは、Y伝搬及びX伝搬±30°の伝搬方位が好ましい。圧電層2の厚みは、特に限定されないが、厚み滑りモードを効果的に励振するには、50nm以上、1000nm以下であることが好ましい。圧電層2は、対向し合う第1の主面2a及び第2の主面2bを有する。圧電層2の第1の主面2a上に、電極3及び電極4が設けられている。ここで電極3が「第1電極」の一例であり、電極4が「第2電極」の一例である。図18及び図19では、複数の電極3が、第1のバスバー電極5に接続されている複数の第1の電極指である。複数の電極4は、第2のバスバー電極6に接続されている複数の第2の電極指である。複数の電極3及び複数の電極4は、互いに間挿し合っている。電極3及び電極4は、矩形形状を有し、長さ方向を有する。この長さ方向と直交する方向において、電極3と、隣りの電極4とが対向している。これら複数の電極3、電極4、第1のバスバー電極5及び第2のバスバー電極6によりIDT(Interdigital Transducer)電極が構成されている。電極3,4の長さ方向、及び、電極3,4の長さ方向と直交する方向はいずれも、圧電層2の厚み方向に交差する方向である。このため、電極3と、隣りの電極4とは、圧電層2の厚み方向に交差する方向において対向しているともいえる。また、電極3,4の長さ方向が図18及び図19に示す電極3,4の長さ方向に直交する方向と入れ替わってもよい。すなわち、図18及び図19において、第1のバスバー電極5及び第2のバスバー電極6が延びている方向に電極3,4を延ばしてもよい。その場合、第1のバスバー電極5及び第2のバスバー電極6は、図18及び図19において電極3,4が延びている方向に延びることとなる。そして、一方電位に接続される電極3と、他方電位に接続される電極4とが隣り合う1対の構造が、上記電極3,4の長さ方向と直交する方向に、複数対設けられている。ここで電極3と電極4とが隣り合うとは、電極3と電極4とが直接接触するように配置されている場合ではなく、電極3と電極4とが間隔を介して配置されている場合を指す。また、電極3と電極4とが隣り合う場合、電極3と電極4との間には、他の電極3,4を含む、ホット電極又はグランド電極に接続される電極は配置されない。この対数は、整数対である必要はなく、1.5対又は2.5対などであってもよい。電極3,4間の中心間距離すなわちピッチは、1μm以上、10μm以下の範囲が好ましい。なお、電極3,4間の中心間距離とは、電極3の長さ方向と直交する方向における電極3の幅寸法の中心と、電極4の長さ方向と直交する方向における電極4の幅寸法の中心とを結んだ距離となる。さらに、電極3,4の少なくとも一方が複数本ある場合(電極3,4を一対の電極組とした場合に、1.5対以上の電極組がある場合)、電極3,4の中心間距離は、1.5対以上の電極3,4のうち隣り合う電極3,4それぞれの中心間距離の平均値を指す。また、電極3,4の幅、すなわち電極3,4の対向方向の寸法は、150nm以上、1000nm以下の範囲が好ましい。 The acoustic wave device 1 has a piezoelectric layer 2 made of, for example, LiNbO 3 . The piezoelectric layer 2 may be made of LiTaO 3 . The cut angle of LiNbO 3 or LiTaO 3 is, for example, a Z cut, but may also be a rotational Y cut or an X cut. Preferably, the propagation directions of Y propagation and X propagation are ±30°. The thickness of the piezoelectric layer 2 is not particularly limited, but in order to effectively excite the thickness shear mode, it is preferably 50 nm or more and 1000 nm or less. The piezoelectric layer 2 has a first main surface 2a and a second main surface 2b that face each other. On the first main surface 2a of the piezoelectric layer 2, an electrode 3 and an electrode 4 are provided. Here, electrode 3 is an example of a "first electrode", and electrode 4 is an example of a "second electrode". In FIGS. 18 and 19, the plurality of electrodes 3 are the plurality of first electrode fingers connected to the first busbar electrode 5. In FIGS. The plurality of electrodes 4 are a plurality of second electrode fingers connected to the second busbar electrode 6. The plurality of electrodes 3 and the plurality of electrodes 4 are interposed with each other. Electrode 3 and electrode 4 have a rectangular shape and have a length direction. The electrode 3 and the adjacent electrode 4 face each other in a direction perpendicular to this length direction. These plurality of electrodes 3, electrodes 4, first busbar electrodes 5, and second busbar electrodes 6 constitute an IDT (Interdigital Transducer) electrode. The length direction of the electrodes 3 and 4 and the direction perpendicular to the length direction of the electrodes 3 and 4 are both directions that intersect the thickness direction of the piezoelectric layer 2. Therefore, it can be said that the electrode 3 and the adjacent electrode 4 face each other in the direction intersecting the thickness direction of the piezoelectric layer 2. Further, the length direction of the electrodes 3 and 4 may be replaced with the direction perpendicular to the length direction of the electrodes 3 and 4 shown in FIGS. 18 and 19. That is, in FIGS. 18 and 19, the electrodes 3 and 4 may be extended in the direction in which the first busbar electrode 5 and the second busbar electrode 6 are extended. In that case, the first busbar electrode 5 and the second busbar electrode 6 will extend in the direction in which the electrodes 3 and 4 extend in FIGS. 18 and 19. A plurality of pairs of structures in which an electrode 3 connected to one potential and an electrode 4 connected to the other potential are adjacent to each other are provided in a direction perpendicular to the length direction of the electrodes 3 and 4. There is. Here, the expression "electrode 3 and electrode 4 are adjacent" does not mean that electrode 3 and electrode 4 are arranged so as to be in direct contact with each other, but when electrode 3 and electrode 4 are arranged with a gap between them. refers to Further, when the electrode 3 and the electrode 4 are adjacent to each other, no electrode connected to the hot electrode or the ground electrode, including the other electrodes 3 and 4, is arranged between the electrode 3 and the electrode 4. This logarithm does not need to be an integer pair, but may be 1.5 pairs, 2.5 pairs, or the like. The center-to-center distance between the electrodes 3 and 4, that is, the pitch, is preferably in the range of 1 μm or more and 10 μm or less. Note that the center-to-center distance between the electrodes 3 and 4 refers to the center of the width dimension of the electrode 3 in the direction orthogonal to the length direction of the electrode 3, and the width dimension of the electrode 4 in the direction orthogonal to the length direction of the electrode 4. It is the distance between the center of Furthermore, if there is a plurality of at least one of the electrodes 3 and 4 (when the electrodes 3 and 4 are a pair of electrode sets, and there are 1.5 or more pairs of electrode sets), the distance between the centers of the electrodes 3 and 4 refers to the average value of the distance between the centers of adjacent electrodes 3 and 4 among 1.5 or more pairs of electrodes 3 and 4. Further, the width of the electrodes 3 and 4, that is, the dimension in the opposing direction of the electrodes 3 and 4, is preferably in the range of 150 nm or more and 1000 nm or less.
 本実施形態において、Zカットの圧電層を用いる場合、電極3,4の長さ方向と直交する方向は、圧電層2の分極方向に直交する方向となる。圧電層2として他のカット角の圧電体を用いた場合には、この限りでない。ここにおいて、「直交」とは、厳密に直交する場合のみに限定されず、略直交(電極3,4の長さ方向と直交する方向と分極方向とのなす角度が例えば90°±10°)でもよい。 In this embodiment, when using a Z-cut piezoelectric layer, the direction perpendicular to the length direction of the electrodes 3 and 4 is the direction perpendicular to the polarization direction of the piezoelectric layer 2. This is not the case when a piezoelectric material having a different cut angle is used as the piezoelectric layer 2. Here, "orthogonal" is not limited to strictly orthogonal, but approximately orthogonal (for example, the angle between the direction orthogonal to the length direction of the electrodes 3 and 4 and the polarization direction is 90°±10°) But that's fine.
 圧電層2の第2の主面2b側には、中間層(接合層とも呼ばれる)7を介して支持基板8が積層されている。中間層7及び支持基板8は、枠状の形状を有し、図20に示すように、開口部7a,8aを有する。それによって、空洞部9が形成されている。空洞部9は、圧電層2の励振領域C(図19参照)の振動を妨げないために設けられている。従って、上記支持基板8は、少なくとも1対の電極3,4が設けられている部分と重ならない位置において、第2の主面2bに中間層7を介して積層されている。なお、中間層7は設けられずともよい。従って、支持基板8は、圧電層2の第2の主面2bに直接または間接に積層され得る。 A support substrate 8 is laminated on the second main surface 2b side of the piezoelectric layer 2 with an intermediate layer (also called a bonding layer) 7 interposed therebetween. The intermediate layer 7 and the support substrate 8 have a frame-like shape, and have openings 7a and 8a, as shown in FIG. Thereby, a cavity 9 is formed. The cavity 9 is provided so as not to hinder the vibration of the excitation region C (see FIG. 19) of the piezoelectric layer 2. Therefore, the support substrate 8 is laminated on the second main surface 2b with the intermediate layer 7 interposed therebetween at a position that does not overlap with the portion where at least one pair of electrodes 3 and 4 are provided. Note that the intermediate layer 7 may not be provided. Therefore, the support substrate 8 can be laminated directly or indirectly on the second main surface 2b of the piezoelectric layer 2.
 中間層7は、例えば、酸化ケイ素からなる。もっとも、酸化ケイ素の他、酸窒化ケイ素、アルミナなどの適宜の絶縁性材料を用いることができる。支持基板8は、Siからなる。Siの圧電層2側の面における面方位は(100)又は(110)であってもよく、(111)であってもよい。好ましくは、抵抗率4kΩ以上の高抵抗のSiが望ましい。もっとも、支持基板8についても適宜の絶縁性材料や半導体材料を用いて構成することができる。支持基板8の材料としては、例えば、酸化アルミニウム、タンタル酸リチウム、ニオブ酸リチウム、水晶などの圧電体、アルミナ、マグネシア、サファイア、窒化ケイ素、窒化アルミニウム、炭化ケイ素、ジルコニア、コージライト、ムライト、ステアタイト、フォルステライトなどの各種セラミック、ダイヤモンド、ガラスなどの誘電体、窒化ガリウムなどの半導体などを用いることができる。 The intermediate layer 7 is made of silicon oxide, for example. However, other than silicon oxide, an appropriate insulating material such as silicon oxynitride or alumina can be used. The support substrate 8 is made of Si. The plane orientation of the Si surface on the piezoelectric layer 2 side may be (100), (110), or (111). Preferably, Si has a high resistivity of 4 kΩ or more. However, the support substrate 8 can also be constructed using an appropriate insulating material or semiconductor material. Examples of materials for the support substrate 8 include aluminum oxide, lithium tantalate, lithium niobate, piezoelectric materials such as crystal, alumina, magnesia, sapphire, silicon nitride, aluminum nitride, silicon carbide, zirconia, cordierite, mullite, and starch. Various ceramics such as tite and forsterite, dielectrics such as diamond and glass, semiconductors such as gallium nitride, etc. can be used.
 上記複数の電極3、電極4、第1のバスバー電極5及び第2のバスバー電極6は、Al、AlCu合金などの適宜の金属もしくは合金からなる。本実施形態では、電極3、電極4、第1のバスバー電極5及び第2のバスバー電極6は、Ti膜上にAl膜を積層した構造を有する。なお、Ti膜以外の密着層を用いてもよい。 The plurality of electrodes 3, electrodes 4, first busbar electrode 5, and second busbar electrode 6 are made of an appropriate metal or alloy such as Al or AlCu alloy. In this embodiment, the electrode 3, the electrode 4, the first busbar electrode 5, and the second busbar electrode 6 have a structure in which an Al film is laminated on a Ti film. Note that an adhesive layer other than the Ti film may be used.
 駆動に際しては、複数の電極3と、複数の電極4との間に交流電圧を印加する。より具体的には、第1のバスバー電極5と第2のバスバー電極6との間に交流電圧を印加する。それによって、圧電層2において励振される厚み滑りモードのバルク波を利用した、共振特性を得ることが可能とされている。また、弾性波装置1では、圧電層2の厚みをd、複数対の電極3,4のうちいずれかの隣り合う電極3,4の中心間距離をpとした場合、d/pは0.5以下とされている。そのため、上記厚み滑りモードのバルク波が効果的に励振され、良好な共振特性を得ることができる。より好ましくは、d/pは0.24以下であり、その場合には、より一層良好な共振特性を得ることができる。なお、本実施形態のように電極3,4の少なくとも一方が複数本ある場合、すなわち、電極3,4を1対の電極組とした場合に電極3,4が1.5対以上ある場合、隣り合う電極3,4の中心間距離pは、各隣り合う電極3,4の中心間距離の平均距離となる。 During driving, an AC voltage is applied between the plurality of electrodes 3 and the plurality of electrodes 4. More specifically, an AC voltage is applied between the first busbar electrode 5 and the second busbar electrode 6. Thereby, it is possible to obtain resonance characteristics using the thickness shear mode bulk wave excited in the piezoelectric layer 2. Further, in the acoustic wave device 1, when the thickness of the piezoelectric layer 2 is d, and the distance between the centers of any adjacent electrodes 3, 4 among the plurality of pairs of electrodes 3, 4 is p, d/p is 0. It is considered to be 5 or less. Therefore, the bulk wave in the thickness shear mode is effectively excited, and good resonance characteristics can be obtained. More preferably, d/p is 0.24 or less, in which case even better resonance characteristics can be obtained. Note that when there is a plurality of at least one of the electrodes 3 and 4 as in this embodiment, that is, when there are 1.5 or more pairs of electrodes 3 and 4 when the electrodes 3 and 4 are one pair of electrodes, The distance p between the centers of the adjacent electrodes 3 and 4 is the average distance between the centers of the adjacent electrodes 3 and 4.
 本実施形態の弾性波装置1では、上記構成を備えるため、小型化を図ろうとして、電極3,4の対数を小さくしたとしても、Q値の低下が生じ難い。これは、両側に反射器を必要としない共振器であり、伝搬ロスが少ないためである。また、上記反射器を必要としないのは、厚み滑りモードのバルク波を利用していることによる。従来の弾性波装置で利用したラム波と、上記厚み滑りモードのバルク波の相違を、図21及び図22を参照して説明する。 Since the elastic wave device 1 of this embodiment has the above configuration, even if the logarithm of the electrodes 3 and 4 is reduced in an attempt to achieve miniaturization, the Q value is unlikely to decrease. This is because the resonator does not require reflectors on both sides and has little propagation loss. Further, the reason why the reflector is not required is because the bulk wave in the thickness shear mode is used. The difference between the Lamb wave used in a conventional elastic wave device and the thickness-shear mode bulk wave will be explained with reference to FIGS. 21 and 22.
 図21は、弾性波装置の圧電膜を伝搬するラム波を説明するための模式的正面断面図である。図21に示すように、特許文献1(日本公開特許公報 特開2012-257019号公報)に記載のような弾性波装置では、圧電膜201中を矢印で示すように波が伝搬する。ここで、圧電膜201では、第1の主面201aと、第2の主面201bとが対向しており、第1の主面201aと第2の主面201bとを結ぶ厚み方向がZ方向である。X方向は、IDT電極の電極指が並んでいる方向である。図21に示すように、ラム波では、波が図示のように、X方向に伝搬していく。板波であるため、圧電膜201が全体として振動するものの、波はX方向に伝搬するため、両側に反射器を配置して、共振特性を得ている。そのため、波の伝搬ロスが生じ、小型化を図った場合、すなわち電極指の対数を少なくした場合、Q値が低下する。 FIG. 21 is a schematic front sectional view for explaining Lamb waves propagating through a piezoelectric film of an acoustic wave device. As shown in FIG. 21, in the elastic wave device described in Patent Document 1 (Japanese Patent Publication No. 2012-257019), waves propagate in the piezoelectric film 201 as indicated by arrows. Here, in the piezoelectric film 201, the first main surface 201a and the second main surface 201b are opposite to each other, and the thickness direction connecting the first main surface 201a and the second main surface 201b is the Z direction. It is. The X direction is the direction in which the electrode fingers of the IDT electrodes are lined up. As shown in FIG. 21, in the Lamb wave, the wave propagates in the X direction as shown. Since it is a plate wave, the piezoelectric film 201 vibrates as a whole, but since the wave propagates in the X direction, reflectors are placed on both sides to obtain resonance characteristics. Therefore, wave propagation loss occurs, and when miniaturization is attempted, that is, when the number of logarithms of electrode fingers is reduced, the Q value decreases.
 これに対して、図22は、弾性波装置の圧電層を伝播する厚み滑りモードのバルク波を説明するための模式的正面断面図である。図22に示すように、本実施形態の弾性波装置1では、振動変位は厚み滑り方向であるから、波は、圧電層2の第1の主面2aと第2の主面2bとを結ぶ方向、すなわちZ方向にほぼ伝搬し、共振する。すなわち、波のX方向成分がZ方向成分に比べて著しく小さい。そして、このZ方向の波の伝搬により共振特性が得られるため、反射器を必要としない。よって、反射器に伝搬する際の伝搬損失は生じない。従って、小型化を進めようとして、電極3,4からなる電極対の対数を減らしたとしても、Q値の低下が生じ難い。 In contrast, FIG. 22 is a schematic front cross-sectional view for explaining a thickness-shear mode bulk wave propagating through a piezoelectric layer of an elastic wave device. As shown in FIG. 22, in the elastic wave device 1 of this embodiment, since the vibration displacement is in the thickness-slip direction, the waves connect the first main surface 2a and the second main surface 2b of the piezoelectric layer 2. It propagates almost in the Z direction, and resonates. That is, the X-direction component of the wave is significantly smaller than the Z-direction component. Since resonance characteristics are obtained by the propagation of waves in the Z direction, a reflector is not required. Therefore, no propagation loss occurs when propagating to the reflector. Therefore, even if the number of electrode pairs consisting of electrodes 3 and 4 is reduced in an attempt to promote miniaturization, the Q value is unlikely to decrease.
 図23は、厚み滑りモードのバルク波の振幅方向を示す図である。厚み滑りモードのバルク波の振幅方向は、図23に示すように、圧電層2の励振領域Cに含まれる第1領域451と、励振領域Cに含まれる第2領域452とで逆になる。図23では、電極3と電極4との間に、電極4が電極3よりも高電位となる電圧が印加された場合のバルク波を模式的に示してある。第1領域451は、励振領域Cのうち、圧電層2の厚み方向に直交し圧電層2を2分する仮想平面VP1と、第1の主面2aとの間の領域である。第2領域452は、励振領域Cのうち、仮想平面VP1と、第2の主面2bとの間の領域である。 FIG. 23 is a diagram showing the amplitude direction of the bulk wave in the thickness shear mode. As shown in FIG. 23, the amplitude direction of the bulk wave in the thickness shear mode is opposite between the first region 451 included in the excitation region C of the piezoelectric layer 2 and the second region 452 included in the excitation region C. FIG. 23 schematically shows a bulk wave when a voltage is applied between electrode 3 and electrode 4 such that electrode 4 has a higher potential than electrode 3. In FIG. The first region 451 is a region of the excitation region C between a virtual plane VP1 that is perpendicular to the thickness direction of the piezoelectric layer 2 and bisects the piezoelectric layer 2, and the first main surface 2a. The second region 452 is a region of the excitation region C between the virtual plane VP1 and the second principal surface 2b.
 上記のように、弾性波装置1では、電極3と電極4とからなる少なくとも1対の電極が配置されているが、X方向に波を伝搬させるものではないため、この電極3,4からなる電極対の対数は複数対ある必要は必ずしもない。すなわち、少なくとも1対の電極が設けられてさえおればよい。 As mentioned above, in the elastic wave device 1, at least one pair of electrodes consisting of the electrode 3 and the electrode 4 are arranged, but since the wave is not propagated in the X direction, the elastic wave device 1 is made up of the electrodes 3 and 4. There does not necessarily have to be a plurality of pairs of electrodes. That is, it is only necessary that at least one pair of electrodes be provided.
 例えば、上記電極3がホット電位に接続される電極であり、電極4がグランド電位に接続される電極である。もっとも、電極3がグランド電位に、電極4がホット電位に接続されてもよい。本実施形態では、少なくとも1対の電極は、上記のように、ホット電位に接続される電極またはグランド電位に接続される電極であり、浮き電極は設けられていない。 For example, the electrode 3 is an electrode connected to a hot potential, and the electrode 4 is an electrode connected to a ground potential. However, the electrode 3 may be connected to the ground potential, and the electrode 4 may be connected to the hot potential. In this embodiment, at least one pair of electrodes is an electrode connected to a hot potential or an electrode connected to a ground potential, as described above, and no floating electrode is provided.
 図24は、図18に示す弾性波装置の共振特性の一例を示す図である。なお、この共振特性を得た弾性波装置1の設計パラメータは以下の通りである。 FIG. 24 is a diagram showing an example of the resonance characteristics of the elastic wave device shown in FIG. 18. Note that the design parameters of the elastic wave device 1 that obtained this resonance characteristic are as follows.
 圧電層2:オイラー角(0°,0°,90°)のLiNbO、厚み=400nm。
 電極3と電極4の長さ方向と直交する方向に視たときに、電極3と電極4とが重なっている領域、すなわち励振領域Cの長さ=40μm、電極3,4からなる電極の対数=21対、電極間中心距離=3μm、電極3,4の幅=500nm、d/p=0.133。
 中間層7:1μmの厚みの酸化ケイ素膜。
 支持基板8:Si基板。
Piezoelectric layer 2: LiNbO 3 with Euler angles (0°, 0°, 90°), thickness = 400 nm.
When viewed in a direction perpendicular to the length direction of electrodes 3 and 4, the area where electrodes 3 and 4 overlap, that is, the length of excitation area C = 40 μm, the logarithm of electrodes consisting of electrodes 3 and 4 = 21 pairs, center distance between electrodes = 3 μm, width of electrodes 3 and 4 = 500 nm, d/p = 0.133.
Intermediate layer 7: silicon oxide film with a thickness of 1 μm.
Support substrate 8: Si substrate.
 なお、励振領域Cの長さとは、励振領域Cの電極3,4の長さ方向に沿う寸法である。 Note that the length of the excitation region C is a dimension along the length direction of the electrodes 3 and 4 of the excitation region C.
 弾性波装置1では、電極3,4からなる電極対の電極間距離は、複数対において全て等しくした。すなわち、電極3と電極4とを等ピッチで配置した。 In the elastic wave device 1, the distances between the electrode pairs made up of the electrodes 3 and 4 were all equal in multiple pairs. That is, the electrodes 3 and 4 were arranged at equal pitches.
 図24から明らかなように、反射器を有しないにもかかわらず、比帯域が12.5%である良好な共振特性が得られている。 As is clear from FIG. 24, good resonance characteristics with a fractional band of 12.5% are obtained despite not having a reflector.
 ところで、上記圧電層2の厚みをd、電極3と電極4との電極の中心間距離をpとした場合、前述したように、本実施形態では、好ましくはd/pは0.5以下、より好ましくは0.24以下である。これを、図25を参照して説明する。 By the way, if the thickness of the piezoelectric layer 2 is d, and the center-to-center distance between the electrodes 3 and 4 is p, then in this embodiment, as described above, d/p is preferably 0.5 or less, More preferably it is 0.24 or less. This will be explained with reference to FIG. 25.
 図24に示した共振特性を得た弾性波装置と同様に、但しd/2pを変化させ、複数の弾性波装置を得た。図25は、隣り合う電極の中心間距離をp、圧電層の厚みをdとした場合のd/2pと、弾性波装置の共振子としての比帯域との関係を示す図である。 A plurality of elastic wave devices were obtained in the same way as the elastic wave devices that obtained the resonance characteristics shown in FIG. 24, except that d/2p was changed. FIG. 25 is a diagram showing the relationship between d/2p and the fractional band as a resonator of an acoustic wave device, where p is the distance between the centers of adjacent electrodes and d is the thickness of the piezoelectric layer.
 図25から明らかなように、d/2pが0.25を超えると、すなわちd/p>0.5では、d/pを調整しても、比帯域は5%未満である。これに対して、d/2p≦0.25、すなわちd/p≦0.5の場合には、その範囲内でd/pを変化させれば、比帯域を5%以上とすることができ、すなわち高い結合係数を有する共振子を構成することができる。また、d/2pが0.12以下の場合、すなわちd/pが0.24以下の場合には、比帯域を7%以上と高めることができる。加えて、d/pをこの範囲内で調整すれば、より一層比帯域の広い共振子を得ることができ、より一層高い結合係数を有する共振子を実現することができる。従って、d/pを0.5以下とすることにより、上記厚み滑りモードのバルク波を利用した、高い結合係数を有する共振子を構成し得ることがわかる。 As is clear from FIG. 25, when d/2p exceeds 0.25, that is, when d/p>0.5, the fractional band is less than 5% even if d/p is adjusted. On the other hand, if d/2p≦0.25, that is, d/p≦0.5, the fractional bandwidth can be increased to 5% or more by changing d/p within that range. In other words, a resonator having a high coupling coefficient can be constructed. Further, when d/2p is 0.12 or less, that is, when d/p is 0.24 or less, the fractional band can be increased to 7% or more. In addition, by adjusting d/p within this range, it is possible to obtain a resonator with an even wider specific band, and it is possible to realize a resonator with an even higher coupling coefficient. Therefore, it can be seen that by setting d/p to 0.5 or less, it is possible to construct a resonator that utilizes the bulk wave of the thickness shear mode and has a high coupling coefficient.
 なお、前述したように、少なくとも1対の電極は、1対でもよく、上記pは、1対の電極の場合、隣り合う電極3,4の中心間距離とする。また、1.5対以上の電極の場合には、隣り合う電極3,4の中心間距離の平均距離をpとすればよい。 Note that, as described above, the at least one pair of electrodes may be one pair, and in the case of one pair of electrodes, the above p is the distance between the centers of adjacent electrodes 3 and 4. Furthermore, in the case of 1.5 or more pairs of electrodes, the average distance between the centers of adjacent electrodes 3 and 4 may be set to p.
 また、圧電層の厚みdについては、圧電層2が厚みばらつきを有する場合、その厚みを平均化した値を採用すればよい。 Further, regarding the thickness d of the piezoelectric layer, if the piezoelectric layer 2 has thickness variations, a value obtained by averaging the thicknesses may be adopted.
 図26は、厚み滑りモードのバルク波を利用する弾性波装置の別の一例の平面図である。 FIG. 26 is a plan view of another example of an elastic wave device that utilizes bulk waves in thickness-shear mode.
 弾性波装置61では、圧電層2の第1の主面2a上において、電極3と電極4とを有する1対の電極が設けられている。なお、図26中のKが交差幅となる。前述したように、本実施形態の弾性波装置では、電極の対数は1対であってもよい。この場合においても、上記d/pが0.5以下であれば、厚み滑りモードのバルク波を効果的に励振することができる。 In the elastic wave device 61, a pair of electrodes including an electrode 3 and an electrode 4 are provided on the first main surface 2a of the piezoelectric layer 2. Note that K in FIG. 26 is the intersection width. As described above, in the elastic wave device of this embodiment, the number of pairs of electrodes may be one. Even in this case, if the above-mentioned d/p is 0.5 or less, bulk waves in the thickness shear mode can be excited effectively.
 本実施形態の弾性波装置では、好ましくは、複数の電極3,4において、いずれかの隣り合う電極3,4が対向している方向に視たときに重なっている領域である励振領域に対する、上記隣り合う電極3,4のメタライゼーション比MRが、MR≦1.75(d/p)+0.075を満たすことが望ましい。その場合には、スプリアスを効果的に小さくすることができる。これを、図27及び図28を参照して説明する。 In the elastic wave device of this embodiment, preferably, in the plurality of electrodes 3 and 4, for an excitation region that is an overlapping region when viewed in the direction in which any of the adjacent electrodes 3 and 4 are facing each other, It is desirable that the metallization ratio MR of the adjacent electrodes 3 and 4 satisfies MR≦1.75(d/p)+0.075. In that case, spurious can be effectively reduced. This will be explained with reference to FIGS. 27 and 28.
 図27は、図18に示す弾性波装置の共振特性の一例を示す参考図である。矢印Bで示すスプリアスが、共振周波数と反共振周波数との間に現れている。なお、d/p=0.08として、かつLiNbOのオイラー角(0°,0°,90°)とした。また、上記メタライゼーション比MR=0.35とした。 FIG. 27 is a reference diagram showing an example of the resonance characteristics of the elastic wave device shown in FIG. 18. A spurious signal indicated by arrow B appears between the resonant frequency and the anti-resonant frequency. Note that d/p=0.08 and the Euler angles of LiNbO 3 (0°, 0°, 90°). Further, the metallization ratio MR was set to 0.35.
 メタライゼーション比MRを、図19を参照して説明する。図19の電極構造において、1対の電極3,4に着目した場合、この1対の電極3,4のみが設けられるとする。この場合、一点鎖線Cで囲まれた部分が励振領域となる。この励振領域とは、電極3と電極4とを、電極3,4の長さ方向と直交する方向すなわち対向方向に視たときに電極3における電極4と重なり合っている領域、電極4における電極3と重なり合っている領域、及び、電極3と電極4との間の領域における電極3と電極4とが重なり合っている領域である。そして、この励振領域の面積に対する、励振領域C内の電極3,4の面積が、メタライゼーション比MRとなる。すなわち、メタライゼーション比MRは、メタライゼーション部分の面積の励振領域の面積に対する比である。 The metallization ratio MR will be explained with reference to FIG. 19. In the electrode structure of FIG. 19, when focusing on a pair of electrodes 3 and 4, it is assumed that only this pair of electrodes 3 and 4 are provided. In this case, the area surrounded by the dashed line C becomes the excitation region. This excitation region is the region where the electrode 3 overlaps the electrode 4 when the electrode 3 and the electrode 4 are viewed in a direction perpendicular to the length direction of the electrodes 3 and 4, that is, in a direction in which they face each other. and a region between electrodes 3 and 4 where electrodes 3 and 4 overlap. Then, the area of the electrodes 3 and 4 in the excitation region C with respect to the area of this excitation region becomes the metallization ratio MR. That is, the metallization ratio MR is the ratio of the area of the metallized portion to the area of the excitation region.
 なお、複数対の電極が設けられている場合、励振領域の面積の合計に対する全励振領域に含まれているメタライゼーション部分の割合をMRとすればよい。 Note that when multiple pairs of electrodes are provided, MR may be the ratio of the metallized portion included in all the excitation regions to the total area of the excitation regions.
 図28は、本実施形態に従って、多数の弾性波共振子を構成した場合の比帯域と、スプリアスの大きさとしての180度で規格化されたスプリアスのインピーダンスの位相回転量との関係を示す図である。なお、比帯域については、圧電層の膜厚や電極の寸法を種々変更し、調整した。また、図28は、ZカットのLiNbOからなる圧電層を用いた場合の結果であるが、他のカット角の圧電層を用いた場合においても、同様の傾向となる。 FIG. 28 is a diagram showing the relationship between the fractional band and the amount of phase rotation of spurious impedance normalized by 180 degrees as the magnitude of spurious when a large number of elastic wave resonators are configured according to the present embodiment. It is. Note that the specific band was adjusted by variously changing the thickness of the piezoelectric layer and the dimensions of the electrode. Further, although FIG. 28 shows the results when a Z-cut piezoelectric layer made of LiNbO 3 is used, the same tendency is obtained when piezoelectric layers with other cut angles are used.
 図28中の楕円Jで囲まれている領域では、スプリアスが1.0と大きくなっている。図28から明らかなように、比帯域が0.17を超えると、すなわち17%を超えると、スプリアスレベルが1以上の大きなスプリアスが、比帯域を構成するパラメータを変化させたとしても、通過帯域内に現れる。すなわち、図27に示す共振特性のように、矢印Bで示す大きなスプリアスが帯域内に現れる。よって、比帯域は17%以下であることが好ましい。この場合には、圧電層2の膜厚や電極3,4の寸法などを調整することにより、スプリアスを小さくすることができる。 In the area surrounded by the ellipse J in FIG. 28, the spurious is as large as 1.0. As is clear from FIG. 28, when the fractional band exceeds 0.17, that is, exceeds 17%, a large spurious with a spurious level of 1 or more will affect the pass band even if the parameters that make up the fractional band are changed. Appear within. That is, as in the resonance characteristic shown in FIG. 27, a large spurious signal indicated by arrow B appears within the band. Therefore, it is preferable that the fractional band is 17% or less. In this case, by adjusting the thickness of the piezoelectric layer 2, the dimensions of the electrodes 3 and 4, etc., the spurious can be reduced.
 図29は、d/2pと、メタライゼーション比MRと、比帯域との関係を示す図である。上記弾性波装置において、d/2pと、MRが異なる様々な弾性波装置を構成し、比帯域を測定した。 FIG. 29 is a diagram showing the relationship between d/2p, metallization ratio MR, and fractional band. Among the above elastic wave devices, various elastic wave devices having different d/2p and MR were constructed and the fractional bands were measured.
 図29の破線Dの右側のハッチングを付して示した部分が、比帯域が17%以下の領域である。このハッチングを付した領域と、付していない領域との境界は、MR=3.5(d/2p)+0.075で表される。すなわち、MR=1.75(d/p)+0.075である。従って、好ましくは、MR≦1.75(d/p)+0.075である。その場合には、比帯域を17%以下としやすい。より好ましくは、図29中の一点鎖線D1で示すMR=3.5(d/2p)+0.05の右側の領域である。すなわち、MR≦1.75(d/p)+0.05であれば、比帯域を確実に17%以下にすることができる。 The hatched area on the right side of the broken line D in FIG. 29 is the area where the fractional band is 17% or less. The boundary between the hatched area and the unhatched area is expressed as MR=3.5(d/2p)+0.075. That is, MR=1.75(d/p)+0.075. Therefore, preferably MR≦1.75 (d/p)+0.075. In that case, it is easy to set the fractional band to 17% or less. More preferably, it is the region to the right of MR=3.5(d/2p)+0.05 indicated by the dashed line D1 in FIG. That is, if MR≦1.75(d/p)+0.05, the fractional band can be reliably set to 17% or less.
 図30は、d/pを限りなく0に近づけた場合のLiNbOのオイラー角(0°,θ,ψ)に対する比帯域のマップを示す図である。 FIG. 30 is a diagram showing a map of fractional bands with respect to Euler angles (0°, θ, ψ) of LiNbO 3 when d/p is brought as close to 0 as possible.
 図30のハッチングを付して示した部分が、少なくとも5%以上の比帯域が得られる領域であり、当該領域の範囲を近似すると、下記の式(1)、式(2)及び式(3)で表される範囲となる。
 (0°±10°,0°~20°,任意のψ)  …式(1)
 (0°±10°,20°~80°,0°~60°(1-(θ-50)/900)1/2) または (0°±10°,20°~80°,[180°-60°(1-(θ-50)/900)1/2]~180°)  …式(2)
 (0°±10°,[180°-30°(1-(ψ-90)/8100)1/2]~180°,任意のψ)  …式(3)
 従って、上記式(1)、式(2)または式(3)のオイラー角範囲の場合、比帯域を十分に広くすることができるため好ましい。
The hatched areas in FIG. 30 are areas where a fractional band of at least 5% can be obtained, and the range of the area can be approximated by the following equations (1), (2), and (3). ).
(0°±10°, 0° to 20°, arbitrary ψ) ...Formula (1)
(0°±10°, 20° to 80°, 0° to 60° (1-(θ-50) 2 /900) 1/2 ) or (0°±10°, 20° to 80°, [180 °-60° (1-(θ-50) 2 /900) 1/2 ] ~ 180°) ...Formula (2)
(0°±10°, [180°-30° (1-(ψ-90) 2 /8100) 1/2 ] ~ 180°, arbitrary ψ) ...Formula (3)
Therefore, the Euler angle range of formula (1), formula (2), or formula (3) above is preferable because the fractional band can be made sufficiently wide.
 図31は、ラム波を利用する弾性波装置の一例を説明するための部分切り欠き斜視図である。 FIG. 31 is a partially cutaway perspective view for explaining an example of an elastic wave device that utilizes Lamb waves.
 弾性波装置81は、支持基板82を有する。支持基板82には、上面に開いた凹部が設けられている。支持基板82上に圧電層83が積層されている。それによって、空洞部9が構成されている。この空洞部9の上方において圧電層83上に、IDT電極84が設けられている。IDT電極84の弾性波伝搬方向両側に、反射器85,86が設けられている。図31において、空洞部9の外周縁を破線で示す。ここでは、IDT電極84は、第1のバスバー電極84aと、第2のバスバー電極84bと、複数本の第1の電極指としての電極84cと、複数本の第2の電極指としての電極84dとを有する。複数本の電極84cは、第1のバスバー電極84aに接続されている。複数本の電極84dは、第2のバスバー電極84bに接続されている。複数本の電極84cと、複数本の電極84dとは間挿し合っている。 The elastic wave device 81 has a support substrate 82. The support substrate 82 is provided with an open recess on the upper surface. A piezoelectric layer 83 is laminated on the support substrate 82 . Thereby, a cavity 9 is formed. An IDT electrode 84 is provided on the piezoelectric layer 83 above the cavity 9 . Reflectors 85 and 86 are provided on both sides of the IDT electrode 84 in the elastic wave propagation direction. In FIG. 31, the outer peripheral edge of the cavity 9 is shown by a broken line. Here, the IDT electrode 84 includes a first busbar electrode 84a, a second busbar electrode 84b, an electrode 84c as a plurality of first electrode fingers, and an electrode 84d as a plurality of second electrode fingers. and has. The plurality of electrodes 84c are connected to the first busbar electrode 84a. The plurality of electrodes 84d are connected to the second busbar electrode 84b. The plurality of electrodes 84c and the plurality of electrodes 84d are interposed with each other.
 弾性波装置81では、上記空洞部9上のIDT電極84に、交流電界を印加することにより、板波としてのラム波が励振される。そして、反射器85,86が両側に設けられているため、上記ラム波による共振特性を得ることができる。 In the elastic wave device 81, by applying an alternating current electric field to the IDT electrode 84 on the cavity 9, a Lamb wave as a plate wave is excited. Since the reflectors 85 and 86 are provided on both sides, the resonance characteristic due to the Lamb wave described above can be obtained.
 このように、本発明の弾性波装置は、ラム波等の板波を利用するものであってもよい。 In this way, the elastic wave device of the present invention may utilize plate waves such as Lamb waves.
 1 弾性波装置
 2 圧電層
 2a 圧電層の第1の主面
 2b 圧電層の第2の主面
 3 第1電極
 4 第2電極
 5 第1のバスバー電極
 6 第2のバスバー電極
 7 中間層
 7a 開口部
 8 支持基板
 8a 開口部
 9 空洞部
 10、10A 弾性波装置
 20 支持部材
 21 圧電層
 21M メンブレン部
 22 機能電極
 23 空洞部
 24 亀裂
 26 配線電極
 28 保護電極
 31 圧電基板
 40 犠牲層
 40A 無機物の犠牲層
 40B 有機物の犠牲層
 41 中間層
 42 支持基板
 50 保護レジスト
 51 エッチング用孔
 52 一様な縦筋
 53 縦筋
 54 へき開面
 61 弾性波装置
 81 弾性波装置
 82 支持基板
 83 圧電層
 84 IDT電極
 84a 第1のバスバー電極
 84b 第2のバスバー電極
 84c 第1電極(第1電極指)
 84d 第2電極(第2電極指)
 85、86 反射器
 90 弾性波装置
 91 支持基板
 92 圧電層
 92a 圧電層の第1の主面
 92b 圧電層の第2の主面
 93 空洞部
 94 上部電極
 95 下部電極
 201 圧電膜
 201a 圧電膜の第1の主面
 201b 圧電膜の第2の主面
 451 第1領域
 452 第2領域
 C 励振領域
 VP1 仮想平面
 T21 圧電層の厚み
 L24 亀裂の長さ
 W24 亀裂の幅
1 Acoustic wave device 2 Piezoelectric layer 2a First main surface of piezoelectric layer 2b Second main surface of piezoelectric layer 3 First electrode 4 Second electrode 5 First busbar electrode 6 Second busbar electrode 7 Intermediate layer 7a Opening Section 8 Support substrate 8a Opening 9 Cavity 10, 10A Acoustic wave device 20 Support member 21 Piezoelectric layer 21M Membrane section 22 Functional electrode 23 Cavity 24 Crack 26 Wiring electrode 28 Protective electrode 31 Piezoelectric substrate 40 Sacrificial layer 40A Inorganic sacrificial layer 40B Organic sacrificial layer 41 Intermediate layer 42 Support substrate 50 Protective resist 51 Etching holes 52 Uniform vertical stripes 53 Vertical stripes 54 Cleavage plane 61 Acoustic wave device 81 Acoustic wave device 82 Support substrate 83 Piezoelectric layer 84 IDT electrode 84a 1st Busbar electrode 84b Second busbar electrode 84c First electrode (first electrode finger)
84d Second electrode (second electrode finger)
85, 86 reflector 90 acoustic wave device 91 support substrate 92 piezoelectric layer 92a first main surface of piezoelectric layer 92b second main surface of piezoelectric layer 93 cavity 94 upper electrode 95 lower electrode 201 piezoelectric film 201a first main surface of piezoelectric film 1 principal surface 201b second principal surface of piezoelectric film 451 first region 452 second region C excitation region VP1 virtual plane T 21 thickness of piezoelectric layer L 24 length of crack W 24 width of crack

Claims (14)

  1.  空洞部を一方主面に有する支持部材と、
     前記空洞部を覆うように前記支持部材の前記一方主面に設けられた圧電層と、
     前記圧電層の少なくとも一方の主面に、前記圧電層の厚み方向から見て少なくとも一部が前記空洞部と重なるように設けられた機能電極と、
    を備え、
     前記圧電層には、前記厚み方向から見て前記空洞部と重なり、かつ、前記機能電極が設けられていない領域において、前記圧電層の厚みよりも幅が小さく、前記圧電層の一方の主面から他方の主面に連通する亀裂が設けられている、
     弾性波装置。
    a support member having a hollow portion on one main surface;
    a piezoelectric layer provided on the one main surface of the support member so as to cover the cavity;
    a functional electrode provided on at least one main surface of the piezoelectric layer so that at least a portion thereof overlaps with the cavity when viewed from the thickness direction of the piezoelectric layer;
    Equipped with
    The piezoelectric layer has a width smaller than the thickness of the piezoelectric layer in a region that overlaps with the cavity and is not provided with the functional electrode when viewed from the thickness direction, and one main surface of the piezoelectric layer. A crack is provided that communicates from one main surface to the other main surface,
    Elastic wave device.
  2.  前記亀裂が設けられた部分の前記圧電層の側面には、前記圧電層の厚み方向に蛇行する縦筋と、前記圧電層の厚み方向に沿った縦筋の無いへき開面とが混在する、
     請求項1に記載の弾性波装置。
    On the side surface of the piezoelectric layer in the portion where the crack is provided, vertical streaks meandering in the thickness direction of the piezoelectric layer and cleavage planes without vertical streaks along the thickness direction of the piezoelectric layer are mixed.
    The elastic wave device according to claim 1.
  3.  前記圧電層には、前記圧電層の厚み方向から見て前記空洞部と重なり、かつ、前記機能電極が設けられていない領域において、前記亀裂以外に前記圧電層を厚み方向に貫通する穴が設けられていない、
     請求項1又は2に記載の弾性波装置。
    The piezoelectric layer is provided with a hole that penetrates the piezoelectric layer in the thickness direction in addition to the crack in a region that overlaps with the cavity when viewed from the thickness direction of the piezoelectric layer and in which the functional electrode is not provided. has not been
    The elastic wave device according to claim 1 or 2.
  4.  前記圧電層を前記厚み方向から見たとき、前記亀裂は、前記空洞部の外周縁と重なる領域に設けられている、
     請求項1~3のいずれか1項に記載の弾性波装置。
    When the piezoelectric layer is viewed from the thickness direction, the crack is provided in a region that overlaps with the outer peripheral edge of the cavity.
    The elastic wave device according to any one of claims 1 to 3.
  5.  前記圧電層を前記厚み方向から見たとき、前記亀裂は、前記空洞部の外周縁を跨ぐ前記機能電極と重なる領域に設けられていない、
     請求項4に記載の弾性波装置。
    When the piezoelectric layer is viewed from the thickness direction, the crack is not provided in a region overlapping with the functional electrode that straddles the outer peripheral edge of the cavity.
    The elastic wave device according to claim 4.
  6.  前記機能電極は、1以上の第1電極と、前記1以上の第1電極が接続された第1のバスバー電極と、1以上の第2電極と、前記1以上の第2電極が接続された第2のバスバー電極と、を有する、
     請求項1~5のいずれか1項に記載の弾性波装置。
    The functional electrode includes one or more first electrodes, a first busbar electrode to which the one or more first electrodes are connected, one or more second electrodes, and the one or more second electrodes to which the functional electrode is connected. a second busbar electrode;
    The elastic wave device according to any one of claims 1 to 5.
  7.  前記圧電層の厚みは、前記1以上の第1電極と前記1以上の第2電極のうち、隣り合う第1電極と第2電極との間の中心間距離をpとした場合に2p以下である、
     請求項6に記載の弾性波装置。
    The thickness of the piezoelectric layer is 2p or less, where p is the center-to-center distance between adjacent first electrodes and second electrodes among the one or more first electrodes and the one or more second electrodes. be,
    The elastic wave device according to claim 6.
  8.  前記圧電層が、ニオブ酸リチウム又はタンタル酸リチウムからなる、
     請求項1~5のいずれか1項に記載の弾性波装置。
    The piezoelectric layer is made of lithium niobate or lithium tantalate,
    The elastic wave device according to any one of claims 1 to 5.
  9.  厚み滑りモードのバルク波を利用可能に構成されている、
     請求項8に記載の弾性波装置。
    It is configured to be able to utilize bulk waves in thickness-slip mode.
    The elastic wave device according to claim 8.
  10.  前記圧電層の厚みをd、前記1以上の第1電極と前記1以上の第2電極のうち、隣り合う第1電極と第2電極との間の中心間距離をpとした場合、d/p≦0.5である、
     請求項6に記載の弾性波装置。
    If the thickness of the piezoelectric layer is d, and the center-to-center distance between adjacent first and second electrodes among the one or more first electrodes and the one or more second electrodes is p, then d/ p≦0.5,
    The elastic wave device according to claim 6.
  11.  d/p≦0.24である、
     請求項10に記載の弾性波装置。
    d/p≦0.24,
    The elastic wave device according to claim 10.
  12.  前記1以上の第1電極と前記1以上の第2電極のうち、隣り合う第1電極と第2電極とが対向している方向に視たときに重なっている励振領域の面積に対する、前記隣り合う第1電極と第2電極との面積の割合であるメタライゼーション比をMR、前記圧電層の厚みをd、前記隣り合う第1電極と第2電極との中心間距離をpとした場合、MR≦1.75(d/p)+0.075である、
     請求項6、10又は11に記載の弾性波装置。
    Of the one or more first electrodes and the one or more second electrodes, the area of the excitation region that overlaps when viewed in the direction in which adjacent first electrodes and second electrodes face each other, When the metallization ratio, which is the area ratio of the first electrode and the second electrode that match, is MR, the thickness of the piezoelectric layer is d, and the distance between the centers of the adjacent first and second electrodes is p, MR≦1.75(d/p)+0.075,
    The elastic wave device according to claim 6, 10 or 11.
  13.  MR≦1.75(d/p)+0.05である、
     請求項12に記載の弾性波装置。
    MR≦1.75(d/p)+0.05,
    The elastic wave device according to claim 12.
  14.  前記ニオブ酸リチウム又はタンタル酸リチウムのオイラー角(φ,θ,ψ)が、以下の式(1)、式(2)又は式(3)の範囲にある、
     請求項8に記載の弾性波装置。
     (0°±10°,0°~20°,任意のψ)  …式(1)
     (0°±10°,20°~80°,0°~60°(1-(θ-50)/900)1/2) または (0°±10°,20°~80°,[180°-60°(1-(θ-50)/900)1/2]~180°)  …式(2)
     (0°±10°,[180°-30°(1-(ψ-90)/8100)1/2]~180°,任意のψ)  …式(3)
    The Euler angles (φ, θ, ψ) of the lithium niobate or lithium tantalate are in the range of the following formula (1), formula (2) or formula (3),
    The elastic wave device according to claim 8.
    (0°±10°, 0° to 20°, arbitrary ψ) ...Formula (1)
    (0°±10°, 20° to 80°, 0° to 60° (1-(θ-50) 2 /900) 1/2 ) or (0°±10°, 20° to 80°, [180 °-60° (1-(θ-50) 2 /900) 1/2 ] ~ 180°) ...Formula (2)
    (0°±10°, [180°-30° (1-(ψ-90) 2 /8100) 1/2 ] ~ 180°, arbitrary ψ) ...Formula (3)
PCT/JP2023/012836 2022-03-31 2023-03-29 Elastic wave device WO2023190697A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US202263325811P 2022-03-31 2022-03-31
US63/325,811 2022-03-31

Publications (1)

Publication Number Publication Date
WO2023190697A1 true WO2023190697A1 (en) 2023-10-05

Family

ID=88202056

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/JP2023/012836 WO2023190697A1 (en) 2022-03-31 2023-03-29 Elastic wave device

Country Status (1)

Country Link
WO (1) WO2023190697A1 (en)

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010136317A (en) * 2008-03-24 2010-06-17 Ngk Insulators Ltd Method of manufacturing bulk-elastic wave device
JP2011029526A (en) * 2009-07-29 2011-02-10 Murata Mfg Co Ltd Method of manufacturing composite substrate
JP2016123016A (en) * 2014-12-25 2016-07-07 株式会社村田製作所 Acoustic wave device and method of manufacturing the same
JP2017108288A (en) * 2015-12-09 2017-06-15 太陽誘電株式会社 Piezoelectric thin film resonator and filter
WO2017221649A1 (en) * 2016-06-21 2017-12-28 株式会社ユーテック Film structure and method for manufacturing same
US20210328575A1 (en) * 2018-06-15 2021-10-21 Resonant Inc. Film bulk acoustic resonator fabrication method

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010136317A (en) * 2008-03-24 2010-06-17 Ngk Insulators Ltd Method of manufacturing bulk-elastic wave device
JP2011029526A (en) * 2009-07-29 2011-02-10 Murata Mfg Co Ltd Method of manufacturing composite substrate
JP2016123016A (en) * 2014-12-25 2016-07-07 株式会社村田製作所 Acoustic wave device and method of manufacturing the same
JP2017108288A (en) * 2015-12-09 2017-06-15 太陽誘電株式会社 Piezoelectric thin film resonator and filter
WO2017221649A1 (en) * 2016-06-21 2017-12-28 株式会社ユーテック Film structure and method for manufacturing same
US20210328575A1 (en) * 2018-06-15 2021-10-21 Resonant Inc. Film bulk acoustic resonator fabrication method

Similar Documents

Publication Publication Date Title
WO2022085581A1 (en) Acoustic wave device
WO2023223906A1 (en) Elastic wave element
WO2023085362A1 (en) Elastic wave device
WO2022138328A1 (en) Surface acoustic wave device
WO2022131309A1 (en) Elastic wave device
WO2022102596A1 (en) Elastic wave device
WO2022124391A1 (en) Elastic wave device
WO2023190697A1 (en) Elastic wave device
WO2023204250A1 (en) Elastic wave device
WO2022210687A1 (en) Elastic wave device
WO2023190700A1 (en) Elastic wave device
WO2022210694A1 (en) Elastic wave device
WO2023195409A1 (en) Elastic wave device and production method for elastic wave device
WO2022071488A1 (en) Elastic wave device
WO2022211103A1 (en) Elastic wave device and method for manufacturing elastic wave device
WO2023199837A1 (en) Elastic wave device
WO2023058715A1 (en) Elastic wave device
WO2023210764A1 (en) Acoustic wave element and acoustic wave device
WO2023195523A1 (en) Elastic wave device
US20240048115A1 (en) Acoustic wave device and method of manufacturing acoustic wave device
WO2023191089A1 (en) Elastic wave device
WO2023140362A1 (en) Acoustic wave device and method for manufacturing acoustic wave device
WO2022211055A1 (en) Elastic wave device
US20230327638A1 (en) Acoustic wave device
WO2023190721A1 (en) Elastic wave device

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 23780706

Country of ref document: EP

Kind code of ref document: A1