Acoustic resonator and filter

A first supporting section provided between a substrate section and a second supporting section. The first supporting section is structured by, e.g., a film formed from a material having a higher acoustic impedance than a piezoelectric body and the substrate section, or a film formed from a material having a smaller Q value than the piezoelectric body and substrate section. By inserting the first supporting section, most vibration from the second supporting section toward the substrate section is reflected, and also a vibration having been transmitted to the substrate section from the second supporting section is prevented from reflecting at the bottom of the substrate section 40 and then returning in a direction of the vibration section.

BACKGROUND OF THE INVENTION

1. Technical Field

The present invention relates to an acoustic resonator and a filter, and particularly to an acoustic resonator, which is capable of suppressing a spurious occurrence, and a filter using the acoustic resonator.

2. Background Art

Components embedded in electronic device such as portable devices are required to decrease in size and weight. For example, a filter used in portable devices is required to decrease in size, and also required to be capable of precisely adjusting a frequency characteristic. A filter using an acoustic resonator is known as a filter satisfying such requirements (refer to Patent Documents 1 to 3).

Hereinafter, a conventional acoustic resonator disclosed in Patent Document 1 will be described with reference toFIGS. 13A to 13D.

FIG. 13Ais a cross-sectional view showing a fundamental structure of the conventional acoustic resonator. The conventional acoustic resonator has a structure in which a piezoelectric body101is provided between an upper electrode102and a lower electrode103. This conventional acoustic resonator is used while mounted on a substrate105in which a cavity104is formed. The cavity104can be formed by performing, on the back of the substrate105, partial etching using microfabrication method. In this conventional acoustic resonator, when a electric field is applied in a thickness direction via the upper and lower electrodes102and103, a vibration occurs in the thickness direction. Next, operations of the conventional acoustic resonator will be described referring to a thickness longitudinal vibration occurring in an infinite plane.

FIG. 13Bis a schematic perspective view for describing the operations of the conventional acoustic resonator. When an electric field is applied between the upper and lower electrodes102and103in the conventional acoustic resonator, an electrical energy is converted into a mechanical energy at the piezoelectric body101. A mechanical vibration induced here is an extensional vibration in the thickness direction, which vibration extends and contracts in a same direction as that of the electric field. In general, the conventional acoustic resonator uses a resonant vibration in the thickness direction in the piezoelectric body101. The conventional acoustic resonator operates to resonate at a frequency whose half wavelength is equivalent to a thickness of the piezoelectric body101. The cavity104shown inFIG. 13Ais used for obtaining a thickness longitudinal vibration of the piezoelectric body101.

As shown inFIG. 13D, in an equivalent circuit of the conventional acoustic resonator, both a serial resonance and a parallel resonance occur. The equivalent circuit comprises: a serial resonance section including a capacitor C1, inductor L1and resistor R1; and a capacitor C0connected in parallel with the serial resonance section. As shown inFIG. 13C, an admittance frequency characteristic of the equivalent circuit in this circuit configuration has an admittance which becomes maximum at a resonance frequency fr and minimum at an antiresonance frequency fa. Here, a relationship between the resonance frequency fr and antiresonance frequency fa is as follows:
fr=1/{2π√{square root over ( )}(L1×C1)}
fa=fr√{square root over ( )}(1+C1/C0)

When the conventional acoustic resonator having the above admittance frequency characteristic is applied as a filter, the resonant vibration of the piezoelectric body101is utilized. This allows the filter to be realized as a small-sized low-loss filter.

Here, a piezoelectric thin film which greatly affects a characteristic of the acoustic resonator is desired to be of high quality. For this reason, various manufacturing methods for realizing a high-quality piezoelectric thin film have been suggested (refer to Patent Document 4).FIG. 14illustrates steps of a conventional acoustic resonator manufacturing method disclosed in Patent Document 4.

First, etching is performed on a substrate111to form, on the substrate111, a hollow which is later formed into a cavity112(FIG. 14(a)). Then, a sacrifice layer115is formed on an entire surface of the substrate111(FIG. 14(b). Next, planarization is performed such that the surface of the substrate111and a surface of the sacrifice layer115have a same height (FIG. 14(c)). Subsequently, a lower electrode121, piezoelectric thin film122and upper electrode123are laminated thereon, whereby a vibration section120is formed (FIG. 14(d)). Lastly, the sacrifice layer115is removed by etching, whereby the cavity112is provided, and thus the acoustic resonator is completed (FIG. 14(e)). In Patent Document 4, a film thickness and flatness of molybdenum (Mo), which is the lower electrode121, are specified so as to improve crystallinity of the piezoelectric thin film. This allows a piezoelectric thin film having a high quality to be realized by using a spatter method.

Patent Document 1: Japanese National Phase PCT Lain-Open Publication No. 60-68711

SUMMARY DISCLOSURE OF THE INVENTION

Since the above-described conventional acoustic resonator is partially fixed on the substrate105, it is inevitable that a vibration from the vibration section is partially transmitted to the substrate105. Such an unnecessary vibration transmitted to the substrate105reflects on the bottom of the substrate105, and then returns to the vibration section. As a result, a main resonant vibration of the vibration section (arrow e ofFIG. 15) is affected.

This causes, as shown inFIG. 16A, a spurious vibration to occur between a resonance frequency of the vibration section and an antiresonance frequency of the vibration section. When acoustic resonators having such a spurious occurrence are connected in parallel to form a filter as shown inFIG. 16B, an unfavorable pass characteristic appears in a passband as shown inFIG. 16C. This pass characteristic causes deterioration in communication quality.

Also, in the conventional manufacturing method, crystallinity of the piezoelectric thin film is greatly affected by a base. Therefore, a material used for the base is required to have high crystallinity and high flatness. When a structure between the vibration section, which is structured by the piezoelectric thin film and upper and lower electrodes, and the substrate is complex, crystallinity and flatness of a base film of the piezoelectric thin film are affected. For this reason, in order to obtain, e.g., desired flatness, such a process as a planarization process is required to be performed before forming the piezoelectric thin film. Thus, there is a problem of, e.g., complex processes.

It is known that in order to realize a high quality piezoelectric thin film, film forming using Metal Organic Chemical Vapor Deposition (MOCVD) is more suitable than film forming using a spatter method. However, MOCVD requires a process performed under a high temperature of approximately 1000° C. For this reason, in the case of a manufacturing method in which film forming and lamination are sequentially performed from a lower part in ascending order, such as the above-described conventional acoustic resonator manufacturing method, there is a problem that a material used for, e.g., an electrode is restricted to the one which endures the high temperature process of MOCVD. A conceivable manufacturing method to overcome the problem of this high temperature process may be a manufacturing method in which film forming and lamination are not sequentially performed from a lower part in ascending order, e.g., a manufacturing method in which an electrode film or the like is formed from a back side of a substrate after the piezoelectric thin film is formed. However, a practical and effective manufacturing method is yet to be realized.

Therefore, an object of the present invention is to provide an acoustic resonator and a filter which are capable of preventing the unnecessary vibration, which returns after reflecting on the bottom of a substrate, and suppressing spurious occurrences.

Another object of the present invention is to provide a manufacturing method using a technique for affixing substrates, which manufacturing method allows an electrode film or the like to be formed after a piezoelectric thin film is formed, thereby enabling, even if a structure of a supporting section is complex, an acoustic resonator using the piezoelectric thin film having high crystallinity to be manufactured.

The present invention is directed to an acoustic resonator which vibrates at a predetermined frequency. In order to achieve the aforementioned object, the acoustic resonator of the present invention comprises: a substrate; a first supporting section provided on the substrate; a second supporting section provided on the first supporting section, or an acoustic mirror section which is a result of alternately layering a low impedance layer and a high impedance layer; and a vibration section provided on the second supporting section or on the acoustic mirror section, the vibration section including at least a piezoelectric body, an upper electrode provided on an upper surface of the piezoelectric body, and a lower electrode provided on a lower surface of the piezoelectric body.

Preferably, the first supporting section is formed from a material having a higher acoustic impedance than the substrate, which material is, e.g., a result of eutectic crystallization of gold and tin. In the case where the second supporting section is provided on the first supporting section, a thickness of the first supporting section is desired to be λ/4 when a resonance frequency excited in the vibration section has a wave Length λ. On the other hand, in the case where the acoustic mirror section is provided on the first supporting section, a thickness of the first supporting section is desired not to be λ/4 when the resonance frequency excited in the vibration section has the wavelength λ.

Although the above-described acoustic resonator of the present invention alone acts as a filter, a filter having various frequency characteristics is realized by connecting, in a ladder type, two or more acoustic resonators of one of the above-described types, or two or more acoustic resonators which are a combination of the above-described types. The filter can be used in a communication device together with, e.g., a switch for switching input signals for output.

The present invention is also directed to an acoustic resonator manufacturing method. The acoustic resonator manufacturing method of the present invention achieves the aforementioned object by sequentially performing the following processes.

A piezoelectric thin film is formed on a sacrifice substrate; a first electrode layer is laminated on the piezoelectric thin film; patterning is performed on the first electrode layer, whereby a lower electrode of an acoustic resonator is formed; a first sacrifice layer is laminated on the piezoelectric thin film and lower electrode; patterning is performed on the first sacrifice layer, whereby a sacrifice section, which functions as a cavity of the acoustic resonator after being removed, is formed; a retention layer for retaining a piezoelectric thin film resonator is formed on the sacrifice section, lower electrode and piezoelectric thin film; a semiconductor substrate is affixed on a surface of the retention layer; after the affixing process, the sacrifice substrate is exfoliated from the semiconductor substrate; a second electrode layer is laminated on the piezoelectric thin film having appeared as a result of exfoliation; patterning is performed on the second electrode layer, whereby an upper electrode of the acoustic resonator is formed; and the cavity is formed by removing the sacrifice section.

The surface of the retention layer may be planarized before the affixing process of the semiconductor substrate. The planarization of the surface of the retention layer is preferred to be performed such that a roughness of the surface becomes 1000 ARMS or lower.

In the affixing process, the retention Layer and semiconductor substrate may be affixed to each other via a bond layer, or by performing eutectic crystallization. It is preferred to use molybdenum or tungsten silicide for forming the sacrifice layer. Further, in the process of forming the piezoelectric thin film, the piezoelectric thin film may be formed on a second sacrifice layer provided on the sacrifice substrate. It is preferred to use nitriding gallium or molybdenum for forming the second sacrifice layer.

Alternatively, the acoustic resonator manufacturing method of the present invention achieves the aforementioned object by sequentially performing the following processes.

A piezoelectric thin film is formed on a sacrifice substrate; a first electrode layer is laminated on the piezoelectric thin film; patterning is performed on the first electrode layer, whereby a lower electrode of an acoustic resonator is formed; a retention layer for retaining the acoustic resonator is formed on the lower electrode and piezoelectric thin film; a mirror layer is formed on the retention layer; a semi conductor substrate is affixed on the mirror layer; after the affixing process, the sacrifice substrate is exfoliated from the semiconductor substrate; a second electrode layer is laminated on the piezoelectric thin film having appeared as a result of exfoliation; and patterning is performed on the second electrode layer, whereby an upper electrode of the acoustic resonator is formed.

The surface of the retention layer may be planarized before the affixing process of the semiconductor substrate. The planarization of the surface of the retention layer is preferred to be performed such that a roughness of the surface becomes 1000 ARMS or lower.

In the affixing process, the mirror layer and semiconductor substrate may be affixed to each other via a bond layer, or by performing eutectic crystallization. Further, in the process of forming the piezoelectric thin film, the piezoelectric thin film may be formed on a sacrifice layer provided on the sacrifice substrate. It is preferred to use nitriding gallium or molybdenum for forming the sacrifice layer.

The acoustic resonator of the above-described present invention is capable of preventing an occurrence of unnecessary vibration which reflects on the bottom of a substrate section and then returns to the vibration section. This allows a favorable admittance frequency characteristic, which does no cause a spurious occurrence between a resonance frequency of the vibration section and an antiresonance frequency of the vibration section, to be obtained.

Further, since the above-described present invention uses a technique for affixing substrates, a monocrystal substrate can be used as a base substrate at the time of forming the piezoelectric thin film which greatly affects a characteristic of the acoustic resonator, or a high-temperature process such as MOCVD can be used. For this reason, the piezoelectric thin film having high crystallinity can be obtained. Further, since the cavity and supporting section are formed after the piezoelectric thin film is formed, crystallinity and flatness of the supporting section or the like do not affect the crystallinity of the piezoelectric thin film. Still further, since the sacrifice layer is used for forming the cavity and the sacrifice layer is removed by etching after the substrate exfoliation, a membrane of the vibration section does not receive damage during a laser lift-off process. As a result, yield is improved.

DESCRIPTION OF THE REFERENCE CHARACTERS

DETAILED DESCRIPTION OF BEST MODE FOR CARRYING OUT THE INVENTION

First Embodiment

FIG. 1shows across-section of a structure of an acoustic resonator according to a first embodiment of the present invention. InFIG. 1, the acoustic resonator according to the first embodiment comprises a substrate section40, a first supporting section30provided on the substrate section40, a second supporting section20provided on the first supporting section30, and a vibration section10provided on the second supporting section20. In order to obtain a longitudinal vibration of the vibration section10, the second supporting section20has a cavity21which is formed so as to penetrate the second supporting section20. The second supporting section20is a supporting layer for enabling the substrate section40to support the vibration section10. The vibration section10comprises: a piezoelectric body11formed from a piezoelectric material such as aluminum nitride (AlN); an upper electrode12provided on an upper surface of the piezoelectric body11; and a lower electrode13provided on a lower surface of the piezoelectric body11. The upper and lower electrodes12and13are formed from, for example, molybdenum (Mo). The vibration section10, having the lower electrode13on a lower side thereof, is mounted on the second supporting section20.

The first supporting section30is a supporting layer for enabling, in cooperation with the second supporting section20, the substrate section40to support the vibration section10. The first supporting section30is also a damping layer. The first supporting section30is structured by, e.g., a film formed from a material having a higher acoustic impedance than the piezoelectric body11and substrate40, or a film formed from a material having a smaller Q value than the piezoelectric body11and substrate40. The material of the first supporting section30may be an insulating material or a conductive material. When the conductive material is used, the first supporting section30may be used as a wiring layer. The first supporting section30having a high impedance may be formed by, for example, eutectic crystallization of gold and tin. For the first supporting section30having a low Q value, adhesive, e.g., polymer adhesive, may be used.

The acoustic resonator according to the first embodiment having the above structure has the following features based on a function of the first supporting section30provided between the substrate section40and second supporting section20.

Firstly, most vibration from the second supporting section20toward the substrate section40is reflected by the first supporting section30(as indicated by an arrow a inFIG. 1). Secondly, a slight vibration transmitted from the second supporting section20to the substrate section40is, even if the slight vibration is reflected at the bottom of the substrate section40and then returns in a direction of the vibration section10, reflected by the first supporting section30(as indicated by an arrow b inFIG. 1). This means that the first supporting section30has a higher acoustic impedance than the substrate section40and second supporting section20.

Other than the structure shown inFIG. 1, a thickness of the second supporting section20, a depth of a cavity21and a thickness of the first supporting section30may be as shown inFIGS. 2 to 4.

FIG. 2is an example of an acoustic resonator in which the cavity21, which has such a shape as not to penetrate the second supporting section20, is provided.FIG. 3is an example of an acoustic resonator in which the second supporting section20and first supporting section30each have a thickness of λ/4 when a resonance frequency excited in the vibration section10has a wavelength λ.FIG. 4is an example of an acoustic resonator in which the second supporting section20has a thickness of λ/2 and the first supporting section30has a thickness of λ/4 when the resonance frequency excited in the vibration section10has the wavelength λ. It is understood that in the above structures ofFIGS. 3 and 4, the cavity21may have such a shape as not to penetrate the second supporting section20.

Second Embodiment

FIG. 5shows a cross-section of a structure of an acoustic resonator according to a second embodiment of the present invention. InFIG. 5, the acoustic resonator according to the second embodiment comprises: the substrate section40; a supporting section30provided on the substrate section40; an acoustic mirror section50provided on the supporting section30; and the vibration section10provided on the acoustic mirror section50. The acoustic mirror section50is an acoustic reflecting layer as a result of alternately laminating a low impedance layer51and a high impedance layer52. In the acoustic mirror section50, a longitudinal vibration of the vibration section10is obtained. The vibration section10comprises: the piezoelectric body11formed from a piezoelectric material such as aluminum nitride (AlN); the upper electrode12provided on an upper surface of the piezoelectric body11; and the lower electrode13provided on a lower surface of the piezoelectric body11. The upper and lower electrodes12and13are formed by, for example, molybdenum (Mo). The vibration section10, having the lower electrode13on a lower side thereof, is mounted on the acoustic mirror section50.

The acoustic resonator according to the second embodiment having the above structure has the following features based on a function of the supporting section30provided between the substrate section40and the acoustic mirror section50.

Firstly, most vibration from the acoustic mirror section50toward the substrate section40is reflected by the supporting section30(as indicated by an arrow c inFIG. 5). Secondly, a slight vibration transmitted from the acoustic mirror section50to the substrate section40is, even if the slight vibration is reflected at the bottom of the substrate section40and then returns in a direction of the vibration section10, reflected by the supporting section30(as indicated by an arrow d inFIG. 5). This means that the supporting section30has a higher acoustic impedance than the substrate section40and acoustic mirror section50.

A structural feature of this acoustic resonator according to the second embodiment is that a thickness of each of the low impedance layer51and high impedance layer52of the acoustic mirror section50is ¼ of a vibration wavelength λ of the acoustic resonator, whereas a thickness of the supporting section30is not λ/4. Here, a thickness of a portion of the supporting section30, on which portion the vibration section10is mounted, may have a different thickness from that of a portion of the supporting section30, on which portion the vibration section10is not mounted. These features provide an improved damping effect. Further, setting the resonance frequency of the vibration section10to be different from resonance frequencies of others allows energy to be confined within the vibration section10, thereby providing a further enhanced damping effect.

The supporting section30is structured by, e.g., a film formed from a material having a higher acoustic impedance than the piezoelectric body11and substrate40, or a film formed from a material having a smaller Q value than the piezoelectric body11and substrate40. The material of the supporting section30may be an insulating material or a conductive material. When the conductive material is used, the supporting section30may be used as a wiring layer. The supporting section30having a high impedance may be formed by, for example, eutectic crystallization of gold and tin. For the supporting section30having a low Q value, adhesive, e.g., polymer adhesive, may be used.

As described above, the acoustic resonators according to the first and second embodiments of the present invention each prevent an occurrence of an unnecessary vibration which reflects at the bottom of the substrate section40and then returns to the vibration section10. This allows a favorable admittance frequency characteristic, which does not cause a spurious occurrence between the resonance frequency of the vibration section10and an antiresonance frequency of the vibration section10, to be obtained.

Note that, the acoustic resonators according to the above first and second embodiments each alone can act as a filter, or a combination of a plurality of such acoustic resonators can act as a filter. Hereinafter, a filter, which is a result of combining a plurality of such acoustic resonators, and a device using the filter will be described.

(First Example of a Filter Using Acoustic Resonators)

FIG. 6Ashows a first example of a filter using acoustic resonators of the present invention. The filter shown inFIG. 6Ais a ladder filter which is a result of connecting the acoustic resonators in L-shape. An acoustic resonator61is connected so as to operate as a serial resonator. To be specific, the acoustic resonator61is serially connected between an input terminal63and output terminal64. An acoustic resonator62is connected so as to operate as a parallel resonator. To be specific, the acoustic resonator62is connected between a ground plane and a path from the input terminal63to the output terminal4. Here, by setting a resonance frequency of the acoustic resonator61to be higher than a resonance frequency of the acoustic resonator62, a ladder filter having a band-pass characteristic is realized. It is preferred to set the resonant frequency of the acoustic resonator61to be substantially equal to or near an anti resonant frequency of the acoustic resonator62, so as to realize a ladder filter having an improved passband flatness.

Although the above first example gives a description of an exemplary L-type ladder filter, the same effect as described above may be obtained with a different type of ladder filter, such as a T-type, π-type or lattice-type ladder filter. The ladder filter may have a single-stage configuration as shown inFIG. 6A, or a multi-stage configuration as shown inFIG. 6B.

(Second Example of a Filter Using Acoustic Resonators)

FIG. 7shows a second example of a filter using acoustic resonators of the present invention. The filter shown inFIG. 7is a stack filter. An acoustic resonator71is serially connected between an input terminal73and output terminal74. An intermediate electrode of the acoustic resonator71is connected to a ground plane. By using, in the above manner, the acoustic resonator71which does not have a spurious occurrence, a stack filter having improved passband flatness is realized. It is understood that the stack filter may have a single-stage configuration as shown inFIG. 7, or a multi-stage configuration.

(An Example of a Device Using Acoustic Resonators)

FIG. 8shows an example of a device using acoustic resonators of the present invention. The device shown inFIG. 8is a communication device using such a filter as shown inFIG. 6A,FIG. 6BorFIG. 7. This device comprises two antennas81and82, a switch83for switching a frequency signal between two frequency signals, and a filter84. This configuration realizes a low-loss communication device.

(First Exemplary Manufacturing Method of an Acoustic Resonator)

FIG. 9Ais an exemplary top view of the acoustic resonator according to the first embodiment, which is manufactured using a first exemplary manufacturing method.FIG. 9Bis a cross-sectional view, taken along a line X-X, of the acoustic resonator shown inFIG. 9A. In the first exemplary manufacturing method, the acoustic resonator is manufactured using a technique to affix two substrates together. Hereinafter, steps of the first exemplary manufacturing method will be described with reference toFIGS. 10A to 10C.

First, a sacrifice layer91is laminated on a sacrifice substrate92(FIG. 10A, process a). Then, a piezoelectric thin film11ais formed on the sacrifice layer91(FIG. 10A, process b). Here, the sacrifice substrate92is a substrate which is temporarily used during a process of forming the acoustic resonator and which is not included in a structure of the acoustic resonator when manufacturing of the acoustic resonator is completed. The sacrifice substrate92is formed from, e.g., sapphire. The sacrifice layer91is a buffer layer which is provided for exfoliating the sacrifice substrate92from the piezoelectric thin film11aafter the later-described affixing process. The sacrifice layer91is formed from, e.g., nitriding gallium (GaN). The piezoelectric thin film11ais formed from aluminum nitride (AlN), and formed on the sacrifice layer91by MOCVD. By using MOCVD, a piezoelectric layer having a high film quality is formed, whereby an acoustic resonator for a wide band, which has a high Q value and high reliability, is manufactured.

Note that, MOCVD is performed under a high temperature of 1050° C. Since nitriding gallium, which is a material having a high melting point, is used as the sacrifice layer91in this example, the sacrifice layer91can endure the high temperature of 1050° C. Thus, using MOCVD for forming the piezoelectric thin film11awould not be a problem in the manufacturing process. Here, instead of nitriding gallium, molybdenum may be used as the sacrifice layer91.

Next, an electrode layer13a, which is a conductive material, is laminated on the piezoelectric thin film11a(FIG. 10A, process c). Thereafter, patterning is performed on the laminated electrode layer13aso as to form a lower electrode13(FIG. 10A, process d). Subsequently, a sacrifice layer21ais laminated on the formed lower electrode13and piezoelectric thin film11a(FIG. 10A, process e). The sacrifice layer21alaminated here is thicker than the lower electrode13. Then, patterning is performed on the laminated sacrifice layer21a, whereby a sacrifice section21is formed (FIG. 10A, process f). The sacrifice section21is a portion to be removed during the later-described cavity forming process. The cavity21of the acoustic resonator is formed as a result of removing this portion. Molybdenum, tungsten silicide or the like may be used as a material for forming the sacrifice layer21a. In such a case, aluminum or the like which is not molybdenum is used as a material for forming the lower electrode13.

Next, a second supporting layer20is laminated on the sacrifice section21, lower electrode13and piezoelectric thin film11a(FIG. 10B, process g). The second supporting layer20is preferred to be an insulator such as silicon oxide (SiO2), silicon nitride (Si3N4) or the like. Then, a planarizing process is performed in order to eliminate steps on a surface of the laminated second supporting layer20(FIG. 10B, process h). The planarizing process is performed so as to allow, in the below-described affixing process, the substrate40to be successfully and uniformly affixed on the entire surface. In the planarizing process, CMP or the like may be used. Here, by setting a roughness of the surface to be RMS20000A or lower, the substrate40can be uniformly affixed thereon.

Next, the substrate40, on which a first supporting layer30formed from gold-tin alloy is formed, is affixed on the second supporting layer20via a surface of the first supporting layer30(FIG. 10B, process i). This substrate40is formed from, for example, silicon. Here, an insulating layer such as silicon oxide, silicon nitride or the like may be formed between the substrate40and first supporting layer30. In this first example, a gold-tin alloy film is formed as the first supporting layer30, and affixing is performed using eutectic bonding of gold and tin. To be specific, the sacrifice substrate92and substrate40facing each other are subjected to a temperature of 375° C. for 10 minutes under the condition where a pressure of 15N/cm2 is applied, whereby these two substrates are affixed to each other. The same effect as described above can be obtained by using alloy which is not gold-tin alloy, as long as the alloy is made of materials which can be eutectically bonded.

Next, the sacrifice substrate92is exfoliated from the substrate40by irradiating an yttrium aluminum garnet (YAG) laser from the back of the sacrifice substrate92to eliminate a bond at the sacrifice layer91formed from nitriding gallium having a small bandgap (FIG. 10B, process j). At this point, the piezoelectric thin film11a, lower electrode13, sacrifice section21and the second supporting layer20, which are formed above the sacrifice layer91, are transferred onto the substrate40. Here, by selecting a laser wavelength of the YAG laser in accordance with a film thickness and a film type of each of the sacrifice substrate92and sacrifice layer91to be used, the YAG laser may be used for the exfoliation even in the case where the bandgap changes due to a difference in thickness of the sacrifice layer91, or in the case where different materials are selected.

Next, an electrode layer12a, which is a conductive body, is laminated on the piezoelectric thin film11ahaving appeared after the exfoliation (FIG. 10C, process k). Thereafter, patterning is performed on the laminated electrode layer12a, whereby the upper electrode12is formed (FIG. 10C, process l). Subsequently, patterning is performed on the piezoelectric thin film11aas necessary, whereby the piezoelectric body11is formed (FIG. 10C, process m). Lastly, the sacrifice section21is removed by, e.g., etching to form the cavity21(FIG. 10C, process n). By the above processes, the acoustic resonator shown inFIG. 9Bis completed.

As described above, the first exemplary manufacturing method uses a technique to affix substrates. This allows a monocrystal substrate formed from, e.g., silicon to be used as a base when a piezoelectric thin film is formed. As a result, even if a film configuration (configuration of the supporting section) is complex, influence from the base is eliminated, and the piezoelectric thin film having a high quality is obtained. Further, a high temperature process such as MOCVD can be used at the time of forming the piezoelectric thin film. This enables an epitaxially grown piezoelectric thin film to be obtained.

Since the sacrifice layer is used for forming the cavity and the sacrifice layer is removed by etching after the substrate exfoliation, a membrane of the vibration section does not receive damage during a laser lift-off process. As a result, yield is improved. Since the substrates can be affixed to each other at the entire surfaces thereof, the manufacturing process is simplified.

Note that, the planarizing process (FIG. 10B, process h) of the second supporting layer20can be omitted depending on a condition in which affixing is performed. Even in the case where the planarizing process is not performed, the characteristic of the acoustic resonator is not affected, because the vibration section10is remote from the affixed surfaces, and thus the acoustic resonator can be manufactured in a simple manner.

Since the surfaces of the second supporting layer20and substrate40, which are affixed to each other, are remote from the vibration section10, adhesive or the like may be used for the first supporting layer30. In this case, surface roughness is not required to be improved, and therefore, the planarizing process (FIG. 10B, process g) can be omitted. As a result, the acoustic resonator is allowed to be manufactured in a simpler manner, and also, a damping effect of the first supporting layer30, which is adhesive, efficiently damps a vibration transmitted to the substrate40.

Further, other than a sapphire substrate, a silicon substrate, silicon carbide (SiC) substrate or the like may be used as the sacrifice substrate92, as long as the piezoelectric thin film11acan be formed thereon. Other than nitriding gallium, any material, which can be easily exfoliated from the substrate and on which a piezoelectric layer can be formed, may be used as the sacrifice layer91. For example, if molybdenum is used as the sacrifice layer91, the sacrifice layer91can be easily exfoliated, by using oxygenated water, from the substrate on which the sacrifice layer91is formed. In this case, even if wet etching or the like is used in a substrate exfoliation process (i.e., the laser lift-off process of this example), the lower electrode13does not receive damage since the vibration section10is covered with the second supporting layer20.

Still further, the manner of forming the piezoelectric thin film11ais not limited to MOCVD. It is understood that the same effect as above is obtained when a spatter method is used. Still further, other than aluminum nitride formed by MOCVD, zinc oxide formed by high-temperature spatter, lead titanate (PbTiO3) on which a high temperature process has been performed, a PZT material such as lead zirconate titanate (PbTiZrO), or the like may be used for the piezoelectric thin film11a. However, in order to form such a film, a high temperature process is required to be performed at approximately 800° C. under the oxygen atmosphere. For this reason, a material used for the sacrifice layer is required to have a heat-resisting property.

Although an exemplary laser lift-off process has been given as the substrate exfoliation process, a different method may be used if, by using the method, the sacrifice substrate92can be removed after the affixing process. It is conceivable to use, for a sacrifice substrate removal process, a method for removing the sacrifice substrate92by etching or the like. For example, when the sacrifice substrate92is a silicon substrate, the sacrifice substrate92can be removed by wet etching using hydrofluoric nitric acid. Even if dry etching is used here, the sacrifice substrate92can be removed in the same manner.

(Second Exemplary Manufacturing Method of an Acoustic Resonator)

FIG. 11is an exemplary cross-sectional view of the acoustic resonator according to the second embodiment which is manufactured using a second exemplary manufacturing method. Also in this second exemplary manufacturing method, the acoustic resonator is manufactured using a technique to affix two substrates together. Hereinafter, steps of the second exemplary manufacturing method will be described with reference toFIGS. 12A to 12C.

First, the sacrifice layer91is laminated on the sacrifice substrate92(FIG. 12A, process A). Then, the piezoelectric thin film11ais formed on the sacrifice layer91(FIG. 12A, process B). Next, the electrode layer13a, which is a conductive body, is laminated on the piezoelectric thin film11a(FIG. 12A, process C). Thereafter, patterning is performed on the laminated electrode layer13a, whereby the lower electrode13is formed (FIG. 12A, process D). Subsequently, a high acoustic impedance layer51is laminated on the formed lower electrode13and piezoelectric thin film11a(FIG. 12A, process E). The high acoustic impedance layer51laminated here is thicker than the lower electrode13. Then, the planarizing process is performed in order to eliminate steps on a surface of the laminated high acoustic impedance layer51(FIG. 12A, process F). Next, a low acoustic impedance layer52is laminated on the planarized high acoustic impedance layer51(FIG. 12B, process G). By repeatedly performing the processes F and G, an acoustic mirror layer50is formed (FIG. 12B, process H).FIG. 12Bshows an example of the acoustic mirror layer50which is a result of alternately laminating, for three times, the high acoustic impedance layer51and low acoustic impedance layer52.

Next, the substrate40, on which the first supporting layer30formed from gold-tin alloy is formed, is affixed on the acoustic mirror layer50via a surface of the first supporting layer30(FIG. 12B, process I). Then, the sacrifice substrate92is exfoliated from the substrate40by irradiating an yttrium aluminum garnet laser from the back of the sacrifice substrate92to eliminate a bond at the sacrifice layer91formed from nitriding gallium having a small bandgap (FIG. 12C, process J). At this point, the piezoelectric thin film11a, lower electrode13and the acoustic mirror layer50, which are formed above the sacrifice layer91, are transferred onto the substrate40. Next, the electrode layer12awhich is a conductive body is laminated on the piezoelectric thin film11ahaving appeared after the exfoliation (FIG. 12C, process K). Lastly, patterning is performed on the laminated electrode layer12a, whereby the upper electrode12is formed (FIG. 12C, process L). By the above processes, the acoustic resonator shown inFIG. 11is completed.

As described above, the second example uses a technique to affix substrates. For this reason, a high temperature process such as MOCVD can be used at the time of forming the piezoelectric thin film. As a result, the piezoelectric thin film having high crystallinity is obtained.

Note that, the process E ofFIG. 12Aillustrates an example where the high acoustic impedance layer51is laminated immediately above the lower electrode13and piezoelectric thin film11a. However, a retention layer formed from an insulating material such as silicon oxide or silicon nitride may be formed before the high acoustic impedance layer51is laminated.

The acoustic resonator and filter of the present invention can be used for, e.g., a mobile phone, radio communication, and wireless Internet connection. The acoustic resonator and filter are particularly useful for, e.g., obtaining an admittance frequency characteristic which suppresses spurious occurrences.

Further, the manufacturing method of the present invention can be used as, e.g., a manufacturing method for manufacturing an acoustic resonator to be used in a radio frequency circuit of a mobile communication terminal such as a mobile phone and a wireless LAN device. The manufacturing method of the present invention is particularly useful for, e.g., realizing a low-loss acoustic resonator for a wide band by using a piezoelectric thin film having high crystallinity.