TEMPERATURE COMPENSATED SURFACE ACOUSTIC WAVE DEVICE HAVING MASS LOADING STRIP WITH BUFFER LAYER
An acoustic wave device and a method of forming the same is disclosed. The acoustic wave device can include a piezoelectric layer, an interdigital transducer electrode formed with the piezoelectric layer, and a temperature compensation layer over the interdigital transducer electrode. The interdigital transducer electrode includes a bus bar and fingers that extend from the bus bar. The fingers each includes an edge portion and a body portion. The acoustic wave device can include a mass loading strip that overlaps the edge portions of the fingers. A portion of the temperature compensation layer is positioned between the mass loading strip and the piezoelectric layer. The acoustic wave device can include a buffer layer that is disposed at least partially between the mass loading strip and the temperature compensation layer. The buffer layer includes a material different from materials of the temperature compensation layer and the mass loading strip.
Any and all applications for which a foreign or domestic priority claim is identified in the Application Data Sheet as filed with the present application, including U.S. Provisional Patent Application No. 63/325,353, filed Mar. 30, 2022, titled “ACOUSTIC WAVE DEVICE HAVING MASS LOADING STRIP WITH BUFFER LAYER,” U.S. Provisional Patent Application No. 63/325,386, filed Mar. 30, 2022, titled “TEMPERATURE COMPENSATED SURFACE ACOUSTIC WAVE DEVICE HAVING MASS LOADING STRIP WITH BUFFER LAYER,” and U.S. Provisional Patent Application No. 63/325,369, filed Mar. 30, 2022, titled “ACOUSTIC WAVE DEVICE HAVING MASS LOADING STRIP WITH THERMAL EXPANSION COMPENSATION BUFFER LAYER,” are hereby incorporated by reference under 37 CFR 1.57 in their entirety.
BACKGROUND Technical FieldEmbodiments of this disclosure relate to acoustic wave devices with a mass loading strip for transverse mode suppression.
Description of Related TechnologyPiezoelectric microelectromechanical systems (MEMS) resonators can be used in radio frequency systems. Piezoelectric MEMS resonators can process electrical signals using mechanically vibrating structures. Example piezoelectric MEMS resonators include surface acoustic (SAW) resonators and temperature compensated surface acoustic wave (TC-SAW) resonators.
Acoustic wave filters can include TCSAW resonators. Acoustic wave filters can filter radio frequency signals in radio frequency electronic systems. For instance, filters in a radio frequency front end of a mobile phone can include acoustic wave filters. Multiple acoustic wave filters can be arranged as a multiplexer, such as a duplexer.
SUMMARYThe innovations described in the claims each have several aspects, no single one of which is solely responsible for its desirable attributes. Without limiting the scope of the claims, some prominent features of this disclosure will now be briefly described.
In one aspect, an acoustic wave device is disclosed. The acoustic wave device can include a piezoelectric layer and an interdigital transducer electrode formed with the piezoelectric layer. The interdigital transducer electrode includes a bus bar and fingers extending from the bus bar. The fingers each including an edge portion and a body portion. The acoustic wave device can include a temperature compensation layer over the interdigital transducer electrode, and a mass loading strip overlapping the edge portions of the fingers. A portion of the temperature compensation layer is positioned between the mass loading strip and the piezoelectric layer. The acoustic wave device can include a buffer layer disposed at least partially between the mass loading strip and the temperature compensation layer. A thickness of the buffer layer is at least one forth a thickness of the mass loading strip.
In one embodiment, the mass loading strip includes a layer having a density that is at least as high as a most dense layer of a material of the interdigital transducer electrode. The mass loading strip can consist of the layer. The mass loading strip can include a second layer.
In one embodiment, the mass loading strip is embedded in the temperature compensation layer.
In one embodiment, the temperature compensation layer is a silicon dioxide layer. The mass loading strip can be a molybdenum layer. The buffer layer can be a molybdenum silicide layer.
In one embodiment, the buffer layer includes a material different from materials of the temperature compensation layer and the mass loading strip.
In one embodiment, the buffer layer has a coefficient of thermal expansion greater than a coefficient of thermal expansion of the temperature compensation layer and less than a coefficient of thermal expansion of the mass loading strip.
In one embodiment, the mass loading strip has a bottom side, an top side, and a sidewall extending between the bottom side and the top side. The buffer layer can be disposed between the top side and the sidewall of the mass loading strip and the temperature compensation layer. The buffer layer can be further disposed between the bottom side of the mass loading strip and the temperature compensation layer.
In one embodiment, the thickness of the buffer layer is at least one third the thickness of the mass loading strip.
In one embodiment, the acoustic wave device further includes a silicon nitride layer over the temperature compensation layer.
In one aspect, an acoustic wave device is disclosed. The acoustic wave device can include a piezoelectric layer, and an interdigital transducer electrode formed with the piezoelectric layer. The interdigital transducer electrode includes a bus bar and fingers extending from the bus bar. The fingers each includes an edge portion and a body portion. The acoustic wave device can include a temperature compensation layer over the interdigital transducer electrode, and a mass loading strip overlapping the edge portions of the fingers. A portion of the temperature compensation layer is positioned between the mass loading strip and the piezoelectric layer. The mass loading strip has a bottom side, an top side, and a sidewall extending between the bottom side and the top side. The acoustic wave device can include a buffer layer disposed at least partially between the bottom side, the top side, and the side wall of the mass loading strip and the temperature compensation layer.
In one embodiment, the mass loading strip includes a layer having a density that is at least as high as a most dense layer of a material of the interdigital transducer electrode. The mass loading strip can consist of the layer. The mass loading strip can include a second layer.
In one embodiment, the mass loading strip is embedded in the temperature compensation layer.
In one embodiment, the temperature compensation layer is a silicon dioxide layer. The mass loading strip can be a molybdenum layer. The buffer layer can be a molybdenum silicide layer.
In one embodiment, the buffer layer includes a material different from materials of the temperature compensation layer and the mass loading strip.
In one embodiment, the buffer layer has a coefficient of thermal expansion greater than a coefficient of thermal expansion of the temperature compensation layer and less than a coefficient of thermal expansion of the mass loading strip.
In one embodiment, the thickness of the buffer layer is at least one third the thickness of the mass loading strip.
In one embodiment, the acoustic wave device further includes a silicon nitride layer over the temperature compensation layer.
In one aspect, an acoustic wave device is disclosed. The acoustic wave device can include a piezoelectric layer, and an interdigital transducer electrode formed with the piezoelectric layer. The interdigital transducer electrode includes a bus bar and fingers extending from the bus bar. The fingers each including an edge portion and a body portion. The acoustic wave device can include a temperature compensation layer over the interdigital transducer electrode, and a mass loading strip overlapping the edge portions of the fingers. A portion of the temperature compensation layer is positioned between the mass loading strip and the piezoelectric layer. The acoustic wave device can include a buffer layer disposed at least partially between the mass loading strip and the temperature compensation layer. The buffer layer includes a material different from materials of the temperature compensation layer and the mass loading strip.
In one embodiment, the mass loading strip includes a layer having a density that is at least as high as a most dense layer of a material of the interdigital transducer electrode. The mass loading strip can consist of the layer. The mass loading strip can include a second layer.
In one embodiment, the mass loading strip is embedded in the temperature compensation layer.
In one embodiment, the temperature compensation layer is a silicon dioxide layer. The mass loading strip can be a molybdenum layer.
In one embodiment, a thickness of the buffer layer is at least one forth a thickness of the mass loading strip.
In one embodiment, the buffer layer has a coefficient of thermal expansion greater than a coefficient of thermal expansion of the temperature compensation layer and less than a coefficient of thermal expansion of the mass loading strip.
In one embodiment, the mass loading strip has a bottom side, an top side, and a sidewall extending between the bottom side and the top side. The buffer layer can be disposed between the top side and the sidewall of the mass loading strip and the temperature compensation layer. The buffer layer can be further disposed between the bottom side of the mass loading strip and the temperature compensation layer.
In one embodiment, a difference between the coefficient of thermal expansion of the temperature compensation layer and the coefficient of thermal expansion of the metal strip is ΔCTE. The coefficient of thermal expansion of the buffer layer can be 0.2ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer. The coefficient of thermal expansion of the buffer layer can be 0.3ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer.
In one embodiment, the acoustic wave device further includes a silicon nitride layer over the temperature compensation layer.
In one aspect, a method of forming an acoustic wave device is disclosed. The method can include forming an interdigital transducer electrode formed with a piezoelectric layer. The interdigital transducer electrode including a bus bar and fingers extending from the bus bar. The fingers each includes an edge portion and a body portion. The method can include forming a temperature compensation layer over the interdigital transducer electrode. The method can include forming a mass loading strip overlapping the edge portions of the fingers. A portion of the temperature compensation layer is positioned between the mass loading strip and the piezoelectric layer. The method can include forming a buffer layer disposed at least partially between the mass loading strip and the temperature compensation layer. The forming the buffer layer includes depositing the mass loading strip.
In one embodiment, the mass loading strip includes a layer having a density that is at least as high as a most dense layer of a material of the interdigital transducer electrode. The mass loading strip can consist of the layer. The mass loading strip can include a second layer.
In one embodiment, the mass loading strip is embedded in the temperature compensation layer.
In one embodiment, the temperature compensation layer is a silicon dioxide layer. The mass loading strip can be a molybdenum layer.
In one embodiment, the buffer layer includes a material different from materials of the temperature compensation layer and the mass loading strip.
In one embodiment, a thickness of the buffer layer is at least one forth a thickness of the mass loading strip.
In one embodiment, the buffer layer includes a material different from materials of the temperature compensation layer and the mass loading strip.
In one embodiment, the buffer layer has a coefficient of thermal expansion greater than a coefficient of thermal expansion of the temperature compensation layer and less than a coefficient of thermal expansion of the mass loading strip.
In one embodiment, the mass loading strip has a bottom side, an top side, and a sidewall extending between the bottom side and the top side. The buffer layer can be disposed between the top side and the sidewall of the mass loading strip and the temperature compensation layer. The buffer layer can be further disposed between the bottom side of the mass loading strip and the temperature compensation layer.
In one embodiment, a difference between the coefficient of thermal expansion of the temperature compensation layer and the coefficient of thermal expansion of the metal strip is ΔCTE. The coefficient of thermal expansion of the buffer layer can be 0.2ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer. The coefficient of thermal expansion of the buffer layer can be 0.3ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer.
In one embodiment, the method further includes forming a silicon nitride layer over the temperature compensation layer.
In one embodiment, the forming the buffer layer includes reacting the mass loading strip and the temperature compensation layer. The forming the temperature compensation layer can include sputtering the temperature compensation layer at a sputtering temperature in a range between 200° C. and 300° C.
In one aspect, an acoustic wave device is disclosed. The acoustic wave device can include a piezoelectric layer, and an interdigital transducer electrode formed with the piezoelectric layer. The interdigital transducer electrode includes a bus bar and fingers extending from the bus bar. The fingers each includes an edge portion and a body portion. The acoustic wave device can include a temperature compensation layer over the interdigital transducer electrode, and a mass loading strip overlapping the edge portions of the fingers. A portion of the temperature compensation layer is positioned between the mass loading strip and the piezoelectric layer. The acoustic wave device can include a buffer layer disposed at least partially between the mass loading strip and the temperature compensation layer. The buffer layer having a coefficient of thermal expansion greater than a coefficient of thermal expansion of the temperature compensation layer and less than a coefficient of thermal expansion of the mass loading strip.
In one embodiment, the mass loading strip includes a layer having a density that is at least as high as a most dense layer of a material of the interdigital transducer electrode. The mass loading strip can consist of the layer. The mass loading strip can include a second layer.
In one embodiment, the mass loading strip is embedded in the temperature compensation layer.
In one embodiment, the temperature compensation layer is a silicon dioxide layer. The mass loading strip can be a molybdenum layer. The buffer layer can be a molybdenum silicide layer.
In one embodiment, the buffer layer includes a material different from materials of the temperature compensation layer and the mass loading strip.
In one embodiment, a thickness of the buffer layer is at least one forth a thickness of the mass loading strip. The thickness of the buffer layer can be at least one third the thickness of the mass loading strip.
In one embodiment, the mass loading strip has a bottom side, an top side, and a sidewall extending between the bottom side and the top side. The buffer layer is disposed between the top side and the sidewall of the mass loading strip and the temperature compensation layer. The buffer layer can be further disposed between the bottom side of the mass loading strip and the temperature compensation layer.
In one embodiment, a difference between the coefficient of thermal expansion of the temperature compensation layer and the coefficient of thermal expansion of the metal strip is ΔCTE. The coefficient of thermal expansion of the buffer layer can be 0.2ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer. The coefficient of thermal expansion of the buffer layer can be 0.3ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer. The coefficient of thermal expansion of the buffer layer can be 0.4ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer.
In one embodiment, the acoustic wave device further includes a silicon nitride layer over the temperature compensation layer.
In one aspect, an acoustic wave device is disclosed. The acoustic wave device can include a piezoelectric layer, and an interdigital transducer electrode formed with the piezoelectric layer. The interdigital transducer electrode including a bus bar and fingers extending from the bus bar. The fingers each includes an edge portion and a body portion. The acoustic wave device can include a temperature compensation layer over the interdigital transducer electrode, and a mass loading strip overlapping the edge portions of the fingers. A portion of the temperature compensation layer is positioned between the mass loading strip and the piezoelectric layer. The mass loading strip includes a layer having a density that is at least as high as a most dense layer of a material of the interdigital transducer electrode. The acoustic wave device can include a buffer layer disposed at least partially between the mass loading strip and the temperature compensation layer. A difference between a coefficient of thermal expansion of the temperature compensation layer and a coefficient of thermal expansion of the metal strip is ΔCTE. A coefficient of thermal expansion of the buffer layer is 0.2ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer.
In one embodiment, the coefficient of thermal expansion of the buffer layer is 0.3ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer.
In one embodiment, a thickness of the buffer layer is at least one forth a thickness of the mass loading strip.
The present disclosure relates to U.S. Patent Application No. ______ [Attorney Docket SKYWRKS.1190A1], titled “ACOUSTIC WAVE DEVICE HAVING MASS LOADING STRIP WITH BUFFER LAYER,” filed on even date herewith, and U.S. Patent Application No. ______ [Attorney Docket SKYWRKS.1190A3], titled “ACOUSTIC WAVE DEVICE HAVING MASS LOADING STRIP WITH THERMAL EXPANSION COMPENSATION BUFFER LAYER,” filed on even date herewith, the entire disclosures of which are hereby incorporated by reference herein.
Embodiments of this disclosure will now be described, by way of non-limiting example, with reference to the accompanying drawings.
The following description of certain embodiments presents various descriptions of specific embodiments. However, the innovations described herein can be embodied in a multitude of different ways, for example, as defined and covered by the claims. In this description, reference is made to the drawings where like reference numerals can indicate identical or functionally similar elements. It will be understood that elements illustrated in the figures are not necessarily drawn to scale. Moreover, it will be understood that certain embodiments can include more elements than illustrated in a drawing and/or a subset of the elements illustrated in a drawing. Further, some embodiments can incorporate any suitable combination of features from two or more drawings.
Acoustic wave filters can filter radio frequency (RF) signals in a variety of applications, such as in an RF front end of a mobile phone. An acoustic wave filter can be implemented with surface acoustic wave (SAW) devices. The SAW devices include SAW resonators, SAW delay lines, and multi-mode SAW (MMS) filters (e.g., double mode SAW (DMS) filters).
In general, high quality factor (Q), large effective electromechanical coupling coefficient (k2eff), high frequency ability, and spurious free can be significant aspects for micro resonators to enable low-loss filters, stable oscillators, and sensitive sensors. SAW resonators can have a relatively strong transverse mode in and/or near a pass band. The presence of the relatively strong transverse modes can hinder the accuracy and/or stability of oscillators and sensors, as well as hurt the performance of acoustic wave filters by creating relatively severe passband ripples and possibly limiting the rejection.
Therefore, transverse mode suppression is significant for SAW resonators. A technical solution for suppressing transverse modes is to create a border region with a different frequency from active region according to the mode dispersion characteristic. This can be referred to as a “piston mode.” A piston mode can be obtained to cancel out the transverse wave vector in a lateral direction without significantly degrading the k2 or Q. By including a relatively small border region with a slower velocity on the edge of the acoustic aperture of a SAW resonator, a propagating mode can have a zero (or approximately zero) transverse wave vector in the active aperture.
One way of achieving a piston mode is to include a material that can cause a magnitude of the velocity in the underlying region of the SAW resonator to be increased. The material can be, for example, silicon nitride (SiN). As an example, SiN can be positioned over a center region of an interdigital transducer electrode (IDT) and the border region of the IDT electrode can be free from the SiN.
A relatively high density IDT electrode, such as tungsten (W) IDT electrode, can be used for downsizing by slowing down the SAW propagation velocity of a temperature-compensated SAW (TCSAW) resonator. Transverse mode suppression can be significant for TCSAW device performance. However, a TCSAW resonator with an IDT electrode that includes tungsten can encounter difficulty in suppressing transverse modes. For instance, a silicon nitride layer with a trench over a temperature compensation layer for a piston mode may not sufficiently suppress transverse modes in such resonators. This can be due to resonator displacement being distributed deep inside a silicon dioxide (SiO2) temperature compensation layer of the TCSAW resonator.
Another way to achieve piston mode is to provide a mass loading strip (e.g., a conductive strip) on edges of an IDT electrode active regions of the SAW resonator. The transverse wave vector can be real in the border region and imaginary on a gap region. A piston mode SAW resonator can have even order modes that have a multiple of full wave lengths in the active region, which should not significantly couple to electrical domain.
An IDT electrode with a tungsten layer has a relatively high density. Acoustic energy can be gathered into the IDT side. In such a case, the perturbation on a surface of a silicon dioxide temperature compensation layer over the IDT electrode can be ineffective. A conductive strip that includes a tungsten layer buried in the silicon dioxide temperature compensation layer can effectively control the velocity of a TCSAW resonator with an IDT electrode that includes tungsten. The combination of the conductive strip material and the IDT electrode material can be significant. For example, a conductive strip with a molybdenum layer may not sufficiently suppress transverse modes in a TCSAW resonator with an IDT electrode that includes tungsten. The conductive strip can include a layer having a density that is at least as high as a density of a most dense layer of the IDT electrode. The conductive strip can include a layer having a density that is at least as high as a density of a material of the IDT electrode that is in contact with a piezoelectric layer of the TCSAW resonator.
Formation of the mass loading trip may cause a void in the temperature compensation layer. A relatively large void in the temperature compensation layer can negatively affect the suppression of transverse modes in the TCSAW resonator. Various embodiments disclosed herein can prevent or mitigate formation of a void, or minimize the size of the void in the TCSAW resonator that include a mass loading strip.
Aspects of this disclosure relate to SAW resonators (e.g., TCSAW resonators) that include mass loading structure (e.g., a metal strip) that includes a relatively high density metal layer. The metal strip can be buried in a temperature compensation layer, such as a silicon dioxide layer. The high density layer has a density at least as high as a density of a material of an IDT electrode that is in contact with piezoelectric layer. The SAW resonators can have a buffer layer that prevents or mitigate formation of a void, or reduce or minimize a size of the void. The buffer layer can be disposed at least partially between the mass loading structure and a temperature compensation layer. The buffer layer has a coefficient of thermal expansion (CTE) greater than a CTE of the temperature compensation layer and less than a CTE of the mass loading structure.
Although embodiments may be discussed with reference to metal strips or conductive strips, any suitable principles and advantages disclosed herein can be applied to a mass loading strip that includes one or more non-conductive layers. Moreover, although embodiments may be discussed with reference to SAW resonators, the principles and advantages discussed herein can be applied to any suitable SAW device and/or any other suitable acoustic wave device. Embodiments will now be discussed with reference to drawings. Any suitable combination of features of the embodiments disclosed herein can be implemented together with each other.
The illustrated metal strip 16 includes a high density metal strip layer 18. The metal strip 16 can be a multi-layer conductive strip in certain embodiments (see, for example,
The metal strip 16 performs a mass loading function. Accordingly, the metal strip 16 is an example of a mass loading strip. In certain applications, a mass loading strip of any suitable non-metal and/or non-conductive material that has a density that is equal to or greater than a density of a most dense layer of the IDT electrode 12 can be implemented in place of the metal strip 16 and/or any metal strip disclosed herein. Such a non-conductive layer can include a heavy dielectric layer such as tantalum pentoxide (Ta2O5), tellurium dioxide (TeO2), or a like dielectric material.
The piezoelectric layer 10 can include any suitable piezoelectric material, such as a lithium niobate (LN) layer or a lithium tantalate (LT) layer. A thickness of the piezoelectric layer 10 can be selected based at least in part on a wavelength λ or L of a surface acoustic wave generated by the surface acoustic wave resonator 1 in certain applications. The IDT electrode 12 has a pitch that sets the wavelength λ or L of the surface acoustic wave resonator 1. The piezoelectric layer 10 can be sufficiently thick to avoid significant frequency variation.
The illustrated IDT electrode 12 includes a first layer 26 and a second layer 28. The IDT electrode 12 includes fingers 22 and bus bars 24, which are illustrated in
The first layer 26 of the IDT electrode 12 can be referred to as a lower electrode layer. The first layer 26 of the IDT electrode 12 is disposed between the second layer 28 of the IDT electrode 12 and the piezoelectric layer 10. As illustrated, the first layer 26 of the IDT electrode 12 has a first side in physical contact with the piezoelectric layer 10 and a second side in physical contact with the second layer 28 of the IDT electrode 12. The first layer 26 can impact acoustic properties of the SAW resonator 1. For instance, a thickness t2 of the first layer 26 of the IDT electrode 12 can impact resonant frequency of the SAW resonator 1.
The second layer 28 of the IDT electrode 12 can be referred to as an upper electrode layer. The second layer 28 of the IDT electrode 12 is disposed between the first layer 26 of the IDT electrode 12 and the temperature compensation layer 14. As illustrated, the second layer 28 of the IDT electrode 12 has a first side in physical contact with the first layer 26 of the IDT electrode 12 and a second side in physical contact with the temperature compensation layer 14. The second layer 28 of the IDT electrode 12 can impact electrical properties of the SAW resonator 1. A thickness t3 of the second layer 28 of the IDT electrode 12 can impact insertion loss of the SAW resonator 1. The thickness t3 of the second layer 28 of the IDT electrode 12 may not significantly impact acoustic properties of the SAW resonator 1.
The IDT electrode 12 can include any suitable material. For example, the first layer 26 can be tungsten (W) and the second layer 28 can be aluminum (Al) in certain embodiments. The IDT electrode 12 may include one or more other metals, such as copper (Cu), Magnesium (Mg), titanium (Ti), molybdenum (Mo), etc. The IDT electrode 12 may include alloys, such as AlMgCu, AlCu, etc.
Although some embodiments disclosed herein include IDT electrodes with two IDT layers, any suitable principles and advantages disclosed herein can be applied to single layer IDT electrodes or multi-layer IDT electrodes that include three or more IDT layers.
The temperature compensation layer 14 can include any suitable temperature compensation material. For example, the temperature compensation layer 14 can be a silicon dioxide (SiO2) layer. The temperature compensation layer 14 can be a layer of any other suitable material having a positive temperature coefficient of frequency for SAW resonators with a piezoelectric layer having a negative coefficient of frequency. For instance, the temperature compensation layer 14 can be a tellurium dioxide (TeO2) layer or a silicon oxyfluoride (SiOF) layer in certain applications. In some other embodiments, the temperature compensation layer 14 can include any suitable combination of SiO2, TeO2, and/or SiOF.
The temperature compensation layer 14 can bring the temperature coefficient of frequency (TCF) of the SAW resonator 1 closer to zero relative to a similar SAW resonator without the temperature compensation layer 14. The temperature compensation layer 14 together with a lithium niobate piezoelectric layer can improve the electromechanical coupling coefficient (k2) of the SAW resonator 1 relative to a similar SAW resonator with a lithium tantalate piezoelectric layer and without the temperature compensation layer 14. This advantage of the temperature compensation layer 14 can be more pronounced when the SAW resonator 1 includes an LN layer as the piezoelectric layer 10.
The buffer layer 17 can be disposed at least partially between the mass loading strip and the temperature compensation layer 14. In some embodiments, as shown in
The buffer layer 17 can include any suitable material. The buffer layer 17 has a coefficient of thermal expansion (CTE) greater than a CTE of the temperature compensation layer 14 and less than a CTE of the mass loading strip (e.g., the metal strip 16). In some embodiments, where a difference between the CTE of the temperature compensation layer 14 and the CTE of the metal strip 16 is ΔCTE, the buffer layer 17 can have a CTE that is 0.2ΔCTE to 0.75ΔCTE greater than the CTE of the temperature compensation layer 14. For example, the buffer layer 17 can have a CTE that is 0.25ΔCTE to 0.75ΔCTE, 0.3ΔCTE to 0.75ΔCTE, 0.4ΔCTE to 0.75ΔCTE, 0.5ΔCTE to 0.75ΔCTE, 0.2ΔCTE to 0.7ΔCTE, 0.2ΔCTE to 0.6ΔCTE, 0.25ΔCTE to 0.7ΔCTE, 0.3ΔCTE to 0.7ΔCTE greater than the CTE of the temperature compensation layer 14. Selecting a material of the buffer layer 17 having a CTE from these ranges can be critical in preventing or mitigating formation of a void, and/or minimizing a size of the void formed due to, for example, delamination of the metal strip 16 from the temperature compensation layer 14 in the TCSAW resonator 1.
In some embodiments in which the temperature compensation layer 14 is a silicon dioxide (SiO2) layer, and the metal strip 16 is a molybdenum (Mo) layer, the buffer layer 17 can include a material having a mixture of Mo, Si, and O (e.g., a molybdenum silicide). For example, the buffer layer 17 can have an average molybdenum content of about 10% to 20%, an average silicon content of about 25% to 35%, and average oxide content of about 50% to 60%.
In some embodiments, the buffer layer 17 can be formed by applying heat. For example, during formation of the temperature compensation layer 14 by way of, for example, sputtering, heat can be applied. A sputtering temperature for the sputtering process can be, for example, in a range between 200° C. and 300° C. In such embodiments, material of the temperature compensation layer 14 and a material of the meatal strip 16 can react to form the buffer layer 17. The material and a thickness of the buffer layer 17 can depend at least in part on the temperature and duration of the sputtering process. In some embodiments, the heat can be applied after forming the temperature compensation layer 14. For example, the temperature compensation layer 14 and the metal strip 16 can be annealed at a temperature in a range between 300° C. to 350° C. The material and a thickness of the buffer layer 17 can depend at least in part on the temperature and duration of the annealing process. The following table (Table 1) shows an example composition of the temperature compensation layer 14, the metal strip 16, and the buffer layer 18 formed during a temperature compensation layer forming process, according to an embodiment.
In some embodiments, the buffer layer 17 can include material that is not included in the temperature compensation layer 14 and the metal strip 16. For example, a material that has a CTE greater than a CTE of the temperature compensation layer 14 and less than a CTE of the mass loading strip (e.g., the metal strip 16) can be disposed between the temperature compensation layer 14 and the metal strip 16 by way of deposition. In some embodiments, where a difference between the CTE of the temperature compensation layer 14 and the CTE of the metal strip 16 is ΔCTE, the material of the buffer layer 17 can have a CTE that is 0.2ΔCTE to 0.75ΔCTE greater than the CTE of the temperature compensation layer 14.
The buffer layer 17 can improve adhesion between the metal strip 16 and the temperature compensation layer 14. The buffer layer 17 can prevent, mitigate, or suppress formation of a void between the metal strip 16 and the temperature compensation layer 14. Accordingly, the buffer layer 17 can enable effective transverse mode suppression by the metal strip 16.
In the illustrated SAW resonator 1 of
In certain applications, the high density metal strip layer 18 of the metal strip 16 can include any suitable metal that has a density that is equal to or greater than the density of the first layer 26 (or the lower electrode layer) of the IDT electrode 12. The conductive strip 16 includes a layer having a density at least as high as a density of a material of the first layer 26. For example, the high density metal strip layer 18 can include molybdenum (Mo), tungsten (W), gold (Au), silver (Ag), ruthenium (Ru), iridium (Ir), or the like, depending on the density of the first layer 26 of the IDT electrode 12.
The metal strip 16 has an inner sidewall 16a and an outer sidewall 16b that extend between a bottom side 16c and a top side 16d of the metal strip 16. The outer sidewall 16b of the metal strip 16 is illustrated as being aligned with the distal ends 22b of the fingers 22 having a gap 25 between the outer sidewall 16b and the bus bar 24. However, in some embodiments, the outer sidewall 16b can be anywhere between the distal end 22b of the finger 22 that extends from one bus bar 24 and the other bus bar 24. In some other embodiments, the outer sidewall 16b may overlap with the bus bar 24 or be outside of the IDT electrodes 12.
The temperature compensation layer 14 has a thickness t1 measured from a lower surface 14a to an upper surface 14b opposite the lower surface 14a. In some embodiments, the thickness t1 of the temperature compensation layer 14 can be in a range from 0.1L to 0.5L. For instance, the thickness t1 can be about 0.3L in certain applications. For example, when the wavelength L is about 4 μm, the thickness t1 of the temperature compensation layer 14 can be about 1200 nm.
The first layer 26 of the IDT electrode 12 has a thickness t2 and the second layer 28 of the IDT electrode 12 has a thickness t3. In some embodiments, the thickness t2 of the first layer 26 can be in a range from 0.03L to 0.10L (e.g., about 0.08L) and the thickness t3 of the second layer 28 can be in a range from 0.02L to 0.08L (e.g., about 0.04L). For example, when the wavelength L is about 4 μm, the thickness t2 of the first layer 26 can be about 320 nm and the thickness t3 of the second layer 28 can be about 160 nm.
The metal strip 16 has a thickness t4 between the bottom side 16c and the top side 16d. The thickness t4 of the metal strip 16 can be a thickness of the high density metal strip layer 18 in the illustrated embodiment of
The buffer layer 17 has a thickness t5. In some embodiments, the thickness t5 of the buffer layer 17 can be at least one fourth the thickness t4 of the metal strip 16. For example, the thickness t5 of the buffer layer 17 can be in a range between one fourth the thickness t4 of the metal strip 16 and the thickness t4 of the metal strip 16. Selection of the thicknesses t1-t5 and the width w1, w2 from the ranges disclosed herein can be critical in providing the advantages disclosed herein.
As illustrated, the metal strip 16 can be positioned over edge portion near the distal end 22b of a finger 22. In some applications, the displacement distance d can be up to 0.1λ. For example, the displacement d can be in a range from 0.01λ to 0.1λ. In some applications, the displacement d can be up to 400 nm. For example, the displacement d can be in a range from 10 nm to 400 nm. With such displacements, the performance of the SAW resonator 1′ should not be significantly degraded relative to the SAW resonator 1.
In an acoustic wave device that includes a metal strip, a void may be formed in a temperature compensation layer along a surface (e.g., a sidewall, a top surface, and/or a bottom surface) of the metal strip. Such a void can negatively affect suppression of the transverse mode. Especially, when a size of the void is relatively large, a proper transverse mode suppression may not be obtained. The buffer layer 17, 17′ can minimize the size of the void or prevent and/or mitigate formation of the void.
In
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After the step shown in
In
The deposition process can include a sputter deposition. A sputtering temperature for forming the upper layer 114b can be in a range between 200° C. and 300° C. In some embodiments, during the deposition process, materials (e.g., chemical components) of the upper layer 114b and the metal strip 16 can react with each other, thereby forming the buffer layer 17 as shown in
In some embodiments, the temperature compensation layer 14 and the metal strip 16 can be annealed at a temperature in a range between, for example, 300° C. and 400° C. During the deposition process, materials (e.g., chemical components) of the upper layer 114b and the metal strip 16 can react with each other, thereby forming the buffer layer 17′ as shown in
In some embodiments, the buffer layer 17 can be formed by way of deposition with or without relying on application of heat to form the buffer layer 17, 17′. For example, the buffer layer 17, 17′ can be deposited over the metal strip 16. For example, the buffer layer 17′ can be deposited on the lower layer 114a before forming the metal strip 16.
In
Any SAW resonator disclosed herein can be manufactured in the same or generally similar manner as the manufacturing processes illustrated in
In some embodiments, the dispersion adjustment layer 21″ can have a thickness up to 150 nm. For example, the dispersion adjustment layer 21″ can have a thickness in a range from 1 nm to 150 nm, in a range from 10 nm to 150 nm, in a range from 50 nm to 150 nm, in a range from 1 nm to 100 nm, in a range from 50 nm to 100 nm, or in a range from 70 nm to 100 nm. In some other embodiments, the thickness of the dispersion adjustment layer 21″ can be thicker than 150 nm. As illustrated in
In some embodiments, the passivation layer 23 can have a thickness up to about 100 nm. For example, the passivation layer 23 can be in a range from 1 nm to 100 nm, in a range from 10 nm to 100 nm, in a range from 50 nm to 100 nm, in a range from 1 nm to 50 nm, in a range from 10 nm to 50 nm, or in a range from 50 nm to 70 nm. In some other embodiments, the thickness of the passivation layer 23 can be thicker than 100 nm.
The adhesion layer 20 can have any suitable thickness t6 that can provide an improved adhesion as compared to the metal strip 16 without the adhesion layer 20. For example, the thickness t6 can be less than about 50 nm. In certain embodiments, the thickness t6 of the adhesion layer 20 can be in a range from 10 nm to 50 nm to provide an improved polarization.
As illustrated in
In some other embodiments, a multi-layer conductive strip can include two or more layers of high density metal. The high density metal layers can be of different high density material. Example high density metals include molybdenum (Mo), tungsten (W), gold (Au), silver (Ag), ruthenium (Ru), copper (Cu), platinum (Pt), iridium (Ir) or the like.
The conductive strips disclosed herein can be disposed at any suitable position that is a distance r from the piezoelectric layer 10 (or from the lower surface 14a of the temperature compensation layer 14). The distance r may be selected relative to the thickness t1 of the temperature compensation layer 14. For example, the distance r can be in a range from 0.2×t1 to 0.8×t1 in some embodiments, in which t1 is the thickness of the temperature compensation layer 14. When the dispersion adjustment layer 21 is disposed over the temperature compensation layer 14, it may be preferable for the distance r to be in a range from 0.4×t1 to 0.6×t1.
The support substrate 31 can be any suitable substrate layer, such as a silicon layer, a quartz layer, a ceramic layer, a glass layer, a spinel layer, a magnesium oxide spinel layer, a sapphire layer, a diamond layer, a silicon carbide layer, a silicon nitride layer, an aluminum nitride layer, or the like. As one example, the SAW resonator 7 can include a piezoelectric layer 10 that is a lithium niobate layer and a support substrate 31 that is silicon substrate.
The support substrate 31 can have a relatively high acoustic impedance. An acoustic impedance of the support substrate 31 can be higher than an acoustic impedance of the piezoelectric layer 10. For instance, the support substrate 31 can have a higher acoustic impedance than an acoustic impedance of lithium niobate and a higher acoustic impedance than lithium tantalate. The acoustic impedance of the support substrate 31 can be higher than an acoustic impedance of the temperature compensation layer 14. The SAW resonator 7 including the piezoelectric layer 10 on a support substrate 31 with relatively high thermal conductivity, such as silicon substrate, can achieve better thermal dissipation compared to a similar SAW resonator without the high impedance support substrate 31.
In certain embodiments, a SAW resonator can include two or more layers on the side of the piezoelectric layer 10 that is opposite to the IDT electrode 12′. In some embodiments, there can be an additional layer between the piezoelectric layer 10 and the support substrate 31. The additional layer can be a low impedance layer that has a lower acoustic impedance than the support substrate 31. In some embodiments, the additional layer can be a silicon dioxide (SiO2) layer. The additional layer can increase an adhesion strength between layers of the multi-layer piezoelectric substrate. In such applications, the additional layer can be referred to as an adhesion layer. Alternatively or additionally, the additional layer can increase heat dissipation in the SAW resonator relative to a similar SAW resonator without the additional layer. In such applications, the additional layer can be referred to as a heat dissipation layer. The additional layer can reduce back reflection of the support substrate in certain applications. In such applications, the additional layer can scatter back reflections by beam scattering. In some instances, the additional layer can be a polycrystalline spinel layer and the support substrate 31 can be a silicon layer.
The mass loading strips disclosed herein can be implemented together with a piston mode structure of an IDT electrode and/or with an overlying layer arranged to adjust acoustic velocity in an underlying region of an acoustic wave device.
For example, the first layer 26 can be tungsten (W) and the second layer 28 can be aluminum (Al) in certain embodiments. As another example, the first layer 26 can be aluminum (Al) and the second layer 28 can be tungsten (W), in certain embodiments. The first layer 26 may include one or more other metals, such as copper (Cu), Magnesium (Mg), titanium (Ti), molybdenum (Mo), etc. The first layer 26 may include alloys, such as AlMgCu, AlCu, etc. The second layer 28 may include one or more other metals, such as copper (Cu), Magnesium (Mg), titanium (Ti), molybdenum (Mo), etc. The second layer 28 may include alloys, such as AlMgCu, AlCu, etc.
The first layer 26 can impact acoustic properties of the SAW resonator and the second layer 28 can impact electrical properties of the SAW resonator, in some embodiments. For example, when the first layer 26 is an aluminum (Al) layer and the second layer 28 is a tungsten (W) layer, the Al layer can impact acoustic properties of the SAW resonator and the W layer can impact electrical properties of the SAW resonator. In some other embodiments, the second layer 28 can impact acoustic properties of the SAW resonator and the first layer 26 can impact electrical properties of the SAW resonator. For example, when the first layer 26 is a W layer and the second layer 28 is an Al layer, the Al layer can impact acoustic properties of the SAW resonator and the W layer can impact electrical properties of the SAW resonator.
The third layer 46 may include one or more of tungsten (W), aluminum (Al), copper (Cu), Magnesium (Mg), titanium (Ti), molybdenum (Mo), etc. The first layer 26 may include alloys, such as AlMgCu, AlCu, etc. For example, the first layer 26 can be titanium (Ti), the second layer 28 can be tungsten (W), and the third layer can be aluminum (Al) in certain embodiments. In some embodiments, the third layer 46 can impact acoustic properties of the SAW resonator. In some other embodiments, the third layer 46 can impact electrical properties of the SAW resonator. When titanium (Ti) is used as the first layer 26, the Ti layer can provide desirable crystal orientation for an overlying layer (the second layer 28 and/or the third layer 46.
A method of manufacturing an acoustic wave resonator according to an embodiment will now be described. The method can include providing an acoustic wave resonator structure with a temperature compensation layer over an interdigital transducer electrode. For example, the interdigital transducer electrode can be positioned on a piezoelectric layer. The interdigital transducer electrode includes fingers extending from a bus bar. The fingers each include an edge portion and a body portion. The method includes forming a conductive strip that overlaps with the edge portions of the fingers of the interdigital transducer electrode. The conductive strip includes a layer having a density at least as high as a density of a material of the interdigital transducer electrode that is in contact with the piezoelectric layer. A portion of the temperature compensation layer is positioned between the conductive strip and the interdigital transducer electrode. Forming the conductive strip may include depositing a second layer of the conductive strip over the piezoelectric layer such that the second layer is positioned between the piezoelectric layer and the layer of the conductive strip.
A method of filtering a radio frequency signal according to an embodiment will now be described. The method includes receiving a radio frequency signal at an input port of an acoustic wave filter that includes an acoustic wave resonator. The acoustic wave resonator includes a piezoelectric layer, an interdigital transducer electrode on the piezoelectric layer, and a conductive strip that overlaps edge portions of fingers of the interdigital transducer electrode. The conductive strip includes a layer having a density that is at least as high as a density of a material of the interdigital transducer electrode that is in contact with the piezoelectric layer. The method also includes filtering the radio frequency signal with the acoustic wave filter. The filtering includes suppressing a transverse mode using the conductive strip of the acoustic wave resonator. The filtering can be performed, for example, with the transmit filter 45 of
A SAW device including any suitable combination of features disclosed herein be included in a filter arranged to filter a radio frequency signal in a fifth generation (5G) New Radio (NR) operating band within Frequency Range 1 (FR1). A filter arranged to filter a radio frequency signal in a 5G NR operating band can include one or more SAW devices disclosed herein. FR1 can be from 410 MHz to 7.125 GHz, for example, as specified in a current 5G NR specification. One or more SAW devices in accordance with any suitable principles and advantages disclosed herein can be included in a filter arranged to filter a radio frequency signal in a 4G LTE operating band and/or in a filter having a passband that includes a 4G LTE operating band and a 5G NR operating band.
The SAW component 76 shown in
The duplexers 85A to 85N can each include two acoustic wave filters coupled to a common node. The two acoustic wave filters can be a transmit filter and a receive filter. As illustrated, the transmit filter and the receive filter can each be band pass filters arranged to filter a radio frequency signal. One or more of the transmit filters 86A1 to 86N1 can include one or more SAW resonators in accordance with any suitable principles and advantages disclosed herein. Similarly, one or more of the receive filters 86A2 to 86N2 can include one or more SAW resonators in accordance with any suitable principles and advantages disclosed herein. Although
The power amplifier 87 can amplify a radio frequency signal. The illustrated switch 88 is a multi-throw radio frequency switch. The switch 88 can electrically couple an output of the power amplifier 87 to a selected transmit filter of the transmit filters 86A1 to 86N1. In some instances, the switch 88 can electrically connect the output of the power amplifier 87 to more than one of the transmit filters 86A1 to 86N1. The antenna switch 89 can selectively couple a signal from one or more of the duplexers 85A to 85N to an antenna port ANT. The duplexers 85A to 85N can be associated with different frequency bands and/or different modes of operation (e.g., different power modes, different signaling modes, etc.).
The RF front end 92 can include one or more power amplifiers, one or more low noise amplifiers, one or more RF switches, one or more receive filters, one or more transmit filters, one or more duplex filters, one or more multiplexers, one or more frequency multiplexing circuits, the like, or any suitable combination thereof. The RF front end 92 can transmit and receive RF signals associated with any suitable communication standards. The filters 93 can include SAW resonators of a SAW component that includes any suitable combination of features discussed with reference to any embodiments discussed above.
The transceiver 94 can provide RF signals to the RF front end 92 for amplification and/or other processing. The transceiver 94 can also process an RF signal provided by a low noise amplifier of the RF front end 92. The transceiver 94 is in communication with the processor 95. The processor 95 can be a baseband processor. The processor 95 can provide any suitable base band processing functions for the wireless communication device 90. The memory 96 can be accessed by the processor 95. The memory 96 can store any suitable data for the wireless communication device 90. The user interface 97 can be any suitable user interface, such as a display with touch screen capabilities.
Although embodiments disclosed herein relate to surface acoustic wave resonators, any suitable principles and advantages disclosed herein can be applied to other types of acoustic wave resonators, such as Lamb wave resonators and/or boundary wave resonators. For example, any suitable combination of features of the conductive strips disclosed herein can be applied to a Lamb wave resonator and/or a boundary wave resonator.
Any of the embodiments described above can be implemented in association with mobile devices such as cellular handsets. The principles and advantages of the embodiments can be used for any systems or apparatus, such as any uplink wireless communication device, that could benefit from any of the embodiments described herein. The teachings herein are applicable to a variety of systems. Although this disclosure includes some example embodiments, the teachings described herein can be applied to a variety of structures. Any of the principles and advantages discussed herein can be implemented in association with RF circuits configured to process signals in a frequency range from about 30 kHz to 300 GHz, such as in a frequency range from about 450 MHz to 8.5 GHz.
Aspects of this disclosure can be implemented in various electronic devices. Examples of the electronic devices can include, but are not limited to, consumer electronic products, parts of the consumer electronic products such as packaged radio frequency modules, uplink wireless communication devices, wireless communication infrastructure, electronic test equipment, etc. Examples of the electronic devices can include, but are not limited to, a mobile phone such as a smart phone, a wearable computing device such as a smart watch or an ear piece, a telephone, a television, a computer monitor, a computer, a modem, a hand-held computer, a laptop computer, a tablet computer, a microwave, a refrigerator, a vehicular electronics system such as an automotive electronics system, a stereo system, a digital music player, a radio, a camera such as a digital camera, a portable memory chip, a washer, a dryer, a washer/dryer, a copier, a facsimile machine, a scanner, a multi-functional peripheral device, a wrist watch, a clock, etc. Further, the electronic devices can include unfinished products.
Unless the context clearly requires otherwise, throughout the description and the claims, the words “comprise,” “comprising,” “include,” “including” and the like are to be construed in an inclusive sense, as opposed to an exclusive or exhaustive sense; that is to say, in the sense of “including, but not limited to.” The word “coupled”, as generally used herein, refers to two or more elements that may be either directly connected, or connected by way of one or more intermediate elements. Likewise, the word “connected”, as generally used herein, refers to two or more elements that may be either directly connected, or connected by way of one or more intermediate elements. Additionally, the words “herein,” “above,” “below,” and words of similar import, when used in this application, shall refer to this application as a whole and not to any particular portions of this application. Where the context permits, words in the above Detailed Description using the singular or plural number may also include the plural or singular number respectively. The word “or” in reference to a list of two or more items, that word covers all of the following interpretations of the word: any of the items in the list, all of the items in the list, and any combination of the items in the list.
Moreover, conditional language used herein, such as, among others, “can,” “could,” “might,” “may,” “e.g.,” “for example,” “such as” and the like, unless specifically stated otherwise, or otherwise understood within the context as used, is generally intended to convey that certain embodiments include, while other embodiments do not include, certain features, elements and/or states. Thus, such conditional language is not generally intended to imply that features, elements and/or states are in any way required for one or more embodiments or that one or more embodiments necessarily include logic for deciding, with or without author input or prompting, whether these features, elements and/or states are included or are to be performed in any particular embodiment.
While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the disclosure. Indeed, the novel apparatus, methods, and systems described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the methods and systems described herein may be made without departing from the spirit of the disclosure. For example, while blocks are presented in a given arrangement, alternative embodiments may perform similar functionalities with different components and/or circuit topologies, and some blocks may be deleted, moved, added, subdivided, combined, and/or modified. Each of these blocks may be implemented in a variety of different ways. Any suitable combination of the elements and acts of the various embodiments described above can be combined to provide further embodiments. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the disclosure.
Claims
1. An acoustic wave device comprising:
- a piezoelectric layer;
- an interdigital transducer electrode formed with the piezoelectric layer, the interdigital transducer electrode including a bus bar and fingers extending from the bus bar, the fingers each including an edge portion and a body portion;
- a temperature compensation layer over the interdigital transducer electrode;
- a mass loading strip overlapping the edge portions of the fingers, a portion of the temperature compensation layer being positioned between the mass loading strip and the piezoelectric layer; and
- a buffer layer disposed at least partially between the mass loading strip and the temperature compensation layer, the buffer layer including a material different from materials of the temperature compensation layer and the mass loading strip.
2. The acoustic wave device of claim 1 wherein the mass loading strip includes a layer having a density that is at least as high as a most dense layer of a material of the interdigital transducer electrode.
3. The acoustic wave device of claim 2 wherein the mass loading strip includes a second layer.
4. The acoustic wave device of claim 1 wherein the mass loading strip is embedded in the temperature compensation layer.
5. The acoustic wave device of claim 1 wherein the temperature compensation layer is a silicon dioxide layer, and the mass loading strip is a molybdenum layer.
6. The acoustic wave device of claim 1 wherein the buffer layer has a coefficient of thermal expansion greater than a coefficient of thermal expansion of the temperature compensation layer and less than a coefficient of thermal expansion of the mass loading strip.
7. The acoustic wave device of claim 1 wherein the mass loading strip has a bottom side, an top side, and a sidewall extending between the bottom side and the top side, the buffer layer is disposed between the top side and the sidewall of the mass loading strip and the temperature compensation layer.
8. The acoustic wave device of claim 1 wherein a difference between the coefficient of thermal expansion of the temperature compensation layer and the coefficient of thermal expansion of the metal strip is ΔCTE, the coefficient of thermal expansion of the buffer layer is 0.2ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer.
9. The acoustic wave device of claim 8 wherein the coefficient of thermal expansion of the buffer layer is 0.3ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer.
10. A method of forming an acoustic wave device, the method comprising:
- forming an interdigital transducer electrode formed with a piezoelectric layer, the interdigital transducer electrode including a bus bar and fingers extending from the bus bar, the fingers each including an edge portion and a body portion;
- forming a temperature compensation layer over the interdigital transducer electrode;
- forming a mass loading strip overlapping the edge portions of the fingers, a portion of the temperature compensation layer being positioned between the mass loading strip and the piezoelectric layer; and
- forming a buffer layer disposed at least partially between the mass loading strip and the temperature compensation layer, the forming the buffer layer including depositing the mass loading strip.
11. The method of claim 10 wherein the mass loading strip includes a layer having a density that is at least as high as a most dense layer of a material of the interdigital transducer electrode, and the mass loading strip is embedded in the temperature compensation layer.
12. The method of claim 10 wherein the temperature compensation layer is a silicon dioxide layer, and the mass loading strip is a molybdenum layer.
13. The method of claim 10 wherein a thickness of the buffer layer is at least one forth a thickness of the mass loading strip.
14. The method of claim 10 wherein the buffer layer has a coefficient of thermal expansion greater than a coefficient of thermal expansion of the temperature compensation layer and less than a coefficient of thermal expansion of the mass loading strip.
15. The method of claim 10 wherein the mass loading strip has a bottom side, an top side, and a sidewall extending between the bottom side and the top side, the buffer layer is disposed between the top side and the sidewall of the mass loading strip and the temperature compensation layer.
16. The method of claim 15 wherein the buffer layer is further disposed between the bottom side of the mass loading strip and the temperature compensation layer.
17. The method of claim 10 wherein a difference between the coefficient of thermal expansion of the temperature compensation layer and the coefficient of thermal expansion of the metal strip is ΔCTE, the coefficient of thermal expansion of the buffer layer is 0.2ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer.
18. The method of claim 17 wherein the coefficient of thermal expansion of the buffer layer is 0.3ΔCTE to 0.75ΔCTE greater than the coefficient of thermal expansion of the temperature compensation layer.
19. The method of claim 10 wherein the forming the buffer layer includes reacting the mass loading strip and the temperature compensation layer.
20. The method of claim 19 wherein the forming the temperature compensation layer includes sputtering the temperature compensation layer at a sputtering temperature in a range between 200° C. and 300° C.
Type: Application
Filed: Mar 28, 2023
Publication Date: Oct 26, 2023
Inventors: Yumi Torazawa (Takatsuki-Shi), Hironori Fukuhara (Ibaraki-Shi), Yuji Yashiro (Kizugawa-Shi), Kenta Morita (Amagasaki-Shi)
Application Number: 18/191,497