Transversely-excited film bulk acoustic resonator with etched conductor patterns

Information

  • Patent Grant
  • 11967943
  • Patent Number
    11,967,943
  • Date Filed
    Thursday, February 17, 2022
    2 years ago
  • Date Issued
    Tuesday, April 23, 2024
    13 days ago
Abstract
An acoustic resonator is fabricated by forming a patterned first photoresist mask on a piezoelectric plate at locations of a desired interdigital transducer (IDT) pattern. An etch-stop layer is then deposited on the plate and first photoresist mask. The first photoresist mask is removed to remove parts of the etch-stop and expose the plate. An IDT conductor material is deposited on the etch stop and the exposed plate. A patterned second photoresist mask is then formed on the conductor material at locations of the IDT pattern. The conductor material is then etched over and to the etch-stop to form the IDT pattern which has interleaved fingers on a diaphragm to span a substrate cavity. A portion of the plate and the etch-stop form the diaphragm. The etch-stop and photoresist mask are impervious to this etch. The second photoresist mask is removed to leave the IDT pattern.
Description
NOTICE OF COPYRIGHTS AND TRADE DRESS

A portion of the disclosure of this patent document contains material which is subject to copyright protection. This patent document may show and/or describe matter which is or may become trade dress of the owner. The copyright and trade dress owner has no objection to the facsimile reproduction by anyone of the patent disclosure as it appears in the Patent and Trademark Office patent files or records, but otherwise reserves all copyright and trade dress rights whatsoever.


BACKGROUND
Field

This disclosure relates to radio frequency filters using acoustic wave resonators, and specifically to filters for use in communications equipment.


Description of the Related Art

A radio frequency (RF) filter is a two-port device configured to pass some frequencies and to stop other frequencies, where “pass” means transmit with relatively low signal loss and “stop” means block or substantially attenuate. The range of frequencies passed by a filter is referred to as the “pass-band” of the filter. The range of frequencies stopped by such a filter is referred to as the “stop-band” of the filter. A typical RF filter has at least one pass-band and at least one stop-band. Specific requirements on a passband or stop-band depend on the specific application. For example, a “pass-band” may be defined as a frequency range where the insertion loss of a filter is better than a defined value such as 1 dB, 2 dB, or 3 dB. A “stop-band” may be defined as a frequency range where the rejection of a filter is greater than a defined value such as 20 dB, 30 dB, 40 dB, or greater depending on application.


RF filters are used in communications systems where information is transmitted over wireless links. For example, RF filters may be found in the RF front-ends of cellular base stations, mobile telephone and computing devices, satellite transceivers and ground stations, IoT (Internet of Things) devices, laptop computers and tablets, fixed point radio links, and other communications systems. RF filters are also used in radar and electronic and information warfare systems.


RF filters typically require many design trade-offs to achieve, for each specific application, the best compromise between performance parameters such as insertion loss, rejection, isolation, power handling, linearity, size and cost. Specific design and manufacturing methods and enhancements can benefit simultaneously one or several of these requirements.


Performance enhancements to the RF filters in a wireless system can have broad impact to system performance. Improvements in RF filters can be leveraged to provide system performance improvements such as larger cell size, longer battery life, higher data rates, greater network capacity, lower cost, enhanced security, higher reliability, etc. These improvements can be realized at many levels of the wireless system both separately and in combination, for example at the RF module, RF transceiver, mobile or fixed sub-system, or network levels.


The desire for wider communication channel bandwidths will inevitably lead to the use of higher frequency communications bands. The current LTE™ (Long Term Evolution) specification defines frequency bands from 3.3 GHz to 5.9 GHz. These bands are not presently used. Future proposals for wireless communications include millimeter wave communication bands with frequencies up to 28 GHz.


High performance RF filters for present communication systems commonly incorporate acoustic wave resonators including surface acoustic wave (SAW) resonators, bulk acoustic wave (BAW) resonators, film bulk acoustic wave resonators (FBAR), and other types of acoustic resonators. However, these existing technologies are not well-suited for use at the higher frequencies proposed for future communications networks.





DESCRIPTION OF THE DRAWINGS


FIG. 1 includes a schematic plan view and two schematic cross-sectional views of a transversely-excited film bulk acoustic resonator (XBAR).



FIG. 2 is an expanded schematic cross-sectional view of a portion of an XBAR with an etch-stop layer.



FIG. 3 is an expanded schematic cross-sectional view of a portion of another XBAR with an etch-stop layer.



FIG. 4 is a graphic illustrating a shear horizontal acoustic mode in an XBAR.



FIG. 5 is a schematic block diagram of a filter using XBARs.



FIG. 6 is a flow chart of a process for fabricating an XBAR.



FIG. 7A and FIG. 7B are collectively a flow chart of a process for forming a conductor pattern using dry etching and an etch-stop layer.



FIG. 8A and FIG. 8B are collectively a flow chart of another process for forming a conductor pattern using dry etching and an etch-stop layer.





Throughout this description, elements appearing in figures are assigned three-digit or four-digit reference designators, where the two least significant digits are specific to the element and the one or two most significant digit is the figure number where the element is first introduced. An element that is not described in conjunction with a figure may be presumed to have the same characteristics and function as a previously-described element having the same reference designator.


DETAILED DESCRIPTION

Description of Apparatus



FIG. 1 shows a simplified schematic top view and orthogonal cross-sectional views of a transversely-excited film bulk acoustic resonator (XBAR) 100. XBAR resonators such as the resonator 100 may be used in a variety of RF filters including band-reject filters, band-pass filters, duplexers, and multiplexers. XBARs are particularly suited for use in filters for communications bands with frequencies above 3 GHz.


The XBAR 100 is made up of a thin film conductor pattern formed on a surface of a piezoelectric plate 110 having parallel front and back surfaces 112, 114, respectively. The piezoelectric plate is a thin single-crystal layer of a piezoelectric material such as lithium niobate, lithium tantalate, lanthanum gallium silicate, gallium nitride, or aluminum nitride. The piezoelectric plate is cut such that the orientation of the X, Y, and Z crystalline axes with respect to the front and back surfaces is known and consistent. In the examples presented in this patent, the piezoelectric plates are Z-cut, which is to say the Z axis is normal to the front and back surfaces 112, 114. However, XBARs may be fabricated on piezoelectric plates with other crystallographic orientations.


The back surface 114 of the piezoelectric plate 110 is attached to a surface of the substrate 120 except for a portion of the piezoelectric plate 110 that forms a diaphragm 115 spanning a cavity 140 formed in the substrate. The portion of the piezoelectric plate that spans the cavity is referred to herein as the “diaphragm” 115 due to its physical resemblance to the diaphragm of a microphone. As shown in FIG. 1, the diaphragm 115 is contiguous with the rest of the piezoelectric plate 110 around all of a perimeter 145 of the cavity 140. In this context, “contiguous” means “continuously connected without any intervening item”.


The substrate 120 provides mechanical support to the piezoelectric plate 110. The substrate 120 may be, for example, silicon, sapphire, quartz, or some other material or combination of materials. The back surface 114 of the piezoelectric plate 110 may be bonded to the substrate 120 using a wafer bonding process. Alternatively, the piezoelectric plate 110 may be grown on the substrate 120 or attached to the substrate in some other manner. The piezoelectric plate 110 may be attached directly to the substrate or may be attached to the substrate 120 via one or more intermediate material layers.


“Cavity” has its conventional meaning of “an empty space within a solid body.” The cavity 140 may be a hole completely through the substrate 120 (as shown in Section A-A and Section B-B) or a recess in the substrate 120. The cavity 140 may be formed, for example, by etching a portion of the substrate 120 to form a separate cavity for a resonator, before or after the piezoelectric plate 110 and the substrate 120 are attached. This etch may be selective by having a chemistry to etch the material of the substrate but not the material piezoelectric plate.


The conductor pattern of the XBAR 100 includes an interdigital transducer (IDT) 130. The IDT 130 includes a first plurality of parallel fingers, such as finger 136, extending from a first busbar 132 and a second plurality of fingers extending from a second busbar 134. The first and second pluralities of parallel fingers are interleaved. The interleaved fingers overlap for a distance AP, commonly referred to as the “aperture” of the IDT. The center-to-center distance L between the outermost fingers of the IDT 130 is the “length” of the IDT.


The first and second busbars 132, 134 serve as the terminals of the XBAR 100. A radio frequency or microwave signal applied between the two busbars 132, 134 of the IDT 130 excites a primary acoustic mode within the piezoelectric plate 110. As will be discussed in further detail, the primary acoustic mode is a bulk shear mode where acoustic energy propagates along a direction substantially orthogonal to the surface of the piezoelectric plate 110, which is also normal, or transverse, to the direction of the electric field created by the IDT fingers. Thus, the XBAR is considered a transversely-excited film bulk wave resonator.


The IDT 130 is positioned on the piezoelectric plate 110 such that at least the fingers of the IDT 130 are disposed on the portion 115 of the piezoelectric plate that spans, or is suspended over, the cavity 140. As shown in FIG. 1, the cavity 140 has a rectangular shape with an extent greater than the aperture AP and length L of the IDT 130. A cavity of an XBAR may have a different shape, such as a regular or irregular polygon. The cavity of an XBAR may more or fewer than four sides, which may be straight or curved.


For ease of presentation in FIG. 1, the geometric pitch and width of the IDT fingers is greatly exaggerated with respect to the length (dimension L) and aperture (dimension AP) of the XBAR. A typical XBAR has more than ten parallel fingers in the IDT 110. An XBAR may have hundreds, possibly thousands, of parallel fingers in the IDT 110. Similarly, the thickness of the fingers in the cross-sectional views is greatly exaggerated.



FIG. 2 is an expanded schematic cross-sectional view of a portion of another XBAR device 200 including an etch-stop layer. The piezoelectric plate 110 is a single-crystal layer of piezoelectrical material having a thickness ts. ts may be, for example, 100 nm to 1500 nm.


The width of XBAR IDT fingers may be 500 nm or greater. The thickness tm of the IDT fingers may be from 100 nm to about equal to the width w. The thickness of the busbars (132, 134 in FIG. 1) of the IDT may be the same as, or greater than, the thickness tm of the IDT fingers.



FIG. 2 also shows two IDT fingers 236, 238 formed on the piezoelectric plate 110 which is a portion of the diaphragm of the XBAR device 200. Traditionally, the IDT fingers, such as the fingers 236, 238, and other conductors of an XBAR device have been formed using a lift-off photolithography process. Photoresist is deposited over the piezoelectric plate and patterned to define the conductor pattern. The IDT conductor layer and, optionally, one or more other layers are deposited in sequence over the surface of the piezoelectric plate. The photoresist may then be removed, which removes, or lifts off, the excess material, leaving the conductor pattern including the IDT fingers. Using a lift-off process does not expose the surface 112 of the piezoelectric plate to reactive chemicals. However, it may be difficult to control the sidewall angle of conductors formed using a lift-off process.


In the XBAR device 200, the IDT fingers 236, 238 are formed using a subtractive or etching process that may provide good control of conductor sidewall angles. One or more metal layers are deposited in sequence over the surface of the piezoelectric plate. The excess metal is then be removed by an anisotropic etch through the conductor layer where it is not protected by a patterned photoresist. The conductor layer can be etched, for example, by anisotropic plasma etching, reactive ion etching, wet chemical etching, and other etching technique.


To protect the surface 112 of the piezoelectric plate 110 from being damaged by the process and chemicals used to etch the conductor layers, the XBAR device 200 includes an etch-stop layer 210 formed on the surface 112 of the piezoelectric plate 110. In FIG. 2, the etch stop layer 210 is shown between but not under the IDT fingers 236, 238. The etch-stop layer 210 may be formed over the entire surface of the piezoelectric plate except under all of the IDT fingers. Alternatively, the etch-stop layer 210 may be formed over the entire surface of the piezoelectric plate except under all conductors.


The etch-stop layer 210 protects the front surface 112 of the piezoelectric plate 110 from the etch process. To this end, the etch-stop layer 210 must be impervious to the etch process or be etched magnitudes slower than the conductor by the etch process. The words “impervious to” have several definitions including “not affected by” and “not allowing etching or to pass through”. Both of these definitions apply to the etch-stop layer 210. The etch-stop layer is not materially affected by the etch process and does not allow the liquid or gaseous etchant used in the etch process to penetrate to the piezoelectric plate 110. The etch-stop layer need not be inert with respect to the etchant but must be highly resistant to the etchant such that a substantial portion of the thickness of the etch stop layer remains after completion of the conductor etch. The remaining etch stop layer 210 is not removed after the IDT fingers 236, 238 and other conductors are formed and becomes a portion of the diaphragm of the XBAR device 200.


The etch-stop layer 210 is formed from an etch-stop material. The etch-stop material must be a dielectric with very low electrical conductivity and low acoustic loss. The etch-stop material must have high adhesion to the surface 112 on which it is deposited. Most importantly, the etch-stop material must be impervious, as previously defined, to the processes and chemicals used to etch the conductors. Alternatively, the etch-stop material must be etched magnitudes slower than the conductor by the processes and chemicals used to etch the conductors. In some cases, a viable etch stop material must withstand the chemistry used to etch IDT material. A material chosen for etch stop purposes may be either etchable with chemistry that does not etch the piezoelectric plate, or be a material that does not degrade the performance of the resonator(s). Suitable etch-stop materials may include oxides such as aluminum oxide and silicon dioxide, sapphire, nitrides including silicon nitride, aluminum nitride, and boron nitride, silicon carbide, and diamond. In some cases, it is an etch stop metal oxide layer.


The XBAR device 200 may include one or more additional dielectric layers that are shown in FIG. 2. A front side dielectric layer 220 may be formed over the IDTs of some (e.g., selected ones) of the XBAR devices in a filter. The “front side” of the XBAR is, by definition, the surface facing away from the substrate. The front-side dielectric layer 220 has a thickness tfd. The front-side dielectric layer 220 may be formed between the IDT fingers 226 and 228. In FIG. 2, the front side dielectric 220 covers the IDT finger 238 but not the IDT finger 236. In a filter, the front side dielectric may be formed over all of the fingers of some XBAR devices. For example, a front side dielectric layer may be formed over the IDTs of shunt resonators to lower the resonance frequencies of the shunt resonators with respect to the resonance frequencies of series resonators. Some filters may include two or more different thicknesses of front side dielectric over various resonators. A back-side dielectric layer (not shown) may optionally be formed on the back side of the piezoelectric plate 110.


Further, a passivation layer 230 may be formed over the entire surface of the XBAR device 200 except for contact pads where electric connections are made to circuity external to the XBAR device. The passivation layer is a thin dielectric layer intended to seal and protect the surfaces of the XBAR device while the XBAR device is incorporated into a package. The front side dielectric layer 220, backside dielectric and the passivation layer 230 may each be, SiO2, Si3N4, Al2O3, some other dielectric material, or a combination of these materials.


Thickness tp may be a thickness that is selected to protect the piezoelectric plate and the metal electrodes from water and chemical corrosion, particularly for power durability purposes. The typical layer thickness tp may range from 10 to 100 nm. The passivation material may consist of multiple oxide and/or nitride coatings such as SiO2 and Si3N4 material.


Examples of thickness tes include between 10 to 30 nm. Thickness tes may be a thickness that is selected to ensure that the etch-stop layer cannot be etched completely through by the etch process used to etch the conductor material that forms the IDT.



FIG. 3 is an expanded schematic cross-sectional view of a portion of another XBAR device 300 including an etch-stop layer. FIG. 3 shows two IDT fingers 236, 238 formed on a piezoelectric plate 110 which is a portion of the diaphragm of the XBAR device 300. The exception of the etch-stop layer 310, all of the elements of the XBAR device 300 have the same function and characteristics as the corresponding element of the XBAR device 200 of FIG. 2. Descriptions of these elements will not be repeated.


The XBAR device 300 differs from the XBAR device 200 in that the etch stop layer 310 extends over the entire surface 112 of the piezoelectric plate 110 including under the IDT fingers 236, 238. The etch-stop layer 310 may be formed over the entire surface of the piezoelectric plate including under all of the conductors including the IDT fingers. The etch-stop layer 310 is an etch-stop material as previously described.



FIG. 4 is a graphical illustration of the primary acoustic mode of interest in an XBAR. FIG. 4 shows a small portion of an XBAR 400 including a piezoelectric plate 410 and three interleaved IDT fingers 430. An RF voltage is applied to the interleaved fingers 430. This voltage creates a time-varying electric field between the fingers. The direction of the electric field is lateral, or parallel to the surface of the piezoelectric plate 410, as indicated by the arrows labeled “electric field”. Due to the high dielectric constant of the piezoelectric plate, the electric field is highly concentrated in the plate relative to the air. The lateral electric field introduces shear deformation, and thus strongly excites a primary shear-mode acoustic mode, in the piezoelectric plate 410. In this context, “shear deformation” is defined as deformation in which parallel planes in a material remain parallel and maintain a constant distance while translating relative to each other. A “shear acoustic mode” is defined as an acoustic vibration mode in a medium that results in shear deformation of the medium. The shear deformations in the XBAR 400 are represented by the curves 460, with the adjacent small arrows providing a schematic indication of the direction and magnitude of atomic motion. The degree of atomic motion, as well as the thickness of the piezoelectric plate 410, have been greatly exaggerated for ease of visualization. While the atomic motions are predominantly lateral (i.e. horizontal as shown in FIG. 4), the direction of acoustic energy flow of the excited primary shear acoustic mode is substantially orthogonal to the surface of the piezoelectric plate, as indicated by the arrow 465.


An acoustic resonator based on shear acoustic wave resonances can achieve better performance than current state-of-the art film-bulk-acoustic-resonators (FBAR) and solidly-mounted-resonator bulk-acoustic-wave (SMR BAW) devices where the electric field is applied in the thickness direction. In such devices, the acoustic mode is compressive with atomic motions and the direction of acoustic energy flow in the thickness direction. In addition, the piezoelectric coupling for shear wave XBAR resonances can be high (>20%) compared to other acoustic resonators. High piezoelectric coupling enables the design and implementation of microwave and millimeter-wave filters with appreciable bandwidth.



FIG. 5 is a schematic circuit diagram and layout for a high frequency band-pass filter 500 using XBARs. The filter 500 has a conventional ladder filter architecture including three series resonators 510A, 510B, 510C and two shunt resonators 520A, 520B. The three series resonators 510A, 510B, and 510C are connected in series between a first port and a second port. In FIG. 5, the first and second ports are labeled “In” and “Out”, respectively. However, the filter 500 is bidirectional and either port and serve as the input or output of the filter. The two shunt resonators 520A, 520B are connected from nodes between the series resonators to ground. All the shunt resonators and series resonators are XBARs.


The three series resonators 510A, B, C and the two shunt resonators 520A, B of the filter 500 are formed on a single plate 530 of piezoelectric material bonded to a silicon substrate (not visible). Each resonator includes a respective IDT (not shown), with at least the fingers of the IDT disposed over a cavity in the substrate. In this and similar contexts, the term “respective” means “relating things each to each”, which is to say with a one-to-one correspondence. In FIG. 5, the cavities are illustrated schematically as the dashed rectangles (such as the rectangle 535). In this example, each IDT is disposed over a respective cavity. In other filters, the IDTs of two or more resonators may be disposed over a single cavity.


Description of Methods



FIG. 6 is a simplified flow chart showing a process 600 for making an XBAR or a filter incorporating XBARs. The process 600 starts at 605 with a substrate 120 and a plate of piezoelectric material 110 and ends at 695 with a completed XBAR or filter. The flow chart of FIG. 6 includes only major process steps. Various conventional process steps (e.g. surface preparation, chemical mechanical processing (CMP), cleaning, inspection, baking, annealing, monitoring, testing, etc.) may be performed before, between, after, and during the steps shown in FIG. 6.


The flow chart of FIG. 6 captures three variations of the process 600 for making an XBAR which differ in when and how cavities are formed in the substrate 120. The cavities may be formed at steps 610A, 610B, or 610C. Only one of these steps is performed in each of the three variations of the process 600.


The piezoelectric plate 110 may be, for example, Z-cut lithium niobate or lithium tantalate as used in the previously presented examples. The piezoelectric plate may be some other material and/or some other cut. The substrate may preferably be silicon. The substrate may be some other material that allows formation of deep cavities by etching or other processing.


In one variation of the process 600, one or more cavities are formed in the substrate 120 at 610A, before the piezoelectric plate is bonded to the substrate at 620. A separate cavity may be formed for each resonator in a filter device. The one or more cavities may be formed using conventional photolithographic and etching techniques. These techniques may be isotropic or anisotropic. Typically, the cavities formed at 610A will not penetrate through the substrate.


At 620, the piezoelectric plate 110 is bonded to the substrate 120. The piezoelectric plate and the substrate may be bonded by a wafer bonding process. Typically, the mating surfaces of the substrate and the piezoelectric plate are highly polished. One or more layers of intermediate materials, such as an oxide or metal, may be formed or deposited on the mating surface of one or both of the piezoelectric plate and the substrate. One or both mating surfaces may be activated using, for example, a plasma process. The mating surfaces may then be pressed together with considerable force to establish molecular bonds between the piezoelectric plate and the substrate or intermediate material layers.


A conductor pattern, including IDTs of each XBAR, is formed at 630 by depositing and patterning one or more conductor layer on the front side of the piezoelectric plate. Alternative techniques to form the conductor pattern will be discuss subsequently with respect to FIG. 7 and FIG. 8. In some cases, forming at 630 occurs prior to bonding at 620, such as where the IDT's are formed prior to bonding the plate to the substrate.


At 640, a front-side dielectric layer or layers may be formed by depositing one or more layers of dielectric material on the front side of the piezoelectric plate, over one or more desired conductor patterns of IDT or XBAR devices. The one or more dielectric layers may be deposited using a conventional deposition technique such as sputtering, evaporation, or chemical vapor deposition. The one or more dielectric layers may be deposited over the entire surface of the piezoelectric plate, including on top of the conductor pattern. Alternatively, one or more lithography processes (using photomasks) may be used to limit the deposition of the dielectric layers to selected areas of the piezoelectric plate, such as only between the interleaved fingers of the IDTs. Masks may also be used to allow deposition of different thicknesses of dielectric materials on different portions of the piezoelectric plate. In some cases, depositing at 640 includes depositing a first thickness of at least one dielectric layer over the front-side surface of selected IDTs, but no dielectric or a second thickness less than the first thickness of at least one dielectric over the other IDTs. An alternative is where these dielectric layers are only between the interleaved fingers of the IDTs.


In a second variation of the process 600, one or more cavities are formed in the back side of the substrate 120 at 610B. A separate cavity may be formed for each resonator in a filter device. The one or more cavities may be formed using an anisotropic or orientation-dependent dry or wet etch to open holes through the back-side of the substrate to the piezoelectric plate. In this case, the resulting resonator devices will have a cross-section as shown in FIG. 1.


In a third variation of the process 600, one or more cavities in the form of recesses in the substrate 120 may be formed at 610C by etching the front side of the substrate using an etchant introduced through openings in the piezoelectric plate. A separate cavity may be formed for each resonator in a filter device.


In all variations of the process 600, the filter or XBAR device is completed at 660. Actions that may occur at 660 include depositing an encapsulation/passivation layer such as SiO2 or Si3O4 over all or a portion of the device; forming bonding pads or solder bumps or other means for making connection between the device and external circuitry; excising individual devices from a wafer containing multiple devices; other packaging steps; and testing. After the filter device is completed, the process ends at 695. FIGS. 2 and 3 may show examples of the fingers of selected IDTs after completion at 660.



FIG. 7A and FIG. 7B are collectively a flow chart of a process 700 for forming a conductor pattern using dry etching and an etch-stop layer. The process 700 is or is included in the forming of conductor patterns at 630 of process 600. Process 700 is a subtractive or etching process that provides good control of conductor sidewall angles for the conductor pattern (e.g., of the IDT and/or fingers herein).


The process 700 starts at 720 with a plate of piezoelectric material 712 and ends at 750 with a completed XBAR conductor pattern 746 formed on the piezoelectric material plate 712. Piezoelectric plate 712 at 720 may be any of plates 110 and/or 410. The completed XBAR conductor pattern 746 on the plate at 750 may be a conductor pattern that is or that includes the IDT patterns and/or fingers described herein for XBAR devices.


The flow chart of FIG. 7 includes only major process steps. Various conventional process steps (e.g. surface preparation, chemical mechanical processing (CMP), cleaning, inspection, baking, annealing, monitoring, testing, etc.) may be performed before, between, after, and during the steps shown in FIG. 7.


At 720 a first patterned photoresist mask 722 is formed over piezoelectric plate 712. The photoresist mask 722 may be a patterned lithography mask that is formed over areas of the piezoelectric plate 712 where the etch stop layer is not desired. These may be areas or locations where the desired conductor pattern of the IDT or fingers are to be formed. The photoresist mask 722 may be deposited over the piezoelectric plate and patterned to define the conductor pattern where the photoresist mask 722 exists after patterning.


At 725 an etch stop material 726 is deposited over the over the piezoelectric plate 712 and over the photoresist mask 722. The etch stop material 726 may be blanket deposited over all of the exposed top surfaces of the plate and mask to form an etch-stop layer. This etch-stop layer may include the etch stop material in the pattern of etch-stop layer 210 as well as etch stop material on the photoresist mask 722. The etch stop material 726 may be a material and/or be deposited as described for etch-stop layer 210.


At 730 the first photoresist mask 722 is removed. At 730 the photoresist mask 722 may then be removed, which removes, or lifts off, the etch stop material 726 which was deposited on the photoresist mask 722, thus leaving the pattern of etch-stop layer 210 on the piezoelectric plate 712. The first photoresist mask 722 is removed using a process that does not expose the surface of the piezoelectric plate 712 to reactive chemicals or a process that will damage or etch the piezoelectric plate 712.


At 735 IDT conductor material 736 is deposited over the etch stop material 724 and over the piezoelectric plate 712 where the first photoresist mask 722 was removed. The conductor material may be an electronically conductive material and/or material used to form a conductor pattern as noted herein. Depositing at 735 may be blanket depositing one or more metal layers in sequence over the top surfaces of the etch stop material 724 and the exposed piezoelectric plate 712. The IDT conductor material 736 may be blanket deposited over all of the exposed top surfaces of the etch-stop layer 724 and of the piezoelectric plate 712.


At 740 a patterned second photoresist mask 742 is formed over the IDT conductor material 736. The photoresist mask 742 may be a patterned lithography mask that is formed over areas of the IDT conductor material 736 where the IDT conductor material 746 is desired. These may be areas or locations where the desired conductor pattern of the IDT or fingers are to be formed. The photoresist mask 742 may be blanket deposited over the IDT conductor material 736 and then patterned to define the conductor pattern 746 where the photoresist mask 742 exists after patterning.


The patterned second photoresist mask 742 may function like an etch stop in that it will be impervious to and/or be etch magnitudes slower than the conductor material by the processes and chemicals used to etch the conductor material 736. Suitable photoresist materials may include oxides such as a light sensitive material, a light-sensitive organic material (e.g., a photopolymeric, photodecomposing, or photocrosslinking photoresist), an oxide or a nitride.


At 745 IDT conductor material 736 is dry etched and removed by an anisotropic etch through the conductor where it is not protected by the second photoresist mask 742, thus forming conductor pattern 746. The conductor layer 736 can be etched, for example, by an anisotropic plasma etching, reactive ion etching, wet chemical etching, and other etching techniques. The etch may be a highly anisotropic, high-energy etch process that can damage (via chemical etch or physical sputtering) the piezoelectric layer where that layer is exposed to the etch.


The dry etch etches or removes the conductor over and to the etch stop material 724. Both, the second photoresist mask 742 and the etch stop material 724 are impervious, as previously defined, to the processes and chemicals used to etch the conductors. Alternatively, they are etched magnitudes slower than the conductor material by the processes and chemicals used to etch the conductors. Thus, this anisotropic etch does not remove the conductor material 736 under the second photoresist mask 742 and does not remove the etch stop material 724 since they are impervious and/or etched magnitudes slower. The conductor material 736 remaining under the second photoresist mask 742 and on the piezoelectric plate 712 is the conductor pattern desired for the IDT and/or fingers.


At 750 the second photoresist mask 742 is removed from the top surface of the conductor material 736. This leaves the pattern of desired conductor material 746 deposited directly onto the piezoelectric plate 712 and the etch stop material 724 between but not under the conductor material. The second photoresist mask 742 is removed using a process that does not expose the surface of the conductor to reactive chemicals or a process that will damage or etch the conductor material 746.


After removing at 750, the remaining desired conductor material 76 may be or include the IDT conductor and/or fingers described herein. It may be the conductor material in the XBAR device 200, such as the IDT fingers 236, 238. The remaining etch stop material 724 may be or be include etch stop layer 210.



FIG. 8A and FIG. 8B are collectively a flow chart of another process 800 for forming a conductor pattern using dry etching and an etch-stop layer. The process 800 is or is included in the forming of conductor patterns at 630 of process 600. Process 800 is a subtractive or etching process that provides good control of conductor sidewall angles for the conductor pattern (e.g., of the IDT and/or fingers herein).


The process 800 starts at 825 with a plate of piezoelectric material 812 and ends at 850 with a completed XBAR conductor pattern 846 formed on the piezoelectric material plate 812. Piezoelectric plate 812 at 825 may be any of plates 110 and/or 410. The completed XBAR conductor pattern 846 on the plate at 850 may be a conductor pattern that is or that includes the IDT patterns and/or fingers described herein for XBAR devices.


The flow chart of FIG. 8 includes only major process steps. Various conventional process steps (e.g. surface preparation, chemical mechanical processing (CMP), cleaning, inspection, baking, annealing, monitoring, testing, etc.) may be performed before, between, after, and during the steps shown in FIG. 8.


At 825 an etch stop material 824 is deposited over the over the piezoelectric plate 812. The etch stop material 824 may be blanket deposited over all of the exposed top surfaces of the plate to form an etch-stop layer. The etch stop material 824 may be a material and/or be deposited as described for etch-stop layer 210.


At 835 IDT conductor material 836 is deposited over the etch stop material 824. The IDT conductor material 836 may be blanket deposited over all of the exposed top surfaces of the etch-stop layer. Depositing at 835 may be depositing one or more metal layers in sequence over the top surfaces of the etch stop material 824.


At 840 a patterned photoresist mask 842 is formed over the IDT conductor material 836. The photoresist mask 842 may be a patterned lithography mask that is formed over areas of the IDT conductor material 836 where the IDT conductor material 846 is desired. These may be areas or locations where the conductor pattern of the IDT or fingers are to be formed. The photoresist mask 842 may be blanket deposited over the IDT conductor material 836 and then patterned to define the conductor pattern 846 where the photoresist mask 842 exists after patterning.


The patterned photoresist mask 842 may function like an etch stop in that it will be impervious to and/or be etch magnitudes slower than the conductor material by the processes and chemicals used to etch the conductor material 836. Suitable photoresist materials may include oxides such as a light sensitive material, a light-sensitive organic material (e.g., a photopolymeric, photodecomposing, or photocrosslinking photoresist), an oxide or a nitride.


At 845 IDT conductor material 836 is dry etched and removed by an anisotropic etch through the conductor where it is not protected by the photoresist mask 842, thus forming conductor pattern 846. The conductor layer 836 can be etched, for example, by an anisotropic plasma etching, reactive ion etching, wet chemical etching, and other etching techniques. The etch may be a highly anisotropic, high-energy etch process that can damage (via chemical etch or physical sputtering) the piezoelectric layer where that layer is exposed to the etch.


The dry etch etches or removes the conductor over and to the etch stop material 824. Both, the photoresist mask 842 and the etch stop material 824 are impervious, as previously defined, to the processes and chemicals used to etch the conductors. Alternatively, they are etched magnitudes slower than the conductor material by the processes and chemicals used to etch the conductors. Thus, this anisotropic etch does not remove the conductor material 836 under the second photoresist mask 842 and does not remove the etch stop material 824 since they are impervious and/or etched magnitudes slower. The conductor material 836 remaining under the second photoresist mask 842 and on the etch stop material 824 is the conductor pattern desired for the IDT and/or fingers.


At 850 the photoresist mask 842 is removed from the top surface of the conductor material 836. This leaves the pattern of desired conductor material 846 deposited directly onto the etch stop material 824 between and under the conductor material 846. The photoresist mask 842 is removed using a process that does not expose the surface of the conductor material 846 to reactive chemicals or a process that will damage or etch the conductor material 846.


After removing at 850, the remaining desired conductor material 846 may be or include the IDT conductor and/or fingers described herein. It may be the conductor material in the XBAR device 300, such as the IDT fingers 336 and 338. The remaining etch stop material 824 may be or be include etch stop layer 310.


Using the subtractive or etching of each of processes 700 and 800 provides better control of conductor sidewall angles of the desired conductor material than a lift-off process. In some cases, processes 700 and 800 provide a predefined deposit-etched IDT with sharp sidewall angles by using a highly anisotropic, high-energy etch process that may damage (via chemical etch or physical sputtering) the piezoelectric layer, and by protecting the piezoelectric layer with a thin layer of insulating etch stop metal oxide layer that is deposited over it. By using the highly anisotropic, high-energy etch process and etch stop layer the processes 700 and 800 allow for better resolution of the IDTs as well as sharper vertical wall angle of the IDTs.


Closing Comments


Throughout this description, the embodiments and examples shown should be considered as exemplars, rather than limitations on the apparatus and procedures disclosed or claimed. Although many of the examples presented herein involve specific combinations of method acts or system elements, it should be understood that those acts and those elements may be combined in other ways to accomplish the same objectives. With regard to flowcharts, additional and fewer steps may be taken, and the steps as shown may be combined or further refined to achieve the methods described herein. Acts, elements and features discussed only in connection with one embodiment are not intended to be excluded from a similar role in other embodiments.


As used herein, “plurality” means two or more. As used herein, a “set” of items may include one or more of such items. As used herein, whether in the written description or the claims, the terms “comprising”, “including”, “carrying”, “having”, “containing”, “involving”, and the like are to be understood to be open-ended, i.e., to mean including but not limited to. Only the transitional phrases “consisting of” and “consisting essentially of”, respectively, are closed or semi-closed transitional phrases with respect to claims. Use of ordinal terms such as “first”, “second”, “third”, etc., in the claims to modify a claim element does not by itself connote any priority, precedence, or order of one claim element over another or the temporal order in which acts of a method are performed, but are used merely as labels to distinguish one claim element having a certain name from another element having a same name (but for use of the ordinal term) to distinguish the claim elements. As used herein, “and/or” means that the listed items are alternatives, but the alternatives also include any combination of the listed items.

Claims
  • 1. An acoustic resonator device comprising: a substrate having a front surface;a piezoelectric plate supported by the front surface of the substrate;interleaved fingers at a diaphragm of the piezoelectric plate spanning a cavity; andan etch-stop layer on a surface of the piezoelectric plate between the interleaved fingers,wherein the etch-stop layer is impervious to an etch process capable of forming the interleaved fingers.
  • 2. The acoustic resonator device of claim 1, wherein the etch-stop layer is on the piezoelectric plate between but not under the interleaved fingers.
  • 3. The acoustic resonator device of claim 1, wherein the etch-stop layer is on the piezoelectric plate between and under the interleaved fingers.
  • 4. The acoustic resonator device of claim 1, wherein the piezoelectric plate is one of lithium niobate and lithium tantalate; and wherein the etch-stop layer is one of an oxide, sapphire, a nitride, silicon carbide, and diamond.
  • 5. The acoustic resonator device of claim 4, wherein the etch-stop layer is aluminum oxide.
  • 6. The acoustic resonator device of claim 4, wherein the etch-stop layer is a high thermal conductivity material selected from aluminum nitride, boron nitride, and the diamond.
  • 7. The acoustic resonator device of claim 1, further comprising: a front-side dielectric layer on the etch stop layer and on the interleaved fingers, wherein the diaphragm includes the piezoelectric plate, the front-side dielectric layer, and the etch-stop layer.
  • 8. The acoustic resonator device of claim 7, wherein the front-side dielectric layer is SiO2, Si3N4, or Al2O3.
  • 9. The acoustic resonator device of claim 7, further comprising: a passivation layer over the front-side dielectric layer.
  • 10. The acoustic resonator device of claim 1, wherein the interleaved fingers and piezoelectric plate are configured such that a radio frequency signal applied to the interleaved fingers excites a shear primary acoustic mode within the piezoelectric plate, and wherein a direction of acoustic energy flow of the shear primary acoustic mode is substantially orthogonal to the front and back surfaces of the piezoelectric plate.
  • 11. The acoustic resonator device of claim 1, wherein the piezoelectric plate is supported by the front surface of the substrate via one or more intermediate material layers.
  • 12. A filter device, comprising: a substrate having a front surface;at least one piezoelectric plate supported by the front surface of the substrate;a plurality of interdigital transducers (IDTs) of a respective plurality of acoustic resonators including a shunt resonator and a series resonator, interleaved fingers of each of the plurality of IDTs at a respective diaphragm of one or more diaphragms of the at least one piezoelectric plate spanning respective cavities; andan etch-stop layer on a surface of the at least one piezoelectric plate between interleaved fingers of the plurality of IDTs,wherein the etch-stop layer is impervious to an etch process capable of forming the interleaved fingers.
  • 13. The filter device of claim 12, further comprising: a frequency setting dielectric layer on a front surface of the etch-stop layer between the interleaved fingers of the IDT of the shunt resonator.
  • 14. The filter device of claim 13, wherein: the frequency setting dielectric layer is a first dielectric layer that has a first thickness that is greater than a second thickness of a second dielectric layer deposited between the fingers of the IDT of the series resonator,a resonance frequency of the shunt resonator is set, at least in part, by the first thickness, anda resonance frequency of the series resonator is set, at least in part, by the second thickness.
  • 15. The filter device of claim 12, wherein the etch-stop layer is on the at least one piezoelectric plate between and under the interleaved fingers.
  • 16. The filter device of claim 12, wherein the etch-stop layer is on the at least one piezoelectric plate between but not under the interleaved fingers.
  • 17. A filter device, comprising: a substrate having a front surface;at least one piezoelectric plate supported by the front surface of the substrate;a plurality of interdigital transducers (IDTs) of a respective plurality of acoustic resonators including at least one shunt resonator and at least series resonator, interleaved fingers of each of the plurality of IDTs disposed on a respective diaphragm of one or more diaphragms spanning respective cavities; andan etch-stop layer on the at least one piezoelectric plate and between interleaved fingers of the plurality of IDTs,wherein the etch-stop layer is a material configured to be impervious to at least one etch process capable of etching the interleaved fingers.
  • 18. The filter device of claim 17, wherein the etch-stop layer is on the at least one piezoelectric plate between but not under the interleaved fingers.
  • 19. The filter device of claim 17, wherein the etch-stop layer is on formed on the front surface of the at least one piezoelectric plate between and under the interleaved fingers.
  • 20. The filter device of claim 17, wherein the at least one etch process is a highly anisotropic, high-energy chemical etch process or physical sputtering etch process.
RELATED APPLICATION INFORMATION

This patent is a continuation of U.S. patent application Ser. No. 17/093,371, filed Nov. 9, 2020, entitled TRANSVERSELY-EXCITED FILM BULK ACOUSTIC RESONATOR WITH ETCHED CONDUCTOR PATTERNS, which claims priority to U.S. provisional patent application No. 63/019,749, titled ETCH STOP LAYER TO ENABLE DEP-ETCH OF IDTS, filed May 4, 2020, which are incorporated herein by reference.

US Referenced Citations (219)
Number Name Date Kind
5204575 Kanda et al. Apr 1993 A
5274345 Gau Dec 1993 A
5446330 Eda et al. Aug 1995 A
5552655 Stokes et al. Sep 1996 A
5726610 Allen et al. Mar 1998 A
5729186 Seki et al. Mar 1998 A
5853601 Krishaswamy Dec 1998 A
6172582 Hickernell Jan 2001 B1
6271617 Yoneda et al. Aug 2001 B1
6377140 Ehara et al. Apr 2002 B1
6516503 Ikada et al. Feb 2003 B1
6540827 Levy et al. Apr 2003 B1
6570470 Maehara et al. May 2003 B2
6707229 Martin Mar 2004 B1
6710514 Ikada et al. Mar 2004 B2
6833774 Abbott et al. Dec 2004 B2
7009468 Kadota et al. Mar 2006 B2
7042132 Bauer et al. May 2006 B2
7345400 Nakao et al. Mar 2008 B2
7463118 Jacobsen Dec 2008 B2
7535152 Ogami et al. May 2009 B2
7684109 Godshalk et al. Mar 2010 B2
7728483 Tanaka Jun 2010 B2
7868519 Umeda Jan 2011 B2
7941103 Iwamoto et al. May 2011 B2
7965015 Tai et al. Jun 2011 B2
8278802 Lee et al. Oct 2012 B1
8294330 Abbott et al. Oct 2012 B1
8344815 Yamanaka et al. Jan 2013 B2
8816567 Zuo et al. Aug 2014 B2
8829766 Milyutin et al. Sep 2014 B2
8932686 Hayakawa et al. Jan 2015 B2
9093979 Wang Jul 2015 B2
9112134 Takahashi Aug 2015 B2
9130145 Martin et al. Sep 2015 B2
9148121 Inoue Sep 2015 B2
9219466 Meltaus et al. Dec 2015 B2
9240768 Nishihara et al. Jan 2016 B2
9276557 Nordquist et al. Mar 2016 B1
9369105 Li et al. Jun 2016 B1
9425765 Rinaldi Aug 2016 B2
9525398 Olsson Dec 2016 B1
9640750 Nakanishi et al. May 2017 B2
9748923 Kando et al. Aug 2017 B2
9762202 Thalmayr et al. Sep 2017 B2
9780759 Kimura et al. Oct 2017 B2
9837984 Khlat et al. Dec 2017 B2
10079414 Guyette et al. Sep 2018 B2
10187039 Komatsu et al. Jan 2019 B2
10200013 Bower et al. Feb 2019 B2
10211806 Bhattacharjee Feb 2019 B2
10284176 Solal May 2019 B1
10389391 Ito et al. Aug 2019 B2
10491192 Plesski et al. Nov 2019 B1
10601392 Plesski et al. Mar 2020 B2
10637438 Garcia et al. Apr 2020 B2
10644674 Takamine May 2020 B2
10756697 Plesski et al. Aug 2020 B2
10790802 Yantchev et al. Sep 2020 B2
10797675 Plesski Oct 2020 B2
10812048 Nosaka Oct 2020 B2
10819309 Turner et al. Oct 2020 B1
10826462 Plesski et al. Nov 2020 B2
10868510 Yantchev et al. Dec 2020 B2
10868512 Garcia et al. Dec 2020 B2
10868513 Yantchev Dec 2020 B2
10911017 Plesski Feb 2021 B2
10911021 Turner et al. Feb 2021 B2
10911023 Turner Feb 2021 B2
10917070 Plesski et al. Feb 2021 B2
10917072 McHugh et al. Feb 2021 B2
10985726 Plesski Apr 2021 B2
10985728 Plesski et al. Apr 2021 B2
10985730 Garcia Apr 2021 B2
10992282 Plesski et al. Apr 2021 B1
10992283 Plesski et al. Apr 2021 B2
10992284 Yantchev Apr 2021 B2
10998877 Turner et al. May 2021 B2
10998882 Yantchev et al. May 2021 B2
11003971 Plesski et al. May 2021 B2
11114996 Plesski et al. Sep 2021 B2
11114998 Garcia et al. Sep 2021 B2
11139794 Plesski et al. Oct 2021 B2
11143561 Plesski Oct 2021 B2
11146231 Plesski Oct 2021 B2
11146232 Yandrapalli et al. Oct 2021 B2
11146238 Hammond et al. Oct 2021 B2
11146244 Yantchev Oct 2021 B2
11165407 Yantchev Nov 2021 B2
11171629 Turner Nov 2021 B2
11201601 Yantchev et al. Dec 2021 B2
11283424 Turner Mar 2022 B2
11418167 Garcia Aug 2022 B2
20020079986 Ruby et al. Jun 2002 A1
20020130736 Mukai Sep 2002 A1
20020158714 Kaitila et al. Oct 2002 A1
20020189062 Lin et al. Dec 2002 A1
20030042998 Edmonson Mar 2003 A1
20030080831 Naumenko et al. May 2003 A1
20030199105 Kub et al. Oct 2003 A1
20040041496 Imai et al. Mar 2004 A1
20040100164 Murata May 2004 A1
20040261250 Kadota et al. Dec 2004 A1
20050077982 Funasaka Apr 2005 A1
20050099091 Mishima et al. May 2005 A1
20050185026 Noguchi et al. Aug 2005 A1
20050218488 Matsuo Oct 2005 A1
20050264136 Tsutsumi et al. Dec 2005 A1
20060152107 Tanaka Jul 2006 A1
20060179642 Kawamura Aug 2006 A1
20070182510 Park Aug 2007 A1
20070188047 Tanaka Aug 2007 A1
20070194863 Shibata et al. Aug 2007 A1
20070267942 Matsumoto et al. Nov 2007 A1
20080246559 Ayazi Oct 2008 A1
20080297280 Thalhammer et al. Dec 2008 A1
20090315640 Umeda et al. Dec 2009 A1
20100019866 Hara et al. Jan 2010 A1
20100064492 Tanaka Mar 2010 A1
20100123367 Tai et al. May 2010 A1
20100212127 Heinze et al. Aug 2010 A1
20100301703 Chen et al. Dec 2010 A1
20110018389 Fukano et al. Jan 2011 A1
20110018654 Bradley et al. Jan 2011 A1
20110102107 Onzuka May 2011 A1
20110109196 Goto et al. May 2011 A1
20110278993 Iwamoto Nov 2011 A1
20120073390 Zaghloul et al. Mar 2012 A1
20120198672 Ueda et al. Aug 2012 A1
20120286900 Kadota et al. Nov 2012 A1
20120326809 Tsuda Dec 2012 A1
20130057360 Meltaus et al. Mar 2013 A1
20130127551 Yamanaka May 2013 A1
20130234805 Takahashi Sep 2013 A1
20130271238 Onda Oct 2013 A1
20130278609 Stephanou et al. Oct 2013 A1
20130321100 Wang Dec 2013 A1
20140009032 Takahashi et al. Jan 2014 A1
20140009247 Moriya Jan 2014 A1
20140113571 Fujiwara et al. Apr 2014 A1
20140130319 Iwamoto May 2014 A1
20140145556 Kadota May 2014 A1
20140151151 Reinhardt Jun 2014 A1
20140152145 Kando et al. Jun 2014 A1
20140173862 Kando et al. Jun 2014 A1
20140225684 Kando et al. Aug 2014 A1
20150014795 Franosch et al. Jan 2015 A1
20150042417 Onodera et al. Feb 2015 A1
20150165479 Lasiter et al. Jun 2015 A1
20150319537 Perois et al. Nov 2015 A1
20150333730 Meltaus et al. Nov 2015 A1
20150365067 Hori et al. Dec 2015 A1
20160028367 Shealy Jan 2016 A1
20160036415 Ikeuchi Feb 2016 A1
20160087187 Burak Mar 2016 A1
20160149554 Nakagawa May 2016 A1
20160182009 Bhattacharjee Jun 2016 A1
20170063332 Gilbert et al. Mar 2017 A1
20170104470 Koelle et al. Apr 2017 A1
20170179225 Kishimoto Jun 2017 A1
20170179928 Raihn et al. Jun 2017 A1
20170187352 Omura Jun 2017 A1
20170214381 Bhattacharjee Jul 2017 A1
20170214387 Burak et al. Jul 2017 A1
20170222617 Mizoguchi Aug 2017 A1
20170222622 Solal et al. Aug 2017 A1
20170264266 Kishimoto Sep 2017 A1
20170290160 Takano et al. Oct 2017 A1
20170359050 Irieda et al. Dec 2017 A1
20170370791 Nakamura et al. Dec 2017 A1
20180005950 Watanabe Jan 2018 A1
20180013405 Takata Jan 2018 A1
20180026603 Iwamoto Jan 2018 A1
20180033952 Yamamoto Feb 2018 A1
20180041191 Park Feb 2018 A1
20180062615 Kato et al. Mar 2018 A1
20180062617 Yun et al. Mar 2018 A1
20180123016 Gong May 2018 A1
20180152169 Goto et al. May 2018 A1
20180191322 Chang et al. Jul 2018 A1
20180278227 Hurwitz Sep 2018 A1
20180316333 Nakamura et al. Nov 2018 A1
20190007022 Goto et al. Jan 2019 A1
20190068155 Kimura et al. Feb 2019 A1
20190068164 Houlden et al. Feb 2019 A1
20190123721 Takamine Apr 2019 A1
20190131953 Gong May 2019 A1
20190181825 Schmalzl et al. Jun 2019 A1
20190181833 Nosaka Jun 2019 A1
20190207583 Miura et al. Jul 2019 A1
20190245518 Ito Aug 2019 A1
20190273480 Lin et al. Sep 2019 A1
20190348966 Campanella-Pineda Nov 2019 A1
20190379351 Miyamoto et al. Dec 2019 A1
20190386635 Plesski et al. Dec 2019 A1
20190386636 Plesski et al. Dec 2019 A1
20200007110 Konaka et al. Jan 2020 A1
20200021272 Segovia Fernandez et al. Jan 2020 A1
20200036357 Mimura Jan 2020 A1
20200235719 Yantchev et al. Jul 2020 A1
20200244247 Maeda Jul 2020 A1
20200259480 Pensala Aug 2020 A1
20200304091 Yantchev Sep 2020 A1
20200313645 Caron Oct 2020 A1
20200321939 Turner et al. Oct 2020 A1
20200328728 Nakagawa et al. Oct 2020 A1
20200350891 Turner Nov 2020 A1
20210013859 Turner et al. Jan 2021 A1
20210265978 Plesski et al. Aug 2021 A1
20210273631 Jachowski et al. Sep 2021 A1
20210313951 Yandrapalli et al. Oct 2021 A1
20210328574 Garcia Oct 2021 A1
20210351762 Dyer et al. Nov 2021 A1
20220103160 Jachowski et al. Mar 2022 A1
20220116015 Garcia et al. Apr 2022 A1
20220123720 Garcia et al. Apr 2022 A1
20220123723 Garcia et al. Apr 2022 A1
20220149808 Dyer et al. May 2022 A1
20220149814 Garcia et al. May 2022 A1
Foreign Referenced Citations (37)
Number Date Country
106788318 May 2017 CN
110417373 Nov 2019 CN
210431367 Apr 2020 CN
113765495 Dec 2021 CN
H10209804 Aug 1998 JP
2001244785 Sep 2001 JP
2002300003 Oct 2002 JP
2003078389 Mar 2003 JP
2004096677 Mar 2004 JP
2004129222 Apr 2004 JP
2004304622 Oct 2004 JP
2006173557 Jun 2006 JP
2007251910 Sep 2007 JP
2010062816 Mar 2010 JP
2010103803 May 2010 JP
2010233210 Oct 2010 JP
2013528996 Jul 2013 JP
2013214954 Oct 2013 JP
2015054986 Mar 2015 JP
2016001923 Jan 2016 JP
2017526254 Sep 2017 JP
2017220910 Dec 2017 JP
2018093487 Jun 2018 JP
2018166259 Oct 2018 JP
2018207144 Dec 2018 JP
2019186655 Oct 2019 JP
2020113939 Jul 2020 JP
2010047114 Apr 2010 WO
2013021948 Feb 2013 WO
2015098694 Jul 2015 WO
2016017104 Feb 2016 WO
2016052129 Apr 2016 WO
2016147687 Sep 2016 WO
2018003273 Jan 2018 WO
2018163860 Sep 2018 WO
2019138810 Jul 2019 WO
2020092414 May 2020 WO
Non-Patent Literature Citations (41)
Entry
A. C. Guyette, “Theory and Design of Intrinsically Switched Multiplexers With Optimum Phase Linearity,” in IEEE Transactions on Microwave Theory and Techniques, vol. 61, No. 9, pp. 3254-3264, Sep. 2013, doi: 10.1109/TMTT.2013.2274963. Sep. 2013.
Acoustic Properties of Solids ONDA Corporation 592 Weddell Drive, Sunnyvale, CA 94089, Apr. 11, 2003, pp. 5 (Year 2003). 2003.
Bahreyni, B. Fabrication and Design of Resonant Microdevices Andrew William, Inc. 2018, NY (Year 2008). 2008.
Buchanan “Ceramic Materials for Electronics” 3rd Edition, first published in 2004 by Marcel Dekker, Inc. pp. 496 (Year 2004). 00 Jan. 2004.
Ekeom, D. & Dubus, Bertrand & Volatier, A . . . (2006). Solidly mounted resonator (SMR) FEM-BEM simulation. 1474-1477. 10.1109/ULTSYM.2006.371.
G. Manohar, “Investigation of Various Surface Acoustic Wave Design Configurations for Improved Sensitivity.” Doctoral dissertation, University of South Florida, USA, Jan. 2012, 7 pages.
Kadota et al. “5.4 Ghz Lamb Wave Resonator on LiNbO3 Thin Crystal Plate and Its Application,” published in Japanese Journal of Applied Physics 50 (2011) 07HD11. (Year: 2011) 2011.
M. Kadota et al.; “Ultrawide Band Ladder Filter using SHO plate Wave in Thin LiNb03 Plate and its Application”; 2014 IEEE International Ultrasonics Symposium Proceedings, 2014, pp. 2031-2034. (Year: 2014).
M. Kadota, S. Tanaka, “Wideband acoustic wave resonators composed of hetero acoustic layer structure,” Japanese Journal of Applied Physics, vol. 57, No. 7S1. Published Jun. 5, 2018. 5 pages.
M.-H. Li et al.; “Temperature Stability Analysis of Thin-Film Lithium Niobate SH0 Plate Wave Resonators”; Journal of Microelectromechanical Systems, vol. 28, No. 5, Oct. 2019, pp. 799-809. (Year: 2019).
Material Properties of Tibtech Innovations, © 2018 TIBTECH Innovations (Year 2018). 2018.
Merriam Webster, dictionary meaning of the word “diaphragm”, since 1828, Merriam Webster (Year: 1828) 1828.
Mizutaui, K. and Toda, K., “Analysis of lamb wave propagation characteristics in rotated Ycut Xpropagation LiNbO3 plates.” Electron. Comm. Jpn. Pt. I, 69, No. 4 (1986): 47-55. doi:10.1002/ecja.4410690406.
Moussa et al. Review on Triggered Liposomal Drug Delivery with a Focus on Ultrasound 2015, Bentham Science Publishers, pp. 16 (Year 2005) 2005.
Namdeo et al. “Simulation on Effects of Electrical Loading due to Interdigital Transducers in Surface Acoustic Wave Resonator”, published in Procedia Engineering 64 ( 2013) of Science Direct pp. 322-330 (Year: 2013) 2013.
Naumenko et al., “Optimal orientations of Lithium Niobate for resonator SAW filters”, 2003 IEEE Ultrasonics Symposium—pp. 2110-2113. (Year: 2003).
R. Olsson III, K. Hattar et al. “A high electromechanical coupling coefficient SH0 Lamb wave lithiumniobate micromechanical resonator and a method for fabrication” Sensors and Actuators A: Physical, vol. 209, Mar. 1, 2014, pp. 183-190.
Rodriguez-Madrid et al., “Super-High-Frequency SAW Resonators on AIN/Diamond”, IEEE Electron Device Letters, vol. 33, No. 4, Apr. 2012, pp. 495-497. Year: 2012) 2012.
Safari et al. “Piezoelectric for Transducer Applications” published by Elsevier Science Ltd., pp. 4 (Year: 2000). 2020.
Santosh, G. , Surface acoustic wave devices on silicon using patterned and thin film ZnO, Ph.D. thesis, Feb. 2016, Indian Institute of technology Guwahati, Assam, India Feb. 2016.
Sorokin et al.Study of Microwave Acoustic Attenuation in a Multi-frequency Bulk Acoustic Resonator Based on a Synthetic Diamond Single CrystalPublished in Acoustical Physics, vol. 61, No. 6, 2015 pp. 675 (Year 2015) 00 Jan. 2015.
T. Takai, H. Iwamoto, et al., “I.H.P.Saw Technology and its Application to Microacoustic Components (Invited).” 2017 IEEE International Ultrasonics Symposium, Sep. 6-9, 2017. pp. 1-8.
USPTO/ISA, International Search Report and Written Opinion for PCT Application No. PCT/US2019/036433 dated Aug. 29, 2019.
USPTO/ISA, International Search Report and Written Opinion for PCT Application No. PCT/US2019/058632 dated Jan. 17, 2020.
USPTO/ISA, International Search Report and Written Opinion for PCT Application No. PCT/US2020/45654 dated Oct. 29, 2020.
USPTO/ISA, International Search Report and Written Opinion for PCT Application No. PCT/US2021/024824 dated Jul. 27, 2021, 9 total pages.
USPTO/ISA, International Search Report and Written Opinion for PCT Application No. PCT/US2021/048505 dated Dec. 1, 2021, 11 total pages.
Y. Yang, A. Gao et al. “5 GHZ Lithium Niobate MEMS Resonators With High FOM of 153”, 2017 IEEE 30th International Conference in Micro Electro Mechanical Systems (MEMS). Jan. 22-26, 2017. pp. 942-945.
Y. Yang, R. Lu et al. “Towards Ka Band Acoustics: Lithium Niobat Asymmetrical Mode Piezoelectric MEMS Resonators”, Department of Electrical and Computer Engineering University of Illinois at Urbana-Champaign, May 2018. pp. 1-2.
Yanson Yang, Ruochen Lu, Songbin Gong, High Q Antisymmetric Mode Lithium Niobate MEMS Resonators With Spurious Mitigation, Journal of Microelectromechanical Systems, vol. 29, No. 2, Apr. 2020. Apr. 2, 2020.
Yu-Po Wong, Luyan Qiu, Naoto Matsuoka, Ken-ya Hashimoto, Broadband Piston Mode Operation for First-order Antisymmetric Mode Resonators, 2020 IEEE International Ultrasonics Symposium, Sep. 2020. Sep. 2020.
Zou, Jie “High-Performance Aluminum Nitride Lamb Wave Resonators for RF Front-End Technology” University of California, Berkeley, Summer 2015, pp. 63 (Year 2015) 00 Jan. 2015.
Chen et al., “Development and Application of SAW Filter,” Micromachines, Apr. 20, 2022, vol. 13, No. 656, pp. 1-15.
Hermann et al., “Properties of shear-horizontal surface acoustic waves in different layered quartz-SiO2 structures,” Ultrasonics, 1999, vol. 37, pp. 335-341.
International Search Report and Written Opinion in PCT/US2022/081068, mailed Apr. 18, 2023, 17 pages.
Lam et al., “A Review of Lame and Lamb Mode Crystal Resonators for Timing Applications and Prospects of Lame and Lamb Mode Piezo MEMS Resonators for Filtering Applications,” 2018 International Symposium on Acoustic Wave Devices for Future Mobile Communication Systems, Mar. 6-7, 2018, 12 pages.
Kadota et al., “Ultra Wideband Ladder Filter Using SHO Plate Wave in Thin LiNbO3 Plate and Its Application to Tunable Filter,” IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control, 2015, vol. 62, No. 5, pp. 939-946.
Gorisse et al., “Lateral Field Excitation of membrane-based Aluminum Nitride resonators”, 2011 Joint Conference of the IEEE International Frequency Control and the European Frequency and Time Forum (FCS) Proceedings, 5 pages.
Pang et al. “Self-Aligned Lateral Field Excitation Film Acoustic Resonator with Very Large Electromechanical Coupling”, 2004 IEEE International Ultrasonics, Ferroelectrics and Frequency Control Joint 50th Anniversary Conference, pp. 558-561.
Xue et al. “High Q Lateral-Field-Excited Bulk Resonator Based on Single-Crystal LiTaO3 for 5G Wireless Communication”, Journal of Electron devices society, vol. 9, Mar. 26, 2021, pp. 353-358.
Yandrapalli et al., “Toward Band n78 Shear Bulk Acoustic Resonators Using Crystalline Y-Cut Lithium Niobate Films with Spurious Suppression”, Journal of Microelectromechanical Systems, vol. 32, No. 4, Aug. 2023, pp. 327-334.
Related Publications (1)
Number Date Country
20220182038 A1 Jun 2022 US
Provisional Applications (1)
Number Date Country
63019749 May 2020 US
Continuations (1)
Number Date Country
Parent 17093371 Nov 2020 US
Child 17674769 US