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.
This disclosure relates to radio frequency filters using acoustic wave resonators, and specifically to filters for use in communications equipment.
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 pass-band 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.
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.
Description of Apparatus
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 surfaces. 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 substrate 120 that provides mechanical support to the piezoelectric plate 110. The substrate 120 may be, for example, silicon, sapphire, quartz, or some other material. The piezoelectric plate 110 may be bonded to the substrate 120 using a wafer bonding process, or grown on the substrate 120, or attached to the substrate in some other manner. The piezoelectric plate may be attached directly to the substrate, or may be attached to the substrate via one or more intermediate material layers.
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 an acoustic wave within the piezoelectric plate 110. As will be discussed in further detail, the excited acoustic wave is a bulk shear wave that propagates in the direction normal 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.
A cavity 140 is formed in the substrate 120 such that a portion 115 of the piezoelectric plate 110 containing the IDT 130 is suspended over the cavity 140 without contacting the substrate 120. “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 (as shown subsequently in
The portion 115 of the piezoelectric plate suspended over the cavity 140 will be referred to herein as the “diaphragm” (for lack of a better term) due to its physical resemblance to the diaphragm of a microphone. The diaphragm may be continuously and seamlessly connected to the rest of the piezoelectric plate 110 around all, or nearly all, of perimeter of the cavity 140.
For ease of presentation in
A front-side dielectric layer 214 may optionally be formed on the front side of the piezoelectric plate 110. The “front side” of the XBAR is, by definition, the surface facing away from the substrate. The front-side dielectric layer 214 has a thickness tfd. The front-side dielectric layer 214 is formed between the IDT fingers 238. Although not shown in
The IDT fingers 238 may be aluminum or a substantially aluminum alloy, copper or a substantially copper alloy, beryllium, gold, or some other conductive material. Thin (relative to the total thickness of the conductors) layers of other metals, such as chromium or titanium, may be formed under and/or over the fingers to improve adhesion between the fingers and the piezoelectric plate 110 and/or to passivate or encapsulate the fingers. The busbars (132, 134 in
Dimension p is the center-to-center spacing or “pitch” of the IDT fingers, which may be referred to as the pitch of the IDT and/or the pitch of the XBAR. Dimension w is the width or “mark” of the IDT fingers. The IDT of an XBAR differs substantially from the IDTs used in surface acoustic wave (SAW) resonators. In a SAW resonator, the pitch of the IDT is one-half of the acoustic wavelength at the resonance frequency. Additionally, the mark-to-pitch ratio of a SAW resonator IDT is typically close to 0.5 (i.e. the mark or finger width is about one-fourth of the acoustic wavelength at resonance). In an XBAR, the pitch p of the IDT is typically 2 to 20 times the width w of the fingers. In addition, the pitch p of the IDT is typically 2 to 20 times the thickness is of the piezoelectric slab 212. The width of the IDT fingers in an XBAR is not constrained to one-fourth of the acoustic wavelength at resonance. For example, the width of XBAR IDT fingers may be 500 nm or greater, such that the IDT can be fabricated using optical lithography. 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
The XBAR 300 shown in
The XBARs of
Referring to
The interposer 450 also includes a base 452 and conductive vias 454 to provide electrical connections between the conductor patters on the piezoelectric plate 410 and circuitry external to the filter (not shown). The term “interposer” is generally used to describe a passive circuit device that provides electrical connections between two different interfaces. The interposer 450 fulfills this function but also forms a structural part of the package of the packaged XBAR filter 400A. The interposer may be, for example, a printed circuit board (PCB), a low temperature cofired ceramic (LTCC) circuit card, a silicon wafer, or some other structure that provides mechanical protection to the diaphragms of the XBARs.
In
As shown in
Referring back to
In addition, the package XBAR filter 400B includes a cap 480 attached to the substrate 420 by a cap seal 485. The cap 480 may be any material suitable to cover the openings where the cavities 440 intersect the surface of the substrate 420. For example, the cap 480 may be silicon, glass, quartz, or a polymer plate or film. The cap seal 485 may be any of the materials and sealing methods previously described with respect to the seal 460.
The XBAR filter chip 605 includes a piezoelectric plate 610 attached to a substrate 620. The substrate 620 may be high resistivity silicon or some other material. Portions of the piezoelectric plate 610 form diaphragms spanning respective cavities 640 in the substrate 620. Commonly, one or more intermediate layers, which are shown in
A second conductor pattern is formed on the surface of the piezoelectric plate 610. The second conductor pattern, which may overlay portions of the first conductor pattern, may be gold, aluminum, copper or some other metal. The second conductor pattern includes a continuous metal ring 662 around the perimeter of the XBAR filter chip 605. The second conductor pattern also includes pads, such as pad 672, in locations where portions of the first conductor pattern must be connected to circuitry external to the packaged XBAR filter.
The interposer 650 includes a base 652, which may be high resistivity silicon or some other material. The base 652 may have recesses 655 so that the surfaces of the base 652 facing the diaphragms (i.e. the bottoms of the recesses 655) are sufficiently far from the diaphragms. A third conductor pattern is formed on the surface of the base 652 facing the XBAR filter chip 605. The third conductor pattern may be the same material as the second conductor pattern. The third conductor pattern includes a continuous metal ring 664 around the perimeter of the base 652. The third conductor pattern also includes pads, such as pad 674, in locations where portions of the first conductor pattern must be connected to circuitry external to the packaged XBAR filter. The arrangement of ring 664 and pads 674 of third conductor pattern is typically a mirror image of the arrangement of the ring 662 and pads 672 of the second conductor pattern.
The interposer 650 also includes vias such as via 676. When the base is silicon, such vias are commonly referred to as “through silicon vias” (TSVs). Vias consist of a metal-coated or metal-filled hole through the base 652. Each via provides an electrical connection between one of the pads, such as pad 674, of the third conductor pattern and a corresponding pad on the external surface (i.e. the lower surface as shown in the figure) of the base 652. While
As shown in
A cap 780 is sealed to the substrate 720 by a cap seal 785. When the substrate 720 of the XBAR filter chip 705 and the base 752 of the interposer 750 are both silicon, the cap 780 may also be silicon to maintain consistency of thermal expansion coefficients. In other cases, the cap 780 may be silicon, borosilicate or other glass, plastic, or some other material. The cap 780 may be attached to the substrate 720 using any of the previously described sealing methods and materials. Typically, the cap 780 will be attached to the substrate 720 immediately after forming the cavities 740 in the substrate. The cap 780 may be attached to the substrate 720 before bonding the XBAR filter chip 705 to the interposer 750.
In the packaged XBAR filter 700B, a perimeter seal between the piezoelectric plate 710 and the base 752 is not made by bonding conductor rings (i.e. conductor rings 762, 772 in
The XBAR filter chips 605 and 705 shown in
The LTCC interposer 850 comprises layers of thin ceramic tape, some or all of which bear printed conductors, that are assembled and then fired to form a rigid multilayer circuit board. In the example of
The LTCC interposer 850 may have recesses 855 to ensure sufficient spacing between the diaphragms and the surfaces of the interposer facing the diaphragms. Such recess may be formed, for example, by punching openings in one or more of the ceramic layers prior to cofiring the layers of the interposer.
The XBAR filter chip 805 is flip-chip mounted to the interposer 850. Flip-chip mounting establishes physical and electric connections between the XBAR filter chip 805 and the interposer 850. As shown in
Since flip-chip mounting does not establish a seal between the XBAR filter chip 805 and the interposer 850, a polymer cover 860 is molded over the assembly to provide a near-hermetic seal.
A cap 980 is sealed to the substrate 920. Since the cap 980 is eventually enclosed by the molded cover 970, the cap's primary function is to prevent intrusion of materials, including the molding compound used for the cover 970, into the cavities 940. This function may be satisfied by a very thin cap, such as a plastic film.
As in previous examples, the XBAR filter chip 1005 includes a piezoelectric plate 1010 attached to a substrate 1020. The substrate 1020 may be high resistivity silicon or some other material. Portions of the piezoelectric plate 1010 form diaphragms spanning respective cavities 1040 in the substrate 1020. Commonly, one or more intermediate layers, which are shown in
The interposer 1050 includes at least three layers sequentially formed on the piezoelectric plate 1010. Walls 1052 surround the diaphragms of the XBAR devices. The thickness of the walls 1052 defines the distance between the diaphragms and a cover layer 1054 that spans the walls creating an enclosed cavity 1055 over each diaphragm. Both the walls 1052 and the cover layer 1054 may be polymer materials. An interposer conductor pattern 1070 includes pads 1072 on the external surface of the cover layer 1054 for connection to circuitry external to the packaged XBAR filter. The conductor pattern 1070 connects the pads 1072 to connection points 1074 on the XBAR filer chip 1005. The conductor pattern 1070 may be aluminum, copper, gold, or a combination of materials.
Description of Methods
The flow chart of
The piezoelectric plate 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 1100, one or more cavities are formed in the substrate at 1110A, before the piezoelectric plate is bonded to the substrate at 1120. 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. Typically, the cavities formed at 1110A will not penetrate through the substrate, and the resulting resonator devices will have a cross-section as shown in
At 1120, the piezoelectric plate is bonded to the substrate. 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 1130 by depositing and patterning one or more conductor layer on the front side of the piezoelectric plate. The conductor layer may be, for example, aluminum, an aluminum alloy, copper, a copper alloy, or some other conductive metal. Optionally, one or more layers of other materials may be disposed below (i.e. between the conductor layer and the piezoelectric plate) and/or on top of the conductor layer. For example, a thin film of titanium, chrome, or other metal may be used to improve the adhesion between the conductor layer and the piezoelectric plate. A conduction enhancement layer of gold, aluminum, copper or other higher conductivity metal may be formed over portions of the conductor pattern (for example the IDT bus bars and interconnections between the IDTs).
The conductor pattern may be formed at 1130 by depositing the conductor layer and, optionally, one or more other metal layers in sequence over the surface of the piezoelectric plate. The excess metal may then be removed by etching through patterned photoresist. The conductor layer can be etched, for example, by plasma etching, reactive ion etching, wet chemical etching, and other etching techniques.
Alternatively, the conductor pattern may be formed at 1130 using a lift-off process. Photoresist may be deposited over the piezoelectric plate. and patterned to define the conductor pattern. The conductor layer and, optionally, one or more other layers may be deposited in sequence over the surface of the piezoelectric plate. The photoresist may then be removed, which removes the excess material, leaving the conductor pattern.
At 1140, a front-side dielectric layer may be formed by depositing one or more layers of dielectric material on the front side of the piezoelectric plate. 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 a second variation of the process 1100, one or more cavities are formed in the back-side of the substrate at 1110B. 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
In the second variation of the process 1100, a cap, such as the caps 480, 780, 980, 1080, may be attached to the substrate at 1150 to cover and seal the cavities formed at 1110B. The cap may a plate of silicon, glass, or some other material or a plate or film of a polymer material. The cap may be attached to the substrate using any of the previously discussed bonding techniques.
In a third variation of the process 1100, one or more cavities in the form of recesses in the substrate may be formed at 1110C by etching 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. The one or more cavities formed at 1110C will not penetrate through the substrate, and the resulting resonator devices will have a cross-section as shown in
In all variations of the process 1100, the XBAR filter chip is completed at 1160. Actions that may occur at 1160 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; and, if necessary, tuning the resonant frequencies of the resonators within the device by adding or removing metal or dielectric material from the front side of the device. At the conclusion of 1160, the XBAR filter chip is ready to be packaged. The process 1100 then ends at 1195.
The process 1200 starts at 1205 and ends at 1295 with a completed packaged XBAR filter.
Referring to
When the XBAR filter chip 605 has back-side etched cavities (as shown by the dot-dash lines), a cover 680 is sealed to the back side of the substrate 620. While the cover 680 is not shown in subsequent cross-sectional views in
A second conductor pattern is formed on the surface of the piezoelectric plate 610. The second conductor pattern, which may overlay portions of the first conductor pattern, may be gold, aluminum, copper or some other metal. The second conductor pattern includes a continuous metal ring 662 around the perimeter of the XBAR filter chip 605. The second conductor pattern also includes pads, such as pad 672, in locations where portions of the first conductor pattern must be connected to circuitry external to the packaged XBAR filter.
At 1220, a partially-completed interposer is prepared. The partially-completed interposer includes a base 652, which may be high resistivity silicon or some other material. A dielectric layer 654, such as silicon dioxide, is formed on the surface of the base that will face the XBAR filter chip. The base 652 may have recesses 655 so that the surfaces of the base 652 that will face the diaphragms (i.e. the bottoms of the recesses 655) are sufficiently far from the diaphragms. The dielectric layer 654 may or may not cover the recesses 655. A third conductor pattern is formed on top of the dielectric layer 654. The third conductor pattern may be the same material as the second conductor pattern. The third conductor pattern includes a continuous metal ring 664 around the perimeter of the base 652. The third conductor pattern also includes pads, such as pad 674, in locations where portions of the first conductor pattern must be connected to circuitry external to the packaged XBAR filter. The arrangement of ring 664 and pads 674 of third conductor pattern is typically a mirror image of the arrangement of the ring 662 and pads 672 of the second conductor pattern.
At 1230, the XBAR filter chip 605 is bonded to the partially-completed interposer. Specifically, the ring 662 of the second conductor pattern is bonded to the ring 664 of the third conductor pattern, forming a hermetic seal around the perimeter of the XBAR filter chip and partially-completed interposer. Simultaneously, pads, such as pad 672, on the XBAR filter chip are bonded to corresponding pads, such as pad 674, on the partially-completed interposer. A preferred method of bonding the XBAR filter chip to the partially competed interposer is thermocompression bonding, which uses a combination of heat and pressure to make bonds between metallic layers. Other methods, including ultrasonic bonding, and solder or eutectic bonding may be used.
Referring now to
After the optional thinning of one or both of the substrate 620 and the base 652, through silicon via are formed in a sequence of actions from 1250 to 1280.
At 1250, deep reactive ion etching (DRIE) is used to etch holes 1252 from the back side (the lower side as shown in
At 1260, a dielectric layer 1262 is deposited over the back side of the base 652 and the interiors of the holes 1252. The dielectric layer may be silicon dioxide, silicon nitride, aluminum oxide, or some other dielectric material. The dielectric layer may be deposited by a conventional process such as evaporation, sputtering, chemical vapor deposition, or some other process.
Referring now to
At 1280, a fourth conductor pattern 1256 is formed to create electric connections from the pads, such as pad 674 of the third conductor pattern, to corresponding pads, such as pad 676 on the exterior surface (the lower surface as shown in
The entire process 1200 may be, and commonly will be, performed on whole wafers. A whole wafer containing multiple XBARs filter chips will be bonded to another wafer containing a corresponding number of partially-completed interposers at 1230. The subsequent actions form TSVs for all of the interposers simultaneously. Individual packaged XBAR filters may then be excised by dicing the bonded wafers after action 1230.
The process 1300 starts at 1305 and ends at 1395 with a completed packaged XBAR filter.
At 1310, a XBAR filter chip 805 is fabricated using, for example, the process 1100 of
When the XBAR filter chip 805 has back-side etched cavities (as shown by the dot-dash lines), a cover 880 is sealed to the back side of the substrate 820. While the cover 880 is not shown in subsequent cross-sectional views in
A second conductor pattern is formed on the surface of the piezoelectric plate 810. The second conductor pattern, which may overlay portions of the first conductor pattern, may be gold, aluminum, copper or some other metal. The second conductor pattern may include pads (not identified) in locations where portions of the first conductor pattern must be connected to circuitry external to the packaged XBAR filter. Solder balls or bumps 872 may be formed on the pads to allow the XBAR filter chip 805 to be reflow soldered to an interposer. Alternatively, gold bumps may be formed on the pads to allow the XBAR filter chip 805 to be thermocompression bonded or ultrasonic bonded to an interposer.
At 1320, a LTCC interposer 850 is fabricated by cofiring thin ceramic layers, some or all of which bear printed conductors. The LTCC interposer 850 will typically be a portion of a larger panel including multiple interposers, An LTCC interposer has at least an upper (as shown in
The LTCC interposer 850 may have recesses 855 to ensure sufficient spacing between the diaphragms and the surfaces of the interposer facing the diaphragms. Such recess may be formed, for example, by punching openings in one or more of the ceramic layers prior to cofiring the layers of the interposer.
At 1330, the XBAR filter chip 850 is flip-chip bonded to the interposer 850. First the XBAR filter chips within a wafer are tested, and good chips are excised from the wafer. The good chips are then bonded to the LTCC interposer 850 by soldering, thermocompression bonding, ultrasonic bonding, or some other bonding method. The bonding physically attaches the XBAR filter chip 805 to the interposer 850 and makes electrical connections between the XBAR filter chip 805 and the interposer 850. The bonding typically does not make a seal to protect the diaphragms of the XBAR filter chip 805.
At 1340, a polymer cover 860 is formed over the XBAR filter chip 805 to seal the space between the XBAR filter chip 805 and the interposer 850. The cover 850 may be formed by injection molding or casting, for example. Individual covers may be formed over each XBAR filter chip, or a unitary cover 850 may be formed over the entire LTCC panel. In either case, packages XBAR filters may be excised from the panel by, for example, sawing. The process 1300 then ends at 1395.
At 1410, a XBAR filter chip 1005 is fabricated using, for example, the process 1100 of
The subsequent actions in the process require liquid materials, such as solvents, photoresist, or photopolymerizable monomers, to be applied to the front side of the piezoelectric plate 1010 after the cavities 1040 have been etched. The process 1400 is not suitable for XBAR filter chips with front-side etched cavities because the liquid materials may pass into the cavities through the etch holes in the diaphragms. Thus, the XBAR filter chip 1005 has back-side etched cavities with a cover 1080 sealed to the back side of the substrate 1020.
At 1420, walls 1052 are formed on the piezoelectric plate 1010. The walls 1052 may be formed with openings over the XBAR diaphragms and openings where electrical connections to the XBAR filter chip will be made in a subsequent process action. The walls 1052 may be formed, for example, by coating the piezoelectric plate 1010 with a photopolymerizable material and then exposing the photopolymerizable material through a suitable mask. Depending on the required thickness of the walls, multiple layers of material may be coated and patterned in succession.
A 1430, a cover layer 1054 is applied over the walls 1052. The cover layer 1054 may be applied, for example, as a continuous film bonded to the walls 1052 by an adhesive. The cover layer 1054 spans the openings in the walls 1052 over the XBAR diaphragms, forming an enclosed cavity 1055 over each diaphragm. The cover layer is pattered to form openings where electrical connections to the XBAR filter chip will be made in a subsequent process action.
At 1440, a conductor pattern 1070 is formed. The conductor pattern 1070 includes pads 1072 on the external surface of the cover layer 1054 for connection to circuitry external to the packaged XBAR filter. The conductor pattern 1070 connects the pads 1072 to connection points 1074 on the XBAR filer chip 1005. The conductor pattern 1070 may be aluminum, copper, gold, or a combination of materials deposited and patterned using conventional techniques. Once the conductor pattern is formed, the process 1400 ends at 1495.
The entire process 1400 may be, and commonly will be, performed on whole wafers. Individual packaged XBAR filters may then be excised by sawing through the bonded wafers after the conductor pattern is formed at 1440.
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.
The patent is a continuation of application Ser. No. 16/841,134, filed Apr. 6, 2020, titled TRANSVERSELY-EXCITED FILM BULK ACOUSTIC RESONATOR PACKAGE AND METHOD, which claims priority to the following provisional patent applications: application Ser. No. 62/830,258, titled XBAR PACKAGING, filed Apr. 5, 2019; application Ser. No. 62/881,749, titled XBAR PACKAGING INCLUDING CAP PLATE, filed Aug. 1, 2019; and application 62/904,416, titled XBAR WAFER-LEVEL PACKAGING, filed Sep. 23, 2019. All of these applications are incorporated herein by reference. This patent is related to application Ser. No. 16/230,443, filed Dec. 21, 2018, entitled TRANSVERSELY-EXCITED FILM BULK ACOUSTIC RESONATOR, now U.S. Pat. No. 10,491,192.
Number | Name | Date | Kind |
---|---|---|---|
5631515 | Mineyoshi et al. | May 1997 | A |
6540827 | Levy et al. | Apr 2003 | B1 |
6570470 | Maehara et al. | May 2003 | B2 |
6833774 | Abbott et al. | Dec 2004 | B2 |
7042132 | Bauer et al. | May 2006 | B2 |
7463118 | Jacobsen | Dec 2008 | B2 |
7535152 | Ogami et al. | May 2009 | B2 |
7684109 | Godshalk et al. | Mar 2010 | B2 |
7868519 | Umeda | Jan 2011 | B2 |
7939987 | Solal et al. | May 2011 | B1 |
7965015 | Tai et al. | Jun 2011 | B2 |
8278802 | Lee et al. | Oct 2012 | B1 |
8294330 | Abbott et al. | Oct 2012 | B1 |
8829766 | Milyutin et al. | Sep 2014 | B2 |
8932686 | Hayakawa et al. | Jan 2015 | B2 |
9112134 | Takahashi | May 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 | Jun 2016 | B1 |
9425765 | Rinaldi | Aug 2016 | B2 |
9525398 | Olsson | Dec 2016 | B1 |
9564873 | Kadota | Feb 2017 | B2 |
9748923 | Kando et al. | Aug 2017 | B2 |
9780759 | Kimura et al. | Oct 2017 | B2 |
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 |
10756697 | Plesski et al. | Aug 2020 | B2 |
10790802 | Yantchev et al. | Sep 2020 | B2 |
10797675 | Plesski | Oct 2020 | B2 |
10819319 | Hyde | Oct 2020 | B1 |
10985728 | Plesski et al. | Apr 2021 | B2 |
10992282 | Plesski et al. | Apr 2021 | B1 |
10998882 | Yantchev et al. | May 2021 | B2 |
11146232 | Yandrapalli et al. | Oct 2021 | B2 |
11201601 | Yantchev et al. | Dec 2021 | B2 |
11418167 | Garcia | Aug 2022 | B2 |
20020079986 | Ruby et al. | Jun 2002 | A1 |
20020158714 | Kaitila et al. | Oct 2002 | A1 |
20020190814 | Yamada et al. | Dec 2002 | A1 |
20040041496 | Imai et al. | Mar 2004 | A1 |
20040090145 | Bauer et al. | May 2004 | A1 |
20040100164 | Murata et al. | May 2004 | A1 |
20040207033 | Koshido | Oct 2004 | A1 |
20040207059 | Hong | Oct 2004 | A1 |
20040207485 | Kawachi et al. | Oct 2004 | A1 |
20040209387 | Hong | Oct 2004 | A1 |
20040261250 | Kadota et al. | Dec 2004 | A1 |
20050218488 | Matsuo | Oct 2005 | A1 |
20060131731 | Sato | Jun 2006 | A1 |
20060152107 | Tanaka | Jul 2006 | A1 |
20070090898 | Kando | Apr 2007 | A1 |
20070182510 | Park et al. | Aug 2007 | A1 |
20070188047 | Tanaka | Aug 2007 | A1 |
20070278898 | Miura et al. | Dec 2007 | A1 |
20070296304 | Fujii et al. | Dec 2007 | A1 |
20080018414 | Inoue et al. | Jan 2008 | A1 |
20080297280 | Thalhammer et al. | Dec 2008 | A1 |
20090315640 | Umeda et al. | Dec 2009 | A1 |
20100064492 | Tanaka | Mar 2010 | A1 |
20100102669 | Yamanaka | Apr 2010 | A1 |
20100123367 | Tai et al. | May 2010 | A1 |
20100223999 | Onoe | Sep 2010 | A1 |
20100301703 | Chen et al. | Dec 2010 | A1 |
20110102107 | Onzuka | May 2011 | A1 |
20110109196 | Goto | May 2011 | A1 |
20110199163 | Yamanaka | Aug 2011 | A1 |
20120181898 | Hatakeyama et al. | Jul 2012 | A1 |
20130021305 | Zuo et al. | Jan 2013 | A1 |
20130057360 | Meltaus et al. | Mar 2013 | A1 |
20130207747 | Nishii et al. | Aug 2013 | A1 |
20130234805 | Takahashi | Sep 2013 | A1 |
20130271238 | Onda et al. | Oct 2013 | A1 |
20140009032 | Takahashi et al. | Jan 2014 | A1 |
20140009247 | Moriya | Jan 2014 | A1 |
20140113571 | Fujiwara et al. | Apr 2014 | A1 |
20140145556 | Kadota | May 2014 | A1 |
20140151151 | Reinhardt | Jun 2014 | A1 |
20140225684 | Kando et al. | Aug 2014 | A1 |
20140312994 | Meltaus et al. | Oct 2014 | A1 |
20150244149 | Van Someren | Aug 2015 | A1 |
20150319537 | Perios et al. | Nov 2015 | A1 |
20150333730 | Meltaus | Nov 2015 | A1 |
20160049920 | Kishino | Feb 2016 | A1 |
20160079958 | Burak | Mar 2016 | A1 |
20160182009 | Bhattacharjee | Jun 2016 | A1 |
20160285430 | Kikuchi et al. | Sep 2016 | A1 |
20160301382 | Iwamoto | Oct 2016 | A1 |
20170063332 | Gilbert et al. | Mar 2017 | A1 |
20170104470 | Koelle et al. | Apr 2017 | A1 |
20170179928 | Raihn et al. | Jun 2017 | A1 |
20170187352 | Omura | Jun 2017 | A1 |
20170201232 | Nakamura et al. | Jul 2017 | A1 |
20170214385 | Bhattacharjee | Jul 2017 | A1 |
20170214387 | Burak et al. | Jul 2017 | A1 |
20170222622 | Solal et al. | Aug 2017 | A1 |
20170264266 | Kishimoto | Sep 2017 | A1 |
20170290160 | Takano et al. | Oct 2017 | A1 |
20180005950 | Watanabe | Jan 2018 | A1 |
20180013400 | Ito et al. | Jan 2018 | A1 |
20180013405 | Takata | Jan 2018 | A1 |
20180026603 | Iwamoto | Jan 2018 | A1 |
20180033952 | Yamamoto et al. | Feb 2018 | A1 |
20180097502 | Yamamoto et al. | Apr 2018 | A1 |
20180152169 | Goto et al. | May 2018 | A1 |
20180212589 | Meltaus et al. | Jul 2018 | A1 |
20180275485 | Hurwitz | Sep 2018 | A1 |
20190068155 | Kimura | Feb 2019 | A1 |
20190068164 | Houlden et al. | Feb 2019 | A1 |
20190131953 | Gong | May 2019 | A1 |
20190148621 | Feldman et al. | May 2019 | A1 |
20190181833 | Nosaka | Jun 2019 | A1 |
20190181825 | Schmalzl et al. | Jul 2019 | A1 |
20190207583 | Miura et al. | Jul 2019 | A1 |
20190245518 | Ito | Aug 2019 | A1 |
20190273480 | Lin | Sep 2019 | A1 |
20190348966 | Campanella-Pineda et al. | Nov 2019 | A1 |
20190386638 | Kimura et al. | Dec 2019 | A1 |
20200007110 | Konaka et al. | Jan 2020 | A1 |
20200021271 | Plesski | Jan 2020 | A1 |
20200021272 | Segovia Fernandez et al. | Jan 2020 | A1 |
20200228087 | Michigami et al. | Jul 2020 | A1 |
20200244247 | Maeda | Jul 2020 | A1 |
20200295729 | Yantchev | Sep 2020 | A1 |
20200304091 | Yantchev | Sep 2020 | A1 |
20200304102 | Kanazawa | Sep 2020 | A1 |
20200321939 | Turner et al. | Oct 2020 | A1 |
20200328728 | Nakagawa et al. | Oct 2020 | A1 |
20200373907 | Garcia | Nov 2020 | A1 |
20210119595 | Turner et al. | Apr 2021 | A1 |
20210273631 | Jachowski et al. | Sep 2021 | A1 |
20210313951 | Yandrapalli et al. | Oct 2021 | A1 |
20210328575 | Hammond et al. | Oct 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 |
20220149814 | Garcia et al. | May 2022 | A1 |
Number | Date | Country |
---|---|---|
106788318 | May 2017 | CN |
110417373 | Nov 2019 | CN |
210431367 | Apr 2020 | 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 |
2004523179 | Jul 2004 | JP |
2004304622 | Oct 2004 | JP |
2006173557 | Jun 2006 | JP |
2007251910 | Sep 2007 | JP |
2007329584 | Dec 2007 | JP |
2010062816 | Mar 2010 | JP |
2010103803 | May 2010 | JP |
2010154505 | Jul 2010 | JP |
2010233210 | Oct 2010 | JP |
2013528996 | Jul 2013 | JP |
2013214954 | Oct 2013 | JP |
2015054986 | Mar 2015 | JP |
2016001923 | Jan 2016 | 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 |
2015098694 | Jul 2015 | WO |
2016017104 | Feb 2016 | WO |
2016017104 | Feb 2016 | WO |
2016052129 | Apr 2016 | WO |
2016147687 | Sep 2016 | WO |
2016208428 | Dec 2016 | WO |
2017188342 | Nov 2017 | WO |
2018003268 | Jan 2018 | WO |
2018003273 | Jan 2018 | WO |
2018163860 | Sep 2018 | WO |
2019117133 | Jun 2019 | WO |
2019138810 | Jul 2019 | WO |
2020092414 | May 2020 | WO |
2020100744 | May 2020 | WO |
Entry |
---|
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. |
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. |
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. |
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. |
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. |
T. Takai, H. Iwamoto, et al., “I.H.P.Saw Technology and its Application to Microacoustic Components (Invited).” 2017 IEEE International Ultrasonics Symposium, Sept. 6-9, 2017. Pages 1-8. |
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. |
M. Kadota, S. Tanaka, “Wideband acoustic wave resonators composed of hetero acoustic layer structure,” Japanese Journal of Applied Physics, vol. 57, No. 751. Published Jun. 5, 2018. 5 pages. |
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. Pages 1-2. |
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. |
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. |
G. Manohar, “Investigation of Various Surface Acoustic Wave Design Configurations for Improved Sensitivity.” Doctoral dissertation, University of South Florida, USA, Jan. 2012, 7 pages. |
Ekeom, D. & Dubus, Bertrand & Volatier, A.. (2006). Solidly mounted resonator (SMR) FEM-BEM simulation. 1474-1477. 10.1109/ULTSYM.2006.371. |
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. |
Naumenko et al., “Optimal orientations of Lithium Niobate for resonator SAW filters”, 2003 IEEE Ultrasonics Symposium—pp. 2110-2113. (Year: 2003). |
Kadota et al., “Ultra-Wideband Ladder Filter Using SH0 Plate Wave in Thin LiNbO3 Plate and Its Application to Tunable Filter”, IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control, vol. 62, No. 5, May 2015, pp. 939-946. |
Abass et al. “Effects of inhomogeneous grain size distribution in polycrystalline silicon solar cells”, Energy Procedia 10(2011) pp. 55-60 © 2011 Published by Elsevier Ltd. |
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. |
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, Mar. 2021, Introduction. |
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. |
Number | Date | Country | |
---|---|---|---|
20210044274 A1 | Feb 2021 | US |
Number | Date | Country | |
---|---|---|---|
62904416 | Sep 2019 | US | |
62881749 | Aug 2019 | US | |
62830258 | Apr 2019 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 16841134 | Apr 2020 | US |
Child | 17067418 | US |