The current trend in acoustic transducer technology has been toward smaller microphones. Currently, electret microphones based on thin, charge-carrying membranes have been used in most applications. However, these microphones suffer from degradation after exposure to high temperatures. Capacitive MEMS microphones are gaining popularity because they can withstand the high temperatures experienced during solder-reflow and, therefore, reduce manufacturing cost. Piezoelectric MEMS microphones have been researched for more than 30 years and can potentially combine the advantages of electret microphones and MEMS capacitive microphones in a cost-effective manner. Unfortunately, piezoelectric MEMS microphones traditionally suffer from high noise floors due, in part, to diaphragm tension caused by residual stress in thin films. For example, diaphragm microphones are constrained on all edges, which leads to high diaphragm tension that results in decreased sensitivity. Conventional cantilevered designs, such as rectangular cantilever beam microphones, also suffer from the effects of residual stress despite being substantially released from the surrounding substrate; instead, the small amount of residual stress causes the cantilever to bend away from the substrate plane, either upwards or downwards. This bending causes the gap around the cantilever to increase, decreasing the acoustic resistance and resulting in an undesirable decrease in low-frequency sensitivity.
Thus, there is a need in the piezoelectric MEMS acoustic transducer field to create a new and useful acoustic transducer with low frequency sensitivity despite residual stresses.
The following description of the preferred embodiments of the invention is not intended to limit the invention to these preferred embodiments, but rather to enable any person skilled in the art of MEMS acoustic transducers to make and use this invention.
Acoustic Transducer
As shown in
As shown in
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As shown in
The cantilevered beam 120 is preferably made from alternating piezoelectric and electrode layers 142. The piezoelectric layers 144 can function to convert applied pressures to voltages, and the electrode layers 142 can function to transmit the generated voltages to an amplifier such as a JFET, a charge amplifier, or an integrated circuit. The piezoelectric layers 144 preferably include aluminum nitride (AlN) due to its CMOS compatibility, but may alternatively include lead zirconate titanate (PZT), zinc oxide (ZnO), polyvinylidene fluoride (PVDF), lead magnesium niobate-lead titanate (PMN-PT), or any other suitable piezoelectric material. The electrode layers 142 preferably include molybdenum (Mo), titanium (Ti), aluminum (Al), or platinum (Pt), but may alternately include any other suitable electrode material. The cantilevered beam 120 preferably includes two piezoelectric layers 144 interspersed between three electrode layers 142. However, the cantilevered beam 120 can include three piezoelectric layers 144 interspersed between the three electrode layers 142, include only three total layers (a first electrode layer 142, a first piezoelectric layer 144, and a top electrode layer 142), or any number of layers in any suitable permutation of electrode layers 142 and piezoelectric layers 144. Preferably, the cantilevered beam 120 incorporates at least one piezoelectric layer 144 and one electrode layer 142. In one example configuration, the electrode layers 142 preferably cover substantially two-thirds of a substantially triangular cantilevered beam 120 area to minimize the noise floor, but can alternately cover more or less of the cantilevered beam 120 depending on the cantilevered beam 120 geometry. Additionally, although each electrode layer 142 preferably defines only one independent electrode per electrode layer 142, the electrode layers 142 may be patterned to define multiple independent electrodes per electrode layer 142. The electrode layers 142 are preferably coupled together by metal traces in series, but may be coupled in parallel or both in series and in parallel.
As shown in
In the preferred transducer, the gaps between the cantilevered beams 120 are approximately less than 1 micron during manufacture, but may be slightly larger. After manufacture, the gaps between the cantilevered beams 120 are preferably maintained under 1 micron, but may be significantly larger due to deformation resulting from residual stress. The cantilevered beams 120 are preferably electrically coupled through one or more electrode layers 142, but may alternately be electrically coupled by conductive traces 146, be electrically isolated from one another, or be a blend, wherein some cantilevered beams 120 are electrically coupled while others are electrically isolated. The cantilevered beams 120 may be coupled in series or in parallel, but are preferably coupled with a blend of the two extremes, wherein some cantilevered beams 120 are coupled in series and others in parallel.
Method of Manufacturing an Acoustic Transducer
As shown in
Block S100 of the preferred method recites depositing alternating piezoelectric and electrode layers onto the substrate. Block S100 preferably functions to create the layers of the cantilever. The piezoelectric layers preferably include aluminum nitride (AlN) due to its CMOS compatibility, but may alternatively include lead zirconate titanate (PZT), zinc oxide (ZnO), polyvinylidene fluoride (PVDF), lead mangnesium niobate-lead titanate (PMN-PT), or any other suitable piezoelectric material. The electrode layers preferably include molybdenum (Mo), titanium (Ti), aluminum (Al) or platinum (Pt), but may alternately include any other suitable electrode material. The cantilever is preferably manufactured using surface micromachining, but may alternatively be manufactured by bulk micromachining. Each layer is preferably deposited onto the previous layer (wherein the first layer is deposited onto a SiO2 layer), then etched into a desired pattern before the next layer is deposited. Each layer is preferably deposited by thin film deposition, but may alternately be deposited by reactive physical vapor deposition, physical vapor deposition, chemical vapor deposition, epitaxy, or any suitable process. Each layer is preferably first patterned by photolithography, then micromachined to remove the material in the areas exposed by photolithography. Micromachining methods may include wet etching (chemical etching) and dry etching (e.g. through reactive ion etching or ion milling), but may include any other suitable etching method. In one embodiment, the electrode layers are patterned such that alternating layers are staggered (as shown in
Block S200 of the preferred method recites processing the deposited layers to define cantilever geometry. Block S200 preferably functions to create gaps that define the gap-controlling geometry of the cantilever. The deposited layers are preferably processed by etching gaps through the deposited layers (e.g. with reactive ion etching, wet etching, ion milling, or any other etching method), but may alternately be otherwise processed to define the cantilevered beams 120 and release them from their neighbors. The gap thicknesses are preferably 1 micron or less, but may alternately be slightly larger. Additionally, the gaps preferably bisect each other to form substantially triangular cantilevered beams, but may alternately intersect at the ends to form the desired gap-controlling geometry. This step preferably creates at least two bisecting gaps, such that at least four triangular cantilevered beams are formed, but may alternately create three, four, or any number of gaps to form any number of cantilevered beams.
Block S300 of the preferred method recites depositing metal traces. Block S300 preferably functions to electrically couple the acoustic transducer to one or more amplifiers. Block S300 can occur before, after, or concurrently with block S200. The metal traces are preferably deposited as a layer then patterned, but may alternately be pre-patterned and deposited onto the acoustic transducer. Block S300 preferably provides a metal trace for each electrode or electrode layer 142, but may provide a single metal trace for a plurality of electrodes, wherein the electrodes are coupled together in parallel. The metal traces preferably extend through the intermediary piezoelectric and/or electrode layers to the relevant electrode layer 142, but may be alternatively coupled to the transducer electrodes in any suitable manner.
Block S400 of the preferred method recites releasing the cantilevered beams from the substrate. Block S400 preferably functions to allow the cantilevered beams to expand, contract or bend as necessary to substantially relieve residual stress. The cantilevered beams are preferably released from the substrate by removing the substrate from underneath the cantilevered beams. This is preferably accomplished using DRIE (deep reactive ion etching), but may be accomplished using wet etching, EDM (electric discharge machining), micromachining processes, or any other processing method that releases the cantilevered beams from the substrate. Alternatively, the cantilevered beams can be entirely released from the substrate and subsequently reattached, either to the same substrate or to a different substrate. The cantilevered beams can be entirely released by providing a sacrificial layer between the substrate and the cantilevered beam layers before beam layer deposition (i.e. before block S100), and subsequently etching away the sacrificial layer in block S500. The sacrificial layer is preferably an oxide, but may be any suitable material dissimilar from the piezoelectric and electrode layer materials that may be selectively removed. The sacrificial layer is preferably etched away with an etchant, such as hydrogen fluoride (HF) in an aqueous solution, plasma etching, or any other suitable etching process. The cantilevered beams are preferably reattached to a substrate along their bases by electrostatic clamping or any suitable technique.
The preferred method can additionally include the step of growing an oxide layer on the substrate in block S500. Block S500 preferably occurs prior to block S100, and preferably functions to control the amount of cantilever beam release in S400. In one variation of block S400, the substrate removal process preferably ends at the oxide layer. In a second variation of block S500, the oxide layer preferably functions as the sacrificial layer. A suitable oxide is preferably grown over the desired active area of the transducer, but may alternatively be grown in the desired release areas of the transducer, over the entire substrate or in any suitable area. The oxide is preferably an oxide grown from the substrate, more preferably silicon dioxide (SiO2), but may be any suitable oxide that is grown or deposited on the substrate. The oxides are preferably grown using general thermal oxidization, but may alternatively be grown using plasma-enhanced chemical vapor deposition (PECVD oxide deposition), chemical vapor deposition (CVD oxide deposition), physical vapor deposition (PVD oxide deposition), or any other suitable oxidization or oxide deposition process. The preferred method can additionally include removing the oxide layer in block S500A, which removes the oxide layer from the transducer by etching or micromachining.
The preferred method can additionally include depositing a seed layer in block S600. The seed layer preferably functions as an active layer on which to build the cantilevered beams. Block S600 preferably occurs before block S100. More preferably, block S600 is performed after block S500 such that the seed layer is arranged between the piezoelectric or electrode layer of the cantilevered beam and oxide layer. The seed layer is preferably aluminum nitride (AlN), but may be any suitable piezoelectric, electrode, or seed material. The seed layer is preferably sputtered using physical vapor deposition (PVD) or any other suitable sputtering technique, but may be otherwise deposited over the oxide layer or substrate.
Example Method and Transducer
As shown in
Throughout performance of the example method, the residual stress is preferably monitored using wafer curvature measurements (e.g. through optical or physical measurements), but may alternately be measured by stress measurements (e.g. stress transducers), nonlinear elastic stress measurements (e.g. ultrasonic or magnetic techniques, X-ray or neutron diffraction), or any other method of measuring the residual stress or curvature in the cantilever. The deposition parameters are then preferably adjusted to minimize the cantilever deflection or stress.
As a person skilled in the art will recognize from the previous detailed description and from the figures and claims, modifications and changes can be made to the preferred embodiments of the invention without departing from the scope of this invention defined in the following claims.
This application is a continuation and claims priority to U.S. application Ser. No. 16/353,934, filed Mar. 14, 2019, which is a continuation and claims priority to U.S. application Ser. No. 14/702,319, filed May 1, 2015, now U.S. Pat. No. 10,284,960, which is a continuation and claims priority to U.S. application Ser. No. 13/398,631, filed Feb. 16, 2012, now U.S. Pat. No. 9,055,372, which claims priority to U.S. provisional application No. 61/470,384 entitled “Acoustic Sensor with Gap-Controlling Geometry and Method of Manufacturing an Acoustic Sensor” and filed Mar. 31, 2011, the entire contents of each of which are incorporated herein by this reference.
Number | Name | Date | Kind |
---|---|---|---|
4456394 | Kolm et al. | Jun 1984 | A |
5633552 | Lee et al. | May 1997 | A |
5956292 | Bernstein | Sep 1999 | A |
6201341 | Fujimoto | Mar 2001 | B1 |
6857501 | Han et al. | Feb 2005 | B1 |
6944922 | Shearer et al. | Sep 2005 | B2 |
7992431 | Shih et al. | Aug 2011 | B2 |
9055372 | Grosh et al. | Jun 2015 | B2 |
10284960 | Grosh | May 2019 | B2 |
11259124 | Grosh | Feb 2022 | B2 |
20040061415 | Shearer et al. | Apr 2004 | A1 |
20040075363 | Malkin et al. | Apr 2004 | A1 |
20040164649 | Xu et al. | Aug 2004 | A1 |
20060087203 | Cho | Apr 2006 | A1 |
20070145861 | Tanner | Jun 2007 | A1 |
20100084721 | Wu et al. | Apr 2010 | A1 |
20100189289 | Takeuchi | Jul 2010 | A1 |
20100254547 | Grosh et al. | Oct 2010 | A1 |
20100290142 | Krastev et al. | Nov 2010 | A1 |
20110075879 | Kim et al. | Mar 2011 | A1 |
20120053393 | Kaltenbacher | Mar 2012 | A1 |
20120250909 | Grosh et al. | Oct 2012 | A1 |
20120270352 | Huffman et al. | Oct 2012 | A1 |
20150271606 | Grosh et al. | Sep 2015 | A1 |
Number | Date | Country |
---|---|---|
101929898 | Dec 2010 | CN |
2011004129 | Jan 2011 | JP |
101053257 | Aug 2011 | KR |
WO-2010002887 | Jan 2010 | WO |
Entry |
---|
KR Grant of Patent in Korean Appln. No. 20207008813, dated Sep. 21, 2020, 2 pages (with English translation). |
Office Action in corresponding U.S. Appl. No. 13/398,631 dated Oct. 22, 2014, pp. 1-13. |
Office Action in corresponding Japanese Application No. 2014-502569, dated Jul. 1, 2014, pp. 1-3. |
Response to Office Action dated Oct. 22, 2014, in corresponding U.S. Appl. No. 13/398,631 dated Jan. 21, 2015, pp. 1-12. |
International Search Report and Written Opinion—PCT/US2012/025487—ISA/EPO—dated May 21, 2012. |
Supplementary European Search Report—EP12804425—Search Authority—Munich—dated Jun. 16, 2014. |
Number | Date | Country | |
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20220248145 A1 | Aug 2022 | US |
Number | Date | Country | |
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61470384 | Mar 2011 | US |
Number | Date | Country | |
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Parent | 16353934 | Mar 2019 | US |
Child | 17675850 | US | |
Parent | 14702319 | May 2015 | US |
Child | 16353934 | US | |
Parent | 13398631 | Feb 2012 | US |
Child | 14702319 | US |