High performance sensors and methods for forming the same

Information

  • Patent Grant
  • 8187902
  • Patent Number
    8,187,902
  • Date Filed
    Wednesday, July 9, 2008
    16 years ago
  • Date Issued
    Tuesday, May 29, 2012
    12 years ago
Abstract
A sensor includes a proof mass suspended by a suspension beam, the suspension beam having a thickness less than a thickness of the proof mass.
Description
FIELD OF THE INVENTION

The present invention relates, in various embodiments, to the fabrication of high-performance microelectromechanical systems sensors.


BACKGROUND

The advent of microelectromechanical systems (MEMS) processing techniques has enabled the fabrication of small, high-performance sensors such as accelerometers and gyroscopes. One particularly useful MEMS sensor is the tuning fork gyroscope, which is utilized to sense angular rate, i.e., angular velocity (and hence, angular displacement) in a variety of applications. A conventional tuning fork gyroscope includes one or two proof masses suspended above a substrate, typically suspended above the substrate by suspension beams that allow the proof masses to vibrate freely. The edges of the proof masses include electrode fingers, or “combs.” Between and to either side of the proof masses is drive circuitry with complementary sets of combs interleaved with the proof mass combs. Voltage applied between the interleaved sets of combs enables the vibration of the proof masses in the plane of the substrate surface. To facilitate fabrication of the gyroscope, i.e., a “comb drive” device, the proof masses, suspension beams, and both sets of interleaved combs typically have the same thickness (typically approximately 20 micrometers (μm), e.g., 23 μm).


When the gyroscope rotates (undergoes angular motion), sense plates below the proof masses detect differential vertical displacement thereof (e.g., by measuring capacitance between the proof masses and the sense plates). This differential vertical displacement is translated directly into a measure of angular rate by the gyroscope. However, the performance of conventional tuning fork gyroscopes for various applications is often limited. For example, the wide-bandwidth rate noise, or “angle random walk,” often may be limited to values of 0.1°/h1/2 or higher. Moreover, bias error over temperature may be limited to values of 10°/h or higher for conventional tuning fork gyroscopes.


Thus, in order to service the demand for higher-performance sensors incorporating comb drives and proof masses (such as tuning fork gyroscopes), improved designs and methods for constructing such sensors are needed.


SUMMARY

In accordance with certain embodiments, a technique is provided for forming high-performance sensors that include thicker proof masses, as well as suspension beams and/or stationary combs having thicknesses less than that of the proof mass (and/or the moving combs at the periphery thereof). As a result, the sensor exhibits superior wide-bandwidth rate noise and bias error over temperature.


In one aspect, embodiments of the invention feature a sensor that includes a proof mass suspended over a substrate by a suspension beam. The thickness of the suspension beam may be less than the thickness of the proof mass, which may be between approximately 50 μm and approximately 1000 μm. In one embodiment, the thickness of the proof mass is greater than approximately 23 μm. The difference between the thickness of the suspension beam and the thickness of the proof mass may be between approximately 10 μm and approximately 50 μm, e.g., approximately 20 μm. The proof mass and the suspension beam may include or consist essentially of silicon, and the substrate may include or consist essentially of glass. The substrate may include or consist essentially of a semiconductor material, e.g., silicon, substantially coated with a dielectric material, e.g., silicon dioxide, on at least one surface thereof.


Embodiments of the invention may include one or more of the following. The sensor may include a stationary comb disposed over the substrate. The stationary comb may have stationary comb fingers interleaved with mobile comb fingers disposed on one or more edges of the proof mass. The thickness of the stationary comb fingers may be less than the thickness of the mobile comb fingers, which may be approximately equal to the thickness of the proof mass. For example, the thickness of the stationary comb fingers may be between approximately 30 μm and approximately 40 μm.


In another aspect, embodiments of the invention feature a method of fabricating a sensor. The method may include forming a first recess in a first surface of a first substrate, as well as bonding a portion of the first surface to a second substrate. A second recess may be formed in a second surface of the first substrate, thereby forming a suspension beam suspending a proof mass over the second substrate. The second recess may be disposed over the first recess. The thickness of the suspension beam may be less than the thickness of the proof mass, and the difference in thicknesses may be approximately equal to the aggregate depth of the first and second recesses. The depths of the first and second recesses may be approximately equal.


Embodiments of the invention may feature one or more of the following. The method may include forming a third recess in the first surface of the first substrate and forming a fourth recess in the second surface of the first substrate, thereby forming a stationary comb finger disposed over the second substrate. The thickness of the stationary comb finger may be less than the thickness of a mobile comb finger disposed on an edge of the proof mass. The depths of the third and fourth recesses may be approximately equal. The first and third recesses may be formed substantially simultaneously and the second and fourth recesses may be formed substantially simultaneously.


In yet another aspect, embodiments of the invention feature a method of sensing angular rate. The method may include providing a sensor including two proof masses, each (i) being suspended over a substrate by a suspension beam having a thickness less than the thickness of the proof mass it suspends and (ii) including a plurality of mobile comb fingers on at least one edge thereof. The sensor may also include a plurality of stationary comb fingers proximate the two proof masses and interleaved with the mobile comb fingers. The method may also include applying a voltage between the stationary comb fingers and the proof masses such that the proof masses vibrate approximately parallel to a surface of the substrate. The differential displacement of the two proof masses in a plane approximately perpendicular to the surface of the substrate may be detected, and an output signal generated based on the differential displacement. The signal may represent the angular rate experienced by the sensor. The thickness of the stationary comb fingers may be less than the thickness of the mobile comb fingers. The thickness of each of the two proof masses may be between approximately 50 μm and approximately 60 μm. The wide-bandwidth rate noise of the sensor may be less than approximately 0.01°/h1/2, and its bias error over temperature may be less than approximately 1°/h.


These and other objects, along with advantages and features of the invention, will become more apparent through reference to the following description, the accompanying drawings, and the claims. Furthermore, it is to be understood that the features of the various embodiments described herein are not mutually exclusive and can exist in various combinations and permutations.





BRIEF DESCRIPTION OF THE DRAWINGS

In the drawings, like reference characters generally refer to the same parts throughout the different views. Also, the drawings are not necessarily to scale, emphasis instead generally being placed upon illustrating the principles of the invention. In the following description, various embodiments of the present invention are described with reference to the following drawings, in which:



FIG. 1 is a plan view of a sensor fabricated in accordance with various embodiments of the invention;



FIGS. 2A-2G are cross-sectional views of a process sequence for fabricating the sensor of FIG. 1 in accordance with an embodiment of the invention; and



FIGS. 3A-3G are cross-sectional views of a process sequence for fabricating the sensor of FIG. 1 in accordance with another embodiment of the invention.





DETAILED DESCRIPTION


FIG. 1 depicts an exemplary sensor 100, e.g., a tuning fork gyroscope, which includes a plurality of (e.g., two) proof masses 110, and corresponding motors 120, bottom sense plates 130, anchors 140, torsion beams 142, base beams 144, suspension beams 146, and electrical contacts 150. Sensor 100 is disposed above a substrate 160, which may include or consist essentially of glass, e.g., borosilicate glass such as PYREX (e.g., Corning 7740), available from Corning Inc. of Corning, N.Y., or BOROFLOAT, available from Schott North America, Inc. of Elmsford, N.Y. In an embodiment, substrate 160 includes or consists essentially of a semiconductor material coated with a dielectric material, e.g., an oxide such as silicon dioxide, on at least one surface. In a preferred embodiment, motors 120, bottom sense plates 130, anchors 140, and electrical contacts 150 are disposed directly in contact with substrate 160. Proof masses 110 may be suspended over substrate 160 (e.g., over recesses formed in the top surface of substrate 160) by torsion beams 142, base beams 144, and suspension beams 146, and be free to move both parallel and perpendicular to the top surface of substrate 160. In accordance with various embodiments of the invention, proof masses 110 include mobile comb fingers 170, which are preferably interleaved with stationary comb fingers 180 attached to motors 120. FIG. 1 depicts torsion beams 142 and suspension beams 146 as being completely or approximately straight, but these features may, in other embodiments, be curved, sinuous, or “folded” in a serpentine fashion.


During operation, proof masses 110 may vibrate along the axis indicated by vector 190 (approximately parallel to the top surface of substrate 160) in response to voltage applied between mobile comb fingers 170 and electrically driven stationary comb fingers 180. The distance between one or both of proof masses 110 and bottom sense plates 130 may vary in response to angular rate of sensor 100 about axis 195 due to the Coriolis effect. The differential displacement of proof masses 110 from their respective bottom sense plates 130 and/or top sense plates (not shown) may be determined by measuring the differential capacitance therebetween. Signals representing the differential displacement (and/or differential capacitance) may be communicated via electrical contacts 150 to circuitry (not shown) which may calculate the angular displacement experienced by sensor 100 and output a signal representing it. Other details of the operation of sensor 100 may be similar to those described in U.S. Pat. No. 5,349,855, the entire disclosure of which is incorporated by reference herein. Sensor 100 may also include top sense plates (not shown) disposed above proof masses 110 (e.g., with a gap therebetween), as described in U.S. Pat. No. 7,172,919, the entire disclosure of which is incorporated by reference herein. The use of both bottom and top sense plates may reduce measurement errors which may result from constant vertical acceleration.


In an embodiment of the invention, each of proof masses 110, mobile comb fingers 170, anchors 140, torsion beams 142, base beams 144, and suspension beams 146 include or consist essentially of a semiconductor material, e.g., silicon, and they all may be formed as a single continuous and seamless structure. Proof masses 110 may have thicknesses greater than the approximately 23 μm thickness of many conventional sensor proof masses. In a preferred embodiment, the thickness of proof masses 110 is between approximately 50 μm and approximately 60 μm, e.g., approximately 54 μm. In various embodiments, the thickness of proof masses 110 is between approximately 50 μm and approximately 500 μm, or even up to approximately 1000 μm. The increased thickness of proof masses 110 enables sensor 100 to exhibit wide-bandwidth rate noise values less than approximately 0.1°/h1/2, less than approximately 0.01°/h1/2, or even less than approximately 0.003°/h1/2. However, the increased thickness of proof masses 110 may result in increased bias errors that may be ameliorated as described below.


The width of suspension beams 146 may be relatively small (e.g., less than approximately 14 μm) in order to reduce thermoelastic damping in sensor 100. Such damping may cause bias error due to coupling of the drive forces and voltages of motors 120 and because proof masses 110 are typically driven at their anti-parallel resonant frequency (in phase with the proof mass velocity and the Coriolis force). Due to processing limitations, the sidewalls of suspension beams 146 may not be completely vertical, i.e., a cross-section of suspension beam 146 may have the shape of a parallelogram (or even a rhombus) rather than of a rectangle. The non-vertical slope of the sidewalls of suspension beams 146 may be less than approximately 1°. Moreover, suspension beams 146 may have a high thickness-to-width aspect ratio (e.g., greater than approximately 3:1, or even greater than approximately 4:1), which, combined with non-vertical sidewalls, may increase bias errors. These bias errors may not be significant, or even detectable, for sensors with proof masses thinner than approximately 30 μm.


The high aspect ratio and sidewall non-verticality may result in cross-coupled thermoelastic damping (or “damping cross-coupling”), an effect heretofore unknown and unconsidered in the art. Such a damping force may operate as a sense-axis force that compromises the accuracy of the output signal. Moreover, since cross-coupled damping may be proportional to temperature and in-phase with the Coriolis force detected by sensor 100, it may lead directly to temperature-sensitive bias errors. This effect may be increased dramatically as the thickness of proof masses 110 is increased from the conventional thickness of approximately 20 μm.


The sidewall non-verticality of suspension beams 146 may also result in stiffness forces being coupled into the sense direction, i.e., stiffness cross-coupling. For conventional proof mass thicknesses, stiffness cross-coupling may be reduced by trimming techniques and electronic quadrature nulling, as described in U.S. Pat. Nos. 5,481,914 and 6,571,630, the entire disclosures of which are incorporated by reference herein. However, proof mass thicknesses greater than approximately 20 μm may result in stiffness cross-coupling large enough to affect yield and/or reliability of sensor 100. Even more problematically, trimming techniques may not be able to reduce stiffness cross-coupling and damping cross-coupling simultaneously, due to their different dependencies on the aspect ratio and dimensions of suspension beams 146.


Thus, in a preferred embodiment, the thickness of suspension beams 146 is less than the thickness of proof masses 110. The thickness of suspension beams 146 may be between approximately 30 μm and approximately 40 μm. The difference in thicknesses between suspension beam 146 and proof mass 110 may be between approximately 10 μm and approximately 50 μm, e.g., approximately 20 μm. The decreased thickness of suspension beams 146 may enable a low width-to-thickness aspect ratio for suspension beams 146, e.g., an aspect ratio less than approximately 3:1 or even less than approximately 2:1. Suspension beams 146 having a smaller thickness than that of proof masses 110 enables sensor 100 to exhibit a high quality factor and/or a reduced bias error due to damping cross-coupling and stiffness cross-coupling. In various embodiments, torsion beams 142 and base beams 144 may also have thicknesses less than that of proof mass 110. The thicknesses of torsion beams 142 and base beams 144 may be substantially equal to the thickness of suspension beams 146. Reduced thickness of torsion beams 142 and base beams 144 may be particularly advantageous for designs of sensor 100 incorporating only a single proof mass 110 or multiple proof masses 110 lacking physical connections therebetween.


Temperature-sensitive bias errors may also arise from vertical misalignment between stationary comb fingers 180 and mobile comb fingers 170. Such misalignment may occur during fabrication and/or assembly of sensor 100, or even may be due to thermal stresses during operation. The bias errors may arise from drive-force cross-coupling, i.e., a deleterious lift force in the vertical direction (i.e., substantially perpendicular to axes 190,195) resulting from a vertical electric field acting on the top and/or bottom surface of mobile comb fingers 170.


Simulations were performed to estimate the magnitude of the drive-force cross-coupling for three different variants of sensor 100. In each variant, 1 V was applied to the stationary comb fingers 180 in order to drive the in-plane vibration of proof masses 110. Proof mass 110, lower sense plate 130, and upper sense plate (not shown in FIG. 1) were assumed to be grounded. A 1 μm vertical displacement of proof mass 110 was also assumed. In the first variant of sensor 100, stationary comb fingers 180 and mobile comb fingers 170 were assumed to have the same thickness (of approximately 54 μm). A net lift force (as a function of comb depth) of −7.1×10−14 N/μm results, a significant amount of force compared with the Coriolis force measured during operation of sensor 100. In the second variant, the thickness of mobile comb fingers 170 was decreased to approximately 34 μm, the mobile comb fingers 170 being “recessed” by approximately 10 μm on both top and bottom surfaces. The resulting lift force was −8.5×10−14 N/μm, a similar value to that found in the first variant. It was found that, although thinning mobile comb fingers 170 tends to decrease the lift force, it also reduces the amount of shielding between the vertical electric field and the sense plate(s) (i.e., it allows interaction therebetween, increasing the deleterious lift force). Thinning the mobile comb fingers 170 to unmanufacturable thicknesses may be required for these opposing effects to effectively reduce the overall lift force. Finally, in the third variant, stationary comb fingers 180 were reduced in thickness relative to mobile comb fingers 170, again by approximately 10 μm on both top and bottom surfaces. In this case, the lift force was decreased to −0.18×10−14 N/μm, a factor of 40 better than the prior art. Vertical electric fields at the top and bottom surfaces of stationary comb fingers 180 were closely matched and did not substantially penetrate to the sense plate(s). These results were found to be substantially linear as a function of vertical displacement, and were valid even for non-vertical comb sidewalls.


Thus, in accordance with various embodiments of the invention, the thickness of stationary comb fingers 180 may be less than the thickness of mobile comb fingers 170 and/or the thickness of proof masses 110, e.g., between approximately 30 μm and approximately 40 μm. The difference in thicknesses between stationary comb fingers 180 and mobile comb fingers 170 may be approximately 20 μm. In various embodiments, the difference in thicknesses between stationary comb fingers 180 and mobile comb fingers 170 is approximately four times the width of the gap separating each stationary comb finger 180 from each mobile comb finger 170 (which may be, e.g., approximately 5 μm). The difference in thicknesses between stationary comb fingers 180 and mobile comb fingers 170 may be approximately four times the width an individual stationary comb finger 180 or mobile comb finger 170 (which may be, e.g., approximately 5 μm). The decreased thickness of stationary comb fingers 180 may enable reduced bias errors caused by the electrostatic drive force coupling into the sense direction of sensor 100. In other embodiments, the thickness of mobile comb fingers 170 may be less than the thickness of stationary comb fingers 180, as such variants may also exhibit reduced bias errors when compared to designs of sensor 100 in which these thicknesses are equal.


In various embodiments of the invention, the thinning of suspension beams 146 and/or stationary comb fingers 180 with respect to the thickness of proof masses 110 (and/or mobile comb fingers 170) enables sensor 100 to exhibit bias error over temperature less than approximately 1°/h.



FIGS. 2A-2G are a series of cross-sectional views depicting an exemplary process for forming sensor 100 which includes suspension beams 146 having a thickness less than that of proof masses 110. Referring to FIG. 2A, recess 200 and mesas 210 may be formed on a surface of substrate 160, preferably simultaneously by masking off regions of substrate 160 where mesas 210 are to be formed and removing material, e.g., by wet or plasma etching, to form recess 200. Alternatively, additional material may be deposited (e.g., by chemical or physical vapor deposition) atop substrate 160 to form mesas 210, thus also forming recess 200. Bottom sense plate 130 may be formed within recess 200 by deposition (e.g., by chemical or physical vapor deposition) of a conductive material, e.g., a metal, and etching, or by a lift-off process. Mesas 210 may act as anchoring bases for various portions of sensor 100 formed directly thereon such as anchors 140 and motors 120.


A second substrate 220, from which proof masses 110, motors 120, anchors 140, torsion beams 142, base beams 144, and suspension beams 146 may be formed, is provided. Second substrate 220 may include device layer 230 disposed over handle wafer 240. In an embodiment, second substrate 220 may include or consist essentially of a semiconductor-on-insulator substrate (e.g., a silicon-on-insulator (SOI) substrate), and insulator layer 250 may be disposed between and in contact with device layer 230 and handle wafer 240. In another embodiment, device layer 230 may include or consist essentially of silicon germanium or heavily p-type-doped silicon, and insulator layer 250 may be absent from second substrate 220. Device layer 230 and/or handle wafer 240 may include or consist essentially of a semiconductor material, e.g., silicon. Insulator layer 250 may include or consist essentially of an oxide, e.g., silicon dioxide. The thickness of device layer 230 may be the approximate desired thickness of proof masses 110 in sensor 100, e.g., greater than approximately 23 μm. In an embodiment, the thickness of device layer 230 is between approximately 50 μm and approximately 1000 μm, e.g., approximately 54 μm. First recesses 260, one for each suspension beam 146 to be fabricated, may be formed in the exposed top surface 261 of device layer 230 (i.e., a first surface of second substrate 220). In an embodiment, the depth of first recesses 260 is approximately 10 μm. In an embodiment, recesses 200 may be formed in second substrate 220 rather than in substrate 160.


Referring to FIG. 2B, substrate 160 and second substrate 220 may be bonded together, i.e., mesas 210 on substrate 160 may be joined to the top surface of device layer 230 by, e.g., anodic bonding. After bonding, handle wafer 240 and insulator layer 250 may be removed by, e.g., two successive selective etches. For example, handle wafer 240 may be removed by exposure to an etchant such as potassium hydroxide (KOH) or ethylene diamine pyrocatechol (EDP). If present, insulator layer 250 may be removed by exposure to an etchant such as hydrofluoric acid (HF). The exposed backside of substrate 160 may be protected from the etchant by a protective layer including or consisting essentially of, e.g., metal or photoresist. After removal of handle wafer 240 and insulator layer 250, features such as proof masses 110 and motors 120 may be fabricated from device layer 230. A first mask 262 may be formed over areas of device layer 230 where thinning and/or material removal is not desired, e.g., areas defining proof masses 110. First mask 262 may include or consist essentially of a conductive material, e.g., a metal such as aluminum, or a dielectric material such as silicon dioxide. In an embodiment, first mask 262 is not formed over regions 263 of device layer 230 disposed over first recesses 260, nor over release regions 264 disposed between mesas 210 which are meant to be entirely etched away, thus releasing suspended portions of sensor 100 such as proof masses 110 (as described further below). Second mask 266 may be formed over first mask 262, as well as over regions 263. In an embodiment, second mask 266 includes or consists essentially of photoresist.


Referring to FIG. 2C, a first release etch, which removes material from release regions 264 (and not from regions protected by second mask 266), is performed on a second surface 268 of device layer 230 (i.e., a second surface of the remaining portion of second substrate 220). In an embodiment, first release etch is an inductively coupled plasma etch such as a “Bosch process” performed in an etcher available from Surface Technology Systems plc of Newport, UK. First release etch may remove a thickness t1 of device layer 230 in release regions 264, which preferably leaves a thickness t2 of device layer 230 in release regions 264. Thickness t2 is preferably greater than zero, and may be less than or approximately equal to a depth of first recesses 260. Thus, thickness t1 may be the approximate difference between the thickness of device layer 230 (which, in an embodiment, defines the thickness of proof masses 110) and the thickness of first recesses 260. In an embodiment, thickness t1 is between approximately 40 μm and approximately 50 μm, e.g., approximately 44 μm. As described further below, thickness t2 may define the depth of second recesses 270 (see FIG. 2E) formed on a top surface of suspension beams 146. In an embodiment, the first release etch may also remove a thickness t1 of material to define one or more apertures 272 (not shown in FIG. 1 for clarity) in regions of device layer 230 where proof masses 110 are to be fabricated. As described further below, each aperture 272 may eventually define an opening through an entire thickness of a proof mass 110, as described in U.S. Pat. No. 6,257,059, the entire disclosure of which is incorporated by reference herein. Apertures 272 may reduce fluid damping in the vertical direction, reduce fluid coupling of drive motion into vertical motion, and/or allow inspection of the gap between proof mass 110 and bottom sense plate 130 during fabrication.


Referring to FIGS. 2D and 2E, second mask 266 may be removed from the surface of device layer 230 and from first mask 262. In an embodiment, second mask 266 is removed by application of a suitable solvent or by ashing with an oxygen plasma. Removal of second mask 266 may expose regions 263 of device layer 230. A second release etch may then be performed. Second release etch preferably removes a thickness of material approximately equal to t2 from regions 263, release regions 264, and apertures 272, thus removing all remaining material from release regions 264 (and apertures 272) and forming second recesses 270 in regions 263. In an embodiment, the depth of second recesses 270 is approximately equal to the depth of first recesses 260, e.g., approximately 10 μm.


Referring to FIGS. 2F and 2G, first mask 262 is removed from the surface of device layer 230, e.g., by wet etching in a mixture of phosphoric acid, nitric acid, and acetic acid. An optional top substrate 280 may be attached to device layer 230 by, e.g., anodic bonding. Top substrate 280 may include or consist essentially of glass, e.g., borosilicate glass such as PYREX (e.g., Corning 7740), available from Corning Inc. of Corning, N.Y., or BOROFLOAT, available from Schott North America, Inc. of Elmsford, N.Y. Top substrate 280 may include upper sense plate 290 disposed approximately directly over lower sense plate 130. Upper sense plate 290 may include or consist essentially of any of the materials previously described in reference to lower sense plate 130. With additional reference to FIG. 1, sensor 100 may include suspension beams 146 having a thickness tB less than a thickness tP of proof mass 110. In an embodiment, each suspension beam 146 is approximately vertically centered with respect to proof mass 110, i.e., the depths of first recesses 260 and second recesses 270 are approximately equal.



FIGS. 3A-3G are a series of cross-sectional views depicting an exemplary process for forming a sensor 100 that includes stationary comb fingers 180 having a thickness less than that of mobile comb fingers 170. Referring to FIG. 3A, recess 200 and mesas 210 may be formed on a surface of substrate 160, preferably as described above in reference to FIGS. 2A-2G. Bottom sense plate 130 may be formed within recess 200 by deposition of a conductive material, e.g., a metal, and etching, or by a lift-off process. Mesas 210 may act as anchoring bases for various portions of sensor 100 formed directly thereon such as anchors 140 and motors 120.


Second substrate 220, from which proof masses 110, motors 120, anchors 140, torsion beams 142, base beams 144, and suspension beams 146 may be formed, is provided. Second substrate 220 may include device layer 230 disposed over handle wafer 240, and may include insulator layer 250. Third recesses 360, one for each stationary comb finger 180 to be fabricated, may be formed in the exposed top surface 261 of device layer 230 (i.e., a first surface of second substrate 220). In an embodiment, the depth of third recesses 360 is approximately 10 μm. Areas of device layer 230 which will eventually become mobile comb fingers 170 are merely outlined in a dashed line in FIGS. 3A-3G for clarity. In an embodiment, mobile comb fingers 170 are not thinned, and therefore have a thickness approximately equal to that of device layer 230 (and proof mass 110).


Referring to FIG. 3B, substrate 160 and second substrate 220 may be bonded together, i.e., mesas 210 on substrate 160 may be joined to the top surface of device layer 230 by, e.g., anodic bonding. After bonding, handle wafer 240 and insulator layer 250 may be removed by, e.g., two successive selective etches, as described above. After removal of handle wafer 240 and insulator layer 250, features such as proof masses 110, motors 120, mobile comb fingers 170, and stationary comb fingers 180 may be fabricated from device layer 230. A third mask 362 may be formed over areas of device layer 230 where thinning and/or material removal is not desired, e.g., areas defining proof masses 110. Third mask 362 may include or consist essentially of a conductive material, e.g., a metal such as aluminum, or a dielectric material such as silicon dioxide. In an embodiment, third mask 362 is not formed over regions 363 of device layer 230 disposed over third recesses 360, nor over release regions 264 disposed between mesas 210 which are meant to be entirely etched away, thus releasing suspended portions of sensor 100 such as proof masses 110. Fourth mask 366 may be formed over third mask 362, as well as over regions 363. In an embodiment, fourth mask 366 includes or consists essentially of photoresist.


Referring to FIG. 3C, a first release etch, which removes material from release regions 264 (and not from regions protected by second mask 366), is performed on a second surface 268 of device layer 230 in a fashion similar to that described above in reference to FIG. 2C. First release etch may remove a thickness t3 of device layer 230 in release regions 264, which preferably leaves a thickness t4 of device layer 230 in release regions 264. Thickness t4 is preferably greater than zero, and may be approximately equal to a depth of third recesses 360. Thus, thickness t4 may be the approximate difference between the thickness of device layer 230 (which, in an embodiment, defines the thickness of proof masses 110) and the thickness of third recesses 360. In an embodiment, thickness t3 is between approximately 40 μm and approximately 50 μm, e.g., approximately 44 μm. As described further below, thickness t4 may define the depth of fourth recesses 370 (see FIG. 3E) formed on a top surface of stationary comb fingers 180. In an embodiment, the third release etch may also remove a thickness t3 of material to define one or more apertures 272 (not shown in FIG. 1 for clarity) in regions of device layer 230 where proof masses 110 are to be fabricated.


Referring to FIGS. 3D and 3E, fourth mask 366 may be removed from the surface of device layer 230 and from third mask 362. In an embodiment, fourth mask 366 is removed by application of a suitable solvent or by ashing with an oxygen plasma. Removal of fourth mask 366 may expose regions 363 of device layer 230. A second release etch may then be performed, as described above with reference to FIGS. 2D and 2E. Second release etch preferably removes a thickness of material approximately equal to t4 from regions 363, release regions 264, and apertures 272, thus removing all remaining material from release regions 264 (and apertures 272) and forming fourth recesses 370 in regions 363. In an embodiment, the depth of fourth recesses 370 is approximately equal to the depth of third recesses 360, e.g., approximately 10 μm.


Referring to FIGS. 3F and 3G, third mask 362 is removed from the surface of device layer 230, e.g., as described above in reference to first mask 262 of FIGS. 2F and 2G. An optional top substrate 280 may be attached to device layer 230 by, e.g., anodic bonding. Top substrate 280 may include upper sense plate 290 disposed approximately directly over lower sense plate 130. With additional reference to FIG. 1, sensor 100 may include stationary comb fingers 180 having a thickness tS less than a thickness tM of mobile comb fingers 170. In an embodiment, each stationary comb finger 180 is approximately vertically centered with respect to proof mass 110 (and/or mobile comb fingers 170), i.e., the depths of first recesses 360 and second recesses 370 are approximately equal.


Herein, the processes depicted in FIGS. 2A-2G and FIGS. 3A-3G are presented as separate or alternative steps in separate exemplary sequences for the fabrication of sensor 100. However, in an embodiment, both sequences are combined into a single process sequence for sensor 100 having thinned suspension beams 146 and stationary comb fingers 180. Such a combined process sequence may be more efficient and less costly than embodiments in which suspension beams 146 and stationary comb fingers 180 are formed in substantially different sequences. In this embodiment, the step depicted in FIG. 2A may be combined with the step depicted in FIG. 3A, FIG. 2B with FIG. 3B, etc. Additionally, first mask 262 and third mask 362 may be the same, as may second mask 266 and fourth mask 366. Further, the depth of first recesses 260 may be substantially equal to the depth of third recesses 360 (and first recesses 260 and third recesses 360 may be formed substantially simultaneously), and the depth of second recesses 270 may be substantially equal to the depth of fourth recesses 370 (and second recesses 270 and fourth recesses 370 may be formed substantially simultaneously). Hence, the final thickness tB of suspension beams 146 may be substantially equal to the final thickness tS of stationary comb fingers 180.


The terms and expressions employed herein are used as terms and expressions of description and not of limitation, and there is no intention, in the use of such terms and expressions, of excluding any equivalents of the features shown and described or portions thereof. In addition, having described certain embodiments of the invention, it will be apparent to those of ordinary skill in the art that other embodiments incorporating the concepts disclosed herein may be used without departing from the spirit and scope of the invention. Accordingly, the described embodiments are to be considered in all respects as only illustrative and not restrictive.

Claims
  • 1. A method of fabricating a sensor, the method comprising: forming a first recess in a first surface of a first substrate;bonding a portion of the first surface of the first substrate to a second substrate;forming a second recess in a second surface of the first substrate, the first substrate consisting essentially of a single material between the first and second surfaces, and the second recess being disposed over the first recess, thereby forming a suspension beam located between the first and second recesses, the suspension beam suspending a proof mass over the second substrate;forming a third recess in the first surface of the first substrate; andforming a fourth recess in the second surface of the first substrate, thereby forming a stationary comb finger located between the third and fourth recesses and disposed over the second substrate.
  • 2. The method of claim 1, wherein a thickness of the suspension beam is less than a thickness of the proof mass.
  • 3. The method of claim 2, wherein a difference between the thickness of the proof mass and the thickness of the suspension beam is approximately equal to an aggregate depth of the first and second recesses.
  • 4. The method of claim 1, wherein a depth of the first recess is approximately equal to a depth of the second recess.
  • 5. The method of claim 1, wherein a thickness of the stationary comb finger is less than a thickness of a mobile comb finger disposed on an edge of the proof mass.
  • 6. The method of claim 1, wherein a depth of the third recess is approximately equal to a depth of the fourth recess.
  • 7. The method of claim 1, wherein the first and third recesses are formed substantially simultaneously and the second and fourth recesses are formed substantially simultaneously.
US Referenced Citations (217)
Number Name Date Kind
3053095 Koril et al. Sep 1962 A
3251231 Hunt et al. May 1966 A
3370458 Dillon Feb 1968 A
3696429 Tressa Oct 1972 A
3913035 Havens Oct 1975 A
4044305 Oberbeck Aug 1977 A
4122448 Martin Oct 1978 A
4144764 Hartzell, Jr. Mar 1979 A
4155257 Wittke May 1979 A
4234666 Gursky Nov 1980 A
4321500 Paros et al. Mar 1982 A
4336718 Washburn Jun 1982 A
4342227 Petersen et al. Aug 1982 A
4381672 O'Connor et al. May 1983 A
4406992 Kurtz et al. Sep 1983 A
4411741 Janata Oct 1983 A
4414852 McNeill Nov 1983 A
4447753 Ochiai et al. May 1984 A
4468584 Nakamura et al. Aug 1984 A
4478076 Bohrer Oct 1984 A
4478077 Bohrer et al. Oct 1984 A
4483194 Rudolf et al. Nov 1984 A
4484382 Kawashima et al. Nov 1984 A
4490772 Blickstein Dec 1984 A
4495499 Richardson Jan 1985 A
4499778 Westhaver et al. Feb 1985 A
4502042 Wuhrl et al. Feb 1985 A
4522072 Sulouff et al. Jun 1985 A
4524619 Staudte Jun 1985 A
4538461 Juptner et al. Sep 1985 A
4585083 Nishiguchi et al. Apr 1986 A
4590801 Merhav et al. May 1986 A
4592242 Kempas et al. Jun 1986 A
4596158 Strugach Jun 1986 A
4598585 Boxenhorn Jul 1986 A
4600934 Aine et al. Jul 1986 A
4619001 Kane et al. Oct 1986 A
4621925 Masuda et al. Nov 1986 A
4628283 Reynolds Dec 1986 A
4629957 Walters et al. Dec 1986 A
4639690 Lewis Jan 1987 A
4644793 Church et al. Feb 1987 A
4651564 Johnson et al. Mar 1987 A
4653326 Danel et al. Mar 1987 A
4654663 Alsenz et al. Mar 1987 A
4665605 Kempas et al. May 1987 A
4670092 Motamedi Jun 1987 A
4671112 Kimura et al. Jun 1987 A
4674180 Zavracky et al. Jun 1987 A
4674319 Muller et al. Jun 1987 A
4674331 Watson Jun 1987 A
4679434 Stewart Jul 1987 A
4680606 Knutti et al. Jul 1987 A
4699006 Boxenhorn Oct 1987 A
4705659 Bernstein et al. Nov 1987 A
4706374 Murakami Nov 1987 A
4712439 North et al. Dec 1987 A
4727752 Peters Mar 1988 A
4735506 Pavlath Apr 1988 A
4736629 Cole Apr 1988 A
4743789 Puskas May 1988 A
4744248 Stewart May 1988 A
4744249 Stewart May 1988 A
4747312 Herzl May 1988 A
4750364 Kawamura et al. Jun 1988 A
4761743 Wittke Aug 1988 A
4764244 Chitty et al. Aug 1988 A
4776924 Delapierre et al. Oct 1988 A
4783237 Aine et al. Nov 1988 A
4789803 Jacobsen et al. Dec 1988 A
4792676 Hojo et al. Dec 1988 A
4805456 Howe et al. Feb 1989 A
4808948 Patel et al. Feb 1989 A
RE32931 Staudte May 1989 E
4834538 Heeks et al. May 1989 A
4851080 Howe et al. Jul 1989 A
4855544 Glenn Aug 1989 A
4869107 Murakami et al. Sep 1989 A
4882933 Petersen et al. Nov 1989 A
4884446 Ljung Dec 1989 A
4890812 Chechile et al. Jan 1990 A
4893509 MacIver et al. Jan 1990 A
4898032 Voles et al. Feb 1990 A
4899587 Staudte Feb 1990 A
4900971 Kawashima et al. Feb 1990 A
4901586 Blake et al. Feb 1990 A
4916520 Kurashima et al. Apr 1990 A
4922756 Henrion May 1990 A
4929860 Hulsing, II et al. May 1990 A
RE33479 Juptner et al. Dec 1990 E
4981359 Tazartes et al. Jan 1991 A
5001383 Kawashima et al. Mar 1991 A
5006487 Stokes Apr 1991 A
5016072 Greiff May 1991 A
5025346 Tang et al. Jun 1991 A
5038613 Takenaka et al. Aug 1991 A
5090809 Ferrar Feb 1992 A
5094537 Karpinski, Jr. Mar 1992 A
5138883 Paquet et al. Aug 1992 A
5203208 Bernstein Apr 1993 A
5205171 O'Brien et al. Apr 1993 A
5226321 Varnham et al. Jul 1993 A
5233874 Putty et al. Aug 1993 A
5241861 Hulsing, II Sep 1993 A
5349855 Bernstein et al. Sep 1994 A
5392650 O'Brien et al. Feb 1995 A
5458000 Burns et al. Oct 1995 A
5481914 Ward Jan 1996 A
5492596 Cho Feb 1996 A
5496436 Bernstein et al. Mar 1996 A
5500549 Takeuchi et al. Mar 1996 A
5507911 Greiff Apr 1996 A
5581035 Greiff Dec 1996 A
5635639 Greiff et al. Jun 1997 A
5646348 Greiff et al. Jul 1997 A
5659195 Kaiser et al. Aug 1997 A
5726480 Pister Mar 1998 A
5747961 Ward et al. May 1998 A
5757103 Lee et al. May 1998 A
5767405 Bernstein et al. Jun 1998 A
5783973 Weinberg et al. Jul 1998 A
5804087 Lee et al. Sep 1998 A
5869760 Geen Feb 1999 A
5892153 Weinberg et al. Apr 1999 A
5894090 Tang et al. Apr 1999 A
5894091 Kubota et al. Apr 1999 A
5911156 Ward et al. Jun 1999 A
5920012 Pinson Jul 1999 A
5952574 Weinberg et al. Sep 1999 A
5992233 Clark Nov 1999 A
5998906 Jerman et al. Dec 1999 A
6000280 Miller et al. Dec 1999 A
6040625 Ip Mar 2000 A
6064169 Ward et al. May 2000 A
6067858 Clark et al. May 2000 A
6125700 Tsugai et al. Oct 2000 A
6143583 Hays Nov 2000 A
6155115 Ljung Dec 2000 A
6230566 Lee et al. May 2001 B1
6232546 DiMatteo et al. May 2001 B1
6232790 Bryan et al. May 2001 B1
6250156 Seshia et al. Jun 2001 B1
6257059 Weinberg et al. Jul 2001 B1
6263735 Nakatani et al. Jul 2001 B1
6277666 Hays et al. Aug 2001 B1
6296779 Clark et al. Oct 2001 B1
6297069 Zappella et al. Oct 2001 B1
6311556 Lefort et al. Nov 2001 B1
6350983 Kaldor et al. Feb 2002 B1
6388789 Bernstein May 2002 B1
6426538 Knowles Jul 2002 B1
6445195 Ward Sep 2002 B1
6481285 Shkel et al. Nov 2002 B1
6487864 Platt et al. Dec 2002 B1
6498996 Vallot Dec 2002 B1
6516666 Li Feb 2003 B1
6544655 Cabuz et al. Apr 2003 B1
6548321 Sawyer Apr 2003 B1
6550329 Watson Apr 2003 B1
6571630 Weinberg et al. Jun 2003 B1
6577929 Johnson et al. Jun 2003 B2
6582985 Cabuz et al. Jun 2003 B2
6591678 Sakai et al. Jul 2003 B2
6621279 Ward Sep 2003 B2
6639289 Hays Oct 2003 B1
6655190 Grossman et al. Dec 2003 B2
6668111 Tapalian et al. Dec 2003 B2
6674294 Ward Jan 2004 B2
6698287 Kubena et al. Mar 2004 B2
6865944 Glenn et al. Mar 2005 B2
6915693 Kim et al. Jul 2005 B2
6978673 Johnson et al. Dec 2005 B2
7013730 Malametz Mar 2006 B2
7036373 Johnson et al. May 2006 B2
7043985 Ayazi et al. May 2006 B2
7051590 Lemkin et al. May 2006 B1
7172919 Weinberg et al. Feb 2007 B2
7258010 Horning et al. Aug 2007 B2
7287428 Green Oct 2007 B2
7300814 Cunningham et al. Nov 2007 B2
7350415 LaFond Apr 2008 B2
20010001928 Kikuchi et al. May 2001 A1
20010042404 Yazdi et al. Nov 2001 A1
20020008121 Doelle Jan 2002 A1
20020023424 Takamatsu et al. Feb 2002 A1
20020066317 Lin Jun 2002 A1
20020081765 Cabuz et al. Jun 2002 A1
20020093067 Knowles Jul 2002 A1
20020167248 Chua et al. Nov 2002 A1
20020171901 Bernstein Nov 2002 A1
20020178817 Selvakumar et al. Dec 2002 A1
20020184949 Gianchandani et al. Dec 2002 A1
20020190607 Paden et al. Dec 2002 A1
20030034870 Becka et al. Feb 2003 A1
20030036214 Eskridge Feb 2003 A1
20030077876 Sawyer Apr 2003 A1
20030080648 Jerman et al. May 2003 A1
20030106372 Adams et al. Jun 2003 A1
20030107317 Touchberry et al. Jun 2003 A1
20030160021 Platt et al. Aug 2003 A1
20030164042 Valentin Sep 2003 A1
20030167842 Platt Sep 2003 A1
20030183006 Platt et al. Oct 2003 A1
20030196491 Platt Oct 2003 A1
20030200785 Platt Oct 2003 A1
20030200803 Platt Oct 2003 A1
20040035206 Ward et al. Feb 2004 A1
20040132227 Horning et al. Jul 2004 A1
20040180464 Horning et al. Sep 2004 A1
20060201249 Horning et al. Sep 2006 A1
20060283245 Konno et al. Dec 2006 A1
20060283246 Weinberg et al. Dec 2006 A1
20070026614 Choo et al. Feb 2007 A1
20070029629 Yazdi Feb 2007 A1
20070214891 Robert et al. Sep 2007 A1
20070222011 Robert et al. Sep 2007 A1
20070266787 LaFond et al. Nov 2007 A1
Foreign Referenced Citations (11)
Number Date Country
0 280 905 Sep 1988 EP
0 664 438 Jul 1998 EP
1 411 024 Apr 2004 EP
1752734 Feb 2007 EP
1835294 Sep 2007 EP
1840582 Oct 2007 EP
2 183 040 May 1987 GB
WO-96-37784 Nov 1996 WO
WO-00-57194 Sep 2000 WO
WO-01-22094 Mar 2001 WO
WO-2005-028359 May 2005 WO
Related Publications (1)
Number Date Country
20100005884 A1 Jan 2010 US