MEMS piezoelectric longitudinal mode resonator
A longitudinal mode resonator that includes a substrate and a bar that is suspended relative to the substrate. The bar is suspended such that it is free to expand and contract longitudinally in response to the application of an electric field across its thickness. The expansion and contraction of the bar achieves resonance in response to the field having a frequency substantially equal to the fundamental frequency of the bar.
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This application is a divisional of, claims priority to and the benefit of, and incorporates herein by reference in its entirety U.S. patent application Ser. No. 10/631,695, which was filed on Jul. 31, 2003 and which claimed priority to and the benefit of U.S. Provisional Patent Application Ser. No. 60/401,580 filed on Aug. 6, 2002, the contents of which are also incorporated herein by reference in their entirety.
STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH OR DEVELOPMENTThe U.S. Government has certain rights in this invention as provided for by the terms of Contract No. DAAH01-01-C-R204 awarded by the United States Army.
TECHNICAL FIELDThe invention relates generally to the field of micro-electro-mechanical systems (MEMS). In particular, the invention relates to piezoelectric MEMS resonators.
BACKGROUND OF THE INVENTIONResonators are traditionally employed as components, in among other things, filters and oscillators. Resonators have gained greater importance lately with the growth of the mobile communications technology and the increasing clock speed of computers. Mobile devices require small precision filters, and computer clocks require oscillators capable of error-free high frequency oscillation. Typical resonator applications require resonators to demonstrate Q values higher than one thousand at an impedance load of approximately 50Ω, be compatible with common voltage ranges of typical integrated circuits, and to resonate at frequencies near or above 1 GHz.
Conventional resonators include, for example, surface acoustic wave (SAW) resonators, fundamental mode thin film resonators (TFRs), flexural mode MEMS beam resonators, guided electromagnetic wave structures, lumped element inductors and capacitors, thin film bulk acoustic resonators (TFBARs), overmoded bulk crystals, and solidly mounted resonators (SMRs). These filters suffer from a variety of shortcomings, for example many are too large for placement onto an integrated circuit, operate in an unsatisfactorily small frequency range, require too high a voltage for operation, and/or cannot achieve a sufficiently high Quality (Q) level with a 50Ω load. Q is a measure of the energy efficiency of a filter and also is a measure of the sharpness of the filter's frequency response, i.e., a high Q filter passes a narrower band of frequencies than a lower Q filter.
Many traditional resonators are too large to incorporate one or more resonators onto an integrated circuit. For example, thin-film resonators (TFRs) commonly have a footprint on the order of hundreds of microns. Surface acoustic wave (SAW) resonators are typically even larger, in some cases requiring substrates as large several centimeters or inches to exhibit desirable performance characteristics.
Several traditional resonators operate in an undesirably limited frequency range. MEMS flexural mode beam resonators typically do not operate satisfactorily in the Ultra-High Frequency range. Similarly, TFBARs and SMRs are difficult to make with center frequencies much below 1 GHz since film stress becomes an issue as the film thickness is increased. Furthermore, with most film based resonators, multiple resonators with differing frequencies cannot be placed on a single integrated circuit because the film thickness is typically uniform across a substrate.
Many MEMS flexural mode beam resonators also suffer from requiring activation voltages that make the resonators difficult to integrate in standard integrated circuits. MEMS flexural mode beam resonators are commonly actuated capacitively, in some cases requiring as much a 50V to achieve resonance.
Many conventional resonators do not exhibit high enough Q levels with a 50Ω load. Typical lumped element inductors, SMRs, and many TFBARs fail to meet the desired Q level of 1000 in response to operating with a 50Ω load. MEMS flexural mode beam resonators can operate with higher Q levels, but usually require operation in a vacuum to do so.
SUMMARY OF THE INVENTIONThe invention overcomes the above discussed shortcomings in conventional resonators, by in one embodiment, providing a micron scale MEMS longitudinal mode resonator that can be readily incorporated into an integrated circuit. According to another advantage, the invention provides resonators that are small enough to incorporate into large resonator arrays, which in turn may be incorporated onto a single substrate. Embodiments of the invention can thus be used to construct bandpass filters around multiple frequencies, and specifically Rx/Tx filters onto a single integrated circuit substrate. In addition, resonators designed in accordance with the invention can operate across a large frequency range, from at least as low as about 150 MHz up to at least around 1.6 GHz. Embodiments of the invention can also be easily integrated into many common integrated circuit designs because embodiments exhibit limited temperature sensitivity and Q levels of over 1000 while operating with an impedance compatible with a 50Ω circuit.
In one aspect, the invention provides a longitudinal mode resonator that includes a substrate and a bar (constructed of a piezoelectric material such as Aluminum Nitride in some embodiments) that is suspended relative to the substrate. For example, in one configuration, two flexural supports suspend the bar over a cavity defined in the substrate. In another configuration, the flexural supports suspend the bar over a substantially flat substrate via insulating mounting pads. In an alternative configuration, a support located substantially beneath the center of the bar supports the bar relative to the substrate. In one such configuration, the support suspends the bar into a cavity defined in a second substrate.
Preferably, regardless of the suspension approach, the bar is suspended such that it is free to expand and contract longitudinally in response to the application of an electric field across its thickness. The expansion and contraction of the bar achieves resonance in response to the field having a frequency substantially equal to the fundamental frequency of the bar. The fundamental frequency of the bar is a function of the bar's length, providing the advantage that a manufacturer can change the frequency of a resonator built according to an embodiment of the invention, post-production, by laser trimming the resonator's bar.
In one embodiment, an input electrode and an output electrode are disposed on first and second surfaces of the bar of the resonator. In the single support configuration described above, the output electrode is disposed in the bottom of the cavity of the second substrate. In some configurations, the longitudinal mode resonator also includes an electrical signal input in electrical communication with the input electrode for providing an electrical signal input to the input electrode.
A further aspect of the invention relates to a method of fabricating a MEMS piezoelectric resonator. The fabrication method includes forming a stack of layers of materials, including at least one piezoelectric material layer, on a substrate. In one embodiment the stack includes a first metal electrode layer, a piezoelectric material layer, and second metal electrode layer. In another embodiment, the stack also includes an insulating layer.
The frequency of the resonator is then set by applying a pattern mask to the top of the stack. A plurality of the layers of the stack are then etched using one or more etching chemicals or techniques. Illustrative etching techniques include reactive ion etching and wet etching. Depending on the materials selected for the stack, one etching chemical or technique may etch more than one layer at a time, reducing the number of etches needed to produce the resonator. In some embodiments, further etching steps can be used to create additional features in individual layers. Such features include current stops and insulating pads. By stacking the layers and etching the common features of the stack first, some additional features can be defined without the need for later realignment.
In another aspect of the invention, embodiments of the longitudinal mode resonators described above are combined into a multi-frequency filter. The multi-frequency filter includes a substrate, an input terminal for receiving an alternating signal, and a first and second resonator. The first resonator includes a first bar having a first length that is suspended relative to the substrate such that the first bar is free to expand and contract longitudinally in response to the application of an electrical field across the first bar's thickness. The first bar achieves resonance in response to the application of an electric field having a frequency that substantially matches the fundamental frequency of the first bar. The multi-frequency filter's second resonator includes a second bar having a second length that is suspended relative to the substrate such that the second bar is free to expand and contract longitudinally in response to the application of an electrical field across the second bar's thickness. The second bar achieves resonance in response to the application of an electric field having a frequency that substantially matches the fundamental frequency of the second bar.
The multi-frequency filter also includes a multiplexer that is in electrical communication with the input terminal, the first resonator, and the second resonator. The multiplexer communicates the alternating signal to at least one of the first resonator and the second resonator. An output terminal is provided that is in communication with the first resonator and the second resonator to receive the filtered alternating signal. In other embodiments, the multi-frequency filter includes a number of additional resonators (up to as many as desired on a single chip) that also are communication with the multiplexer.
In another aspect of the invention, embodiments of the longitudinal mode resonators described above are combined into a multi-frequency oscillator. The multi-frequency oscillator includes a substrate, a nonlinear feedback element, such as an amplifier, for providing a signal, and a first and second resonator. The first resonator includes a first bar having a first length that is suspended relative to the substrate such that the first bar is free to expand and contract longitudinally in response to the application of an electrical field across the first bar's thickness. The first bar achieves resonance in response to the application of an electric field having a frequency that substantially matches the fundamental frequency of the first bar. The multi-frequency oscillator's second resonator includes a second bar having a second length that is suspended relative to the substrate such that the second bar is free to expand and contract longitudinally in response to the application of an electrical field across the second bar's thickness. The second bar achieves resonance in response to the application of an electric field having a frequency that substantially matches the fundamental frequency of the second bar.
The multi-frequency oscillator also includes a multiplexer that is in electrical communication with the input terminal, the first resonator, and the second resonator. The multiplexer communicates the signal to at least one of the first resonator and the second resonator. An output terminal is provided that is in communication with the first resonator and the second resonator to receive the oscillated signal. In other embodiments, the multi-frequency oscillator includes a number of additional resonators (up to as many as desired for a single integrated circuit) that also are in communication with the multiplexer and output terminal.
Other aspects and advantages of the invention will become apparent from the following detailed description, taken in conjunction with the accompanying drawings, illustrating the principles of the invention by way of example only.
BRIEF DESCRIPTION OF THE DRAWINGSThe foregoing and other objects, features, and advantages of the invention, as well as the invention itself, will be more fully understood from the following description and accompanying drawings. In the drawings, like reference characters generally refer to the same parts through the different views. The drawings are not necessarily to scale but rather illustrate the principles of the invention.
As shown in the drawings for the purposes of illustration, the invention may be embodied, for example, as a MEMS longitudinal mode resonator, a multi-frequency oscillator circuit utilizing more than one MEMS longitudinal mode resonator, and/or a multi-frequency filter utilizing more than one MEMS longitudinal mode resonator.
In the illustrative embodiment, the flexural supports 102 and 104 and the bar 106 are about 0.5 μm thick and formed from a single piezoelectric material, such as aluminum nitride. Piezoelectric materials deform in the presence of a voltage and similarly produce a voltage across the material if the material is deformed. The characteristic arises from an uneven distribution of charge within the material. The resonator 100 capitalizes upon this characteristic of piezoelectric materials to excite the bar 106 into resonance.
More particularly, the electrode 108 is an input electrode. The other electrode 110 is an output electrode. According to the illustrative embodiment, the input electrode 108 is made of nickel and the output electrode 110 is made of molybdenum. The choice of which electrode is used for input and which electrode is used for output is preferably interchangeable, depending on the layout of the remainder of the circuit into which the resonator is integrated. The metals used for the electrodes 108 and 110 differ for fabrication purposes such that the electrodes 108 and 110 can be selectively etched using different etching chemicals. In other fabrication processes, the electrodes 108 and 110 are constructed of the same metal.
In operation, an alternating electrical signal is applied to the input electrode 108. The alternating electrical signal generates an electrical field between the input electrode 108 and the output electrode 110 through the bar 106. The electrodes 108 and 110 may appear to cover either side of the entire resonator 100, however, current stops 116 and 118 are preferably etched through the input electrode 108 and through the output electrode 110, respectively, such that electrode material in electrical communication with other parts of the device is only located on one side of each flexure 104 and 106. As a result, predominately only along the bar 106 is there electrode material on opposing sides of the resonator 100 that is in communication with other parts of the device. The remaining electrode materials 111 and 113 are an artifact of the fabrication process (see below for more detail on one illustrative fabrication process).
As a result of the bar 106 being constructed of a piezoelectric material, in response to the electrical field being across the bar 106, the bar 106 either expands or contracts depending upon the field. While the bar expands and contracts to varying degrees across its entirety in all directions, the bar expands and contracts predominately at its ends in a longitudinal direction 117 (i.e. in a longitudinal mode) as a result of the shape of the bar and the symmetrical application of the field across its thickness. The expansion and contraction is accompanied by a rearrangement of the charge distribution within the bar 106 resulting in an output current flowing through the output electrode, 110. In response to the frequency of the electrical signal substantially matching the fundamental frequency (f0) of the bar 106, the bar 106 achieves resonance in its longitudinal mode, and the output current generated by the expansion and contraction has a frequency closely resembling the frequency of the electrical field. Illustratively, resonance can also be achieved at higher harmonics. The induced piezoelectric current acts to pass the electrical signal through the device, whereas non-resonance inducing signals are damped out by irregularly induced piezoelectric current. In some illustrative embodiments, the device exhibits similar response characteristics to a simple Resistor, Inductor, Capacitor (RLC) circuit.
The fundamental frequency (f0) of the bar 106 is dictated by the length (L) 115 of the bar
The modulus and density are constants associated with the material from which the bar 106 is constructed. As a result, resonators with different frequencies can be designed by changing the length L 115 of the bar. For example, a 6 μm long bar has a center frequency of approximately 780 MHz and a 5 μm long bar has a center frequency of about 1 GHz.
Devices built according to the invention also exhibit sufficiently high Q values for use in many common resonator applications. As mentioned above, Q reflects the level of energy lost by the device in relation to the energy input and the sharpness of the device's frequency response. Q levels greater than 1,000 are generally desired for many applications. The use of mechanical resonance, longitudinal resonance, and piezoelectric materials reduces thermo-elastic energy loss, yielding Q values in excess of 10,000.
The resonator 100 is attached to a substrate 114, typically made of a semiconductor, such as Silicon, Silicon Germanium, or Gallium Arsenide. The selection of the substrate material is based partially on the fabrication process so that the material of the substrate 114 responds appropriately to the various etches employed. The substrate 114 defines a cavity 112 in its surface over which the flexural supports 102 and 104 suspend the bar 106. The dimensions of the cavity 112 preferably exceed that of the bar 106 at its peak expansion 120. The cavity 112 enables the bar 106 to expand and contract without causing any friction with the substrate 114.
In one embodiment, the capacitive plate 226 is disposed at the bottom of a cavity 212′ in a second substrate 214′. The resonator 200 is then inverted and suspended in the cavity 212′ from the support 222.
The first step 302 is to form a stack 430 (see
Next, a pattern mask is applied to the top of the stack 430 (step 303), and the metal electrode layers 436 and 440 and the piezoelectric material layer 438 are patterned using a series of etches to create the rough form 442 of the resonator 400 (step 304) (see
In step 306, the second metal electrode layer 440 is chemically etched to create a first current stop 416 (see
In step 308, the first metal electrode layer 436 is chemically etched to create the second current stop 418 (see
In step 310, the insulating layer 434 is etched away such that the insulating material beneath the bar 406 and the flexural supports 402 and 404 is removed, and insulating material remains beneath the mounting pads 444 and 446 to form the insulating pads 426 and 428 (see
Sample resonators built using the fabrication process 300 have bars 406 ranging from about 3 microns to about 10 microns in length, yielding fundamental frequencies ranging from about 500 MHz to about 1.6 GHz. The flexural supports 402 and 404 range in length from about 5 microns to about 29 microns and have widths ranging from about 1 micron to about 3 microns.
The receiver 602, in one illustrative embodiment, includes an antenna. The receiver 602 passes the input signal to the multiplexer 604. The multiplexer 604, in response to the control signals 608 from the controller 605, directs the input signal to one or more of the resonators 606a-606n to selectively filter the input signal. The small size of the MEMS longitudinal mode resonators 606a-606n enables one to build a single integrated circuit incorporating multiple filter elements.
A similar integrated circuit can be used to design a multi-frequency oscillator according to another illustrative embodiment of the invention. The oscillator is created by substituting a nonlinear feedback element, such as an amplifier, in place of the receiver 602. A user can then, by switching the multiplexer via the control signals 608, direct the electrical signal from the nonlinear feedback element to different resonators 606a-606n, to create an output signal having different frequencies.
One skilled in the art will realize the invention may be embodied in other specific forms without departing from the spirit or essential characteristics thereof. The foregoing embodiments are therefore to be considered in all respects illustrative rather than limiting of the invention. The scope of the invention is not limited to just the foregoing description.
Claims
1. A method of fabricating a MEMS piezoelectric resonator having a predetermined resonant frequency, the method comprising the steps of:
- forming a stack of layers on a substrate, the stack having a top layer and comprising at least one piezoelectric material layer;
- setting the predetermined frequency of the resonator by selecting a pattern mask having a length that dictates the frequency, and applying the mask to the top layer of the stack; and
- etching a plurality of layers of the stack based on the pattern mask, beginning from the top, to shape the resonator.
2. The method of claim 1 wherein the stack comprises:
- a first metal electrode layer;
- a piezoelectric bar layer; and
- a second metal electrode layer.
3. The method of claim 2 wherein the stack further comprises an insulating layer.
4. The method of claim 2 further comprising applying an etchant to space at least a part of the stack from the substrate.
5. The method of claim 1 wherein after the layers of the stack are etched, the method further comprises etching individual layers of the stack.
6. The method of claim 1 further comprising, after the layers of the stack are etched, etching individual layers of the stack to define at least one current stop in one of the first and second metal electrode layers.
7. The method of claim 6 wherein the step of etching individual layers of the stack to form a current stop in one of the first and second metal electrode layers further comprises applying a voltage to one of the first and second metal electrodes.
8. The method of claim 1 further comprising, after the layers of the stack are etched:
- etching the first and second metal electrode layers to form at least one current stop and one undesired current stop; and
- applying a conducting patch to fill the undesired current stop.
Type: Application
Filed: Oct 19, 2005
Publication Date: Oct 18, 2007
Applicant: The Charles Stark Draper Laboratory, Inc. (Cambridge, MA)
Inventors: Amy Duwel (Cambridge, MA), David Carter (Maynard, MA), Mark Mescher (West Newton, MA), Mathew Varghese (Arlington, MA), Bernard Antkowiak (Sutton, MA), Marc Weinberg (Needham, MA)
Application Number: 11/253,451
International Classification: H04R 17/00 (20060101);