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I SSCC 2 0 1 2 Tutorial Getting I n Touch w ith MEMS: The Electrom echanical I nterface Dr. Aaron Partridge ap@sitime.com SiTime, Corp. February 19, 2012 Overview These slides accompany the 2012 ISSCC Tutorial, Getting In Touch with MEMS:


  1. I SSCC 2 0 1 2 Tutorial Getting I n Touch w ith MEMS: The Electrom echanical I nterface Dr. Aaron Partridge ap@sitime.com SiTime, Corp. February 19, 2012

  2. Overview These slides accompany the 2012 ISSCC Tutorial, Getting In Touch with MEMS: The Electromechanical Interface. The tutorial is written for practicing IC engineers and students. No MEMS background is needed. The goal is to expand the attendee’s potential role from circuit designer to system designer. From “Here is the MEMS device, design the interface circuit.” into “Here is the problem, define an optimal solution.” Aaron Partridge Getting In Touch with MEMS: 2 of 70 The Electromechanical I nterface

  3. Outline o MEMS Materials, Processes, and Example Applications o Electrical Interfaces o Scaling Laws o Packaging is Critical o CMOS Integration o How to Succeed o References Aaron Partridge Getting In Touch with MEMS: 3 of 70 The Electromechanical I nterface

  4. o MEMS Materials, Processes, and Example Applications o Electrical Interfaces o Scaling Laws o Packaging is Critical o CMOS Integration o How to Succeed o References Aaron Partridge Getting In Touch with MEMS: 4 of 70 The Electromechanical I nterface

  5. Materials o Standard Semiconductor Materials n Silicon (single crystal and poly). n Oxide (thermal and deposited). n Nitride. n Alum inum . o Unusual Materials n Gold, various other metals. n Piezoelectrics (AlN mostly). n Plastics (e.g. SU-8). n And then just about anything else. Aaron Partridge Getting In Touch with MEMS: 5 of 70 The Electromechanical I nterface

  6. Processes o Early in MEMS many unusual etches were comm on. o Now standard fab process are preferred when possible. o A few special processes Tuning fork resonator, Bosch 2003 n Bosch etch. n HF vapor etch. n Oxide plasma release. n Xenon difluoride (XeF2) release. o Deep etches are com mon. S. Pourkam ali, F. Ayazi, 2004 Aaron Partridge Getting In Touch with MEMS: 6 of 70 The Electromechanical I nterface

  7. Example Applications o MEMS will find its way into practically every application. o Right now, it is strong in n Automotive (pressure, acceleration, rotation). n Consumer (acceleration, rotation, time). n Industrial and Military (pressure, acceleration). n Medicinal (pressure, biological sensors). o Future hot apps will be n Medical, for diagnostic tools. n Timing, to replace quartz. n RF Filters, switches, etc. n Inertial, to sense motion of all types. Aaron Partridge Getting In Touch with MEMS: 7 of 70 The Electromechanical I nterface

  8. Pressure Sensors Sensimed intraocular pressure sensor in contact lens Aaron Partridge Getting In Touch with MEMS: 8 of 70 The Electromechanical I nterface

  9. Accelerometers & Gyroscopes Freescale accelerometer Aaron Partridge Getting In Touch with MEMS: 9 of 70 The Electromechanical I nterface

  10. Microphones Akustica microphone Aaron Partridge Getting In Touch with MEMS: 10 of 70 The Electromechanical I nterface

  11. Light Modulators & Projectors Two pixels in a TI DLP mirror array Aaron Partridge Getting In Touch with MEMS: 11 of 70 The Electromechanical I nterface

  12. Resonators & Oscillators SiTime oscillator Aaron Partridge Getting In Touch with MEMS: 12 of 70 The Electromechanical I nterface

  13. RF Switches G. Rebeiz UCSD, RF switch Aaron Partridge Getting In Touch with MEMS: 13 of 70 The Electromechanical I nterface

  14. o MEMS Materials, Processes, and Example Applications o Electrical Interfaces o Scaling Laws o Packaging is Critical o CMOS Integration o How to Succeed o References Aaron Partridge Getting In Touch with MEMS: 14 of 70 The Electromechanical I nterface

  15. Capacitive Overview o Capacitive transduction is used in 90% of MEMS interfaces. o Good Points: n Easy to build, no need for special materials. n With the Bosch etch we can make beautiful cap structures. n Can move small to large distances. n Can move in-plane and out-of-plane. n Can sense tiny displacements. o Bad points: n Often will not deliver as much force as desired. n Needs bias voltage, sometimes large. n Output signals can be very small. Aaron Partridge Getting In Touch with MEMS: 15 of 70 The Electromechanical I nterface

  16. Capacitive Drive o How does capacitive drive work? g Take a parallel plate example: ε wh = 2 c F V 2 2 g w Were F= force, � 0 = permittivity, o w= width, h= height, g= capacitive gap, V= voltage. F h o The voltage squared gives attractive forces and drive nonlinearity. V o The gap squared gives displacement nonlinearity. Aaron Partridge Getting In Touch with MEMS: 16 of 70 The Electromechanical I nterface

  17. Capacitive Drive o Want bipolar force? g o We can offset the attraction (pull more and pull less) with DC bias w and AC drive. = ε wh + 2 c F ( V V ) bias drive 2 2 g F h o Set V bias > > V drive and we get a bipolar offset drive. ε wh ≈ c F V V offset bias drive 2 g o As bias is increased and drive is V bias + V drive decreased the linearity improves. Aaron Partridge Getting In Touch with MEMS: 17 of 70 The Electromechanical I nterface

  18. Capacitive Drive o Second option for bipolar is g g differential (pull one way, pull the other), = ε ( ) wh − 2 2 c F V V w dif left right 2 2 g o Offset and differential can be F dif combined, h ε ( ) wh ≈ − c F V V V dif bias right left 2 g o Typical bias and drive are 5V and 0.5V. V left V right Aaron Partridge Getting In Touch with MEMS: 18 of 70 The Electromechanical I nterface

  19. Capacitive Drive o Interdigitated fingers g (combs) can move further and are m ore linear. p ε h = 2 c F N V dif g F c o N is the number of fingers. h o Since p does not effect F c it is linear in displacement. o Pairs of fingers can be V V used differentially to linearize V and push-pull. Aaron Partridge Getting In Touch with MEMS: 19 of 70 The Electromechanical I nterface

  20. Capacitive Sense o For capacitive sensing, we cap C need to think about charge, = , = Q CV i dQ / dt o We all learned that, i = C ( dV / dt ) o But for MEMS sensing we sometimes care more about, = i i V ( dC / dt ) dc Any structures with dC/ dx o And we use a bias V dc , often work. Fingers are common. about 5V but can be 100’s! Aaron Partridge Getting In Touch with MEMS: 20 of 70 The Electromechanical I nterface

  21. Capacitive Sense o What you will need to do as an engineer n Because capacitances are small, sense currents are small. n Design the lowest noise sense amps possible. n If noise is not critical then shrink the MEMS. n Always push the circuits, always simplify the MEMS. o Drive Circuits n For AC system (gyros, vibrometers, oscillators) we need to sense AC current. n For DC systems (accelerometers) we need to modulate a carrier. n Clasic accelerometer drives a differential signal on plates and measures current with a lock-in amplifier. Aaron Partridge Getting In Touch with MEMS: 21 of 70 The Electromechanical I nterface

  22. Capacitive Sense sensor diff A OUT osc phase trim o Differential lock-in sense amp for accelerometers. Aaron Partridge Getting In Touch with MEMS: 22 of 70 The Electromechanical I nterface

  23. Aaron Partridge Getting In Touch with MEMS: 23 of 70 The Electromechanical I nterface M. Dugger, Sandia Labs

  24. Piezoresistive Overview o Transduces strain to resistance. o One of the earliest MEMS interfaces and still important. o Good points: n There is mechanical gain, typically about 30x. n The common sensor structure is a Wheatstone bridge. n Silicon-friendly fabrication, doped resistors work well. o Bad points: n Main problem is temperature sensitivity – moderately doped silicon resistors change about 0.5% per C or more. n 1/ f noise and drift can be problematic. n Only senses, does not drive. Aaron Partridge Getting In Touch with MEMS: 24 of 70 The Electromechanical I nterface

  25. Piezoresistive Sense o A simple idea with may coefficients – strain changes resistivity. R ∆ ρ 6 ∑ = π σ ω ωλ λ ρ λ = 1 ���� = change in resistivity, � � � are o � piezo coefficients, � � � are stress. The � � � form a sparse 6x6 matrix. o For specific cases the equation can be simplified to, ∆ R = π σ effective axial R Aaron Partridge Getting In Touch with MEMS: 25 of 70 The Electromechanical I nterface

  26. Piezoresistive Sense o Typical sense circuits are bridges. n This minimizes the tem perature sensitivity that can swamp signals. n Input offset often vital – use switched caps, diversity, etc. n Often must minimize 1/ f noise – use switched topologies. n Temperature compensation of offset and gain variation is often needed. o See: A.A. Barlian, W-T. Park, J.R. Mallon Jr., A.J. Rastegar, and B.L. Pruitt, “Review: Semiconductor Piezoresistance for Microsystems”, Proceedings of the IEEE, v.97, n.3, March 2009. Aaron Partridge Getting In Touch with MEMS: 26 of 70 The Electromechanical I nterface

  27. Piezoresistive Sense V bias OUT offset gain A trim trim OUT temp sense sensor o Bridge amp with temperature offset and gain correction Aaron Partridge Getting In Touch with MEMS: 27 of 70 The Electromechanical I nterface

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