1 / 28

Case Studies in MEMS

Case Studies in MEMS. Case study Technology Transduction Packaging. Pressure sensor Bulk micromach. Piezoresistive sensing Plastic + bipolar circuitry of diaphragm deflection

ivana-hebert
Télécharger la présentation

Case Studies in MEMS

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Case Studies in MEMS Case study Technology Transduction Packaging Pressure sensor Bulk micromach. Piezoresistive sensing Plastic + bipolar circuitry of diaphragm deflection Accelerometer Surface micromach. Capacitive detection of Metal can proof of mass motion Electrostatic Surface micromach. Electrostatic torsion of Glass bonded projection displays + XeF2 release suspended tensile beams Catalytic combustible Surface micromach. Resistance change due Custom mount gas sensor to heat of reaction RF switches Surface micromach. Cantilever actuation Glass bonded DNA amplification Bonded etched glass Pressure driven flow Microcapillaries with PCR across T-controlled zones Lab on a chip Bulk & Surface Electrophoresis & Microfluidics micromachining electrowetting & Polymers

  2. A project on the frontier application areas of MEMS/NEMS Required: A written report + Presentation The project should address the following issues: (1) What is new or novel about this application? (2) Is there any new physical principle being used (3) Where is this headed? (commercial potential, offshoot into new areas of engineering …) (4) Most importantly, YOUR ideas for improvement. Presentations (15 minutes/team of two) on May 26 (Thursday) 6:30 – 8 pm

  3. A Piezoresistive Pressure Sensor • Piezoresistance: the variation of electrical resistance with strain • Origin in the deformation of semiconductor energy bands • NOT the same as piezo-electricity • Transduction of stress into voltage • Application: Manifold-Absolute-Pressure (MAP) sensor: Motorola • One of the largest market segments of mechanical MEMS devices

  4. Piezoresistivity Piezoresistive effect is described by a fourth-rank tensor E = re [1 + Π·s] · Jat small strains Electric field Resistivity tensor (2nd rank) Stress Current density

  5. sxx syy szz tyz tzx txy exx eyy ezz gyz gzx gxy sxxtxytxz tyxsyytyz tzxtzyszz exxgxygxz gyxeyygyz gzxgzyezz sij eij ≡ ≡ Tensor notation Stress Strain 4th rank tensor (81 elements) sij = Cijkl ekl From symmetry (no net force in equilibrium) sij = sji  6 independent variables

  6. sxx syy szz tyz tzx txy exx eyy ezz gyz gzx gxy Contracted tensor notation C11 C12 C13 C14 C15 C16 C12 C22 C23 C24 C25 C26 C13 C23 C33 C34 C35 C36 C14 C24 C34 C44 C45 C46 C15 C25 C35 C45 C55 C56 C16 C26 C36 C46 C56 C66 ≡ (6 X 6) matrix, 21 independent elements (as, Cij = Cji)

  7. For cubic materials, e.g. single crystal Silicon, there are only 3 independent constants C11 C12 C12 000 C12 C11 C12 0 0 0 C12 C12 C11 000 0 0 0C44 0 0 0 0 0 0 C44 0 0 0 0 0 0 C44

  8. Piezoresistivity for Silicon

  9. Piezoresistivity E1 = [1+ p11s1 + p12(s2 + s3)] J1 + p44(t12J2+ t13J3) E2 = [1+ p11s2 + p12(s1 + s3)] J2 + p44(t12J1+ t23J3) E3 = [1+ p11s3 + p12(s1 + s2)] J3 + p44(t13J1+ t23J2) re re re Piezoresistive effect is described by a fourth-rank tensor E = re [1 + Π·s] · J Electric field Resistivity tensor (2nd rank) Stress Current density x 1, y2, z 3, [11, 22, 33, 23, 31, 12]  [1, 2, 3, 4, 5, 6] Piezoresistive coefficients rep11 = Π1111 rep12 = Π1122 rep44 = 2Π2323

  10. Measurement of Piezoresistance coefficients

  11. Practical Piezoresistance measurements

  12. Slide courtesy: M. Wu

  13. Longitudinal & transverse piezoresistance DR = plsl + ptstl: longitudinal, t: transverse R Longitudinal & Transverse piezoresistance coefficients • Longitudinal pl Transverse pt • direction direction • (100) p11 (010) p12 • (001) p11 (110) p12 • (111) 1/3 (p11+p12+ 2 p44)(110) 1/3 (p11+2 p12- 2 p44) • (110) 1/2 (p11+p12+ p44) (111) 1/3 (p11+2 p12- p44) • (110) 1/2 (p11+p12+ p44) (001) p44 • (110) 1/2 (p11+p12+ p44) (110) 1/2 (p11 + p12 - p44)

  14. Piezoresistive coefficients of Si - decrease as the doping level/temperature increases C.S. Smith, Phys. Rev. B, vol. 94, pp.42-59, (1954).

  15. Concept of a piezoresistive sensing scheme Max. surface stress Proof Mass Substrate Flexure If piezo-resistor is along [110]: n-type: pl: -31.2 · 10-11 Pa-1, pt: -17.6 · 10-11 Pa-1 p-type: pl: 71.8 · 10-11 Pa-1, pt: -66.3 · 10-11 Pa-1 Transverse Longitudinal - more sensitive - easier to align

  16. R3 R2 + - R1 R4 V DR1 = (pl + npt)sl = (67.6 · 10-11) sl R1 Principle of measurement Diaphragm Poisson ratio, n = 0.06 CROSS-SECTION TOP VIEW DR2 = - (61.7· 10-11) sl R2 R2 WHEATSTONE BRIDGE R3 R1 R4 Vo R1 = R3 = (1+ a1) Ro R2 = R4 = (1 - a2) Ro ai = Σpisi

  17. Support Cantilever Piezoresistors 2 3 wmax Cantilever tip displacement (w) for a point load = 2 d2w x x dx2 1- Lc 3Lc Resistance change due to stress Lc: cantilever length x: distance from support t: thickness x = 3 wmax (Lc - x) Radius of curvature = 1/r = Lc3 [(t/2)/r] = E sl DR = pl sl R Stress = E · Strain

  18. The Motorola MAP sensor http://www.motorola.com/automotive/prod_sensors.html • MAP: Manifold Absolute Pressure • Sensor measures mass airflow into the engine, to control • air-fuel ratio • Uses piezoresistance to measure diaphragm bending with • integrated signal-conditioning and calibration circuitry S. Senturia, page 461, Microsystem design

  19. MAP sensor specifications Diaphragm size 1000 mm X 1000 mm, thickness: 20 mm Pressure range 15 – 250 kPa Power supply 5 V Output current drive up to 1 mA Temperature range -40 oC to 125 oC Mechanical shock (5 – 100) g

  20. Al metallization OXIDE n+ - collector n-epi p-type piezoresistor n+ - Emitter p-base <100> p-Si substrate n+ - buried layer Process flow for MAP sensor • Bipolar (NPN) instead of MOS processing on (100) wafers • uses only one piezo-resistor: Xducer

  21. Pressure sensor fabrication and packaging Piezoresistor element DIAPHRAGM Glass frit/Anodic bond

  22. Wafer bonding • To permanently bond two wafers together • to form patterned 3-dimensional structures • Most commonly used: • > Si-Si fusion bonding • > Anodic bonding • > Eutectic bonding

  23. O – Si – O H H O O – Si – Silicon fusion bonding Surface preparation: clean and hydrate (smooth < 0.5 nm rough.) surfaces Contact: Bring surfaces into contact and apply pressure at one point to initiate pressure wave High temperature anneal: 800 oC < T < 1200 oC Void formation

  24. Anodic Bonding 4 Na+ + 4 e- 4 Na Si + 2 O2-  SiO2 + 4 e- + - Glass Vs Silicon Hot plate 200 oC < T < 500 oC 200 V < Vs < 1000 V Bond strength increases with Vs, Temperature and is better on hydrophilic surfaces Can induce stress

  25. MAP sensor: X-ducer piezoresistor Piezoresistor DIAPHRAGM Anodic bond TOP VIEW piezoresistor Voltage taps

  26. Piezoresistivity E1 = [1+ p11s1 + p12(s2 + s3)] J1 + p44(t12J2+ t13J3) E2 = [1+ p11s2 + p12(s1 + s3)] J2 + p44(t12J1+ t23J3) E3 = [1+ p11s3 + p12(s1 + s2)] J3 + p44(t13J1+ t23J2) re re re Piezoresistive effect is described by a fourth-rank tensor E = re [1 + Π·s] · J Electric field Resistivity tensor (2nd rank) Stress Current density x 1, y2, z 3, [11, 22, 33, 23, 31, 12]  [1, 2, 3, 4, 5, 6] Piezoresistive coefficients rep11 = Π1111 rep12 = Π1122 rep44 = 2Π2323

  27. Other issues in MAP sensor integration • Signal conditioning and calibration, offset compensation • Temperature compensation (as T increases, R increases but p decreases) • Device Noise • Higher order issues (detailed modeling of stress, placement of piezoresistors …)

  28. Piezoresistive strain gauges

More Related