Isotropic Anisotropic

Slides:



Advertisements
Similar presentations
MICROELECTROMECHANICAL SYSTEMS ( MEMS )
Advertisements

Gyroscopes based on micromechanical systems, MEMS gyroscopes are miniaturized variant of Coriolis vibratory gyros (CVG). Miniaturization is that a vibrating.
A brief history of MEMS fabrication
BASIC SENSORS AND PRINCIPLES. ① Strain gages Measurement of extremely small displacement ① Potentiometers Translational and Rotational displacement ②.
Electronics and Cybernetics 1 Denne forelesningen Membranbaserte piezoresistiv trykksensor (våtetset) Stressfordelingen Piezoresistivitets tensoren ”Vanlig”
MetalMUMPs Process Flow
İsmail Erkin Gönenli Advisor: Zeynep Çelik-Butler Department of Electrical Engineering The University of Texas, Arlington.
Jump to first page 1 Normal stress = Chapter 2 Mechanics of Materials Example: Estimate the normal stress on a shin bone ( 脛骨 ) ATensile stress (+) Compressive.
Micromachining of Silicon and Its Applications in MEMS and Intelligent Sensors Mustafa G. Guvench, Ph.D. University of Southern Maine.
Microelectromechanical Systems (MEMS) An introduction
Bulk Micromachining of Silicon for MEMS Mustafa G. Guvench, Ph.D. University of Southern Maine.
Applications: Angular Rate Sensors (cont’d)
Strain Gages Electrical resistance in material changes when the material is deformed R – Resistance ρ – Resistivity l – Length A – Cross-sectional area.
Applications: CO Gas Sensor
SOIMUMPs Process Flow Keith Miller Foundry Process Engineer.
Bulk MEMS 2013, Part 2
Chang Liu Micro Actuators, Sensors, Systems Group
MEMs Fabrication Alek Mintz 22 April 2015 Abstract
Case Studies in MEMS Case study Technology Transduction Packaging
1 5. Strain and Pressure Sensors Piezoresistivity Applied stress gives the change in resistance  = F/A  =  x/x  R/R (stress) (strain) In the case of.
RF MEMS devices Prof. Dr. Wajiha Shah. OUTLINE  Use of RF MEMS devices in wireless and satellite communication system. 1. MEMS variable capacitor (tuning.
Surface micromachining
1 ME 381R Fall 2003 Micro-Nano Scale Thermal-Fluid Science and Technology Lecture 18: Introduction to MEMS Dr. Li Shi Department of Mechanical Engineering.
Slide # 1 MESA Isolation Source-Drain Contact DEPOSITION Schottky Contact DEPOSITION Bonding Pad DEPOSITION Top Cantilever OUTLINE ETCH BACK POCKET ETCH.
Bulk Micromachining of Silicon for MEMS
ES 176/276 – Section # 2 – 09/19/2011 Brief Overview from Section #1 MEMS = MicroElectroMechanical Systems Micron-scale devices which transduce an environmental.
Surface MEMS 2014 Part 1
Materials Science in MEMS GSA: Brooks A. Gross
Click mouse or hit space bar to advance slides All slides property of Cronos, all rights reserved Silicon Substrate Add nitride.
SEMINAR ON MICRO-ELECTRO-MECHANICAL SYSTEMS (MEMS) A.RADHAKRISHNAN MECHANICAL ENGINEERING, CPT COLLEGE THIRUVANANTHAPURAM PART-1.
1 Absolute Pressure Sensors Z. Celik-Butler, D. Butler and M. Chitteboyina Nanotechnology Research and Teaching Facility University of Texas at Arlington.
IC Process Integration
Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.
Case Studies in MEMS Case study Technology Transduction Packaging Pressure sensor Bulk micromach.Piezoresistive sensing Plastic + bipolar circuitryof diaphragm.
Copyright Prentice-Hall Chapter 29 Fabrication of Microelectromechanical Devices and Systems (MEMS)
© Pearson & GNU Su-Jin Kim MEMS Manufacturing Processes MEMS Devices The MEMS(Microelectromechanical systems) devices can be made through the IC Process:
MEMS devices: How do we make them?
ES050 – Introductory Engineering Design and Innovation Studio 1 ECE Case Study Accelerometers in Interface Design – Part II Prof. Ken McIsaac
EE235 Presentation I CNT Force Sensor Ting-Ta YEN Feb Y. Takei, K. Matsumoto, I. Shimoyama “Force Sensor Using Carbon Nanotubes Directly Synthesized.
ECE Case Study Accelerometers in Interface Design – Part II
Introduction to Prototyping Using PolyMUMPs
ISAT 436 Micro-/Nanofabrication and Applications
Top Down Manufacturing
Surface Micromachining
1 M. Chitteboyina, D. Butler and Z. Celik-Butler, Nanotechnology Research and Teaching Facility University of Texas at Arlington
Are mechanical laws different at small scales? YES! If we scale quantities by a factor ‘S’ Area  S 2 Volume  S 3 Surface tension  SElectrostatic forces.
1 3 MEMS FABRICATION Ken Gilleo PhD ET-Trends LLC 24%
Surface Micromachining Dr. Marc Madou, Fall 2012, UCI Class 10.
Micro/Nanofabrication
MEMS devices: How do we make them? Sandia MEMS Gear chain Hinge Gear within a gear A mechanism.
CMOS VLSI Fabrication.
Are mechanical laws different at small scales? YES! If we scale quantities by a factor ‘S’ Area  S 2 Volume  S 3 Surface tension  SElectrostatic forces.
Claudio Piemonte Firenze, oct RESMDD 04 Simulation, design, and manufacturing tests of single-type column 3D silicon detectors Claudio Piemonte.
MEMS 2016 Part 2 (Chapters 29 & 30)
(Chapters 29 & 30; good to refresh 20 & 21, too)
Micro Electro Mechanical Systems (MEMS) Device Fabrication
7. Surface Micromachining Fall 2013 Prof. Marc Madou MSTB 120
5. Strain and Pressure Sensors
MEMS, Fabrication Cody Laudenbach.
Solid mechanics Define the terms
MEMS TECHNOLOGY By Rogerio Furlan.
Add nitride Silicon Substrate.
Process flow part 2 Develop a basic-level process flow for creating a simple MEMS device State and explain the principles involved in attaining good mask.
Memscap - A publicly traded MEMS company
Micro-Electro-Mechanical-Systems
(2) Incorporation of IC Technology Example 18: Integration of Air-Gap-Capacitor Pressure Sensor and Digital readout (I) Structure It consists of a top.
SILICON MICROMACHINING
BONDING The construction of any complicated mechanical device requires not only the machining of individual components but also the assembly of components.
Chapter 2 Mechanics of Materials
Add nitride Silicon Substrate
Presentation transcript:

Isotropic Anisotropic Bulk micromachining Wet Chemical etching: Masking layer Bulk Si Bulk Si Isotropic Anisotropic

Surface micromachining Carving of layers put down sequentially on the substrate by using selective etching of sacrificial thin films to form free-standing/completely released thin-film microstructures http://www.darpa.mil/mto/mems HF can etch Silicon oxide but does not affect Silicon Release step crucial

MEMS: Foundry services SAMPLES: Sandia Agile MEMS Prototyping, Layout tools, Education and Services (Current process: SUMMIT V) Sandia’s Ultra-planar Multi-level MEMS Technology) - 5 levels of poly-silicon - $10,000 / design MUMPS: Multi-user MEMS processes - Derived from the BSAC processes at U.C. Berkeley - 3-levels of poly-Si

Process steps for fabricating a MEMS device MUMPS: Multi-user MEMS processes > Commercially operated, a repository of processing, design libraries > Standard processing steps, can be custom-designed Poly-MUMPS: Three-layer polysilicon process Metal-MUMPS: Ni electroplating process SOI-MUMPS: Silicon-on-Insulator micromachining process

The CRONOS process for a micro-motor e.g., Synchronous motor Stator Rotor

The CRONOS process for a micro-motor Poly-silicon (POLY): Structural Material Silicon Oxide/PSG (OXIDE): Sacrificial material Silicon Nitride (NITRIDE): for isolation - 8 photo-masks: 8 levels of processing

The cross-sections are depicted in MEMS processing … http://mems.sandia.gov/

Photoresist washed away Photoresist (PR) Photoresist RIE removes POLY0 Photoresist washed away Oxide sacrificial layer deposited by LPCVD PR applied, dimples patterned, and PR washed away (PSG : OXIDE) Oxide patterned and etched, Poly1 deposited

-contd. OXIDE 2 Pattern POLY1 (4th level), OXIDE & POLY etched: RIE Deposit & pattern OXIDE 2, (Level 5) Deposit PR (Level 6) and pattern an ANCHOR contacting POLY 0

- contd. Deposit POLY 2 and OXIDE (PSG) Pattern POLY 2 (7th level) and

STATOR ROTOR STATOR -contd. Deposit and pattern METAL (Level 8) POLY 2 RELEASE structure, OXIDES are sacrificial STATOR ROTOR STATOR

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

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)

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

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

Tensor notation Stress Strain sij eij sij = Cijkl ekl sxx txy txz tyx syy tyz tzx tzy szz sij ≡ exx gxy gxz gyx eyy gyz gzx gzy ezz eij ≡ 4th rank tensor (81 elements) sij = Cijkl ekl From symmetry (no net force in equilibrium) sij = sji  6 independent variables 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 sxx syy szz tyz tzx txy exx eyy ezz gyz gzx gxy ≡ (6 X 6) matrix, 21 independent elements (as, Cij = Cji)

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

Piezoresistivity for Silicon

Piezoresistivity 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 E1 = [1+ p11s1 + p12(s2 + s3)] J1 + p44(t12J2+ t13J3) re re p11 = Π1111 re p12 = Π1122 E2 = [1+ p11s2 + p12(s1 + s3)] J2 + p44(t12J1+ t23J3) re re p44 = 2Π2323 E3 = [1+ p11s3 + p12(s1 + s2)] J3 + p44(t13J1+ t23J2) re

Measurement of Piezoresistance coefficients

Practical Piezoresistance measurements

Slide courtesy: M. Wu

Longitudinal & transverse piezoresistance DR = plsl + ptst l: 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)

Piezoresistive coefficients of Si - decrease as the doping level/temperature increases Type Resistivity p11 p12 p44 Units W-cm 10-11 Pa-1 n-type 11.7 -102.2 53.4 -13.6 p-type 7.8 6.6 -1.1 138.1 C.S. Smith, Phys. Rev. B, vol. 94, pp.42-59, (1954).

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

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

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

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

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

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