EE C245 - ME C218 Introduction to MEMS Design Fall Today s Lecture
|
|
- Mitchell Hicks
- 5 years ago
- Views:
Transcription
1 EE 45 ME 8 ntroduction to MEMS Design Fall 003 Roger Howe and Thara Srinivasan Lecture 6 Micromechanical Resonators EE 45 ME 8 Fall 003 Lecture 6 Today s Lecture ircuit models for micromechanical resonators Microresonator oscillators: sustaining amplifiers, amplitude limiters, and noise Resonant inertial sensors: accelerometers and gyroscopes EE 45 ME 8 Fall 003 Lecture 6
2 Reading/Reference List. T.. Nguyen, h.d. Thesis, Dept. of EES, U Berkeley, 994. T. A. Roessig, R. T. Howe, A.. isano, and J. H. Smith, Surfacemicromachined resonant accelerometer, Transducers 97, hicago, ll., June 69, 997, pp A. A. Seshia, R. T. Howe, and S. Montague, An integrated microelectromechanical resonantoutput gyroscope, EEE MEMS 00, Las egas, Nevada, January 00. net lecture. T.. Nguyen, Transceiver frontend architectures using vibrating micromechanical signal processors, Topical Meeting on Silicon Monolithic ntegrated ircuits in RF Systems, Sept. 4, 00, pp. 33. J. Wang, Z. Ren, and. T.. Nguyen, Selfaligned.4 GHz vibrating radialmode disk resonator, Transducers 03, Boston, Mass., June 8, 003, pp B. Bircumshaw, et al, The radial bulk annular resonator: towards a 50Ω RF MEMS filter, Transducers 03, Boston, Mass., June 8, 003. M. U. Demirci, M. A. Abdelmoneum, and. T.. Nguyen, Mechanically cornercoupled square microresonator array for reduced series motional resistance, Transducers 03, Boston, Mass., June 8, 003, pp Kaaakari, et al, Squareetensional mode singlecrystal silicon micromechanical RFresonator, Transducers 03, Boston, Mass., June 8, 003, pp EE 45 ME 8 Fall 003 Lecture 6 3 ombdrive Lateral Resonator Anchor connects ground plane and resonator Typical bias: O 0 D voltage across drive and sense electrodes to resonator EE 45 ME 8 Fall 003 Lecture 6. T.. Nguyen, h.d. Thesis, EES Dept., U Berkeley, 994 4
3 The Lateral Resonator as a Twoort EE 45 ME 8 Fall 003 Lecture 6. T.. Nguyen, h.d. Thesis, EES Dept., U Berkeley, nput urrent nput current i t is the derivative of the charge q v D dv i t v dt d dt D D The capacitance has a D component and a timevarying component due to the motion of the structure t o m m t t linearized case t Substitute to find the input current: vd t v t v t dv dv i t o m v dt dt t t EE 45 ME 8 Fall 003 Lecture 6 i t 6 3
4 4 7 EE 45 ME 8 Fall 003 Lecture 6 nput Motional Admittance Y w hasor form of the motional current i : X Y The displacementtovoltage ratio can be reepressed in terms of the drive force F d The input motional admittance inverse of impedance is the ratio of the phasor motional current to the ac drive voltage: X F F X Y d d F F X Y d d 8 EE 45 ME 8 Fall 003 Lecture 6 nput Admittance ont. The electrostatic force component at the drive frequency is: t v t v t f D d, The mechanical response of the resonator is Lecture 9: F d o o d Q k F X / / The input admittance is: Q k o o / / o o Q k / /
5 Series LR Admittance The current through an LR branch is: L / o R o L R Match terms in motional admittance find equivalent elements EE 45 ME 8 Fall 003 Lecture 6 9 Equivalent ircuit for nput ort A series LR circuit results in the identical epression find equivalent values L,, and R m L η η k km R η Qη electromechanical coupling coefficient o L R At resonance, the impedances of the inductance and the capacitance cancel out R EE 45 ME 8 Fall 003 Lecture 6 0 5
6 6 EE 45 ME 8 Fall 003 Lecture 6 Output ort Model onsider first the current due to driving the input set v 0 t t t i n phasor form, / / Q k X o o and are related by the forward current gain φ : φ model by a currentcontrolled current source EE 45 ME 8 Fall 003 Lecture 6 Twoort Equivalent ircuit v 0 L R o φ 0
7 omplete Twoort Model L L o φ φ o R R Symmetry implies that modeling can be done from port, with port shorted superimpose the two models EE 45 ME 8 Fall 003 Lecture 6 3 Equivalent ircuit for Symmetrical Resonator f f. T.. Nguyen, h.d., U Berkeley, 994 EE 45 ME 8 Fall 003 Lecture 6 4 7
8 455 khz ombdrive Resonator alues L assumes vacuum not small huge! mindboggling! EE 45 ME 8 Fall 003 Lecture 6. T.. Nguyen, h.d., U Berkeley, DoubleEnded Tuning Fork Resonators i 0 urrent through structure more resistance decreases Q more feedthroughto substrate EE 45 ME 8 Fall 003 Lecture 6 T. Roessig, h.d.,me, U Berkeley,
9 deal Tuning Fork Twoort Response hase change of 80 o at resonance pins the frequency, with drifts in the feedback amplifier having little effect Response assumes no feedthroughcapacitance between input and output ports EE 45 ME 8 Fall 003 Lecture 6 T. Roessig, h.d.,me, U Berkeley, Tuning Fork Response with apacitive Feedthrough f Feedthroughcapacitance results in a null in the amplitude response and an added sense current which increases with frequency and which can obscure the resonance entirely! R int drive v d int f R eq L eq eq o o structure node EE 45 ME 8 Fall 003 Lecture 6 R int int i s Net lecture: f and its control sense T. Roessig, h.d.,me, U Berkeley,
10 Microresonator Oscillator EE 45 ME 8 Fall 003 Lecture 6. T.. Nguyen and R. T. Howe, EEE J. SolidState ircuits, 34, urrenttooltage or Transresistance Amplifier R f i in i 0 v out R f i in The feedback resistor can be implemented using a MOSFET biased in the triode region EE 45 ME 8 Fall 003 Lecture 6 0 0
11 Microresonator Oscillator Schematic Transresistance amplifier: M 3 implements a variable resistance R f M M implement a simple inverting amplifier M 6 M 7 implement a second amplifying stage EE 45 ME 8 Fall 003 Lecture 6. T.. Nguyen and R. T. Howe, EEE J. SolidState ircuits, 34, ntegrated 6.5 khz Microresonator Oscillator MOS with tungsten metallization olysi lateral resonator. T.. Nguyen and R. T. Howe, EEE J. SolidState ircuits, 34, EE 45 ME 8 Fall 003 Lecture 6 Erratic chaotic behavior observed for high D biases in this and other MEMS oscillators was later eplained by Kim Turner h.d. ornell, 999, now USB
12 ierce Oscillator Schematic crystal doubleended tuning fork Advantage over transr configuration: capacitive impedances determine loop gain lower noise, higher gain EE 45 ME 8 Fall 003 Lecture 6 A. A. Seshia, et al, MSM0, San Juan, uerto Rico 3 TuningFork Oscillator Neararrier Spectrum ierce Topology output power dbc/hz Measured rmsnoise thermal electronic noise A. A. Seshia, et al, EEE MEMS0. EE 45 ME 8 Fall 003 Lecture 6 frequency 0 5 Hz 4
13 Differential Resonant Accelerometer nertial force is coupled from a proof mass through a leverage system to two DETF oscillators in a pushpull manner tension compression EE 45 ME 8 Fall 003 Lecture 6 T. Roessig, h.d.,me, U Berkeley, Leverage Mechanism DETF oscillators are etremely stiff to forces along their length, which makes mechanical amplification feasible n the ideal case of a perfect pivot, Archimedes F out / F in r in / r out EE 45 ME 8 Fall 003 Lecture 6 T. Roessig, h.d.,me, U Berkeley,
14 Resonant Accelerometer erformance Fractional RA measures instability of an oscillator as a function of integration time. RA min at τ sec for 70 khz DETF oscillators f min Hz. Sensitivity 45 Hz/g a min 90 µg EE 45 ME 8 Fall 003 Lecture 6 T. Roessig, h.d.,me, U Berkeley, ResonantOutput Rate Gyroscope frame suspension outer frame direction of motion tuning fork oscillator proof mass oscillator lever arm tuning fork oscillator F c Ω z z fied free y drive fleure EE 45 ME 8 Fall 003 Lecture 6 sense direction A. A. Seshia, h.d. Thesis EES Dept., U Berkeley May
15 ResonantOutput Gyro: Mechanical Element reference resonator proof mass fleure tuning fork force sensor tuning fork force sensor proof mass error correction outer frame EE 45 ME 8 Fall 003 Lecture 6 selftest electrodes lever arm A. A. Seshia, et al, EEE MEMS0. 9 ResonantOutput Gyroscope Die Shot Tuning Fork Drive Electronics roof Mass Drive Electronics Mechanical Structure 4.5 mm EE 45 ME 8 Fall 003 Lecture 6 z y A. A. Seshia, et al, EEE MEMS0. Sandia MEMS MEMSfirst process 30 5
16 Oscillator output power dbm Sideband Modulation by oriolis Force DETF oscillator output oriolis offset Nominal peak Frequency 0 5 Hz oriolis offset EE 45 ME 8 Fall 003 Lecture 6 sideband output in presence of an applied deg/sec rotation rate at 6 Hz. Output sideband power dbµ Output sideband power dbµ Rotation rate signal Offset Frequency offset from carrier Hz A. A. Seshia, et al, EEE MEMS0. sideband output in the absence of rotation Frequency offset from carrier Hz 3 6
EE C245 - ME C218 Introduction to MEMS Design Fall Today s Lecture
EE 45 ME 8 Introduction to MEMS Design Fall 003 Roger Howe and Thara Srinivasan Lecture 6 Micromechanical Resonators I Today s Lecture ircuit models for micromechanical resonators Microresonator oscillators:
More informationPROBLEM SET #7. EEC247B / ME C218 INTRODUCTION TO MEMS DESIGN SPRING 2015 C. Nguyen. Issued: Monday, April 27, 2015
Issued: Monday, April 27, 2015 PROBLEM SET #7 Due (at 9 a.m.): Friday, May 8, 2015, in the EE C247B HW box near 125 Cory. Gyroscopes are inertial sensors that measure rotation rate, which is an extremely
More informationSurface Micromachining
Surface Micromachining An IC-Compatible Sensor Technology Bernhard E. Boser Berkeley Sensor & Actuator Center Dept. of Electrical Engineering and Computer Sciences University of California, Berkeley Sensor
More informationMechanical Spectrum Analyzer in Silicon using Micromachined Accelerometers with Time-Varying Electrostatic Feedback
IMTC 2003 Instrumentation and Measurement Technology Conference Vail, CO, USA, 20-22 May 2003 Mechanical Spectrum Analyzer in Silicon using Micromachined Accelerometers with Time-Varying Electrostatic
More informationAN INTEGRATED MICROELECTROMECHANICAL RESONANT OUTPUT GYROSCOPE
In Proceedings, 15th IEEE Micro Electro Mechanical Sstems Conference, Las Vegas, NV, Jan. 0-4 00. AN INTEGRATED MICROELECTROMECHANICAL RESONANT OUTPUT GYROSCOPE Ashwin A. Seshia *, Roger T. Howe * and
More informationDigitally Tuned Low Power Gyroscope
Digitally Tuned Low Power Gyroscope Bernhard E. Boser & Chinwuba Ezekwe Berkeley Sensor & Actuator Center Dept. of Electrical Engineering and Computer Sciences University of California, Berkeley B. Boser
More informationLecture 10: Accelerometers (Part I)
Lecture 0: Accelerometers (Part I) ADXL 50 (Formerly the original ADXL 50) ENE 5400, Spring 2004 Outline Performance analysis Capacitive sensing Circuit architectures Circuit techniques for non-ideality
More informationEE C245 ME C218 Introduction to MEMS Design
EE C45 ME C18 Introduction to MEMS Design Fall 008 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 9470 Lecture 7: Noise &
More informationRF Micro/Nano Resonators for Signal Processing
RF Micro/Nano Resonators for Signal Processing Roger T. Howe Depts. of EECS and ME Berkeley Sensor & Actuator Center University of California at Berkeley Outline FBARs vs. lateral bulk resonators Electrical
More informationEE C245 ME C218 Introduction to MEMS Design Fall 2007
EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 1: Definition
More informationEE C245 ME C218 Introduction to MEMS Design
EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 21: Gyros
More informationINF 5490 RF MEMS. LN10: Micromechanical filters. Spring 2012, Oddvar Søråsen Department of Informatics, UoO
INF 5490 RF MEMS LN10: Micromechanical filters Spring 2012, Oddvar Søråsen Department of Informatics, UoO 1 Today s lecture Properties of mechanical filters Visualization and working principle Modeling
More informationReference Diagram IDG-300. Coriolis Sense. Low-Pass Sensor. Coriolis Sense. Demodulator Y-RATE OUT YAGC R LPY C LPy ±10% EEPROM TRIM.
FEATURES Integrated X- and Y-axis gyro on a single chip Factory trimmed full scale range of ±500 /sec Integrated low-pass filters High vibration rejection over a wide frequency range High cross-axis isolation
More informationThe Design of 2.4GHz Bipolar Oscillator by Using the Method of Negative Resistance Cheng Sin Hang Tony Sept. 14, 2001
The Design of 2.4GHz Bipolar Oscillator by Using the Method of Negative Resistance Cheng Sin Hang Tony Sept. 14, 2001 Introduction In this application note, the design on a 2.4GHz bipolar oscillator by
More informationEE C245 ME C218 Introduction to MEMS Design
EE C245 ME C218 Introduction to MEMS Design Fall 2008 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 1: Definition
More informationMicromechanical Circuits for Wireless Communications
Micromechanical Circuits for Wireless Communications Clark T.-C. Nguyen Center for Integrated Microsystems Dept. of Electrical Engineering and Computer Science University of Michigan Ann Arbor, Michigan
More informationINF 5490 RF MEMS. L12: Micromechanical filters. S2008, Oddvar Søråsen Department of Informatics, UoO
INF 5490 RF MEMS L12: Micromechanical filters S2008, Oddvar Søråsen Department of Informatics, UoO 1 Today s lecture Properties of mechanical filters Visualization and working principle Design, modeling
More informationMEMS Reference Oscillators. EECS 242B Fall 2014 Prof. Ali M. Niknejad
MEMS Reference Oscillators EECS 242B Fall 2014 Prof. Ali M. Niknejad Why replace XTAL Resonators? XTAL resonators have excellent performance in terms of quality factor (Q ~ 100,000), temperature stability
More informationIntegrated Dual-Axis Gyro IDG-1215
Integrated Dual-Axis Gyro FEATURES Integrated X- and Y-axis gyros on a single chip ±67 /s full-scale range 15m/ /s sensitivity Integrated amplifiers and low-pass filter Auto Zero function Integrated reset
More informationIntroduction to Microeletromechanical Systems (MEMS) Lecture 12 Topics. MEMS Overview
Introduction to Microeletromechanical Systems (MEMS) Lecture 2 Topics MEMS for Wireless Communication Components for Wireless Communication Mechanical/Electrical Systems Mechanical Resonators o Quality
More informationReconfigurable 4-Frequency CMOS Oscillator Based on AlN Contour-Mode MEMS Resonators
From the SelectedWorks of Chengjie Zuo October, 2010 Reconfigurable 4-Frequency CMOS Oscillator Based on AlN Contour-Mode MEMS Resonators Matteo Rinaldi, University of Pennsylvania Chengjie Zuo, University
More informationWafer Level Vacuum Packaged Out-of-Plane and In-Plane Differential Resonant Silicon Accelerometers for Navigational Applications
58 ILLHWAN KIM et al : WAFER LEVEL VACUUM PACKAGED OUT-OF-PLANE AND IN-PLANE DIFFERENTIAL RESONANT SILICON ACCELEROMETERS FOR NAVIGATIONAL APPLICATIONS Wafer Level Vacuum Packaged Out-of-Plane and In-Plane
More informationMiniaturising Motion Energy Harvesters: Limits and Ways Around Them
Miniaturising Motion Energy Harvesters: Limits and Ways Around Them Eric M. Yeatman Imperial College London Inertial Harvesters Mass mounted on a spring within a frame Frame attached to moving host (person,
More informationNon-linear frequency noise modulation in a resonant MEMS accelerometer
IEEE SENSORS JOURNAL 1 Non-linear frequency noise modulation in a resonant MEMS accelerometer Xudong Zou and Ashwin A. Seshia Abstract Resonant MEMS accelerometers offer the potential for very high resolution
More informationIntegrated Dual-Axis Gyro IDG-1004
Integrated Dual-Axis Gyro NOT RECOMMENDED FOR NEW DESIGNS. PLEASE REFER TO THE IDG-25 FOR A FUTIONALLY- UPGRADED PRODUCT APPLICATIONS GPS Navigation Devices Robotics Electronic Toys Platform Stabilization
More informationEE C245 ME C218 Introduction to MEMS Design
EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 20: Equivalent
More informationINF 5490 RF MEMS. LN10: Micromechanical filters. Spring 2011, Oddvar Søråsen Jan Erik Ramstad Department of Informatics, UoO
INF 5490 RF MEMS LN10: Micromechanical filters Spring 2011, Oddvar Søråsen Jan Erik Ramstad Department of Informatics, UoO 1 Today s lecture Properties of mechanical filters Visualization and working principle
More informationMEMS Technologies and Devices for Single-Chip RF Front-Ends
MEMS Technologies and Devices for Single-Chip RF Front-Ends Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Science University of Michigan Ann Arbor, Michigan 48105-2122 CCMT 06 April 25,
More informationDesign of Temperature Sensitive Structure for Micromechanical Silicon Resonant Accelerometer
Design of Temperature Sensitive Structure for Micromechanical Silicon Resonant Accelerometer Heng Li, Libin Huang*, Qinqin Ran School of Instrument Science and Engineering, Southeast University Nanjing,
More informationIntegrated Dual-Axis Gyro IDG-500
Integrated Dual-Axis Gyro FEATURES Integrated X- and Y-axis gyros on a single chip Two separate outputs per axis for standard and high sensitivity: X-/Y-Out Pins: 500 /s full scale range 2.0m/ /s sensitivity
More informationCRYSTAL oscillators are widely used to generate precision
440 IEEE JOURNAL OF SOLID-STATE CIRCUITS, VOL. 34, NO. 4, APRIL 1999 An Integrated CMOS Micromechanical Resonator High- Oscillator Clark T.-C. Nguyen, Member, IEEE, and Roger T. Howe, Fellow, IEEE Abstract
More informationMICRO YAW RATE SENSORS
1 MICRO YAW RATE SENSORS FIELD OF THE INVENTION This invention relates to micro yaw rate sensors suitable for measuring yaw rate around its sensing axis. More particularly, to micro yaw rate sensors fabricated
More information6.776 High Speed Communication Circuits and Systems Lecture 14 Voltage Controlled Oscillators
6.776 High Speed Communication Circuits and Systems Lecture 14 Voltage Controlled Oscillators Massachusetts Institute of Technology March 29, 2005 Copyright 2005 by Michael H. Perrott VCO Design for Narrowband
More informationDesigning a 960 MHz CMOS LNA and Mixer using ADS. EE 5390 RFIC Design Michelle Montoya Alfredo Perez. April 15, 2004
Designing a 960 MHz CMOS LNA and Mixer using ADS EE 5390 RFIC Design Michelle Montoya Alfredo Perez April 15, 2004 The University of Texas at El Paso Dr Tim S. Yao ABSTRACT Two circuits satisfying the
More informationA Doubly Decoupled X-axis Vibrating Wheel Gyroscope
19 Xue-Song Liu and Ya-Pu ZHAO* State Key Laboratory of Nonlinear Mechanics, Institute of Mechanics, Chinese Academy of Sciences Beijing 100190, People s Republic of China Abstract: In this paper, a doubly
More informationThe steeper the phase shift as a function of frequency φ(ω) the more stable the frequency of oscillation
It should be noted that the frequency of oscillation ω o is determined by the phase characteristics of the feedback loop. the loop oscillates at the frequency for which the phase is zero The steeper the
More informationRF MEMS for Low-Power Communications
RF MEMS for Low-Power Communications Clark T.-C. Nguyen Center for Wireless Integrated Microsystems Dept. of Electrical Engineering and Computer Science University of Michigan Ann Arbor, Michigan 48109-2122
More informationISSCC 2006 / SESSION 16 / MEMS AND SENSORS / 16.1
16.1 A 4.5mW Closed-Loop Σ Micro-Gravity CMOS-SOI Accelerometer Babak Vakili Amini, Reza Abdolvand, Farrokh Ayazi Georgia Institute of Technology, Atlanta, GA Recently, there has been an increasing demand
More informationSemiconductor Detector Systems
Semiconductor Detector Systems Helmuth Spieler Physics Division, Lawrence Berkeley National Laboratory OXFORD UNIVERSITY PRESS ix CONTENTS 1 Detector systems overview 1 1.1 Sensor 2 1.2 Preamplifier 3
More informationPART MAX2605EUT-T MAX2606EUT-T MAX2607EUT-T MAX2608EUT-T MAX2609EUT-T TOP VIEW IND GND. Maxim Integrated Products 1
19-1673; Rev 0a; 4/02 EVALUATION KIT MANUAL AVAILABLE 45MHz to 650MHz, Integrated IF General Description The are compact, high-performance intermediate-frequency (IF) voltage-controlled oscillators (VCOs)
More informationEE C245 ME C218 Introduction to MEMS Design Fall 2010
Instructor: Prof. Clark T.-C. Nguyen EE C245 ME C218 Introduction to MEMS Design Fall 2010 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley
More informationLab 4. Crystal Oscillator
Lab 4. Crystal Oscillator Modeling the Piezo Electric Quartz Crystal Most oscillators employed for RF and microwave applications use a resonator to set the frequency of oscillation. It is desirable to
More informationEE C245 ME C218 Introduction to MEMS Design Fall 2010
Basic Concept: Scaling Guitar Strings EE C245 ME C218 ntroduction to MEMS Design Fall 21 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley
More information6.976 High Speed Communication Circuits and Systems Lecture 11 Voltage Controlled Oscillators
6.976 High Speed Communication Circuits and Systems Lecture 11 Voltage Controlled Oscillators Michael Perrott Massachusetts Institute of Technology Copyright 2003 by Michael H. Perrott VCO Design for Wireless
More informationSystem Level Simulation of a Digital Accelerometer
System Level Simulation of a Digital Accelerometer M. Kraft*, C. P. Lewis** *University of California, Berkeley Sensors and Actuator Center 497 Cory Hall, Berkeley, CA 94720, mkraft@kowloon.eecs.berkeley.edu
More informationRFIC DESIGN EXAMPLE: MIXER
APPENDIX RFI DESIGN EXAMPLE: MIXER The design of radio frequency integrated circuits (RFIs) is relatively complicated, involving many steps as mentioned in hapter 15, from the design of constituent circuit
More informationLast Name Girosco Given Name Pio ID Number
Last Name Girosco Given Name Pio ID Number 0170130 Question n. 1 Which is the typical range of frequencies at which MEMS gyroscopes (as studied during the course) operate, and why? In case of mode-split
More informationETI , Good luck! Written Exam Integrated Radio Electronics. Lund University Dept. of Electroscience
und University Dept. of Electroscience EI170 Written Exam Integrated adio Electronics 2010-03-10, 08.00-13.00 he exam consists of 5 problems which can give a maximum of 6 points each. he total maximum
More informationVIBRATING mechanical tank components, such as crystal. High-Order Medium Frequency Micromechanical Electronic Filters
534 JOURNAL OF MICROELECTROMECHANICAL SYSTEMS, VOL. 8, NO. 4, DECEMBER 1999 High-Order Medium Frequency Micromechanical Electronic Filters Kun Wang, Student Member, IEEE, and Clark T.-C. Nguyen, Member,
More information77 GHz VCO for Car Radar Systems T625_VCO2_W Preliminary Data Sheet
77 GHz VCO for Car Radar Systems Preliminary Data Sheet Operating Frequency: 76-77 GHz Tuning Range > 1 GHz Output matched to 50 Ω Application in Car Radar Systems ESD: Electrostatic discharge sensitive
More informationNoise Reduction in Transistor Oscillators: Part 3 Noise Shifting Techniques. cross-coupled. over other topolo-
From July 2005 High Frequency Electronics Copyright 2005 Summit Technical Media Noise Reduction in Transistor Oscillators: Part 3 Noise Shifting Techniques By Andrei Grebennikov M/A-COM Eurotec Figure
More informationeasypll UHV Preamplifier Reference Manual
easypll UHV Preamplifier Reference Manual 1 Table of Contents easypll UHV-Pre-Amplifier for Tuning Fork 2 Theory... 2 Wiring of the pre-amplifier... 4 Technical specifications... 5 Version 1.1 BT 00536
More informationEE12: Laboratory Project (Part-2) AM Transmitter
EE12: Laboratory Project (Part-2) AM Transmitter ECE Department, Tufts University Spring 2008 1 Objective This laboratory exercise is the second part of the EE12 project of building an AM transmitter in
More informationMEMS-FABRICATED ACCELEROMETERS WITH FEEDBACK COMPENSATION
MEMS-FABRICATED ACCELEROMETERS WITH FEEDBACK COMPENSATION Yonghwa Park*, Sangjun Park*, Byung-doo choi*, Hyoungho Ko*, Taeyong Song*, Geunwon Lim*, Kwangho Yoo*, **, Sangmin Lee*, Sang Chul Lee*, **, Ahra
More informationMichael S. McCorquodale, Ph.D. Founder and CTO, Mobius Microsystems, Inc.
Self-Referenced, Trimmed and Compensated RF CMOS Harmonic Oscillators as Monolithic Frequency Generators Integrating Time Michael S. McCorquodale, Ph.D. Founder and CTO, Mobius Microsystems, Inc. 2008
More informationK-BAND HARMONIC DIELECTRIC RESONATOR OS- CILLATOR USING PARALLEL FEEDBACK STRUC- TURE
Progress In Electromagnetics Research Letters, Vol. 34, 83 90, 2012 K-BAND HARMONIC DIELECTRIC RESONATOR OS- CILLATOR USING PARALLEL FEEDBACK STRUC- TURE Y. C. Du *, Z. X. Tang, B. Zhang, and P. Su School
More informationA Self-Sustaining Ultra High Frequency Nanoelectromechanical Oscillator
Online Supplementary Information A Self-Sustaining Ultra High Frequency Nanoelectromechanical Oscillator X.L. Feng 1,2, C.J. White 2, A. Hajimiri 2, M.L. Roukes 1* 1 Kavli Nanoscience Institute, MC 114-36,
More informationDifferential Amplifier : input. resistance. Differential amplifiers are widely used in engineering instrumentation
Differential Amplifier : input resistance Differential amplifiers are widely used in engineering instrumentation Differential Amplifier : input resistance v 2 v 1 ir 1 ir 1 2iR 1 R in v 2 i v 1 2R 1 Differential
More informationA Vacuum Packaged Surface Micromachined Resonant Accelerometer
784 JOURNAL OF MICROELECTROMECHANICAL SYSTEMS, VOL. 11, NO. 6, DECEMBER 2002 A Vacuum Packaged Surface Micromachined Resonant Accelerometer Ashwin A. Seshia, Member, IEEE, Moorthi Palaniapan, Trey A. Roessig,
More informationUnderstanding VCO Concepts
Understanding VCO Concepts OSCILLATOR FUNDAMENTALS An oscillator circuit can be modeled as shown in Figure 1 as the combination of an amplifier with gain A (jω) and a feedback network β (jω), having frequency-dependent
More informationOperational Amplifiers
Operational Amplifiers Table of contents 1. Design 1.1. The Differential Amplifier 1.2. Level Shifter 1.3. Power Amplifier 2. Characteristics 3. The Opamp without NFB 4. Linear Amplifiers 4.1. The Non-Inverting
More informationLow-Power Ovenization of Fused Silica Resonators for Temperature-Stable Oscillators
Low-Power Ovenization of Fused Silica Resonators for Temperature-Stable Oscillators Zhengzheng Wu zzwu@umich.edu Adam Peczalski peczalsk@umich.edu Mina Rais-Zadeh minar@umich.edu Abstract In this paper,
More informationCHAPTER - 6 PIN DIODE CONTROL CIRCUITS FOR WIRELESS COMMUNICATIONS SYSTEMS
CHAPTER - 6 PIN DIODE CONTROL CIRCUITS FOR WIRELESS COMMUNICATIONS SYSTEMS 2 NOTES 3 INTRODUCTION PIN DIODE CONTROL CIRCUITS FOR WIRELESS COMMUNICATIONS SYSTEMS Chapter 6 discusses PIN Control Circuits
More informationOscillators. An oscillator may be described as a source of alternating voltage. It is different than amplifier.
Oscillators An oscillator may be described as a source of alternating voltage. It is different than amplifier. An amplifier delivers an output signal whose waveform corresponds to the input signal but
More informationMiniproject: AM Radio
Objective UNIVERSITY OF CALIFORNIA AT BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences EE05 Lab Experiments Miniproject: AM Radio Until now, the labs have focused
More informationLab 4. Crystal Oscillator
Lab 4. Crystal Oscillator Modeling the Piezo Electric Quartz Crystal Most oscillators employed for RF and microwave applications use a resonator to set the frequency of oscillation. It is desirable to
More informationDr.-Ing. Ulrich L. Rohde
Dr.-Ing. Ulrich L. Rohde Noise in Oscillators with Active Inductors Presented to the Faculty 3 : Mechanical engineering, Electrical engineering and industrial engineering, Brandenburg University of Technology
More informationIndex. bias current, 61, 145 critical, 61, 64, 108, 161 start-up, 109 bilinear function, 11, 43, 167
Bibliography 1. W. G. Cady. Method of Maintaining Electric Currents of Constant Frequency, US patent 1,472,583, filed May 28, 1921, issued Oct. 30, 1923. 2. G. W. Pierce, Piezoelectric Crystal Resonators
More informationVibrating MEMS resonators
Vibrating MEMS resonators Vibrating resonators can be scaled down to micrometer lengths Analogy with IC-technology Reduced dimensions give mass reduction and increased spring constant increased resonance
More informationCharacteristics of Crystal. Piezoelectric effect of Quartz Crystal
Characteristics of Crystal Piezoelectric effect of Quartz Crystal The quartz crystal has a character when the pressure is applied to the direction of the crystal axis, the electric change generates on
More informationMEMS Real-Time Clocks: small footprint timekeeping. Paolo Frigerio November 15 th, 2018
: small footprint timekeeping Paolo Frigerio paolo.frigerio@polimi.it November 15 th, 2018 Who? 2 Paolo Frigerio paolo.frigerio@polimi.it BSc & MSc in Electronics Engineering PhD with Prof. Langfelder
More informationIN-CHIP DEVICE-LAYER THERMAL ISOLATION OF MEMS RESONATOR FOR LOWER POWER BUDGET
Proceedings of IMECE006 006 ASME International Mechanical Engineering Congress and Exposition November 5-10, 006, Chicago, Illinois, USA IMECE006-15176 IN-CHIP DEVICE-LAYER THERMAL ISOLATION OF MEMS RESONATOR
More informationTest Your Understanding
074 Part 2 Analog Electronics EXEISE POBLEM Ex 5.3: For the switched-capacitor circuit in Figure 5.3b), the parameters are: = 30 pf, 2 = 5pF, and F = 2 pf. The clock frequency is 00 khz. Determine the
More informationEVALUATION KIT AVAILABLE 10MHz to 1050MHz Integrated RF Oscillator with Buffered Outputs. Typical Operating Circuit. 10nH 1000pF MAX2620 BIAS SUPPLY
19-1248; Rev 1; 5/98 EVALUATION KIT AVAILABLE 10MHz to 1050MHz Integrated General Description The combines a low-noise oscillator with two output buffers in a low-cost, plastic surface-mount, ultra-small
More informationMicro-nanosystems for electrical metrology and precision instrumentation
Micro-nanosystems for electrical metrology and precision instrumentation A. Bounouh 1, F. Blard 1,2, H. Camon 2, D. Bélières 1, F. Ziadé 1 1 LNE 29 avenue Roger Hennequin, 78197 Trappes, France, alexandre.bounouh@lne.fr
More informationElectronics basics for MEMS and Microsensors course
Electronics basics for course, a.a. 2017/2018, M.Sc. in Electronics Engineering Transfer function 2 X(s) T(s) Y(s) T S = Y s X(s) The transfer function of a linear time-invariant (LTI) system is the function
More informationImproved Second Source to the EL2020 ADEL2020
Improved Second Source to the EL ADEL FEATURES Ideal for Video Applications.% Differential Gain. Differential Phase. db Bandwidth to 5 MHz (G = +) High Speed 9 MHz Bandwidth ( db) 5 V/ s Slew Rate ns Settling
More informationSymmetrical and decoupled nickel microgyroscope on insulating substrate
Sensors and Actuators A 115 (2004) 336 350 Symmetrical and decoupled nickel microgyroscope on insulating substrate Said Emre Alper, Tayfun Akin Department of Electrical and Electronics Engineering, Middle
More informationA HIGH FIGURE-OF-MERIT LOW PHASE NOISE 15-GHz CMOS VCO
82 Journal of Marine Science and Technology, Vol. 21, No. 1, pp. 82-86 (213) DOI: 1.6119/JMST-11-123-1 A HIGH FIGURE-OF-MERIT LOW PHASE NOISE 15-GHz MOS VO Yao-hian Lin, Mei-Ling Yeh, and hung-heng hang
More informationEE C245 ME C218 Introduction to MEMS Design
EE C245 ME C218 Introduction to MEMS Design Fall 2008 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 2: Benefits
More informationCommunication Systems. Department of Electronics and Electrical Engineering
COMM 704: Communication Lecture 6: Oscillators (Continued) Dr Mohamed Abd El Ghany Dr. Mohamed Abd El Ghany, Mohamed.abdel-ghany@guc.edu.eg Course Outline Introduction Multipliers Filters Oscillators Power
More informationMAHALAKSHMI ENGINEERING COLLEGE TIRUCHIRAPALLI
MAHALAKSHMI ENGINEERING COLLEGE TIRUCHIRAPALLI-621213. QUESTION BANK DEPARTMENT: EEE SUBJECT CODE: EE2203 SEMESTER : III SUBJECT NAME: ELECTRONIC DEVICES &CIRCUITS UNIT 4-AMPLIFIERS AND OSCILLATORS PART
More informationIn order to suppress coupled oscillation and drift and to minimize the resulting zero-rate drift, various devices have been reported employing indepen
Distributed-Mass Micromachined Gyroscopes for Enhanced Mode-Decoupling Cenk Acar Microsystems Laboratory Mechanical and Aerospace Engineering Dept. University of California at Irvine Irvine, CA, USA cacar@uci.edu
More informationPhase-locked loop PIN CONFIGURATIONS
NE/SE DESCRIPTION The NE/SE is a versatile, high guaranteed frequency phase-locked loop designed for operation up to 0MHz. As shown in the Block Diagram, the NE/SE consists of a VCO, limiter, phase comparator,
More informationA Real-Time kHz Clock Oscillator Using a mm 2 Micromechanical Resonator Frequency-Setting Element
0.0154-mm 2 Micromechanical Resonator Frequency-Setting Element, Proceedings, IEEE International Frequency Control Symposium, Baltimore, Maryland, May 2012, to be published A Real-Time 32.768-kHz Clock
More information12.92 GHz to GHz MMIC VCO with Half Frequency Output HMC1169
Data Sheet 12.92 GHz to 14.07 GHz MMIC VCO with Half Frequency Output FEATURES Dual output frequency range fout = 12.92 GHz to 14.07 GHz fout/2 = 6.46 GHz to 7.035 GHz Output power (POUT): 11.5 dbm SSB
More informationSP 22.3: A 12mW Wide Dynamic Range CMOS Front-End for a Portable GPS Receiver
SP 22.3: A 12mW Wide Dynamic Range CMOS Front-End for a Portable GPS Receiver Arvin R. Shahani, Derek K. Shaeffer, Thomas H. Lee Stanford University, Stanford, CA At submicron channel lengths, CMOS is
More informationElectrically coupled MEMS bandpass filters Part I: With coupling element
Sensors and Actuators A 122 (2005) 307 316 Electrically coupled MEMS bandpass filters Part I: With coupling element Siavash Pourkamali, Farrokh Ayazi School of Electrical and Computer Engineering, Georgia
More informationNon-linear circuits and sensors
ELEC3106, Electronics Non-linear circuits and sensors 1 ELEC3106 Electronics: lecture 10 summary Non-linear circuits and sensors Torsten Lehmann School of Electrical Engineering and Telecommunication The
More informationPYKC 7 Feb 2019 EA2.3 Electronics 2 Lecture 13-1
In this lecture, we will look back on all the materials we have covered to date. Instead of going through previous lecture materials, I will focus on what you have learned in the laboratory sessions, going
More information12.17 GHz to GHz MMIC VCO with Half Frequency Output HMC1167
9 0 3 4 5 6 9 7 6.7 GHz to 3.33 GHz MMIC VCO with Half Frequency Output FEATURES Dual output frequency range fout =.7 GHz to 3.330 GHz fout/ = 6.085 GHz to 6.665 GHz Output power (POUT): 0.5 dbm Single-sideband
More informationCMOS-Electromechanical Systems Microsensor Resonator with High Q-Factor at Low Voltage
CMOS-Electromechanical Systems Microsensor Resonator with High Q-Factor at Low Voltage S.Thenappan 1, N.Porutchelvam 2 1,2 Department of ECE, Gnanamani College of Technology, India Abstract The paper presents
More informationGHz-band, high-accuracy SAW resonators and SAW oscillators
The evolution of wireless communications and semiconductor technologies is spurring the development and commercialization of a variety of applications that use gigahertz-range frequencies. These new applications
More informationISSCC 2006 / SESSION 33 / MOBILE TV / 33.4
33.4 A Dual-Channel Direct-Conversion CMOS Receiver for Mobile Multimedia Broadcasting Vincenzo Peluso, Yang Xu, Peter Gazzerro, Yiwu Tang, Li Liu, Zhenbiao Li, Wei Xiong, Charles Persico Qualcomm, San
More information11.41 GHz to GHz MMIC VCO with Half Frequency Output HMC1166
9 6 3 30 29 VTUNE 28 27 26.4 GHz to 2.62 GHz MMIC VCO with Half Frequency Output FEATURES Dual output frequency range fout =.4 GHz to 2.62 GHz fout/2 = 5.705 GHz to 6.3 GHz Output power (POUT): dbm Single-sideband
More informationOSCILLATORS AND WAVEFORM-SHAPING CIRCUITS
OSILLATORS AND WAVEFORM-SHAPING IRUITS Signals having prescribed standard waveforms (e.g., sinusoidal, square, triangle, pulse, etc). To generate sinusoidal waveforms: o Positive feedback loop with non-linear
More informationTL072 TL072A - TL072B
A - B LOW NOISE J-FET DUAL OPERATIONAL AMPLIFIERS WIDE COMMON-MODE (UP TO V + CC ) AND DIFFERENTIAL VOLTAGE RANGE LOW INPUT BIAS AND OFFSET CURRENT LOW NOISE e n = 15nV/ Hz (typ) OUTPUT SHORT-CIRCUIT PROTECTION
More informationWafer-level Vacuum Packaged X and Y axis Gyroscope Using the Extended SBM Process for Ubiquitous Robot applications
Proceedings of the 17th World Congress The International Federation of Automatic Control Wafer-level Vacuum Packaged X and Y axis Gyroscope Using the Extended SBM Process for Ubiquitous Robot applications
More informationPhase Noise Modeling of Opto-Mechanical Oscillators
Phase Noise Modeling of Opto-Mechanical Oscillators Siddharth Tallur, Suresh Sridaran, Sunil A. Bhave OxideMEMS Lab, School of Electrical and Computer Engineering Cornell University Ithaca, New York 14853
More informationReceiver Architecture
Receiver Architecture Receiver basics Channel selection why not at RF? BPF first or LNA first? Direct digitization of RF signal Receiver architectures Sub-sampling receiver noise problem Heterodyne receiver
More information