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EE C245 – ME C218Introduction to MEMS Design
Fall 2008Fall 2008
Prof Clark T C NguyenProf. Clark T.-C. Nguyen
Dept of Electrical Engineering & Computer SciencesDept. of Electrical Engineering & Computer SciencesUniversity of California at Berkeley
Berkeley, CA 94720y
L t 2 B fit f S li
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 1
Lecture 2: Benefits of Scaling
Lecture Outline
• Reading: Senturia, Chapter 1g p• Lecture Topics:
Benefits of MiniaturizationExamplesExamples
GHz micromechanical resonatorsChip-scale atomic clockpMicro gas chromatograph
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 2
Technology Trend and Roadmap for MEMSs
108
109
DistributedStructural Digital Micromirror
Pentium 4
ompu
te
sist
ors
106
107Structural
ControlTerabit/cm2
Data Storage
DisplaysADXL-50
Digital MicromirrorDevice (DMD)CPU’s
Phased Array
bilit
y to
co
of T
rans
104
105
10
Adaptive
Integrated FluidicSystems
InertialNavigationOn a Chip
Displays
W
OMM 32x32
i-STAT 1Caliper
Phased-ArrayAntenna
crea
sing
ab
mbe
r o
2
103
104 AdaptiveOptics
Optical Switches& Aligners
Weapons,Safing, Arming,
and FusingADXL-278
Future MEMSIntegration Levels
Enabled Applications
Caliper
inc
Num
101
102
ADXL-78ADXRS
Number of Mechanical Components
100
100 101 102 103 104 105 106 107 108 109Majority of
Early MEMS
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 3
increasing ability to sense and actNumber of Mechanical Componentsy
Devices(mostly sensors)
Example: Micromechanical Accelerometer
• The MEMS Advantage:>30X size reduction for accelerometer mechanical element m
Tiny mass means small output need
accelerometer mechanical elementallows integration with IC’s
Basic Operation Principle
400
μmintegrated transistor circuits to compensate
xo
Basic Operation Principle
maFx i =∝
xSpring
Displacement
a Inertial Force
Spring
A l ti
Proof Mass
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 4
AccelerationAnalog Devices ADXL 78
Technology Trend and Roadmap for MEMSs
108
109
DistributedStructural Digital Micromirror
Pentium 4
DisplaysPhased Arrayompu
te
sist
ors
106
107Structural
ControlTerabit/cm2
Data StorageADXL-50
Digital MicromirrorDevice (DMD)CPU’s
Analog Devices ADXRS
OMM 8x8 OpticalCross-Connect Switch
Adv.: faster switching, lowDisplaysPhased-ArrayAntenna
bilit
y to
co
of T
rans
104
105
10
Adaptive
Integrated FluidicSystems
InertialNavigationOn a Chip
W
OMM 32x32
i-STAT 1Caliper
gIntegrated Gyroscope
Adv.: small size
Adv.: faster switching, low loss, larger networks
crea
sing
ab
mbe
r o
2
103
104 AdaptiveOptics
Optical Switches& Aligners
Weapons,Safing, Arming,
and FusingADXL-278
Future MEMSIntegration Levels
Enabled Applications
Caliper
inc
Num
101
102
ADXL-78ADXRSCaliper Microfluidic Chip
Ad l l f tTI Digital Micromirror Device
Number of Mechanical Components
100
100 101 102 103 104 105 106 107 108 109Majority of
Early MEMS
Adv.: low loss, fast switching, high fill factor
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 5
increasing ability to sense and actNumber of Mechanical Componentsy
Devices(mostly sensors)Adv.: small size, small
sample, fast analysis speed
Technology Trend and Roadmap for MEMSs
108
109
DistributedStructural Digital Micromirror
Pentium 4
ompu
te
sist
ors
106
107Structural
ControlTerabit/cm2
Data StorageADXL-50
Digital MicromirrorDevice (DMD)CPU’s
umpt
ion
DisplaysPhased Array
bilit
y to
co
of T
rans
104
105
10
Adaptive
Integrated FluidicSystems
InertialNavigationOn a Chip
W
OMM 32x32
ower
con
s
i-STAT 1Caliper
DisplaysPhased-ArrayAntenna
crea
sing
ab
mbe
r o
2
103
104 AdaptiveOptics
Optical Switches& Aligners
Weapons,Safing, Arming,
and FusingADXL-278
Future MEMSIntegration Levels
Enabled Applicationsreas
ing
po Caliper
inc
Num
101
102
ADXL-78incr ADXRS
Lucrative Ultra-Low Power Territory(e.g, mechanically powered devices)
Number of Mechanical Components
100
100 101 102 103 104 105 106 107 108 109Majority of
Early MEMS
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 6
increasing ability to sense and actNumber of Mechanical Componentsy
Devices(mostly sensors)
Benefits of Size Reduction: MEMS• Benefits of size reduction clear for IC’s in elect. domain
size reduction speed, low power, complexity, economy•MEMS: enables a similar concept but MEMS extends the benefits of size reduction
beyond the electrical domain
•MEMS: enables a similar concept, but …
beyond the electrical domain
Performance enhancements for applicationdomains beyond those satisfied by electronics
in the same general categories in the same general categories Speed
P C nsumpti nFrequency , Thermal Time Const. A t ti n En H tin P Power Consumption
ComplexityE
Actuation Energy , Heating Power Integration Density , Functionality B t h F b P t ( f k i )
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 7
Economy Batch Fab. Pot. (esp. for packaging)Robustness g-Force Resilience
Vibrating RF MEMSVibrating RF MEMS
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 8
Basic Concept: Scaling Guitar Strings h l Guitar String
e
μMechanical Resonatorm
plitu
de
Low Q
High Q
Vib.
Am
Vibrating “A”String (110 Hz)
110 Hz Freq.Performance:
L =40 8μm[Bannon 1996]
String (110 Hz)
Stiffnessfo=8.5MHzQvac =8,000
Qair ~50
Lr 40.8μmmr ~ 10-13 kg
Wr=8μm, hr=2μmd=1000Å, VP=5V
ro
kf 1=
Freq. Equation:air , P
Press.=70mTorr
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 9
Guitar ro m
fπ2
Freq. Mass
Frequency of a Stretched Wire
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 10
Frequency of a Clamped-Clamped Beam
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 11
Frequency of a Clamped-Clamped Beam
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 12
Basic Concept: Scaling Guitar Strings h l Guitar String
e
μMechanical Resonatorm
plitu
de
Low Q
High Q
Vib.
Am
Vibrating “A”String (110 Hz)
110 Hz Freq.Performance:
L =40 8μm[Bannon 1996]
String (110 Hz)
Stiffnessfo=8.5MHzQvac =8,000
Qair ~50
Lr 40.8μmmr ~ 10-13 kg
Wr=8μm, hr=2μmd=1000Å, VP=5V
ro
kf 1=
Freq. Equation:air , P
Press.=70mTorr
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 13
Guitar ro m
fπ2
Freq. Mass
3CC 3λ/4 Bridged μMechanical Filter
VPPerformance:fo=9MHz, BW=20kHz, PBW=0.2%
I L =2 79dB Stop Rej =51dB
0
In OutI.L.=2.79dB, Stop. Rej.=51dB
20dB S.F.=1.95, 40dB S.F.=6.45
-10
0
B]
-30
-20
ssio
n [d
B
Pin=-20dBm Sharper roll-off Design:
L 40-40
Tran
smis
Loss PoleLr=40μm
Wr=6.5μm hr=2μm
L 3 5
-60
-50T Lc=3.5μmLb=1.6μm VP=10.47VP= 5dBm
[S.-S. Li, Nguyen, FCS’05]
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 14
8.7 8.9 9.1 9.3Frequency [MHz]
P=-5dBmRQi=RQo=12kΩ
[Li, et al., UFFCS’04]
1.51-GHz, Q=11,555 Nanocrystalline Diamond Disk μMechanical Resonatorm μ
• Impedance-mismatched stem for reduced anchor dissipation
•O t d i th 2nd di l t d•Operated in the 2nd radial-contour mode•Q ~11,555 (vacuum); Q ~10,100 (air)• Below: 20 μm diameter disk Design/Performance:
R 10 t 2 2 d 800Å V 7V
-84
Below: 20 μm diameter disk
Polysilicon Stem(Impedance Mismatched ]
R=10μm, t=2.2μm, d=800Å, VP=7Vfo=1.51 GHz (2nd mode), Q=11,555
§
-90-88-86
P l ili
(Impedance Mismatchedto Diamond Disk)
ude
[dB
]
fo = 1.51 GHzQ = 11,555 (vac)Q = 10,100 (air)
§
96-94-9290Polysilicon
Electrode RA
mpl
itu Q = 10,100 (air)
-100-98-96
1507 4 1507 6 1507 8 1508 1508 2G dCVD DiamondM h i l Di k
Mix
ed A
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 15
1507.4 1507.6 1507.8 1508 1508.2GroundPlane
μMechanical DiskResonator Frequency [MHz]
[Wang, Butler, Nguyen MEMS’04]
163-MHz Differential Disk-Array Filter
VFilter Coupler
Com. Array Couplers
vi+ vo+VP
λ/2
Port1 Port3
λ/2
λ/4
λ λ
λ/4
vi- vo-VP
λ/2Port2 Port4
λ/2Diff. Array Couplers
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 16
Couplers
[Li, Nguyen Trans’07]
Linear MEMS in Wireless CommsHigh Q and good linearity of micromechanical resonators
Filters for front-end frequency selection
n [d
B]
ansm
issi
on
Frequency [MHz]
Tra
Micromechanical Bandpass Filter
A/DDiplexer
Mixer I LPF I
AGC
Antenna
Wireless Phone
90o0o
RF PLLRF RXRF LO
Xstal Osc
Q
AGC
LNA
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 17
A/DFrom TXBPF
Mixer Q LPF
Q
AGC
LNA
Miniaturization of RF Front Ends
Diplexer
925-960MHz
RF Power Amplifier
RF SAW Filter
1805-1880MHz RF SAW Filter
897.5±17.5MHz RF SAW Filter
26-MHz Xstal Oscillator
RF SAW FilterDual-Band Zero-IF
Transistor ChipOscillator
3420-3840MHz VCO
Problem: high-Q passives pose a bottleneck against miniaturization
A/DDiplexer
Mixer I LPF I
AGC
Antenna
Wireless Phone
90o0o
RF PLLRF RXRF LO
Xstal Osc
Q
AGC
LNA
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 18
A/DFrom TXBPF
Mixer Q LPF
Q
AGC
LNA
I
Multi-Band Wireless Handsets
LPF
Duplexer
LNA RF BPFCDMACDMA
0o
I
A/D IAGCRF BPF GSM 900GSM 900
From TX90o
0o
Antenna
A/DI
LPF
QAGC
RF BPF PCS 1900PCS 1900
LNA Q
90o0o
RXRF LO
LNA
LNARF BPF DCS 1800DCS 1800 ÷ (N+1)/N Xstal
OscRXRF ChannelSelect PLL
Q
Duplexer RF BPF
LNA
LNA
CDMACDMA--20002000 Tank
Duplexer
LNAFrom TX
RF BPF
CDMACDMA 20002000
• The number of off-chip high-Qpassives increases dramatically
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 19
LNAWCDMAWCDMA From TX
passives increases dramatically•Need: on-chip high-Q passives
All High-Q Passives on a Single Chip
0.25 mm
Vibrating Resonator62-MHz, Q~161,000
Vibrating Resonator1.5-GHz, Q~12,000
GSM 900 RF Filter
CDMA RF Filters(869-894 MHz) Optional RF
Oscillator Ultra-High Q
PCS 1900 RF Filter(1930-1990 MHz)
(935-960 MHz)
Low Freq.
Ultra-High QTanks
CDMA 2000
DCS 1800 RF Filter(1805-1880 MHz)
Low Freq. Reference Oscillator Ultra-High
Q Tank
WCDMA
CDMA-2000RF Filters
(1850-1990 MHz)
Q Tank
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 20
WCDMARF Filters
(2110-2170 MHz)
Chip-Scale Atomic Clocks (CSAC)Chip Scale Atomic Clocks (CSAC)
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 21
NIST F1 Fountain Atomic Clock
Vol: ~3.7 mVol: ~3.7 m33
Power: ~500 WPower: ~500 WAcc: Acc: 11××1010––1515
Stab: 3.3x10Stab: 3.3x10--1515/hr/hr
After 1 sec Error: 10-15 sec
Loses 1 sec every y30 million years!
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 22
Physics Package
Benefits of Accurate Portable TimingNetworked Sensors
Better Timing
Secure CommunicationsLarger networks withMore efficient
spectrum utilizationLarger networks with
longer autonomy
Faster frequency hop rates
Longer autonomy periods GPS
Faster acquire of pseudorandom signals
Fewer satellites needed
Superior resilience Higher jamming
margin
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 23
pagainst jamming or
interception Faster GPS acquire
NIST F1 Fountain Atomic Clock
Vol: ~3.7 mVol: ~3.7 m33
Power: ~500 WPower: ~500 WAcc: Acc: 11××1010––1515
Stab: 3.3x10Stab: 3.3x10--1515/hr/hr
After 1 sec Error: 10-15 sec
Loses 1 sec every y30 million years!
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 24
Physics Package
Tiny Physics Package Performance• Experimental Conditions:
Cs D2 ExcitationExternal (large) Magnetic Shielding
Dime
NIST’s Chip-Scale
External (large) Magnetic ShieldingExternal Electronics & LO Cell Temperature: ~80 ºCCell Heater Power: 69 mWC p Sca e
Atomic Physics Package
Cell Heater Power: 69 mWLaser Current/Voltage: 2mA / 2VRF Laser Mod Power: 70μW
Open Loop Resonance: Drift to Be Removed
10-9σ y
Stability Measurement:Drift IssueCs (D2)
5.67
[V]
7.1 kHz
Removed in Phase 3
Sufficient to meet
10-10
Dev
iatio
n,
Q =1.3x106
5.66
PD S
igna
l
Contrast: 0.91% 2.4e-10 Allandeviation @ 1 s
to meet CSAC
program goals
10-11
Alla
n D
Rb (D1) 1 day1 day1 hour1 hour
EE C245: Introduction to MEMS Design Lecture 2 C. Nguyen 9/2/08 25
40 50 60 70 80 905.65
Frequency Detuning, Δ [kHz] from 9,192,631,770 Hz
100 101 102 103 104 10510-12
Integration Time, τ [s]
1 day1 day1 hour1 hour