piezoelectric mems: materials, devices, and applications
TRANSCRIPT
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Piezoelectric MEMS: Materials, Devices, and Applications
Professor David HorsleyCo-director, Berkeley Sensor & Actuator Center (BSAC)
Mechanical and Aerospace EngineeringUniversity of California, Davis
e-mail: [email protected]://mae.engr.ucdavis.edu/~memslab
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Outline• Piezo-MEMS devices today
– companies & foundries in the market today– products on the market today– Comparison of piezo materials: PZT & AlN
• Future piezo-MEMS devices– Piezoelectric micromachined ultrasonic transducers (PMUTs)– Air-coupled devices for ranging & gesture sensing– Fluid-coupled devices for biometrics
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Horsley Group Research
Ultrasonics
New materials & fabrication
Optical MEMS
Magnetic MEMS
Gyro & magnetometer
Diamond MEMS
Microactuators
Si fluidics
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Piezoelectric MEMS Commercialization Status
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Film Bulk Acoustic Resonators (FBAR)
• Avago produces 1 Billion AlN FBAR’s per year.
LTE Band Duplexer (Avago)
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
6Images: Harmeet Bhugra, IDT
IDT: Timing Oscillators
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Other Commercial Piezo-MEMS Devices
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Panasonic Gyroscope
Microgen Energy Harvester
poLight Varifocal Lens
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
2013 2014 2015 2016 2017 2018
Timeline
Dro
nes
Thin Film PZT – Sensors & ActuatorsPlayers roadmap – expected year for market entry
Ultr
asou
ndM
EM
S
Iner
tial
ME
MS
IR
dete
ctor
sM
EM
S
foun
drie
s
…
Expected year of foundry service readiness for thin film PZT technology
Expected year of foundry service readiness for thin film PZT technology
TFP Technology - Gyros
(Yole Developpement, Nov. 2013)
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Piezoelectric MaterialsMechanical strain ↔ electrical polarization
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e = cd
d: [pm/V]
e: [C/m2]
stiffness tensor
D = eS + εTEstrain
Piezoelectric coefficients
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Comparing Piezoelectric Materials: Materials for Acoustic Transducers
Metric Property Units AlN PZT ZnOTransmitter Sensitivity e31,f C m-2 -1.05 -14.9 -1.0
ε33 - 10.5 1020 10.9Receiver
Sensitivitye31,f / ε33ε0
GV/m -11.3 -1.64 -10.3
[S Trolier-McKinstry & P. Muralt, J. Electroceram. 12(7-17), 2004.] 11
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
AlN Deposition: Reactive Sputtering
• Deposition rate > 50 nm/min• Low substrate temperature: 400°C• Bottom electrode materials: Mo, Pt, Al• AlN crystalline structure characterized by XRD Rocking Curve
– Typically ~1.5° FWHM for highly c-axis oriented film 12
V. Felmetsger, OEM Group
XRD of AlN on Mo
Magnetron S-gun
Plasma
Wafer
Sputtering Chamber
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Piezoelectric MicromachinedUltrasonic Transducers (PMUTs)
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Ultrasonic MEMS: Current Research Areas• Air-coupled PMUTs
– Diameter ~0.5 mm– Operating frequencies: 40 kHz – 800 kHz– Applications: gesture recognition, ranging, autofocus, gas metering
• Fluid-coupled PMUTs– Diameter ~50 microns– Operating frequencies: > 10 MHz– Applications: medical imaging, biometrics (fingerprint sensing)
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
• Medical imaging• Ranging/obstacle avoidance• Robotics• Non destructive testing• Gesture recognition
Ultrasound Applications
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
• Advantages:– Large output pressure– Directional, if desired
• Disadvantages:– Inefficient coupling to air– Matching layers required– Too big for consumer electronics– Dumb sensor. Lots of external electronics required.
Existing Ultrasound Transducers
10 mm
senscomp.com 5.2 mm
muratamericas.com
maxbotix.com
20 mm
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
• Suspended plate structure• Increased coupling due to low acoustic impedance• Array fabrication possible• Micro-scale features
Micromachined Ultrasound Transducers
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Air-Coupled Acoustic TransducersWant:• Large output pressure despite air’s low acoustic impedance
→ Large transducer displacement→ Piezoelectric Actuation
[Wygant et al., IEEE TUFFC 2009]
[Shelton et al., 2009 IEEE Ultrasonics Symp.]
[Przybyla et al., IEEE Sensors J. 2011]
Capacitive (CMUT) Piezoelectric (PMUT)
MoAlNAlN
Al
vs.
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
fo ≈ 200 kHz
BW ≈ 10 kHz
–
Aluminum Nitride (AlN) PMUT Cross Section
Si
Al
450μm250μm
+
AlN
AlNMo
AlNAl
1μm
2μm
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Chip-Scale Arrays Enable 3D Ranging
• 2D array of transducers:– Output power on-axis: N2
– Number of elements sets beam width
• Beam width ~180○/N for linear array
– Individual electrodes enable electrical beam steering
– Spacing ~λ/2 = 0.9mm for 180○beam steering
37-Element Array
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Single element 2D array
S. Shelton, A. Guedes, R. Przybyla, R. Krigel, B. Boser, D.A. Horsley, 2012 Solid-State Sensors Actuators & Microsystems Workshop, Hilton Head SC, June 2012.
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Narrow beam improves SNR & spatial resolution
Phased Arrays are Directional
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
2D arrayOutput SPL Scales with N
0 5 10 15 200
5
10
15
20
Number of Transducers
Rel
ativ
e O
utpu
t Pre
ssur
e (a
.u.)
Measured Data Linear Fit
S. Shelton, A. Guedes, R. Przybyla, R. Krigel, B. Boser, D.A. Horsley, 2012 Solid-State Sensors Actuators & Microsystems Workshop, Hilton Head SC, June 2012.
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Phased Arrays are DirectionalNarrow beam improves SNR & spatial resolution
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Range Measurement – Received Signal
Time
Time of Flight
≅ mm
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Range Resolution
Voltage
Time
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
x-angle [deg]
Ran
ge [m
]
-40 -30 -20 -10 0 10 20 30 400
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
y-an
gle
[deg
]
-15
-10
-5
0
5
10
15
20
25
www.chirpmicro.com
Single Pulse Image
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For 1 m max range design, @50 cm:
Z-axis: 0.4 mm rms
X-axis: 0.2o rms
Y-axis: 0.8o rms
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Ultrasonic Fingerprint Sensor
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• Requires PMUTs similar to medical transducers– Center frequency > 20 MHz– 50 m resolution
• Significant performance advantages over existing fingerprint sensors– Sub-surface dermal imaging.– Wet/dry fingers can be imaged.
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
State of the art: Commercial Ultrasonic Fingerprint Sensor
Reference: Ultra-scan®, U.S. patent 5224174
lens
transducer
Mechanical motion
Pros:Dermal detection
Cons: Large system mechanical scanning
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Bulk Piezo Fingerprint Sensors
Sonavation Inc.
Drawbacks:
• Interconnect is challenging
• Readout based on resonator Q (no advantage over capacitance)
• High manufacturing cost.
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
72 x 9 PMUT Array
Cross-section of 40 µm PMUT
Y. Lu et al, 2014 Solid State Sensor, Actuator, and Microsystem Workshop. 29
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Coupling the Array to Skin
PDMSPDMS
Polyethylene
Fluid
Hydrophone
Test Setup Concept
250 m
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Mapping the Pressure Field
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40 m Needle Hydrophone
x/z
x/y
PMUT Array
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Experimental Beamforming: AlN PMUTs
12V input
15 elements
8 channels
140 um pitchLateral distance (m)
Axi
al d
ista
nce
(mm
)
-200 -100 0 100 2001.3
1.35
1.4
1.45
1.5
1.55
1.6
1.65
10
20
30
40
50
60
70kPa15 elements/ 8 channels, 140 m Pitch
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100 µm
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
System diagram: pulse-echo imaging
PMUT Array
Collaboration w/ Bernhard Boser, UC Berkeley33
David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
1 D ultrasonic imaging
1 cm
Lateral distance (mm)
Axi
al d
ista
nce
(mm
)
-5 -4 -3 -2 -1 0 1 2 3 4 5
1.2
1.4
1.6
1.8
2
2.2
2.4
2.6
2.8
3
0.1
0.2
0.3
0.4
0.5
0.6
100 µm scanning step
4 6 8 10 12 14 16-600
-400
-200
0
200
400
600
Pul
se e
cho
(mV
)
Time (s)
Pulse echoEnvelope
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
2 D Scanning
1 cm
Lateral distance (mm)
Long
itudi
nal d
ista
nce
(mm
)
-4 -2 0 2 4
-2
-1
0
1
2
0
0.2
0.4
0.6
0.8
1
X scanning step 150 µmY scanning step 200 µm
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Summary & Conclusions• Current piezo MEMS devices:
– Several piezo-MEMS devices are now in high volume production.– Growing maturity of manufacturing base will enable new devices.
• Future piezo MEMS devices: PMUTs– Today’s ultrasound sensors lack capabilities for consumer
electronics applications.– In air: Tiny 0.5 mm PMUTs have up to 1 m range.– In tissue: pulse-echo imaging demonstrated w/ 1.8V supply. – PMUTs are a disruptive technology for gesture sensing and
biometrics.
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David Horsley, UC Davis September 2014 Berkeley Sensor & Actuator Center
Acknowledgements• Prof. Bernhard Boser’s group (UC Berkeley)
– Richard Przybyla, Hao-Yen Tang, Igor Izyumen• Horsley group (UC Davis)
– Stefon Shelton, Yipeng Lu, Ofer Rozen, Andre Guedes, Stephanie Fung
• Sponsors– NSF & DARPA– Texas Instruments– Invensense– Capella Microsystems– Qualcomm
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