introduction to rfmems (microelectromechanical...
TRANSCRIPT
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Microsystems Integration Laboratory
Introduction to RFMEMS (Microelectromechanical Systems)
Yu-Ting Cheng
Microsystems Integration Laboratory (MIL)
Department of Electronics Engineering
National Chiao Tung University
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Microsystems Integration Laboratory
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Microsystems Integration Laboratory
Rf mems components and technology Antennas:
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Microsystems Integration Laboratory
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Microsystems Integration Laboratory
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Microsystems Integration Laboratory
dx
dxdLzdx
zdxdL
ddx
dzdL
x
)(
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Microsystems Integration Laboratory
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Microsystems Integration Laboratory
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Microsystems Integration Laboratory
Capacitive Transducers
• Parallel-plate capacitor:
dg
dCV
A
QW
A
gQ
C
QW(Q)
εA
QECVQdqqVW
g
A
q
2222
0
2
1
2Force,
22 :Energy Potential Stored
:Field Electrical, :Charge ,)( :Energy
C :eCapacitanc
Fixed plate
W g
V
I
L
Movable plate
Z •We can store energy in the capacitor by either fixing the gap and changing the charge Q, or by fixing the charge and changing the gap.
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Microsystems Integration Laboratory
Two-Port Electro-Mechanical Capacitor
• The capacitor has two port as shown in the following figure:
• Electrical parameters: voltage V and current I • Mechanical parameters: Force F and velocity v
W (Q, d)
Capacitor
F V
I=-dQ/dt v=dg/dt
A
QgV
A
QW
A
gQ
C
QW(Q)
2Force
,22
2
22
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Microsystems Integration Laboratory
Sensitivity
g
W
S
S
vs.
dx
dC
CC
SS
dx
dCS
ca
cg
ccr
c
:area overlap varying gap varyingof Comparison
1:ysensitivit Normalized
:ySensitivit
00
From Prof. K.
Najafi’s MEMS Slides
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Microsystems Integration Laboratory
Mechanical-Electrical Equivalent
From Prof. K.
Najafi’s MEMS Slides
Mechanical Electrical
Variable Velocity
Force
Current
Voltage
Lumped Elements Compliance (1/k)
Mass (m)
Damper (c, or b)
Capacitor (C)
Inductor (L)
Resistance (R)
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Microsystems Integration Laboratory
Factors in The Design
• Fringing Fields: around the perimeter of the electrodes in a capacitive device, the electrical field lines have to bend which are called fringing fields. The fringing fields will make the actual area between the two plates appear larger.
• Air Damping: for many capacitive transducers, we see limitation on bandwidth caused by a phenomenon called air damping. Most of these sensors operate at atmospheric pressures, and when the movable electrode moves, it has to push or squeeze air in and out of the very small gap in between electrodes which is called” squeeze film damping”. There is also viscous drag damping when two plates move parallel to another.
)ln(2
g
WW
g
AC
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Microsystems Integration Laboratory
Squeeze Film and Viscous Drag Damping
• Squeeze film damping
• Viscous Drag Damping
)./101.81 :(air fluidambient ofViscosity :
,~
5- smkg
MKA
dQ
air moving out of the gap
Plate moving down
separation Gap :
Length :
width: where
)()/( 3
g
L
W
Lg
WLWfb
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Microsystems Integration Laboratory
RF MEMS Type Switch
Series contact switch:
contacts.between separation physical theis and
capacitor, theof area effective : voltage,applied :
ratio. sPoisson' and modulus sYoung' theare and
ly.respective beam, theof
thicknessand length, width, thware and , , where
2
)1(6
2
2
0
3
332
g
AV
E
tLW
g
AVF
Wt
L
E
LF
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Varadan et al., RF MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Hysteresis Behavior
Varadan et al., RF MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
MEMS Switch Factors
MEMS switches, in general, work with very high driving
voltage which is about several tens voltage. Such high
actuation voltage make the switches far beyond the
compatibility of standard IC technology because for RF
applications and microelectronic systems the voltage
should be around 5V.
In order to achieve the goal, several approaches have
been implemented for the design of the RF MEMS
switches: (a)increasing the area of actuation (b)
decreasing the gap between the switch and the bottom
electrode, ( c ) designing the structure with a low spring
constant.
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Microsystems Integration Laboratory
Flexible Structural Design
Varadan et al., RF MEMS
and Their Applications ,
Wiley
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Microsystems Integration Laboratory
Rf mems components and technology SP3T switch
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Microsystems Integration Laboratory
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Microsystems Integration Laboratory
RF MEMS Capacitive Switches
• Voltage actuation For voltage actuation, a dc potential is applied between the bridge and the base
electrode. The force downward on a charged beam above a ground plane is
proportional to the square of the electric field E on the beam.
V: applied voltage
g: the height of the beam above the ground plane
go: is the undeflected height
A : the area
K: spring constant include the beam thickness,
length, and width, the Young's modulus, residual
stress
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Microsystems Integration Laboratory
RF MEMS Capacitive Switches
• Voltage actuation
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RF MEMS Capacitive Switches
• Capacitance Ratio
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RF MEMS Switch
Top view of the NTU capacitive shunt
switch
Cross section
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RF MEMS Capacitors
Feature
• Remove lossy substrate from
beneath
• Tunable with movable,metallic
MEMS structure
Characteristics
• High quality factor (Q)
• Tunable
Suspended capacitor
Suspended metal-insulator-metal capacitor
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Microsystems Integration Laboratory
RF MEMS Capacitors
Top view of the the three-plate polysilicon MEMS varactor
Cross section
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High Performance Capacitors
A metal-insulator-metal (MIM) capacitor fabricated on a suspended
membrane shows that the best Q of a 2.6pF capacitor exceeds 100 at
2GHz as compared wit the same capacitor fabricated directly on silicon
which has a Q less than 10.
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
MEMS Gap-Tuning Capacitor
Structure: the electrodes are 200um by 200um with2 um by 2um holes
spaced 10um apart.
Performance: Q~62. The capacitance varied from 2.11 to 2.46 pF when
applied voltage changed from 0 to 5.5.V, which corresponds to a tuning
range of 16%
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Fundamentals of MEMS Gap-Tuning Capacitor
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
MESA (MicroElevator by Self-Assembly) Capacitor
The 250x250 um2 polysilicon plate is raised above the substrate by four
300um long side supports which are controlled by microactuators. The
capacitance is changed from 500fF to 20fF when the suspended
electrode is raised by 250um.
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
MEMS Area-Tuning Capacitors
The variable capacitor provides
a capacitance change from
0.035pF to 0.1pF with bias
voltages ranging from 80 to 200V.
The capacitor provides
continuous tuning range of at
least 200% or 3:1 tuning ratio.
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
RF MEMS Capacitors
Top view of the University of Illinois Wide-tuning-range
varactor
Cross section
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PZT (PizeoElectric-actuator) Tuning Capacitor
A MEMS capacitor integrating
with pizeoelectric actuator has
advantages such as low driving
voltages and linear tuning
capacitance
The PZT actuators are fabricated
on silicon substrate and are diced
and bonded to TML on a quartz
substrate using flip-chip bonding
technology.
Low driving voltage ~6V
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Planar Inductors
High Q’s (> 30) RF components
are required for high frequency
selectivity in communication
systems especially for the high-
performance low power RF
transceivers.
For the compactness requirement,
on-chip planar inductor and diode
capacitor design becomes the
major approach in the fabrication of
RF front end transceivers.
In general, the Qs of planar spiral
inductors or junction dioide
capacitors are only of the order of
low 10s at higher frequencies.
inductance mutual the:
segments.straight theall
of inductance self theof sum the:
.inductance total the:
0
0
M
L
L
MLL
T
T
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Cont.
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Cont.
The quality factor Q of an inductor is written as Q=L/R, where is the
operating frequency.
The separation between lines should be as small as possible.
The circular spiral inductor has a shorter conductor then square spiral
and the Q is about 10% higher than that of a square spiral having the
same value of d0
Higher Q can be achieved with increasing the number of turns per unit
area; however, it also lowers the self-resonance frequency as a result of
the increase in capacitance
To avoid parasitic effects, the maximum diameter of the inductor should
be less than /30.
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Microsystems Integration Laboratory
Lumped Model of An Planar Spiral
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Substrate Effect
Simulation Results:
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Air Gap Design
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Spiral Inductor with Air Gap
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Resistance Effect
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Microsystems Integration Laboratory
MEMS Type Inductor Design
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Cont.
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Summary
Varadan et al., RF MEMS and Their Applications , Wiley
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Microsystems Integration Laboratory
Cont.
Varadan et al., RF MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Cont.
Varadan et al., RF MEMS and
Their Applications , Wiley
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Microsystems Integration Laboratory
Evolution of MEMS Type Capacitors
Varadan et al., RF MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
Filters
Low-pass filter, high-pass filter, bandpass filter, and bandstop filter are
very important components in RF circuit which are designed to accept or
reject frequencies containing desired information.
Varadan et al., RF
MEMS and Their
Applications , Wiley
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Microsystems Integration Laboratory
The Micromachined Suspended Inductor and The Reliability Issue
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Microsystems Integration Laboratory
The Process Flow of The Optimum Design
Un-Deformed Spiral Inductor
ANSYS Simulator for Mechanical Analysis
Node Solution and Node Coordinate
Deformed Spiral Inductor with Node Coordinate
Re-building the Deformed Spiral Inductor in HFSS Simulator
Equivalent Circuit Model Parameters Extraction
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The Inductance Variation of the Suspended Inductor Due to the Accelerative
Disturbance
•Morphology deformation would result in large inductance variation
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The Suspended Inductor with the Blanket Membrane Supporting
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The Reliability Issue of The Blanket Membrane Inductor
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Microsystems Integration Laboratory
The Fields Analysis and The Mechanical Analysis of the Micromachined Inductor
The surrounding magnetic
fields
Orthogonal Magnetic Fileds
Weak Magnetic Coupling
Parallel Magnetic Fields
Strong Magnetic Coupling
The surrounding magnetic
fields
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Microsystems Integration Laboratory
The Thermal Stress Analysis of the Optimized Micromachined Inductor
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The Fabrication Procedure of the Optimized Micromachined Inductor
The proposed optimum inductor.
The process flow of the optimum inductor.
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Microsystems Integration Laboratory
Result & Discussion -Temperature Variation
The inductance
variation is
increased with
the increasing
frequency.
The increasing
trend of the
inductance
variation is
shifted to the
higher
frequency.
Due to the
unstable
suspended
structure and the
complex motion,
the inductance
variation is not
related with
frequency directly.
The thermal stress can
be released by the
corner region
The deformation can be
shifted to the corner.
Low restrictive region
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The Comparison of the Performance Between the Suspended, Blanket Membrane
and Cross Membrane Inductors
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The Modeling of Micromachined Inductor
Ls Rs
Cs
Ls : physics-based closed-form expression [1]
Cs : Distributed capacitance model (DCM) [2]
Rs :
depthskintheist
w
lRs
,
exp1
freq (2.000GHz to 12.00GHz)
S(2
1,2
1)
S(2
1,2
2)
S(2
5,2
5)
S(2
5,2
6)
S(2
4,2
4)
S(2
4,2
3)
3 4 5 6 7 8 9 10 112 12
-10
-8
-6
-4
-2
-12
0
freq, GHz
dB
(S(2
1,2
1))
dB
(S(2
5,2
5))
dB
(S(2
4,2
4))
dB[S11]
Simulated by equivalent model
Simulated by HFSS
Measured result
Compare the model, simulation, and measured results
of inductor @2.3nH for frequency 2~12 GHz.
dB
S11
S11
S12
Complete optimized design
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Microsystems Integration Laboratory
Physics-Based Closed-Form Inductance Expression
l
nd
l
nd
nd
l
nd
lnn
twn
llLp
441
441ln147.02.0ln
2
22
0
1231123
i
ii
Nn
NNnswd
Distributed Capacitance Model (DCM)
1
1
2)]1(1[4
1n
k
kmms kdkdlCC
kk hhhhkd 121
kkk
k lllllll
h 121, .
1ln
0)(
tw
sC
effr
mm
where w is the metal width, s is the spacing between segments, n is the number of turns,
Ni is the integer part of n, and l is the total length of inductor
ococps LLLL , is the contribution of inductance of the bridge.
, the capacitance per unit length between adjacent metal tracks.
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Microsystems Integration Laboratory
Kramers Kronig Relations
• Anomalous Dispersion
• Standing Wave B.C.’s
• Compton Scattering
• Inductance
'
'Im''
2Re
0 220
dP
'
'Re'
2Im
0 22
0
dP
rh
qrE ˆ
12csc2
4sin8
4
1)(
22
0
))(Re1(02
dI
dvBHL
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Microsystems Integration Laboratory
• Electron kinetic energy in sample metal
Determination of Self-Resonant Frequency
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Microsystems Integration Laboratory
• Scattering potential in corners
Determination of Self-Resonant frequency
inductor) (circular for , 7.24
24
4
for , 2
csc8
4sin8
4
2
3/2
2
2
22
32
2
eff
effC
NV
q
NV
q
E
• Self-resonant frequency
CLr ENE
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Microsystems Integration Laboratory
• Frequency-depended form of inductance
Determination of Inductance
1
2
0
3
0 rec 1exp 2
TkAn
lnL
B
rrtotale
1
2
0
3
0 oct 1exp 5
3
TkAn
lnL
B
rrtotale
1
2
0
3
0 cir 1exp
TkAn
lnL
B
rrtotale
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Microsystems Integration Laboratory
Model Validation
Comparisons (n=3.5)
SRF based on the model (GHz)
SRF based on HFSS (GHz)
Rectangular 23.9 22.9
Octagonal 24.9 23.6
Circular 25.8 24.6
Number of Turns 1.5 2.5 3.5 4.5 5.5
ωr for HFSS (GHz) 39.5 27.1 22.9 20.6 19.4
ωr for the model 38.6 28.6 23.9 21.4 19.9
ωr for G model X X X X X
L for HFSS @ 3GHz(nH) 1.58 2.94 4.27 5.31 6.01
L for the model @ 3GHz 1.18 2.65 4.13 5.32 5.95
L for G model @ 3GHz 1.60 3.02 4.28 5.18 5.60
L for HFSS @ 5GHz 1.58 2.99 4.38 5.49 6.21
L for the model @ 5GHz 1.19 2.71 4.25 5.51 6.20
L for HFSS @ 9GHz 1.63 3.22 4.92 6.31 7.23
L for the model @ 9GHz 1.24 2.91 4.74 6.33 7.30
Less CPU processing time 6400 times difference (Ansoft HFSS)
*3.4GHz double CPUs and 2048MB DDR2 RAMs.
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Microsystems Integration Laboratory
RF MEMS Inductors
Feature
• Remove substrate from
beneath coil
• Achieve 3D coil
geometry
Characteristics
• High quality factor (Q)
• High resonant frequency
• Compact size
Micromachined inductors on thin
membranes.
The resonant frequency 70 GHz for
the 1.1 nH inductor.
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Microsystems Integration Laboratory
RF MEMS Inductors
An on-chip tunable micro
inductor with moveable
magnetic core in the 3D on-
chip solenoid coil
Schematic of an on-chip tunable micro inductor
http://mems.utdallas.edu/pictures/rfid/index.htmhttp://mems.utdallas.edu/pictures/rfid/index.htm
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Microsystems Integration Laboratory
RF MEMS Inductors
An on-chip 3D arch-shape
solenoid inductor
A 3D on-chip toroidal
inductor
http://mems.utdallas.edu/pictures/rfid/index.htmhttp://mems.utdallas.edu/pictures/rfid/index.htm
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Microsystems Integration Laboratory
RF MEMS Inductors
Micromachined 3D copper
spiral inductors integrated on
a TSMC-fabricated
RFIC chip
A 3D on-chip solenoid
inductor with nano magnet wire
core integrated in it
http://mems.utdallas.edu/pictures/rfid/index.htmhttp://mems.utdallas.edu/pictures/rfid/index.htm
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Microsystems Integration Laboratory
RF MEMS Transmission Lines
Feature
• Substrate removed from
between or beneath
coplanar waveguide
transmission lines
Characteristics
• Greatly reduced
dielectric loss
• Transmission is
conductor loss limited
• Reduction in unwanted
moding of CPW
W-band micromachined coupled-line filter
Cross-section of the filter structure
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Microsystems Integration Laboratory
MEMS Distributed Phase Shifters
Periodic loading of transmission lines with MEMS
capacitive switches creates a structure with a variable phase
velocity
• Circuit schematic of the phase shifter
• Equivalent Circuit
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Microsystems Integration Laboratory
MEMS Distributed Phase Shifters
• Photograph of the fabricated one bit phase shifter
• Photograph of the fabricated three bit phase shifter
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MEMS Switched delay line Phase Shifters
The switches of the phase shifters in a cascaded are
configured in different lines which can be selectively
controlled for the propagation of RF signals
• Circuit schematic of the phase shifter
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Microsystems Integration Laboratory
MEMS Switched delay line Phase Shifters
• Photograph of the fabricated switched
delay line phase shifter
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Phase Array Antenna
Principle of a phased array antenna using phase shifters
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MEMS Resonator
Vertically-Driven Micromechanical Resonator
• To date, most used design to achieve VHF frequencies
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Microsystems Integration Laboratory
MEMS Resonator
• Photograph of the fabricated
HF MEMS Resonator
• Extracted Q =8,000
(vacuum)
• Freq. influenced by dc-
bias and Anchor effect
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Microsystems Integration Laboratory
Transceiver Front-End Architecture Using Vibrating Micromechanical Signal Processers
•Proposed and Developed by Professor Nguyen at UM
•Courtesy by Professor Nguyen
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Microsystems Integration Laboratory
MEMS Filter
• Photograph of the fabricated HF Spring-
Coupled Micromechanical Filter
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MEMS-Based Transceiver Architecture
Micromechanics are shaded in green
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Microsystems Integration Laboratory
MEMS-Based Transceiver Architecture
Micromechanics are shaded in green
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Microsystems Integration Laboratory
RF MEMS Circuit
C. T. C. Nguyen, Proceeding,
1998, Sensors Expo. 447~455.
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Microsystems Integration Laboratory
Wine-Glass Micromechanical-Disk Reference Oscillator -Nguyen
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Microsystems Integration Laboratory
Wine-Glass Micromechanical
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Microsystems Integration Laboratory
Wine-Glass Micromechanical-Disk Reference Oscillator -Nguyen
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Microsystems Integration Laboratory
Packaging Object
• MEMS packaging: Object: a system
IC +Mechanical+Optical+Bio...
Function:
protect system and provide
special environment for inside
devices
Cost:
More than 30% of product
expense in IC than MEMS cost
more!!!
ADXL50 by Analog Devices. Inc.
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Microsystems Integration Laboratory
Packaging Challenge
• MEMS Packaging Challenge : no universal solutions, cost could be very high, multi-disciplines required but very few research effort.
Hermetic/vacuum package
Low temperature package
High density IC interconnects (with IC integration)
Chemical resistant
Special requirements: high precision, high g shock, and high melting point…….
• Solution: Using existing IC packaging solutions:
MCM, BGA, Flip chip techniques, 3-D stacking….etc..
Developing several unit processes for MEMS packaging applications
Wafer to wafer bonding using anodic or fusion bonding
Localized heating and bonding (LHB) technique
High precise splicing using micropipes
Metal composite for 3-D through via Interconnects
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Microsystems Integration Laboratory
• Post-process packaging method: lid sealing, wafer bonding, and microshell encapsulation
More process flexibility in the system
Hermetic Encapsulation Approach
• Integrated encapsulation:
DC V
AC V
DC V
AC V
DC V
AC V
DC V
AC V
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Microsystems Integration Laboratory
Localized Heating
• Finite element analysis shows isotherms around a 5 m wide microheater capped with a pyrex glass substrate
5m
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Microsystems Integration Laboratory
mechanical Resonators with On-chip Resistive heaters
• Design layout • Close SEM View
• SEM of µ-mechanical resonators before vacuum encapsulation
Aluminum(Si) Solder
Folded-Beam, Comb Drive
µMechanical Resonator
• SEM of the resonator after breaking glass cap
Ground Pad Bias Pad
Sense Pad
Drive Pad
Anneal Pad
Aluminum/Si Solder
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Microsystems Integration Laboratory
Device Fabrication Processes
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Microsystems Integration Laboratory
Scheme of Vacuum Encapsulation
Device Substrate
Glass Cap
Pressure
Heating Pad
PECVD
Vacuum ~ 25 mtorr,
input power: 3.4 W,
bonding time: 10 mins
1st Step : resonator and glass cap fabrication
2nd Step : alignment and contact
3rd Step : vacuum and bonding
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Microsystems Integration Laboratory
Vacuum Encapsulated High Q resonator
•Transmission spectrum with 120 mins. waiting time
-80
-65
-50
-35
-20
57.68 57.73 57.78 57.83 57.88
Frequency [KHz]
Tra
ns
mis
sio
n [
dB
] Q=9600
•Q factor vs. Pressure Q factor vs. Pressure
0
2000
4000
6000
8000
10000
12000
0.0001 0.01 1 100 10000Torr
Q f
ac
tor
Before
Annealing
After
Annealing
Before
Annealing
with higher Q
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Microsystems Integration Laboratory
Reliability
•IEEE/ASME, JMEMS, Oct. , 2002, ~54 weeks
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Microsystems Integration Laboratory
Wafer Level Chip Scale Packaging Design
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Microsystems Integration Laboratory
What is SOC?
• SOC means “System on a Chip”. It is defined that the system contains embedded CPU, memory, interface circuits, such as USB, PCI, Internet, and mixed-signal blocks..etc.
• In fact, it should contains more and more functional chips including MEMS sensors and actuators in the future.
• Driving forces: demanding application, shrinking product cycles, process technology, and the need for mass productivity with lower cost.
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Microsystems Integration Laboratory
Is Hermetic Package Necessary to MEMS?
• Wafer level process cost • Structure release or dicing first?
•Failed capacitive accelerometer.
(a) washed out during the dicing process.
(b) stuck to the bottom electrode during the dicing process.
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Microsystems Integration Laboratory
Low temperature wafer level hermetic encapsulation
• Low temperature wafer level hermetic encapsulation using UV curable adhesive (IEEE 54TH ECTC, 2004)
Figure 10. Four inch wafer level bonding.
Air Trapping
600μm
Figure 11. A packaged overlapping parallel capacitor.
Capacitor
Wafer
Contact Pad
Glass Protection Cap
•Encapsulated accelerometer
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Microsystems Integration Laboratory
Packaging Process
Figure 2. UV curable adhesive wafer level bonding scheme
Transparent Vacuum Chuck
Contact Pads
UV Curable Adhesive
Wafer
Glass Protection Cap
Device
Separation Cut
Die Cut
Figure 4. The removal of glass over contact pads.
Contact Pad
Dummy
Clip
Glass Cap
Vacuum Chuck Windshield
Double Side Tape
Figure 7. Second spin setup.
(a)
Glass Protection Cap
Silicon Substrate
UV Curable
Adhesive
Residue
Bonding
Region
Glass Protection
Cap
Silicon Substrate
Bonding
Region
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Microsystems Integration Laboratory
Systems on a Package (SOP)
•Goal: With the same performance as SOC (Systems on a Chip) using standard Si processes but with lower cost and higher manufacture yield.
SCC
DRAM
DRAM DRAM
DRAM
CPUs with e-DRAM
MSC
Transceivers
Transducers SCC SCD SCD MSC
•Sze et al.,
•2-D MCM
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Microsystems Integration Laboratory
SoC: From Board to Chip
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Microsystems Integration Laboratory
SoC (System-on-chip)
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Microsystems Integration Laboratory
Trends of Process Technology
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Microsystems Integration Laboratory
Cu Interconnects
Moore’s Law: the number of transistors per square inch on integrated
circuitry had doubled every year since the integrated circuit was invented.
Although in subsequent years, the pace slowed down a bit, but data
density has doubled approximately every 18 months, and this is the current
definition of Moore's Law.
Chip Area (mm2)
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Microsystems Integration Laboratory
Cu Interconnects
The speed limitations of circuitry caused by interconnects can be
simply estimated based on the delay time:
linect interconne theofy resistivit theis and field fringing the todue isK
oxide, theofconstant dielectric theis K where
1189.089.0
I
ox
2
0
sox
oxILWLHx
LKKRC
Ref. Havemann et al. IEEE,
2001
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Microsystems Integration Laboratory
Capacitive Delay of Interconnections
An interconnection can be treated as a capacitor which
can either be charged and discharged using the inverter
circuit as shown in the following since the capacitance
arises in part from the metal conductors of the
interconnect and ground circuitry. The stray capacitance is
also introduced by the physical proximity of other
interconnects.
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Microsystems Integration Laboratory
國立交通大學 電子與資訊研究中心 National Chiao-Tung University
Microelectronics and Information Systems Research Center
110
2003 ITRS Roadmap
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Microsystems Integration Laboratory
Challenges in the Present and Future System Integration
• Data communication speed limited
• Process limited; hard to optimize system performance
• High testing cost and thermal problem in a complex
SOC system
• Signal Integrity
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Microsystems Integration Laboratory
DRIE for Packaging Applications
Recent 3-D Packaging Structure; Sharp.
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Microsystems Integration Laboratory
3-D Stacked Chip Concept
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Microsystems Integration Laboratory
3-D Stacked Chip Concepts
RPI Fraunhofer Institute
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Microsystems Integration Laboratory
Packaging Technology Roadmap
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Microsystems Integration Laboratory
Si Based Heterogeneous Integration
Performance Cost Form Factor Process Complexity
Conventional SOC
(System-on-Chip)
Excellent Low
(Batch Process)
Small Complicate
Silicon Based
SOP
(System-on-Package)
Could be Similar to SOC
Could be the Same (Batch Process)
Could be Same Area to SOC but thicker structure
Could be Simpler
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Microsystems Integration Laboratory
MEMS Challenges
• From device fabrication point of view: the challenge is to integrated and process all of these heterogeneous materials together in a complex microsystems. Sometimes it has to include planar, nonplanar fabrication technologies, such as IC processes, micromilling, laser micromachining, wafer bonding…etc.,
• From product point of view: there is no reliable method yet that would qualify as a versatile post-process packaging for MEMS with the rigorous process requirements of low temperature, hermetic sealing, and long-term stability….etc.