Components for Wireless Communication Mechanical/Electrical … · 2017-12-14 · Wireless...

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11

Texas Christian University Department of Engineering Ed Kolesar

Introduction toMicroeletromechanical Systems

(MEMS)Lecture 12 Topics

• MEMS for Wireless CommunicationComponents for Wireless CommunicationMechanical/Electrical Systems

Mechanical Resonatorso Quality Factor

OscillatorsVoltage-Tunable CapacitorsMicromachined InductorsFiltersSwitchesAntennas

Texas Christian University Department of Engineering Ed Kolesar

MEMS Overview

Micromachining: lithography, deposition, etching, …

Processes & Foundries

Devices & Structures

Methodology

History & Market

Introduction &

Background

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Texas Christian University Department of Engineering Ed Kolesar

MEMS for Wireless Communication

Why microfabrication?• Process integration• Mass fabrication• Beyond cell phones: combine sensing, actuation,

computation, and communication → intelligent sensor/actuator network (“smart dust”)

Why mechanical components?• High-frequency oscillators (GHz range and more)• Stability w.r.t. temperature, aging• Low loss oscillators (high quality factor)• Tunable oscillators (voltage controlled)

Texas Christian University Department of Engineering Ed Kolesar

Components for Wireless MEMS• Antennas• Amplifiers

• SwitchesResistively coupledCapacitively coupled

• Resonators• Filters• Oscillators

It is difficult to build integrated high quality electronic resonators for high-frequency applications (»1MHz)

→ Use discrete components, or→ Use corresponding micromechanical devices instead

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Texas Christian University Department of Engineering Ed Kolesar

Mechanical / Electrical Systems

Vi

L

C Vo

R

mK

mbm

ssFxsH

KbmFtKxtxbtxmxF

++==

=++

2

1

)(

:functionTransfer stiffness damping, mass,

)()()(nt displaceme :Output force external :Input

&&&

LCLRLC

i

o

iC

o

i

ssVVsH

CRLVtqtqRtqL

VV

12

1

1

)(

:functionTransfer capacit. resist., induct.,

)()()(

voltage :Output voltage :Input

++==

=++ &&&

x

F

b

Km

Texas Christian University Department of Engineering Ed Kolesar

Mechanical / Electrical Systems

Vi

L

C VoR

LCRC

LC

i

o

iCRCL

o

i

ssVVsH

CRLVtqtqtqL

VV

112

1

1

)(

:functionTransfer ecapacitanc ,resistance ,inductance

)()()(

voltage :Output voltage :Input

++==

=++ &&&

Alternative circuit:

44

Texas Christian University Department of Engineering Ed Kolesar

Resonators

• Analogy between mechanical and electrical system:Mass m - inductivity LSpring K - capacitance CDamping b - resistance R (depending where R is placed in circuit)

• Solution to 2nd order differential equation:

factorquality

system electrical system, mechanical

frequency natural 2

)(

100

00

20

2

20

0

Q

ωω

πfω

sssH

LCmK

Q

==

=

++=

ωωω

Texas Christian University Department of Engineering Ed Kolesar

Mechanical Resonator

• Frequency and phase shift under damping:

• Energy dissipation:

shift phase 4

-14

1-1

timedamping

)cos()(

2

0220

01

12

ϕ

ωτω

ωω

τ

ϕωτ

Kmb

bm

tAetxt

==

=

+= −

τt

eEtE −= 0)(

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Texas Christian University Department of Engineering Ed Kolesar

Quality Factor

• How fast does energy dissipate?• What is the maximum amplitude for a given frequency?

Definition: Quality factor (Q factor)Ratio of stored energy

and lost energy:

Mechanical system:

Similar for electric systems: (a)

(b)

bKm

bmQ == 0ω

CL

RRLQ 1

0 ==ω

τωτππ 022 ==∆

=TE

EQ

LCRRCQ == 0ω

Texas Christian University Department of Engineering Ed Kolesar

Quality Factor

• How fast does energy dissipate?

• What is the maximum amplitude for a given frequency?At resonance, amplitude is Q times the DC response

l)(mechanica 0 b

mQ== τ

ωτ

ω (1/s)

Gain (dB)

0

ω0

66

Texas Christian University Department of Engineering Ed Kolesar

Summary: Mechanical/Electrical Resonator

Mechanical resonator:

Torsional resonator:

Electrical resonator:

) small(for frequency natural

stiffness damping, mass, 0)()()(

0 bmK

KbmtKxtxbtxm

=

=++

ω

&&&

Ik

kbItktbtI

=

=++

0frequency natural

stiffness damping, inertia, ofmoment 0)()()(

ω

θθθ &&&

LC

CRL

tqC

tqRtqL

1frequency natural

ecapacitanc ,resistance y,inductivit

0)(1)()(

0 =

=++

ω

&&&

Texas Christian University Department of Engineering Ed Kolesar

Wireless Communication

Frequency Spectrum

2015105

RF

VLFLF

MFHF

VHFUHF

SHFEHF

IR

visible

UV X-rays

10n Hz

cm µmwavelength

77

Texas Christian University Department of Engineering Ed Kolesar

Wireless Communication Components

[Nguyen et al., 1998]

Texas Christian University Department of Engineering Ed Kolesar

Oscillators for Wireless Communication

• Current Technology:Quartz crystalSurface acoustic wave (SAW)Discrete elements (variable capacitors and inductors)

• Advantages:High quality factor: > 10,000Extremely high stability against thermal variations and agingExtremely selective filtering (small channel bandwidth)

• Problem: requires incompatible materials (e.g.,GaAs) → assembly necessary

88

Texas Christian University Department of Engineering Ed Kolesar

Oscillators for Wireless Communication

• Goals:High Q oscillatorsIntegrated VCO’s (voltage controlled oscillators)Compatibility with micromachining processesLow cost

• Challenges:Q is proportional to L (inductivity) or m (mass)Tunable devicesMEMS devices with sufficiently high C and LNoise from temperature changes, vibrations, agingInductor losses: eddy currents in substrate

Texas Christian University Department of Engineering Ed Kolesar

Oscillator Stability

[Nguyen et al., 1998]

99

Texas Christian University Department of Engineering Ed Kolesar

Voltage-Tunable Capacitors

[Young and Boser 1996]200µm

Texas Christian University Department of Engineering Ed Kolesar

Voltage-Tunable Capacitors

[Young and Boser 1996]

4 tunable parallel capacitors 2.04pF … 2.35pF3V tuning voltage, Q=62 at 1GHz

1010

Texas Christian University Department of Engineering Ed Kolesar

Micromachined Inductors

[Najafi et al., 1997]

NiFe core under planar metal spiral

2.7 µH inductanceQ=6.6 at 4MHz

Spiral inductor on substrate-isolating platform/membrane

1.2 nH inductanceQ=60-80 at 40GHz

Texas Christian University Department of Engineering Ed Kolesar

Micromachined Inductors

[Young and Boser 1997]

Electroplated 3D coil inductors with 4nH, Q=30 at 1GHz

1111

Texas Christian University Department of Engineering Ed Kolesar

Thin-Film Bulk Acoustic Resonators

[Lakin, Kline and McCarron 1995]

Thin-film bulk-acoustic mode piezoelectric resonator (FBAR)

Q > 100f0 = 1.5 - 7.5 GHz

Thin-film resonator on substrateAcoustic isolation by strategic

selection of separating layers

Texas Christian University Department of Engineering Ed Kolesar

Comb-Drive Resonator

Vp DC biasVd drive signal at ωd

I0 output current ∝ VpdC/dt

feedback via transimpedance amplifier

Vc carrier signal at ωc

output signal:frequency spectrum includes ωd , ωc , but also ωc±ωd

basis for frequency transfer (heterodyning)

[Figure: Maluf 2000]

1212

Texas Christian University Department of Engineering Ed Kolesar

Bandpass Filters

Intuition:• Two resonance modes• Loosely coupled

resonators: resonance modes are close and effectively form bandpass

• Additional coupled resonators widen frequency bandpass

[Figure: Maluf, 2000]

Texas Christian University Department of Engineering Ed Kolesar

Resonators and Filters

[Nguyen et al., 1998]

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Texas Christian University Department of Engineering Ed Kolesar

MEMS Medium Frequency Filters

[Nguyen et al., 1998]

Texas Christian University Department of Engineering Ed Kolesar

Cantilever Beam Switches

Issues:• Maxium current when ON, max. voltage when OFF• Impedance for DC to GHz frequency range• Speed, stiction, lifespan, contact deterioration

[de los Santos 1999]

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Texas Christian University Department of Engineering Ed Kolesar

Mercury Switches

• Side-driven mercury switch [Saffer et al. 1996]• Curved electrodes achieve small gap size (large el.stat. force)

over larger actuation range• Bumpers prevent electrode contact / short• Mercury drop (selectively deposited only on Au patches)• Originally fabricated in MUMPs

[S. Saffer et al., 1996]

Texas Christian University Department of Engineering Ed Kolesar

Capacitive Switches

• Metal membrane• Electrostatic actuation• Avoid stiction with

dielectric layer • Capacitive, not resistive

coupling • No DC component,

which is ok for microwave frequencies

[Goldsmith et al., 1996]

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Texas Christian University Department of Engineering Ed Kolesar

Antennas

[Gauthier, Courtay and Rebeiz 1997]

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