ee143 f2010 lecture 24 micro-electro-mechanical systems (mems) fabrication fabrication...
TRANSCRIPT
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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• Fabrication Considerations– Stress-Strain, Thin-film Stress, Stiction
• Special Process Modules for MEMS– Bonding, Cavity Sealing, Deep RIE, Spatial
forming (Molding), Layer Transfer
• Principle of Sensing and Actuation– Beam and Thin-Plate Deflections
• Micromachining Process Flows– MEMS-IC Integration
– BioMEMS, PhotoMEMS
Micro-Electro-Mechanical Systems (MEMS)
Fabrication
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Axial Stress and Strain
Stress s: force per unit area acting on a material
[unit: Newtons/m2 (pascal)]
s = F/A , A = area
s > 0 tensile
s < 0 compressive
Strain e: displacement per unit length (dimensionless)
e = L/ Lo
* Figure assumes there is no change in lateral dimensions
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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E = s / e [ in N/m2 (Pascal) ]
Poisson’s Ratio
= 0.5 volume conserved
E in GPa ( 1E9 N/m2)
Si 190
SiO2 73
Diamond 1035
Young’s Modulus of a material
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Stress-Strain CharacteristicFor low stress:
• material responds in elastic fashion
• (Hooke’s Law) stress/strain = constant
sy = yield stress
Ultimate stress - material will break;
For Si (brittle) ultimate stress ~ yield stress
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Mechanical Properties of Microelectronic Materials
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Material Choices
(a) Stiffness (b) Strength
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Poly-Si For MEMS Structure
• Effect of substrate:
single-crystal substrate
(clean surface)
epitaxial layer
amorphous substrate
polycrystalline film
• Average grain size
depends on
deposition &
annealing conditions
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Stress in LPCVD Poly-Si Films
• Stress varies significantly with process conditions
– strong correlation between microstructure and stress
Str
ain
vs. t a
nn
ea
l:
Tdep~620oC
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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1) Begin with a bonded SOI wafer. Grow
and etch a thin thermal oxide layer to act
as a mask for the silicon etch.
2) Etch the silicon device layer to expose
the buried oxide layer.
3) Etch the buried oxide layer in buffered
HF to release free-standing structures.
Si device layer, 20 µm thick
buried oxide layer
Si handle wafer
oxide mask layer
silicon
Thermal oxide
Use of SOI for MEMS Process
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Origins of Thin-film Stress
• Extrinsic– Applied stress
– Thermal expansion
– Plastic deformation
• Intrinsic– Growth
morphology
– Lattice misfit
– Phase transformation
stot = sth + sint + sext
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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substratesubstrate
Effect of Thin-film Stress Gradient on Cantilever Deflection
substrate
z
(1) No stress gradient along z-direction
(2) Higher tensile stress
near top surface of cantilever
before release from substarte
(3) Higher compressive stress
near top surface of cantilever
before release from substrate
Cantilever
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Thin-films Stress Gradient Effects on MEMS Structures
Top of beam more tensile
Top of beam more compressive
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Stressing along the x-direction, all layers take the same strain
Ex = fA EA+ fB EB
fA and fB are fractional volumes
* Material with larger E takes the larger stress
Stressing along the y-direction, all layers take the same stress
Ey =1/ [ fA / EA+ fB / EB ] * Material with smaller E takes the larger strain
AB
Effective Young’s Modulus of Composite Layers
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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PECVD silicon nitride using the SiH+ NH+ N chemistry.
Substrate RF bias is used to induce ion bombardment.
Because of the light mass, H+ ions can be assumed as the
dominant ion bombardment flux
H+ bombardment energy (eV)
Mechanical
Stress in nitride (in 1E8 Pa)
0
1000eV
Compressive
Tensile
-3
-6
+3
+6
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Use of Stressed Composite layer to reduce bending
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Thermal Strain
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Lecture 24EE143 F2010
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Biaxial Stress in Thin Film on Thick Substrate
No stress occurs in direction normal to substrate (sz=0)
Assume isotropic film (ex=ey=e so that sx=sy=s)
* See derivation in EE143 handout
(Tu et al, Electronic Thin Film Science)
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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t s
= substrate thickness
t f
= film thickness
E = Young’s modulus of substrate
n = Poisson’s ratio of substrate
Radius of Curvature of warpage
“Stoney Equation”
r = Es ts
2
( 1- )s 6 sf tf
See handout for derivation
Substrate Warpage
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Typical Thin Film stress: 108 to 5x1010 dynes/cm2
(107 dynes/cm2 = 1 MPa)
• Compressive (e <0)
– film tends to expand upon release
--> buckling, blistering, delamination
• Tensile (e >0)
– film tends to contract upon release
--> cracking if forces > fracture limit
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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The oxide stress is compressive
since r changes from 300m to
200m (Si wafer more curved)
Calculate Film Stress from change of curvature
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Deflection of Microstructures - Thin Plate approximation
Cantilever Beam with length L, width w, and thickness t
F in Newton
in N/meter
* Assumes L >> w and t, small deflection approximation
where
L = length of beam (in meter)
t =thickness of beam (in meter)
I = bending moment of inertia
= wt3/12 (in meter4) For reference only
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Deflection of Circular thin membrane
r = radius, t=thickness, P= uniform pressure (in N/m2)
For small deflections, maximum deflection in center
A more accurate
relationship
For reference only
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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kHz
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Stiction
Poly-Si beam released
without stiction after
sacrificial layer etching
Poly-Si beam
with two stiction points
after sacrificial layer etching
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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As the etching liquid is removed during a dehydration cycle, a liquid bridge is formed between the
suspended member and the substrate. An attractive capillary force which may be sufficiently strong
to collapse it. Even after drying, the inter-solid adhesion will not release the structure.
Solutions
• Dry etching (e.g. XeF2)
• Super-critical drying (e.g. rinse solution gradually
replaced by liquid CO2 under
high pressure)
• Hydrophobic Coatings
• Use textured surfaces
See C. H. Mastrangelo, “Adhesion-Related Failure Mechanisms in
Micromechanical Devices”, Tribology Letters, 1997
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Super-critical drying
i) release by immersion in aqueous HF;
ii) substrate and structure hydrophilic
passivation by immersion in a sulfuric
peroxide or hydrogen peroxide solution
resulting in hydrophilic silicon surfaces;
iii) thorough deionized water rinses
followed by a methanol soak to displace
the water;
iv) methanol-soaked samples placed in
the supercritical drying chamber for
drying.
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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* Dry, isotropic, vapor-phase etch
XeF2 vapor pressure (~3.8 Torr at 25 °C)
2 XeF2 + Si 2 Xe (g) + SiF4
(g)
Advantages :
• Highly selective to silicon with respect to Al, photoresist, and SiO2.
• Isotropic, large structures can be undercut.
• Fast ( ~10mm per hour)
• Gas phase etching, no stiction between freed structure and substrate
Disadvantages:
• No known etch stops for Si substrate
XeF2 Etching of Si
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Wafer Bonding
• Anodic bonding (E-field enhanced)
• Adhesive bonding (molten metal, epoxy)
• Direct wafer bonding
*can produce unique MEMS structures
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Anodic Bonding
Anodic Bonding: Low to moderate Temp, Rapid Process
glass
silicon
-1kV
T=300oC
* works mainly with alkaline-containing glass
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Example of Anodic Bonding
Pressure Transducer using membrane deflection
glass
glassglass
glass
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Bump
Chiao and Lin, UCB
Vibrating resonator
Al width=125 mm
Nitride
Water outsideAir inside
• After RTP for
750oC/10secs
• Al sealing ring
width=125mm
• Water is blocked outside
• Al does not wet glass well.
Add Cr adhesion layer
between Al and glass
Liquid Phase Bonding
Top viewCross-section
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Heat
Direct Bonding
Examples: Si-Si bonding and Si-SiO2 bonding
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Plasma TreatmentGases Used:
O2, He, N2, Ar
Pressure
200mTorr
Power
50W-300W
Time
15-30 seconds
+
O2
Bond Strengthening Annealing
Room Temp Bonding
Chemical Cleaning:
Piranha + RCA
-
Plasma Assisted Direct Bonding
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Requirements of Direct Bonding Surfaces
Surface micro-roughness ~ nm
No macroscopic wafer warpage
Minimal particle density and size: 1mm particle will give 1000mm void
Contamination free surface
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Permanent Bond Formation
O
O
O
O
Si
Si Si
O
OSi
Si Si
O
Si
Si Si
Formation of
Covalent bondHydrogen Bonding
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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3-D circuit with a metal
interconnect (at top), followed by a
memory substrate, a bond
interface, then logic metal, logic
transistors and a logic substrate.
• Bond memory substrate and
logic substrate.
• Thin both substrates with
grinding and CMP.
• Etch vias and metallization to
connect the two die.
http://www.ziptronix.com
Logic substrate
Memory substrate
Metal interconnects
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Uses high density plasma to alternatively
etch silicon and deposit an etch-resistant
polymer on side walls
Polymer deposition Silicon etch using
SF6 chemistry
Polymer
Deep Reactive Ion Etching
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Lithography , electroplating, and molding processes
to produce microstructures.
Very
thick
resist
Metal platingPlastic molding
Final microstructure
MoldingExample:LIGA Process (Lithographie, Galvanoformung, Abformung)
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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1) Deep silicon mold etch. 2) Sacrificial layer deposition.
3) Structural layer deposition. 4) Chemical-mechanical polish (optional).
and Deposition and patterning of a second polysilicon layer forms cross
linkages between the high-aspect-ratio molded polysilicon structures.
5) Release and extract molded part. Source: Keller and Ferrari
Professor N Cheung , U.C. Berkeley
Lecture 24EE143 F2010
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Thermal
OxidationDeposition
Sealing of Cavities