NIETZSCHE’S HELMBRECHT, OR: HOW TO PHILOSOPHISE WITH A PLOUGHSHARE
Professor Richard S. MullerMichael A. Helmbrecht MEMS for Adaptive Optics Michael A. Helmbrecht...
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Transcript of Professor Richard S. MullerMichael A. Helmbrecht MEMS for Adaptive Optics Michael A. Helmbrecht...
Professor Richard S. MullerMichael A. Helmbrecht
MEMS for Adaptive OpticsMEMS for Adaptive Optics
Michael A. Helmbrecht
Professor R. S. Muller
Professor Richard S. MullerMichael A. Helmbrecht
MEMS for Adaptive OpticsMEMS for Adaptive OpticsAdaptable-Mirror Section
Mirror Substrate
Solder-BumpElectrical Connections
Movable Mirror ElementsScale ~10s to 100s m
Scale ~ mm to cm
Current-DriverElectronics
Array of Elevating Mirrors
Professor Richard S. MullerMichael A. Helmbrecht
How Can We Elevate the Mirror Elements?
How Can We Elevate the Mirror Elements?
• Magnetic Actuation– Solenoidal structures
• Electrostatic Actuation– Vertical comb-drives
• Thermal Actuation– Thermal-bimorph structures– Our initial design approach
Professor Richard S. MullerMichael A. Helmbrecht
Thermal-Bimorph ActuationThermal-Bimorph Actuation
Large force Low voltage Long life
• 107 cycles without failure measured at BSAC
Actuators can be hidden under mirror
- Heat dissipation• Possible mirror
distortions• Possible electronics
problems
- Complicated linkage• Must be compliant when
bending• Must result in pure
translation of mirrors
Professor Richard S. MullerMichael A. Helmbrecht
Actuator DesignActuator Design
Static anchor anddrive electrodes
Mirror-bondingsiteTorsional flexure
Bimorphactuator
Side View
Front View
Static anchor anddrive electrodes
Mirror-bondingsiteTorsional flexure
Bimorphactuator
Side View
Front View
Static anchor anddrive electrodes
Mirror-bondingsiteTorsional flexure
BimorphactuatorStatic anchor - and -drive electrodes
Mirror-bondingsiteTorsional flexureBimorphactuator Side ViewFront View
Static anchor - and -drive electrodes
Mirror-bondingsite
Torsional flexure
Bimorphactuator
Side View
Front View
Professor Richard S. MullerMichael A. Helmbrecht
Mirror-Element LayoutMirror-Element Layout
Trench Flexure
Bimorph Layer 2
Bimorph Layer 1
Mirror Bond
Mirror
Contact
Professor Richard S. MullerMichael A. Helmbrecht
Thermal-Bimorph ActuatorsThermal-Bimorph Actuators• Tip deflects when 1
• is the coefficient of expansion
• hT-T0), (2-1), 1/w• Theoretical plot shown for:
• T-T0 =70°C• (2-1)=23.4 ppm/°C• w=1m
Theoretical Bimorph Deflection
0
10
20
30
40
50
0 100 200 300 400
Beam Length (m)
(Mirror Height
)m
h=1.5m
1
1
2
2
1
2
012
21
5))((2
3
−
√√↵
√√↵
+
+−−=
EE
EE
TTwl
h 2
ww
h
l
Professor Richard S. MullerMichael A. Helmbrecht
Bimorph Mechanical ModelBimorph Mechanical Model• Mirror element size l• Bimorph length l• Au- or Al-film on 10 m-
thick silicon (SOI)– Neglect bimorph mass
• Each bimorph layer thickness w
• Bimorph width b=20 m– Power scales with b
303)( TTl
h
bfR −∝
l
w
Mirror Mm
kb
wm
Torsional flexure
Professor Richard S. MullerMichael A. Helmbrecht
Mechanical-Resonance Frequency (h=10 m)
Mechanical-Resonance Frequency (h=10 m)
432
865
1.3E3
1.73E32.16E3
2.6E3
3.03E3 3.46E3
3.9E3 4.33E3
4.76E3 5.2E3 5.63E3
100 120 140 160 180 200 220 240 260 280 30010
20
30
40
50
60
Mechanical Resonance Frequency (Hz)
Bimorph Length (m)
T-T
0 (K
)
T-T
(K
) 0.15
0.29
0.44
0.59
0.73
0.88
1.0
1.2
1.3
1.5
1.6
1.8
100 120 140 160 180 200 220 240 260 280 30010
20
30
40
50
60Bimorph-Layer Thickness (m)
0
Bimorph Length (m)
Professor Richard S. MullerMichael A. Helmbrecht
Bimorph Thermal ModelBimorph Thermal Model
• Losses through the substrate dominate– Convection losses are negligible
• Mirror heats up to a fraction of the bimorph temperature (T - T0)mirror = (0.33 down to 0.125) (T - T0), for 100 m < l < 300 m
l
w
Mirror
Rbsgap
Rbmgap
Rb
Cb
IR2
Rmsgap
wm
Torsional flexure
Professor Richard S. MullerMichael A. Helmbrecht
1.2
2.4
3.6
4.8 6.07.2
8.4
9.6 11 12 13 14
100 120 140 160 180 200 220 240 260 280 30010
20
30
40
50
60Power (mW)
T-T0
K
Bimorph Length (m)
Thermal-Time-Constant -3dB Frequency and Power DensityThermal-Time-Constant -3dB Frequency and Power Density
2.33E3
4.66E3
7E3
9.33E3
11.7E3
14E3
100 120 140 160 180 200 220 240 260 280 30010
20
30
40
50
60Thermal Actuation -3dB Frequency (Hz)
Bimorph Length (m)
T-T
0 (K
)
Professor Richard S. MullerMichael A. Helmbrecht
• Mirror
Berkeley Bimorph ProcessBerkeley Bimorph Process
• Single-mask process
• Low-stress nitride (SixNy) and aluminum bimorph
• Other processes under consideration– Hidden actuators – Electrostatic actuators– Bonded mirrors
Current path
Mirror
Die photo - actuated, released mirrors
Professor Richard S. MullerMichael A. Helmbrecht
ConclusionsConclusions
• Bimorph actuator is small and can be fabricated under the mirror– Fill factor > 98%
• Bimorph actuators can be tiled in an arrays to actuate large numbers of mirrors
• Bimorph actuator provides large tip deflection (h = 10 m)• Models show frequency requirements are met (f>1 kHz)• Bimorph actuators have been fabricated
– Testing is underway