Mechanics and Tribology of MEMS Materials - prod.sandia.gov ...
Mechanics and Tribology of MEMS Materials - prod.sandia.gov ...
Mechanics and Tribology of MEMS Materials - prod.sandia.gov ...
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captured the Si2p, C1s, O1s <strong>and</strong> W4f peaks. Si, O <strong>and</strong> W peaks were acquired at 0.2 eV/step,<br />
while C was acquired at 0.1 eV/step. After analysis, the spectra were smoothed using a 19-point<br />
Savitsky-Golay algorithm, satellite subtraction was performed, <strong>and</strong> the spectra were shifted to<br />
provide a constant Si2p3/2 peak position at 99.3 eV. Atomic concentrations were calculated from<br />
the detailed scans using h<strong>and</strong>book sensitivity factors.<br />
8.2.3 Tribological Measurements <strong>of</strong> Tungsten-Coated Surfaces<br />
The dynamic friction coefficient <strong>of</strong> tungsten coated devices was determined using the<br />
<strong>MEMS</strong> devices shown in Figure 7.1. All measurements were conducted in laboratory ambient<br />
atmosphere (23°C, 20% relative humidity) using bare die <strong>and</strong> drive signals applied with probes<br />
making contact with electrical contact pads on the device. A DC voltage was applied to the<br />
loading actuator to bring the beam into contact with the post (Figure 7.1b). Normal load is<br />
estimated at 10 µN based on the applied voltage <strong>and</strong> displacement <strong>of</strong> the beam. A square wave<br />
is applied to the oscillation axis to drive the beam back <strong>and</strong> forth against the post at some<br />
amplitude. A frame grabber is triggered at each end <strong>of</strong> the stroke <strong>of</strong> the beam, <strong>and</strong> images <strong>of</strong> the<br />
relative position <strong>of</strong> the movable beam with respect to the post are acquired. Image processing<br />
was used to calculate the displacement <strong>of</strong> the beam as a function <strong>of</strong> voltage applied to the<br />
oscillation actuator. The amplitude <strong>of</strong> the beams motion when in contact with the post,<br />
compared to the motion amplitude in the absence <strong>of</strong> contact, allows the friction force at the<br />
beam/post interface to be calculated as described by Senft <strong>and</strong> Dugger [8.5], using the lateral<br />
stiffness <strong>of</strong> springs in the friction structure <strong>and</strong> the calibration parameters for displacement<br />
versus voltage.<br />
8.3 Results <strong>and</strong> Discussion<br />
A polycrystalline structure treated with selective tungsten is shown in Figure 8.1. The<br />
tungsten forms a thin layer that covers the polycrystalline silicon conformally, even in shadowed<br />
surfaces. Transmission electron microscopy revealed that the coating process forms a layer <strong>of</strong><br />
tungsten that is self-limiting, <strong>and</strong> on the order <strong>of</strong> 20 nm thick [8.4].<br />
Si<br />
polySi<br />
Fig. 8.1 Cross section <strong>of</strong> a polycrystalline silicon (polySi) anchor on single crystal Si, treated<br />
with selective tungsten. The silicon has been etched back to reveal the thin layer <strong>of</strong><br />
tungsten covering all surfaces.<br />
76<br />
W<br />
1 µm