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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strength. The subsequent chapter discusses the observed strength behavior, using this improved<br />
test methodology.<br />
1.2 Improvement <strong>of</strong> <strong>MEMS</strong> Tensile Strength Evaluation Methodology<br />
Several testing techniques have been published with widely varying tensile strengths<br />
appearing in the literature - between 1 to 4 GPa [1.1-1.6]. Much <strong>of</strong> the variation between authors<br />
has been explained in terms <strong>of</strong> microstructural differences due to deposition conditions, sample<br />
size effects <strong>and</strong> release processing. A previous cross comparison exercise involving direct <strong>and</strong><br />
indirect testing techniques using the same material, but different releases techniques, reported<br />
significant variations [1.7].<br />
Tensile data was collected from five investigators that employed two essentially different<br />
types <strong>of</strong> samples, with further variations in size within each group. The larger sized group <strong>of</strong><br />
samples were designed to be gripped with an electrostatic force applied to the enlarged end <strong>of</strong> a<br />
sample, the tensile force application <strong>and</strong> measurement were performed with a macro scale<br />
system; slightly different versions <strong>of</strong> this system were used by Tsuchiya [1.8], <strong>and</strong> Sharpe <strong>and</strong><br />
Coles [1.9]. Chasiotis <strong>and</strong> Knauss also tested this size sample, but used the electrostatic force<br />
only to assist in the adhesive bonding <strong>of</strong> the sample to the grip [1.10]. Samples <strong>of</strong> four sizes<br />
were tested by these three labs, with widths <strong>of</strong> 6 <strong>and</strong> 20 µm <strong>and</strong> lengths <strong>of</strong> 250 <strong>and</strong> 1000 mm.<br />
The second sample type, tested by Read [1.11], <strong>and</strong> by LaVan at S<strong>and</strong>ia [1.12], is 1.8 µm wide<br />
<strong>and</strong> 15 to 1000 µm long.<br />
All <strong>of</strong> the samples were <strong>prod</strong>uced using S<strong>and</strong>ia National Labs SUMMiT TM IV polysilicon<br />
process – they were patterned in the poly1-2 composite layer that is 2.5 mm thick. Samples <strong>of</strong><br />
all sizes were <strong>prod</strong>uced side by side on the same die, five or more die were sent to each<br />
participant. The films were deposited as n-type, fine grained polysilicon from silane in a low<br />
pressure chemical vapor deposition (LPCVD) furnace at ~580°C. The intervening sacrificial<br />
oxide layers were also deposited in an LPCVD furnace from tetraethylorthosilicate (TEOS) at<br />
~720°C. This process usually uses 6-inch, (100) n-type silicon wafers <strong>of</strong> 2 to 20 ohm/cm<br />
resistivity covered by 6000 Å <strong>of</strong> thermal oxide followed by 8000 Å <strong>of</strong> LPCVD silicon nitride for<br />
electrical isolation. Thickness was accurately controlled during the deposition process <strong>and</strong> was<br />
measured, along with width, in a calibrated SEM after release (accuracy 0.1 µm). The samples<br />
were released, coated with a self-assembling monolayer (SAM) such as octadecyltrichlorosilane<br />
(ODTS) or perfluorodecyltrichloro-silane (FDTS) as an anti-stiction coating <strong>and</strong> then dried with<br />
super-critical CO2. The microstructure <strong>and</strong> crystallographic texture <strong>of</strong> this polysilicon have been<br />
well characterized. The texture is r<strong>and</strong>om. The grain morphology is columnar, with a mean<br />
column diameter <strong>of</strong> 300-400 nm. Most <strong>of</strong> the grains bridge from the top to bottom surface <strong>of</strong> the<br />
film. More details <strong>of</strong> the process may be found in [1.13].<br />
As shown in Fig. 1.2, the strength values measured at S<strong>and</strong>ia, had both a higher mean<br />
strength <strong>and</strong> a higher scatter in strength. Since all other participants obtained values within a<br />
reasonable scatter b<strong>and</strong> <strong>of</strong> each other, the S<strong>and</strong>ia methodology was suspected <strong>of</strong> inducing<br />
anomalous strength values.<br />
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