Novel Architecture for Inertial Grade SOI MEMS Inertial Sensors
Ahmed Abdel Aziz
1
, Abdel-Hameed Sharaf
1, 2
, Mohamed Serry
3
and Sherif Sedky
1, 4
1
Science and Technology Research Center (STRC), American University in Cairo (AUC), Cairo, Egypt
2
National Center for Radiation Research and Technology (NCRRT), Egyptian Atomic Energy Authority
(EAEA), Cairo, Egypt
3
King Abdullah University of Science and Technology (KAUST), Thuwal, Saudi Arabia
4
Physics Department, AUC, Cairo, Egypt
E-mail: sedky@aucegypt.edu and aksa@aucegypt.edu
This work reports, for the first time, on a
novel architecture for realizing high performance
miniaturized micromachined inertial sensors based
on Silicon on Insulator (SOI) technology. The new
sensors are essential components for high precision
Inertial Navigation Systems (INS) serving a wide
range of applications varying from automotive to
space. Similar to the state-of-the-art designs and
architectures, our novel architecture utilizes SOI
technology, which is crucial for realizing such
electro-mechanical sensors. This is mainly due to
the fact that it allows for having stress free
suspensions and relatively very large proof masses
(for bulk rather than surface micromachined
MEMS) coupled with the flexibility of choosing
between the presence or absence of electrical
isolation between the upper and lower parts of the
SOI wafer depending on the sensor’s layout. This
accordingly enables having the electrical contacts
isolated from the rest of the sensor’s structure.
Typically, vibratory micromachined gyroscopes
(VMG) and accelerometers are designed in-plane,
i.e. the suspension and the proof mass vibrate in the
same plane parallel to the substrate surface. Such
in-plane architecture reduces dramatically the
sensor's fill factor (typically around 17%); hence
the Brownian noise level and overall sensitivity are
degraded due to the reduced proof mass. Thus, a
dramatic enhancement in performance can be
achieved by improving the fill factor as this has a
direct impact on increasing the proof mass
significantly. Accordingly, we introduced, for the
first time, the vertically suspended micromachined
inertial sensor displayed in Figs. 1 and 2. Such
design allows increasing the fill factor by more
than a factor of four (up to 80-90%). Moreover,
this design offers a decoupled geometric design of
the proof mass and the support stiffness
dimensions. The performance of the proposed
sensors was analyzed using Finite Element Method
(FEM) to determine the natural mode shapes and
frequencies in addition to the mechanical stability
and the drive-sense mode decoupling (1-2% similar
to common designs) for the MEMS gyroscopes.
Tables I and II give a comparison between
the proposed design and two of the state-of-the-art
designs [1, 2]. By inspecting Table I, it is clear that
for the same device area, the proof mass is
increased by more than a factor of 20 due to the
increased fill factor (80%). In addition, the proof
mass thickness is increased to 200 µm. It should be
noted that the proposed design offers the flexibility
of increasing the thickness of the proof mass up to
the whole wafer thickness without introducing any
additional lithography masks as in the conventional
SOI architectures where extra-mass is employed
[1]. Moreover, the mode resonance frequency is
significantly reduced due to the reduced mode
stiffness. This serves to suppress the thermo-elastic
damping and support losses that dominate in high
performance vacuum operation. The new
architecture also suppresses the noise floor by more
than one order of magnitude, enhances signal
sensitivity by more than two orders of magnitude
and Signal to Noise Ratio (SNR) up to three orders
of magnitude. Table II reflects similar
improvements for the proposed inertial grade
MEMS accelerometer. Furthermore, the proposed
process flow for the novel sensors consists only of
four masks where all the steps rely only on Deep
Reactive Ion Etching (DRIE). This reveals that the
main limitation to fabrication is the DRIE aspect
ratio. The etching aspect ratio has been found
experimentally to be as high as 1:50 as illustrated
by the Scanning Electron Microscopy (SEM)
image in Fig. 3 for deep 80 µm Silicon trenches. It
is worth noting that such a high ratio does not
impose a limitation to the fabrication of the various
sensors’ geometries investigated. Finally, the new
architecture allows additionally, and for the first
time, to realize a quad mass sensing scheme, i.e.
dual differential sensing, for common mode
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