1104 M.A. Huff et al.
deflection into an electrical signal including piezoresistive, optical, capacitive, and
piezoelectric, among others. Nevertheless, it is most common to employ the piezore-
sistive effect of silicon in these sensors. The piezoresistive effect is demonstrated in
semiconductors whereby a relatively large change in resistance occurs when the
semiconductor is subjected to a strain; it was first reported by Smith in 1954 [24].
Basically, the piezoresistors are positioned on the diaphragm at locations where the
strain is the largest as the diaphragm is deflected. This transduction mechanism is
attractive due to the large size of the effect in semiconductors, the relative simplicity
of implementation and readout circuitry required, and low cost.
These types of sensors have now been on the market for several decades. Given
the length of time that these devices have been produced for the commercial mar-
ketplace, it should be no surprise that there has been a significant progression of
technology development associated with silicon-based pressure sensors over the
years. In fact, the historical development of pressure sensors in many ways reflects
the broader development of silicon micromachining and MEMS technology with the
first use of isotropic and anisotropic wet chemical etching, eutectic bonding, anodic
bonding, and direct silicon fusion bonding.
Brysek et al. and Sze [25, 26] have excellent reviews of the history of MEMS
pressure sensors. It is interesting to note that initially (circa 1958) the individ-
ual silicon piezoresistors were glued to diaphragms made of metal. This was
before the capability of silicon micromachining had been developed and as a
result, these combined silicon and metal sensors suffered from low yields and
poor stability, mostly due to the large thermal mismatch between the silicon to
glue to metal interface. Subsequently, in the early 1960s, dopants were selectively
diffused into the silicon to make regions of piezoresistive material on a silicon sub-
strate that was then epoxied to a metal constraint. This improved the yield and
performance of the sensors as well as lowered the cost. The next improvement
around 1970 was to replace the epoxied bond with a silicon–gold eutectic bond
and to thin the silicon diaphragm using mechanical milling or chemical isotropic
etching. Subsequently in 1975, the eutectic bond was replaced with a glass frit
bond and the silicon diaphragm was machined using anisotropic wet chemical
etchant solutions. This allowed the diaphragm to be made thinner and more uni-
form in thickness thereby increasing the sensitivity, performance and yield still
further.
In the 1980s the piezoresistors were made using ion implantation rather than
diffusion, which allowed increased control of the bridge resistance and offset. In
addition, the glass frit bond was replaced with an anodic bond wherein the glass sub-
strate was closely matched in its thermal expansion coefficient to that of the silicon
substrate to which it was bonded. This helped to improve the temperature stability,
improved yield, and allowed the die size to be reduced thereby reducing cost. In
the late 1980s silicon-to-silicon direct bonding was introduced which allowed the
thermal matching to be improved even more and the die size to be radically shrunk
thereby reducing cost as well as opening up many additional application opportuni-
ties, inasmuch as high-performance pressure sensors having a die size of less than
1 mm could be produced with very high yields.