This paper reviews cantilever-based resonant chemical microsensors, which detect an analyte of interest via a change of the resonance frequency of a characteristic vibration mode, caused by the added mass upon sorption of the analyte into a sensing film deposited on the cantilever surface. While the focus of the paper is on silicon-based, hammer-like resonant sensors that comprise a head region suspended by a cantilever support structure, the results can be applied to other material systems and resonator geometries as well. The cantilever vibrations are excited electrothermally and sensed using four piezoresistors arranged in a Wheatstone bridge. Approaches to address the three 'S' metrics of chemical sensors, i.e., sensitivity, selectivity, and stability are highlighted. In particular, the benefits of localized deposition of the sensing film and the analysis of signal transients are explored.
Mass-Sensitive Chemical SensorsWhile most chemical analyses are still performed today using bench-top analytical instruments, because of their high accuracy, high selectivity, and excellent reproducibility, there is an ever increasing demand for chemical sensors in applications that require fast response times, in-field sensing capabilities, portability and low-cost, even if they show reduced performance with respect to sensitivity, selectivity and stability compared to bench-top instruments. To this end, a wide variety of microfabricated chemical sensors utilizing either electrochemical, thermal, optical or gravimetric/mechanical transduction schemes have been explored over the past decades (1,2). This paper focuses on cantilever-based resonant chemical microsensors, which detect an analyte of interest via a change of the resonance frequency of a characteristic vibration mode, caused by the added mass upon sorption of the analyte into a sensing film deposited on the cantilever surface (3-6). Besides ease of fabrication, such mass-sensitive chemical microsensors benefit from a well-understood transduction mechanism and the fact that frequencies and frequency changes can be sensed with high accuracy. At a particular vibration mode, the resonance frequency f is determined by the effective spring constant k eff and effective mass m eff of the microstructure, resulting in a relative frequency change ∆f/f upon sorption of mass into the sensing film that depends on the effective mass change ∆m eff : f = $ %& k eff m eff ∆f f = -1 2 ∆m eff m eff [1] 10.1149/07517.0027ecst ©The Electrochemical Society ECS Transactions, 75 (17) 27-34 (2016) 27 ) unless CC License in place (see abstract). ecsdl.org/site/terms_use address. Redistribution subject to ECS terms of use (see 132.239.1.231 Downloaded on 2017-04-24 to IP