IOP PUBLISHING JOURNAL OF PHYSICS D: APPLIED PHYSICS
J. Phys. D: Appl. Phys. 41 (2008) 125306 (8pp) doi:10.1088/0022-3727/41/12/125306
Theoretical analysis of resonance
frequency change induced by adsorption
Ji-Qiao Zhang, Shou-Wen Yu
1
and Xi-Qiao Feng
Department of Engineering Mechanics, Tsinghua University, Beijing 100084, People’s Republic of China
E-mail: yusw@tsinghua.edu.cn
Received 22 February 2008, in final form 23 April 2008
Published 29 May 2008
Online at stacks.iop.org/JPhysD/41/125306
Abstract
Microcantilever-based techniques can be used to explore the autonomy and property of
molecules (e.g. DNA and single actin filaments) adsorbed on a surface. A theoretical model is
presented here to predict the resonance frequency of a cantilever induced by physically
adsorbed atoms/molecules. The cantilever is modelled as a sandwich beam containing two
surface layers of a finite thickness and a bulk layer between them. It is found that the
resonance frequency shift depends sensitively on both the mass and bending stiffness
variations of the cantilever induced by the adsorbed atoms/molecules. The adsorptions of
O atoms on Si(1 0 0), of O atoms on Au(1 0 0) and of H atoms on Au(1 0 0) are taken as three
representative examples. We demonstrate that physisorption can induce distinctly different
resonant responses of cantilevers, depending not only on the adatoms but also on the substrate
material. This study is helpful for the optimal design of microcantilever-based measurement
techniques.
1. Introduction
Due to their advantages of high sensitivity, enhanced reliability,
fast response, reduced size and low costs, microfabricated
beams or cantilevers have been widely used as sensors,
actuators and transducers in physical, chemical and biological
applications [1–5]. Microcantilever-based sensing techniques
are based on the changes in physical quantities that are easily
measured, e.g. deflection, resonance frequency and quality
factor of the beam. They can be used to explore, for example,
the autonomy and property of biomacromolecules (e.g. DNA
and single actin filaments) [6–8] and to detect the mass of
particles deposited onto the cantilever [9–15]. Therefore,
a deep understanding of the cantilever’s response upon
adsorption is important to optimize the structural parameters
and to improve the performance of the sensor devices.
Experimental observations have demonstrated that
adsorbates on the surface of a microcantilever can cause
a shift in its resonance frequency [9–19]. This provides
a direct measure of the mass of adsorbates by assuming
that the spring constant remains fixed. By measuring the
resonance frequency, Cleveland et al [9] detected the nanogram
mass of particulates deposited onto a cantilever. Using a
1
Author to whom any correspondence should be addressed.
similar method, Thundat and co-workers [10, 11] estimated the
relative amount of adsorbates on the cantilever with picogram
mass resolution. Another remarkable improvement in this
technique comes from the work of Ilic and co-workers [12, 13],
who measured the mass of a single Escherichia coli with
micromechanical oscillators. Gupta et al [14] fabricated
even smaller cantilevers for detecting a single vaccinia virus.
Recently, Ilic et al [15] fabricated nanomechanical sensors
with subattogram mass detection sensitivity. In many cases,
however, adsorption also alters the spring constant of a
microcantilever. Early in 1975, Lagowski et al [16] found that
the normal mode of vibration of thin crystals depends strongly
on the surface preparation and on the ambient atmosphere
and attributed this change to the effects of surface stresses.
Chen et al [17] and Cherian and Thundat [18] showed that
the resonance frequency of a cantilever depends on both the
mass increase and the spring constant change induced by
surface adsorption of chemicals. Wang et al [19] studied
the nanomechanical properties of ultra-thin single-crystal
silicon resonators, with emphasis on their surface effects
associated with thermal treatments and gas adsorption. Lu
et al [20] analysed the influence of pure surface stresses and
adsorption-induced surface stresses on the vibration frequency
of a cantilever sensor. As an extension of Dareing and
Thundat’s work [21], Huang et al [22] investigated the
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