In this article, a novel nanoscale broadband viscoelastic spectroscopy approach is proposed. The proposed approach utilizes the recently developed model-less inversionbased iterative control (MIIC) technique for accurate measurement of the material response to the applied excitation force over a broad frequency band. Current nanomechanical measurement is slow and narrow-banded and thus not capable of measuring rate-dependent phenomena of materials. In the proposed approach, an input force signal with dynamic characteristics of band-limited white-noise is utilized to rapidly excite the nanomechanical response of the material over a broad frequency range. Then, the MIIC technique is used to compensate for the hardware adverse effects, thereby allowing the precise applications of such an excitation force and measurement of the material response (to the applied force). The proposed approach is illustrated by implementing it to measure the creep compliance of poly(dimethylsiloxane) (PDMS) over a broad frequency range over 3 orders of magnitude.
I. INTRODUCTIONIn this article, a novel nanoscale broadband viscoelastic spectroscopy (NBVS) methodology is proposed. The proposed NBVS approach utilizes the recently developed modelless inversion-based iterative control (MIIC) technique [1] to allow rapid excitation and subsequent measurement of the nanomechanical behavior of materials over a broad frequency band. The scanning probe microscope (SPM) has become an enabling tool to quantitatively measure the mechanical properties of a wide variety of materials [2]. Current SPMbased force measurements, however, are limited by the slow operation of SPM to measure the rate-dependent phenomena of materials [3], and large measurement (temporal) errors can be generated when dynamic evolution of the material is involved during the measurement. Operating speed of current SPMs is limited by: (1) the excitation force applied, which is either quasi-static or resonant-oscillation based, is either too narrow-banded in frequency (quasi-static) or too slow (resonant oscillation based) to rapidly excite the nanomechanical behavior of materials over a broad frequency band; and (2) the hardware adverse effects can be coupled into the measured data if the measurement is at high-speed and over a broad frequency range. These adverse effects include the hysteresis of the piezo actuator (used to position the probe relative to the sample), the vibrational dynamics of the piezo actuator and the probe along with the mechanical parts, and the dynamics uncertainties.