Abstract

The thermomechanical motion imposes the fundamental noise limit in room-temperature resonant sensors and oscillators. Due to the inherently low sensitivity of capacitive transduction in microelectromechanical (MEM) resonators, its effects are often masked by noise in the subsequent amplifier and measurement stages. In this work, we demonstrate a capacitive transduction scheme for measuring kHz-MHz frequency MEM resonators across 1 $\mu \text{m}$ capacitive gaps with 99.8% thermomechanical-noise-limited resolution. We delineate the transimpedance gain and noise of our custom off-chip differential transimpedance amplifier setup. The thermomechanical noise spectrum can provide estimates of the resonant frequency, quality factor, and electromechanical transduction factor comparable to the commonly used driven response, without the downsides of capacitive feedthrough or nonlinearity. [2019-0115]

Highlights

  • M ICROELECTROMECHANICAL resonators are playing an increasing role in commercial oscillators [1], filters [2], [3], and atomic force microscopes ( [4], [5]) for measuring biological materials [6]–[8], microfluidic resonators for cell characterization [9]–[11], and studying nanoscale energy transport [12]–[14]

  • Capacitive transduction is not precluded from achieving excellent measurement resolution; when micromechanical resonators are cooled to cryogenic temperatures and nanometer-scale gaps are employed, capacitive sensing can detect down to the quantum noise level, more than ten orders of magnitude smaller than the thermomechanical noise motion at room-temperature

  • By comparing measurements of a micromechanical beam actuated by an external electrostatic drive or thermomechanical noise to an electromechanical model, we show that the thermomechanical noise and driven response yield similar estimates for the electromechanical transduction factor and the gap size

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Summary

INTRODUCTION

M ICROELECTROMECHANICAL resonators are playing an increasing role in commercial oscillators [1], filters [2], [3], and atomic force microscopes ( [4], [5]) for measuring biological materials [6]–[8], microfluidic resonators for cell characterization [9]–[11], and studying nanoscale energy transport [12]–[14]. With careful amplifier design and sufficiently narrow gaps, the noise of a capacitively-transduced MEM sensor or oscillator can be limited by the thermomechanical noise near the mechanical resonance frequencies instead of the noise in the subsequent amplifier stages. Capacitive transduction is not precluded from achieving excellent measurement resolution; when micromechanical resonators are cooled to cryogenic temperatures and nanometer-scale gaps are employed, capacitive sensing can detect down to the quantum noise level, more than ten orders of magnitude smaller than the thermomechanical noise motion at room-temperature This can be accomplished by capacitively coupling the mechanical resonator to a superconducting single-electron transistor [48], [49] or a superconducting microwave circuit with a Josephson parametric amplifier readout [50], [51]. By comparing measurements of a micromechanical beam actuated by an external electrostatic drive or thermomechanical noise to an electromechanical model, we show that the thermomechanical noise and driven response yield similar estimates for the electromechanical transduction factor and the gap size

FABRICATED MICROMECHANICAL BEAMS
MODEL FOR CAPACITIVE TRANSDUCTION
LOW NOISE AMPLIFIER DESIGN
MEASUREMENTS
CONCLUSION AND FUTURE WORK
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