Abstract

Thermal motion of nanomechanical probes directly impacts their sensitivities to external forces. Its proper understanding is therefore critical for ultimate force sensing. Here, we investigate a vectorial force field sensor: a singly-clamped nanowire oscillating along two quasi-frequency-degenerate transverse directions. Its insertion in a rotational optical force field couples its eigenmodes non-symmetrically, causing dramatic modifications of its mechanical properties. In particular, the eigenmodes lose their intrinsic orthogonality. We show that this circumstance is at the origin of an anomalous excess of noise and of a violation of the fluctuation dissipation relation. Our model, which quantitatively accounts for all observations, provides a novel modified version of the fluctuation dissipation theorem that remains valid in non-conservative rotational force fields, and that reveals the prominent role of non-axial mechanical susceptibilities. These findings help understand the intriguing properties of thermal fluctuations in non-reciprocally-coupled multimode systems.

Highlights

  • Thermal motion of nanomechanical probes directly impacts their sensitivities to external forces

  • Nanoresonators with similar geometry were employed in MRFM applications[20, 26], in electrostatic force field sensing[17,18,19], but all the developments presented here apply to doubly clamped nanobeams oscillating in and out of plane[4, 27,28,29,30] and more generally to multimode mechanical systems coupled through any external force field

  • It was theoretically suggested that it could generate a warping of the eigenmode basis and an altered dynamics, but no experimental proof could be drawn since only a scalar 1D readout was available at that time

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Summary

Introduction

Thermal motion of nanomechanical probes directly impacts their sensitivities to external forces. We investigate the thermal noise and the driven dynamics of a singly clamped suspended nanowire oscillating along both transverse directions immersed in a optical tunable rotational force field.

Results
Conclusion

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