Tailoring bistability in optical tweezers with vortex beams and spherical aberration

TL;DR

This paper demonstrates a bistable optical trap using vortex laser beams, combining experimental and theoretical analysis to control microsphere states via spherical aberration and focal plane adjustments, with potential applications in stochastic thermodynamics.

Contribution

It introduces a tunable bistable optical trapping system with a comprehensive theoretical model validated experimentally, enabling real-time control of optical force fields.

Findings

Bistable trapping achieved with vortex beams and spherical aberration.

Theoretical model accurately predicts experimental results.

Control of microsphere states via focal plane adjustments.

Abstract

We demonstrate a bistable optical trap by tightly focusing a vortex laser beam. The optical potential has the form of a Mexican hat with an additional minimum at the center. The bistable trapping corresponds to a non-equilibrium steady state (NESS), where the microsphere continually hops, due to thermal activation, between an axial equilibrium state and an orbital state driven by the optical torque. We develop a theoretical model for the optical force field, based entirely on experimentally accessible parameters, combining a Debye-type non-paraxial description of the focused vortex beam with Mie scattering by the microsphere. The theoretical prediction that the microsphere and the annular laser focal spot should have comparable sizes is confirmed experimentally by taking different values for the topological charge of the vortex beam. Spherical aberration introduced by refraction at the interface between the glass slide and the sample is taken into account and allows to fine tune between axial, bistable and orbital states as the sample is shifted with respect to the objective focal plane. We find an overall agreement between theory and experiment for a rather broad range of topological charges. Our results open the way for applications in stochastic thermodynamics as it establishes a new control parameter, the height of the objective focal plane with respect to the glass slide, that allows to shape the optical force field in real time and in a controllable way.