Abstract

The optical cell rotator (OCR) is a modified dual-beam laser trap for the holding and controlled rotation of suspended dielectric microparticles, such as cells. In contrast to optical tweezers, OCR uses two counter-propagating divergent laser beams, which are shaped and delivered by optical fibers. The rotation of a trapped specimen is carried out by the rotation of a dual-mode fiber, emitting an asymmetric laser beam. Experiments were performed on human erythrocytes, promyelocytic leukemia cells (HL60), and cell clusters (MCF-7). Since OCR permits the rotation of cells around an axis perpendicular to the optical axis of any microscope and is fully decoupled from imaging optics, it could be a suitable and expedient tool for tomographic microscopy.

Highlights

  • Since Ashkin introduced optical traps in the 1970s [1] they have become versatile tools for the micromanipulation of biological objects

  • Typical time series of the rotation of red bood cells (RBC), HL60 cells, and MCF7 cell clusters are shown in Fig. 4 – 6

  • With optical cell rotator (OCR) we present a novel type of optical trap for the controlled rotation of anisotropic dielectric objects, such as cells, with significant advantages over existing techniques

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Summary

Introduction

Since Ashkin introduced optical traps in the 1970s [1] they have become versatile tools for the micromanipulation of biological objects. Laser beams carrying net angular momentum, which can either be spin [4, 5] or orbital angular momentum [6, 7], can be used to induce a continuous spinning of trapped samples While this can potentially be used for the operation of optically driven micromachines, the stable orientation of particles in a particular orientation, as required by microscopy, is only possible with a complicated closed-loop feedback mechanism. Another approach rotates the sample together with a trapping beam of reduced symmetry. The creation of multiple traps by means of holographic optics has been shown to allow for the rotation of micro bead clusters around arbitrary axis [12]

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