Expand this Topic clickable element to expand a topic
Skip to content
Optica Publishing Group

Real-time interactive 3D manipulation of particles viewed in two orthogonal observation planes

Open Access Open Access

Abstract

The generalized phase contrast (GPC) method has been applied to transform a single TEM00 beam into a manifold of counterpropagating-beam traps capable of real-time interactive manipulation of multiple microparticles in three dimensions (3D). This paper reports on the use of low numerical aperture (NA), non-immersion, objective lenses in an implementation of the GPC-based 3D trapping system. Contrary to high-NA based optical tweezers, the GPC trapping system demonstrated here operates with long working distance (>10 mm), and offers a wider manipulation region and a larger field of view for imaging through each of the two opposing objective lenses. As a consequence of the large working distance, simultaneous monitoring of the trapped particles in a second orthogonal observation plane is demonstrated.

©2005 Optical Society of America

Full Article  |  PDF Article
More Like This
GPC-based optical micromanipulation in 3D real-time using a single spatial light modulator

Peter John Rodrigo, Ivan R. Perch-Nielsen, Carlo Amadeo Alonzo, and Jesper Glückstad
Opt. Express 14(26) 13107-13112 (2006)

Real-time three-dimensional optical micromanipulation of multiple particles and living cells

Peter John Rodrigo, Vincent Ricardo Daria, and Jesper Glückstad
Opt. Lett. 29(19) 2270-2272 (2004)

Autonomous and 3D real-time multi-beam manipulation in a microfluidic environment

Ivan R. Perch-Nielsen, Peter John Rodrigo, Carlo Amadeo Alonzo, and Jesper Glückstad
Opt. Express 14(25) 12199-12205 (2006)

Supplementary Material (3)

Media 1: AVI (2495 KB)     
Media 2: AVI (1349 KB)     
Media 3: AVI (1670 KB)     

Cited By

Optica participates in Crossref's Cited-By Linking service. Citing articles from Optica Publishing Group journals and other participating publishers are listed here.

Alert me when this article is cited.


Figures (3)

Fig. 1.
Fig. 1. Schematic showing the optical setup. The angles of incidence on the spatial light modulators are kept as small as possible. L1–L3 are achromatic lenses. Focal lengths of L1 and L2=300 mm. Focal length of L3=400 mm. Top and bottom objectives, 50x. A 20x objective is used for side view. The computer acquires video input from two cameras and controls the two SLMs based on user interaction.
Fig. 2.
Fig. 2. (AVI, 2.5 MB) A: Four 3 µm polystyrene beads levitated 15 µm above the bottom surface. The reflection of the beads in the lower glass surface can be seen due to the slightly angled side view. B-D: User-interactive control of the relative z-positions of the beads showing ~30 µm axial dynamic range. The x-y viewing system is set to sharply image the plane 15 µm above the bottom surface.
Fig. 3.
Fig. 3. A-B: (AVI, 1.4 MB) Three 3 µm beads at the vertices of a rotating imaginary triangle in the x-y plane while each particle encounters a height-stroke during each revolution. C-D: (AVI, 1.7 MB) Nine 3 µm beads collectively forming a 3D crystal-like structure rotated around the z-axis.
Select as filters


Select Topics Cancel
© Copyright 2024 | Optica Publishing Group. All rights reserved, including rights for text and data mining and training of artificial technologies or similar technologies.