Orbital motion of optically trapped particles in Laguerre–Gaussian beams
JOSA A, Vol. 27, Issue 9, pp. 2061-2071 (2010)
http://dx.doi.org/10.1364/JOSAA.27.002061
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Abstract
A theoretical examination of off-axial trapping in non-paraxial Laguerre–Gaussian beams is presented for both the Rayleigh and Mie regimes. It is well known that the force acting on a particle may be divided into a term proportional to the intensity gradient and another representing the scattering force. The latter term may be further sub-divided into a dissipative radiation force and a term dependent on the electric field gradient. For Rayleigh particles in Laguerre–Gaussian beams, it is shown that the field gradient term contributes exactly half of the scattering force. This may be compared with a plane wave, in which it makes zero contribution. The off-axis trapping positions for spheres with radii varying from 0.1 to
© 2010 Optical Society of America
OCIS Codes
(290.4020) Scattering : Mie theory
(290.5870) Scattering : Scattering, Rayleigh
(350.4855) Other areas of optics : Optical tweezers or optical manipulation
(050.4865) Diffraction and gratings : Optical vortices
ToC Category:
Scattering
History
Original Manuscript: April 1, 2010
Revised Manuscript: July 22, 2010
Manuscript Accepted: July 26, 2010
Published: August 24, 2010
Virtual Issues
Vol. 5, Iss. 13 Virtual Journal for Biomedical Optics
Citation
Stephen H. Simpson and Simon Hanna, "Orbital motion of optically trapped particles in Laguerre–Gaussian beams," J. Opt. Soc. Am. A 27, 2061-2071 (2010)
http://www.opticsinfobase.org/vjbo/abstract.cfm?URI=josaa-27-9-2061
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