1996
DOI: 10.1364/ol.21.000827
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Optical vortex trapping of particles

Abstract: We demonstrate three-dimensional trapping of low-index particles (20-microm-diameter hollow glass spheres in water) by using a single, strongly focused, stationary dark optical vortex laser beam. The holographically generated vortex, which is similar to a TEM(01)* mode beam, was also used to trap and form ring patterns of high-index particles.

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Cited by 839 publications
(387 citation statements)
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“…Figure 2 is the interference pattern obtained from the experimental setup shown in Figure 1(a) in which we record the formation of optical vortex arrays (OVAs) using the interference of three plane waves. At the exit of CBS 4 as shown in the Figure 1(a), we obtain two optical vortex arrays International Journal of Optics (Figure 1(a)) is similar to the generation of vortex lattices by four or more plane waves as has been demonstrated previously using multiple beam interferometers [15][16][17].…”
Section: Reconstruction Of Phasesupporting
confidence: 73%
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“…Figure 2 is the interference pattern obtained from the experimental setup shown in Figure 1(a) in which we record the formation of optical vortex arrays (OVAs) using the interference of three plane waves. At the exit of CBS 4 as shown in the Figure 1(a), we obtain two optical vortex arrays International Journal of Optics (Figure 1(a)) is similar to the generation of vortex lattices by four or more plane waves as has been demonstrated previously using multiple beam interferometers [15][16][17].…”
Section: Reconstruction Of Phasesupporting
confidence: 73%
“…Both IFP 1 and 2 propagate in space and reflected by mirror M 1 and again transmitted through CBS 4 . The beam input 3 in the second (lower) arm of the interferometer is reflected by CBS 3 and after propagation in space again reflected by CBS 4 where it interferes with IFP 1 and IFP 2 at the output. At the end of the interferometer, optical vortex arrays are generated by interference of three beams.…”
Section: Optical Vortex Array Generationmentioning
confidence: 99%
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“…The self-focusing action of the nonlinearity compensated by diffraction results in self-sustained bright spatial solitons [12], which can exist as isolated states or form complex ensembles, sometimes interacting in a particle-like fashion [169][170][171][172][173][174][175]. Also, dark solitons [176][177][178][179][180][181][182][183][184] and optical vortices [185][186][187][188][189][190][191][192][193][194][195][196] have been described and experimentally observed. In such a mirrorless configuration feedback is absent, and one obtains not a spontaneous pattern formation, but just a nonlinear transformation of the input distribution.…”
Section: Mirrorless Configurationmentioning
confidence: 99%
“…Optimum conditions for particle trapping are dictated by the optical properties of the particles and the surrounding medium, as well as the physical nature of the light-mediated trapping forces. For instance, while high light intensity attracts and traps transparent high-index objects in a low-index medium, it in fact repels low index particles in a high index environment [166]. That is why hollow (or doughnut) beams are used for efficient trapping in the latter case.…”
Section: Introductionmentioning
confidence: 99%