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Scattering of a Bessel beam by a sphere

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TLDR
The exact scattering by a sphere centered on a Bessel beam is expressed as a partial wave series involving the scattering angle relative to the beam axis and the conical angle of the wave vector components of the Besselbeam.
Abstract
The exact scattering by a sphere centered on a Bessel beam is expressed as a partial wave series involving the scattering angle relative to the beam axis and the conical angle of the wave vector components of the Bessel beam. The sphere is assumed to have isotropic material properties so that the nth partial wave amplitude for plane wave scattering is proportional to a known partial-wave coefficient. The scattered partial waves in the Bessel beam case are also proportional to the same partial-wave coefficient but now the weighting factor depends on the properties of the Bessel beam. When the wavenumber-radius product ka is large, for rigid or soft spheres the scattering is peaked in the backward and forward directions along the beam axis as well as in the direction of the conical angle. These properties are geometrically explained and some symmetry properties are noted. The formulation is also suitable for elastic and fluid spheres. A partial wave expansion of the Bessel beam is noted.

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Citations
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Journal ArticleDOI

Optical pulling force

TL;DR: Theoretical analysis suggests that there exists an optical attractive force capable of "pulling" microparticles towards a light source as mentioned in this paper, which is generated by using interference to optimize the scattering of light in the forwards direction.
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Radiation force of a helicoidal Bessel beam on a sphere

TL;DR: The partial-wave series for the scattering of an acoustic helicoidal Bessel beam by a sphere centered on the axis of the beam is applied to the calculation of the acoustic radiation force by the beam on the sphere in an inviscid fluid.
Journal ArticleDOI

Negative axial radiation forces on solid spheres and shells in a Bessel beam.

TL;DR: The prediction of negative acoustic radiation force is extended to the cases of a solid poly(methylmethacrylate) PMMA sphere in water and an empty aluminum spherical shell in water to help the development of acoustic tweezers and methods for manipulating objects during space flight.
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Perspective on light-induced transport of particles: from optical forces to phoretic motion

TL;DR: In this paper, a review of light-induced mechanisms for the controlled transport of microscopic particles is presented, focusing on the direct transfer of momentum between the particles and the incident light waves, on the combination of optical forces with external forces of other nature, and on light-triggered phoretic motion.
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Acoustic radiation force on a sphere in standing and quasi-standing zero-order Bessel beam tweezers

TL;DR: In this paper, the authors derived the exact acoustic scattering from a sphere immersed in an ideal fluid and centered along the propagation axis of a standing or quasi-standing zero-order Bessel beam, and explicit partial-wave representations for the radiation force were derived.
References
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Journal ArticleDOI

Diffraction-free beams.

TL;DR: The first experimental investigation of nondiffracting beams, with beam spots as small as a few wavelengths, can exist and propagate in free space, is reported.
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Exact solutions for nondiffracting beams. I. The scalar theory

TL;DR: In this paper, exact nonsingular solutions of the scalar-wave equation for beams that are non-diffracting were presented, which means that the intensity pattern in a transverse plane is unaltered by propagating in free space.
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Quantum Mechanics, 3rd ed.

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Bessel beams: Diffraction in a new light

TL;DR: In this article, the theoretical foundation of the Bessel beam is described and various experiments that make use of Bessel beams are discussed: these cover a wide range of fields including non-linear optics, where the intense central core of the bessel beam has attracted interest; short pulse non-diffracting fields; atom optics, and optical manipulation where the reconstruction properties of the beam enable new effects to be observed that cannot be seen with Gaussian beams.
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