Abstract
The Gaussian vortex beam is assumed to be linearly polarized. The analytical expression of the electric field of a linearly polarized Gaussian vortex beam propagating in free space is derived by using the vectorial Rayleigh-Sommerfeld integral formulae. The propagating magnetic field of the linearly polarized Gaussian vortex beam is presented by taking the curl of the electric field. By employing the electromagnetic field of the linearly polarized Gaussian vortex beam beyond the paraxial approximation, the analytical expression of the angular momentum density of the linearly polarized Gaussian vortex beam is derived. The three components of the angular momentum density of a linearly polarized Gaussian vortex beam are demonstrated in the reference plane. The effects of the linearly polarized angle and the topological charge on the three components of the angular momentum density are investigated. To acquire the more longitudinal angular momentum density requires such an optimal choice that the linearly polarized angle is set to be zero and the topological charge increases. This research is useful to the optical trapping, the optical guiding, and the optical manipulation.
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Zhou, G., Wang, X., Dai, C. et al. Angular momentum density of a Gaussian vortex beam. Sci. China Phys. Mech. Astron. 57, 619–627 (2014). https://doi.org/10.1007/s11433-013-5276-1
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DOI: https://doi.org/10.1007/s11433-013-5276-1