2016
DOI: 10.1364/josaa.33.001004
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Formation of vortices by interference of surface plasmon polaritons

Abstract: The TM-mode of surface plasmon polaritons (SPPs) can be excited at the interface of a metal layer and a dielectric medium. The E-mode of the SPPs is excited due to reflection of the TM-mode from the boundary of inhomogeneity in the metal layer. The interference of these modes leads to the formation of the SPP vortices in the points of minima of the mode field in some components of the Poynting vector of the SPP. The SPP interference vortex pattern changes depending on the curvature of the boundary of inhomogen… Show more

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Cited by 10 publications
(4 citation statements)
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“…This demonstrates that the transmitted optical field can be decomposed into two orthogonal spin components: one part preserves the same spin with the incidence, and the other is converted to the reversed spin with an additional phase of 2σβ. For the SPP wave, the z-polarization electric field is considered a dominant field component, where dE spp at the field point can be described as [41]:…”
Section: Methodsmentioning
confidence: 99%
“…This demonstrates that the transmitted optical field can be decomposed into two orthogonal spin components: one part preserves the same spin with the incidence, and the other is converted to the reversed spin with an additional phase of 2σβ. For the SPP wave, the z-polarization electric field is considered a dominant field component, where dE spp at the field point can be described as [41]:…”
Section: Methodsmentioning
confidence: 99%
“…SPPs from the inhomogeneity of permittivity with curvilinear boundary [35][36][37]. The plasmon vortices do not arise in case of superposition of the modes reflected from a straight line boundary of the inhomogeneity.…”
Section: Kne Energy and Physicsmentioning
confidence: 99%
“…Each of the nanoslits in the segmented spiral can be regarded as a source element that can generate an elementary SPP field d E spp at the field point Q ( R , φ). This can be expressed asdboldnormalEspp= etrue^zE0ZeknormalzzeiboldnormalkrboldnormalRboldnormalrErr,θrdθwhere kz=(kspp2k02)1/2, k r = − k r ê r = − 2π/λ spp ê r , r = r m is the radius of the segmented spiral, and k r ( R − r ) = k r r − R cos(φ −θ). In the above equation, only a z ‐polarized electric field was considered as it is the dominant field component of SPPs.…”
Section: Principle and Structure Designmentioning
confidence: 99%