DOI: 10.4995/thesis/10251/31207
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Design and implementation of plasmonic metamaterials and devices

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“…However, in more complicated (yet typical cases of) structured optical fields (such as optical vortices and near-field phenomena), the direction of the Poynting vector can differ from the wavevector direction. [15][16][17][18] In these cases, the Poynting vector p acquires an additional spin momentum density p s , introduced for the first time by Belifante, 19,20 and can be expressed 3 as a sum of canonical and spin contributions: p = p o + p s .…”
Section: Resultsmentioning
confidence: 99%
“…However, in more complicated (yet typical cases of) structured optical fields (such as optical vortices and near-field phenomena), the direction of the Poynting vector can differ from the wavevector direction. [15][16][17][18] In these cases, the Poynting vector p acquires an additional spin momentum density p s , introduced for the first time by Belifante, 19,20 and can be expressed 3 as a sum of canonical and spin contributions: p = p o + p s .…”
Section: Resultsmentioning
confidence: 99%