2015
DOI: 10.1007/s00339-015-9165-5
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Improvement of surface-enhanced Raman scattering by dipolar resonance mode of silver half-shell array

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Cited by 4 publications
(1 citation statement)
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“…In the wavelength range 600−800 nm, the electric fields are localized sharply at the junctions between two adjacent halfshells, as indicated with the arrows in Figure c‐f. Similar behaviors were reported for 2D structures of Ag semishells on polystyrene spheres,, Au semishells on hollow TiO 2 spheres, and Cu halfshells on SiO 2 spheres . It has been reported that an isolated metal halfshell shows two different plasmon modes: a transverse electron oscillation parallel to the rotational symmetry axis of the halfshell (α mode), and a longitudinal electron oscillation perpendicular to the axis (β mode) .…”
Section: Resultssupporting
confidence: 77%
“…In the wavelength range 600−800 nm, the electric fields are localized sharply at the junctions between two adjacent halfshells, as indicated with the arrows in Figure c‐f. Similar behaviors were reported for 2D structures of Ag semishells on polystyrene spheres,, Au semishells on hollow TiO 2 spheres, and Cu halfshells on SiO 2 spheres . It has been reported that an isolated metal halfshell shows two different plasmon modes: a transverse electron oscillation parallel to the rotational symmetry axis of the halfshell (α mode), and a longitudinal electron oscillation perpendicular to the axis (β mode) .…”
Section: Resultssupporting
confidence: 77%