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. Author manuscript; available in PMC: 2013 Aug 21.

Published in final edited form as: IEEE Trans Nanotechnol. 2007;6(6):627–638. doi: 10.1109/TNANO.2007.909074

Fig. 8 — (a) Real part of the surface charge density for prolate shells of differing shell thicknesses (5%, 10%, 15%, 20%, 25%) with a fixed aspect ratio (2 to 1) for a longitudinally incident field. The dashed curve is the charge density of the solid prolate spheroid. In each case, the charge density is evaluated at the blunt end (ϑ = 0°) of the shell.

(b) Imaginary part of the prolate longitudinal response for different shell thicknesses.

Fig. 8 — (a) Real part of the surface charge density for prolate shells of differing shell thicknesses (5%, 10%, 15%, 20%, 25%) with a fixed aspect ratio (2 to 1) for a longitudinally incident field. The dashed curve is the charge density of the solid prolate spheroid. In each case, the charge density is evaluated at the blunt end (ϑ = 0°) of the shell.

(b) Imaginary part of the prolate longitudinal response for different shell thicknesses.