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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. 3.

Fig. 3

Fig. 3

(a) Real part of the surface charge density for prolate spheroidal shells for a longitudinally incident field with the aspect ratios 1 (sphere), 2, 3, and 4. The charge density is evaluated at the end (ϑ = 0°) of the shell.

(b) Imaginary part of prolate longitudinal response.