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note
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We note that some previous analytical calculations (say, Ref.) predicted that the current distribution along a thin metallic strip should be a Maxwellian form in which the current density diverges on the edges of the metallic strip. For the case that we studied, as the wavelength we considered is much larger than the width of the ring, the current in a Maxwellian form is almost uniform in the strip except in the region very close to the edges (see Ref.), which is indeed the case found in our FDTD simulations. However, since our FDTD mesh is not dense enough, we failed to find the divergences near the edges (see Fig. 1). Nevertheless, we note that the uniform distribution that we took is still a valid (although quite rough) approximation of the true current distribution and yields good results of resonance frequencies as compared with FDTD simulations (see Fig. 2). The reason of such good agreement is also partly due to the fact that the resonance frequency is a variational quantity which does not depend much on the detailed forms of the current distribution.
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