Fig. 1

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An anisotropic material with a constant εy (x) and tailored εx (x) , εz (x) (inset) (β (x) = cos(πx/L)2sin(2πx/L) exp(− x2), α (x) = x2sin(2πx/L) exp(− x2)) inside the slab is designed such that it (top) does not reflect either TE or TM waves at grazing incidence. The results obtained from COMSOL Multiphysics are shown as dots. The field profiles at grazing incidence (bottom) are shown to decay to non-zero constants of equal amplitudes outside the slab region, as required for a half–bound state.

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