By Dr. Yong Zhang, Angelo Mascarenhas (auth.), Dr. Clifford M. Krowne, Dr. Yong Zhang (eds.)
This publication bargains with the topic of optical and digital damaging refraction (NR) and unfavourable index fabrics NIM). various methods for attaining NR and NIM are coated, corresponding to utilizing photonic crystals, phononic crystals, split-ring resonators (SRRs) and non-stop media, focusing of waves, guided-wave habit, and nonlinear results. particular issues taken care of are polariton thought for LHMs (left passed materials), focusing of waves, guided-wave habit, nonlinear optical results, magnetic LHM composites, SRR-rod realizations, low-loss guided-wave bands utilizing SRR-rods unit cells as LHMs, NR of electromagnetic and digital waves in uniform media, box distributions in LHM guided-wave constructions, dielectric and ferroelectric NR bicrystal heterostructures, LH metamaterial photonic-crystal lenses, subwavelength focusing of LHM/NR photonic crystals, focusing of sound with NR and NIMs, and LHM quasi-crystal fabrics for focusing.
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4. 2 GHz for the transverse electric Et vector for the LHM device in Figs. 3. M. 300e + 00 −10 0 X (mm) Fig. 5. 2 GHz for the transverse magnetic Ht vector for the LHM device in Figs. 3. 0 GHz, we consider the permittivity tensor cases ⎡ ⎤ ⎡ ⎤ ⎡ ⎤ εn 0 0 εn 0 0 εn 0 0 ε¯(a) = ⎣ 0 εn 0 ⎦ , ε¯(b) = ⎣ 0 4εn 0 ⎦ , ε¯(c) = ⎣ 0 εn 0 ⎦ , 0 0 εn 0 0 εn 0 0 4εn ⎡ ⎤ ⎡ ⎤ εn 0 0 4εn 0 0 ε¯(d) = ⎣ 0 4εn 0 ⎦ , ε¯(e) = ⎣ 0 4εn 0 ⎦ . 163) 0 0 4εn 0 0 4εn Again, the first tensor ε¯(a) represents isotropy, and the next three tensors [ε¯(b), ε¯(c), and ε¯(d)] are anisotropic, so their field distribution deviations from ε¯(a) show the effect of anisotropy.
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