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Fig. 2. Forward (left) and backward (right) reflection and transmission S-parameters of a bi-anisotropic MM slab.

Figure 2 Forward (left) and backward (right) reflection and transmission S-parameters of a bi-anisotropic MM slab.

Related Figures (12)

Fig. 1. Analyzed multilayer structure composed of sequential combi- nations of bi-anisotropic MM slab and conventional material. U.C. Hasar et al. / Photonics and Nanostructures — Fundamentals and Applications xxx (2014) xxx—xxx
Fig. 1. Analyzed multilayer structure composed of sequential combi- nations of bi-anisotropic MM slab and conventional material. U.C. Hasar et al. / Photonics and Nanostructures — Fundamentals and Applications xxx (2014) xxx—xxx
Fig. 3. Unit cell of the studied bi-anisotropic MM slab. U.C. Hasar et al. / Photonics and Nanostructures — Fundamentals and Applications xxx (2014) xxx-xxx
Fig. 3. Unit cell of the studied bi-anisotropic MM slab. U.C. Hasar et al. / Photonics and Nanostructures — Fundamentals and Applications xxx (2014) xxx-xxx
Fig. 4. Dependencies of (a) transmitted powers, (b) reflected powers (over 0.1—20.0 GHz), (c) absorbed powers (over 0.1—20.0 GHz), and (d) forward reflected and absorbed powers (over 1.0-5.5 GHz) of low-loss periodic multilayered structures (the low-loss slab and the lossless conventional material) with periods of P=2, P=3, and P=4 and for Lpig=5.0 mm and Lo, =5.0 mm [Here, the subscripts ‘f’ and ‘b’ in parenthesis denote, respectively, the forward and backward directions]. U.C. Hasar et al. / Photonics and Nanostructures — Fundamentals and Applications xxx (2014) xxx-xxx
Fig. 4. Dependencies of (a) transmitted powers, (b) reflected powers (over 0.1—20.0 GHz), (c) absorbed powers (over 0.1—20.0 GHz), and (d) forward reflected and absorbed powers (over 1.0-5.5 GHz) of low-loss periodic multilayered structures (the low-loss slab and the lossless conventional material) with periods of P=2, P=3, and P=4 and for Lpig=5.0 mm and Lo, =5.0 mm [Here, the subscripts ‘f’ and ‘b’ in parenthesis denote, respectively, the forward and backward directions]. U.C. Hasar et al. / Photonics and Nanostructures — Fundamentals and Applications xxx (2014) xxx-xxx
Fig. 5. Dependencies of (a) transmitted powers, (b) reflected powers (over 0.1—20.0 GHz), (c) absorbed powers (over 0.1-—20.0 GHz), and (d) forward reflected and absorbed powers (over 1.0-5.5 GHz) of lossy periodic multilayered structures (the lossy slab and the lossy conventional material) with periods of P=2, P=3, and P=4 and for Lyiqg=5.0 mm and Leo, =5.0 mm [Here, the subscripts ‘f’ and ‘b’ in parenthesis denote, respectively, the forward and backward directions].
Fig. 5. Dependencies of (a) transmitted powers, (b) reflected powers (over 0.1—20.0 GHz), (c) absorbed powers (over 0.1-—20.0 GHz), and (d) forward reflected and absorbed powers (over 1.0-5.5 GHz) of lossy periodic multilayered structures (the lossy slab and the lossy conventional material) with periods of P=2, P=3, and P=4 and for Lyiqg=5.0 mm and Leo, =5.0 mm [Here, the subscripts ‘f’ and ‘b’ in parenthesis denote, respectively, the forward and backward directions].
Fig. 6. Dependencies of (a) transmitted powers, (b) reflected powers, and (c) absorbed powers of the low-loss (LL) and lossy (HL) bi-anisotropic (Bian.) MM slab (Lpiq = 5.0 mm) and the lossless (NL) and lossy (HL) conventional (Conven.) material (Leo, =5.0 mm) [Here, the subscripts ‘f’ and ‘b’ in parenthesis denote, respectively, the forward and backward directions.] ~ a In the simulations, perfect electric (magnetic) con- ductors are assumed to be present over xy (xz) planes to obtain a periodic MM slab in yz plane. Waveguide ports are located over x axes to supply and extract the energy of plane electromagnetic wave (Plane wave option of CST 2014 Microwave Studio can also be applied for the Please cite this article in press as: U.C. Hasar, et al. Investigation of transmitted, reflected, and absorbed powers of periodic and aperiodic multilayered structures composed of bi-anisotropic metamaterial slab and conventional material, Photon Nanostruct: Fundam Appl (2014), http://dx.doi.ore/10.1016/).photonics.2014.12.003
Fig. 6. Dependencies of (a) transmitted powers, (b) reflected powers, and (c) absorbed powers of the low-loss (LL) and lossy (HL) bi-anisotropic (Bian.) MM slab (Lpiq = 5.0 mm) and the lossless (NL) and lossy (HL) conventional (Conven.) material (Leo, =5.0 mm) [Here, the subscripts ‘f’ and ‘b’ in parenthesis denote, respectively, the forward and backward directions.] ~ a In the simulations, perfect electric (magnetic) con- ductors are assumed to be present over xy (xz) planes to obtain a periodic MM slab in yz plane. Waveguide ports are located over x axes to supply and extract the energy of plane electromagnetic wave (Plane wave option of CST 2014 Microwave Studio can also be applied for the Please cite this article in press as: U.C. Hasar, et al. Investigation of transmitted, reflected, and absorbed powers of periodic and aperiodic multilayered structures composed of bi-anisotropic metamaterial slab and conventional material, Photon Nanostruct: Fundam Appl (2014), http://dx.doi.ore/10.1016/).photonics.2014.12.003
Fig. 7. A periodic multilayered structure with P=1 (a bi-anisotropic slab and a conventional material) for power analysis.
Fig. 7. A periodic multilayered structure with P=1 (a bi-anisotropic slab and a conventional material) for power analysis.
Fig. 8. Dependencies of forward reflected powers of the low-loss multilayered structure with (a) different periods P=2 and P=4 (Leon = Lpia = 5.0 mm) and (b) different Leon values for a fixed period P=2 (Lpiq =5.0 mm).
Fig. 8. Dependencies of forward reflected powers of the low-loss multilayered structure with (a) different periods P=2 and P=4 (Leon = Lpia = 5.0 mm) and (b) different Leon values for a fixed period P=2 (Lpiq =5.0 mm).
Fig. 9. Dependencies of (a) transmitted powers, (b) forward reflected powers, (c) backward reflected powers, (d) forward absorbed powers, and (e) backward absorb powers of low-loss aperiodic multilayered structures with 8 layers (N = 8) when Lpjq identified by a superscript of each bi-anisotropic slab is set to 7.0mm with the remaining Lpjq fixed at 5.0 mm (Leo, = 5.0 mm for all conventional layers).
Fig. 9. Dependencies of (a) transmitted powers, (b) forward reflected powers, (c) backward reflected powers, (d) forward absorbed powers, and (e) backward absorb powers of low-loss aperiodic multilayered structures with 8 layers (N = 8) when Lpjq identified by a superscript of each bi-anisotropic slab is set to 7.0mm with the remaining Lpjq fixed at 5.0 mm (Leo, = 5.0 mm for all conventional layers).
Fig. 10. Dependencies of (a) transmitted powers, (b) forward reflected powers, (c) backward reflected powers, (d) forward absorbed powers, and (e) backward absorb powers of lossy aperiodic multilayered structures with 8 layers (V=8) when Lypjq identified by a superscript of each bi-anisotropic slab is set to 7.0mm with the remaining Lpjq fixed at 5.0 mm (Leo, = 5.0 mm for all conventional layers).
Fig. 10. Dependencies of (a) transmitted powers, (b) forward reflected powers, (c) backward reflected powers, (d) forward absorbed powers, and (e) backward absorb powers of lossy aperiodic multilayered structures with 8 layers (V=8) when Lypjq identified by a superscript of each bi-anisotropic slab is set to 7.0mm with the remaining Lpjq fixed at 5.0 mm (Leo, = 5.0 mm for all conventional layers).
Fig. 11. Dependencies of (a) transmitted powers, (b) forward reflected powers, (c) backward reflected powers, (d) forward absorbed powers, and (e) backward absorb powers of low-loss aperiodic multilayered structures with 8 layers (NV = 8) when Lo, identified by a superscript of each conventional material is set to 7.0 mm with the remaining Leo, fixed at 5.0 mm (Lpiq =5.0 mm for all bi-anisotropic MM slabs).
Fig. 11. Dependencies of (a) transmitted powers, (b) forward reflected powers, (c) backward reflected powers, (d) forward absorbed powers, and (e) backward absorb powers of low-loss aperiodic multilayered structures with 8 layers (NV = 8) when Lo, identified by a superscript of each conventional material is set to 7.0 mm with the remaining Leo, fixed at 5.0 mm (Lpiq =5.0 mm for all bi-anisotropic MM slabs).
Fig. 12. Dependencies of (a) transmitted powers, (b) forward reflected powers, (c) backward reflected powers, (d) forward absorbed powers, and (e) backward absorb powers of lossy aperiodic multilayered structures with 8 layers (V=8) when Lo, identified by a superscript of each conventional material is set to 7.0 mm with the remaining Lo, fixed at 5.0 mm (Lpjq =5.0 mm for all bi-anisotropic MM slabs).
Fig. 12. Dependencies of (a) transmitted powers, (b) forward reflected powers, (c) backward reflected powers, (d) forward absorbed powers, and (e) backward absorb powers of lossy aperiodic multilayered structures with 8 layers (V=8) when Lo, identified by a superscript of each conventional material is set to 7.0 mm with the remaining Lo, fixed at 5.0 mm (Lpjq =5.0 mm for all bi-anisotropic MM slabs).
Related topics:
Materials ScienceOpticsNanotechnologyOptical physicsNatural FrequenciesResonance FrequenciesPeriodic StructuresForward Chaining and Backward ChainingConventional Materialsoptical Anisotropy
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