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Omnidirectional photonic band gap enlarged by one-dimensional ternary unmagnetized plasma photonic crystals based on a new Fibonacci quasiperiodic structure
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10.1063/1.4765063
/content/aip/journal/pop/19/11/10.1063/1.4765063
http://aip.metastore.ingenta.com/content/aip/journal/pop/19/11/10.1063/1.4765063
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Schematic diagram of 4th order Fibonacci quasiperiodic 1D ternary PPCs consisting of quartz glass (A), air (B), and plasma (P) under any incidence angle (θ) for TE and TM waves.

Image of FIG. 2.
FIG. 2.

Reflectance spectra of 1D binary PPCs consisting of alternate dielectrics A and B at various incidence angles with dA  = 5 mm and dB  = 5 mm. The black solid (red dash dot) curves are for TM (TE) wave.

Image of FIG. 3.
FIG. 3.

Reflectance spectra of Fibonacci quasiperiodic 1D ternary PPCs based on a new structure at various incidence angles with dA  = 5 mm, dB  = 5 mm, and dp  = 1 mm. The black solid (red dash dot) curves are for TM (TE) wave, and the gray regions and the gray areas correspond to the OBG.

Image of FIG. 4.
FIG. 4.

Normal incident reflection spectra for the different order Fibonacci structures as a function of the frequency with (a) G 3, (b) G 4, (c) G 5, and (d) G 7.

Image of FIG. 5.
FIG. 5.

Normal incident reflection spectra for the different order Fibonacci structures as a function of the frequency with (a) G 9, (b) G 10, (c) G 11, and (d) G 12.

Image of FIG. 6.
FIG. 6.

Reflectance of Fibonacci quasiperiodic 1D ternary PPCs based on a new structure versus frequency at normal incidence with different plasma thicknesses.

Image of FIG. 7.
FIG. 7.

Reflection coefficients of Fibonacci quasiperiodic 1D ternary PPCs based on a new structure versus frequency as a function of the plasma thickness at normal incidence.

Image of FIG. 8.
FIG. 8.

The frequency range of OBG for Fibonacci quasiperiodic 1D ternary PPCs based on a new structure as a function of the plasma thickness.

Image of FIG. 9.
FIG. 9.

Reflectance of Fibonacci quasiperiodic 1D ternary PPCs based on a new structure versus frequency at normal incidence with different plasma densities.

Image of FIG. 10.
FIG. 10.

Reflection coefficients of Fibonacci quasiperiodic 1D ternary PPCs versus based on a new structure frequency as a function of the plasma density at normal incidence.

Image of FIG. 11.
FIG. 11.

The frequency range of omnidirectional band gap for Fibonacci quasiperiodic 1D ternary PPCs based on a new structure as a function of the plasma density.

Image of FIG. 12.
FIG. 12.

Reflectance of Fibonacci quasiperiodic 1D ternary PPCs based on a new structure versus frequency at normal incidence with different plasma collision frequencies.

Image of FIG. 13.
FIG. 13.

The frequency range of OBGs for Fibonacci quasiperiodic 1D ternary PPCs based on a new structure as a function of log10 v c/ v 0.

Image of FIG. 14.
FIG. 14.

Reflectance of 1D PCs versus frequency at normal incidence with different structures: (a) PCs without plasma, (b) conventional ternary PPCs, (c) conventional ternary Fibonacci quasiperiodic PPC, and (d) the PPCs with new Fibonacci quasiperiodic structure, respectively.

Image of FIG. 15.
FIG. 15.

Photonic band structure of (a) new Fibonacci quasiperiodic 1D ternary PPCs, (b) conventional Fibonacci quasiperiodic 1D ternary PPCs, and (c) conventional 1D ternary PPCs in terms of angular frequency and incidence angle, respectively. The areas between two white lines are the OBGs.

Image of FIG. 16.
FIG. 16.

The reflectance spectra of Fibonacci unit cell and new PPCs various incidence angles. The gray regions and the gray areas correspond to theOBG.

Image of FIG. 17.
FIG. 17.

Normal incident reflection spectra for the different number of periods as a function of the frequency with (a) N 2 = 5, (b) N 2 = 10, (c) N 2 = 15, and (d) N 2 = 20.

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/content/aip/journal/pop/19/11/10.1063/1.4765063
2012-11-05
2014-04-18
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Omnidirectional photonic band gap enlarged by one-dimensional ternary unmagnetized plasma photonic crystals based on a new Fibonacci quasiperiodic structure
http://aip.metastore.ingenta.com/content/aip/journal/pop/19/11/10.1063/1.4765063
10.1063/1.4765063
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