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The properties of photonic band gaps for three-dimensional plasma photonic crystals in a diamond structure
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10.1063/1.4801043
/content/aip/journal/pop/20/4/10.1063/1.4801043
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/4/10.1063/1.4801043
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Schematic structure of three-dimensional unmagnetized plasma photonic crystals with diamond lattices. (a) type-1 with dielectric spheres in plasma background and (b) type-2 with plasma sphere immersed in dielectric background.

Image of FIG. 2.
FIG. 2.

Brillouin zone showing symmetry point used for computing the band structures.

Image of FIG. 3.
FIG. 3.

The band structure of EM waves for type-1 three-dimensional PPCs with εa  = 12 and f = 0.35 but with different plasma frequency and collision frequency. (a) ωp  = 0, νc  = 0, and (b) ωp  = 0.15ωp 0, νc  = 0.02ωp . The red shaded regions indicate PBGs.

Image of FIG. 4.
FIG. 4.

The band structure of EM waves for type-2 three-dimensional PPCs with εa  = 12 and f = 0.35 but with different plasma frequency and collision frequency. (a) ωp  = 0, νc  = 0, and (b) ωp  = 0.15ωp 0, νc  = 0.02ωp . The red shaded regions indicate PBG.

Image of FIG. 5.
FIG. 5.

The effects of relative dielectric constant on the PBGs for two types of three-dimensional PPCs with ωp  = 0.15ωp 0 and νc  = 0.02ωp , respectively. The shaded regions indicate the PBGs. (a) type-1 structure with f = 0.35, (b) type-2 structure with f = 0.5.

Image of FIG. 6.
FIG. 6.

The gap over the midgap frequency as a function of relative dielectric constant for the PBGs of both types of three-dimensional PPCs with ωp  = 0.15ωp0 and νc  = 0.02ωp , respectively. (a) type-1 structure with f = 0.35, (b) type-2 structure with f = 0.5.

Image of FIG. 7.
FIG. 7.

The effects of filling factor on the PBGs for both types of three-dimensional PPCs with εa  = 12, ωp  = 0.15ωp 0 and νc  = 0.02ωp , respectively. The shaded regions indicate the PBGs. (a) type-1 structure, (b) type-2 structure.

Image of FIG. 8.
FIG. 8.

The gap over the midgap frequency as a function of filling factor for the PBGs of both types of three-dimensional PPCs with εa  = 12, ωp  = 0.15ωp 0, and νc  = 0.02ωp , respectively. (a) type-1 structure, (b) type-2 structure.

Image of FIG. 9.
FIG. 9.

The effects of plasma frequency on the PBGs for both types of three-dimensional PPCs with εa  = 12 and νc  = 0.02ωp , respectively. The shaded regions indicate the PBGs. (a) type-1 structure with f = 0.35, (b) type-2 structure with f = 0.5.

Image of FIG. 10.
FIG. 10.

The gap over the midgap frequency as a function of plasma frequency for the PBGs of two types of three-dimensional PPCs with εa  = 12 and νc  = 0.02ωp , respectively. (a) type-1 structure with f = 0.35, (b) type-2 structure with f = 0.5.

Image of FIG. 11.
FIG. 11.

The effects of plasma collision frequency on the PBGs for both types of three-dimensional PPCs with εa  = 12 and ωp  = 0.15ωp0 , respectively. The shaded regions indicate the PBGs. (a) type-1 structure with f = 0.35, (b) type-2 structure with f = 0.5.

Image of FIG. 12.
FIG. 12.

The gap over the midgap frequency as a function of plasma collision frequency for the PBGs of both types of three-dimensional PPCs εa  = 12 and ωp  = 0.15ωp0 , respectively. (a) type-1 structure with f = 0.35, (b) type-2 structure with f = 0.5.

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/content/aip/journal/pop/20/4/10.1063/1.4801043
2013-04-12
2014-04-23
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: The properties of photonic band gaps for three-dimensional plasma photonic crystals in a diamond structure
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/4/10.1063/1.4801043
10.1063/1.4801043
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