2011
DOI: 10.1063/1.3549834
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Thermally tunable and omnidirectional terahertz photonic bandgap in the one-dimensional photonic crystals containing semiconductor InSb

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Cited by 83 publications
(40 citation statements)
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“…The second gap with a lower band edge around 4 THz is the so-called Bragg gap, which is consistent with the result of Figure 3 in Ref. [28]. It is also worthy to mention that the band edge and the gap width in the second gap cannot be estimated by usual formulas in the theory of Bragg reflector because InSb is strongly dispersive medium.…”
Section: Numerical Results and Discussionsupporting
confidence: 76%
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“…The second gap with a lower band edge around 4 THz is the so-called Bragg gap, which is consistent with the result of Figure 3 in Ref. [28]. It is also worthy to mention that the band edge and the gap width in the second gap cannot be estimated by usual formulas in the theory of Bragg reflector because InSb is strongly dispersive medium.…”
Section: Numerical Results and Discussionsupporting
confidence: 76%
“…The calculated CPBSs here are in sharp contrast with those in Ref. [28], where there is no K i and nonbending in K r in the first band gap because the damping frequency γ = 0 has been taken.…”
Section: Numerical Results and Discussioncontrasting
confidence: 51%
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“…= √ 2 ( 0 ⁄ ). The carrier density N depends strongly on the temperature T, which makes the plasma frequency tunable by changing the temperature T. In the following calculations, the adopted parameters of the Drude model for InSb are set as ∞ = 15.68, = 0.015 (where is the mass of electron) and = 0.1 THz [34]. Figure 2 (a) shows the real part of the permittivity of InSb (Re(InSb)) as functions of the operating temperature (T) and frequency of incident wave (f).…”
Section: ≪ 1 ⁄mentioning
confidence: 99%