TY - JOUR
T1 - Terahertz transmission properties of a triadic-Cantor-set photonic crystal containing a semiconductor
AU - King, Tzu Chyang
AU - Liu, Chi Chung
AU - Huang, Chih Hsi
AU - Wu, Chien Jang
N1 - Publisher Copyright:
© 2016 Elsevier B.V. All rights reserved.
PY - 2016/8/1
Y1 - 2016/8/1
N2 - Terahertz transmission properties of a stage 3 triadic-Cantor-set photonic crystal (S3 TCS PC) containing a semiconductor of n-InSb are theoretically investigated. With the resonant frequency in the permittivity function of n-InSb, transmission responses can be classified as three regions. In the two regions with frequencies well above and below the resonant frequency, the permittivity functions are nearly a positive constant and n-InSb is dielectric-like. For these two regions, transmittance response of S3 TCS PC at a given number of periods Np reveals that, within a photonic band gap, there are two groups of defect modes with numbers of Np and Np-1, respectively. Defect modes are shown to be blue-shifted as the angle of incidence increases for both TE and TM waves. Additionally, adjusting the layer thickness enables us to control mode positions for the group of (Np-1)-mode, but the one with Np-mode is not able to be controlled. In a region of 5.1-6.2 THz, where the loss is large, there also are many transmission modes.
AB - Terahertz transmission properties of a stage 3 triadic-Cantor-set photonic crystal (S3 TCS PC) containing a semiconductor of n-InSb are theoretically investigated. With the resonant frequency in the permittivity function of n-InSb, transmission responses can be classified as three regions. In the two regions with frequencies well above and below the resonant frequency, the permittivity functions are nearly a positive constant and n-InSb is dielectric-like. For these two regions, transmittance response of S3 TCS PC at a given number of periods Np reveals that, within a photonic band gap, there are two groups of defect modes with numbers of Np and Np-1, respectively. Defect modes are shown to be blue-shifted as the angle of incidence increases for both TE and TM waves. Additionally, adjusting the layer thickness enables us to control mode positions for the group of (Np-1)-mode, but the one with Np-mode is not able to be controlled. In a region of 5.1-6.2 THz, where the loss is large, there also are many transmission modes.
KW - Cantor multilayer
KW - Defect modes
KW - Negative permittivity
KW - Semiconductor
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U2 - 10.1016/j.optcom.2016.04.010
DO - 10.1016/j.optcom.2016.04.010
M3 - Article
AN - SCOPUS:84963632258
SN - 0030-4018
VL - 372
SP - 91
EP - 97
JO - Optics Communications
JF - Optics Communications
ER -