TY - JOUR
T1 - Use of single-negative material as a tunable defect in a dielectric photonic crystal heterostructure
AU - Chang, Tsung Wen
AU - Cheng, Chih Jen
AU - Wu, Chien Jang
N1 - Publisher Copyright:
© 2016 Optical Society of America.
PY - 2016/2/1
Y1 - 2016/2/1
N2 - The defect mode in a photonic crystal heterostructure of (1/2)N(2/1)N can be tuned by using a single-negative layer as a defect layer; that is, the structure to be considered is (1/2)ND(2/1)N, where 1, 2 are dielectrics, N is the stack number, and D is a defect layer taken to be a single-negative material. The results show that when D is a mu-negative (μ < 0) medium, the defect mode frequency is redshifted as a function of the thickness of D as well as the static permittivity. On the other hand, if D is an epsilon-negative (ε < 0) medium, the defect mode frequency is blueshifted as the defect layer thickness increases, but it is independent of the static permeability. We also investigate the angular dependence of the defect frequency for both two polarizations, transverse electric (TE) wave and transverse magnetic (TM) wave. The defect mode frequency is shown to be blueshifted as a function of the angle of incidence. Additionally, the shift in the TE wave is larger than that in the TM wave.
AB - The defect mode in a photonic crystal heterostructure of (1/2)N(2/1)N can be tuned by using a single-negative layer as a defect layer; that is, the structure to be considered is (1/2)ND(2/1)N, where 1, 2 are dielectrics, N is the stack number, and D is a defect layer taken to be a single-negative material. The results show that when D is a mu-negative (μ < 0) medium, the defect mode frequency is redshifted as a function of the thickness of D as well as the static permittivity. On the other hand, if D is an epsilon-negative (ε < 0) medium, the defect mode frequency is blueshifted as the defect layer thickness increases, but it is independent of the static permeability. We also investigate the angular dependence of the defect frequency for both two polarizations, transverse electric (TE) wave and transverse magnetic (TM) wave. The defect mode frequency is shown to be blueshifted as a function of the angle of incidence. Additionally, the shift in the TE wave is larger than that in the TM wave.
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U2 - 10.1364/AO.55.000825
DO - 10.1364/AO.55.000825
M3 - Article
AN - SCOPUS:84962124781
SN - 0003-6935
VL - 55
SP - 825
EP - 829
JO - Applied Optics
JF - Applied Optics
IS - 4
ER -