TY - JOUR
T1 - Photonic band gap materials comprising positive-phase-velocity and negative-phase-velocity layers in waveguides
AU - Gómez, Álvaro
AU - Martínez Ricci, María L.
AU - Depine, Ricardo A.
AU - Lakhtakia, Akhlesh
N1 - Funding Information:
Álvaro Gómez was supported by the Dirección General de Investigación of the Spanish Ministerio de Educación y Ciencia, under the project/grant TEC2006–13268– C03–01. Akhlesh Lakhtakia thanks the Charles Godfrey Binder Endowment at Penn State for partial support. María Luz Martínez Ricci and Ricardo Depine acknowledge financial support from Consejo Nacional de Investigaciones CientíEcas y Técnicas (CONICET), Agencia Nacional de Promoción CientíEca y Tecnológica (BID1728/OC–AR PICT-11–1785) and Universidad de Buenos Aires (UBA-X062).
PY - 2009/9
Y1 - 2009/9
N2 - We have analyzed electromagnetic wave propagation in photonic bandgap (PBG) structures comprising alternating layers of isotropic dielectric-magnetic materials with positive phase velocity and negative phase velocity, implemented in different waveguides of uniform cross-section (parallel-plate, rectangular, circular, and coaxial) and perfectly conducting walls. The structures could be either ideal (i.e. of infinite extent along the waveguide axis) or real (i.e. terminated at both ends with homogeneously filled waveguide sections). The spectral locations of the band gaps do not directly depend on the cross-sectional shape and dimensions, but on the cut-off parameter instead, for ideal structures. The band gaps of an ideal structure are located in spectral regions where the reflectance of the corresponding real structure is large. The real structures show four types of band gaps, only one type of which is due to the periodically repetitive constitution of the PBG structure; the remaining three types are not of the Bragg type.
AB - We have analyzed electromagnetic wave propagation in photonic bandgap (PBG) structures comprising alternating layers of isotropic dielectric-magnetic materials with positive phase velocity and negative phase velocity, implemented in different waveguides of uniform cross-section (parallel-plate, rectangular, circular, and coaxial) and perfectly conducting walls. The structures could be either ideal (i.e. of infinite extent along the waveguide axis) or real (i.e. terminated at both ends with homogeneously filled waveguide sections). The spectral locations of the band gaps do not directly depend on the cross-sectional shape and dimensions, but on the cut-off parameter instead, for ideal structures. The band gaps of an ideal structure are located in spectral regions where the reflectance of the corresponding real structure is large. The real structures show four types of band gaps, only one type of which is due to the periodically repetitive constitution of the PBG structure; the remaining three types are not of the Bragg type.
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U2 - 10.1080/09500340903289128
DO - 10.1080/09500340903289128
M3 - Article
AN - SCOPUS:74549179655
SN - 0950-0340
VL - 56
SP - 1688
EP - 1697
JO - Journal of Modern Optics
JF - Journal of Modern Optics
IS - 15
ER -