A one-dimensional ͑1D͒ photonic metal parallel plate waveguide is presented in the spectral range of 0.5-3 THz that has high throughput and stop bands with up to the experimental limit of 40 dB of dynamic range. By incorporating a defect into the periodic bottom plate of the waveguide, a transmission resonance is generated in the first stop band with a Q value of 120 and a dynamic range of over 17 dB. The 1D geometry allows the utilization of the mode matching technique to analytically calculate the transmission of the photonic waveguide. © 2007 American Institute of Physics. ͓DOI: 10.1063/1.2710002͔The metal parallel plate waveguide ͑PPWG͒ is the ideal structure for single transverse electromagnetic ͑TEM͒ mode guiding of subpicosecond pulses with frequencies in the terahertz regime due to its low loss, undistorted propagation and ease of coupling.1,2 Waveguide terahertz time-domain spectroscopy ͑THz-TDS͒ has detected water layers as thin as 20 nm. 3 The sensitivity of waveguide terahertz TDS can be further increased by adiabatic compression of the waveguide plates, combining the benefits of a closer plate spacing to increase sensitivity along with higher coupling at optimal plate spacing. 4 More recently, cooling the PPWG to liquid nitrogen temperatures has enabled the measurement of linewidths as much as five times narrower than has been previously observed for a variety of thin organic films.
5In addition to the above spectroscopic work, there have also been studies of the effect of photonic band gap ͑PBG͒ materials inside the waveguide with transmission through the PBG structure, 6,7 and alternatively in an air gap adjacent to the PBG structure. 8,9 The strong band gaps produced by these structures are useful for their filtering capabilities and also allow the opportunity to integrate defects. A high Q filter inside a PPWG would couple the waveguide sensitivity enhancement with a longer interaction time between the sample and the resonating frequency for increased sensitivity. By placing a sample film over the PBG surface, small changes in the defect resonance frequency would occur, indicating the potential utilization as a sensor. As the Q value increases, smaller frequency shifts can be observed, and the more sensitive the sensor becomes.Previous experiments in which a two-dimensional metallic PBG structure was used as the bottom plate of a PPWG were promising, demonstrating sharp band gap turn-ons and high dynamic range.8 Despite these intriguing results, the ratio of component size to wavelength prevented the use of circuit theory approximations for theoretical predictions, as used on similar structures in the microwave regime.10-12 Additionally, the two-dimensional periodicity blocked the calculation of the theoretical output of such a structure. As such physical insight into the locations and strength of the band gaps was not possible.Here, in order to obtain a tractable theoretical problem in our frequency range of 0.5-3 THz and to enable the design of filters with specified properties, the periodicit...