to adherence issues between the PDMS substrate and copper thin film), higher than expected dielectric loss for PDMS and scattering associated with variations in device dimensions along the length of the experimental structures.The peak in the attenuation constant at 12.0 GHz, as seen in Figure 5, is most likely due to a TE 11 -like mode that is excited near this frequency. Therefore, we can say that, mode-free, quasi-TEM operation is achievable with these structures with an operational bandwidth of around 12 GHz. A traditional coax structure of comparable dimensions has a cutoff frequency of 11.4 GHz. Given the quasi-TEM nature of the structure, it is expected that the 2.5-D MicroCoax can readily operate at higher frequencies, with little or no change in characteristic impedance, when the dimensions are scaled down in a proportionate fashion.
CONCLUSIONBy utilizing the vertical dimension, thereby changing the surface area of the center conductor, we can increase the number of basic design parameters without affecting the size of the structure's footprint. We have found the 2.5-D MicroCoax structure to have a number of useful features, such as, a large degree of dispersion and impedance control, and potentially high power-handling capability while providing lower cross-talk between adjacent signal lines due to its inherent shielded construction.In general, nonplanar 3-D structures can offer many advantages over traditional 2-D planar types, such as: less dispersion, lower losses, and lower effective dielectric constant. With the structure described here, by varying the center conductor's height, greater flexibility can be exercised over key design parameters such as the characteristic impedance, phase velocity, and attenuation without having to change the center conductor's width or conductor to ground spacing. As a result, conduction and dielectric losses are minimized; current crowding is reduced while power-handling capability is increased-all without sacrificing single mode operation.
DUAL-BAND MONOPOLE