The plasma jet device is composed of a porous alumina dielectric element, an outer electrode, and a hollow inner electrode.
In practice, to describe the experimental data satisfactorily, one needs to replace the interface capacitor with a constant-phase-angle (CPA) element and to add a non-Debye dielectric element parallel to the resistor to represent the local ionic movement.
Research in nanophotonics is shifting towards all-dielectric elements, particularly in designing tunable and experimentally feasible light manipulating metasurfaces [1, 2].
These devices may find applications in the areas of imaging, polarization control, spectroscopy, and on-chip optoelectronic systems etc., and our studies may richen the design of all-dielectric optical elements at visible wavelength.
The effects of the stiffness of the adhesive bond between the host structure and piezoelectric element, the dielectric loss in a piezoelectric element, and the internal resistance of an inductor are considered in the theoretical analysis.
10a, b Figure 2a displays a gripping element based on dielectric elastomers, 10b the element was fabricated using planar process steps only.
To describe the observed role of the phase interconnectivity on the dielectric properties, Finite Element Modeling calculations were performed.
Therefore, for the graphene-dielectric
The design principles that are required to develop low-dielectric MOFs and structural elements that influence their behavior, as well as the integration of MOFs into metal insulator metal (MIM) devices are discussed.
