{ "help": "Return the metadata of a dataset (package) and its resources. :param id: the id or name of the dataset :type id: string", "success": true, "result": { "id": "8cb15716-7479-4f8b-8991-95fbcc9701a5", "url": "https://www.inptdat.de/node/106", "source": { "name": "DBD", "application": "film deposition, PECVD", "specification": "AC, low frequency, atmospheric pressure, non-thermal", "properties": "
Atmospheric pressure DBD between plane electrodes covered by dielectrics (glass and Macor); Powered electrode: Macor covered, thickness of dielectric: 3.5 mm; Grounded electrode: glass covered, thickness of dielectric: 3.0 mm; Discharge gap: 2 mm; Discharge area: 216 cm^2; Voltage supply: sinusoidal voltage with amplitude of 3.9 kV and frequency of 20 kHz; RMS current: about 50 mA
\n" }, "medium": { "name": "Ar, HMDSO", "properties": "Gas temperature: 300 K; Pressure: 1 atm; Gas mixture: Ar + 20 to 1600 ppm HMDSO
\n" }, "target": [], "diagnostics": { "name": "fluid-Poisson model", "properties": "The time-dependent, spatially one-dimensional fluid-Poisson model includes particle balance equations for the densities of electrons, relevant neutral particles and ions, the electron energy balance equation to determine the mean electron energy, the Poisson equation to calculate the electric potential and field, as well as a balance equation for the surface charge density to consider the accumulation of charge carriers on the dielectric surfaces. Details about the basic equations, the reaction kinetics model, the transport properties and rate coefficients, the boundary conditions and the solution method are reported in Loffhagen et al. (https://doi.org/10.1002/ctpp.201700060).
\n" }, "resource": [ { "id": "a05f6413-eb86-4a4f-8063-e88f9f6faedb", "url": "https://www.inptdat.de/system/files/node106_data-table_plasmaparameters.csv", "filetype": "csv", "datatype": "data table", "range": "Ar-HMDSO mixture at 1 atm including 20 to 1600 ppm HMDSO", "quality": "verified" } ] } }