Show source-provided references
4. D.Ramaccia A.Monti M.Barbuto et al. “Reconfigurability in Electromagnetic Metasurfaces and Metamaterials for Antennas Systems: State‐of‐the‐art Technical Approaches Limitations and Application ”IEEE Antennas and Propagation Magazine(2025) in press.
10.36227/techrxiv.171527069.96967113/v1 ↗23. K.Kanth Varikuntla M.Ali Babar Abbasi andO.Yurduseven “Reconfigurable Plasma Frequency Selective Surface ” in2025 URSI Int. Symp. on Electromagnetic Theory (EMTS)(2025) 1–4.
10.23919/EuCAP63536.2025.10999840 ↗28. Tunable Transmissive Metagratings Using Single Layer Cylindrical Plasma Discharges
29. Shun'ko E. V. · 2009
31. Bittencourt J. A. · 2013
33. COMSOL “Comsol Multiphysics ”https://www.comsol.com/plasma‐module.
34. COMSOL “The Plasma Module User's Guide ”https://doc.comsol.com/5.4/doc/com.comsol.help.plasma/PlasmaModuleUsersGuide.pdf.
35. COMSOL “Introduction to the Plasma Module ”https://doc.comsol.com/5.5/doc/com.comsol.help.plasma/IntroductionToPlasmaModule.pdf.
36. COMSOL “Dc Glow Discharge ”https://www.comsol.com/model/dc‐glow‐discharge‐8640.
37. Phelps “Phelps Database ”https://www.lxcat.net.
45. LXCat Project Database.
46. The average electron velocity (magnitude) v¯$\bar{v}$ can be calculated from the Maxwellian distribution functionf(v)=2π(mekBTe)3/2v2e−mv2/2kBTe$f(v)=\sqrt {\frac{2}{\pi }} (\frac{m_e}{k_B T_e})3/2v^2e-mv^2/2k_B T_e$ asv¯=∫0∞vf(v)dv$\bar{v}=\int _0\infty vf(v)dv$. The distribution functionf(v)$f(v)$is obtained by the standard Maxwell–Boltzmann distribution function f(v)$f({\bf v})$ in 3D after decomposition is spherical coordinates.v=|v|$v=|{\bf v}|$.
48. A.Ashrafian F.Sadeghikia J. A.Rashed Mohassel M.Himdi andM.Magarotto “Tunable Rectangular Waveguide Bandpass Filter Based on Plasma Technology ” in2024 18th European Conf. on Antennas and Propagation (EuCAP)(2024) 1–4.
10.23919/EuCAP60739.2024.10501406 ↗