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Analytical model investigates S-band RF wave reflection in cylindrical plasma, indicating design potential for adaptive systems.
We present a three-component analytical model for the phase of S-band (2.86 GHz) radio frequency (RF) waves reflected from cylindrical plasma columns. The total reflected phase is decomposed into volumetric propagation inside the plasma, surface reflection at the air–plasma interface, and an effective-boundary-displacement term, all derived from the frequency-dependent Drude permittivity. Independent full-wave FDTD simulations confirm the model’s accuracy. Parametric analysis across plasma radius, gas type, and electron density reveals that electron density primarily sets the overall reflection magnitude, while the column radius and electron–neutral collision frequency fine-tune amplitude and phase. For a mid-range radius ( ∼ 7 mm ) at reference density, argon produces a reflected amplitude of ∼ 0 . 36 , nitrogen ∼ 0 . 12 , and air ∼ 0 . 06 , with total phases spanning 30 0 ∘ − 35 5 ∘ . Denser argon plasmas at smaller radii achieve near-complete reflection ( ∼ 0 . 8 ) with phases around 18 0 ∘ − 20 0 ∘ , enabling constructive interference in resonant structures. These results demonstrate a physically transparent, quantitatively validated framework for designing tunable S-band plasma switches and adaptive reflective waveguide elements, highlighting the potential of plasma columns as reconfigurable phase- and amplitude-engineered RF components.
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Taghinejad et al. (2026) studied this question.
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