Interface Impedance of the Envelope Touch-Wave Packet: Definition, Analysis, and Predictions

This paper defines the interface impedance of the Envelope Touch-Wave Packet and derives its properties. Starting from the definitions of the dielectron Oₑ and the fluxon O_Φ in the Fluxon and Dielectron paper, we derive that the interface impedance is Z = Φ/e = sqrt(μₓ/εₓ). In the WQT framework, the two entries — one through permeability and permittivity, one through magnetic flux and charge — give exactly the same expression, and therefore the same value. This is not a coincidence: it is a consequence of the fact that ε and μ share the same denominator in the WQT framework, differing only in their numerators e² and Φ². We further show that this impedance is the direct manifestation of the indentation depth of the touch-wave packet on the parent envelope interface: the deeper the indentation, the larger the deviation of K from 1, and the larger the deviation of the impedance from its baseline value. We identify the source of the discrepancy in standard physics: standard physics computes sqrt(μ₀/ε₀) = μ₀c = 376.73 Ω and Φ₀/e = h/e² = 25812.8 Ω, two values that differ by a factor of 1/(2α) = 68.5. This discrepancy is not physical; it is a consequence of the fact that ε₀ and μ₀ are defined through two different experimental routes (Coulomb force and Ampere force), each carrying different geometric factors. In the WQT framework, ε and μ share the same definition route, and the two impedances unify into a single quantity. Finally, this paper makes a set of falsifiable predictions: the interface impedance is not a universal constant but a layer-dependent projection reading, and therefore varies with heliocentric distance and local electromagnetic environment. Keywords: interface impedance, envelope touch-wave packet, touch-wave packet indentation, dielectron, fluxon, electromagnetic scaling factor, Kₒ, fine-structure constant, layer-dependent constant, falsifiable prediction