Combining eq A8, All, and A12 r¡ = L2/(wAp) (A13) establishes a relation between the characteristic decay time and the ionic mobility in terms of the distance between the probes and the applied potential. Using eq A10 and A13 N¡ = n exp(-x/L) -L < x < L (A14) which agrees with the solution found for the so-called plasma-capacitor in the limit of low charge density (23). Due to the absence of the diffusion term in eq A5, the charge density does not obey the boundary conditions 1V¡(±L) = 0.