“…With the variable X = √ z, the resistivity problem is reduced to studying the sequence of Padé approximants R n = r n,n+1 (X), n = 1, 2...l/2, with X ∈ [0, ∞), and analogy with the Stieltjes truncated moment problem [1,14,34], is complete as long as the resistivity expands at X → ∞ in the Laurent polynomial with the signalternating coefficients, coinciding with the "Stieltjes-moments" µ k (see e.g., [49,48], were the original work of Stieltjes is explained very clearly).…”