“…ε , which cannot be additively decomposed into "independent" parts pertaining to the soft and stiff components, owing to the transmission interface conditions on the common boundary Γ of the two, the M -function turns out to be additive (cf., e.g., [27], where this additivity was observed and exploited in an independent, but closely related, setting of scattering). In what follows we will observe that the resolvent (A Alongside the transmission problem (9), whose boundary conditions can now be (so far, formally) represented as Γ 1 u = 0, u ∈ dom A 0 ran Π, in what follows we consider a wider class of problems, formally given by transmission conditions of the type…”