Paper 20:Dynamical Closure of the Scale-Space Framework: Complex Scale Potential, Newtonian Recovery, and the Hidden Configurational Sector

Papers 10–11 of the Scale-Space programme established the corrected five-dimensional metric gtt = − (1 +2/L) c² and identified a configurational energy deficit that required a dynamical source. This paper provides that source through a systematic dynamical closure. We first identify the correct primary variable (gAB) and derive the effective scale potential ΦR = c²/L from the Paper 10 clock factor, making L a derived parameter. The Paper 11 deficit is then rewritten as a nonlinear potential-density relation for ΦR. We show that a purely real closure leads to an unscreened logarithmic correction to Newtonian gravity that is empirically dangerous, and that this is resolved by extending ΦR to a complex scale potential Ψs = ΦR + iΦI. The action for Ψs is: LΨ = − α/2 ∇AΨ∗s∇AΨs − αγ/4 (|Ψs|² − Ψ²0) ² − 2λρm Re (Ψs), λ = −4παG. The Euler-Lagrange equation is derived exactly and its polar decomposition yields a phase-current equation sourced by ordinary matter. Integrating over a spherical source establishes that mass sources exterior phase flux universally, and the real projection of the exterior solution recovers Newtonian gravity ΦR ≈ −GM/r at leading order, with corrections O (r^−4). The imaginarycomponent ΦI ≈ Ψ0 − G²M²/ (2Ψ0r²) constitutes a hidden configurational sector that carries the nonlinear scale-sector stress without appearing directly in observable gravity. All four validation tests (real-limit recovery, logarithm screening, hidden-sector regularity, observable-projection) are satisfied. We further show that superposition of phase fluxes from multiple sources recovers standard Newtonian multi-body gravity exactly. We then address the structural question of whether Ψs alone can supply the Paper 11 anisotropic background deficit. It cannot: a complex scalar yields an isotropic cosmological-constant-like stress, not the required pure clock-sector form. We resolve this by deriving a constrained configurational action with a clock-ordering covector nA, which supplies Tᶜonf AB = E (ΦR) nAnB exactly, with E = −3/ (κ5L³). This reproduces the Paper 11 deficit with no unwanted spatial or scale components. A candidate 5D covariant form of the full action is stated. Two items remain open: the value of Ψ0 from a background constraint calculation; and the interior solution matching.