Recent breakthroughs in many-body quantum dynamics have unexpectedly revealed that the growth of entanglement entropy and quantum decoherence strictly follow the Kardar-Parisi-Zhang (KPZ) universality class, an equation originally formulated to describe macroscopic stochastic surface growth. In this paper, we theoretically bridge this empirical observation with the Dynamic Metric Topology (DMT) framework. We demonstrate that the macroscopic "roughness" governed by the KPZ equation in quantum spin systems is not driven by fundamentally stochastic noise, but by a deterministic topological friction between the spinorial phase and the scalar field pseudo-Riemannian manifold. By explicitly mapping the KPZ non-linear growth term to the DMT scalar impedance threshold at H˜ = 114.12 GeV via the fine structure constant (α), we provide a unified tensorial master equation. This integration redefines quantum noise as an uncompensated metric drag, providing a definitive proof through the deterministic evolution of Bell’s inequality parameters.
Understanding how complex entanglement structures emerge is a central problem in quantum many-body physics. Recent work by Zhang et al. [Phys. Rev. Lett. 137, 020404 (2026)] has considered structured initial states prepared by evolving a product state under a chaotic Hamiltonian for a finite time before quenching to the target Hamiltonian. In this setup, total entanglement entropy growth in many-body localized systems exhibits two distinct regimes, first increasing and then decreasing as the initial entanglement is tuned. In this work, we identify the physical origin of this behavior by analyzing the dynamics of both the Rényi entanglement entropy and the Wehrl-Rényi entropy in the random-field XXZ model, the latter of which characterizes multipartite entanglement. We show that a similar non-monotonic dependence on the initial entanglement also appears in the net growth of the Wehrl-Rényi entropy for product states polarized along the z-direction. The first regime is governed by a finite magnetization associated with local integrals of motion, while the second reflects inter-site correlations. In contrast, for product states in the x/y-direction, the entanglement growth exhibits a monotonic decay. Our results provide a more fine-grained picture of how distinct initial-state properties shape entanglement dynamics in many-body localized systems.