Entanglement is often introduced as a bipartite resource defined by the non-factorization of a joint state across tensor-product subsystems. While operationally powerful in finite-dimensional quantum me- chanics, this notion becomes conceptually and technically inadequate in relativistic quantum field theory (QFT), where there is no canonical Hilbert-space factorization into spatial subsystems and local von Neu- mann algebras are typically of type III. We develop an algebraic, modular formulation of entanglement in which correlations are intrinsic properties of global states on nets of local operator algebras. Using Tomita–Takesaki theory, we show that faithful states induce canonical modular flows that generically intertwine local subalgebras, yielding a holistic (non-n-counting) multipartite entanglement structure independent of any particle-based decomposition. We further connect this viewpoint to thermality and nonequilibrium structure. Modular dynamics naturally unifies entanglement with KMS equilibrium, and motivates state-based witnesses of modular mixing that are directly tied to expectation values. In this spirit, recent high-precision large-statistics tests of Born-rule outcome frequencies on superconducting quantum processors can be interpreted as probing equilibrium fixed points of an underlying modular balance, with controlled, normalization- preserving deviations in nonequilibrium regimes. Although such devices are finite (type I) systems and do not realize type III locality, they provide laboratory analogues in which modular structure emerges effectively at the statistical level. The resulting framework yields an observer-independent notion of entanglement in relativistic quantum theory and clarifies its links to nonequilibrium quantum thermo- dynamics and emergent geometric structure.