Topological Structures of Large Scale Interacting Systems via Uniform Functions and Forms
Kenichi Bannai, Yukio Kametani, Makiko Sasada
TL;DR
The paper develops a new, purely algebraic framework—uniform cohomology—for analyzing macroscopic observables in large-scale interacting systems on infinite graphs. By introducing uniform functions and forms on the configuration space S^X, it proves that the zeroth uniform cohomology H^0_unif(S^X) naturally corresponds to conserved quantities and that higher uniform cohomology vanishes, facilitating a clean separation of local and global effects. The central result is a Varadhan-type decomposition in a broad, group-action setting: for irreducibly quantified interactions and locales with a free G-action, the space of shift-invariant closed uniform forms modulo exact forms is canonically isomorphic to Hom(G, Consv^φ(S)), with a decompositional split C ≅ E ⊕ Hom(G, Consv^φ(S)). This framework, which avoids spectral-gap arguments, provides a universal, cohomological lens to understand hydrodynamic limits and macroscopic evolution across a wide class of nongradient models, tying microscopic conserved quantities to macroscopic flows through a group-cohomology perspective.
Abstract
In this article, we investigate the topological structure of large scale interacting systems on infinite graphs, by constructing a suitable cohomology which we call the uniform cohomology. The central idea for the construction is the introduction of a class of functions called uniform functions. Uniform cohomology provides a new perspective for the identification of macroscopic observables from the microscopic system. As a straightforward application of our theory when the underlying graph has a free action of a group, we prove a certain decomposition theorem for shift-invariant closed uniform forms. This result is a uniform version in a very general setting of the decomposition result for shift-invariant closed $L^2$-forms originally proposed by Varadhan, which has repeatedly played a key role in the proof of the hydrodynamic limits of nongradient large scale interacting systems. In a subsequent article, we use this result as a key to prove Varadhan's decomposition theorem for a general class of large scale interacting systems.
