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Collective ordering in correlated electron systems produces emergent, non-Markovian dynamics that cannot be closed at the level of coarse-grained observables alone. This paper proposes a graph-recurrent neural network (GRNN) that fuses gated recurrent memory with graph message passing to learn finite-time evolution maps directly from trajectories, bypassing repeated microscopic force evaluations. Site-resolved hidden states encode unresolved history and communicate across neighboring sites via graph-coupled hidden messages, giving a scalable, translationally invariant update rule. The authors demonstrate the approach on charge-density-wave domain coarsening in the semiclassical Holstein model, showing quantitative agreement with kernel-polynomial-method reference dynamics.
Bridging quantum-mechanical accuracy with mesoscopic length and time scales remains a grand challenge in materials modeling. This paper develops an ab initio phase-field framework that derives the mesoscopic evolution equation from molecular dynamics via Mori–Zwanzig projection, leaving only the free energy and mobility to be learned by neural networks from short machine-learning-interatomic-potential trajectories. The result is a data-efficient approach that propagates ab initio accuracy to scales far beyond direct atomistic simulation, demonstrated here on iron–boron melts and hydrogen–helium mixtures under planetary conditions.
Recent theoretical models of diffusion as coupled Ornstein-Uhlenbeck processes predict a hierarchy of interaction timescales creating a synchronization gap between global and local committing modes. This work investigates how this gap mechanistically emerges within pretrained Diffusion Transformers by introducing a controlled architectural realization of replica coupling via symmetric cross-attention gates with strength $g$. Through linearized analysis and empirical probing of DiT-XL/2 across all 28 layers, the authors demonstrate that the gap is an intrinsic, depth-localized property that collapses under strong coupling as $\mathcal{O}(\frac{1-g}{1+g})$, providing a bridge between continuous statistical physics and discrete transformer dynamics.