Learning Manifold and Itô Dynamics with Branched Neural Rough Differential Equations

Luke Thompson, Dai Shi, Lequan Lin, Junbin Gao, Andi Han
6/3/2026
cs.LG

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Abstract

Neural rough differential equations (NRDEs) stay accurate under irregular sampling while taking far fewer integration steps than standard neural differential equations, summarising a finely sampled driver by its log-signature and advancing the hidden state over coarse intervals using the log-ODE method. This efficiency rests on the shuffle algebra, the algebraic counterpart of Stratonovich calculus. This reliance means NRDEs cannot expose the quadratic-variation terms Itô dynamics require, nor the ordered covariant derivatives that govern Itô flows on connection-equipped manifolds. Ameliorating this, we introduce Branched Neural Rough Differential Equations (B-NRDEs), a Hopf-algebraic framework that recasts the NRDE log-ODE step as geometric numerical integration on the state-space manifold, matching the driving algebra to the governing calculus: Grossman--Larson rooted trees for Euclidean Itô dynamics, Munthe-Kaas--Wright planar rooted trees for ordered covariant derivatives on manifolds, and the shuffle algebra in the classical Stratonovich case. This yields intrinsic coarse-step dynamics that exactly preserve manifold constraints. Finally, we introduce a branched signature-kernel objective to enable Itô-consistent law matching by making quadratic-variation terms visible during training. On rough Bergomi volatility, sim-to-real $\mathrm{SO}(3)$ dynamics forecasting, and SPD covariance dynamics, B-NRDEs offer a unified, effective approach to stochastic and manifold-valued dynamics beyond the Euclidean--Stratonovich setting.

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@article{thompson2026learning,
  title  = {Learning Manifold and Itô Dynamics with Branched Neural Rough Differential Equations},
  author = {Luke Thompson and Dai Shi and Lequan Lin and Junbin Gao and Andi Han},
  year   = {2026},
  eprint = {2606.05272},
  archivePrefix = {arXiv},
  url    = {http://arxiv.org/abs/2606.05272v1}
}

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