Hodge-Metric Sector Coordinates
Implementation & benchmark of arXiv:2608.01596 — Beyond $K$-Theory: Geometry and Holomorphy in Hyperbolic Band Theory
Source paper: Beyond $K$-Theory: Geometry and Holomorphy in Hyperbolic Band Theory arXiv:2608.01596 ⓘ · analyzed Aug 31, 2026
AI-generated research hypothesis, automatically tested. Not peer-reviewed.
Idea description
Parameterize continuous representation sectors using the Hodge geometry of the character torus rather than arbitrary Euclidean coordinates. Use the resulting metric to encode sector locations and impose local spectral smoothness, allowing a model to interpolate between geometrically nearby twists while retaining non-topological variation.
Formulas
Mathematical statement
For a closed hyperbolic surface X, abelian sectors are characters chi: Gamma -> U(1) and form the Jacobian torus H^1(X;R)/(2 pi H^1(X;Z)). Choose a basis omega_1,...,omega_{2g} of harmonic one-forms and write a sector as theta in [0,2 pi)^{2g}, with chi_theta(gamma)=exp(i theta^T n_gamma), where n_gamma in Z^{2g} is the homology coordinate of gamma. The paper states that, up to an area-dependent normalization, the bottom-band Hessian is the Hodge inner product on H^1(X;R): the Hessian of E_0 at theta=0 is proportional to the Hodge Gram matrix G. The local squared distance is d_G(theta,theta')^2 = delta^T G delta, where delta is the wrapped torus difference. The transferable asset is this explicit positive-definite metric, which gives a principled notion of nearby representation sectors.
Implementation notes
1. Integration point: add a continuous sector coordinate to a graph encoder, neural operator, or surrogate model for twisted Hamiltonians. The input is a graph or sample x together with a character coordinate theta. Encode theta using Fourier features after whitening by the Hodge matrix G, then inject the embedding into the first MLP block or into graph-message biases. 2. Pseudocode: estimate a positive-definite matrix G; compute a Cholesky factor G=L L^T; for every sector theta compute the wrapped coordinate delta=wrap(theta) and q=L^T delta; form e_theta=[sin(Bq), cos(Bq)] for a fixed or learned frequency matrix B; predict f(x,theta)=Net(x,e_theta). During training, sample sector pairs theta_a and theta_b and add the kernel-weighted consistency loss from the displayed formula to the task loss. 3. In the paper, G is the Hodge inner-product matrix, proportional to the bottom-band Hessian. In a generic implementation it can be estimated by finite differences of a scalar response E_0(theta): G_ij approximately equals [E_0(h e_i+h e_j)-E_0(h e_i-h e_j)]/(4h^2), followed by symmetrization and eigenvalue clipping. The loss weight, bandwidth sigma, and Fourier bandwidth B are empirical choices. 4. First cheap experiment: use a small twisted-graph Hamiltonian generator with genus g=2, sample many theta sectors, and train a three-layer MLP or GNN to predict the lowest eigenvalue and selected eigenvector observables. Compare raw-coordinate Fourier features, ordinary Euclidean smoothness, and Hodge-whitened coordinates at equal sample count. Measure interpolation error and extrapolation error on held-out sectors, especially along anisotropic directions. Success is lower error per training sector while preserving sharp nonconstant spectral variation.
Verification
This idea has not been verified yet.
Verification happens in two stages: Stage 1 — a mechanism check on a toy system confirms the claimed mathematical phenomenon reproduces; Stage 2 — a benchmark implements the idea on a real (small) neural network task and compares it against a tuned baseline over 8 paired seeds with a permutation test.
Artifacts
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