Architecture ideas

Attention variants, state-space and recurrent cells, normalization and token-mixing schemes — each tested against the standard block it replaces.

✗ Failed on benchmark 2026

Non-Abelian Event-Order Memory

Augment an RNN or state-space model with a three-dimensional auxiliary spin updated by noncommuting rotations associated with event types or token classes. The ordered product preserves information that additive counters discard: two sequences with the same number of each event can produce different final spins when their event order differs. Train the spin axes, angles, and readout jointly with the task model while constraining every update to remain on the sphere.

Useful8/10
Difficulty5/10
Novelty8/10
Paper: Non-Abelian Spin Counting of Ordered Stochastic Trajectories: Reentrant Finite-Time Chern Numbers arXiv:2608.23533
✗ Mechanism failed 2026

SU(d) Spectral Associative Memory

Replace vector-valued Hopfield neurons by SU(d)-valued latent states and construct Hebbian couplings from matrix memories. Recall is performed by iterating toward the dominant eigenmode of the induced lifted coupling operator, with each iterate projected back onto SU(d); the larger matrix representation should reduce random crosstalk and increase critical memory capacity.

Useful8/10
Difficulty7/10
Novelty8/10
Paper: High-Capacity Generalized Hopfield Networks arXiv:2608.08226
✓✓ Beats tuned baseline 2026

Power-Balanced Modular Neural Block

Represent each neural module as a Hamiltonian storage system and connect modules through a state-dependent skew or Dirac interconnection instead of arbitrary residual additions. The coupling may change with the hidden state, but its internal power contribution cancels exactly, so total stored energy is controlled only by external inputs and explicitly added dissipation.

Useful8/10
Difficulty5/10
Novelty5/10
Paper: Port-Hamiltonian modelling of coupled rigid/flexible multibody systems arXiv:2608.05143
△ Mechanism confirmed, baseline not beaten 2026

Monotone transport-map latent space

Represent every nonnegative equal-mass one-dimensional state by its CDT quantile map relative to a fixed reference density, then train the neural dynamics model in this transformed space rather than on Eulerian grid values. The latent manifold for translations and transport-dominated evolution is substantially flatter: linear transport lies in the span of the initial transformed state and the constant function, while nonlinear conservative dynamics have algebraic approximation error bounds.

Useful8/10
Difficulty5/10
Novelty6/10
Paper: Reduced Order Modeling of One-Dimensional Conservative PDEs via the Cumulative Distribution Transform arXiv:2607.17066
△ Mechanism confirmed, baseline not beaten 2026

Hypoelliptic transport-diffusion layer

Replace an isotropic local mixing layer with a kinetic layer that smooths features in x and transports them in y along the characteristic direction x. The layer should be useful for phase-space data, learned simulators, and world models in which positions or transported quantities evolve through coupled drift and diffusion rather than independent Euclidean motion.

Useful7/10
Difficulty5/10
Novelty7/10
Paper: Boundary Harnack inequalities for Kolmogorov equations in asymptotically cylindrical Lipschitz domains arXiv:2608.29813
✗ Failed on benchmark 2026

Hyperplane-Gated Piecewise Neural Dynamics

Replace a single smooth neural vector field with a finite collection of smooth subnetworks selected by learned affine hyperplanes. The architecture exposes switching geometry directly, allowing it to represent friction-like or threshold dynamics without approximating discontinuities using excessively steep activations.

Useful7/10
Difficulty5/10
Novelty6/10
Paper: Learning piecewise-smooth dynamical systems arXiv:2608.19785
△ Mechanism confirmed, baseline not beaten 2026

Harmonic-Mode Branch for Topological Memory

Do not force Hodge dissipation onto harmonic edge modes, because these modes are precisely the obstruction to global coercivity. Split the latent state into dissipative coexact modes and a finite-dimensional harmonic branch, and use harmonic-decoupled interactions so each harmonic coordinate defines an invariant affine fibre with its own attractor.

Useful7/10
Difficulty6/10
Novelty7/10
Paper: Hodge Coercivity and Global Dynamics in Two-Field Edge-Cochain Systems with MHD-Type Cancellation arXiv:2608.19360
△ Mechanism confirmed, baseline not beaten 2026

Graded Levy-area recurrent state

Replace additive recurrent pooling with a graded state containing the current feature increment, an antisymmetric order-sensitive area matrix, and an optional symmetric quadratic-variation accumulator. Compose chunks using the paper's exact group law, allowing a sequence model to retain compressed pairwise ordering information without explicitly forming all token pairs.

Useful7/10
Difficulty5/10
Novelty7/10
Paper: Infinite-Dimensional Levy Area: Probability-Selected Critical Geometry and Sharp Spectral Selection arXiv:2608.08756
△ Mechanism confirmed, baseline not beaten 2026

Toda-Krylov adaptive polynomial layer

Replace a fixed-order polynomial or recurrent state-space block by an Arnoldi basis built from a learned operator and the current input, and use subdiagonal coefficients as geometry-aware gates over Krylov depth. The gates quantify how much genuinely new direction each operator application contributes, allowing the layer to stop early near Krylov breakdown and suppress redundant or unstable directions.

Useful7/10
Difficulty5/10
Novelty7/10
Paper: Two-dimensional Toda--Arnoldi correspondence: Holomorphic Krylov geometry and counterdiabatic transport arXiv:2608.04850
✗ Mechanism failed 2026

Volume-Threshold Contracting State Layer

Construct a recurrent or state-space layer as a skew product: an expanding bounded feature coordinate drives a linearly contracting hidden state. Constrain the hidden transition matrix A to have spectral radius below one, and monitor the predicted transition ell times the absolute determinant of A equals one: below it, hidden trajectories should occupy a thin or fractal set, while above it they should have substantially higher-dimensional state coverage without losing local contraction.

Useful7/10
Difficulty5/10
Novelty7/10
Paper: Geometric Properties of Higher Dimensional Solenoidal Attractors arXiv:2607.27089
✓✓ Beats tuned baseline 2026

Symmetry-Block Neural PDE Solver

Build an implicit or unrolled graph neural operator on a symmetric simplicial mesh, and perform every symmetry-compatible linear solve in a fixed representation-theoretic basis rather than the original edge/face basis. The same basis can be reused for Poisson, Maxwell, diffusion, and learned linear combinations of DEC operators, yielding parallel independent blocks and lower peak memory without changing the discretized solution.

Useful7/10
Difficulty6/10
Novelty6/10
Paper: Parallelisation of Discrete Exterior Calculus via Representation Theory on Curved and Three-Dimensional Meshes arXiv:2607.25192
✓✓ Beats tuned baseline 2026

Multiplicative Manifold Unscented Recurrent Cell

Replace the Euclidean hidden-state update of a recurrent or state-space neural network with a mixed manifold state containing a rotation component and Euclidean features. Propagate uncertainty with sigma points in tangent error coordinates, retract rotational perturbations through the exponential map, and compute the training loss from the predicted covariance. This avoids invalid rotations and captures second-order curvature effects that a first-order EKF-style recurrent cell misses at large…

Useful7/10
Difficulty6/10
Novelty7/10
Paper: Fully Multiplicative Attitude and Orbit Determination for Deep space Navigation arXiv:2607.10072
✗ Failed on benchmark 2026

Two-Scale Parabolic Filter Block

Construct a spatiotemporal neural block from localized functions of a learned parabolic operator instead of unrestricted attention or convolution. Use one filter for fine-scale diffusion and another for coarse-scale temporal aggregation, with the scale ratio controlling information propagation. The block should suppress distant interactions while still permitting long-range mixing through coarse filters.

Useful7/10
Difficulty6/10
Novelty6/10
Paper: $\mathrm{L}^p$ bounds for parabolic Riesz transforms with rough coefficients: The case $1<p \leq 2$ arXiv:2607.05181
✓✓ Beats tuned baseline 2026

Conformal-symplectic sandwich layer

Replace an unconstrained one-step transition network with a symmetric damping–symplectic-core–damping composition. The damping strength is one learned scalar rate and is applied through positive exponential diagonal factors, so every step has a known contraction law while the neural core models nonlinear conservative transport.

Useful7/10
Difficulty5/10
Novelty7/10
Paper: CSympNet-ID: conformal-symplectic map learning for linearly damped Hamiltonian systems arXiv:2607.03339
Unverified 2026

Symplectic Polar Transition Normalization

Normalize a learned symplectic recurrent transition using the paper's explicit positive-definite factor instead of projecting the entire matrix onto an orthogonal group. Retain the compact unitary dynamics as the stable transport component and separately damp only the noncompact factor, providing a tunable stability mechanism that preserves symplectic structure.

Useful6/10
Difficulty6/10
Novelty5/10
Paper: Maslov Indicies In Symplectic Geometry Revisited arXiv:2609.03061
Unverified 2026

Sector-Parametrized Neural Operator

Replace a recurrent, SSM, or residual linear operator W by an exact affine image of a contractive matrix sigma. The resulting W lies in a prescribed matrix ball and, for the positive-real choice of parameters, satisfies a sector inequality such as W+W^* >= 0. This gives an anisotropic, learnable alternative to plain spectral normalization: the allowable operator set is convex and its center and left/right radii can encode known directional scales.

Useful6/10
Difficulty5/10
Novelty6/10
Paper: Hyperpositive functions, sector bounded functions and a trace formula arXiv:2609.03403
Unverified 2026

Bicomplex Spatio-Temporal Residual Encoder

Replace independent per-sensor temporal encoders with a shared two-dimensional transform whose temporal and spatial phase channels remain algebraically distinguishable. Train a neural residual detector and localization head on the transformed coefficients, forcing perturbations with the same temporal signature but different positions to differ primarily in their spatial phase.

Useful6/10
Difficulty5/10
Novelty8/10
Paper: Multivariable Geometric Laplace Transform and Fault Detection in Distributed-Converter Lines arXiv:2609.02431
Unverified 2026

Normal Spectral Linear Layer

Replace an unconstrained dense transition or recurrent matrix with a normal matrix $A=U\operatorname{diag}(\lambda)U^*$, where $U$ is unitary and $\lambda$ contains learnable eigenvalues. The layer can be initialized by fitting a normal matrix to input-output pairs through the paper's objective, then trained with Riemannian updates that keep $U$ unitary and preserve the normal-operator structure.

Useful6/10
Difficulty6/10
Novelty6/10
Paper: The Normal Procrustes Problem: A Riemannian Optimization Approach arXiv:2608.19513
Unverified 2026

Integrable Elliptic Memory Cell

Replace an unconstrained recurrent transition with block-diagonal planar rotations whose angles are learned or conditioned on a slowly varying context variable. The resulting hidden-state norm and each two-dimensional block energy are exactly invariant in the ideal recurrence, preventing exploding or vanishing recurrent dynamics while retaining phase information over long horizons.

Useful6/10
Difficulty4/10
Novelty4/10
Paper: Outer Contact Billiards arXiv:2608.19393
Unverified 2026

Nielsen Quaternionic Hyperbolic Latent Layer

Represent each recurrent latent state as a pair of unit quaternions \((q_1,q_2)\in\mathrm{SU}(2)^2\), and evolve it with a composition of elementary Nielsen maps corresponding to a chosen hyperbolic matrix \(A\in\mathrm{SL}(2,\mathbb{Z})\). The layer exactly preserves the group manifold and Haar volume, preserves the commuting locus \(q_1q_2=q_2q_1\), and reproduces toral hyperbolic dynamics there, giving a structured long-horizon prior instead of an unconstrained matrix recurrence.

Useful6/10
Difficulty5/10
Novelty8/10
Paper: Quaternionic Extensions of Hyperbolic Toral Automorphisms arXiv:2608.08252
Unverified 2026

Curved-Critical Residual Lattice

Construct a 2D recurrent or residual neural lattice with slowly varying local couplings, while parameterizing those couplings so that an anisotropy invariant remains constant across all spatial and depth locations. The network obtains controlled local propagation velocities rather than arbitrary inhomogeneous amplification, enabling depth-dependent receptive fields while preserving near-critical signal propagation.

Useful6/10
Difficulty6/10
Novelty8/10
Paper: Two dimensional inhomogeneous classical systems at criticality arXiv:2608.02903
Unverified 2026

Schur-Agler contractive gated layer

Replace an unconstrained recurrent or residual transition with a block-structured contractive realization whose input-dependent multiplier is a direct sum of bounded branches. The resulting layer has a built-in non-expansive energy bound on the chosen normalized input domain, while still allowing different branches to respond to different coordinates or feature groups.

Useful6/10
Difficulty5/10
Novelty5/10
Paper: Function theory of the hexablock and applications to the tetrablock and Euclidean biball arXiv:2608.00819
Unverified 2026

Null-form quadratic wave layer

Replace an unconstrained quadratic interaction between channel derivatives with a learnable combination of Lorentzian and antisymmetric null forms. For wave-equation surrogates, this enforces exact cancellation when two interacting features have parallel null directions, suppressing resonant derivative products that otherwise cause unstable long-horizon rollouts.

Useful6/10
Difficulty5/10
Novelty7/10
Paper: Recovery of a Null Form in the Wave Equation from Scattering Data arXiv:2607.28917
Unverified 2026

Threshold-Projection Recurrent Memory

Replace or augment a recurrent cell with multiple hysteresis memory branches whose states remain unchanged while the input stays within a branch-specific radius, then move toward the current input only when that radius is exceeded. The resulting cell has explicit persistence and bounded state changes, giving it an inductive bias for temporal hysteresis and reducing the need for the network to learn long-term memory behavior from scratch.

Useful6/10
Difficulty4/10
Novelty7/10
Paper: Accounting for Hysteresis and Eddy Currents in Finite Element Simulations of Ferromagnetic Laminated Cores using a Recurrent Neural Network arXiv:2607.14321