Beyond Diagonal State Space Models: Exact Non-Abelian Group Tracking, Solvability Barriers, and Geometric Physical Manifolds
Organizations: School of Biomedical Engineering and Technology, Tianjin Medical University, Medical School, Tianjin University · School of Biomedical Engineering and Technology, Tianjin Medical University · Medical School, Tianjin University
Abstract
Selective state space models (SSMs), such as Mamba, S4D, and LRU, are bounded by transition matrix commutativity (A_t A_t' = A_t' A_t) and solvable affine transformation groups (Aff_D of derived length <= 2). Consequently, stacked multi-layer diagonal networks face severe optimization degradation on non-solvable simple groups such as A_5 due to the exponential circuit emulation depth required to simulate non-abelian commutators. We propose Non-Commutative State Space Models (NC-SSM), their real-orthogonal counterpart SO(3)-SSM, and arbitrary-dimension Cayley-SSM, lifting state transitions to compact Lie groups SU(2), SO(3), and SO(N). Via closed-form Euler-Rodrigues maps and rational Cayley transforms, NC-SSM achieves exact norm-preserving isometry (||U_t|| = 1). We introduce pure Hopf-fibration Bloch projective readouts (S^3/{+-1} =~ S^2 =~ SO(3)) to eliminate sign ambiguity, true quaternion parallel prefix scans (9.06x speedup at T=2048), and Identity-Gated Lie SSMs to eliminate sparse syntax phase drift. Extensive benchmarks across 14 experimental regimes show: (1) NC-SSM achieves 100% tracking on S_3, D_4, Q_8 and simple group A_5, where a 3-layer deep diagonal baseline collapses to 6.60% (p = 8.81e-4); (2) Cayley-SO(5)-SSM breaks Klein's 1884 ceiling on symmetric group S_5 (50.92% vs diagonal 5.25%, p = 0.0015, delivering 7.8x variance reduction over SO(3)); (3) SO(3)-SSM preserves Riemannian manifolds across 300 steps (< 3.12e-6 drift, > 580,000x advantage), achieving 0.04 deg dead-reckoning error and active tangent denoising; (4) NC-SSM achieves 74.36% on Dyck-2 and 30.26% on deep AST scope tracking (p = 0.0081); and (5) ablation confirms strict isometry is mathematically necessary for lossless long-range associative memory.
Figures & tables
| Task / Benchmark | Metric | Baseline-SSM | Ablated / Alt | NC-SSM / SO(3) / Cayley / SE(3) | Statistical Test |
|---|---|---|---|---|---|
| Tracking ( ) | Acc (%) | ||||
| Tracking ( ) | Acc (%) | ||||
| Pure Bloch ( ) | Acc (%) | Exact Quotient Invariance | |||
| Simple Group ( ) | Acc (%) | ||||
| Full-Affine ( ) | Acc (%) | (prefix) | Solvability barrier collapse | ||
| Deep-3Layer ( ) | Acc (%) | (final) |
| Group Type | Group | Commutative-Diag | Full-Affine-Diag | Deep-Affine-Diag | NC-SSM ( ) | Cayley-SO5-SSM |
|---|---|---|---|---|---|---|
| Solvable | (order 6) | |||||
| (order 8) | ||||||
| (order 8) | ||||||
| Non-Solvable | (order 60) | |||||
| (order 120) |
State Space Models
State space models represent sequences through evolving latent states, enabling efficient temporal modeling, system identification, and forecasting.
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