Definition
A stratified manifold with continuous fibers is a representation space admitting a decomposition into discrete basins (each basin associated with one value of a discrete output variable, e.g. one predicted digit), such that within and across basin boundaries there exist continuous fibers — 1-dimensional curves parametrized by a separate continuous quantity (not the discrete basin index) — along which varies smoothly even as the fiber crosses from one basin into an adjacent basin . Formally, for a state with discrete label and continuous fiber coordinate , nearby points along a fixed fiber satisfy (adjacent-basin transitions only) while (up to the fiber’s own local variation) — the discrete and continuous coordinates are both locally meaningful, but at different scales: basin identity is the macroscopic/coarse coordinate, fiber position is the microscopic/fine one.
Intuition
Picture a stack of discrete plates (the basins) with several ropes running through holes drilled near each plate’s edge, so that each rope threads continuously from one plate to the next: from far away, you see only discrete, stacked plates (the coarse clustering); from close up, following any one rope, you see a spiraling continuous path that happens to pass through several plates in sequence. Neither description alone (just plates, or just one long undifferentiated rope) captures the full picture — the structure is genuinely two-scale.
Properties
- Coexistence of discrete clustering and continuous stratification is the falsifiable claim, not either alone. A purely discrete-cluster claim (e.g. Neural Collapse-style class clusters) or a purely continuous-manifold claim (e.g. 1D continuum manifold alone) would each be a simpler, weaker structure; the distinguishing content here is that the same representation exhibits both, and that the fine continuous structure is what predicts fine-grained behavioral outcomes (e.g. specific error types) that the coarse discrete structure alone cannot.
- First quantified instance in this map: digit basins stratified by carry-potential fibers in LLM arithmetic. Wen, Zhu, Huang, Li & Gao (2026) apply UMAP (cosine distance) to Qwen3-4B’s final-layer activations during multi-operand addition and find ten discrete digit basins (one per output digit 0-9, UMAP trustworthiness 0.9953 vs. 0.8633 for PCA and 0.9907 for t-SNE), each basin’s interior further organized by continuous “Iso-Raw-Sum Trajectories” (IRSTs) — fibers connecting states that share a raw positional sum across adjacent basins as the carry varies, where the Carry Potential is a continuous quantity whose fractional part indexes exact fiber position. A noisy-quantization model (, ; predicted error rate for ) fits the empirical per-position error-rate “bathtub curve” at () in Qwen3-4B, replicating at in Qwen3-8B (, 12-digit) and Gemma-3-4B-IT (, 10-digit) — states near an integer boundary of (a carry “flip point”) are quantifiably more error-prone than states well inside a basin, directly tying fiber position to a specific behavioral failure mode (93.19% of all model errors are off-by-one, i.e. exactly one basin-transition away from correct). See
wen-etal-2026-digit-basins-stratified-by-carry-potential-fibers-predict-off-by-one-arithmetic-errors-via-a-noisy-quantization-bathtub-curve. - Causally validated via contrastive-centroid steering along a fiber, with basin-boundary-dependent thresholds. A steering vector built from the difference between adjacent-basin fiber centroids, injected into the residual stream, flips the model’s predicted digit at a magnitude that depends on the target state’s fiber position: states already near the noisy-quantization boundary (small or near 1) flip at much smaller (e.g. for a near-boundary “hallucination” state) than states deep inside a basin (e.g. for a stable interior state) — the causal manipulability of the representation varies continuously with fiber position, not just with basin identity.
- Relation to prior helical/circular arithmetic-geometry claims: an explicit refinement, not an independent alternative. The paper positions its stratified-fiber structure as refining Kantamneni & Tegmark’s generalized-helix hypothesis and Nanda et al.’s original circular/rotational modular-arithmetic geometry: rather than a smooth rotational manifold where errors would be uniform around a loop, the digit basins here do not wrap circularly (0 and 9 are not adjacent, unlike a clock face), and the specific off-by-one error pattern is explained by local carry-fiber slippage near quantization boundaries rather than by global rotational dynamics — a different, more locally-grounded mechanistic account of a structurally related phenomenon (multi-digit arithmetic geometry), evaluated with entirely different tools (UMAP-based basin/fiber decomposition and a probabilistic quantization-noise model, versus Fourier-period helix fitting and activation patching).
Exercises
Base
- Why does a purely discrete-cluster description (just “ten digit basins, one per output digit”) fail to explain why errors are overwhelmingly off-by-one (93.19%) rather than uniformly spread across all possible wrong digits?
Solution
A purely discrete-cluster description has no notion of “distance” or “adjacency” beyond same-cluster/different-cluster — it cannot in principle predict that errors land preferentially in neighboring basins rather than arbitrary ones, since it discards exactly the continuous fiber coordinate that tracks how close a given state is to a specific neighboring basin’s boundary. The off-by-one pattern requires the continuous stratification (fiber position relative to a quantization boundary) to explain which neighbor an error lands in and why nearby-boundary states are disproportionately affected.
- The bathtub-curve model predicts error probability rises near and (both quantization boundaries) and is lowest near (basin interior). Explain this shape in terms of the noisy-quantization model .
Solution
The floor function only differs from the true when the noise is large enough to push across an integer boundary. If is close to an integer ( near 0 or 1), only a small noise perturbation is needed to cross that boundary, so the error probability (governed by the Gaussian tail, the -function) is high; if is near the middle of its interval (), a much larger noise perturbation is required to reach either neighboring integer, so the error probability is low — producing the characteristic “bathtub” shape (high at both edges of , low in the middle) as a direct consequence of the model’s Gaussian-noise assumption.
Middle
- The paper reports that boundary states (“hallucination,” ) flip under steering at , while a deep-basin state () requires . Using the fiber-coordinate framework, explain why this is expected rather than an unrelated finding.
Solution
has , very close to the upper quantization boundary (, where the floor jumps from 1 to 2) — the state is already almost at the basin transition, so only a small steering push in the direction that increases past the boundary is needed to flip the discrete output. has , comfortably inside its basin’s interior — a much larger push is needed to cross either boundary. This mirrors the bathtub-curve logic applied to causal intervention rather than naturally occurring noise: proximity to a boundary in the continuous fiber coordinate predicts ease of flipping under an external perturbation, just as it predicts susceptibility to naturally-occurring representational noise.