Source

Picozzi (2026), LIT-936, read in NOTE-755: Part I (Eq. 1, Theorem 2, Lemma 2, Propositions 1 and 3), Part II (agreement measurements, Theorems 6 and 8, Remark 2, SN18, SN19) and the synthetic language assignment (SN3.1).

What was actually shown

Identification, by construction. For a battery of contexts, the relational geometry is the matrix d_ij = 2 arccos Σ_a √(p_i(a) p_j(a)) of Fisher–Rao distances between next-token laws. It is a function of the laws, so it is unchanged by any reparameterization that leaves outputs unchanged (Lemma 2(a), “immediate”). Activation geometry is not: for every A ∈ GL(d), (g ∘ A⁻¹) ∘ (A h) has the same outputs and a different Gram matrix (Prop. 1). Two models with identical outputs can have hidden relational geometries whose rank agreement is −4/17 (Prop. 3), so output agreement puts no floor under activation agreement. Random anisotropic reparameterizations leave output agreement constant to machine precision while activation CKA, mutual k-NN and cosine RSA degrade.

Sharing, proved only through the laws. On a shared outcome space, E{d_A − d_B}² ≤ 4(ε_A + ε_B) for root-probability distances, where ε is each model’s excess risk to a common law (Thm 6), and rank agreement tends to 1 as the risks vanish (Thm 8). On real models the worst-case form is “vacuous” (Remark 2). The measured stability is explained instead by low coherence: the directions in which models disagree are nearly orthogonal to the relational structure (median coherence 0.024–0.034).

Measured agreement. Over ten models from 70M to 7B parameters, seven training pipelines and four tokenizers, the mean Spearman agreement of output distance matrices is 0.88 on natural text, against 0.62 for mid-layer and 0.61 for last-layer activation geometry, with a bootstrap interval on the gap excluding zero. At the first byte, cross-tokenizer agreement is 0.91.

What exceeds the laws (SN18). The top-six cross-family eigenvector overlap is 0.698. A null matched in displacement magnitude, which follows from the shared output laws alone, gives 0.636. The residual, +0.063 (+0.056 to +0.070), is “about 9% of the raw overlap”.

The law decides, in synthetic languages (SN3.1). Three architectures at two capacities trained on eight pairs of synthetic languages: the assigned law recovers 0.998 of the imposed separation, and changing architecture within a law leaves the geometry nearly unchanged.

What could have failed: architectures fitted to one corpus could have disagreed in output geometry as much as they do in activations. They did not.

What this does not say

  • Not a signature identified beyond the probes. The geometry is identified because it is a function of the observed laws, the in-probe case QUESTION-027 calls automatic. The two results that reach past the battery, a 40-anchor probe transferred between models (0.659 against 0.724 within model, chance 0.125) and a risk-to-human-alignment relation applied to unseen families (r = 0.758), are empirical and narrow.
  • Not that the models share something beyond their behaviour. Only about 9% of the eigenvector overlap does, and it is graded by training lineage. The paper does not separate law from corpus on natural text.
  • Not that the bounds explain the agreement. Theorems 6 and 8 are vacuous on real models. The explanation offered, low coherence, is a measurement, and the paper says a pair disagreeing along relational directions “could agree far less at the same per-context excess risk”.
  • Not that the shared geometry is semantic. Its alignment with a Sentence-BERT geometry is 0.044 on natural text.
  • Not across tokenizers in the native vocabulary. Convergence is proved on a shared outcome space; native cross-tokenizer agreement is measured only.
  • Not the steering, editing and fine-tuning results. Most of the paper uses the pullback Fisher metric for interventions. That is machine-learning practice and belongs in the anthology.

Connections

  • THEORY-002. A measured form of the Platonic hypothesis recast in output geometry, where convergence follows from predictive fit. It fits THEORY-002’s reading that what converges is fixed only up to the symmetry of what is observed: here what is observed is the law, and the geometry is a function of it.
  • CLAIM-148. Propositions 1 and 3 restate its point for networks: the GL(d) gauge of a hidden layer is not a symmetry of anything observable.
  • CLAIM-142 and CLAIM-193. Agreement on the battery holds because disagreement falls in directions the battery’s relational structure does not see, a measured instance of agreement relative to probes.
  • THEORY-175. Distances to matched anchors transfer between models with loss, here with Fisher–Rao distances on outputs instead of cosines on activations. Transfer goes through the consensus; the model-specific residual transfers at 0.091, below chance.
  • QUESTION-052. The output Fisher’s leading eigenspace is where cross-model sharing concentrates. It is the eigenspace of a per-context covariance operator, not of the pair operator the question defines.
  • QUESTION-027 and CLAIM-209. Evidence for the unrestricted form only.

Note of 2026-10-20: the identification, re-derived

For the promotion audit (batch 049). The relational geometry is d_ij = 2 arccos Σ_a √(p_i(a) p_j(a)) over the battery, a function of the next-token laws p_i alone. Any reparameterization that leaves every output unchanged leaves every p_i, and so d, unchanged; two models with identical laws on the battery have the same matrix. For the hidden layer, take an invertible A and replace the hidden state h by Ah and the readout g by g ∘ A⁻¹. Every output is unchanged, and the Gram matrix becomes hᵢᵀAᵀAhⱼ, which differs from hᵢᵀhⱼ unless A is orthogonal (Prop. 1). The measured numbers are as NOTE-755 reports them from the text and SN18. The residual +0.063 is 0.063 / 0.698 ≈ 9% of the raw overlap.