Contribution

It picks a model small enough that singular learning theory can be carried out exactly, derives the local learning coefficients of its critical points by hand, uses the free energy formula to predict where the Bayesian posterior jumps, checks the prediction by MCMC — and then, separately, watches SGD and asks whether the same jumps appear. The answer is partly. That “partly” is the paper.

Key insight

Occam’s razor is not a prior somebody chose; it falls out of the free energy, and it is a function of how much data you have. With F_n ≈ min_α [n L_n(w*_α) + λ_α log n + c_α], at small n the complexity term dominates and the posterior prefers a simple, badly-fitting solution; at large n the loss term dominates and it will pay complexity for fit. Learning, in the Bayesian picture, is a sequence of such swaps.

The corollary is the caution. That sequence is indexed by sample size. A training curve is indexed by step. These are different orderings over different objects, and the paper is the first thing in this record to say so and then measure both.

Assumptions

  • The Toy Model of Superposition (Elhage et al.) with r = 2 hidden dimensions, in the high-sparsity limit. Tiny, deliberately.
  • The k-gon classification is not claimed exhaustive: “we do not claim to have found all possible critical points of the TMS”.
  • The free energy formula absorbs the volume constant and log log n terms into a constant c_α treated as effectively constant — the paper notes the constants “can play a nontrivial role” at low n.
  • λ̂ estimates are used where theoretical values are unavailable, with caveats the paper localizes to an appendix.
  • MCMC classification “becomes increasingly uncertain” below n = 400, and MCMC fails outright for n much above the reported range.

Key results

  • k-gons are critical points, proved for r = 2; standard k-gons for k ∈ {5,6,7,8} with k < c are minimally singular, and the k = c case is non-degenerate. Exact local learning coefficients are derived for the ones MCMC actually visits.
  • The local free energy formula. F_n(W_α) = n L_n(w*_α) + λ_α log n − (m_α − 1) log log n + O_p(1). A Bayesian phase transition α → β occurs when F_n(W_β) − F_n(W_α) changes sign.
  • A number, predicted and then observed. The 5 → 6 transition is predicted at n_cr ≈ 600 and appears in the MCMC phase proportions at 600 ≤ n ≤ 700. Holds when: n ≳ 400, below which the classification is unreliable and the paper says not to read the correspondence.
  • The same critical points explain SGD plateaus, which the paper argues is not a coincidence: SLT associates posterior phases with singularities of the KL divergence, and nonlinear dynamics associates trajectory behaviour with singularities of a potential.
  • And the negative result. “There is no necessary relation between these two kinds of transitions.” The 5 → 6 Bayesian transition has not been observed as a dynamical transition — possibly because the regions are distant or separated by high energy barriers, possibly because it occurs with low probability per step.
  • The Bayesian Antecedent Hypothesis (BAH). Dynamical transitions encountered in training have Bayesian antecedents. Its obstruction is that a Bayesian transition requires λ to increase. The paper’s analysis finds antecedents for the dynamical transitions it observed, with two cases where the analysis is inconclusive.

Limitations

Two hidden dimensions. This is the price of being able to derive anything. Nothing here transfers by argument; what transfers is the distinction and the demonstration that the two kinds of transition can come apart.

The BAH is a conjecture and is labelled one. It is the bridge from a well-defined theory to the phenomena people care about, and it is the least supported thing in the paper.

The constants matter where the data is thin. The c_α term is treated as constant and the paper notes it is not, at exactly the small-n end where Bayesian transitions are densest.

Bearing on the record

Every grokking mechanism this record holds is dynamical. THEORY-072 (a walk down the weight norm), THEORY-071 (norm moving between circuits) and THEORY-070 (leaving the lazy regime) are all claims about a trajectory, all Proposed, and none is general. Everything singular learning theory proves is about a posterior indexed by sample size. This paper is where the gap between those two things is named, and the record needed that before it could hold both literatures without conflating them.

It also bears on SOTA-200. A capability that appears suddenly at some scale is a claim about n, which is the Bayesian axis; a capability that appears suddenly during training is a claim about t. The practice’s third check now says “move the regime and see whether the discontinuity moves”, and n is one of the regimes — with, in this model, a predicted crossing point.

Open questions

  • Is the BAH true? Nothing outside this paper tests it, and two of its own cases are inconclusive.
  • Does a Bayesian transition with no dynamical counterpart mean anything for a practitioner? The 5 → 6 case is the most striking result here and the record cannot say what to do with it.