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Scaling Collapse Reveals Universal Dynamics in Compute-Optimally Trained Neural Networks

Qiu et al. show that compute-optimally trained neural networks exhibit a striking scaling symmetry: loss curves from models of different sizes collapse onto a single universal curve after normalizing compute and reducible loss to unity at the end of training. With learning-rate decay, the collapse becomes so tight that cross-scale deviations fall below the noise floor of individual runs across random seeds — a phenomenon the authors term supercollapse. The paper provides both an empirical demonstration (transformers on CIFAR-5M and Lichess next-move, plus MLPs on power-law Fourier features) and a theoretical explanation grounded in power-law scaling laws and a simple noisy-quadratic SGD model. Supercollapse serves as a sensitive diagnostic: mis-parameterization (dropping µP for constant LR across widths) or a wrong compute-optimal data exponent both break the collapse well before final loss differences are visible.

  • Under compute-optimal training with µP, affinely rescaling loss curves as L~=(LL)/(Lfinal(N,ζ)L)\tilde{L} = (L - L_\infty)/(L_{\text{final}}(N,\zeta) - L_\infty) against normalized compute τ=t/T(N)\tau = t/T^*(N) collapses curves across model sizes onto one universal shape [§2.3, Fig. 1].
  • Under LR decay, the collapse deviation Δ\Delta drops below the per-model seed-to-seed noise floor σ\sigma for a substantial fraction of training — supercollapse — reaching Δσ/2.5\Delta \le \sigma/2.5 [§2.5, Fig. 1].
  • Normalizing by the stochastic final loss (not the expected final loss) is essential for supercollapse: it acts as a control-variate that exploits the strong time-correlation of noise along a single trajectory, cancelling shared noise and sharply reducing variance in the collapsed curve [§3.3].
  • For a family of expected loss curves L(t,N)=A/Nα+B/tβ+LL(t,N) = A/N^\alpha + B/t^\beta + L_\infty, compute-optimal scaling tNα/βt \propto N^{\alpha/\beta} balances the two power-law terms in the derivative and the terms themselves, yielding an exact collapse; this equivalence is unique up to a multiplicative constant [§3.1, Eq. 7].
  • A simple noisy-quadratic SGD model predicts full loss curves across LR schedules via a two-term formula involving the schedule integral and the preconditioned gradient covariance trace trΣ\text{tr}\,\Sigma; a single fitted constant cc reproduces empirical curves across model sizes, schedules, and training horizons [§3.2, Eq. 16, Fig. 6].
  • The preconditioned gradient covariance trace under µP appears schedule-dependent but weakly model-size-dependent, verified empirically on regression and next-token prediction — this is the ingredient that transfers constant-LR collapse to arbitrary decay schedules [§3.2.3, Eq. 17, Fig. 7].
  • Supercollapse variance-reduction magnitude scales with the incremental optimization noise between time tt and the end of training, not the cumulative noise; LR decay directly suppresses this incremental term, quantitatively matching the noisy-quadratic prediction [§3.3, Eq. 24, Fig. 8].
  • Replacing µP with a constant LR across widths breaks collapse even at small scales where final losses look indistinguishable, so collapse is a more sensitive probe of proper scaling than final loss alone [§2.6, Fig. 4 top].
  • When the data exponent ζ\zeta deviates from the compute-optimal value, larger models make faster early relative progress and decelerate later, producing a systematic downward shift of the normalized curve — offering a novel way to tune ζ\zeta by maximizing collapse quality rather than fitting Pareto-frontier points [§2.6, Fig. 4 bottom].

The setup is a scaling ladder of models trained compute-optimally: for each task (transformer next-token prediction on CIFAR-5M and Lichess; 7-layer MLPs on power-law Fourier features), the authors estimate T(N)=kNα/βT^*(N) = kN^{\alpha/\beta} from the constant-LR Pareto frontier and reuse it as the horizon under other LR schedules. Losses are affine-rescaled by subtracting the fitted irreducible loss LL_\infty and dividing by the per-seed final reducible loss Lfinal(N,ζ)LL_{\text{final}}(N,\zeta) - L_\infty, then plotted against training fraction. Collapse quality is quantified by Δ(τ)2=VarN,ζ[L~]/EN,ζ[L~]2\Delta(\tau)^2 = \text{Var}_{N,\zeta}[\tilde{L}]/\text{E}_{N,\zeta}[\tilde{L}]^2 and compared against the per-model noise floor σ(τ)2=EN[Varζ[L~]/Eζ[L~]2]\sigma(\tau)^2 = \text{E}_N[\text{Var}_\zeta[\tilde{L}]/\text{E}_\zeta[\tilde{L}]^2].

Theoretically, the paper first proves collapse for sum-of-power-law loss laws under compute-optimal token allocation, then extends via a noisy-quadratic SGD/gradient-flow model that predicts the expected loss as forcing_function + Σ EMA_i(η·tr Σ) — where the forcing function is schedule-independent and the excess loss is a schedule-dependent EMA of gradient noise. Under an approximation where trΣ\text{tr}\,\Sigma tracks the loss itself with weak N-dependence (verified empirically), the paper derives Eq. 16 which predicts target losses from a reference constant-LR trajectory using a single fit parameter. The same model then gives the variance-reduction formula Eq. 24 that explains supercollapse quantitatively.

  • On CIFAR-5M transformers (~10M–80M params), Lichess transformers, and Fourier MLPs, collapse deviation quickly saturates at Δσ\Delta \approx \sigma under constant LR and drops well below σ\sigma once LR decay is turned on [Fig. 1, Fig. 3].
  • The Eq. 16 predictor with a single fitted cc reproduces empirical loss curves across three schedules and multiple model widths on CIFAR-5M; larger MLP experiments give even sharper agreement [Fig. 6, App. I].
  • Constant-LR loss curves are well fit by L(t,N)=A/Nα+B/tβ+LL(t,N) = A/N^\alpha + B/t^\beta + L_\infty on CIFAR-5M with the fitted exponents that also yield the best power-law Pareto frontier; deviating from the optimal data exponent breaks both the fit and collapse simultaneously [Fig. 5, Fig. 4 bottom].
  • Under µP, collapse holds; under a constant LR across widths (mis-scaling), collapse fails even at small scales — the paper positions this as a precise scaling diagnostic strictly stronger than comparing final losses [Fig. 4 top].
  • Depth scaling (rather than width) produces similar collapse [App. B], supporting the conjecture that collapse persists under joint width/depth/batch/weight-decay scaling ladders — the setup Scaling with Collapse: Efficient and Predictable Training of LLM Families later tests at LLM scale.

This is the paper that puts whole training-loss-curve prediction on the wiki. Everything filed so far under Hyperparameter scaling laws has been about picking scalars — η(N,D)\eta^*(N,D), τ\tau^*, TPP — from a scaling law. Qiu et al. show that under proper compute-optimal scaling, the loss trajectory itself is universal, and that supercollapse can identify mis-parameterization earlier and more sensitively than final-loss comparisons — a diagnostic sharper than any of the point-scalar tools currently on the page. The noisy-quadratic derivation shares DNA with the SDE reparameterization line in The Design Space of Tri-Modal Masked Diffusion Models and directly complements Universal One-third Time Scaling in Learning Peaked Distributions‘s “the slope is structural” thesis: both argue key training-dynamics quantities are set by a small number of coarse controls (softmax/CE for the slope; power-law compute-optimality + LR schedule for the whole curve shape) rather than by details of architecture or optimizer.