Source

  • Entezari, Sedghi, Saukh & Neyshabur (2022), LIT-652, read in NOTE-537: Conjecture 1, Theorem 3.1, §2 (Figs. 2–3) and §4.
  • Ainsworth, Hayase & Srinivasa (2023), Git Re-Basin, LIT-661, read in NOTE-532: §§3, 5.1, 5.3, Figs. 2 and 4, and Appendix A.6.
  • Ferbach, Goujaud, Gidel & Dieuleveut (2024), LIT-680, read in NOTE-543: Theorems 3.1 and 5.2–5.4, Lemma B.3 and §6.
  • Theus, Cabodi, Anagnostidis, Orvieto, Singh & Boeva (2025), LIT-664, read in NOTE-540: §§3–4, Table 2, Figs. 5 and 7.
  • Bo Zhao, Dehmamy, Walters & Yu (2025), LIT-655, read in NOTE-528: Propositions 4.1, 5.2–5.4 and §5.2.

The claim, assembled

The conjecture. Entezari et al., LIT-652, conjecture that for wide enough networks most SGD solutions can each be permuted so that the straight line between any two has about zero barrier: one basin, seen through different labellings of the hidden units (Conjecture 1). Their own evidence is indirect. Across width, depth, architecture and dataset, in more than 3,000 networks, barriers between independent solutions look like barriers between random permutations of one solution. Their simulated-annealing search lowered barriers only for shallow networks on easy data, and did nothing for VGG or ResNet (§4).

Removing the permutation removes the barrier, where the network is wide. Git Re-Basin, LIT-661, aligns one network’s units to another’s by weight matching. That is coordinate descent over per-layer assignment problems, it needs no data, and it runs in seconds. After alignment, MNIST MLPs show zero barrier, and so do ResNet-20s on CIFAR-10 at 32× width. That was the first zero-barrier connection between independently trained ResNets (Figs. 2 and 4). The authors’ conclusion is that permutations are “a necessary piece, though not a complete picture” (§5.3). Ferbach et al., LIT-680, prove the conjecture beyond Entezari et al.’s random one-hidden-layer case. Aligning a layer’s neurons is optimal transport between the empirical distributions of their weights (Lemma B.3). So when neurons are independent draws, Wasserstein convergence bounds how wide a layer must be for the permuted line to stay low-loss. That gives connectivity for wide two-layer networks trained by mean-field SGD (Theorem 3.1) and for deep networks with i.i.d. neuron weights (Theorem 5.2).

The group is the architecture’s full one. Permutations are the symmetries of an elementwise nonlinearity. Bo Zhao et al., LIT-655, place them inside a larger group. For a full-rank linear network the minimum is homeomorphic to GL_h(ℝ)^{l−1} and has 2^{l−1} components (Proposition 4.1). A permutation with negative determinant joins components that continuous symmetries cannot, so for h ≥ 2 permutations connect them all (Proposition 5.2). Theus et al., LIT-664, carry this to transformers. Feed-forward units take permutations. Attention heads take a semi-permutation. The residual stream, once LayerNorm is rewritten as RMSNorm, takes one orthogonal map. Their test-loss barriers (Table 2) are 1.69–4.34 with no alignment. Learned matching restricted to permutations leaves 0.29–1.60, which already removes 63–90% of the vanilla barrier. The full group brings it to 0.00 on CIFAR-10, CIFAR-100 and Tiny ImageNet, 0.02 on Tiny Shakespeare and 0.42 on BookCorpus. The data-free version leaves 0.34–1.56. What permutations leave is in the rotation: learned matching keeps weight matching’s permutations and corrects the orthogonal map (Fig. 5), and iterating orthogonal matching keeps lowering the barrier while iterating permutation matching does not (Fig. 7). On a transformer, then, permutations alone already remove most of the barrier, and the orthogonal map on the residual stream is what removes the rest. This is narrower than “most of a transformer’s barrier is a rotation”, which Table 2 does not show.

Width and depth. This clause was filed as a candidate theory of its own and is folded in here, because it is a statement about how much alignment can remove. Stated on its own, “width lowers barriers and depth raises them”, it is false for curved paths. Draxler et al., LIT-653, find barriers on their minimum-energy paths falling as networks get “wider and especially deeper” (Fig. 5). Garipov et al., LIT-673, also find width easing curved connection (A.7). On straight lines after alignment the width half holds, and is in the title. The depth half is only suggested, and is QUESTION-317’s:

  • Width lowers it. Git Re-Basin’s barrier after weight matching falls with width for VGG-16 and ResNet-20 on CIFAR-10, to zero at large width; at 1× neither is linearly connected (Fig. 4). Ferbach et al.’s bounds are bounds on width. Before any alignment, Entezari et al.’s barrier first rises with width, peaking near the width that just fits the training data, then falls (Fig. 2). For VGG and ResNet it stays saturated high at every width they tried.
  • Depth raises it. With width fixed, adding layers raises the unaligned barrier quickly for MLPs and shallow CNNs. VGG(11–19) and ResNet(18–50) saturate high, and depth, not width, is what the authors blame (Entezari et al., Fig. 3). The examples they give of zero barrier after their search are MNIST MLPs of depth 1 at every width and of depths 2 and 4 at width 2¹⁰ (Fig. 7), which is suggestive and no more. In Ferbach et al. the width that layer ℓ needs is Õ((T_ℓ/ε)^{m̃_{ℓ−1}}), exponential in the width before it, so the requirement compounds with depth. Their lower bound shows this rate is tight for independent neurons (Theorem 5.3). It falls if weights concentrate near a low-dimensional subspace (Theorem 5.4).

Where it stops

  • Thin models and ImageNet. At 1× width neither VGG-16 nor ResNet-20 is linearly connected after weight matching, and on ImageNet ResNet-50 the barrier falls by 67% but not to zero (Git Re-Basin, §§5.1, 5.3). The authors cannot rule out a better permutation.
  • Barriers that are disagreement. Lubana et al., LIT-669, train models that do and do not rely on a synthetic cue. They are joined by quadratic paths but keep a linear barrier after activation-matching permutation, because they compute different things. For a one-hidden-layer ReLU network they prove that linear connectivity forces shared activation patterns. Their endpoints are trained on different data, so they are not the same-data seeds this account is about. But they show that a barrier surviving alignment can be real, which is why the title says what alignment removed in each network measured, and not that a residual barrier is symmetry.
  • Solutions training reaches. Git Re-Basin constructs two perfect solutions of a two-hidden-layer, two-unit network that no permutation connects (Appendix A.6). Bo Zhao et al. use rescaling to construct minima in one component whose straight-line barrier is unbounded, even under a last-layer permutation (Propositions 5.3–5.4). Neither is a minimum SGD is shown to find, and both papers say so. As in THEORY-109, the claim is about found solutions.
  • Learned alignment optimises what it reports. Theus et al.’s zero barriers come from alignment trained against the loss at the path’s midpoint, on training data, and measured on test data. A zero from data-free alignment would be stronger evidence of a pre-existing shared basin.
  • Small models. The transformers are 6- to 8-layer ViTs at 44–84% accuracy and 6-layer GPT-2s.

What this does not say

  • It does not say permutation is the whole story anywhere. For transformers the orthogonal map is needed to reach zero. For thin convnets nothing found reaches zero.
  • It does not say a barrier is always symmetry. Lubana et al.’s barriers are mechanism. The claim is about same-data solutions, and only what alignment removed where it was measured.
  • It does not say alignment works at initialization. That is THEORY-114: at practical widths the aligned barrier is high at the start of training and falls during it.

Connections

  • THEORY-109. This account extends it. That account says the solutions training finds lie in one connected set joined by curves. This one says that, once symmetry is factored out, the set is nearly convex: the curve straightens. Git Re-Basin reads the pair the same way, crediting Benton et al. (LIT-656) with the connected volume and Entezari et al. with conjecturing it convex modulo permutation.
  • THEORY-110 keeps the quotient by symmetry and weakens convex to star-shaped, which reaches below the widths at which this account holds.
  • THEORY-114 is its time axis.
  • Across the boundary. The anthology’s ANTH-THEORY-010 holds that most of the barrier between two independently trained networks is permutation, not disagreement. It is Proposed there and names “the account demonstrated on a transformer” as one condition for promotion. This account agrees with it for MLPs and CNNs. For transformers, Theus et al. bear it out in its letter, since permutations alone remove 63–90% of the barrier. They also show that reaching zero needs a symmetry that is not a permutation. Lubana et al.’s mechanism barriers name the case its account leaves out. This is for the coordinator to report there; the anthology is not edited from here.