Contribution

The paper makes an ablation in which the activation function is the only part of a network that singles out a basis. Encoder, decoder and hidden maps are affine, initialised by rotation-invariant Xavier-normal weights and zero biases, and trained by momentum SGD on mean-squared reconstruction, all of which commute with rotations. Changing the activation from an elementwise form to a radial one switches basis-aligned clustering of the latent representations on and off. It also introduces a visualisation, the privileged-plane projective (PPP) method, to see that clustering.

Key insight

An elementwise nonlinearity is equivariant only to a finite group, the signed permutations B_n for tanh and the permutations S_n for Leaky-ReLU. It gives the representation space a frame, and training moves representations toward the frame’s directions, even upstream of the nonlinearity. An O(n)-equivariant nonlinearity must be radial, f(x) = h(‖x‖)x̂, and gives no frame. So the axis-aligned, near-discrete structure seen in such networks is put there by the primitive, not found in the data.

Assumptions

  • Setting. Autoencoders on CIFAR-10 (3,072-d) or MNIST (784-d):
    • an affine encoder to width n ∈ {12, 18, 24, 32};
    • L ∈ {0, 1, 2, 3} hidden blocks, each an activation then an n → n affine map;
    • an activation and an affine decoder.
  • Training. Batch 24, momentum 0.9, learning rate 0.08, MSE loss, float64, 125 epochs. Xavier-normal weights, zero biases.
  • Inputs. Main-text results use raw [0, 1] pixels. Appendix results standardise each pixel over the training set.
  • The activation pairs.
    • Elementwise tanh, Σᵢ tanh(x·êᵢ)êᵢ, B_n-equivariant, against isotropic tanh, tanh(‖x‖)x̂, O(n)-equivariant. The two agree on the basis directions.
    • Elementwise Leaky-ReLU (α = 10⁻²), S_n-equivariant, against an isotropic Leaky-ReLU, αx inside the ball ‖x‖ < ε = 1 and outside it printed as x − (1 − α)ε. That is dimensionally a vector minus a scalar, presumably x − (1 − α)εx̂.
    • Two B_n Leaky-ReLUs: an elementwise one with a dead zone (Eq. 9) and a max-norm one (Eq. 10).
  • The measurement. For a chosen basis, all pairs of basis vectors span planes. A representation is plotted in a plane if ‖v_∥‖/‖v‖ > ε = 0.75. Densities are summed over all planes. The basis measured is the standard one unless stated.
  • The latent layer studied is usually layer 0, after the encoder and before any activation.

Key results

  • Tanh, raw CIFAR, width 18 (Fig. 1).
    • Over 125 epochs the five elementwise-tanh networks form “distinct, highly dense, approximately discrete” beams along (horizontal and vertical) or against (diagonal) the basis directions.
    • The five isotropic-tanh networks stay “circularly symmetric, continuous”, becoming less clustered with training.
    • The only number given: about 2,000 representations pass the PPP threshold early in training and in all isotropic networks, against about 200,000 late in anisotropic training, two orders of magnitude.
  • Deeper networks (Fig. 2, three hidden blocks).
    • Anisotropic beams drift and merge onto the axes during training.
    • Isotropic networks form some clusters, but not along the basis (rows 6, 8 and 9). The author reads these as task-driven.
  • Leaky-ReLU (Fig. 3, Figs. 18–21). The same contrast holds.
    • Elementwise Leaky-ReLU at layer 0 “always” gives two antipodal beams on one diagonal, the ±1 direction.
    • The author ties this to S_n lacking sign flips. Only the orthant of 1 is mapped by the identity, and its share of the domain is 2⁻ⁿ.
  • Hyperoctahedral Leaky-ReLU (Figs. 22–27). Basis-aligned beams like hyperoctahedral tanh’s, and unlike S_n Leaky-ReLU’s. This is the paper’s best evidence that the group, not the function’s other properties, predicts the arrangement. Fig. 25 is the cleanest instance.
  • Width (Figs. 8–10). With width, isotropic densities thin out, as a spread distribution over a growing sphere should. Anisotropic ones concentrate more about the axes. At width 12 some anisotropic networks instead avoid the axes.
  • Later layers (App. B.3). Anisotropic structure usually sharpens with layer and isotropic structure smooths, with exceptions (Fig. 17).
  • MNIST (App. B.5). Same contrast, fainter (Figs. 28–30).
  • Controls on the method (App. A).
    • PPP of Gaussian samples with random orthogonal bases shows small spurious over- and under-densities along the basis, because planes overlap there.
    • Uniform [0, 1] data under a random linear map gives spurious antipodal clusters. Per-pixel standardisation removes most of it.
    • Neither artefact produces the late-training beams, and both apply to the two arms alike.
  • First-order mechanism (App. C.2). One step on a single affine layer moves the pre-activation by Δz = −η(‖x‖² + 1)J_fᵀg.
    • Elementwise: J_f = diag(ψ′), so the step is ψ′ ⊙ g, each component rescaled separately according to the orthant.
    • Radial: J_f = (ϕ′(r) − ϕ(r)/r)x̂x̂ᵀ + (ϕ(r)/r)I, so the step is a multiple of g plus a radial term, the same in every direction.
    • The author offers this as a description of how symmetry enters, not a derivation of beams.
  • “Affine divergence” (App. C.2.1). The factor (‖x‖² + 1) makes the realised step on z differ from −η∂L/∂z per sample. The author proposes z = (Wx + b)/√(1 + ‖x‖²) as a correction. Speculative and untested.
  • Reconstruction (App. D). With standardised inputs, isotropic networks reach lower test error than elementwise ones in every tanh configuration shown (Fig. 31), and in all Leaky-ReLU cases (Fig. 36). Without standardisation the result is mixed (Figs. 32–33). Five seeds each. The author calls this preliminary.

Claims

idclaimstrengthsupport
C1In these autoencoders, elementwise activations produce basis-aligned near-discrete latent clusters that radial ones do notmoderatepaired ablations, five seeds each, many widths, depths, layers and two datasets; visual only, one threshold count
C2The effect reaches layers that no activation precedesmoderatelayer-0 measurements throughout
C3The arrangement follows the activation’s symmetry group (B_n against S_n) more than its functional formweak to moderatetwo function families and two B_n Leaky-ReLUs; qualitative comparison of plots
C4The discrete clusters are a prerequisite for grandmother neurons, superposition and possibly neural collapseweakargued by connection to the author’s earlier SRM paper, not tested
C5Isotropic activations reconstruct betterweakpreliminary error curves, mixed without standardisation
C6The component-wise Jacobian deflects updates per orthant and so creates attractorsweakfirst-order single-layer calculation, App. C.2

Method

The PPP method:

  1. For a set of unit vectors b̂ᵢ (usually the standard basis), take each pair and orthonormalise it, ê₁ = b̂₁ and ê₂ ∝ b̂₂ − (b̂₂·b̂₁)b̂₁.
  2. Project each representation onto the plane by the pseudo-inverse.
  3. Keep it if ‖v_∥‖/‖v‖ > ε.
  4. Place a narrow Gaussian at its in-plane coordinates and sum over all planes and all representations.

The colour scale is fixed per row, so early-training density can be invisible next to late-training beams. A random subset of size N^0.9 was plotted where N was large.

Concepts

  • Anisotropic / isotropic function. One whose maximal algebraic equivariance group is discrete (S_n, B_n) or the orthogonal group O(n). It is a property of the map’s form, not of any distribution.
  • Distinguished directions / privileged basis. The directions an anisotropic form singles out.
  • Quantisation. Representations collapsing from a continuous spread into a few narrow beams.
  • Task-agnostic structure. Structure that recurs across seeds and datasets in the arrangement fixed by the primitive’s group. The author distinguishes it from clustering the task calls for.

Connections

The paper continues the author’s Spotlight Resonance Method (ICLR 2025 workshop), which found alignment to the activation’s basis and that it moves when the basis is rotated, and his “Isotropic Deep Learning” (Zenodo 2025), which proposed the radial primitives and predicted this result. It cites Elhage et al.’s toy models of superposition for the privileged basis, Godfrey et al. on network symmetries, and Papyan et al. on neural collapse.

Bearing on the record

  • QUESTION-058 lists the architecture as a possible source of a group in a representation. This paper isolates the activation as such a source. The beams are arranged by B_n or S_n, groups with no counterpart in reconstructing CIFAR or MNIST, and they vanish when the activation is made O(n)-equivariant. So a discrete group read off a trained network can be the network’s own. LIT-976’s filing note said the paper finds that “the algebraic symmetry of network primitives predicts task-agnostic representational structure”. That is a fair summary of the claim. The support is visual, from small autoencoders, with the B_n/S_n distinction resting on one family’s comparison.
  • THEORY-184 shows that a permutation-equivariant update preserves the symmetry it starts with. Bird’s elementwise networks have the same permutation symmetry, yet their representations move from spread to concentrated. THEORY-184 constrains distances between neurons, while Bird reports the distribution of examples in the neuron basis, so the two do not conflict. Together they say that the update keeps the group and the primitive imprints it on the data’s representation.
  • THEORY-017 holds that a basis is extra data supplied from outside the space. Bird gives a learned case in which the basis is supplied by the activation: with only rotation-equivariant parts, no direction is privileged, and the training procedure is rotation-equivariant in distribution. That last step is the record’s inference from the setup, not the paper’s statement.
  • THEORY-022 says the group in the grokking network “comes from the task, not the network”. Bird shows the opposite source for a different kind of structure: discrete axis alignment, not characters. The two are compatible, but THEORY-022’s “not the network” should not be read as general.
  • THEORY-210. In the isotropic networks every hidden layer has an O(n) gauge, a continuous symmetry, and the paper’s conjecture that they depend less on initialisation is the kind of claim THEORY-210 bears on. Bird does not test it.
  • THEORY-083 (neural collapse). Bird uses autoencoders to avoid the permutation symmetry of one-hot heads, and speculates that collapse is related. It is not tested.
  • Filed from this reading: THEORY-288.
  • The recommendations to re-evaluate activation functions, to prefer isotropic primitives for generative models, and to correct the affine map are machine-learning practice and belong to the anthology.

Limitations

  • No statistic. The comparisons are density plots. The author says quantitative measures “may further strengthen the certainty” and leaves them to future work. The only count is the about-100× rise in above-threshold samples.
  • Small models. Widths up to 32 and depths up to 3 hidden blocks, on CIFAR and MNIST only. Transformers, convolutions and residual networks are discussed (App. C.1) but not run.
  • The isolation is of a pair, not of symmetry alone. Every O(n)-equivariant map is radial, so each pair also contrasts coordinate-wise against radial nonlinearity. The hyperoctahedral Leaky-ReLU results are the evidence that the group matters beyond that. They are qualitative.
  • Artefacts. The method has known biases along the basis it measures in, discussed and partly controlled in App. A.
  • Single author, unrefereed. The paper was revised three times; v4 was read.
  • The downstream claims (grandmother neurons, superposition, neural collapse) and the pathologies (adversarial fragility, capacity) are conjectures here.

Open questions

  • A statistic for beam formation, with seeds and a null from random orthogonal bases, so that the contrast has an effect size.
  • Whether a network with the even-sign-flip group D_n, between S_n and B_n, shows an intermediate arrangement. The author’s attempt failed to train.
  • Whether the effect persists in classifiers and in large models, where residual connections, normalisation and attention each bring their own symmetry.