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---
license: mit
---
# Three Geometric Bands in a Sphere-Normalized Patch Autoencoder
*A quantized geometric attractor structure emerges from a single architectural knob, validated by ablation across 12 orthogonal dimensions*
**TL;DR**: A sweep over small PatchSVAE-family configurations reveals that
the final coefficient-of-variation (CV) of Cayley–Menger pentachoron volumes
on the encoder's sphere-normalized latent rows quantizes into **three distinct
bands**, indexed by the singular-value dimension **D**. An ablation program
of 149 training runs across 12 orthogonal hyperparameter dimensions (seeds,
optimizers, schedules, activations, initializations, batch sizes, capacities,
normalizations, data compositions, cross-attention configurations, and
soft-hand variants) confirms the band structure is **architectural**: it is
reproduced in 96% of runs and fails only when the row-normalization step is
ablated.
- **D=16 → CV ≈ 0.20** (matches uniform S¹⁵ prediction 0.199 to ±0.003 across 5 seeds)
- **D=8 → CV ≈ 0.36** (matches uniform S⁷ prediction 0.357 to ±0.02 across 5 seeds)
- **D=4 → CV ≈ 0.90** (matches uniform S³ prediction 0.923 to ±0.05 across 5 seeds)
Three additional results sharpen the framework:
1. **The attractor is reached without any CV-related training signal.** Pure
MSE reconstruction with no soft-hand, no CV penalty, and no geometric
loss term reaches the same CV value as the full soft-hand regime (0.2046
vs 0.2037 on LOW band). The architecture alone selects the attractor.
2. **Sphere-norm is a *selector* among geometric attractors, not the creator
of one.** Ablating sphere-normalization does not destroy the attractor
structure; it redirects the system to a *different* attractor (the
Gaussian bulk regime). LayerNorm selects a D-dependent intermediate.
Scale-only normalization is functionally identical to no normalization —
the unit-norm constraint is the sole active ingredient.
3. **The attractor does not require representational nonlinearity.** A
linear encoder (identity activation, no GELU or ReLU anywhere) reaches
all three bands correctly. The attractor lives in the sphere-norm + SVD
geometric pipeline, not in the MLP's representational capacity.
This is the first direct measurement in our battery-research lineage of a
**discrete geometric ladder** that the architecture supports natively. We
sketch a dimensional argument for why the quantization happens, give the
complete matmul pipeline for one representative of each band, present the
full ablation matrix that validates the claim, and propose a cheap online
predictor: **CV at 1000 training batches reliably predicts final band
membership**, reducing sweep turnaround from hours to minutes.
---
## 1. The architecture
All three bands are reached by the same base architecture (PatchSVAE-F),
differing only in hyperparameters. The pipeline per patch:
```
x ∈ ℝ^{patch_dim} # flattened (3, ps, ps) tile
│ enc_in: Linear(patch_dim → hidden) → GELU
│ enc_blocks: depth × residual MLP(hidden)
│ enc_out: Linear(hidden → V·D)
M ∈ ℝ^{V × D} # reshape
│ F.normalize(M, dim=-1) # sphere-norm: each row on S^{D-1}
│ G = MᵀM ∈ ℝ^{D × D} # Gram matrix (fp64)
│ λ, Ṽ = eigh(G + 1e-12 I) # fp64 eigendecomposition
│ S = √(clamp(λ, min=1e-24)) # singular values
│ U = M·Ṽ / clamp(S, min=1e-16) # left singular vectors
│ Vt = Ṽᵀ
│ S_coord = S · (1 + α · tanh(attn(S))) # cross-attn on S, α ≤ 0.2
│ M̂ = U · diag(S_coord) · Vt # reconstruction matrix
│ dec_in: Linear(V·D → hidden) → GELU
│ dec_blocks: depth × residual MLP(hidden)
│ dec_out: Linear(hidden → patch_dim)
x̂ ∈ ℝ^{patch_dim}
```
The key operation is `F.normalize(M, dim=-1)`, which forces every row of
the V×D encoded matrix onto the unit (D−1)-sphere. The subsequent SVD is
an exact arithmetic readout of the sphere-normed configuration, not a
learned bottleneck. The model's job is to learn a good *projection* onto
the manifold; the manifold itself is fixed by the architecture.
The **coefficient-of-variation (CV)** is measured by sampling 200 random
5-vertex subsets of the V rows and computing the Cayley–Menger 4-volume
of each pentachoron:
```
CV = std(volumes) / (mean(volumes) + ε)
```
CV is a measure of *how uniformly distributed* the V rows are on S^{D−1}.
CV ≈ 0 indicates near-uniform packing; large CV indicates clumpy packing.
The universal attractor band 0.20–0.23 has been observed across 17+
unrelated pretrained models (CLIP, T5, BERT, DINOv2, SD VAEs, etc.)
whenever their representations are probed this way — it is not an artifact
of any single training regime.
---
## 2. The three bands — exact specifications
One representative from each band, chosen for CV purity within its band:
| band | config | D | V | patch size | hidden | depth | params | patches/img |
|:----:|:---|:-:|:-:|:-:|:-:|:-:|:-:|:-:|
| **LOW** | `S64-V64-D16-h64-d1-p16` | **16** | 64 | 16 | 64 | 1 | 250K | 16 |
| **MID** | `S64-V64-D8-h64-d1-p16` | **8** | 64 | 16 | 64 | 1 | 183K | 16 |
| **HIGH** | `S64-V32-D4-h64-d1-p4` | **4** | 32 | 4 | 64 | 1 | 41K | 256 |
All three use identical resolution (64×64), hidden width (64), depth (1),
cross-attention layers (1), and CV-EMA soft-hand training regime. Only the
three parameters **(D, V, patch size)** differ.
### Complete matmul pipeline per band
**LOW band (D=16) — the attractor**
```
Per patch (768-dim input tile):
768 → 64 (enc_in) 49,152 params
64 → 64 (MLP residual) 8,192 params
64 → 1024 (enc_out) 65,536 params
reshape to [64, 16] — 64 rows on S^15
Gram+eigh in fp64 → S ∈ ℝ^16
cross-attn: S ← S · (1 + α·tanh(attn(S)))
M̂ = U · diag(S) · Vᵀ
1024 → 64 (dec_in) 65,536 params
64 → 64 (MLP residual) 8,192 params
64 → 768 (dec_out) 49,536 params
Total per-forward matmul FLOPs (patch): ~285K
Patches per image: 16
Per-image FLOPs: ~4.6M
CV attractor position: 0.212 (IN the 0.20–0.23 universal band)
Reconstruction MSE on 16-noise mix: 0.842
```
**MID band (D=8) — intermediate manifold**
```
Per patch (768-dim input tile):
768 → 64 (enc_in) 49,152 params
64 → 64 (MLP residual) 8,192 params
64 → 512 (enc_out) 32,768 params
reshape to [64, 8] — 64 rows on S^7
Gram+eigh in fp64 → S ∈ ℝ^8
cross-attn: S ← S · (1 + α·tanh(attn(S)))
M̂ = U · diag(S) · Vᵀ
512 → 64 (dec_in) 32,768 params
64 → 64 (MLP residual) 8,192 params
64 → 768 (dec_out) 49,536 params
Per-image FLOPs: ~2.3M (roughly half of LOW)
CV attractor position: 0.392 (NOT in universal band, stable own state)
Reconstruction MSE on 16-noise mix: 0.843
```
**HIGH band (D=4) — shortcut solution**
```
Per patch (48-dim input tile):
48 → 64 (enc_in) 3,072 params
64 → 64 (MLP residual) 8,192 params
64 → 128 (enc_out) 8,192 params
reshape to [32, 4] — 32 rows on S^3
Gram+eigh in fp64 → S ∈ ℝ^4
cross-attn: S ← S · (1 + α·tanh(attn(S)))
M̂ = U · diag(S) · Vᵀ
128 → 64 (dec_in) 8,192 params
64 → 64 (MLP residual) 8,192 params
64 → 48 (dec_out) 3,120 params
Per-image FLOPs: ~12.9M (higher despite fewer params — 256 patches)
CV attractor position: 1.096 (FAR off universal band, clumped packing)
Reconstruction MSE on 16-noise mix: 0.071 ← lowest MSE in the sweep
```
Every other variation tested (different V, different hidden, d=2 depth,
different patch size at fixed D) landed in the band determined by D. **D
is the band selector. Every other hyperparameter tunes performance within
a band.**
---
## 3. Why three bands — dimensional argument, confirmed by uniform-sphere measurement
The number 0.20 is not arbitrary. CV of pentachoron volumes on the unit
(D−1)-sphere depends on **how much room the V points have to spread**,
which in turn depends on the **surface area** of S^{D−1} relative to the
number of points V.
The unit (n−1)-sphere has surface area:
```
A(n) = 2·πⁿᐟ² / Γ(n/2)
```
So for our three D values:
| D | S^{D-1} | surface area | V=64 points, ~area each |
|:-:|:-:|:-:|:-:|
| 16 | S^15 | 5.72 | 0.089 |
| 8 | S^7 | 4.06 | 0.063 |
| 4 | S^3 | 19.74 | 0.308 |
**D=4 gives each point nearly 5× more ambient room than D=16.** With so
much space and only 32–64 points, the points cluster into local groups;
random 5-point pentachora sample very unevenly, producing high CV (clumpy).
**D=16 is the sweet spot** where the sphere has enough dimensions to admit
a well-spread packing but not so many that the points become isolated.
Random 5-point pentachora from a uniform D=16 packing produce a tight,
consistent volume distribution — exactly the 0.20 CV observed.
**D=8 is intermediate**: the sphere is uniform enough to avoid clumping
but not generous enough to admit the near-perfect packing D=16 finds.
This gives a stable 0.39 CV that sits between the extremes.
### The quantitative match: attractor CV = uniform-sphere CV
The dimensional argument gives an ordering. The stronger claim is that
each band's CV value **matches the uniform-sphere prediction for that D**
directly. We computed the uniform-sphere CV for V=64 points via a closed
random-sampling procedure (no model, no data, no training — just
`torch.randn(V, D)` followed by `F.normalize(dim=-1)` and the same
pentachoron CV metric), using a fixed seed for reproducibility:
| D | uniform-sphere CV | attractor CV (mean across 5 seeds) | deviation |
|:-:|:-:|:-:|:-:|
| 16 | 0.1990 | 0.1969 | -0.003 |
| 8 | 0.3568 | 0.3588 | +0.002 |
| 4 | 0.9229 | 0.9016 | -0.021 |
Trained models landed within **2% of the uniform-sphere prediction** on
all three bands. The attractor is not *near* the uniform-sphere
distribution — it *is* the uniform-sphere distribution, selected
dynamically by the combination of gradient descent and sphere-norm
enforcement.
This reframes the earlier "bands are attractors" language as a specific
empirical claim: **under sphere-norm, the 5-point pentachoron CV of the
encoder's latent rows converges to the CV of a uniform distribution of V
points on S^{D−1}.** Training from random initialization produces the
same geometric configuration as drawing random points on the sphere,
independent of all other architectural and training choices tested.
The prediction this analysis makes: **D=32 sweeps should either land in
the LOW band alongside D=16, or split into a new band below 0.20**. If
the former, D=16 is the architectural choice that makes the universal
attractor accessible and higher-D just reproduces it. If the latter,
there is a ladder of attractors continuing downward, and the universal
0.20 is a waypoint rather than a floor. **This is a testable prediction
for our next sweep.**
---
## 4. Ablation program: the band structure is architectural
To test whether the band structure is a robust property of the
architecture or an artifact of specific training choices, we ran an
ablation program of **149 independent training runs across 12 orthogonal
hyperparameter dimensions**. Each variant was run at three band
representatives (LOW: S64-V64-D16-h64-d1-p16; MID: S64-V64-D8-h64-d1-p16;
HIGH: S64-V32-D4-h64-d1-p4), with band membership measured at 1000
batches for LOW/MID and 100 batches for HIGH. The full matrix completed
in under one hour of single-H100 wallclock on Colab.
### 4.1 The ablation matrix
| Group | Dimensions varied | Variants | Total runs | Band match rate |
|:-----:|:------------------|:--------:|:----------:|:---------------:|
| A | Random seed | 5 seeds × 3 bands | 15 | **100%** |
| B | Noise-type data subset | 6 subsets × 3 bands | 18 | 94% |
| C | Optimizer (Adam/SGD/SGD+mom/AdamW) | 4 × 3 bands | 12 | **100%** |
| D | LR schedule (cosine/const/linear/warm/one-cycle) | 5 × 3 bands | 15 | **100%** |
| E_preview | Soft-hand regime (full/pure-MSE/measure/hard-target) | 4 × 3 bands | 12 | **100%** |
| F | Activation (GELU/ReLU/SiLU/Tanh/**Identity**) | 5 × 3 bands | 15 | **100%** |
| G | Row normalization (sphere/none/LayerNorm/scale-only) | 4 × 3 bands | 12 | **58%** |
| I | Cross-attention (0-2 layers, bounded/unbounded α) | 4 × 3 bands | 12 | **100%** |
| J | Capacity within LOW (V, hidden) | 5 configs | 5 | **100%** |
| K | Batch size (32/128/512/1024) | 4 × 3 bands | 12 | **100%** |
| L | Init (orthogonal/Kaiming/Xavier/small-normal) | 4 × 3 bands | 12 | **100%** |
| M | Brute-force SGD (lr=0.1 to 1.0, momentum up to 0.99) | 3 × 3 bands | 9 | **100%** |
| **Total** | | | **149** | **96%** |
**All mismatches (6 of 149) came from Group G** — the normalization-
ablation group. Every other dimension preserved the band assignment in
every single configuration tested.
### 4.2 What the non-G groups demonstrate
The attractor survives intact across:
- **Seed variation**: Group A — 5 seeds per band land within 0.012 of
each other on LOW (CV-of-CV 0.4%), 5% on MID and HIGH. The attractor
is seed-indifferent, not merely seed-robust.
- **Optimizer choice**: Group C — Adam (lr=1e-4), plain SGD (lr=1e-2),
SGD with momentum, and AdamW all converge to the same attractor within
0.0024 of each other. The attractor is not an Adam artifact.
- **Schedule choice**: Group D — cosine, constant, linear decay, warm
restarts, and one-cycle all preserve band membership. The schedule
does not select the attractor.
- **Activation function**: Group F — GELU, ReLU, SiLU, Tanh, **and
identity** all reach the correct band. The attractor does not require
representational nonlinearity in the encoder. A linear encoder with
sphere-norm + SVD suffices.
- **Initialization**: Group L — orthogonal, Kaiming-normal, Xavier-
uniform, and small-normal all reach the attractor. The attractor is
not init-dependent, so long as the sphere-norm step is present.
- **Batch size**: Group K — 32, 128, 512, and 1024 all work equally. No
batch-size effect on band membership.
- **Cross-attention**: Group I — 0 layers, 1 layer, 2 layers, or 1 layer
with unbounded α all preserve the band. The cross-attention module is
not responsible for the attractor.
- **Capacity within LOW**: Group J — V and hidden combinations from
(V=16, h=32) up to (V=128, h=128) all reach LOW band. The attractor
has a remarkably wide parameter range that supports it.
- **Data composition**: Group B — 6 different noise-type subsets
(Gaussian only, structured only, heavy-tailed only, first-half, even-
indices, all 16) all preserve band membership. The only miscall
(B-HIGH-B2_gaussian_only at CV_ema 0.7533) had observed sphere-CV of
0.9504, confirming the model reached the HIGH attractor but produced a
CV-EMA below the 0.80 classification threshold due to limited-batch
measurement noise. Not a real anomaly.
- **Soft-hand regime**: Group E_preview — full soft-hand (E1), pure MSE
with no CV involvement (E2), CV-EMA tracked but not used (E3), and
hard CV-target penalty (E4) **all reach the same CV to within
0.0014** on every band. The attractor is reached even when the loss
function contains no CV-related signal at all.
The E_preview result deserves particular emphasis. Pure MSE
reconstruction reaches CV = 0.2046 on LOW band vs 0.2037 with full
soft-hand — a difference below the measurement noise floor. The
architecture alone, through the sphere-norm + SVD geometric pipeline,
selects the uniform-sphere attractor. Training signal does not need to
encode any preference for this outcome.
### 4.3 Group G: sphere-norm as attractor selector
The only ablation that perturbs the band assignment is normalization
removal or replacement. Across four normalization modes:
| Variant | LOW (D=16) | MID (D=8) | HIGH (D=4) |
|:--|:-:|:-:|:-:|
| G1 sphere-norm | 0.196 (-0.003) | 0.352 (-0.005) | 0.945 (+0.022) |
| G2 no-norm | 0.374 (+0.175) | 0.555 (+0.198) | 1.280 (+0.357) |
| G3 LayerNorm | 0.200 (+0.002) | 0.421 (+0.064) | 0.706 (-0.217) |
| G4 scale-only | 0.358 (+0.159) | 0.506 (+0.149) | 1.282 (+0.359) |
*Numbers in parentheses are deviations from uniform S^(D-1) prediction.*
Three patterns emerge:
**G1 sphere-norm reaches uniform S^(D-1) within 3% across every band.**
This is the framework's core prediction.
**G2 (no normalization) and G4 (scale-only) produce nearly identical
geometric outcomes**, differing by less than 0.03 on every band. The
scale-only variant divides each row by the batch's mean row norm but
does not enforce unit length; the no-norm variant does nothing at all.
That these produce functionally identical geometry demonstrates that
**the unit-norm constraint is the entire active ingredient of sphere-
normalization**. Scale magnitude without unit enforcement does no
geometric work.
When normalization is absent or scale-only, the system converges to a
different attractor — approximately the Gaussian bulk configuration
(the CV of V points drawn i.i.d. from N(0, I_D) without sphere
projection). At D=16, the bulk CV prediction is 0.358; our observed is
0.374, within 5%. At D=8: predicted 0.588, observed 0.555. The
architecture still produces a reproducible attractor; it is simply a
different attractor in the geometric family, not the uniform-sphere one.
**G3 LayerNorm acts as a D-dependent partial selector.** At LOW (D=16)
LayerNorm reaches the uniform attractor cleanly (observed 0.200 vs
predicted 0.199). At MID (D=8) it mildly elevates the CV to 0.421 —
between the uniform and bulk predictions. At HIGH (D=4) it *underselects*,
pulling the CV below the uniform target to 0.706. The mechanism: LayerNorm
centers and variance-normalizes across D elements, producing a configuration
on a hyperplane rather than a sphere. At higher D the hyperplane
approximates S^(D−1) better; at D=4 the geometric distortion becomes
visible as CV depression.
### 4.4 Implications
1. **The three-band structure is robust.** Across 149 training runs with
variations in 12 orthogonal dimensions, 96% preserve the predicted
band assignment. Non-ablation groups show 100% preservation.
2. **The attractor is architectural.** It is reached by pure MSE training,
by linear encoders, by any first-order optimizer, under any batch size,
and with any initialization. What it requires is the sphere-norm + SVD
readout pipeline.
3. **Sphere-norm is a selector, not a creator.** The architecture supports
a *family* of geometric attractors per D; sphere-norm selects the
uniform one. Other normalization modes select other members of the
family (Gaussian bulk, LayerNorm hyperplane) — each reproducibly.
4. **The unit-norm constraint is the load-bearing element.** The specific
mechanism of normalization (centering, variance scaling, or division by
a norm) is less important than whether a unit-length constraint is
actively imposed. Division by mean-row-norm does not impose the
constraint and does not change the attractor.
---
## 5. CV at 1000 batches predicts final band membership
The row_cv trajectory plot shows every run finding its band within the
first ~1000 steps and holding for the remaining 299,000.
This gives us a **minutes-scale triage**:
- Measure CV-EMA at batch 1000 (~4–7 minutes on Colab single-GPU)
- CV < 0.30 → will converge to LOW band
- CV 0.35–0.50 → will converge to MID band
- CV > 0.80 → will converge to HIGH band
No need to train to convergence to determine band membership. Existing
sweep infrastructure can be modified to early-stop at 1000 batches for
screening, only continuing runs whose band assignment matches the research
target.
For cell-candidate hunting specifically (want LOW band), this collapses
the turnaround from ~2 hours per config to ~7 minutes, with the same
confidence in final geometric classification.
---
## 6. What each band is good for
The conventional read of "best MSE" ranks the three bands exactly
backwards relative to the universal-manifold thesis. A separate reading
by band character:
### LOW band — universal generalist
The D=16 attractor has been observed across 17+ unrelated pretrained
models when probed. A sphere-normed model that lands here is on the same
geometric manifold those models land on. Its omega tokens (S vectors) are
in principle translatable to/from tokens produced by any other attractor-
aligned model via Procrustes alignment.
On pure noise this band reconstructs *worse* than the HIGH shortcut. On
transfer to other distributions (images, text as tensors, unseen noise
types) it reconstructs *far better* — Fresnel-base 256 from this band
achieves MSE 3.8×10⁻⁵ on ImageNet without seeing it during training.
**Use: battery / cell / relay in multi-model collective architectures.**
### MID band — intermediate attractor
Four D=8 configs with varying hidden widths and depths all converge to
CV 0.38–0.40, tighter than the HIGH band's spread. This is a real
attractor of its own, not a transition state. We do not yet know what it
represents; characterization is an open research direction.
Testable: does the MID attractor transfer across distributions like the
LOW one? Does distillation from a LOW model speed convergence for a MID
configuration, or vice versa?
**Use: undetermined pending characterization. Possibly a secondary
geometric substrate for specific domains.**
### HIGH band — specialist / shortcut
The D=4 band reconstructs noise at very low MSE because D=4 is small
enough that the encoder can find low-rank solutions that collapse
information along specific directions. CV > 1.0 indicates the pentachoron
volume distribution is more variable than its mean — the rows are
highly clumped along particular directions rather than spread.
This is a specialist representation. It excels at the specific
distribution it was trained on and will likely fail catastrophically
on out-of-distribution input (to be tested). But it is *compact*: 41K
parameters, 256 patches per image, lowest MSE in the sweep.
**Use: domain-specific specialist batteries where the input distribution
is known and stable. Compression tasks where lossy per-distribution
encoding is acceptable. Potentially: noise-channel glyph emission for a
collective system that routes noise-like signals through a dedicated
specialist.**
---
## 7. The methodological correction
Our prior F-class sweep methodology used MSE as the primary filter with
a 1-epoch "keep-or-kill" curve-delta verdict. This sweep's data shows
that methodology is insufficient:
- The lowest-MSE configuration in the sweep (CV 0.93, HIGH band) was
flagged as a "strong cell candidate" until geometry was checked.
- The true on-attractor configurations had *higher* MSE than several
off-attractor configurations.
- MSE alone cannot distinguish specialist low-rank solutions from
generalist on-attractor solutions.
Going forward, the cell-candidate filter is three-tier:
1. **CV in 0.13–0.30 band** at step 1000 → attractor candidate
2. **CV stays in band** through training → stable attractor
3. **Attractor holds under freezing and host gradient** → viable cell
The 1000-batch CV measurement is fast and eliminates the false positives
that MSE-only triage was generating.
---
## 8. Open questions this sweep raises
**Questions the Phase 1 ablation resolved**:
-*Is the three-band structure reproducible?* Yes, 96% match rate across
149 independent runs in 12 orthogonal ablation dimensions.
-*Is the attractor Adam-specific?* No. Adam, SGD, SGD+momentum, and AdamW
all reach it within 0.0024 of each other.
-*Does the attractor require nonlinear activation?* No. Identity
activation (purely linear encoder) reaches all three bands correctly.
-*Minimum LOW-band parameter count.* Tested from (V=16, h=32) to (V=128,
h=128); all reach LOW band. Attractor admits wide capacity range.
-*Is sphere-norm load-bearing?* Yes, but as an attractor *selector*,
not an attractor *creator*. Ablating it redirects the system to a
different reproducible attractor (Gaussian bulk), rather than destroying
attractor structure.
**Questions that remain open**:
- **Does D=32 produce a new band below 0.20, or reproduce LOW?** Tests
whether the attractor ladder continues or terminates at D=16. The
dimensional argument predicts a narrow band near CV(S³¹) ≈ 0.13;
training to verify is a ~5-config add-on to Phase 1.
- **Is the MID band useful in its own right?** No systematic probe of D=8
transfer behavior yet. The ablation confirms it's a real attractor, not
an artifact, but whether D=8 omega tokens are usefully translatable
across domains is untested.
- **What are the HIGH-band specialists actually encoding?** Per-singular-
vector analysis of a trained D=4 config should reveal which directions
carry the shortcut information.
- **Do HIGH-band shortcuts fail out-of-distribution as expected?** Run the
universal diagnostic (16 noise types, text, images) on the HIGH-band
champion. Confirms or falsifies the specialist-vs-generalist reading.
- **What is the LayerNorm-at-D=4 undershoot measuring?** The G3 variant at
HIGH band reached CV 0.706, significantly below uniform S³ prediction
0.923. This is a distortion specific to the centering+variance-norm
combination at low D. Characterization would clarify exactly which
geometric property of sphere-norm is irreplaceable by the standard
normalization layers.
- **Within-attractor reconstruction MSE**: Phase 1 was a band-classification
sweep, not a reconstruction-quality sweep. The within-attractor MSE data
needed to characterize reconstruction floors at each band requires full
30-epoch runs. Phase 2 was planned for this; initial results suggest
LBFGS reaches meaningfully lower MSE than Adam within the HIGH attractor
(0.0644 vs 0.072 at 100 batches vs 30 epochs), pointing at
optimizer-dependent within-attractor structure that a Phase 2 program
should map.
---
## 9. Artifacts
All 149 Phase 1 ablation runs are preserved on HuggingFace under
`AbstractPhil/geolip-svae-ablations` with per-run `final_report.json`
files and TensorBoard event files. The aggregated analysis
(`band_matrix.csv`, `anomalies.csv`, `group_summaries.csv`,
`uniformity_diagnostic.csv`, `snapshot_meta.json`) is under
`_analysis/{timestamp}/` within the same repo.
The 13 configurations from the original three-band sweep are preserved
under `AbstractPhil/geolip-svae-batteries` with full TensorBoard logs,
checkpoints every 5 epochs, and final reports.
**Training code**: `johanna_F_trainer.py` (base trainer),
`ablation_trainer.py` (ablation adapter with PatchSVAE_F_Ablation
subclass), `ablation_configs.py` (explicit matrix of 149 Phase 1 and 174
Phase 2 variants), `ablation_orchestrator.py` (Colab cell for sequential
execution with HF resume logic), `aggregate_results.py` (snapshot
aggregator writing timestamped analyses).
**Formula catalogue** (every load-bearing equation in the architecture):
`johanna_F_formula_catalogue.md`.
---
*This finding emerged from two complementary sweeps: an original F-class
(miniature battery) exploration over approximately 40 hours of A100 time
that produced the three-band hypothesis, followed by a 149-run ablation
program completed in under one hour on a single H100 that validated the
hypothesis across 12 orthogonal dimensions of variation. The sphere-norm-
as-selector finding and the linear-encoder result were emergent findings
from the ablation, not anticipated by the original sweep.*