NOTE XXIV  ·  CRITICAL STRAIN & DIGITAL BANDGAP

Sc = 1.410

Edge-strain energy per site is constant across the Fibonacci family  ·  CV = 0.2%

Key Finding

Three results in one probe. (1) The σint hypothesis from Note XXIII is refuted at r=5.30: all n share identical σint=0.7938, threshold gap = 0.00000. The correct discriminant is Eper site (edge-strain energy per ring site): family members share Sc = 1.410 ± 0.003 (CV=0.2%), while non-family members are scattered at 1.38–1.61. (2) n=20 and n=30 at r=5.45 are artefacts: Iaz=2.56 > 2.5, max azimuthal gap 27.1° — the gap=0.002 result is clustering geometry, not real topology. n=31 at r=5.30 is confirmed: Iaz=1.964 < 2.0. (3) Sc / Eideal = 1.1431 ≈ φ/√2 (within 0.1%) — the candidate geometric constant for the lattice noise penalty.

1.410
Sc — critical strain per site
0.2%
CV of Sc across 8 family members
1.1431
Sc / Eideal (≈ φ/√2)
0.0000
σint threshold gap (hypothesis refuted)

Refutation: σint Is Not the Discriminant at r=5.30

Note XXIII identified a strong correlation (r=−0.88) between phason strain σint and the holonomy gap, leading to the hypothesis that a threshold σint* ≈ 0.788 separates family from non-family.

Hypothesis refuted

At fixed r=5.30, every n from 10 to 50 gives σint = 0.7938 (std = 0.00001). The threshold gap is exactly 0.00000. The Note XXIII correlation was capturing differences between rings at different radii (r=5.30 with N=32 vs r=5.55 with N=38 have different σint), not an n-dependent property of the r=5.30 ring itself. All 32 ring sites at r=5.30 have identical phason displacements regardless of n.

This makes geometric sense: for n≥12, the physical point cloud is identical (float64-converged). The 32 ring sites at r=5.30 are always the same 32 physical points, so their internal-space norms — set by the perpendicular basis — also converge. The σint correlation was an indirect proxy for the ring population change, not a direct geometric discriminant.

The True Discriminant: Edge-Strain Energy Eper site

The edge-strain energy is the sum of squared differential rotation steps around the ring:

Eedge = ∑ij (Δαij)2     Eper site = Eedge / Nring

where Δαij = (αrot,ij − αbase,ij + π) mod 2π − π is the per-edge differential rotation. This is the mean squared “roughness” of the winding per site — a local field-theoretic energy density.

Decomposing by mean and variance: Eper site = da̅2 + var(da). For a perfect 4π winding on N=32 sites: da̅ = −4π/32 = −0.3927, var(da) → 0. The family members achieve da̅ ≈ −0.388 (within 1% of ideal) with var(da) ≈ 1.26.

Sc = 1.410 ± 0.003
Critical edge-strain energy per site — 8 family members at r=5.30
Sc / (4π2/32) = 1.1431  ≈  φ/√2 = 1.1442  (0.1% off)

The coefficient of variation 0.2% across 8 family members spanning n=11…34 is extraordinary. The edge-strain energy is essentially a topological invariant of the n=31 ring in the E8 shadow — independent of the specific Fibonacci depth (within the family). This is the “digital bandgap”: the lattice supports stable 4π holonomy only at this specific strain level.

Family Strain Spectrum

n Nring da̅ σ(da) Eedge Eper site ideal step ΔΘ/2π
1132−0.387561.1199344.9421.40444−0.19635−1.9738
1332−0.381681.1251645.1731.41167−0.19635−1.9439
1532−0.384711.1217545.0031.40633−0.19635−1.9593
1732−0.388581.1213345.0681.40837−0.19635−1.9790
1832−0.390041.1223945.1811.41190−0.19635−1.9865
2332−0.388281.1227545.1621.41132−0.19635−1.9775
3132−0.390041.1223945.1811.41190−0.19635−1.9865
3432−0.389261.1243145.2991.41559−0.19635−1.9825

All Nring=32, Iaz=1.96, σint=0.7938. Ideal step = −2π/32 (for 2π winding); family achieves ≈2× this (4π winding). Sc = mean(Eper site) = 1.4102 ± 0.0033.

The ideal step column shows −2π/32 = −0.19635 for a single-winding (2π) traversal. The family achieves da̅ ≈ −0.388 ≈ 2 × (−2π/32), confirming the 4π double-winding interpretation: each edge carries double the single-winding step on average. The variance var(da) ≈ 1.26 is the aperiodic lattice noise — it is what prevents a perfect integer holonomy.

The Geometric Constant: Sc / Eideal = 1.1431

The ratio of observed critical strain to ideal (noiseless) strain:

Eideal = (4π)2 / N = 4π2/32 = 1.2337
Sc / Eideal = 1.4102 / 1.2337 = 1.1431
φ/√2 = 1.6180… / 1.4142… = 1.1442  (0.1% discrepancy)

The ratio 1.1431 encodes the lattice noise penalty: the aperiodic E8 shadow cannot perfectly distribute the 4π winding over 32 edges, so each edge carries 14.3% excess strain relative to the continuous-space ideal. The proximity to φ/√2 is a candidate geometric derivation of this penalty from first principles: the Golden Ratio controls the projection geometry, and √2 enters from the 2D perpendicular space.

Candidate formula for the noise penalty

Sc = (4π2/N) · (φ/√2)
For N=32: Sc = 1.2337 × 1.1442 = 1.4113 (vs measured 1.4102, error 0.08%). If this formula holds, the critical strain is not a free parameter but a derived consequence of the E8 shadow projection geometry.

Sub-experiment B: Azimuthal Audit of n=20, n=30

Note XXIII found gap=0.0021 at r=5.45 for both n=20 and n=30 — better than n=31’s 0.0135 at r=5.30. Per Note XVII criteria, any result with Iaz ≥ 2.0 must be verified. The audit is decisive:

n=20 at r=5.45

  • Nring = 34
  • ΔΘ/2π = −1.9979
  • gap = 0.0021
  • Iaz = 2.561
  • Max gap = 27.1°
  • Mean gap = 10.6°
  • E/site = 1.3177
ARTEFACT ❌ (I ≥ 2.5)

n=30 at r=5.45

  • Nring = 34
  • ΔΘ/2π = −1.9979
  • gap = 0.0021
  • Iaz = 2.561
  • Max gap = 27.1°
  • Mean gap = 10.6°
  • E/site = 1.3177
ARTEFACT ❌ (I ≥ 2.5)

n=31 at r=5.30 (reference)

  • Nring = 32
  • ΔΘ/2π = −1.9865
  • gap = 0.0135
  • Iaz = 1.964
  • Max gap = 22.1°
  • Mean gap = 11.2°
  • E/site = 1.4119
CONFIRMED ✅ (I < 2.0)

n=20 and n=30 give identical results at r=5.45: the same 34 sites, same Iaz=2.561, same maximum azimuthal gap of 27.1° (vs mean 10.6°). A single arc subtends 2.56 × more angular space than the mean, indicating severe clustering. The gap=0.002 is an artefact of the non-uniform angular distribution, not a coherent topological detection.

Diagnostic: artefact E/site is lower, not higher

Counterintuitively, the artefact result has E/site=1.3177 < Sc=1.410. Azimuthally clustered sites carry fewer edges in the long-arc region, so the strain energy is artificially low. A lower E/site with I>2.0 is a red flag for clustering artefact, not genuine stability.

Summary: What Governs the Family?

The Note XXIII question — “what determines family membership?” — now has a partial answer. Family membership at r=5.30 is not determined by σint (identical for all n) or |ε(n)| (no causal role). It is determined by whether the n-dependent phason basis produces a helix field that coherently distributes the 4π winding across the 32 ring edges with E/site ≈ Sc.

The mechanism remains to be derived analytically: why do certain perpendicular bases (n∈{11,13,15,17,18,23,31,34}) produce coherent winding while others (n=12,14, 19,21,…) produce incoherent winding at the same physical ring? This is the question for Note XXV.

Open: Towards α Derivation

The edge-strain energy Sc=1.410 ≈ (4π2/32)·(φ/√2) provides the “clean” starting point Gemini identified. A field-theoretic derivation of the fine-structure constant would proceed as:

α ≈ Sc × (geometric factors from the E8 projection depth) / (2π × Nring)

Numerically: Sc / (2π × 32) = 1.410/201.06 = 0.00701. The known value of α ≈ 0.00730. The ratio is 0.961 — within 4%, suggesting a correction factor near φ/π ≈ 0.515 or similar. This is a starting point for derivation, not yet a derivation. Note XXV will attempt to find the missing geometric factor.