The spectral determinant of the scalar Laplacian on each ALE space in the ADE series, compared against the E7 target derived from the fine structure constant.
Every finite subgroup Γ ⊂ SU(2) defines a 4D ALE space (asymptotically locally Euclidean) as the smooth resolution of C2/Γ. These are classified by the ADE Dynkin diagrams. Each ALE space has a scalar Laplacian, and its zeta-function-regulated spectral determinant is a geometric number. The conjecture: the E7 ALE space (resolving C2/2O, where 2O is the binary octahedral group) has spectral determinant equal to −(1/α − 137) = −0.035999. This page computes all An cases, finds the An series diverges, and states what is needed to reach E7.
The finite subgroups of SU(2) are classified by ADE:
| Dynkin | Group Γ | |Γ| | χ(ALE) | Exceptional divisors |
|---|---|---|---|---|
| An | Zn+1 (cyclic) | n+1 | n+1 | n |
| Dn | BD4(n-2) (binary dihedral) | 4(n-2) | n | n-1 |
| E6 | 2T (binary tetrahedral) | 24 | 7 | 6 |
| E7 | 2O (binary octahedral) | 48 | 8 | 7 |
| E8 | 2I (binary icosahedral) | 120 | 9 | 8 |
For each ALE space, the smooth crepant resolution (Kronheimer’s construction) carries a hyper-Kähler metric. The scalar Laplacian on this metric has a zeta-function-regulated spectral determinant. We compute the relative determinant: the ALE space versus (1/|Γ|) times flat C2.
The E7 theory derives the fractional part of 1/α from the self-consistent quadratic:
The fractional part is:
The conjecture is that this number appears as the E7 ALE spectral determinant:
If this holds, the geometry of the binary octahedral resolution would directly encode α without any free parameters. The computation is the test.
The A1 ALE space is the Eguchi–Hanson manifold: the minimal resolution of C2/Z2. The relative spectral determinant of the scalar Laplacian uses the Barnes double-zeta function:
The ingredients:
Evaluated at a = 1/2 and a = 1 using the Barnes G-function and Glaisher constant:
The target is −0.035999177. The gap:
A1 is already within 2% of the conjectured E7 value. The question is whether the remaining 0.000748 is closed by ascending the ADE ladder to E7.
For general An (Zn+1), the relative spectral determinant is:
The heat-kernel coefficient zeta_rel(0) = n/12 grows linearly with n (each exceptional divisor contributes 1/12). The derivative ΔAn computed numerically:
| Space | |Γ| | χ | Δ (spectral det.) | Gap from target |
|---|---|---|---|---|
| A1 | 2 | 2 | −0.036747 | 0.000748 |
| A2 | 3 | 3 | +0.029103 | 0.065102 |
| A3 | 4 | 4 | +0.143862 | 0.179862 |
| A4 | 5 | 5 | +0.286936 | 0.322936 |
| A5 | 6 | 6 | +0.448451 | 0.484451 |
| A6 | 7 | 7 | +0.622930 | 0.658930 |
| A7 | 8 | 8 | +0.807017 | 0.843017 |
| Target E7 | 48 | 8 | −0.035999 | — |
The divergence is not surprising once you see the reason. The An groups are abelian (cyclic). The D and E groups are non-abelian. The spectral determinant formula changes structurally:
For the binary octahedral group 2O (|2O| = 48), the elements fall into 8 conjugacy classes. The spectral determinant receives contributions weighted by the irreducible representations, not by a simple angular-sector sum. The An series is not the right path to E7.
The D4 ALE space resolves C2/BD8 where BD8 is the binary dihedral group of order 8 (the quaternion group Q8). It has 5 conjugacy classes: {e}, {−e}, {±i}, {±j}, {±k}. The spectral determinant requires:
The group BD8 acts on C2 with two non-trivial types of elements (order 4 and order 2), requiring two distinct angular integrals versus the single integral in the A1 case. Doable in principle; not yet computed.
The binary octahedral group 2O of order 48 has 8 conjugacy classes. The Kronheimer hyper-Kähler metric on the E7 ALE space is not explicitly known in closed form (it exists by construction, not by formula). Two methods are available:
Either method would give a definite number. If that number equals −0.035999177 = −(1/α − 137), the conjecture survives. If not, it is killed.
Despite the An ladder being killed, A1 itself is notable. The Eguchi–Hanson spectral determinant −0.036747 lands within 2% of the target −0.035999 without any tuning. The exact A1 value is:
This is a closed-form expression in standard transcendental constants. It is not 1/137, but it is close enough to suggest the E7 target is in the right neighborhood. Whether the additional group structure of 2O versus Z2 produces exactly the 0.000748 correction is the question the computation would answer.
A dedicated computational project (2O_Spectral_Determinant_Project) is running the E7/2O case directly through 9 cycles. Full attack history below.
The direct approach — compute nl(2O) via the Molien series, subtract the free-field baseline, weight by F(l) = −2ζH'(0, l+1) — was run to high cutoff:
| Cutoff L | Partial Δ2O |
|---|---|
| L = 100 | ~3.5 × 106 |
| L = 500 | ~3.2 × 109 |
| L = 1000 | ~5.9 × 1010 |
| L = 5000 | ~4.7 × 1013 |
| Target | −0.035999 |
Growth consistent with δl ~ −l2/48 leading to an L3 log L divergence. The naive method fails — higher-order polynomial tails must be removed analytically before the finite oscillatory part is accessible.
Cycle 9 replaced the earlier monolithic solver with a clean three-term decomposition:
Best 3-front combination (old resolution + new orbifold + new cross + new oscillatory):
Sign is now correct. Gap reduced by factor >2 versus previous best (+0.028). The new first-principles resolution (G/h mass) was the hidden dominant lever — the old normalization bug masked it across 8 prior cycles.
4-front (all new pieces, default coefficients): −0.10423 — expected overshoot from the large new resolution term. Joint retuning of orbifold coefficient and intrinsic coupling against the G/h resolution is the live math.
If the same G/h = 48/18 mass scaling is applied uniformly to all three geometric terms (resolution, orbifold, cross), the gap collapses by another order of magnitude:
Best result to date. The G/h uniform rescaling is the principled move — when you change the divisor-basis normalization from probability weights (divide by G) to affine Kac weights (divide by h), every linear-in-charge term must scale by the same factor for the relative physics to be preserved.
Even with the mass-consistent gap of −0.000681, two O(1) coefficients still sat inside the v11 character-projection modules: orb_coeff = 0.75 and cross_intrinsic = 0.00018. Rounds 1–6 of a dedicated attack tried to derive these from the same McKay graph / exact E7~ Cartan / representation-ring data using four natural conditions (determinant-style, variational, A1 normalization, lowest-mode). None reproduced the empirical ratio; closest was off by ~2.9×.
Round 7–8 of the attack imposed a new global constraint: the relative strengths chosen for E7/2O must reduce exactly to the known closed form on any A1 sub-system (where no extra boost is required). Combined with mass-rescaling stationarity, this gives a hard fixed point:
Off the (uncorrected) empirical 0.19175 by 1.21×. The closest pure first-principles number across all 8 rounds.
Independent audit then found that the v11 character table was lumping two distinct 2O conjugacy classes at θ = π/2 (face vs edge π/2 rotations are different conjugacy classes; v11 treated them as one). The character-weighted orbifold kernel:
| Table | raw_orb |
|---|---|
| v11 7-class (lumped) | 6.442 |
| Proper 8-class (split) | 4.971 |
| Ratio | 0.772 (23% systematic) |
The "empirical 0.19175" was computed with the lumped table, so it inherits the same systematic bias. Correcting:
| λ | |
|---|---|
| A1-hard first-principles derived | 0.2327 |
| Character-table-corrected empirical | 0.2485 |
| Ratio | 1.068× (7%) |
The first-principles derivation and the corrected empirical agree to 7%. The "two surviving free coefficients" framing from Step 5 is superseded at the orbifold-coefficient level: ADE subgroup consistency is the missing principle there.
Plugging the proper 8-class orbifold kernel into the full mass-consistent three-term solver:
| Configuration | Gap |
|---|---|
| 7-class table, original winning coefficients | −0.000681 (previous best) |
| 8-class table, same coefficients | −0.083 |
| 8-class table, orbifold coeff ×1.93 | −0.061 (best with single-knob retune) |
| 8-class table, orbifold coeff ×3.5–4 | −0.000681 (matches old best, but ~4× the old coefficient) |
The kernel ratio alone (1/0.7716 ≈ 1.30×) is far short of what's actually needed. Recovering anything close to the previous gap requires 3.5–4× the old effective orbifold coefficient. This means the cross and orbifold pieces in the 7-class pipeline were not just individually slightly biased — they were structurally compensating each other's lumping errors. Correcting one without the other exposes a multiplicative artifact.
Honest takeaway: the orbifold-coefficient principle (ADE consistency → λ ≈ 0.23) survives in isolation but cannot rescue the total three-term match alone.
Audit of the cross-term's character-weighted kernel under the proper 8-class table:
| Quantity | 7-class | 8-class | Shift |
|---|---|---|---|
| raw cross / raw orb ratio | ~1.89 | ~9.19 | ~5× |
The cross-orb relative geometric strength shifted by ~5× when the π/2 class is split — the 7-class lumping was distorting the cross's χ2·sin² inner product even more than the orbifold sin² kernel. This rules out any single-knob retune.
Three consequences:
Net position (Step 9): the 2O numerical pipeline is structurally open. Closing it requires rebuilding the cross sector on the proper 8-class table, deriving sector-specific scaling (not uniform G/h), and re-checking whether the res/orb/cross decomposition is even the right organizing structure under the corrected characters.
Sweeping the cross multiplier on the proper 8-class raw cross geometric (orbifold and resolution held first-principles):
| Cross multiplier | Gap to target |
|---|---|
| Uniform G/h ≈ 2.67 (old mass-consistent rule) | ~+4.06 |
| ~0.03109 (proper-table best fit) | +0.000438 |
| ~0.03036 (matches old −0.000681 magnitude) | −0.000681 |
The proper 8-class three-term solver does reach the target with a sector-specific cross multiplier ~0.03 — almost two orders of magnitude smaller than the uniform G/h boost that the 7-class pipeline used. The mass-consistent rule was never uniform; it was masquerading as uniform under the lumped characters.
Higher-precision fitting gives a measured cross multiplier ~0.0308. Three structural candidates were tested:
| Candidate | Value | Off measured |
|---|---|---|
| 1 / 32 (= 4 · χ(ALEE7)) | 0.03125 | 1.42% |
| 1 / (2π² · φ) | 0.03131 | 1.61% |
| 1 / 33 (33rd prime = 137) | 0.03030 | 1.65% (below) |
None of the three candidates hit the measured value at precision-fit accuracy. 1/32 and 1/(2π²φ) both overshoot by ~1.5%; 1/33 undershoots by similar. The precision fit has not selected a structural form — it has actually pushed all three candidates out of the "clean match" zone.
Three honest possibilities going forward:
Honest takeaway: the cross-sector scaling rule is sector-specific and small (~0.03), confirmed across multiple fits. The full proper-table three-term solver does reach +0.0004 of the spectral-determinant target. But the structural identification of the cross multiplier is not yet pinned down at precision-fit accuracy — ~1.5% remains between the measurement and the nearest framework-natural candidates.
The clean claim: not “E7 gives α.”
The clean claim is: “A1 gives −0.036747. Target is −0.035999. With the lumped 7-class table the 2O mass-consistent result reached −0.036680, but that match was a compound artifact of the lumping — matching it on the proper 8-class table requires ~3.5–4× the old orbifold coefficient. ADE consistency derives a coefficient near the corrected kernel ratio (~1.21−1.30×) but that's not enough to close the full gap. The 2O case is genuinely open; the principle direction is identified, the numerical match is not.”
Related pages: E7 Uniqueness Theorem · Electroweak Scale · The α Fixed Point · Why Three Generations · Theory Index