V2.116 - The Spectral Proof — Mode-by-Mode Entanglement-Energy Identity
V2.116: The Spectral Proof — Mode-by-Mode Entanglement-Energy Identity
Executive Summary
This experiment decomposes the V2.115 aggregate vacuum energy–entropy identity (E_vac/α is field-independent) into its per-channel components on the 3+1D spherical lattice. The findings are:
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Per-channel ratios E_l/S_l and E_l/α_l are NOT constant across angular momentum l. They grow strongly with l (CV = 81% and 41% respectively). The “identity” does NOT hold mode-by-mode in the naive sense.
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But: field independence is STRUCTURAL, not numerical. The coupling matrix K_l depends only on l and mass — it is identical for scalars, vectors, and all bosonic fields. Therefore E_l, S_l, α_l, and the full entanglement spectrum are automatically field-independent at every l. This is a proof, not a measurement.
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Entanglement is extremely concentrated. At each angular momentum channel, effectively only one mode out of n_sub carries significant entanglement (n_eff ≈ 1.03–1.26). The entropy is determined by ~l_max boundary modes, while the vacuum energy sums over all N × l_max bulk modes. The aggregate identity E_vac/α ∝ tr(1) holds despite this asymmetry.
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The modular Hamiltonian is NOT proportional to the physical Hamiltonian (CV = 35%, R² = 0.86). The Bisognano-Wichmann theorem does not generalize exactly to the sphere. However, H_sub and K_mod are linearly correlated, meaning physical energy and entanglement structure are strongly linked.
The overall conclusion: V2.115’s aggregate identity is not a coincidence of summation — it follows necessarily from the structural field-independence of K_l plus degeneracy counting. Λ_bare = 2π ρ_vac/α is a pure geometric quantity because ρ_vac/α is determined by geometry alone at every angular momentum.
Motivation
V2.115 showed E_vac/α is field-independent to 0.48% in aggregate. Two interpretations were possible:
- Deep: The identity holds mode-by-mode — vacuum energy and entropy are the same physics at every scale.
- Shallow: The identity holds only in aggregate due to both quantities being proportional to tr(1).
V2.116 tests which is correct.
Phase 1: Per-Channel Energy-Entropy Ratio
Setup: N = 100 radial sites, n_sub = 33, angular momentum l = 0 to 40.
Result: E_l/S_l grows from 100 (l = 0) to 3400 (l = 40). CV = 80.7%.
| l | E_l | S_l | E_l/S_l |
|---|---|---|---|
| 0 | 63.93 | 0.639 | 100 |
| 5 | 69.34 | 0.304 | 228 |
| 10 | 77.31 | 0.203 | 382 |
| 20 | 96.05 | 0.109 | 880 |
| 40 | 138.62 | 0.040 | 3438 |
Why it grows: E_l grows linearly with l (centrifugal barrier raises all mode frequencies), while S_l decays exponentially with l (higher angular momentum = less boundary entanglement). These are different physical effects: vacuum energy is a bulk property, entropy is a boundary property.
The l-dependence fits: E_l/S_l ≈ 216 − 11.3l + 2.21l², a purely geometric function of l.
N-dependence at l = 0: E_0/S_0 grows roughly linearly with N (from 53 at N = 40 to 135 at N = 150), confirming it’s a geometric/cutoff-dependent quantity.
Honest assessment: The per-channel identity does NOT hold as a flat ratio. E_l/S_l depends strongly on l. But this l-dependence is geometric — identical for all field types.
Phase 2: Spectral Universality — The One-Mode Theorem
The most striking finding: entanglement is carried by essentially one mode per channel.
| l | S_l | n_entangled | n_eff | ν_max |
|---|---|---|---|---|
| 0 | 0.639 | 1 | 1.26 | 0.735 |
| 5 | 0.304 | 1 | 1.08 | 0.586 |
| 10 | 0.203 | 1 | 1.03 | 0.550 |
| 20 | 0.109 | 1 | 1.01 | 0.523 |
Out of n_sub = 33 symplectic eigenvalues per channel, only ONE deviates significantly from the vacuum value ν = 1/2. The spectral entropy (Shannon entropy of the per-mode entropy distribution) gives n_eff ≈ 1, meaning all the entanglement resides in a single boundary mode.
Physical interpretation: The entangling surface at radius r = n_sub supports one entangled degree of freedom per angular momentum channel. This is the lattice realization of the “entanglement across the horizon” picture: each (l, m) partial wave contributes one entangled bit, and the area law S ~ l_max² arises from summing (2l+1) copies.
Entropy decay: S_l ∝ exp(−6.69 × ω_min), where ω_min is the minimum mode frequency (set by the centrifugal barrier). Higher angular momentum → larger gap → less entanglement.
Phase 3: Modular vs Physical Energy
Result: H_sub/K_mod is NOT constant across channels (CV = 35%).
| l | H_sub | K_mod | H_sub/K_mod |
|---|---|---|---|
| 0 | 17.1 | 376 | 0.045 |
| 10 | 29.2 | 402 | 0.073 |
| 20 | 45.8 | 412 | 0.111 |
| 29 | 61.8 | 418 | 0.148 |
The modular Hamiltonian is NOT proportional to the physical Hamiltonian. The Bisognano-Wichmann theorem (which guarantees proportionality for Rindler wedges) does not generalize exactly to the sphere.
However, H_sub and K_mod are linearly correlated: H_sub = 1.13 × K_mod − 419, R² = 0.86. Physical energy and entanglement structure are strongly linked, just not proportional.
H_sub/K_mod grows with l because the physical energy H_sub grows (centrifugal barrier), while the modular energy K_mod is approximately constant (dominated by the nearly-unentangled bulk modes at ν ≈ 1/2, which contribute large β × ν terms).
Phase 4: The Structural Proof of Field Independence
This is the central result. The coupling matrix K_l for the radial chain is:
K_l[j,j] = ((j-1/2)² + (j+1/2)² + l(l+1)) / j² + m²
K_l[j,j+1] = -(j+1/2)² / (j(j+1))
This depends only on l, m, and N. It does not depend on the spin of the field.
For a scalar, the total entropy is S = Σ_l (2l+1) S_l. For a vector, it is S = Σ_l 2(2l+1) S_l (with l ≥ 1).
Since S_l is identical for both at each l, the vector/scalar ratio is:
α_vector / α_scalar = [Σ_l 2(2l+1) α_l] / [Σ_l (2l+1) α_l]
This equals 2 exactly if the l = 0 channel is negligible (it contributes < 1% at large C). The measured ratio 2.005 (V2.74) is the residual from the l = 0 scalar-only contribution.
The same structural argument applies to vacuum energy: E_vector/E_scalar = 2.000 because E_l is field-independent at each l.
Therefore: The V2.115 aggregate identity E_vac/α = field-independent follows NECESSARILY from:
- K_l is field-independent (structural fact)
- Degeneracy counting: d_l = tr(1) × (2l+1)
This is not a numerical coincidence. It is a theorem of the lattice construction.
Phase 5: E_l/α_l — Geometric Variation
E_l/α_l varies from 22,341 (l = 0) to 49,603 (l = 34). It grows monotonically with l (94% of consecutive pairs are increasing).
This variation encodes the geometry of the lattice:
- E_l grows linearly with l (more vacuum energy at higher angular momentum)
- α_l decreases with l (less entropy per boundary site at higher angular momentum, because the centrifugal barrier suppresses boundary entanglement)
Crucially: this variation is GEOMETRIC, not field-dependent. For any bosonic field, E_l/α_l at angular momentum l is identically the same number. The aggregate ratio E_vac/α is then determined by:
E_vac/α = [Σ d_l E_l] / [Σ d_l α_l]
which is a weighted average of E_l/α_l with weights d_l × α_l. Since both d_l and the E_l/α_l function are field-independent, the aggregate is field-independent — QED.
What This Means for Λ_bare = 0
The argument now has three layers:
Layer 1 (V2.115, aggregate): E_vac/α is field-independent to 0.48%. → ρ_vac/α is a pure geometric quantity. → Λ_bare = 2π ρ_vac/α is determined by geometry alone.
Layer 2 (V2.116, per-channel): K_l is structurally field-independent. → The aggregate identity is not an artifact of cancellation — it holds because of the mathematics of the radial chain. → E_l = α_l × F(l, N) where F is a geometric function.
Layer 3 (V2.116, spectral): Entanglement resides in one mode per channel. → The entropy counts boundary modes (one per l-channel on the entangling surface). → The vacuum energy counts bulk modes (N per l-channel in the volume). → Despite this asymmetry, E/α is field-independent because BOTH are computed from the SAME coupling matrix K_l.
The physical picture: the coupling matrix K_l encodes ALL the physics — vacuum energy, entanglement entropy, area coefficient, and modular Hamiltonian. Different quantities extract different functions of K_l’s eigenvalues and eigenvectors, but they are all determined by the same underlying data. Adding Λ_bare = 8πGρ_vac uses G from α (extracted from K_l) and ρ_vac (also extracted from K_l) — it’s the same information counted twice.
What Did NOT Work
Being honest about negative results:
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E_l/S_l is NOT l-independent. The per-channel “identity” does not hold as a flat ratio. The l-variation is strong (CV = 81%).
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H_sub ≠ const × K_mod. The Bisognano-Wichmann proportionality does not hold for the sphere. The modular Hamiltonian is NOT simply related to the physical Hamiltonian.
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The “mode-by-mode” identity ν_k = f(ω_k) does not exist in a simple form, because the ν spectrum has n_sub values while the ω spectrum has N values. The mapping is through the eigenvector matrix V, not a simple function.
These are important limitations. The spectral proof works at the STRUCTURAL level (K_l is field-independent), not at the level of individual eigenvalue relationships.
Implications for the Overall Science
V2.116 sharpens the Λ_bare = 0 argument from “E_vac and α have the same field-type ratio” (V2.115) to “E_vac and α are computed from the same field-independent coupling matrix K_l, making their ratio a geometric invariant.” This is stronger because:
- It explains WHY the aggregate identity holds (not just that it does)
- It shows the identity is structural, not approximate
- It identifies entanglement concentration (one mode per channel) as the mechanism
Combined with V2.115’s BSM spectroscopy, the program now has:
- A 4% (or 0.27%) prediction of Λ/Λ_obs
- A structural proof that Λ_bare is geometric (not independent)
- Falsifiable predictions about BSM field content
- Consistency across black hole and cosmological horizons (V2.107–V2.114)
Technical Notes
- Lattice: Lohmayer radial chain, N = 40–150, l = 0–40
- Entanglement spectrum: symplectic eigenvalues of √(X_sub P_sub)
- Modular energy: ⟨K_mod⟩ = Σ_k β_k ν_k where β_k = ln((ν_k+1/2)/(ν_k-1/2))
- Physical subsystem energy: ⟨H_sub⟩ = (1/2)(tr(P_sub) + tr(K_sub X_sub))
- Runtime: 0.1 seconds
- All 13 tests pass