Experiments / V2.306
V2.306
Deriving Λ_bare = 0 COMPLETE

V2.306 - Symplectic Spectral Flow — Per-Mode QNEC Structure

V2.306: Symplectic Spectral Flow — Per-Mode QNEC Structure

Motivation

The QNEC gives d²S/dn² = 8πα − δ/n² (2 terms, asymptotically). This is a sum over all symplectic modes: d²S = Σ_k d²s_k. Does each mode contribute a 2-term structure, or does the 2-term form emerge only from the sum?

If per-mode → Λ_bare=0 is a fundamental per-mode constraint. If emergent → Λ_bare=0 relies on collective cancellation across modes.

Method

Track symplectic eigenvalues ν_k(n) as subsystem size n varies from 8 to 27. For each mode k, compute per-mode entropy s_k(n) = (ν_k+½)ln(ν_k+½) − (ν_k−½)ln(ν_k−½), then fit d²s_k to:

  • 2-term: A_k + B_k/n²
  • 3-term: A_k + B_k/n² + C_k·ln(n)/n²

Modes are tracked by rank (top-1 = largest ν, top-2 = second largest, etc.).

Key Results

1. Two Classes of Modes

The symplectic eigenvalues split into two distinct populations:

Bulk modes (top-1 through top-5 at l=5): Well-separated from ν=0.5, with ν_max ≈ 0.517. These carry essentially all the entanglement entropy.

ModeR² (2-term)R² (3-term)C_k (log coeff)
top-10.99900.999988.7×10⁻³
top-20.99791.000001.4×10⁻²
top-30.99210.999813.3×10⁻²
top-40.98210.999305.9×10⁻²
top-50.95610.994651.1×10⁻¹

Edge modes (top-6 through top-8): Near ν=0.5, appearing/disappearing as n changes.

ModeR² (2-term)R² (3-term)
top-60.2040.546
top-70.2240.252
top-80.0980.129

2. Per-Mode Structure Needs a Log Term

For bulk modes, the 2-term model (A + B/n²) achieves R² > 0.95, but adding a log correction (A + B/n² + C·ln(n)/n²) pushes R² to 0.999–1.000. The true per-mode structure is:

d²s_k = A_k + B_k/n² + C_k·ln(n)/n²

This 3-parameter structure holds across all channels tested:

lModeR² (2-term)R² (3-term)
0top-10.99941.000000
0top-20.99990.999999
2top-10.99851.000000
5top-10.99910.999998
10top-10.99970.999916
20top-10.96700.999905

The log term C_k grows for deeper modes (top-1 → top-5) and for higher l.

3. Edge Modes Are Chaotic

Modes near ν = 0.5 (the entanglement ground state) have erratic d²s_k because:

  • New modes “activate” (cross from ν = 0.5 to ν > 0.5) as n increases
  • This creates discontinuities in the per-mode tracking
  • The edge modes have POSITIVE B_k (opposite sign to bulk modes)

At l=5, bulk modes have B_k ≈ −0.04 to −0.07, while edge modes have B_k ≈ +0.04 to +0.13. Partial cancellation between bulk and edge modes occurs in the total.

4. Sum Rule

For l=3, summing per-mode parameters and comparing to the total:

  • Σ A_k vs A_total: 89% error
  • Σ B_k vs B_total: 9.1% error

The A sum rule fails badly because the total 2-term fit itself is poor (R² = 0.78 for single-channel total at l=3). The per-mode decomposition is mathematically exact (d²S = Σ d²s_k), but fitting each piece independently introduces compounding errors from the edge modes.

5. Channel Dependence

lTotal R² (2-term)Top-1 R² (2-term)
00.9990.999
20.9420.999
50.5530.999
100.0601.000
200.0790.967

Low-l channels have clean total 2-term structure. High-l channels do not — the edge mode contamination dominates. The FULL QNEC (summed over all l with degeneracy 2l+1) must reconstruct the 2-term form through massive cancellation across channels.

6. Full QNEC at C=5

Summing over all channels with degeneracy (2l+1):

  • 2-term: α = 0.0671, δ = −16.3, R² = 0.365
  • 3-term (with log): R² = 0.518

The R² is low because n = 10–23 at C = 5 is below the asymptotic regime. The 2-term structure emerges only at larger n (known from V2.250, V2.296).

Physical Interpretation

The 2-Term QNEC Structure is EMERGENT

The per-mode structure is 3-parameter (A_k + B_k/n² + C_k·ln(n)/n²), not 2-parameter. The ln(n)/n² term is individually significant for each mode (improving R² from 0.99 to 0.99999).

The 2-term structure d²S = A + B/n² for the TOTAL entropy arises because:

  1. The ln(n)/n² contributions from bulk modes partially cancel
  2. Edge mode contributions (opposite sign B_k) partially cancel bulk modes
  3. The sum over channels with (2l+1) degeneracy provides further cancellation

This means Λ_bare = 0 (which follows from 2-term completeness) is a collective property of the entanglement spectrum, not a per-mode constraint. No individual mode “knows” that Λ_bare = 0 — it emerges from the conspiracy of all modes.

Connection to Trace Anomaly

The per-mode log term C_k·ln(n)/n² is reminiscent of the trace anomaly contribution to entanglement entropy (the δ·ln(A) term). At the per-mode level, the anomaly manifests as a ln(n)/n² correction to d²s_k. When summed:

  • Σ B_k → δ (the log coefficient)
  • Σ C_k·ln(n) → absorbed into the effective δ

The total δ is a sum over modal contributions that include both B_k and C_k·ln(n) terms.

Implications for Λ_bare = 0

This result slightly WEAKENS the Λ_bare = 0 argument from QNEC completeness. The 2-term structure (V2.250, V2.257) is exact in the total but emergent from a richer per-mode structure. This means:

  • The “no room for Λ_bare” argument applies to the TOTAL entropy, not per-mode
  • A subtle modification (adding Λ_bare) could potentially be absorbed into the per-mode log terms without changing the total structure
  • The constraint is less rigid than if each mode independently demanded 2 terms

However, the argument remains valid at the level of the total entropy: the map {α, δ} → {G, Λ} is bijective, and the TOTAL d²S has exactly 2 macro-scale terms asymptotically.

Honest Assessment

Achieved

  • First decomposition of QNEC into per-mode symplectic contributions
  • Discovered per-mode needs 3 parameters (A + B/n² + C·ln(n)/n²), not 2
  • Identified two mode populations: bulk (clean) and edge (chaotic)
  • Established that 2-term QNEC structure is emergent, not fundamental
  • The 3-term per-mode structure achieves R² = 0.99999+ for bulk modes at l=0

Not Achieved

  • Cannot quantify how the log terms cancel in the full channel sum (would need larger n, C)
  • Edge mode tracking is inherently noisy (modes appear/disappear)
  • Sum rules have significant errors due to edge mode contamination
  • Does not resolve whether a Λ_bare slot could hide in the per-mode log terms