V2.255 - GSL with Nonzero Λ_bare — Second Law Cannot Constrain Λ_bare
V2.255: GSL with Nonzero Λ_bare — Second Law Cannot Constrain Λ_bare
Status: COMPLETE — 27/27 unit tests, 10/10 experiment tests
Motivation
Approach D of the RESEARCH_GUIDE asks: does Λ_bare ≠ 0 violate the generalised second law (GSL) at the cosmological horizon? V2.250 briefly checked this and found the GSL is satisfied for all positive Λ. This experiment performs the full analysis: cosmic evolution through radiation → matter → de Sitter eras, entropy accounting in physical Planck units, and a systematic scan over Λ_bare values.
Method
Friedmann dynamics
Standard ΛCDM: H²/H0² = Ω_r/a⁴ + Ω_m/a³ + Ω_Λ_total, where Ω_Λ_total = R + Λ_bare_frac × Ω_Λ_obs. The framework predicts R = |δ|/(6α) ≈ 0.665 (SM) or 0.688 (SM+grav) as the entanglement contribution.
Entropy in Planck units
S_gen = α A_H + δ ln(A_H), where A_H is the physical apparent horizon area in Planck units: A_H = 4π/(H_phys²) with H_phys = H_dimless × H0_Planck.
Physical scale: A_H(today) ≈ 9.0 × 10¹²² l_P².
GSL condition
dS/dt = (α + δ/A_H) × dA_H/dt ≥ 0
This requires either:
- dA/dt ≥ 0 and α + δ/A_H > 0 (standard case), OR
- dA/dt ≤ 0 and α + δ/A_H < 0 (only possible at Planck scale)
Results
1. GSL holds for ALL Λ_bare values
| Λ_bare/Λ_obs | Ω_Λ_total | GSL violations | ΔS (l_P²) |
|---|---|---|---|
| -0.9 | 0.048 | 0 | 5.2 × 10¹²⁴ |
| -0.5 | 0.322 | 0 | 7.8 × 10¹²³ |
| 0.0 | 0.665 | 0 | 3.8 × 10¹²³ |
| 1.0 | 1.349 | 0 | 1.9 × 10¹²³ |
| 5.0 | 4.088 | 0 | 6.1 × 10¹²² |
| 10.0 | 7.512 | 0 | 3.3 × 10¹²² |
Zero violations across all eras (radiation, matter, transition, de Sitter) for every Λ_bare value tested.
2. Why the GSL is trivially satisfied
The critical area where the log term could compete with the area term is:
A_crit = |δ|/α ≈ 4.0 l_P²
The smallest cosmological horizon in the evolution (at a = 10⁻⁶) is:
A_min ≈ 9.9 × 10¹⁰² l_P²
The ratio A_min/A_crit ≈ 2.5 × 10¹⁰². The log correction contributes 4.4 × 10⁻¹²³ of the area term at the present epoch. The GSL is satisfied by a margin of 10¹²² orders of magnitude.
3. First law vs second law
| Law | Constraint on Λ_bare | Strength |
|---|---|---|
| First (QNEC) | Λ_bare = 0 exactly | EXACT |
| Second (GSL) | None | Trivially satisfied |
The first law (V2.250) constrains Λ_bare through S”(n) = 8πα - δ/n², which has exactly two terms uniquely fixing G and Λ. The second law provides no constraint because the cosmological horizon is 10¹²² times larger than the critical scale.
4. When could GSL fail?
Two scenarios (neither occurs in ΛCDM):
- Planck-scale horizons: A_H < |δ|/α ≈ 4 l_P² — never in cosmology
- Phantom dark energy: w < -1 causes dA/dt < 0 — not in standard model
5. Friedmann consistency (repeated from V2.250)
| Model | Ω_Λ predicted | Deviation from obs |
|---|---|---|
| SM (R = 0.665) | 0.665 | 2.8σ |
| SM+grav (R = 0.688) | 0.688 | 0.4σ |
Λ_bare needed to match observations:
- SM: Λ_bare = 0.029 × Λ_obs (2.8σ tension)
- SM+grav: Λ_bare = -0.005 × Λ_obs (0.4σ, consistent with zero)
Key Findings
The GSL does not constrain Λ_bare — CONFIRMED
This is a negative result for Approach D: the second law of thermodynamics at the cosmological horizon cannot distinguish Λ_bare = 0 from Λ_bare ≠ 0. The reason is quantitative: the log correction δ that determines Λ is 10⁻¹²³ of the area term α that determines G. The GSL is dominated by the area term and is insensitive to the log correction.
The paradox of the log term
The log correction is:
- Negligible for the second law (10⁻¹²³ of the area term in dS/dt)
- Essential for the first law (determines Λ through S”(n) = 8πα - δ/n²)
This is not a contradiction. The first law (QNEC) probes the functional form of S(n) — specifically its second derivative — which separates the constant and 1/n² contributions cleanly regardless of their relative magnitude. The second law only checks the sign of dS/dt, which is dominated by the area term.
Implications
- Approach D (GSL) is closed: The GSL cannot derive Λ_bare = 0.
- Approach D.2 (modular flow) remains possible but needs separate analysis.
- The constraint hierarchy is established:
- QNEC (first law): determines G AND Λ, forces Λ_bare = 0
- GSL (second law): trivially satisfied, no constraint
- This parallels ordinary thermodynamics where the first law (energy conservation) is more constraining than the second (entropy increase).
Files
src/gsl_analysis.py: Friedmann dynamics, GSL computation, critical analysistests/test_gsl.py: 27 unit tests (all passing)run_experiment.py: 10-test experiment across 9 partsresults/summary.json: Full numerical results
Significance for the Framework
This experiment closes the GSL branch of Approach D. Together with V2.252 (closing Approach C), the derivation of Λ_bare = 0 now rests firmly on two pillars:
- Approach B (V2.249/251): Modular Hamiltonian double-counting (operator-level)
- Approach D via QNEC (V2.250): Entropy completeness (first law)
The remaining open experiment from the RESEARCH_GUIDE is D.2: Modular flow inconsistency — testing whether Λ_bare ≠ 0 contradicts Bisognano-Wichmann modular flow at the cosmological horizon.