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CLASS_SYMT — Afterglow Dark Energy

Afterglow Dark Energy

An independent derivative of the CLASS Boltzmann code (not a fork) implementing Afterglow Dark Energy:

T. G. Martin and I.-G. Koh, Afterglow Dark Energy: Apparent Phantom Crossing from Hidden Confinement, Tested Against Planck, DESI DR2, and Pantheon+, submitted to PDU (2026). SSRN: Preprint on SSRN · Code archive DOI: DOI

Link to Preprint

The model in brief

If gravity is a macroscopic thermodynamic equation of state in Jacobson's sense, a Lorentz-invariant equilibrium vacuum contributes no null heat flow and drops out of the source law; cosmic acceleration then requires a medium that is persistently out of equilibrium. This model supplies one. A hidden pure SU(2) sector confines at a dynamically generated meV scale, and the gapped post-confinement phase is described causally (Müller–Israel–Stewart) by a memory variable Σ with relaxation time c_D/H. The homogeneous branch gives ρ_X = 3c_DΣ and an intrinsic, non-phantom equation of state

w_X = −1 + 1/(3c_D)        (accelerating for c_D > 1/2, never phantom)

Matter loading renormalises the relaxation rate through one fixed signed kernel,

Ψ(r) = 4r(r−1)/(1+r)³,     r = ρ_c/ρ_X,

whose zero sits at matter–dark-energy equality. That single structure fixes the exchange law Q = −(β/c_D) H Ψ(r) ρ_X, its sign reversal at equality, and an effective equation of state w_eff = −1 + [1 − βΨ(r)]/(3c_D) that can appear to cross −1 while the physical fluid never does. One amplitude, β, carries the interaction; the data resolve the ratio g ≡ β/c_D. Two negatives are derived rather than assumed: the intrinsic sector cannot cross the phantom divide, and the interaction cannot solve the coincidence problem (no fixed point of the density-ratio flow exists below g* ≈ 0.7).

Status: Phase 3 constraints (2026)

Planck NPIPE CamSpec TTTEEE + low-ℓ + lensing, DESI DR2 BAO, and Pantheon+, three converged MCMC branches (Cobaya, R−1 ≤ 6.7×10⁻³):

  • the isolated β = 0 branch survives the full stack;
  • g ≡ β/c_D < 0.20 at 95% credibility, set through geometry and the CMB;
  • reconstructed transition amplitude ε_Σ = 0.012 (+0.023 / −0.008);
  • Bayesian evidence vs ΛCDM inconclusive on all branches, |Δlog Z| < 1, with a mild lean toward finite c_D.

Posterior summaries, per-branch marginals, and the ledger of what these chains do and do not support: phase3_summary.md. The growth-channel extension (Phase 3.5) is pre-registered, with priors fixed in the paper's Appendix F and timed to the DESI 2025–2026 releases.

Quick start

make clean; make -j class
./class afterglow.ini          # ΛCDM-compatible defaults
python -m pytest test/         # 65 assertions, background + perturbations

Tag afterglow (commit b9d78d9) is the exact state behind the paper's chains.

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Key equations implemented (numbering follows the SSRN preprint)

Eq. Meaning
(31) Intrinsic EoS w_X = −1 + 1/(3c_D)
(32) Density ratio r = ρ_c/ρ_X
(35) Signed kernel Ψ(r)
(37)–(38) Loading–unloading relaxation law
(42) Derived exchange law Q
(44)–(45) Background continuity equations
(47) Effective equation of state w_eff
(84), (86)–(88) Stabilised closure and perturbation system
(65), (56) Source-free scaling and late-time asymptotics

Numbers refer to the preprint (SSRN 10.2139/ssrn.7097478). In-code comments reference the working draft's numbering; the mapping is maintained in PLAN_AFTERGLOW.md.

Conventions

Synchronous gauge, CLASS normalisations. The glue functions return d/dN with N = ln a; relate to cosmic time by d/dt = H · d/dN.

Citing

Publications using this code should cite the reference paper above and CLASS II (D. Blas, J. Lesgourgues, and T. Tram, JCAP 07 (2011) 034). Chains produced with the pipeline should also cite Cobaya (J. Torrado and A. Lewis, JCAP 05 (2021) 057).

License and attribution

Original CLASS portions remain under the CLASS authors' terms, free use with citation of CLASS II; the afterglow modifications are MIT, © 2025–2026 T. G. Martin and I.-G. Koh. See LICENSE and ATTRIBUTION.md.

Contact

Tom.Martin@suffolk.edu · issues welcome via the tracker.

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