Reactive Substrate Theory (RST): Cosmology and Provisional Priors — Unified Review
Reactive Substrate Theory (RST): Cosmology and Provisional Priors — Unified Review
Introduction
Reactive Substrate Theory (RST) is a non‑standard theoretical physics model proposing that all of reality emerges from a single, continuous, elastic Substrate (S) field. While unconventional, RST can be checked against cosmological observations. This unified article combines two posts:
- Post 1: Plugging known RST values into the substrate–cosmology picture
- Post 2: Appendix: Provisional RST numeric priors
Together, they show how RST can reproduce key features of the standard cosmological model (ΛCDM) and outline numeric priors that make RST predictive and testable.
Part 1 — Plugging known RST values into cosmology
This section demonstrates that the core dynamics of RST replicate the successes of ΛCDM without requiring a true cosmological constant. It uses an effective fluid description for the substrate tension component.
- Dark energy equivalence: The substrate tension uses an equation‑of‑state parameter wS ≈ −0.95. This causes the substrate tension density ρS to dilute extremely slowly with redshift, effectively mimicking dark energy.
- Cosmic balance: Assuming a transition redshift zt ≈ 0.34 where matter density equals substrate tension density, the inferred present‑day fractions are ΩS0 ≈ 0.69 and Ωm0 ≈ 0.30, matching the observed matter–dark energy split.
- Accelerated expansion: The present‑day deceleration parameter is q0 ≈ −0.49, indicating robust cosmic acceleration consistent with observations.
- Nonlinear dynamics: The substrate field equation
∂t2S − c2∇2S + βS3 = …
includes a cubic term βS3 that introduces amplitude‑dependent stiffness, suggesting potential, testable gravitational‑wave dispersion on cosmological scales once β is determined.
Key outcomes from Part 1
- Energy fractions reproduced: ΩS0 ≈ 0.69 and Ωm0 ≈ 0.30
- Acceleration reproduced: q0 ≈ −0.49
- Interpretation difference: Acceleration arises from substrate tension, not a cosmological constant
Part 2 — Appendix: Provisional RST numeric priors
This section provides educated, provisional numeric values ("priors") for constants needed to make RST quantitative and testable. These are starting points, not measurements.
| Symbol | Description | Provisional Value | Interpretation |
|---|---|---|---|
| β | Nonlinear elasticity constant | ≈ 1 × 10−26 m−2·J−1 | Nonlinear effects (e.g., GW dispersion) appear on horizon scales, not locally. |
| S0 | Field amplitude today | ≈ 2.3 × 10−5 J1/2·m−3/2 | Normalizes the current background state of the Substrate field. |
| cs,S | Effective sound speed of substrate component | ≈ 0.97c | Near‑stiff response on large scales in the effective fluid picture. |
| kNL | GW dispersion crossover wavenumber | ≈ 7.7 × 10−27 m−1 | Scale where deviations from luminal GW propagation could appear. |
Additional working values used
- Equation of state: wS ≈ −0.95
- Transition redshift: zt ≈ 0.34
- Present‑day fractions: ΩS0 ≈ 0.69, Ωm0 ≈ 0.30
- Deceleration parameter: q0 ≈ −0.49
RST vs. ΛCDM — alignment and differences
| Topic | RST (Reactive Substrate Theory) | ΛCDM (Standard Cosmology) |
|---|---|---|
| Acceleration driver | Substrate tension with wS ≈ −0.95 | Cosmological constant Λ with w = −1 |
| Energy fractions today | ΩS0 ≈ 0.69; Ωm0 ≈ 0.30 | ΩΛ ≈ 0.69; Ωm0 ≈ 0.30 |
| Onset of acceleration | zt ≈ 0.34 | zt ≈ 0.3–0.7 (data/model dependent) |
| Singularities | Elastic limits avoid infinities (finite cores, bounce) | Classical GR allows singularities (quantum gravity may resolve) |
| GW propagation | Potential horizon‑scale dispersion from βS3 | Luminal in GR; modifications only with new physics |
Unified conclusions
- Viability in principle: With wS ≈ −0.95 and zt ≈ 0.34, RST reproduces the observed energy split and acceleration without a cosmological constant.
- Distinctive interpretation: Acceleration is due to substrate tension rather than Λ, aligning with data while changing the underlying picture.
- Testable predictions: The βS3 nonlinearity suggests horizon‑scale gravitational‑wave dispersion that could be probed with cosmological datasets.
- Next steps: Calibrate β and the matter coupling via supernovae, BAO, CMB, and GW observations to distinguish RST from ΛCDM.
Publishing note
This unified review is designed for clarity and comparability. It ties RST’s effective fluid behavior to mainstream cosmology, lists working numeric priors, and outlines concrete tests to move from qualitative viability to quantitative validation.