Version 6: The Swygert Theory of Everything AO / V = E·Y: Substrate Modulation with Inflationary Priors, EFT Implementation, and n-Point Forecasts
V = E·Y: Substrate Modulation with Inflationary Priors, EFT Implementation, and n-Point Forecasts
Abstract
We refine V = E·Y—observables arise when encoded equilibrium operators act on primordial opportunity —into a testable cosmological model with microphysical priors and concrete analysis paths. Building on variance-level encoding and one-loop/EFT nonlinearities, we (1) derive inflation-based priors for the log-periodic modulation , (2) specify IR-resummed EFT-of-LSS implementation for , (3) extend to bispectrum forecasts for resonant non-Gaussianity, and (4) provide model selection criteria that distinguish substrate modulation from smooth CPL dark energy and CDM. We state hard falsifiability thresholds aligned with DESI DR3 / Euclid DR1.
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1. Setup and Notation
Core law (variance level):
P(k,z)=E(z,k)\,Y(k)+\mathcal{N}(E,Y),\quad
E(z,k)=[D(z)T(k)]^2\,f_{\text{sub}}(z,k),\quad Y(k)=P_{\rm prim}(k).
Nonlinear term (schematic):
\mathcal{N}_{1\text{-loop}}=\!\int\! d^3q\,F_2^2(\mathbf{q},\mathbf{k-q})P_{\rm lin}(q)P_{\rm lin}(|\mathbf{k-q}|)\,+\,\mathcal{N}_{\rm EFT}.
Substrate modulation (log-periodic):
f_{\text{sub}}(z,k)=1+\epsilon\cos\!\big(\beta\ln k+\phi\big)(1+z)^{-\nu}.
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2. Inflationary Microphysics → Parameter Priors
We motivate via resonant inflation/axion-monodromy–type dynamics:
V(\phi)=\tfrac{1}{2}m^2\phi^2+\Lambda^4\cos(\phi/f)\;\Rightarrow\;
P_{\rm prim}(k)\propto k^{n_s-1}\!\left[1+\epsilon_\star\cos\!\big(\beta\ln(k/k_\star)+\phi\big)\right].
Amplitude : small-feature regime ⇒ (broad, theory-driven to avoid strong CMB constraints; tightened by joint CMB+LSS fits).
Frequency : at horizon crossing; take (log-space oscillations resolvable in LSS; very high damped by transfer/EFT).
Phase : uninformative prior .
Redshift exponent : slow dilution of modulation in late growth ⇒ (prior allows modest time evolution).
> These are theory priors, not data-informed posteriors; analyses should report prior→posterior flow explicitly.
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3. Nonlinear Accuracy: IR-Resummed EFT Implementation
To achieve sub-percent predictions in :
(a) Wiggle/no-wiggle split:
P_{\rm lin}(k)=P_{\rm nw}(k)+P_{\rm w}(k),\quad
P_{\rm w}(k)\to e^{-k^2\Sigma^2/2}P_{\rm w}(k),
(b) EFT counterterms:
\mathcal{N}_{\rm EFT}=2\,c_s^2\,k^2\,P_{\rm lin}(k) + \text{higher orders},
(c) Substrate insertion: apply to the wiggle channel (most sensitive to oscillations):
P_{\rm w}(k)\;\mapsto\; e^{-k^2\Sigma^2/2}\,f_{\text{sub}}(z,k)\,P_{\rm w}(k),
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4. Beyond 2-Point: Resonant Bispectrum Forecast
Tree-level matter bispectrum:
B(k_1,k_2,k_3)=2F_2(k_1,k_2)P_{\rm lin}(k_1)P_{\rm lin}(k_2)+\text{cyc}.
B_{\rm res}(k_1,k_2,k_3)\propto f_{\rm NL}^{\rm res}\,
\frac{\sin\!\big[\beta\ln\!(k_t/k_\star)+\phi\big]}{(k_1k_2k_3)^2}\;,\quad k_t\!=\!k_1\!+\!k_2\!+\!k_3.
SNR forecast (schematic):
\mathrm{SNR}^2=\sum_{\{k\}}\frac{\big[B_{\rm res}(\vec k)\big]^2}{\mathrm{Var}[B(\vec k)]}\;\;\text{with}\;\;\mathrm{Var}[B]\approx s\,\frac{(2\pi)^3}{V}\,P_{\rm tot}(k_1)P_{\rm tot}(k_2)P_{\rm tot}(k_3),
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5. Distinguishing from CPL DE and CDM
Key difference: smooth or extra neutrino mass cannot create log-periodic features in . We therefore propose nested model comparison:
Models:
: ΛCDM(+EFT);
: CPL (+EFT);
: ΛCDM+ (+EFT);
: substrate (+EFT).
Evidence & Bayes factors: compute .
Require (decisive) for claim of substrate detection; to falsify .
Frequentist cross-check: look for periodogram peaks in residuals of and oscillatory templates in , controlling look-elsewhere effects via prior.
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6. Concrete Analysis Recipe (CLASS/CAMB + EFT)
1. Primordial spectrum: enable oscillatory with .
2. Transfer/growth: standard Boltzmann output .
3. IR resummation: BAO wiggle/no-wiggle split; apply .
4. EFT counterterms: fit per bin.
5. Substrate insertion: multiply wiggle term by .
6. Likelihoods: DESI DR2/3 , RSD; Euclid DR1 lensing + bispectrum (mock covariance).
7. Parameters: .
8. Outputs: posteriors + against , , .
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7. Updated Predictions with Priors
Oscillatory BAO residuals:
in ;
with and damping from IR/EFT.
Scale-dependent growth:
\gamma(k)\approx \gamma_0+\delta\gamma\,\cos(\beta\ln k+\phi),\quad
\gamma_0\approx 0.57,\; |\delta\gamma|\lesssim \mathcal{O}(10^{-2}),
Void statistics: slope plus ellipticity skewness correlated with of the surrounding spectrum (distinct from log-normal ΛCDM).
Bispectrum: resonant with oscillations; forecast SNR for few, given Euclid volume and (to be validated in mocks).
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8. Hard Falsifiability (unchanged, now tied to )
Falsify substrate modulation if any holds:
DESI DR3 P(k): no periodic peak in residuals with amplitude over and .
Euclid DR1 growth: consistent with constant (no k-dependence) and .
Euclid voids: no ellipticity skewness beyond ΛCDM mocks and .
Euclid bispectrum: no oscillatory template detection at and .
Passing any one “no-signal + decisive Bayes” test rules out the substrate model under the stated priors.
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9. Discussion and Scope
Ansatz specificity: now tied to a concrete inflation sector; priors restrict flexibility.
Small-scale fidelity: IR-resummed EFT specifies damping/counterterms; extendable to two-loop if needed.
Universality: cosmology is fully worked; cross-domain mappings (thermo/QFT) remain heuristic and are not used for inference here.
Distinctiveness: periodicity in and -dependent are not produced by smooth CPL or CDM.
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10. Conclusion
Version 6 pins V = E·Y to: inflation-motivated with priors, an IR-resummed EFT pipeline usable today, and n-point forecasts (bispectrum) that yield unique, falsifiable signatures. With decisive Bayes thresholds pre-declared, DESI DR3 and Euclid DR1 will either validate a substrate-encoded extension or falsify it cleanly.
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