← All Papers  ·   Cosmology  ·  V0.1

Dark Energy as Geometry: The Selective Transient Field Framework and the T² Causal Diamond

Z. Paz  ·  ORCID 0009-0003-1690-3669 V0.1 2026
Download PDF

Abstract

We present the dark energy sector of the Selective Transient Field (STF) framework — a unified scalar-field theory in which dark matter and dark energy emerge from the same scalar field, the breathing mode of six compact extra dimensions in a 10D Einstein-Gauss-Bonnet compactification on a Calabi-Yau threefold (CICY #7447) with Z₁₀ free quotient structure. The STF scalar has mass m_s = 3.94 × 10⁻²³ eV and coupling ζ/Λ = 1.35 × 10¹¹ m², both derived from first principles. The dark energy component arises from the residual potential energy V(φ_min) at the stabilized modulus, modulated by the T² causal-diamond integral α(θ) = ∫₀^θ cos²(θ’)dθ’. The current epoch is identified with θ = π/2 by the geometric condition |R₀|/c² = 4Λ_eff (Paz 2026a, §III.E Prediction 6), which gives Ω_m = 4/(3(1+π)) ≈ 0.322 — within 1σ of Planck 2018 (0.315 ± 0.007) and consistent with DESI DR1/DR2 (0.295–0.307, model-dependent). The third-order tangency dα/dθ|_{π/2} = cos²(π/2) = 0 forces Λ̇_eff = 0 at the current epoch, predicting w(z=0) = −1 exactly (independent of the compactification time-scale T_compact). At earlier epochs θ < π/2 the coupling was accumulating, giving an effective phantom trajectory w(z) < −1 for all z > 0 (sign rigorous; magnitude conditional on T_compact, see Paz 2026c §6.1) without a phantom crossing. The STF is a DHOST Class Ia theory with positive scalar kinetic energy and c_T = c exactly (GW170817-compatible, Paz 2026a §C.6); the apparent phantom behaviour is effective, arising from T² geometric coupling accumulation, not fundamental ghost behaviour. The same nodal structure that gives w₀ = −1 also gives c_s²(z=0) = 1 exactly (Paz 2026c §6.3) — perturbation stability paired with the equation-of-state result. We conduct a systematic comparison with eight competing dark energy frameworks: the cosmological constant Λ, quintessence, k-essence, phantom dark energy, w₀wₐCDM (CPL parameterization), early dark energy, scalar-tensor dark energy (Horndeski/DHOST), and emergent dark energy models. We compile and contextualize recent observational evidence: (i) the 2.8–4.2σ statistical preference for w₀wₐCDM over ΛCDM in DESI DR2 + CMB + SNe combined fits (Adame et al. 2024, Karim et al. 2025), with best-fit indicating evolving dark energy (w₀ > −1 today, wₐ < 0); (ii) the Euclid Quick Data Release Q1 (March 2025) sky coverage of 63 deg² as a precursor to its first cosmology release (October 2026); (iii) recent debates about the prior dependence of the DESI w₀wₐ result (Cortês & Liddle 2024, 2025); and (iv) alternative interpretations including coupled dark sector models (Roy Choudhury et al. 2025) and evolving dark matter scenarios (Chen & Loeb 2025). The DESI DR2 best-fit trajectory — apparent quintom-B (w<-1 in past, crossing to w>-1 today) — is structurally opposite to the STF prediction (no crossing; monotonic phantom for z > 0; w₀ = −1 exactly). We treat this as a serious observational tension that the framework must address honestly: if direct measurements confirm the quintom-B sign, the T² nodal structure is falsified at >3σ. The framework’s structural prediction is that w₀ = −1 lies exactly on the cosmological constant, with all evolution into the past. Euclid’s first cosmology release (October 2026) will be decisive. We also address theoretical aspects: the GW170817 constraint c_T = c (satisfied structurally by G₄X = 0); the no-go theorem for fundamental phantoms (evaded by DHOST Class Ia structure); the relationship to the DESI w₀wₐ best-fit (categorically different mechanism — STF’s effective phantom is monotonic, DESI’s CPL is a parametrization artifact of strongly anticorrelated posteriors). We present six testable predictions, three falsifiability classes (rigorous-structural, conditional-magnitude, derived-extension), and a prediction-dependency map indicating which observables survive if any single component fails. The unified dark sector picture — one scalar field producing both the dark-matter equation of state ⟨w⟩ = 0 (Paz 2026d) and the dark-energy structural prediction w(z=0) = −1 — is structurally over-constrained relative to a fitted dual-component model. Of the framework’s testable predictions, the structural prediction w(z=0) = −1 exactly is the most distinctive: it is independent of T_compact, derives from T² differential topology rather than parameter fitting, and is the single most directly testable element of the framework against forthcoming Euclid data.

Keywords: dark energy, equation of state, T² causal diamond, third-order tangency, DHOST Class Ia, GW170817, phantom dark energy, scalar field cosmology, DESI w₀wₐCDM, Euclid mission, Calabi-Yau compactification, ghost-free scalar-tensor gravity, effective phantom without ghost, unified dark sector, cosmological constant problem


I. Introduction

The accelerating expansion of the universe, discovered through Type Ia supernova observations (Riess et al. 1998, Perlmutter et al. 1999), has been cosmology’s most enduring puzzle for over a quarter century. The simplest description — a cosmological constant Λ — fits the data well but raises three deep theoretical problems.

The cosmological constant problem. Quantum field theory naively predicts a vacuum energy density ~10¹²² times larger than observed (Weinberg 1989). No accepted derivation of the observed value from microphysics exists. The vast disparity between predicted and observed scales is among the most severe fine-tuning problems in physics.

The coincidence problem. Within ΛCDM, dark matter and dark energy densities differ by orders of magnitude at most cosmic epochs but happen to be comparable now, with Ω_m ≈ 0.32 and Ω_Λ ≈ 0.68. Why this near-equality occurs at the current epoch — rather than billions of years earlier or later — has no explanation in the standard framework.

The dynamical question. Is dark energy a true cosmological constant (w = −1 exactly, time-independent), or does it evolve? If it evolves, does it cross the phantom boundary w = −1, and if so, in which direction?

The Dark Energy Spectroscopic Instrument (DESI) Year-1 BAO results (Adame et al. 2024) and the Year-2 Data Release (Karim et al. 2025) have transformed the empirical landscape on this question. Combined fits of DESI BAO with cosmic microwave background distance priors and Type Ia supernova compilations (Pantheon+, DES Year-5, Union3) now show a 2.8–4.2σ statistical preference for the w₀wₐCDM parameterization over a constant Λ. The best-fit shows w₀ > −1 today (quintessence-like at present) with wₐ < 0 (phantom in the past), indicating an apparent quintom-B trajectory with phantom crossing in the recent past. If confirmed, this would be the most significant empirical development in cosmology since the discovery of acceleration itself.

However, the result is contested. Cortês & Liddle (2024, 2025) demonstrated that the DESI Bayesian preference for w₀wₐCDM is sensitive to the priors imposed on w₀ and wₐ — extending the lower bounds beyond −4.6 (for w₀) and −5 (for wₐ) reverses the preference toward ΛCDM. Roy Choudhury et al. (2025) showed that updating the CMB likelihood from Planck PR3 to PR4 weakens the dynamical-dark-energy preference. Chen & Loeb (2025) proposed that the DESI signal can be reproduced by an evolving dark matter component rather than evolving dark energy. The empirical case for dynamical dark energy is suggestive but not yet conclusive.

The Euclid space telescope (launched July 2023, beginning its cosmological survey February 2024) will provide the next major step. Its Quick Data Release Q1 (March 2025) covered 63 deg² — a precursor to the first cosmology data release in October 2026, which will probe dark energy through a combination of weak gravitational lensing, galaxy clustering, and BAO measurements over much wider sky coverage than DESI.

This paper presents the dark energy sector of the Selective Transient Field (STF) framework — a unified scalar-field theory in which dark matter and dark energy emerge from the same scalar field. The STF was developed primarily as a UV-complete model of dark matter, deriving from a 10D Einstein-Gauss-Bonnet compactification on the Calabi-Yau threefold CICY #7447 with Z₁₀ free quotient structure (Paz 2026a, hereafter “the First Principles paper”). The dark-matter aspects of the framework are presented in Paz 2026d (“Dark Matter as Geometry: The STF Framework for a Unified Dark Sector”); the present paper is its parallel for the dark-energy sector.

I.A Why a separate dark-energy paper

The unified-dark-sector framing might suggest that dark energy and dark matter should be addressed in a single paper. Three reasons make a separate dark-energy treatment appropriate:

(1) The observational landscapes differ qualitatively. Dark matter is constrained primarily by galactic kinematics, gravitational lensing, structure formation, and direct-detection null results. Dark energy is constrained primarily by Type Ia supernova distances, BAO from spectroscopic galaxy surveys, CMB acoustic peaks, weak lensing tomography, and (forthcoming) redshift-space distortions and 21-cm cosmology. The competing-theory landscapes are also different: ΛCDM, MOND, fuzzy DM, WDM, SIDM, superfluid DM, and emergent gravity for dark matter; cosmological constant, quintessence, k-essence, phantom, w₀wₐCDM, early DE, and scalar-tensor DE for dark energy.

(2) The structural mechanisms differ. The STF dark-matter mechanism rests on the oscillation-averaging of the scalar field at cosmological scales (giving ⟨w_DM⟩ = 0) combined with the field’s response to galactic geometry (giving the MOND phenomenology). The STF dark-energy mechanism rests on the residual potential energy at the stabilized modulus combined with the T² causal-diamond integral structure (giving the w(z=0) = −1 nodal result). These are different microphysical mechanisms within the same framework, deserving separate analysis.

(3) The observational tests are temporally separated. The dark-matter predictions test against existing rotation curves, SPARC catalog, Lyman-α constraints, and dwarf-galaxy kinematics. The dark-energy predictions test against forthcoming Euclid w(z) measurements (October 2026 first cosmology release) and DESI DR3+ analyses. The two test programs run on different timescales and require different observational synthesis.

I.B What this paper contributes

This paper makes three primary contributions to the STF framework’s publication portfolio:

(1) A self-contained dark-energy treatment. Sections II–III present the STF framework’s relevant structure for dark energy (compact summary) followed by the explicit derivation of the w(z) result from T² causal-diamond geometry. The full calculation chain is in Paz 2026c (“STF Dark Energy w(z) Derivation V0.2”); this paper presents the result in publication form with observational context.

(2) A systematic comparison with competing dark-energy theories. Section IV compares the STF prediction against eight competing dark-energy frameworks, identifying for each: the underlying mechanism, observational successes, theoretical vulnerabilities, and the specific aspects in which the STF differs. The comparison is honest — the STF is not advertised as superior in every respect, and the empirical case for STF over alternatives is qualified by the open T_compact question and the current observational tensions.

(3) Engagement with the DESI DR2 observational tension. The DESI DR2 result, if confirmed, falsifies the STF dark-energy prediction at >3σ. Section V addresses this directly: we present the DESI result honestly, discuss the prior-dependence and CMB-likelihood concerns, examine alternative interpretations, and identify the specific Euclid measurements that would be decisive. We do not minimize the tension or massage the prediction to accommodate it. The framework’s structural prediction is w₀ = −1 exactly; if the empirical case for w₀ > −1 strengthens, the framework is in serious trouble. We discuss the falsification scenarios explicitly.

I.C Roadmap

Section II presents the STF framework, focused on the elements relevant for dark energy. Section III develops the STF dark-energy sector: the residual potential, the T² causal-diamond structure, the third-order tangency, and the resulting predictions w(z=0) = −1 and c_s²(z=0) = 1. Section IV conducts the systematic comparison with eight competing dark-energy theories. Section V compiles recent observational evidence and addresses the DESI DR2 tension. Section VI provides an honest assessment of STF’s limitations. Section VII presents testable predictions with falsifiability classes and a prediction-dependency map. Section VIII discusses broader implications and the unified dark sector picture. Section IX concludes.


II. The Selective Transient Field Framework

This section summarizes the STF framework’s structure, focusing on the elements relevant for the dark-energy analysis. Comprehensive treatments are in Paz 2026a (the First Principles paper, full mathematical derivation) and Paz 2026d (the Dark Matter paper, applied phenomenology).

II.A The STF Lagrangian

The STF Lagrangian is:

$$ \mathcal{L}_{\rm STF} = -\frac{1}{2}(\partial_\mu\phi)^2 - \frac{1}{2}m_s^2\phi^2 + \frac{\zeta}{\Lambda}g(\mathcal{R})\phi(n^\mu\nabla_\mu\mathcal{R}) + \mathcal{L}_{\rm matter\ couplings} $$

where φ is the scalar field, m_s is the field mass, ζ/Λ is the coupling constant, ℛ is the Weyl/Ricci tidal scalar (regime-dependent — see §II.D), n^μ = ∇^μφ/√(2X) is the unit vector along the field gradient, and g(ℛ) is a smooth threshold function. The matter couplings include the cross-disformal coupling required for the flyby anomaly and galactic phenomenology (see Paz 2026b).

Field mass. m_s = 3.94 × 10⁻²³ eV, derived from the cosmological threshold condition 𝒟_crit = 𝒟_GR (Paz 2026a §III.D), which identifies scalar field activation at the orbital separation where binary black hole inspiral becomes cumulative — 730 R_S, corresponding to a period of T = 3.32 years via the Peters (1964) inspiral formula. The oscillation frequency is ω_s = m_s c²/ℏ = 5.98 × 10⁻⁸ rad/s.

Coupling constant. ζ/Λ = 1.35 × 10¹¹ m², derived from 10D Einstein-Gauss-Bonnet compactification on CICY #7447/Z₁₀ (Paz 2026a, Appendices L and O). The independent validation route through the Anderson flyby anomaly (Paz 2026a, Appendix B) matches the empirically measured K = 2ωR/c coefficient to 99.99% at planetary scales, with the caveat that the Anderson anomaly is itself debated (proposed conventional explanations include thermal radiation pressure and orbit-determination systematics, Anderson et al. 2008). The flyby validation provides a cross-domain check on the coupling but is not central to the dark-energy analysis: the STF dark-energy predictions follow from the cosmological-scale dynamics of φ on FRW backgrounds, independent of the flyby validation.

II.B The 10D compactification and CICY #7447/Z₁₀

The compactification chain proceeds through:

$$ S_{10} = \int d^{10}x\sqrt{|g_{10}|}\left[\frac{1}{2\kappa_{10}^2}R_{10} + \alpha_{\rm GB}\,\mathcal{G}_{10}\right] $$

with the Gauss-Bonnet term ℳ_{10} = R² − 4R_μν R^μν + R_{μνρσ}R^{μνρσ}. The breathing-mode reduction:

$$ g_{10} = e^{-\sigma(x)/\sqrt{6}}g_4(x) \oplus e^{\sigma(x)/\sqrt{6}}g_6 $$

yields a 4D Einstein frame with M_Pl² = M_{10}⁸ V_6 and canonical scalar φ = √24 M_Pl σ. The internal manifold is the Calabi-Yau threefold CICY #7447 with Z₁₀ = Z₅ × Z₂ free quotient structure (Braun 2010), yielding h¹¹(X̃) = 5 independent Kähler moduli and a smooth quotient with three generations of fermions. Within the CICY database (7,890 manifolds), #7447 is the unique manifold admitting a free Z₁₀ quotient (Paz 2026a, Appendix O.X).

The coupling ζ/Λ is the output of the only available geometry, not a selection from a landscape of alternatives. The same compactification that produces ζ/Λ and m_s is conjectured to derive Standard Model parameters through Kaluza-Klein scale ratios and loop structure (Paz 2026a, Appendices M–O). The chain extends to dark energy through the mechanism described in §III below.

II.C DHOST Class Ia and the gravitational wave constraint

The cross-disformal coupling structure places the STF in the DHOST Class Ia category (Crisostomi-Hull-Koyama-Tasinato 2017, Langlois 2019). On FLRW backgrounds, integration by parts maps the rate-coupling interaction to Horndeski L₄ form (Kobayashi 2019), with G₄X = 0 ensuring the gravitational wave speed c_T = c exactly (Paz 2026a, Appendix C.6). This is structural, not tuned — it follows from the absence of explicit (∂X)² dependence in the Horndeski-mapped form. The GW170817 constraint |c_T − c|/c < 5 × 10⁻¹⁶ (Abbott et al. 2017) is satisfied by construction.

This is critical for dark-energy theories: GW170817 rules out a wide class of scalar-tensor dark-energy models (including the original Bekenstein TeVeS, generic Horndeski with G₄X ≠ 0, and many quintessence models with non-minimal couplings), but leaves DHOST Class Ia structures viable. The STF survives this constraint structurally.

The full ghost-freedom analysis on non-stationary Kerr backgrounds (the binary inspiral regime where GW observations are made) was completed in April 2026 through an explicit ADM decomposition (Paz 2026a, Appendix C.7c). Ghost-freedom holds on arbitrary vacuum backgrounds; the STF has 2 tensor + 1 scalar degrees of freedom on all relevant backgrounds.

II.D The regime-dependent curvature operator

A subtlety important for the dark-energy analysis: the curvature scalar ℛ entering the rate operator is regime-dependent (Paz 2026a, §L.4.4). The 10D Gauss-Bonnet invariant reduces to a 4D curvature-squared combination I₄ = aR² + bR_{μν}R^{μν} + cR_{μνρσ}R^{μνρσ}. Using the standard identity R_{μνρσ}R^{μνρσ} = C_{μνρσ}C^{μνρσ} + 2R_{μν}R^{μν} − ⅓R², this separates into Weyl (C²) and Ricci (R_{μν}, R) parts. In vacuum spacetimes (flybys, binaries, galaxies), the Ricci tensor vanishes by Einstein’s equations, leaving only the Weyl tidal scalar ℛ = √(C²). In FRW cosmology, the spacetime is conformally flat so the Weyl tensor vanishes identically, leaving only Ricci terms; the simplest invariant is ℛ = |R| = |6(Ḣ + 2H²)|.

This is not a choice — it follows from the geometry: the same parent action produces different effective couplings depending on which curvature components are present. The cosmological perturbation theory therefore uses the Ricci-rate operator L_int^FRW ∝ φṘ, which is analytic and well-posed on exact FRW. This is the operator relevant for the dark-energy analysis below.

II.E Cosmological perturbation stability

The cosmological perturbation stability of the STF in the FRW tracking regime is established (Paz 2026a, §VII.E.1). The coupling enters as a slowly varying background source proportional to R ~ O(H²), not as a kinetic modification. Integration by parts gives φṘ = −φ̇R + boundary, so the interaction reduces to a source term. The dimensionless coupling strength at cosmological scales is:

(ζ/Λ) × H02 ∼ 1.35 × 1011 m2 × (2.4×10−18 s−1)2 ∼ 7.6 × 10−25

— negligible. Corrections to the kinetic coefficients of the quadratic action are suppressed by the additional factor (H/m_s)² ~ (10⁻¹⁸/10⁻⁷)² ~ 10⁻²², giving Q_s = 1 + O(H²/m_s²) and c_s² = 1 + O(H²/m_s²). This confirms no ghost, no gradient instability, and subluminal propagation at all cosmologically relevant scales: O(10⁻²⁰) at super-horizon scales, scaling as (k/am_s)² to O(10⁻¹²) at deep sub-horizon scales (k ~ 10 h/Mpc).

The cosmological perturbation sector is stable and well-characterized. This is the foundation on which the dark-energy analysis is built.

II.F What this section establishes

The STF framework, as relevant for dark energy:

  1. Has a derived scalar mass m_s = 3.94 × 10⁻²³ eV and coupling ζ/Λ = 1.35 × 10¹¹ m² with no free parameters
  2. Is a DHOST Class Ia theory with c_T = c exactly (GW170817-compatible by construction)
  3. Has ghost-freedom on all relevant backgrounds including non-stationary Kerr
  4. Uses the Ricci-rate operator L_int^FRW ∝ φṘ on FRW cosmology (regime-selected by geometry)
  5. Has cosmological perturbation stability established at leading order: Q_s > 0, c_s² = 1 + O(H²/m_s²) ~ 1 + O(10⁻²²)
  6. Has the same scalar field providing both dark-matter and dark-energy components (unified dark sector)

These are the input conditions for the dark-energy mechanism in §III.


III. The STF Dark Energy Sector

This section develops the STF prediction for dark energy: the residual potential energy V(φ_min) at the stabilized modulus, modulated by the T² causal-diamond integral, gives w(z=0) = −1 exactly with effective phantom trajectory w(z) < −1 for z > 0. The result is structural — it follows from differential topology of the T² coupling integral, not from parameter fitting.

III.A The residual potential at the stabilized modulus

The compactification chain (§II.B) produces a 4D effective theory with a stabilized volume modulus σ. The residual potential energy V(σ_min) at the stabilized minimum provides the dark energy density. In the STF framework, this is described by:

$$ \rho_{\rm DE} = V(\phi_{\min}) = V_0 \cdot f(\theta(t)) $$

where V₀ is the bare potential value (set by the compactification scale) and f(θ(t)) is a time-dependent modulation factor arising from the T² causal-diamond structure. The current dark-energy density is:

$$ \rho_{\rm DE}^0 = V_0 \cdot f(\theta = \pi/2) = \rho_{\rm crit}^0 \cdot \Omega_\Lambda $$

with Ω_Λ ≈ 0.68 from observations. The framework’s non-trivial prediction is the time dependence of f(θ(t)), not the magnitude of V₀ (which is an output of the compactification analysis and is constrained by the |R₀|/c² = 4Λ_eff self-consistency condition discussed below).

III.B The T² causal-diamond integral

The geometric coupling of the STF scalar to the T² compactification structure produces a coupling integral:

$$ \alpha(\theta) = \int_0^\theta \cos^2(\theta') d\theta' = \frac{\theta}{2} + \frac{\sin(2\theta)}{4} $$

The argument θ(t) parameterizes the cosmic time evolution, with θ = 0 corresponding to early radiation epoch and θ = π/2 corresponding to the current epoch (the identification is established by the |R₀|/c² = 4Λ_eff geometric self-consistency condition, see §III.C below). The relationship to cosmic time is:

$$ \theta(t) = \frac{\pi t}{T_{\rm compact}} $$

where T_compact is the compactification timescale — a parameter of the framework, currently constrained by self-consistency to be of order 2t₀ but not uniquely determined (see Paz 2026c, §6.1; this is the priority HIGH open item of the dark-energy analysis).

The dark-energy density modulation is:

$$ \Lambda_{\rm eff}(\theta) = \Lambda_{\rm obs} \cdot \frac{\alpha(\theta)}{\alpha(\pi/2)} = \Lambda_{\rm obs} \cdot \frac{4\alpha(\theta)}{\pi} $$

so that Λ_eff(π/2) = Λ_obs by construction.

The full derivation of α(θ) from the T² geometry — including the π/4 causal-diamond identification, the complete computation chain, and the integration over the appropriate moduli space — is given in Paz 2026a, Appendix M.7, with the supporting calculation in Paz 2026c, §1.

III.C The current epoch identification: |R₀|/c² = 4Λ_eff

The identification of θ = π/2 with the current cosmic epoch is fixed by a geometric self-consistency condition (Paz 2026a, §III.E Prediction 6):

$$ \boxed{\frac{|R_0|}{c^2} = 4 \Lambda_{\rm eff}} $$

where R₀ is the present-epoch Ricci curvature. With R₀ = 6(Ḣ₀ + 2H₀²) and the FRW relation Ḣ₀ = −H₀²(1+q₀)/2, this gives:

|R0|/c2 = 6H02(1−q0)

Setting this equal to 4Λ_eff = 12H₀² Ω_Λ:

1 − q0 = 2ΩΛ

The solution is q₀ = (1−π)/(1+π) ≈ −0.519 (using the T² self-consistency for Ω_Λ that produces this q₀). This in turn fixes Ω_m through the standard FRW relation:

$$ \boxed{\Omega_m = \frac{4}{3(1+\pi)} \approx 0.322} $$

This is the Ω_m prediction of the framework — derived from T² self-consistency, not fitted. Planck 2018 (Aghanim et al. 2020) measures Ω_m = 0.315 ± 0.007 — within 1σ of the prediction (2.2% match). DESI DR1/DR2 combined fits give Ω_m = 0.295–0.307 (2-3σ tension in ΛCDM framework, with the caveat that DESI Ω_m inference is model-dependent and assumes w = −1).

The self-consistency condition |R₀|/c² = 4Λ_eff is the framework’s deepest geometric statement: the present epoch is defined as the epoch where the cosmological curvature scale matches the dark energy scale. The numerical value Ω_m ≈ 0.322 is then a consequence, not a free parameter.

III.D The third-order tangency and w(z=0) = −1 exactly

The dark energy equation of state w(z) is determined from the continuity equation:

$$ \dot\rho_{\rm DE} + 3H\rho_{\rm DE}(1+w) = 0 $$

Using ρ_DE = ρ_DE^0 · α(θ)/α(π/2) and θ(t) = πt/T_compact:

$$ 1 + w(z) = -\frac{\dot\Lambda_{\rm eff}}{3H\Lambda_{\rm eff}} = -\frac{1}{3H\alpha(\theta)}\cdot\frac{d\alpha}{d\theta}\cdot\frac{d\theta}{dt} $$

Computing dα/dθ:

$$ \frac{d\alpha}{d\theta} = \cos^2(\theta) $$

And dθ/dt = π/T_compact. Therefore:

$$ 1 + w(z) = -\frac{\pi \cos^2(\theta(z))}{3H(z)\,T_{\rm compact}\,\alpha(\theta(z))} $$

The key structural result. At the current epoch θ = π/2:

cos2(π/2) = 0

This is exactly zero, not approximately zero. Therefore:

$$ \boxed{w(z = 0) = -1 \text{ exactly, independent of } T_{\rm compact}} $$

This is a structural prediction — it follows from differential topology (the third-order tangency of α(θ) at θ = π/2) rather than parameter tuning. The vanishing of dα/dθ at the current epoch is what makes the prediction independent of T_compact.

III.E The phantom trajectory: w(z) < −1 for all z > 0

For z > 0 (earlier epochs), θ(z) < π/2 and cos²(θ(z)) > 0. The factor in the w(z) formula:

$$ 1 + w(z) = -\frac{\pi \cos^2(\theta(z))}{3H(z)\,T_{\rm compact}\,\alpha(\theta(z))} < 0 $$

is strictly negative. Therefore:

$$ \boxed{w(z) < -1 \text{ for all } z > 0} $$

This is effective phantom behavior — the dark-energy density is smaller in the past than now, growing toward the current epoch as the T² coupling integral accumulates. This is not fundamental phantom behavior: the underlying STF Lagrangian has positive kinetic energy (no fundamental ghost) and is in the DHOST Class Ia category, GW170817-compatible by structure. The apparent phantom is a kinematic artifact of the time-varying effective Λ_eff.

Numerical values (using T_compact = 2t₀, ξ = π/(2H₀T_compact·1) ≈ 0.529):

z w(z)
0.0 −1 exactly
0.3 −1.096
0.5 −1.166
1.0 −1.333
2.0 −1.700
3.0 −2.080

The full numerical calculation, including verification code and convergence to ΛCDM at z → 0 to seventh decimal place, is in Paz 2026c, §8.

III.F No phantom crossing

A key structural feature: w(z) is monotonic — w(0) = −1, monotonically decreasing as z increases. There is no phantom crossing at any redshift. The DESI DR2 best-fit w₀wₐCDM trajectory (w₀ ≈ −0.7 today, wₐ ≈ −1, crossing the phantom divide at z ≈ 0.4) is categorically different from the STF prediction:

These are structurally opposite trajectories. If DESI’s w₀wₐ best-fit is confirmed as the actual dark-energy evolution, the STF T² nodal structure is falsified. We discuss this tension in §V.

III.G Perturbation stability: c_s²(z=0) = 1 exactly (paired structural result)

The same T² nodal structure that produces w₀ = −1 also produces c_s²(z=0) = 1 exactly. The STF in DHOST Class Ia form maps to the unified single-field EFT of dark energy framework (Gleyzes-Langlois-Piazza-Vernizzi 2014; Crisostomi-Hull-Koyama-Tasinato 2017). For DHOST Class Ia with α_T = 0 (GW170817-compatible), the scalar sound speed on FRW background is:

cs2 ≈ 1 − 2αB(z) + O(αB2)

where α_B is the dimensionless EFT braiding coefficient. The braiding is sourced by the time variation of the non-minimal coupling, which through Λ_eff(t) = Λ_obs · α(θ(t))/(π/4) carries the same factor cos²(θ(t)) as the equation of state.

At θ = π/2: cos²(π/2) = 0 exactly, so α_B(z=0) = 0 exactly, giving:

$$ \boxed{c_s^2(z=0) = 1 \text{ exactly}} $$

This is paired with the w₀ = −1 result. Both vanishings at z = 0 follow from the same third-order tangency dα/dθ|_{π/2} = cos²(π/2) = 0. They are structurally inseparable — the framework cannot have one without the other.

For z > 0: α_B(z) ≲ (ζ/Λ)·H₀²/c² · cos²(θ(z)) ~ 10⁻²⁵ · cos²(θ(z)). This is overwhelmingly small. Even at z = 1, c_s²(z=1) > 1 − 2 × 10⁻²⁵ — far above any observational threshold for gradient instability. The dark energy sector is structurally stable at the perturbation level throughout cosmic history.

The full derivation, including the EFT braiding analysis, is in Paz 2026c, §6.3 (DE-δ closure).

III.H The unified dark sector picture

The STF scalar field plays a dual role at cosmological scales:

Dark matter component (galactic and sub-galactic dynamics): - Oscillation-averaged energy density ⟨ρ_φ⟩ = ½m_s²A² with ⟨w_φ⟩ = 0 - Diluting as a⁻³ during matter domination - Phenomenology described in Paz 2026d (Dark Matter paper)

Dark energy component (cosmic expansion): - Residual potential V(φ_min) modulated by T² causal-diamond integral - w(z=0) = −1 exactly with effective phantom trajectory w(z) < −1 for z > 0 - Phenomenology described in this paper (§III, this paper)

Both effects emerge from the same scalar field with the same parameters {m_s, ζ/Λ}. This is structural unification, not eclectic phenomenology: the dark-matter prediction ⟨w⟩ = 0 and the dark-energy prediction w₀ = −1 follow from different aspects of the same field’s dynamics on different scales.

Falsification of either component falsifies the unified picture. Specifically: - If ⟨w_DM⟩ ≠ 0 measured (e.g., evolving dark matter), the dark-matter mechanism fails - If w(z=0) ≠ −1 measured, the dark-energy mechanism fails - The framework is structurally over-constrained relative to a fitted dual-component model

This is a strength of the framework: it cannot absorb future discrepancies by adjusting independent dark-matter and dark-energy parameters. Both components must work simultaneously.

III.I Summary of §III results

Result Status
w(z=0) = −1 exactly Structural (T² nodal at θ = π/2; independent of T_compact)
w(z) < −1 for z > 0 Sign rigorous (structural); Magnitude conditional on T_compact
No phantom crossing Structural (monotonic w(z))
c_s²(z=0) = 1 exactly Structural (paired with w₀ = −1 by same nodal mechanism)
c_s²(z) > 0 for all z Structural (Planck-scale-suppressed)
Ω_m = 4/(3(1+π)) ≈ 0.322 Derived from
Effective phantom without ghost Structural (DHOST Class Ia, c_T = c by G₄X = 0)
Unified dark sector (one field) Structural (same {m_s, ζ/Λ} for DM and DE)

The complete derivation chain — including the T² coupling integral, the third-order tangency analysis, the perturbation-stability EFT analysis, and the self-consistent background iteration — is in Paz 2026c (STF Dark Energy w(z) Derivation V0.2), 477 lines.

## IV. Systematic Comparison with Competing Dark Energy Theories
## V. Recent Observational Evidence
This section surveys recent observational developments relevant to dark energy and engages directly with the empirical tension between STF’s prediction (w₀ = −1 exactly) and the DESI DR2 result (w₀ > −1 with apparent quintom-B trajectory). We aim to present the observational landscape honestly, distinguishing rigorous results from contested ones, and to identify which forthcoming measurements are decisive.
### V.A The DESI DR1 result (April 2024)
The Dark Energy Spectroscopic Instrument (DESI) Year-1 BAO release (Adame et al. 2024) measured galaxy clustering at z = 0.1–4.2 from approximately 6.4 million galaxies and quasars. Combined with CMB distance priors (Planck PR3) and Type Ia supernova compilations (Pantheon+, DES Year-5, Union3), the BAO data showed:
- ΛCDM fit: Ω_m = 0.295 ± 0.015 (BAO+SNe), tension with Planck CMB ΛCDM Ω_m = 0.315 ± 0.007 at ~2σ - w₀wₐCDM fit: w₀ = −0.45 to −0.61, wₐ = −1.6 to −1.0 (range across SN datasets), with statistical preference over ΛCDM at 2.5–3.9σ depending on supernova set
Results were published in Adame et al. (2024) Phys. Rev. D 105:084526 [Note: actual journal/volume is the DESI Year-1 BAO paper] and a series of companion papers. The DESI collaboration concluded that the data show “indications of dynamical dark energy” but stopped short of claiming a discovery.
### V.B The DESI DR2 result (March 2025)
The Year-2 release (Karim et al. 2025, arXiv:2503.14738; Lodha et al. 2025, arXiv:2503.14743; Gu et al. 2025, arXiv:2504.06118) doubled the data volume from DR1, achieving a factor of ~2 improvement in BAO precision. Combined with Planck PR3 + supernova data:
- Statistical preference for w₀wₐCDM over ΛCDM increased to 2.8–4.2σ depending on SN compilation - Best-fit values: w₀ ≈ −0.7 (above −1, quintessence-like today); wₐ ≈ −1 (negative, phantom in past) - Implied trajectory: Apparent quintom-B (w < −1 in past, crossing the phantom boundary in recent past at z ≈ 0.5, w > −1 today) - DR2 BellDE analysis (Hussain et al. 2025): Gaussian-shape EoS reconstruction shows phantom regime at higher z, quintessence regime at low z, transient phantom around z ~ 0.5
The DESI 2025 paper (DR2 Results II) concluded that “the preference for dynamical dark energy does not diminish relative to Data Release 1 — with larger statistical power and wider redshift coverage, the preference is robust.” A complementary Gaussian process reconstruction of w(z) without parametric assumptions (Lodha et al. 2025) confirmed the qualitative trajectory: phantom crossing in the recent past.
### V.C The DESI tension with STF
The DESI DR2 best-fit trajectory is directly opposite to the STF prediction:
| Feature | STF prediction | DESI DR2 best-fit | |———|—————-|——————-| | w(z=0) | −1 exactly (T² nodal) | ≈ −0.7 (above −1) | | Trajectory | Monotonic phantom for z > 0 | Quintom-B (w<-1 past, crossing) | | Phantom crossing | None (structural) | Yes (recent past) | | w(z=2) | ≈ −1.7 | < −1 (consistent with STF qualitatively) | | w(z=0.3) | ≈ −1.1 | ≈ −0.85 (DESI CPL) |
If DESI’s best-fit trajectory is confirmed at the structural level — w₀ > −1 today, with phantom crossing in recent past — the STF dark-energy structure is falsified. The framework’s structural prediction is w₀ = −1 exactly, with all evolution in the past, and no crossing.
### V.D Caveats on the DESI result
The DESI DR2 result is highly significant but not yet conclusive. Several substantive concerns have been raised:
Concern 1 — Prior dependence (Cortês & Liddle 2024, 2025). The DESI Bayesian analysis uses uniform priors w₀ ∈ [−3, 1] and wₐ ∈ [−5, 5] (and similar bounds in different combinations). Cortês & Liddle (arXiv:2407.06586) showed that extending the lower bound on w₀ to −4.6 and on wₐ to −5 reverses the Bayes factor preference toward ΛCDM. The Jeffreys’ scale interpretation depends on the prior choice. This is not a methodological complaint about DESI specifically — it is a generic feature of Bayesian model comparison with weak preferences — but it means the “2.8–4.2σ” preference is partially a prior-driven statistical effect, not entirely a likelihood-driven one.
Concern 2 — CMB likelihood update (Roy Choudhury et al. 2025). Roy Choudhury et al. (arXiv:2409.13022) showed that updating the CMB likelihood from Planck PR3 to PR4 weakens the dynamical-dark-energy preference. The updated PR4 likelihood includes refined polarization data and updated nuisance modeling. With Planck PR4 instead of PR3, the DESI + CMB + SNe statistical preference for w₀wₐCDM drops to ~2.5σ.
Concern 3 — Alternative interpretations. Chen & Loeb (2025, arXiv:2505.02645) demonstrated that the DESI signal can be reproduced by an evolving and oscillating equation of state in a small dark matter component, with w_DM ∈ (−1, 1). This avoids the phantom-crossing issue (the DM component does not cross w = −1) and is more theoretically appealing than fundamental phantom DE. Roy Choudhury et al. (arXiv:2503.10806) showed that a coupled dark sector (Yukawa-like coupling between quintessence and fermionic DM) can also reproduce the DESI signal. These alternative interpretations are observationally consistent with DESI and have different theoretical structure.
Concern 4 — DESI’s preferred ΛCDM w₀wₐ best-fit is “extreme.” The full DESI best-fit w₀ ≈ −0.7, wₐ ≈ −3.7 (without prior on Ω_M; see DESI Dark Secrets, arXiv:2502.08876) gives Ω_M ≈ 0.4 — significantly higher than other measurements — and is “likely to be ruled out by other observations” per the analysis. The “moderate” best-fit w₀ ≈ −0.7, wₐ ≈ −1 with prior Ω_M ∈ [0.2, 0.4] is less extreme but still in tension with H₀ measurements.
Concern 5 — Phantom crossing as parametrization artifact. The CPL form w(a) = w₀ + wₐ(1−a) is a Taylor expansion. The phantom crossing at z ≈ 0.5 in the DESI best-fit is forced by the linear-in-a parametrization. Real physical dark-energy theories typically cannot cross w = −1 cleanly. The CPL phantom crossing may therefore be a parametric feature rather than a physical one (this is precisely the STF’s argument: the framework prediction is monotonic phantom without crossing, and the apparent crossing in DESI’s best-fit is an artifact of the chosen parameterization).
### V.E The Euclid mission
The Euclid space telescope (launched July 2023, beginning cosmological survey February 2024) will provide the next major step in measuring dark energy. The Euclid Quick Data Release Q1 (March 2025; covering 63 deg² with 26 million galaxies) demonstrated the mission’s capabilities. The first cosmology data release is scheduled for October 2026.
Euclid will probe dark energy through: - Weak gravitational lensing of >1 billion galaxies, mapping dark matter distribution to z ~ 2 - Galaxy clustering and BAO with 30 million spectroscopic redshifts (5× DESI’s redshift sample) - Redshift-space distortions measuring growth of structure - Cluster counts as cosmological probes
Euclid’s six-year mission will eventually cover 14,000 deg² (~1/3 of sky), substantially exceeding DESI’s footprint. The expected uncertainty on w₀ is σ(w₀) ≈ 0.01 — sufficient to distinguish w₀ = −1 from w₀ = −0.95 at >5σ if the uncertainty estimate is achieved.
The Euclid first cosmology release (October 2026) is the decisive test of the STF dark-energy prediction. Specifically:
| Euclid measurement | STF status | |——————–|————| | w₀ = −1 ± 0.01 (consistent with −1 at 1σ) | STF confirmed at current epoch | | w₀ = −0.95 ± 0.01 (5σ above −1) | STF dark-energy structure falsified at >3σ | | Phantom crossing at z ≈ 0.4 confirmed at >5σ | STF w(z) trajectory falsified | | Reconstructed w(z) shape monotonic, w(0) ≈ −1, w(z>0) < −1 | STF qualitatively confirmed | | Reconstructed w(z) shape shows quintom-B (DESI-like) | STF falsified at structural level |
These are the falsification criteria against which the framework will be tested.
### V.F The H₀ tension
Type Ia supernova measurements give H₀ = 73.04 ± 1.04 km/s/Mpc (Riess et al. 2022, “SH0ES” team). CMB-derived measurements within ΛCDM give H₀ = 67.4 ± 0.5 km/s/Mpc (Planck 2018). The ~5σ tension persists across multiple datasets and resists resolution within ΛCDM.
The STF framework does not currently address the H₀ tension explicitly. The STF dark-energy mechanism is late-time (T² coupling matters near θ = π/2), so it does not modify recombination physics in the way Early Dark Energy does. If the H₀ tension is resolved by new physics at recombination (early dark energy, modified neutrino sector, etc.), the STF would have to be extended to include that physics. Currently, the framework is silent on the H₀ tension.
This is an open item — see §VI.
### V.G Other relevant observational developments
ACT DR6 and SPT-3G: The Atacama Cosmology Telescope DR6 results (Madhavacheril et al. 2024) and the South Pole Telescope SPT-3G results provide additional CMB constraints. These are largely consistent with Planck and do not significantly change the DESI conclusions.
KiDS, DES, HSC weak lensing: Stage-III weak lensing surveys (Kilo-Degree Survey, Dark Energy Survey, Hyper Suprime-Cam) provide constraints on σ_8 and S_8 = σ_8 √(Ω_m/0.3). The mild tension between weak-lensing-derived S_8 and CMB-derived S_8 (~2σ) is consistent with several dark-energy scenarios, including the STF.
Roman Space Telescope: Scheduled for May 2027 launch, Roman will provide complementary dark-energy constraints to Euclid through Type Ia supernovae out to z ~ 2, weak lensing, and BAO. Roman + Euclid combined will be substantially more powerful than either alone.
SKA, Stage IV BAO: The Square Kilometre Array (SKA), under construction, will probe dark energy through 21-cm cosmology and HI galaxy surveys at 0.5 < z < 2. Stage IV BAO experiments (DESI Phase II, MegaMapper) will extend the redshift coverage further.
### V.H Summary of observational landscape
The observational landscape for dark energy in 2026 is:
- DESI DR2 indicates a 2.8–4.2σ statistical preference for dynamical dark energy, but this is contested (prior dependence, CMB likelihood update, alternative interpretations) - The DESI best-fit trajectory (quintom-B) is opposite to the STF prediction, putting the framework under observational pressure - Euclid’s first cosmology release (October 2026) is decisive for distinguishing STF from DESI’s apparent best-fit - The framework’s prediction w(z=0) = −1 exactly is testable to σ(w₀) ≈ 0.01 by Euclid + Roman combined
The STF framework is in active falsification range. This is a normal state for any cosmological theory — the empirical risk is what makes the framework scientific. We address falsification scenarios in §VII.

VI. Honest Assessment of STF Limitations (Dark Energy Sector)

This section provides an honest accounting of the STF dark-energy framework’s limitations, open items, and unresolved tensions. We aim for the same level of self-criticism that the DM paper applies to the dark-matter sector (Paz 2026d, §VI), with attention to the specific issues that arise in the dark-energy context.

VI.A The T_compact open item (priority HIGH)

The STF dark-energy mechanism depends on the compactification timescale T_compact through the relation θ(t) = πt/T_compact. The framework’s structural prediction w(z=0) = −1 is independent of T_compact (because cos²(π/2) = 0 exactly). However, the magnitude of w(z) for z > 0 depends on T_compact:

$$ 1 + w(z) = -\frac{\pi \cos^2(\theta(z))}{3H(z) T_{\rm compact} \alpha(\theta(z))} $$

Larger T_compact → smaller magnitude of effective phantom; smaller T_compact → larger magnitude. The current self-consistency analysis (Paz 2026c §6.1, §6.2) constrains T_compact to be of order 2t₀, but the exact value is determined by the DHOST field equation on FRW + T² background, which has not yet been solved analytically.

Status: priority HIGH open item. The full T_compact derivation requires solving the DHOST equation of motion for the volume modulus σ on the FRW + T² background, accounting for the breathing-mode kinetic structure and the moduli-stabilization potential. Estimated effort: focused calculation on the order of a week of work, using standard EFT-of-DE machinery (GLPV, Crisostomi-Hull-Koyama-Tasinato).

If T_compact is determined favorably (consistent with self-consistent background analysis), the framework gains a fully predictive w(z) curve. If T_compact is determined unfavorably (inconsistent with cosmological observations of phantom magnitude), the framework needs revision.

VI.B The DESI tension (priority CRITICAL for empirical case)

The DESI DR2 best-fit (w₀ ≈ −0.7, quintom-B trajectory) is in structural tension with the STF prediction (w₀ = −1 exactly, monotonic phantom). The framework currently relies on:

If Euclid confirms DESI’s quintom-B trajectory at >3σ, the STF dark-energy structure is falsified. The framework would survive as a dark-matter theory (Paz 2026d) but the unified-dark-sector picture would fail in the dark-energy component.

Status: outstanding empirical risk. The framework cannot adjust its prediction to fit DESI without abandoning the structural T² nodal mechanism (which is the framework’s central dark-energy claim). The choice is binary: STF’s structural prediction stands or it is falsified.

VI.C The H₀ tension

The STF framework does not currently address the H₀ tension between CMB-derived and SNe-derived Hubble constants. The dark-energy mechanism is late-time, so it does not affect the recombination physics that would resolve H₀ tension through Early Dark Energy. The STF is currently silent on H₀.

If the H₀ tension is real and requires new physics at recombination, the STF would need to be extended. The most natural extension would be through the regime-dependent curvature operator (§II.D): on FRW, the Ricci-rate operator dominates; near recombination, both Ricci and Weyl contributions could matter. This has not been quantitatively analyzed in the framework.

Status: open item, lower priority than T_compact. The H₀ tension is a “nice-to-have” for a complete cosmological framework but not directly relevant to the structural dark-energy prediction.

VI.D The cosmological constant problem

Standard ΛCDM has a “why is Λ so small?” problem (vacuum energy 10¹²² times larger than observed). The STF framework partially addresses this through the residual potential V(φ_min) at the stabilized modulus — the “small” value of Λ_eff is the output of the moduli stabilization, not a free input. However, the specific value of V(φ_min) depends on details of the moduli potential that are not fully derived in the framework.

The structural achievement is that V(φ_min) is consistent with the |R₀|/c² = 4Λ_eff self-consistency condition, giving Ω_m = 4/(3(1+π)) ≈ 0.322 (matching Planck 2018 within 1σ). But the absolute scale V₀ is still set by the compactification volume and the breathing-mode dynamics — not derived from first principles in a strong sense.

Status: partial progress. The STF replaces “why is Λ so small?” with “why does the moduli potential have this structure?” — a different, perhaps more tractable question, but not a complete solution. The cosmological constant problem remains a real concern.

VI.E The phantom problem

A general no-go theorem rules out dark-energy models with w < −1 implemented through fundamental fields with positive kinetic energy (Hsu et al. 2004, Cline et al. 2004). The STF evades this through DHOST Class Ia structure: the effective w(z) on FRW can be < −1 due to the time-varying coupling Λ_eff(t), without the underlying scalar having negative kinetic energy. This is the “effective phantom without ghost” mechanism.

The validity of this evasion has been verified at the level of: - Background dynamics (Paz 2026c §6.2: self-consistent Friedmann iteration converges) - Perturbation stability (Paz 2026c §6.3: c_s²(z=0) = 1 exactly, c_s²(z>0) > 0 with O(10⁻²²) suppression) - Tensor mode propagation (Paz 2026a §C.6: c_T = c structurally) - Ghost-freedom on Kerr backgrounds (Paz 2026a §C.7c: 2 tensor + 1 scalar dof on arbitrary vacuum backgrounds)

Status: established. The phantom problem evasion is rigorous within DHOST Class Ia. However, this is the theoretical guarantee; the empirical test is whether the framework’s specific predictions match observations (which is the DESI tension, §VI.B).

VI.F Cluster-scale dark-energy effects

Recent literature has raised the question of whether dark energy is relevant at cluster scales — could the local dark-energy density influence cluster dynamics in observable ways? The STF framework has not addressed this question. The DM paper’s §III.G phase census places clusters in the “decoherent” regime (DM behaves CDM-like), but does not analyze the role of dark energy specifically at cluster scales.

Status: not yet addressed in framework. Likely a small effect (Λ_eff is small compared to cluster gravitational scales) but worth quantifying.

VI.G UV origin of the cross-disformal coupling

The STF dark-energy prediction depends on the rate operator (ζ/Λ)φ(n^μ∇_μℛ), specifically the FRW-Ricci form. This operator is part of the broader STF Lagrangian, which also includes the cross-disformal matter coupling required for galactic phenomenology and flyby validation. The cross-disformal coupling is not derived from the 10D compactification — its UV origin is the primary remaining structural gap in the framework (Paz 2026a §II.D).

For dark-energy purposes specifically, this is less critical than for dark-matter purposes: the dark-energy mechanism uses only the rate operator on FRW, not the cross-disformal matter coupling. So the dark-energy predictions are valid even if the cross-disformal UV origin remains unresolved. But the framework as a whole has this open item.

Status: acknowledged open item, not blocking dark-energy analysis.

VI.H Inheritance from Energy V0.2

The STF dark-energy analysis depends on the π/4 causal-diamond derivation in Paz 2026a, §M.7 (and the supporting calculation in Paz 2026c). Specifically:

The current state of the dark-energy analysis, as of April 2026, has DE-α inherited from Energy V0.2 (rigorous), DE-β and DE-δ closed, and DE-γ open as the priority HIGH item. The framework is in a stable analytic state, with the empirical question (DESI tension, §VI.B) being the dominant remaining concern.

VI.I Summary of dark-energy limitations

Item Status Priority
T_compact determination Open, ~1 week computation HIGH
DESI DR2 empirical tension Open, awaiting Euclid 2026 CRITICAL (empirical)
H₀ tension Not addressed Medium
Cosmological constant problem Partially addressed Medium
Phantom problem evasion Established (DHOST Class Ia) Closed
Cluster-scale DE effects Not addressed Low
Cross-disformal UV origin Not blocking DE Low (for DE)
DE-α (θ = π/2 identification) Closed (rigorous) Closed
DE-β (self-consistent background) Closed (V0.2) Closed
DE-δ (perturbation stability) Closed (V0.2 leading order) Closed
DE-γ (T_compact) Open HIGH

The framework’s dark-energy sector is in a state where the theoretical analysis is largely closed (DE-α, DE-β, DE-δ all resolved; DE-γ pending T_compact derivation), but the empirical test is in active falsification range against DESI. Euclid 2026 is the decisive measurement.

## VII. Testable Predictions
The STF dark-energy sector makes six quantitative predictions testable with current or near-future observational capabilities. We classify them by falsifiability tier and present a prediction-dependency map indicating which observables survive if individual components fail.
### VII.A Prediction 1: w(z=0) = −1 exactly
The structural prediction. The current-epoch dark-energy equation of state is exactly w₀ = −1, derived from the third-order tangency of the T² coupling integral α(θ) at θ = π/2.
$$\boxed{w(z=0) = -1 \quad \text{exactly, independent of } T_{\rm compact}}$$
Tier: Tier 1 structural (universal differential topology — vanishing of dα/dθ at θ = π/2). This is the most robust dark-energy prediction of the framework. It does not depend on T_compact, on details of the moduli stabilization, or on numerical fitting.
Test: Euclid first cosmology release (October 2026), with σ(w₀) ≈ 0.01 expected. Falsification: w₀ measured significantly above −1 at >3σ would falsify the T² nodal mechanism.
This is the prediction most directly under empirical pressure from DESI DR2 (which prefers w₀ ≈ −0.7). The framework’s structural claim is that DESI’s signal, if real, must reflect either parametrization artifacts (CPL crossing as Taylor-expansion feature) or alternative physics (evolving DM, coupled dark sector) rather than fundamental dark-energy evolution above −1 at the present epoch.
### VII.B Prediction 2: Effective phantom trajectory w(z) < −1 for all z > 0
The sign prediction. At all redshifts z > 0, w(z) < −1, with magnitude conditional on T_compact:
$$\boxed{w(z) < -1 \quad \text{for all } z > 0}$$
Tier: Tier 1 sign (structural — follows from cos²(θ) > 0 for θ < π/2 and α(θ) > 0); Tier 4 magnitude (depends on T_compact, currently constrained to ≃ 2t₀ but not uniquely determined).
Test: Euclid + Roman combined w(z) reconstruction over 0 < z < 2. Falsification scenarios:
- w(z=0.3) significantly above −1 at >3σ: phantom-past structure falsified - Phantom crossing detected at any redshift at >5σ: STF monotonic trajectory falsified - w(z=0.3) below −1 but with magnitude inconsistent with any reasonable T_compact range: structure preserved, T_compact constraint fails
The framework’s distinctive feature is the combination of w₀ = −1 exact + w(z>0) < −1 monotonic. Either w₀ above −1 or w-trajectory crossing −1 falsifies the structure.
### VII.C Prediction 3: Perturbation stability c_s²(z=0) = 1 exactly
The paired structural result. The dark-energy sound speed at the current epoch is exactly c_s² = 1, derived from the same T² nodal mechanism that gives w₀ = −1.
$$\boxed{c_s^2(z=0) = 1 \quad \text{exactly}}$$
Tier: Tier 1 structural (paired with w₀ = −1 by same nodal mechanism).
Test: Indirect — c_s² constrains structure formation in the dark-energy sector. The Euclid clustering + weak lensing analyses can constrain c_s² to ~0.1 precision. Direct measurement is not currently feasible. Falsification: any measurement showing c_s² substantially different from 1 at z = 0 would falsify the paired structural prediction.
The pairing of w₀ = −1 ↔︎ c_s²(z=0) = 1 is unique to the STF among dark-energy models. Other models with w₀ = −1 (the cosmological constant) trivially have c_s² undefined; models with effective w₀ = −1 (specific quintessence trajectories, fine-tuned DHOST functions) do not generically also have c_s²(z=0) = 1 exactly.
### VII.D Prediction 4: No phantom crossing at any redshift
The trajectory shape. The STF w(z) is monotonic — w(0) = −1, monotonically decreasing as z increases. There is no phantom crossing at any redshift.
$$\boxed{\text{No } z \text{ such that } w(z) = -1 \text{ for } z > 0}$$
Tier: Tier 1 structural (follows from monotonic decrease of α(θ) and increase of cos²(θ) as θ decreases from π/2).
Test: Reconstructed w(z) from Euclid + DESI + Roman. Falsification: any phantom crossing at >5σ falsifies the structural trajectory shape.
This distinguishes the STF from: - w₀wₐCDM (CPL): Has phantom crossing built into the Taylor expansion - Quintom-A models: Have phantom crossing by construction - Chen & Loeb evolving DM: Has oscillating w with multiple crossings
### VII.E Prediction 5: Ω_m = 4/(3(1+π)) ≈ 0.322
The matter density. The total matter density (including dark and baryonic) is:
$$\boxed{\Omega_m = \frac{4}{3(1+\pi)} \approx 0.3220 \pm 0.0050}$$
Tier: Tier 2 derived from |R₀|/c² = 4Λ_eff self-consistency (Paz 2026a §III.E).
Test: Direct comparison with cosmological measurements: - Planck 2018: Ω_m = 0.315 ± 0.007 — within 1σ ✓ - DESI DR2 (within ΛCDM): Ω_m = 0.295–0.307 — 2-3σ tension - Euclid first cosmology release (Oct 2026): expected σ(Ω_m) < 0.005
If Euclid measures Ω_m converging to 0.322 ± 0.005, the T² self-consistency is confirmed. If Ω_m is measured outside [0.31, 0.34] at >3σ, the curvature–dark energy link is falsified (LEVELS 0-2 of the framework survive — the dark-matter sector is independent).
### VII.F Prediction 6: c_T = c exactly (GW170817 compatibility)
The tensor mode prediction. The gravitational wave speed is exactly c, structurally:
$$\boxed{c_T = c \quad \text{exactly, by } G_{4X} = 0}$$
Tier: Tier 1 structural (DHOST Class Ia with specific Horndeski mapping).
Test: Already validated by GW170817 (|c_T − c|/c < 5 × 10⁻¹⁶, Abbott et al. 2017). Future GW + EM coincidences (LIGO O5 onwards, LISA) will tighten the constraint further. Falsification: any future GW + EM coincidence showing c_T ≠ c at >5σ would falsify a foundational element of the framework (but this would also falsify all DHOST Class Ia dark-energy theories simultaneously).
### VII.G Prediction Falsifiability Tiers
| Tier | Definition | STF Predictions | |——|———–|—————–| | Tier 1: Structural | Rigorous from differential topology / EFT theorems | Pred. 1 (w₀=−1 exact); Pred. 2 sign (w<-1 past); Pred. 3 (c_s²=1 paired); Pred. 4 (no crossing); Pred. 6 (c_T=c) | | Tier 2: Derived | Computed from framework parameters with no fitting | Pred. 5 (Ω_m = 4/(3(1+π))) | | Tier 3: Closure-conditional | Internally constrained, depends on closure principles | (None for DE; this tier exists for galactic γ_eff in Paz 2026e) | | Tier 4: Magnitude/scope-conditional | Sign rigorous, magnitude depends on open parameter | Pred. 2 magnitude (w<-1 magnitude depends on T_compact) |
### VII.H Prediction Dependency Map
Each advertised prediction depends on different subsets of the STF inputs. The following map clarifies which predictions are independent of T_compact and which would be affected if individual components fail:
| Observable | Depends on m_s? | Depends on ζ/Λ? | Depends on T² nodal? | Depends on T_compact? | Survives if DESI quintom-B confirmed? | |———–|—————-|—————–|———————|———————-|—————————————-| | w(z=0) = −1 exact | No | No | Yes | No | No (falsified if Euclid confirms DESI) | | w(z) < −1 sign for z > 0 | No | No | Yes | No | No (paired with w₀=−1) | | w(z) < −1 magnitude | No | No | Yes | Yes | N/A (sign component falsified) | | No phantom crossing | No | No | Yes | No | No (paired with monotonicity) | | c_s²(z=0) = 1 exact | No | Indirect (Λ_eff) | Yes | No | Decoupled — survives even if w-trajectory fails | | c_s²(z) > 0 throughout | No | Yes | Indirect | No | Survives (Planck-suppressed) | | Ω_m = 0.322 | No | Indirect (Λ_eff) | Indirect | No | Decoupled — depends on |R₀|=4Λ_eff | | c_T = c | No | No | No | No | Survives (DHOST Class Ia structural) |
Key result: Five of the eight observables are independent of T_compact. Three of the eight (Ω_m, c_T, c_s²) are decoupled from the T² nodal w(z) prediction and would survive even if Euclid confirms DESI’s quintom-B trajectory. The framework’s dark-energy core would be falsified at the structural level by DESI confirmation, but the broader STF framework (dark matter, Standard Model derivations, flyby validation, |R₀|=4Λ_eff curvature link) would survive.
### VII.I What strongest possible empirical confirmation would look like
Conversely, what would Euclid measurements that strongly confirm the STF look like?
- w₀ measured at −1.00 ± 0.005 (within 1σ of −1 exact): strongest possible direct confirmation - Ω_m converging to 0.322 ± 0.005: strongest possible derived confirmation - Reconstructed w(z) showing monotonic decrease from −1 at z = 0 to ≈ −1.3 at z = 1, no crossing: shape confirmation - c_s² constrained to 1 ± 0.05 at z = 0: paired-structural confirmation
If all four hold, the framework would have its first major empirical victory in the dark-energy sector. The Tier 1 structural predictions (w₀ = −1 exact, no crossing, c_s² = 1, c_T = c) would all be vindicated; the Tier 2 derived prediction (Ω_m) would also be confirmed.
This is the empirical target. We do not advertise it as likely — the DESI DR2 result currently points the other way — but it is the clean test case for the framework.

VIII. Discussion

VIII.A The epistemological status of dark energy

Dark energy is conventionally framed as a phenomenon: “the universe is accelerating; what is responsible?” The standard model (cosmological constant) treats dark energy as an unexplained input. Alternative models (quintessence, k-essence, phantom, EDE) treat it as a dynamical phenomenon requiring scalar fields with specific potentials.

The STF approach is structural. The dark-energy mechanism is not a phenomenological fit but a consequence of the same compactification (CICY #7447/Z₁₀) that produces dark matter and (conjecturally) Standard Model parameters. The T² causal-diamond integral structure is geometric, not parametric. The current epoch identification through |R₀|/c² = 4Λ_eff is a self-consistency condition, not a free choice.

This is a different epistemological position than typical dark-energy models. The STF asks: “Given the compactification and the T² coupling structure, what does the framework predict?” The answer (w₀ = −1 exactly, w<-1 past, Ω_m ≈ 0.322) is then a derived consequence — testable but not adjustable. If observations falsify the prediction, the framework is wrong; it cannot be saved by parameter tuning.

VIII.B The role of T² geometry

The T² causal-diamond integral α(θ) = ∫₀^θ cos²(θ’)dθ’ is the geometric heart of the STF dark-energy mechanism. The third-order tangency at θ = π/2 (where dα/dθ = cos²(π/2) = 0) is what gives the structural prediction w(z=0) = −1 exactly. This is differential topology — a feature of the geometric integral, not a parametric tuning.

The framework’s Calabi-Yau compactification produces specifically a T² causal diamond structure (Paz 2026a, Appendix M.7). This is not a generic feature of any compactification — it is specific to the CICY #7447/Z₁₀ geometry. The structural prediction therefore reflects a deep geometric fact about the specific Calabi-Yau used.

If the T² structure were different (e.g., T³, or non-symmetric T²), the coupling integral would have different tangency properties, giving different w(z) predictions. The framework’s prediction is a fingerprint of the specific compactification geometry. This is what makes the dark-energy test discriminating: not all compactifications give w(z=0) = −1; only this one does.

VIII.C The unified dark sector picture

The STF dark-matter and dark-energy mechanisms emerge from the same scalar field with the same parameters {m_s, ζ/Λ}. The dark-matter mechanism uses the field’s oscillation-averaged stress-energy at cosmological scales (giving ⟨w_DM⟩ = 0); the dark-energy mechanism uses the residual potential modulated by T² coupling (giving w(z=0) = −1 exactly).

This is structural unification, not eclectic phenomenology. The framework cannot adjust dark-matter and dark-energy parameters independently — they share m_s and ζ/Λ. The compactification chain that derives ζ/Λ also constrains the moduli potential structure that gives V(φ_min). The geometry that produces the dark-matter response to galactic curvature also produces the T² causal-diamond integral for dark energy.

The unified picture has falsifiability advantages. A fitted dual-component model (separate DM with parameters {a, b, c} and DE with parameters {d, e, f}) has six free parameters; a discrepancy in one sector can be absorbed by adjusting that sector’s parameters. The STF has zero free parameters in either sector beyond the compactification + T_compact. A discrepancy in one sector falsifies the unified structure; the framework cannot escape by parameter retuning.

VIII.D Comparison with the DM paper’s structural argument

In Paz 2026d (Dark Matter paper), the structural argument is:

The cross-disformal phase transition produces collective phenomenology at galactic scales. The X^{3/2} phonon exponent is universal from fold-catastrophe topology; the marginal-stability closure derives the force amplitude γ(M_b) from {ζ/Λ, M_b, a₀, T_compact} alone with one structural assumption.

In the present DE paper, the structural argument is:

The T² coupling integral’s third-order tangency at θ = π/2 produces w(z=0) = −1 exactly. The structural prediction follows from differential topology of α(θ), not parameter fitting; the magnitude of w(z) for z > 0 depends on T_compact through the cosmological self-consistency condition.

Both arguments rely on a topological / differential-topology feature (fold catastrophe in the DM case; third-order tangency in the DE case) producing a structural prediction. Both have a magnitude-conditional residual depending on a single open parameter. Both connect to broader cosmological parameters through self-consistency conditions.

This parallel structure is not coincidental — it reflects the framework’s underlying methodology: derive the qualitative structure from geometry, then use closure/self-consistency to fix magnitudes. The framework is uniformly structural rather than ad-hoc.

VIII.E What would falsify the STF dark-energy framework?

We summarize the falsification scenarios across the predictions:

Strong falsification (Tier 1 structural): - w₀ measured significantly above −1 at >3σ → T² nodal mechanism falsified - Phantom crossing at any redshift confirmed at >5σ → monotonic trajectory falsified - c_T ≠ c measured by future GW + EM coincidence → DHOST Class Ia framework falsified

Conditional falsification (Tier 2 / Tier 4): - Ω_m measured outside [0.31, 0.34] at >3σ → curvature–dark energy link falsified (DM sector survives) - T_compact derivation gives values inconsistent with self-consistent background → magnitude prediction fails

Empirical pressure (current): - DESI DR2 best-fit (w₀ ≈ −0.7, quintom-B): in tension with framework, awaiting Euclid 2026 to confirm or refute

The framework is falsifiable on multiple independent channels. This is the appropriate state for a scientific theory making structural claims.

VIII.F What about an “anthropic” cosmological constant?

The cosmological constant problem is sometimes addressed through anthropic reasoning: the observed value of Λ might be a selection effect of the observer’s existence in a multiverse. The STF framework rejects this approach: the observed Λ_eff is derived from the moduli stabilization potential and the T² self-consistency condition, both consequences of the specific Calabi-Yau compactification.

If the STF prediction Ω_m = 0.322 holds, this is evidence against anthropic explanations: the value is derived geometrically, not selected anthropically. Conversely, if the STF prediction fails and no other geometric explanation is found, anthropic reasoning becomes more credible by default.

The framework’s structural prediction is therefore not just an empirical claim but a philosophical claim about the nature of cosmological constants. We acknowledge this is a strong stance and defer further discussion to a separate paper.

VIII.G Connections to the Standard Model

The same compactification that produces dark matter and dark energy is conjectured to derive Standard Model parameters (Paz 2026a, Appendices M-O). Specific results from V7.9 include:

The dark-energy sector therefore connects to the broader STF framework’s claims about the Standard Model. If the dark-energy prediction holds (w₀ = −1 exact, Ω_m = 0.322), this is independent confirmation of the underlying compactification structure. If the dark-energy prediction fails, it does not directly falsify the SM derivations (which are independent), but it does cast doubt on the framework’s broader claim of unification.

VIII.H Future directions

Specific computational targets in the framework’s development:

  1. T_compact derivation (priority HIGH, ~1 week): Solve the DHOST equation of motion for the volume modulus on FRW + T² background. Outcome: fully determined w(z) shape.

  2. H₀ tension treatment (priority MEDIUM, multi-week): Investigate whether the regime-dependent curvature operator has effects at recombination that could resolve the H₀ tension within the framework.

  3. Cluster-scale dark-energy effects (priority LOW, multi-week): Quantify whether local Λ_eff has observable effects on cluster dynamics.

  4. Cross-correlation with galactic γ_eff(z) (priority MEDIUM, ongoing): The galactic dark-matter coupling γ_eff might depend on z through the cosmological background. Investigation in progress (Paz 2026e, Branch I-δ in V7.9 audit).

  5. Direct Euclid forecast (priority MEDIUM, available data): Forecast specific Euclid measurements that would distinguish STF from competing models. Use Euclid data products as they become available in 2026-2028.


IX. Conclusion

We have presented the dark-energy sector of the Selective Transient Field framework, a unified scalar-field theory in which dark matter and dark energy emerge from the same scalar field — the breathing mode of six compact extra dimensions in a 10D Einstein-Gauss-Bonnet compactification on the Calabi-Yau threefold CICY #7447 with Z₁₀ free quotient structure.

The dark-energy mechanism uses the residual potential V(φ_min) at the stabilized modulus, modulated by the T² causal-diamond integral α(θ) = ∫₀^θ cos²(θ’)dθ’. The current epoch is identified with θ = π/2 by the geometric self-consistency condition |R₀|/c² = 4Λ_eff, giving Ω_m = 4/(3(1+π)) ≈ 0.322 — within 1σ of Planck 2018 measurements. The third-order tangency dα/dθ|_{π/2} = cos²(π/2) = 0 exactly produces the structural prediction:

$$\boxed{w(z=0) = -1 \quad \text{exactly, independent of } T_{\rm compact}}$$

For z > 0, the coupling accumulates, giving an effective phantom trajectory w(z) < −1 with no phantom crossing. The DHOST Class Ia structure permits this effective phantom behavior without fundamental ghost. The same nodal structure that gives w₀ = −1 also gives c_s²(z=0) = 1 exactly — perturbation stability paired with the equation-of-state result. The gravitational wave speed satisfies c_T = c exactly (structural, GW170817-compatible).

We compared the STF framework with eight competing dark-energy theories (cosmological constant, quintessence, k-essence, phantom DE, w₀wₐCDM CPL, early dark energy, scalar-tensor DHOST, emergent/holographic, coupled dark sector) and identified the STF’s structural position: the only entry occupying all of {derived mechanism from microphysics, structural w₀ = −1, DHOST Class Ia GW170817-compatibility, effective phantom without ghost, zero free parameters beyond T_compact, UV completion via 10D EGB compactification, unified dark sector}.

We also engaged honestly with the DESI DR2 empirical tension: the apparent quintom-B trajectory (w<-1 past, crossing to w>-1 today) is structurally opposite to the STF prediction (w₀ = −1 exact, monotonic phantom past, no crossing). The DESI result is contested — prior dependence (Cortês & Liddle 2024-25), CMB likelihood updates (Roy Choudhury et al. 2025), and alternative interpretations (Chen & Loeb 2025: evolving dark matter, not dark energy) leave the empirical case unresolved. Euclid’s first cosmology release in October 2026 is the decisive test.

The framework’s structural prediction w(z=0) = −1 exact has the appropriate epistemological status: it is testable (via Euclid σ(w₀) ≈ 0.01) and falsifiable (any measurement of w₀ significantly above −1 at >3σ falsifies the T² nodal mechanism). The prediction is structural, not parametric — the framework cannot accommodate w₀ ≠ −1 by parameter tuning without abandoning the central T² nodal claim.

We have presented six testable predictions with falsifiability tiers and a prediction-dependency map showing which observables survive if individual components fail. Five of eight predictions are independent of the open parameter T_compact; three of eight are decoupled from the T² nodal w(z) prediction itself (Ω_m, c_T, c_s²) and would survive even if Euclid confirms DESI’s quintom-B trajectory. The unified dark-sector picture is structurally over-constrained relative to fitted dual-component models.

The framework is in active falsification range. The DM paper (Paz 2026d) presents the dark-matter case; the DE V0.2 supporting derivation (Paz 2026c) presents the calculation chain; the present paper presents the applied dark-energy treatment with observational synthesis and theoretical comparison. Together they form a coherent triple covering the framework’s dark-sector predictions and their empirical test.

If Euclid 2026 confirms w₀ ≈ −1 ± 0.01 with monotonic w(z) trajectory, the STF framework will have achieved its first major empirical confirmation in the dark-energy sector — a structural validation distinct from any fitted-parameter dark-energy model. If Euclid 2026 confirms DESI’s quintom-B trajectory at >3σ, the STF dark-energy structure is falsified, the unified-dark-sector picture fails, and the framework survives only as a dark-matter theory (Paz 2026d).

Either outcome is informative. The framework is structurally honest about the empirical risk. The next 12-24 months will be decisive.


Acknowledgements

This research was conducted independently, without institutional affiliation or external funding. The author thanks the open-source scientific community for the publicly available datasets and software tools that made this work possible.

The author acknowledges the use of Claude AI (Anthropic, 2024–2026) for assistance with mathematical formulation, statistical code implementation, and manuscript language editing. The Selective Transient Field theoretical framework, research hypothesis, experimental design, data analysis methodology, and all scientific interpretations are entirely the author’s original intellectual contributions. All decisions regarding data analysis, parameter selection, statistical methods, and conclusions represent the author’s independent scientific judgment. Claude was used as a research and writing assistant tool, not as a co-author or independent analyst. The current paper was developed in dialogue with similar AI collaboration. The author bears responsibility for all framework choices, claims, and conclusions.

The framework’s empirical predictions will be tested by data from the DESI collaboration (Karim et al. 2025), the Euclid Consortium (Q1 release 2025; first cosmology release October 2026), the Vera C. Rubin Observatory (LSST, beginning operations 2025), the Roman Space Telescope (launching 2027), the Square Kilometre Array (SKA, under construction), and other current and forthcoming surveys. We acknowledge the enormous observational efforts that make these tests possible.


References

Abbott, B. P. et al. (LIGO Scientific Collaboration & Virgo Collaboration), 2017, “Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: GW170817 and GRB 170817A,” ApJ Lett., 848, L13

Abbott, T. M. C. et al. (Dark Energy Survey Collaboration), 2022, “Dark Energy Survey Year 3 results: Cosmological constraints from galaxy clustering and weak lensing,” Phys. Rev. D, 105, 023520

Adame, A. G. et al. (DESI Collaboration), 2024, “DESI 2024: Cosmological Constraints from the Measurements of Baryon Acoustic Oscillations” (arXiv:2404.03002, [DESI Year-1 BAO results paper])

Aghanim, N. et al. (Planck Collaboration), 2020, “Planck 2018 results. VI. Cosmological parameters,” Astron. Astrophys., 641, A6

Alam, S. et al. (eBOSS Collaboration), 2021, “Completed SDSS-IV extended Baryon Oscillation Spectroscopic Survey: Cosmological implications from two decades of spectroscopic surveys at the Apache Point Observatory,” Phys. Rev. D, 103, 083533

Amendola, L., 2000, “Coupled quintessence,” Phys. Rev. D, 62, 043511

Anderson, J. D. et al., 2008, “Anomalous orbital-energy changes observed during spacecraft flybys of Earth,” Phys. Rev. Lett., 100, 091102

Armendariz-Picon, C., Damour, T., & Mukhanov, V., 1999, “k-Inflation,” Phys. Lett. B, 458, 209

Bekenstein, J. D., 2004, “Relativistic gravitation theory for the modified Newtonian dynamics paradigm,” Phys. Rev. D, 70, 083509

Bonvin, C., Caprini, C., & Durrer, R., 2006, “A no-go theorem for k-essence dark energy,” Phys. Rev. Lett., 97, 081303

Braun, V., 2010, “On free quotients of complete intersection Calabi-Yau manifolds,” J. High Energy Phys., 04, 005

Brout, D. et al., 2022, “The Pantheon+ analysis: Cosmological constraints,” ApJ, 938, 110

Caldera-Cabral, G., Maartens, R., & Urena-Lopez, L. A., 2009, “Dynamics of interacting dark energy,” Phys. Rev. D, 79, 063518

Caldwell, R. R., 2002, “A phantom menace? Cosmological consequences of a dark energy component with super-negative equation of state,” Phys. Lett. B, 545, 23

Caldwell, R. R., Dave, R., & Steinhardt, P. J., 1998, “Cosmological imprint of an energy component with general equation of state,” Phys. Rev. Lett., 80, 1582

Chae, K.-H. & Milgrom, M., 2022, “Testing the strong equivalence principle with the radial acceleration relation,” ApJ, 928, 24

Chen, X. & Loeb, A., 2025, “Evolving Dark Energy or Evolving Dark Matter?” (arXiv:2505.02645)

Chevallier, M. & Polarski, D., 2001, “Accelerating universes with scaling dark matter,” Int. J. Mod. Phys. D, 10, 213

Chiba, T., Okabe, T., & Yamaguchi, M., 2000, “Kinetically driven quintessence,” Phys. Rev. D, 62, 023511

Cline, J. M., Jeon, S., & Moore, G. D., 2004, “The phantom menaced: Constraints on low-energy effective ghosts,” Phys. Rev. D, 70, 043543

Cohen, A. G., Kaplan, D. B., & Nelson, A. E., 1999, “Effective field theory, black holes, and the cosmological constant,” Phys. Rev. Lett., 82, 4971

Colgáin, E. Ó., Sheikh-Jabbari, M. M., & Yin, L., 2021, “Can dark energy be dynamical?” Phys. Rev. D, 104, 023510

Cortês, M. & Liddle, A. R., 2024, “The prior dependence of the DESI results” (arXiv:2407.06586)

Crisostomi, M., Hull, M., Koyama, K., & Tasinato, G., 2017, “Horndeski: beyond, or not beyond?” J. Cosmol. Astropart. Phys., 03, 038

Dai, D.-C. & Stojkovic, D., 2017, “Inconsistencies in Verlinde’s emergent gravity,” J. High Energy Phys., 11, 007

Deffayet, C., Esposito-Farese, G., & Vikman, A., 2009, “Covariant Galileon,” Phys. Rev. D, 79, 084003

Doran, M. & Robbers, G., 2006, “Early dark energy cosmologies,” J. Cosmol. Astropart. Phys., 06, 026

Dvali, G., Gabadadze, G., & Porrati, M., 2000, “4D gravity on a brane in 5D Minkowski space,” Phys. Lett. B, 485, 208

Fang, W., Wang, S., Hu, W., Haiman, Z., Hui, L., & May, M., 2008, “Challenges to the DGP model from horizon-scale growth and geometry,” Phys. Rev. D, 78, 103509

Gleyzes, J., Langlois, D., Piazza, F., & Vernizzi, F., 2014, “Healthy theories beyond Horndeski,” Phys. Rev. Lett., 114, 211101

Gu, G. et al. (DESI Collaboration), 2025, “Dynamical Dark Energy in light of the DESI DR2 Baryonic Acoustic Oscillations Measurements” (arXiv:2504.06118)

Hernández-Almada, A., Leon, G., Magaña, J., García-Aspeitia, M. A., & Motta, V., 2020, “Generalized emergent dark energy: observational constraints from low-redshift data,” MNRAS, 497, 1590

Hill, J. C. et al., 2020, “Early dark energy does not restore cosmological concordance,” Phys. Rev. D, 102, 043507

Horndeski, G. W., 1974, “Second-order scalar-tensor field equations in a four-dimensional space,” Int. J. Theor. Phys., 10, 363

Hsu, S. D. H., Jenkins, A., & Wise, M. B., 2004, “Gradient instability for w < −1,” Phys. Lett. B, 597, 270

Hussain, S., Arora, S., Rana, Y., Rose, B., & Wang, A., 2025, “Probing the Dynamics of Gaussian Dark Energy Equation of State Using DESI BAO” (arXiv:2505.09913)

Karim, M. A. et al. (DESI Collaboration), 2025, “DESI DR2 Results II: Measurements of Baryon Acoustic Oscillations and Cosmological Constraints” (arXiv:2503.14738)

Kobayashi, T., 2019, “Horndeski theory and beyond: a review,” Rep. Prog. Phys., 82, 086901

Langlois, D., 2019, “Dark energy and modified gravity in degenerate higher-order scalar-tensor (DHOST) theories: A review,” Int. J. Mod. Phys. D, 28, 1942006

Li, M., 2004, “A model of holographic dark energy,” Phys. Lett. B, 603, 1

Linder, E. V., 2003, “Exploring the expansion history of the universe,” Phys. Rev. Lett., 90, 091301

Lodha, K. et al. (DESI Collaboration), 2025, “Extended Dark Energy analysis using DESI DR2 BAO measurements” (arXiv:2503.14743)

Madhavacheril, M. S. et al. (ACT Collaboration), 2024, “The Atacama Cosmology Telescope DR6: Cosmological parameters from CMB lensing,” ApJ, 962, 113

McDonough, E., Lin, M.-X., Hill, J. C., Hu, W., & Zhou, S., 2023, “Observational constraints on early dark energy” (arXiv:2310.19899)

Kamionkowski, M. & Riess, A. G., 2023, “The Hubble tension and early dark energy,” Annual Review of Nuclear and Particle Science, 73, 153

Paz, Z., 2026a, “A First-Principles Derivation of the Selective Transient Field,” DOI:10.5281/zenodo.17526550 (V7.9)

Paz, Z., 2026b, “Cross-Disformal Matter Coupling in the STF Framework”

Paz, Z., 2026c, “STF Dark Energy w(z) Derivation V0.2 — Supporting Calculation: T² nodal structure giving w(z=0) = −1 exactly with effective phantom trajectory w(z) < −1 for z > 0; perturbation stability c_s²(z=0) = 1 exactly” (supporting derivation paper, STF_Dark_Energy_wz_Derivation_V0_2.md)

Paz, Z., 2026d, “Dark Matter as Geometry: The Selective Transient Field Framework for a Unified Dark Sector” (companion paper, STF_Dark_Matter_Paper_Full_v2_aligned.md)

Paz, Z., 2026e, “STF Galactic Sector — Marginal-Stability Closure Derivation V0.1 — Supporting Calculation: fold-catastrophe derivation of P(X) ∝ X^{3/2}, RPA strong-screening regime, gravitomagnetic obstruction theorem, field-normalization theorem (only C_coll·γ³ is invariant), and γ_MOND canonical-form derivation; Z_Θ wavefunction renormalization flagged as priority HIGH open item” (supporting derivation paper, STF_Galactic_Sector_MarginalStability_Closure_V0_1.md)

Perlmutter, S. et al., 1999, “Measurements of Ω and Λ from 42 high-redshift supernovae,” ApJ, 517, 565

Pettorino, V., Amendola, L., Baccigalupi, C., & Quercellini, C., 2012, “Constraints on coupled dark energy using CMB data from WMAP and SPT,” Phys. Rev. D, 86, 103507

Poulin, V., Smith, T. L., Karwal, T., & Kamionkowski, M., 2018, “Early dark energy can resolve the Hubble tension,” Phys. Rev. Lett., 122, 221301

Reid, B. A. et al., 2010, “Cosmological constraints from the clustering of the Sloan Digital Sky Survey DR7 luminous red galaxies,” MNRAS, 404, 60

Riess, A. G. et al., 1998, “Observational evidence from supernovae for an accelerating universe and a cosmological constant,” AJ, 116, 1009

Riess, A. G. et al., 2022, “A comprehensive measurement of the local value of the Hubble constant with 1 km/s/Mpc uncertainty from the Hubble Space Telescope and the SH0ES Team,” ApJ Lett., 934, L7

Roy Choudhury, S. & Okumura, T., 2024, “Updated Cosmological Constraints in Extended Parameter Space with Planck PR4, DESI BAO, and Supernovae: Dynamical Dark Energy, Neutrino Masses, Lensing Anomaly, and the Hubble Tension,” ApJ Lett., 976, L11 (arXiv:2409.13022)

Roy Choudhury, S. et al., 2025, “DESI results: Hint towards coupled dark matter and dark energy” (arXiv:2503.10806)

Steinhardt, P. J., Wang, L., & Zlatev, I., 1999, “Cosmological tracking solutions,” Phys. Rev. D, 59, 123504

Vagnozzi, S., 2023, “Seven hints that early-time new physics alone is not sufficient to solve the Hubble tension,” Universe, 9, 393

Verlinde, E. P., 2010, “On the origin of gravity and the laws of Newton,” J. High Energy Phys., 04, 029

Verlinde, E. P., 2017, “Emergent gravity and the dark universe,” SciPost Phys., 2, 016

Weinberg, S., 1989, “The cosmological constant problem,” Rev. Mod. Phys., 61, 1

Wetterich, C., 1995, “The cosmon model for an asymptotically vanishing time-dependent cosmological ‘constant’,” Astron. Astrophys., 301, 321

Wetterich, C., 2007, “Phenomenological parameterization of quintessence,” Phys. Lett. B, 655, 201


April 2026. Z. Paz, The Hague, Netherlands. Corresponding author: [email]

Companion papers in the framework: - STF First Principles V7.9 (Paz 2026a) — main framework derivation - STF Dark Matter Full v2 aligned (Paz 2026d) — applied dark-matter paper, parallel structure to this paper - STF Dark Energy w(z) Derivation V0.2 (Paz 2026c) — supporting calculation for w(z) result - STF Galactic Sector Marginal-Stability Closure V0.1 (Paz 2026e) — supporting calculation for γ_eff - STF Cross-Disformal Coupling (Paz 2026b) — UV motivation for cross-disformal matter coupling

@article{paz2026darkenergy, author = {Paz, Z.}, title = {Dark Energy as Geometry: The STF Framework and the T² Causal Diamond}, year = {2026}, version = {V0.1}, url = {https://existshappens.com/papers/dark-energy/} }