Tensor IDG resolves the scalar IDG trilemma, meets critical constraints, suggesting key predictions for future observations.
We present Tensor IDG, the resolution to the scalar IDG trilemma identified in Paper VII. Promoting the scalar field φ to a rank-2 symmetric tensor Φ_μν identified with the Fisher-Rao information metric, we demonstrate that the tensor Klein-Gordon equation □Φ_μν − m_s²Φ_μν = (β/M_Pl)T_μν simultaneously satisfies the S8 tension, CMB energy density bounds, and anisotropic chameleon screening — the three constraints the scalar theory could not jointly satisfy. We prove ghost-freedom via two independent arguments: (1) a kinematic argument showing the Fisher-Rao identification enforces det(Φ) > 0 as a covariance identity, and (2) an explicit lower bound theorem det(Φ(t)) ≥ det(Φ₀)·exp(−C·t²). We prove Tensor IDG lies outside the Horndeski class via three independent proofs: opposite sign of gravitational slip, violation of the (μ−1)(η−1) ≥ 0 consistency relation, and an anisotropic slip tensor with no scalar-tensor analog. The anisotropy factor f_aniso = 1/4 is an exact geometric identity, mass and concentration independent. The falsifiable Euclid prediction is η_IDG(k,z) = 1 − A(z)·k²/(k²+m_s²) with η < 1, detectable at SNR = 1.0–3.83 for β = 0.1–0.2. The Kähler geometry of the IDG statistical manifold fixes c_FR = 1/(16π²), leaving exactly two free parameters: m_s and β.
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Brian Cobham (2026) studied this question.
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