The joint variational problem reveals a coupled Einstein-Yang-Mills system, suggesting new structural hierarchies in gravity and gauge dynamics.
The companion papers Gravity 3.0 and Q12 derived, respectively, the Einstein tensor as the horizontal a₂ response and the Yang–Mills equations as the vertical a₄ response of the projective spectral entropy functional S_Π[g,A] = 1/2log' Ag,A. The present paper carries out the gauge–gravity synthesis and establishes its central conceptual consequence: gravity and gauge dynamics are not unified by enlarging the symmetry group or adding fields, but are stratified by the Seeley–DeWitt level at which the same admissible operator responds to variation. The conventional question ``what symmetry unifies gravity and gauge?'' is thereby replaced by ``at what spectral order does the projection respond?'' We solve the joint variational problem δg,AS_Π = 0 and derive the coupled Einstein–Yang–Mills system: the Yang–Mills stress tensor sources gravity through the metric dependence of the a₄ coefficient, with coupling constant 8π GN = cYM/cEH fixed by the Seeley–DeWitt expansion alone. We compute the a₆ coefficient and identify the leading gauge–gravity cross-coupling RμνρσFμνFρσ. The Eddington–Born–Infeld completion of the joint functional is constructed from the same Born–Infeld saturation bound that governs the gravitational sector . The gauge–gravity hierarchy is a structural output of the spectral stratification: gravity is induced at a₂ (quadratic UV divergence) and gauge at a₄ (logarithmic UV divergence), from the same cutoff ₛₚ, giving: \[ G_N g^2YM \;~\; {ₛₚ^2}{ V} ·[logΛ/μ]⁻¹ \;\; 1, \] without fine-tuning. The spectral stratification a₂ → gravity,\; a₄ → gauge,\; a₆ → mixed coupling predicts that fermionic structure should appear at a dedicated spectral level carrying a Dirac-type admissible operator, which is the central open question for the continuation of the programme. The gauge group G_Π is inherited from the spectral admissibility sub-programme ; the SU(3) sector is unconditional: [H-color]eff (equality of capacity exponents) and [H-color]pointwise (exact equality at finite q) are both established analytically in .
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Jérôme Beau (2026) studied this question.
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