TFP: Covariant Formulation

 

Covariant Formulation

We promote all derivatives to covariant derivatives with respect to the emergent metric gμν(x)g_{\mu\nu}(x):

  • Dμϕ=μϕ+aμD_\mu \phi = \nabla_\mu \phi + a_\mu

  • fμν=μaννaμ​

  • Action (for fields on M,gμν\mathcal{M}, g_{\mu\nu}):

S=d4xg[14fμνfμν+12A2gμν(μϕ+aμ)(νϕ+aν)V(A)]S = \int d^4x \sqrt{-g} \left[ -\frac{1}{4} f_{\mu\nu} f^{\mu\nu} + \frac{1}{2} A^2 g^{\mu\nu} ( \nabla_\mu \phi + a_\mu ) ( \nabla_\nu \phi + a_\nu ) - V(A) \right]

This is the gravitationally-coupled scalar-vector system with a flow-induced mass scale.


Step 2: Equations of Motion in Curved Spacetime

(a) Gauge field aμa_\mu

Varying SS with respect to aμa_\mu, we get:

νfνμ+A2(μϕ+aμ)=0\nabla^\nu f_{\nu\mu} + A^2 ( \nabla_\mu \phi + a_\mu ) = 0

Compare with curved-space Proca equation with a source from the scalar phase.

(b) Scalar phase ϕ\phi

Varying SS with respect to ϕ\phi, we find:

μ(A2(μϕ+aμ))=0\nabla_\mu \left( A^2 ( \nabla^\mu \phi + a^\mu ) \right) = 0

This is a conserved current condition for the total covariant flow of temporal phase plus gauge field.

(c) Metric gμνg_{\mu\nu}

To get the gravitational response, vary SS with respect to the metric:

Tμν=2gδSδgμν=fμαfν α14gμνfαβfαβ+A2(μϕ+aμ)(νϕ+aν)gμν[12A2(αϕ+aα)2V(A)]T_{\mu\nu} = \frac{2}{\sqrt{-g}} \frac{\delta S}{\delta g^{\mu\nu}} = f_{\mu\alpha} f_{\nu}^{\ \alpha} - \frac{1}{4} g_{\mu\nu} f_{\alpha\beta} f^{\alpha\beta} + A^2 \left( \nabla_\mu \phi + a_\mu \right) \left( \nabla_\nu \phi + a_\nu \right) - g_{\mu\nu} \left[ \frac{1}{2} A^2 (\nabla^\alpha \phi + a^\alpha)^2 - V(A) \right]

This stress-energy tensor now sources the Einstein field equations (or their TFP-modified analog):

Gμν+(TFP corrections)=8πGTμνG_{\mu\nu} + \text{(TFP corrections)} = 8\pi G \, T_{\mu\nu}

Step 3: Interpretation in TFP

In this model:

  • The metric gμν(x)g_{\mu\nu}(x) emerges from flow fluctuation correlations:

    gμν(x)=μδF(x)νδF(x)g_{\mu\nu}(x) = \langle \partial_\mu \delta F(x) \partial_\nu \delta F(x) \rangle
  • The gauge field aμa_\mu arises from phase gradients and temporal alignment

  • The scalar ϕ\phi tracks internal flow clock time

Gravity, in this picture, is not imposed — it’s generated by the very temporal flow coherence whose misalignment gives rise to gauge interactions.

So the Einstein equations are not assumed, but arise via variation of an effective action Γ[gμν,Fˉ]\Gamma[g_{\mu\nu}, \bar{F}], as I’ve been constructing.

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