SECTION 8 — UNIFIED CLASSICAL FIELDS (v8.3)
Geometry, Electromagnetism, and Scalar Dynamics from Coarse-Grained Alignment
By John Gavel
8.0 Overview
The coarse-grained alignment field \( A(x,t) \) (Section 2.3) is the fundamental classical observable of Temporal Flow Physics. All classical fields — scalar, vector, and metric — emerge as derived quantities:
- Scalar field: \( \phi(x,t) \equiv A(x,t) \)
- Vector potential: \( A_\mu \) from charge and current (Section 6)
- Metric: \( g_{\mu\nu} \) from correlations (Section 3)
No new fields are postulated. The unified classical action is the continuum limit of substrate tension minimization (Axiom 6).
8.1 Scalar Field as Alignment Order Parameter
From Section 2.3.1, the alignment field is:
\[ \phi(x,t) = A(x,t) = \lim_{R \to x} \frac{1}{|R|} \sum_{i \in R} F_i(t) \tag{8.1} \]
Its dynamics derive from the tension functional (Section 5.2.9.2):
\[ T[\phi] = \int d^d x \left[ \frac{1}{2} D (\nabla \phi)^2 - \frac{1}{2} \mu_{\text{eff}}^2 \phi^2 \right] \tag{8.2} \]
where:
- \( D = k_{\text{avg}} a^2 / (T_{\text{eff}} \tau_0) \) (Eq 2.12) penalizes spatial misalignment
- \( \mu_{\text{eff}}^2 = \kappa \tau_0 \) (Eq 5.21) reflects instability of mixed states (\( \phi = 0 \))
The equation of motion is \( \partial T / \partial \phi = 0 \):
\[ D \nabla^2 \phi - \mu_{\text{eff}}^2 \phi = 0 \quad \Rightarrow \quad \nabla^2 \phi = \frac{\mu_{\text{eff}}^2}{D} \phi \tag{8.3} \]
This is the static Klein-Gordon equation, with mass scale \( m_\phi^2 = \mu_{\text{eff}}^2 / D \) (Section 5.4).
8.2 Electromagnetic Coupling
From Section 4.5.1, charge density is net alignment:
\[ \rho_{\text{dim}} = \phi \tag{8.4} \]
From Section 4.10, motif velocity \( \mathbf{v}_C \) defines current:
\[ \mathbf{J}_{\text{dim}} = \phi \mathbf{v}_C \tag{8.5} \]
Charge conservation (Section 6.1.2) gives:
\[ \frac{\partial \phi}{\partial t} + \nabla \cdot (\phi \mathbf{v}_C) = 0 \tag{8.6} \]
The vector potential is the convolution (Section 6.3):
\[ A_\mu^{\text{dim}} = \left( \Phi_{\text{dim}}, \mathbf{A}_{\text{dim}} \right) = \int \frac{j_\mu^{\text{dim}}(\mathbf{x}')}{|\mathbf{x} - \mathbf{x}'|} d^3x' \tag{8.7} \]
where \( j_\mu^{\text{dim}} = (\rho_{\text{dim}}, \mathbf{J}_{\text{dim}}) \). In physical units (Section 5):
\[ A_\mu^{\text{phys}} = A_\mu^{\text{dim}} \cdot \frac{q_0}{L_c} \tag{8.8} \]
8.3 Gravitational Coupling
From Section 3.2, the metric \( g_{\mu\nu} \) is defined by operational distance \( d_{ij} \). In the continuum, minimal coupling replaces partial derivatives with covariant derivatives:
\[ \partial_\mu \phi \to \nabla_\mu \phi = \partial_\mu \phi - \Gamma^\lambda_{\mu\nu} \phi \tag{8.9} \]
The scalar field action becomes:
\[ S_\phi = \int d^4x \sqrt{-g} \left[ \frac{1}{2} g^{\mu\nu} \nabla_\mu \phi \nabla_\nu \phi - V(\phi) \right] \tag{8.10} \]
where \( V(\phi) = -\frac{1}{2} \mu_{\text{eff}}^2 \phi^2 \) (from Eq 8.2). This couples \( \phi \) to curvature via \( \sqrt{-g} \) and \( g^{\mu\nu} \) (Section 7).
8.4 Unified Classical Action
Combining scalar, vector, and metric sectors, the total action is:
\[ S = \int d^4x \sqrt{-g} \left[ \frac{1}{2} g^{\mu\nu} \nabla_\mu \phi \nabla_\nu \phi - V(\phi) - \frac{1}{4} F_{\mu\nu} F^{\mu\nu} \right] \tag{8.11} \]
where \( F_{\mu\nu} = \partial_\mu A_\nu - \partial_\nu A_\mu \) (Section 6.4). All terms derive from:
- \( \phi \): coarse-grained alignment (Section 2.3)
- \( A_\mu \): charge/current convolution (Section 6.3)
- \( g_{\mu\nu} \): correlation geometry (Section 3.2)
No external coupling constants are introduced — all scales are fixed by \( D \), \( \mu_{\text{eff}} \), \( L_c \), \( T_c \) (Sections 2, 5).
8.5 Field Equations
Varying (8.11) yields the classical field equations:
8.5.1 Scalar (Klein-Gordon)
\[ \nabla_\mu \nabla^\mu \phi + V'(\phi) = 0 \quad \Rightarrow \quad \Box \phi - \mu_{\text{eff}}^2 \phi = 0 \tag{8.12} \]
8.5.2 Vector (Maxwell)
\[ \nabla_\mu F^{\mu\nu} = j^\nu \tag{8.13} \]
where \( j^\nu = q_0 (\phi, \phi \mathbf{v}_C) \) (Section 6.1).
8.5.3 Tensor (Einstein)
\[ G_{\mu\nu} = 8\pi G_{\text{obs}} T_{\mu\nu} \tag{8.14} \]
with stress-energy:
\[ T_{\mu\nu} = \nabla_\mu \phi \nabla_\nu \phi - g_{\mu\nu} \left[ \frac{1}{2} (\nabla \phi)^2 - V(\phi) + \frac{1}{4} F_{\alpha\beta} F^{\alpha\beta} \right] \tag{8.15} \]
and \( G_{\text{obs}} = L_c^3 / (M_c T_c^2) \) (Eq 7.14).
8.6 Axiomatic Closure
| Field Concept | Substrate Origin | Axiom |
|---|---|---|
| Scalar \( \phi \) | Coarse-grained alignment \( A(x,t) \) | A2, A3 |
| Vector \( A_\mu \) | Charge/current convolution | A2, A6 |
| Metric \( g_{\mu\nu} \) | Correlation distance \( d_{ij} \) | A3 |
| Unified Action | Tension functional + calibration | A6, Section 5 |
8.7 Bridge to Section 9 — Quantization
Section 8 provides:
- Classical scalar field \( \phi = A(x,t) \)
- Unified action coupling \( \phi \), \( A_\mu \), and \( g_{\mu\nu} \)
- Field equations with no free parameters
Section 9 quantizes these fields by identifying \( \phi \) with flow multiplets \( \Psi = [F^{(0)}, F^{(1)}, F^{(2)}, F^{(3)}] \) (Section 13.3), recovering uncertainty, superposition, and CPT symmetry from substrate dynamics.
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