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===== #### ===== # Surface Geometry (4πr²): This is correctly built into the action, matching your idea that energy interactions happen over a spherical surface. # Field Formulation: Using a scalar field φ(t, r) lets us model energy/momentum flow across the surface over time—consistent with the QAT concept of unfolding time via photon-electron interactions. # Lagrangian Form: The form we’ve used is standard in classical and quantum field theory. We’ve only omitted the potential term V(ϕ)V(\phi)V(ϕ), which could later encode QAT-specific geometry or quantization. ====== - No Explicit h2π\frac{h}{2\pi}2πh: While geometry is built-in, Planck’s constant hasn't yet been embedded. The action should be dimensionally consistent with energy × time (or hhh), so that will need to be added next. ====== * No Coupling to Curvature Yet: This only represents flat-space spherical dynamics. We haven’t yet linked this to spacetime curvature as in the Einstein Field Equation. ====== We can insert the Planck constant h/2πh/2\pih/2π explicitly into this action as a coefficient to preserve dimensionality and link to QAT's quantum origin. That gives: ====== S=h2π∫dt dr [2πr2((∂ϕ∂t)2−(∂ϕ∂r)2)]S = \frac{h}{2\pi} \int dt \, dr \, \left[ 2\pi r^2 \left( \left( \frac{\partial \phi}{\partial t} \right)^2 - \left( \frac{\partial \phi}{\partial r} \right)^2 \right) \right]S=2πh∫dtdr[2πr2((∂t∂ϕ)2−(∂r∂ϕ)2)] Or, pulling out hhh: S=h∫dt dr r2((∂ϕ∂t)2−(∂ϕ∂r)2)S = h \int dt \, dr \, r^2 \left( \left( \frac{\partial \phi}{\partial t} \right)^2 - \left( \frac{\partial \phi}{\partial r} \right)^2 \right)S=h∫dtdrr2((∂t∂ϕ)2−(∂r∂ϕ)2) This would imply the process is quantized per action unit hhh and spatially governed by spherical symmetry — directly supporting QAT. Would you like to now: # Extend this to derive a wave equation via the Euler-Lagrange principle? # Add a potential term to model symmetry-breaking (e.g., charge separation)? # Link this to spacetime curvature by inserting a curvature term RRR?
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