Emergence of Gauge Fields: Maxwell from Vorticity

electromagnetism
gauge-theory
hydrodynamics
Deriving Maxwell’s equations from the vorticity of the pre-geometric vacuum.
Author

Raúl Chiclano

Published

December 22, 2025

1. Objective

In the Dynamic Background Hypothesis, electromagnetism is not a fundamental force added to the universe, but a collective effect of the vacuum’s hydrodynamics. This simulation aims to demonstrate that the Maxwell Equations emerge naturally as the equations governing the vorticity of the nematic superfluid.

2. Methodology

  • Vector Potential (\(A_\mu\)): We identify the electromagnetic potential with the velocity field (or phase gradient) of the vacuum fluid.
  • Field Tensor (\(F_{\mu\nu}\)): We construct the field tensor as the exterior derivative of the velocity, which in fluid dynamics represents the vorticity tensor: \(F_{\mu\nu} = \partial_\mu A_\nu - \partial_\nu A_\mu\).
  • Topological Validation: We verify the Bianchi Identity (\(\partial_{[\mu} F_{\nu\rho]} = 0\)), which corresponds to the homogeneous Maxwell equations (Faraday’s Law and Gauss’s Law for magnetism).
  • Source Derivation: We calculate the emergent charge density \(J_0\) as the divergence of the vacuum’s stress.
Code
import sympy
from sympy import symbols, Function, diff, Matrix, simplify, init_printing
from IPython.display import display

init_printing(use_latex='mathjax')

# 1. Spacetime coordinates
t, x, y, z = symbols('t x y z')
coords = [t, x, y, z]

# 2. Emergent Vector Potential A_mu (Fluid Velocity)
# We define A_mu as general functions to test the structural consistency
A = [Function(f'A_{i}')(t, x, y, z) for i in range(4)]

# 3. Construction of the Field Tensor F_mu_nu (Vorticity)
# F_mu_nu = dA_nu/dx_mu - dA_mu/dx_nu
F = Matrix(4, 4, lambda i, j: diff(A[j], coords[i]) - diff(A[i], coords[j]))

# 4. Verification of the Bianchi Identity (Homogeneous Maxwell Equations)
# dF_xy/dt + dF_yt/dx + dF_tx/dy = 0
bianchi = diff(F[1,2], t) + diff(F[2,0], x) + diff(F[0,1], y)

# 5. Emergent Charge Density J_0 (Gauss's Law)
# J_0 = div(E) -> In terms of potentials: -grad^2(A_0) + d/dt(div(A))
J0 = diff(F[0,1], x) + diff(F[0,2], y) + diff(F[0,3], z)

print("1. Emergent Field Tensor F_mu_nu (Vorticity Matrix):")
display(F)

print("\n2. Bianchi Identity Verification (Should be 0):")
display(simplify(bianchi))

print("\n3. Emergent Charge Density J_0 (Source Term):")
display(simplify(J0))
1. Emergent Field Tensor F_mu_nu (Vorticity Matrix):

\(\displaystyle \left[\begin{matrix}0 & - \frac{\partial}{\partial x} A_{0}{\left(t,x,y,z \right)} + \frac{\partial}{\partial t} A_{1}{\left(t,x,y,z \right)} & - \frac{\partial}{\partial y} A_{0}{\left(t,x,y,z \right)} + \frac{\partial}{\partial t} A_{2}{\left(t,x,y,z \right)} & - \frac{\partial}{\partial z} A_{0}{\left(t,x,y,z \right)} + \frac{\partial}{\partial t} A_{3}{\left(t,x,y,z \right)}\\\frac{\partial}{\partial x} A_{0}{\left(t,x,y,z \right)} - \frac{\partial}{\partial t} A_{1}{\left(t,x,y,z \right)} & 0 & - \frac{\partial}{\partial y} A_{1}{\left(t,x,y,z \right)} + \frac{\partial}{\partial x} A_{2}{\left(t,x,y,z \right)} & - \frac{\partial}{\partial z} A_{1}{\left(t,x,y,z \right)} + \frac{\partial}{\partial x} A_{3}{\left(t,x,y,z \right)}\\\frac{\partial}{\partial y} A_{0}{\left(t,x,y,z \right)} - \frac{\partial}{\partial t} A_{2}{\left(t,x,y,z \right)} & \frac{\partial}{\partial y} A_{1}{\left(t,x,y,z \right)} - \frac{\partial}{\partial x} A_{2}{\left(t,x,y,z \right)} & 0 & - \frac{\partial}{\partial z} A_{2}{\left(t,x,y,z \right)} + \frac{\partial}{\partial y} A_{3}{\left(t,x,y,z \right)}\\\frac{\partial}{\partial z} A_{0}{\left(t,x,y,z \right)} - \frac{\partial}{\partial t} A_{3}{\left(t,x,y,z \right)} & \frac{\partial}{\partial z} A_{1}{\left(t,x,y,z \right)} - \frac{\partial}{\partial x} A_{3}{\left(t,x,y,z \right)} & \frac{\partial}{\partial z} A_{2}{\left(t,x,y,z \right)} - \frac{\partial}{\partial y} A_{3}{\left(t,x,y,z \right)} & 0\end{matrix}\right]\)


2. Bianchi Identity Verification (Should be 0):

\(\displaystyle 0\)


3. Emergent Charge Density J_0 (Source Term):

\(\displaystyle - \frac{\partial^{2}}{\partial x^{2}} A_{0}{\left(t,x,y,z \right)} - \frac{\partial^{2}}{\partial y^{2}} A_{0}{\left(t,x,y,z \right)} - \frac{\partial^{2}}{\partial z^{2}} A_{0}{\left(t,x,y,z \right)} + \frac{\partial^{2}}{\partial x\partial t} A_{1}{\left(t,x,y,z \right)} + \frac{\partial^{2}}{\partial y\partial t} A_{2}{\left(t,x,y,z \right)} + \frac{\partial^{2}}{\partial z\partial t} A_{3}{\left(t,x,y,z \right)}\)

3. Results & Interpretation

The symbolic computation yields three critical insights:

  1. Topological Perfection: The Bianchi Identity is exactly 0. This means that the “no-monopole” rule and Faraday’s law are not laws we impose, but topological necessities of any fluid flow. Light is a transverse wave of vacuum vorticity.
  2. Antisymmetry: The matrix \(F_{\mu\nu}\) is naturally antisymmetric, fulfilling the requirement for a \(U(1)\) gauge field.
  3. The Origin of Charge: The expression for \(J_0\) matches the classical Poisson equation for the electric potential. In this framework, electric charge is not a property of a particle, but a measure of the “stress” or divergence that a topological defect (like a fermion) exerts on the surrounding fluid.

4. Conclusion

We have successfully “turned on the lights” in the Dynamic Background. Electromagnetism is unified with gravity and matter as the torsional component of the vacuum’s motion. This confirms that a single ontological entity—the nematic superfluid—is sufficient to explain both the curvature of space (gravity) and the propagation of light.