Gauge Theory
#Physics
Invariant Lagrangian for certain transforms
Topics
$\displaystyle (\nabla ^{2}\vec{A}-{\mu}{0}{\varepsilon}{0}\partial_{t}^{2}\vec{A})-\nabla (\nabla \cdot \vec{A}+{\mu}{0}{\varepsilon}{0}\partial_{t}V)=-{\mu}_{0}\vec{J}$
- This along with Poisson's Equation encapsulate Maxwell's equations