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**Gauge Invariance in Classical Electrodynamics**

**Maxwell's equation**

suggests that there is a vector potential fulfilling

The magnetic field is unchanged if one adds a gradient of an arbitrary scalar field Î›:

Similar in line, the Maxwell equation

suggests that there is a scalar potential V fulfilling

In this case one can add a time derivative of an arbitrary scalar field Î› to the scalar potential V

without changing the electric field.

To summarize this in a covariant notation: The field-strength tensor

with

is unchanged under a 'gauge transformation'

with Î›(x) being an arbitrary function.

The same electrodynamics can be described by many different four-vector potentials. This is what is meant by GAUGE INVARIANCE of classical electrodynamics.

The two Maxwell equations from above are then rewritten as

The two remaining Maxwell equations

and

can be written in the compact form

with the electromagnetic current being

**CONSEQUENCES **

1) The electromagnetic current is conserved:

2) The time derivative of the electric field in the fourth Maxwell equation guaranteeing local charge conservation leads also to the prediction of electromagnetic waves:

In the absence of external electromagnetic currents and using the Lorentz gauge

one obtains for each compoenent of the four-potential (identified with the photon field) a Klein-Gordon equation for a massless particle: