An accelerated electron emits photons (which once was the problem for the old atomic model because it implies the electron should spiral down on the nucleus, which it to a certain extent does in discrete steps, but it halts in the lowest available orbital). It's discussed in this question.
Bremsstrahlung (German for "deceleration radiation") occurs when a charge is decelerated. For example, a charge entering an electric field, or interacting with another electron. Which is understandable as the field around the electron undergoes a sudden change.
If we express this by means of a Feynman diagram with the time axis vertically and the space axis horizontally (a procedure which can be doubted, but defended just as well), the associated Feynman diagram is simple:
Do we simply add a curly external leg to an outgoing leg, corresponding to a real photon? Like we can add bubbles to them, like for the anomalous magnetic moment:
The right side of the diagram stays the same.
Can we, for Bremsstrahlung, just add a real external photon curly?

