  The problem of maintaining gauge invariance in the 2PI formulation of QED is
discussed. A modified form of the 2PI effective action is suggested in which
Ward identities for external (background field) and internal (quantum field)
gauge transformations are both satisfied, but in different manners. The
residual gauge-fixing dependence in this modified 2PI formulation vanishes in a
certain low momentum limit, which allows it to be used reliably for calculating
quantities such as transport coeffcients and soft field relaxation in hot gauge
theories.
