  We reassess the problem of symmetry restoration induced by observers'
acceleration within the context of interacting quantum field theories in
Minkowski spacetime. We argue that the imposition of a frame-independent
renormalization condition negates any observed symmetry restoration by a
Rindler observer. Technically, we compute the one-loop effective potential of a
$\lambda\varphi^4$ theory for an accelerated observer, employing a distinct
methodology from prior investigations. Emphasizing the intricacies of the
model's renormalization, the analysis offers novel insights into the interplay
between acceleration and spontaneous symmetry breaking in quantum field theory.
