We investigate several possible generalisations of \( T\overline{T} \) deformations to three- and higher-dimensional field theories. Starting from the two-dimensional \( T\overline{T} \) flow, we work out its higher-dimensional uplift, which results in a non-local and non-isotropic three-dimensional theory. Starting instead from the relation between the Nambu-Goto action and \( T\overline{T} \) in d = 2, we study the flow equation obeyed by the Dirac-Nambu-Goto actions in d > 2 dimensions, written in terms of the stress-energy tensor only. Similarly, we derive the stress-tensor flow obeyed by the Born-Infeld actions in d dimensions and by the Dirac-Born-Infeld actions in d = 2 and d = 3.