“…The Griffith energy (G) is approximated by the functionalŝ Ω (v + η ε )f p (e(u)) + (1 − v) 2 4ε + ε q−1 |∇v| q dx , lim ε→0 η ε ε p−1 = 0 , (G ε ) for u ∈ W 1,p u 0 (Ω; R n ) := W 1,p (Ω; R n )∩{u : tr ∂Ω (u−u 0 ) = 0 on ∂ D Ω}, v ∈ W 1,q 1 (Ω; [0, 1]) := W 1,q (Ω; [0, 1]) ∩ {v : tr ∂Ω v = 1 on ∂ D Ω}, and +∞ otherwise: such approximation has been proven without any a priori assumption on u, for any p > 1, and in any dimension in [25], together with compactness for minimisers (see [26]), assuming that O δ,x 0 (∂ D Ω) ⊂ Ω for δ ∈ (0, δ), (1.2) for some δ > 0 and x 0 ∈ R n , where O δ,x 0 (x) := x 0 + (1 − δ)(x − x 0 ). This generalises [21,22,51], assuming a priori u ∈ L 2 and p = 2, [28], requiring u ∈ L p , p > 1, and [43], obtained in dimension 2 (see also e.g. [45,18,53] for the antiplane shear case and different approximations).…”