“…For constant ansatz functions we define C 0 := {0 d−1 }, whereas for q = 1 the set C 1 consists of the corners of the reference element [−1, 1] d−1 . The non-conforming ansatz was proposed in [36] and convergence is shown for an elastic two-body problem in [29]. In the case of lower polynomial degrees q = 0, 1, this ansatz becomes conforming, since the choice of C q leads to a uniform sign condition on the elements E ∈ B H .…”