“…We refer to this setting as the Euclidean one, since the fundamental group leaving the Dirac operator ∂ invariant is the special orthogonal group SO(m; R), which is doubly covered by the Spin(m) group of the Clifford algebra R 0,m . In case the dimension m is even, say m = 2n, so-called hermitian Clifford analysis was recently introduced as a refinement of Euclidean Clifford analysis (see the books [44,25] and the series of papers [45,28,5,6,18,29,11]). The considered functions now take values in the complex Clifford algebra C 2n or in complex spinor space S n .…”