K-Monogenic Functions Over 6-Dimensional Euclidean Space

Abstract

Recently, physicists are interested in 6-dimensional physics including the massless field operators on Lorentzian space \(\mathbb R^{5,1}\). The elliptic version \(\mathcal {D}_{k}\) of these operators coincides with the higher spin massless field operators on \(\mathbb R^{6}\) introduced by Soucek earlier. The embedding of \(\mathbb R^{6}\) into the space of complex antisymmetric matrices allows us to use two-component notation, generating the Penrose two-spinor notation for dimension 4, which makes the spinor calculus on \(\mathbb R^6\) more concrete and explicit. A function annihilated by \(\mathcal {D}_{k}\) is called k-monogenic. Applying the Penrose integral formula, which can be checked by direct differentiation, we give infinite number of such k-monogenic polynomials for fixed k. So the function theory of k-monogenic functions is abundant and interesting.