2013/11/17 by Matthias Fischmann, Fischmann, Matthias · 1 citation
Mathematics · Physics and Astronomy · #53A30 (Primary) 53C27 #53C80 (Secondary) #Advanced Differential Geometry Research #Advanced Topics in Algebra #Algebraic and Geometric Analysis #Differential Geometry (math.DG) #FOS: Mathematics
paper · pdf · doi:10.48550/arxiv.1311.4182
openalex publication_date 2013/11/17 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
The well known conformal covariance of the Dirac operator acting on spinor fields over a semi Riemannian spin manifold does not extend to powers thereof in general. For odd powers one has to add lower order curvature correction terms in order to obtain conformal covariance. We derive an algorithmic construction in terms of associated tractor bundles to compute these correction terms. Depending on the signature of the semi Riemannian manifold in question, the obtained conformal powers of the Dirac operator turn out to be formally self-adjoint with respect to the L2-scalar product, or formally anti-self-adjoint, respectively. Working out this algorithm we present explicit formulas for the conformal third and fifth power of the Dirac operator. Furthermore, we present a new family of conformally covariant differential operators acting on the spin tractor bundle which are induced by conformally covariant differential operators acting on the spinor bundle. Finally, we will give polynomial structures for the first examples of conformal powers in terms of first order differential operators acting on the spinor bundle.