Spinor Pairs and the Concentration Principle for Dirac operators

preprint2015arXivOpen access

Abstract

We study perturbed Dirac operators of the form Ds=D+sA:Γ(E)→Γ(F) D_s= D + s{\cal A} :Γ(E)\rightarrow Γ(F) over a compact Riemannian manifold (X,g)(X, g) with symbol cc and special bundle maps A:E→F{\cal A} : E\rightarrow F for s>>0s>>0. Under a simple algebraic criterion on the pair (c,A)(c, {\cal A}), solutions of Dsψ=0D_sψ=0 concentrate as s→∞s\to\infty around the singular set $Z_\A\subset X$ of A{\cal A}. We give many examples, the most interesting ones arising from a general ``spinor pair'' construction.

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