Conformal invariants of twisted Dirac operators and positive scalar curvature

preprint2013arXivOpen access

Abstract

For a closed, spin, odd dimensional Riemannian manifold (Y,g)(Y,g), we define the rho invariant ρspin(Y,E,H,g)ρ_{spin}(Y,E,H, g) for the twisted Dirac operator DHED^E_H on YY, acting on sections of a flat hermitian vector bundle EE over YY, where H=∑ij+1H2j+1H = \sum i^{j+1} H_{2j+1} is an odd-degree closed differential form on YY and H2j+1H_{2j+1} is a real-valued differential form of degree 2j+1{2j+1}. We prove that it only depends on the conformal class of the pair [H,g][H,g]. In the special case when HH is a closed 3-form, we use a Lichnerowicz-Weitzenbock formula for the square of the twisted Dirac operator, to show that whenever YY is a closed spin manifold, then ρspin(Y,E,H,g)=ρspin(Y,E,g)ρ_{spin}(Y,E,H, g)= ρ_{spin}(Y,E, g) for all ∣H∣|H| small enough, whenever g is a Riemannian metric of positive scalar curvature. When HH is a top-degree form on an oriented three dimensional manifold, we also compute ρspin(Y,E,H,g)ρ_{spin}(Y,E,H, g).

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