Eta forms and the odd pseudodifferential families index

preprint2011arXivOpen access

Abstract

Let A(t)A(t) be an elliptic, product-type suspended (which is to say parameter-dependant in a symbolic way) family of pseudodifferential operators on the fibres of a fibration ϕϕ with base Y.Y. The standard example is A+itA+it where AA is a family, in the usual sense, of first order, self-adjoint and elliptic pseudodifferential operators and $t\in\bbR$ is the `suspending' parameter. Let $π_{\cA}:\cA(ϕ)\longrightarrow Y$ be the infinite-dimensional bundle with fibre at y∈Yy\in Y consisting of the Schwartz-smoothing perturbations, q,q, making Ay(t)+q(t)A_y(t)+q(t) invertible for all $t\in\bbR.$ The total eta form, $η_{\cA},$ as described here, is an even form on $\cA(ϕ)$ which has basic differential which is an explicit representative of the odd Chern character of the index of the family: % dη_{\cA}=π_{\cA}^*γ_A, \Ch(\ind(A))=[γ_{A}]\in H^{\odd}(Y). \tag{*}\label{efatoi.5} % The 1-form part of this identity may be interpreted in terms of the ττ invariant (exponentiated eta invariant) as the determinant of the family. The 2-form part of the eta form may be interpreted as a B-field on the K-theory gerbe for the family AA with \eqref{efatoi.5} giving the `curving' as the 3-form part of the Chern character of the index. We also give `universal' versions of these constructions over a classifying space for odd K-theory. For Dirac-type operators, we relate $η_{\cA}$ with the Bismut-Cheeger eta form.

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