The Callias Index Formula Revisited

preprint2016arXivOpen access

Abstract

We revisit the Callias index formula for Dirac-type operators LL in odd space dimension nn, and prove that \begin{align} \text{ind} \, (L) =\bigg(\frac{i}{8π}\bigg)^{\frac{n-1}{2}}\frac{1}{2(\frac{n-1}{2})!} \lim_{Λ\to\infty}\frac{1}{Λ}\sum_{i_{1},\dots,i_{n} = 1}^n \varepsilon_{i_{1}\dots i_{n}} \int_{ΛS_{n-1}}\text{tr}_{\mathbb{C}^d}\, (U(x)(\partial_{i_{1}}U)(x)\dots (\partial_{i_{n-1}}U)(x)) x_{i_{n}}\, d^{n-1} σ(x), \, (*) \end{align} where U(x)=sgn (Φ(x))U(x) = \text{sgn} \,(Φ(x)) and LL in L2(Rn)2n^dL^{2}(\mathbb{R}^{n})^{2^{\widehat n}d} is of the form L=Q+Φ, L= \mathcal{Q} + Φ, where Q=(∑j=1nγj,n∂j)Id, \mathcal{Q} = \bigg(\sum_{j=1}^{n}γ_{j,n}\partial_{j}\bigg) I_d, with γj,nγ_{j,n} elements of the Euclidean Dirac algebra, and n=2n^n=2{\widehat n} or n=2n^+1n=2{\widehat n}+1. Here ΦΦ is assumed to satisfy the following conditions: \begin{align} & Φ\in C_{b}^{2}\big(\mathbb{R}^{n};\mathbb{C}^{d\times d}\big), \quad d \in \mathbb{N}, \\ & Φ(x)=Φ(x)^{*}, \end{align} there exists c>0c>0, R≥0R\geq0 such that ∣Φ(x)∣≥cId,x∈Rn\B(0,R), |Φ(x)|\geq c I_d, \quad x\in\mathbb{R}^{n}\backslash B(0,R), and there exists ε>1/2\varepsilon> 1/2 such that for all α∈N0nα\in\mathbb{N}_{0}^{n}, ∣α∣<3|α|<3, there is κ>0κ>0 such that ∥(∂αΦ)(x)∥≤{κ(1+∣x∣)−1,∣α∣=1,κ(1+∣x∣)−1−ε,∣α∣=2,x∈Rn. \|(\partial^αΦ)(x)\|\leq \begin{cases} κ(1+|x|)^{-1}, & |α|=1,\\ κ(1+ |x|)^{-1-\varepsilon}, & |α|=2, \end{cases}\quad x\in\mathbb{R}^{n}. These conditions on ΦΦ render LL a Fredholm operator, and appear to be the most general conditions known to date for which Callias' index formula has been derived. Generalizations of the index formula (∗)(*) to certain classes of non-Fredholm operators LL invoking the (generalized) Witten index are also discussed.

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