We revisit the Callias index formula for Dirac-type operators in odd space dimension , and prove that \begin{align} , (L) =\bigg(\frac{i}{8\pi}\bigg)^{\frac{n-1}{2}}\frac{1}{2(\frac{n-1}{2})!} \lim_{\Lambda \to\infty}\frac{1}{\Lambda }\sum_{i_{1},\dots,i_{n} = 1}^n \varepsilon_{i_{1}\dots i_{n}} \int_{\Lambda S_{n-1}}{^d}, (U(x)(\partial{i_{1}}U)(x)\dots (\partial_{i_{n-1}}U)(x)) x_{i_{n}}, d^{n-1} \sigma(x), , () \end{align} where and in is of the form where with elements of the Euclidean Dirac algebra, and or $n=2{\widehat n}+1\Phi$ is assumed to satisfy the following conditions: \begin{align} & \Phi\in C_{b}^{2}\big(^{n};^{d\times d}\big), \quad d \in , \ & \Phi(x)=\Phi(x)^{}, \end{align} there exists , such that and there exists such that for all , , there is such that These conditions on render 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 invoking the (generalized) Witten index are also discussed.

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