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Let \[(U,V,\theta, \phi)\] be Kruskal coordinates on the Kruskal manifold, where \[\large-UV=\left(\frac{r}{2m}-1\right)e^{r/2m},\hspace{1cm} t=2m\ln\left(\frac{-V}{U}\right)\] and θ and ϕ are the usual polar angles. The metric is \[\large ds^2=\frac{-32m^3}{r}e^{\frac{-r}{2m}}dUdV+r^2d\Omega^2\] The killing vector is: \[\xi=-U\partial_U+V\partial_V\] express ξ in exterior Schwarzschild coordinates.
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