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For some metric, we can calculate the horizon $g_{rr} = 0$, and therefore we can move to a set of coordinates where this horizon is removed.
E.g. for Kerr, move to a set of coordinates where the one-form filed $l_\mu = (- \Delta, - \Sigma, 0, \Delta a \sin^2 \theta)$ associated with the ingoing principle null congruences of the spacetime becomes $l_{\tilde{\mu}} = (-1, -1, 0, a \sin^2 \tilde{\theta})$.
The PNCs can be derived from the Weyl tensor acting on null vectors of the spacetime.
We can then build a Jacobian that maps from the Boyer Lindquist coordinates to the ingoing Kerr-Schild coordinates, giving an horizon-penetrating form of the metric.
I reckon we can probably come up with a way of numerically solving for this transformation, and then transforming the metric on the fly as we do ray tracing. This would be particularly useful for studying weird spacetimes.
For some metric, we can calculate the horizon$g_{rr} = 0$ , and therefore we can move to a set of coordinates where this horizon is removed.
E.g. for Kerr, move to a set of coordinates where the one-form filed$l_\mu = (- \Delta, - \Sigma, 0, \Delta a \sin^2 \theta)$ associated with the ingoing principle null congruences of the spacetime becomes $l_{\tilde{\mu}} = (-1, -1, 0, a \sin^2 \tilde{\theta})$ .
The PNCs can be derived from the Weyl tensor acting on null vectors of the spacetime.
We can then build a Jacobian that maps from the Boyer Lindquist coordinates to the ingoing Kerr-Schild coordinates, giving an horizon-penetrating form of the metric.
I reckon we can probably come up with a way of numerically solving for this transformation, and then transforming the metric on the fly as we do ray tracing. This would be particularly useful for studying weird spacetimes.
https://arxiv.org/abs/2408.09893
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