For , an ingoing chart with has metric . In its future interior, is future timelike, so every future causal curve decreases and cannot reach future null infinity. The singularity is spacelike. A Kruskal–Szekeres coordinates extension has the same qualitative Penrose diagram as Schwarzschild spacetime, with two exterior regions, a future black-hole interior and a past white hole interior. The past interior has the same radial interval but is not a black hole region; specifying the radial interval alone does not identify the future component. For , the physical exterior has everywhere and outgoing null rays escape from arbitrarily near a timelike naked singularity.

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