A regular hypersurface , with , is a null hypersurface if its normal covector has zero squared norm:Its normal vector is then also tangent to the hypersurface; the induced metric tensor is degenerate.
For the Kerr metric the normal to a constant- surface has squared normFor the two roots are positive and distinct. To verify that they are genuine regular null hypersurfaces, rather than trusting singular Boyer-Lindquist coordinates, introduce ingoing Kerr coordinatesSubstitution givesThere are no terms. At either root , and the determinant is away from the angular coordinate poles. Thus the metric tensor extends smoothly across each root. The raised normal on either surface isThis is a nonzero null Killing vector field normal to the surface. Both surfaces are Killing horizons, with horizon angular velocities .
The event-horizon terminology in the paper needs qualification. In the usual asymptotically flat Kerr black hole extension, relative to a chosen exterior's future null infinity, the future branch of is the event horizon, the boundary . In the intervening black-hole region , the coordinate has timelike gradient and future-directed curves move toward smaller ; they cannot return across the outer boundary to that exterior. The inner surface is a Cauchy horizon, not a second event horizon for the same asymptotic end. Nullness is a local property; identifying an event horizon additionally requires this global causal structure.[ref]
General Relativity by David Tong. Sections 6.3.2 and 6.2.4: regular extension across the two Kerr roots, global diagram and the inner Cauchy horizon
The allowed endpoint provides an especially concrete counterexample to the unrestricted description of both roots. The Kerr metric then becomes Schwarzschild spacetime, is its regular event horizon, but is a curvature singularity:It is not a regular inner null hypersurface. Thus the two-horizon calculation above assumes .
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