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 norm
For 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 coordinates
Substitution gives
There 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 is
This 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]
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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