At every point its second fundamental form is a scalar multiple of its induced metric. Equivalently its shape operator is scalar, so all principal normal curvatures agree. For a three-dimensional hypersurface, and . The sign of its intrinsic scalar in a vacuum Lorentzian ambient space then follows from the Gauss equation for a nonnull hypersurface.
For a timelike unit normal with squared norm epsilon and vanishing ambient Ricci tensor, contraction of the Gauss equation for a nonnull hypersurface gives the displayed formula. In signature the timelike normal has epsilon plus one, so the scalar of the induced negative-definite metric is nonnegative. In signature the positive-definite spatial metric instead has scalar . Replacing the induced metric by its negative reverses the scalar, so the inequality must not be transferred between these conventions without adjustment.
// Target: general-relativity.bigb
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