Abstract
where s(Ht ) and s M denote, respectively, the scalar curvature of level hypersurface Ht and M at the point γ (t) and θ(t) is the mean curvature of Ht along γ (t). To calculate the upperbound of the volume expansion rate along a timelike geodesic γ in a Lorentzian manifold, we used the above differential Eq. (1). But we neglected the sign when we take the trace of the Gauss equation (p. 408). Taking the sign of an unit speed timelike geodesic into account, Eq. (1) must be corrected to
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.