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 | | The smooth function $\mathcal{T}(x,t)=t$ is a {time-function}, that is the Lorentzian gradient $\nabla^L \mathcal{T}$ is a timelike vector field, where $$ \nabla^L\mathcal{T}(x,t) = \big({\bf 0},-\frac{1}{\beta(x)}\big). |
 | | Trajectories joining two given events have been studied in \cite{ba}, \cite{cm} on complete {\em stationary} Lorentzian manifolds, in \cite{ba1}, \cite{cm1} on open subsets of stationary Lorentzian manifolds and in \cite{agm} in a different setting. |
 | | Explicitly, from (\ref{electric}) and the expression of $\nabla$ in a static manifold (see for example \cite[Proposition 7.35]{onei}) \begin{equation} \label{ele} E = -(\beta)^{1/2} \nabla A_2 -\nabla \beta. |
| www.ma.hw.ac.uk /EJDE/Volumes/2004/10/bartolo-tex (5104 words) |
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