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IX. Spherically Symmetric Spacetimes
Photons
with frequency 4-vector ${\mathbf{k}} = (\nu ,\vec k)$, $\nu = \left| {\vec k}
\right|$, follow null trajectories ${{\mathbf{k}}^2} = 0$ specified by
the geodesic equation ${\mathbf{k}} \cdot D{\mathbf{k}} = 0$. A radial null
trajectory has tangent
\[{\mathbf{k}} = \nu ({{\mathbf{e}}_t} \mp
{{\mathbf{e}}_r}){\qquad}\nu : = {\mathbf{k}} \cdot {{\mathbf{e}}_t}\]
The minus sign applies to a light ray towards the center; the plus
sign to an outward light ray. The frequency $\nu $ is measured by
a radially free-falling observer (at rest at infinity).
From
(9.3) with (9.7), one derives the tangent in coordinate representation
\[{\mathbf{k}} = \nu {{\mathbf{g}}_t} -
\nu \left( { \pm 1 + \sqrt {2M/r} } \right) {{\mathbf{g}}_r}\]
It follows that the velocity along the photon path is
\[\frac{{dr}}{{dt}} = \pm 1 - \sqrt
{\frac{{2M}}{r}} \]
This result could have been directly obtained from the PG-metric
(9.6.) by setting $ds = 0$, $d\theta = 0$, $d\phi = 0$.
At the event
horizon, the speed of light (9.16) vanishes for rays shining outward
$(+)$: $dr/dt = 0$. More strangely, inside the event horizon, $r <
{r_{\text{S}}}$, this light ray moves toward the center, implying that
light cannot escape. It gets stuck at the event horizon which marks the
boundary between the interior region that cannot signal to the outer region.
Thus, everything inside the event horizon is hidden from the outside world: it
is a Black Hole.
Matter
can only move inwards from the event horizon. If any object collapses
to within its event horizon, it must carry on collapsing to form a central
singularity. There is no force capable of preventing the collapse. This is
because matter is always constrained to follow timelike paths, and if the
entire future light-cone points inwards towards the singularity, no matter can
escape. All paths for in-falling matter terminate on the singularity.