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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.