Causality
Let events
and
have spacetime coordinates (
, 0, 0,
) and (
, 0, 0,
) in some inertial
reference frame,
. Suppose that event
causes event
. It follows that
. In other words, event
necessarily precedes event
in time. Let
 |
(3.126) |
be the velocity with which information flows from event
to event
in order to allow the former event to cause the latter. Let us observe the two events in a second inertial frame,
, that moves at velocity
with respect to
, and is in a standard configuration with respect to
.
According to Equation (3.103),
 |
(3.127) |
or
 |
(3.128) |
Now, irrespective of the value of
, whose magnitude can never exceed
, event
can never occur prior to event
in
, otherwise we could classify inertial frames into two groups; those in which event
appears to cause event
, and
those in which event
appears to cause event
. However, this state of affairs is forbidden by Einstein's first postulate.
Thus, we require
for all
. It is clear from Equation (3.128) that this is only possible if
. Hence, we deduce that
information can never propagate faster than the speed of light in vacuum, in any inertial reference frame, otherwise it is possible to find other inertial reference frames in which causality appears to be violated.