Two events and in a two-dimensional Minkowski-space. For the first observer (with space axis denoted by and time axis denoted by ), the two events are simultaneous, but not for the second observer (with axis and .)
For a four-velocity of an observers with the decomposition
the set of points
(events)
of the form with a fixed
is called the space at the time . The points from this set are called simultaneous for the observer . For another observer with the four-velocity , these points are not simultaneous. The concept of simultaneity of the observer depends on his decomposition of the Welt into space component and time component. If, for example, the four-velocity of the second observer is given, with respect to a Minkowski-basis of the first observer, by , then
is an orthonormal basis of the space component of the second observer. For the first observer, the events
and
are simultaneous, but they are not simultaneous for the second observer, because the first vector has the same description, and the second vector equals
The time component of the second event with respect to the second observer vector is .