Four-vectors, Minkowsky spacetime.

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SUMMARY

This discussion focuses on the concepts of timelike, spacelike, and lightlike separations in Minkowski spacetime, particularly in the context of relativistic electrodynamics. Timelike events have a positive spacetime interval (ds² > 0), spacelike events have a negative interval (ds² < 0), and lightlike events have a zero interval (ds² = 0). The Minkowski metric is defined as ηαβ = diag(1, -1, -1, -1), which determines the nature of the separation between events. The physical implications include the ability of observers to perceive events as simultaneous or occurring at the same location based on their separation type.

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  • Understanding of Minkowski metric (ηαβ = diag(1, -1, -1, -1))
  • Familiarity with spacetime diagrams and lightcones
  • Basic knowledge of four-vectors in physics
  • Concept of causality in relativistic physics
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norbert
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somebody know about this terms: "timelike, spacelike or lightlike"
they often are used in relativistic electrodynamic
i.e when I´m referring to the lightcone in a spacetime diagram.
I would like some physics-interpretation of this concepts.
thanks.
D. Norbert
 
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These basically apply to three different possibilities for the spacetime distance between two events: positive, negative or zero. Lightlike (or null separated) events have zero distance between them; how timelike and spacelike match up with positive and negative depends on the signature of your metric. Suppose we use Minkowski metric \eta_{\alpha\beta}=diag(1,-1,-1,-1), then spacelike means ds^2&lt;0 and timelike means ds^2&gt;0. Here's where the names come from.

If we have two events such that the spatial distance between them is equal to the time between them times the speed of light, i.e. ds^2=c^2dt^2-dx^2-dy^2-dz^2=0 then the events are lightlike since they can be connected by the path of a photon.

If there are two events that can't be joined by the path of any real particle (i.e. one traveling at or below the speed of light) then the events are spacelike. An example is two simultaneous (in a given frame) events at different spatial locations. Then dt^2=0 since no time elapses between the events, and ds^2=-dx^2-dy^2-dz^2&lt;0. You can sort of think of it as being that they are spacelike because there is `more space than time between them'.

Finally, two events which can be joined by the path of a massive particle (i.e. traveling with v<c) are timelike - e.g. `more time than space between them' such as two events that happen in the same place but at different times. Then there is no spatial distance between them so dx^2=dy^2=dz^2=0 and we have ds^2=c^2dt^2&gt;0.
 
Just to add to mikeu's post,
timelike is a direction from the vertex pointing inside the lightcone,
lightlike (or null) is a direction from the vertex pointing along the lightcone,
spacelike is a direction from the vertex pointing outside the lightcone.


These adjectives apply to the generic four-vector, as well as the displacement four-vector.

Physically:
Timelike-related events are said to be "chronologically connected".
Nonspacelike-related events are said to be "causally connected".
Spacelike-related events are not causally connected. Such events cannot influence each other.
 
The physical interpretation is:

  • If two events have a timelike separation, then there is an inertial observer who thinks they occur at the same place
  • If two events have a spacelike separation, then there is an inertial observer who thinks they occur at the same time
  • If two events have a null (lightlike) separation, then a photon can pass between them
 

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