Minkowski Metric and the Sign of the Fourth Dimension

Click For Summary
SUMMARY

The discussion centers on the Minkowski metric and the necessity of the time unit vector being opposite in sign to spatial unit vectors in Minkowski spacetime, specifically the signature (-,+,+,+). This configuration is essential for maintaining the invariance of the speed of light across all reference frames, a fundamental aspect of relativity. The presence of Lorentz transformations allows for the mixing of time and space while preserving the light cone, which is a unique property of Minkowski space compared to Euclidean or Galilean spaces. The ten-dimensional Poincaré group, which includes translations and rotations, is also discussed as a critical framework for understanding these transformations.

PREREQUISITES
  • Understanding of Minkowski spacetime and its signature (-,+,+,+)
  • Familiarity with Lorentz transformations and their implications
  • Knowledge of the Poincaré group and its role in physics
  • Basic concepts of light cones and invariant vectors in spacetime
NEXT STEPS
  • Study the mathematical foundations of Lorentz transformations in detail
  • Explore the implications of the Poincaré group in theoretical physics
  • Investigate the differences between Minkowski, Euclidean, and Galilean spaces
  • Learn about the concept of invariant vectors and their significance in relativity
USEFUL FOR

Physicists, mathematicians, and students of theoretical physics who are interested in the geometric properties of spacetime and the foundational principles of relativity.

Epistimonas
Messages
9
Reaction score
0
Why is the unit vector for time in Minkowski space i.e. the fourth dimension unit vector always opposite in sign to the three other unit vectors?

The standard signature for Minkowski spacetime is either (-,+,+,+) or (+,-,-,-).

Is there some particular reason or advantage for making time opposite to the spatial dimensions?
 
Physics news on Phys.org
A mixed signature space has certain geometric properties different from ordinary, Euclidean space. One of them is the presence of directions that don't change regardless of "rotations" that mix up space and time. These "rotations" are Lorentz transformations, and these directions that are unchanged are the paths of light rays. Minkowski space is the only flat space with this property* being in line with what we know about relativity.

*You can have a (0,+,+,+) space where the timelike vector is invariant, but you can show this corresponds to Galilean invariance, which we know not to be present in the physical world.
 
Right okay that is a grand answer to my question, thank you. I am familiar with the Poincare group that contains the isometries of Minkowski spacetime. Essentially the answer you gave me was, "The negative time unit vector is required to fulfill the requirements of the 10-dimensional Poincare group, consisting of a translation through time, a transition through any 3 directions of space, a rotation around any of the three spatial axes, and a boost in any of the three directions."

If the time unit vector was not negative the the group of isometries of the spacetime of metric (+,+,+,+) would only be 7-dimensional, lacking in the rotation around any of the spatial axes.

Is this correct?
 
No, the group of isometries in (++++) signature is still ten-dimensional (6 rotations in the 6 orthogonal planes, and 4 translations).

The reason spacetime has the Minkowski signature (-+++) is because of the experimental fact that light has the same speed in every reference frame. Lorentz transformations can rotate among the 3 spatial directions, or they can mix time and space (via 3 boosts), but they always leave the lightcone intact.
 
If the time unit vector was not negative the the group of isometries of the spacetime of metric (+,+,+,+) would only be 7-dimensional, lacking in the rotation around any of the spatial axes.

Hm, I don't think so. Even a 4d Euclidean space would have 4 translational and 6 rotational degrees of freedom. The point I was trying to make was that the Minkowski signature is chosen because, in general terms, out of the three possibilities for a flat space--Euclidean, Galilean, and Minkowskian--only the latter has the correct notion for the principle of relativity. The others can be ruled out experimentally.

If you're asking from a pure math standpoint, then I'm not sure I understand the question.
 
Ben Niehoff said:
The reason spacetime has the Minkowski signature (-+++) is because of the experimental fact that light has the same speed in every reference frame. Lorentz transformations can rotate among the 3 spatial directions, or they can mix time and space (via 3 boosts), but they always leave the lightcone intact.

Okay so there must be a mathematical way of showing that for a (+,+,+,+) signature the speed of light is not the same in every reference frame, and that for a (-,+,+,+) or it's equivalent the speed of light has a constant speed in every frame?

And if that can be shown, then it could then be shown that the constant that the speed of light travels at is equivalent to the speed a massless particle travels?
 
Epistimonas said:
Okay so there must be a mathematical way of showing that for a (+,+,+,+) signature the speed of light is not the same in every reference frame, and that for a (-,+,+,+) or it's equivalent the speed of light has a constant speed in every frame?

And if that can be shown, then it could then be shown that the constant that the speed of light travels at is equivalent to the speed a massless particle travels?

The key is to show that, under generalized rotations, a Euclidean space has no invariant vectors in the plane of the rotation, whereas a Minkowski space does.
 
Okay so is what you're saying that the definition of a vector is that it is invariant under translation and rotation, and that in Euclidean space, vectors are not invariant under rotation and that in Minkowski space they are?
 
Definition of a vector, no. Obviously not every vector is invariant under rotations. But for there to be lightlike paths, there must be some vectors that are invariant under rotations, even when that vector is in the plane of rotation.
 

Similar threads

  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 22 ·
Replies
22
Views
1K
  • · Replies 40 ·
2
Replies
40
Views
3K
  • · Replies 32 ·
2
Replies
32
Views
3K
  • · Replies 17 ·
Replies
17
Views
2K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 32 ·
2
Replies
32
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
Replies
20
Views
3K
  • · Replies 8 ·
Replies
8
Views
2K