Can 4-velocity Have Negative Component in Curved M?

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SUMMARY

The discussion centers on the allowance of a negative zeroth-component of a four-velocity V^0 in a curved space metric with signature -+++. It establishes that while timelike vectors can represent an observer's frame of reference, the mathematical framework permits velocity vectors to lie on either side of the timelike light cone. The conversation emphasizes that special relativity (SR) and general relativity (GR) do not impose restrictions on the directionality of velocity vectors due to time-reversal invariance. Furthermore, it highlights that a timelike geodesic remains within the timelike region, ensuring that inertial observers do not cross into spacelike territory.

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  • Understanding of four-vectors in the context of special relativity
  • Familiarity with the concepts of timelike and spacelike vectors
  • Knowledge of curved space metrics and their signatures
  • Basic principles of general relativity and time-reversal invariance
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  • Investigate the properties of timelike and spacelike geodesics in general relativity
  • Study the mathematical framework of vector spaces in the context of relativity
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Physicists, particularly those specializing in relativity, cosmologists, and students of theoretical physics seeking to deepen their understanding of four-velocity and its implications in curved spacetime.

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Is a negative zeroth-component of a four-velocity V^0 with a curved space metric of signature -+++ allowed?
 
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I assume we're talking about timelike vectors. A spacelike vector that had a positive timelike component in one frame could have a negative one in a different frame. I think the question is better posed as whether we can prohibit velocity vectors from lying in a certain side of the timelike light cone.

If we restrict ourselves to timelike vectors, then any velocity vector can represent the frame of reference of an observer.

Mathematically either side of the light cone is certainly allowed, because this is a vector space, and one of the axioms of linear algebra is that if v is a vector, there's a vector -v.

Physically, SR is time-reversal invariant, so there is no fundamental physical distinction between the forward and backward directions of time. Therefore there is no fundamental way to state a prohibition on velocity vectors that point a certain way instead of the opposite way. GR inherits all the same local symmetries as SR, so this applies to GR as well. (Spacetimes in GR don't even have to be time-orientable.)

There are reasons that we have an arrow of time, but those reasons can't be found within the fundamental kinematical laws of relativity.

There is at least some kinematical guarantee of sanity, which is that a timelike geodesic always stays timelike. That implies that in SR an inertial observer will never have a velocity vector that wanders from one side of the light cone to the opposite side. (To do that, it would have to pass through the spacelike region.)

For particles, you can interpret this kind of thing in terms of matter/antimatter symmetry, i.e., flipping the velocity four-vector of an electron makes it an antielectron.
 
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Thank you, bcrowell!
 

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