Orthogonality of timelike and null vector

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    Orthogonality Vector
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Discussion Overview

The discussion centers on the orthogonality of timelike and null vectors within the context of spacetime geometry. Participants explore mathematical relationships and properties of these vectors, referencing concepts from differential geometry and the implications of Lorentz transformations.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants assert that if a vector \(X\) is timelike and another vector \(Y\) is orthogonal to \(X\), then \(Y\) must be spacelike.
  • One participant elaborates on the properties of vectors in a spacetime \( (M,g) \), using an orthonormal basis to show that certain inequalities imply \(Y\) is spacelike.
  • Another participant argues that a timelike vector can be transformed to be purely time-like, while a null vector has specific conditions that may prevent orthogonality.
  • Some participants reference the Cauchy-Schwarz inequality to support their claims about the relationship between the components of the vectors.
  • A participant expresses confusion regarding the notation used in the discussion, indicating a potential barrier for those less familiar with the topic.

Areas of Agreement / Disagreement

There is no consensus on the orthogonality of timelike and null vectors, with some participants supporting the idea that they can be orthogonal under certain conditions, while others argue against it based on the properties of null vectors.

Contextual Notes

Participants reference specific mathematical inequalities and properties of vectors, but the discussion does not resolve the implications of these relationships fully. There are also varying levels of familiarity with the notation and concepts presented.

Who May Find This Useful

This discussion may be of interest to students and researchers in geometry, physics, and mathematics, particularly those exploring the properties of vectors in spacetime and the implications of Lorentz transformations.

nomather1471
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Can we show orthogonality of timelike and null vector?
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If X is timelike, and Y is orthogonal to X, then Y is spacelike.
 
I just want to expand upon what George said. Let ##(M,g)## be a space-time and ##p\in M##. Furthermore, let ##X## be a time-like vector in ##T_p M## and ##Y## a non-zero vector in ##T_p M## such that ##g_p(X,Y) = 0##. Finally, let ##\{e_i \}## be an orthonormal basis for ##T_p M## so that ##X = X^i e_i## and ##Y = Y^i e_i##.

Then ##(X^2)^2 + (X^3)^2 + (X^4)^2 < (X^1)^2## and ##X^1 Y^1 = X^2 Y^2 + X^3Y^3 + X^4Y^4##.
Note this immediately implies that ##(X^1)^2 > 0## and that ##(Y^2)^2 + (Y^3)^2 + (Y^4)^2 > 0##.

Therefore (X^1 Y^1)^2 \leq ((X^2)^2 + (X^3)^2 + (X^4)^2)((Y^2)^2 + (Y^3)^2 + (Y^4)^2)&lt; (X^1)^2((Y^2)^2 + (Y^3)^2 + (Y^4)^2) thus ##(Y^1)^2 < (Y^2)^2 + (Y^3)^2 + (Y^4)^2## i.e. ##Y## is space-like.
 
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WannabeNewton said:
Finally, let ##\{e_i \}## be an orthonormal basis

WLOG, choose ##X = \{e_0 \}##.
 
A time-like vector can be Lorentz transformed to be purely time-like:x^\mu=(t,0).
A null vector always has x=t, so they can't be orthogonal.
 
Last edited by a moderator:
WannabeNewton said:
I just want to expand upon what George said. Let ##(M,g)## be a space-time and ##p\in M##. Furthermore, let ##X## be a time-like vector in ##T_p M## and ##Y## a non-zero vector in ##T_p M## such that ##g_p(X,Y) = 0##. Finally, let ##\{e_i \}## be an orthonormal basis for ##T_p M## so that ##X = X^i e_i## and ##Y = Y^i e_i##.

Then ##(X^2)^2 + (X^3)^2 + (X^4)^2 < (X^1)^2## and ##X^1 Y^1 = X^2 Y^2 + X^3Y^3 + X^4Y^4##.
Note this immediately implies that ##(X^1)^2 > 0## and that ##(Y^2)^2 + (Y^3)^2 + (Y^4)^2 > 0##.

Therefore (X^1 Y^1)^2 \leq ((X^2)^2 + (X^3)^2 + (X^4)^2)((Y^2)^2 + (Y^3)^2 + (Y^4)^2)&lt; (X^1)^2((Y^2)^2 + (Y^3)^2 + (Y^4)^2) thus ##(Y^1)^2 < (Y^2)^2 + (Y^3)^2 + (Y^4)^2## i.e. ##Y## is space-like.
I think you have to show that:
(X^1 Y^1)^2 \leq ((X^2)^2 + (X^3)^2 + (X^4)^2)((Y^2)^2 + (Y^3)^2 + (Y^4)^2)
 
nomather1471 said:
I think you have to show that:
(X^1 Y^1)^2 \leq ((X^2)^2 + (X^3)^2 + (X^4)^2)((Y^2)^2 + (Y^3)^2 + (Y^4)^2)

I had forgotten completely that one has the freedom to Lorentz boost to a frame wherein ##X = e_0## as stated by George and Clem above, which makes the calculation much simpler. Nevertheless, the above inequality follows directly from the Cauchy-Schwarz inequality.
 
I am student at geometry so your notation is quite different for me but thanks for everyone for all replies...
 

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