A Lot of Basic Question About Lorentz-Minkowski Geometry

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Discussion Overview

The discussion revolves around various questions regarding Lorentz-Minkowski geometry, focusing on the properties of the Lorentz metric, the nature of spacelike, timelike, and lightlike vectors, and the relationships between different subspaces in this geometric framework. The questions touch on theoretical aspects and mathematical proofs related to these concepts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question whether the Lorentz metric is degenerate or non-degenerate, with one asserting it is non-degenerate based on the definition.
  • There is confusion about the inclusion of null and spacelike vectors in timelike subspaces and whether lightlike subspaces can contain spacelike vectors.
  • One participant challenges the claim that the sum of a spacelike vector and a timelike vector is always a null vector, providing counterexamples to illustrate this point.
  • Another participant discusses the dimensionality of subspaces, suggesting that timelike subspaces can only be one-dimensional, while spacelike subspaces can be three-dimensional.
  • There is a request for clarification on the relationship between null vectors and lightlike subspaces, with one participant expressing uncertainty about the definitions and implications of these terms.

Areas of Agreement / Disagreement

Participants express differing views on several questions, particularly regarding the properties of vector sums and the nature of subspaces. There is no consensus on the correctness of the claims made, and multiple competing interpretations are present.

Contextual Notes

Some participants use different conventions for the Lorentz metric, which may affect their interpretations. The discussion includes various assumptions about the vectors and their relationships, which remain unresolved.

Who May Find This Useful

This discussion may be of interest to those studying Lorentz-Minkowski geometry, including students and researchers in physics and mathematics, particularly in the context of special relativity and differential geometry.

nomather1471
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Hi there, i have a lot of question about Lorentz-Minkowski geometry:

1)
Is Lorentz metric degenere or non-degenere? Why?

2) In spacelike subspaces only spacelike vectors live in it there is not problem here but how can

we say that timelike subspaces include null and spacelike vectors and lightlike subspaces include

spacelike vector?

3) Let E1 spacelike and E2 timelike vector then E1+E2 is null vector, proof...?

4) If Sp{E1,E2} spacelike, Sp{E1,E3} and Sp{E2,E3}

are timelike planes Sp{E1,E2+E3} is lightlike plane?

5) E1+E2+E3 is spacelike vector but

Sp{E1,E1+E2+E3} is lightlike plane?

6) E2+E3 is lightlike vector but Sp{E2+E3,E3} is timelike plane?
 
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That is a lot of questions.
nomather1471 said:
3) Let E1 spacelike and E2 timelike vector then E1+E2 is null vector, proof...?
This is not true in general. In units where c=1 and using the (-+++) signature, then the sum of
E1=(0,1,0,0) and E2=(1,0,0,0) is null
E1=(0,1,0,0) and E2=(5,0,0,0) is timelike
E1=(0,5,0,0) and E2=(1,0,0,0) is spacelike

Hopefully other people will address the other questions.
 
DaleSpam said:
That is a lot of questions.This is not true in general. In units where c=1 and using the (-+++) signature, then the sum of
E1=(0,1,0,0) and E2=(1,0,0,0) is null
E1=(0,1,0,0) and E2=(5,0,0,0) is timelike
E1=(0,5,0,0) and E2=(1,0,0,0) is spacelike

Hopefully other people will address the other questions.

Thanks, i agree with you, these questions are from the Rafael Lopez Minkowski Lectures, about question 3 the author able to think the unit vectors, the original is E2+E3 is null so if we take E2=(0,1,0) and E3=(0,0,1) then E2+E3=(0,1,1) which is a null vector, here the signature is (+,+,-) in E13...
 
nomather1471 said:
Hi there, i have a lot of question about Lorentz-Minkowski geometry:

1)
Is Lorentz metric degenere or non-degenere? Why?

It's non-degenerate, because the representing matrix (\eta_{\mu \nu}=\mathrm{diag}(1,-1,-1,-1) (sorry for changing the convention within the thread, I'm used to the west-coast convention; if I'd change it, most probably I'd get confused myself).

nomather1471 said:
2) In spacelike subspaces only spacelike vectors live in it there is not problem here but how can we say that timelike subspaces include null and spacelike vectors and lightlike subspaces include spacelike vector?

I don't know, what you mean by "subspace". In the usual sense of subspaces of a vector space, indeed there exist three-dimensional subspaces of time-like vectors. They can be defined as to be 3D subspaces Minkowski-perpendicular to an arbitrary time-like vector.

Proof: Let n a time-like unit vector, i.e., n \cdot n=\eta_{\mu \nu} n^{\mu} n^{\mu}=1. Then you can build the following Lorentz transformation
({\Lambda^{\mu}}_{\nu})=\begin{pmatrix}<br /> n^0 &amp; \vec{n}^t \\<br /> \vec{n} &amp; 1+\frac{n^0-1}{\vec{n}^2} \vec{n} \otimes \vec{n}<br /> \end{pmatrix}<br />
in obvious notation. Then
E_0&#039;=n=\Lambda E_0, \quad E_j&#039;=\Lambda E_j
build a new Minkowski-orthonormal system, and \text{span}(E_1&#039;,E_2&#039;,E_3&#039;) is a 3D subspace containing only space-like vectors.

On the other hand subspaces with only time-like vectors are necessarily one-dimensional, because suppose you have two linearly independent space-like vectors n_1 and n_2 you can construct the vector
a=n_1-\frac{(n_1 \cdot n_2)}{n_2 \cdot n_2} n_2 \neq 0
within the subspace. It's Minkowski-perpendicular to the space-like vector n_2, but then it must be either spacelike or lightlike.

To prove this you just take a \cdot n_2=0 and write it out in components
a^0 \cdot n_2^0-\vec{a} \cdot \vec{n}=0 \; \Rightarrow \; |a^0|=\frac{|\vec{a} \cdot \vec{n}|}{n^0} \geq \frac{|\vec{a} \cdot \vec{n}|}{|\vec{n}|} \geq |\vec{a}|,
and thus
a \cdot a=(a^0)^2-\vec{a}^2 \leq 0.

In contradiction to the assumption the subspace necessarily contains at least one spacelike or lightlike vector. In conclusion, subspaces that contain only time-like vectors are one-dimensional.

nomather1471 said:
3) Let E1 spacelike and E2 timelike vector then E1+E2 is null vector, proof...?
is wrong as shown by the counter example by DaleSpam as are the other claims, or are their additional restrictions on the vectors E_j?
 
Sorry but i can't understand anything with physics notation, i think Lorentz metric be a non-degenerate because of the definition of degenere metric...I mean subspaces by subset of Lorentz space, timelike subspaces are space which has a non-degenerate metric on it and lightlike subspace are space which has a degenerate metric and different from {0}, but how can we guarantiate the lightlike space has a spacelike vector, our teach told this with tangent plane to the timeconi but i am not sure of the truth, the question is if any subspace contain null vector is this set must be a lightlike subspace?
 

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