The Minkowski so-called 'metric'

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Discussion Overview

The discussion revolves around the nature of Lorentzian metrics, particularly the Minkowski metric, and whether they can be classified as true metrics or pseudometrics. Participants explore the definitions and properties of metrics in mathematical contexts, especially in relation to general relativity and pseudo-Riemannian spaces.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question whether Lorentzian metrics can be considered metrics at all, noting that they do not meet the criteria of traditional metrics or pseudometrics.
  • Others argue that a metric is defined as a symmetric non-degenerate tensor field of type (0,2), suggesting that the metric of general relativity, while not positive definite, still qualifies as a metric.
  • A participant emphasizes the primitive mathematical definition of a metric space and outlines the axioms that must be satisfied, raising concerns about the Minkowski metric's adherence to these axioms.
  • One participant cites a response from another user, Ambitwistor, indicating that the conditions for metrics in pseudo-Riemannian spaces are relaxed enough to accommodate the Minkowski metric.
  • Another participant reiterates that while the Minkowski metric does not fit the traditional definition of a metric, it serves a similar purpose in measuring distances and intervals in a vector space.
  • There is a discussion about the relationship between metrics and metric tensors, with some suggesting that the distinction is minimal as a metric tensor defines the metric for a vector space.

Areas of Agreement / Disagreement

Participants express differing views on whether Lorentzian metrics should be classified as metrics or pseudometrics, indicating that multiple competing perspectives remain unresolved.

Contextual Notes

Some participants highlight limitations in the definitions and properties of metrics, particularly in relation to the requirements for a set and metric to form a metric space, and the implications of these definitions in the context of pseudo-Riemannian geometry.

jcsd
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I've just been thinking (prolly a bad idea): Lorentzian metrics aren't actually metrics at all are they? In fact they're not even pseudometrics, so what are they exactly and why do we call them metrics (Actually I can probably guess that as they perform the same role a mteric does and they are symmetric and obey the triangle inequality)?
 
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A metric is just a just a symmetric non-degenerate tensor field of type (0,2). The metric of general relativity is not positive definite so it can't be called Riemannian, but it's still a metric.
 
I know it's not positive definite and it's pseudo-Riemannian, what I am actually talking about is 'metric' in the most primitive mathematical sense. i.e. a set S forms a metric space when combined with a function [itex]d:S^2 \rightarrow R[/itex], known as the metric which obeys the following axioms for all [itex]x,y,z \in S[/itex].

[tex]d(x,y) = d(y,x)[/tex]
[tex]d(x,y) \geq 0[/tex]
[tex]d(x,y) = 0 \iff x=y[/tex]
[tex]d(x,z) + d(y,z) \geq d(x,y)[/tex]
 
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Ambitwistor (to give credit where it's due) has supplied me with the answer:

The conditions on the metric in a pseudo-Riemannian metric space are sufficiently relaxed that the metric may be of the form of the Minkowksi metric.
 
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jcsd said:
I've just been thinking (prolly a bad idea): Lorentzian metrics aren't actually metrics at all are they? In fact they're not even pseudometrics, so what are they exactly and why do we call them metrics (Actually I can probably guess that as they perform the same role a mteric does and they are symmetric and obey the triangle inequality)?

The term "metric" means "to measure". The functions you gave are metrics in the sense that they provide some sort of measure. The metric *tensor* is an example of a mapping from vectors to scalars, e.g. ds^2 = g_ab dx^a dx^b where dx = vector and it gives a "measure" of the norm of a vector 'length' and the 'interval' between two points.

Pete
 
pmb_phy said:
The term "metric" means "to measure". The functions you gave are metrics in the sense that they provide some sort of measure. The metric *tensor* is an example of a mapping from vectors to scalars, e.g. ds^2 = g_ab dx^a dx^b where dx = vector and it gives a "measure" of the norm of a vector 'length' and the 'interval' between two points.

Pete

yes obviously it performs the same role as a metric does in a metric space and can intutively be thought as the distance. It was just that the Minkowski metirc does not meet the normal definition of a metric, which worried me as after all when defining a metric for a vector space we usually require the set of vectors and the metric to form a metric space and we usually treat (for example) the set of all radius vectors in Minkowski space as a real vector space.

As I said Ambitwistor answerd this for me by saying that the conditions on the metric in a pseudo-Riemannian metric space were sufficently relaxed that the Minkowski metric is a suitable function to act as a metric in such a space.

There's no great distinction between a metric and a metric tensor , a metric tensor merely defines the metric for a vector space.
 
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