Do Metric Tensors Always Have Inverses?

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Discussion Overview

The discussion centers on the existence of inverses for metric tensors, particularly in the context of musical isomorphisms and their application in raising and lowering indices. Participants explore whether one can assume that a metric tensor always has an inverse, especially in relation to its properties in various geometrical frameworks, such as pseudo-Riemannian geometry.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants question whether the inverse of a metric tensor can always be assumed to exist, particularly in the context of musical isomorphisms.
  • Others note that in cases of relativity, transformations between frames of reference imply the existence of an inverse transformation, which raises questions about the inverse of the metric tensor.
  • One participant suggests that for a metric tensor to have an inverse, its determinant must be non-zero, referencing the properties of bilinear forms.
  • A later reply asserts that in pseudo-Riemannian geometry, the metric is non-degenerate, implying that an inverse always exists.
  • Another participant discusses the relationship between the vector space and its double dual, suggesting that the inverse may depend on the choice of basis.
  • One participant concludes that the non-degeneracy of the tensor in its matrix representation implies its invertibility.

Areas of Agreement / Disagreement

Participants express differing views on the assumption of the existence of an inverse for metric tensors. While some argue that non-degeneracy guarantees invertibility, others highlight the dependence on specific conditions or contexts, indicating that the discussion remains unresolved.

Contextual Notes

Participants mention the importance of the determinant of the metric tensor and its implications for the existence of an inverse. The discussion also touches on the implications of basis choices in relation to the identification of vector spaces and their duals.

jv07cs
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I am reading about musical isomorphisms and for the demonstration of the index raising operation from the sharp isomorphism, we have to multiply the equation by the inverse matrix of the metric. Can we assume that this inverse always exists? If so, how could I prove it?
 
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In the cases of relativity, transformation of spacetime coordinates from one Frame of Reference to another should have inverse transformation which corresponds to another to one. But I have no idea of inverse of metric tensor. How do we use it ?

You say about music and I am sorry to have scarce knowledge of metric tensor in music. If is is just an ordinary matrix, its determinant would not be zero to have an inverse matrix.
 
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anuttarasammyak said:
In the cases of relativity, transformation of spacetime coordinates from one Frame of Reference to another should have inverse transformation which corresponds to another to one. But I have no idea of inverse of metric tensor. How do we use it ?

You say about music and I am sorry to have scarce knowledge of metric tensor in music.
The musical isomorphisms are just isomorphisms between the vector space and its dual that lead us to the operations of lowering and raising index. The term musical is because we use the symbols flat ##\flat## and sharp ##\sharp## to denote them (kind of an analogy with "flat" meaning lower in pitch and "sharp" meaning higher in pitch, and the idea of lowering and raising indices).

In this specific case we take a vector space endowed with a metric g and define the following flat isomorphism:
$$^\flat: V \rightarrow V^*$$ $$v \mapsto v^\flat$$

where ##v^\flat \in V^*## is defined as:
$$v^\flat(w) = g(v,w)$$
We can show that this is indeed an isomorphism and we get to the relation ##v_i = g_{ij}v^j##, the lowering index operation, where ##v_i## are the components of ##v^\flat##.

The ##\sharp## isomorphism is then defined as the inverse of the flat isomorphism: ##\sharp = \flat^{-1}## and we can arrive at the raising index operation by basically multiplying both sides of ##v_i = g_{ij}v^j## by the inverse matrix ##g^{ik}## and we arrive at ##v^k = g^{ik}v_i##.

My question is regarding this process. Because for us to multiply by the inverse matrix we first have to assume that there is one and my question is if we can state that a metric always has an inverse? Or if, for this demonstration, one should include "assuming that g has an inverse"?
 
Thanks for explaining in detail.
I see it and assume that
g_{ik}g^{kj}=\delta_i^j
g_{ik}=g_{ki},g^{kj}=g^{jk}
If so as I noted in #2 determinant g of {g_ik} should not be zero to have {g^kj}, e.g. g=-1 for SR.

But I am afraid my primitive knowledge does no good to your high mathematics.
 
Last edited:
anuttarasammyak said:
Thanks for explaining in detail.
I see it and assume that
g_{ik}g^{kj}=\delta_i^j
g_{ik}=g_{ki},g^{kj}=g^{jk}
If so as I noted in #2 determinant g of {g_ik} should not be zero to have {g^kj}, e.g. g=-1 for SR.

But I am afraid my primitive knowledge does no good to your high mathematics.
I just found out that there is a theorem that states that, for finite dimensional vector spaces, a "bilinear form is degenerate if and only if the determinant of the associated matrix is zero", which would mean that the matrix associated with a non-degenerate bilinear form is non-singular. Since the metric tensor is a symmetric non-degenerate bilinear form, it will always have an inverse. This answers my question.

Thank you very much for the replies.
 
jv07cs said:
I am reading about musical isomorphisms and for the demonstration of the index raising operation from the sharp isomorphism, we have to multiply the equation by the inverse matrix of the metric. Can we assume that this inverse always exists? If so, how could I prove it?
In pseudo-riemannian geometry the metric is non-degenerate, so yes, an inverse always exists.
 
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Isn't this inverse defined by identifying the vector space with its double dual?
 
haushofer said:
Isn't this inverse defined by identifying the vector space with its double dual?
Not sure your question, but if you have a basis and a dual basis, then you can identify the double dual basis and have a way to map vectors and covectors to each other. However, this correspondence depends on a choice of basis. In other words, the inverse will vary with a different basis, I believe.

With a metric tensor, you can map covectors and vectors to each other in a basis independent way via the musical isomorphisms.
 
I think the non-degeneracy of the tensor in its matrix representation implies its invertibility.
 

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