Minkowski Spacetime KVF Symmetries

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Discussion Overview

The discussion centers on the properties of Killing Vector Fields (KVFs) in Minkowski spacetime, particularly focusing on the number of independent KVFs and the implications of the Lie derivative in this context. Participants explore theoretical aspects and mathematical formulations related to symmetries in spacetime.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant notes that Minkowski spacetime has 10 independent KVFs, derived from counting isometries as translations and rotations.
  • Another participant clarifies that the Lie derivative is linear in the vector field only with constant coefficients, suggesting that linear combinations of KVFs must be carefully considered.
  • A participant presents the Killing equation in Galilean coordinates and derives conditions for KVFs, leading to the conclusion that the KVFs correspond to the Poincare group symmetries.
  • Concerns are raised about the nature of generic smooth vector fields on Minkowski spacetime and their relation to KVFs, questioning why not all smooth vector fields qualify as KVFs.
  • Further discussion emphasizes that non-trivial functions of coordinates in vector fields can lead to additional terms that violate the conditions for KVFs.
  • One participant introduces a separate question regarding whether assigning a metric structure to a smooth manifold qualifies it as a metric space, leading to a brief exchange on the properties of Riemannian and pseudo-Riemannian manifolds.
  • Another participant elaborates on the intuitive meaning of the Lie derivative, explaining how it describes changes in vector fields as one moves through spacetime.

Areas of Agreement / Disagreement

Participants express differing views on the implications of the Lie derivative and the conditions under which vector fields can be considered KVFs. There is no consensus on the broader implications of these discussions, particularly regarding the nature of smooth vector fields in relation to KVFs.

Contextual Notes

Participants highlight limitations in understanding the linearity of the Lie derivative and its implications for KVFs, as well as the potential for confusion arising from index notation and mathematical derivations.

  • #31
Orodruin said:
$$
\mathcal L_\xi T = \lim_{s\to 0}[(\phi_{s\xi}^*T - T)/s].
$$ As the pullback defines a map between different points in the manifold, we are not in need of a connection in order to compute the Lie derivative.
A doubt about the limit involved in the Lie derivative definition. At first sight that limit makes sense when we pick a chart in the differentiable atals and do the calculation there. Does it imply a notion of limit from an invariant coordinate-free point of view ?
 
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  • #32
Sure, this is a definition completely independent of any choice of coordinates. Since all the manipulations used to define the limit are manifestly covariant, it maps the arbitrary tensor field ##T## to another tensor field of the same rank.
 
  • #33
vanhees71 said:
Sure, this is a definition completely independent of any choice of coordinates. Since all the manipulations used to define the limit are manifestly covariant
Ah ok, indeed the operations involved in the definition are part of tensor space structure that exist at each point of the manifold. Namely a difference between (0,2) tensors defined at the same point (i.e. elements of the same tensor space) and a scalar multiplication for ##1/s##.
 
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