Discussion Overview
The discussion revolves around the computation of the Riemann tensor components in the context of gravitational waves from a binary merger, specifically comparing results in the source gauge and the transverse traceless (TT) gauge. Participants explore the implications of tensor invariance and the behavior of tensor components under different coordinate transformations.
Discussion Character
- Technical explanation
- Debate/contested
Main Points Raised
- One participant references a book by Hobson, noting the computed Riemann tensor components in both the source and TT gauges, questioning why they differ despite the invariance of the Riemann tensor.
- Another participant argues that the term "invariant" is misleading, suggesting "covariant" is more appropriate, and clarifies that individual tensor components do not remain the same across different coordinate charts.
- A further contribution emphasizes that while tensors are invariant objects, their components transform with changes in the basis, which could clarify the misunderstanding.
- One participant reiterates the point about invariance, stating that in the linearized theory of gravity, the Riemann tensor components can be shown to be invariant to first order in the metric perturbation.
- Another participant challenges the claim about invariance, drawing a parallel to special relativity, stating that components of a 4-vector do not remain unchanged under Lorentz transformations, only scalar quantities derived from them do.
Areas of Agreement / Disagreement
Participants express disagreement regarding the interpretation of tensor invariance and the behavior of tensor components under coordinate transformations. There is no consensus on the implications of these concepts in the context of the Riemann tensor for the given problem.
Contextual Notes
Participants note the distinction between invariance of tensors and the transformation of their components, highlighting the complexity of the discussion in the context of linearized gravity and the specific gauges used.