Discussion Overview
The discussion revolves around the definition of "general covariance" in the context of physics, particularly in relation to theories expressed in terms of tensors. Participants explore whether being written solely in terms of tensors is sufficient or necessary for a theory to be considered generally covariant.
Discussion Character
- Exploratory
- Technical explanation
- Debate/contested
Main Points Raised
- Some participants reference Einstein's definition, suggesting that general covariance means laws of nature are expressed by equations valid for all coordinate systems.
- There is uncertainty regarding whether a theory written only in terms of tensors is sufficient for general covariance, with one participant questioning if such a theory could exist that does not hold in all coordinate systems.
- Another participant argues that a theory cannot have "prior geometry" independent of matter sources to qualify as generally covariant.
- References to Dirac's work indicate that covariant differentiation is necessary for general covariance, implying that tensors are essential for this process.
- Participants note that the term "covariant" has multiple meanings, which can lead to confusion in discussions about general covariance.
- Invariance is distinguished from covariance, with invariance requiring that the content of equations remains unchanged under coordinate transformations.
Areas of Agreement / Disagreement
Participants express differing views on the necessity and sufficiency of tensors for general covariance, indicating that the discussion remains unresolved with multiple competing perspectives.
Contextual Notes
Some limitations include the ambiguity of the term "covariant" and the need for clarity on the definitions and conditions under which general covariance applies.