Discussion Overview
The discussion revolves around the concept of tensors with both covariant and contravariant components, particularly in the context of General Relativity (GR). Participants explore the definitions, properties, and implications of such tensors, as well as their relationship to tangent vector spaces and manifolds.
Discussion Character
- Exploratory, Technical explanation, Conceptual clarification, Debate/contested
Main Points Raised
- One participant expresses confusion about how a single tensor can have both covariant and contravariant indices, seeking clarification on the concept.
- Another participant introduces the idea of a type (1,1) tensor as a linear map from the tangent vector space to itself, prompting further inquiry.
- A participant clarifies that the underlying manifold has the tangent vector space, not the tensor itself, and explains the transformation properties of type (1,1) tensors.
- There is a discussion about the Kronecker delta being an example of a type (1,1) tensor, which has one covariant and one contravariant index.
- One participant suggests that a tensor could represent a mixture of contravariant and covariant indices, using distances or volumes and rates or densities as examples.
- A participant emphasizes the importance of understanding manifolds and tangent vectors when studying GR.
- Another participant provides a definition of tensors as multilinear maps involving vector spaces and their duals, relating this to tensor fields in differential geometry.
Areas of Agreement / Disagreement
Participants exhibit a mix of understanding and confusion regarding the nature of tensors with both covariant and contravariant components. While some definitions and examples are provided, there is no consensus on the clarity of these concepts or their implications.
Contextual Notes
Some participants express uncertainty about the definitions and properties of tensors, tangent vector spaces, and manifolds, indicating a need for further exploration of these foundational concepts.