Discussion Overview
The discussion revolves around the definition of redshift for photons, particularly in the context of cosmological redshift within Friedmann-Robertson-Walker (FRW) spacetime. Participants explore the relationship between energy, proper time, and the scale factor in cosmology, as well as the implications of using different forms of energy expressions.
Discussion Character
- Technical explanation
- Conceptual clarification
- Debate/contested
- Mathematical reasoning
Main Points Raised
- One participant questions whether the correct form for associating a timelike Killing vector field (KVF) with energy should be ##\dot{t}^2## or ##\dot{t}##, suggesting a preference for the former based on classical analogies.
- Another participant clarifies that the energy measured by an observer is ##m dt / d\tau##, where ##m## is the invariant mass, and distinguishes this from energy associated with a timelike KVF, which involves the metric tensor and 4-momentum.
- There is a discussion about the proper times of observers and the light ray, with one participant noting that the light ray does not have a proper time since its worldline is null.
- Participants explore the implications of the scale factor in FRW spacetime on redshift, stating that the wavelength increases if ##a(t_2) > a(t_1)##.
- One participant expresses confusion about the relationship between energy and wavelength, questioning how to deduce energy changes from wavelength variations.
- Another participant emphasizes that the energy formula ##E=mdt/d\tau## applies to timelike objects and seeks clarification on its application in the context of the discussion.
- There is a suggestion that a change in frequency, related to wavelength, causes a change in energy, linking ##E=\hbar\nu## and ##\nu=c/\lambda##.
Areas of Agreement / Disagreement
Participants exhibit a mix of agreement and disagreement, particularly regarding the application of energy formulas and the relevance of timelike KVFs in the context of FRW spacetime. The discussion remains unresolved on several points, particularly concerning the proper interpretation of energy in relation to redshift.
Contextual Notes
There are limitations in the discussion regarding the assumptions made about the observers and the definitions of terms used, particularly concerning the invariant mass and the nature of the energy being discussed. The relevance of the timelike KVF in FRW spacetime is also contested.