SUMMARY
The discussion centers on the correct association of energy with a timelike Killing vector field (KVF) in the context of cosmological redshift. It clarifies that the energy associated with a timelike KVF is given by the equation gμν kμ Pν, where gμν is the metric tensor, kμ is the KVF, and Pν is the 4-momentum of an object. The discussion also emphasizes that the invariant mass m pertains to the body whose energy is being measured, not the observer. The relationship between emitted and observed wavelengths is derived using the Friedmann-Robertson-Walker (FRW) metric, confirming that the redshift is proportional to the change in the scale factor between emission and reception.
PREREQUISITES
- Understanding of timelike Killing vector fields in general relativity
- Familiarity with the Friedmann-Robertson-Walker (FRW) metric
- Knowledge of energy-momentum relations in relativistic physics
- Basic grasp of cosmological redshift concepts
NEXT STEPS
- Study the derivation of cosmological redshift in the context of FRW spacetime
- Learn about the implications of timelike Killing vector fields in general relativity
- Explore the relationship between frequency, wavelength, and energy in quantum mechanics
- Investigate the role of the metric tensor in general relativity and its applications
USEFUL FOR
Physicists, cosmologists, and students of general relativity seeking to deepen their understanding of energy measurements in curved spacetime and the implications for cosmological phenomena.