- #1
center o bass
- 560
- 2
When deriving different properties from the FRW-metric $$ds^2 = -dt^2 + a^2 (d\chi^2 + S_k^2(\chi) d\Omega^2)$$ -- considering the propagation of light such that ##ds^2 = 0## -- one always assumes ##d\Omega = 0##. But how do we know that ##d\Omega## always vanish for propagating light?