- #1
- 6,724
- 429
Here are some different descriptions of Doppler shifts:
1. The gamma rays in the Pound-Rebka experiment were Doppler shifted.
2a. We make a cosmological model using coordinates in which an object moving with the Hubble flow has a zero coordinate velocity, so all galaxies are "at rest." An observer in galaxy A observes a red-shifted photon from cosmologically distant galaxy B.
2b. This is exactly the same physical situation as in 2a, but we pick coordinates in which A is at rest but B is in motion, and furthermore we decide to pick these coordinates such that the special-relativistic equation for the Doppler shift gives the observed result when we plug in the coordinate velocity attributed to B.
By general covariance, 2a and 2b are physically indistinguishable. The difference between them is purely verbal.
Everyone would describe 1 using the term "gravitational Doppler shift."
If we have to make the purely verbal distinction between 2a and 2b, probably most people would describe 2b as a "kinematic Doppler shift." Personally I'm in the habit of describing 2a as a "gravitational Doppler shift," but I think my usage may be nonstandard, and it does have the disadvantage that 2a, unlike 1, can't be computed from a gravitational potential, so in some sense the same word is being used to describe dissimilar phenomena.
Is there a better or more standard term for 2a? The only thing I can think of is something cumbersome like "Doppler shift due to the expansion of space."
-Ben
1. The gamma rays in the Pound-Rebka experiment were Doppler shifted.
2a. We make a cosmological model using coordinates in which an object moving with the Hubble flow has a zero coordinate velocity, so all galaxies are "at rest." An observer in galaxy A observes a red-shifted photon from cosmologically distant galaxy B.
2b. This is exactly the same physical situation as in 2a, but we pick coordinates in which A is at rest but B is in motion, and furthermore we decide to pick these coordinates such that the special-relativistic equation for the Doppler shift gives the observed result when we plug in the coordinate velocity attributed to B.
By general covariance, 2a and 2b are physically indistinguishable. The difference between them is purely verbal.
Everyone would describe 1 using the term "gravitational Doppler shift."
If we have to make the purely verbal distinction between 2a and 2b, probably most people would describe 2b as a "kinematic Doppler shift." Personally I'm in the habit of describing 2a as a "gravitational Doppler shift," but I think my usage may be nonstandard, and it does have the disadvantage that 2a, unlike 1, can't be computed from a gravitational potential, so in some sense the same word is being used to describe dissimilar phenomena.
Is there a better or more standard term for 2a? The only thing I can think of is something cumbersome like "Doppler shift due to the expansion of space."
-Ben