DiracPool said:
So in the scenario above, are we assuming that Bob is "comoving" or in the same comoving frame as the CMB, that this qualifies as Bob and the CMB being in the same inertial rest frame (IRF), and the "test" of such is that the universe appears to be homogeneous and isotropic, to Bob?
Yes.
DiracPool said:
here is a galaxy with an earth-like planet far far away receding from the Earth at 0.9c, Does an inhabitant on that planet also see the universe as homogeneous and isotropic as well as being in the same rest frame or comoving with the CMB?
If the galaxy is "comoving" yes. As you have stated it, it's impossible to tell; the recession velocity of the galaxy alone isn't enough. You would also need to know the proper distance from Earth to the galaxy, so you could compare the recession velocity of the galaxy with what it would be for a comoving object at the same distance.
(Note that we are assuming here that the Earth is comoving, which it actually isn't; the CMB as we see it from Earth has a significant dipole anisotropy, corresponding to a velocity for Earth relative to a "comoving" observer of about 600 km/s. This dipole anisotropy is almost always removed before displaying charts of CMB observations, since the purpose of those charts is to look for patterns as they would be seen by a "comoving" observer.)
DiracPool said:
We can say that Alice during her trip breaks symmetry with Bob and travels a different "distance" through spacetime due to her departing from Bob's (and the CMB's) IRF, and thus shows a different age when she shows up back on Earth.
This is OK except for the term "IRF". There is no such thing as an IRF covering the universe, because the spacetime of the universe is not flat. If Alice doesn't go that far away from Bob, and returns in a short enough time (anything we humans are going to achieve in the foreseeable future will count as "not very far away" and a "short enough time"), then we can analyze the entire scenario in a single local inertial frame covering Bob's and Alice's worldlines during the experiment. But that won't work for objects farther away; see below.
DiracPool said:
what about the guy in the receding galaxy? Is he also traveling a different distance through spacetime than Bob seeing as he's traveling at 0.9c relative to Bob?
"Distance through spacetime" is ambiguous; "distance" between what events? Alice and Bob share a pair of events (the start and end of the experiment), so that question has an easy answer. But for the distant galaxy, you have to adopt a simultaneity convention in order to pick out "corresponding" events on the two worldlines (Bob's and the galaxy's). If both of them are "comoving" (which we can test by seeing if they both see the universe as isotropic), then the obvious simultaneity convention is the one for "comoving" observers; each spacelike hypersurface of constant time in the standard FRW coordinate chart is a surface of simultaneity for comoving observers. Then each such observer will have the same elapsed proper time ("distance" in spacetime) between a given pair of such surfaces (i.e., between two given values of FRW coordinate time--in fact, FRW coordinate time is the same as proper time for "comoving" observers).
The fact that the above is true even though Bob and the galaxy are in relative motion should make clear why you can't construct an inertial frame that covers the universe. (Bob and the galaxy are also in free fall, i.e., they are inertial observers, which makes this point even clearer.)