Fra said:
I don't understand exactly what it means but that sounds interesting to me!
Perhaps I need to look this up more. Do you recall where you might have seen this example of time indexation?
From my viewpoint I don't see how it would be possible to define, even from the point of view of a given observer, a global time index. This is because the references are I think not in general evolving deterministically.
Well, they discuss this general problem of "how to index" on page 5 of the
first paper. Their stated general problem with this approach here is that it rules out or makes difficult theories in which the spacetime manifold is not smooth:
Why are physical quantities assumed to be real-valued?... If conceded, this claim means that the assumption that physical quantities are real-valued is problematic in a theory in which space, or space-time, is not modeled by a smooth manifold. Admittedly, if the theory employs a background space, or space-time—and if this background is a manifold—then the use of real-valued physical quantities is justified in so far as their value-space can be related to this background... however, caution is needed with this argument since the background structure may arise only in some ‘sector’ of the theory; or it may exist only in some limiting, or approximate, sense.
On the next page they have a confusing digression on the subject of giving unusual types to probabilities.
They cover the notion of "time dependence" for the first time on page 14-15 of the first paper. They then go into it in more detail on page 28 of the
second paper, section 4.2.5. I honestly do not understand how they deal with the problem you observe, that there is in reality no "global time" and therefore the global time index they seem to be nonchalantly defining is difficult to interpret. I
think the answer is hinted at in the second paper's 4.2.5, where they define a set of truth objects (which interpret the truth or falsehood of propositions, based on some state |psi> internal to the truth object), indexed by "t" and mention that "the states |psi>_t satisfy
the time-dependent Schroedinger equation."
In other words, I guess it appears those parts of their paper which are making use of these "time-dependent" truth values are actually representing
nonrelativistic quantum theory, where the time-dependent Schroedinger equation can be used and we simply assume a global time parameter. One would hope they somewhere have, or eventually intend to, move beyond this to define a version of their theory with a more flexible notion of time... I unfortunately do not understand what they are doing well enough to say whether they are actually close to doing this.