...A second thought on the above however, seemed to suggest it is too deliberate. It seems more likely the below situation will happen instead, meaning you can only delay a predestinated future, only up to right before the event will then become self inconsistent, or worse, the events A and B are already entangled, thus upon receiving the journal article, the measurement had already taken place on $g$, projecting to one of the $g(\phi)$ s where event A and B is fixed and well defined,
and O will have no way to know about it
I actually suspect if time travel is possible and under quantum gravity situations, CTCs might actually behave like a pair of entangled events stretching across timelike distances
Thus put it bluntly, the moment you have interacted with something from the future that is uncaused, you will have no choice but to close the loop at some determined but unpredictable time in the future
except maybe, you construct some crazy $g'$ with some kind of gravity technology such that the state $g$ changes, thus breaking the correlation between events A and B due to the measurement at A (which is really a joint measurement because A and B are entangled due to the CTC structure)
and thereby, freeing you from the CTC at the cost of a topology change in spacetime (which is not known to be allowed in classical GR)
If this is the case, then time travel may be even more interesting in the quantum gravity regime because then you can scramble causal diagrams of events so badly such that no two diagrams between two timelike separated regions of spacetime are connected, and thus as long you expend energy to change the topology of spacetime, you can change the past however you like without causing any paradoxes
But if that is the case, does time have meaning anymore globally speaking...?
Anyway, this is just speculation based on the existing theories plus some naive generalisation, I don't think quantum gravity, being in such a strong interacting regime, will be a linear theory, thus superposition may not hold in general