anuttarasammyak
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Here, I assume that all inertial frames agree that the collapse occurs when the reading of clock B is the smallest, namely at T−L/c.anuttarasammyak said:Observers in different inertial frames who were making observations in the vicinity of measurement at A hold a meeting and present their respective viewpoints. It turns out that each of them is making a rational judgment. As a conclusion of the meeting, they adopt the earliest possible reading of B’s clock, T−L/c where L is distanbe between A and B, as the common consensus. This is because B’s behavior corresponding to clock readings between T−L/c and T+L/c is unknown, and measurement at B may occur during this interval. The only choice consistent with this possibility is the earliest time, T−L/c.
This is consistent with the viewpoint of each inertial frame in the sense that, in every frame, B is in the collapsed state only afterward (although the observation itself is performed at A).
Next, let us consider the situation from B toward A.
If we take the collapsed state of B as the starting point, then, due to the relativity of simultaneity, in some inertial frames the state of A appears to have collapsed at a time earlier than the observation. The earliest such time is when the reading of clock A is T−2L/c. Let us again assume that this is accepted by all inertial frames as well.
If we continue this kind of reasoning back and forth between A and B, tracing further and further into the past, we arrive at the conclusion that, ever since the moment when A and B were at the same location for the purpose of generating quantum entanglement, the states of A and B had in fact already collapsed.
What was regarded as an entangled state up until the observation by A is, after the observation, reinterpreted as having been a collapsed state extending retroactively into the past, back to the time of entanglement generation.
In this way, it seems that there is no longer any need to worry about spooky long-distance correlations.
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