Equation 69 · No Particle Without a Cosigner
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This is not the same kind of zero-over-infinity problem that shows up when comparing two accelerated trajectories, and the difference matters. For an eternal accelerated trajectory, both the numerator and the denominator of the naive, un-normalized response functional are proportional to the (formally infinite) total elapsed proper time, and that shared infinity cancels cleanly in the ratio, which is exactly the standard trick — divide the total accumulated response by the total proper time elapsed — used throughout this literature to extract a finite rate from an eternally switched-on detector. For the eternal inertial trajectory, the numerator does not merely fail to diverge fast enough to…
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This is not the same kind of zero-over-infinity problem that shows up when comparing two accelerated trajectories, and the difference matters. For an eternal accelerated trajectory, both the numerator and the denominator of the naive, un-normalized response functional are proportional to the (formally infinite) total elapsed proper time, and that shared infinity cancels cleanly in the ratio, which is exactly the standard trick — divide the total accumulated response by the total proper time elapsed — used throughout this literature to extract a finite rate from an eternally switched-on detector. For the eternal inertial trajectory, the numerator does not merely fail to diverge fast enough to survive the ratio: it vanishes on the nose, for every gap, at every order. There is no shared infinity to cancel against, so there is nothing left for the ratio trick to rescue. against an inertial comparison worldline in this idealized limit is not small. It is not defined.
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