Equation 108 · No Particle Without a Cosigner
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No experiment has isolated an Unruh-like signal from this system, and this article does not claim otherwise. Measured storage-ring polarizations match the standard Sokolov-Ternov prediction, once ordinary QED corrections are included, at the percent level, and circular motion is not uniform linear acceleration — a fact Bell and Leinaas themselves stressed, since the field seen by a circulating charge is not simply a Rindler wedge, and the comparison to 's idealized eternal-linear-acceleration spectrum is only approximate even before synchrotron backgrounds are considered. What the storage-ring case does supply, honestly, is a parameter range: it is the one setting where the…
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No experiment has isolated an Unruh-like signal from this system, and this article does not claim otherwise. Measured storage-ring polarizations match the standard Sokolov-Ternov prediction, once ordinary QED corrections are included, at the percent level, and circular motion is not uniform linear acceleration — a fact Bell and Leinaas themselves stressed, since the field seen by a circulating charge is not simply a Rindler wedge, and the comparison to 's idealized eternal-linear-acceleration spectrum is only approximate even before synchrotron backgrounds are considered. What the storage-ring case does supply, honestly, is a parameter range: it is the one setting where the acceleration scale entering is large enough for an Unruh-like correction to be even nominally comparable to measured precision, and the percent-level agreement between observed and standard-model-predicted polarization bounds any anomalous, acceleration-induced departure from ordinary detector response at that same percent level in this one geometry. Every other trajectory discussed in this article — flat-space uniform acceleration at laboratory-achievable scales, curved-spacetime stationary orbits — sits at accelerations many orders of magnitude below where any such bound has ever been tested.
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