Equation 85 · The Atlas That Refuses to Close
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The response to Hegerfeldt’s obstruction that has actually held up is to stop asking for a sharp position operator at all. Werner’s screen observables replace the eigenvalue-and-projector structure of or with a positive-operator-valued measure: a family of positive operators, one for each region of a detection screen, that sum to the identity and assign a probability to “a click registered in this region” without ever claiming the particle possessed a definite position immediately beforehand [ 9 ] . A POVM chart is a genuinely different mathematical type from every chart built so far, not a self-adjoint operator with a spectral decomposition into sharp…
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The response to Hegerfeldt’s obstruction that has actually held up is to stop asking for a sharp position operator at all. Werner’s screen observables replace the eigenvalue-and-projector structure of or with a positive-operator-valued measure: a family of positive operators, one for each region of a detection screen, that sum to the identity and assign a probability to “a click registered in this region” without ever claiming the particle possessed a definite position immediately beforehand [ 9 ] . A POVM chart is a genuinely different mathematical type from every chart built so far, not a self-adjoint operator with a spectral decomposition into sharp positions but a measure-valued object whose value on any given trial is a probability distribution over an actual detector’s actual geometry. It sidesteps Hegerfeldt’s theorem because it never asserts exact localization to begin with; its resolution is set by the physical smearing of the detection scheme rather than driven to zero by fiat, and the causality argument that dooms a sharp projector has no state to act on that it can call “exactly here.”
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