Equation 14 · No Particle Without a Cosigner
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Symbol W
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where W is the field’s two-point Wightman function evaluated along the trajectory [ 5 ] . Three things in this expression are worth fixing in the reader’s mind before anything else happens to it. First, is proper time — the detector’s own clock, the only time variable with unambiguous physical meaning for a single worldline — never the coordinate time of whatever chart the trajectory happens to be written in. Second, is conjugate to that same proper time; it is an energy gap measured in the detector’s own instantaneous rest frame, not a coordinate-frame frequency. Third, the field state enters only through W , and changing the field state — the ordinary vacuum, a thermal state,…
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where W is the field’s two-point Wightman function evaluated along the trajectory [ 5 ] . Three things in this expression are worth fixing in the reader’s mind before anything else happens to it. First, is proper time — the detector’s own clock, the only time variable with unambiguous physical meaning for a single worldline — never the coordinate time of whatever chart the trajectory happens to be written in. Second, is conjugate to that same proper time; it is an energy gap measured in the detector’s own instantaneous rest frame, not a coordinate-frame frequency. Third, the field state enters only through W , and changing the field state — the ordinary vacuum, a thermal state, the Boulware, Hartle-Hawking, or Unruh state of a black-hole exterior — changes even for a fixed trajectory. Keeping these three inputs — proper time, proper-frame gap, and field state — cleanly separated is what prevents an ordinary coordinate-time effect, like gravitational redshift between two static observers at different heights, from being mistaken for a genuine disagreement about particle content. A redshift is a fact about clocks. A response-spectrum disagreement, once clocks are correctly accounted for, is a fact about the field and the worldline together.
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