Equation 119 · The Clock That Comes Back Wrong by Exactly Its Mass
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Here is the strongest objection this construction has to survive, and it is not hypothetical — it was argued in print for over a decade. In 2010, Müller, Peters, and Chu proposed that an ordinary light-pulse atom interferometer’s gravimeter phase already constitutes a measurement of the gravitational redshift at the atom’s Compton frequency m/ , reading the standard interferometer as an implicit realization of exactly the proper-time phase this paper formalizes [ 6 ] . Wolf, Blanchet, Bordé, Reynaud, Salomon, and Cohen-Tannoudji objected immediately: the standard three-pulse Mach–Zehnder gravimeter phase, computed by the ordinary classical-action method, is k_{…
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Here is the strongest objection this construction has to survive, and it is not hypothetical — it was argued in print for over a decade. In 2010, Müller, Peters, and Chu proposed that an ordinary light-pulse atom interferometer’s gravimeter phase already constitutes a measurement of the gravitational redshift at the atom’s Compton frequency m/ , reading the standard interferometer as an implicit realization of exactly the proper-time phase this paper formalizes [ 6 ] . Wolf, Blanchet, Bordé, Reynaud, Salomon, and Cohen-Tannoudji objected immediately: the standard three-pulse Mach–Zehnder gravimeter phase, computed by the ordinary classical-action method, is \,g\, , a quantity built entirely from the laser wavevector, gravitational acceleration, and pulse timing, with no dependence on the atom’s mass at all [ 7 ] . Sinha and Samuel sharpened the point into a slogan worth taking literally: an atom in this configuration is not a clock ticking at the Compton frequency, because nothing in the standard phase formula reads out that frequency [ 8 ] .
Sources cited in the surrounding passage
- [6] A Precision Measurement of the Gravitational Redshift by the Interference of Matter Waves ↗
- [7] Atom Gravimeters and Gravitational Redshift ↗
- [8] Atom Interferometry and the Gravitational Redshift ↗
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