Equation 13 · The Bend an Elevator Cannot Fake
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For a static observer at position in a stationary spacetime, define U() := d/dt , the local rate of proper time relative to coordinate time. Two clocks compared through any phase-coherent link that depends only on their respective proper frequencies report the ratio / = U()/U() — a fact about stationary spacetimes that follows from the timelike Killing vector generating t -translations, and one on which the standard treatments of relativity in a geodetic or navigational setting already rely [ 10 , 14 ] . The dependence on endpoints only, never on the path connecting them, is not an approximation: because / t generates a…
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For a static observer at position in a stationary spacetime, define U() := d/dt , the local rate of proper time relative to coordinate time. Two clocks compared through any phase-coherent link that depends only on their respective proper frequencies report the ratio / = U()/U() — a fact about stationary spacetimes that follows from the timelike Killing vector generating t -translations, and one on which the standard treatments of relativity in a geodetic or navigational setting already rely [ 10 , 14 ] . The dependence on endpoints only, never on the path connecting them, is not an approximation: because / t generates a genuine symmetry of a stationary metric, the redshift between any two static observers is fixed entirely by the value of U at each observer’s own location, so a network’s fitted node potential can be compared against a measurement made over any convenient physical route without first specifying which route was used. Define the dimensionless node potential := U() and the edge observable actually recorded between linked clocks i and j ,
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