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Equation 11 · The Bend an Elevator Cannot Fake

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ϕ(x):=ln⁡U(x)\phi(\mathbf x) := \ln U(\mathbf x)

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Inputs and operationsln U(mathbf x)
Result or conditionphi(mathbf x) :
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ϕ\phi

Symbol phi

phi is part of the quantity the equation computes from the expression on the right.

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xx

Symbol x

x is an argument of the function-like quantity on the left; its role is set by that function’s stated inputs.

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UU

Symbol U

U is an input to the expression that computes the quantity on the left.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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What the article says around this equation

For a static observer at position x\mathbf x in a stationary spacetime, define U(x\mathbf x) := dτ\tau/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 νj\nu_j/νi\nu_i = U(xj\mathbf x_j)/U(xi\mathbf x_i) — 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 ∂\partial/∂\partial t generates a…
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For a static observer at position x\mathbf x in a stationary spacetime, define U(x\mathbf x) := dτ\tau/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 νj\nu_j/νi\nu_i = U(xj\mathbf x_j)/U(xi\mathbf x_i) — 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 ∂\partial/∂\partial 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 ϕ(x)\phi(\mathbf x) := ln⁡\ln U(x\mathbf x) and the edge observable actually recorded between linked clocks i and j ,

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