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Δϕ=−mc2Δτ/ℏ\Delta\phi=-mc^2\Delta\tau/\hbar

Why this formula appears here

The sign convention on the proper-time form follows the phase of a free relativistic particle, Δ\Deltaϕ\phi=-mc2c^2Δ\Deltaτ\tau/ℏ\hbar , so that mopm_{\rm op}=-(ℏ\hbar/c2c^2)\,∂\partialΔ\Deltaϕ\phi/∂\partialΔ\Deltaτ\tau recovers m identically when Δ\Deltaϕ\phi has no other dependence. Both forms require sweeping the loop’s own parameter — hold time, translation distance, boost velocity — across at least two settings and fitting the slope, exactly as a spectroscopist extracts an energy gap from a swept detuning rather than from one photon count. A single unswept measurement cannot report a mass gauge at all; it can only report a phase.

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Δϕ=−mc2Δτ/ℏ\Delta\phi=-mc^2\Delta\tau/\hbar

Equation 71 · Evolutionary Physics

The Clock That Comes Back Wrong by Exactly Its Mass

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions.

The sign convention on the proper-time form follows the phase of a free relativistic particle, Δ\Deltaϕ\phi=-mc2c^2Δ\Deltaτ\tau/ℏ\hbar , so that mopm_{\rm op}=-(ℏ\hbar/c2c^2)\,∂\partialΔ\Deltaϕ\phi/∂\partialΔ\Deltaτ\tau recovers m identically when Δ\Deltaϕ\phi has no other dependence. Both forms require sweeping the loop’s own parameter — hold time, translation distance, boost velocity — across at least two settings and fitting the slope, exactly as a spectroscopist extracts an energy gap from a swept detuning rather than from one photon count. A single unswept measurement cannot report a mass gauge at all; it can only report a phase.

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