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Equation 97 · The Clock That Comes Back Wrong by Exactly Its Mass

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LP\mathcal L_{\rm P}

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LPL_{\rm P}

Symbol L_rm P

where mass stops being a fixed label and becomes something an object can carry a little more or less of depending on what it is doing internally.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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The proper-time loop LP\mathcal L_{\rm P} is where mass stops being a fixed label and becomes something an object can carry a little more or less of depending on what it is doing internally. A composite system with an internal excitation of energy Δ\Delta E above its ground configuration carries additional rest mass Δ\Delta E/c2c^2 , by ordinary mass–energy equivalence — no redefinition of either the relativistic or the everyday meaning of mass, simply the standard bookkeeping in which a system’s total rest energy Mc2c^2 includes whatever internal energy HintH_{\rm int} it holds: M=M0M_0+HintH_{\rm int}/c2c^2 . If the same object is sent along two paths that differ in proper time by Δ\Deltaτ\tau , and its…
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The proper-time loop LP\mathcal L_{\rm P} is where mass stops being a fixed label and becomes something an object can carry a little more or less of depending on what it is doing internally. A composite system with an internal excitation of energy Δ\Delta E above its ground configuration carries additional rest mass Δ\Delta E/c2c^2 , by ordinary mass–energy equivalence — no redefinition of either the relativistic or the everyday meaning of mass, simply the standard bookkeeping in which a system’s total rest energy Mc2c^2 includes whatever internal energy HintH_{\rm int} it holds: M=M0M_0+HintH_{\rm int}/c2c^2 . If the same object is sent along two paths that differ in proper time by Δ\Deltaτ\tau , and its internal state differs between the two paths — ground on one, excited on the other — then the two branches’ free-particle phases differ by

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