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τ0≠τ1\tau_0\neq\tau_1

Why this formula appears here

The second, LP\mathcal L_{\rm P} , lives in spacetime itself: send a system from event A to event B along worldline γ0\gamma_0 , and imagine comparing it against a return trip along the reverse of a different worldline γ1\gamma_1 that also connects A to B . The loop closes in space and time — it starts and ends at A — but the two worldlines need not have the same proper time, τ0\tau_0≠\neqτ1\tau_1 , precisely because proper time is path dependent once gravity or acceleration is present. This is not a new observation; it is the entire content of general relativity’s twin-paradox structure, imported into a single-particle quantum phase by early clock-interferometry proposals [ 10 ] .

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τ0\tau_0

Symbol tau_0

tau0u_0 is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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τ1\tau_1

Symbol tau_1

tau1u_1 is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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Published contexts (1)

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τ0≠τ1\tau_0\neq\tau_1

Equation 16 · Evolutionary Physics

The Clock That Comes Back Wrong by Exactly Its Mass

This mathematical expression combines the displayed quantities; its precise role follows from the surrounding article text.

The second, LP\mathcal L_{\rm P} , lives in spacetime itself: send a system from event A to event B along worldline γ0\gamma_0 , and imagine comparing it against a return trip along the reverse of a different worldline γ1\gamma_1 that also connects A to B . The loop closes in space and time — it starts and ends at A — but the two worldlines need not have the same proper time, τ0\tau_0≠\neqτ1\tau_1 , precisely because proper time is path dependent once gravity or acceleration is present. This is not a new observation; it is the entire content of general relativity’s twin-paradox structure, imported into a single-particle quantum phase by early clock-interferometry proposals [ 10 ] .

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