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Equation 145 · The Bit Comes Back Before the Bearing

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tLt_L

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tLt_L

Symbol t_L

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subscript

subscript

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Every number above is a derivation about an idealized, maximally chaotic evaporation process, and no experiment has isolated anything like it from a real horizon. One side of the mechanism, though, has been tested on hardware that exists. Landsman and colleagues built a seven-qubit ion-trap circuit engineered to scramble like the toy models this literature is built on, then used a conditional teleportation protocol — the same family Yoshida and Kitaev’s efficient decoder belongs to — to check whether information injected into the circuit could be recovered from the output exactly when, and only when, the circuit’s internal dynamics were actually scrambling rather than merely randomizing…
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Every number above is a derivation about an idealized, maximally chaotic evaporation process, and no experiment has isolated anything like it from a real horizon. One side of the mechanism, though, has been tested on hardware that exists. Landsman and colleagues built a seven-qubit ion-trap circuit engineered to scramble like the toy models this literature is built on, then used a conditional teleportation protocol — the same family Yoshida and Kitaev’s efficient decoder belongs to — to check whether information injected into the circuit could be recovered from the output exactly when, and only when, the circuit’s internal dynamics were actually scrambling rather than merely randomizing without the specific correlational structure scrambling requires [ 16 ] . The teleportation fidelity rose sharply above the classical baseline precisely in the scrambling regime and did not in a matched non-scrambling control — a real, if entirely non-gravitational, confirmation that the logical-recovery mechanism behind tLt_L is a genuine physical effect and not merely an artifact of an idealized calculation.

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