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Equation 105 · The Bit Comes Back Before the Bearing

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gg

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gg

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This model has an explicit conservation ceiling built in: it cannot be extended past the compass’s own total intrinsic Fisher information FQ(0)F_Q^{(0)} = 4Var⁡\operatorname{Var}J^\hat J/ℏ2\hbar^2 , since no amount of radiation can reveal more about g than the original state ever carried. A tolerance δ\delta tighter than 1/FQ(0)\sqrt{F_Q^{(0)}} is not a slower recovery — it is a request for better precision than the compass itself possessed, which no observer, inside or outside any horizon, could ever meet. Within that ceiling, tG(δ)t_G(\delta) grows toward the hole’s full evaporation lifetime as δ\delta is tightened, which is a specific, checkable form of the “information remnant” Nakata, Wakakuwa, and Koashi found…
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This model has an explicit conservation ceiling built in: it cannot be extended past the compass’s own total intrinsic Fisher information FQ(0)F_Q^{(0)} = 4Var⁡\operatorname{Var}J^\hat J/ℏ2\hbar^2 , since no amount of radiation can reveal more about g than the original state ever carried. A tolerance δ\delta tighter than 1/FQ(0)\sqrt{F_Q^{(0)}} is not a slower recovery — it is a request for better precision than the compass itself possessed, which no observer, inside or outside any horizon, could ever meet. Within that ceiling, tG(δ)t_G(\delta) grows toward the hole’s full evaporation lifetime as δ\delta is tightened, which is a specific, checkable form of the “information remnant” Nakata, Wakakuwa, and Koashi found directly in their symmetry-constrained analysis of the Hayden-Preskill protocol: a residue that a purely logical decoder never has to wait for, because it was never entitled to it in the first place [ 8 ] .

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