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ϵL(t)  =  min⁡R[ 1−Fe(R∘Nt,  id) ],tL(ϵ)  =  min⁡{ t:ϵL(t)≤ϵ }\epsilon_L(t) \;=\; \min_{\mathcal R}\Big[\,1 - F_e\big(\mathcal R \circ \mathcal N_t,\; \mathrm{id}\big)\,\Big], \qquad t_L(\epsilon) \;=\; \min\{\,t : \epsilon_L(t) \le \epsilon\,\}

Why this formula appears here

For the qubit, returned means: there exists a recovery channel R\mathcal R , built from quantum operations an agent holding both the full early radiation R and a further batch of radiation CtC_t collected up to time t can actually perform, whose entanglement fidelity to the identity channel on A is within ϵ\epsilon of perfect, ϵL(t)  =  min⁡R[ 1−Fe(R∘Nt,  id) ],tL(ϵ)  =  min⁡{ t:ϵL(t)≤ϵ }\epsilon_L(t) \;=\; \min_{\mathcal R}\Big[\,1 - F_e\big(\mathcal R \circ \mathcal N_t,\; \mathrm{id}\big)\,\Big], \qquad t_L(\epsilon) \;=\; \min\{\,t : \epsilon_L(t) \le \epsilon\,\}. Nt\mathcal N_t is the effective channel from A to R\!∪\cup\!CtC_t induced by the hole’s own scrambling dynamics up to time t ; ϵL(t)\epsilon_L(t) is a dimensionless number in [0,1] , and tLt_L has units of time. This is a yes-or-no-shaped promise sharpened into a number: either a decoder within ϵ\epsilon of perfect exists on the stated resources, or it does not,…

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Published contexts (1)

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ϵL(t)  =  min⁡R[ 1−Fe(R∘Nt,  id) ],tL(ϵ)  =  min⁡{ t:ϵL(t)≤ϵ }.\epsilon_L(t) \;=\; \min_{\mathcal R}\Big[\,1 - F_e\big(\mathcal R \circ \mathcal N_t,\; \mathrm{id}\big)\,\Big], \qquad t_L(\epsilon) \;=\; \min\{\,t : \epsilon_L(t) \le \epsilon\,\}.

Equation 23 · Evolutionary Physics

The Bit Comes Back Before the Bearing

This equation states a bound: one expression must stay on the indicated side of the other under the article’s assumptions.

For the qubit, returned means: there exists a recovery channel R\mathcal R , built from quantum operations an agent holding both the full early radiation R and a further batch of radiation CtC_t collected up to time t can actually perform, whose entanglement fidelity to the identity channel on A is within ϵ\epsilon of perfect, ϵL(t)  =  min⁡R[ 1−Fe(R∘Nt,  id) ],tL(ϵ)  =  min⁡{ t:ϵL(t)≤ϵ }\epsilon_L(t) \;=\; \min_{\mathcal R}\Big[\,1 - F_e\big(\mathcal R \circ \mathcal N_t,\; \mathrm{id}\big)\,\Big], \qquad t_L(\epsilon) \;=\; \min\{\,t : \epsilon_L(t) \le \epsilon\,\}. Nt\mathcal N_t is the effective channel from A to R\!∪\cup\!CtC_t induced by the hole’s own scrambling dynamics up to time t ; ϵL(t)\epsilon_L(t) is a dimensionless number in [0,1] , and tLt_L has units of time. This is a yes-or-no-shaped promise sharpened into a number: either a decoder within ϵ\epsilon of perfect exists on the stated resources, or it does not,…

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