Manuscript En02-E@2 · En02-E-v2.tex · section · c2769986

Scope, dependencies, and evidence

Scope, dependencies, and evidence · lines 170–254

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The construction separates the following objects:

\begin{gathered}
\text{specified field state}
\longrightarrow
\text{selected packet state}
\longrightarrow
\text{finite flagged representation},\\
\text{declared encoding interface}
\longrightarrow
\text{message channel}
\longrightarrow
\text{complete recovery protocol}.
\end{gathered}
A field state does not determine the second line.
Connections between the lines are proved only for explicitly stated
interfaces.

\paragraph{Route A.}
We construct and approximate the full selected radiation state,
including multiparticle occupation and packet correlations.

\paragraph{Route B.}
We transfer its vacuum/nonvacuum probability to an independently
specified logical benchmark. This is a nonvacuum-calibrated recovery
model, not a derived microscopic evaporation channel.

The stationary field formulation is the one specified in the supplied
Em03-A manuscript \cite{Em03A}, with the external Unruh-state
construction retained \cite{DMP}. The operational benchmark is a
specialization of the supplied En02-D model \cite{En02D}; its needed
claims are proved here.

\begin{center}
\renewcommand{\arraystretch}{1.13}
\begin{tabular}{@{}p{0.26\textwidth}p{0.27\textwidth}p{0.38\textwidth}@{}}
\toprule
Ingredient & Dependency & Status in this paper\\
\midrule
Stationary boundary covariance
& Em03-A; standard Hawking model
& Explicitly stated analytical input\\
Bulk state identification
& Dappiaggi--Moretti--Pinamonti
& External construction and Hadamard theorem\\
Radial scattering
& Specified Schwarzschild ODE
& Flux-normalized construction; approximation bounds\\
Selected density operator
& Quasifree field restriction
& Proved finite-mode representation\\
Occupation cutoff
& This paper
& Deterministic CPTP map and explicit errors\\
Message encoding and core
& Operational specification
& Additional model inputs\\
Recovery performance
& Specified channel and interface
& Analytical optima; numerical checks unexecuted\\
\bottomrule
\end{tabular}
\end{center}

\paragraph{Evidence status.}
No Python, solver, or pdfLaTeX execution is asserted.
The numerical appendix is an implementation specification, not a
results section. Analytical examples are explicitly identified.
An executed incorporation study requires actual archived runs and
inspection of their numerical and compilation records.

We use \(c=\hbar=k_B=1\), \(G>0\), and base-two entropy.
For states and channels,
\[
d_{\mathrm{tr}}(\rho,\sigma)=\frac12\left\lVert \rho-\sigma\right\rVert_1,\qquad
d_\diamond(\Phi,\Psi)=\frac12\left\lVert \Phi-\Psi\right\rVert_\diamond.

Channel comparisons include arbitrary references. Matrix denotes operator norm and denotes Frobenius norm.

Displayed formulas in this passage

  • unlabeled · line 174

    \begin{gathered}
    \text{specified field state}
    \longrightarrow
    \text{selected packet state}
    \longrightarrow
    \text{finite flagged representation},\\
    \text{declared encoding interface}
    \longrightarrow
    \text{message channel}
    \longrightarrow
    \text{complete recovery protocol}.
    \end{gathered}
    A field state does not determine the second line.
    Connections between the lines are proved only for explicitly stated
    interfaces.
    
    \paragraph{Route A.}
    We construct and approximate the full selected radiation state,
    including multiparticle occupation and packet correlations.
    
    \paragraph{Route B.}
    We transfer its vacuum/nonvacuum probability to an independently
    specified logical benchmark. This is a nonvacuum-calibrated recovery
    model, not a derived microscopic evaporation channel.
    
    The stationary field formulation is the one specified in the supplied
    Em03-A manuscript \cite{Em03A}, with the external Unruh-state
    construction retained \cite{DMP}. The operational benchmark is a
    specialization of the supplied En02-D model \cite{En02D}; its needed
    claims are proved here.
    
    \begin{center}
    \renewcommand{\arraystretch}{1.13}
    \begin{tabular}{@{}p{0.26\textwidth}p{0.27\textwidth}p{0.38\textwidth}@{}}
    \toprule
    Ingredient & Dependency & Status in this paper\\
    \midrule
    Stationary boundary covariance
    & Em03-A; standard Hawking model
    & Explicitly stated analytical input\\
    Bulk state identification
    & Dappiaggi--Moretti--Pinamonti
    & External construction and Hadamard theorem\\
    Radial scattering
    & Specified Schwarzschild ODE
    & Flux-normalized construction; approximation bounds\\
    Selected density operator
    & Quasifree field restriction
    & Proved finite-mode representation\\
    Occupation cutoff
    & This paper
    & Deterministic CPTP map and explicit errors\\
    Message encoding and core
    & Operational specification
    & Additional model inputs\\
    Recovery performance
    & Specified channel and interface
    & Analytical optima; numerical checks unexecuted\\
    \bottomrule
    \end{tabular}
    \end{center}
    
    \paragraph{Evidence status.}
    No Python, solver, or pdfLaTeX execution is asserted.
    The numerical appendix is an implementation specification, not a
    results section. Analytical examples are explicitly identified.
    An executed incorporation study requires actual archived runs and
    inspection of their numerical and compilation records.
    
    We use \(c=\hbar=k_B=1\), \(G>0\), and base-two entropy.
    For states and channels,
    \[
    d_{\mathrm{tr}}(\rho,\sigma)=\frac12\left\lVert \rho-\sigma\right\rVert_1,\qquad
    d_\diamond(\Phi,\Psi)=\frac12\left\lVert \Phi-\Psi\right\rVert_\diamond.