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\documentclass[11pt,a4paper]{article}
\usepackage[utf8]{inputenc}
\usepackage[T1]{fontenc}
\usepackage[margin=1in]{geometry}
\usepackage{amsmath,amssymb,amsthm,mathtools}
\usepackage{hyperref}
\usepackage{enumitem}
\usepackage{microtype}
\usepackage{booktabs}
\title{Terminal Rigidity Witnesses and the Einstein--Rosen Bridge:\\
A Zero-Capacity Invariant for Physical Inference}
\author{Inacio F. Vasquez\\Independent Researcher}
\date{January 2026}
\newtheorem{theorem}{Theorem}
\newtheorem{lemma}{Lemma}
\newtheorem{definition}{Definition}
\newtheorem{corollary}{Corollary}
\newcommand{\Capacity}{\mathrm{Cap}}
\newcommand{\TC}{\mathrm{TC}}
\newcommand{\SIGC}{\mathbf{SIGC}}
\begin{document}
\maketitle
\begin{abstract}
We formalize the notion of a \emph{Terminal Rigidity Witness}: a physical system whose global
structure is nontrivial while its operational information capacity is exactly zero.
We show that the classical Einstein--Rosen bridge provides a canonical example.
\end{abstract}
\section{Transcript Capacity}
For an interface producing transcript $Y_{1:T}$ from hidden state $X$, define
\[
\TC(T) := \sup I(X;Y_{1:T}).
\]
\section{Terminal Rigidity}
A system $S$ is a terminal rigidity witness if
\[
\Capacity(\mathcal C_S) = 0
\]
while $S$ has nontrivial global structure.
\section{Einstein--Rosen Bridge}
Topological censorship implies no causal curve connects the two asymptotic regions of the
maximal Schwarzschild extension. Hence the induced channel has zero capacity.
\begin{theorem}
The Einstein--Rosen bridge is a terminal rigidity witness.
\end{theorem}
\end{document}