This commit is contained in:
Zheyuan Wu
2026-03-29 18:08:48 -05:00
parent dd10a1969b
commit 2949c3e5b6
14 changed files with 720 additions and 663 deletions

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@@ -551,7 +551,7 @@ Thus entanglement entropy is the von Neumann entropy of a subsystem, and it meas
\begin{block}{Projective-space estimate from Gromov}
For $0<\kappa<1$,
$$
\obdiam(\mathbb{C}P^n(1);-\kappa)\leq O(\sqrt{n}).
\obdiam(\mathbb{C}P^n(1);-\kappa)\leq O\left(\frac{1}{\sqrt{n}}\right).
$$
\end{block}
@@ -562,7 +562,7 @@ Thus entanglement entropy is the von Neumann entropy of a subsystem, and it meas
\end{itemize}
Hayden's work suggests that if the entropy function is a ``good'' proxy for the observable diameter, the difference of \textbf{the order of the growth} between $\obdiam(\mathbb{C}P^n(1);-\kappa)$ and $\obdiam(S^{2n+1}(1);-\kappa)$ should be smaller than $O(\sqrt{n})$.
Hayden's work suggests that if the entropy function is a ``good'' proxy for the observable diameter, the difference of \textbf{the order of the growth} between $\obdiam(\mathbb{C}P^n(1);-\kappa)$ and $\obdiam(S^{2n+1}(1);-\kappa)$ should be smaller than $O\left(\frac{1}{\sqrt{n}}\right)$.
\end{frame}
\begin{frame}{A conjecture}
@@ -570,7 +570,7 @@ Thus entanglement entropy is the von Neumann entropy of a subsystem, and it meas
For $0<\kappa<1$,
$$
\obdiam(\mathbb{C}P^n(1);-\kappa)= O(\sqrt{n}).
\obdiam(\mathbb{C}P^n(1);-\kappa)= O\left(\frac{1}{\sqrt{n}}\right).
$$
\end{block}