bugfix
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@@ -551,7 +551,7 @@ Thus entanglement entropy is the von Neumann entropy of a subsystem, and it meas
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\begin{block}{Projective-space estimate from Gromov}
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For $0<\kappa<1$,
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$$
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\obdiam(\mathbb{C}P^n(1);-\kappa)\leq O(\sqrt{n}).
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\obdiam(\mathbb{C}P^n(1);-\kappa)\leq O\left(\frac{1}{\sqrt{n}}\right).
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$$
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\end{block}
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@@ -562,7 +562,7 @@ Thus entanglement entropy is the von Neumann entropy of a subsystem, and it meas
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\end{itemize}
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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 $O(\sqrt{n})$.
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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 $O\left(\frac{1}{\sqrt{n}}\right)$.
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\end{frame}
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\begin{frame}{A conjecture}
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@@ -570,7 +570,7 @@ Thus entanglement entropy is the von Neumann entropy of a subsystem, and it meas
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For $0<\kappa<1$,
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$$
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\obdiam(\mathbb{C}P^n(1);-\kappa)= O(\sqrt{n}).
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\obdiam(\mathbb{C}P^n(1);-\kappa)= O\left(\frac{1}{\sqrt{n}}\right).
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$$
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\end{block}
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