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Justus Kuhlmann 2024-07-30 00:48:33 +02:00
parent ef123b5ddd
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talk.tex
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@ -116,7 +116,7 @@
\begin{center}
\begin{tabular}{cc|c|c|c|c}
\toprule
$L/a$ & $\beta$ & $\kappa_{1}\approx\kappa_{\rm cr}$ & $\kappa_{2}$ & $\kappa_{3}\approx\kappa_{\rm sym}$&$a$\\
$L/a$ & $\beta$ & $\kappa_{1}\approx\kappa_{\rm cr}$ & $\kappa_{2}$ & $\kappa_{3}\approx\kappa_{\rm sym}$&$\tilde a$\\
\midrule
24&3.685&0.1396980&0.1395500&0.1394400&0.120\\
32&3.80&0.1392500&---&0.1389630&0.095\\
@ -189,7 +189,7 @@
\begin{frame}
\frametitle{First scaling test of improvement}
\begin{itemize}
\item Example: Calculate $f_\pi/K$ with stabilised WIlson fermions
\item Example: Calculate $f_\pi/K$ with stabilised Wilson fermions
\item symmetric point \openlat~ensembles
\item improve with $\ca = 0$ vs $\ca(g_0^2)|_{\rm chi}$ vs $\ca(g_0^2)|_{\rm sym}$
$$f_{\rm A}^{RI} = Z_{\rm A} (1+b_{\rm A} m_{\rm q})(1+\bar{b}_{\rm A} \Tr[M_{\rm q}])f\frac{\sqrt{2} \mathcal{A}_{\rm A_0P}}{\sqrt{\mathcal{A}_{\rm PP} m_\pi}}$$