diff --git a/.datalad/config b/.datalad/config index 9aadc54..3298dba 100644 --- a/.datalad/config +++ b/.datalad/config @@ -1,5 +1,2 @@ [datalad "dataset"] id = 56aad42b-b483-4f65-9c63-d24ef3cac2c2 -[datalad "containers.TeX"] - image = .images/texlive - cmdexec = docker run {img} {cmd} diff --git a/cA_analysis b/cA_analysis index 6fd3a49..af344f1 160000 --- a/cA_analysis +++ b/cA_analysis @@ -1 +1 @@ -Subproject commit 6fd3a4938973adfa7b6444e8caf5d6282072c0ba +Subproject commit af344f1f55496eb05232ac7bc497a2100682d792 diff --git a/justfile b/justfile deleted file mode 100644 index f9c5a5b..0000000 --- a/justfile +++ /dev/null @@ -1,9 +0,0 @@ -_default: - @just --list - -compile MESSAGE: update-plots - datalad save -m "{{MESSAGE}}" talk.tex - datalad run -o talk.pdf -i talk.tex -m "build pdf" "lualatex talk.tex && lualatex talk.tex" - -update-plots: - datalad run -o plots -m "update plots" "bash plt_update.sh" \ No newline at end of file diff --git a/justfile b/justfile new file mode 120000 index 0000000..799f574 --- /dev/null +++ b/justfile @@ -0,0 +1 @@ +.git/annex/objects/ZZ/ZQ/MD5E-s312--c7c1fdc72cdf960f7ad7299d761074d1/MD5E-s312--c7c1fdc72cdf960f7ad7299d761074d1 \ No newline at end of file diff --git a/plots/T48L48_b4.00_k0.1384942/plot_dr_ds10-0124projection-wgcorr.pdf b/plots/T48L48_b4.00_k0.1384942/plot_dr_ds10-0124projection-wgcorr.pdf deleted file mode 120000 index 3534740..0000000 --- a/plots/T48L48_b4.00_k0.1384942/plot_dr_ds10-0124projection-wgcorr.pdf +++ /dev/null @@ -1 +0,0 @@ -../../.git/annex/objects/KZ/VK/MD5E-s15402--1c37f44962b8c3ae17584a237ea24d53.pdf/MD5E-s15402--1c37f44962b8c3ae17584a237ea24d53.pdf \ No newline at end of file diff --git a/plots/T48L48_b4.00_k0.1384942/plot_m_eff_P-0124projection-wgcorr.pdf b/plots/T48L48_b4.00_k0.1384942/plot_m_eff_P-0124projection-wgcorr.pdf deleted file mode 120000 index 5535c08..0000000 --- a/plots/T48L48_b4.00_k0.1384942/plot_m_eff_P-0124projection-wgcorr.pdf +++ /dev/null @@ -1 +0,0 @@ -../../.git/annex/objects/v6/9G/MD5E-s19583--53aa1c2167f4f91a219cae041f4d2c29.pdf/MD5E-s19583--53aa1c2167f4f91a219cae041f4d2c29.pdf \ No newline at end of file diff --git a/plots/T56L56_b4.10_k0.1381410/plot_dr_ds10-0124projection-wgcorr.pdf b/plots/T56L56_b4.10_k0.1381410/plot_dr_ds10-0124projection-wgcorr.pdf deleted file mode 120000 index 2f78368..0000000 --- a/plots/T56L56_b4.10_k0.1381410/plot_dr_ds10-0124projection-wgcorr.pdf +++ /dev/null @@ -1 +0,0 @@ -../../.git/annex/objects/fF/xf/MD5E-s16516--07e54acdcb61b8a95684bfb4afe9abfa.pdf/MD5E-s16516--07e54acdcb61b8a95684bfb4afe9abfa.pdf \ No newline at end of file diff --git a/plots/T56L56_b4.10_k0.1381410/plot_m_eff_P-0124projection-wgcorr.pdf b/plots/T56L56_b4.10_k0.1381410/plot_m_eff_P-0124projection-wgcorr.pdf deleted file mode 120000 index 37723c9..0000000 --- a/plots/T56L56_b4.10_k0.1381410/plot_m_eff_P-0124projection-wgcorr.pdf +++ /dev/null @@ -1 +0,0 @@ -../../.git/annex/objects/F6/g9/MD5E-s20786--5588f21cefc0aa7d831ba5df5d565c35.pdf/MD5E-s20786--5588f21cefc0aa7d831ba5df5d565c35.pdf \ No newline at end of file diff --git a/plots/ca2sym_b3.9.pdf b/plots/ca2sym_b3.9.pdf index 5326abc..58a6e5e 120000 --- a/plots/ca2sym_b3.9.pdf +++ b/plots/ca2sym_b3.9.pdf @@ -1 +1 @@ -../.git/annex/objects/3W/xG/MD5E-s15046--24f1eabf567a36fd075c012b14461706.9.pdf/MD5E-s15046--24f1eabf567a36fd075c012b14461706.9.pdf \ No newline at end of file +../.git/annex/objects/1g/K1/MD5E-s15046--bf0ab1e4bb9433d0cd294bdcb37528f4.9.pdf/MD5E-s15046--bf0ab1e4bb9433d0cd294bdcb37528f4.9.pdf \ No newline at end of file diff --git a/plots/ca2sym_b4.1.pdf b/plots/ca2sym_b4.1.pdf new file mode 120000 index 0000000..3edd9e1 --- /dev/null +++ b/plots/ca2sym_b4.1.pdf @@ -0,0 +1 @@ +../.git/annex/objects/6z/V6/MD5E-s15345--35daf76fc2bf3f2456596dada3d73214.1.pdf/MD5E-s15345--35daf76fc2bf3f2456596dada3d73214.1.pdf \ No newline at end of file diff --git a/plots/ca2sym_b4.pdf b/plots/ca2sym_b4.pdf index 90fc66a..33b1818 120000 --- a/plots/ca2sym_b4.pdf +++ b/plots/ca2sym_b4.pdf @@ -1 +1 @@ -../.git/annex/objects/j8/2p/MD5E-s15404--105a9b2fb44c4312cb5bc8b342093125.pdf/MD5E-s15404--105a9b2fb44c4312cb5bc8b342093125.pdf \ No newline at end of file +../.git/annex/objects/Kw/1V/MD5E-s15404--b75157f027d9e94d5e681c6a0c89229b.pdf/MD5E-s15404--b75157f027d9e94d5e681c6a0c89229b.pdf \ No newline at end of file diff --git a/plots/fix_sym_b3.9.pdf b/plots/fix_sym_b3.9.pdf index fb428fb..c832123 120000 --- a/plots/fix_sym_b3.9.pdf +++ b/plots/fix_sym_b3.9.pdf @@ -1 +1 @@ -../.git/annex/objects/zV/87/MD5E-s21143--f35d0804e7f94ed2ded33739cca4d926.9.pdf/MD5E-s21143--f35d0804e7f94ed2ded33739cca4d926.9.pdf \ No newline at end of file +../.git/annex/objects/P5/3V/MD5E-s21143--4a699d1536673f8706ad02885689edc8.9.pdf/MD5E-s21143--4a699d1536673f8706ad02885689edc8.9.pdf \ No newline at end of file diff --git a/plots/fix_sym_b4.1.pdf b/plots/fix_sym_b4.1.pdf new file mode 120000 index 0000000..bfc0af3 --- /dev/null +++ b/plots/fix_sym_b4.1.pdf @@ -0,0 +1 @@ +../.git/annex/objects/mf/KQ/MD5E-s21018--d579caf997fcc0f45b1b9ae51261fda1.1.pdf/MD5E-s21018--d579caf997fcc0f45b1b9ae51261fda1.1.pdf \ No newline at end of file diff --git a/plots/fix_sym_b4.pdf b/plots/fix_sym_b4.pdf index 8eb9797..68051c3 120000 --- a/plots/fix_sym_b4.pdf +++ b/plots/fix_sym_b4.pdf @@ -1 +1 @@ -../.git/annex/objects/Gj/z9/MD5E-s21036--4409bd5d72b3d7d678b913288d652f3e.pdf/MD5E-s21036--4409bd5d72b3d7d678b913288d652f3e.pdf \ No newline at end of file +../.git/annex/objects/zq/Fp/MD5E-s21036--57382f1fc56bd304ae27c2f135bb0960.pdf/MD5E-s21036--57382f1fc56bd304ae27c2f135bb0960.pdf \ No newline at end of file diff --git a/plots/g0sq_chi.pdf b/plots/g0sq_chi.pdf index de57bf7..232e086 120000 --- a/plots/g0sq_chi.pdf +++ b/plots/g0sq_chi.pdf @@ -1 +1 @@ -../.git/annex/objects/Kx/F1/MD5E-s20086--bac2b7f5102e68b001f01b14f0a73c62.pdf/MD5E-s20086--bac2b7f5102e68b001f01b14f0a73c62.pdf \ No newline at end of file +../.git/annex/objects/kz/mZ/MD5E-s20071--63797fdd400035849b1bd06ea3b76f81.pdf/MD5E-s20071--63797fdd400035849b1bd06ea3b76f81.pdf \ No newline at end of file diff --git a/plots/g0sq_sym.pdf b/plots/g0sq_sym.pdf index e298037..8177674 120000 --- a/plots/g0sq_sym.pdf +++ b/plots/g0sq_sym.pdf @@ -1 +1 @@ -../.git/annex/objects/04/f4/MD5E-s20401--6a13a0a0544ed1542f580b8e9ebad42c.pdf/MD5E-s20401--6a13a0a0544ed1542f580b8e9ebad42c.pdf \ No newline at end of file +../.git/annex/objects/pV/2m/MD5E-s20432--9e1ca9bcf2606c369e33342243db08bd.pdf/MD5E-s20432--9e1ca9bcf2606c369e33342243db08bd.pdf \ No newline at end of file diff --git a/plots/test_f_part_ZA_chi_imp.pdf b/plots/test_f_part_ZA_chi_imp.pdf deleted file mode 120000 index 667e6a7..0000000 --- a/plots/test_f_part_ZA_chi_imp.pdf +++ /dev/null @@ -1 +0,0 @@ -../.git/annex/objects/vX/35/MD5E-s27909--5d40d50f3aff4fd9aca6002702e6a833.pdf/MD5E-s27909--5d40d50f3aff4fd9aca6002702e6a833.pdf \ No newline at end of file diff --git a/plt_update.sh b/plt_update.sh index 21ee95c..6de0a92 100644 --- a/plt_update.sh +++ b/plt_update.sh @@ -1,15 +1,6 @@ #! /bin/bash -rm -rf plots/* -mkdir plots/{T48L48_b4.00_k0.1384942,T56L56_b4.10_k0.1381410} - -datalad update -d cA_analysis --how=merge -datalad get cA_analysis/plot_vault/{overview,interpolations,T48L48_b4.00_k0.1384942,T56L56_b4.10_k0.1381410} - -cp ./cA_analysis/plot_vault/overview/plateaus_{chi,sym}_0.2_0.3_0124_ee_ee_total_quad.pdf plots -cp ./cA_analysis/plot_vault/interpolations/fix_sym_b{3.9,4}.pdf plots -cp ./cA_analysis/plot_vault/interpolations/ca2sym_b{3.9,4}.pdf plots -cp ./cA_analysis/plot_vault/interpolations/g0sq_{chi,sym}.pdf plots -cp ../../research_env2/charmonium_analysis/plot_vault/decay_constants/test_f_part_ZA_chi_imp.pdf plots - -cp ./cA_analysis/plot_vault/T48L48_b4.00_k0.1384942/plot_{dr_ds10,m_eff_P}-0124projection-wgcorr.pdf plots/T48L48_b4.00_k0.1384942 -cp ./cA_analysis/plot_vault/T56L56_b4.10_k0.1381410/plot_{dr_ds10,m_eff_P}-0124projection-wgcorr.pdf plots/T56L56_b4.10_k0.1381410 \ No newline at end of file +rm plots/* +cp ../../research_env2/cA_analysis/plot_vault/overview/plateaus_{chi,sym}_0.2_0.3_0124_ee_ee_total_quad.pdf plots +cp ../../research_env2/cA_analysis/plot_vault/interpolations/fix_sym_b{3.9,4}.pdf plots +cp ../../research_env2/cA_analysis/plot_vault/interpolations/ca2sym_b{3.9,4}.pdf plots +cp ../../research_env2/cA_analysis/plot_vault/interpolations/g0sq_{chi,sym}.pdf plots \ No newline at end of file diff --git a/talk.pdf b/talk.pdf index cfaf992..e069213 120000 --- a/talk.pdf +++ b/talk.pdf @@ -1 +1 @@ -.git/annex/objects/7V/7P/MD5E-s446841--cdc44d630eb943ea5cb4bc1f4d1a00c2.pdf/MD5E-s446841--cdc44d630eb943ea5cb4bc1f4d1a00c2.pdf \ No newline at end of file +.git/annex/objects/zK/3g/MD5E-s367460--c68ea62437ece7020a749496a366b2ba.pdf/MD5E-s367460--c68ea62437ece7020a749496a366b2ba.pdf \ No newline at end of file diff --git a/talk.tex b/talk.tex index f7da0af..350e3ec 100644 --- a/talk.tex +++ b/talk.tex @@ -75,40 +75,36 @@ \frametitle{Determination of $\ca$} \begin{itemize} \item Schrödinger functional boundary conditions - \item similar to quenched \arxivtag{hep-lat/9609035}, $N_{\rm f} = 2$ \arxivtag{hep-lat/0503003} and std. Wilson-Clover $N_{\rm f} = 3$ \arxivtag{1502.04999, hep-lat/0703006} + \item similar to quenched \arxivtag{hep-lat/9609035}, $N_{\rm f} = 2$ \arxivtag{hep-lat/0503003} and std. Wilson-Clover $N_{\rm f} = 3$ \arxivtag{1502.04999} \item derive from PCAC mass \end{itemize} \vspace{.5cm} $$m_{\rm PCAC} = \frac{\partial_0 f_{\rm A}}{2f_{\rm P}} + \ca~a\frac{\partial^2_0 f_{\rm P}}{2f_{\rm P}} = r + \ca~as$$ $$m_{\rm PCAC}^{(0)} = m_{\rm PCAC}^{(1)}\quad\Leftrightarrow\quad\ca = - \frac{r^{(1)} - r^{(0)}}{s^{(1)} - s^{(0)}}$$ - \begin{itemize} - \item states (0) and (1) are the PS ground and first excited state in our setup - \item PCAC relation holds for both - \end{itemize} \end{frame} \begin{frame} \frametitle{The wavefunction method} \begin{itemize} - \item construct pseudoscalar states + \item mimic pionic sources on boundaries $\pi^{(0)}, \pi^{(1)}$ and require PCAC relation to hold for both \begin{itemize} - \item H-like basis wavefunctions: - $\omega_{1} = e^{-r/a_0}\;,\quad\omega_{2} = r~e^{-r/a_0}\;,\quad\omega_{3} = e^{-r/(2a_0)}$ - \item also include $\omega_{4} = {\rm cons.}\;,\quad\omega_{5} = -r^2~e^{-r/a_0}$ + \item basis wavefunctions: + $\omega_{\rm b1} = e^{-r/a_0}\;,\quad\omega_{\rm b2} = r~e^{-r/a_0}\;,\quad\omega_{\rm b3} = e^{-r/(2a_0)}$ + \item also include $\omega_{\rm b4} = {\rm cons.}\;,\quad\omega_{\rm b5} = -r^2~e^{-r/a_0}$ \quad with $r=|\vec{y}-\vec{x}|$ \end{itemize} \pause - \item diagonalise boundary-to-boundary corr. func. $(F_1)_{i,j} = -\langle O(\omega_{i}) O'(\omega_{j})\rangle$ + \item eigenvectors of boundary-to-boundary corr. func. $(F_1)_{i,j} = -\langle O(\omega_{{\rm b}i}) O'(\omega_{{\rm b}j})\rangle$ \vspace{.5cm} \pause - \item employ eigenvectors of $(F_1)_{i,j}$ to project $f_{\rm A}(x_0)$ and $f_{\rm P}(x_0)$ onto the eigenstates + \item diagonalise $(F_1)_{i,j}$ \& project $f_{\rm A}(x_0)$ and $f_{\rm P}(x_0)$ onto the eigenstates % Question: do we include all wavefunctions or just some? % How does this interplay with the states that we achieve? % Which is the optimal wf combination? % \item also: where on the lattice do we define $c_{\rm A}$? \vspace{.5cm} \pause - \item evaluate $c_{\rm A}(x_0)$ with projected correlation functions + \item evaluate $c_{\rm A}(x_0)$ with these source terms \item later: choice of $x_0$ and wavefunction basis is part of the improvement condition \end{itemize} \end{frame} @@ -120,7 +116,7 @@ \begin{center} \begin{tabular}{cc|c|c|c|c} \toprule - $L/a$ & $\beta$ & $\kappa_{1}\approx\kappa_{\rm cr}$ & $\kappa_{2}$ & $\kappa_{3}\approx\kappa_{\rm sym}$&$\approx a\;{\rm [fm]}$\\ + $L/a$ & $\beta$ & $\kappa_{1}\approx\kappa_{\rm cr}$ & $\kappa_{2}$ & $\kappa_{3}\approx\kappa_{\rm sym}$&$\approx a$\\ \midrule 24&3.685&0.1396980&0.1395500&0.1394400&0.120\\ 32&3.80&0.1392500&---&0.1389630&0.095\\ @@ -182,7 +178,7 @@ \begin{frame} \frametitle{Improvement of the axial-vector current} - \framesubtitle{Interpolations in $g_0^2$} + \framesubtitle{Final interpolations in $g_0^2$} \begin{tabular}{cc} \includegraphics[width=\halflinewidth]{plots/g0sq_chi.pdf}& \includegraphics[width=\halflinewidth]{plots/g0sq_sym.pdf} @@ -193,27 +189,24 @@ \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 $\ca(g_0^2)|_{\rm sym}$ - $$f_{\pi K}^{\rm RI} = Z_{\rm A} (1+b_{\rm A} am_{\rm q}+\bar{b}_{\rm A} a\Tr[M_{\rm q}])\frac{\sqrt{2} \mathcal{A}_{\rm A_0P}}{\sqrt{\mathcal{A}_{\rm PP} m_\pi}}$$ - with $C_{XX} \propto \mathcal{A}_{XX}{\rm e}^{-mx_0}$ + $$f_{\rm A}^{RI} = Z_{\rm A} (1+b_{\rm A} m_{\rm q})(1+\bar{b}_{\rm A} \Tr[M_{\rm q}])f\frac{\sqrt{2} \mathcal{A}_{\rm A_0P}}{\sqrt{\mathcal{A}_{\rm PP} m_\pi}}$$ \item renormalisation: $Z_{\rm A}$ preliminary, $b_{\rm A}$ from pert. theory, $\bar{b}_{\rm A}$ neglected \end{itemize} \end{frame} \begin{frame} - \frametitle{First scaling test of improvement} + \frametitle{First study of improvement} \framesubtitle{Results} - \vspace{-.3cm} - \centering - \includegraphics[width=.6\linewidth]{plots/test_f_part_ZA_chi_imp.pdf} + %\includegraphics{plots/test_f.pdf} \end{frame} \begin{frame} \frametitle{Outlook} \begin{itemize} - \item finish $\za$, $\zv$, $\bV$ and $\bar{b}_{\rm V}$ through SF + \item finish $\zv$, $\bV$ and $\bar{b}_{\rm V}$ through SF \item further improvement and renormalisation currently in the works: \begin{itemize} \item vector and tensor current improvement ($c_{\rm V}$, $c_{\rm T}$) @@ -222,22 +215,4 @@ \end{itemize} \end{itemize} \end{frame} - -\begin{frame} - \frametitle{Backup} - \framesubtitle{$\Delta r$ and $\Delta s$ behaviour} - \begin{tabular}{cc} - \includegraphics[width=\halflinewidth]{plots/T48L48_b4.00_k0.1384942/plot_dr_ds10-0124projection-wgcorr.pdf}& - \includegraphics[width=\halflinewidth]{plots/T56L56_b4.10_k0.1381410/plot_dr_ds10-0124projection-wgcorr.pdf} - \end{tabular} -\end{frame} - -\begin{frame} - \frametitle{Backup} - \framesubtitle{Behaviour of $\fp$ projected} - \begin{tabular}{cc} - \includegraphics[width=\halflinewidth]{plots/T48L48_b4.00_k0.1384942/plot_m_eff_P-0124projection-wgcorr.pdf}& - \includegraphics[width=\halflinewidth]{plots/T56L56_b4.10_k0.1381410/plot_m_eff_P-0124projection-wgcorr.pdf} - \end{tabular} -\end{frame} \end{document}