{"file_name":"2003.07090_cohen_20200314_journal_table_0.png","ground_truth":"\\begin{tabular}{lccccl}[NEWLINE]\\hline\\hline[NEWLINE]Frequency\u0026R\u0026$\\Phi$\u0026$\\Psi$\\\\[NEWLINE]GHz\u0026\u0026(degr)\u0026(degr)\\\\\\hline[NEWLINE]8.35\u00260.95\u002610\u002690\\\\[NEWLINE]10.45\u00261.05\u002610\u002690\\\\[NEWLINE]\\hline[NEWLINE]\\end{tabular}"}
{"file_name":"2003.07092_main_table_0.png","ground_truth":"\\begin{tabular}{|l|c|c|c|c|c|}[NEWLINE]\\hline[NEWLINE]$b_{00}$\u0026$F_3$\u0026$t_{EH}(0)$\\\\[NEWLINE]\\hline[NEWLINE]\\hline[NEWLINE]$10^{-1}$\u0026-1\u00260.146174\\\\[NEWLINE]\\hline[NEWLINE]$10^{-1}$\u0026-5\u00260.586922\\\\[NEWLINE]\\hline[NEWLINE]$10^{-1}$\u0026-20\u00260.646240\\\\[NEWLINE]\\hline[NEWLINE]$10^{-1}$\u0026-50\u00260.646667\\\\[NEWLINE]\\hline[NEWLINE]$10^{-1}$\u0026-100\u00260.646667\\\\[NEWLINE]\\hline[NEWLINE]$10^{-1}$\u0026-200\u00260.646667\\\\[NEWLINE]\\hline[NEWLINE]$10^{-2}$\u0026-1\u00260.170522\\\\[NEWLINE]\\hline[NEWLINE]$10^{-2}$\u0026-5\u00260.609225\\\\[NEWLINE]\\hline[NEWLINE]$10^{-2}$\u0026-20\u00260.664501\\\\[NEWLINE]\\hline[NEWLINE]$10^{-2}$\u0026-50\u00260.664667\\\\[NEWLINE]\\hline[NEWLINE]$10^{-2}$\u0026-100\u00260.664667\\\\[NEWLINE]\\hline[NEWLINE]$10^{-2}$\u0026-200\u00260.664668\\\\[NEWLINE]\\hline[NEWLINE]\\end{tabular}"}
{"file_name":"2003.07101_paper_table_0.png","ground_truth":"\\begin{tabular}{|c||c|c|c|}[NEWLINE]\\hline[NEWLINE]method\u0026Top-1\u0026Top-5\u0026\\#params\\\\\\hline\\hline[NEWLINE]chance\u00260.8\\%\u00263.9\\%\u0026-\\\\\\hline[NEWLINE]HED\u00260.4\\%\u00263.2\\%\u002614.7M\\\\\\hline[NEWLINE]MSE\u00261.3\\%\u00264.9\\%\u0026\\textbf{17.0M}\\\\\\hline\\hline[NEWLINE]PSim\u002637.9\\%\u002660.2\\%\u0026\\textbf{17.0M}\\\\\\hline[NEWLINE]PSim+flip\u002647.1\\%\u002669.2\\%\u0026\\textbf{17.0M}\\\\\\hline[NEWLINE]PSim+flip+AdaIN\u002661.4\\%\u002679.9\\%\u002618.2M\\\\\\hline[NEWLINE]PSim+flip+AdaIN+skip1\u002662.3\\%\u002680.7\\%\u002619.2M\\\\\\hline[NEWLINE]PSim+flip+AdaIN+skip\u0026\\textbf{66.6\\%}\u0026\\textbf{85.6\\%}\u002621.3M\\\\\\hline\\hline[NEWLINE]groundtruth\u002691\\%\u002698\\%\u0026-\\\\\\hline[NEWLINE]\\end{tabular}"}
{"file_name":"2003.07107_SWIPTMISOCIMMDCSK_table_0.png","ground_truth":"\\begin{tabular}{|c|c|c|c|c|c|c|}[NEWLINE]\\hline[NEWLINE]\\multirow{2}{*}{Antennas}\u0026[NEWLINE]\\multicolumn{3}{c|}{Channelgains}\u0026\\multicolumn{3}{c|}{Pathdelay}\\\\[NEWLINE]\\cline{2-7}[NEWLINE]\u0026$\\E[\\alpha_{1}^2]$\u0026$\\E[\\alpha_{2}^2]$\u0026$\\E[\\alpha_{3}^2]$\u0026$\\tau_1$\u0026$\\tau_2$\u0026$\\tau_3$\\\\[NEWLINE]\\hline[NEWLINE]$1$\u00260.7\u00260.2\u00260.1\u00260\u00262\u00265\\\\[NEWLINE]\\hline[NEWLINE]$2$\u00260.6\u00260.25\u00260.15\u00260\u00263\u00266\\\\[NEWLINE]\\hline[NEWLINE]$3$\u00260.8\u00260.12\u00260.08\u00260\u00261\u00262\\\\[NEWLINE]\\hline[NEWLINE]$4$\u00260.28\u00260.42\u00260.3\u00260\u00262\u00264\\\\[NEWLINE]\\hline[NEWLINE]\\end{tabular}"}
{"file_name":"2003.07111_uav_table_0.png","ground_truth":"\\begin{tabular}{lll}[NEWLINE]\\hline[NEWLINE]Case\u0026Author\u0026Executiontime($\\mu$s)\\\\\\hline[NEWLINE]$fHf$\u0026Our\u002614\\\\[NEWLINE]\u0026Ding~\\etal{}~\\cite{ding-etal-2019-iccv}\u00261052\\\\[NEWLINE]$fEf$\u0026Kukelova~\\etal{}~\\cite{kukelova-etal-2017-cvpr}\u0026103\\\\\\hline[NEWLINE]$Hf$\u0026Our\u00265\\\\[NEWLINE]\u0026Ding~\\etal{}~\\cite{ding-etal-2019-iccv}\u0026124\\\\[NEWLINE]$Ef$\u0026Kukelova~\\etal{}~\\cite{kukelova-etal-2017-cvpr}\u002625\\\\\\hline[NEWLINE]$f_1Hf_2$\u0026Our\u00269\\\\[NEWLINE]\u0026Ding~\\etal{}.~\\cite{ding-etal-2019-iccv}\u002647\\\\[NEWLINE]$f_1Ef_2$\u0026Bougnoux~\\cite{bougnoux-iccv-1998}\u002627\\\\\\hline[NEWLINE]\\end{tabular}"}
{"file_name":"2003.07111_uav_table_1.png","ground_truth":"\\begin{tabular}{lll}[NEWLINE]\\hline[NEWLINE]Case\u0026Author\u0026Executiontime(ms)\\\\\\hline[NEWLINE]$fHf$\u0026Our\u00260.035\\\\[NEWLINE]\u0026Ding~\\etal{}~\\cite{ding-etal-2019-iccv}\u002619.32\\\\[NEWLINE]$fEf$\u0026Kukelova~\\etal{}~\\cite{kukelova-etal-2017-cvpr}\u00260.118\\\\\\hline[NEWLINE]%$Hf$\u0026Our\u00265\\\\[NEWLINE]%\u0026Ding~\\etal{}~\\cite{ding-etal-2019-iccv}\u0026124\\\\[NEWLINE]%$Ef$\u0026Kukelova~\\etal{}~\\cite{kukelova-etal-2017-cvpr}\u002625\\\\\\hline[NEWLINE]%$f_1Hf_2$\u0026Our\u00269\\\\[NEWLINE]%\u0026Ding~\\etal{}.~\\cite{ding-etal-2019-iccv}\u002647\\\\[NEWLINE]%\u0026Bougnoux~\\cite{bougnoux-iccv-1998}\u002627\\\\\\hline[NEWLINE]\\end{tabular}"}
{"file_name":"2003.07116_f_0_spectra_and_psi_radiative_decay_to_f_0_-1205_table_0.png","ground_truth":"\\begin{tabular}{cccc}[NEWLINE]\\hline[NEWLINE]\\hline[NEWLINE]~~\u0026~~experimentalvalue~~\u0026~~schemeI~~\u0026~~schemeII~~\\\\[NEWLINE]\\hline[NEWLINE]$R^{f_0(1370)}_{\\pi\\pi/K\\barK}$\u0026$\u003e1$\u0026$3.98\\sim11.68$\u0026$1.22\\sim1.88$\\\\[NEWLINE]$R^{f_0(1370)}_{\\eta\\eta/\\pi\\pi}$\u0026\u0026$0.01\\sim0.05$\u0026$0.12\\sim0.21$\\\\[NEWLINE]$R^{f_0(1370)}_{K\\barK/\\eta\\eta}$\u0026\u0026$5.53\\sim7.44$\u0026$3.84\\sim4.31$\\\\[NEWLINE]%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%[NEWLINE]$R^{f_0(1500)}_{\\pi\\pi/K\\barK}$\u0026$4.1\\pm0.5$\u0026$1.81\\sim9520.07$\u0026$0.02\\sim0.47$\\\\[NEWLINE]$R^{f_0(1500)}_{\\eta\\eta/\\pi\\pi}$\u0026$0.173\\pm0.024$\u0026$8.65\\times10^{-5}\\sim0.14$\u0026$0.78\\sim17.32$\\\\[NEWLINE]$R^{f_0(1500)}_{K\\barK/\\eta\\eta}$\u0026$1.43\\pm0.24$\u0026$0.48\\sim10.72$\u0026$2.71\\sim3.31$\\\\[NEWLINE]%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%[NEWLINE]$R^{f_0(1710)}_{\\pi\\pi/K\\barK}$\u0026$0.23\\pm0.05$\u0026$0.30\\sim0.41$\u0026$0.71\\sim112.38$\\\\[NEWLINE]$R^{f_0(1710)}_{\\eta\\eta/\\pi\\pi}$\u0026$2.09\\pm0.80$\u0026$0.59\\sim0.82$\u0026$9.69\\times10^{-4}\\sim4.87$\\\\[NEWLINE]$R^{f_0(1710)}_{\\eta\\eta/K\\barK}$\u0026$0.48\\pm0.15$\u0026$0.24\\sim0.25$\u0026$6.86\\times10^{-4}\\sim114.20$\\\\[NEWLINE]\\hline[NEWLINE]\\hline[NEWLINE]\\end{tabular}"}
{"file_name":"2003.07116_f_0_spectra_and_psi_radiative_decay_to_f_0_-1205_table_1.png","ground_truth":"\\begin{tabular}{cccc}[NEWLINE]\\hline[NEWLINE]\\hline[NEWLINE]~~\u0026~~resultsfromRef.\\cite{Cheng:2015iaa}~~\u0026~~withoutglueballcomponent~~\u0026~~withglueballcomponent~~\\\\[NEWLINE]\\hline[NEWLINE]$\\frac{\\Gamma(f_0(1370)\\to\\gamma\\gamma)}{\\Gamma(f_0(1500)\\to\\gamma\\gamma)}$\u00269.3\u0026$27.2\\sim1.93\\times10^7$\u0026$19.0\\sim3208.3$\\\\[NEWLINE]$\\frac{\\Gamma(f_0(1710)\\to\\gamma\\gamma)}{\\Gamma(f_0(1500)\\to\\gamma\\gamma)}$\u00261.7\u0026$5.8\\sim4.13\\times10^6$\u0026$0.003\\sim33.0$\\\\[NEWLINE]$\\frac{\\Gamma(f_0(1710)\\to\\gamma\\gamma)}{\\Gamma(f_0(1370)\\to\\gamma\\gamma)}$\u00260.183\u0026$0.087\\sim0.261$\u0026$6.8\\times10^{-5}\\sim0.016$\\\\[NEWLINE]\\hline[NEWLINE]\\hline[NEWLINE]\\end{tabular}"}
{"file_name":"2003.07118_IEEE-cross-spectrum_table_0.png","ground_truth":"\\begin{tabular}{||r||rrrr|rr||}[NEWLINE]\\hline[NEWLINE]\\hline[NEWLINE]\\multirow{4}{1.6cm}{\\textbf{Expectedprobabilities(\\%)}}\u0026\\multicolumn{6}{c||}{\\textbf{Trueprobabilities(\\%)}}\\\\[NEWLINE]\\cline{2-7}[NEWLINE]\u0026\\multicolumn{4}{c|}{Degreesoffreedom:2}\u0026\\multicolumn{2}{c||}{dof:8}\\\\[NEWLINE]\\cline{2-7}[NEWLINE]\u0026\\multicolumn{4}{c|}{$\\sigma_C^2=$0}\u00260\u00260.5\\\\[NEWLINE]\\cline{2-7}[NEWLINE]\u0026$\\sigma_B^2=$2\u00261\u00262/3\u00261/2\u00261\u00261\\\\[NEWLINE]\\hline[NEWLINE]\\hline[NEWLINE]\\multicolumn{1}{||l||}{Quantiles}\u0026\u0026\u0026\u0026\u0026\u0026\\\\[NEWLINE]%\\input{all_bounds.tex}[NEWLINE]0.5\u00260.50\u00260.39\u00260.25\u00260.16\u00260.35\u00260.39\\\\[NEWLINE]2.5\u00262.50\u00262.10\u00261.58\u00261.19\u00261.98\u00262.13\\\\[NEWLINE]5.0\u00265.00\u00264.36\u00263.51\u00262.82\u00264.18\u00264.44\\\\[NEWLINE]16.0\u002616.00\u002614.95\u002613.43\u002612.05\u002614.68\u002615.18\\\\[NEWLINE]50.0\u002650.00\u002650.01\u002650.00\u002650.00\u002650.00\u002649.99\\\\[NEWLINE]84.0\u002684.00\u002685.07\u002686.59\u002687.96\u002685.32\u002684.58\\\\[NEWLINE]95.0\u002695.00\u002695.65\u002696.50\u002697.19\u002695.82\u002695.37\\\\[NEWLINE]97.5\u002697.50\u002697.91\u002698.43\u002698.82\u002698.02\u002697.73\\\\[NEWLINE]99.5\u002699.50\u002699.62\u002699.75\u002699.84\u002699.65\u002699.57\\\\[NEWLINE]\\hline[NEWLINE]\\hline[NEWLINE]\\multicolumn{1}{||l||}{Intervals}\u0026\u0026\u0026\u0026\u0026\u0026\\\\[NEWLINE]%\\input{all_intervals.tex}[NEWLINE]68.0\u002668.00\u002670.12\u002673.16\u002675.91\u002670.64\u002669.41\\\\[NEWLINE]90.0\u002690.00\u002691.29\u002692.98\u002694.37\u002691.64\u002690.93\\\\[NEWLINE]95.0\u002695.00\u002695.82\u002696.84\u002697.63\u002696.04\u002695.60\\\\[NEWLINE]99.0\u002699.00\u002699.23\u002699.50\u002699.68\u002699.30\u002699.18\\\\[NEWLINE]\\hline[NEWLINE]\\hline[NEWLINE]\\end{tabular}"}
{"file_name":"2003.07118_IEEE-cross-spectrum_table_1.png","ground_truth":"\\begin{tabular}{c|rr|c}[NEWLINE]\\multicolumn{1}{c|}{Target$Z_0$(a.u.)}\u0026\\multicolumn{2}{c|}{95\\%bound}\u0026\\multicolumn{1}{c}{Trueprob.(\\%)}\\\\[NEWLINE]\\multicolumn{1}{c|}{}\u0026Emp\u0026Theo\u0026\\multicolumn{1}{c}{}\\\\[NEWLINE]\\hline[NEWLINE]-1.00\u002614.04\u002613.65\u002694.90\\\\[NEWLINE]0.00\u002615.11\u002613.65\u002694.53\\\\[NEWLINE]0.10\u002614.52\u002614.27\u002694.91\\\\[NEWLINE]0.20\u002614.98\u002614.90\u002694.96\\\\[NEWLINE]0.32\u002615.87\u002615.66\u002694.94\\\\[NEWLINE]0.50\u002617.37\u002616.90\u002694.87\\\\[NEWLINE]1.00\u002620.40\u002620.14\u002694.93\\\\[NEWLINE]2.00\u002627.61\u002628.65\u002695.18\\\\[NEWLINE]3.16\u002638.19\u002639.08\u002695.08\\\\[NEWLINE]5.00\u002657.15\u002656.55\u002694.91\\\\[NEWLINE]10.00\u0026109.66\u0026104.82\u002694.78[NEWLINE]\\end{tabular}"}