Added average error figure and changed figure positioning to h
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@ -357,7 +357,7 @@ using a \ac{BP} decoder, as a reference.
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The results from Wadayama et al. are shown with solid lines,
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The results from Wadayama et al. are shown with solid lines,
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while the newly generated ones are shown with dashed lines.
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while the newly generated ones are shown with dashed lines.
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\begin{figure}[H]
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\begin{figure}[h]
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\centering
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\centering
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\begin{tikzpicture}
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\begin{tikzpicture}
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@ -434,12 +434,11 @@ Evidently, while the decoding performance does depend on the value of
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$\gamma$, there is no single optimal value offering optimal performance, but
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$\gamma$, there is no single optimal value offering optimal performance, but
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rather a certain interval in which it stays largely unchanged.
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rather a certain interval in which it stays largely unchanged.
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When examining a number of different codes (figure
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When examining a number of different codes (figure
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\ref{fig:prox:results_3d_multiple}), \todo{Move figure to appendix?}
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\ref{fig:prox:results_3d_multiple}), it is apparent that while the exact
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it is apparent that while the exact
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landscape of the graph depends on the code, the general behaviour is the same
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landscape of the graph depends on the code, the general behaviour is the same
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in each case.
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in each case.
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\begin{figure}[H]
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\begin{figure}[h]
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\centering
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\centering
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\begin{tikzpicture}
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\begin{tikzpicture}
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@ -509,7 +508,7 @@ similar values of the two step sizes.
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Again, this consideration applies to a multitude of different codes, as
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Again, this consideration applies to a multitude of different codes, as
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depicted in figure \ref{fig:prox:gamma_omega_multiple}.
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depicted in figure \ref{fig:prox:gamma_omega_multiple}.
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\begin{figure}[H]
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\begin{figure}[h]
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\centering
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\centering
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\begin{tikzpicture}
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\begin{tikzpicture}
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@ -528,7 +527,7 @@ depicted in figure \ref{fig:prox:gamma_omega_multiple}.
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point meta min=-5.7,
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point meta min=-5.7,
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point meta max=-0.5,
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point meta max=-0.5,
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colorbar style={
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colorbar style={
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title={$E_b / N_0$},
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title={\acs{BER}},
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ytick={-5,-4,...,-1},
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ytick={-5,-4,...,-1},
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yticklabels={$10^{-5}$,$10^{-4}$,$10^{-3}$,$10^{-2}$,$10^{-1}$}
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yticklabels={$10^{-5}$,$10^{-4}$,$10^{-3}$,$10^{-2}$,$10^{-1}$}
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}]
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}]
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@ -558,18 +557,60 @@ the average error is inspected.
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This time $\gamma$ and $\omega$ are held constant and the average error is
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This time $\gamma$ and $\omega$ are held constant and the average error is
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observed during each iteration of the decoding process for a number of
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observed during each iteration of the decoding process for a number of
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different \acp{SNR}.
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different \acp{SNR}.
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The plots have been generated by averaging the error over TODO decodings.
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The plots have been generated by averaging the error over $\SI{500000}{}$ decodings.
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As some decodings go one for more iterations than others, the number of values
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As some decodings go one for more iterations than others, the number of values
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which are averaged for each datapoints vary.
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which are averaged for each datapoints vary.
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This explains the bump visible around $k=\text{TODO}$, since after
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This explains the dip visible in all curves around $k=20$, since after
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this point more and more correct decodings converge and stop iterating,
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this point more and more correct decodings stop iterating,
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leaving more and more faulty ones to be averaged.
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leaving more and more faulty ones to be averaged.
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A this point the decline in the average error stagnates, rendering an
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increase in $K$ counterproductive as it only raises the average timing
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requirements of the decoding process.
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The higher the \ac{SNR}, the fewer decodings are present at each iteration
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to average, since a solution is found earlier.
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This explains the decreasing smootheness of the lines as the \ac{SNR} rises.
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Remarkably, the \ac{SNR} seems to not have any impact on the number of
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Remarkably, the \ac{SNR} seems to not have any impact on the number of
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iterations necessary to reach the point at which the average error
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iterations necessary to reach the point at which the average error
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stabilizes.
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stabilizes.
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Furthermore, the improvement in decoding performance stagnates at a particular
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point, rendering an increase in $K$ counterproductive as it only raises the
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\begin{figure}[h]
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average timing requirements of the decoding process.
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\centering
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\begin{tikzpicture}
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\begin{axis}[
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grid=both,
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xlabel={Iterations},
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ylabel={Average $\lVert \boldsymbol{c}-\boldsymbol{\hat{c}} \rVert$},
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legend pos=outer north east,
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width=0.6\textwidth,
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height=0.45\textwidth,
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]
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\addplot [ForestGreen, mark=none, line width=1pt]
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table [col sep=comma, discard if not={omega}{0.0774263682681127}, x=k, y=err]
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{res/proximal/2d_avg_error_20433484_1db.csv};
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\addlegendentry{$E_b / N_0 = \SI{1}{dB}$}
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\addplot [NavyBlue, mark=none, line width=1pt]
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table [col sep=comma, discard if not={omega}{0.0774263682681127}, x=k, y=err]
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{res/proximal/2d_avg_error_20433484_3db.csv};
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\addlegendentry{$E_b / N_0 = \SI{3}{dB}$}
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\addplot [RedOrange, mark=none, line width=1pt]
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table [col sep=comma, discard if not={omega}{0.052233450742668434}, x=k, y=err]
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{res/proximal/2d_avg_error_20433484_5db.csv};
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\addlegendentry{$E_b / N_0 = \SI{5}{dB}$}
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\addplot [RoyalPurple, mark=none, line width=1pt]
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table [col sep=comma, discard if not={omega}{0.052233450742668434}, x=k, y=err]
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{res/proximal/2d_avg_error_20433484_8db.csv};
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\addlegendentry{$E_b / N_0 = \SI{8}{dB}$}
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\end{axis}
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\end{tikzpicture}
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\caption{Average error for $\SI{500000}{}$ decodings\protect\footnotemark{}}
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\end{figure}%
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%
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\footnotetext{(3,6) regular \ac{LDPC} code with n = 204, k = 102
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\cite[\text{204.33.484}]{mackay_enc}; $\gamma=0.05, \omega = 0.05, K=200, \eta=1.5$
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}%
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%
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Changing the parameter $\eta$ does not appear to have a significant effect on
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Changing the parameter $\eta$ does not appear to have a significant effect on
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the decoding performance when keeping the value within a reasonable window
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the decoding performance when keeping the value within a reasonable window
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2001
latex/thesis/res/proximal/2d_avg_error_20433484_1db.csv
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2001
latex/thesis/res/proximal/2d_avg_error_20433484_1db.csv
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@ -0,0 +1,8 @@
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{
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"duration": 397.47346705402015,
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"name": "2d_avg_error_20433484",
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"platform": "Linux-6.1.6-arch1-3-x86_64-with-glibc2.36",
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"SNR": 1,
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"K": 200,
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"end_time": "2023-01-24 23:34:34.589607"
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}
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2001
latex/thesis/res/proximal/2d_avg_error_20433484_3db.csv
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2001
latex/thesis/res/proximal/2d_avg_error_20433484_3db.csv
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{
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"duration": 297.83671288599726,
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"name": "2d_avg_error_20433484",
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"platform": "Linux-6.1.6-arch1-3-x86_64-with-glibc2.36",
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"SNR": 3,
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"K": 200,
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"end_time": "2023-01-24 23:26:41.141614"
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}
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2001
latex/thesis/res/proximal/2d_avg_error_20433484_5db.csv
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2001
latex/thesis/res/proximal/2d_avg_error_20433484_5db.csv
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@ -0,0 +1,8 @@
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{
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"duration": 555.086431461008,
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"name": "2d_avg_error_20433484",
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"platform": "Linux-6.1.6-arch1-3-x86_64-with-glibc2.36",
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"SNR": 5,
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"K": 200,
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"end_time": "2023-01-24 23:17:21.185610"
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}
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2001
latex/thesis/res/proximal/2d_avg_error_20433484_8db.csv
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2001
latex/thesis/res/proximal/2d_avg_error_20433484_8db.csv
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@ -0,0 +1,8 @@
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{
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"duration": 870.158950668003,
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"name": "2d_avg_error_20433484",
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"platform": "Linux-6.1.6-arch1-3-x86_64-with-glibc2.36",
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"SNR": 8,
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"K": 200,
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"end_time": "2023-01-24 23:06:24.712365"
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}
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