Fixed mistake in implementation details; |N_v(i)| -> d_i
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@ -134,8 +134,8 @@ examplary code, which is described by the generator and parity-check matrices%
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and has only two possible codewords:
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%
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\begin{align*}
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\mathcal{C} = \left\{ \begin{bmatrix} 0 & 0 & 0 \end{bmatrix},
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\begin{bmatrix} 0 & 1 & 1 \end{bmatrix} \right\}
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\mathcal{C} = \left\{ \begin{bmatrix} 0 \\ 0 \\ 0 \end{bmatrix},
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\begin{bmatrix} 0 \\ 1 \\ 1 \end{bmatrix} \right\}
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.\end{align*}
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%
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Figure \ref{fig:lp:poly:exact_ilp} shows the domain of exact \ac{ML} decoding.
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@ -631,7 +631,7 @@ The same is true for $\left( \boldsymbol{\lambda}_j \right)_i$.}
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\cite[Sec. III. B.]{original_admm}:%
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%
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\begin{alignat*}{3}
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\tilde{c}_i &\leftarrow \frac{1}{\left| N_v\left( i \right) \right|} \left(
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\tilde{c}_i &\leftarrow \frac{1}{d_i} \left(
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\sum_{j\in N_v\left( i \right) } \Big( \left( \boldsymbol{z}_j \right)_i
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- \frac{1}{\mu} \left( \boldsymbol{\lambda}_j \right)_i \Big)
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- \frac{\gamma_i}{\mu} \right)
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@ -652,7 +652,7 @@ This representation can be slightly simplified by substituting
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$\boldsymbol{\lambda}_j = \mu \cdot \boldsymbol{u}_j \,\forall\,j\in\mathcal{J}$:%
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%
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\begin{alignat*}{3}
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\tilde{c}_i &\leftarrow \frac{1}{\left| N_v\left( i \right) \right|} \left(
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\tilde{c}_i &\leftarrow \frac{1}{d_i} \left(
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\sum_{j\in N_v\left( i \right) } \Big( \left( \boldsymbol{z}_j \right)_i
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- \left( \boldsymbol{u}_j \right)_i \Big)
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- \frac{\gamma_i}{\mu} \right)
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@ -692,7 +692,7 @@ while $\sum_{j\in\mathcal{J}} \lVert \boldsymbol{T}_j\tilde{\boldsymbol{c}} - \b
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- \boldsymbol{z}_j$
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end for
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for $i$ in $\mathcal{I}$ do
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$\tilde{c}_i \leftarrow \frac{1}{\left| N_v\left( i \right) \right|} \left(
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$\tilde{c}_i \leftarrow \frac{1}{d_i} \left(
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\sum_{j\in N_v\left( i \right) } \Big(
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\left( \boldsymbol{z}_j \right)_i - \left( \boldsymbol{u}_j
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\right)_i
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@ -724,7 +724,7 @@ The method chosen here is the one presented in \cite{lautern}.
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\section{Implementation Details}%
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\label{sec:lp:Implementation Details}
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The development process used to implement this decoding algorithm is the same
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The development process used to implement this decoding algorithm was the same
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as outlined in section
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\ref{sec:prox:Implementation Details} for proximal decoding.
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At first, an initial version was implemented in Python, before repeating the
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@ -752,11 +752,10 @@ Using this observation, the sum can be written as%
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- \boldsymbol{u}_j \right) \right)_i
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.\end{align*}
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Further noticing that the vectors
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$\boldsymbol{T}_j^\text{T}\left( \boldsymbol{z}_j - \boldsymbol{u}_j \right),
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\hspace{1mm} j\in\mathcal{J} $
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$\boldsymbol{T}_j^\text{T}\left( \boldsymbol{z}_j - \boldsymbol{u}_j \right)$
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unrelated to \ac{VN} $i$ have $0$ as the $i$th component, the set of indices
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the summation takes place over can be extended to $\mathcal{J}$, allowing the
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expression to be rewritten to%
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expression to be rewritten as%
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%
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\begin{align*}
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\sum_{j\in \mathcal{J}}\left( \boldsymbol{T}_j^\text{T} \left( \boldsymbol{z}_j
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@ -771,12 +770,12 @@ Defining%
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\boldsymbol{D} := \begin{bmatrix}
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d_1 \\
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\vdots \\
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d_m
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d_n
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\end{bmatrix}%
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\hspace{5mm}%
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\text{and}%
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\hspace{5mm}%
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\boldsymbol{M} := \sum_{j\in\mathcal{J}} \boldsymbol{T}_j^\text{T}
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\boldsymbol{s} := \sum_{j\in\mathcal{J}} \boldsymbol{T}_j^\text{T}
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\left( \boldsymbol{z}_j - \boldsymbol{u}_j \right)
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\end{align*}%
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%
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@ -784,7 +783,7 @@ the $\tilde{\boldsymbol{c}}$ update can then be rewritten as%
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%
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\begin{align*}
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\tilde{\boldsymbol{c}} \leftarrow \boldsymbol{D}^{\circ -1} \circ
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\left( \boldsymbol{M} - \frac{1}{\mu}\boldsymbol{\gamma} \right)
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\left( \boldsymbol{s} - \frac{1}{\mu}\boldsymbol{\gamma} \right)
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.\end{align*}
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%
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