\top -> T
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		@@ -125,8 +125,8 @@ Moreover, we show that their scheme remains unforgeable under the $\SXDH$ assump
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    \setlength{\arraycolsep}{0.3em}\def\arraystretch{1.3}
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    \left(\begin{array}{c|c|c|c}
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    g & \mathbf{1}_{{}_{\ell+1}} & \mathbf{1}_{{}_{\ell+1}} & h \\ \hline
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    \vec{v}^\top & g^{\mathbf{I}_{\ell+1}} & h^{\mathbf{I}_{\ell+1}}
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	  & \mathbf{1}_{{}_{\ell+1}}^\top
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    \vec{v}^T & g^{\mathbf{I}_{\ell+1}} & h^{\mathbf{I}_{\ell+1}}
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	  & \mathbf{1}_{{}_{\ell+1}}^T
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	  \end{array}\right) ,
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  \end{equation}
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  where $\mathbf{1}_{{}_{\ell+1}}=(1_{\GG},\ldots,1_{\GG})\in\GG^{\ell+1}$.
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@@ -403,8 +403,8 @@ If DDH holds in $\GG$, for each $k \in
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    \def\arraystretch{1.5}
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    \begin{array}{c|c}
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      \mathbf{I}_{\ell+1} & a \cdot \mathbf{I}_{\ell + 1}\\ \hline
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      \boldsymbol{0}_{\ell + 1}^{\top} &  ac \cdot( m_1 | \cdots | m_\ell | 1) \\ \hline
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      \boldsymbol{0}_{\ell + 1}^{\top} & a s_1 \cdot( m_1^\star | \cdots | m_\ell^\star | 1)
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      \boldsymbol{0}_{\ell + 1}^{T} &  ac \cdot( m_1 | \cdots | m_\ell | 1) \\ \hline
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      \boldsymbol{0}_{\ell + 1}^{T} & a s_1 \cdot( m_1^\star | \cdots | m_\ell^\star | 1)
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    \end{array}
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    \egroup
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    \right) \cdot
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