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@ -25,7 +25,7 @@ In particular, the cost of moving to dynamic group is reasonable: while using th
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Signature & $\widetilde{\mathcal{O}}(\lambda)\cdot \log N_\mathsf{gs}$ & $\widetilde{\mathcal{O}}(\lambda + \log^2 N_\mathsf{gs})$ & $\widetilde{\mathcal{O}}(\lambda)\cdot \log N_\mathsf{gs}$ & $\widetilde{\mathcal{O}}(\lambda)\cdot \log N_\mathsf{gs}$ & $ \widetilde{\mathcal{O}}(\lambda)\cdot \log N_\mathsf{gs}$ \\
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\hline
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\end{tabular}
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\caption{Efficiency comparison among recent lattice-based group signatures for static groups and our dynamic scheme. The evaluation is done with respect to $2$ governing parameters: security parameter $\lambda$ and the maximum expected group size $N_\mathsf{gs}$. We do not include the earlier schemes~\cite{GKV10,CNR12} that have signature size $\widetilde{\mathcal{O}}(\lambda^2)\cdot N_\mathsf{gs}$.}
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\caption[Comparison between recent lattice-based group signatures]{Efficiency comparison among recent lattice-based group signatures for static groups and our dynamic scheme. The evaluation is done with respect to $2$ governing parameters: security parameter $\lambda$ and the maximum expected group size $N_\mathsf{gs}$. We do not include the earlier schemes~\cite{GKV10,CNR12} that have signature size $\widetilde{\mathcal{O}}(\lambda^2)\cdot N_\mathsf{gs}$.}
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\label{table:lattice-gs-comparison}
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\end{table}
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@ -81,7 +81,6 @@ the user's capability of efficiently proving knowledge of the underlying secret
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Given the state of $\NIZK$ proofs in the lattice setting, it seems hard to provide group signature schemes in the standard model.
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In the forthcoming sections, we first provide the description of our signature with efficient protocols; then a description of our dynamic group signature will be given and finally, we will explain how to use the Stern abstraction of \cref{sse:stern} to provide the required zero-knowledge arguments.
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\section{A Lattice-Based Signature with Efficient Protocols} \label{se:gs-lwe-sigep}
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