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2018-06-15 16:04:10 +02:00
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@ -25,7 +25,7 @@ In particular, the cost of moving to dynamic group is reasonable: while using th
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}$ \\
\hline
\end{tabular}
\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 $\widetilde{\mathcal{O}}(\lambda^2)\cdot N_\mathsf{gs}$.}
\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 $\widetilde{\mathcal{O}}(\lambda^2)\cdot N_\mathsf{gs}$.}
\label{table:lattice-gs-comparison}
\end{table}
@ -81,7 +81,6 @@ the user's capability of efficiently proving knowledge of the underlying secret
Given the state of $\NIZK$ proofs in the lattice setting, it seems hard to provide group signature schemes in the standard model.
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.
\section{A Lattice-Based Signature with Efficient Protocols} \label{se:gs-lwe-sigep}