From the two main generalizations of the von Neumann entropy:
\begin{equation} S(\rho)=-\operatorname{Tr}(\rho \log \rho) \end{equation}
meaning Rényi:
\begin{equation} R_{\alpha}(\rho)=\frac{1}{1-\alpha} \log \operatorname{Tr}\left(\rho^{\alpha}\right), \alpha \in(0,1) \cup(1, \infty) \end{equation}
and Tsallis:
\begin{equation} T_{q}(\rho)=\frac{1}{1-q}\left(\operatorname{Tr}\left(\rho^{q}\right)-1\right), q \in(0,1) \cup(1, \infty) \end{equation}
we know that in both cases the limit to 1 for the entropic parameters gives us back the von Neumann entropy:
\begin{equation} S(\rho)=\lim _{q \rightarrow 1} T_{q}(\rho)=\lim _{\alpha \rightarrow 1} R_{\alpha}(\rho). \end{equation}
In the case of the quantum Rényi entropy we also know its two limits:
\begin{equation} R_{0}(\rho)=\lim _{\alpha \rightarrow 0} R_{\alpha}(\rho)=\log \operatorname{rank}(\rho) \end{equation}
and
\begin{equation} R_{\infty}(\rho)=\lim _{\alpha \rightarrow \infty} R_{\alpha}(\rho)=-\log \|\rho\|. \end{equation}
I couldn't find anything similar for the quantum Tsallis case? Is there something that is considered trivial?