I would like to understand under which assumptions the following statement holds \begin{equation} (\lambda,v) \text{ is an eigenpair of the matrix } A \Leftrightarrow (\exp(\lambda\Delta),v) \text{ is an eigenpair of the matrix } \exp(A\Delta) \end{equation} where $\Delta$ is a positive real constant and $A$ is a $\mathbb{R}^{n\times n}$-valued matrix.
$\Rightarrow$ can be proved by induction, see for example Eigenvector and eigenvalue for exponential matrix. I am wondering under which assumption $\Leftarrow$ holds. Indeed, $\log(\exp(A\Delta))$ is not uniquely defined as the matrix $A$.
Example where I got stuck in the proof. To prove $\Leftarrow$, I assume $(\exp(\Delta\lambda),v)$ eigenpair of $\exp(A\Delta)$, therefore $\exp(A\Delta)v=\exp(\Delta\lambda)v$. Considering the definition of the exponential matrix and the taylor expansion of $\exp(\lambda\Delta)$ we get
\begin{equation}
\sum_{k=0}^\infty \frac{\Delta^kA^k}{k!}v=\sum_{k=0}^\infty \frac{\Delta^k\lambda^k}{k!}v
\end{equation}
which is equivalent to
\begin{equation}
\sum_{k=0}^\infty \frac{\Delta^k\left(A^k-\lambda^kI_n\right)v}{k!}=0.
\end{equation}
If I assume by contradiction that $\lambda$ is not an eigenvalue of $A$, how can I prove that the previous series is different from $0$?