I assume [itex]A[/itex] is a linear operator or a matrix, that the space of operators has a norm, and there are convergence properties that justify my rearrangements (below) of infinites series. In physics, we typically pretend that everything is okay and proceed formally.
From [itex]A^2 = 1[/itex], [itex]A^n = 1[/itex] if [itex]n[/itex] is even, and [itex]A^n = A[/itex] if [itex]n[/itex] is odd.
[tex]
\begin{equation*}<br />
\begin{split}<br />
\exp{ixA} &= 1 + ixA + \frac{1}{2!}\left(ixA\right)^2 + \frac{1}{3!}\left(ixA\right)^3 ...\\<br />
&= \left(1 - \frac{1}{2!} x^2A^2 + ...\right) + \left(ixA - \frac{1}{3!}ix^3A^3 + ...\right)\\<br />
&= \left(1 - \frac{1}{2!}x^2 + ... \right) + i\left(x - \frac{1}{3!}x^3 + ... \right)A<br />
\end{split}<br />
\end{equation*}[/tex]