complexification of $SO(2)$ While computing the complexification of Lie group $SO(2)$, I get the result is all the matrix of the following form 
$$\left(\begin{array}{cc}
\frac{e^{t-\sqrt{-1}\theta}+e^{-t+\sqrt{-1}\theta}}{2} & \frac{e^{-t+\sqrt{-1}\theta}-e^{t-\sqrt{-1}\theta}}{2\sqrt{-1}} \\
-\frac{e^{-t+\sqrt{-1}\theta}-e^{t-\sqrt{-1}\theta}}{2\sqrt{-1}}& \frac{e^{t-\sqrt{-1}\theta}+e^{-t+\sqrt{-1}\theta}}{2} \\
\end{array}
\right),$$
for $t$ and $\theta$ are both real numbers. I want to know what are this matrices like, or there is another description. Specially $SO(2)$ can act on $\mathbb{C}$ as a rotation? How could its complexification acts on $\mathbb{C}$ naturally?

I struggled with this for a while so I just wanted to complement Dietrich's answer with a way of coming up with this isomorphism.
The way that I found natural is to note that the vector representation of $SO(2,\mathbb{C})$ on $\mathbb{C}^2$ is not irreducible. In fact, following the technique suggested in Decompose the representation $V$ of $SO_2$ into irreducible representations, one sees that it splits into a direct sum of 1-dimensional irreducible representations $\mathbb{C}^2=V_+\oplus V_-$. On $V_{\pm}=\text{span}_\mathbb{C}\{(1,\mp i)\}$ an element of the form $e^{aJ}\in SO(2,\mathbb{C})$, with
$$J=\begin{pmatrix}0 & -1\\1 & 0\end{pmatrix},$$
acts like $t^{\pm1}=e^{\pm ia}=\cos(a)+i\sin(a)\in\mathbb{C}^\times$. Moreover,
$$e^{aJ}=\begin{pmatrix}\cos(a) & -\sin(a)\\ \sin(a) & \cos(a)\end{pmatrix}=\begin{pmatrix}\frac{t+t^{-1}}{2} & -\frac{t-t^{-1}}{2i}\\\frac{t+t^{-1}}{2i} & \frac{t+t^{-1}}{2} \end{pmatrix}$$
