What we will do is construct a generalization of the real Jordan canonical form. I will mostly omit proofs, since they are simple computations. This will work for any endomorphism $\phi$ over a finite dimensional $\mathbb{K}$-vector space $V$ such that the splitting field of the polynomial characteristic of $\phi$ is of degree $2$.
Let $L$ be said extension of $\mathbb{K}$, i.e. $L = \mathbb{K}(\alpha)$. Every element of $L$ can be written as $z = x + \alpha y$, with $x$ and $y \in \mathbb{K}$. In lack of a better notation, since i do not know if there is one, i will use $\text{Re}(z)$ to mean $x$ and $\text{Im}(z)$ for y, and call them respectively real and imaginary part of $z$, taking inspiration from the real and complex numbers. If you know a better one, or a more used one, please let me know.
We consider now the endomorphism $\phi \otimes Id_L$ of $V \otimes_\mathbb{K} L$, and by abuse of notation denote it by $\phi$ again. In the real case, this corresponds to complexification. The important thing is that the matrix representing $\phi$ and $\phi \otimes Id_L$ are the same, and have the same characteristic polynomial (since the matrices are the same) and the same minimal polynomial (see, for example Minimal polynomial is invariant under field extensions).
We first note that the spectrum of $\phi$ is the union of the eigenvalues belonging to $\mathbb{K}$ and those belonging to $L \setminus \mathbb{K}$. Those belonging to $L \setminus \mathbb{K}$ come in "conjugate" pairs, in the sense that if $\mu = a + \alpha b$ is an eigenvalue, $\bar{\mu} = a - \alpha b$ is another eigenvalue and both have the same algebraic multiplicity. Denoting $V(\lambda)'$ the generalized eigenspace relative to the eigenvalue $\lambda$, we can decompose $V \otimes L$ as $V \otimes L = \bigoplus_{\lambda_j} V(\lambda_j)'$. This is possible since the characteristic polynomial of $\phi$ is split in $L[t]$, so it admits a Jordan canonical form as $L$-matrix. For the eigenvalues belonging to $\mathbb{K}$, all $\ker(\phi - \lambda I)^j$ have the same dimensions both when seeing them as $\mathbb{K}$-vector spaces and as $L$-vector spaces, so we can find a real Jordan basis for $V(\lambda)$. Regarding the eigenvalues in $L \setminus \mathbb{K}$, it can be easily proven that if $\{z_1, \dots, z_k\}$ is a Jordan basis for $V(\lambda)'$, then $\{\bar{z_1}, \dots, \bar{z_k}\}$ is a Jordan basis for $V(\bar{\lambda})'$. Moreover, there is a basis made of elements of $V$ for $ V(\lambda)' \oplus V(\bar{\lambda})'$ by noting that $\text{Re}(z) = \frac{z + \bar{z}}{2}$ and $\text{Im}(z) = \frac{z - \bar{z}}{2 \alpha}$. From this, it is easy to see the real and imaginary parts of the elements of the basis $\{z_1, \dots..., z_k, \bar{z_1}, \dots, \bar{z_k}\}$ form a basis.
We can now find, supposing $\mu \in L \setminus \mathbb{K}$, what is the matrix associated to $\phi$ restricted to $V(\mu)' \oplus V(\bar{\mu})'$ with respect to a real basis of a Jordan basis. I will denote the real parts of $z$ by $x$ and the imaginary ones by $y$, and let $\{z_1, \dots, z_k, \bar{z_1}, \dots, \bar{z_k}\}$ a Jordan basis for $V(\mu)' \oplus V(\bar{\mu})$.
If $z_j$ is such that $\phi (z_j) = \mu z_j$, then $$\phi(x_j) = \phi(\frac{z_j + \bar{z_j}}{2}) = \text{Re}(\mu z_j) = \frac{\mu z_j + \bar{\mu} \bar{z_j}}{2} = \text{Re}(\mu)x_j + \alpha^2 \text{Im}(\mu)y_j$$ and $$\phi (y_j) = \text{Im}(\mu z_j) = \text{Im}(\mu)x_j + \text{Re}(\mu)y_j$$
If, on the other hand, $z_j$ is such that $\phi(z_j) = \mu z_j + z_{j-1}$, we get $$\phi(x_j) = \phi(\frac{z_j + \bar{z_j}}{2}) = \frac{\mu z_j +z_{j-1} + \bar{\mu} \bar{z_j} + \bar{z_{j_1}}}{2} = \text{Re}(\mu)x_j + \alpha^2 \text{Im}(\mu)y_j + x_{j-1}$$ and $$\phi(y_j) = \text{Im}(\mu)x_j + \text{Re}(\mu)y_j + y_{j-1}$$
Then it is immediate to find the matrix representing $\phi$ restricted to $\text{Span} \{x_i, y_i \}$ wrt the basis $\{x_i, y_i \}$:
$$
\begin{bmatrix}
\text{Re}(\mu) & \alpha^2 \text{Im}(\mu) \\
\text{Im}(\mu) & \text{Re}(\mu)
\end{bmatrix}
$$
In our case, the eigenvalue is $\mu = \sqrt{3} = 0 + 1 \sqrt{3}$ so the matrix will be
$$
\begin{bmatrix}
0 & 3 \\
1 & 0
\end{bmatrix}
$$
and the Jordan generalized form is
$$
\begin{bmatrix}
J(2, 2) & 0 & 0 & 0 & 0 \\
0 & J(2, 2) & 0 & 0 & 0 \\
0 & 0 & J(\sqrt{3}, 2) & 0 & 0 \\
0 & 0 & 0 & J(\sqrt{3}, 2) & I_2 \\
0 & 0 & 0 & 0 & J(\sqrt{3}, 2)
\end{bmatrix}
$$
where $J(2, 2)$ is a block of size two corresponding to the eigenvalue 2, and $J(\sqrt{3}, 2)$ is the $2 x 2$ matrix written above and $I_2$ is an identity block of size $2$.
