Calling
$$
M = \left(
\begin{array}{cc}
A & B \\
B & C \\
\end{array}
\right)
$$
we have
$$
\left(
\begin{array}{c}
\partial t \\
\partial x \\
\end{array}
\right)^{\dagger}M\left(
\begin{array}{c}
\partial t \\
\partial x \\
\end{array}
\right)u=0
$$
or
$$
\left(
\begin{array}{c}
\partial t \\
\partial x \\
\end{array}
\right)^{\dagger}T^{-1}\Lambda T\left(
\begin{array}{c}
\partial t \\
\partial x \\
\end{array}
\right)u=0
$$
with
$$
T = \left(
\begin{array}{cc}
\frac{A-C-\sqrt{4 B^2+(A-C)^2}}{2 B} & 1 \\
\frac{A-C+\sqrt{4 B^2+(A-C)^2}}{2 B} & 1 \\
\end{array}
\right)\\
\Lambda=\left(
\begin{array}{cc}
\frac{1}{2} \left(A+C-\sqrt{4 B^2+(A-C)^2}\right) & 0 \\
0 & \frac{1}{2} \left(A+C+\sqrt{4 B^2+(A-C)^2}\right) \\
\end{array}
\right) = \left(
\begin{array}{cc}
\lambda_1 & 0 \\
0 & \lambda_2 \\
\end{array}
\right)
$$
and now calling
$$
\left(
\begin{array}{c}
\partial \eta \\
\partial \xi \\
\end{array}
\right) = T\left(
\begin{array}{c}
\partial t \\
\partial x \\
\end{array}
\right)
$$
the PDE reduces to
$$
\lambda_1 u_{\eta\eta}+\lambda_2 u_{\xi\xi}=0
$$
and also we can verify by substitution that
$$
u(\eta,\xi) = f(\eta)+g(\xi)
$$
is a solution, or changing variables again
$$
u(t,x) = f\left(\frac{\lambda_1}{B} t + x\right) + g\left(\frac{\lambda_2}{B} t+x\right)
$$