If one would solve this problem for example with PMP then you would get the following state and co-state dynamics
$$
\begin{bmatrix}
\dot{x} \\ \dot{\lambda}
\end{bmatrix} = \underbrace{
\begin{bmatrix}
A & -\frac{1}{2\,\rho}B\,B^\top \\
-2\,I & -A^\top
\end{bmatrix}}_\hat{A}
\begin{bmatrix}
x \\ \lambda
\end{bmatrix} + \underbrace{
\begin{bmatrix}
0 \\ 2\,I
\end{bmatrix}}_\hat{B} x_T
$$
In general those dynamics have to the following solution in time
$$
\begin{bmatrix}
x(t) \\ \lambda(t)
\end{bmatrix} = e^{\hat{A}\,t}
\begin{bmatrix}
x(0) \\ \lambda(0)
\end{bmatrix} + \int_0^t e^{\hat{A}(t - \tau)}d\tau\,\hat{B}\,x_T.
$$
By defining the following submatrices
$$
e^{\hat{A}\,T} =
\begin{bmatrix}
X_{11} & X_{12} \\ X_{21} & X_{22}
\end{bmatrix}, \quad
\int_0^T e^{\hat{A}(T - \tau)}d\tau\,\hat{B} =
\begin{bmatrix}
Y_1 \\ Y_2
\end{bmatrix}
$$
then it is possible obtain the following expression
$$
x(T) = X_{11}\,x(0) + X_{12}\,\lambda(0) + Y_1\,x_T
$$
since $x(T)=x_T$ and $x(0)=x_0$, then this can be used to solve for $\lambda(0)$
$$
\lambda(0) = X_{12}^{-1} ((I - Y_1)\,x_T - X_{11}\,x_0) =
\begin{bmatrix}
-X_{12}^{-1}\,X_{11} & X_{12}^{-1} (I - Y_1)
\end{bmatrix}
\begin{bmatrix}
x_0 \\ x_T
\end{bmatrix}.
$$
Combining this with the expression for the state as a function of time yields
$$
\begin{bmatrix}
x(t) \\ \lambda(t)
\end{bmatrix} = e^{\hat{A}\,t}
\begin{bmatrix}
I & 0 \\
-X_{12}^{-1}\,X_{11} & X_{12}^{-1} (I - Y_1)
\end{bmatrix}
\begin{bmatrix}
x_0 \\ x_T
\end{bmatrix} + \int_0^t e^{\hat{A}(t - \tau)}d\tau\,\hat{B}\,x_T
$$
so from this it can be concluded that the solution of the state $x$ as a function of time should be linear in $x_0$ and $x_T$
$$
x(t) = \Phi(t)
\begin{bmatrix}
x_0 \\ x_T
\end{bmatrix}
$$
where $\Phi(t)$ is a function of time, independently of $x$. But the solution for $\Phi(t)$ might change if a difference $A$, $B$, $\rho$ or $T$ would be used. If $x\in\mathbb{R}^n$ then $\Phi(t)\in\mathbb{R}^{n\times2\,n}$.
I have only quickly skimmed through the paper you linked to, but I am not sure why that author states there are only 56 "transitions" (which should correspond to the columns of $\Phi(t)$), while the state space dimension is of size 129. Since in the general case I would actually expect twice as many transitions as states, so 258. But maybe the author put constraints on the allowed $x_0$ and $x_T$ which reduces the span of $\Phi(t)$.