In a thesis, [1] I found the following statement:
To determine [characteristic impedance and] dispersion relationships for an arbitrary reciprocal network having the transmission matrix
$$ \begin{bmatrix} A & B \\ C & D \end{bmatrix}, $$
one sets the determinant of
$$ \begin{bmatrix} A-e^{-\gamma d} & B \\ C & D-e^{-\gamma d} \end{bmatrix} $$
to zero where gamma is the complex propagation constant and d is the physical length of the whole network.
I can calculate this, and use it to verify the propagation constant of an element of an artifical transmission line, for example.
But can someone give a compelling, concise explanation why do we subtract $$\mathbf{I} e^{-\gamma d}$$ from the ABCD matrix and set the determinant to zero? What is it about the determinant that gives us the propagation constant? What is the intuition.
(I definitely see a similarity to determining eigenvalues via the characteristic polynomial, for example, but I don't see how this plays here)
[1] Michael Garth Case, Nonlinear Transmission Lines for Picosecond Pulse, Impulse and Millimeter-Wave Harmonic Generation