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Localized Displacement Excitations

Whenever two adjacent components of $ \underline{x}_K$ are initialized with equal amplitude, only a single $ W$-variable will be affected. For example, the initial conditions (for time $ n+1$)

\begin{eqnarray*}
y_{n,m-1} &=& 1\\
y_{n-1,m} &=& 1
\end{eqnarray*}

will initialize only $ y^{-}_{n,m-1}$, a solitary left-going pulse of amplitude 1 at time $ n=0$, as can be seen from Eq.$ \,$(P.11) by adding the leftmost columns explicitly written for $ \mathbf{T}^{-1}$. Similarly, the initialization

\begin{eqnarray*}
y_{n-1,m-2} &=& 1\\
y_{n,m-1} &=& 1
\end{eqnarray*}

gives rise to an isolated right-going pulse $ y^{+}_{n,m-1}$, corresponding to the leftmost column of $ \mathbf{T}^{-1}$ plus the first column on the left not explicitly written in Eq.$ \,$(P.11). The superposition of these two examples corresponds to a physical impulsive excitation at time 0 and position $ m-1$:

$\displaystyle y_{n-1,m-2}$ $\displaystyle =$ $\displaystyle 1$  
$\displaystyle y_{n,m-1}$ $\displaystyle =$ $\displaystyle 2$  
$\displaystyle y_{n-1,m}$ $\displaystyle =$ $\displaystyle 1$ (P.12)

Thus, the impulse starts out with amplitude 2 at time 0 and position $ m-1$, and afterwards, impulses of amplitude 1