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For two wave equations
\begin{align*} &u_{tt}-c_1^2u_{xx}=0 && \text{as } x>0,\\[3pt] &u_{tt}-c_2^2u_{xx}=0 && \text{as } x<0, \end{align*}
intertwined through boundary conditions \begin{align*} u|_{x=0^+}&=u|_{x=0^-}\\[3pt] u_x|_{x=0^+}&=k u_x|_{x=0^-} \end{align*} with $k>0$.
In this case
with $\psi(t) =-\beta \phi(t)$, $\chi(t)=\alpha \phi(t)$, $\alpha = 2c_2(kc_1+c_2)^{-1}$, $\beta=(kc_1-c_2)(kc_1+c_2)^{-1}$.
Then we have two outgoing waves: reflected wave $\psi (t-c_1^{-1} x)$ and refracted wave $\chi(t+c_2^{-1} x)$.