Solution of wave equation I posted this question for the first time on Physics Stack Exchange more than one year ago. The question was closed as off topic. Even if I reworked the question no one considered the possibility ro reopen if. For this reason I decided to poste the question on Math Stack Exchange. Even if my question is related to a physical problem, the difficulty I am facing are related to the math only.
I am dealing with the solution of the wave equation in two different cases represented in figure by Case A and Case B. The two figures were obtained by shining a slab with an incident wave coming from the right (Case A) and from the left (Case B). I verified the solution for Case A. It appears to be correct. Thus I used the same methodology to derive the solution for Case B. However I suspect the solution for Case B is wrong, even if I am not able to understand why.
Independently of the correct/wrong result of the wave equation in case B, I would like to know if there is a way to derive the solution of the wave equation in Case B from that of Case A by applying a kind of symmetry.
The slab is defined between $x=0$ and $x=L$, and a solution for a slab between  $x=-L/2$ and $x=L/2$ is not acceptable.
Please note that $\eta(x)$ does not necessarely any symmetry with respect to  $x$.
This is my solution. Given the wave equation:
\begin{equation}
\frac{d^2y(x)}{dx^2}+k^2 \left(1+\eta(x)\right) y(x)=0
\end{equation}
Its solution can be found by using the Green function method. Details of the method are provided for Case B. When applied to Case A the wave equation has the solution: 
\begin{equation}
y(x)=c_1 e^{-j k x}+c_2 e^{j k x}+\frac{j k}{2} \int_0^Le^{j k |x-t|} \eta(t) y(t) dt
\end{equation}
where $j^2 = -1$ and $c_1$ and $c_2$ are the integration constant. In order to determine the constants we have to consider the boundary conditions. 
When referring to the case A in figure it is possible to distinguis an incident wave and a reflected wave on the right hand side, and a transmitted wave on the left hand side. In this case the following boundatry conditions hold:
\begin{align}
y(L)=1+R_L\\
y'(L)=-jk(2-y(L))\\
y(0)=T_L\\
y'(0)=-jky(0)
\end{align}
By applying these boundary condition while distinguish the two cases $t-x>0$ (left side of the picture) and $t-x<0$ (right side of the picture) it is possibler to find a differential equation in $T_L$. 
Now I would like to repeat the same kind of computation on the second picture (Case B). In this picture the incident wave is coming from the left side, while the transmitted wave is on the right side. In the case A a wave propagating in the same direction of the x axis has a positive exponential term. I have a doubt concerning figure B. In this case a wave travelling in the same direction of the x axis has a dependance on $-x$. Is this correct?
I suppose that it's just a question of conventions. The boundary condition for the case in figure B are of course switched:
\begin{align}
y(0)=1+R_L\\
y'(0)=-jk(2-y(0))\\
y(L)=T_L\\
y'(L)=-jky(L)
\end{align}
Concerning the case A, I first differentiate the general solution:
\begin{equation}
y'(x)=-jk c_1 e^{-jk x}+jk c_2 e^{+jk x}+\frac{j k}{2} \int_0^L\frac{d}{dx}\left(e^{j k |x-t|} \right) \eta(t) y(t) dt
\end{equation}
Now I considered two different cases: when $t-x>0$ (left) and $t-x<0$ (right).
For $t-x>0$ I can write:
\begin{equation}
y'(x)=-jk c_1 e^{-jk x}+jk c_2 e^{+jk x}-jk U(x)
\end{equation}
where
\begin{equation}
U(x)= \frac{j k}{2} \int_0^L\left(e^{-j k (x-t)} \right) \eta(t) y(t) dt
\end{equation}
Then
\begin{equation}
y'(x)=-jk \left( c_1 e^{-jk x}- c_2 e^{+jk x} + U(x) \right)
\end{equation}
While when $t-x<0$ I have:
\begin{equation}
y'(x)=-jk \left( c_1 e^{-jk x}- c_2 e^{+jk x}- K(x) \right)
\end{equation}
where
\begin{equation}
K(x)= \frac{j k}{2} \int_0^L\left(e^{j k (x-t)} \right) \eta(t) y(t) dt
\end{equation}
The boundary conditions in $x=0$ correspond to the case $t-x>0$, while the boundary conditions in $x=L$ correspond to the case $t-x<0$. For $x=0$ we have
\begin{align}
y(0)=c_1+c_2+U(0)\\
y'(0)=-jk(c_1-c_2+U(0))\\
\end{align}
So that $c_2=0$. By repeating the same computation in $x=L$ it is possible to determine that $c_1=e^{jkL}$. Then the solution is:
\begin{equation}
y(x)=e^{j k(L- x)}+\frac{j k}{2} \int_0^Le^{j k |x-t|} \eta(t) y(t) dt
\end{equation}
Now the case in figure B. This is where I'm not sure. According to the picture $e^{-jkx}$ is the forward propagating wave. The Green functions are for $x>L$:
\begin{equation}
\begin{cases}
y_1(x)=C_1 e^{-jkx}\\
y_1(L)=A'
\end{cases}
\end{equation}
While for $x<0$:
\begin{equation}
\begin{cases}
y_2(x)=c_2 e^{jkx}\\
y_2(0)=B'
\end{cases}
\end{equation}
Then
\begin{equation}
\begin{cases}
y_1(L)=c_1 e^{-jkL}=A' & \Rightarrow y_1(x)=A' e^{jk(L-x)}\\
y_2(0)=c_2=B' & \Rightarrow y_2(x)=B' e^{jkx}
\end{cases}
\end{equation}
The Wronskian is
\begin{equation}
W=
\begin{vmatrix}
A' e^{jk(L-x)} & B' e^{jkx}\\
-jk A' e^{jk(L-x)} & jk B' e^{jkx}\\
\end{vmatrix}
=2 jk A'B' e^{jkL}
\end{equation}
So that the Green function is
\begin{equation}
G(x,t)=
\begin{cases}
\frac{A' e^{jk(L-x)} B' e^{jkt}}{2 jk A'B' e^{jkL}}\\
\frac{A' e^{jk(L-t)} B' e^{jkx}}{2 jk A'B' e^{jkL}}\\
\end{cases}
\end{equation}
Which reduces to
\begin{equation}
G(x,t)=\frac{1}{2jk} e^{jk|t-x|}
\end{equation}
So that the solution of the differential equation for the case in figure B is
\begin{equation}
y(x)=c_1 e^{-j k x}+c_2 e^{j k x}+\frac{j k}{2} \int_0^Le^{j k |t-x|} \eta(t) y(t) dt
\end{equation}
 A: Case A and B cannot be directly compared. We have to distinguish the following cases:

*

*Propagation from Left To Right (LTR) when the field propagating in the positive z direction is given by $e^{-jkx}$. This is the Case B.

*Propagation from Left To Right (LTR) when the field propagating in the positive z direction is given by $e^{+jkx}$.

*Propagation from Right To Left (RTL) when the field propagating in the positive z direction is given by $e^{-jkx}$.

*Propagation from Right To Left (RTL) when the field propagating in the positive z direction is given by $e^{+jkx}$. This is the Case A.

As it is possible to see, to be consistent, we can only compare cases (1) and (3) or cases (2) and (4), i.e. we cannot mix the engineering and physic sign conventions. The engineering convention uses a minus sign for forward propagating waves, while the physic convention uses a positive sign. The sign convention has a direct implication on the wave vector ($k=\beta - j \alpha$ while applying the engineering sign convention, and $k=\beta + j \alpha$ while applying the physic sign convention), on the complex permittivity ($\epsilon=\epsilon' - j \epsilon''$ while applying the engineering sign convention, and $\epsilon=\epsilon' + j \epsilon''$ while applying the physic sign convention) as well as on the temporal and spatial Fourier transform.
