Green's function for 1D modified Helmoltz' equation My equation is $-k^2 \phi + \frac{\partial^2{\phi}}{\partial{z^2}} = -2 \delta(z)$ with $\phi =0 $ on $z=\pm a$
How do I show the Green's function is 
$\phi = \frac{\sinh(k(z+a))}{k\cosh(ka)}$ if $z<0$
and $\;\phi = \frac{\sinh(k(a-z))}{k\cosh(ka)}$ if $z>0$
$-k^2 \phi + \frac{\partial^2{\phi}}{\partial{z^2}} = 0$
Solving this I get $\phi = A\sinh(kz) + B\cosh(kz)$
applying the BCs i get:
for $z<0$, $0= A\sinh(-ka) + B\cosh(-ka)$
and $z>0$, $0= A\sinh(ka) + B\cosh(ka)$ 
but am unsure how to proceed
 A: For $z > 0$, you have $B = - \sinh(ka) / \cosh (ka)$, so
$$ \phi = \frac{A}{\cosh (ka)} \left( \cosh (ka) \sinh (kz) - \sinh(ka) \cosh(kz) \right) = \frac{A}{\cosh(ka)} \sinh(k(z-a)).$$ 
[By the way, if you had written the general solution in the form $\phi = C \sinh(k(z - a)) + D \cosh (k(z - a))$, then it would have been obvious that $D = 0$ from the boundary condition at $z = a$, which would have led you immediately to this expression for $\phi$. Of course, $C = A / \cosh(ka)$.]
Similarly, for $z < 0$, we have
$$ \phi = \frac{A'}{\cosh (ka)}\sinh(k(z + a)).$$
All that remains is to find $A$ and $A'$. You do this by matching the boundary conditions at $z = 0$.
The original equation is
$$ -k^2 \phi + \frac{d^2\phi}{dz^2} = -2\delta(z).$$
If we integrate both sides over an infinitesimally thin interval around $z = 0$, we have
$$ \lim_{z \to 0^+} \frac{d\phi }{dz} - \lim_{z \to 0^-} \frac{d\phi }{dz} = -2$$
So you need to choose $A$ and $A'$ such that $d\phi / dz$ has a discontinuity of $-2$ at $z = 0$ (but such that $\phi$ itself is continuous). In other words, you need
$$ \frac{A}{\cosh (ka)} \times k\cosh(k(0-a)) - \frac{A'}{\cosh(ka)} \times k\cosh(k(0+a)) = -2$$
$$ \frac{A}{\cosh (ka)} \times \sinh(k(0-a)) + \frac{A'}{\cosh(ka)} \times \sinh(k(0+a)) = 0$$
and this is solved by
$$ A = -1, \ \ \ A' = +1.$$
