Green's function for the Helmholtz equation

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SUMMARY

The discussion focuses on proving that the function $$ G(x,x') = \left\{ \begin{array}{ll} \frac{1}{2ik} e^{i k (x-x')} & x > x' \\ \frac{1}{2ik} e^{-i k (x-x')} & x < x' \end{array} \right. $$ is a Green's function for the 1D Helmholtz equation, defined as $$ \left( \frac{\partial^2}{\partial x^2} + k^2 \right) G(x,x') = \delta(x-x'). $$ The key insight is that a discontinuity in the first derivative of the Green's function leads to the appearance of a Dirac delta function in the second derivative, confirming that the function satisfies the Helmholtz equation.

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DrClaude
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Homework Statement


Show that
$$
G(x,x') = \left\{ \begin{array}{ll} \frac{1}{2ik} e^{i k (x-x')} & x > x' \\ \frac{1}{2ik} e^{-i k (x-x')} & x < x' \end{array} \right.
$$
is a Green's function for the 1D Helmholtz equation, i.e.,
$$
\left( \frac{\partial^2}{\partial x^2} + k^2 \right) G(x,x') = \delta(x-x')
$$

Homework Equations


See above.

The Attempt at a Solution


I am having problems making a Dirac delta appear. I get that the first derivative is discontinuous, but the second derivative is continuous. I don't see any singularity appearing when putting the Green's function into the Helmholtz equation.

Any help appreciated.
 
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DrClaude said:

Homework Statement


Show that
$$
G(x,x') = \left\{ \begin{array}{ll} \frac{1}{2ik} e^{i k (x-x')} & x > x' \\ \frac{1}{2ik} e^{-i k (x-x')} & x < x' \end{array} \right.
$$
is a Green's function for the 1D Helmholtz equation, i.e.,
$$
\left( \frac{\partial^2}{\partial x^2} + k^2 \right) G(x,x') = \delta(x-x')
$$

Homework Equations


See above.

The Attempt at a Solution


I am having problems making a Dirac delta appear. I get that the first derivative is discontinuous, but the second derivative is continuous. I don't see any singularity appearing when putting the Green's function into the Helmholtz equation.

Any help appreciated.

You should show some of your work. But take the example of ##f(x)=|x|##. The first derivative is discontinuous at 0. Away from 0 the second derivative is zero. If you want to integrate the second derivative to get the first derivative you need to put a delta function at 0. A discontinuity in the first derivative means "delta function" in the second.
 
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Dick said:
You should show some of your work.
You are right, I should've have set a better example.

Dick said:
But take the example of ##f(x)=|x|##. The first derivative is discontinuous at 0. Away from 0 the second derivative is zero. If you want to integrate the second derivative to get the first derivative you need to put a delta function at 0. A discontinuity in the first derivative means "delta function" in the second.
I see now that I have
$$
G(x,x') = \frac{1}{2ik} e^{i k |x-x'|}
$$
so
$$
\frac{\partial^2}{\partial x^2} e^{i k |x-x'|} = 2 i k \delta(x-x') - k^2 e^{i k |x-x'|}
$$
and ##G(x,x')## is indeed a Green's function.
 

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