MHB Pole shifting for Fourier transform

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The discussion centers on the mathematical concept of pole shifting in the context of a Green function for simple harmonic oscillation. The user has derived the Fourier transform of the Green function, which reveals poles at $\omega=\pm\omega_{0}$. They seek guidance on how to mathematically shift these poles, specifically in the form $\omega_{0} \rightarrow \omega_{0} + i\epsilon$. A response indicates that there are numerous methods for relocating poles, prompting the user to explore these techniques further. The conversation emphasizes the importance of understanding pole shifting in relation to system behavior in physics.
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Hi, I have a simple harmonic oscillation problem whose Green function is given by

$$\Bigl[\frac {d^2}{dt^2}+ \omega_{0}^{2}\Bigl] G(t, t') = \delta(t-t')$$

Now I found out the Fourier transform of $G(t, t')$ to be $$G(\omega)= \frac{1}{2\pi} \frac{1}{\omega_{0}^{2}-\omega^2}$$ which has poles at $\omega=\pm\omega_{0}$

now how can i identify the way the poles can be shifted , like shifting $\omega_{0}\rightarrow \omega_{0}+ i\epsilon$
my instructor said there are four ways to shift. can you please guide me mathematically to pole shifting ?

also suggest me the reading materials to know about these shifting .
regards
 
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There are far more than 4 ways to have your system's poles be relocated to some desired location. In any case, did you happen to find out what these particular ways are?
 
Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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