Green's Functions, Wave Equation

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SUMMARY

The discussion focuses on solving the integral for a driven oscillator without damping, specifically the expression { exp[-iw(t-t')] / (w)^2 - (w_0)^2 } .dw, where w_0 represents the natural frequency. Participants clarify that the poles of the integrand are located in the lower half-plane due to the behavior of the integral when (t - t') < 0, which results in a value of zero. The conversation emphasizes the necessity of considering complex values for w to properly evaluate the integral, particularly when addressing the poles situated at \pm \omega_0 on the real axis.

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  • Understanding of complex analysis, particularly residue theory.
  • Familiarity with integral calculus and contour integration techniques.
  • Knowledge of oscillatory systems and natural frequency concepts.
  • Experience with the wave equation and its mathematical representations.
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Master J
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In solving the driven oscillator without damping, I need to solve the integral

{ exp[-iw(t-t')] / (w)^2 - (w_0)^2 } .dw

where w_0 is the natural frequency.

I know the poles lie in the lower half plane, yet I cannot see why. If (t - t') < 0, the integral is zero. I am not exactly sure how this?
 
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Aren't the poles situated on the real axis at [itex]\pm \omega_0[/itex] ?
 
Isn't it the idea though, that to integrate it, you let w be complex, so that when the real part equals zero, there is still the imaginary part?
 

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