Take the causal solution, extending the input and output by zero before the device starts at . The two zero initial conditions ensure that this extension adds no impulsive terms to the first two distributional derivatives. The Fourier transform of a derivative is multiplication by , so
Factoring the quadratic and taking partial fraction decomposition yields
The inverse Fourier transform follows directly by integrating decaying exponentials:
where is the Heaviside step function. This damped-oscillator impulse response has and , as required for a unit impulse.

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