The Riemann-Lebesgue Lemma is a fundamental result in analysis that describes the behavior of Fourier coefficients of integrable functions. Specifically, it states that if is a Lebesgue-integrable function on the interval , then the Fourier coefficients defined by
tend to zero as approaches infinity. This means that as the frequency of the oscillating function increases, the average value of weighted by these oscillations diminishes.
In essence, the lemma implies that the contributions of high-frequency oscillations to the overall integral diminish, reinforcing the idea that "oscillatory integrals average out" for integrable functions. This result is crucial in Fourier analysis and has implications for signal processing, where it helps in understanding how signals can be represented and approximated.
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