Can You Establish the Riemann-Lebesgue Theorem?

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SUMMARY

The Riemann-Lebesgue Theorem states that if a function \( f \) is integrable, then the limit of the integral of \( f(x) \cos(nx) \) as \( n \) approaches infinity equals zero. This theorem is crucial in the field of Fourier analysis and has implications for the convergence of Fourier coefficients. The discussion highlights the lack of responses to the problem posed, indicating a gap in engagement or understanding of this fundamental theorem.

PREREQUISITES
  • Understanding of integrable functions in the context of Lebesgue integration
  • Familiarity with Fourier analysis concepts
  • Knowledge of limits and convergence in mathematical analysis
  • Basic proficiency in mathematical notation and terminology
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  • Study the proof of the Riemann-Lebesgue Theorem in detail
  • Explore applications of the Riemann-Lebesgue Theorem in Fourier series
  • Learn about Lebesgue integration and its advantages over Riemann integration
  • Investigate related theorems in harmonic analysis
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Mathematicians, students of analysis, and anyone interested in the applications of the Riemann-Lebesgue Theorem in Fourier analysis and signal processing.

Chris L T521
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Here's this week's problem.

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Problem: Establish the Riemann-Lebesgue Theorem: If $f$ is integrable, then
\[\lim_{n\to\infty}\int_{\mathbb{R}}f(x)\cos nx\,dm = 0.\]

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No one answered this week's question. You can find my solution below.

We will need to use the following fact that I will state without proof (I may add a proof for this statement in the next couple days):

Lemma: Let $f$ be integrable over $\mathbb{R}$, and let $\epsilon>0$. Then there is a step function $\psi$ on $\mathbb{R}$ which vanishes outside a closed, bounded interval and $\displaystyle\int_{\mathbb{R}} |f-\psi|<\epsilon$.

Proof
: Suppose $f$ is integrable on $\mathbb{R}=(-\infty,\infty)$. By the Lemma, given $\epsilon>0$, there is a step function $\psi$ such that $\int_{\mathbb{R}}|f-\psi|< \epsilon/2$. Now,
\[\left|\int_{\mathbb{R}} f(x)\cos nx\,dx\right|\leq \int_{\mathbb{R}} |(f(x)-\psi(x))\cos nx|\,dx + \int_{\mathbb{R}} |\psi(x)\cos nx|\,dx<\epsilon/2 + \int_{\mathbb{R}} |\psi(x)\cos nx|\,dx.\]
Integrating $|\psi(x)\cos nx|$ over each interval on which $\psi$ is constant, we see that $\int_{\mathbb{R}} |\psi(x)\cos nx|\,dx \rightarrow 0$ as $n\to\infty$. Thus, there exists $N$ such that $\int_{\mathbb{R}}|\psi(x)\cos nx|\,dx<\epsilon/2$ for $n\geq N$ so $\left|\int_{\mathbb{R}} f(x)\cos nx\,dx\right|<\epsilon$ for $n\geq N$, i.e.
\[\lim_{n\to\infty}\int_{\mathbb{R}} f(x)\cos nx \,dx = 0.\]
 

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