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Homework Statement
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Suppose we have a [itex]2\pi[/itex]-periodic, integrable function [itex]f: \mathbb{R} \rightarrow \mathbb{C}[/itex] whose Fourier coefficients are known. Parseval's theorem tells us that:
[tex]\sum_{n = -\infty}^{\infty}|\widehat{f(n)}|^2 = \frac{1}{2\pi}\int_{-\pi}^{\pi}|f(x)|^{2}dx,[/tex]
where [itex]\widehat{f(n)}[/itex] are the Fourier coefficients of [itex]f[/itex].
Suppose we instead want to replace [itex]f(x)[/itex] with [itex]f(x)^{q},[/itex] say: then it would suffice to determine the Fourier coefficients of the [itex]q[/itex]-th power of [itex]f[/itex]. Is repeated application of the convolution theorem the usual way of finding powers of the Fourier coefficients of functions, where the Fourier coefficients of the original function are already known?
Homework Equations
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[itex]f \ast g[/itex] denotes the convolution of [itex]f[/itex] and [itex]g[/itex], given by [itex](f \ast g)(t) := \int_{-\infty}^{\infty} f(\tau)g(t - \tau)d\tau,[/itex] and [itex]\widehat{f \ast g} = \hat{f} \cdot \hat{g}[/itex] is the convolution theorem for the Fourier transforms of [itex]f[/itex] and [itex]g[/itex].
The Attempt at a Solution
Suppose that we are interested in [itex]\int_{-\pi}^{\pi}|f(x)|^{4} dx[/itex]. I would like to know if it is valid to say the following:
[tex]\frac{1}{2\pi}\int_{-\pi}^{\pi}|f(x)|^{4}dx = \frac{1}{2\pi}\int_{-\pi}^{\pi}|(f(x))^{2}|^{2}dx = \sum_{n = -\infty}^{\infty} |\widehat{f(n)^{2}}|^{2} = \sum_{n = -\infty}^{\infty} | (\hat{f} \ast \hat{f})(n)|^{2}.[/tex]
The reason I am interested in this is because I'm working on bounding a class of [itex]L^{p}[/itex]-norms using the asymptotics of Fourier coefficients, and hoping to modify this slightly to integrate functions over a [itex]d[/itex]-cube [itex][0,2\pi)^d[/itex]. This seems to be a complicated procedure however, since additional conditions need to be imposed on the functions to guarantee the convergence of the integral in [itex]\mathbb{R}^d[/itex].
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