Questions tagged [fourier-analysis]

Fourier analysis, also known as spectral analysis, encompasses all sorts of Fourier expansions, including Fourier series, Fourier transform and the discrete Fourier transform (and relatives). The non-commutative analog is (representation-theory).

Fourier analysis is the study of how general functions can be decomposed into trigonometric or exponential functions with definite frequencies. There are two types of Fourier expansions:

  • Fourier series: If a (reasonably well-behaved) function is periodic, then it can be written as a discrete sum of trigonometric or exponential functions with specific frequencies.
  • Fourier transform: A general function that isn’t necessarily periodic (but that is still reasonably well-behaved) can be written as a continuous integral of trigonometric or exponential functions with a continuum of possible frequencies.

The reason why Fourier analysis is so important is that many (although certainly not all) of the differential equations that govern physical systems are linear, which implies that the sum of two solutions is again a solution. Therefore, since Fourier analysis tells us that any function can be written in terms of sinusoidal functions, we can limit our attention to these functions when solving the differential equations. And then we can build up any other function from these special ones. This is a very helpful strategy, because it is invariably easier to deal with sinusoidal functions than general ones.

Fourier series

Consider a function $f(x)$ that is periodic on the interval $0 ≤ x ≤ L$, then Fourier’s theorem states that $f(x)$ can be written as $$f(x)={a_0}+\sum_{n=1}^{\infty}\left[a_n \cos\left(\frac{2n\pi x}{L}\right)+b_n \sin \left(\frac{2n\pi x}{L}\right)\right]$$ where the constant coefficients $a_n$ and $b_n$ are called the Fourier coefficients of $f$ and is given by $$a_0=\frac{1}{L}\int_0^L f(x)\mathrm{d}x$$ $$a_n=\frac{2}{L}\int_0^L f(x)\cos\left(\frac{2\pi nx }{L}\right)\mathrm{d}x$$ $$b_n=\frac{2}{L}\int_0^L f(x)\sin\left(\frac{2\pi nx }{L}\right)\mathrm{d}x$$

Reference:

http://www.people.fas.harvard.edu/~djmorin/waves/Fourier.pdf

https://en.wikipedia.org/wiki/Fourier_analysis

http://mathworld.wolfram.com/FourierSeries.html

Fourier Transform:

For this part find the following link

https://math.stackexchange.com/tags/fourier-transform/info

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Fourier transform of a tempered distribution zero has supported at the origin?

Hello. I am reviewing the book Classical Analysis by Grafakos and I cannot fully understand this proof. Why $\widehat{u}$ is supported at the origin? pd:
eraldcoil
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Logic behind extracting the fourier transform of dirac comb

I have a goal of arriving to the fourier transform of dirac-comb $\omega_T(t)$ so i calculated the fourier series $\omega_T(t) = \frac{1}{T} + \frac{2}{T} \sum_{n=1}^\infty \cos(n \frac{2 \pi}{T} t)$ i think the next step to obtaining the fourier…
HellBoy
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Fourier transform of distributions: exercises

I was doing some exercises but I have some doubts. Here are some of the problems that I'm facing: Compute the F.T. of $\mathcal{F}D^kT$, where $D^k$ is the $k$-th derivative of the distribution $T$. I did the following steps: let $\phi(x)\in…
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Looking for a source: Fourier inversion of $f \in L^1$

Is there a book where I can find a thorough proof of the following assertion? Let $f \in L^1(\mathbb{R}^d)$ be continuous at zero and $\hat{f}\ge0$. Then $\hat{f} \in L^1(\mathbb{R}^d)$ and $$f(t) = \int_{\mathbb{R}^d} \hat{f}(\xi)e^{2\pi i\,…
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A problem with generating the Fourier coefficients and series on a piece-wise function

I have the given function \begin{equation} f(t)=\begin{cases} 2, \ \ \ \ -2\le t<-1 \\ 1, \ \ \ \ -1\le t<0 \\ 2, \ \ \ \ 0\le t<1 \\ 3, \ \ \ \ 1\le t\le2 \end{cases} \end{equation} and I want to generate the…
Luthier415Hz
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$ \int_{-\infty}^{\infty} \frac{|\widehat{\psi}(\omega)|^2}{|\omega|}d\omega = C_{\psi} < \infty \implies \widehat{\psi}(0) = 0$

Let $\psi \in L^2( \mathbb{R})$ and suppose that it satisfies the admissibility condition $$ \int_{-\infty}^{\infty} \frac{|\widehat{\psi}(\omega)|^2}{|\omega|}d\omega = C_{\psi} < \infty $$ where $ \widehat{\psi}$ denotes the fourier transform of…
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Unsure How to Take This Fourier Transform's Inverse?

I have to convolve the following signal and its impulse response, and I thought taking the Fourier Transform would be the best approach: $$x(t) = te^{-2t}*u(t)$$ $$ h(t) = e^{-4t}*u(t)$$ Where $u(t)$ is the unit step/Heaviside function. I know that…
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Fourier Transform of short pulse

I'm trying to take the fourier transform of a short laser pulse, represented by $E(t) = E_oe^{-(t/\Delta T)^2}\times e^{-i \omega t}$ E is the electric field of the laser pulse. $E_o$ and $\Delta T$ are both constants. Specifically I want to know if…
Zar
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Character on product of LCA groups is trivial on almost every factor

Folland's book on Fourier analysis proves a result about products of compact groups, except I have no idea where his proof uses compactness (and not just local compactness). Can someone enlighten me? Here's the result. Assume $G = \prod_i G_i$ is a…
user960774
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Proof of an integral identity involving $\sin(\pi\omega) \sin(\omega x)/\omega$

I have to prove that, $$\int_0^\infty \frac{\sin(\pi\omega)}{\omega}\cdot \sin(\omega x) \,\textrm{d}\omega = \begin{cases}\frac{\pi \sin (\pi x)}{2} & 0 \leq x \leq \pi \\\\ 0 & x \gt \pi \end{cases}$$ What I can see is it is in the form of…
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How to extract specific frequencies in Discrete Fourier Transform.

I'm collecting accelerometer data and interested in extracting frequencies from 1-10 Hz. I'm aware of how to do the FFT but not sure how to extract these frequencies 1Hz, 3Hz and 10Hz. Any pointers?
M-T-A
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A Fourier Coefficients (Series) problem

Let $\alpha$ be a number such that $\alpha/\pi$ is not rational. Prove that (1) $$\lim_{N\to\infty}\sum_{n=1}^{N} e^{ik(x+n\alpha)}=\frac{1}{2\pi}\int_{-\pi}^{\pi} e^{ikt}\,dt,$$ (2) for any continuous function $f:R\to C$ with period…
XLDD
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Are the Fourier sine and cosine transforms injective?

Are the Fourier sine and cosine transforms defined by $$\mathcal{F}_s[f(x)](t)=\int_0^\infty f(x)\sin(x t)\text{d}x$$ and $$\mathcal{F}_c[f(x)](t)=\int_0^\infty f(x)\cos(x t)\text{d}x$$ injective? That is to say, does…
pshmath0
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Time-Restricted Bourgain Spaces

The Bourgain space $X^{s,b}$ is the closure of the set of Schwartz functions $\mathcal S_{t,x}$ under the norm $$\|u\|_{X^{s,b}}:=\|\langle\xi\rangle^s\langle\tau-h(\xi)\rangle^b\hat u(\tau,\xi)\|_{L_{\tau,\xi}^2}$$ for $\{s,b\}\subset\mathbb R$…
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Singular Integrals with Even Kernels

I am reading GTM249 Classical Fourier Analysis, I have a question about the proof of Theorem 5.2.10, which is as follows: Theorem 5.2.10. Let $n \geq 2$ and let $\Omega$ be an even integrable function on $\mathbf{S}^{n-1}$ with mean value zero that…