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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Finding a function via convolution

Let $f \in L^1(\mathbb{R})$ be such that $f'$ is continuous and $f' \in L^1(\mathbb{R})$. Find a function $g \in L^1(\mathbb{R})$ such that $$g(t) = \int_{-\infty}^{t} e^{u-t} g(u) du - f'(t), \quad t\in \mathbb{R}$$ We identify the integral as…
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Showing that a function cannot be at once Gabor, smooth, and compactly supported.

From a textbook on Harmonic Analysis: Attempt: Let $g$ be Gabor, smooth, and compactly supported. Then $g$ is Schwartz, and hence $\widehat{g}$ is also Schwartz, and hence Theorem 9.11 is contradicted. Is this correct?
user1770201
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How do I find the fourier series of $\sin^3x$ using $\cos$ and $\sin$?

I want to express $$f(x) = \sin^3x$$ in terms of its fourier series using the fourier series of $sin2x$ and $cos^2 x$ between the interval $[-\pi, \pi]$ for a period of $2\pi$. Respectively here is what I found: $$\sin2x = \sum^{\infty}_1b_n…
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How do I show this fourier series relationship?

I want to show that $$\int^a_0\sin(mx)\sin(nx)\ dx = 0$$ for $m, n$ positive integers and $m\neq n$, and $a = k\pi$, i.e. the integer multiple of $\pi$. I have tried expressing the equation in a fourier series: $$f(x) = \frac{a_0}{2} + \sum^\infty_1…
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Relation between $\ell ^1$ and the $L^1$ space on the circle

Suppose $\hat{f}(n)$ is the fourier coefficient of a function $f$ on the circle. I have seen in class that for $p=2,$ if $\{\hat{f}(n)\}_{n \mathbb{zZ}}$ is in $\ell^p$, then we have f is in the $L^p$ space. I.e. if $\sum|\hat{f}(n)|^2< \infty,$…
usere5225321
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$L^{\infty}(\mathbb{T})$ and $C(\mathbb{T})$ do not admit conjugaison on circle?

I have seen in class that for any homogeneous Banach space B $S_N[f] \rightarrow f$ in norm iff B admits conjugaison, I.e. $\forall f \in B,$ exists a $f^* \in B$ with $S[f^*]=S^*[f]=\sum_{n \in \mathbb{z}} -i sgn(n) \hat{f}(n) e^{int}$ Note…
usere5225321
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convergence of fourier series.

Let $$F_n(x)=\frac{a_0}{2}+\sum_{k=1}^\infty \left(a_n\cos(n\pi x)+b_n\sin(n\pi x)\right),$$ the ourier serie of a $2\pi-$periodic function $f:\mathbb R\longrightarrow \mathbb R$. I have a theorem in my course that says that if $f$ is $\alpha…
MSE
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showing $\hat{f}(n-\tau)= \hat{f}(n) e^{-in \tau}$ for a fixed $\tau \in \mathbb{T}$

Suppose that I have an integrable function $f$ on the circle $\mathbb{T}$ and $f$ is a $2 \pi $ periodic function on the real line. Using the fact that $\hat{f}(n)=\frac{1}{2 \pi} \int_{\mathbb{T}} f(t) e^{-i nt}dt,$ I want to show the following…
abc
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Functions with the same Fourier transform

In $l_1$ space we may define the Fourier transform, but the inverse Fourier transform doesn't always exist. If $f$ and $g$ have the same Fourier transform function, do we necessarily have that $f=g\quad a.e.$? (I think there exists this question in…
pqros
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What are the necessary conditions for a function to be representable as a Fourier Series?

My first question regarding the Fourier Series is: What are the "certain conditions" necessary for a function to be expressible as a Fourier Series? Most treatments I've come across are either very involved, or omit any further discussion of these…
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angular velocity of fourier series

In my textbooks intro to Fourier series, it says that we can represent any periodic function with a combination of the fundamental and harmonics fundamental = $\sin{\omega t}+\cos{\omega t}$ harmonics = $\sin{n \omega t}+\cos{n \omega t}$ so we get…
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Showing a Set is Orthonormal in $\mathbb{C}^N$

1 Context Fix natural $N > 0$ for $\mathbb{C}^N$. Let $$ \omega := e^{2 \pi i / N} $$ for $$ e_n(k) := {1 \over \sqrt{N}} \omega^{kn} \text{ for } k \in \{0,1 \ldots, N-1\} $$ 2 Problem From a book on Harmonic Analysis: 3 Attempt Let $l,j \in…
user1770201
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A question on when Fourier Transform on the circle get vanished.

I am given $f\in L^1 (\mathbb{T})$, and $f(x+\frac{2\pi}{k})=f(x)$ for some natural number $k$. I want to show that $f$'s Fourier transform gets vanished for $n=rk+d$ where $1\leq d
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pointwise convergence and a function f_n

I'm trying to do a task in my Fourier class. I have to check for pointwise convergenge and i can't really understand some terms. I tried reading in the book and around the internet, i might just confuse myself. Anyways i have a function. $ …
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Fourier transformation of positive lobes of cosine

I'm trying to Fourier transform the following function: $$ y(t) = 2\cos(2\pi Bt) \sum_{k=-\infty}^\infty rect(2Bt-2k) $$ It's a normalized cosine with the negative lobes zeroed out. I'm not sure I got the expression right, so here's how I got…