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1 Algebraic and Analytic MethodsTopics of Discussion

§1.8 Fourier Series

Contents
  1. §1.8(i) Definitions and Elementary Properties
  2. §1.8(ii) Convergence
  3. §1.8(iii) Integration and Differentiation
  4. §1.8(iv) Poisson’s Summation Formula
  5. §1.8(v) Examples

§1.8(i) Definitions and Elementary Properties

Formally, if f(x) is a real- or complex-valued 2\pi-periodic function,

1.8.1 f(x)=\tfrac{1}{2}a_{0}+\sum^{\infty}_{n=1}(a_{n}\cos\left(nx\right)+b_{n}\sin%
\left(nx\right)),

The series (1.8.1) is called the Fourier series of f(x), and a_{n},b_{n} are the Fourier coefficients of f(x).

If f(-x)=f(x), then b_{n}=0 for all n.

If f(-x)=-f(x), then a_{n}=0 for all n.

Alternative Form

1.8.3 f(x)=\sum^{\infty}_{n=-\infty}c_{n}{\mathrm{e}}^{\mathrm{i}nx},

Here c_{n} is related to a_{n} and b_{n} in (1.8.1), (1.8.2) by c_{n}=\frac{1}{2}(a_{n}-\mathrm{i}b_{n}), c_{-n}=\frac{1}{2}(a_{n}+\mathrm{i}b_{n}) for n>0 and c_{0}=\frac{1}{2}a_{0}.

Parseval’s Formula

1.8.5 \frac{1}{\pi}\int^{\pi}_{-\pi}{\left|f(x)\right|}^{2}\,\mathrm{d}x=\tfrac{1}{2%
}{\left|a_{0}\right|}^{2}+\sum^{\infty}_{n=1}({\left|a_{n}\right|}^{2}+{\left|%
b_{n}\right|}^{2}),
1.8.6 \frac{1}{2\pi}\int^{\pi}_{-\pi}{\left|f(x)\right|}^{2}\,\mathrm{d}x=\sum^{%
\infty}_{n=-\infty}{\left|c_{n}\right|}^{2},

where f(x) is square-integrable on [-\pi,\pi] and a_{n},b_{n},c_{n} are given by (1.8.2), (1.8.4). If g(x) is also square-integrable with Fourier coefficients a_{n}^{\prime},b_{n}^{\prime} or c_{n}^{\prime} then

1.8.6_1 \frac{1}{\pi}\int^{\pi}_{-\pi}f(x)\overline{g(x)}\,\mathrm{d}x=\tfrac{1}{2}a_{%
0}\overline{a_{0}^{\prime}}+\sum^{\infty}_{n=1}(a_{n}\overline{a^{\prime}_{n}}%
+b_{n}\overline{b^{\prime}_{n}}),
1.8.6_2 \frac{1}{2\pi}\int^{\pi}_{-\pi}f(x)\overline{g(x)}\,\mathrm{d}x=\sum^{\infty}_%
{n=-\infty}c_{n}\overline{c_{n}^{\prime}}.

Asymptotic Estimates of Coefficients

If f(x) is of period 2\pi, and f^{(m)}(x) is piecewise continuous, then

1.8.7 a_{n},b_{n},c_{n}=o\left(n^{-m}\right),n\to\infty.

Uniqueness of Fourier Series

If f(x) and g(x) are continuous, have the same period and same Fourier coefficients, then f(x)=g(x) for all x.

Lebesgue Constants

1.8.8 L_{n}=\frac{1}{\pi}\int^{\pi}_{0}\frac{\left|\sin\left(n+\frac{1}{2}\right)t%
\right|}{\sin\left(\frac{1}{2}t\right)}\,\mathrm{d}t,n=0,1,\dots.

Riemann–Lebesgue Lemma

For f(x) piecewise continuous on [a,b] and real \lambda,

1.8.10 \int^{b}_{a}f(x){\mathrm{e}}^{\mathrm{i}\lambda x}\,\mathrm{d}x\to 0,as \lambda\to\infty.

(1.8.10) continues to apply if either a or b or both are infinite and/or f(x) has finitely many singularities in (a,b), provided that the integral converges uniformly (§1.5(iv)) at a,b, and the singularities for all sufficiently large \lambda.

§1.8(ii) Convergence

Let f(x) be an absolutely integrable function of period 2\pi, and continuous except at a finite number of points in any bounded interval. Then the series (1.8.1) converges to the sum

1.8.11 \tfrac{1}{2}f(x-)+\tfrac{1}{2}f(x+)

at every point at which f(x) has both a left-hand derivative (that is, (1.4.4) applies when h\to 0-) and a right-hand derivative (that is, (1.4.4) applies when h\to 0+). The convergence is non-uniform, however, at points where f(x-)\neq f(x+); see §6.16(i).

For other tests for convergence see Titchmarsh (1962b, pp. 405–410).

§1.8(iii) Integration and Differentiation

If a_{n} and b_{n} are the Fourier coefficients of a piecewise continuous function f(x) on [0,2\pi], then

If a function f(x)\in C^{2}[0,2\pi] is periodic, with period 2\pi, then the series obtained by differentiating the Fourier series for f(x) term by term converges at every point to f^{\prime}(x).

§1.8(iv) Poisson’s Summation Formula

1.8.13 Moved to (1.8.6_1).

Suppose that f(x) is twice continuously differentiable and f(x) and \left|f^{\prime\prime}(x)\right| are integrable over (-\infty,\infty). Then

It follows from definition (1.14.1) that the integral in (1.8.14) is equal to \sqrt{2\pi}\mathscr{F}\left(f\right)\left(-2\pi n\right).

An alternative formulation is as follows. Suppose that f(x) is continuous and of bounded variation on [0,\infty). Suppose also that f(x) is integrable on [0,\infty) and f(x)\to 0 as x\to\infty. Then

§1.8(v) Examples

For collections of Fourier-series expansions see Prudnikov et al. (1986a, v. 1, pp. 725–740), Gradshteyn and Ryzhik (2015, §§1.44–1.45), and Oberhettinger (1973).