Abstract
We have discussed basic contents of the theory of Fourier series on a general Hilbert space. We now proceed to the classical problem concerning the Fourier series expansion of an integrable function with respect to the trigonometric functions. If we choose \(\mathfrak {L}^2([-\pi , \pi ], \mathbb {C})\) as a Hilbert space and
as a complete orthonormal system, the Fourier series of \(f\in \mathfrak {L}^2([-\pi , \pi ],\mathbb {C})\) is given in the form
where
This Fourier series converges to f in \(\mathfrak {L}^2\)-norm.
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Weierstrass-type. Let \(g[a,b]\rightarrow \mathbb {R}\) be integrable and \(h: [a,b]\rightarrow \mathbb {R}\) be bounded and monotone. Then there exists some η ∈ [a, b] such that
$$\displaystyle \begin{aligned} \int_{a}^{b} g(x)h(x)dx = h(a) \int_{a}^{\eta } g(x) dx + h(b) \int_{\eta }^{b} g(x) dx \end{aligned}$$(cf. Stromberg [16] pp. 328–329, Takagi [17] pp. 287–288).
Bonnet-type. Let \(g: [a,b]\rightarrow \mathbb {R}\) be integrable and \(h: [a,b] \rightarrow \mathbb {R}\) be nonnegative and nonincreasing. Then there exists some η ∈ [a, b] such that
$$\displaystyle \begin{aligned} \int_{a}^{b} g(x)h(x)dx = h(a) \int_{a}^{\eta } g(x) dx. \end{aligned}$$If h is nonnegative and nondecreasing, then there exists some η ∈ [a, b] such that
$$\displaystyle \begin{aligned} \int_{a}^{b} g(x) h(x) dx = h(b) \int_{\eta }^{b} g(x) dx \end{aligned}$$ - 4.
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The proof here is due to Kawata [11] p. 85.
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Kolmogorov– Fomin [14] II, pp. 390–391.
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Banach–Steinhaus resonance theorem: Let \(\mathfrak {X}\) be a Banach space, \(\mathfrak {Y}\) a normed space, and {T α|α ∈ A} a family of bounded linear operators of \(\mathfrak {X}\) into \(\mathfrak {Y}\). If {T α x|α ∈ A} is bounded in \(\mathfrak {Y}\) for each \(x\in \mathfrak {X}\), then {T α|α ∈ A} is uniformly bounded, i.e. supα ∈ A∥T α∥ < ∞. (The converse is obvious.) cf. Dunford– Schwartz [2] pp. 52–53, Maruyama [15] pp. 344–345, Yosida [18] p. 69.
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Let u be absolutely continuous and v be integrable on [a, b]. Then u, v is also integrable. Denoting by V the indefinite integral of v, we obtain the formula:
$$\displaystyle \begin{aligned} \int_a^b u(t)v(t)dt=u(b)V(b)-u(a)V(a)-\int_a^b u'(t)V(t)dt. \end{aligned}$$ - 11.
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The proof given here is due to Kolmogorov– Fomin [14], pp. 391–392.
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Maruyama, T. (2018). Convergence of Classical Fourier Series. In: Fourier Analysis of Economic Phenomena. Monographs in Mathematical Economics, vol 2. Springer, Singapore. https://doi.org/10.1007/978-981-13-2730-8_2
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