Continuity, Integration and Fourier Theory pp 137-169 | Cite as
Fourier Series of Summable Functions
Chapter
Abstract
Given f ∈L1(π,µ)the Fourier coefficients (c n : n = 0, ±1, ±2,…) of f were introduced in Definition 8.1 by defining where Δ is any interval of length 2π. To indicate that the Fourier coefficients are those of the function f, the notation c n (f) does sometimes occur. Frequently the notation fˆ(n) instead of cn(f) is also used. The sequence (fˆ(n) : n = 0, ±1, ±2,…) is then denoted by fˆ. For any f ∈ L1(ℝ,µ) there is an analogous notion, although now it is not a sequence of numbers but again a function defined on the whole of ℝ. Precisely formulated, for f ∈ L1(ℝ,µ) the Fourier transform fˆ of f is the function, defined for any x ∈ ℝ by
$${c_n} = {(2\pi )^{ - 1}}\int\limits_\Delta {f(x){e^{ - inx}}} dx,$$
(1)
$${{f}^{{\left( x \right)}}} = \int\limits_{\mathbb{R}} {f(y){{e}^{{ - ixy}}}} dy.$$
(2)
Keywords
Hilbert Space Fourier Series Fourier Coefficient Pointwise Convergence Summable Function
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
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© Springer-Verlag Berlin Heidelberg 1989