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A Fourier series is a representation of a function in terms of a summation of an infinite number of harmonically-related sinusoids with different amplitudes and phases. The amplitude and phase of a sinusoid can be combined into a single complex number, called a Fourier ''coefficient''. The Fourier series is a periodic function. So it cannot represent any arbitrary function. It can represent either: :(a) a periodic function, or :(b) a function that is defined only over a finite-length interval; the values produced by the Fourier series outside the finite interval are irrelevant. When the function being represented, whether finite-length or periodic, is discrete, the Fourier series coefficients are periodic, and can therefore be described by a finite set of complex numbers. That set is called a discrete Fourier transform (DFT), which is subsequently an overloaded term, because we don't know whether its (periodic) inverse transform is valid over a finite or an infinite interval. The term discrete Fourier series (DFS) is intended for use instead of ''DFT'' when the original function is periodic, defined over an infinite interval. ''DFT'' would then unambiguously imply only a transform whose inverse is valid over a finite interval. But we must again note that a Fourier series is a time-domain representation, not a frequency domain transform. So DFS is a potentially confusing substitute for DFT. A more technically valid description would be DFS coefficients. ==See also== *Fourier series *Fast Fourier transform *Laplace transform *Discrete Fourier transform * *DFT matrix *Discrete-time Fourier transform *Fractional Fourier transform *Linear canonical transform *Fourier sine transform *Short-time Fourier transform *Analog signal processing *Transform (mathematics) 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Discrete Fourier series」の詳細全文を読む スポンサード リンク
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