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Sinc filter : ウィキペディア英語版
Sinc filter

In signal processing, a sinc filter is an idealized filter that removes all frequency components above a given cutoff frequency, without affecting lower frequencies, and has linear phase response. The filter's impulse response is a sinc function in the time domain, and its frequency response is a rectangular function.
It is an "ideal" low-pass filter in the frequency sense, perfectly passing low frequencies, perfectly cutting high frequencies; and thus may be considered to be a ''brick-wall filter''.
Real-time filters can only approximate this ideal, since an ideal sinc filter (aka ''rectangular filter'') is non-causal and has an infinite delay, but it is commonly found in conceptual demonstrations or proofs, such as the sampling theorem and the Whittaker–Shannon interpolation formula.
In mathematical terms, the desired frequency response is the rectangular function:
:H(f) = \mathrm \left( \frac \right)
where B\, is an arbitrary cutoff frequency (aka ''bandwidth''). The impulse response of such a filter is given by the inverse Fourier transform of the frequency response:
:
\begin
h(t) = \mathcal^ \ & = 2B \frac \\
& = 2B \, \mathrm(2 B t)
\end

the normalized sinc function.
As the sinc filter has infinite impulse response in both positive and negative time directions, it must be approximated for real-world (non-abstract) applications; a windowed sinc filter is often used instead. Windowing and truncating a sinc filter kernel in order to use it on any practical real world data set reduces its ideal properties.
==Brick-wall filters==
An idealized electronic filter, one that has full transmission in the pass band, and complete attenuation in the stop band, with abrupt transitions, is known colloquially as a "brick-wall filter", in reference to the shape of the transfer function. The sinc filter is a brick-wall low-pass filter, from which brick-wall band-pass filters and high-pass filters are easily constructed.
The lowpass filter with brick-wall cutoff at frequency ''B''''L'' has impulse response and transfer function given by:
: h_(t) = 2B_L \, \mathrm\left(2B_L t\right)
: H_(f) = \mathrm\left( \frac \right).
The band-pass filter with lower band edge ''B''''L'' and upper band edge ''B''''H'' is just the difference of two such sinc filters (since the filters are zero phase, their magnitude responses subtract directly):
: h_(t) = 2B_H \, \mathrm\left(2B_H t\right) - 2B_L \, \mathrm\left(2B_L t\right)
: H_(f) = \mathrm\left( \frac \right) - \mathrm\left( \frac \right).
The high-pass filter with lower band edge ''B''''H'' is just a transparent filter minus a sinc filter, which makes it clear that the Dirac delta function is the limit of a narrow-in-time sinc filter:
: h_(t) = \delta(t) - 2B_H \, \mathrm\left(2B_H t\right)
: H_(f) = 1 - \mathrm\left( \frac \right).
Brick-wall filters that run in realtime are not physically realizable as they have infinite latency (i.e., its compact support in the frequency domain forces its time response not to have compact support meaning that it is ever-lasting) and infinite order (i.e., the response cannot be expressed as a linear differential equation with a finite sum), but approximate implementations are sometimes used and they are frequently called brick-wall filters.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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