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Fredholm integral equation : ウィキペディア英語版
Fredholm integral equation
In mathematics, the Fredholm integral equation is an integral equation whose solution gives rise to Fredholm theory, the study of Fredholm kernels and Fredholm operators. The integral equation was studied by Ivar Fredholm.
==Equation of the first kind==

Fredholm Equation is an Integral Equation in which the term containing the Kernel Function (defined below) has constants as integration limits. A closely related form is the Volterra integral equation which has variable integral limits.
An inhomogeneous Fredholm equation of the first kind is written as:
:g(t)=\int_a^b K(t,s)f(s)\,\mathrms
and the problem is, given the continuous kernel function K(t,s) and the function g(t), to find the function f(s).
If the kernel is a function only of the difference of its arguments, namely K(t,s)=K(t-s), and the limits of integration are \pm \infty, then the right hand side of the equation can be rewritten as a convolution of the functions ''K'' and ''f'' and therefore the solution will be given by
:f(t) = \mathcal_\omega^\left(\omega)}
\right]=\int_^\infty _t()(\omega)}e^ \mathrm\omega
where \mathcal_t and \mathcal_\omega^ are the direct and inverse Fourier transforms respectively.

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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