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EQUATION OF THE FIRST KIND An Inhomogeneous Fredholm equation of the first kind is written as: : 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 , and the limits of integration are , 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 : where and are the direct and inverse Fourier transforms respectively. EQUATION OF THE SECOND KIND An inhomogeneous Fredholm equation of the second kind is given as : Given the kernel ''K(t,s)'', and the function , the problem is typically to find the function . A standard approach to solving this is to use the Resolvent Formalism ; written as a series, the solution is known as the Liouville-Neumann Series . GENERAL THEORY The general theory underlying the Fredholm equations is known as Fredholm Theory . One of the principal results is that the kernel ''K'' is a Compact Operator , known as the Fredholm Operator . Compactness may be shown by invoking Equicontinuity . As an operator, it has a Spectral Theory that can be understood in terms of a discrete spectrum of Eigenvalue s that tend to 0. SEE ALSO REFERENCES
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