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A 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.
In mathematics, Fredholm theory is a theory of integral equations. In the narrowest sense, Fredholm theory concerns itself with the solution of the Fredholm integral equation. In a broader sense, the abstract structure of Fredholm's theory is given in terms of the spectral theory of Fredholm operators and Fredholm kernels on Hilbert space.
Linear: An integral equation is linear if the unknown function u (x) and its integrals appear linear in the equation. [ 1 ] Hence, an example of a linear equation would be: 1 As a note on naming convention: i) u (x) is called the unknown function, ii) f (x) is called a known function, iii) K (x,t) is a function of two variables and often called ...
Fredholm's theorem. In mathematics, Fredholm's theorems are a set of celebrated results of Ivar Fredholm in the Fredholm theory of integral equations. There are several closely related theorems, which may be stated in terms of integral equations, in terms of linear algebra, or in terms of the Fredholm operator on Banach spaces.
Fredholm alternative. In mathematics, the Fredholm alternative, named after Ivar Fredholm, is one of Fredholm's theorems and is a result in Fredholm theory. It may be expressed in several ways, as a theorem of linear algebra, a theorem of integral equations, or as a theorem on Fredholm operators. Part of the result states that a non-zero ...
In mathematics, Fredholm operators are certain operators that arise in the Fredholm theory of integral equations.They are named in honour of Erik Ivar Fredholm.By definition, a Fredholm operator is a bounded linear operator T : X → Y between two Banach spaces with finite-dimensional kernel and finite-dimensional (algebraic) cokernel = / , and with closed range .
A Green's function, G(x,s), of a linear differential operator L = L(x) acting on distributions over a subset of the Euclidean space , at a point s, is any solution of. (1) where δ is the Dirac delta function. This property of a Green's function can be exploited to solve differential equations of the form.
The Liouville–Neumann series is defined as. which, provided that is small enough so that the series converges, is the unique continuous solution of the Fredholm integral equation of the second kind, {\displaystyle f (x)=\phi (x)-\lambda \int _ {a}^ {b}K (x,s)\phi (s)\,ds.} If the n th iterated kernel is defined as n −1 nested integrals of n ...