Fredholm alternative

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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 complex number in the spectrum of a compact operator is an eigenvalue.

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Linear algebra

If is a -dimensional vector space, with finite, and is a linear transformation, then exactly one of the following holds:

  1. For each vector in there is a vector in so that . In other words: is surjective (and so also bijective, since is finite-dimensional).

A more elementary formulation, in terms of matrices, is as follows. Given an matrix and a column vector , exactly one of the following must hold:

  1. Either: has a solution
  2. Or: has a solution with .

In other words, has a solution if and only if for any such that , it follows that .

Integral equations

Let be an integral kernel, and consider the homogeneous equation, the Fredholm integral equation,

and the inhomogeneous equation

The Fredholm alternative is the statement that, for every non-zero fixed complex number either the first equation has a non-trivial solution, or the second equation has a solution for all .

A sufficient condition for this statement to be true is for to be square integrable on the rectangle (where a and/or b may be minus or plus infinity). The integral operator defined by such a K is called a Hilbert–Schmidt integral operator.

Functional analysis

Results about Fredholm operators generalize these results to complete normed vector spaces of infinite dimensions; that is, Banach spaces.

The integral equation can be reformulated in terms of operator notation as follows. Write (somewhat informally) to mean with the Dirac delta function, considered as a distribution, or generalized function, in two variables. Then by convolution, induces a linear operator acting on a Banach space of functions given by with given by

In this language, the Fredholm alternative for integral equations is seen to be analogous to the Fredholm alternative for finite-dimensional linear algebra.

The operator given by convolution with an kernel, as above, is known as a Hilbert–Schmidt integral operator. Such operators are always compact. More generally, the Fredholm alternative is valid when is any compact operator. The Fredholm alternative may be restated in the following form: a nonzero either is an eigenvalue of or lies in the domain of the resolvent

Elliptic partial differential equations

The Fredholm alternative can be applied to solving linear elliptic boundary value problems. The basic result is: if the equation and the appropriate Banach spaces have been set up correctly, then either

(1) The homogeneous equation has a nontrivial solution, or
(2) The inhomogeneous equation can be solved uniquely for each choice of data.

The argument goes as follows. A typical simple-to-understand elliptic operator would be the Laplacian plus some lower order terms. Combined with suitable boundary conditions and expressed on a suitable Banach space (which encodes both the boundary conditions and the desired regularity of the solution), becomes an unbounded operator from to itself, and one attempts to solve

where is some function serving as data for which we want a solution. The Fredholm alternative, together with the theory of elliptic equations, will enable us to organize the solutions of this equation.

A concrete example would be an elliptic boundary-value problem like

supplemented with the boundary condition

where is a bounded open set with smooth boundary and is a fixed coefficient function (a potential, in the case of a Schrödinger operator). The function is the variable data for which we wish to solve the equation. Here one would take to be the space of all square-integrable functions on , and is then the Sobolev space , which amounts to the set of all square-integrable functions on whose weak first and second derivatives exist and are square-integrable, and which satisfy a zero boundary condition on .

If has been selected correctly (as it has in this example), then for the operator is positive, and then employing elliptic estimates, one can prove that is a bijection, and its inverse is a compact, everywhere-defined operator from to , with image equal to . We fix one such , but its value is not important as it is only a tool.

We may then transform the Fredholm alternative, stated above for compact operators, into a statement about the solvability of the boundary-value problem (*)–(**). The Fredholm alternative, as stated above, asserts:

Let us explore the two alternatives as they play out for the boundary-value problem. Suppose . Then either

(A) is an eigenvalue of there is a solution of is an eigenvalue of .

(B) The operator is a bijection is a bijection is a bijection.

Replacing by , and treating the case separately, this yields the following Fredholm alternative for an elliptic boundary-value problem:

The latter function solves the boundary-value problem (*)–(**) introduced above. This is the dichotomy that was claimed in (1)–(2) above. By the spectral theorem for compact operators, one also obtains that the set of for which the solvability fails is a discrete subset of (the eigenvalues of ). The eigenvalues’ associated eigenfunctions can be thought of as "resonances" that block the solvability of the equation.

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