Fredholm solvability

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In mathematics, Fredholm solvability encompasses results and techniques for solving differential and integral equations via the Fredholm alternative and, more generally, the Fredholm-type properties of the operator involved. The concept is named after Erik Ivar Fredholm.

Let Template:Math be a real Template:Math-matrix and bn a vector.

The Fredholm alternative in n states that the equation Ax=b has a solution if and only if bTv=0 for every vector vn satisfying ATv=0. This alternative has many applications, for example, in bifurcation theory. It can be generalized to abstract spaces. So, let E and F be Banach spaces and let T:EF be a continuous linear operator. Let E*, respectively F*, denote the topological dual of E, respectively F, and let T* denote the adjoint of T (cf. also Duality; Adjoint operator). Define

(kerT*)={yF:(y,y*)=0 for every y*kerT*}

An equation Tx=y is said to be normally solvable (in the sense of F. Hausdorff) if it has a solution whenever y(kerT*). A classical result states that Tx=y is normally solvable if and only if T(E) is closed in F.

In non-linear analysis, this latter result is used as definition of normal solvability for non-linear operators.

References

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  • F. Hausdorff, "Zur Theorie der linearen metrischen Räume" Journal für die Reine und Angewandte Mathematik, 167 (1932) pp. 265 [1] [2]
  • V. A. Kozlov, V.G. Maz'ya, J. Rossmann, "Elliptic boundary value problems in domains with point singularities", Amer. Math. Soc. (1997) [3] [4]
  • A. T. Prilepko, D.G. Orlovsky, I.A. Vasin, "Methods for solving inverse problems in mathematical physics", M. Dekker (2000) [5][6]
  • D. G. Orlovskij, "The Fredholm solvability of inverse problems for abstract differential equations" A.N. Tikhonov (ed.) et al. (ed.), Ill-Posed Problems in the Natural Sciences, VSP (1992) [7]