Friedrichs extension
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functional analysis Functional analysis is a branch of mathematical analysis, the core of which is formed by the study of vector spaces endowed with some kind of limit-related structure (e.g. Inner product space#Definition, inner product, Norm (mathematics)#Defini ...
, the Friedrichs extension is a
canonical The adjective canonical is applied in many contexts to mean "according to the canon" the standard, rule or primary source that is accepted as authoritative for the body of knowledge or literature in that context. In mathematics, "canonical example ...
self-adjoint In mathematics, and more specifically in abstract algebra, an element ''x'' of a *-algebra is self-adjoint if x^*=x. A self-adjoint element is also Hermitian, though the reverse doesn't necessarily hold. A collection ''C'' of elements of a sta ...
extension of a non-negative densely defined
symmetric operator In mathematics, a self-adjoint operator on an infinite-dimensional complex vector space ''V'' with inner product \langle\cdot,\cdot\rangle (equivalently, a Hermitian operator in the finite-dimensional case) is a linear map ''A'' (from ''V'' to its ...
. It is named after the mathematician
Kurt Friedrichs Kurt Otto Friedrichs (September 28, 1901 – December 31, 1982) was a noted German-American mathematician. He was the co-founder of the Courant Institute at New York University, and a recipient of the National Medal of Science. Biography Friedri ...
. This extension is particularly useful in situations where an operator may fail to be essentially self-adjoint or whose essential self-adjointness is difficult to show. An operator ''T'' is non-negative if : \langle \xi \mid T \xi \rangle \geq 0 \quad \xi \in \operatorname\ T


Examples

Example. Multiplication by a non-negative function on an ''L''2 space is a non-negative self-adjoint operator. Example. Let ''U'' be an open set in R''n''. On ''L''2(''U'') we consider
differential operator In mathematics, a differential operator is an operator defined as a function of the differentiation operator. It is helpful, as a matter of notation first, to consider differentiation as an abstract operation that accepts a function and return ...
s of the form : \phix) = -\sum_ \partial_ \ \quad x \in U, \phi \in \operatorname_c^\infty(U), where the functions ''a''''i j'' are infinitely differentiable real-valued functions on ''U''. We consider ''T'' acting on the dense subspace of infinitely differentiable complex-valued functions of compact support, in symbols : \operatorname_c^\infty(U) \subseteq L^2(U). If for each ''x'' ∈ ''U'' the ''n'' × ''n'' matrix : \begin a_(x) & a_(x) & \cdots & a_(x) \\ a_(x) & a_ (x) & \cdots & a_(x) \\ \vdots & \vdots & \ddots & \vdots \\ a_(x) & a_(x) & \cdots & a_(x) \end is non-negative semi-definite, then ''T'' is a non-negative operator. This means (a) that the matrix is
hermitian {{Short description, none Numerous things are named after the French mathematician Charles Hermite (1822–1901): Hermite * Cubic Hermite spline, a type of third-degree spline * Gauss–Hermite quadrature, an extension of Gaussian quadrature meth ...
and : \sum_ a_(x) c_i \overline \geq 0 for every choice of complex numbers ''c''1, ..., ''c''n. This is proved using
integration by parts In calculus, and more generally in mathematical analysis, integration by parts or partial integration is a process that finds the integral of a product of functions in terms of the integral of the product of their derivative and antiderivative. ...
. These operators are
elliptic In mathematics, an ellipse is a plane curve surrounding two focal points, such that for all points on the curve, the sum of the two distances to the focal points is a constant. It generalizes a circle, which is the special type of ellipse in ...
although in general elliptic operators may not be non-negative. They are however bounded from below.


Definition of Friedrichs extension

The definition of the Friedrichs extension is based on the theory of closed positive forms on Hilbert spaces. If ''T'' is non-negative, then : \operatorname(\xi, \eta) = \langle \xi \mid T \eta \rangle + \langle \xi \mid \eta \rangle is a sesquilinear form on dom ''T'' and : \operatorname(\xi, \xi) = \langle \xi \mid T \xi\rangle + \langle \xi \mid \xi \rangle \geq \, \xi\, ^2. Thus Q defines an inner product on dom ''T''. Let ''H''1 be the completion of dom ''T'' with respect to Q. ''H''1 is an abstractly defined space; for instance its elements can be represented as
equivalence class In mathematics, when the elements of some set S have a notion of equivalence (formalized as an equivalence relation), then one may naturally split the set S into equivalence classes. These equivalence classes are constructed so that elements a ...
es of
Cauchy sequence In mathematics Mathematics is an area of knowledge that includes the topics of numbers, formulas and related structures, shapes and the spaces in which they are contained, and quantities and their changes. These topics are represented in m ...
s of elements of dom ''T''. It is not obvious that all elements in ''H''1 can be identified with elements of ''H''. However, the following can be proved: The canonical inclusion : \operatorname\ T \rightarrow H extends to an ''injective'' continuous map ''H''1 → ''H''. We regard ''H''1 as a subspace of ''H''. Define an operator ''A'' by : \operatorname\ A = \ In the above formula, ''bounded'' is relative to the topology on ''H''1 inherited from ''H''. By the
Riesz representation theorem :''This article describes a theorem concerning the dual of a Hilbert space. For the theorems relating linear functionals to measures, see Riesz–Markov–Kakutani representation theorem.'' The Riesz representation theorem, sometimes called the R ...
applied to the linear functional φξ extended to ''H'', there is a unique ''A'' ξ ∈ ''H'' such that : \operatorname(\xi,\eta) = \langle A \xi \mid \eta \rangle \quad \eta \in H_1 Theorem. ''A'' is a non-negative self-adjoint operator such that ''T''1=''A'' - I extends ''T''. ''T''1 is the Friedrichs extension of ''T''.


Krein's theorem on non-negative self-adjoint extensions

M. G. Krein has given an elegant characterization of all non-negative self-adjoint extensions of a non-negative symmetric operator ''T''. If ''T'', ''S'' are non-negative self-adjoint operators, write : T \leq S if, and only if, * \operatorname(S^) \subseteq \operatorname(T^) * \langle T^ \xi \mid T^ \xi \rangle \leq \langle S^ \xi \mid S^ \xi \rangle \quad \forall \xi \in \operatorname(S^) Theorem. There are unique self-adjoint extensions ''T''min and ''T''max of any non-negative symmetric operator ''T'' such that : T_ \leq T_, and every non-negative self-adjoint extension ''S'' of ''T'' is between ''T''min and ''T''max, i.e. : T_ \leq S \leq T_.


See also

* Energetic extension *
Extensions of symmetric operators In functional analysis, one is interested in extensions of symmetric operators acting on a Hilbert space. Of particular importance is the existence, and sometimes explicit constructions, of self-adjoint extensions. This problem arises, for example ...


Notes

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References

* N. I. Akhiezer and I. M. Glazman, ''Theory of Linear Operators in Hilbert Space'', Pitman, 1981. Operator theory Linear operators