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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 modern mathematics ...
, especially
operator theory In mathematics, operator theory is the study of linear operators on function spaces, beginning with differential operators and integral operators. The operators may be presented abstractly by their characteristics, such as bounded linear operat ...
, subnormal operators are
bounded operator In functional analysis and operator theory, a bounded linear operator is a linear transformation L : X \to Y between topological vector spaces (TVSs) X and Y that maps bounded subsets of X to bounded subsets of Y. If X and Y are normed vector s ...
s on a
Hilbert space In mathematics, Hilbert spaces (named after David Hilbert) allow generalizing the methods of linear algebra and calculus from (finite-dimensional) Euclidean vector spaces to spaces that may be infinite-dimensional. Hilbert spaces arise natural ...
defined by weakening the requirements for
normal operator In mathematics, especially functional analysis, a normal operator on a complex Hilbert space ''H'' is a continuous linear operator ''N'' : ''H'' → ''H'' that commutes with its hermitian adjoint ''N*'', that is: ''NN*'' = ''N*N''. Normal operat ...
s. Some examples of subnormal operators are
isometries In mathematics, an isometry (or congruence, or congruent transformation) is a distance-preserving transformation between metric spaces, usually assumed to be bijective. The word isometry is derived from the Ancient Greek: ἴσος ''isos'' mea ...
and
Toeplitz operator In operator theory, a Toeplitz operator is the compression of a multiplication operator on the circle to the Hardy space. Details Let ''S''1 be the circle, with the standard Lebesgue measure, and ''L''2(''S''1) be the Hilbert space of square-inte ...
s with analytic symbols.


Definition

Let ''H'' be a Hilbert space. A bounded operator ''A'' on ''H'' is said to be subnormal if ''A'' has a
normal extension In abstract algebra, a normal extension is an algebraic field extension ''L''/''K'' for which every irreducible polynomial over ''K'' which has a root in ''L'', splits into linear factors in ''L''. These are one of the conditions for algebraic ext ...
. In other words, ''A'' is subnormal if there exists a Hilbert space ''K'' such that ''H'' can be embedded in ''K'' and there exists a normal operator ''N'' of the form :N = \begin A & B\\ 0 & C\end for some bounded operators :B : H^ \rightarrow H, \quad \mbox \quad C : H^ \rightarrow H^.


Normality, quasinormality, and subnormality


Normal operators

Every normal operator is subnormal by definition, but the converse is not true in general. A simple class of examples can be obtained by weakening the properties of
unitary operator In functional analysis, a unitary operator is a surjective bounded operator on a Hilbert space that preserves the inner product. Unitary operators are usually taken as operating ''on'' a Hilbert space, but the same notion serves to define the con ...
s. A unitary operator is an isometry with
dense Density (volumetric mass density or specific mass) is the substance's mass per unit of volume. The symbol most often used for density is ''ρ'' (the lower case Greek letter rho), although the Latin letter ''D'' can also be used. Mathematically ...
range Range may refer to: Geography * Range (geographic), a chain of hills or mountains; a somewhat linear, complex mountainous or hilly area (cordillera, sierra) ** Mountain range, a group of mountains bordered by lowlands * Range, a term used to i ...
. Consider now an isometry ''A'' whose range is not necessarily dense. A concrete example of such is the
unilateral shift In mathematics, and in particular functional analysis, the shift operator also known as translation operator is an operator that takes a function to its translation . In time series analysis, the shift operator is called the lag operator. Shift ...
, which is not normal. But ''A'' is subnormal and this can be shown explicitly. Define an operator ''U'' on :H \oplus H by : U = \begin A & I - AA^* \\ 0 & - A^* \end. Direct calculation shows that ''U'' is unitary, therefore a normal extension of ''A''. The operator ''U'' is called the ''
unitary dilation In operator theory, a dilation of an operator ''T'' on a Hilbert space ''H'' is an operator on a larger Hilbert space ''K'', whose restriction to ''H'' composed with the orthogonal projection onto ''H'' is ''T''. More formally, let ''T'' be a boun ...
'' of the isometry ''A''.


Quasinormal operators

An operator ''A'' is said to be quasinormal if ''A'' commutes with ''A*A''. A normal operator is thus quasinormal; the converse is not true. A counter example is given, as above, by the unilateral shift. Therefore, the family of normal operators is a proper subset of both quasinormal and subnormal operators. A natural question is how are the quasinormal and subnormal operators related. We will show that a quasinormal operator is necessarily subnormal but not vice versa. Thus the normal operators is a proper subfamily of quasinormal operators, which in turn are contained by the subnormal operators. To argue the claim that a quasinormal operator is subnormal, recall the following property of quasinormal operators: Fact: A bounded operator ''A'' is quasinormal if and only if in its
polar decomposition In mathematics, the polar decomposition of a square real or complex matrix A is a factorization of the form A = U P, where U is an orthogonal matrix and P is a positive semi-definite symmetric matrix (U is a unitary matrix and P is a positive semi ...
''A'' = ''UP'', the partial isometry ''U'' and positive operator ''P'' commute. Given a quasinormal ''A'', the idea is to construct dilations for ''U'' and ''P'' in a sufficiently nice way so everything commutes. Suppose for the moment that ''U'' is an isometry. Let ''V'' be the unitary dilation of ''U'', : V = \begin U & I - UU^* \\ 0 & - U^* \end = \begin U & D_ \\ 0 & - U^* \end . Define : Q = \begin P & 0 \\ 0 & P \end. The operator ''N'' = ''VQ'' is clearly an extension of ''A''. We show it is a normal extension via direct calculation. Unitarity of ''V'' means :N^*N = QV^*VQ = Q^2 = \begin P^2 & 0 \\ 0 & P^2 \end. On the other hand, :N N^* = \begin UP^2U^* + D_ P^2 D_ & -D_P^2 U \\ -U^* P^2 D_ & U^* P^2 U \end. Because ''UP = PU'' and ''P'' is self adjoint, we have ''U*P = PU*'' and ''DU*P = DU*P''. Comparing entries then shows ''N'' is normal. This proves quasinormality implies subnormality. For a counter example that shows the converse is not true, consider again the unilateral shift ''A''. The operator ''B'' = ''A'' + ''s'' for some scalar ''s'' remains subnormal. But if ''B'' is quasinormal, a straightforward calculation shows that ''A*A = AA*'', which is a contradiction.


Minimal normal extension


Non-uniqueness of normal extensions

Given a subnormal operator ''A'', its normal extension ''B'' is not unique. For example, let ''A'' be the unilateral shift, on ''l''2(N). One normal extension is the bilateral shift ''B'' on ''l''2(Z) defined by :B (\ldots, a_, , a_1, \ldots) = (\ldots, , a_0, a_1, \ldots), where ˆ denotes the zero-th position. ''B'' can be expressed in terms of the operator matrix : B = \begin A & I - AA^* \\ 0 & A^* \end. Another normal extension is given by the unitary dilation ''B' '' of ''A'' defined above: : B' = \begin A & I - AA^* \\ 0 & - A^* \end whose action is described by : B' (\ldots, a_, a_, , a_1, a_2, \ldots) = (\ldots, - a_, , a_0, a_1, a_2, \ldots).


Minimality

Thus one is interested in the normal extension that is, in some sense, smallest. More precisely, a normal operator ''B'' acting on a Hilbert space ''K'' is said to be a minimal extension of a subnormal ''A'' if '' K' '' ⊂ ''K'' is a reducing subspace of ''B'' and ''H'' ⊂ '' K' '', then ''K' '' = ''K''. (A subspace is a
reducing subspace In linear algebra, a reducing subspace W of a linear map T:V\to V from a Hilbert space V to itself is an invariant subspace of T whose orthogonal complement W^\perp is also an invariant subspace of T. That is, T(W) \subseteq W and T(W^\perp) \subse ...
of ''B'' if it is invariant under both ''B'' and ''B*''.) One can show that if two operators ''B''1 and ''B''2 are minimal extensions on ''K''1 and ''K''2, respectively, then there exists a unitary operator :U: K_1 \rightarrow K_2. Also, the following intertwining relationship holds: :U B_1 = B_2 U. \, This can be shown constructively. Consider the set ''S'' consisting of vectors of the following form: : \sum_^n (B_1^*)^i h_i = h_0+ B_1 ^* h_1 + (B_1^*)^2 h_2 + \cdots + (B_1^*)^n h_n \quad \text \quad h_i \in H. Let ''K' '' ⊂ ''K''1 be the subspace that is the closure of the linear span of ''S''. By definition, ''K' '' is invariant under ''B''1* and contains ''H''. The normality of ''B''1 and the assumption that ''H'' is invariant under ''B''1 imply ''K' '' is invariant under ''B''1. Therefore, ''K' '' = ''K''1. The Hilbert space ''K''2 can be identified in exactly the same way. Now we define the operator ''U'' as follows: : U \sum_^n (B_1^*)^i h_i = \sum_^n (B_2^*)^i h_i Because : \left\langle \sum_^n (B_1^*)^i h_i, \sum_^n (B_1^*)^j h_j\right\rangle = \sum_ \langle h_i, (B_1)^i (B_1^*)^j h_j\rangle = \sum_ \langle (B_2)^j h_i, (B_2)^i h_j\rangle = \left\langle \sum_^n (B_2^*)^i h_i, \sum_^n (B_2^*)^j h_j\right\rangle , , the operator ''U'' is unitary. Direct computation also shows (the assumption that both ''B''1 and ''B''2 are extensions of ''A'' are needed here) :\text g = \sum_^n (B_1^*)^i h_i , :\text U B_1 g = B_2 U g = \sum_^n (B_2^*)^i A h_i. When ''B''1 and ''B''2 are not assumed to be minimal, the same calculation shows that above claim holds verbatim with ''U'' being a
partial isometry In functional analysis a partial isometry is a linear map between Hilbert spaces such that it is an isometry on the orthogonal complement of its kernel. The orthogonal complement of its kernel is called the initial subspace and its range is called ...
.


References

{{DEFAULTSORT:Subnormal Operator Operator theory