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In [[operator theory]], '''quasinormal operators''' is a class of [[bounded operator]]s defined by weakening the requirements of a [[normal operator]].
 
Every quasinormal operator is a [[subnormal operator]]. Every quasinormal operator on a finite-dimensional [[Hilbert space]] is normal.
 
== Definition and some properties ==
=== Definition ===
Let ''A'' be a bounded operator on a Hilbert space ''H'', then ''A'' is said to be '''quasinormal''' if ''A'' commutes with ''A*A'', i.e.
 
:<math>A(A^*A) = (A^*A) A.\,</math>
 
=== Properties ===
 
A normal operator is necessarily quasinormal.
 
Let ''A'' = ''UP'' be the [[polar decomposition]] of ''A''. If ''A'' is quasinormal, then ''UP = PU''. To see this, notice that
the positive factor ''P'' in the polar decomposition is of the form (''A*A'')<sup>&frac12;</sup>, the unique positive square root of ''A*A''. Quasinormality means ''A'' commutes with ''A*A''. As a consequence of the [[continuous functional calculus]] for [[self adjoint operator]]s, ''A'' commutes with ''P'' = (''A*A'')<sup>&frac12;</sup> also, i.e.
 
:<math>U P P = P U P.\,</math>
 
So ''UP = PU'' on the range of ''P''. On the other hand, if ''h'' &isin; ''H'' lies in kernel of ''P'', clearly ''UP h''  = 0. But ''PU h'' = 0 as well. because ''U'' is a [[partial isometry]] whose initial space is closure of range ''P''. Finally, the self-adjointness of ''P'' implies that ''H'' is the direct sum of its range and kernel. Thus the argument given proves ''UP'' = ''PU'' on all of ''H''.
 
On the other hand, one can readily verify that if ''UP'' = ''PU'', then ''A'' must be quasinormal. Thus the operator ''A'' is quasinormal if and only if ''UP'' = ''PU''.
 
When ''H'' is finite dimensional, every quasinormal operator ''A'' is normal. This is because that in the finite dimensional case, the partial isometry ''U'' in the polar decomposition ''A'' = ''UP'' can be taken to be unitary. This then gives
 
:<math>A^*A = (UP)^* UP =  PU (PU)^* = AA^*.\,</math>
 
In general, a partial isometry may not be extendable to a unitary operator and therefore a quasinormal operator need not be normal. For example, consider the [[unilateral shift]] ''T''. ''T'' is quasinormal because ''T*T'' is the identity operator. But ''T'' is clearly not normal.
 
== Quasinormal invariant subspaces ==
 
It is not known that, in general, whether a bounded operator ''A'' on a Hilbert space ''H'' has a nontrivial invariant subspace. However, when ''A'' is normal, an affirmative answer is given by the [[spectral theorem]]. Every normal operator ''A'' is obtained by integrating the identity function with respect to a spectral measure ''E'' = {''E<sub>B</sub>''} on the spectrum of ''A'', ''&sigma;''(''A''):
 
:<math>A = \int_{\sigma(A)} \lambda d E (\lambda).\,</math>
 
For any Borel set ''B'' &sub; ''&sigma;''(''A''), the projection ''E<sub>B</sub>'' commutes with ''A'' and therefore the range of ''E<sub>B</sub>'' is an invariant subpsace of ''A''.
 
The above can be extended directly to quasinormal operators. To say ''A'' commutes with ''A*A'' is to say that ''A'' commutes with (''A*A'')<sup>&frac12;</sup>. But this implies that ''A'' commutes with any projection ''E<sub>B</sub>'' in the spectral measure of (''A*A'')<sup>&frac12;</sup>, which proves the invariant subspace claim. In fact, one can conclude something stronger. The range of ''E<sub>B</sub>'' is actually a ''reducing subspace'' of ''A'', i.e. its orthogonal complement is also invariant under ''A''.
== References ==
*P. Halmos, A Hilbert Space Problem Book, Springer, New York 1982.  
 
[[Category:Operator theory]]
[[Category:Invariant subspaces]]

Revision as of 19:08, 24 January 2014

In operator theory, quasinormal operators is a class of bounded operators defined by weakening the requirements of a normal operator.

Every quasinormal operator is a subnormal operator. Every quasinormal operator on a finite-dimensional Hilbert space is normal.

Definition and some properties

Definition

Let A be a bounded operator on a Hilbert space H, then A is said to be quasinormal if A commutes with A*A, i.e.

Properties

A normal operator is necessarily quasinormal.

Let A = UP be the polar decomposition of A. If A is quasinormal, then UP = PU. To see this, notice that the positive factor P in the polar decomposition is of the form (A*A)½, the unique positive square root of A*A. Quasinormality means A commutes with A*A. As a consequence of the continuous functional calculus for self adjoint operators, A commutes with P = (A*A)½ also, i.e.

So UP = PU on the range of P. On the other hand, if hH lies in kernel of P, clearly UP h = 0. But PU h = 0 as well. because U is a partial isometry whose initial space is closure of range P. Finally, the self-adjointness of P implies that H is the direct sum of its range and kernel. Thus the argument given proves UP = PU on all of H.

On the other hand, one can readily verify that if UP = PU, then A must be quasinormal. Thus the operator A is quasinormal if and only if UP = PU.

When H is finite dimensional, every quasinormal operator A is normal. This is because that in the finite dimensional case, the partial isometry U in the polar decomposition A = UP can be taken to be unitary. This then gives

In general, a partial isometry may not be extendable to a unitary operator and therefore a quasinormal operator need not be normal. For example, consider the unilateral shift T. T is quasinormal because T*T is the identity operator. But T is clearly not normal.

Quasinormal invariant subspaces

It is not known that, in general, whether a bounded operator A on a Hilbert space H has a nontrivial invariant subspace. However, when A is normal, an affirmative answer is given by the spectral theorem. Every normal operator A is obtained by integrating the identity function with respect to a spectral measure E = {EB} on the spectrum of A, σ(A):

For any Borel set Bσ(A), the projection EB commutes with A and therefore the range of EB is an invariant subpsace of A.

The above can be extended directly to quasinormal operators. To say A commutes with A*A is to say that A commutes with (A*A)½. But this implies that A commutes with any projection EB in the spectral measure of (A*A)½, which proves the invariant subspace claim. In fact, one can conclude something stronger. The range of EB is actually a reducing subspace of A, i.e. its orthogonal complement is also invariant under A.

References

  • P. Halmos, A Hilbert Space Problem Book, Springer, New York 1982.