Difference between revisions of "Spectral operator"
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''spectral measure'' | ''spectral measure'' | ||
− | A bounded [[Linear operator|linear operator]] | + | A bounded [[Linear operator|linear operator]] $ A $ |
+ | mapping a [[Banach space|Banach space]] $ X $ | ||
+ | into itself and such that for the $ \sigma $- | ||
+ | algebra $ {\mathcal B} $ | ||
+ | of Borel subsets $ \delta $ | ||
+ | in the plane there is a [[Resolution of the identity|resolution of the identity]] $ E ( \delta ) $ | ||
+ | with the following properties: 1) for any $ \delta \in {\mathcal B} $ | ||
+ | the projector $ E ( \delta ) $ | ||
+ | reduces $ A $, | ||
+ | that is, $ E ( \delta ) A = A E ( \delta ) $ | ||
+ | and the spectrum $ \sigma ( A _ \delta ) $ | ||
+ | lies in $ \overline \delta \; $, | ||
+ | where $ A _ \delta $ | ||
+ | is the restriction of $ A $ | ||
+ | to the invariant subspace $ E ( \delta ) X $; | ||
+ | 2) the mapping $ \delta \mapsto E ( \delta ) $ | ||
+ | is a homeomorphism of $ {\mathcal B} = \{ \delta \} $ | ||
+ | into the Boolean algebra $ \{ E ( \delta ) \} $; | ||
+ | 3) all projectors $ E ( \delta ) $ | ||
+ | are bounded, that is, $ \| E ( \delta ) \| \leq M $, | ||
+ | $ \delta \in {\mathcal B} $; | ||
+ | and 4) the resolution of the identity $ E ( \delta ) $ | ||
+ | is countably additive in the strong topology of $ X $, | ||
+ | that is, for any $ x \in X $ | ||
+ | and any sequence $ \{ \delta _ {n} \} \subset {\mathcal B} $ | ||
+ | of pairwise disjoint sets, | ||
− | + | $$ | |
+ | E \left ( \cup _ { n= } 1 ^ \infty \delta _ {n} \right ) x = \sum _ { n= } 1 ^ \infty E ( \delta _ {n} ) x . | ||
+ | $$ | ||
− | The concept of a spectral operator can be generalized to the case of closed unbounded operators. In 1), the additional requirement is then that the inclusion | + | The concept of a spectral operator can be generalized to the case of closed unbounded operators. In 1), the additional requirement is then that the inclusion $ E ( \delta ) D ( A) \subset D ( A) $ |
+ | holds, where $ D ( A) $ | ||
+ | is the domain of definition of $ A $, | ||
+ | and $ E ( \delta ) X \subset D ( A) $ | ||
+ | for bounded $ \delta $. | ||
All linear operators on a finite-dimensional space and all self-adjoint and normal operators on a Hilbert space are spectral operators. For example, the operator | All linear operators on a finite-dimensional space and all self-adjoint and normal operators on a Hilbert space are spectral operators. For example, the operator | ||
− | + | $$ | |
+ | A x ( t) = t x( t) + \int\limits _ {- \infty } ^ \infty | ||
+ | K ( t , s ) x ( s) d s | ||
+ | $$ | ||
− | on < | + | on $ L _ {p} ( - \infty , \infty ) $, |
+ | $ 1 < p < \infty $, | ||
+ | is spectral on | ||
− | + | $$ | |
+ | D ( A) = \left \{ {x ( t) } : { | ||
+ | \int\limits _ {- \infty } ^ \infty | t x ( t) | ^ {2} d t | ||
+ | < \infty } \right \} | ||
+ | $$ | ||
− | if the kernel | + | if the kernel $ K ( t , s ) $ |
+ | is the Fourier transform of a Borel measure $ \mu $ | ||
+ | on the plane of total variation $ \mathop{\rm var} \mu < 1 / 2 \pi $ | ||
+ | and is such that | ||
− | + | $$ | |
+ | \int\limits _ {- \infty } ^ \infty K ( t , s ) | ||
+ | x ( s) d s ,\ \int\limits _ {- \infty } ^ \infty | ||
+ | K ( t , s ) x ( t) d t | ||
+ | $$ | ||
− | are bounded linear operators on | + | are bounded linear operators on $ L _ {p} ( - \infty , \infty ) $. |
Spectral operators have many important properties, such as: | Spectral operators have many important properties, such as: | ||
− | + | $$ | |
+ | \lambda \in \delta ( A) \iff \exists \ | ||
+ | \{ x _ {n} \} \subset X , \| x _ {n} \| | ||
+ | = 1 , ( A - \lambda I ) x _ {n} \rightarrow 0 . | ||
+ | $$ | ||
− | If | + | If $ X $ |
+ | is separable, the point and residual spectra of $ A $ | ||
+ | are at most countable. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> N. Dunford, J.T. Schwartz, "Linear operators. Spectral operators" , '''3''' , Interscience (1971)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> N. Dunford, "A survey of the theory of spectral operators" ''Bull. Amer. Math. Soc.'' , '''64''' (1958) pp. 217–274</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> N. Dunford, J.T. Schwartz, "Linear operators. Spectral operators" , '''3''' , Interscience (1971)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> N. Dunford, "A survey of the theory of spectral operators" ''Bull. Amer. Math. Soc.'' , '''64''' (1958) pp. 217–274</TD></TR></table> |
Revision as of 08:22, 6 June 2020
spectral measure
A bounded linear operator $ A $ mapping a Banach space $ X $ into itself and such that for the $ \sigma $- algebra $ {\mathcal B} $ of Borel subsets $ \delta $ in the plane there is a resolution of the identity $ E ( \delta ) $ with the following properties: 1) for any $ \delta \in {\mathcal B} $ the projector $ E ( \delta ) $ reduces $ A $, that is, $ E ( \delta ) A = A E ( \delta ) $ and the spectrum $ \sigma ( A _ \delta ) $ lies in $ \overline \delta \; $, where $ A _ \delta $ is the restriction of $ A $ to the invariant subspace $ E ( \delta ) X $; 2) the mapping $ \delta \mapsto E ( \delta ) $ is a homeomorphism of $ {\mathcal B} = \{ \delta \} $ into the Boolean algebra $ \{ E ( \delta ) \} $; 3) all projectors $ E ( \delta ) $ are bounded, that is, $ \| E ( \delta ) \| \leq M $, $ \delta \in {\mathcal B} $; and 4) the resolution of the identity $ E ( \delta ) $ is countably additive in the strong topology of $ X $, that is, for any $ x \in X $ and any sequence $ \{ \delta _ {n} \} \subset {\mathcal B} $ of pairwise disjoint sets,
$$ E \left ( \cup _ { n= } 1 ^ \infty \delta _ {n} \right ) x = \sum _ { n= } 1 ^ \infty E ( \delta _ {n} ) x . $$
The concept of a spectral operator can be generalized to the case of closed unbounded operators. In 1), the additional requirement is then that the inclusion $ E ( \delta ) D ( A) \subset D ( A) $ holds, where $ D ( A) $ is the domain of definition of $ A $, and $ E ( \delta ) X \subset D ( A) $ for bounded $ \delta $.
All linear operators on a finite-dimensional space and all self-adjoint and normal operators on a Hilbert space are spectral operators. For example, the operator
$$ A x ( t) = t x( t) + \int\limits _ {- \infty } ^ \infty K ( t , s ) x ( s) d s $$
on $ L _ {p} ( - \infty , \infty ) $, $ 1 < p < \infty $, is spectral on
$$ D ( A) = \left \{ {x ( t) } : { \int\limits _ {- \infty } ^ \infty | t x ( t) | ^ {2} d t < \infty } \right \} $$
if the kernel $ K ( t , s ) $ is the Fourier transform of a Borel measure $ \mu $ on the plane of total variation $ \mathop{\rm var} \mu < 1 / 2 \pi $ and is such that
$$ \int\limits _ {- \infty } ^ \infty K ( t , s ) x ( s) d s ,\ \int\limits _ {- \infty } ^ \infty K ( t , s ) x ( t) d t $$
are bounded linear operators on $ L _ {p} ( - \infty , \infty ) $.
Spectral operators have many important properties, such as:
$$ \lambda \in \delta ( A) \iff \exists \ \{ x _ {n} \} \subset X , \| x _ {n} \| = 1 , ( A - \lambda I ) x _ {n} \rightarrow 0 . $$
If $ X $ is separable, the point and residual spectra of $ A $ are at most countable.
References
[1] | N. Dunford, J.T. Schwartz, "Linear operators. Spectral operators" , 3 , Interscience (1971) |
[2] | N. Dunford, "A survey of the theory of spectral operators" Bull. Amer. Math. Soc. , 64 (1958) pp. 217–274 |
Spectral operator. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Spectral_operator&oldid=48761