Difference between revisions of "Diagonal operator"
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− | + | An operator $ D $ | |
+ | defined on the (closed) [[Linear closure|linear span]] of a basis $ \{ e _ {k} \} _ {k \geq 1 } $ | ||
+ | in a normed (or only locally convex) space $ X $ | ||
+ | by the equations $ De _ {k} = \lambda _ {k} e _ {k} $, | ||
+ | where $ k \geq 1 $ | ||
+ | and where $ \lambda _ {k} $ | ||
+ | are complex numbers. If $ D $ | ||
+ | is a continuous operator, one has | ||
− | + | $$ | |
+ | \sup _ {k \geq 1 } | \lambda _ {k} | < + \infty . | ||
+ | $$ | ||
− | + | If $ X $ | |
+ | is a Banach space, this condition is equivalent to the continuity of $ D $ | ||
+ | if and only if $ \{ e _ {k} \} _ {k \geq 1 } $ | ||
+ | is an unconditional basis in $ X $. | ||
+ | If $ \{ e _ {k} \} _ {k \geq 1 } $ | ||
+ | is an orthonormal basis in a Hilbert space $ H $, | ||
+ | then $ D $ | ||
+ | is a normal operator, and $ \| D \| = \sup _ {k \geq 1 } | \lambda _ {k} | $, | ||
+ | while the spectrum of $ D $ | ||
+ | coincides with the closure of the set $ \{ {\lambda _ {k} } : {k = 1 , 2 , . . . } \} $. | ||
+ | A normal and completely-continuous operator $ N $ | ||
+ | is a diagonal operator in the basis of its own eigen vectors; the restriction of a diagonal operator (even if it is normal) to its invariant subspace need not be a diagonal operator; given an $ \epsilon > 0 $, | ||
+ | any normal operator $ N $ | ||
+ | on a separable space $ H $ | ||
+ | can be represented as $ N = D + C $, | ||
+ | where $ D $ | ||
+ | is a diagonal operator, $ C $ | ||
+ | is a completely-continuous operator and $ \| C \| < \epsilon $. | ||
+ | |||
+ | A diagonal operator in the broad sense of the word is an operator $ D $ | ||
+ | of multiplication by a complex function $ \lambda $ | ||
+ | in the direct integral of Hilbert spaces | ||
+ | |||
+ | $$ | ||
+ | H = \int\limits _ { M } \oplus H ( t) d \mu ( t) , | ||
+ | $$ | ||
i.e. | i.e. | ||
− | + | $$ | |
+ | ( D f )( t) = \lambda ( t) f ( t) ,\ t \in M ,\ f \in H . | ||
+ | $$ | ||
Cf. [[Block-diagonal operator|Block-diagonal operator]]. | Cf. [[Block-diagonal operator|Block-diagonal operator]]. | ||
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====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> I.M. Singer, "Bases in Banach spaces" , '''1''' , Springer (1970)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> J. Wermer, "On invariant subspaces of normal operators" ''Proc. Amer. Math. Soc.'' , '''3''' : 2 (1952) pp. 270–277</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> I.D. Berg, "An extension of the Weyl–von Neumann theorem to normal operators" ''Trans. Amer. Math. Soc.'' , '''160''' (1971) pp. 365–371</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> I.M. Singer, "Bases in Banach spaces" , '''1''' , Springer (1970)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> J. Wermer, "On invariant subspaces of normal operators" ''Proc. Amer. Math. Soc.'' , '''3''' : 2 (1952) pp. 270–277</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> I.D. Berg, "An extension of the Weyl–von Neumann theorem to normal operators" ''Trans. Amer. Math. Soc.'' , '''160''' (1971) pp. 365–371</TD></TR></table> | ||
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====Comments==== | ====Comments==== |
Latest revision as of 19:55, 27 February 2021
An operator $ D $
defined on the (closed) linear span of a basis $ \{ e _ {k} \} _ {k \geq 1 } $
in a normed (or only locally convex) space $ X $
by the equations $ De _ {k} = \lambda _ {k} e _ {k} $,
where $ k \geq 1 $
and where $ \lambda _ {k} $
are complex numbers. If $ D $
is a continuous operator, one has
$$ \sup _ {k \geq 1 } | \lambda _ {k} | < + \infty . $$
If $ X $ is a Banach space, this condition is equivalent to the continuity of $ D $ if and only if $ \{ e _ {k} \} _ {k \geq 1 } $ is an unconditional basis in $ X $. If $ \{ e _ {k} \} _ {k \geq 1 } $ is an orthonormal basis in a Hilbert space $ H $, then $ D $ is a normal operator, and $ \| D \| = \sup _ {k \geq 1 } | \lambda _ {k} | $, while the spectrum of $ D $ coincides with the closure of the set $ \{ {\lambda _ {k} } : {k = 1 , 2 , . . . } \} $. A normal and completely-continuous operator $ N $ is a diagonal operator in the basis of its own eigen vectors; the restriction of a diagonal operator (even if it is normal) to its invariant subspace need not be a diagonal operator; given an $ \epsilon > 0 $, any normal operator $ N $ on a separable space $ H $ can be represented as $ N = D + C $, where $ D $ is a diagonal operator, $ C $ is a completely-continuous operator and $ \| C \| < \epsilon $.
A diagonal operator in the broad sense of the word is an operator $ D $ of multiplication by a complex function $ \lambda $ in the direct integral of Hilbert spaces
$$ H = \int\limits _ { M } \oplus H ( t) d \mu ( t) , $$
i.e.
$$ ( D f )( t) = \lambda ( t) f ( t) ,\ t \in M ,\ f \in H . $$
References
[1] | I.M. Singer, "Bases in Banach spaces" , 1 , Springer (1970) |
[2] | J. Wermer, "On invariant subspaces of normal operators" Proc. Amer. Math. Soc. , 3 : 2 (1952) pp. 270–277 |
[3] | I.D. Berg, "An extension of the Weyl–von Neumann theorem to normal operators" Trans. Amer. Math. Soc. , 160 (1971) pp. 365–371 |
Comments
For the notion of an unconditional basis see Basis.
For diagonal operators in the broad sense (and the corresponding notion of a diagonal algebra) see [a1].
References
[a1] | M. Takesaki, "Theory of operator algebras" , 1 , Springer (1979) pp. 259, 273 |
[a2] | P.R. Halmos, "A Hilbert space problem book" , Springer (1982) |
Diagonal operator. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Diagonal_operator&oldid=17619