Riesz projector explained
In mathematics, or more specifically in spectral theory, the Riesz projector is the projector onto the eigenspace corresponding to a particular eigenvalue of an operator (or, more generally, a projector onto an invariant subspace corresponding to an isolated part of the spectrum). It was introduced by Frigyes Riesz in 1912.[1] [2]
Definition
Let
be a closed linear operator in the Banach space
. Let
be a simple or composite rectifiable contour, which encloses some region
and lies entirely within the
resolvent set
(
) of the operator
. Assuming that the contour
has a positive orientation with respect to the region
, the Riesz projector corresponding to
is defined by
})^\,\mathrmz;here
} is the
identity operator in
.
If
is the only point of the spectrum of
in
, then
is denoted by
.
Properties
The operator
is a projector which commutes with
, and hence in the decomposition
ak{B}=ak{L}\Gamma ⊕ ak{N}\Gamma
ak{L}\Gamma=P\Gammaak{B},
ak{N}\Gamma=(Iak{B
}-P_\Gamma)\mathfrak,both terms
and
are
invariant subspaces of the operator
.Moreover,
- The spectrum of the restriction of
to the subspace
is contained in the region
;
- The spectrum of the restriction of
to the subspace
lies outside the closure of
.
If
and
are two different contours having the properties indicated above, and the regions
and
have no points in common, then the projectors corresponding to them are mutually orthogonal:
See also
Notes and References
- Book: Functional Analysis. Riesz, F.. Sz.-Nagy, B.. Blackie & Son Limited. 1956.
- Book: Gohberg, I. C. Kreĭn, M. G.. Introduction to the theory of linear nonselfadjoint operators. 1969. American Mathematical Society, Providence, R.I..