In General > s.a. measure [operator-valued].
* Operations on operators:
Adjoint, extensions (e.g., Friedrich
extension).
@ General references: Murray & Von Neumann AM(36),
AM(43); Dunford & Schwartz 58, 63, 71; Dixmier
69; Beals 71.
@ Hilbert space: Achiezer & Glazman 61; Jordan 69; Cirelli & Gallone
74; Reed & Simon 72–78; Schechter 81.
@ Related topics: Atiyah 74 [elliptic]; Lahti et al JMP(99)
[operator integrals].
Types of Operators > s.a. Projector; Subnormal; Symmetric.
* Bounded: An operator A:
1
→
2 such
that there exists c in R, for all v in
1,
Av
2 < c
v
1 (c is
its norm).
* Hermitian: An operator A on
a Hilbert space such that ![]()
,
A![]()
=
A
,
![]()
,
for all
and
in
(A), i.e.,
complex symmetric; Relationships: This condition is weaker than self-adjointness
(it could
be that A
A),
but it still implies that ![]()
, A![]()
R;
However, if A and A2 are
maximal hermitian, then A is
self-adjoint.
* Essentially self-adjoint:
A Hermitian one defined on a dense subspace; It admits a unique self-adjoint
extension.
* Self-adjoint: An operator A such
that A*
= A,
i.e., A is Hermitian and with
(A*)
=
(A); Useful
because (1) The eigenvalues
are real; (2) There are complete orthonormal sets of eigenvectors; (3) One
can meaningfully define functions f(A), with f Borel
measurable.
* Normal: A matrix/operator A such that A*A = AA*;
It can be diagonalized; The unitary geometry of the rows is the same as that
of
the columns.
* Trace-class: An operator T : X → Y between
Banch spaces which can be written as T(x) =
i=1infty
i xi(x)
yi, with
xi
1,
yi
1,
and {
i}
in
1;
one can then define the trace of T by tr T:= inf
i=1infty
i .
@ General references: Reed & Simon 72 [infinite-dimensional spaces].
@ Self-adjoint: Dubin et al JPA(02) [spectral and semispectral measures]
@ Self-adjoint extensions: Bonneau et al AJP(01)qp [self-adjoint
extension examples];
> s.a. scattering.
@ PT-symmetric: Caliceti et al a0705 [non-selfadjont, with real discrete spectrum].
@ Unbounded: Bagarello RVMP(07) [algebras, intro and applications].
Spaces of Operators > s.a. observable
algebras [von Neumann].
*
(
): The space of bounded operators on a (separable) Hilbert
space, a W*-algebra; Its topological dual is the space of trace-class operators.
*
(
): The
space of compact operators on
;
Its topological dual is
(
).
@ General references: Blackadar 06 [C*-algebras and von Neumann algebras].
@ Maps between operator algebras: Salgado & Sánchez-Gómez mp/04-in
[Jamiolkowski positivity criterion].
Related Concepts > s.a. Boundary
Value Problems; matrix [determinant];
norm; series [Taylor]; Stone's
Theorem.
@ Spectral theory: Cirelli 72; Müller-Pfeiffer 81; Friedrichs
80; Hislop & Sigal 95; > s.a. Bloch
Theory, Toeplitz.
@ Eigenvalues/eigenvectors: Andrew & Miller PLA(03)
[continuous + point
spectrum, Lanczos algorithm].
@ Operations on operators: Gill & Zachary JPA(05) [fractional powers of linear
operators].
Differential Operators > s.a. conformal
structures [invariant]; D'Alambertian; laplacian.
* Zero modes: The eigenfunctions of a differential operator with zero
eigenvalue; They physically correspond to massless excitations of the field.
* Pseudodifferential operators:
Used in quantization, especially in the phase space (Wigner-Moyal) formulation
and in quantum field theory in surved spacetime.
@ Spectrum: Giacomini & Mouchet JPA(07)-a0706 [1D,
finding gaps in spectrum].
In Physics > s.a. observable
algebras.
@ Dynamical systems: Sakai 91.
@ Quantum theory: De Lange & Raab 91; Svozil qp/96 [discrete
operators and observables]; Bonneau et al AJP(01)qp [self-adjoint
extensions]; Kempf PRD(01)
[symmetric operators
and symmetries];
D'Ariano PLA(02)
[universal observables]; Ozorio de Almeida & Brodier qp/05/JPA
[semi-classical evolution]; > s.a. annihilation, creation, formulations and representations
of quantum mechanics.
@ Unitary operators: Accardi & Sabbadini qp/00 [enhancing
specified components].
Main page – Abbreviations – Journals – Comments – Other
sites – Acknowledgements
Send feedback and suggestions to bombelli at olemiss.edu – Modified
11 jul 2008