In mathematics, the Calkin correspondence, named after mathematician John Williams Calkin, is a bijective correspondence between two-sided ideals of bounded linear operators of a separable infinite-dimensional Hilbert space and Calkin sequence spaces (also called rearrangement invariant sequence spaces). The correspondence is implemented by mapping an operator to its singular value sequence.
It originated from John von Neumann's study of symmetric norms on matrix algebras.[1] It provides a fundamental classification and tool for the study of two-sided ideals of compact operators and their traces, by reducing problems about operator spaces to (more resolvable) problems on sequence spaces.
A two-sided ideal J of the bounded linear operators B(H) on a separable Hilbert space H is a linear subspace such that AB and BA belong to J for all operators A from J and B from B(H).
A sequence space j within l∞ can be embedded in B(H) using an arbitrary orthonormal basis n=0∞. Associate to a sequence a from j the bounded operator
{\rmdiag}(a)=
infty | |
\sum | |
n=0 |
an|en\rangle\langleen|,
A Calkin (or rearrangement invariant) sequence space is a linear subspace j of the bounded sequences l∞ such that if a is a bounded sequence and μ(n,a) ≤ μ(n,b), n 0, 1, 2, ..., for some b in j, then a belongs to j.
Associate to a two-sided ideal J the sequence space j given by
j=\{a\inlinfty:{\rmdiag}(\mu(a))\inJ\}.
J=\{A\inB(H):\mu(A)\inj\}.
Calkin correspondence: The two-sided ideals of bounded operators on an infinite dimensional separable Hilbert space and the Calkin sequence spaces are in bijective correspondence.
It is sufficient to know the association only between positive operators and positive sequences, hence the map μ: J+ → j+ from a positive operator to its singular values implements the Calkin correspondence.
Another way of interpreting the Calkin correspondence, since the sequence space j is equivalent as a Banach space to the operators in the operator ideal J that are diagonal with respect to an arbitrary orthonormal basis, is that two-sided ideals are completely determined by their diagonal operators.
Suppose H is a separable infinite-dimensional Hilbert space.