Manuscript V-B@1 · V-B-v1.tex · section · 3fadc1ad
A common finite response carrier
Finite compression and the complete Enter interface › A common finite response carrier · lines 1733–1773
V-B@1#eq:compression
Let
The external field acts as ; the mixed coefficient acts as in (eq:mixed); and the cubic form is extended by the identity oscillator form.
Choose an isometry
whose image is spanned by finitely many orthonormal vectors of . For each setting , choose one of the symmetric response forms proved above and define its finite matrix
For operator settings this is the usual compression. For the cubic setting it is a form compression, requiring no unproved unregulated operator.
The finite matrix is not an invariant subspace realization of the full response operator. In particular,
is not identified with a compression of a continuum unitary. The compressed matrix is the operational observable declared here.
Choose a common with , and define
Displayed formulas in this passage
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