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

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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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