Quantum and CircuitsReading edition

Filtering a signal with something to remove

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1.8 Filtering a signal with something to remove

Take the off-band perturbation

\[ b(n)=3\cos(\pi n/2)+2. \]

The constant occupies frequency zero, and the cosine occupies labels three and nine. These labels all lie outside \(U_{12}\). The perturbation has the literal rational vector

\[ b=(5,2,-1,2,5,2,-1,2,5,2,-1,2). \]

Set \(x=c+b\), giving

\[ x=(9,2,1,2,3,2,-5,2,3,2,1,2). \]

Theorem QA11: Exact filter recovery and orthogonal energy

The test signal satisfies

\[ Pc=c, \qquad Pb=0, \qquad Px=c, \qquad (I-P)x=b, \]

and

\[ \langle c,b\rangle=0, \qquad \|c\|^2=48, \qquad \|b\|^2=102, \qquad \|x\|^2=150=48+102. \]

Proof

QA05 gives the support of \(\widehat c\). Write the cosine as

\[ 3\cos(\pi n/2)=\frac32(\zeta^{3n}+\zeta^{9n}). \]

Thus \(\widehat b\) equals twenty-four at zero, eighteen at three and nine, and zero elsewhere. Multiplication by \(D\) fixes the spectrum of \(c\) and kills the spectrum of \(b\), proving the filter identities. Their supports are disjoint, so Parseval for inner products gives \(\langle c,b\rangle=0\). QA05 gives \(\|c\|^2=12\cdot4=48\), and

\[ \|b\|^2=\frac{24^2+18^2+18^2}{12}=102. \]

QA07 then gives \(\|x\|^2=48+102=150\). The same numbers follow by direct rational squaring of the displayed vectors. \(\square\)

The discarded component is part of a complete explanation of the input. It is called a perturbation because the example declares \(c\) to be the target. It is a perfectly exact signal component rather than an error introduced by the representation. If the task were to recover all of \(x\), deleting \(b\) would lose valid information.

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