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Exact query count for the finite-grid iterative estimator

Statement

Across the finite-grid schedule with K≥1 and S≥1, forward A calls equal S∑k=0K(mk+1), inverse A∗ calls equal S∑k=0Kmk, and both zero-input reflections and good-predicate reflections equal S∑k=0Kmk. Thus the total number of A/A∗ calls is S∑k=0K(2mk+1)=S(1+∑k=1K(2k+1))=O(S2K). This count gives no finite-sample success guarantee.

For all integers K,S,J≥1, the finite-grid procedure terminates and returns a uniquely determined exact algebraic output under its least-label tie rule. Its displayed factors are the Bernoulli likelihood factors of the prescribed independent shots; no finite-sample accuracy guarantee is asserted.

Facts & Assumptions

Given: The finite-grid iterative schedule and its explicitly supplied and charged prepared-success-subspace access contract.

[F1]

Stage k has S shots and uses mk Grover iterates after one fresh A preparation (Iterative no-QFT amplitude estimation by finite-grid likelihood).

[F2]

The signed iterate is Q=−AS0A∗Sgood, and the matching prepared-success-subspace contract supplies and charges one call to each of A,A∗,S0,Sgood per uncontrolled iterate (Amplitude estimation and counting input/output contract, Prepared unitary and success subspace for amplitude amplification).

[F3]

The query model counts these oracle uses separately from ordinary gates (Quantum query complexity).

[F21]

The Grover iterate rotates the prepared state so that after m iterates its good probability is sin⁡2((2m+1)θ) (Grover eigenphases encode the good probability).

[F22]

The measurement outcomes are the two orthogonal good/bad projections (Finite projective measurements).

[F23]

The real likelihood values are finite cyclotomic algebraic numbers and admit terminating exact comparisons (Finite exact comparison of real cyclotomic values).

[F24]

Each oracle/state-preparation call is an explicit query resource (Quantum query algorithm).

[F25]

The fixed-count amplification procedure applies exactly the declared number of signed Q iterates and then the good/bad projective instrument, with no controlled-A call (Amplitude amplification with a fixed integer iteration count).

[F28]
[F29]

sin⁡2x=(1−cos⁡(2x))/2 and cos⁡2x=(1+cos⁡(2x))/2 (Double-angle and quadratic power-reduction identities).

Proof

1.1givenF21F22algebra

Suppose first that 0<a<1, so the normalized vectors B,G are defined. Inductively applying the rotation matrix from [F21] to cos⁡θB+sin⁡θG gives Qmkψ=cos⁡((2mk+1)θ)B+sin⁡((2mk+1)θ)G. Its good projection therefore has squared norm sin⁡2((2mk+1)θ), so the listed good/bad measurement has the Bernoulli likelihood factors displayed in the definition.

1.2givenF21F22algebra

If a=0, then Πgoodψ=0 and θ=0. The endpoint clause of [F21]’s supplier gives Qψ=ψ, hence Qmkψ=ψ for every mk≥0, including m0=0. The good/bad probabilities are therefore 0 and 1, equal to sin⁡2((2mk+1)0) and cos⁡2((2mk+1)0). Almost surely every hk=0; any record with a good outcome has probability zero under this endpoint model. The displayed Bernoulli factors give exactly these probabilities: a positive good exponent gives a zero factor, while the prescribed zero-exponent convention makes 00=1 when no good outcome occurs. No normalized good vector or conditional state on a zero-probability outcome is used.

1.3givenF23F26F27F28F29algebra

Set s=2J and ζs=e2πi/s. For each k,j, use the residues rkj,rkj′ in the algorithm's polynomial factors and put α=(2mk+1)θj. By [F26], ζsrkj=e2iα and ζsrkj′=e−2iα; [F27]–[F28] give their sum as 2cos⁡(2α). Therefore [F29] gives Ukj(ζs)=sin⁡2α and Vkj(ζs)=cos⁡2α. It follows that Pj(ζs)=Lj for each j. The comparison procedure [F23] decides every pair exactly, including equality; the nonempty finite set {0,…,J} therefore has a maximizing label, and the least-label tie rule determines a unique output, including when all Lj=0 (then the chosen label is j=0). Its output polynomial Ej^(ζs) is exactly sin⁡2θj^ by the same identity.

1.4givenF1F2algebra

A shot in stage k uses one initial A and then mk iterates. Each iterate contributes one more A, one A∗, one zero-input reflection, and one good reflection by [F2]. Therefore the per-stage counts are respectively S(mk+1), Smk, Smk, and Smk.

2.1givenF21F22step 1.1algebra

If a=1, orthogonality gives ∥(I−Πgood)ψ∥2=1−a=0, so Πgoodψ=ψ and θ=π/2. The other endpoint clause of [F21]’s supplier gives Qψ=−ψ, hence Qmkψ=(−1)mkψ for every mk≥0, including m0=0. Its good/bad probabilities are 1 and 0, agreeing with sin⁡2((2mk+1)π/2)=1 and cos⁡2((2mk+1)π/2)=0. Almost surely every hk=S; a record containing a bad outcome has probability zero under this model. The bad factor is zero exactly when its exponent is positive, and the same 00=1 convention applies when no bad outcome occurs. No normalized bad vector or conditional state on a zero-probability outcome is used. Together with step 1.1, these cases establish the claimed Bernoulli likelihood factors on the whole task domain.

2.2F1F3step 1.4algebra

Summing over k=0,…,K gives the first four formulas. Since m0=0 and mk=2k−1 for k≥1, 2mk+1=2k+1 for k≥1, yielding the stated total. The geometric sum is O(2K), so the total is O(S2K).

3.1givenF24F25step 1.1step 1.2step 2.1step 1.3

Every stage has finitely many shots and iterates because K,S are finite. Fresh state preparations and measurements are part of the instructions, so no controlled Q or QFT call is used. The likelihood selection is finite by step 1.3, but this argument establishes neither a sample-size error bound nor an ϵ,δ guarantee.

4.1givenF1F3step 1.4step 2.2∎

The call totals established in step 1.4 and step 2.2 only tally explicitly invoked queries. By [F1], the analyzed procedure is a finite-grid likelihood schedule with no finite-sample success guarantee; [F3] counts its declared query actions but supplies no probability or approximation-error bound. Thus this resource count establishes no success theorem.

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Used by

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Cited to discharge well-definedness by Iterative no-QFT amplitude estimation by finite-grid likelihood.

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