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Exact query count for the finite-grid iterative estimator
Statement
Across the finite-grid schedule with and , forward calls equal , inverse calls equal , and both zero-input reflections and good-predicate reflections equal . Thus the total number of calls is . This count gives no finite-sample success guarantee.
For all integers , 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.
Stage has shots and uses Grover iterates after one fresh preparation (Iterative no-QFT amplitude estimation by finite-grid likelihood).
The signed iterate is , and the matching prepared-success-subspace contract supplies and charges one call to each of per uncontrolled iterate (Amplitude estimation and counting input/output contract, Prepared unitary and success subspace for amplitude amplification).
The query model counts these oracle uses separately from ordinary gates (Quantum query complexity).
The Grover iterate rotates the prepared state so that after iterates its good probability is (Grover eigenphases encode the good probability).
The measurement outcomes are the two orthogonal good/bad projections (Finite projective measurements).
The real likelihood values are finite cyclotomic algebraic numbers and admit terminating exact comparisons (Finite exact comparison of real cyclotomic values).
Each oracle/state-preparation call is an explicit query resource (Quantum query algorithm).
The fixed-count amplification procedure applies exactly the declared number of signed iterates and then the good/bad projective instrument, with no controlled- call (Amplitude amplification with a fixed integer iteration count).
The complex exponential is additive, and its kernel is (, and the complex exponential extends the real exponential, , and exactly when ).
For real , (, , and ).
Sine is odd and cosine is even (Parity and the Pythagorean identity for sine and cosine).
Proof
Suppose first that , so the normalized vectors are defined. Inductively applying the rotation matrix from [F21] to gives . Its good projection therefore has squared norm , so the listed good/bad measurement has the Bernoulli likelihood factors displayed in the definition.
If , then and . The endpoint clause of [F21]’s supplier gives , hence for every , including . The good/bad probabilities are therefore and , equal to and . Almost surely every ; 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 when no good outcome occurs. No normalized good vector or conditional state on a zero-probability outcome is used.
Set and . For each , use the residues in the algorithm's polynomial factors and put . By [F26], and ; [F27]–[F28] give their sum as . Therefore [F29] gives and . It follows that for each . The comparison procedure [F23] decides every pair exactly, including equality; the nonempty finite set therefore has a maximizing label, and the least-label tie rule determines a unique output, including when all (then the chosen label is ). Its output polynomial is exactly by the same identity.
A shot in stage uses one initial and then iterates. Each iterate contributes one more , one , one zero-input reflection, and one good reflection by [F2]. Therefore the per-stage counts are respectively , , , and .
If , orthogonality gives , so and . The other endpoint clause of [F21]’s supplier gives , hence for every , including . Its good/bad probabilities are and , agreeing with and . Almost surely every ; 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 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.
Summing over gives the first four formulas. Since and for , for , yielding the stated total. The geometric sum is , so the total is .
Every stage has finitely many shots and iterates because are finite. Fresh state preparations and measurements are part of the instructions, so no controlled 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 guarantee.
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.
Depends on
- Iterative no-QFT amplitude estimation by finite-grid likelihood
- Prepared unitary and success subspace for amplitude amplification
- Quantum query complexity
- Amplitude estimation and counting input/output contract
- Amplitude amplification with a fixed integer iteration count
- Grover eigenphases encode the good probability
- Finite projective measurements
- Quantum query algorithm
- Finite exact comparison of real cyclotomic values
- $\exp(x+iy)=e^x(\cos y+i\sin y)$, $|\exp(x+iy)|=e^x$, and $e^{i\pi}+1=0$
- Parity and the Pythagorean identity for sine and cosine
- $\exp(z+w)=\exp z\,\exp w$, and the complex exponential extends the real exponential
- $\ker(\exp)=2\pi i\mathbb Z$, and $\exp z=\exp w$ exactly when $z-w\in2\pi i\mathbb Z$
- Double-angle and quadratic power-reduction identities
Used by
Nothing in the library uses this result yet.
Cited to discharge well-definedness by Iterative no-QFT amplitude estimation by finite-grid likelihood.
Dependency tree · two levels
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Sources
- Brassard, Høyer, Mosca, and Tapp, Quantum Amplitude Amplification and Estimation, complete article, §§4–5, Theorems 11–18 (standard reference, not scraped)
- Andrew M. Childs, Lecture Notes on Quantum Algorithms, complete lecture notes, §§19.1–19.3 (standard reference, not scraped)
- Ronald de Wolf, Quantum Computing: Lecture Notes, complete 239-page notes, §7.3 (standard reference, not scraped)
- Suzuki et al., Amplitude estimation without phase estimation, complete article, §§2–3.2 (standard reference, not scraped)