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Dyadic positive-mean estimator under an L2 bound
Statement
Let be a nonnegative finite-valued output of a coherent sampler, , and let be rational with and . Let be the subroutine defined in Variance-aware quantum Monte Carlo. Its output satisfies with probability at least . For , its calls use prepared output-state copies and uses of the supplied state reflection when its binned QAE calls use repeated controlled- access. The accuracy and prepared-copy bounds also hold in supplied controlled-power access; in that mode sum the separately declared power-query costs rather than infer this reflection count. All input access, band comparison, value arithmetic, controlled rotation, and finite-precision costs remain separately charged.
Facts & Assumptions
Given: The finite-valued nonnegative sampler output , rational with , , and the subroutine in Variance-aware quantum Monte Carlo. For the state-reflection count use the repeated controlled- implementation of its binned QAE calls; accuracy and the prepared-copy bound permit either access mode.
Variance-aware quantum Monte Carlo defines , , the bands and , their scaled observables, and the median repetitions.
Quantum bounded-expectation guarantee and query cost: for an observable of mean , a phase register gives error radius at the stated confidence, and each QAE run uses controlled-Grover calls in repeated controlled- access, or separately priced supplied-power queries when .
Amplitude-estimation expectation estimator lets the call in [F2] select exactly the chosen by setting target .
One-sided concentration bound for independent median trials: a median of independent trials with failure probability at most fails with probability at most ; Quantum query algorithm specifies fresh independent executions.
Coherent finite sampler and observable value requires the sampler and inverse, value, comparator, rotation, and reflection implementations to be supplied and charged separately.
Holder's inequality for random variables with exponents gives .
Expectation of a real random variable on a finite probability space: expectation is the finite weighted sum for the sampler law; in particular .
The natural logarithm as the inverse of the exponential function fixes the natural logarithm used to choose the finite repetition count.
Rational bounds for pi used in finite schedules gives ; Square roots exist: a unique with ; the positives are and Squaring is monotone on the nonnegatives give from , and for nonnegative , implies .
A terminating rational enclosure for the natural logarithm returns an interval of width at most containing for every positive rational ; its upper endpoint satisfies , and its loop terminates.
Expectation agrees with the published finite weighted sum identifies the general expectations used in [F6] with the finite weighted sums in [F7].
Proof
The intervals are disjoint and cover . Write for the scaled band output in [F1], , and . By [F7] and finite-sum additivity, Since on the tail, .
By [F2]–[F3], the th estimate has error at most except with probability . A union bound over bands makes all estimates satisfy these bounds with probability at least . On that event, the deterministic estimation error is at most
The least-dyadic choice in [F1] gives , since this positive threshold exceeds . Each binned call has median repetitions. In repeated controlled- access it has controlled-Grover calls per repetition by [F1]–[F3]; each includes one supplied state reflection. There are bins. The outer repetitions are because [F10] makes . Each repetition prepares one fresh state in either access mode. Therefore the total state-copy count is , and in repeated access the total reflection count is . In supplied-power access each repetition instead makes power queries, whose actual declared prices are summed; no reflection expansion is assumed.
By [F11], the general expectations in the Hölder application [F6] equal their finite weighted-sum values in [F7]. For the lowest band, [F6] with and gives , since by [F7]; hence . For , on its band, so . Finite Cauchy–Schwarz on the band terms gives , because the bands are disjoint. Thus .
The parameter choice in [F1] gives with , so [F9] implies ; also because , and minimality gives , hence . Thus . By [F9], and . Thus the first error term in step 1.2 is less than , and the second less than . Together with from step 1.1, their sum is at most , since for .
A single binned execution succeeds with probability at least by step 1.2, hence at least , and has the stated error by step 3.1. For its median over independent executions, a failure requires at least half the runs to fail; their failure probability is at most , so the deviation from its mean is at least . By [F4] and the chosen , this probability is at most : the algorithm uses and [F10] gives . This proves the confidence claim.
The reflection count is an oracle coordinate only. By [F5], sampler preparation/inverse, controlled access, data loading, band comparison, value arithmetic, and rotation compilation are additional declared costs.
Depends on
- Variance-aware quantum Monte Carlo
- Amplitude-estimation expectation estimator
- Quantum bounded-expectation guarantee and query cost
- Coherent finite sampler and observable value
- Expectation of a real random variable on a finite probability space
- Expectation agrees with the published finite weighted sum
- Holder's inequality for random variables
- Rational bounds for pi used in finite schedules
- Square roots exist: a unique $\sqrt{a} \ge 0$ with $(\sqrt{a})^2 = a$; the positives are $\{x^2 : x \neq 0\}$
- Squaring is monotone on the nonnegatives
- Controlled Unitary Access
- Inverse Unitary Access
- Circuit-family and computation cost model
- One-sided concentration bound for independent median trials
- Quantum query algorithm
- The natural logarithm as the inverse of the exponential function
- A terminating rational enclosure for the natural logarithm
Used by
Dependency tree · two levels
96 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Ashley Montanaro, Quantum speedup of Monte Carlo methods, Algorithm 2 and Lemma 4 (standard reference, not scraped)
- Gilles Brassard, Peter Høyer, Michele Mosca, and Alain Tapp, Quantum Amplitude Amplification and Estimation, Theorem 12 (standard reference, not scraped)