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arXiv:2609.39621

Weakly Measured Loops for Quantum Amplitude Amplification: Oracle Savings and Adaptive Search with Unknown Target Probability

Wang Fang, Chris Heunen

quant-phSubmitted Sep 30, 2026• Announced Oct 1, 2026• 0 citations
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Abstract

We present a family of quantum amplitude amplification algorithms that interleave ordinary Grover rotations with tunable weak measurements in loops. A successful measurement yields the target state and stops the algorithm, while after a failure, the loop resumes from the post-measurement state without restarting. We express the leading costs in expected Grover iterations as $p \to 0$. For a known target probability $p$, an exact weak measurement-conditioned loop for states near the angle $π/4$ uses $(π/8+1/4+o(1))/\sqrt{p}$ iterations, improving on the standard Grover constant $π/4$ and on optimised restart Grover, and matching the corresponding infimum in our continuous-angle analysis. When only a lower bound $0 < p_0 \leq p < 1/2$ is available, a discrete Lyapunov equation gives the exact expected oracle cost for every fixed measurement strength and a closed-form optimal strength. Using the strength selected from $p_0$, the expected number of Grover iterations is at most $\frac{1}{2\sqrt{2}}(\frac{1}{\sqrt{p}}+\frac{1}{\sqrt{p_0}})$, where the expected cost decreases as the actual $p$ increases, and gives the leading constant $1/\sqrt{2}$ at the promise boundary $p = p_0$. For completely unknown $p$, we identify measurement strength $κ(t)=Θ(1/t)$ as the critical scale within the regular schedules considered here and analyse $κ_b(t)=\min\{1/2,b/t\}$. For each fixed $b > 2$, we rigorously derive a closed-form Gamma-function expression $C(b)$ giving $(C(b)/2+o(1))/\sqrt{p}$ expected iterations. Numerical minimisation of this explicit expression gives $b \approx 5.2$ and $C(b)/2 \approx 1.01$. The results show that weak measurements preserve the $Θ(1/\sqrt{p})$ search scale while adding an explicit fixed-point control mechanism and provable oracle savings.

Comments
41 pages, 3 figures

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We present a family of quantum amplitude amplification algorithms that interleave ordinary Grover rotations with tunable weak measurements in loops. A successful measurement yields the target state and stops the algorithm, while after a failure, the loop resumes from the post-measurement state without restarting. We express the leading costs in expected Grover iterations as p→0p \to 0p→0. For a known target probability ppp, an exact weak measurement-conditioned loop for states near the angle π/4π/4π/4 uses (π/8+1/4+o(1))/p(π/8+1/4+o(1))/\sqrt{p}(π/8+1/4+o(1))/p​ iterations, improving on the standard Grover constant π/4π/4π/4 and on optimised restart Grover, and matching the corresponding infimum in our continuous-angle analysis. When only a lower bound 0<p0≤p<1/20 < p_0 \leq p < 1/20<p0​≤p<1/2 is available, a discrete Lyapunov equation gives the exact expected oracle cost for every fixed measurement strength and a closed-form optimal strength. Using the strength selected from p0p_0p0​, the expected number of Grover iterations is at most 122(1p+1p0)\frac{1}{2\sqrt{2}}(\frac{1}{\sqrt{p}}+\frac{1}{\sqrt{p_0}})22​1​(p​1​+p0​​1​), where the expected cost decreases as the actual ppp increases, and gives the leading constant 1/21/\sqrt{2}1/2​ at the promise boundary p=p0p = p_0p=p0​. For completely unknown ppp, we identify measurement strength κ(t)=Θ(1/t)κ(t)=Θ(1/t)κ(t)=Θ(1/t) as the critical scale within the regular schedules considered here and analyse κb(t)=min⁡{1/2,b/t}κ_b(t)=\min\{1/2,b/t\}κb​(t)=min{1/2,b/t}. For each fixed b>2b > 2b>2, we rigorously derive a closed-form Gamma-function expression C(b)C(b)C(b) giving (C(b)/2+o(1))/p(C(b)/2+o(1))/\sqrt{p}(C(b)/2+o(1))/p​ expected iterations. Numerical minimisation of this explicit expression gives b≈5.2b \approx 5.2b≈5.2 and C(b)/2≈1.01C(b)/2 \approx 1.01C(b)/2≈1.01. The results show that weak measurements preserve the Θ(1/p)Θ(1/\sqrt{p})Θ(1/p​) search scale while adding an explicit fixed-point control mechanism and provable oracle savings.
Grover's quantum search and its generalization, quantum amplitude amplification, provide quadratic advantage over classical algorithms for a diverse set of tasks, but are tricky to use without knowing beforehand what fraction λ\lambdaλ of the initial state is comprised of the target states. In contrast, fixed-point search algorithms need only a reliable lower bound on this fraction, but, as a consequence, lose the very quadratic advantage that makes Grover's algorithm so appealing. Here we provide the first version of amplitude amplification that achieves fixed-point behavior without sacrificing the quantum speedup. Our result incorporates an adjustable bound on the failure probability, and, for a given number of oracle queries, guarantees that this bound is satisfied over the broadest possible range of λ\lambdaλ.
Grover's quantum search and its generalization, quantum amplitude amplification, provide a quadratic advantage over classical algorithms for a diverse set of tasks but are tricky to use without knowing beforehand what fraction λ of the initial state is comprised of the target states. In contrast, fixed-point search algorithms need only a reliable lower bound on this fraction but, as a consequence, lose the very quadratic advantage that makes Grover's algorithm so appealing. Here we provide the first version of amplitude amplification that achieves fixed-point behavior without sacrificing the quantum speedup. Our result incorporates an adjustable bound on the failure probability and, for a given number of oracle queries, guarantees that this bound is satisfied over the broadest possible range of λ.
Quantum Amplitude Amplification (QAA), the generalization of Grover's algorithm, is capable of yielding optimal solutions to combinatorial optimization problems with high probabilities. In this work we extend the conventional 2-dimensional representation of Grover's (orthogonal collective states) to oracles which encode cost functions such as QUBO, and show that linear cost functions are a special case whereby an exact formula exists for determining optimal oracle parameter settings. Using simulations of problem sizes up to 40 qubits we demonstrate QAA's algorithmic performance across all possible solutions, with an emphasis on the closeness in Grover-like performance for solutions near the global optimum. We conclude with experimental demonstrations of generalized QAA on both IBMQ (superconducting) and IonQ (trapped ion) qubits, showing that the observed probabilities of each basis state match our equations as a function of varying the free parameters in the oracle and diffusion operators.
Grover's algorithm searches an unstructured database of NNN entries, finding a marked element in time O(N)\mathcal{O}(\sqrt{N})O(N​). The algorithm was later generalised to amplitude amplification. The original algorithm succeeds with probability close to one and needs to run for a number of iterations chosen ahead of time. We discuss an implementation of amplitude amplification that, instead, runs for a number of iterations unspecified a priori and only halts on success. We prove that this approach maintains the quadratic speed-up of the original quantum algorithm. The key component is a feedback loop controlled by a weak measurement that allows limited monitoring of the evolution of the quantum state.
This paper presents the Single-Rotation Quantum Search Algorithm, which achieves amplitude-amplification with exactly one oracle call and one rotation operation. We prove that for unstructured search over N items, a single rotation by π/4 radians is both necessary and sufficient to amplify the marked state probability from 1/N to 1/2. This represents the theoretical minimum: no algorithm can succeed with fewer than one oracle call, and no additional rotations are needed beyond the single π/4 rotation. We provide explicit closed forms for the rotation operator with numerical values, demonstrating complete physical realizability. The algorithm is implemented by one oracle call, one diffusion call, and log(N) reflections. For N = 2n search spaces, the algorithm achieves success probability exactly 1/2 with one iteration, compared to O( N ) iterations for Grover’s algorithm.
Grover’s algorithm represents a cornerstone quantum attack against symmetric cryptography, offering a quadratic speedup for exhaustive key search. While its theoretical properties are well established, the practical robustness of Grover’s algorithm under non-ideal oracle execution remains insufficiently quantified, particularly in security-relevant contexts. This work presents a comprehensive quantitative analysis of Grover’s robustness against intermittent oracle failures, modeling realistic execution imperfections that may arise in practical quantum attack scenarios. Using a reduced two-dimensional representation of amplitude amplification, we define and measure a practical reliability threshold beyond which Grover’s success probability collapses abruptly. Our results demonstrate that this threshold decreases exponentially with problem size, scaling as p∗(n)∝2−n/2 p^{\ast}(n) \propto 2^{-n/2} p∗(n)∝2−n/2, implying that cryptographically relevant problem sizes require unrealistically high oracle reliability to preserve quantum advantage. For n=40 n=40 n=40, the oracle must fail less than once every ∼800,000 \sim 800{,}000 ∼800,000 iterations to preserve practical advantage, a requirement that becomes exponentially more stringent for larger key sizes. These findings do not contradict Grover’s theoretical correctness but highlight critical robustness limitations that must be explicitly considered when assessing quantum threats to symmetric cryptography. We provide actionable insights for post-quantum security assessment by translating abstract quantum assumptions into concrete reliability requirements, demonstrating that the practical feasibility of Grover-based attacks may be significantly lower than commonly assumed under realistic hardware constraints.