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    Quantum Amplitude Amplification and Estimation

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    Consider a Boolean function χ:X→{0,1}\chi: X \to \{0,1\} that partitions set XX between its good and bad elements, where xx is good if χ(x)=1\chi(x)=1 and bad otherwise. Consider also a quantum algorithm A\mathcal A such that A∣0⟩=∑x∈Xαx∣x⟩A |0\rangle= \sum_{x\in X} \alpha_x |x\rangle is a quantum superposition of the elements of XX, and let aa denote the probability that a good element is produced if A∣0⟩A |0\rangle is measured. If we repeat the process of running AA, measuring the output, and using χ\chi to check the validity of the result, we shall expect to repeat 1/a1/a times on the average before a solution is found. *Amplitude amplification* is a process that allows to find a good xx after an expected number of applications of AA and its inverse which is proportional to 1/a1/\sqrt{a}, assuming algorithm AA makes no measurements. This is a generalization of Grover's searching algorithm in which AA was restricted to producing an equal superposition of all members of XX and we had a promise that a single xx existed such that χ(x)=1\chi(x)=1. Our algorithm works whether or not the value of aa is known ahead of time. In case the value of aa is known, we can find a good xx after a number of applications of AA and its inverse which is proportional to 1/a1/\sqrt{a} even in the worst case. We show that this quadratic speedup can also be obtained for a large family of search problems for which good classical heuristics exist. Finally, as our main result, we combine ideas from Grover's and Shor's quantum algorithms to perform amplitude estimation, a process that allows to estimate the value of aa. We apply amplitude estimation to the problem of *approximate counting*, in which we wish to estimate the number of x∈Xx\in X such that χ(x)=1\chi(x)=1. We obtain optimal quantum algorithms in a variety of settings.Comment: 32 pages, no figure
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