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中国科学通报:英文版

What is the largest separation between quantum and classical query complexity?

Shao-Ming Fei

Published Jun 13, 2017• 0 citations
Publisher
DOI
10.1016/j.scib.2017.06.002

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We achieve essentially the largest possible separation between quantum and classical query complexities. We do so using a property-testing problem called Forrelation, where one needs to decide whether one Boolean function is highly correlated with the Fourier transform of a second function. This problem can be solved using 1 quantum query, yet we show that any randomized algorithm needs Ω(N/log⁡N)\Omega(\sqrt{N}/\log N)Ω(N​/logN) queries (improving an Ω(N1/4)\Omega(N^{1/4})Ω(N1/4) lower bound of Aaronson). Conversely, we show that this 1 versus Ω~(N)\widetilde{\Omega}(\sqrt{N})Ω(N​) separation is optimal: indeed, any ttt-query quantum algorithm whatsoever can be simulated by an O(N1−1/2t)O(N^{1-1/2t})O(N1−1/2t)-query randomized algorithm. Thus, resolving an open question of Buhrman et al. [ SIAM J. Comput., 37 (2008), pp. 1387--1400] from 2002, there is no partial Boolean function whose quantum query complexity is constant and whose randomized query complexity is linear. We conjecture that a natural generalization of Forrelation achieves the optimal ttt versus Ω(N1−1/2t)\Omega(N^{1-1/2t})Ω(N1−1/2t) separation for all ttt. As a bonus, we show that this generalization is BQP{BQP}BQP-complete. This yields what is arguably the simplest BQP{BQP}BQP-complete problem yet known and gives a second sense in which Forrelation “captures the maximum power of quantum computation.”
In 1986, Saks and Wigderson conjectured that the largest separation between deterministic and zero-error randomized query complexity for a total boolean function is given by the function f on n=2k bits defined by a complete binary tree of NAND gates of depth k, which achieves R0(f) = O(D(f)0.7537…). We show this is false by giving an example of a total boolean function f on n bits whose deterministic query complexity is Ω(n/log(n)) while its zero-error randomized query complexity is Õ(√n). We further show that the quantum query complexity of the same function is Õ(n1/4), giving the first example of a total function with a super-quadratic gap between its quantum and deterministic query complexities.
In the paper, we consider the problem of searching for the Largest empty rectangle in a 2D map, and the one-dimensional version of the problem is the problem of searching for the largest empty segment. We present a quantum algorithm for the Largest Empty Square problem and the Largest Empty Rectangle of a fixed width ddd for n×nn\times nn×n-rectangular map. Query complexity of the algorithm is O~(n1.5)\tilde{O}(n^{1.5})O~(n1.5) for the square case, and O~(nd)\tilde{O}(n\sqrt{d})O~(nd​) for the rectangle with a fixed width ddd case, respectively. At the same time, the lower bounds for the classical case are Ω(n2)Ω(n^2)Ω(n2), and Ω(nd)Ω(nd)Ω(nd), respectively. The Quantum algorithm for the one-dimensional version of the problem has O(nlog⁡nlog⁡log⁡n)O(\sqrt{n}\log n\log\log n)O(n​lognloglogn) query complexity. The quantum lower bound for the problem is Ω(n)Ω(\sqrt{n})Ω(n​) which is almost equal to the upper bound up to a log factor. The classical lower bound is Ω(n)Ω(n)Ω(n). So, we obtain the quadratic speed-up for the problem.