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arXiv:quant-ph/0111102

Quantum Lower Bound for the Collision Problem

Scott Aaronson

Published Nov 20, 2001• 0 citations
arXivHTMLPDF

Abstract

The collision problem is to decide whether a function X:{1,..,n}->{1,..,n} is one-to-one or two-to-one, given that one of these is the case. We show a lower bound of Theta(n^{1/5}) on the number of queries needed by a quantum computer to solve this problem with bounded error probability. The best known upper bound is O(n^{1/3}), but obtaining any lower bound better than Theta(1) was an open problem since 1997. Our proof uses the polynomial method augmented by some new ideas. We also give a lower bound of Theta(n^{1/7}) for the problem of deciding whether two sets are equal or disjoint on a constant fraction of elements. Finally we give implications of these results for quantum complexity theory.

DOI
10.48550/arxiv.quant-ph/0111102

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The collision problem is to decide whether a function X:{1,..,n}->{1,..,n} is one-to-one or two-to-one, given that one of these is the case. We show a lower bound of Theta(n^{1/5}) on the number of queries needed by a quantum computer to solve this problem with bounded error probability. The best known upper bound is O(n^{1/3}), but obtaining any lower bound better than Theta(1) was an open problem since 1997. Our proof uses the polynomial method augmented by some new ideas. We also give a lower bound of Theta(n^{1/7}) for the problem of deciding whether two sets are equal or disjoint on a constant fraction of elements. Finally we give implications of these results for quantum complexity theory.
(MATH) The collision problem is to decide whether a function X: { 1,…,n} → { 1, …,n} is one-to-one or two-to-one, given that one of these is the case. We show a lower bound of Ω(n1/5) on the number of queries needed by a quantum computer to solve this problem with bounded error probability. The best known upper bound is O(n1/3), but obtaining any lower bound better than Ω(1) was an open problem since 1997. Our proof uses the polynomial method augmented by some new ideas. We also give a lower bound of Ω(n1/7) for the problem of deciding whether two sets are equal or disjoint on a constant fraction of elements. Finally we give implications of these results for quantum complexity theory.
(MATH) The collision problem is to decide whether a function X: { 1,…,n} → { 1, …,n} is one-to-one or two-to-one, given that one of these is the case. We show a lower bound of Ω(n1/5) on the number of queries needed by a quantum computer to solve this problem with bounded error probability. The best known upper bound is O(n1/3), but obtaining any lower bound better than Ω(1) was an open problem since 1997. Our proof uses the polynomial method augmented by some new ideas. We also give a lower bound of Ω(n1/7) for the problem of deciding whether two sets are equal or disjoint on a constant fraction of elements. Finally we give implications of these results for quantum complexity theory.
Given a function f as an oracle, the collision problem is to find two distinct indexes i and j such that f ( i ) = f ( j ), under the promise that such indexes exist. Since the security of many fundamental cryptographic primitives depends on the hardness of finding collisions, our lower bounds provide evidence for the existence of cryptographic primitives that are immune to quantum cryptanalysis. We prove that any quantum algorithm for finding a collision in an r -to-one function must evaluate the function Ω(( n / r ) 1/3 ) times, where n is the size of the domain and r | n . This matches an upper bound of Brassard, Høyer, and Tapp. No lower bound better than constant was previously known. Our result also implies a quantum lower bound of Ω( n 2/3 ) queries for the element distinctness problem, which is to determine whether n integers are all distinct. The best previous lower bound was Ω(√ n ) queries.
Given a function f as an oracle, the collision problem is to find two distinct inputs i and j such that f(i)=f(j), under the promise that such inputs exist. In this paper, we prove that any quantum algorithm for finding a collision in an r-to-one function must evaluate the function /spl Omega/ ((n/r)/sup 1/3/) times, where n is the size of the domain and r|n. This lower bound matches, up to a constant factor, the upper bound of Brassard, Hoyer and Tapp (1997), which uses the quantum algorithm of Grover (1996) in a novel way. The previously best quantum lower bound is /spl Omega/ ((n/r)/sup 1/5/) evaluations, due to Aaronson (2002). Our result implies a quantum lower bound of /spl Omega/ (n/sup 2/3/) queries to the inputs for another well studied problem, the element distinctness problem, which is to determine whether or not the given n real numbers are distinct. The previous best lower bound is /spl Omega/ (/spl radic/n) queries in the black-box model; and /spl Omega/ (/spl radic/n log n) comparisons in the comparisons-only model, due to Hoyer Neerbek, and Shi (2001).
Abstract Collision resistance is one of the most fundamental properties in cryptography. With the development of quantum computing, significant attention has been directed toward understanding the quantum query complexity of collision-finding problems in hash functions. The quantum query complexity of collision-finding in general non-uniform random functions remained an open problem until the recent work of Peng et al. (ASIACRYPT 2025), who nearly resolved it by introducing a novel parameter γ\gammaγ γ . Based on this parameter, they established an upper bound of O(γ1/6)O(\gamma ^{1/6})O(γ1/6) O ( γ 1 / 6 ) and a matching lower bound of Ω~(γ1/6)\tilde{\Omega }(\gamma ^{1/6})Ω~(γ1/6) Ω ~ ( γ 1 / 6 ) . However, the quantum query complexity of finding multi-collisions in non-uniform random functions has remained open. A s -collision to a function f is a set of distinct input x1,…,xsx_1,\dots , x_sx1​,…,xs​ x 1 , ⋯ , x s such that f(x1)=f(x2)⋯=f(xs)f(x_1)=f(x_2)\dots =f(x_s)f(x1​)=f(x2​)⋯=f(xs​) f ( x 1 ) = f ( x 2 ) ⋯ = f ( x s ) . In this work, we address this challenge by similarly introducing a new generalized parameter γs\gamma _sγs​ γ s . Based on this parameter, we establish nearly tight bounds—an upper bound of O(γs)O(\gamma _s)O(γs​) O ( γ s ) and a lower bound of Ω~(γs)\tilde{\Omega }(\gamma _s)Ω~(γs​) Ω ~ ( γ s ) —thereby nearly resolving this open problem. Moreover, although the existing results for 2-collisions do not generalize straightforwardly to the case of s -collision ( s>2s>2s>2 s > 2 ), we demonstrate that the result of Peng et al. can be viewed as a special case of our more general framework. This clearly establishes our work as a direct generalization of their contribution.
A collision for a function fff is two distinct inputs x1≠x2x_1\neq x_2x1​=x2​ such that fff outputs the same value on both inputs: f(x1)=f(x2)f(x_1)=f(x_2)f(x1​)=f(x2​). The quantum query complexity of finding collisions has been shown~\cite{BHT1997,AS2004, Ambainis05, Kutin05} in some settings to be Θ(N1/3)\Theta(N^{1/3})Θ(N1/3); however, these results do not apply to random functions. The issues are two-fold. First, the Ω(N1/3)\Omega(N^{1/3})Ω(N1/3) lower bound only applies when the domain is no larger than the co-domain, which precludes many of the cryptographically interesting applications. Second, most of the results in the literature only apply to rrr-to-1 functions, which are quite different from random functions. Understanding the collision problem for random functions is of great importance to cryptography, and we seek to fill the gaps of knowledge for this problem. To that end, we prove that, as expected, a quantum query complexity of Θ(N1/3)\Theta(N^{1/3})Θ(N1/3) holds for all interesting domain and co-domain sizes. Our proofs are simple, and combine existing techniques with several novel tricks to obtain the desired results. Using our techniques, we also give an optimal Ω(M1/3)\Omega(M^{1/3})Ω(M1/3) lower bound for the set equality problem. This lower bound can be used to improve the relationship between classical randomized query complexity and quantum query complexity for so-called permutation-symmetric functions.