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arXiv:2201.13450

An efficient quantum algorithm for lattice problems achieving subexponential approximation factor

Lior Eldar, Sean Hallgren

Published Jan 31, 2022• 2 citations
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Abstract

We give a quantum algorithm for solving the Bounded Distance Decoding (BDD) problem with a subexponential approximation factor on a class of integer lattices. The quantum algorithm uses a well-known but challenging-to-use quantum state on lattices as a type of approximate quantum eigenvector to randomly self-reduce the BDD instance to a random BDD instance which is solvable classically. The running time of the quantum algorithm is polynomial for one range of approximation factors and subexponential time for a second range of approximation factors. The subclass of lattices we study has a natural description in terms of the lattice's periodicity and finite abelian group rank. This view makes for a clean quantum algorithm in terms of finite abelian groups, uses very relatively little from lattice theory, and suggests exploring approximation algorithms for lattice problems in parameters other than dimension alone. A talk on this paper sparked many lively discussions and resulted in a new classical algorithm matching part of our result. We leave it as a challenge to give a classcial algorithm matching the general case.

DOI
10.48550/arxiv.2201.13450

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We give a quantum algorithm for solving the Bounded Distance Decoding (BDD) problem with a subexponential approximation factor on a class of integer lattices. The quantum algorithm uses a well-known but challenging-to-use quantum state on lattices as a type of approximate quantum eigenvector to randomly self-reduce the BDD instance to a random BDD instance which is solvable classically. The running time of the quantum algorithm is polynomial for one range of approximation factors and subexponential time for a second range of approximation factors. The subclass of lattices we study has a natural description in terms of the lattice's periodicity and finite abelian group rank. This view makes for a clean quantum algorithm in terms of finite abelian groups, uses very relatively little from lattice theory, and suggests exploring approximation algorithms for lattice problems in parameters other than dimension alone. A talk on this paper sparked many lively discussions and resulted in a new classical algorithm matching part of our result. We leave it as a challenge to give a classcial algorithm matching the general case.
In this paper, we provide a comprehensive overview of a recent debate over the quantum versus classical solvability of bounded distance decoding (BDD). Specifically, we review the work of Eldar and Hallgren [EH22], [Hal21] demonstrating a quantum algorithm solving λ12−Ω(klog⁡q)λ_1 2^{-Ω(\sqrt{k \log q})}λ1​2−Ω(klogq​)-BDD in polynomial time for lattices of periodicity qqq, finite group rank kkk, and shortest lattice vector length λ1λ_1λ1​. Subsequently, we prove the results of [DvW21a], [DvW21b] with far greater detail and elaboration than in the original work. Namely, we show that there exists a deterministic, classical algorithm achieving the same result.
The most important computational problem on lattices is the Shortest Vector Problem (SVP). In this paper, we present new algorithms that improve the state-of-the-art for provable classical/quantum algorithms for SVP. We present the following results. ∙\bullet∙ A new algorithm for SVP that provides a smooth tradeoff between time complexity and memory requirement. For any positive integer 4≤q≤n4\leq q\leq \sqrt{n}4≤q≤n​, our algorithm takes q13n+o(n)q^{13n+o(n)}q13n+o(n) time and requires poly(n)⋅q16n/q2poly(n)\cdot q^{16n/q^2}poly(n)⋅q16n/q2 memory. This tradeoff which ranges from enumeration (q=nq=\sqrt{n}q=n​) to sieving (qqq constant), is a consequence of a new time-memory tradeoff for Discrete Gaussian sampling above the smoothing parameter. ∙\bullet∙ A quantum algorithm for SVP that runs in time 20.950n+o(n)2^{0.950n+o(n)}20.950n+o(n) and requires 20.5n+o(n)2^{0.5n+o(n)}20.5n+o(n) classical memory and poly(n) qubits. In Quantum Random Access Memory (QRAM) model this algorithm takes only 20.835n+o(n)2^{0.835n+o(n)}20.835n+o(n) time and requires a QRAM of size 20.293n+o(n)2^{0.293n+o(n)}20.293n+o(n), poly(n) qubits and 20.5n2^{0.5n}20.5n classical space. This improves over the previously fastest classical (which is also the fastest quantum) algorithm due to [ADRS15] that has a time and space complexity 2n+o(n)2^{n+o(n)}2n+o(n). ∙\bullet∙ A classical algorithm for SVP that runs in time 21.669n+o(n)2^{1.669n+o(n)}21.669n+o(n) time and 20.5n+o(n)2^{0.5n+o(n)}20.5n+o(n) space. This improves over an algorithm of [CCL18] that has the same space complexity. The time complexity of our classical and quantum algorithms are obtained using a known upper bound on a quantity related to the lattice kissing number which is 20.402n2^{0.402n}20.402n. We conjecture that for most lattices this quantity is a 2o(n)2^{o(n)}2o(n). Assuming that this is the case, our classical algorithm runs in time 21.292n+o(n)2^{1.292n+o(n)}21.292n+o(n), our quantum algorithm runs in time 20.750n+o(n)2^{0.750n+o(n)}20.750n+o(n) and our quantum algorithm in QRAM model runs in time 20.667n+o(n)2^{0.667n+o(n)}20.667n+o(n).
Decomposing finite Abelian black-box groups into cyclic factors is a basic problem in quantum computation. We give a quantum algorithm for decomposing finite Abelian black-box groups by adapting the quantum sampling and classical lattice-reduction method of Regev's factoring algorithm. The algorithm computes an invariant-factor decomposition and corresponding cyclic generators with high probability. For a group G of order at most 2^n with unique encodings and reversible group-operation cost T_op = Omega(sqrt(n)), our algorithm uses O(sqrt(n)) quantum circuits, each with O~(n T_op) gates and executed at most O(n) times. For comparison, we consider the Cheung-Mosca algorithm, which decomposes the Sylow p-subgroups separately. We also consider the common-modulus implementation of the extended Cheung-Mosca algorithm. Our algorithm reduces the sum of the circuit gate counts from O~(n^2 T_op) to O~(n^(3/2) T_op). The total quantum time bound reduces from O~(n^3 T_op) to O~(n^(5/2) T_op), and the quantum space bound reduces from O(n^2) to O(n) qubits. The classical computation uses polynomially many bit operations and group-operation queries. These improvements rely on two technical ingredients. We prove that the integer relation lattices used in our algorithm admit, with high probability, integral bases whose vectors have Euclidean norm at most exp(O(sqrt(n))). We preserve the circuit-size advantage of Regev's algorithm for group decomposition by incorporating all O(n) sampled generators while keeping the lattice-reduction dimension at O(sqrt(n)).
Abstract. The most important computational problem on lattices is the shortest vector problem ([Formula: see text]). In this paper, we present new algorithms that improve the state-of-the-art for provable classical/quantum algorithms for [Formula: see text]. We present the following results: (1) A new algorithm for [Formula: see text] that provides a smooth tradeoff between time complexity and memory requirement. For any positive integer [Formula: see text], our algorithm takes [Formula: see text] time and requires [Formula: see text] memory. This tradeoff, which ranges from enumeration ([Formula: see text]) to sieving ([Formula: see text] constant), is a consequence of a new time-memory tradeoff for discrete Gaussian sampling above the smoothing parameter. (2) A quantum algorithm for [Formula: see text] that runs in time [Formula: see text] and requires [Formula: see text] classical memory and [Formula: see text] qubits. In a quantum random access memory (QRAM) model, this algorithm takes only [Formula: see text] time and requires a QRAM of size [Formula: see text], [Formula: see text] qubits and [Formula: see text] classical space. This improves over the previously fastest classical (which is also the fastest quantum) algorithm due to [D. Aggarwal et al., Solving the shortest vector problem in 2 n time using discrete Gaussian sampling: Extended abstract, in Proceedings of the Forty-Seventh Annual ACM on Symposium on Theory of Computing (STOC), 2015, pp. 733–742] that has a time and space complexity [Formula: see text]. (3) A classical algorithm for [Formula: see text] that runs in time [Formula: see text] time and [Formula: see text] space. This improves over an algorithm of [Y. Chen, K. Chung, and C. Lai, Quantum Inf. Comput., 18 (2018), pp. 285–306] that has the same space complexity. The time complexity of our classical and quantum algorithms are obtained using a known upper bound on a quantity related to the lattice kissing number, which is [Formula: see text]. We conjecture that for most lattices this quantity is a [Formula: see text]. Assuming that this is the case, our classical algorithm runs in time [Formula: see text], our quantum algorithm runs in time [Formula: see text], and our quantum algorithm in a QRAM model runs in time [Formula: see text]. As a direct application of our result, using the reduction in [L. Ducas, Des. Codes. Cryptogr., 92 (2024), pp. 909–916], we obtain a provable quantum algorithm for the lattice isomorphism problem in the case of the trivial lattice [Formula: see text] ([Formula: see text] LIP ) that runs in time [Formula: see text]. Our algorithm requires a QRAM of size [Formula: see text], [Formula: see text] qubits and [Formula: see text] classical space.
The most important computational problem on lattices is the Shortest Vector Problem (SVP). In this paper, we present new algorithms that improve the state-of-the-art for provable classical/quantum algorithms for SVP. We present the following results. 1) A new algorithm for SVP that provides a smooth tradeoff between time complexity and memory requirement. For any positive integer 4 ≤ q ≤ √n, our algorithm takes q^{13n+o(n)} time and requires poly(n)⋅ q^{16n/q²} memory. This tradeoff which ranges from enumeration (q = √n) to sieving (q constant), is a consequence of a new time-memory tradeoff for Discrete Gaussian sampling above the smoothing parameter. 2) A quantum algorithm that runs in time 2^{0.9533n+o(n)} and requires 2^{0.5n+o(n)} classical memory and poly(n) qubits. This improves over the previously fastest classical (which is also the fastest quantum) algorithm due to [Divesh Aggarwal et al., 2015] that has a time and space complexity 2^{n+o(n)}. 3) A classical algorithm for SVP that runs in time 2^{1.741n+o(n)} time and 2^{0.5n+o(n)} space. This improves over an algorithm of [Yanlin Chen et al., 2018] that has the same space complexity. The time complexity of our classical and quantum algorithms are expressed using a quantity related to the kissing number of a lattice. A known upper bound of this quantity is 2^{0.402n}, but in practice for most lattices, it can be much smaller and even 2^o(n). In that case, our classical algorithm runs in time 2^{1.292n} and our quantum algorithm runs in time 2^{0.750n}.
We give efficient quantum algorithms for the problems of Hidden Translation and Hidden Subgroup in a large class of nonabelian solvable groups, including solvable groups of constant exponent and of constant length derived series. Our algorithms are recursive. For the base case, we solve efficiently Hidden Translation in Zn p, whenever p is a fixed prime. For the induction step, we introduce the problem Translating Coset generalizing both Hidden Translation and Hidden Subgroup and prove a powerful self-reducibility result: Translating Coset in a finite solvable group G is reducible to instances of Translating Coset in G/N and N, for appropriate normal subgroups N of G. Our self-reducibility framework, combined with Kuperberg’s subexponential quantum algorithm for solving Hidden Translation in any abelian group, leads to subexponential quantum algorithms for Hidden Translation and Hidden Subgroup in any solvable group.