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arXiv:0910.4952

Quantum Leader Election

Maor Ganz

Published Oct 26, 2009• 8 citations
arXivHTMLPDF

Abstract

Leader election between n parties is known to be impossible classically. This work gives a simple algorithm that does it, based on the weak coin flipping protocol with arbitrarily small bias derived by Mochon in 2007, and recently published and simplified in Aharonov et al in 2016. A protocol with linear number of coin flipping rounds is quite simple to achieve; We further provide an improvement to logarithmic number of coin flipping rounds. This is a much improved journal version of a preprint posted in 2009: many typos are corrected, proofs are more rigorous and accurate, and the analysis of complexity is significantly tightened which gives a stronger result in terms of efficiency; The first protocol with linear number of rounds, was achieved independently also by Aharon and Silman in 2010.

DOI
10.48550/arxiv.0910.4952

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Leader election between n parties is known to be impossible classically. This work gives a simple algorithm that does it, based on the weak coin flipping protocol with arbitrarily small bias derived by Mochon in 2007, and recently published and simplified in Aharonov et al in 2016. A protocol with linear number of coin flipping rounds is quite simple to achieve; We further provide an improvement to logarithmic number of coin flipping rounds. This is a much improved journal version of a preprint posted in 2009: many typos are corrected, proofs are more rigorous and accurate, and the analysis of complexity is significantly tightened which gives a stronger result in terms of efficiency; The first protocol with linear number of rounds, was achieved independently also by Aharon and Silman in 2010.
Mochon's proof [Quantum Weak Coin Flipping with Arbitrarily Small Bias, preprint, arXiv:0711.4114, 2007] of the existence of quantum weak coin flipping with arbitrarily small bias is a fundamental result in quantum cryptography, but at the same time one of the least understood. Though used several times as a black box in important follow-up results [M. Ganz, Quantum Leader Election, preprint, arXiv:0910.4952, 2009; A. Chailloux and I. Kerenidis, in Proceedings of the 50th Annual IEEE Symposium on Foundations of Computer Science, IEEE Computer Society, Los Alamitos, CA, 2009, pp. 527--533; N. Aharon and J. Silman, New J. Phys., 12 (2010), 033027; A. Chailloux and I. Kerenidis, in Proceedings of the 52nd Annual IEEE Symposium on Foundations of Computer Science, IEEE Computer Society, Los Alamitos, CA, 2011; I. Kerenidis and S. Zhang, in Theory of Quantum Computation, Communication, and Cryptography, Lecture Notes in Computer Science 7582, Springer, Berlin, 2013, pp. 13--28], the result has not been peer reviewed, its novel techniques (and, in particular, Kitaev's point game formalism) have not been applied anywhere else, and an explicit protocol is missing. We believe that truly understanding the existence proof and the novel techniques it relies on would constitute a major step in quantum information theory, leading to deeper understanding of entanglement and of quantum protocols in general. In this work, we make a first step in this direction. We simplify parts of Mochon's construction considerably, making about 202020 pages of analysis in the original proof superfluous, clarifying some other parts of the proof on the way, and presenting the proof in a way which is conceptually easier to grasp. We believe the resulting proof of existence is easier to understand, more readable, and certainly verifiable. Moreover, we analyze the resources neededto achieve a bias ε\varepsilonε and show that the number of qubits is O(log⁡1ε)O(\log \frac{1}{\varepsilon})O(logε1​), while the number of rounds is (1ε)O(1ε)(\frac{1}{\varepsilon})^{O(\frac{1}{\varepsilon})}(ε1​)O(ε1​). A true understanding of the proof, including Kitaev's point-game techniques and their applicability, as well as completing the task of constructing an explicit (and also simpler and more efficient) protocol, are left to future work.
The anonymous network model was introduced by Angluin in (STOC '80, pages 82-93) to understand the fundamental properties of distributed computing by examining how much each party in a network needs to know about its own identity and the identities of other parties. In this model, all parties with the same number of communication links are identical. When studying the model, the problem of electing a unique leader is the central problem in the sense that once a unique leader is elected, he can assign a unique identity to each party. It was proved in the literature, however, that it is impossible to deterministically solve the leader election problem with any finite amount of communication. This contrasts sharply with the situation in the quantum setting: the present authors gave quantum algorithms that exactly solve the problem on anonymous quantum networks, where quantum communication and computation can be performed (TOCT, vol.4, no.1, article 1). The core of their algorithm consists of somewhat tricky unitary operators, which eliminate the possibility of ties during (quantum) coin flipping and thereby reduce the number of leader candidates with certainty. This paper presents a new quantum leader election algorithm that is based on quantum reduction via exact amplitude amplification to a classically solvable problem, computing a certain symmetric function, which provides more intuitive reasoning behind the existence of exact quantum algorithms for leader election. The algorithm first achieves a round complexity that is linear in the number of parties, i.e., the largest possible diameter plus one of the underlying graph of the network.
Coin-flipping is a fundamental task in two-party cryptography where two remote mistrustful parties wish to generate a shared uniformly random bit. While quantum protocols promising near-perfect security exist for weak coin-flipping -- when the parties want opposing outcomes -- it has been shown that they must be inefficient in terms of their round complexity, and it is an open question of how space efficient they can be. In this work, we consider a variant called cheat-penalised weak coin-flipping in which if a party gets caught cheating, they lose ΛΛΛ points (compared to 000 in the standard definition). We find that already for a small cheating penalty, the landscape of coin-flipping changes dramatically. For example, with Λ=0.01Λ=0.01Λ=0.01, we exhibit a protocol where neither Alice nor Bob can bias the result in their favour beyond 1/2+10−81/2 + 10^{-8}1/2+10−8, which uses 242424 qubits and 101610^{16}1016 rounds of communication (provably 10710^{7}107 times better than any weak coin-flipping protocol with matching security). For the same space requirements, we demonstrate how one can choose between lowering how much a malicious party can bias the result (down to 1/2+10−101/2 + 10^{-10}1/2+10−10) and reducing the rounds of communication (down to 25,18025,18025,180), depending on what is preferred. To find these protocols, we make two technical contributions. First, we extend the point game-protocol correspondence introduced by Kitaev and Mochon, to incorporate: (i) approximate point games, (ii) the cheat-penalised setting, and (iii) round and space complexity. Second, we give the first (to the best of our knowledge) numerical algorithm for constructing (approximate) point games that correspond to high security and low complexity. Our results open up the possibility of having secure and practical quantum protocols for multiparty computation.
Weak coin flipping is an important cryptographic primitive$\unicode{x2013}$it is the strongest known secure two-party computation primitive that classically becomes secure only under certain assumptions (e.g. computational hardness), while quantumly there exist protocols that achieve arbitrarily close to perfect security. This breakthrough result was established by Mochon in 2007 [arXiv:0711.4114]. However, his proof relied on the existence of certain unitary operators which was established by a non-constructive argument. Consequently, explicit protocols have remained elusive. In this work, we give exact constructions of related unitary operators. These, together with a new formalism, yield a family of protocols approaching perfect security thereby also simplifying Mochon's proof of existence. We illustrate the construction of explicit weak coin flipping protocols by considering concrete examples (from the aforementioned family of protocols) that are more secure than all previously known protocols. 76 pages. This is the TheoretiCS journal version
The anonymous network model was introduced by Angluin in [STOC '80, to understand the fundamental properties of distributed computing by examining how much each party in a network needs to know about its own identity and the identities of other parties.In this model, all parties with the same number of communication links are identical.When studying the model, the problem of electing a unique leader is the central problem in the sense that once a unique leader is elected, he can assign a unique identity to each party.It was proved in the literature, however, that it is impossible to deterministically solve the leader election problem with any finite amount of communication.This contrasts sharply with the situation in the quantum setting: the present authors gave quantum algorithms that exactly solve the problem on anonymous quantum networks, where quantum communication and computation can be performed [TOCT, vol.4,no.1, article 1].The core of their algorithm consists of somewhat tricky unitary operators, which eliminate the possibility of ties during (quantum) coin flipping and thereby reduce the number of leader candidates with certainty.This paper presents a new quantum leader election algorithm that is based on quantum reduction via exact amplitude amplification to a classically solvable problem, computing a certain symmetric function, which provides more intuitive reasoning behind the existence of exact quantum algorithms for leader election.The algorithm first achieves a round complexity that is linear in the number of parties, i.e., the largest possible diameter plus one of the underlying graph of the network.
How can two parties with competing interests carry out a fair coin flip across a quantum communication channel? This problem (quantum weak coin-flipping) was formalized more than 15 years ago, and, despite some phenomenal theoretical progress, practical quantum coin-flipping protocols with vanishing bias have proved hard to find. In the current work we show that there is a reason that practical weak quantum coin-flipping is difficult: any quantum weak coin-flipping protocol with bias є must use at least exp( Ω (1/√є )) rounds of communication. This is a large improvement over the previous best known lower bound of Ω ( log log(1/є )) due to Ambainis from 2004. Our proof is based on a theoretical construction (the two-variable profile function) which may find further applications.