Quantum Byzantine Agreement Against Full-information Adversary
September 03, 2024 Β· Declared Dead Β· π International Symposium on Distributed Computing
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Authors
Longcheng Li, Xiaoming Sun, Jiadong Zhu
arXiv ID
2409.01707
Category
quant-ph: Quantum Computing
Cross-listed
cs.DC
Citations
3
Venue
International Symposium on Distributed Computing
Last Checked
5 months ago
Abstract
We exhibit that, when given a classical Byzantine agreement protocol designed in the private-channel model, it is feasible to construct a quantum agreement protocol that can effectively handle a full-information adversary. Notably, both protocols have equivalent levels of resilience, round complexity, and communication complexity. In the classical private-channel scenario, participating players are limited to exchanging classical bits, with the adversary lacking knowledge of the exchanged messages. In contrast, in the quantum full-information setting, participating players can exchange qubits, while the adversary possesses comprehensive and accurate visibility into the system's state and messages. By showcasing the reduction from quantum to classical frameworks, this paper demonstrates the strength and flexibility of quantum protocols in addressing security challenges posed by adversaries with increased visibility. It underscores the potential of leveraging quantum principles to improve security measures without compromising on efficiency or resilience. By applying our reduction, we demonstrate quantum advantages in the round complexity of asynchronous Byzantine agreement protocols in the full-information model. It is well known that in the full-information model, any classical protocol requires $Ξ©(n)$ rounds to solve Byzantine agreement with probability one even against Fail-stop adversary when resilience $t=Ξ(n)$. We show that quantum protocols can achieve $O(1)$ rounds (i) with resilience $t<n/2$ against a Fail-stop adversary, and (ii) with resilience $t<n/(3+Ξ΅)$ against a Byzantine adversary for any constant $Ξ΅>0$, therefore surpassing the classical lower bound.
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