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arXiv:2603.13654v1 Announce Type: new Abstract: Modern cryptography relies on keyed symmetric ciphers to ensure the secrecy and authenticity of high bandwidth data transfer. While the advent of quantum computers poses a challenge for public key cryptography, unbroken ciphers are considered safe against quantum attacks if their key is sufficiently long. However, concrete bounds on the required key length thus far remain elusive: Despite the well known asymptotic complexity of Grover's quantum sea
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Quantum Physics
[Submitted on 13 Mar 2026]
Thermodynamic Limits of Quantum Search
Ralf Riedinger
Modern cryptography relies on keyed symmetric ciphers to ensure the secrecy and authenticity of high bandwidth data transfer. While the advent of quantum computers poses a challenge for public key cryptography, unbroken ciphers are considered safe against quantum attacks if their key is sufficiently long. However, concrete bounds on the required key length thus far remain elusive: Despite the well known asymptotic complexity of Grover's quantum search, the optimal algorithm to recover a secret key, no implementation-agnostic tight bounds were established. Here, we discuss the quantum thermodynamic limits of generic search algorithms, and find a work-runtime trade-off for autonomous computers with a fundamental lower bound. By devising an application-specific quantum protocol, which outperforms circuit and adiabatic implementations, and saturates this bound, we demonstrate that it is tight. Applying this limit, we find that a secret key of 831 bit length cannot be reconstructed deterministically in an expanding, dark-energy-dominated universe until star formation is expected to cease. Implications for post quantum cryptography, and quantum key distribution are discussed.
Subjects: Quantum Physics (quant-ph)
Cite as: arXiv:2603.13654 [quant-ph]
(or arXiv:2603.13654v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2603.13654
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Submission history
From: Ralf Riedinger [view email]
[v1] Fri, 13 Mar 2026 23:30:35 UTC (34 KB)
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