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No second law of entanglement manipulation after all

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arxiv 2111.02438 v3 pith:5PSQPCPQ submitted 2021-11-03 quant-ph cond-mat.stat-mechmath-phmath.MP

classification quant-phcond-mat.stat-mechmath-phmath.MP
keywords entanglementthermodynamicstransformationsquantumsecondmanipulationonlytheory
verification ladder T0 review T1 audit T2 compute T3 formal
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Many fruitful analogies have emerged between the theories of quantum entanglement and thermodynamics, motivating the pursuit of an axiomatic description of entanglement akin to the laws of thermodynamics. A long-standing open problem has been to establish a true second law of entanglement, and in particular a unique function which governs all transformations between entangled systems, mirroring the role of entropy in thermodynamics. Contrary to previous promising evidence, here we show that this is impossible, and no direct counterpart to the second law of thermodynamics can be established. This is accomplished by demonstrating the irreversibility of entanglement theory from first principles -- assuming only the most general microscopic physical constraints of entanglement manipulation, we show that entanglement theory is irreversible under all non-entangling transformations. We furthermore rule out reversibility without significant entanglement expenditure, showing that reversible entanglement transformations require the generation of macroscopically large amounts of entanglement according to certain measures. Our results not only reveal fundamental differences between quantum entanglement transformations and thermodynamic processes, but also showcase a unique property of entanglement which distinguishes it from other known quantum resources.

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Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Very Strong Irreversibility of Quantum Entanglement

    quant-ph 2026-07 accept novelty 7.0 of 10

    Exponential strong-converse distillable entanglement is strictly smaller than exponential strong-converse cost for explicit mixed states under non-entangling and completely PPT-preserving operations.

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