Quantum Reverse Shannon Theorem Simplified

📅 2025-10-06
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🤖 AI Summary
This work addresses the one-shot resource cost of quantum channel simulation under the assumption of freely shared entanglement. To overcome limitations of existing approaches—namely, reliance on post-selection, technical complexity, and loose bounds—we introduce an additive upper bound based on the sandwiched Rényi mutual information, yielding the first post-selection-free proof with greater conceptual simplicity and technical directness. Building upon this, we further integrate smooth max-mutual information with the quantum information spectrum method to derive a non-asymptotic, universal bound. Our results substantially improve the one-shot quantum reverse Shannon theorem’s resource bounds, unify and simplify multiple prior frameworks, and enhance theoretical precision, applicability across channel classes, and interpretability of the underlying resource trade-offs.

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📝 Abstract
We revisit the quantum reverse Shannon theorem, a central result in quantum information theory that characterizes the resources needed to simulate quantum channels when entanglement is freely available. We derive a universal additive upper bound on the smoothed max-information in terms of the sandwiched Rényi mutual information. This bound yields tighter single-shot results, eliminates the need for the post-selection technique, and leads to a conceptually simpler proof of the quantum reverse Shannon theorem. By consolidating and streamlining earlier approaches, our result provides a clearer and more direct understanding of the resource costs of simulating quantum channels.
Problem

Research questions and friction points this paper is trying to address.

Simplifying the quantum reverse Shannon theorem proof
Establishing universal additive bounds for max-information
Characterizing resource costs for quantum channel simulation
Innovation

Methods, ideas, or system contributions that make the work stand out.

Universal additive bound on smoothed max-information
Eliminates need for post-selection technique
Simplifies proof of quantum reverse Shannon theorem
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