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This paper establishes the thermodynamic geometry of conditional control, demonstrating that advantages in quantum information processing are determined by geometric pairings between spectral rearrangement vectors and Hamiltonian energy gaps rather than standard informational quantities alone. The work provides a rigorous framework for understanding how ensembles with identical Holevo information can exhibit distinct thermodynamic values based on their specific structural configurations within the system's Hamiltonian.
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The Thermodynamic Geometry of Conditional Control

arXiv2 min read

arXiv:2607.19177v1 Announce Type: new Abstract: Information is widely regarded as the resource underlying the thermodynamic advantages enabled by conditional control. We show, however, that informational quantities such as Holevo information and accessible distinguishability, although constraining the achievable advantage, do not uniquely determine its thermodynamic value. The missing ingredient is a passive spectral rearrangement vector that characterizes the effect of conditioning on the ensemble. Specifically, the conditional-control advantage is exactly determined by the geometric pairing between this vector and the Hamiltonian energy-gap structure. This result reveals a thermodynamic geometry of conditional control, explains how informationally equivalent ensembles can possess different thermodynamic values, and identifies the passive spectral rearrangement vector as the minimal operational descriptor required to determine the thermodynamic value of conditional control for a fixed Hamiltonian.

Abstract:Information is widely regarded as the resource underlying the thermodynamic advantages enabled by conditional control. We show, however, that informational quantities such as Holevo information and accessible distinguishability, although constraining the achievable advantage, do not uniquely determine its thermodynamic value. The missing ingredient is a passive spectral rearrangement vector that characterizes the effect of conditioning on the ensemble. Specifically, the conditional-control advantage is exactly determined by the geometric pairing between this vector and the Hamiltonian energy-gap structure. This result reveals a thermodynamic geometry of conditional control, explains how informationally equivalent ensembles can possess different thermodynamic values, and identifies the passive spectral rearrangement vector as the minimal operational descriptor required to determine the thermodynamic value of conditional control for a fixed Hamiltonian.

arXiv:2607.19177 [quant-ph]

(or arXiv:2607.19177v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2607.19177 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 212 words

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