Equivalence of states and bimodule quantum channels
Abstract
We study the action of quantum channels on states on a von Neumann algebra ℳ with conserved quantities encoded by a subalgebra 𝒩. We define a phase as an equivalence class of normal states on ℳ under the action of quantum channels preserving 𝒩. First, we establish a relative quasi-entropic characterization of phase equivalence using the Petz recovery map. We further introduce the operator algebra (OA) symmetry of a state and define an equivalence relation between OA symmetries via bishifts of biprojections. When 𝒩⊆ℳ is an irreducible finite-index subfactor of type II1, we prove that phase equivalence implies OA symmetry equivalence. Consequently, OA symmetry breaking provides a sufficient mechanism for detecting phase transitions. Furthermore, combining finite-index subfactor theory with quantum Fourier analysis, we prove that the cardinality of each phase is finite and obtain an explicit upper bound depending only on the Jones index.
Related
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- Quantum-State Oblivious Transfer over Quantum Erasure Channels
BibTeX
@misc{huang2026equivalence,
title = {{Equivalence of states and bimodule quantum channels}},
author = {Linzhe Huang and Chunlan Jiang and Zhengwei Liu and Jinsong Wu},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.20879},
eprint = {2609.20879},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.20879},
}
RIS
TY - UNPB
TI - Equivalence of states and bimodule quantum channels
AU - Linzhe Huang
AU - Chunlan Jiang
AU - Zhengwei Liu
AU - Jinsong Wu
PY - 2026
DA - 2026/09/16
PB - arXiv
DO - 10.48550/arxiv.2609.20879
UR - https://arxiv.org/abs/2609.20879
AB - We study the action of quantum channels on states on a von Neumann algebra ℳ with conserved quantities encoded by a subalgebra 𝒩. We define a phase as an equivalence class of normal states on ℳ under the action of quantum channels preserving 𝒩. First, we establish a relative quasi-entropic characterization of phase equivalence using the Petz recovery map. We further introduce the operator algebra (OA) symmetry of a state and define an equivalence relation between OA symmetries via bishifts of biprojections. When 𝒩⊆ℳ is an irreducible finite-index subfactor of type II_1, we prove that phase equivalence implies OA symmetry equivalence. Consequently, OA symmetry breaking provides a sufficient mechanism for detecting phase transitions. Furthermore, combining finite-index subfactor theory with quantum Fourier analysis, we prove that the cardinality of each phase is finite and obtain an explicit upper bound depending only on the Jones index.
ER -