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Main Authors: Arzano, Michele, Del Prete, Antonio, Frattulillo, Domenico
Format: Preprint
Published: 2026
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Online Access:https://arxiv.org/abs/2602.07887
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author Arzano, Michele
Del Prete, Antonio
Frattulillo, Domenico
author_facet Arzano, Michele
Del Prete, Antonio
Frattulillo, Domenico
contents In recent years, growing attention has been devoted to the possibility that theories with deformed symmetries, associated with certain models of non-commutative spacetime, may encode a fundamental form of decoherence. This effect should be described by a Lindblad-like evolution governed by the non-trivial Hopf algebra structure of the time-evolution generators. In this work we provide a detailed analysis of such possibility for similar Hopf algebra deformations of the Hamiltonian of a qubit. Starting from a critical examination of the very definition of time evolution through the generalized adjoint action, we explore whether a coherent and physically viable framework can be established. In particular, our analysis shows that a more general combination of adjoint actions always guarantees a von Neumann dynamics and, also in the case of deformed spacetime symmetries considered in the literature, a physically viable Lindblad evolution cannot be established.
format Preprint
id arxiv_https___arxiv_org_abs_2602_07887
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Quantum Evolution of Hopf Algebra Hamiltonians
Arzano, Michele
Del Prete, Antonio
Frattulillo, Domenico
Quantum Physics
General Relativity and Quantum Cosmology
High Energy Physics - Theory
In recent years, growing attention has been devoted to the possibility that theories with deformed symmetries, associated with certain models of non-commutative spacetime, may encode a fundamental form of decoherence. This effect should be described by a Lindblad-like evolution governed by the non-trivial Hopf algebra structure of the time-evolution generators. In this work we provide a detailed analysis of such possibility for similar Hopf algebra deformations of the Hamiltonian of a qubit. Starting from a critical examination of the very definition of time evolution through the generalized adjoint action, we explore whether a coherent and physically viable framework can be established. In particular, our analysis shows that a more general combination of adjoint actions always guarantees a von Neumann dynamics and, also in the case of deformed spacetime symmetries considered in the literature, a physically viable Lindblad evolution cannot be established.
title Quantum Evolution of Hopf Algebra Hamiltonians
topic Quantum Physics
General Relativity and Quantum Cosmology
High Energy Physics - Theory
url https://arxiv.org/abs/2602.07887