Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:2312.01094 · Quantum Information Processing

On reconstruction of states from evolution induced by quantum dynamical semigroups perturbed by covariant measures

Grigori Gennadievich Amosov, Egor Leonidovich Baitenov, Alexander Nikolaevich Pechen

Published Nov 4, 2023• 1 citation
arXivHTMLPDF
DOI
10.1007/s11128-023-04162-3

Related papers

Covariant quantum dynamical semigroups: Unbounded generators

A. S. Holevo

arXiv:quant-ph/9701037•Springer eBooks•Apr 6, 2008•16 citations

On conservativity of covariant dynamical semigroups

Alexander Semenovich Holevo

Reports on Mathematical Physics•Aug 1, 1993•39 citations

On the Structure of Covariant Dynamical Semigroups

Alexander Semenovich Holevo

Journal of Functional Analysis•Aug 1, 1995•45 citations

A note on covariant dynamical semigroups

Alexander Semenovich Holevo

Reports on Mathematical Physics•Apr 1, 1993•104 citations

RECONSTRUCTION THEOREM FOR STATIONARY MONOTONE QUANTUM MARKOV PROCESSES

Jaeseong Heo, V. P. Belavkin, Un Cig Ji

Based on the Hilbert $C^*$ -module structure we study the reconstruction theorem for stationary monotone quantum Markov processes from quantum dynamical semigroups. We prove that the quantum stochastic monotone process constructed from a covariant quantum dynamical semigroup is again covariant in the strong sense.

Bulletin of the Korean Mathematical Society•Jan 31, 2012•5 citations

HTSD operators and local measurement theory in locally covariant quantum field theory

Christoph Hartmann

This paper is part of a broader project on the Hartmann Operator Geometry (HTSD) developed in the monograph “The Hartmann Operator Geometry – Volume I”. This preprint investigates the reduced Heisenberg evolution induced by local system–probe measurements in the Fewster–Verch framework of locally covariant quantum field theory. Starting from locally covariant system and probe functors and a local coupling in a compact region, the work considers the induced completely positive unital maps on the system algebra and assumes a weak–coupling / short–time regime that yields a norm–continuous Markovian semigroup. Under this local Markovianity assumption, the generator of the reduced dynamics is shown to have a purely diffusion–type Lindblad form built from finitely many selfadjoint “pointer” observables. Each pointer observable defines a local inner derivation, and the generator can be written as a Laplace–type operator of HTSD form, i.e. as a quadratic combination of these derivations. In this way, HTSD operator geometry appears as a natural differential structure underlying local measurement dynamics in locally covariant AQFT, with an associated Dirichlet form and curvature tensor encoding energy and non-integrability properties of the measurement–induced evolution.

•Nov 24, 2025•0 citations
Based on the Hilbert C∗C^*C∗ -module structure we study the reconstruction theorem for stationary monotone quantum Markov processes from quantum dynamical semigroups. We prove that the quantum stochastic monotone process constructed from a covariant quantum dynamical semigroup is again covariant in the strong sense.
This paper is part of a broader project on the Hartmann Operator Geometry (HTSD) developed in the monograph “The Hartmann Operator Geometry – Volume I”. This preprint investigates the reduced Heisenberg evolution induced by local system–probe measurements in the Fewster–Verch framework of locally covariant quantum field theory. Starting from locally covariant system and probe functors and a local coupling in a compact region, the work considers the induced completely positive unital maps on the system algebra and assumes a weak–coupling / short–time regime that yields a norm–continuous Markovian semigroup. Under this local Markovianity assumption, the generator of the reduced dynamics is shown to have a purely diffusion–type Lindblad form built from finitely many selfadjoint “pointer” observables. Each pointer observable defines a local inner derivation, and the generator can be written as a Laplace–type operator of HTSD form, i.e. as a quadratic combination of these derivations. In this way, HTSD operator geometry appears as a natural differential structure underlying local measurement dynamics in locally covariant AQFT, with an associated Dirichlet form and curvature tensor encoding energy and non-integrability properties of the measurement–induced evolution.