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

Springer series in solid-state sciences

Quantum Theory in Liouville Space

Eugen Fick, Günter Sauermann

Published Jan 1, 1990• 0 citations
Publisher
DOI
10.1007/978-3-642-83715-9_3

Related papers

Classical and quantum statistical mechanics in a common Liouville space

S. Twareque Ali, Eduard Prugovečki

Physica A Statistical Mechanics and its Applications•Dec 1, 1977•53 citations

Lie Algebra and Liouville-Space Methods in Quantum Optics

Masashi Ban

CRC Press eBooks•Oct 8, 2018•0 citations

Liouville-space extension of quantum mechanics and N-body problems

Gonzalo E. Ordonez

•Jan 1, 1997•1 citation

Liouville space theory of sequential quantum processes. I. General theory

Bryan J. Dalton

The theory of sequential quantum processes has been extended to Liouville space via the use of non-Hermitian projection operators in order to treat the evolution of the quantum density operator and to enable physically important matrix elements of the density operator to be calculated. The formal relationship of master equation methods to the theory of sequential quantum processes is established, and a new set of coupled master equations is derived. Special choices of projection operators lead to further simplification of the results. The Markoff approximation is also examined.

Journal of Physics A Mathematical and General•Jul 1, 1982•23 citations

ON THE QUANTUM LIOUVILLE SPACE

Ioannis E. Antoniou, Z. Suchanecki

•Oct 1, 2004•2 citations

Rigged Liouville space formulation for quasi-Hermitian Liouville operators

Shousuke Ohmori, Junichi Takahashi

We discuss a super bra-ket formalism for quasi-Hermitian Liouvillian operators within the framework of rigged Hilbert spaces (RHS). An RHS in terms of the Liouville space, referred to as a rigged Liouville space (RLS), is reconstructed by exploiting the mathematical fact that the space of Hilbert-Schmidt operators is unitarily equivalent to the tensor product of Hilbert spaces. The obtained RLS endows a rigorous foundation of the construction for the super bra-ket and for the spectral decompositions of both Hermitian and quasi-Hermitian Liouville operators, which are characterized by the generalized eigenvectors in the dual spaces. Furthermore, within this framework, the non-Hermitian Liouvillian operator and its adjoint can be constructed symmetrically, with their symmetric structure preserved. As an application of our RLS methodology, we examine the Liouville operators corresponding to Hermitian and non-Hermitian harmonic oscillators and elucidate the differences between their spectral decomposition forms.

math-phCross-listedarXiv:2604.26322•Journal of Mathematical Physics•Apr 30, 2026•0 citations
The theory of sequential quantum processes has been extended to Liouville space via the use of non-Hermitian projection operators in order to treat the evolution of the quantum density operator and to enable physically important matrix elements of the density operator to be calculated. The formal relationship of master equation methods to the theory of sequential quantum processes is established, and a new set of coupled master equations is derived. Special choices of projection operators lead to further simplification of the results. The Markoff approximation is also examined.
We discuss a super bra-ket formalism for quasi-Hermitian Liouvillian operators within the framework of rigged Hilbert spaces (RHS). An RHS in terms of the Liouville space, referred to as a rigged Liouville space (RLS), is reconstructed by exploiting the mathematical fact that the space of Hilbert-Schmidt operators is unitarily equivalent to the tensor product of Hilbert spaces. The obtained RLS endows a rigorous foundation of the construction for the super bra-ket and for the spectral decompositions of both Hermitian and quasi-Hermitian Liouville operators, which are characterized by the generalized eigenvectors in the dual spaces. Furthermore, within this framework, the non-Hermitian Liouvillian operator and its adjoint can be constructed symmetrically, with their symmetric structure preserved. As an application of our RLS methodology, we examine the Liouville operators corresponding to Hermitian and non-Hermitian harmonic oscillators and elucidate the differences between their spectral decomposition forms.