{ "id": "2204.07734", "version": "v1", "published": "2022-04-16T07:03:54.000Z", "updated": "2022-04-16T07:03:54.000Z", "title": "The Franke-Gorini-Kossakowski-Lindblad-Sudarshan (FGKLS) Equation for Two-Dimensional Systems", "authors": [ "Alexander A. Andrianov", "Mikhail V. Ioffe", "Ekaterina A. Izotova", "Oleg O. Novikov" ], "comment": "27 p.p", "journal": "Symmetry, 14 (2022) 754", "doi": "10.3390/sym14010754", "categories": [ "quant-ph", "hep-th", "math-ph", "math.MP" ], "abstract": "Open quantum systems are, in general, described by a density matrix that is evolving under transformations belonging to a dynamical semigroup. They can obey the Franke-Gorini-Kossakowski-Lindblad-Sudarshan (FGKLS) equation. We exhaustively study the case of a Hilbert space of dimension $2$. First, we find final fixed states (called pointers) of an evolution of an open system, and we then obtain a general solution to the FGKLS equation and confirm that it converges to a pointer. After this, we check that the solution has physical meaning, i.e., it is Hermitian, positive and has trace equal to $1$, and find a moment of time starting from which the FGKLS equation can be used - the range of applicability of the semigroup symmetry. Next, we study the behavior of a solution for a weak interaction with an environment and make a distinction between interacting and non-interacting cases. Finally, we prove that there cannot exist oscillating solutions to the FGKLS equation, which would resemble the behavior of a closed quantum system.", "revisions": [ { "version": "v1", "updated": "2022-04-16T07:03:54.000Z" } ], "analyses": { "keywords": [ "two-dimensional systems", "fgkls equation", "franke-gorini-kossakowski-lindblad-sudarshan", "open quantum systems", "density matrix" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }