Spectral-angular parametrization of open qudit dynamics
arXiv QuantumArchived Apr 15, 2026✓ Full text saved
arXiv:2604.11864v1 Announce Type: new Abstract: We present a parametrization of density matrices (mixed states) in a finite-dimensional Hilbert space $\mathbb{C}^n$, particularly suited to the description of their time evolution as open quantum systems governed by GKLS dynamics. A generic (non-degenerate) density matrix $rho_{\mathbf{r},\pmb{\phi}}$, characterized by $n^2-1$ real parameters, naturally decomposes into two sets: (i) an $(n-1)$-tuple $\mathbf{r}$ of spectral parameters, constrained
Full text archived locally
✦ AI Summary· Claude Sonnet
Quantum Physics
[Submitted on 13 Apr 2026]
Spectral-angular parametrization of open qudit dynamics
Jean-Pierre Gazeau, Kaoutar El Bachiri, Zakaria Bouameur, Yassine Hassouni
We present a parametrization of density matrices (mixed states) in a finite-dimensional Hilbert space \mathbb{C}^n, particularly suited to the description of their time evolution as open quantum systems governed by GKLS dynamics. A generic (non-degenerate) density matrix rho_{\mathbf{r},\pmb{\phi}}, characterized by n^2-1 real parameters, naturally decomposes into two sets: (i) an (n-1)-tuple \mathbf{r} of spectral parameters, constrained to lie in a convex polytope, and (ii) a set of n^2-n angular variables \pmb{\phi}, associated with the flag manifold \simeq \mathrm{SU}(n)/\mathbb{T}^{n-1}, where \mathbb{T}^{n-1} is the standard maximal diagonal torus, in the spirit of the Tilma--Sudarshan construction. A key observation is that the spectral parameters \mathbf{r} = (r_1, \ldots, r_{n-1}) admit a natural Lie-algebraic interpretation: they are precisely the simple root coordinates of the eigenvalue vector in the Cartan subalgebra of A_{n-1} = \mathfrak{sl}(n), with each r_i = p_i - p_{i+1} corresponding to the simple root \alpha_i = e_i - e_{i+1}. The convex polytope constraining \mathbf{r} is thus the positive Weyl chamber of A_{n-1}, and the full spectral domain R_{n-1} is the corresponding weight polytope. This parametrization leads to a partial decoupling of the dynamics: the evolution of the angular variables depends on both the Hamiltonian and the dissipative part of the Lindblad generator, whereas the evolution of the spectral parameters involves only the dissipative contribution. Low-dimensional examples for n=2 and n=3 are discussed in detail, including an application to the trichromatic structure of human colour perception, and we propose an alternative definition of purity expressed solely in terms of the spectral parameters \mathbf{r}.
Comments: 30 pages, 4 figures
Subjects: Quantum Physics (quant-ph)
MSC classes: 81P16, 81R05, 81R30, 81S22
Cite as: arXiv:2604.11864 [quant-ph]
(or arXiv:2604.11864v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2604.11864
Focus to learn more
Submission history
From: Jean Pierre Gazeau [view email]
[v1] Mon, 13 Apr 2026 16:02:24 UTC (30 KB)
Access Paper:
HTML (experimental)
view license
Current browse context:
quant-ph
< prev | next >
new | recent | 2026-04
References & Citations
INSPIRE HEP
NASA ADS
Google Scholar
Semantic Scholar
Export BibTeX Citation
Bookmark
Bibliographic Tools
Bibliographic and Citation Tools
Bibliographic Explorer Toggle
Bibliographic Explorer (What is the Explorer?)
Connected Papers Toggle
Connected Papers (What is Connected Papers?)
Litmaps Toggle
Litmaps (What is Litmaps?)
scite.ai Toggle
scite Smart Citations (What are Smart Citations?)
Code, Data, Media
Demos
Related Papers
About arXivLabs
Which authors of this paper are endorsers? | Disable MathJax (What is MathJax?)