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

Theoretical and Mathematical Physics

A Priori Estimates for Quantum Dynamical Semigroups

Alexander Mikhailovich Chebotarev

Published Feb 1, 2003• 1 citation
Publisher
DOI
10.1023/a:1022219919058

Related papers

A priori estimates for a class of Quantum Dynamical Semigroups and applications

J. C. García, Roberto B. Quezada

Reporte interno - CINVESTAV•Jan 1, 1998•4 citations

A PRIORI ESTIMATES AND EXISTENCE THEOREMS FOR THE LINDBLAD EQUATION WITH UNBOUNDED TIME-DEPENDENT COEFFICIENTS(Recent Trends in Infinite Dimensional Non-Commutative Analysis)

Alexander Mikhailovich Chebotarev, Julio C. García, Roberto B. Quezada

We prove new a priori estimates for the resolvent of a class of minimal Quantum Dynamical Semigroup (QDS).These estimates simplify the proof of the unital property of QDS and suggest a continuity condition for time-dependent in- finitesimal generators to ensure existence and conservativity of the Markov master evolution equation. \S 1. INTRODUCTION.The theory of the Markov $\mathrm{m}\mathrm{a}s$ ter equation has been intensively studied dur- ing the recent years [1][2][3][4][5][6][7][8][9][10].Important applications of this theory were contributed to qu.antum chemistry [3] and quantum optics [4-6].Numerical Monte-Carlo and Runge-Kutta algorithms for these equations are discussed in [7-8].One of efficient analytical tools in the theory of master equation is the interaction representation technique [6-7], where the Markov $\mathrm{m}.$.aster equations with time-dependent coeffi- cients arise in a natural way.To study Markov $\mathrm{m}\mathrm{a}s$ ter equations with unbounded time-dependent coefficients describing evolution of observables from the algebra $B(\mathcal{H})$ of bounded operators or states from the algebra $\mathcal{T}(\mathcal{H})$ of operators with finite trace, we introduce the continuity conditions for the generator.We recall that one parameter contraction semigroup $P_{t}(\cdot)$ acting in $B(\mathcal{H})$ is called a Quantum Dynamical Semigroup (QDS) if it is completely positive, normal, conservative, and ultraweak continuous $[2, 11]$ .Normal and ultraweak continuity properties mean respectively that l.u.b. $P_{t}(xn)=P_{t}(1.\mathrm{u}.\mathrm{b}.x_{n})$ and $\mathrm{T}\mathrm{r}\{\rho(P_{t}(B)-$ $B)\}arrow 0$ as $tarrow \mathrm{O}$ for any $\rho\in \mathcal{T}(\mathcal{H})$ and $B\in B(\mathcal{H})$ .In the Heisenberg rep- resentation, the conservative (or unital) property means the conservation of the unit operator $I$ in the algebra $B(\mathcal{H})$ of observables: $P_{t}(I)\equiv I\forall t\geq 0$ ; in the Schr\"odinger representation, it means the conservation of the trace of an initial state $\rho\in \mathcal{T}(\mathcal{H})$ during the evolution: $\mathrm{T}\mathrm{r}T_{t}(\beta)\equiv \mathrm{b}\rho t\geq 0$ , where $T_{t}$ : $\mathcal{T}(\mathcal{H})arrow \mathcal{T}(\mathcal{H})$ and $P_{t}$ : $B(\mathcal{H})arrow B(\mathcal{H})$ are dual semigroups: $\mathrm{T}\mathrm{r}\{\tau_{t}(\rho)B\}=\mathrm{T}\mathrm{r}\{\rho P_{t}(B)\}$ .The semigroup $T_{t}=P_{t}^{1}$ is called the predual of the semigroup $P_{t}$ .The dagger "\dagger '' is used to denote predual operators and maps.The map. $P(\cdot)$ with the predual $P^{\uparrow}(\cdot)$ is referred to as a completely positive $(CP)$ if $\sum_{i,j}\mathrm{T}\mathrm{r}\{P(B_{i}^{*}B_{j})\sigma j\sigma_{i}\}*\geq 0$ or equivalently $\sum_{i,j}\mathrm{T}\mathrm{r}\{B^{*}iBjP^{\mathrm{t}}(\sigma_{j}\sigma_{i})*\}\geq 0$ (1.1)

•Apr 1, 1998•5 citations

On quantum dynamical semigroups

Wawrzyniec Guz

Reports on Mathematical Physics•Dec 1, 1974•7 citations

The classical limit for quantum dynamical semigroups

E. B. Davies

Communications in Mathematical Physics•Jun 1, 1976•20 citations

Perturbative Criteria for the Ergodicity of Interacting Dissipative Quantum Lattice Systems

Lorenzo Bertini, Alberto De Sole, Gustavo Posta +1 more

Abstract We analyze a class of quantum Feller semigroups describing the evolution of interacting quantum lattice systems, specified either as generic qudits or as fermions. The corresponding generators, which include both conservative and dissipative evolutions, are given by the superposition of local generators in the Lindblad form. The associated infinite volume dynamics can be obtained as the strong limit of the finite volume dynamics. By regarding the interacting evolution as a perturbation of a non-interacting dissipative dynamics, we obtain a quantitative criterion that yields the uniqueness of the stationary state together with the exponential convergence of local observables. The analysis is based on suitable a priori bounds on the resolvent equation which yield quantitive estimates on the evolution of local observables.

arXiv:2402.15488•Communications in Mathematical Physics•May 28, 2025•2 citations

Extension of quantum dynamical semigroups

Andrzej Posiewnik

Reports on Mathematical Physics•Jun 1, 1979•1 citation
We prove new a priori estimates for the resolvent of a class of minimal Quantum Dynamical Semigroup (QDS).These estimates simplify the proof of the unital property of QDS and suggest a continuity condition for time-dependent in- finitesimal generators to ensure existence and conservativity of the Markov master evolution equation. \S 1. INTRODUCTION.The theory of the Markov mas\mathrm{m}\mathrm{a}smas ter equation has been intensively studied dur- ing the recent years [1][2][3][4][5][6][7][8][9][10].Important applications of this theory were contributed to qu.antum chemistry [3] and quantum optics [4-6].Numerical Monte-Carlo and Runge-Kutta algorithms for these equations are discussed in [7-8].One of efficient analytical tools in the theory of master equation is the interaction representation technique [6-7], where the Markov m.\mathrm{m}.m..aster equations with time-dependent coeffi- cients arise in a natural way.To study Markov mas\mathrm{m}\mathrm{a}smas ter equations with unbounded time-dependent coefficients describing evolution of observables from the algebra B(H)B(\mathcal{H})B(H) of bounded operators or states from the algebra T(H)\mathcal{T}(\mathcal{H})T(H) of operators with finite trace, we introduce the continuity conditions for the generator.We recall that one parameter contraction semigroup Pt(⋅)P_{t}(\cdot)Pt​(⋅) acting in B(H)B(\mathcal{H})B(H) is called a Quantum Dynamical Semigroup (QDS) if it is completely positive, normal, conservative, and ultraweak continuous [2,11][2, 11][2,11] .Normal and ultraweak continuity properties mean respectively that l.u.b. Pt(xn)=Pt(1.u.b.xn)P_{t}(xn)=P_{t}(1.\mathrm{u}.\mathrm{b}.x_{n})Pt​(xn)=Pt​(1.u.b.xn​) and Tr{ρ(Pt(B)−\mathrm{T}\mathrm{r}\{\rho(P_{t}(B)-Tr{ρ(Pt​(B)− B)}arrow0B)\}arrow 0B)}arrow0 as tarrowOtarrow \mathrm{O}tarrowO for any ρ∈T(H)\rho\in \mathcal{T}(\mathcal{H})ρ∈T(H) and B∈B(H)B\in B(\mathcal{H})B∈B(H) .In the Heisenberg rep- resentation, the conservative (or unital) property means the conservation of the unit operator III in the algebra B(H)B(\mathcal{H})B(H) of observables: Pt(I)≡I∀t≥0P_{t}(I)\equiv I\forall t\geq 0Pt​(I)≡I∀t≥0 ; in the Schr\"odinger representation, it means the conservation of the trace of an initial state ρ∈T(H)\rho\in \mathcal{T}(\mathcal{H})ρ∈T(H) during the evolution: TrTt(β)≡bρt≥0\mathrm{T}\mathrm{r}T_{t}(\beta)\equiv \mathrm{b}\rho t\geq 0TrTt​(β)≡bρt≥0 , where TtT_{t}Tt​ : T(H)arrowT(H)\mathcal{T}(\mathcal{H})arrow \mathcal{T}(\mathcal{H})T(H)arrowT(H) and PtP_{t}Pt​ : B(H)arrowB(H)B(\mathcal{H})arrow B(\mathcal{H})B(H)arrowB(H) are dual semigroups: Tr{τt(ρ)B}=Tr{ρPt(B)}\mathrm{T}\mathrm{r}\{\tau_{t}(\rho)B\}=\mathrm{T}\mathrm{r}\{\rho P_{t}(B)\}Tr{τt​(ρ)B}=Tr{ρPt​(B)} .The semigroup Tt=Pt1T_{t}=P_{t}^{1}Tt​=Pt1​ is called the predual of the semigroup PtP_{t}Pt​ .The dagger "\dagger '' is used to denote predual operators and maps.The map. P(⋅)P(\cdot)P(⋅) with the predual P↑(⋅)P^{\uparrow}(\cdot)P↑(⋅) is referred to as a completely positive (CP)(CP)(CP) if ∑i,jTr{P(Bi∗Bj)σjσi}∗≥0\sum_{i,j}\mathrm{T}\mathrm{r}\{P(B_{i}^{*}B_{j})\sigma j\sigma_{i}\}*\geq 0∑i,j​Tr{P(Bi∗​Bj​)σjσi​}∗≥0 or equivalently ∑i,jTr{B∗iBjPt(σjσi)∗}≥0\sum_{i,j}\mathrm{T}\mathrm{r}\{B^{*}iBjP^{\mathrm{t}}(\sigma_{j}\sigma_{i})*\}\geq 0∑i,j​Tr{B∗iBjPt(σj​σi​)∗}≥0 (1.1)
Abstract We analyze a class of quantum Feller semigroups describing the evolution of interacting quantum lattice systems, specified either as generic qudits or as fermions. The corresponding generators, which include both conservative and dissipative evolutions, are given by the superposition of local generators in the Lindblad form. The associated infinite volume dynamics can be obtained as the strong limit of the finite volume dynamics. By regarding the interacting evolution as a perturbation of a non-interacting dissipative dynamics, we obtain a quantitative criterion that yields the uniqueness of the stationary state together with the exponential convergence of local observables. The analysis is based on suitable a priori bounds on the resolvent equation which yield quantitive estimates on the evolution of local observables.