2009
DOI: 10.1007/s00023-009-0017-8
|View full text |Cite
|
Sign up to set email alerts
|

Repeated and Continuous Interactions in Open Quantum Systems

Abstract: We consider a finite quantum system S coupled to two environments of different nature. One is a heat reservoir R (continuous interaction) and the other one is a chain C of independent quantum systems E (repeated interaction). The interactions of S with R and C lead to two simultaneous dynamical processes. We show that for generic such systems, any initial state approaches an asymptotic state in the limit of large times. We express the latter in terms of the resonance data of a reduced propagator of S + R and s… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
18
0

Year Published

2013
2013
2022
2022

Publication Types

Select...
7
1

Relationship

2
6

Authors

Journals

citations
Cited by 13 publications
(18 citation statements)
references
References 29 publications
0
18
0
Order By: Relevance
“…The reservoir R is a thermal reservoir of free Fermi particles at a temperature T R > 0, in the thermodynamic limit. Its description was originally given in the work by Araki and Wyss [AW] (see also [JP2,BJM4]). The Hilbert space is the anti-symmetric Fock space B(H R ) = Γ − (h) where G is an 'auxiliary space' (typically an angular part like L 2 (S 2 )).…”
Section: The Additional Reservoirmentioning
confidence: 99%
“…The reservoir R is a thermal reservoir of free Fermi particles at a temperature T R > 0, in the thermodynamic limit. Its description was originally given in the work by Araki and Wyss [AW] (see also [JP2,BJM4]). The Hilbert space is the anti-symmetric Fock space B(H R ) = Γ − (h) where G is an 'auxiliary space' (typically an angular part like L 2 (S 2 )).…”
Section: The Additional Reservoirmentioning
confidence: 99%
“…The literature on repeated interaction systems we are aware of can be classified into two categories. In a first one, effective evolution equations are derived by taking continuous interaction limits [5,6,2,3,33,34,21] and in a second category, the dynamics is left discrete, but the time-asymptotics is investigated [11,12,13,14,8,9,22,31]. To our knowledge, repeated interaction systems have been first proposed in [27,28] and in [5,6] as approximations for system-environment type models, where it is proven that the discrete evolution converges to that of a quantum Langevin equation, in the limit of ever shorter system-probe interaction times.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The eigenvalues m of M are the possible measurement outcomes. Due to finite dimensionality, the random variables X n have finite range.The present work can be viewed as the continuation of recently developed techniques for the mathematical analysis of repeated interaction quantum systems [11,12,13,14]. In these references, asymptotic properties of the scatterer have been investigated, without considering the fate of the outcoming probes, and without quantum measurements.…”
mentioning
confidence: 99%
“…We remark that the setup specified so far is identical to the framework of repeated interactions or collisional models as considered in Refs. [17,[45][46][47]. Next, we want to explicitly include measurements and conditioning in the description.…”
Section: Autonomous Modelmentioning
confidence: 99%